%year,Day,Kx (Range 0),O1 (nT),Counts @ O,Ky (Range 0),O2 (nT),Counts @ O,Kz (Range 0), O3 (nT),Counts @ O
2018   335.5   0.0146328    22.2     -1514   0.0144910   -17.3      1191   0.0142581   -30.1      2110
2018   336.5   0.0146328    22.2     -1514   0.0144910   -17.3      1191   0.0142581   -29.8      2088
2018   337.5   0.0146328    22.2     -1520   0.0144910   -17.1      1182   0.0142581   -30.0      2101
2018   338.5   0.0146328    22.2     -1517   0.0144910   -17.1      1182   0.0142581   -30.0      2102
2018   339.5   0.0146328    22.2     -1514   0.0144910   -17.1      1182   0.0142581   -30.0      2103
2018   340.5   0.0146328    22.1     -1512   0.0144910   -17.1      1183   0.0142581   -30.0      2103
2018   341.5   0.0146328    22.1     -1510   0.0144910   -17.1      1183   0.0142581   -30.0      2105
2018   342.5   0.0146328    22.0     -1507   0.0144910   -17.1      1183   0.0142581   -30.0      2105
2018   343.5   0.0146328    22.2     -1516   0.0144910   -17.5      1211   0.0142581   -30.2      2117
2018   344.5   0.0146328    22.3     -1525   0.0144910   -17.3      1195   0.0142581   -30.3      2128
2018   345.5   0.0146328    22.5     -1535   0.0144910   -17.1      1179   0.0142581   -30.5      2140
2018   346.5   0.0146328    22.5     -1534   0.0144910   -17.1      1179   0.0142581   -30.4      2132
2018   347.5   0.0146328    22.4     -1534   0.0144910   -17.1      1181   0.0142581   -30.3      2125
2018   348.5   0.0146328    22.4     -1532   0.0144910   -17.1      1182   0.0142581   -30.2      2117
2018   349.5   0.0146328    22.4     -1531   0.0144910   -17.1      1183   0.0142581   -30.1      2110
2018   350.5   0.0146328    22.4     -1531   0.0144910   -17.2      1184   0.0142581   -30.0      2103
2018   351.5   0.0146328    22.5     -1537   0.0144910   -17.0      1172   0.0142581   -30.0      2103
2018   352.5   0.0146328    22.5     -1541   0.0144910   -17.1      1177   0.0142581   -30.0      2103
2018   353.5   0.0146328    22.6     -1545   0.0144910   -17.1      1179   0.0142581   -30.0      2102
2018   354.5   0.0146328    22.2     -1519   0.0144910   -17.3      1195   0.0142581   -30.0      2102
2018   355.5   0.0146328    22.3     -1524   0.0144910   -17.3      1192   0.0142581   -30.0      2104
2018   356.5   0.0146328    22.4     -1529   0.0144910   -17.3      1191   0.0142581   -30.0      2106
2018   357.5   0.0146328    22.4     -1534   0.0144910   -17.2      1189   0.0142581   -30.1      2108
2018   358.5   0.0146328    22.5     -1538   0.0144910   -17.2      1187   0.0142581   -30.1      2110
2018   359.5   0.0146328    22.5     -1538   0.0144910   -17.0      1170   0.0142581   -30.0      2103
2018   360.5   0.0146328    22.5     -1537   0.0144910   -17.2      1184   0.0142581   -29.9      2097
2018   361.5   0.0146328    22.5     -1538   0.0144910   -16.9      1169   0.0142581   -30.2      2116
2018   362.5   0.0146328    22.5     -1540   0.0144910   -17.3      1195   0.0142581   -30.2      2116
2018   363.5   0.0146328    22.5     -1536   0.0144910   -17.3      1192   0.0142581   -30.1      2108
2018   364.5   0.0146328    22.4     -1534   0.0144910   -17.2      1188   0.0142581   -29.9      2100
2018   365.5   0.0146328    22.4     -1531   0.0144910   -17.2      1186   0.0142581   -29.8      2092
Note:										
The raw magnetic field B(nT) to Counts conversion are based on the scale factor table from the document		
STEREO/IMPACT Magnetometer Experiment Preliminary Report (11/15/05)						
by Dr. Mario H. Acuna (NASA)										
	B (nT) = K(x,y,z) * (32768 - Counts)									
Howerer, the code in the MAG idl routine have already dealed with the center data around zero issue, 
therefore,	
	Counts = -B/K									
The offsets O1, O2 and O3 are to be subtracted to any values converted to nominal B(nT)				
The "Counts @ O" should be subtracted for all Range 0 data in counts to center data around zero.