%year,Day,Kx (Range 0),O1 (nT),Counts @ O,Ky (Range 0),O2 (nT),Counts @ O,Kz (Range 0), O3 (nT),Counts @ O
2019    32.5   0.0146328    22.3     -1525   0.0144910   -17.3      1195   0.0142581   -30.0      2108
2019    33.5   0.0146328    22.3     -1525   0.0144910   -17.3      1195   0.0142581   -30.0      2108
2019    34.5   0.0146328    22.3     -1525   0.0144910   -17.3      1195   0.0142581   -30.0      2108
2019    35.5   0.0146328    22.3     -1525   0.0144910   -17.2      1186   0.0142581   -30.0      2108
2019    36.5   0.0146328    22.4     -1531   0.0144910   -17.1      1182   0.0142581   -30.0      2101
2019    37.5   0.0146328    22.4     -1532   0.0144910   -17.2      1189   0.0142581   -29.9      2099
2019    38.5   0.0146328    22.4     -1533   0.0144910   -17.2      1186   0.0142581   -29.9      2097
2019    39.5   0.0146328    22.4     -1534   0.0144910   -17.1      1181   0.0142581   -29.9      2095
2019    40.5   0.0146328    22.5     -1536   0.0144910   -17.1      1183   0.0142581   -29.9      2096
2019    41.5   0.0146328    22.4     -1534   0.0144910   -17.2      1186   0.0142581   -30.1      2110
2019    42.5   0.0146328    22.5     -1535   0.0144910   -17.0      1177   0.0142581   -30.1      2108
2019    43.5   0.0146328    22.6     -1546   0.0144910   -17.2      1189   0.0142581   -30.0      2105
2019    44.5   0.0146328    22.8     -1557   0.0144910   -17.1      1181   0.0142581   -30.0      2101
2019    45.5   0.0146328    23.0     -1568   0.0144910   -17.0      1175   0.0142581   -29.9      2098
2019    46.5   0.0146328    22.6     -1547   0.0144910   -17.0      1170   0.0142581   -30.0      2105
2019    47.5   0.0146328    22.4     -1529   0.0144910   -17.1      1178   0.0142581   -30.0      2101
2019    48.5   0.0146328    22.6     -1546   0.0144910   -17.1      1181   0.0142581   -29.9      2094
2019    49.5   0.0146328    22.5     -1536   0.0144910   -17.1      1182   0.0142581   -30.0      2107
2019    50.5   0.0146328    22.4     -1528   0.0144910   -17.1      1179   0.0142581   -30.1      2112
2019    51.5   0.0146328    22.2     -1521   0.0144910   -17.0      1175   0.0142581   -30.2      2117
2019    52.5   0.0146328    22.1     -1513   0.0144910   -17.0      1172   0.0142581   -30.3      2123
2019    53.5   0.0146328    22.0     -1506   0.0144910   -17.1      1178   0.0142581   -29.8      2089
2019    54.5   0.0146328    22.1     -1510   0.0144910   -17.0      1175   0.0142581   -29.8      2091
2019    55.5   0.0146328    21.9     -1498   0.0144910   -17.0      1177   0.0142581   -29.7      2085
2019    56.5   0.0146328    22.1     -1508   0.0144910   -17.2      1185   0.0142581   -29.8      2091
2019    57.5   0.0146328    22.2     -1514   0.0144910   -17.2      1186   0.0142581   -29.8      2093
2019    58.5   0.0146328    22.1     -1511   0.0144910   -17.0      1175   0.0142581   -29.9      2096
2019    59.5   0.0146328    21.9     -1496   0.0144910   -17.2      1189   0.0142581   -29.7      2082
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.