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Table A.1

Spectroscopic constants in the diagonal blocks of the Hamiltonian for the 15 ⇔ ν14 ⇔ 3ν11 triad of vibrational states in vinyl cyanide compared with those for the ground state.

Ground state 15 ν14 11

A/MHz 49 850.69655(43)a 51 864.336(36) 50 344.872(21) 47 990.329(47)
B/MHz 4971.212565(37) 4977.66513(90) 4974.53973(78) 5028.9277(13)
C/MHz 4513.828516(39) 4532.01579(78) 4519.08450(62) 4537.6921(11)
ΔJ/kHz 2.244058(13) 2.23613(25) 2.26543(26) 2.31540(32)
ΔJK/kHz -85.6209(35) -101.725(13) -81.531(12) -62.131(12)
ΔK/kHz 2715.4213(94) 4021.39(65) 2752.53(50) 1416.57(67)
δJ/kHz 0.4566499(32) 0.44884(16) 0.45991(16) 0.48731(24)
δK/kHz 24.4935(22) 26.477(90) 27.126(82) 32.642(96)
ΦJ/Hz 0.0064338(17) 0.006223(44) 0.006097(45) 0.006248(56)
ΦJK/Hz -0.00425(40) 0.129(16) 0.063(15) 0.094(17)
ΦKJ/Hz -7.7804(39) -25.21(11) -7.03(10) 4.74(10)
ΦK/Hz 384.762(63) 1391.8(35) 395.8(16) -317.0(41)
φJ/Hz 0.00236953(79) 0.002184(22) 0.002218(23) 0.002359(33)
φJK/Hz 0.14283(40) 0.126(16) 0.088(16) 0.252(17)
φK/Hz 37.011(58) 66.2(24) 42.9(21) 27.1(21)
LJ/mHz -0.000026315(71) [0.] [0.] [0.]
LJJK/mHz -0.001077(29) [0.] [0.] [0.]
LJK/mHz 0.4279(30) [0.] [0.] [0.]
LKKJ/mHz 0.012(12) 9.07(38) 3.62(38) 3.64(22)
LK/mHz -61.41(17) -658.9(84) -77.6(88) 161.3(94)
lJ/mHz -0.000011602(36) [0.] [0.] [0.]
lJK/mHz -0.000956(20) [0.] [0.] [0.]
lKJ/mHz -0.1436(46) [0.] [0.] 0.988(40)
lK/mHz 8.91(18) 16.3(10) 8.03(88) -25.43(69)
PKJ/mHz -0.0000156(31) [0.] [0.] [0.]
PKKJ/mHz -0.0001977(57) [0.] [0.] [0.]
PK/mHz 0.00867(15) [0.] [0.] [0.]
ΔEb/MHz 0.0 549 163.34(55) 694 443.66(90)
ΔE/cm-1 0.0 18.31812(2) 23.16415(3)
N lines c 4490,0 1329,52 1287,53 1250,81
σfitd/MHz 0.144 0.265e 0.228e 0.309e
σ rms d 0.713 1.980 1.467 2.329

Notes.

(a)

Round parentheses enclose standard errors in units of the last quoted digit of the value of the constant; square parentheses enclose assumed values.

(b)

The fitted vibrational energy difference relative to the lowest vibrational state in the triad.

(c)

The number of distinct frequency fitted lines and the number of lines rejected at the 10σ fitting criterion of the SPFIT program.

(d)

Deviations of fit for the different vibrational subsets.

(e)

The coupled fit for the complete triad encompasses 3866 lines, at an overall σfit of 0.269 MHz and requires also the use of constants reported in Table A.3.

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