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xviii | |
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List of abbreviations and acronyms |
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xix | |
About the authors |
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xxiii | |
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1 | (2) |
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2 | (1) |
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2 Physical background (historical outline) |
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3 | (20) |
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2.1 Polar geomagnetic disturbances influenced by solar wind |
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3 | (3) |
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2.2 Structure of electric fields in polar ionosphere |
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6 | (2) |
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2.3 Magnetospheric field-aligned currents |
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8 | (2) |
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2.4 Relation of field-aligned currents to aurora and particle precipitation |
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10 | (2) |
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2.5 Model computations of field-aligned currents and ionospheric electric field and currents |
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12 | (2) |
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2.6 Approaches to the idea of PC index |
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14 | (2) |
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14 | (1) |
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14 | (2) |
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16 | (1) |
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16 | (7) |
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3 A method for the PC index determination |
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23 | (18) |
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3.1 Coefficients determining relationship between coupling function and magnetic activity |
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24 | (5) |
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3.1.1 Level of reference for magnetic disturbance value δF |
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24 | (1) |
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3.1.2 Direction of disturbance vectors and link between the δF and EKL values |
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24 | (5) |
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3.2 Calculation of the PC index |
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29 | (1) |
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3.3 Interference of DP3 and DP4 disturbances |
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30 | (3) |
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3.4 Verification of the derived PC indices |
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33 | (3) |
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3.5 Physical meaning of the PC index |
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36 | (2) |
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38 | (1) |
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39 | (2) |
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4 Special features of procedure for on-line PC index derivation |
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41 | (36) |
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4.1 A need in producing 1 -min PC index |
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41 | (1) |
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4.2 Postulates used as a basis for the on-line PC index derivation |
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42 | (2) |
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4.3 Derivation of quiet daily curve (QDC) |
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44 | (12) |
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4.3.1 Methods used to determine a level of reference and their inadequacy |
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44 | (2) |
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4.3.2 Parameterization of geomagnetic variations for distinguishing quiet periods |
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46 | (1) |
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4.3.3 A procedure for calculating a daily quiet curve (QDC) |
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46 | (2) |
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4.3.4 Interpolation of a QDC for each day |
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48 | (3) |
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4.3.5 Extrapolation of a QDC for subsequent days |
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51 | (2) |
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4.3.6 Validity of the QDC derivation method |
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53 | (3) |
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4.4 Allowance for IMF sector structure |
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56 | (10) |
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4.4.1 Necessity of SS evaluation for QDC derivation |
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56 | (2) |
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4.4.2 Separation of the sector structure effect in long series of observational data |
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58 | (3) |
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4.4.3 On-line identification of the SS effect by ground magnetic data |
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61 | (5) |
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4.5 Invariability of parameters α β and in a solar activity cycle |
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66 | (9) |
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4.5.1 The role of QDC in determination of parameters, α and β |
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66 | (5) |
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4.5.2 Comparison of parameters α β calculated for solar maximum and minimum cpochs |
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71 | (4) |
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75 | (1) |
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75 | (2) |
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5 Solar wind-magnetosphere-ionosphere coupling and the PC index |
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77 | (26) |
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5.1 Concepts of solar wind-magnetosphere coupling |
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77 | (6) |
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5.1.1 Dungey's concept of reconnection |
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77 | (3) |
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5.1.2 Concept of `viscous-like' interaction |
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80 | (1) |
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5.1.3 Concept of magnetospheric plasma gradients as a driver for field-aligned currents |
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80 | (3) |
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5.2 Solar wind-magnetosphere-ionosphere coupling and field-aligned currents |
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83 | (2) |
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5.3 Solar wind-magnetosphere coupling functions |
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85 | (2) |
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5.4 Saturation of cross-polar cap potential |
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87 | (3) |
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90 | (3) |
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93 | (1) |
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94 | (9) |
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6 PC index response to solar wind geoeffective variations |
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103 | (26) |
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6.1 PC index timing vs. interplanetary electric field variations |
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103 | (1) |
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6.2 Solar wind dynamic pressure variations |
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104 | (12) |
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6.2.1 Solar wind dynamic pressure impact on magnetospheric processes |
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104 | (2) |
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6.2.2 PC index timing vs. sudden changes in solar wind dynamic pressure |
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106 | (2) |
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6.2.3 Statistical relationships between the PC index and pressure pulses P |
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108 | (7) |
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6.2.4 Relationships between PC and Psw under conditions of negative pressure gradients and northward IMF |
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115 | (1) |
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6.3 Dynamics of the polar convection patterns related to solar wind pressure pulses |
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116 | (3) |
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6.4 Field-aligned currents determining the response of the PC index to solar wind pressure pulses |
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119 | (7) |
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126 | (1) |
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126 | (3) |
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7 PC index as an indicator of substorm development |
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129 | (40) |
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7.1 Previous analyzes of relations between polar cap magnetic activity and magnetosphere substorms |
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129 | (1) |
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130 | (10) |
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7.3 Periodically repetitive magnetic disturbances (sawtooth substorms) |
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140 | (18) |
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7.3.1 Definition of sawtooth substorms |
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140 | (4) |
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7.3.2 Examples of sawtooth magnetic disturbances |
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144 | (4) |
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7.3.3 Statistical relationship between PC (EKL) variation and sawtooth magnetic disturbances development |
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148 | (9) |
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7.3.4 Evaluation of substorm back influence on polar cap magnetic activity |
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157 | (1) |
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7.4 PC index as a precursor of magnetic substorm development |
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158 | (4) |
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7.5 Threshold-dependent driven mode of magnetospheric substorms |
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162 | (2) |
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164 | (1) |
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165 | (4) |
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8 PC index as an indicator of magnetic storm development |
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169 | (18) |
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8.1 Identification of magnetic storms and separation of growth and decay parts in the main storm phase |
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169 | (3) |
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8.2 A PC index value required for the storm beginning |
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172 | (6) |
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8.3 Relationship between storm parameters and PC (EKL) values |
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178 | (2) |
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8.4 `Dst index saturation' and interplanetary electric field - magnetosphere coupling function |
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180 | (4) |
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184 | (1) |
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185 | (2) |
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9 Specific features of magnetic disturbances occurring under conditions of a steadily high energy input into the magnetosphere |
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187 | (32) |
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9.1 Inconsistency of substorm magnetic and aurora signatures in the case of powerful sawtooth substorms |
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187 | (14) |
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9.2 Relationships between PC index and substorm (AL) and storm (ASYM) indices in conditions of the steadily high solar wind energy input into the magnetosphere |
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201 | (14) |
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9.2.1 Existing ideas on interplay between magnetic storms and substorms |
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201 | (1) |
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9.2.2 Relationships between PC, AL and ASYM indices for individual substorms |
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202 | (4) |
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9.2.3 Relationships between PC, AL and ASYM indices during `PC growth phase' and `PC decline phase' |
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206 | (7) |
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9.2.4 A concept of powerful substorms reverse effect |
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213 | (2) |
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215 | (1) |
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216 | (3) |
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10 Magnetic disturbances developing under conditions of northward IMF |
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219 | (12) |
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10.1 Input of the IMF azimuthal component in coupling function EKL |
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219 | (2) |
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10.2 Magnetic storms developed under conditions of a northward IMF |
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221 | (1) |
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10.3 Magnetospheric substorms developed under conditions of a northward IMF |
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221 | (3) |
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10.4 Magnetospheric substorms triggered by sharp changes in the IMF vertical or azimuthal components |
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224 | (4) |
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228 | (1) |
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228 | (3) |
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11 Causative discrepancies between summer and winter PC indices: physical implications |
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231 | (16) |
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11.1 Reasons for discrepancy between summer and winter PC indices |
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231 | (1) |
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11.2 Effects of IMF northward and azimuthal components |
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232 | (2) |
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11.3 Effect of solar proton events |
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234 | (2) |
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11.4 Effect of solar wind dynamic pressure pulses |
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236 | (1) |
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11.5 Substorm development effect |
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237 | (3) |
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11.6 Role of auroral ionosphere in supporting the magnetic activity in the winter polr cap |
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240 | (2) |
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11.7 Statistical significance of PC seasonal differences |
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242 | (1) |
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243 | (1) |
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244 | (3) |
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12 Monitoring of the auroral ionosphere |
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247 | (10) |
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12.1 Parameters characterizing an auroral ionosphere state |
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247 | (1) |
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248 | (5) |
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12.3 Ionospheric Es and F2 layers |
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253 | (2) |
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255 | (1) |
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255 | (2) |
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13 PC index as indicator of anomalous atmospheric processes in the winter Antarctica |
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257 | (22) |
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13.1 Solar activity influence on the Earth's atmosphere: variations in cosmic rays flow or changes in solar wind parameters? |
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257 | (4) |
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13.2 Distinctive features of atmospheric circulation over the winter Antarctica |
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261 | (4) |
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13.3 Cloudiness and sudden warmings in central Antarctica |
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265 | (3) |
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13.4 Changes in height profiles of temperature and pressure above Vostok station |
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268 | (2) |
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13.5 Anomalous winds at the Antarctic stations and their relation to the PC index |
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270 | (5) |
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13.6 Mechanisms suggested to explain solar wind influence on atmospheric processes |
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275 | (1) |
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276 | (1) |
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276 | (3) |
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279 | (4) |
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281 | (2) |
Acknowledgements |
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283 | (2) |
Index |
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285 | |