Table 3
Spectroscopic constants for skew acrylamide in the ground state tunneling doublet (A-reduction, Ir -representation).
This work | Marstokk et al. (2000) (a) | ||||
---|---|---|---|---|---|
0+ | 0− | 0+ | 0− | ||
A / MHz | 10 049.46072 (34) (b) | 9996.61018 (39) | 10 049.549 (22) | 10 002.8 (5) | |
B / MHz | 4287.87861 (14) | 4291.77177 (19) | 4287.924 (12) | 4292.160 (24) | |
C / MHz | 3035.794577 (67) | 3050.747935 (98) | 3035.806 (12) | 3050.385 (33) | |
ΔJ / kHz | 0.990767 (85) | 0.95662 (11) | 1.14 (9) | 1.15 (16) | |
ΔJK / kHz | 3.47106 (38) | 4.24560 (48) | 4.20 (12) | 3.35 (18) | |
ΔK / kHz | 7.0201 (13) | 5.0704 (15) | 8.0 (6) | 8.0 | |
δJ / kHz | 0.166200 (44) | 0.194935 (60) | 0.283 (9) | 0.28 | |
δK / kHz | 5.03612 (65) | 4.64196 (99) | 3.23 (15) | 3.2 | |
ΦJ / Hz | 0.002027 (27) | 0.000986 (39) | ... | ... | |
ΦJK / Hz | –0.00838 (29) | –0.00530 (29) | ... | ... | |
ΦKJ / Hz | –0.2776 (11) | –0.1182 (12) | ... | ... | |
ΦK / Hz | 0.1495 (16) | 0.0781 (18) | ... | ... | |
ϕJ / Hz | –0.000622 (14) | –0.000261 (19) | ... | ... | |
ϕJK / Hz | 0.02621 (24) | 0.00500 (34) | ... | ... | |
ϕK / Hz | –0.1939 (23) | –0.0737 (26) | ... | ... | |
ΔE / MHz | 415050.244 (55) | ... | |||
ΔE / cm−1 | 13.8445859 (18) | ... | |||
Fbc / MHz | 4.08214 (95) | ... | |||
![]() |
–0.14465 (66) | ... | |||
![]() |
1.1873 (37) | ... | |||
![]() |
0.001568 (53) | ... | |||
![]() |
0.0624 (25) | ... | |||
Fac / MHz | –1.2209 (94) | ... | |||
![]() |
–0.2239 (41) | ... | |||
![]() |
3.407 (25) | ... | |||
Jmin∕Jmax | 4 / 76 | 6 / 77 | 4 / 27 | 6 / 8 | |
![]() |
0 / 24 | 0 / 24 | 0 / 8 | 2 / 7 | |
N(c) | 1419 | 1255 | 53 | 14 | |
σfit (d) / MHz | 0.040 | 0.035 | 0.196 | 0.129 | |
σw (e) | 1.03 | 1.08 | ... | ... |
Notes. (a)The ground state and the excited C–C torsional state in Marstokk et al. (2000) correspond to 0+ and 0− states, respectively. (b)The numbers in parentheses are the parameter uncertainties in units of the last decimal digit. Their values are close to 1σ standard uncertainties (67% confidence level) because the unitless (weighted) deviation of the fit is close to 1.0. SPFIT/SPCAT program package (Pickett 1991) was used for the analysis. (c)Number of distinct frequency lines in the fit. (d)Root mean square deviation of the fit. (e)Unitless (weighted) deviation of the fit.
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