Modeling the behavior of ionosphere above Millstone Hill during the September 21-27, 1998 storm

A theoretical ionospheric model is employed to investigate the ionospheric behavior as observed by the incoherent-scatter radar (ISR) at Millstone Hill during the September 21-27, 1998 storm. The observed NmF2 presented a significant negative phase on September 25, and a G condition (h(m)F(2) < 200 km) was also observed. The model results based on the standard input parameters (climatological model values) are in good agreement with the observed electron densities under quiet conditions, but there are large discrepancies during disturbed periods. The exospheric temperature T-ex, neutral winds, atomic oxygen density [O] and molecular nitrogen density [N-2], and solar flux are inferred from the ISR ion temperature profiles and from the electron density profiles. Our calculated results show that the maximum T-ex is higher than 1700 K, and an averaged decrease in [O] is a factor of 2.2 and an increase in [N-2] at 300 km is about 1.8 times for the disturbed day, September 25, relative to the quiet day level. Therefore, the large change of [N-2]/[O] ratio gives a good explanation for the negative phase at Millstone Hill during this storm. Furthermore, at the disturbed nighttime the observations show a strong NmF2 decrease, accompanied by a significant h(m)F(2) increase after the sudden storm commencement (SSC). Simulations are carried out based on the inferred T-ex. It is found that the uplift of F-2 layer during the period from sunset to post-midnight is mainly associated with the large equatorward winds, and a second rise in h(m)F(2) after midnight results from the depleted N-e in the bottom-side of F-2 layer due to the increased recombination, while the "midnight collapse" of h(m)F(2) is attributed to the large-scale traveling atmospheric disturbances. (C) 2004 Elsevier Ltd. All rights reserved.

[1]  J. G. Foster,et al.  Daytime thermosphere above Millstone Hill during severe geomagnetic storms , 1997 .

[2]  P. Waldteufel Combined incoherent‐scatter F 1‐region observations , 1971 .

[3]  M. Buonsanto,et al.  Comparison of models and data at Millstone Hillduring the 5–11 June 1991 storm , 1999 .

[4]  M. Buonsanto,et al.  Comparison of model electron densities and temperatures with Millstone Hill observations during undisturbed periods and the geomagnetic storms of 16–23 March and 6–12 April 1990 , 1997 .

[5]  K. Schlegel,et al.  Self-consistent modelling of the daytime electron density profile in the ionospheric F region , 1997 .

[6]  F. Fehsenfeld,et al.  Afterglow Studies of the Reactions He+, He(23S), and O+ with Vibrationally Excited N2 , 1968 .

[7]  W. R. Oliver Incoherent scatter radar studies of the daytime middle thermosphere , 1979 .

[8]  A. Hedin Extension of the MSIS Thermosphere Model into the middle and lower atmosphere , 1991 .

[9]  W. Tobiska Modeled soft X-ray solar irradiances , 1994 .

[10]  A. Nier,et al.  Recombination of O2 + in the ionosphere , 1976 .

[11]  Jack Sugar,et al.  Forbidden Lines in ns2npk Ground Configurations and nsnp Excited Configurations of Beryllium through Molybdenum Atoms and Ions , 1986 .

[12]  M. Buonsanto,et al.  Using steady state vibrational temperatures to model effects of N2* on calculations of electron densities , 1996 .

[13]  F. Fehsenfeld,et al.  Temperature dependence of some ionospheric ion-neutral reactions from 300°–900°K , 1974 .

[14]  L. Cogger,et al.  Dynamical behaviour of the nighttime ionosphere at Arecibo , 1971 .

[15]  J. Mitchell,et al.  Dissociative recombination and excitation of N+2 , 1989 .

[16]  A. Hedin MSIS‐86 Thermospheric Model , 1987 .

[17]  P. Richards,et al.  Behavior of the ionosphere and thermosphere at a southern midlatitude station during magnetic storms in early March 1995 , 1998 .

[18]  P. Richards An improved algorithm for determining neutral winds from the height of the F2 peak electron density , 1991 .

[19]  L. H. Andersen,et al.  Dissociative recombination and excitation of H2O+ and HDO+ , 1999 .

[20]  W. Wan,et al.  A new approach to the derivation of dynamic information from ionosonde measurements , 2003 .

[21]  G. Proêlss Ionospheric F-Region Storms: Unsolved Problems , 2006 .

[22]  M. Rees Physics and Chemistry of the Upper Atmosphere , 1989 .

[23]  J. Titheridge Atmospheric winds calculated from diurnal changes in the mid-latitude ionosphere , 1993 .

[24]  Marsha R. Torr,et al.  The role of metastable species in the thermosphere , 1982 .

[25]  C. Ng,et al.  A state-selected study of the ion{endash}molecule reactions O{sup +}({sup 2}D,{sup 2}P)+H{sub 2}O , 1997 .

[26]  G. Dunn,et al.  Measurement of total cross sections for electron recombination with NO+ and O2 + using ion storage techniques , 1974 .

[27]  J. Fox,et al.  The vibrational distribution of N2 + in the terrestrial ionosphere , 1985 .

[28]  P. Richards,et al.  The ionosphere and thermosphere at southern midlatitudes during the November 1993 ionospheric storm: A comparison of measurement and modeling , 1998 .

[29]  W. Kent Toriska Modeled soft X-ray solar irradiances , 1994 .

[30]  E. Chiavassa,et al.  The reaction from to , 1998 .

[31]  M. Buonsanto Ionospheric Storms — A Review , 1999 .

[32]  J. Foster,et al.  Effects of magnetospheric electric fields and neutral winds on the low‐middle latitude ionosphere during the March 20‐21, 1990, storm , 1993 .

[33]  M. Buonsanto,et al.  The Millstone Hill ionospheric model and its application to the May 26–27, 1990, ionospheric storm , 1999 .

[34]  A. Viggiano,et al.  RATE CONSTANTS FOR THE REACTIONS OF N+ AND N2+ WITH O2 AS A FUNCTION OF TEMPERATURE (300-1800 K) , 1997 .

[35]  J. R. Peterson,et al.  Dissociative recombination and excitation of N2+: Cross sections and product branching ratios , 1998 .

[36]  P. Burke,et al.  SCATTERING OF ELECTRONS BY C, N, O, N$sup +$, O$sup +$, AND O² . , 1969 .

[37]  A. Viggiano,et al.  Rate constants for the reactions of O+ with N2 and O2 as a function of temperature (300–1800 K) , 1997 .

[38]  J. Picone,et al.  The upper atmosphere during June 5–11, 1991 , 2000 .

[39]  W. Wan,et al.  Model results for the ionospheric lower transition height over mid-latitude , 2004 .

[40]  F. Fehsenfeld The reaction of O+2 with atomic nitrogen and NO+· H2O and NO+2 with atomic oxygen , 1977 .

[41]  R. Johnsen,et al.  Laboratory measurements of the O+(²D) + N2 and O+(²D) + O2 reaction rate coefficients and their ionospheric implications , 1980 .

[42]  Gerd W. Prölss,et al.  On explaining the local time variation of ionospheric storm effects , 1993 .

[43]  J. Lastovicka,et al.  Eects of geomagnetic storms on the ionosphere and atmosphere , 2001 .

[44]  Glenn Joyce,et al.  Sami2 is Another Model of the Ionosphere (SAMI2): A new low-latitude ionosphere model , 2000 .

[45]  H. Volland,et al.  Handbook of atmospheric electrodynamics , 1995 .

[46]  S. Fukao,et al.  Data modeling and assimilation studies with the MU radar , 1999 .

[47]  J. St.‐Maurice,et al.  Erratum: Nonthermal rate coefficients in the ionosphere: the reactions of O+ with N2, O2, and NO , 1978 .

[48]  Susan K. Avery,et al.  Empirical wind model for the upper, middle and lower atmosphere , 1996 .

[49]  P. Richards,et al.  EUVAC: A solar EUV Flux Model for aeronomic calculations , 1994 .

[50]  P. Blelly,et al.  The TEC and F2 parameters as tracers of the ionosphere and thermosphere , 2002 .

[51]  A. Pavlov The role of vibrationally excited nitrogen in the formation of the mid-latitude negative ionospheric storms , 1994 .

[52]  J. Foster,et al.  Model/data comparison of F region ionospheric perturbation over Millstone Hill during the severe geomagnetic storm of July 15–16, 2000 , 2001 .

[53]  Xiaoye S. Li,et al.  A state-selected study of the ion–molecule reactions O+(4S,2D,2P)+N2 , 1997 .

[54]  W. Pesnell,et al.  Momentum transfer collision frequency of O+‐O , 1993 .

[55]  D. Albritton,et al.  Energy dependence and branching ratio of the N2 + + O reaction , 1974 .

[56]  J. Titheridge Direct allowance for the effect of photoelectrons in ionospheric modeling , 1996 .

[57]  S. Fukao,et al.  Solar EUV flux, exospheric temperature and thermospheric wind inferred from incoherent scatter measurements of the electron density profile at Millstone Hill and Shigaraki , 2002 .

[58]  A. Mitra A review of D-region processes in non-polar latitudes , 1968 .

[59]  P. Richards,et al.  Reevaluation of the O+(²P) reaction rate coefficients derived from Atmosphere Explorer C observations , 1993 .

[60]  S. Kawamura,et al.  Extraction of solar and thermospheric information from the ionospheric electron density profile , 2001 .

[61]  T. Young,et al.  The nighttime ionosphere: E region and lower F region , 1974 .

[62]  T. Fuller‐Rowell,et al.  Intercomparison of physical models and observations of the ionosphere , 1998 .

[63]  P. Waldteufel,et al.  Diurnal variations of the atomic oxygen density and temperature determined from incoherent scatter measurements in the ionospheric F region , 1970 .

[64]  D. Drob,et al.  Nrlmsise-00 Empirical Model of the Atmosphere: Statistical Comparisons and Scientific Issues , 2002 .

[65]  J. Evans Millstone Hill Thomson Scatter Results for 1965 , 1967 .