%year,Day,Kx (Range 0),O1 (nT),Counts @ O,Ky (Range 0),O2 (nT),Counts @ O,Kz (Range 0), O3 (nT),Counts @ O
2018   244.5   0.0146328    22.6     -1546   0.0144910   -17.2      1187   0.0142581   -29.8      2092
2018   245.5   0.0146328    22.6     -1546   0.0144910   -17.2      1187   0.0142581   -29.8      2092
2018   246.5   0.0146328    22.6     -1547   0.0144910   -17.1      1177   0.0142581   -29.8      2093
2018   247.5   0.0146328    22.7     -1549   0.0144910   -17.0      1177   0.0142581   -29.8      2089
2018   248.5   0.0146328    22.7     -1549   0.0144910   -17.1      1179   0.0142581   -29.8      2089
2018   249.5   0.0146328    22.6     -1548   0.0144910   -16.9      1164   0.0142581   -29.9      2096
2018   250.5   0.0146328    22.8     -1555   0.0144910   -17.2      1187   0.0142581   -29.8      2091
2018   251.5   0.0146328    22.5     -1540   0.0144910   -17.1      1179   0.0142581   -29.8      2087
2018   252.5   0.0146328    22.5     -1534   0.0144910   -17.1      1181   0.0142581   -29.8      2087
2018   253.5   0.0146328    22.4     -1527   0.0144910   -17.1      1182   0.0142581   -29.8      2087
2018   254.5   0.0146328    22.4     -1534   0.0144910   -17.0      1177   0.0142581   -29.9      2094
2018   255.5   0.0146328    22.5     -1539   0.0144910   -17.1      1177   0.0142581   -30.0      2102
2018   256.5   0.0146328    22.6     -1546   0.0144910   -17.0      1172   0.0142581   -29.8      2087
2018   257.5   0.0146328    22.8     -1556   0.0144910   -17.2      1188   0.0142581   -29.6      2080
2018   258.5   0.0146328    22.5     -1541   0.0144910   -17.3      1196   0.0142581   -29.6      2079
2018   259.5   0.0146328    22.3     -1526   0.0144910   -17.4      1204   0.0142581   -29.6      2078
2018   260.5   0.0146328    22.3     -1526   0.0144910   -17.1      1181   0.0142581   -29.8      2090
2018   261.5   0.0146328    22.6     -1543   0.0144910   -17.0      1175   0.0142581   -30.0      2101
2018   262.5   0.0146328    22.5     -1539   0.0144910   -17.0      1175   0.0142581   -29.9      2096
2018   263.5   0.0146328    22.5     -1534   0.0144910   -16.9      1166   0.0142581   -29.8      2091
2018   264.5   0.0146328    22.4     -1530   0.0144910   -16.8      1157   0.0142581   -29.8      2087
2018   265.5   0.0146328    22.3     -1523   0.0144910   -16.8      1162   0.0142581   -29.7      2084
2018   266.5   0.0146328    22.2     -1516   0.0144910   -16.9      1167   0.0142581   -29.7      2082
2018   267.5   0.0146328    22.1     -1509   0.0144910   -17.0      1172   0.0142581   -29.6      2079
2018   268.5   0.0146328    22.0     -1502   0.0144910   -17.0      1177   0.0142581   -29.6      2076
2018   269.5   0.0146328    21.9     -1495   0.0144910   -17.1      1181   0.0142581   -29.6      2074
2018   270.5   0.0146328    21.8     -1488   0.0144910   -17.3      1195   0.0142581   -29.5      2071
2018   271.5   0.0146328    21.8     -1493   0.0144910   -17.2      1186   0.0142581   -29.9      2094
2018   272.5   0.0146328    22.0     -1503   0.0144910   -17.1      1178   0.0142581   -30.1      2110
2018   273.5   0.0146328    22.1     -1508   0.0144910   -17.1      1182   0.0142581   -30.0      2106
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.