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1 d-shifted (low pH) or blue-shifted (high pH) absorption maxima.
2 blue shifts in the fluorescence emission and absorption maxima.
3 some acylations also affect the anthocyanin absorption maxima.
4 5R(D)), there is no shift in the two-photon absorption maxima.
5 he meso substituents had a greater impact on absorption maxima.
6 LWS cone pigment results in a blue shift in absorption maxima.
7 are responsible for the 10 nm blue shift in absorption maxima.
8 pectively), on the basis of both the visible absorption maxima (530 versus 490 nm) and photocycle kin
10 c addition, resulting in a blue shift of the absorption maxima and a dramatic decrease in fluorescenc
11 aining 9- or 11-cis-retinal had blue-shifted absorption maxima and altered photo-bleaching properties
12 s of up to approximately 100 nm in localized absorption maxima and increased electron affinities.
13 eveal a Barlow-type relationship between the absorption maxima and the thermal isomerization rate sug
14 ith smaller side chains, (c) blue-shifted Qy absorption maxima, and (d) a sigmoid-shaped circular dic
16 tical properties with the longest wavelength absorption maxima around 500-800 nm, which gradually rea
17 ase domain thus prepared exhibits UV-visible absorption (maxima at 419 and 553 nm, shoulder at approx
18 opsin on the basis of the shift in the batho absorption maxima at 10 K [lambda(max) band (native) = 5
20 the formation of reaction intermediates with absorption maxima at 227 and 280 nm are diminished and d
21 obic conditions, reconstituted FNR exhibited absorption maxima at 315 nm and 420 nm, which were repla
25 l-protein intermediate states, with apparent absorption maxima at 380 nm and 440 nm, respectively.
30 of both the wild-type and F190I MnP exhibit absorption maxima at 429, 529, and 558 nm, resembling th
31 pectral shift of about 38 nm, giving rise to absorption maxima at 432, 462, and 492 nm in 20 mM Tris-
32 tion was supported by H2O2 and exhibited the absorption maxima at 435 and 930 nm characteristic of an
33 g both chromophores) exhibits characteristic absorption maxima at 435 nm due to the PYP domain and at
35 yl)ethenyl], which leads to derivatives with absorption maxima at 503, 587, and 668 nm, respectively.
37 ith PCB and apophycocyanin, the products had absorption maxima at 635 nm and very low fluorescence yi
38 chromophore have been synthesized; both have absorption maxima at 650 nm, where all the shellfish ext
39 bsence of dioxygen, indicated a species with absorption maxima at approximately 330 and approximately
44 nding, the rate of NO release, and the Soret absorption maxima for nitrophorin I were all pH dependen
46 h sensitive cone pigments have shifted their absorption maxima from the UV to the visible regions of
47 A = H); these include red-shifted (20-50 nm) absorption maxima, highly solvatochromic emission profil
49 were able to reproduce the trend of observed absorption maxima in both A1 and A2 rhodopsins, reveal a
50 from 4-(dimethylamino)phenylethyne (7), have absorption maxima in methanol of 594, 631, and 672 nm, r
51 steps from p-aminophenylacetylene (9), have absorption maxima in methanol of 623, 654, and 680 nm fo
53 pped in polyurethane hydrogel D4 and feature absorption maxima in the range 660-710 nm and fluorescen
54 sis of 294 A1 and A2 cone pigment literature absorption maxima indicates that the selection of a 6- s
55 e 21,23-core-modified porphyrins gave band I absorption maxima (lambda(max) of 689-717 nm) at longer
56 iaporphyrins 1-4 had little effect on either absorption maxima (lambda(max) of 696-701 nm for band I)
57 ncluding a large separation (70 nm) in their absorption maxima (lambda(max)) and a 2.5-fold increase
58 ynamic properties, including shifted optical absorption maxima (lambdamax) and decreased redox midpoi
59 colorimetric method involving probing of the absorption maxima (lambdamax) on the d-d electronic spec
60 tetramer (9) and pentamer (10) both exhibit absorption maxima matching those of the corresponding si
61 tween GPR and BPR as well as their different absorption maxima may be explained as an adaptation to t
63 V) and bovine blue cone visual pigments have absorption maxima of 358 and 438 nm, respectively, while
64 o long-lived pH-dependent photopigments with absorption maxima of 469 +/- 2.4 and 370 +/- 7.3 nm.
65 vocal bathochromic shifts of 10-15 nm of the absorption maxima of anilines in frozen samples compared
68 on spectral shifts, i.e., differences in the absorption maxima of colorless and colored forms, observ
69 been examined, revealing that the wavelength absorption maxima of each form increases with increasing
71 ations accurately reproduce the experimental absorption maxima of rhodopsin and the red, green, and b
72 at the two wavelengths corresponding to the absorption maxima of the chromophores, 675 and 750 nm.
73 ch results in a 95 nm difference between the absorption maxima of the two forms, and (ii) induction o
76 core heteroatoms had little effect on either absorption maxima or quantum yields of singlet oxygen ge
77 hermal stability without affecting the dyes' absorption maxima originates from the twisted geometry o
79 ineering gave rise to chimeric variants with absorption maxima ranging from 526 to 545 nm, dovetailin
80 e zinc chlorins exhibit long-wavelength peak absorption maxima ranging from 626 to 667 nm, indicating
81 hytochromobilin adduct displayed red-shifted absorption maxima relative to purified algal phytochrome
82 with red-shifted (D380E, lambdamax = 533 nm) absorption maxima relative to the wild-type protein (lam
83 cted evolution generated 70 GR variants with absorption maxima shifted by up to +/-80nm, extending th
84 ies and the position of its two ground state absorption maxima suggest it as a candidate for controll
85 Two sequential intermediates were found with absorption maxima that exhibit red shifts from the resti
86 te structure is demonstrated by plotting the absorption maxima versus the wavenumber of a Raman band
87 h thermally stability, hypsochromic shift of absorption maxima wavelengths of initial and cyclic form
88 fluorophore emission maxima, and nearly all absorption maxima were significantly red-shifted when co
90 significantly affects the position of UV-vis absorption maxima, which can be tuned in a broad range o
91 degrees of blue-shift in the flavin visible absorption maxima while visible CD spectra of the Y93A,
93 obtained from the wavelengths of UV/Visible absorption maxima with solute H-bond parameters obtained
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