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1 e lifetimes by decreasing radiative rates of fluorescence decay.
2 a lower impact of the ultrafast component on fluorescence decay.
3  of anthocyanins in solution shortened their fluorescence decay.
4 olysis products, furan, were responsible for fluorescence decay.
5  of the brief lifetime component of the qBBr fluorescence decay.
6 g to noninducing conditions and by measuring fluorescence decay.
7 for the previously described monoexponential fluorescence decay.
8 onential terms describing the time-dependent fluorescence decay.
9 intermediates were observed from femtosecond fluorescence decays.
10 spectroscopy based on statistical fitting of fluorescence decays, 2D FCS can resolve species whose fl
11 om the analysis of the I(VV)(t) and I(VH)(t) fluorescence decays acquired with a standard time-resolv
12 he acquisition and analysis of time-resolved fluorescence decays acquired with a vertically polarized
13 400 nm to both steady-state fluorescence and fluorescence decay across picosecond and nanosecond time
14                                              Fluorescence decay after photoactivation (FDAP) and fluo
15 Ts in axon-like processes, we used a refined fluorescence decay after photoactivation approach and si
16 e, we observed by quantitative imaging using fluorescence decay after photoactivation recordings of p
17               This study introduces a global fluorescence decay analysis that substantially simplifie
18 ed in earlier work have little effect on the fluorescence decay and appear to occur away from the try
19 igated by experimental measurements of Trp37 fluorescence decay and compared with theoretical measure
20 troscopy revealed a strong dependence of the fluorescence decay and electron-transfer/charge-recombin
21 ntly fluorogen dissociation, leading to fast fluorescence decay and fluorogen-concentration-dependent
22               Q6H2 was found to prevent both fluorescence decay and generation of lipid peroxides (LO
23                                  The greater fluorescence decay and more rapid breakup for the high c
24 nce of LHCBM9 resulted in faster chlorophyll fluorescence decay and reduced production of singlet oxy
25 c studies (emission quenching, time-resolved fluorescence decay, and transient absorption spectroscop
26                     The in-plane depolarized fluorescence decays are described by a stretched exponen
27 nce decays, 2D FCS can resolve species whose fluorescence decays are linked by the rate constants in
28                                        dsRed fluorescence decays as a single exponential with a 3.65
29 photophysical features of bilirubin make its fluorescence decay at picosecond time scale sensitive to
30 of Corti, we show that the time constants of fluorescence decay at the basolateral pole of IHCs and a
31 sion is spectrally isolated, analysis of the fluorescence decay can distinguish changes in membrane f
32  fluorescence lifetime; (2) amplitude of the fluorescence decay components; and (3) thylakoid membran
33         This was followed by a biexponential fluorescence decay containing fast and slow components,
34 rates were uncovered by deconvolution of the fluorescence decay curve.
35 ce spectroscopy (TRFS), i.e., measurement of fluorescence decay curves for different excitation and/o
36       In agreement with our conclusions, the fluorescence decay curves of 6-fluorotryptophan-containi
37                                              Fluorescence decay curves of each are monoexponential ex
38                                              Fluorescence decay curves were measured with high precis
39 r time divided by that of an earlier image), fluorescence decay curves, fluorescence decay rates, and
40 ed and fit-free analysis of multiexponential fluorescence decay curves.
41                                Time-resolved fluorescence decay data for the Cu(I)-saturated probe in
42 ng global analysis to simultaneously fit the fluorescence decay data of all pixels in an image or dat
43 allows us to fit both the prompt and delayed fluorescence decay data quantitatively.
44                               Fitting of the fluorescence decay data using the method of least square
45  (E), based on three-exponential fits to the fluorescence decay data, is 2.5 +/- 0.7% (SEM, N = 12).
46 icability of a rotamer model to describe the fluorescence decay data.
47                             In monellin, the fluorescence decay displays multiexponential character w
48                                          The fluorescence decay due to photobleaching of the immobile
49                                              Fluorescence decay due to tangential flow would be expec
50 uire an accurate subnanosecond time-resolved fluorescence decay every 0.1 ms after stopped flow.
51 uorescence recovery after photobleaching and fluorescence decay experiments, we find that the stable
52 uch slower in the native rubredoxin; the Trp fluorescence decay extends to 10 ps and longer, reflecti
53 ed four kinetic components: an initial, fast fluorescence decay, followed by a transient increase, an
54 ingle crystals, we have established that the fluorescence decay function of AP shows a pronounced, ch
55                           Analysis of the AP fluorescence decay function reveals conformational heter
56                                          The fluorescence decay functions of individual, specifically
57 sicle containing solutions, multiexponential fluorescence decays imply separate solute populations in
58  that does not require global fitting of the fluorescence decay in every spatial position of the samp
59 n the amplitude of the 60-70 ps component of fluorescence decay in open Chl b-containing PS II center
60                                     However, fluorescence decay in the presence of DCMU, which monito
61 peal of the phasor representation of complex fluorescence decays in biological systems is that a visu
62                             Dual exponential fluorescence decay is assigned to the two conformers of
63 ly suggest that the extent of nonexponential fluorescence decay is governed primarily by the efficien
64                         However, chlorophyll fluorescence decay kinetics after a single saturating fl
65 ins lacking photosystem I did not change the fluorescence decay kinetics after illumination, and ther
66 fer process was examined mechanistically via fluorescence decay kinetics and fluorescence anisotropy
67                                   The actual fluorescence decay kinetics can be fit to one exponentia
68                                              Fluorescence decay kinetics in the absence of DCMU indic
69                                              Fluorescence decay kinetics in the presence of DCMU indi
70                                         Trp4 fluorescence decay kinetics measured for the F4W protein
71 II (PSII), exhibits complex multiexponential fluorescence decay kinetics that for decades has been as
72                  In this study, we have used fluorescence decay kinetics to quantitatively probe Phot
73 al processor allows extraction of the sample fluorescence decay kinetics without distortions which ca
74 ophan residue that exhibits multiexponential fluorescence decay kinetics, was also examined as a more
75 tensity by up to 500% and induce complicated fluorescence decay kinetics.
76  fast and slow components of the flash-probe fluorescence decay kinetics.
77  pseudo-first-order rate constant describing fluorescence decay (kobs) increases linearly with [cytoc
78 ce peak intensity at 390 nm (I(375)/I(390)), fluorescence decay lifetime (tau), or rotational correla
79                                  Independent fluorescence decay lifetime and rotational dynamics para
80 hat the bases are stacked; at the same time, fluorescence decay lifetimes are heterogeneous, indicati
81 rescent protein (GFPuv) that exhibit altered fluorescence decay lifetimes.
82                        According to variable fluorescence decay measurements in DCMU-treated cells, c
83 ient absorption spectroscopy, and picosecond fluorescence decay measurements permits detailed analysi
84                                Time-resolved fluorescence decay measurements upon Chl excitation show
85 dynamics were examined through time-resolved fluorescence decay measurements.
86  differs between different dyes; the initial fluorescence decay mirrors the loss of granule contents
87 ns typically entails fitting data to complex fluorescence decay models but such experiments are frequ
88 ich occurs within the mixing time; and 2), a fluorescence decay occurring between approximately 100 a
89  explanation for the unusual monoexponential fluorescence decay of 5-fluorotryptophan (5FTrp) in sing
90                         We have analyzed the fluorescence decay of anthocyanins by fluorescence lifet
91 , a linear correlation was found between the fluorescence decay of BODIPY 581/591 C11 and the concent
92                                 In contrast, fluorescence decay of calcium-bound jRCaMP1a occurs by t
93                                     However, fluorescence decay of calcium-bound jRGECO1a follows a d
94 tive component (deltagamma(r)(-1)(t)) of the fluorescence decay of chromophores in proteins also is e
95                            Oxidation-induced fluorescence decay of diphenylhexatriene-labeled phospha
96     Western blot analysis indicated that the fluorescence decay of EGFP-MODC-(422-461) was correlated
97 d relaxation of protein water to explain the fluorescence decay of monellin.
98                                          The fluorescence decay of Rev M11 delta 14 was resolved into
99                                          The fluorescence decay of the cis-W3 zwitterion was biexpone
100                            The time-resolved fluorescence decay of the donor in each labeled junction
101                                              Fluorescence decay of the solute molecules is collected
102 provide compelling evidence that the complex fluorescence decay of the tryptophan zwitterion originat
103                        Analysis of the donor fluorescence decay of the unfolded subpopulation of both
104                                          The fluorescence decay of Trp246 is a triple exponential wit
105                                          The fluorescence decay of Trp45 in wild-type Rev was resolve
106  the origin of the ubiquitous nonexponential fluorescence decay of tryptophan in proteins.
107  conducted whereby the I(VV)(t) and I(VH)(t) fluorescence decays of a series of oligoquinolines label
108                                          The fluorescence decays of all five peptides and Rev M9 delt
109                              Analysis of the fluorescence decays of DNA-EB quenched by Cu(2+) and Ni(
110        In this paper, the best model for the fluorescence decays of solute molecules is selected with
111                                          The fluorescence decay parameters also correlated with the c
112 ing microscopy (FLIM) of NAD(P)H and FAD, so fluorescence decay parameters and the optical redox rati
113 quantifying cellular metabolism by measuring fluorescence decay parameters of endogenous fluorophores
114 s demonstrated that changes in the ultrafast fluorescence decay parameters of the bilirubin are sensi
115                              The analysis of fluorescence decay poses a challenging problem for the c
116                     Rather, heterogeneity in fluorescence decay processes was accommodated by the bre
117                                              Fluorescence decay profiles were obtained showing a mono
118 e model should display the same trend as the fluorescence decay profiles when an experimental conditi
119 cavity, we demonstrate an enhancement of the fluorescence decay rate by a factor of F = 6.89.
120                                              Fluorescence decay rate for the low concentration condit
121  Fluoro-Gold between 720 and 990 nm, and its fluorescence decay rate in aqueous solution and murine b
122 red with GCaMP-s and jRGECO1a-type GECI: the fluorescence decay rate of f-RCaMP1 was 21 s(-1), compar
123 ples at the molecular level by measuring the fluorescence decay rate of fluorescent probes.
124 roscopy furnishes radiative and nonradiative fluorescence decay rates in various solvent polarities.
125 n earlier image), fluorescence decay curves, fluorescence decay rates, and histograms of estimated te
126  these states do not directly impact NAD(P)H fluorescence decay rates.
127 otected from such surface quenching, and its fluorescence decay reflects reacidification kinetics.
128                              Analysis of the fluorescence decay resolved two lifetimes, corresponding
129                                              Fluorescence decay signals from PSII reconstituted with
130 nt and incompetent states that have distinct fluorescence decay signatures indicating different base
131 t is based on deep learning (DL) to quantify fluorescence decays simultaneously over a whole image an
132                                          The fluorescence decay spanned a full three orders of magnit
133                               Changes in the fluorescence decay suggest that FAD can exist in four co
134  of oxygen from solution lowered the rate of fluorescence decay, suggesting strategies that can be em
135                   The apparent half-time for fluorescence decay (t(1/2)) in PSII(-Mn) increased from
136 asor approach is a transformation of complex fluorescence decays that does not use fits to model deca
137  to screen the different membrane phases via fluorescence decay time analysis, making this new probe
138 n solution and in gas phase by measuring the fluorescence decay time and ion-neutral collision cross
139                2AP does not exhibit the long fluorescence decay time characteristic of the free nucle
140                  The absorption spectrum and fluorescence decay time components of the complex at roo
141 d emission spectra (TRES) indicate that this fluorescence decay time should be ascribed to a highly q
142 ervations: the scaling of the characteristic fluorescence decay time with the vesicle diameter and th
143 roperties, such as high solubility and short fluorescence decay time, could be obtained from fluoroph
144 cifically, we use the difference between the fluorescence decay times of fluorescently tagged antibod
145                     Nonlinear fitting of the fluorescence decay times provides activation parameters
146  of different complexes led to variations in fluorescence decay times.
147 o for 15 ms to 1000 s and then to follow the fluorescence decay upon chemical dilution into excess ac
148 ain, we simultaneously record the time-lapse fluorescence decay upon pulsed laser excitation within a
149                            The initial, fast fluorescence decay was assigned to DC6C dissociation fro
150 bit low fluorescence quantum yields, and the fluorescence decay was studied in different solvents, hi
151                       However, the identical fluorescence decay waveforms for saturating amounts of d
152               Kinetic circular dichroism and fluorescence decays were measured simultaneously to moni
153 he electron donor, measured by time-resolved fluorescence decay, were positively correlated with the
154  analysis of simulated I(VV)(t) and I(VH)(t) fluorescence decays which were found to match perfectly
155 at AppAwt and Y21F mutant protein exhibits a fluorescence decay with a lifetime of 0.6 ns.
156 ior to data collection shows monoexponential fluorescence decay with a lifetime of 1.0 ns.
157 ted AppAwt but not Y21F also exhibits slower fluorescence decay with a lifetime of 1.7 ns.
158                                          Trp fluorescence decay with the onset of solvation dynamics
159  yields of 0.04-0.24, and triple exponential fluorescence decays with lifetimes of 4.4-6.6, 1.4-3.2,
160 its a respectable quantum yield and a simple fluorescence decay, with marginal amounts of dark specie

 
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