%year,Day,Kx (Range 0),O1 (nT),Counts @ O,Ky (Range 0),O2 (nT),Counts @ O,Kz (Range 0), O3 (nT),Counts @ O
2019     1.5   0.0146328    22.3     -1521   0.0144910   -17.0      1177   0.0142581   -29.8      2087
2019     2.5   0.0146328    22.0     -1507   0.0144910   -17.2      1189   0.0142581   -29.7      2086
2019     3.5   0.0146328    22.7     -1552   0.0144910   -17.5      1208   0.0142581   -30.0      2106
2019     4.5   0.0146328    22.6     -1544   0.0144910   -17.3      1194   0.0142581   -30.2      2122
2019     5.5   0.0146328    22.5     -1538   0.0144910   -17.3      1195   0.0142581   -30.2      2118
2019     6.5   0.0146328    22.4     -1531   0.0144910   -17.5      1206   0.0142581   -30.1      2114
2019     7.5   0.0146328    22.4     -1528   0.0144910   -17.4      1201   0.0142581   -30.1      2109
2019     8.5   0.0146328    22.3     -1526   0.0144910   -17.3      1197   0.0142581   -30.0      2104
2019     9.5   0.0146328    22.3     -1523   0.0144910   -17.3      1192   0.0142581   -29.9      2099
2019    10.5   0.0146328    22.3     -1521   0.0144910   -17.2      1188   0.0142581   -29.9      2097
2019    11.5   0.0146328    22.2     -1519   0.0144910   -17.1      1183   0.0142581   -29.9      2096
2019    12.5   0.0146328    22.4     -1530   0.0144910   -17.2      1190   0.0142581   -30.4      2129
2019    13.5   0.0146328    22.4     -1533   0.0144910   -17.2      1186   0.0142581   -30.0      2104
2019    14.5   0.0146328    22.4     -1533   0.0144910   -16.9      1168   0.0142581   -29.9      2096
2019    15.5   0.0146328    22.4     -1534   0.0144910   -17.0      1171   0.0142581   -29.8      2087
2019    16.5   0.0146328    22.5     -1541   0.0144910   -17.1      1183   0.0142581   -30.2      2117
2019    17.5   0.0146328    22.5     -1537   0.0144910   -17.2      1184   0.0142581   -30.1      2109
2019    18.5   0.0146328    22.1     -1514   0.0144910   -17.2      1184   0.0142581   -30.0      2102
2019    19.5   0.0146328    22.1     -1512   0.0144910   -17.1      1183   0.0142581   -29.9      2096
2019    20.5   0.0146328    22.2     -1515   0.0144910   -17.1      1182   0.0142581   -30.0      2103
2019    21.5   0.0146328    22.4     -1527   0.0144910   -17.1      1182   0.0142581   -30.0      2103
2019    22.5   0.0146328    22.3     -1526   0.0144910   -17.1      1182   0.0142581   -30.0      2103
2019    23.5   0.0146328    22.3     -1525   0.0144910   -17.1      1183   0.0142581   -30.0      2103
2019    24.5   0.0146328    22.3     -1523   0.0144910   -17.1      1183   0.0142581   -30.0      2103
2019    25.5   0.0146328    22.3     -1521   0.0144910   -17.1      1183   0.0142581   -30.0      2103
2019    26.5   0.0146328    22.2     -1520   0.0144910   -17.2      1184   0.0142581   -30.0      2103
2019    27.5   0.0146328    22.2     -1519   0.0144910   -16.8      1161   0.0142581   -30.0      2103
2019    28.5   0.0146328    22.2     -1516   0.0144910   -16.9      1166   0.0142581   -30.0      2103
2019    29.5   0.0146328    22.2     -1515   0.0144910   -17.0      1172   0.0142581   -30.0      2103
2019    30.5   0.0146328    22.1     -1514   0.0144910   -17.1      1178   0.0142581   -30.0      2103
2019    31.5   0.0146328    22.1     -1514   0.0144910   -17.1      1183   0.0142581   -30.0      2103
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.