Commit bbd87dc759b11d1627faf26d62ab7d2496574e23
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MEPA PA
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NumericalData/CDPP-AMDA/CCE/MEPA/cce-mepa-pa.xml
... | ... | @@ -71,7 +71,7 @@ |
71 | 71 | <ObservedRegion>Earth.Magnetosphere.Magnetotail</ObservedRegion> |
72 | 72 | <ObservedRegion>Heliosphere.NearEarth</ObservedRegion> |
73 | 73 | <Parameter> |
74 | - <Name>nb flux para</Name> | |
74 | + <Name>ion flux para</Name> | |
75 | 75 | <ParameterKey>cce_mepa_pa_para</ParameterKey> |
76 | 76 | <Description> |
77 | 77 | Number flux for particles with velocities nearly parallel to the measured magnetic field. |
... | ... | @@ -82,7 +82,7 @@ |
82 | 82 | </RenderingHints> |
83 | 83 | </Parameter> |
84 | 84 | <Parameter> |
85 | - <Name>nb flux perp</Name> | |
85 | + <Name>ion flux perp</Name> | |
86 | 86 | <ParameterKey>cce_mepa_pa_perp</ParameterKey> |
87 | 87 | <Description> |
88 | 88 | Number flux for particles with velocities nearly perpendicular to the measured magnetic field. |
... | ... | @@ -93,10 +93,10 @@ |
93 | 93 | </RenderingHints> |
94 | 94 | </Parameter> |
95 | 95 | <Parameter> |
96 | - <Name>nb flux E0</Name> | |
96 | + <Name>ion flux E0</Name> | |
97 | 97 | <ParameterKey>cce_mepa_pa_E0</ParameterKey> |
98 | 98 | <Description> |
99 | - Number flux for both pitch angle bins at Energy E0. E0 is varying due to gain shift from range 25-34 to 76-100 keV | |
99 | + Number flux for both pitch angle bins at Energy E0. E0 is varying due to gain shift from range 25-76 to 34-100 keV | |
100 | 100 | </Description> |
101 | 101 | <Units>1/cm^2/s/sr</Units> |
102 | 102 | <RenderingHints> |
... | ... | @@ -117,10 +117,10 @@ |
117 | 117 | </Structure> |
118 | 118 | </Parameter> |
119 | 119 | <Parameter> |
120 | - <Name>nb flux E1</Name> | |
120 | + <Name>ion flux E1</Name> | |
121 | 121 | <ParameterKey>cce_mepa_pa_E1</ParameterKey> |
122 | 122 | <Description> |
123 | - Number flux for both pitch angle bins at Energy E1. E1 is varying due to gain shift from range 34-50 to 100-150 keV | |
123 | + Number flux for both pitch angle bins at Energy E1. E1 is varying due to gain shift from range 34-100 to 50-150 keV | |
124 | 124 | </Description> |
125 | 125 | <Units>1/cm^2/s/sr</Units> |
126 | 126 | <RenderingHints> |
... | ... | @@ -141,10 +141,10 @@ |
141 | 141 | </Structure> |
142 | 142 | </Parameter> |
143 | 143 | <Parameter> |
144 | - <Name>nb flux E2</Name> | |
144 | + <Name>ion flux E2</Name> | |
145 | 145 | <ParameterKey>cce_mepa_pa_E2</ParameterKey> |
146 | 146 | <Description> |
147 | - Number flux for both pitch angle bins at Energy E2. E2 is varying due to gain shift from range 50-83 to 150-250 keV | |
147 | + Number flux for both pitch angle bins at Energy E2. E2 is varying due to gain shift from range 50-150 to 83-250 keV | |
148 | 148 | </Description> |
149 | 149 | <Units>1/cm^2/s/sr</Units> |
150 | 150 | <RenderingHints> |
... | ... | @@ -165,10 +165,10 @@ |
165 | 165 | </Structure> |
166 | 166 | </Parameter> |
167 | 167 | <Parameter> |
168 | - <Name>nb flux E3</Name> | |
168 | + <Name>ion flux E3</Name> | |
169 | 169 | <ParameterKey>cce_mepa_pa_E3</ParameterKey> |
170 | 170 | <Description> |
171 | - Number flux for both pitch angle bins at Energy E3. E3 is varying due to gain shift from range 83-151 to 250-460 keV | |
171 | + Number flux for both pitch angle bins at Energy E3. E3 is varying due to gain shift from range 83-250 to 151-460 keV | |
172 | 172 | </Description> |
173 | 173 | <Units>1/cm^2/s/sr</Units> |
174 | 174 | <RenderingHints> |
... | ... | @@ -189,10 +189,10 @@ |
189 | 189 | </Structure> |
190 | 190 | </Parameter> |
191 | 191 | <Parameter> |
192 | - <Name>nb flux E4</Name> | |
192 | + <Name>ion flux E4</Name> | |
193 | 193 | <ParameterKey>cce_mepa_pa_E4</ParameterKey> |
194 | 194 | <Description> |
195 | - Number flux for both pitch angle bins at Energy E4. E4 is varying due to gain shift from range 151-285 to 460-860 keV | |
195 | + Number flux for both pitch angle bins at Energy E4. E4 is varying due to gain shift from range 151-460 to 285-860 keV | |
196 | 196 | </Description> |
197 | 197 | <Units>1/cm^2/s/sr</Units> |
198 | 198 | <RenderingHints> | ... | ... |