1 1 Introduction to Special Issue on High Speed Solar Wind Streams and 2 Geospace Interactions (HSS-GI). 3 4 M. H. Denton1, J. E. Borovsky2, R. B. Horne3, R. L. McPherron4, S. K. Morley5, and B. T. Tsurutani6. 5 6 7 1 2 Department of Communication Systems, Lancaster University, Lancaster, UK. Space Science and Applications, Los Alamos National Laboratory, Los Alamos, USA. 8 3 British 9 4 IGPP, 10 11 Antarctic Survey, Cambridge, UK. University of California at Los Angeles, Los Angeles, USA. 5 University 6 Jet of Newcastle, Newcastle, Australia. Propulsion Laboratory, California Institute of Technology, Pasadena, USA. 12 13 14 1 2 15 1. Introduction 16 This special issue of the Journal of Atmospheric and Solar-Terrestrial Physics is devoted to research into high 17 speed solar wind streams (HSSs) and their effects on the region of near-Earth space commonly known as 18 ‘geospace’. Interest in the effects of HSSs has increased during the last solar cycle and, following the successful 19 meeting focusing on corotating solar wind streams in Manaus, Brazil [Tsurutani et al., 2006], we recognised the 20 need for further work on the topic, with particular focus on HSSs and their effects in the inner magnetosphere, 21 ionosphere, and neutral atmosphere. As a result the High Speed Solar Wind Streams and Geospace Interactions 22 (HSS-GI) Workshop was held at Hilltop, St. Martin’s College in Ambleside, UK, from 2 nd to 7th September, 23 2007 [Kavanagh and Denton, 2007; Denton et al., 2008], sponsored by the Department of Communication 24 Systems at Lancaster University. The majority of the work presented in this special issue was prompted by 25 discussion and interaction at the workshop. It is indeed an indication of the importance of HSSs that the papers 26 in this issue cover the entire region from the Sun and solar wind, through the magnetosphere, and into the 27 ionosphere, thermosphere, and down to the stratosphere. It is hoped that this research will stimulate more 28 understanding, appreciation, and research, into these important drivers of physical phenomena within geospace. 29 30 2. High Speed Solar Wind Streams - Recent Progress 31 Periodic high speed solar wind streams have been known to exist since research by Snyder et al. [1963], with the 32 source of such streams being traced to solar coronal holes by Krieger et al. [1973]. Since this early work, 33 further links between HSSs and recurrent activity within geospace have been reported by numerous authors, and 34 the relationship between such events and phenomena within the magnetosphere has become increasingly 35 apparent. Superposed epoch analyses of the solar wind characteristics of HSSs reveal their broad features, the 36 response of geomagnetic indices during their passage of the magnetosphere, and the Russell-McPherron 37 dependence of the coupling between the solar wind and the magnetosphere [McPherron et al., 2008]. 38 39 As is widely known, HSSs typically produce less significant deflections in geomagnetic indices such as Dst than 40 transient phenomena such as coronal mass ejections (CMEs). As a result HSSs are sometimes regarded as less 41 important drivers of geomagnetic activity. This has led to many studies, where event-selection is based solely on 42 the Dst signature, overlooking HSS-events and hence neglecting their significance. At the workshop, this was 43 referred to as ‘the Dst mistake’. Comparisons between HSS-driven events and CME-driven events do reveal 44 important differences in their effects within all regions of geospace (e.g. Lindsay et al. [1995]; Borovsky and 45 Denton [2006]) and whilst CME-events certainly produce the largest geomagnetic storms, HSS-events are 2 3 46 particularly important for phenomena such as relativistic electron acceleration, radiation belt enhancements and 47 satellite anomalies (e.g. Wrenn et al. [2008]). In terms of the energy input to the magnetosphere, HSSs are 48 found to input a total-energy-per-event which is similar in magnitude to that during CMEs; indeed the ratio of 49 the energy-deposited-in-the-magnetosphere to the energy-input-to-the-magnetosphere appears to be greater for 50 HSSs than for CMEs (e.g. Turner et al. [2006; 2008]; Kozyra et al. [2006]; Guarnieri et al. [2006]). 51 52 It is known that HSSs are particularly important for acceleration and loss processes in the Earth’s radiation belts 53 and in recent years much interest in the community has focused on determining the principal acceleration and 54 loss mechanisms (e.g. Tsurutani et al. [2006]; Horne, [2007]; Liemohn and Chen, [2007]; Reeves [2008]). An 55 important source population for the ring current/radiation belts is the Earth’s plasma sheet and in this issue the 56 timescales for delivery of plasma sheet material to the inner magnetosphere during HSSs are evaluated by 57 Denton and Borovsky [2008]. Results indicate a super-hot and super-dense plasma sheet forms at the onset of a 58 HSS-driven storm and is convected Earthwards in a period of a few hours. Energisation of this plasma sheet 59 population during HSSs leads to formation of a enhanced ring current [Jordanova et al., 2008; Sørbø et al., 60 2008] which is subsequently energised leading to enhanced fluxes in the radiation belts. Fluxes within the belts 61 may fluctuate rapidly during HSSs revealing the balance between sources and sinks, and also our ability to 62 reproduce such fluctuations using theoretical models [Lam et al., 2008]. The derivation of radiation belt radial 63 diffusion coefficients during periods of high speed solar wind is discussed by Rae et al. [2008] who also 64 examine the solar wind speed dependence of ULF wave power using ground-based magnetometer data. 65 66 Recently, a number of authors have revealed the importance of a 9-day periodicity in the solar wind speed and 67 consequences for the lower atmosphere (e.g. Temmer et al., [2007]; Lei et al. [2008]; Mlynczak et al. [2008]; 68 Thayer et al. [2008]). In this issue Emery et al. [2008] show that the global electron hemispheric power (a proxy 69 for the strength of auroral activity) also exhibits a 9-day periodicity. Loss of energetic particles from the 70 magnetosphere into the atmosphere induces detectable changes in the Earth’s ionosphere where an 71 decrease/increase in spectral hardness is evident during HSSs [Birch et al., 2008]. Such energetic particle 72 precipitation (particularly relativistic electron precipitation during HSSs) may induce the generation of NOx 73 (odd nitrogen) at lower altitudes, with possible subsequent links to ozone depletion in the stratosphere [Turunen 74 et al., 2008]. 75 3 4 76 The large amplitude Alfvénic fluctuations which occur during HSSs have implications for the generation of 77 recurrent substorms [Lyons et al., 2008; Morley et al., 2008], HILDCAAs [Tsurutani and Gonzalez, 1987], 78 source and loss processes within the radiation belts [Sandanger et al., 2008], and for resultant auroral activity 79 [D’Amicis et al., 2008]. Whilst it is clear that the southward-IMF coupling between the solar wind and the 80 magnetosphere during Alfvénic fluctuations is important, it is still not clear whether there is a significant 81 difference between the driving of the magnetosphere in an on-off fashion versus a steady average fashion 82 [Denton et al., 2008]. In the future we plan to determine whether or not such on-off driving is important. 83 84 Although the papers contained in this special issue highlight the importance of high speed solar wind streams, 85 and also reveal how physical processes within geospace respond to HSS-events, it is clear that much remains to 86 be discovered about these fascinating phenomena. 87 88 3. Acknowledgements 89 The authors would like to thank everyone who helped make the 2007 Ambleside workshop such a successful and 90 productive meeting. Thanks are due to the Faculty of Science and Technology, the Photonic Band Gap Research 91 Group, and InfoLab21 at Lancaster University, all of whom provided funding in support of the workshop. 92 Particular thanks are due to Jill Greenwood and Joanna Denton for assistance in organising the workshop and to 93 our hosts at St. Martin’s College in Ambleside. The authors also express their thanks to Meta Ottevanger, Tim 94 Horscroft, William Lokto, and the staff at Elsevier for making this special issue possible. 95 4 5 96 References 97 Birch et al., 2008 (THIS ISSUE) 98 99 100 Borovsky, J. E., and M. H. Denton, The differences between CME-driven storms and CIR-driven storms, J. Geophys. Res., 111, A07S08, 2006. 101 102 D’Amicis et al., 2008 (THIS ISSUE) 103 104 Denton, M. H., and J. E. Borovsky, 2008 (THIS ISSUE) 105 106 Denton, M. H., J. E. Borovsky, R. B. Horne, R. L. McPherron, S. K. Morley, and B. T. Tsurutani, High speed 107 solar wind streams: A call for key research, EOS Trans., AGU, 89(7), 62-63, 2008. 108 109 Emery et al., 2008 (THIS ISSUE) 110 111 Guarnieri, F. L., The nature of auroras during high-intensity long-duration continuous AE activity (HILDCAA) 112 events: 1998 to 2001, in Recurrent Magnetic Storms: Corotating Solar Wind Streams, Edited by B. Tsurutani, 113 R. L. McPherron, W. D. Gonzalez, G. Lu, J. H. A. Sobral, and N. Gopalswamy, Geophysical Monograph Series 114 167, AGU, 2006. 115 116 Horne, R. B., Acceleration of killer electrons, Nature Physics, 3, 590-591, 2007 117 118 Jordanova et al., 2008 (THIS ISSUE) 119 120 Kavanagh, A. J., and M. H. Denton, High speed solar wind streams and geospace interactions, Astron. Geophys., 121 48, 6.24-6.26, 2007. 122 123 Kozyra, J. U., et al., Response of the upper/middle atmosphere to coronal holes and powerful high-speed solar 124 wind streams in 2003, in Recurrent Magnetic Storms: Corotating Solar Wind Streams, Edited by B. Tsurutani, 125 R. L. McPherron, W. D. Gonzalez, G. Lu, J. H. A. Sobral, and N. Gopalswamy, Geophysical Monograph Series 126 167, AGU, 2006. 5 6 127 128 Krieger, A. S., A. F. Timothy, and E. C. Roelof, A coronal hole and its identification as the source of a high 129 velocity solar wind stream, Sol. Phys., 23, 123, 1973. 130 131 Lam et al., 2008 (THIS ISSUE) 132 133 Lei J., J. P. Thayer, J. M. Forbes, E. K. Sutton, R. S. Nerem, Rotating solar coronal holes and periodic 134 modulation of the upper atmosphere, Geophys. Res. Lett., 35, L10109, doi:10.1029/2008GL033875, 2008. 135 136 Liemohn, M. W., and A. A. Chan, Unravelling the causes of radiation belt enhancements, EOS Trans., AGU, 137 88(42), 425-426, doi:10.1029/2007EO420001, 2007. 138 139 Lindsay, G. M., C. T. Russell, and J. G. Luhmann, Coronal mass ejection and stream interaction region 140 characteristics and their potential geomagnetic effectiveness, J. Geophys. Res., 100, 16999-17013, 1995. 141 142 Lyons et al., 2008 (THIS ISSUE) 143 144 McPherron et al., 2008 (THIS ISSUE) 145 146 Mlynczak M. G., F. J. Martin-Torres, C. J. Mertens, B. T. Marshall, R. E. Thompson, J. U. Kozyra, E. E. 147 Remsberg, L. L. Gordley, J. M. Russell III, T. Woods, Solar-terrestrial coupling evidenced by periodic behavior 148 in geomagnetic indexes and the infrared energy budget of the thermosphere, Geophys. Res. Lett., 35, L05808, 149 doi:10.1029/2007GL032620, 2008. 150 151 Morley et al., 2008 (THIS ISSUE) 152 153 Rae et al., 2008 (THIS ISSUE) 154 155 Reeves, G. D., Radiation Belt Storm Probes: A new mission for space weather forecasting, Space Weather, 5, 156 S11002, doi:10.1029/2007SW000341, 2008. 157 6 7 158 Sørbø et al., 2008 (THIS ISSUE) 159 160 Sandanger et al., 2008 (THIS ISSUE) 161 162 Snyder, C. W., M. Neugebauer, and U. R. Rao, The solar wind velocity and its correlation with cosmic-ray 163 variations and with solar and geomagnetic activity, J. Geophys. Res., 68, 6361-6370, 1963. 164 165 Temmer, M. B., Vršnak, and A. M. Veronig, Periodic appearance of coronal holes and the related variation of 166 solar wind parameters, Sol. Phys., 241, 371-383, doi:10.1007/s11207-007-0336-1, 2007. 167 168 Thayer J. P., J. Lei, J. M. Forbes, E. K. Sutton, R. S. Nerem, Thermospheric density oscillations due to periodic 169 solar wind high-speed streams, J. Geophys. Res., 113, A06307, doi:10.1029/2008JA013190, 2008. 170 171 Tsurutani, B. T., R. L. McPherron, W. D. Gonzalez, G. Lu, J. H. A. Sobral, and N. Gopalswamy, Introduction to 172 special section on corotating solar wind streams and recurrent geomagnetic activity, J. Geophys. Res., 111, 173 A07S00, doi:10.1029/2006JA011745, 2006. 174 175 Tsurutani, B. T., and W. D. Gonzalez, The cause of high-intensity long-duration continuous AE activity 176 (HILDCAAs): interplanetary Alfvén wave trains, Planet. Space Sci., 35, 405, 1987. 177 178 Turner, N. E., E. J. Mitchell, D. J. Knipp, and B. A. Emery, Energetics of magnetic storms driven by corotating 179 interaction regions: A study of geoeffectiveness, in Recurrent Magnetic Storms: Corotating Solar Wind Streams, 180 Edited by B. Tsurutani, R. L. McPherron, W. D. Gonzalez, G. Lu, J. H. A. Sobral, and N. Gopalswamy, 181 Geophysical Monograph Series 167, AGU, 2006. 182 183 Turner et al., 2008 (THIS ISSUE) 184 185 Turunen et al., 2008 (THIS ISSUE) 186 187 Wrenn et al., 2008 (THIS ISSUE) 7