Table 7
Fitted parameters of the RAM Hamiltonian for 13C acetaldehyde isotopologs.
Operator1 | n tr 2 | Parameter | 12CH312CHO | 13CH312CHO | 12CH313CHO | |
value3 (cm-1) | value3 (cm-1) | value3 (cm-1) | ||||
|
||||||
pα2 | 220 | F | 7.56708175(35) | 7.5652791(19) | 7.5068034(55) | |
(1/2) (1−cos(3α)) | 220 | V 3 | 407.59768(20) | 407.91172(18) | 407.58042(26) | |
pαPa | 211 | ρ | 0.328632673(20) | 0.328300981(35) | 0.322541154(65) | |
Pa2 | 202 | A RAM | 1.884881309(61) | 1.88013742(13) | 1.848976496(63) | |
Pb2 | 202 | B RAM | 0.348706489(16) | 0.337726802(58) | 0.348720666(61) | |
Pc2 | 202 | C RAM | 0.3031840478(44) | 0.294817724(11) | 0.302179145(18) | |
{Pa,Pb} | 202 | D ab | −0.122669037(94) | −0.11817144(38) | −0.12175149(39) | |
(1/2) (1−cos(6α)) | 440 | V 6 | −11.63964(50) | -11.67172(20) | -11.71571(65) | |
pα4 | 440 | F m | −0.424416(38) × 10-3 | −0.427829(96) × 10-3 | −0.42834(12) × 10-3 | |
pα3Pa | 431 | ρ m | −0.832163(52) × 10-3 | −0.82821(11) × 10-3 | −0.81162(16) × 10-3 | |
P2(1−cos(3α)) | 422 | V 3 J | 0.5577894(41) × 10-3 | 0.524776(16) × 10-3 | 0.529795(22) × 10-3 | |
Pa2(1−cos(3α)) | 422 | V 3 K | −0.19313906(98) × 10-1 | −0.1898291(17) × 10-1 | −0.1953217(29) × 10-1 | |
(Pb2− Pc2)(1−cos(3α)) | 422 | V 3 bc | 0.2114597(52) × 10-3 | 0.192215(19) × 10-3 | 0.213208(15) × 10-3 | |
(1/2){Pa,Pb}(1−cos(3α)) | 422 | V 3 ab | 0.4235363(70) × 10-2 | 0.405222(33) × 10-2 | 0.443922(36) × 10-2 | |
pα2P2 | 422 | F J | −0.291704(53) × 10-5 | −0.26533(11) × 10-5 | −0.31536(19) × 10-5 | |
pα2Pa2 | 422 | F K | −0.982545(30) × 10-3 | −0.972792(46) × 10-3 | −0.944979(89) × 10-3 | |
pα2(Pb2− Pc2) | 422 | F bc | 0.14720(12) × 10-5 | 0.13745(31) × 10-5 | 0.16632(37) × 10-5 | |
(1/2){Pa,Pc}sin(3α) | 422 | D 3 ac | −0.1405503(49) × 10-1 | −0.135881(17) × 10-1 | −0.142957(18) × 10-1 | |
(1/2){Pb,Pc}sin(3α) | 422 | D 3 bc | 0.59173(13) × 10-3 | 0.55489(43) × 10-3 | 0.63859(48) × 10-3 | |
pαPaP2 | 413 | ρ J | 0.958253(42) × 10-5 | 0.91984(11) × 10-5 | 0.91075(15) × 10-5 | |
pαPa3 | 413 | ρ K | −0.571407(12) × 10-3 | −0.564681(12) × 10-3 | −0.549548(31) × 10-3 | |
(1/2){Pa,(Pb2− Pc2)}pα | 413 | ρ bc | −0.5536(12) × 10-6 | −0.5763(36) × 10-6 | −0.2887(35) × 10-6 | |
− P4 | 404 | Δ J | 0.3244101(54) × 10-6 | 0.306742(20) × 10-6 | 0.325255(24) × 10-6 | |
− P2Pa2 | 404 | Δ JK | −0.581770(50) × 10-5 | −0.556079(86) × 10-5 | −0.571647(79) × 10-5 | |
− Pa4 | 404 | Δ K | 0.1308173(26) × 10-3 | 0.1292582(29) × 10-3 | 0.1263888(56) × 10-3 | |
−2P2(Pb2− Pc2) | 404 | δ J | 0.778472(23) × 10-7 | 0.709225(70) × 10-7 | 0.786517(69) × 10-7 | |
−{Pa2,(Pb2− Pc2)} | 404 | δ K | 0.94268 (17) × 10-6 | 0.105094(90) × 10−5 | 0.10255(12) × 10−5 | |
{Pa,Pb}P2 | 404 | D abJ | 0.867443(32) × 10-6 | 0.81273(20) × 10-6 | 0.85179(14) × 10-6 | |
{Pa3,Pb} | 404 | D abK | 0.30498(25) × 10-5 | 0.29239(46) × 10-5 | 0.27116(33) × 10-5 | |
(1/2) (1−cos(9α)) | 660 | V 9 | −0.20318(11) | −0.14153(11) | −0.2413(14) | |
pα6 | 660 | F mm | −0.5066(16) × 10-6 | −0.8986(20) × 10-6 | −0.7480(55) × 10-6 | |
pα5Pa | 651 | ρ mm | −0.7147(34) × 10-6 | −0.14955(33) × 10−5 | −0.1138(11) × 10−5 | |
P2(1−cos(6α)) | 642 | V 6 J | 0.557997(73) × 10-4 | 0.54132(35) × 10-4 | 0.58065(59) × 10-4 | |
Pa2(1−cos(6α)) | 642 | V 6 K | −0.37191(19) × 10-3 | −0.37805(54) × 10-3 | −0.33899(20) × 10-3 | |
(1/2){Pa,Pb}(1−cos(6α)) | 642 | V 6 ab | −0.13638(10) × 10-3 | −0.12574(40) × 10-3 | −0.12853(37) × 10-3 | |
(Pb2− Pc2)(1−cos(6α)) | 642 | V 6 bc | − | 0.1222(48) × 10−5 | −0.829(29) × 10-6 | |
pα4P2 | 642 | F mJ | −0.1259(18) × 10-9 | − | −0.4837(88) × 10−8 | |
pα4Pa2 | 642 | F mK | −0.1712(36) × 10-6 | −0.8131(17) × 10-6 | −0.5599(92) × 10-6 | |
pα4(Pb2− Pc2) | 642 | F mbc | 0.1197(22) × 10-8 | − | − | |
(1/2){Pb,Pc}sin(6α) | 642 | D 6 bc | −0.72949(57) × 10-4 | −0.6730(24) × 10-4 | −0.7137(16) × 10-4 | |
(1/2){Pa,Pc}sin(6α) | 642 | D 6 ac | 0.46097(67) × 10-3 | 0.4258(12) × 10-3 | 0.5301(10) × 10-3 | |
(1/2){Pa,Pc,pα2,sin(3α)} | 642 | D 3 acm | −0.3178(66) × 10-5 | − | − | |
pα3Pa3 | 633 | ρ mK | 0.2946(23) × 10-6 | − | 0.754(45) × 10−7 | |
pα3PaP2 | 633 | ρ mJ | −0.5306(26) × 10-8 | −0.3235(44) × 10-8 | −0.968(12) × 10-8 | |
(1/2){Pa,Pb,Pc,pα,sin(3α)} | 633 | ρ 3 bc | 0.47689(54) × 10-5 | − | − | |
(1/2){Pa,(Pb2− Pc2)}pα3 | 633 | ρ mbc | 0.4347(38) × 10-8 | −0.995(35) × 10-9 | − | |
P4(1 − cos(3α)) | 624 | V 3 JJ | −0.77602(42) × 10-8 | −0.4499(21) × 10-8 | −0.5065(25) × 10-8 | |
P2Pa2(1−cos(3α)) | 624 | V 3 J K | − | −0.23620(40) × 10-6 | − | |
Pa4(1−cos(3α)) | 624 | V 3 KK | 0.115646(94) × 10-5 | 0.11145(17) × 10-5 | 0.12880(30) × 10-5 | |
pα2P4 | 624 | F J J | − | 0.2343(39) × 10-10 | 0.1768(58) × 10-10 | |
pα2P2Pa2 | 624 | F JK | −0.6904(18) × 10-8 | −0.5620(48) × 10-8 | −0.9637(65) × 10-8 | |
pα2Pa4 | 624 | F KK | 0.30324(86) × 10-6 | 0.22248(28) × 10-6 | 0.2220(15) × 10-6 | |
P2(Pb2− Pc2)(1−cos(3α)) | 624 | V 3 bcJ | −0.17920(30) × 10-8 | − | −0.2040(11) × 10-8 | |
(1/2){Pa3,Pc}sin(3α) | 624 | D 3 acK | 0.1246(10) × 10-5 | 0.1141(18) × 10-5 | 0.171(10) × 10−6 | |
(1/2){Pa,Pc}P2sin(3α) | 624 | D 3 acJ | 0.10821(34) × 10-7 | 0.7636(98) × 10-7 | 0.372(14) × 10-7 | |
(1/2){Pb,Pc}P2sin(3α) | 624 | D 3 bcJ | −0.7436(17) × 10-8 | −0.6126(43) × 10-8 | −0.5837(99) × 10-8 | |
(1/2){Pa2,Pb,Pc}sin(3α) | 624 | D 3 bcK | 0.14846(12) × 10-5 | −0.2309(55) × 10-6 | −0.713(55) × 10-7 | |
(1/2)({Pa,Pb3} – {Pa,Pb,Pc2})cos(3α) | 624 | V 3 ab 3 | 0.38167(73) × 10-7 | 0.5101(22) × 10-7 | 0.5078(27) × 10-7 | |
P2Pa2(1−cos(3α)) | 624 | V 3 JK | −0.23880(36) × 10-6 | − | −0.28455(63) × 10-6 | |
(1/2){Pa,Pb}P2(1−cos(3α)) | 624 | V 3ab J | − | −0.566(26) × 10−8 | − | |
(1/2){Pa3,Pb}(1−cos(3α)) | 624 | V 3abK | 0.1562(36) × 10-6 | 0.2057(47) × 10-6 | 0.4345(43) × 10-6 | |
P2(Pb2− Pc2)(1−cos(3α)) | 624 | V 3 bcJ | − | −0.1586(11) × 10−8 | − | |
(1/2){Pa2,(Pb2− Pc2)}(1−cos(3α)) | 624 | V 3 bc K | − | 0.28389(89) × 10-6 | 0.2838(15) × 10-6 | |
(1/2){Pa,Pc3}sin(3α) | 624 | D 3ac3 | −0.3543(24) × 10-7 | −0.3397(69) × 10-7 | − | |
(1/2)({Pb3,Pc} − {Pb,Pc3})sin(3α) | 624 | D 3 bc 3 | − | −0.2447(29) × 10-8 | −0.2554(33) × 10-8 | |
pα2(Pb2− Pc2)P2 | 624 | F bc J | − | − | 0.1505(72) × 10-10 | |
(1/2){Pa2,(Pb2− Pc2)}pα2 | 624 | F bcK | 0.7853(30) × 10-8 | − | − | |
pα2(Pc4+Pb4) | 624 | F b 2 c 2 | 0.49528(94) × 10-10 | − | − | |
(Pb4+Pc4)cos3a | 624 | V 3 b 2 c 2 | −0.32294(69) × 10-8 | 0.770(22) × 10−9 | 0.684(31) × 10−9 | |
pαPaP4 | 615 | ρ J J | − | − | −0.2008(54) × 10-10 | |
pαPa3P2 | 615 | ρ JK | −0.40507(54) × 10-8 | −0.3627(21) × 10-8 | −0.4479(25) × 10-8 | |
pαPa5 | 615 | ρ KK | 0.12126(20) × 10-6 | 0.10832(11) × 10-6 | 0.10436(34) × 10-6 | |
(1/2){Pa,(Pb2− Pc2)}P2pα | 615 | ρ bcJ | −0.15285(93) × 10-10 | − | − | |
(1/2){Pa3,(Pb2− Pc2)}pα | 615 | ρ bcK | 0.6381(14) × 10-8 | 0.1989(33) × 10-8 | 0.1085(16) × 10-8 | |
{Pa,Pb}P4 | 606 | D abJJ | −0.16905(91) × 10-11 | −0.1419(35) × 10-11 | − | |
{Pa3,Pb}P2 | 606 | D abJK | 0.8607(65) × 10-10 | 0.478(19) × 10-10 | 0.3802(27) × 10−9 | |
{Pa5,Pb} | 606 | D abKK | 0.11154(82) × 10-8 | 0.888(24) × 10−9 | 0.4607(23) × 10-8 | |
P6 | 606 | Φ J | 0.80483(59) × 10-12 | 0.6874(26) × 10-12 | 0.7043(10) × 10-12 | |
P4Pa2 | 606 | Φ JK | −0.2732(10) × 10-10 | −0.1630(29) × 10-10 | −0.4677(31) × 10-10 | |
P2Pa4 | 606 | Φ K J | −0.14266(25) × 10-8 | −0.12937(55) × 10-8 | −0.17957(56) × 10-8 | |
Pa6 | 606 | Φ K | 0.19759(23) × 10-7 | 0.18596(18) × 10-7 | 0.18908(47) × 10-7 | |
2P4(Pb2− Pc2) | 606 | φ J | 0.38476(25) × 10-12 | 0.3246(12) × 10-12 | 0.34399(69) × 10-12 | |
P2{Pa2,(Pb2− Pc2)} | 606 | φ JK | −0.9470(55) × 10-11 | −0.653(13) × 10-11 | −0.1633(14) × 10-10 | |
{Pa4,(Pb2− Pc2)} | 606 | φ K | 0.54529(21) × 10-9 | 0.3514(59) × 10-9 | − | |
(1/2) (1−cos(12α)) | 880 | V 12 | 0.10123(15) | − | 0.1718(18) | |
pα8 | 880 | F mmm | −0.8628(32) × 10-8 | − | − | |
pα7Pa | 871 | ρ mmm | −0.20698(86) × 10-7 | − | − | |
P2(1−cos(9α)) | 862 | V 9 J | −0.15703(56) × 10-5 | −0.1211(24) × 10-5 | −0.3590(49) × 10-5 | |
Pa2(1 – cos(9α)) | 862 | V 9 K | 0.3044(14) × 10-4 | 0.4013(45) × 10-4 | − | |
(Pb2− Pc2)(1−cos(9α)) | 862 | V 9 bc | −0.11444(53) × 10-5 | −0.1967(52) × 10-5 | − | |
(1/2){Pa,Pb}(1−cos(9α)) | 862 | V 9 ab | − | −0.608(35) × 10-5 | −0.599(34) × 10-5 | |
(1/2){Pa,Pc}sin(9α) | 862 | D 9 ac | − | 0.1409(39) × 10−4 | − | |
(1/2){Pb,Pc}sin(9α) | 862 | D 9 bc | 0.884(13) × 10-6 | − | −0.343(10) × 10-5 | |
Pa2pα6 | 862 | F mmK | −0.2202(11) × 10-7 | −0.1406(33) × 10−9 | − | |
(1/2){Pa,Pb}pα6 | 862 | F mmab | 0.2906(29) × 10-10 | − | − | |
Pa3pα5 | 853 | ρ mmK | −0.13762(98) × 10-7 | − | − | |
pα4Pa4 | 844 | F mKK | −0.5734(57) × 10-8 | − | − | |
(1/2)P2{Pa,Pc}sin(6α) | 844 | D 6 acJ | −0.6552(93) × 10-8 | − | − | |
(1/2){Pa3,Pc}sin(6α) | 844 | D 6 acK | − | − | 0.425(37) × 10-7 | |
(1/2){Pb,Pc}P2sin(6α) | 844 | D 6 bcJ | 0.6210(71) × 10-9 | 0.748(21) × 10-9 | − | |
(1/2)({Pb3,Pc} − {Pb,Pc3})sin(6α) | 844 | D 6bc 3 | − | 0.5148(97) × 10-9 | 0.996(12) × 10-9 | |
P4(1−cos(6α)) | 844 | V 6 JJ | −0.799(16) × 10-10 | − | − | |
Pa4(1−cos(6α)) | 844 | V 6 KK | 0.15152(47) × 10-6 | 0.1380(11) × 10-6 | 0.1679(26) × 10-6 | |
(1/2){Pa,Pb}P2(1 − cos(6α)) | 844 | V 6 ab J | − | −0.554(14) × 10-8 | − | |
(1/2){Pa3,Pb}(1 − cos(6α)) | 844 | V 6 abK | −0.6966(58) × 10-7 | −0.542(21) × 10-7 | − | |
P2(Pb2− Pc2)(1−cos(6α)) | 844 | V 6 bcJ | − | − | −0.2303(65) × 10-9 | |
(1/2)({Pa,Pb3} – {Pa,Pb,Pc2})cos(6α) | 844 | V 6 ab 3 | − | −0.430(16) × 10-8 | − | |
pα3PaP4 | 835 | ρ m JJ | − | −0.873(21) × 10-13 | − | |
pα3Pa5 | 835 | ρ mKK | −0.1656(23) × 10-8 | − | − | |
(1/2){Pa,Pb3,Pc,pα,sin(3α)} − (1/2){Pa,Pb,Pc3,pα,sin(3α)} | 835 | ρ 3 bc 3 | −0.2511(23) × 10-10 | − | − | |
P6(1 − cos(3α)) | 826 | V 3 JJJ | 0.1344(25) × 10-13 | − | − | |
P4Pa2(1−cos(3α)) | 826 | V 3 JJK | 0.3715(39) × 10-11 | − | − | |
P2Pa4(1−cos(3α)) | 826 | V 3 JKK | 0.472(13) × 10-10 | 0.303(11) × 10-10 | − | |
(1/2)P2{Pa3,Pb}(1−cos(3α)) | 826 | V 3 ab J K | − | 0.3426(55) × 10-10 | − | |
(1/2){Pa5,Pb}(1−cos(3α)) | 826 | V 3 abKK | −0.2031(61) × 10-9 | − | − | |
(1/2)P2{Pa3,Pc}sin(3α) | 826 | D 3 acJK | −0.5470(82) × 10-10 | − | − | |
(1/2){Pa5,Pc}sin(3α) | 826 | D 3 ac K K | − | 0.450(27) × 10-10 | − | |
(1/2)P2{Pa2,Pb,Pc}sin(3α) | 826 | D 3 bcJK | 0.854(18) × 10-11 | − | − | |
(1/2){Pa4,Pb,Pc}sin(3α) | 826 | D 3 bc K K | − | − | −0.1697(63) × 10-9 | |
(1/2){Pa3,Pc3}sin(3α) | 826 | D 3 ac3K | 0.6486(74) × 10-10 | − | − | |
pα2Pa6 | 826 | F KKK | −0.3325(57) × 10-9 | − | − | |
pαPa3P4 | 817 | ρ J J K | − | − | 0.842(43) × 10-13 | |
pαPa7 | 817 | ρ KKK | −0.4300(86) × 10-10 | − | −0.353(15) × 10-11 | |
P8 | 808 | L J | −0.3808(46) × 10-17 | −0.358(24) × 10-17 | − | |
P4Pa4 | 808 | L JK | 0.5000(60) × 10-14 | − | 0.372(14) × 10-13 | |
Pa8 | 808 | L K | −0.2743(71) × 10-11 | − | −0.1256(48) × 10-11 | |
2P6(Pb2− Pc2) | 808 | l J | −0.1626(22) × 10-17 | −0.1332(63) × 10-17 | −0.1426(83) × 10-17 | |
pα8Pa2 | 1082 | F mmm K | − | 0.281(16) × 10-12 | − | |
(1/2)P2{Pa,Pb}(1−cos(9α)) | 1064 | V 9 abJ | −0.1960(28) × 10-8 | − | − | |
P4Pa2(1−cos(6α)) | 1046 | V 6 JJK | − | − | 0.3164(60) × 10-11 | |
P2Pa4(1−cos(6α)) | 1046 | V 6 JKK | − | − | −0.222(11) × 10-10 | |
(1/2){Pa5,Pb}(1−cos(6α)) | 1046 | V 6 abKK | −0.585(13) × 10-10 | − | − | |
pα2Pa8 | 1028 | F KKKK | 0.1427(47) × 10-14 | − | − |
Notes.
{ A,B } = AB + BA; { A,B,C } = ABC + CBA; { A,B,C,D } = ABCD + DCBA. The product of the operator in the first column of a given row and the parameter in the third column of that row gives the term actually used in the torsion-rotation Hamiltonian of the program, except for F, ρ, and ARAM, which occur in the Hamiltonian in the form .
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