Author name code: altrock ADS astronomy entries on 2022-09-14 author:"Altrock, Richard C." ------------------------------------------------------------------------ Title: Deciphering Solar Magnetic Activity: 140 Years of the `Extended Solar Cycle' - Mapping the Hale Cycle Authors: McIntosh, Scott W.; Leamon, Robert J.; Egeland, Ricky; Dikpati, Mausumi; Altrock, Richard C.; Banerjee, Dipankar; Chatterjee, Subhamoy; Srivastava, Abhishek K.; Velli, Marco Bibcode: 2021SoPh..296..189M Altcode: 2020arXiv201006048M We investigate the occurrence of the "extended solar cycle" (ESC) as it occurs in a host of observational data spanning 140 years. Investigating coronal, chromospheric, photospheric, and interior diagnostics, we develop a consistent picture of solar activity migration linked to the 22-year Hale (magnetic) cycle using superposed epoch analysis (SEA) and previously identified Hale cycle termination events as the key time for the SEA. Our analysis shows that the ESC and Hale cycle, as highlighted by the terminator-keyed SEA, is strongly recurrent throughout the entire observational record studied, some 140 years. Applying the same SEA method to the sunspot record confirms that Maunder's butterfly pattern is a subset of the underlying Hale cycle, strongly suggesting that the production of sunspots is not the fundamental feature of the Hale cycle, but the ESC is. The ESC (and Hale cycle) pattern highlights the importance of 55 latitude in the evolution, and possible production, of solar magnetism. Title: Fe XIV Synoptic Observations as a Predictor for the Time of Solar Maximum in Cycle 24 Authors: Altrock, Richard Bibcode: 2015TESS....130805A Altcode: In 2012 (Am. Geophys. Union Fall Meeting, Abstract SH12A-05) and 2013 (Solar Phys. Online First, DOI 10.1007/s11207-012-0216-1) Altrock discussed the status of Cycle 24 relative to synoptic observations ofFe XIV from Sacramento Peak (http://nsosp.nso.edu/corona). He found that using earlier cycles, in which solar maximum occurred when Fe XIV emission features associated with the classic "Rush to the Poles" reached latitudes 76 ± 2 degrees, the *northern hemisphere* Fe XIV features predicted a maximum in the north at 2011.6 ± 0.3. This was confirmed by hemispheric sunspot numbers from SIDC (http://www.sidc.be/silso/) and sunspot areas from NASA MSFC http://solarscience.msfc.nasa.gov/greenwch.shtml). The earlier papersalso noted that southern high-latitude Fe XIV emission indicated the possibility of a southern maximum early in 2014. At low latitudes, earlier cycles reached solar maximum when Fe XIV emission features reached latitudes 20 ± 1.7 degrees. In 2013, these features were at 21 and 15 degrees in the north, again indicating that northern maximum had already occurred. In the south, the Fe XIV features were at 24 degrees. Gopalswamy et al. (2012, Ap. J. Let. 750:L42) come to similar conclusions from a study of microwave brightness and prominence eruptions. This paper will extend the previous studies up to 2014 to include the recent extraordinary surge of activity in the southern hemisphere. In particular we will examine in more detail the relationship between hemispheric Fe XIV emission features and both global and hemispheric sunspot numbers to see (i) if the previous studies correctly predicted the times of hemispheric solar maxima and (ii) what we can learn from the inclusion of two more years of data. The observations used herein are the result of a cooperative program of the Air Force Research Laboratory and the National Solar Observatory. Title: Solar Coronal Temperature During the Rise of Cycle 24 Authors: Altrock, Richard C. Bibcode: 2014AAS...22432332A Altcode: Observations of the solar corona are obtained with the photoelectric coronal photometer fed by the 40-cm coronagraph in the John W. Evans Solar Facility at the National Solar Observatory at Sacramento Peak in Sunspot, NM. The observations consist of daily scans every 3° in latitude at 1.15 solar radii in Fe XIV 530.3 nm and Fe X 637.4 nm. The scans were obtained from 1983 to 2013. The coronal temperature (Tc) may be calculated as a function of the ratio of the intensities of Fe XIV and Fe X, as shown by Guhathakurta, Fisher and Altrock (1993, Astrophys. J. Lett., 414, L145). In this paper, I use this technique to study the long-term, large-scale variation of Tc over the last 3 solar cycles. The observations are used to determine the variation of Tc at latitudes above 30°. Latitudes below 30° are not studied, because the technique used to determine Tc is not applicable to active regions, where the assumption of a uniform temperature along the line-of-sight is denied by the presence of many active-region loops of varying temperatures. Suitable temporal averages are taken to reduce noise.Prior to the last solar minimum we find that (i) a well-defined solar-cycle variation of Tc at 1.15 Ro was seen, varying by 0.4 MK near the poles, (ii) Tc near solar minimum decreased strongly toward thepoles above 60° latitude, and (iii) a variation ~ 0.1 MK was seen in the average Tc above 30° latitude.However, since the last solar maximum, we show that the pattern established during the previous two cycles was broken. The most important new conclusions are Tc since minimum reached maximum earlier in the North than in the South, and Tc at the maximum of Cycle 24 is significantly lower than in previous cycles. We also found that (i) the polar Tc only decreased by 0.3 MK from solar maximum to minimum instead of 0.4 MK, (ii) Tc near solar minimum did not decrease strongly toward the poles above 60° latitude, which it did in earlier cycles, (iii) the average Tc above 30° latitude reached a record low value of 1.4 MK, but the minimum polar Tc was 0.13 MK hotter than the previous cycle, and (iv) the latitude-variation of Tc at solar minimum was less than 0.1 MK. Title: Forecasting the Maxima of Solar Cycle 24 with Coronal Fe XIV Emission Authors: Altrock, Richard C. Bibcode: 2014SoPh..289..623A Altcode: 2012arXiv1209.2963A The onset of the "Rush to the Poles" of polar-crown prominences and their associated coronal emission is a harbinger of solar maximum. Altrock (Solar Phys.216, 343, 2003) showed that the "Rush" was well observed at 1.15 Ro in the Fe XIV corona at the Sacramento Peak site of the National Solar Observatory prior to the maxima of Cycles 21 to 23. The data show that solar maximum in those cycles occurred when the center line of the Rush reached a critical latitude of 76±2. Furthermore, in the previous three cycles solar maximum occurred when the highest number of Fe XIV emission features per day (averaged over 365 days and both hemispheres) first reached latitudes 20±1.7. Applying the above conclusions to Cycle 24 is difficult due to the unusual nature of this cycle. Cycle 24 displays an intermittent Rush that is only well-defined in the northern hemisphere. In 2009 an initial slope of 4.6 year−1 was found in the north, compared to an average of 9.4±1.7 year−1 in the previous cycles. An early fit to the Rush would have reached 76 at 2014.6. However, in 2010 the slope increased to 7.5 year−1 (an increase did not occur in the previous three cycles). Extending that rate to 76±2 indicates that the solar maximum in the northern hemisphere already occurred at 2011.6±0.3. In the southern hemisphere the Rush to the Poles, if it exists, is very poorly defined. A linear fit to several maxima would reach 76 in the south at 2014.2. In 1999, persistent Fe XIV coronal emission known as the "extended solar cycle" appeared near 70 in the North and began migrating towards the equator at a rate 40 % slower than the previous two solar cycles. However, in 2009 and 2010 an acceleration occurred. Currently the greatest number of emission features is at 21 in the North and 24 in the South. This indicates that solar maximum is occurring now in the North but not yet in the South. Title: The 2011 Northern Hemisphere Solar Maximum Authors: Altrock, Richard C. Bibcode: 2013AAS...22141505A Altcode: Altrock (1997, Solar Phys. 170, 411) discusses a process in which Fe XIV 530.3 nm emission features appear at high latitudes and gradually migrate towards the equator, merging with the sunspot "butterfly diagram". In cycles 21 - 23 solar maximum occurred when the number of Fe XIV emission regions per day > 0.19 (averaged over 365 days and both hemispheres) first reached latitudes 18°, 21° and 21°, for an average of 20° ± 1.7°. Another high-latitude process is the "Rush to the Poles" of polar crown prominences and their associated coronal emission, including Fe XIV. The Rush is a harbinger of solar maximum (cf. Altrock, 2003, Solar Phys. 216, 343). Solar maximum in cycles 21 - 23 occurred when the center line of the Rush reached a critical latitude. These latitudes were 76°, 74° and 78°, respectively, for an average of 76° ± 2°. Cycle 24 displays an intermittent Rush that is only well-defined in the northern hemisphere. In 2009 an initial slope of 4.6°/yr was found in the north, compared to an average of 9.4 ± 1.7 °/yr in the previous three cycles. However, in 2010 the slope increased to 7.5°/yr. Extending that rate to 76° ± 2° indicates that the solar maximum smoothed sunspot number in the northern hemisphere already occurred at 2011.6 ± 0.3. In the southern hemisphere the Rush is very poorly defined. A linear fit to several maxima would reach 76° in the south at 2014.2. In 1999, persistent Fe XIV coronal emission connected with the ESC appeared near 70° in the north and began migrating towards the equator at a rate 40% slower than the previous two solar cycles. A fit to the early ESC would not reach 20° until 2019.8. However, in 2009 and 2010 an acceleration occurred. Currently the greatest number of emission regions is at 21° in the north and 24°in the south. This indicates that solar maximum is occurring now in the north but not yet in the south. The latest global smoothed sunspot numbers show an inflection point in late 2011, which could represent solar maximum in the northern hemisphere. Sunspot areas in the northern hemisphere reached a maximum in late 2011. The southern areas are still increasing. Title: The Extended Solar Cycle Tracked High into the Corona Authors: Tappin, S. J.; Altrock, R. C. Bibcode: 2013SoPh..282..249T Altcode: 2012arXiv1209.2969T; 2012SoPh..tmp..241T We present observations of the extended solar cycle activity in white-light coronagraphs, and compare them with the more familiar features seen in the Fe XIV green-line corona. We show that the coronal activity zones seen in the emission corona can be tracked high into the corona. The peak latitude of the activity, which occurs near solar maximum, is found to be very similar at all heights. But we find that the equatorward drift of the activity zones is faster at greater heights, and that during the declining phase of the solar cycle, the lower branch of activity (that associated with the current cycle) disappears at about 3R. This implies that during the declining phase of the cycle, the solar wind detected near Earth is likely to be dominated by the next cycle. The so-called "rush to the poles" is also seen in the higher corona. In the higher corona it is found to start at a similar time but at lower latitudes than in the green-line corona. The structure is found to be similar to that of the equatorward drift. Title: Coronal Activity and Extended Solar Cycles Authors: Altrock, R. C. Bibcode: 2012AGUFMSH12A..05A Altcode: Wilson et al. (1988, Nature 333, 748) discussed a number of solar parameters, which appear at high latitudes and gradually migrate towards the equator, merging with the sunspot "butterfly diagram". They found that this concept had been identified by earlier investigators extending back to 1957. They named this process the "Extended Solar Cycle" (ESC). Altrock (1997, Solar Phys. 170, 411) found that this process continued in Fe XIV 530.3 nm emission features. In cycles 21 - 23 solar maximum occurred when the number of Fe XIV emission regions per day > 0.19 (averaged over 365 days and both hemispheres) first reached latitudes 18°, 21° and 21°, for an average of 20° ± 1.7°. Other recent studies have shown that Torsional Oscillation (TO) negative-shear zones are co-located with the ESC from at least 50° down to the equator and also in the zones where the Rush to the Poles occur. These phenomena indicate that coronal activity occurring up to 50° and higher latitudes is related to TO shear zones, another indicator that the ESC is an important solar process. Another high-latitude process, which appears to be connected with the ESC, is the "Rush to the Poles" ("Rush") of polar crown prominences and their associated coronal emission, including Fe XIV. The Rush is is a harbinger of solar maximum (cf. Altrock, 2003, Solar Phys. 216, 343). Solar maximum in cycles 21 - 23 occurred when the center line of the Rush reached a critical latitude. These latitudes were 76°, 74° and 78°, respectively, for an average of 76° ± 2°. Applying the above conclusions to Cycle 24 is difficult due to the unusual nature of this cycle. Cycle 24 displays an intermittent "Rush" that is only well-defined in the northern hemisphere. In 2009 an initial slope of 4.6°/yr was found in the north, compared to an average of 9.4 ± 1.7 °/yr in the previous three cycles. This early fit to the Rush would have reached 76° at 2014.6. However, in 2010 the slope increased to 7.5°/yr (an increase did not occur in the previous three cycles). Extending that rate to 76° ± 2° indicates that the solar maximum smoothed sunspot number in the northern hemisphere already occurred at 2011.6 ± 0.3. In the southern hemisphere the Rush to the Poles, if it exists, is very poorly defined. A linear fit to several maxima would reach 76° in the south at 2014.2. In 1999, persistent Fe XIV coronal emission connected with the ESC appeared near 70° in the north and began migrating towards the equator at a rate 40% slower than the previous two solar cycles. A fit to the early ESC would not reach 20° until 2019.8. However, in 2009 and 2010 an acceleration occurred. Currently the greatest number of emission regions is at 21° in the north and 24°in the south. This indicates that solar maximum is occurring now in the north but not yet in the south. Gopalswamy et al. (2012, Ap. J. Let. 752, L42 1919) come to similar conclusions from a study of microwave brightness and prominence eruptions. The latest global smoothed sunspot numbers show an inflection point in late 2011, which could represent solar maximum in the northern hemisphere. The observations used herein are the result of a cooperative program of the Air Force Research Laboratory and the National Solar Observatory. Title: Cycle 24 Northern-Hemisphere Solar Maximum Observed in Fe XIV Authors: Altrock, Richard C. Bibcode: 2012AAS...22012303A Altcode: The onset of the "Rush to the Poles" of polar crown prominences and their associated coronal emission is a harbinger of solar maximum. Altrock (2003, Solar Phys. 216, 343) showed that the "Rush" was well-observed in the the Fe XIV corona at the Sacramento Peak site of the National Solar Observatory prior to the maxima of Cycles 21 to 23. He found that solar maximum in those cycles occurred when the center line of the Rush reached a critical latitude. These latitudes were 76°, 74° and 78°, respectively, for an average of 76° ± 2°.

Applying this method to Cycle 24 is difficult due to the unusual nature of this cycle. Cycle 24 displays an intermittent "Rush" that is only definable in the northern hemisphere. In 2009 an initial slope of 4.6°/yr was found, compared to an average of 9.4 ± 1.7 °/yr in the previous cycles. However, in 2010 the slope increased to 7.5°/yr (an increase did not occur in the previous three cycles). Extending that rate to 76° ± 2° indicates that the maximum smoothed sunspot number in the northern hemisphere ALREADY OCCURRED at 2011.6 ± 0.3. Unfortunately, the smoothed sunspot number uses 12-month running means, so the result may not be testable for several more months. Solar maximum may not be detectable in the southern hemisphere. Title: Coronal Fe XIV Emission During the Whole Heliosphere Interval Campaign Authors: Altrock, Richard C. Bibcode: 2011SoPh..274..251A Altcode: 2011arXiv1106.3998A Solar Cycle 24 is having a historically long and weak start. Observations of the Fe XIV corona from the Sacramento Peak site of the National Solar Observatory show an abnormal pattern of emission compared to observations of Cycles 21, 22, and 23 from the same instrument. The previous three cycles have shown a strong, rapid "Rush to the Poles" (previously observed in polar crown prominences and earlier coronal observations) in the parameter N(t,l,dt) (average number of Fe XIV emission features per day over dt days at time t and latitude l). Cycle 24 displays a weak, intermittent, and slow "Rush" that is apparent only in the northern hemisphere. If the northern Rush persists at its current rate, evidence from the Rushes in previous cycles indicates that solar maximum will occur in early 2013 or late 2012, at least in the northern hemisphere. At lower latitudes, solar maximum previously occurred when the time maximum of N(t,l,365) reached approximately 20° latitude. Currently, this parameter is at or below 30° and decreasing in latitude. Unfortunately, it is difficult at this time to calculate the rate of decrease in N(t,l,365). However, the southern hemisphere could reach 20° in 2011. Nonetheless, considering the levels of activity so far, there is a possibility that the maximum could be indiscernible. Title: Solar Coronal Temperature and Line Emission During the Long Minimum and the Rise of Cycle 24 Authors: Altrock, R. C. Bibcode: 2011AGUFMSH33A2029A Altcode: Solar Cycle 24 had a weak start following an extraordinarily long minimum. Observations of the Fe XIV corona from the Sacramento Peak site of the National Solar Observatory showed an abnormal pattern of emission compared to observations of Cycles 21, 22, and 23 from the same instrument. The previous three cycles had a strong, rapid "Rush to the Poles" in Fe XIV. Cycle 24 displays a delayed, weak, intermittent, and slow "Rush" that is mainly apparent in the northern hemisphere. This paper discusses (i) the characteristics of emission from Fe XIV and other coronal ions and (ii) the coronal temperature calculated from the NSO observations in order to further characterize coronal conditions during this epoch and their implications for Cycle 24 maximum. Title: The slow rise of Cycle 24 as seen in Fe XIV Authors: Altrock, Richard C. Bibcode: 2011shin.confE.150A Altcode: Solar Cycle 24 had a historically prolonged and weak start. Observations of the Fe XIV corona from the Sacramento Peak site of the National Solar Observatory showed an abnormal pattern of emission compared to observations of Cycles 21, 22, and 23 from the same instrument. The previous three cycles had a strong, rapid Rush to the Poles" in Fe XIV. Cycle 24 displays a delayed, weak, intermittent, and slow "Rush" that is mainly apparent in the northern hemisphere. If this Rush persists at its current rate, evidence from previous cycles indicates that solar maximum will occur in approximately early 2013. At lower latitudes, solar maximum previously occurred when the greatest number of Fe XIV emission regions* first reached approximately 20° latitude. Currently, the value of this parameter at 20° is approximately 0.15. Previous behavior of this parameter indicates that solar maximum should occur in approximately two years, or 2013. Thus, both techniques yield an expected time of solar maximum in early 2013.

*annual average number of Fe XIV emission features per day > 0.19 Title: Torsional Oscillations and Coronal Activity Authors: Altrock, Richard C. Bibcode: 2011shin.confE...8A Altcode: Howe et al. (2009) demonstrate that solar activity appears to move towards the equator somewhat parallel to the latitude motion of torsional oscillation flows. However, Snodgrass (1987) had previously suggested that the regions between the fast and slow torsional oscillation flows represent zones where magnetic field is concentrated, which results in the formation of activity. In an attempt to test this suggestion, Altrock et al. (2008) compared the location of bright Fe XIV coronal regions to the latitude derivative of torsional oscillation frequencies and found that the bright regions occurred over regions where the latitude derivative was at its lowest (negative) value; i.e., between the fast and slow streams, thus verifying Snodgrass' suggestion. This paper extends and verifies the results of Altrock et al., that solar activity occurs over the "shear" zone between fast and slow torsional oscillation flows. Title: Whither goes Cycle 24? A View from the Fe XIV Corona Authors: Altrock, Richard C. Bibcode: 2011SPD....42.1804A Altcode: 2011BAAS..43S.1804A Solar Cycle 24 had a historically prolonged and weak start. Observations of the Fe XIV corona from the Sacramento Peak site of the National Solar Observatory showed an abnormal pattern of emission compared to observations of Cycles 21, 22, and 23 from the same instrument. The previous three cycles had a strong, rapid "Rush to the Poles" in Fe XIV. Cycle 24 displays a delayed, weak, intermittent, and slow "Rush" that is mainly apparent in the northern hemisphere. If this Rush persists at its current rate, evidence from previous cycles indicates that solar maximum will occur in approximately early 2013. At lower latitudes, solar maximum previously occurred when the greatest number of Fe XIV emission regions* first reached approximately 20° latitude. Currently, the value of this parameter at 20° is approximately 0.15. Previous behavior of this parameter indicates that solar maximum should occur in approximately two years, or 2013. Thus, both techniques yield an expected time of solar maximum in early 2013.

*annual average number of Fe XIV emission features per day greater than 0.19 Title: What is the relationship between solar torsional oscillations and solar activity? Authors: Altrock, R. C. Bibcode: 2010AGUFMSH53B..04A Altcode: Howe et al. (2009) demonstrate that solar activity appears to move towards the equator somewhat parallel to the latitude motion of torsional oscillation flows. However, Snodgrass (1987) had previously suggested that the regions between the fast and slow torsional oscillation flows represent zones where magnetic field is concentrated, which results in the formation of activity. In an attempt to test this suggestion, Altrock et al. (2008) compared the location of bright Fe XIV coronal regions to the latitude derivative of torsional oscillation frequencies and found that the bright regions occurred over regions where the latitude derivative was at its lowest (negative) value; i.e., between the fast and slow streams, thus verifying Snodgrass' suggestion. This paper extends and verifies the results of Altrock et al., that SOLAR ACTIVITY OCCURS OVER THE ``SHEAR'' ZONE BETWEEN FAST AND SLOW TORSIONAL OSCILLATION FLOWS. References: Howe, R., et al., ApJ Letters 701, L87, 2009; Snodgrass, H., ApJ 316, L91, 1987; Altrock, R., et al., ASPCS 363, 335, 2008. Thanks to R. Howe and R. Ulrich for providing their torsional oscillation data. Fe XIV coronal bright regions (shading) and MWO torsional oscillation latitude derivative (contours) from 1982 to 2007. Title: What happened to Cycle 24? Evidence from the Fe XIV corona. Authors: Altrock, Richard C. Bibcode: 2010shin.confE.151A Altcode: Cycle 24 is having a historically long and weak start. Observations of the Fe XIV corona from the Sacramento Peak site of the National Solar Observatory show a peculiar pattern of emission, when compared to observations of cycles 21, 22 and 23 from the same instrument. The previous three cycles have shown a strong, rapid Title: The Progress of Solar Cycle 24 at High Latitudes Authors: Altrock, R. C. Bibcode: 2010ASPC..428..147A Altcode: 2010arXiv1002.2401A The "extended" solar cycle 24 began in 1999 near 70° latitude, similarly to cycle 23 in 1989 and cycle 22 in 1979. The extended cycle is manifested by persistent Fe XIV coronal emission appearing near 70° latitude and slowly migrating towards the equator, merging with the latitudes of sunspots and active regions (the "butterfly diagram") after several years. Cycle 24 began its migration at a rate 40% slower than the previous two solar cycles, thus indicating the possibility of a peculiar cycle. However, the onset of the "Rush to the Poles" of polar crown prominences and their associated coronal emission, which has been a precursor to solar maximum in recent cycles (cf. Altrock 2003), has just been identified in the northern hemisphere. Peculiarly, this "rush" is leisurely, at only 50% of the rate in the previous two cycles. The properties of the current "Rush to the Poles" yields an estimate of 2013 or 2014 for solar maximum. Title: High-Latitude Coronal Fe XIV Emission During the Long Minimum and its Implications for Cycle 24 Authors: Altrock, Richard C. Bibcode: 2010AAS...21640102A Altcode: 2010BAAS...41..857A The "extended" solar cycle 24 began in 1999 near 70° latitude, similarly to cycle 23 in 1989 and cycle 22 in 1979. The extended cycle is manifested by persistent Fe XIV coronal emission appearing near 70° latitude and slowly migrating towards the equator, merging with the latitudes of sunspots and active regions (the "butterfly diagram") after several years. Cycle 24 began its migration at a rate 40% slower than the previous two solar cycles, thus indicating the possibility of a peculiar cycle. However, the onset of the "Rush to the Poles" of polar crown prominences and their associated coronal emission, which has been a precursor to solar maximum in recent cycles (cf. Altrock 2003), has been identified in the northern hemisphere. Peculiarly, this "Rush" is leisurely, at only 50% of the rate in the previous two cycles. The properties of the current "Rush to the Poles" yields an estimate of 2013 or 2014 for solar maximum. Title: "Extended-Solar-Cycle" Activity During the Current Solar Minimum Authors: Altrock, R. C. Bibcode: 2009AGUFMSH14A..04A Altcode: Altrock (1997, Solar Phys. 170, 411) and earlier authors discussed the high-latitude "extended" solar cycle seen in the Fe XIV corona prior to the appearance of sunspots and active regions at lower latitudes. For example, persistent coronal emission appeared near 70 degrees latitude in 1979 and 1989 and slowly migrated towards the equator, merging with the latitudes of sunspots and active regions after several years. Altrock (2007AGUFMSH53A1052A) showed that the high-latitude coronal emission was situated above the high-latitude neutral line of the large-scale photospheric magnetic field seen in Wilcox Solar Observatory synoptic maps, thus implying a connection with the solar dynamo. In 1999, persistent Fe XIV coronal emission appeared near 70 degrees latitude and began migrating towards the equator, but at a rate 40% slower than the previous two solar cycles. However, the onset of the "Rush to the Poles" of polar crown prominences and their associated coronal emission, which has preceded solar maximum by approximately two years in recent cycles (cf. Altrock, 2003, Solar Phys. 216, 343), has just occurred. Implications of these two events for predictions of the timing of the maximum of cycle 24 will be discussed. The observations used herein are the result of a cooperative program of the Air Force Research Laboratory and the National Solar Observatory. Title: The Progress of Solar Cycle 24 at High Latitudes Authors: Altrock, Richard C. Bibcode: 2009SPD....40.2405A Altcode: Altrock (Solar Phys., 170, 411, 1997) and earlier authors discussed the high-latitude "extended" solar cycle seen in the Fe XIV corona prior to the appearance of sunspots and active regions at lower latitudes. For example, persistent coronal activity appeared near 70 degrees latitude in 1979 and 1989 and slowly migrated towards the equator, merging with the latitudes of sunspots and active regions after several years. Altrock (2007AGUFMSH53A1052A) showed that the high-latitude coronal activity was situated above the high-latitude neutral line of the large-scale photospheric magnetic field seen in Wilcox Solar Observatory synoptic maps, thus implying a connection with the solar dynamo.

In 1999, persistent Fe XIV coronal activity appeared near 70 degrees latitude and began slowly migrating towards the equator at a rate similar to the previous two solar cycles. Thus, it appears that the solar dynamo that will produce the activity of cycle 24 is progressing normally. The current state of the extended solar cycle will be presented, with emphasis on determining whether the "Rush to the Poles" that will herald the cycle 24 maximum has begun (cf. Altrock, Solar Phys., 216, 343, 2003). Samples of current solar-minimum coronal activity will be shown. Title: Solar Torsional Oscillations and Their Relationship to Coronal Activity Authors: Altrock, R. C.; Howe, R.; Ulrich, R. Bibcode: 2008AGUSMSP31D..03A Altcode: Torsional Oscillations (TO) were first observed on the surface of the Sun as waves of small deviations from differential rotation, which propagate from high latitudes to the equator over solar-cycle time scales. More recently they have been inferred from observations of solar global oscillations to occur in the convection zone. Long-lived brightenings in the corona have also been observed to propagate from near the poles to the equator over similar time scales. This paper will discuss the relationship between TO as observed on the solar surface and in the convection zone and brightenings in the corona. We find that there is an apparent connection between these two phenomena that extends from the equator to latitudes as high as 70 to 80 degrees. This may imply control of both of these phenomena by the driver of the solar cycle (the solar dynamo) and thus place observational constraints on dynamo models. R. C. Altrock was supported by the Air Force Office of Scientific Research. Title: Solar Torsional Oscillations and Their Relationship to Coronal Activity Authors: Altrock, R.; Howe, R.; Ulrich, R. Bibcode: 2008ASPC..383..335A Altcode: Torsional Oscillations (TO) were first observed on the surface of the Sun as waves of small deviations from differential rotation, which propagate from high latitudes to the equator over solar-cycle time scales. More recently they have been inferred from observations of solar global oscillations to occur in the convection zone. Long-lived brightenings in the corona have also been observed to propagate from near the poles to the equator over similar time scales. This paper will discuss the relationship between TO as observed on the solar surface and in the convection zone and brightenings in the corona. We find that there is an apparent connection between these two phenomena that extends from the equator to latitudes as high as 70° to 80°. This may imply control of both of these phenomena by the driver of the solar cycle (the solar dynamo) and thus place observational constraints on dynamo models. Title: The Fe XIV Corona Approaching Solar Minimum Authors: Altrock, R. C. Bibcode: 2007AGUFMSH53A1052A Altcode: Although the solar disk is often devoid of sunspots around solar minimum, the upper atmosphere never rests. The most prominent features approaching the minimum of coronal activity are dense regions overlying mid-latitude boundaries of the large scale magnetic field. Seen above the limb, these features typically give the impression of "ears" (and "jowls"). Samples of these features will be shown, and the relationship to the "extended solar cycle" running from near the poles to the equator over 18 years will be discussed. Title: The Fe XIV and Fe X Corona at Solar Minimum Authors: Altrock, Richard C. Bibcode: 2007AAS...210.2506A Altcode: 2007BAAS...39..132A Although the solar disk is often devoid of sunspots around solar minimum, the upper atmosphere never rests. The most prominent features at the absolute minimum of coronal activity are dense regions overlying high latitude boundaries of the large scale magnetic field. Seen above the limb, these features typically give the impression of "ears" (and "jowls"). Samples of these features will be shown and their cause (the "extended solar cycle" running from near the poles to the equator over 18 years) explained. The author was supported by the Air Force Office of Scientific Research. Title: Using Solar-Minimum Polar Coronal Activity to Predict the Magnitude of the Following- Cycle Maximum Authors: Altrock, R. C. Bibcode: 2006AGUFMSH21A0323A Altcode: Observations of the Fe XIV solar corona have been obtained for the past three solar activity cycles at the Sacramento Peak site of the National Solar Observatory with the 40-cm coronagraph and the photoelectric coronal photometer. This study compares the properties of these observations near the poles near solar minimum with the maximum sunspot number of the following solar cycle. Preliminary results indicate that the number of coronal bright regions near the poles near solar minimum may be inversely correlated with the maximum amplitude of the following solar cycle. Using these results from previous cycles, a prediction will be made of the maximum sunspot number for cycle 24. Title: Solar Torsional Oscillations and Their Relationship to Coronal Activity Authors: Altrock, Richard C.; Howe, R.; Ulrich, R. Bibcode: 2006SPD....37.3203A Altcode: 2006BAAS...38..258A Torsional Oscillations were first observed on the surface of the sun aswaves of small deviations from differential rotation, which propagatefrom the pole to the equator over solar-cycle time scales. Morerecently they have been inferred from observations of solar globaloscillations to occur in the convection zone. Long-lived brighteningsin the corona have also been observed to propagate from near the polesto the equator over similar time scales. This paper will discuss therelationship between torsional oscillations as observed on the surfaceand in the convection zone and brightenings in the corona. We findthat there is an apparent connection between these two phenomena thatextends from the equator to latitudes as high as 70 to 80 degrees.R. C. Altrock was supported by the Air Force Office of ScientificResearch. Title: A Search for Torsional Oscillations in the Fe XIV Solar Corona Authors: Altrock, R. C. Bibcode: 2005AGUFMSH41B1132A Altcode: Previous studies of the rotation of the solar corona have found evidence for variations with time in the differential rotation rate similar to what has been referred to as torsional oscillations in the photosphere and the convection zone. However, the consistent data set of Fe XIV intensities obtained at Sacramento Peak since 1973 has not been exhaustively studied to determine if such oscillations exist. This data set has the advantage that a single photoelectric technique has been used to obtain the data over its entire length, whereas other studies have used data sets compiled from data obtained in a variety of methods from several observatories. The use of the Sacramento Peak database also has the advantage that the data have been corrected for sky-background variations in real time and thus are very precise over the time required to take a single scan. The results of this analysis will be presented and compared with those using other data sets. Title: Comparison of the Sacramento Peak Fe XIV Index with a Model Index Computed from Differential Emission Measure Maps Authors: Cook, J. W.; Newmark, J. S.; Altrock, R. C. Bibcode: 2005ApJ...633..518C Altcode: We compare the Sacramento Peak Fe XIV 5303 Å green line index with a model index time series for the period of operations of the EUV Imaging Telescope (EIT) on board the Solar and Heliospheric Observatory (SOHO), covering the years 1996-2002, from cycle minimum past the peak of the current activity cycle 23. We compute a differential emission measure (DEM) map for each day using images from the four channels of EIT at 171, 195, 284, and 304 Å. From the daily DEM map we then calculate a daily synthetic Fe XIV 5303 Å intensity image. The Sacramento Peak index is an average intensity, measured using a circular aperture 1.1 arcmin in diameter, sampling the off-limb corona in 3° steps around disk center. It is taken at several different heights beyond the daily white light limb. We modeled the daily index values, for the aperture center at 1.15 and 1.25 Rsolar from disk center, as the weighted average intensity within an annulus covering 1.11-1.19 and 1.21-1.29 Rsolar superposed on the daily synthetic intensity image. We compare the observed index with our model results and find a high correlation of the short-term values but a long-term systematic difference in the absolute values. We examine the accuracy of the respective calibrations and argue that the model results, based on the calibration of the EIT images used to produce the daily DEM maps, are more plausible in absolute value. Title: Solar Torsional Oscillations and the Extended Solar Cycle Authors: Altrock, R. C.; Howe, R. Bibcode: 2005AGUSMSP32A..04A Altcode: Torsional Oscillations were first observed on the surface of the sun as waves of small deviations from differential rotation, which propagate from the pole to the equator over solar-cycle time scales. More recently they have been inferred from observations of solar global oscillations to occur in the convection zone. Other solar phenomena, such as ephemeral regions and brightenings in the corona, have also been observed to propagate from near the poles to the equator over similar time scales. These other phenomena have been collectively referred to as the "Extended Solar Cycle". This paper will discuss the relationship between torsional oscillations as observed on the surface and in the convection zone and the "Extended Solar Cycle" as observed in the corona. R. C. Altrock was supported by the Air Force Office of Scientific Research. Title: Solar Torsional Oscillations and the Extended Solar Cycle Authors: Altrock, R.; Howe, R. Bibcode: 2004AGUFMSH53B0312A Altcode: Torsional Oscillations were first observed on the surface of the sun as waves of small deviations from differential rotation, which propagate from the pole to the equator over solar-cycle time scales. More recently they have been inferred from observations of solar global oscillations to occur in the convection zone. Other solar phenomena, such as ephemeral regions and brightenings in the corona, have also been observed to propagate from near the poles to the equator over similar time scales. These other phenomena have been collectively referred to as the "Extended Solar Cycle". This paper will discuss the relationship between torsional oscillations as observed in the convection zone and the "Extended Solar Cycle" as observed in the corona. Title: Solar Torsional Oscillations and the Extended Solar Cycle Authors: Altrock, R. C.; Howe, R. Bibcode: 2004AAS...205.4301A Altcode: 2004BAAS...36.1411A Torsional Oscillations were first observed on the surface of the sun as waves of small deviations from differential rotation, which propagate from the pole to the equator over solar-cycle time scales. More recently they have been inferred from observations of solar global oscillations to occur in the convection zone. Other solar phenomena, such as ephemeral regions and brightenings in the corona, have also been observed to propagate from near the poles to the equator over similar time scales. These other phenomena have been collectively referred to as the "Extended Solar Cycle". This paper will discuss the relationship between torsional oscillations as observed in the convection zone and the "Extended Solar Cycle" as observed in the corona.

R. C. Altrock was supported by the Air Force Office of Scientific Research. Title: The Solar Mass-Ejection Imager (SMEI) Mission Authors: Jackson, B. V.; Buffington, A.; Hick, P. P.; Altrock, R. C.; Figueroa, S.; Holladay, P. E.; Johnston, J. C.; Kahler, S. W.; Mozer, J. B.; Price, S.; Radick, R. R.; Sagalyn, R.; Sinclair, D.; Simnett, G. M.; Eyles, C. J.; Cooke, M. P.; Tappin, S. J.; Kuchar, T.; Mizuno, D.; Webb, D. F.; Anderson, P. A.; Keil, S. L.; Gold, R. E.; Waltham, N. R. Bibcode: 2004SoPh..225..177J Altcode: We have launched into near-Earth orbit a solar mass-ejection imager (SMEI) that is capable of measuring sunlight Thomson-scattered from heliospheric electrons from elongations to as close as 18 to greater than 90 from the Sun. SMEI is designed to observe time-varying heliospheric brightness of objects such as coronal mass ejections, co-rotating structures and shock waves. The instrument evolved from the heliospheric imaging capability demonstrated by the zodiacal light photometers of the Helios spacecraft. A near-Earth imager can provide up to three days warning of the arrival of a mass ejection from the Sun. In combination with other imaging instruments in deep space, or alone by making some simple assumptions about the outward flow of the solar wind, SMEI can provide a three-dimensional reconstruction of the surrounding heliospheric density structures. Title: The Temperature of the Low Corona During Solar Cycles 21 23 Authors: Altrock, Richard C. Bibcode: 2004SoPh..224..255A Altcode: 2005SoPh..224..255A Observations of the forbidden coronal lines Fe XIV 530.3 nm and Fe X 637.4 nm obtained at the National Solar Observatory at Sacramento Peak are used to determine the variation of coronal temperature at latitudes above 30 during solar activity cycles 21-23. Features of the long-term variation of emission in the two lines are also discussed. Temperatures at latitudes below 30 are not studied because the technique used to determine the coronal temperature is not applicable in active regions. The polar temperature varies cyclically from approximately 1.3 to 1.7 MK. The temperatures are similar in both hemispheres. The temperature near solar minimum decreases strongly from mid-latitudes to the poles. The temperature of the corona above 80 latitude generally follows the sunspot cycle, with minima in 1985 and 1995-1996 (cf. 1986 and 1996 for the smoothed sunspot number, Rz) and maxima in 1989 and 2000 (cf. 1989 and 2000 for Rz). The temperature of the corona above 30 latitude at solar maximum is nearly uniform, i.e., there is little latitude dependence. If the maximum temperatures of cycles 22 and 23 are aligned in time (superposed epochs), the average annual N + S temperature (average of the northern and southern hemisphere) in cycle 23 is hotter than that in cycle 22 at all times both above 80 latitude and above 30 latitude. The difference in the average annual N + S maximum temperature between cycles 23 and 22 was 56 kK near the poles and 64 kK for all latitudes above 30. Cycle 23 was also hotter at mid-latitudes than cycle 22 by 60 kK. The last 3 years of cycle 21 were hotter than the last 3 years of cycle 22. The difference in average annual N + S temperatures at the end of cycles 21 and 22 was 32 kK near the poles and 23 kK for all latitudes above 30. Cycle 21 was also hotter at mid-latitudes than cycle 22 by at least 90 kK. Thus, there does not seem to be a solar-cycle trend in the low-coronal temperature outside of active regions. Title: Observations of the "Extended Solar Cycle" During Solar Cycle 23 Authors: Altrock, R. C. Bibcode: 2004AAS...204.2007A Altcode: 2004BAAS...36..687A Altrock (1997, Solar Phys. 170, 411-423) previously observed high-latitude Fe XIV 530.3 nm emission features during solar cycles 21 and 22 at the National Solar Observatory at Sacramento Peak. He found that the observations supported the concept of "Extended" Solar Cycles, which begin every 11 years but last for approximately 19-20 years. This concept is based on observations by several earlier investigators extending back to 1957 (see Wilson et al., 1988, Nature 333, 748-750, for references). More recent investigations of high-latitude coronal activity have used satellite observations (cf. Benevolenskaya, Kosovichev and Scherrer, 2001, Astrophys. J. 554, L107-L110). This paper will compare the results of Altrock (1997) with newer data to determine if the earlier inferences of Extended Solar Cycles find added support during solar cycle 23. In addition, I will compare the results of these ground-based studies with those obtained using satellite data. Title: Sky Brightness and Transparency at the National Solar Observatory at Sacramento Peak Authors: Altrock, R. C. Bibcode: 2003AGUFMSH21B0141A Altcode: Records of sky brightness and transparency have been kept at the National Solar Observatory at Sacramento Peak in Sunspot, NM, for the past 20 years. Annual variations and long-term trends will be analyzed and presented. Title: Use of ground-based coronal data to predict the date of solar-cycle maximum Authors: Altrock, Richard C. Bibcode: 2003SoPh..216..343A Altcode: Prediction of the exact date of the maximum of the 11-year solar activity cycle is a matter of disagreement among solar scientists and of some importance to satellite operators, space-system designers, etc. Most predictions are based on physical conditions occurring at or before the solar-cycle minimum preceding the maximum in question. However, another indicator of the timing of the maximum occurs early in the rise phase of the solar cycle. A study of the variation over two previous solar cycles of coronal emission features in Fe xiv from the National Solar Observatory at Sacramento Peak has shown that, prior to solar maximum, emission features appear above 50° latitude in both hemispheres and begin to move towards the poles at a rate of 8° to 11° of latitude per year. This motion is maintained for a period of 3 or 4 years, at which time the emission features disappear near the poles. This phenomenon has been referred to as the `Rush to the Poles'. These observations show that the maximum of solar activity, as seen in the sunspot number, occurs approximately 19 ± 2 months before the features reach the poles. In 1997, Fe xiv emission features appeared near 55° latitude, and began to move towards the poles. Using the above historical data from cycles 21 and 22, we will see how the use of progressively more data from cycle 23 affects the prediction of the date of solar maximum. The principal conclusion is that the date of solar maximum for cycle 23 could be predicted to within 6 months as early as 1997. For solar cycle 24, when this phenomenon first becomes apparent later this decade, the average parameters for cycles 21-23 can be used to predict the date of solar maximum. Title: Is the Solar Corona getting hotter? Authors: Altrock, R. C. Bibcode: 2003SPD....34.1912A Altcode: 2003BAAS...35..844A Observations of the forbidden coronal lines Fe XIV 530.3 nm and Fe X 637.4 nm obtained at the National Solar Observatory at Sacramento Peak are used to determine the variation of coronal temperature at latitudes above 30 degrees during solar activity cycles 21, 22 and 23. Latitudes below 30 degrees are not studied, because the technique used to determine the coronal temperature is not applicable in active regions. The variation of temperature as a function of latitude and time is seen to be nearly symmetric about solar maximum and consistent between the northern and southern hemisphere during all three cycles. The variation with time at various latitudes will be studied in order to determine any long-term trends in coronal temperature.

The author was supported by the Air Force Office of Scientific Research. Title: A Study of the Rotation of the Solar Corona Authors: Altrock, Richard C. Bibcode: 2003SoPh..213...23A Altcode: Synoptic photoelectric observations of the coronal Fe xiv and Fe x emission lines at 530.3 nm and 637.4 nm, respectively, are analyzed to study the rotational behavior of the solar corona as a function of latitude, height, time and temperature between 1976 (1983 for Fe x) and 2001. An earlier similar analysis of the Fe xiv data at 1.15 R over only one 11-year solar activity cycle (Sime, Fisher, and Altrock, 1989, Astrophys. J.336, 454) found suggestions of solar-cycle variations in the differential (latitude-dependent) rotation. These results are tested over the longer epoch now available. In addition, the new Fe xiv 1.15 R results are compared with those at 1.25 R and with results from the Fe x line. I find that for long-term averages, both ions show a weakly-differential rotation period that may peak near 80° latitude and then decrease to the poles. However, this high-latitude peak may be due to sensing low-latitude streamers at higher latitudes. There is an indication that the Fe xiv rotation period may increase with height between 40° and 70° latitude. There is also some indication that Fe x may be rotating slower than Fe xiv in the mid-latitude range. This could indicate that structures with lower temperatures rotate at a slower rate. As found in the earlier study, there is very good evidence for solar-cycle-related variation in the rotation of Fe xiv. At latitudes up to about 60°, the rotation varies from essentially rigid (latitude-independent) near solar minimum to differential in the rising phase of the cycle at both 1.15 R and 1.25 R. At latitudes above 60°, the rotation at 1.15 R appears to be nearly rigid in the rising phase and strongly differential near solar minimum, almost exactly out of phase with the low-latitude variation. Title: Use of Ground-Based Coronal Data to Predict the Time of Solar-Cycle Maximum Authors: Altrock, R. C. Bibcode: 2002AAS...20113001A Altcode: 2002BAAS...34.1314A Prediction of the exact time of solar-cycle maximum is a matter of disagreement among solar scientists and of some importance to satellite operators, space-system designers, etc. Most predictions are based on physical conditions occurring at or before the long-term minimum of activity preceding the maximum in question. However, another indicator of the timing of the maximum occurs early in the rise phase of the solar activity cycle. A study of the variation over two previous solar cycles of coronal emission features in Fe XIV from the National Solar Observatory at Sacramento Peak has shown that, prior to solar maximum, emission features appear near 55 degrees latitude in both hemispheres and begin to move towards the poles at a rate of 9 to 13 degrees of latitude per year. This motion is maintained for a period of 3 or 4 years, at which time the emission features disappear near the poles. This phenomenon has been referred to as the "Rush to the Poles". These observations show that the maximum of solar activity, as seen in the sunspot number, occurs approximately 15 +/- 1 months before the features reach the poles. In 1997, Fe XIV emission features appeared near 55 degrees latitude, and began to move towards the poles. Using the above historical data from cycles 21 and 22, we will see how the use of progressively more data from cycle 23 affects the prediction of the time of solar maximum. For example, based on observations up through April 1999, the extrapolated Rush to the Poles is predicted to reach the poles in approximately June 2001, which results in a prediction for solar maximum of between January and April 2000. The actual smoothed sunspot number maximized in April 2000. This work was supported by the Air Force Office of Scientific Research. Title: Long-Term Variation of Solar Coronal Fe XIV and Fe X Fluxes Authors: Altrock, R. C. Bibcode: 2002AAS...200.8809A Altcode: 2002BAAS...34..790A Synoptic photoelectric observations of the coronal Fe XIV and Fe X emission lines at 530.3 nm and 637.4 nm, respectively, are analyzed to study the output of the solar corona in these lines as a function of time. The data used are measurements made with the NSO/Sacramento Peak 40-cm coronagraph and Emission-Line Coronal Photometer of the intensity of these lines observed at 1.15 solar radii between 1973 (1984 for Fe X) and 2002. A new calibration determination is used to convert relative intensities to absolute intensities. The solar-cycle variation of these fluxes will be compared to each other and to other solar-cycle parameters. One interesting result is that a constant minimum or basal corona may exist at solar minimum. This paper was supported by the Air Force Office of Scientific Research. Title: Long-term variation of solar coronal Fe XIV and Fe X fluxes Authors: Altrock, R. Bibcode: 2002cosp...34E1003A Altcode: 2002cosp.meetE1003A Synoptic photoelectric observations of the coronal Fe XIV and Fe X emission lines at 530.3 nm and 637.4 nm, respectively, are analyzed to study the output of the solar corona in these lines as a function of time. The data used are measurements made with the NSO/Sacramento Peak 40-cm coronagraph and Emission-Line Coronal Photometer of the intensity of these lines observed at 1.15 solar radii between 1973 (1984 for Fe X) and 2002. A new calibration determination is used to convert relative intensities to absolute intensities. The solar-cycle variation of these fluxes will be compared to each other and to other solar-cycle parameters. One interesting result is that a constant minimum or basal corona may exist at solar minimum. This paper was supported by the Air Force Office of Scientific Research. Title: Long-Term Variation of the Rotation of the Solar Corona Authors: Altrock, R. C. Bibcode: 2002mwoc.conf..337A Altcode: Synoptic photoelectric observations of the coronal Fe XIV and Fe X emission lines at 530.3 nm and 637.4 nm, respectively, are analyzed to study the rotational behavior of the solar corona as a function of latitude, height and time. The data used are measurements made with the Sacramento Peak 40-cm coronagraph and Emission-Line Coronal Photometer of the intensity of these lines observed at 1.15 to 1.45 solar radii (Ro) between 1973 (1984 for Fe X) and 2000. An earlier similar temporal-correlation analysis of the Fe XIV data at 1.15 Ro over only one 11-year solar activity cycle (Sime, Fisher and Altrock 1989, Astrophys. J. 336, 454) found suggestions of solar-cycle variations in the differential-rotation and latitude-averaged-rotation patterns that combined the effects of large-scale patterns seen in the white-light corona and smaller-scale patterns seen in chromospheric and photospheric rotation. These results will be tested over the longer epoch now available. In addition, the new 1.15 Ro Fe XIV results will be compared with those at greater heights and with results from the Fe X line and radio frequencies (Vats et al. 2001, Astrophys. J., 548, L87) to form a global picture of solar rotation throughout the corona and over more than two solar cycles. Title: Further Results on the Rotation of the Solar Corona Authors: Altrock, R. C. Bibcode: 2001AGUFMSH11A0700A Altcode: Synoptic photoelectric observations of the coronal Fe XIV and Fe X emission lines at 530.3 nm and 637.4 nm, respectively, are analyzed to study the rotational behavior of the solar corona as a function of latitude, height and time. The data used are measurements made with the Sacramento Peak 40-cm coronagraph and Emission-Line Coronal Photometer of the intensity of these lines observed at 1.15 to 1.45 solar radii (Ro) between 1973 (1984 for Fe X) and 2000. An earlier similar temporal-correlation analysis of the Fe XIV data at 1.15 Ro over only one 11-year solar activity cycle (Sime, Fisher and Altrock 1989, Astrophys. J. 336, 454) found suggestions of solar-cycle variations in the differential-rotation and latitude-averaged-rotation patterns that combined the effects of large-scale patterns seen in the white-light corona and smaller-scale patterns seen in chromospheric and photospheric rotation. These results will be tested over the longer epoch now available. In addition, the new 1.15 Ro Fe XIV results will be compared with those at greater heights and with results from the Fe X line and radio frequencies (Vats et al. 2001, Astrophys. J., 548, L87) to form a global picture of solar rotation throughout the corona and over more than two solar cycles. Title: Long-Term Variation of the Rotation of the Solar Corona Authors: Altrock, R. C. Bibcode: 2001AGUSM..SP61A04A Altcode: Synoptic photoelectric observations of the coronal Fe XIV and Fe X emission lines at 530.3 nm and 637.4 nm, respectively, are analyzed to study the rotational behavior of the solar corona as a function of latitude, height and time. The data used are measurements made with the Sacramento Peak 40-cm coronagraph and Emission-Line Coronal Photometer of the intensity of these lines observed at 1.15 to 1.45 solar radii (Ro) between 1973 (1984 for Fe X) and 2000. An earlier similar temporal-correlation analysis of the Fe XIV data at 1.15 Ro over only one 11-year solar activity cycle (Sime, Fisher and Altrock 1989, Astrophys. J. 336, 454) found suggestions of solar-cycle variations in the differential-rotation and latitude-averaged-rotation patterns that combined the effects of large-scale patterns seen in the white-light corona and smaller-scale patterns seen in chromospheric and photospheric rotation. These results will be tested over the longer epoch now available. In addition, the new 1.15 Ro Fe XIV results will be compared with those at greater heights and with results from the Fe X line and radio frequencies (Vats et al. 2001, Astrophys. J., 548, L87) to form a global picture of solar rotation throughout the corona and over more than two solar cycles. Title: Comparison of Sac Peak Fe XIV Index with Model Index Computed from EIT Differential Emission Measure Maps Authors: Cook, J. W.; Newmark, J. S.; Altrock, R. C. Bibcode: 2001AGUSM..SP32B05C Altcode: We compare the Sac Peak Fe XIV green line index with a model index time series for the period of operations of the Extreme-ultraviolet Imaging Telescope (EIT) aboard the Solar and Heliospheric Observatory (SOHO), covering the years 1996-2000, from cycle minimum to the peak of the current activity cycle 23. We compute a differential emission measure (DEM) map for each day using images from the four channels of EIT at 171 Å, 195 Å, 284 Å, and 304 Å. From the daily DEM map we then calculate a daily Fe XIV 5304 Å intensity image (see Cook et al. 1999, Proceedings of the 8th SOHO Workshop, ESA SP-446, pp. 241-246). The Sac Peak index is an average intensity, measured using a circular aperture 1 arcmin in diameter sampling the corona in 1 degree steps around disk center. It is taken at several different heights beyond the daily limb. We modeled the index values, for the aperture center at 1.15 Rodot from disk center, as the average intensity within a daily annulus covering 1.12 - 1.18 Rodot imposed on the model intensity image. We compare the observed index with our model results, and discuss in terms of the accuracy of the model intensities which can be determined from our EIT-based DEM curves. We actually produce a daily Fe XIV image for the entire EIT field-of-view. The Sac Peak index provides one well calibrated, long term check on the reliability of the DEM model calculation. This work has been supported by NASA under W-19,348, and by the Office of Naval Research. Title: Variation of the Large-Scale Coronal Temperature at Mid-to-High Latitudes over 1.5 Solar Cycles Authors: Altrock, R. C. Bibcode: 2000SPD....31.0225A Altcode: 2000BAAS...32..815A Observations of the forbidden coronal lines Fe XIV 530.3 nm and Fe X 637.4 nm obtained at the National Solar Observatory at Sacramento Peak are used to determine the variation of coronal temperature at latitudes above 30 degrees outside of active regions during cycles 22 and 23. A pattern, which is symmetric about solar maximum during cycle 22 and consistent between the northern and southern hemisphere, is seen. Beginning near solar minimum in 1985, the temperature above 60 degrees latitude is at a minimum value, varying from about 1.3 MK near the poles to about 1.5 MK near 60 degrees. Near the time that the "Rush-to-the-Poles" begins in 1987, the high-latitude temperature increases abruptly, reaching values of 1.7 MK at the North pole and 1.6 MK at the South pole in 1989. After 1990, the process reverses, and temperatures at the poles are below 1.3 MK by 1995. The rise to the maximum of cycle 23 will be compared with that of cycle 22. Title: Coronal index of solar activity for 1998 Authors: Altrock, R. C.; Rybansky, M.; Minarovjech, M.; Rusin, V. Bibcode: 1999CoSka..29..105A Altcode: We present the Fe XIV 530.3 nm (green line) coronal index (CI) of solar activity for 1998. A systematic increase of CI was observed from January to October 1998. Toward the end of the year the rate of increase slowed remarkably. A comparison of CI with similar indices of solar activity (2800 MHz radio flux, the Wolf sunspot number and the SUSIM Mg II index) shows a good correlation. Title: Verification of a Method for Predicting the Time of Solar Maximum Authors: Altrock, R. C. Bibcode: 1999AAS...194.9209A Altcode: 1999BAAS...31..987A Prediction of the exact time of solar maximum is a matter of disagreement among solar scientists and of some importance to satellite operators, space-system designers, etc. Most predictions are based on physical conditions occurring at or before the long-term minimum of activity preceding the maximum in question. However, a perhaps-more-reliable indicator of the timing of the maximum occurs early in the rise phase of the solar cycle. A study of the long-term variation of coronal emission features in Fe XIV from the National Solar Observatory at Sacramento Peak has shown that, prior to solar maximum, emission features appear near 55 degrees latitude in both hemispheres and begin to move towards the poles at a rate of 9 to 13 degrees of latitude per year. This motion is maintained for a period of 3 or 4 years, at which time the emission features disappear near the poles. This phenomenon has been referred to as the "Rush to the Poles". The maximum of solar activity historically occurs approximately 16 +/- 1 months before the features reach the poles. In 1997, Fe XIV emission features appeared near 55 degrees latitude, and subsequent observations have shown that these features are moving towards the poles. This then is the Rush to the Poles observed in previous solar cycles. Based on observations up through October 1998 over three cycles, these features will reach the poles in approximately October 2000, which results in a prediction for solar maximum of between June and August 1999, substantially earlier than many other predictions. A maximum smoothed sunspot number of approximately 160 is inferred from the similarity of the rate of progression towards the poles in this cycle compared to the two previous cycles. The current status of Rush to the Poles and of the solar cycle will be reviewed and conclusions drawn about the reliability of this method. This work was supported by the Air Force Office of Scientific Research. Title: Determination of the solar minimum period between cycles 22 and 23 from the coronal index of solar activity Authors: Altrock, R. C.; Rybanský, M.; Rušin, V.; Minarovjech, M. Bibcode: 1999SoPh..184..317A Altcode: We present the coronal index of solar activity (CI) for 1997 and use the 1996 and 1997 data to examine the properties of the solar minimum between cycles 22 and 23. To compute CI, we used only the intensities of the green corona from Lomnický Štít and Sacramento Peak coronal stations. Values of CI were low in the first half of 1997 with an increase from September toward the end of 1997. We determined the minimum in the green corona to be May 1996, which is in coincidence with the results from 2800 MHz radio flux, the Mg II index and the Wolf number. Title: Synoptic Coronal Temperature; Magnetic Field and He 11083 NM Observations Authors: Penn, M.; Altrock, R. C.; Henry, T.; Guhathakurta, M. Bibcode: 1998ASPC..140..325P Altcode: 1998ssp..conf..325P No abstract at ADS Title: Variation of Solar Coronal Intensity and Temperature in Cycle 22 Authors: Altrock, Richard C. Bibcode: 1998ASPC..140..339A Altcode: 1998ssp..conf..339A No abstract at ADS Title: Electron Temperature Distribution in Coronal Holes Authors: Halas, C. D.; Habbal, S. R.; Penn, M.; Uitenbroek, H.; Esser, R.; Altrock, R.; Guhathakurta, M. Bibcode: 1997AAS...191.7413H Altcode: 1997BAAS...29Q1326H Knowledge of the electron temperature within coronal holes is extremely important for constructing solar wind models and for understanding the coronal heating process. We report on the two-dimensional CCD observations of the Fe IX 4585, Fe X 6374, Fe XI 7892 and Fe XIV 5303 { Angstroms} emission lines made using a coronagraph at the National Solar Observatory at Sacramento Peak. These iron lines, which have a peak formation temperature of 5 10(5) , 10(6) , 1.2 10(6) , and 2 10(6) K, respectively, allow the examination of different temperature plasmas within the same large scale magnetic structure. To account for possible line of sight ambiguities from hot material in the foreground or background of the coronal hole, Yohkoh data were used to determine the extent of the coronal hole along the line of sight. Intensities and widths of these spectral lines as a function of heliocentric distance out to 1.15 R_s will be presented. A comparison will be made between coronal hole and streamer observations. Title: Design for the Solar Mass Ejection Imager (SMEI) Authors: Keil, S. L.; Altrock, R. C.; Kahler, S. W.; Jackson, B. V.; Buffington, A.; Hick, P. L.; Simnett, G.; Eyles, C.; Webb, D. F.; Anderson, P. Bibcode: 1997SPD....28.0227K Altcode: 1997BAAS...29..897K The Solar Mass Ejection Imager (SMEI) experiment is designed to detect and measure transient plasma features in the heliosphere, including coronal mass ejections (CMEs), shock waves, and structures such as streamers which corotate with the Sun. SMEI will provide measurements of the propagation of solar plasma clouds and high-speed streams which can be used to forecast their arrival at Earth from one to three days in advance. Data from SMEI will be used to develop models and techniques that will, for the first time, allow us to predict the onset and magnitude of geomagnetic storms that disrupt space operations and affect communications and surveillance activities. We will present the current design and observational plans for SMEI. SMEI is currently under construction with instrument completion expected in 1999. We plan to launch SMEI near the next solar maximum and will make the data available to the scientific and space weather forecast communities. Title: The High-Latitude Variation of Solar Coronal Temperature in Cycle 22 Authors: Altrock, Richard C. Bibcode: 1997SPD....28.0705A Altcode: 1997BAAS...29..911A Observations at 1.15 R_⊙ of the forebidden coronal lines Fe XIV 530.3 nm and Fe X 637.4 nm obtained at the National Solar Observatory at Sacramento Peak are used to determine the variation of coronal temperature at high latitudes during Cycle 22. An unexpected pattern, symmetric about solar maximum and consistent between the northern and southern hemisphere, is seen. Beginning near solar minimum in 1985, the temperature above 60deg latitude is seen to be at a minimum value, varying from about 1.3 MK near the poles to about 1.5 MK near 60deg . Near the time that the "Rush-to-the-Poles" begins in 1987, the high-latitude temperature increases abruptly, reaching values of 1.7 MK at the North pole and 1.6 MK at the South pole in 1989. After 1990, the process reverses, and temperatures at the poles are below 1.3 MK by 1995. This pattern may be consistent with the latitude variations of polar-crown prominences. The author was supported by the Air Force Office of Scientific Research. Title: Coronal index of solar activity for 1996 Authors: Altrock, R. C.; Rybansky, M.; Rusin, V.; Minarovjech, M. Bibcode: 1997CoSka..27...25A Altcode: We present the coronal index of solar activity (CI) for 1996. To compute CI, we used only the intensities of the green corona from Lomnicky Stit and Sacramento Peak coronal stations. Values of CI were low with an increase toward the end of 1996. It appears that the minimum of solar activity in the green corona occurred in March 1996. The rotational rate of CI, as measured during the last half of 1996, is 26 days. The results are compared to the Wolf number and 2800 MHz flux over the entire cycle 22 (1986-1996). Title: An `EXTENDED Solar Cycle' as Observed in fe XIV Authors: Altrock, Richard C. Bibcode: 1997SoPh..170..411A Altcode: Investigation of the behavior of coronal intensity above the limb in Fexiv emission (530.3 nm) obtained at the National Solar Observatory at Sacramento Peak over the last 23 years has resulted in the confirmation of a second set of zones of solar activity at high latitudes, separate from the Main Activity Zones (MAZ). Localized high-latitude intensity maxima, which I will call High-latitude Emission Features (HEF), are observed at 0.15 solar radii above the limb throughout the solar cycle. They persist long enough at a given latitude to be visible in long-term (e.g., annual) averages. I identify two types of HEF. Poleward-moving HEF, which may be identified with the `Rush to the Poles' phenomenon seen in polar-crown prominences, were first seen to appear in this investigation near latitude 60° in 1978. In 1979 equatorward-moving HEF branched off from the poleward-moving HEF (which continued on to reach the pole in 1980) at a latitude of 70° to 80°. They evolved approximately parallel to the MAZ. Near solar minimum, these HEF evolved into the MAZ of cycle 22, and the emission continues its path towards the equator, where it should disappear soon. Title: The Solar Mass Ejection Imager (SMEI) Authors: Jackson, B.; Buffington, A.; Hick, P.; Keil, S.; Altrock, R.; Kahler, S.; Simnett, G.; Eyles, C.; Webb, D.; Anderson, P. Bibcode: 1997IAUJD..19E..27J Altcode: The Solar Mass Ejection Imager (SMEI) experiment is designed to detect and measure transient plasma features in the heliosphere, including coronal mass ejections (CMEs), shock waves, and structures such as streamers which co-rotate with the Sun. SMEI will provide measurements of the propagation of solar plasma clouds and high-speed streams which can be used to forecast their arrival at Earth from one to three days in advance. SMEI consists of three cameras, each imaging a 60o times 3o field of view for a total image size of 180o times 3o. As the satellite orbits the earth, repeated images are used to build up a view of the entire heliosphere at resolutions of better than one degree. Here, we will show the most recent progress on this instrument, now under prototype construction. Title: Solar Mass Ejection Imager (SMEI) Authors: Keil, Stephen L.; Altrock, Richard C.; Kahler, Stephen; Jackson, Bernard V.; Buffington, Andrew; Hick, Paul; Simnett, George M.; Eyles, Christopher J.; Webb, David; Anderson, Peter Bibcode: 1996SPIE.2804...78K Altcode: The Solar Mass Ejection Imager (SMEI) experiment is designed to detect and measure transient plasma features in the heliosphere, including coronal mass ejections, shock waves, and structures such as streamers which corotate with the Sun. SMEI will provide measurements of the propagation of solar plasma clouds and high-speed streams which can be used to forecast their arrival at Earth from one to three days in advance. The white light photometers on the HELIOS spacecraft demonstrated that visible sunlight scattered from the free electrons of solar ejecta can be sensed in interplanetary space with an electronic camera baffled to remove stray background light. SMEI promises a hundred-fold improvement over the HELIOS data, making possible quantitative studies of mass ejections. SMEI measurements will help predict the rate of energy transfer into the Earth's magnetospheric system. By combining SMEI data with solar, interplanetary and terrestrial data from other space and ground-based instruments, it will be possible to establish quantitative relationships between solar drivers and terrestrial effects. SMEI consists of three cameras, each imaging a 60 degree(s) X 3 degree(s) field of view for a total image size of 180 degree(s) X 3 degree(s). As the satellite orbits the earth, repeated images are used to build up a view of the entire heliosphere. Title: Coronal synoptic temperature maps derived from the Fe XIV/Fe X intensity ratio Authors: Hick, P.; Jackson, B. V.; Altrock, R. C. Bibcode: 1996AIPC..382..169H Altcode: The large-scale temperature structure of the low corona is investigated using synoptic temperature maps, derived from the intensity ratio of the green (Fe XIV) and red (Fe X) coronal lines as observed at the National Solar Observatory/Sacramento Peak. This intensity ratio is sensitive to coronal plasma with temperatures of 1-2 MK, a range of temperatures usually associated with the quiet corona. The synoptic maps indicate an association between high coronal temperature and the large-scale magnetic field. A comparison with Stanford `source surface' synoptic maps shows that, especially when the heliospheric current sheet is stable over several rotations, the large-scale high-temperature features follow the current sheet remarkably well. For recent Carrington rotations, temperature maps are available for four heights between 1.15 and 1.45 Rsolar. For these maps the correspondence with the current sheet (calculated at 2.5 Rsolar) improves with height. Discrepancies between temperature structure and magnetic structure appear to be largest when the magnetic structure changes rapidly from rotation to rotation. Title: The solar mass ejection imager Authors: Jackson, B. V.; Buffington, A.; Hick, P. L.; Kahler, S. W.; Altrock, R. C.; Gold, R. E.; Webb, D. F. Bibcode: 1996AIPC..382..536J Altcode: We are designing a Solar Mass Ejection Imager (SMEI) capable of observing Thomson-scattered signals from transient density features in the heliosphere from a spacecraft situated near 1 AU. The imager is designed to trace these features, which include coronal mass ejections, corotating structures and shock waves, to elongations greater than 90° from the Sun. The instrument may be regarded as a progeny of the heliospheric imaging capability shown possible by the zodiacal light photometers of the HELIOS spacecraft. The instrument we are designing would make more effective use of in situ solar wind data from spacecraft in the vicinity of the imager by extending their observations to the surrounding environment. An imager in Earth orbit could allow up to three days warning of the arrival of a mass ejection from the Sun. Title: The Solar Coronal Temperature Structure and the Heliospheric Current Sheet Authors: Altrock, R. C.; Hick, P.; Jackson, B. V.; Slater, G.; Henry, T. W. Bibcode: 1996AAS...188.8004A Altcode: 1996BAAS...28..956A We explore the large-scale temperature structure of the low corona using synoptic temperature maps, derived from the intensity ratio of the green (Fe XIV) and red (Fe X) coronal lines as observed at the National Solar Observatory/Sacramento Peak, and temperature maps derived from the Al0.1 and AlMgMn filter intensity ratio measured by the Yohkoh/SXT instrument. The red/green intensity ratio is sensitive to coronal plasma with temperatures in the range of 1--2 MK and is therefore useful for studying the `quiet' corona. The Yohkoh/SXT filter ratio covers a much wider range of coronal temperature (>= 1 MK) and, in particular, is sensitive to the high temperatures (>= 3 MK) commonly observed above active regions. We use the temperature maps to study the evolution of the large-scale coronal temperature distribution, in particular in relation to the large-scale magnetic field, as given by the `source surface' maps derived from the Stanford potential field model. We find that the large-scale high-temperature features follow the heliospheric current sheet remarkably well, especially when the current sheet is stable over several rotations. Title: Solar coronal structure: a comparison of NSO/SP ground-based coronal emission line intensities and temperatures with YOHKOH SXT and WSO magnetic data Authors: Altrock, R. C.; Hick, P.; Jackson, B. V.; Hoeksema, J. T.; Zhao, X. P.; Slater, G.; Henry, T. W. Bibcode: 1996AdSpR..17d.235A Altcode: 1996AdSpR..17..235A The large-scale structure of the solar corona is investigated using synoptic maps produced from Fe XIV (530.3 nm), Fe X (637.4 nm) and Ca XV (569.4 nm) data obtained at NSO/SP, Yohkoh/SXT X-ray data and Wilcox Solar Observatory (WSO) `source surface' maps. We find that the Fe XIV data are an excellent proxy for spatially-averaged Yohkoh/SXT data. Isolated emission features and large-scale structures are nearly identical in SXT and Fe XIV maps. In addition, coronal holes and other low-emission regions are very similar. Synoptic temperature maps, calculated from the Fe X/Fe XIV ratio, show a tendency for the highest temperatures to occur where the large-scale magnetic fields change polarity at high latitudes (cf. /1/), while lower-latitude features, including active regions, have lower apparent temperatures. Regions of enhanced temperature generally follow the heliospheric current sheet (HCS) as defined by the WSO maps. Further, emission in Ca XV (formed at T ~ 3 MK), generally occurs only over low-latitude regions that are bright in both Fe X (T ~ 1 MK) and Fe XIV (T ~ 2 MK). Thus, there is evidence for low (~1 MK), moderate (~2 MK) and high (~3 MK) temperatures in close proximity in the low corona. Title: IPS observations of heliospheric density structures associated with active regions Authors: Hick, P.; Jackson, B. V.; Altrock, R.; Woan, G.; Slater, G. Bibcode: 1996AdSpR..17d.311H Altcode: 1996AdSpR..17..311H Interplanetary scintillation (IPS) measurements of the `disturbance factor' g, obtained with the Cambridge (UK) array can be used to explore the heliospheric density structure. We have used these data to construct synoptic (Carrington) maps, representing the large-scale enhancements of the g-factor in the inner heliosphere. These maps emphasize the stable corotating, rather than the transient heliospheric density enhancements. We have compared these maps with Carrington maps of Fe XIV observations (NSO, Sacramento Peak) and maps based on Yohkoh/SXT X-ray observations. Our results indicate that the regions of enhanced g tend to map to active regions rather than the current sheet. The implication is that active regions are the dominant source of the small-scale (≈ 200 km) density variations present in the quiet solar wind. Title: The Coronal Temperature Structure and the Current Sheet Authors: Hick, Paul; Jackson, B. V.; Altrock, R. C.; Slater, G.; Henry, T. Bibcode: 1996ASPC...95..358H Altcode: 1996sdit.conf..358H No abstract at ADS Title: The Solar Mass Ejection Imager (SMEI): Development and Use in Space Weather Forecasting Authors: Keil, S. L.; Altrock, R. C.; Kahler, S. W.; Jackson, B. V.; Buffington, A.; Hick, P. L.; Simnett, G.; Eyles, C.; Webb, D. F.; Anderson, P. Bibcode: 1996ASPC...95..158K Altcode: 1996sdit.conf..158K No abstract at ADS Title: Prediction of Coronal-Hole Solar Wind Velocities at ULYSSES from NSO/SP Coronal Data Authors: Altrock, Richard C.; Henry, Timothy W. Bibcode: 1996ASPC...95..324A Altcode: 1996sdit.conf..324A No abstract at ADS Title: Using Fe X 6374 Å and Fe XIV 5303 Å spectral line intensities to study the effect of line of sight integration on coronal temperature inferences Authors: Esser, R.; Brickhouse, N. S.; Habbal, S. R.; Altrock, R. C.; Hudson, H. S. Bibcode: 1995JGR...10019829E Altcode: Polar coronal holes are relatively stable structures persisting over many solar rotations. The appearance of coronal holes in remote observations, however, can change on a daily basis due to variations of the denser and hotter plasma surrounding them. We explore the effect of these denser and hotter surrounding regions on coronal hole observations, using daily intensity measurements at 1.15 RS of the green Fe XIV 5303 Å and red Fe X 6374 Å spectral lines. The observations, which were carried out at the National Solar Observatory a Sacramento Peak, New Mexico, cover at time period of about four solar rotations.

We show that the ``coronal hole'' temperatures derived using the line ratio technique, vary by more than 0.8×106 K over the time interval considered here. We also provide a short discussion of the expected accuracy of the atomic data for these two iron spectral lines. Using intensity measurements as a function of distance from the Sun, we briefly discuss how the regions surrounding the coronal holes might influence the inference of the temperature gradient in the coronal holes. The line of sight effect on the temperature gradient should be explored in more detail in the future using daily observations of the line intensities as a function of distance. These observations could be provided by ground-based coronagraphs and by instruments on board SOHO. Title: The Solar Mass Ejection Imager Authors: Jackson, B. V.; Buffington, A.; Hick, P. L.; Kahler, S. W.; Altrock, R. C.; Gold, R. E.; Webb, D. F. Bibcode: 1995sowi.confR..97J Altcode: We are designing a Solar Mass Ejection Imager (SMEI) capable of observing the Thomson-scattered signal from transient density features in the heliosphere from a spacecraft situated near AU. The imager is designed to trace these features, which include coronal mass ejections. corotating structures and shock waves, to elongations greater than 90 deg from the Sun. The instrument may be regarded as a progeny of the heliospheric imaging capability shown possible by the zodiacal-light photometers of the HELIOS spacecraft. The instrument we are designing would make more effective use of in-situ solar wind data from spacecraft in the vicinity of the imager by extending these observations to the surrounding environment. The observations from the instrument should allow deconvolution of these structures from the perspective views obtained as they pass the spacecraft. An imager at Earth could allow up to three days warning of the arrival of a mass ejection from the Sun . Title: Coronal synoptic temperature maps derived from the Fe XIV/Fe X intensity ratio Authors: Hick, P.; Jackson, B. V.; Altrock, R. Bibcode: 1995sowi.confQ..69H Altcode: The large-scale temperature structure of the low corona is investigated using synoptic temperature maps, derived from the intensity ratio of the green (Fe XIV) and red (Fe X) coronal lines as observed at the National Solar Observatory/Sacramento Peak. This intensity ratio is sensitive to coronal plasma with temperatures in the range of 1-2 MK. The synoptic maps indicate an association between high coronal temperature and the large-scale magnetic field. A comparison with WSO 'source surface' synoptic maps shows that especially when the heliospheric current sheet is stable over several rotations, the large-scale high-temperature features follow the current sheet remarkably well. For recent Carrington rotations temperature maps have been constructed for various heights between 1.15 and 1.45 solar radii. For these maps the correspondence with the current sheet (calculated at 2.5 solar radii) improves with height. Deviations between temperature structure and magnetic structure appears to be largest when the magnetic structure changes rapidly from rotation to rotation. Title: Short-Term Periodicities in Soft X-ray Solar Flares Authors: Airapetian, V. A.; Balasubramanian, K. S.; Altrock, R. C.; Radick, R. R. Bibcode: 1995SPD....26.1213A Altcode: 1995BAAS...27..985A No abstract at ADS Title: The Track of Ulysses Across the Solar Southern Polar Coronal Hole as Defined by NSO/SP Fe XIV Data, and Comparisons of the Two Data Sets Authors: Altrock, R. C.; Gosling, J. T.; Henry, T. W. Bibcode: 1995SPD....26..902A Altcode: 1995BAAS...27..973A No abstract at ADS Title: Association of Solar Coronal Temperature and Structure from Ground-Based Emission-Line Data with Global Magnetic Field Models and Yohkoh SXT Data (Abstract only) Authors: Altrock, R. C.; Hick, P.; Jackson, B. V.; Hoeksema, J. T.; Zhao, X. P.; Slater, G.; Henry, T. W. Bibcode: 1995itsa.conf...45A Altcode: No abstract at ADS Title: Photometric imaging observations of the emission corona Authors: Altrock, R. C.; Smartt, R. N. Bibcode: 1994ESASP.373..425A Altcode: 1994soho....3..425A No abstract at ADS Title: Coronal Index of Solar Activity - Part Seven - Years 1988-1991 Authors: Rybansky, M.; Rusin, V.; Gaspar, P.; Altrock, Richard C. Bibcode: 1994SoPh..152..487R Altcode: A brief description is given of the coronal index of solar activity (CI) derived from ground-based observations of the green coronal line 530.3 nm (FeXIV) and its computation. The final data of CI are presented in graphical form over the period 1988-1991. The maximum of CI coincided with the Wolf number in cycle 22, and no second maximum, sometimes seen two years after the first one, was observed in this cycle. Title: The solar cycle variation of coronal temperature and density during cycle 21-22 Authors: Guhathakurta, M.; Fisher, R. R.; Altrock, R. C. Bibcode: 1994AdSpR..14d..49G Altcode: 1994AdSpR..14...49G In this paper we characterize the temperature and the density structure of the corona utilizing co-spatial spectrophotometric observations during the descending phase of cycle 21 through the ascending phase of cycle 22. The data include ground-based intensity observations of the green (5303Å Fe XIV) and red (6374Å Fe X) coronal forbidden lines from Sacramento Peak and synoptic maps of white-light K-coronal polarized brightness, pB from the High Altitude Observatory, and photospheric magnetographs from the National Solar Observatory, Sacramento Peak. A determination of plasma temperature T can be derived unambiguously from the intensity ratio Fe X/Fe XIV, since both emission lines come from ionized states of Fe, and the ratios are only weakly dependent on density. The latitudinal variation of the temperature and the density within the descending and the ascending phases of solar cycle 21 and 22 are presented. There is a large-scale organization of the inferred coronal temperature distribution; these structures tend to persist through most of the magnetic activity cycle. This distribution differs in spatial and temporal characterization from the traditional picture of sunspot and active region evolution over the range of sunspot cycle. Title: Groundbased observations of the Sun's corona following the perihelia of sungrazing comets. Authors: St. Cyr, O. C.; Altrock, R. C. Bibcode: 1993BAAS...25.1303S Altcode: No abstract at ADS Title: Groundbased Observations of the Sun's Corona Following the Perihelia of Sungrazing Comets Authors: Cyr, O. C. St.; Altrock, R. C. Bibcode: 1993AAS...183.0904C Altcode: 1993BAAS...25Q1303C During the period 1979-1989, two spaceborne coronagraphs discovered 16 sungrazing comets in observations of the white-light corona. All of the comets discovered by NRL's Solwind telescope on the USAF satellite P78-1 and HAO's C/P telescope on NASA's SMM were members of the Kreutz family of sungrazers. All of these comets were observed in the hours prior to their individual perihelia, but none were detected post-perihelion by the spaceborne coronagraphs. Further, none of these comets were directly detected by groundbased observers. There was, however, a single report by Czech observers of a coronal enhancement in Fe X following the first Solwind comet. To investigate the possibility of a cometary signature in the solar atmosphere we examined groundbased coronal observations made at the National Solar Observatory site at Sacramento Peak with the Fisher-Smartt Emission Line Coronal Photometer. For 13 of the 16 comets described above, there were synoptic observations made at 5303A (Fe XIV) at Sacramento Peak both the day before and the day after the comets' perihelia. For a few cases, there were also scans at 5694A (Ca XV) and 6374A (Fe X). We report here on this work in progress. *Operated by AURA Inc., under cooperative agreement with the NSF. Partial support for NSO is provided by USAF under a Memorandum of Understanding with the NSF. RCA gratefully acknowledges support from the US Air Force Office of Scientific Research, Task PL011. Title: Large-Scale Coronal Temperature and Density Distributions, 1984--1992 Authors: Guhathakurta, M.; Fisher, R. R.; Altrock, R. C. Bibcode: 1993ApJ...414L.145G Altcode: We characterize the temperature and the density structure of the corona utilizing spectrophotometric observations at different heights but at the same latitude during the descending phase of cycle 21 through the ascending phase of cycle 22. The data include ground-based intensity observations of the green (Fe XIV 5303) and red (Fe X 6374) coronal forbidden lines, photospheric magnetographs from the National Solar Observatory, Kitt Peak, and synoptic maps of white-light K-coronal polarized brightness from the High Altitude Observatory. A determination of plasma temperature, T, can be estimated from the intensity ratio Fe X/Fe XIV (where T is inversely proportional to the ratio), since both emission lines come from ionized states of Fe, and the ratio is only weakly dependent on density. Distributions of the electron temperature from the line ratio and the polarized brightness which yields electron density of the corona during the descending and the ascending phases of solar cycles 21 and 22 are presented. These data refer to structures of the corona which are relatively large scale, having a temporal coherence of at least two or more synoptic rotation periods, such as the streamer belts, the individual helmet streamers, and the larger coronal holes. Title: The Coronal Index of Solar Activity, 1988-1991 Authors: Altrock, R. C.; Rybansky, M.; Rusin, V.; Gaspar, P. Bibcode: 1993BAAS...25.1200A Altcode: No abstract at ADS Title: The Solar Mass Ejection Imager Authors: Jackson, B. V.; Buffington, A.; Kahler, S. W.; Webb, D. F.; Altrock, R.; Gold, R. Bibcode: 1993BAAS...25.1191J Altcode: No abstract at ADS Title: Coronal photometry and analysis of the eclipse corona of July 22, 1990 Authors: Koutchmy, S.; Altrock, R. C.; Darvann, T. A.; Dzubenko, N. I.; Henry, T. W.; Kim, I.; Koutchmy, O.; Martinez, P.; Nitschelm, C.; Rubo, G. A. Bibcode: 1992A&AS...96..169K Altcode: Results are presented of aircraft-based observations and ground observations from multiple stations, made during the July 1990 eclipse. The main results of the analysis of the large-scale features of the inner corona concern the measurement of the flattening index of the near-maximum-activity corona; the occurrence of a large coronal hole; and the importance of the line emissions recorded on the broadband white-light pictures, due to the presence of numerous large or faint prominences all around the limb. Title: Ground-based coronagraphic observations of solar streamers. Authors: Altrock, Richard C. Bibcode: 1992ESASP.348...83A Altcode: 1992cscl.work...83A The purpose of this paper is two-fold: first, to demonstrate that ground-based coronagraphs can observe coronal streamers and, secondly, to give examples of the type of streamer properties that can be deduced from such observations. Emission-line and white-light (K-coronagraph) observations relating to streamer electron density, magnetic field and polarization, population, intensity, large-scale organization, rotation, temperature and periodicities are included. This paper will demonstrate the types of work that can be done. Title: The Current Status of the ``Extended Solar Cycle'' as Observed in Fe XIV Authors: Altrock, Richard C. Bibcode: 1992AAS...180.1104A Altcode: 1992BAAS...24..746A Investigation of the behavior of coronal intensity above the limb in Fe XIV emission (5303 Angstroms) obtained at the National Solar Observatory at Sacramento Peak over the last nineteen years has resulted in the confirmation of a second zone of solar activity at high latitudes separate from the Main Activity Zones (MAZ). Localized high-latitude intensity maxima are observed at 0.15 Rsun above the limb throughout the solar cycle. They persist long enough at a given latitude to be visible in long-term (e.g., annual) averages and thus form High-latitude Activity Zones (HAZ). We identify two types of HAZ. Poleward-moving PHAZ, which we identify with the ``Rush to the Poles'' phenomenon seen in polar-crown prominences, appeared near latitude 60(deg) in 1978 (possibly earlier at lower latitudes). In 1979 equatorward-moving EHAZ branched off from the PHAZ (which continued on to reach the poles in 1980) near 70 to 80(deg) . They evolved approximately parallel to the MAZ. Near solar minimum, the EHAZ evolved into the MAZ of Cycle 22, and the emission continues its monotonous path towards the equator, where it should disappear around 1998. As of early 1992, it is clear that the pattern seen earlier is repeating. The PHAZ became apparent near the beginning of 1988 near 60(deg) in the North and South hemispheres. The northern PHAZ reached the pole during late 1989 to 1990, and polar emission effectively ceased at the end of 1990. The southern PHAZ moved more slowly, and the southern-most emission regions reached the pole in mid-1991. South-polar emission was still occurring as of the latest observations. The EHAZ that are the precursors of sunspot Cycle 23 became clearly established in the Northern hemisphere near the beginning of 1990 at approximately 70(deg) . Currently the zone is at about 55(deg) . The appearance of the EHAZ in the South was less dramatic but probably began in mid-1990 near 70(deg) . Its current position is also near 55(deg) . These recent observations increase the evidence for parallel overlapping solar cycles that begin every 11 years but last for approximately 19-20 years. Title: Coronal Density and Temperature Structure from Coordinated Observations Associated with the Total Solar Eclipse of 1988 March 18 Authors: Guhathakurta, M.; Rottman, G. J.; Fisher, R. R.; Orrall, F. Q.; Altrock, R. C. Bibcode: 1992ApJ...388..633G Altcode: This paper explores and compares diagnostics for temperature and density within large-scale structures of the inner corona based on cospatial and cotemporal spectrophotometric observations made at the time of the total solar eclipse of 1988 March 17/18. In the analysis a determination of plasma temperature T can be derived unambiguously from the intensity ratios Fe XIV/XUV or Fe XIV/Fe X since all the emission lines come from the ionized state of Fe and the ratios are only weakly dependent on density. These temperatures and the densities found in well-defined large-scale coronal structures are discussed. The emission-line temperature is found to be high (local maxima) in the coronal structures with enhanced white-light emission and associated with new cycle high-latitude magnetic fields separated from the old cycle polar field of opposite polarity. Also the average of the ratio of scale-height temperature/temperature over the entire range of position angle is roughly unity although the ratio is higher than unity (1.3-1.6) in the three most prominent streamers. Title: Considerations of a Solar Mass Ejection Imager in a Low Earth Orbit Authors: Jackson, B. V.; Webb, D. F.; Altrock, R. C.; Gold, R. Bibcode: 1992LNP...399..322J Altcode: 1992esf..coll..322J; 1992IAUCo.133..322J We are designing an imager capable of observing the Thomson scattering signal from transient, diffuse features in the heliosphere[1]. The imager is expected to trace these features, which include coronal mass ejections, co-rotating structures and shock waves, to elongations greater than 90° from the Sun from a spacecraft in an 800 km Earth orbit. The predecessor of this instrument was the zodiacal-light photometer experiment on the HELIOS spacecraft which demonstrated the capability of remotely imaging transient heliospheric structures [2]. The HELIOS photometers have shown it possible to image mass ejections, co-rotating structures and the density enhancements behind shock waves. The second-generation imager we are designing, would have far higher spatial resolution enabling us to make a more complete description of these features from the Sun to 1 AU. In addition, an imager at Earth could allow up to three days warning of the arrival of a solar mass ejection. Title: The Solar Cycle Variation of Coronal Temperature during Cycle 22 Authors: Guhathakurta, M.; Altrock, R. C. Bibcode: 1992ASPC...27..395G Altcode: 1992socy.work..395G No abstract at ADS Title: Fe XIV and Fe X Limb Flux as Proxies for Space and Ground-Based Global Solar Parameters Authors: Altrock, R. C.; Henry, T. W. Bibcode: 1991BAAS...23.1068A Altcode: No abstract at ADS Title: The solar mass ejection imager Authors: Jackson, B.; Gold, R.; Altrock, R. Bibcode: 1991AdSpR..11a.377J Altcode: 1991AdSpR..11..377J We have designed an imager capable of observing the Thomson scattering signal from transient, diffuse features in the heliosphere from a spacecraft situated near 1 AU. The imager is expected to trace these features, which include coronal mass ejections, co-rotating structures and shock waves, to elongations greater than 90° from the Sun. The instrumentation ultimately may be regarded as a successor to the heliospheric imaging cabability shown possible by the zodiacal-light photometers of the HELIOS spacecraft. The second-generation instrument we have designed, would make far more effective use of in-situ solar wind data from spacecraft in the vicinity of the imager by extending these observations to the structures surrounding it. In addition, an imager at Earth could allow up to three days warning of the arrival of a mass ejection from the Sun.

Operated by the Association of Universities for Research in Astronomy, Inc., under cooperative agreement with the National Science Foundation. Partial support for NSO is provided by the USAF under a Memorandum of Understanding with the NSF. Title: The variation of solar Fe XIV and Fe X flux over 1.5 solar activity cycles. Authors: Altrock, Richard C. Bibcode: 1990NASCP3086..287A Altcode: 1990cisv.nasa..287A This paper presents a new source of data on the solar output, namely "limb flux" from the one- and two-million degree corona. This parameter is derived from data obtained at the National Solar Observatory at Sacramento Peak with the 40 cm coronagraph of the John W. Evans Solar Facility and the Emission Line Coronal Photometer. The limb flux is defined to be the latitude-averaged intensity in millionths of the brightness of disk center from an annulus of width 1.1' centered at a height of 0.15 Rsun above the limb of emission from lines at 6374 Å (Fe X) or 5303 Å (Fe XIV). Fe XIV data have been obtained since 1973 and Fe X since 1984. Examination of the Fe XIV data shows that there is ambiguity in the definition of the last two solar activity minima, which can affect the determination of cylce rise times and lengths. There is an indication that a constant minimum or basal corona may exist at solar minimum. Cycle 22 has had a much faster onset than Cycle 21 and has now overtaken Cycle 21. The rise characteristics of the two cycles were very similar up until Jul-Aug 1989, at which time a long-term maximum occurred in Fe X and Fe XIV, which could possibly be the "solar maximum". Another maximum is developing at the current time. Cycle 21 was characterized in Fe XIV by at least 4 major thrusts or bursts of activity, each lasting on the order of a year and all having similar maximum limb fluxes, which indicates that coronal energy output is sustained over periods in which the sunspot number declines significantly. Dramatic increases in the limb fluxes occur from minimum to maximum, ranging from factors of 14 to 21 in the two lines. Two different techniques to predict the epoch of solar maximum have been applied to the Fe XIV data, resulting in estimates of Apr 1989 (±1 mo) and May 1990 (±2 mo). Title: A Search for Non-Rotational Periodicities in Solar Fe XIV and Fe X Flux During Solar Cycles 21 and 22 Authors: Altrock, R. C.; Radick, R. R.; Henry, T. W. Bibcode: 1990BAAS...22..873A Altcode: No abstract at ADS Title: The Onset of Solar Cycle 22 in Coronal Emission Lines Authors: Altrock, R. C. Bibcode: 1989BAAS...21..829A Altcode: No abstract at ADS Title: Rotation Characteristics of the Fe XIV (5303 Angstrom ) Solar Corona Authors: Sime, D. G.; Fisher, R. R.; Altrock, R. C. Bibcode: 1989ApJ...336..454S Altcode: The rotational characteristics of the solar corona as revealed by the coronal Fe XIV line at 5303 A are examined. Measurements of the intensity at 5303 A observed at a radius of 1.15 solar radii between 1973 and 1985 are presented. It is found that, on average, the Fe XIV corona rotates more rigidly than do features in the photosphere or chromosphere. The observations support the theory that the Fe XIV coronal signal arises from the effects of local heating on the large-scale density structure of the corona. Title: SYSTEMATIC OBSERVATIONS OF THE SUN (In honour of Helen Dodson Prince): Observations Authors: McIntosh, P.; Snodgrass, H.; Mouradian, Z.; Harvey, K.; Altrock, R.; Simon, P.; Legrand, J. -P.; Alissandrakis, G.; Neckel, H.; Petropoulos, P.; Poulakis, X.; Gokhale, M. H.; Sivaraman, K. R.; Pap, J. Bibcode: 1989HiA.....8..672M Altcode: No abstract at ADS Title: Further Evidence for an Extended Solar Cycle Authors: Altrock, R. C. Bibcode: 1988BAAS...20..723A Altcode: No abstract at ADS Title: Observations of the Sun and Corona for the 1988 March 18 Total Solar Eclipse Authors: Orrall, F. Q.; Lindsey, C. A.; Mickey, D. L.; Dulk, G.; Rottman, G.; Altrock, R. C.; Fisher, R. R.; Sime, D. G. Bibcode: 1988BAAS...20..703O Altcode: No abstract at ADS Title: Solar and stellar coronal structure and dynamics. A Festschrift in honor of Dr. John W. Evans. Proceedings. Authors: Altrock, Richard C. Bibcode: 1988sscd.conf.....A Altcode: Contents: 1. Stellar coronae. 2. Winds, holes, and bright points. 3. Waves, oscillations, and heating. 4. Prominence interface. 5. Structures and miscellaneous. 6. Solar-cycle variations. 7. Observations and models of magnetic fields. 8. Mass ejections, transients, and flares. Appendices. Title: The solar emission-line corona: current and future ground-based observational research. Authors: Altrock, R. C. Bibcode: 1988sscd.conf..288A Altcode: This is a review of discussions on the status of ground-based solar coronal research, which took place during the Workshop on Solar and Stellar Coronal Structure and Dynamics. Topics of discussion included current observational capabilities, research problems suitable for attack now and in the future, and possible future instrumentation, including the Advanced Reflecting Coronagraph. Title: Variation of solar coronal Fe XIV 5303 Å emission during solar Cycle 21. Authors: Altrock, Richard C. Bibcode: 1988sscd.conf..414A Altcode: Investigation of the behavior of coronal intensity above the limb in Fe XIV emission (5303 Å) obtained at Sacramento Peak Observatory over the last fourteen years has resulted in the corfirmation of a second set of zones of solar activity at high latitudes separate from the Main Activity Zones (MAZ). Localized emission peaks in Fe XIV 5303 Å are observed through most of the cycle at high latitudes in individual daily scans, annual averages, and solar-cycle summary plots of the location of all local maximum intensities at 0.15 Rsun above the limb. Near solar minimum, the high-latitude coronal activity zones that appeared after the beginning of Cycle 21 monotonically evolved into the MAZ of Cycle 22. It thus appears that we have evidence for parallel overlapping solar cycles that begin every 11 years but last for approximately 19 - 20 years Title: The Fe 15 solar corona at 5303 angstroms: an atlas of synoptic charts from the Sacramento Peak coronal photometer, May 1973-December 1985 Authors: Altrock, R. C.; Gilliam, L. B.; Sime, D. G.; Fisher, R. R. Bibcode: 1987scasc....Q....A Altcode: Synoptic photoelectric observations of the solar corona in the emission from the green line (5303A) of Fe 15 were begun at the Sacramento Peak Observatory in June 1973 and continue to the present. The observations made during this program provide a record of the distribution and brightness of the hotter regions of the corona (1,800,000 K) over an entire solar cycle. As such, the green line data may provide a link between the active regions of the chromosphere and the large scale structure of the corona. In order to allow comparison of these data with other observations of the Sun and corona, we present here an atlas of the green line measurements in the same format as that used to display the white light coronal structure recorded by the High Altitude Observatory's K-coronameters on Mauna Loa, in previously published atlases. It is our intent that this atlas be brought up to date periodically as the observations permit. Title: Long Term Variations in the Integrated Fe XIV Green Line Flux (5303 Å) from the Solar Corona Authors: Yasukawa, E. A.; Altrock, R. C.; Sime, D. G.; Fisher, R. R. Bibcode: 1987BAAS...19..926Y Altcode: No abstract at ADS Title: Fe XIV solar corona at 5303 angstroms: an atlas of synoptic charts from the Sacramento Peak coronal photometer, May 1973-December 1985 Authors: Altrock, R. C.; Gilliam, L. B.; Sime, D. G.; Fisher, R. R. Bibcode: 1987scasc....R....A Altcode: Presented is an atlas of synoptic charts from the Sacramento Peak Coronal Photometer, of the Fe XIV solar corona at 5303 Angstroms. The data covers the period from May 1973 until December 1985. Title: The SOLAR-CYCLE-21 Variation of High-Latitude Coronal Fexiv Emission Authors: Altrock, R. C. Bibcode: 1986PASP...98.1100A Altcode: No abstract at ADS Title: Overlapping Solar Cycles as Discovered in Coronal Fe XIV Emission Authors: Altrock, R. C. Bibcode: 1986BAAS...18.1010A Altcode: No abstract at ADS Title: The Solar-Cycle 21 Variation of High-Latitude Coronal Fe XIV Emission Authors: Altrock, R. C. Bibcode: 1986BAAS...18R.709A Altcode: No abstract at ADS Title: Coronal Emission-Line Data and Solar-Terrestrial Predictions Authors: Altrock, R. Bibcode: 1986stp..conf..131A Altcode: 1986STP.....2..131A No abstract at ADS Title: The Relationship of Emission-Line Transients in the Low Solar Corona to Hα Activity Authors: Altrock, R. C.; Smith, R. C. Bibcode: 1985BAAS...17Q.842A Altcode: No abstract at ADS Title: Coronal-Hole Detectability on Solar-type Stars Authors: Altrock, R. C. Bibcode: 1985ASSL..116..243A Altcode: 1985rst..conf..243A It is shown that light from the solar corona, which is integrated over the visible disk (coronal flux or irradiance), can be used to infer the disk passage of large coronal holes. Observations above the limb of Fe XIV 5303 A are used to produce a synoptic intensity map of the solar disk as it would appear in coronal light. The intensity at each point on the map is summed to produce a daily value of coronal irradiance. The time variation of this quantity shows a decrease of 28 percent, followed by recovery, as a large coronal hole transits the disk from March 21 through April 7, 1984. The occurrence of a coincident geomagnetic disturbance implies that the associated high-speed solar-wind stream strikes the earth. Other solar data sets, specifically sunspot number and 10.7 cm radio flux, do not have unambiguous coronal hole signatures during this period. This technique suggests that coronal holes might be observed on stars, if a suitable method for isolating coronal radiation is used; e.g., radio or EUV. Title: Results from the Coronal Photometry Program at NSO, I: Three-Line Observations of the Corona in 1984 Authors: Altrock, R. C.; Fisher, R. R.; Sime, D. G. Bibcode: 1985BAAS...17..637A Altcode: No abstract at ADS Title: Results from the Coronal Photometry Program at NSO, III: The Green Line and White Light Corona Compared Authors: Fisher, R. R.; Altrock, R. C.; Sime, D. G. Bibcode: 1985BAAS...17..638F Altcode: No abstract at ADS Title: Results from the Coronal Photometry Program at NSO, II: Rotation of the Green Corona over the Solar Cycle Authors: Sime, D. G.; Fisher, R. R.; Altrock, R. C. Bibcode: 1985BAAS...17..638S Altcode: No abstract at ADS Title: Solar coronal white light, Fe 10, Fe 14 and CA 15 observations during 1984: an atlas of synoptic charts Authors: Sime, D. G.; Fisher, R. R.; Altrock, R. C. Bibcode: 1985STIN...8616179S Altcode: Synoptic observations of the solar corona in white light and in three emission lines (CaXV at 5964 A, FeXIV at 5303 A, and Fe X at 6374 A) were carried out during most of 1984 at the High Altitude Observatory's Mauna Loa Solar Observatory and at Sacramento Peak Observatory. These observations were partly in support of the scientific program of the repaired SMM spacecraft. The observations provide a record of the distribution and brightness of the hotter regions of the corona over the year. The authors present these data in the form of synoptic maps for each rotation during the year for the purpose of providing a context for the investigations which are to take place during the Joint Study of Coronal and Prominence Plasmas organized by Goddard Space Flight Center/NASA. In this way, they propose both to describe the data coverage achieved and summarize the large scale properties of the corona in this late descending phase of the solar cycle. Title: Coronal-Hole Detectability on Solar-Type Stars Authors: Altrock, R. C. Bibcode: 1984BAAS...16..939A Altcode: No abstract at ADS Title: Sacramento Peak Observatory Observing Weather and the El Nino Phenomenon Authors: Altrock, R. C. Bibcode: 1984BAAS...16..478A Altcode: No abstract at ADS Title: The Evolution of an Average Solar Granule Authors: Altrock, R. C. Bibcode: 1984ssdp.conf..130A Altcode: High-resolution photographic spectra of the center of the solar disk have been obtained with the Vacuum Tower Telescope at Sacramento Peak Observatory. A weak iron line and the neighboring continuum were recorded with 40 sec time resolution and better than 1arcsec spatial resolution over a period of 37 min. Intensity and velocity fluctuations were obtained in the line and continuum as a function of time and space, and 300 sec oscillations were filtered out. The resulting fluctuations, due solely to granulation, were assembled into an ensemble average of the center of a granule and the center of an intergranular lane, as a function of time. It is found that the line parameters are distinctly out of phase with continuum brightness. Title: Coronal transients in Fe XIV 5303 Å: first two-dimensional photoelectric ground-based observations. Authors: Altrock, R. C.; Demastus, H. L. Bibcode: 1983NASCP.2280..63A Altcode: 1983sowi.conf...63A An observational program was undertaken at Sacramento Peak Observatory to photoelectrically detect coronal transients. Continuous observations are made in the Fe XIV 5303A green line, utilizing the 40 cm coronagraph and the Photoelectric Coronal Photometer. Scans at three heights above the limb are combined to form a low resolution picture of the greenline corona every 20 to 30 minutes. Difference pictures, relative to an initial scan, are generated to search for sudden changes in the corona. The first few days of operation of this program have yielded three low-lying events ( 1.55 solar radii) following minor chromospheric activity (a surge and eruptive prominences), which propagated up through the corona with velocities on the order of 100 km/s. Title: Solar Continuum-Intensity Oscillations in the Five-Minute Band Authors: Altrock, R. C. Bibcode: 1983BAAS...15..952A Altcode: No abstract at ADS Title: Coronal Transients as Observed in Fe XIV 5303 A at Sacramento Peak Observatory Authors: Altrock, R. C.; Demastus, H. L. Bibcode: 1983BAAS...15R.706A Altcode: No abstract at ADS Title: The Evolution of an Average Solar Granule Authors: Altrock, R. C.; Musman, S. Bibcode: 1981BAAS...13..879A Altcode: No abstract at ADS Title: Is Granulation a Periodic Phenomenon? Authors: Altrock, R. C.; Musman, S. Bibcode: 1980BAAS...12..894A Altcode: No abstract at ADS Title: Solar Photospheric Evolution During the Lifetime of a Granule Authors: Altrock, R. C. Bibcode: 1980BAAS...12..474A Altcode: No abstract at ADS Title: Anomalous Satellite Drag and the Green Line Corona (refereed) Authors: Altrock, R. C. Bibcode: 1980STP.....4....1A Altcode: No abstract at ADS Title: The Evolution of an Average Solar Granule Authors: Altrock, R. C. Bibcode: 1980LNP...114...51A Altcode: 1980sttu.coll...51A; 1980IAUCo..51...51A No abstract at ADS Title: Physical Development of an Average Solar Granule Authors: Altrock, R. C.; Musman, S. Bibcode: 1979BAAS...11..641A Altcode: No abstract at ADS Title: Recurrent geomagnetic disturbances and coronal holes as observed in Fe XIV λ5303 Å Authors: Musman, S.; Altrock, R. C. Bibcode: 1978JGR....83.4817M Altcode: We present data obtained with the Fe XIV λ5303-Å coronal photometer of the Sacramento Peak Observatory for the period October 3 to December 22, 1976. During this period there was a pattern of three coronal holes and three emission regions near the solar equator. Recurrent geomagnetic disturbances were associated with two of these three holes. We propose a simple method for predicting recurrent geomagnetic disturbances were associated with two of these three holes. We propose a simple method for predicting recurrent geomagnetic disturbances at times of low solar activity based on coronal brightness and test it on our data. We show that the method gives correct results 72% of the time, compared with 64% for 27 day recurrence. Title: Time Development of Solar Granulation Authors: Altrock, R. C.; Musman, S. Bibcode: 1978BAAS...10..623A Altcode: No abstract at ADS Title: Intensity, velocity and temperature fluctuations in the upper solar atmosphere. Authors: Altrock, R. C.; Keil, S. L. Bibcode: 1977A&A....57..159A Altcode: High-spatial-resolution photographic spectra of the Mg I 4571-A line at 10 solar disk positions from center to limb are reduced to yield intensity and velocity (line-shift) fluctuations along the spectrograph slit for a height of about 300 km above the continuum level. The data obtained are used to compute rms intensity and velocity fluctuations corrected for instrument smearing. Comparison of the results with those of Cannon and Wilson (1971) reveals a flatter distribution of the rms intensity fluctuation as a function of heliocentric angle and a 60% larger fluctuation at the disk center. It is inferred that the correlation between velocity and intensity fluctuations exhibits a large-scale random structure. The intensity-fluctuation data are analyzed by calculating the emergent intensity from a three-dimensional atmosphere having a sinusoidal checkerboard pattern of temperature with a height-dependent amplitude, taking into account fluctuations in electron pressure. The range of solutions for temperature fluctuations is found to indicate that there are causes other than oscillations for the temperature fluctuations in the upper photosphere. Title: Coronal holes as observed in Fe XIV 5303 Å. Authors: Altrock, R. C.; Musman, S. A. Bibcode: 1977BAAS....9R.432A Altcode: No abstract at ADS Title: The horizontal variation of temperature in the low solar photosphere. Authors: Altrock, R. C. Bibcode: 1976SoPh...47..517A Altcode: Observations of the rms intensity fluctuations in the continuum obtained by Pravdjuk et al. (Solnechnye Dannye, No. 2, p. 70, 1974) from white-light photographs made with the Soviet Stratospheric Solar Observatory are analyzed to obtain a horizontal temperature-fluctuation amplitude as a function of depth. The results indicate that temperature fluctuations increase with depth monotonically from a small value at τ5000≅0.5 (cf. Figure 2). The initial rise of ΔT appears quite steep, having a slope of approximately 20 K km−1. The model of Wilson (Solar Phys.9, 303, 1969) is incompatible with the data. Convective flux in the present model is approximately 6% of the total flux at τ5000 = 1. Title: Convective Flux in the Visible Photosphere Authors: Altrock, R. C. Bibcode: 1976BAAS....8..324A Altcode: No abstract at ADS Title: Physical conditions in granulation. Authors: Altrock, R. C.; Musman, S. Bibcode: 1976ApJ...203..533A Altcode: High-resolution spectroheliograms made in the Ti I and Fe I 5016-A lines with the diode array of a tower telescope are analyzed. Temperature perturbations (delta T) were introduced into the Harvard-Smithsonian Reference Atmosphere and varied empirically until the calculated line profiles matched the observed profiles. It is found that the absolute value of delta T increases going downward in the low photosphere. In the middle photosphere, the absolute value does not exceed 70 K. It is also found that the large buoyant forces implied by the solutions for delta T are inconsistent with the small observed accelerations in the granular flow. It is concluded that this incompatibility provides additional evidence besides line broadening for the existence of microturbulence in the low photosphere. The convective flux at an optical thickness of 3 (5000 A) is small compared with the total flux. Also, the temperature fluctuations are much larger than those that would be produced by the observed convective velocities alone. Thus, the observable low photosphere appears to be near radiative equilibrium. Title: Research at Sacramento Peak Observatory Authors: Altrock, Richard Bibcode: 1976srca.conf...89A Altcode: No abstract at ADS Title: Physical condition in granulation Authors: Altrock, R. C.; Musman, S. Bibcode: 1976pmas.conf..285A Altcode: No abstract at ADS Title: Heights of Formation of Non-Magnetic Solar Lines Suitable for Velocity Studies Authors: Altrock, R. C.; November, L. J.; Simon, G. W.; Milkey, R. W.; Worden, S. P. Bibcode: 1975SoPh...43...33A Altcode: Heights of formation of lines that do not exhibit Zeeman splitting are calculated using an LTE, partial non-LTE, and full non-LTE approach. Non-magnetic (g=0) lines are valuable for velocity investigations in quiet-Sun magnetic field regions, and a knowledge of their formation heights is useful for obtaining three dimensional velocity profiles in these regions. Title: Horizontal Temprature Fluctuations in the Low Solar Photosphere. Authors: Altrock, R. C. Bibcode: 1975BAAS....7..406A Altcode: No abstract at ADS Title: The Formation of Mg I 4571 Å in the Solar Atmosphere. V: The Multi-Dimensional Structure of the Photosphere and Low Chromosphere Authors: Altrock, R. C.; Cannon, C. J. Bibcode: 1975SoPh...42..289A Altcode: The two-dimensional equation of transfer is solved for the case of locally-controlled source function (LTE) and radiationally-controlled ionization. Horizontal fluctuations in electron temperature and macroscopic velocity fields are superposed on the basic one-dimensional model (cf. Altrock and Cannon, 1972). Output intensities are compared with observed rms intensity fluctuations and spatially-averaged intensities in Mg I 4571 Å. We find that at least one model (with a height-independent temperature fluctuation ΔT/T=±0.02 in the range 0⩽h⩽450 km) can predict the magnitude of the intensity fluctuations in both the continuum and λ4571 Å. The asymmetry of the line can be explained by adding a height-independent, temperature-correlated flow of amplitude 1 to 2 km s−1. The relationship between these results and other multi-dimensional analyses is discussed. Title: Physical Conditions in Granulation Authors: Altrock, R. C.; Musman, S. Bibcode: 1975BAAS....7..362A Altcode: No abstract at ADS Title: Analysis of the solar magnesium I spectrum. Authors: Altrock, R. C.; Canfield, R. C. Bibcode: 1974ApJ...194..733A Altcode: Without assuming local thermodynamic equilibrium (LTE), we simultaneously solve the equations of statistical equilibrium and radiative transfer for a model Mg I atom that includes the lines 4571, 5172 (b2), and 2852 A, which we then compare with observations. From this comparison we determine by trial and error an optimum model of run with height of electron temperature, electron density, and total hydrogen density, and microturbulent velocity in the solar atmosphere up to approximately h = 1000 km. In addition, we show that the assumption of LTE for the 4571 A source function is valid to a high degree of precision. Title: The multi-dimensional structure of the photosphere and low chromosphere of the sun. Authors: Altrock, R. C.; Cannon, C. J. Bibcode: 1974BAAS....6..428A Altcode: No abstract at ADS Title: A Two-Dimensional Analysis of Intensity Fluctuations in MgI 4571 A on the Solar Disk Authors: Altrock, Richard C.; Cannon, C. J. Bibcode: 1974BAAS....6Q.284A Altcode: No abstract at ADS Title: The Formation of Mg I 4571 Å in the Solar Atmosphere. IV: Empirical vs Synthetic Analyses Authors: Altrock, Richard C. Bibcode: 1974SoPh...34...37A Altcode: A comparison is made of synthetic and empirical analyses for the 4571 Å line of Mg I. First, several different inversion techniques are applied to synthetic line profiles. The results show that at least some of these techniques are able to correctly reproduce the input atmosphere to a reasonable degree. Secondly, these same techniques are applied to equivalent observational data. In this case some of the techniques yield results that can be shown to be of comparable quality to the synthetic analysis. I conclude that although the synthetic method is the best method to use in analyzing observations, some of the simpler empirical methods produce acceptable results in specified restricted cases. Title: A Non-L.T.E. Analysis of the Solar Mg I Spectrum. Authors: Altrock, R. C.; Canfield, R. C. Bibcode: 1974BAAS....6..220A Altcode: No abstract at ADS Title: A non-L.T.E. analysis of the solar Mg I spectrum. Authors: Altrock, R. C.; Canfield, R. C. Bibcode: 1974BAAS....6..219A Altcode: No abstract at ADS Title: Erratum: "The formation of Mg I 4571 Å in the solar atmosphere. II: The effect of one-dimensional macroscopic velocity fields [Sol. Phys., Vol. 29, p. 275 - 286 (1973)]. Authors: Altrock, R. C.; Cannon, C. J. Bibcode: 1973SoPh...31..524A Altcode: No abstract at ADS Title: The Formation of Mg I 4571 Å in the Solar Atmosphere. II: The Holweger Solar Model Authors: Altrock, Richard C.; Cannon, C. J. Bibcode: 1973SoPh...30...31A Altcode: No abstract at ADS Title: The Formation of Mg I 4571 Å in the Solar Atmosphere. II: The Effect of One-Dimensional Macroscopic Velocity Fields Authors: Altrock, Richard C.; Cannon, C. J. Bibcode: 1973SoPh...29..275A Altcode: An analysis of the 4571 Å line of neutral magnesium is presented in which one-dimensional macroscopic velocity fields are included. It is shown that gradients over restricted heights in the vertical and horizontal components of the velocity field of order -0.005 s−1 and -0.004 s−1 (such that velocity towards the observer decreases as height increases), respectively, result in asymmetries in the computed line profile similar to those observed. The heights in the solar atmosphere at which these velocity gradients exist are shown to be very critical in reproducing the observations. It was found that the best results were obtained when the gradients existed in the height range from ∼ 200 km to ∼ 300 km below the temperature minimum. The results indicate that for the Mg I 4571 Å line model calculations that do not include one-dimensional flow velocities may safely be compared with frequency-averaged observations. Title: A One-Dimensional Approximation to the Macroturbulent Velocity Field in the Solar Atmosphere Authors: Altrock, R. C.; Cannon, C. J. Bibcode: 1973BAAS....5R.268A Altcode: No abstract at ADS Title: Empirical analysis of solar absorption line profiles. Authors: Altrock, R. C. Bibcode: 1973PASP...85R.529A Altcode: No abstract at ADS Title: Erratum: The Minimum Temperature in the Solar Atmosphere. Authors: Altrock, R. C.; Cannon, C. J. Bibcode: 1972BAAS....4..426A Altcode: No abstract at ADS Title: The Formation of Mg I 4571 Å in the Solar Atmosphere. I: A Model Analysis of a One-Dimensional Static Atmosphere Authors: Altrock, Richard C.; Cannon, C. J. Bibcode: 1972SoPh...26...21A Altcode: A one-dimensional analysis of the 4571 Å line of neutral magnesium is presented. The Harvard-Smithsonian Reference Atmosphere (HSRA) and the Bilderberg Continuum Atmosphere (BCA) are used to compute the emergent line profiles at various positions on the solar disc. The resultant profiles, when compared to the observations, indicate that the HSRA electron temperature distribution is a more satisfactory representation of the solar atmosphere in the region of the temperature minimum than is the BCA. A slight modification to the HSRA is suggested which reduces the minimum temperature to 4140K and enables an even more satisfactory `fit' to the available data. Title: The Minimum Temperature in the Solar Atmosphere. Authors: Altrock, R. C.; Cannon, C. J. Bibcode: 1972BAAS....4..310A Altcode: No abstract at ADS Title: Observations of Photospheric Pole-Equator Temperature Differences Authors: Altrock, Richard C.; Canfield, Richard C. Bibcode: 1972SoPh...23..257A Altcode: Using photoelectric methods we have repeated Plaskett's (1970) measurements of poleequator temperature differences. We average many limb-darkening scans to reduce statistical errors. We then analyze the differences between the average polar and equatorial scans. Plaskett's large poleequator temperature differences are not confirmed. Our data yield a pole-equator temperature difference of 1.5K±0.6K, although we cannot rule out systematic errors of 3-4 K. Title: Observations of the variation of temperature with latitude in the upper solar photosphere. Authors: Altrock, R. C.; Canfield, R. C. Bibcode: 1972BAAS....4..268A Altcode: No abstract at ADS Title: Measurements of the limb darkening in the forbidden Mg i line at 4571.1 Å Authors: White, O. R.; Altrock, R. C.; Brault, J. W.; Slaughter, C. D. Bibcode: 1972SoPh...23...18W Altcode: We report high resolution measurements of the center-to-limb variation of the MgI line at 4571.1 Å. This forbidden line is of interest because it should be formed in LTE. Comparison of our measurements with the Harvard-Smithsonian Reference Atmosphere show that the line center radiation originates in the temperature minimum region from 330 to 550 km above the point where τcontinuum = 1. Observations near the limb confirm that the temperature minimum is ∼4200K. Title: Observations of the Variation of Temperature with Lattitude in the Upper Solar Photosphere Authors: Altrock, Richard C.; Canfield, Richard C. Bibcode: 1972ApJ...171L..71A Altcode: We made photoelectric meridional and equatorial limb-darkening scans during the period 15-22 June 1971, using a spectral region of 30 mA width centered 0.77 A to the red of Ca II K3. The radiation observed originates at r5000 10 . At the time of our observations the temperature relative to the equatorial temperature was enhanced by 8 K + 2.5 K at active-region latitudes and 5 K + 2 K at latitude 50 N. Title: An empirical analysis of the infrared triplet of O I. Authors: Altrock, R. C. Bibcode: 1971BAAS....3..259A Altcode: No abstract at ADS Title: The Empirical Analysis of Triplet Line Profiles Authors: Altrock, Richard C. Bibcode: 1970BAAS....2S.290A Altcode: No abstract at ADS Title: Source Functions of Infrared Fraunhofer Lines from Equivalent Widths Authors: Altrock, Richard C. Bibcode: 1969BAAS....1T.270A Altcode: No abstract at ADS Title: Interpretation of Infrared Oxygen Spectroheliograms Authors: Altrock, Richard C. Bibcode: 1969SoPh....7..343A Altcode: Spectroheliograms have been obtained in the line cores of two infrared multiplets of neutral oxygen. Those made in the lines of the 7770 Å multiplet show a very smooth intensity distribution, with faculae and sunspot penumbrae at a very low contrast with respect to the undisturbed photosphere. Spectroheliograms made in the core of λ 8446.37 Å show evidence of coupling with chromospheric features and of blending with a line of neutral iron. Title: Source Functions of Infrared Fraunhofer Lines from Equivalent Widths Authors: Altrock, Richard C. Bibcode: 1969SoPh....7....3A Altcode: A method for obtaining the source function and value of r0 □ kc/kL,0 from the variation of equivalent width across the solar disk has been applied to several infrared Fraunhofer lines. The results indicate that most of the lines investigated have non-L.T.E. source functions which are less than or equal to the mean continuum intensity. DE JAGER and NEVEN (1968) appear to have underestimated the departures from L.T.E. in a number of cases. Title: A New Method for the Analysis of Equivalent Widths and its Application to Solar Photospheric Oxygen Authors: Altrock, Richard C. Bibcode: 1968SoPh....5..260A Altcode: Six neutral atomic oxygen Fraunhofer multiplets were observed at nine disk positions at Sacramento Peak Observatory. I filtered the data, corrected them for the instrumental profile and obtained equivalent widths. Title: A Study of Neutral Atomic Oxygen in the Solar Atmosphere. Authors: Altrock, Richard Charles Bibcode: 1968PhDT.........1A Altcode: No abstract at ADS