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We note that it would be deceptive to Fourier transform numerically extracted oscillatory components alone because important details such as peak intensities in the transformed spectra depend sensitively on the method used to subtract off the underlying nonexponential excited-state population decay. Hence, we present in Figures 2 and 5 the DFTS of whole fluorescence transients.
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note
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- of the chromophore, although the H-bond energy is smaller in E46Q mutant compared with that of native PYP.
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61
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1542273822
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note
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39 for the similar modes for both native chromophore model (HCET) as well as locked chromophore analogue model (HCCET) and the later modes are marked with a dash.
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62
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0029731183
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Kroon, A. R.; Hoff, W. D.; Fennema, H.; Koomen, G. J.; Verhoeven, J. W.; Crielaard, W.; Hellingwerf, K. J. J. Biol. Chem. 1996, 271, 31949.
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(1996)
J. Biol. Chem.
, vol.271
, pp. 31949
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Kroon, A.R.1
Hoff, W.D.2
Fennema, H.3
Koomen, G.J.4
Verhoeven, J.W.5
Crielaard, W.6
Hellingwerf, K.J.7
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63
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1542363746
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note
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We note that a principal difference between low-frequency in-plane and out-of-plane modes might not be very clear in the real PYP system; i.e., in the low-frequency region, almost all modes might contain both in-plane and out-of-plane characteristics.
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