Table 7.
Rovibrational constants (in cm−1) used for 14N14N16O
| Vib. state | v0 | Bv | Dv×107 | Hv×1014 | Lv×1017 |
|---|---|---|---|---|---|
| 0000 | 0.0 | 0.419 011 006(15)a | 1.760 91(19) | −1.66(21) | |
| 0110 | 588.767 741(163) | 0.419 573 590(23) | 1.788 70(33) | −0.82(46) | |
| 0200 | 1168.132 418(198) | 0.419 919 855(52) | 1.871 21(85) | −8.18(368) | |
| 0220 | 1177.744 555(85) | 0.420 124 817(41) | 1.816 72(78) | 5.25(504) | −2.14(69) |
| 0001 | 1284.903 289(124) | 0.417 255 066(20) | 1.725 67(24) | 11.30(42) | 0.444(27) |
| 0310 | 1749.064 972(166) | 0.420 331 191(67) | 1.911 42(80) | −11.89(205) | |
| 0330 | 1766.911 896(161) | 0.420 664 523(346) | 1.852 1(64) | 17.4(405) | |
| 0111 | 1880.265 695(150) | 0.417 918 446(50) | 1.733 61(53) | 14.15(126) | 0.288(102) |
| 1000 | 2223.756 693(124) | 0.415 559 512(18) | 1.754 67(20) | −1.359(218) | |
| 0400 | 2322.572 934(211) | 0.420 618 036(216) | 1.943 02(155) | −384.4(164) | |
| 0420 | 2331.121 460(124) | 0.420 768 166(253) | 1.990 06(230) | 321.2(158) | |
| 0440 | [2356.251 397]b | [0.421 193 718] | [1.90] | [0.0] | |
| 0201 | 2461.996 447(242) | 0.418 147 317(318) | 1.892 76(175) | [0.0] | |
| 0221 | 2474.798 428(324) | 0.418 530 238(655) | 1.750 31(257) | [0.0] | |
| 0002 | 2563.339 334(169) | 0.415 605 588(268) | 1.639 20(152) | 64.40(224) | |
| 1110 | 2798.292 466(200) | 0.416 159 111(81) | 1.782 02(46) | −0.47(58) | |
| 0311 | 3046.212 560(931) | 0.418 567 39(164) | 1.904 70(539) | [0.0] | |
| 0331 | [3068.720 525] | [0.419 107] | [1.818] | [0.0] | |
| 0112 | 3165.853 959(214) | 0.416 382 245(410) | 1.632 92(294) | 48.70(571) | |
| 1310 | 3931.248 302(341) | 0.416 994 90(118) | 1.909 53(549) | [0.0] | |
| 1330 | 3948.285 330(370) | 0.417 327 81(195) | 1.835 5(123) | [0.0] |
The uncertainty in the last digits (twice the estimated standard error) is given in parentheses.
The values enclosed in square brackets were fixed during the analysis.