Table 4.
Tentative relationships between observed Chl-a Qy vibrational modes (Reimers et al., 2013) from fluorescence excitation (Avarmaa and Rebane, 1985) in wet (Reimers et al., 2014) ether at 4.2 K and observed S0 modes from FLN in 1-propanol or TEA at 4.5 K, see Tables 1, 2.
| 1Qy FE wet ether | 1Qy calc. | 1Qy assignment in terms of S0 modes | S0 calc. | S0 ΔFLN TEA | S0 ΔFLN 1-propanol | |||||
|---|---|---|---|---|---|---|---|---|---|---|
| νi | λi | νi | λi | νi | λi | νi | λi | νi | λi | |
| – | - | 22 | 0.3 | - | - | |||||
| 64 | 16 | 42% 64, 28% 41, 19% 54 | 41, 64 | 12 | ||||||
| 110 | 1 | 96,99 | 7 | 100% 93, 89% 99 | 93,99 | 7 | 99 | 2 | 92b | 4b |
| 190 | 1 | 155 | 5 | 98% 154 | 154 | 5 | 170–210 | 1 | 194 | 3 |
| 263 | 2 | 241,263 | 3 | 96% 244, 95% 267 | 244,267 | 3 | 263 | 4 | 267 | 9 |
| 344 | 3 | 343 | 4 | 98% 345 | 345 | 2 | 349 | 6 | 353 | 11 |
| 370–390 | 3 | 375,385 | 4 | 95% 388, 82% 391 | 388,391 | 3 | 370–390 | 5 | 370–390 | 7 |
| 435–470 | 1 | 464 | 2 | 75% 470 | 470 | 2 | 430–450 | 1 | 430–450 | 5 |
| 494 | 2 | 81% 501 | 501 | 3 | ||||||
| 515 | 0.3 | 505 | 3 | 75% 513 | 513 | 1 | 520 | 4 | 519 | 7 |
| 563 | 3 | 589 | 2 | 99% 593 | 593 | 2 | 570 | 2 | 573 | 7 |
| 739 | 11 | 731,735 | 20 | 60% 737, 51% 749, 35% 739 | 737,739 | 16 | 742 | 12 | 745 | 36 |
| 788 | 3 | 837 | 4 | 87% 839 | 839 | 2 | 798 | 3 | 798 | 9 |
| 925 | 3 | 917 | 7 | 39% 895, 24% 897 | 895,897 | 15 | 915 | 13 | 914 | 25 |
| 966 | 23 | 977,979 | 36 | 87% 977, 45% 986 | 977 | 40 | 986 | 25 | 985 | 31 |
| 1,034 | 6 | 1,046 | 7 | 1,043 | 25c | |||||
| 1,070 | 8 | 1,084, 1,092 | 8 | 91% 1093 | 1,093 | 1 | 1,071 | 5 | 1,064 | 18c |
| 1,107 | 4 | 1,110 | 2 | 50% 1,110, 17% 1,102, 18% 1,122 | 1,102, 1,122 | 3 | 1,109 | 5 | 1,107 | 13c |
| 1,132 | 5 | 1,131 | 15 | 70% 1,131, 18% 1,149 | 1,131 | 10 | 1,117 | 5 | 1,120 | 18 |
| 1,149a | 12 | 1,144 | 18 | 1,146 | 42 | |||||
| 1,165 | 8 | 1,159 | 14 | 37% 1167 | 1,167 | 12 | 1,183 | 18 | 1,183 | 55 |
| 1,196 | 5 | 1,193 | 9 | 38% 1,184, 5% 1,192 | 1,192 | 5 | 1,209 | 17 | ||
| 1,212 | 5 | 33% 1,221, 60% 1,211 | 1,211 | 26 | 1,236 | 9 | ||||
| 1,228 | 15 | 1,224 | 47 | 23% 1,211, 60% 1,221 | 1,221 | 35 | 1,223 | 17 | 1,224 | 69 |
| 1,253 | 18 | 1,260 | 15 | 89% 1262 | 1,262 | 11 | 1,263 | 8 | 1,261 | 10 |
| 1,286 | 16 | 1,285, 1,287, 1,288 | 13 | 86% 1,283, 82% 1,286, 60% 1,287 | 1,286, 1,287, 1,288 | 9 | 1,288 | 7 | 1,288 | 18 |
| 1,306 | 6 | 26% 1,288, 16% 1,312, 17% 1348 | 1,288a | 3 | ||||||
| 1,323 | 10 | 46% 1324, 20% 1338, 11% 1331 | 1,324 | 17 | 1,306 | 4 | 1,306 | 24 | ||
| 1,329 | 12 | 31% 1,321, 27% 11,348, 15% 1,338 | 1,321a | 37 | 1,329 | 23 | 1,324 | 39 | ||
| 1,332 | 18 | 1,332 | 17 | 56% 1,331, 16% 1,321, 11% 1,338 | 1,331 | 0 | ||||
| 1,338a | 4 | 1,354 | 4 | 1,352 | 12 | |||||
| 1,369 | 10 | 1,364 | 4 | 44% 1,366, 12% 1,380, 13% 1,388 | 1,366 | 2 | 1,374 | 2 | 1,374 | 10 |
| 1,393 | 7 | 1,392 | 7 | 22% 1,396, 17% 1,380, 14% 1,384 | 1,396 | 5 | 1,390 | 6 | 1,388 | 12 |
| 1,415 | 6 | 1,423 | 10 | 31% 1,458, 18% 1,441 | ||||||
| 1,424 | 5 | 48% 1,422, 25% 1,441 | 1,422 | 5 | ||||||
| 1,441 | 5 | 1,435 | 15 | 1,436 | 23 | |||||
| 1,459 | 0 | 57% 1,465 | 1,458 | 5 | 1,467 | 1 | 1,488 | 6 | ||
| 1,446 | 8 | 1,466 | 3 | 45% 1,470, 13% 1,522 | 1,470 | 0 | ||||
| 1,510d | 18 | 1,501 | 15 | 55% 1,481,1,486 | 1,481, 1,486 | 24 | 1,519 | 5 | 1,517 | 18 |
| 1,530 | 9 | 1,530 | 66 | 46% 1,538, 24% 1,590 | 1,538 | 26 | 1,537 | 22 | 1,531 | 18 |
| 1,587 | 11 | 1,570 | 42 | 24% 1,562, 17% 1,568 | 1,568 | 11 | 1,552 | 15 | 1,552 | 17 |
| 1,595 | 29 | 54% 1,617, 19% 1,590 | 1,617 | 8 | 1,686 | 6 | 1,654 | 10 | ||
| 1,665 | 4 | 1,608 | 3 | 45% 1,590, 24% 1,617 | 1,590 | 11 | 1,610 | 4 | 1,596 | 2 |
| 188 | 415 | Total, listed modes | 355 | 301 | 500 | |||||
| 262 | 567 | Total, all modes | 492 | 370 | 650 | |||||
These are obtained by assigning the observed lines to modes calculated for methyl Chl-a using CAM-B3LYP and the calculated Duschinsky matrix elements to map the calculated modes of Qy onto those of S0.
No clear assignment, distributed over many Qy modes.
It is unclear as to whether all or part of this emission should be attributed to intramolecular vibrations, as reported in this table and elsewhere, or else to intermolecular phonons; modes of lower frequency are not easily identifiable in spectra.
No plausible assignment.
Broad band, originally listed at 1,493 cm-1 but the peak in this region is at 1,510 cm−1.