<h2> Cassini Magnetosperic IMaging Investigation (MIMI) - Low Energy Magnetospheric Measurements System (LEMMS) data at AMDA </h2>

 
<UL>

  <li> Cassini MIMI-LEMMS data are taken from the PDS (Planetary Data System),
    <a href="http://ppi.pds.nasa.gov/index.jsp">site</a>.

  <li> This measures ions and electrons in the energy range 0.03 to 18 MeV for ions and 0.015 to 0.884 MeV for electrons. The available datasets are :
    <UL>
      <li> <b>acc_1hour</b> : One hour average particle intensity data for accumulator rate ion and electron channels
      <li> <b>acc_1min</b> : One minute average particle intensity data for accumulator rate ion and electron channels
      <li> <b>pha_1hour</b> : One hour average particle intensity data for PHA (Pulse Height Analysis) ion and electron channels
      <li> <b>pha_1min</b> : One minute average particle intensity data for PHA (Pulse Height Analysis) ion and electron channels
    </UL>

  <li> <b>These data are background subtracted, and thus occasionally there will be negative values when the count rate falls below the background level.</b>

  <li> Parameter plotting arguments for PHA datasets :
    <UL>
      <li><b>backgrdChan</b> : substraction of background noise defined by a channel index
      <li><b>backgrdVal</b> : substraction of background noise defined by a constant value
      <li><b>minCount</b> : count data must be greater or egal than minCount to be plot
      <li><b>minCount</b> : count data must be lower or egal than maxCount to be plot
      <li><b>channel</b> : plot a specific channel index
    </UL>

  <li>
    <TABLE BORDER CELLPADDING=5>
      <TR>
        <TH align="center"> Sources </TH>
        <TH align="center"> Datasets </TH>
        <TH align="center"> Status </TH>
        <TH align="center"> Last Update </TH>
      </TR>
      <TR>
        <TD> <a href="http://ppi.pds.nasa.gov/search/view/?f=yes&id=pds://PPI/COMIMI_L001">COMIMI_L001</a> </TD>
        <TD> acc_1hour, acc_1min, pha_1hour, pha_1min </TD>
        <TD> Calibrated  </TD>
        <TD> 2013-03-21 </TD>
      </TR>
    </TABLE>

  <li>
  <TABLE BORDER CELLPADDING=4>
    <CAPTION ALIGN="bottom"><b>Energy bands for accumulator rate datasets</b></CAPTION>
    <TR><TD></TD><TD></TD><TD COLSPAN=2 align="center">Energy bands</TD></TR>
    <TR>
      <TH align="center"> Channel </TH>
      <TH align="center"> Species </TH>
      <TH align="center"> Min (keV) </TH>
      <TH align="center"> Max (keV) </TH>
    </TR>
    <TR><TD>A0</TD><TD>p</TD><TD>27</TD><TD>35</TD></TR>
    <TR><TD>A1</TD><TD>p</TD><TD>35</TD><TD>56</TD></TR>
    <TR><TD>A2</TD><TD>p</TD><TD>56</TD><TD>106</TD></TR>
    <TR><TD>A3</TD><TD>p</TD><TD>106</TD><TD>255</TD></TR>
    <TR><TD>A4</TD><TD>p</TD><TD>255</TD><TD>506</TD></TR>
    <TR><TD>A5</TD><TD>p</TD><TD>506</TD><TD>805</TD></TR>
    <TR><TD>A6</TD><TD>p</TD><TD>805</TD><TD>1600</TD></TR>
    <TR><TD>A7</TD><TD>p</TD><TD>1615</TD><TD>4000</TD></TR>
    <TR><TD>A8</TD><TD>He</TD><TD>1270</TD><TD>3930</TD></TR>
    <TR></TR>
    <TR><TD>C0</TD><TD>e</TD><TD>18</TD><TD>40</TD></TR>
    <TR><TD>C1</TD><TD>e</TD><TD>27</TD><TD>48</TD></TR>
    <TR><TD>C2</TD><TD>e</TD><TD>41</TD><TD>60</TD></TR>
    <TR><TD>C3</TD><TD>e</TD><TD>56</TD><TD>100</TD></TR>
    <TR><TD>C4</TD><TD>e</TD><TD>92</TD><TD>183</TD></TR>
    <TR><TD>C5</TD><TD>e</TD><TD>175</TD><TD>300</TD></TR>
    <TR><TD>C6</TD><TD>e</TD><TD>265</TD><TD>550</TD></TR>
    <TR><TD>C7</TD><TD>e</TD><TD>510</TD><TD>832</TD></TR>
    <TR></TR>
    <TR><TD>E0</TD><TD>e</TD><TD>110</TD><TD>365</TD></TR>
    <TR><TD>E1</TD><TD>e</TD><TD>220</TD><TD>485</TD></TR>
    <TR><TD>E2</TD><TD>e</TD><TD>340</TD><TD>1350</TD></TR>
    <TR><TD>E3</TD><TD>e</TD><TD>600</TD><TD>4950</TD></TR>
    <TR><TD>E4</TD><TD>p</TD><TD>790</TD><TD>4750</TD></TR>
    <TR></TR>
    <TR><TD>P1</TD><TD>p</TD><TD>1424</TD><TD>2278</TD></TR>
    <TR><TD>P2</TD><TD>p</TD><TD>2280</TD><TD>4492</TD></TR>
    <TR><TD>P3</TD><TD>p</TD><TD>4491</TD><TD>5744</TD></TR>
    <TR><TD>P4</TD><TD>p</TD><TD>13200</TD><TD>25400</TD></TR>
    <TR><TD>P5</TD><TD>p</TD><TD>8311</TD><TD>11449</TD></TR>
    <TR><TD>P6</TD><TD>p</TD><TD>11474</TD><TD>13433</TD></TR>
    <TR><TD>P7</TD><TD>p</TD><TD>12101</TD><TD>58902</TD></TR>
    <TR><TD>P8</TD><TD>p</TD><TD>25185</TD><TD>59000</TD></TR>
    <TR><TD>P9</TD><TD>p</TD><TD>58650</TD><TD>158700</TD></TR>
  </TABLE>

  <li>

  <TABLE BORDER CELLPADDING=7>
    <CAPTION ALIGN="bottom"><b>Energy bands for PHA datasets</b></CAPTION>
    <TR><TD></TD><TD COLSPAN=2 align="center">A channels</TD><TD COLSPAN=2 align="center">E channels</TD><TD COLSPAN=2 align="center">F1 channels</TD></TR>
    <TR>
      <TH align="center"> Channel Index </TH>
      <TH align="center"> Min (keV) </TH>
      <TH align="center"> Max (keV) </TH>
      <TH align="center"> Min (keV) </TH>
      <TH align="center"> Max (keV) </TH>
      <TH align="center"> Min (keV) </TH>
      <TH align="center"> Max (keV) </TH>
    </TR>
<TR>
<TD>0</TD>
<TD>2.49E+01</TD>
<TD>2.65E+01</TD>
<TD>1.98E+01</TD>
<TD>2.07E+01</TD>
<TD>2.00E+02</TD>
<TD>2.13E+02</TD>
</TR>
<TR>
<TD>1</TD>
<TD>2.65E+01</TD>
<TD>2.82E+01</TD>
<TD>2.07E+01</TD>
<TD>2.16E+01</TD>
<TD>2.13E+02</TD>
<TD>2.26E+02</TD>
</TR>
<TR>
<TD>2</TD>
<TD>2.82E+01</TD>
<TD>2.98E+01</TD>
<TD>2.16E+01</TD>
<TD>2.25E+01</TD>
<TD>2.26E+02</TD>
<TD>2.40E+02</TD>
</TR>
<TR>
<TD>3</TD>
<TD>2.98E+01</TD>
<TD>3.14E+01</TD>
<TD>2.25E+01</TD>
<TD>2.42E+01</TD>
<TD>2.40E+02</TD>
<TD>2.53E+02</TD>
</TR>
<TR>
<TD>4</TD>
<TD>3.14E+01</TD>
<TD>3.30E+01</TD>
<TD>2.42E+01</TD>
<TD>2.60E+01</TD>
<TD>2.53E+02</TD>
<TD>2.71E+02</TD>
</TR>
<TR>
<TD>5</TD>
<TD>3.30E+01</TD>
<TD>3.46E+01</TD>
<TD>2.60E+01</TD>
<TD>2.77E+01</TD>
<TD>2.71E+02</TD>
<TD>2.88E+02</TD>
</TR>
<TR>
<TD>6</TD>
<TD>3.46E+01</TD>
<TD>3.62E+01</TD>
<TD>2.77E+01</TD>
<TD>2.95E+01</TD>
<TD>2.88E+02</TD>
<TD>3.06E+02</TD>
</TR>
<TR>
<TD>7</TD>
<TD>3.62E+01</TD>
<TD>3.79E+01</TD>
<TD>2.95E+01</TD>
<TD>3.12E+01</TD>
<TD>3.06E+02</TD>
<TD>3.28E+02</TD>
</TR>
<TR>
<TD>8</TD>
<TD>3.79E+01</TD>
<TD>3.95E+01</TD>
<TD>3.12E+01</TD>
<TD>3.30E+01</TD>
<TD>3.28E+02</TD>
<TD>3.51E+02</TD>
</TR>
<TR>
<TD>9</TD>
<TD>3.95E+01</TD>
<TD>4.11E+01</TD>
<TD>3.30E+01</TD>
<TD>3.56E+01</TD>
<TD>3.51E+02</TD>
<TD>3.73E+02</TD>
</TR>
<TR>
<TD>10</TD>
<TD>4.11E+01</TD>
<TD>4.43E+01</TD>
<TD>3.56E+01</TD>
<TD>3.82E+01</TD>
<TD>3.73E+02</TD>
<TD>3.95E+02</TD>
</TR>
<TR>
<TD>11</TD>
<TD>4.43E+01</TD>
<TD>4.76E+01</TD>
<TD>3.82E+01</TD>
<TD>4.08E+01</TD>
<TD>3.95E+02</TD>
<TD>4.22E+02</TD>
</TR>
<TR>
<TD>12</TD>
<TD>4.76E+01</TD>
<TD>5.08E+01</TD>
<TD>4.08E+01</TD>
<TD>4.34E+01</TD>
<TD>4.22E+02</TD>
<TD>4.53E+02</TD>
</TR>
<TR>
<TD>13</TD>
<TD>5.08E+01</TD>
<TD>5.40E+01</TD>
<TD>4.34E+01</TD>
<TD>4.61E+01</TD>
<TD>4.53E+02</TD>
<TD>4.84E+02</TD>
</TR>
<TR>
<TD>14</TD>
<TD>5.40E+01</TD>
<TD>5.72E+01</TD>
<TD>4.61E+01</TD>
<TD>4.87E+01</TD>
<TD>4.84E+02</TD>
<TD>5.15E+02</TD>
</TR>
<TR>
<TD>15</TD>
<TD>5.72E+01</TD>
<TD>6.05E+01</TD>
<TD>4.87E+01</TD>
<TD>5.22E+01</TD>
<TD>5.15E+02</TD>
<TD>5.50E+02</TD>
</TR>
<TR>
<TD>16</TD>
<TD>6.05E+01</TD>
<TD>6.53E+01</TD>
<TD>5.22E+01</TD>
<TD>5.57E+01</TD>
<TD>5.50E+02</TD>
<TD>5.86E+02</TD>
</TR>
<TR>
<TD>17</TD>
<TD>6.53E+01</TD>
<TD>7.02E+01</TD>
<TD>5.57E+01</TD>
<TD>5.92E+01</TD>
<TD>5.86E+02</TD>
<TD>6.26E+02</TD>
</TR>
<TR>
<TD>18</TD>
<TD>7.02E+01</TD>
<TD>7.50E+01</TD>
<TD>5.92E+01</TD>
<TD>6.35E+01</TD>
<TD>6.26E+02</TD>
<TD>6.79E+02</TD>
</TR>
<TR>
<TD>19</TD>
<TD>7.50E+01</TD>
<TD>7.99E+01</TD>
<TD>6.35E+01</TD>
<TD>6.79E+01</TD>
<TD>6.79E+02</TD>
<TD>7.15E+02</TD>
</TR>
<TR>
<TD>20</TD>
<TD>7.99E+01</TD>
<TD>8.47E+01</TD>
<TD>6.79E+01</TD>
<TD>7.23E+01</TD>
<TD>7.15E+02</TD>
<TD>7.68E+02</TD>
</TR>
<TR>
<TD>21</TD>
<TD>8.47E+01</TD>
<TD>8.96E+01</TD>
<TD>7.23E+01</TD>
<TD>7.67E+01</TD>
<TD>7.68E+02</TD>
<TD>8.21E+02</TD>
</TR>
<TR>
<TD>22</TD>
<TD>8.96E+01</TD>
<TD>9.60E+01</TD>
<TD>7.67E+01</TD>
<TD>8.19E+01</TD>
<TD>8.21E+02</TD>
<TD>8.75E+02</TD>
</TR>
<TR>
<TD>23</TD>
<TD>9.60E+01</TD>
<TD>1.02E+02</TD>
<TD>8.19E+01</TD>
<TD>8.80E+01</TD>
<TD>8.75E+02</TD>
<TD>9.28E+02</TD>
</TR>
<TR>
<TD>24</TD>
<TD>1.02E+02</TD>
<TD>1.09E+02</TD>
<TD>8.80E+01</TD>
<TD>9.41E+01</TD>
<TD>9.28E+02</TD>
<TD>9.99E+02</TD>
</TR>
<TR>
<TD>25</TD>
<TD>1.09E+02</TD>
<TD>1.17E+02</TD>
<TD>9.41E+01</TD>
<TD>1.00E+02</TD>
<TD>9.99E+02</TD>
<TD>1.05E+03</TD>
</TR>
<TR>
<TD>26</TD>
<TD>1.17E+02</TD>
<TD>1.25E+02</TD>
<TD>1.00E+02</TD>
<TD>1.07E+02</TD>
<TD>1.05E+03</TD>
<TD>1.12E+03</TD>
</TR>
<TR>
<TD>27</TD>
<TD>1.25E+02</TD>
<TD>1.33E+02</TD>
<TD>1.07E+02</TD>
<TD>1.14E+02</TD>
<TD>1.12E+03</TD>
<TD>1.19E+03</TD>
</TR>
<TR>
<TD>28</TD>
<TD>1.33E+02</TD>
<TD>1.41E+02</TD>
<TD>1.14E+02</TD>
<TD>1.22E+02</TD>
<TD>1.19E+03</TD>
<TD>1.28E+03</TD>
</TR>
<TR>
<TD>29</TD>
<TD>1.41E+02</TD>
<TD>1.51E+02</TD>
<TD>1.22E+02</TD>
<TD>1.33E+02</TD>
<TD>1.28E+03</TD>
<TD>1.37E+03</TD>
</TR>
<TR>
<TD>30</TD>
<TD>1.51E+02</TD>
<TD>1.62E+02</TD>
<TD>1.33E+02</TD>
<TD>1.40E+02</TD>
<TD>1.37E+03</TD>
<TD>1.46E+03</TD>
</TR>
<TR>
<TD>31</TD>
<TD>1.62E+02</TD>
<TD>1.74E+02</TD>
<TD>1.40E+02</TD>
<TD>1.50E+02</TD>
<TD>1.46E+03</TD>
<TD>1.57E+03</TD>
</TR>
<TR>
<TD>32</TD>
<TD>1.74E+02</TD>
<TD>1.85E+02</TD>
<TD>1.50E+02</TD>
<TD>1.61E+02</TD>
<TD>1.57E+03</TD>
<TD>1.66E+03</TD>
</TR>
<TR>
<TD>33</TD>
<TD>1.85E+02</TD>
<TD>1.98E+02</TD>
<TD>1.61E+02</TD>
<TD>1.71E+02</TD>
<TD>1.66E+03</TD>
<TD>1.78E+03</TD>
</TR>
<TR>
<TD>34</TD>
<TD>1.98E+02</TD>
<TD>2.11E+02</TD>
<TD>1.71E+02</TD>
<TD>1.82E+02</TD>
<TD><BR></TD>
<TD><BR></TD>
</TR>
<TR>
<TD>35</TD>
<TD>2.11E+02</TD>
<TD>2.25E+02</TD>
<TD>1.82E+02</TD>
<TD>1.96E+02</TD>
<TD><BR></TD>
<TD><BR></TD>
</TR>
<TR>
<TD>36</TD>
<TD>2.25E+02</TD>
<TD>2.45E+02</TD>
<TD>1.96E+02</TD>
<TD>2.06E+02</TD>
<TD><BR></TD>
<TD><BR></TD>
</TR>
<TR>
<TD>37</TD>
<TD>2.45E+02</TD>
<TD>2.58E+02</TD>
<TD>2.06E+02</TD>
<TD>2.20E+02</TD>
<TD><BR></TD>
<TD><BR></TD>
</TR>
<TR>
<TD>38</TD>
<TD>2.58E+02</TD>
<TD>2.77E+02</TD>
<TD>2.20E+02</TD>
<TD>2.34E+02</TD>
<TD><BR></TD>
<TD><BR></TD>
</TR>
<TR>
<TD>39</TD>
<TD>2.77E+02</TD>
<TD>2.96E+02</TD>
<TD>2.34E+02</TD>
<TD>2.51E+02</TD>
<TD><BR></TD>
<TD><BR></TD>
</TR>
<TR>
<TD>40</TD>
<TD>2.96E+02</TD>
<TD>3.16E+02</TD>
<TD>2.51E+02</TD>
<TD>2.69E+02</TD>
<TD><BR></TD>
<TD><BR></TD>
</TR>
<TR>
<TD>41</TD>
<TD>3.16E+02</TD>
<TD>3.35E+02</TD>
<TD>2.69E+02</TD>
<TD>2.86E+02</TD>
<TD><BR></TD>
<TD><BR></TD>
</TR>
<TR>
<TD>42</TD>
<TD>3.35E+02</TD>
<TD>3.61E+02</TD>
<TD>2.86E+02</TD>
<TD>3.07E+02</TD>
<TD><BR></TD>
<TD><BR></TD>
</TR>
<TR>
<TD>43</TD>
<TD>3.61E+02</TD>
<TD>3.80E+02</TD>
<TD>3.07E+02</TD>
<TD>3.25E+02</TD>
<TD><BR></TD>
<TD><BR></TD>
</TR>
<TR>
<TD>44</TD>
<TD>3.80E+02</TD>
<TD>4.06E+02</TD>
<TD>3.25E+02</TD>
<TD>3.49E+02</TD>
<TD><BR></TD>
<TD><BR></TD>
</TR>
<TR>
<TD>45</TD>
<TD>4.06E+02</TD>
<TD>4.32E+02</TD>
<TD>3.49E+02</TD>
<TD>3.70E+02</TD>
<TD><BR></TD>
<TD><BR></TD>
</TR>
<TR>
<TD>46</TD>
<TD>4.32E+02</TD>
<TD>4.64E+02</TD>
<TD>3.70E+02</TD>
<TD>3.98E+02</TD>
<TD><BR></TD>
<TD><BR></TD>
</TR>
<TR>
<TD>47</TD>
<TD>4.64E+02</TD>
<TD>4.97E+02</TD>
<TD>3.98E+02</TD>
<TD>4.23E+02</TD>
<TD><BR></TD>
<TD><BR></TD>
</TR>
<TR>
<TD>48</TD>
<TD>4.97E+02</TD>
<TD>5.29E+02</TD>
<TD><BR></TD>
<TD><BR></TD>
<TD><BR></TD>
<TD><BR></TD>
</TR>
<TR>
<TD>49</TD>
<TD>5.29E+02</TD>
<TD>5.68E+02</TD>
<TD><BR></TD>
<TD><BR></TD>
<TD><BR></TD>
<TD><BR></TD>
</TR>
<TR>
<TD>50</TD>
<TD>5.68E+02</TD>
<TD>6.00E+02</TD>
<TD><BR></TD>
<TD><BR></TD>
<TD><BR></TD>
<TD><BR></TD>
</TR>
<TR>
<TD>51</TD>
<TD>6.00E+02</TD>
<TD>6.45E+02</TD>
<TD><BR></TD>
<TD><BR></TD>
<TD><BR></TD>
<TD><BR></TD>
</TR>
<TR>
<TD>52</TD>
<TD>6.45E+02</TD>
<TD>6.84E+02</TD>
<TD><BR></TD>
<TD><BR></TD>
<TD><BR></TD>
<TD><BR></TD>
</TR>
<TR>
<TD>53</TD>
<TD>6.84E+02</TD>
<TD>7.36E+02</TD>
<TD><BR></TD>
<TD><BR></TD>
<TD><BR></TD>
<TD><BR></TD>
</TR>
<TR>
<TD>54</TD>
<TD>7.36E+02</TD>
<TD>7.81E+02</TD>
<TD><BR></TD>
<TD><BR></TD>
<TD><BR></TD>
<TD><BR></TD>
</TR>

  </TABLE>

</UL>