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1
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0004015037
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McGraw-Hill: London; Chapter 8
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Long, D. A. Raman Spectroscopy; McGraw-Hill: London, 1977; Chapter 8.
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Raman Spectroscopy
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Long, D.A.1
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9
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0002192623
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Hudson, B. S.; Kohler, B. E.; Schulten, K. Excited States 1982, 6, 1.
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Excited States
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Hudson, B.S.1
Kohler, B.E.2
Schulten, K.3
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10
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0001519011
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Birge, R. R.; Bennett, J. A.; Hubbard, L. M.; Fang, H. L.; Pieace, B. M.; Kliger, D. S.; Leroi, G. E. J. Am. Chem. Soc. 1982, 104, 2519.
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Birge, R.R.1
Bennett, J.A.2
Hubbard, L.M.3
Fang, H.L.4
Pieace, B.M.5
Kliger, D.S.6
Leroi, G.E.7
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11
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0011224958
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note
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2h, of the polyene backbone.
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16
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0020405878
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Curry, B.; Broek, A.; Lugtenburg, J.; Mathies, R. J. Am. Chem. Soc. 1982, 104, 5274.
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J. Am. Chem. Soc.
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Curry, B.1
Broek, A.2
Lugtenburg, J.3
Mathies, R.4
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18
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0011202912
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note
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-2, and the pulse duration was 4 ps. Since the hyper-Raman intensity is proportional to the square of the incident excitation intensity, the intensity of the hyper-Raman scattering generated from unit area per pulse in our setup is expected to be 1600 times higher than theirs. However, our repetition rate (1 kHz) is 5 orders of magnitude lower than theirs (76 MHz), so that the intensity of hyper-Raman scattering generated from unit area per unit time in our setup is estimated to be even ∼50 times weaker than that in their setup. Although comparison for other experimental conditions (the focus size, the detection sensitivity) cannot be made, this estimation suggests that the high hyper-Raman intensity observed in the present measurement is not merely due to the difference in the excitation laser power.
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19
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0027691234
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Clays, K.; Hendrickx, E.; Triest, M.; Verbiest, T.; Persoons, A.; Dehu, C.; Brédas, J.-L. Science 1993, 262, 1419.
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(1993)
Science
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Clays, K.1
Hendrickx, E.2
Triest, M.3
Verbiest, T.4
Persoons, A.5
Dehu, C.6
Brédas, J.-L.7
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20
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0029141221
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Hendrickx, E.; Clays, K.; Persoons, A.; Dehu, C.; Brédas, J.-L. J. Am. Chem. Soc. 1995, 117, 3547.
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J. Am. Chem. Soc.
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Hendrickx, E.1
Clays, K.2
Persoons, A.3
Dehu, C.4
Brédas, J.-L.5
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22
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0011243263
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note
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The hyper-Raman scattering from solvent molecules was not recognized in the present measurement, whereas it was clearly observed in resonance Raman spectra of the same solution excited with double the excitation energy. It manifests that the observed resonance hyper-Raman scattering is not identical with resonance Raman scattering excited by the resonance hyper-Rayleigh scattering (or resonance second harmonic generation).
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23
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0011160750
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note
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Since we could not measure hyper-Rayleigh scattering of methanol with pulse energy of 2μJ, we measured it with the pulse energy of 10 μJ. Because hyper-Rayleigh intensity from methanol showed nice quadratic dependence to the laser energy in the range up to 30 μJ, we could safely estimate the hyper-Rayleigh intensity at the excitation energy used for hyper-Raman measurements.
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24
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4243425793
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Doukas, A. G.; Aton, B.; Callendar, R. H.; Honig, B. Chem. Phys. Lett. 1978, 56, 248.
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(1978)
Chem. Phys. Lett.
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, pp. 248
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Doukas, A.G.1
Aton, B.2
Callendar, R.H.3
Honig, B.4
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