Table A.2:

Spectroscopic parametersa (MHz) for SiC2 obtained in the present investigation compared to a previous study.
Parameter This work He et al. (2008)
A-(B+C)/2 40674.000 (81) 40674.191 (100)
(B+C)/2 11800.11932 (84) 11800.11861 (99)
(B-C)/4 678.41182 (76) 678.41301 (130)
DK -1.3429 (185) -1.2880 (227)
DJK 1.624141 (59) 1.624219 (88)
$D_J \times 10^3$ -1.1651 (80) -1.1845 (115)
$d_1 \times 10^3$ -2.4371 (53) -2.4392 (111)
$d_2 \times 10^3$ -7.1766 (30) -7.2002 (80)
$H_{KJ} \times 10^6$ 669.68 (104) 670.39 (151)
$H_{JK} \times 10^6$ -138.26 (12) -138.66 (39)
$H_J \times 10^6$ 0.9810 (187) 1.0079 (201)
$h_1 \times 10^9$ -193.0 (101) -180.2 (247)
$h_2 \times 10^9$ -578.1 (84) -513.3 (301)
$h_3 \times 10^9$ 185.8 (67) 157.0 (93)
$L_{KKJ} \times 10^9$ -135.4 (69) -138.5 (80)
$L_{JK} \times 10^9$ 14.68 (175) 14.34 (266)
$L_{JJK} \times 10^9$ -12.11 (28) -11.06 (78)
$L_J \times 10^{12}$ 138.9 (166) -
$P_{KKKJ} \times 10^{12}$ 20.b 20.b

Notes. (a) Watson's S-reduction was used in the representation Ir. Numbers in parentheses are 1 $\sigma$ uncertainties in units of the least significant figures. (b) Kept fixed to estimated value.


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