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Table 3:

Measured hyperfine splitting $\Delta ^a$ (kHz) and residual o-c of DCO+, DNC, and HN13C relative to a selected hyperfine component.
Transition Splitting Residualb
DCO+: F = 2-1 at 72 039.306 (3) MHz
1-1 +47.58 (144) 1.20
0-1 -64.64 (144) 0.80
DNC: I,F = 2,1-2,2 / 2,1-0,0 at 76305.512 (3) MHz
1,1-1,1 115.30 (100) -0.18
2,3-2,2 175.44 (100) -0.72
1,2-1,1 204.63 (100) 1.38
2,2-2,2 277.57 (100) -0.82
0,1-0,0    
0,1-2,2    
1,0-1,1 325.50 (250) 1.60
HN13C: F1,F2,F = 0,1,1-1,2,2 at 87 090.675 (3) MHz
2,2,2-1,1,1 115.5 (50) -7.3
2,2,2-1,2,2    
2,2,1-1,1,0    
2,2,1-1,2,1    
2,3,3-1,2,2 158.5 (50) 5.0
2,3,2-1,1,1    
2,3,2-1,2,1    
1,1,1-1,1,1 210.7 (50) 1.5
1,2,2-1,2,1    
1,2,2-1,2,2    

If no numbers are given for the value of a measured splitting and its residual, the hyperfine component overlaps with the previous component. The values of the splitting and the residual refer to the respective intensity weighted averages.
a Numbers in parentheses are one standard deviation in units of the least significant figures.
b Residuals for DCO+ refer to fit with CI kept fixed. The residuals are zero if CI is released as two pieces of information are then used to derive two parameters.


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