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1 hich probably plays an important role in the photophysics.
2 ects on molecular reactivity and chromophore photophysics.
3 what is commonly observed in condensed phase photophysics.
4 e interpreted on the basis of intramolecular photophysics.
5 a careful analysis of contributions from dye photophysics.
6 r environmental influences on intrinsic 2-AP photophysics.
7 gned to test the rotamer model of tryptophan photophysics.
8  have potentially interesting fullerene-like photophysics.
9 ameters, chemical kinetics, and fluorescence photophysics.
10  for concentration, mobility, chemistry, and photophysics.
11  the impact of phonon nuclear motions on the photophysics.
12 status within polaritonic photochemistry and photophysics.
13 arrier-phonon interplay and the rich polaron photophysics.
14  quantifying mode-selective contributions to photophysics.
15 tical techniques to resolve delicate exciton photophysics.
16 ed by a lack of understanding of its complex photophysics.
17 rkable advancement in the field of aggregate photophysics.
18 ur understanding of dissolved organic matter photophysics.
19 d by metal ion binding profoundly affect DNA photophysics.
20 lecular orientation in mediating interfacial photophysics.
21  range of applications in photochemistry and photophysics.
22 ruct EEM data based on a model for LAURDAN's photophysics.
23 h combines PAINT and active control of probe photophysics.
24 devices on demand and uncover defect-related photophysics.
25 ling stoichiometries and complex fluorophore photophysics.
26 cal assembly, nanoscience, and metal cluster photophysics.
27 re other models for dissolved organic matter photophysics.
28 rid perovskites, especially those related to photophysics.
29         The chromophores also have favorable photophysics.
30 olubilizing groups to optimize excited-state photophysics.
31 s, and analyze how the solvent modulates the photophysics.
32 interest and significance in their anomalous photophysics.
33   It also enables a comparative study of the photophysics across multiple size and dopant regimes, wh
34  In this review, we focus on materials whose photophysics allow for the use of these materials in bio
35  new avenues into unexplored single molecule photophysics and appear as a promising tool for nanoscal
36  in catalysis, synthesis, materials science, photophysics and bioinorganic chemistry.
37                         By investigating the photophysics and charge transport characteristics of (Cz
38  used as molecular models to investigate the photophysics and chemistry of aqueous electrolyte soluti
39                        The electrochemistry, photophysics and ECL of Ru(bpy)3(2+) in the presence of
40 view is arranged by catalyst class where the photophysics and electrochemical characteristics of each
41                     An overview of the basic photophysics and electron transfer theory is presented i
42 ity, but also provides a pathway to modulate photophysics and electronics of multidimensional functio
43  of activated OCP, to directly determine the photophysics and heterogeneity of OCP-quenched phycobili
44 re-evaluation of current theories of polyene photophysics and highlights the robustness of carotenoid
45 statistics being independent of the detailed photophysics and its parameters being transferable, the
46  These data show that (i) coupled oscillator photophysics and metal-mediated cross-coupling can be ex
47                                          The photophysics and morphology of thin films of N,N-bis(2,6
48                     Relevant fundamentals of photophysics and photochemistry are discussed first, fol
49  review aims at providing an overview of the photophysics and photochemistry at play in neutral and c
50 mplexity as well as an opening to modify the photophysics and photochemistry beyond what normally can
51 esent a detailed study of the time-dependent photophysics and photochemistry of a known conformation
52                                          The photophysics and photochemistry of DNA is of great impor
53 es, advance the current understanding of the photophysics and photochemistry of first-row transition
54  coupling is essential for understanding the photophysics and photochemistry of heptamethine cyanines
55                            Understanding the photophysics and photochemistry of molecular pai-stacked
56 ades as a model system for understanding the photophysics and photochemistry of organic chromophores.
57                          Here, we review the photophysics and photochemistry of organic fluorophores
58  ways in which a better understanding of the photophysics and photochemistry of sunscreen molecules s
59                                          The photophysics and photochemistry of these hairpins were i
60 ped holes have profound consequences for the photophysics and photochemistry of these materials.
61 tation and host-guest interactions; (iv) the photophysics and photochemistry that lead to photochromi
62 provides new opportunities for innovation in photophysics and photochemistry through polynuclear arch
63 uently, we establish a critical link between photophysics and photochemistry with a theory based on t
64       Nonadiabatic effects are ubiquitous in photophysics and photochemistry, and therefore, many the
65 namics play an essential role in quantum dot photophysics and photochemistry, and they are primarily
66 apply their synthetic and other knowledge to photophysics and photochemistry, and we intend to stimul
67 levant in the greater context of sustainable photophysics and photochemistry, as well as for possible
68 ng one of the most fundamental principles of photophysics and photochemistry, Kasha's rule, and opens
69 T states for next-generation applications in photophysics and photochemistry.
70  form the basis for numerous applications in photophysics and photochemistry.
71  d-orbitals more amenable to applications in photophysics and photochemistry.
72 e transfer) excited states that lead to rich photophysics and photochemistry.
73 s have recently become an important focus in photophysics and photoredox catalysis due to metal-cente
74 nd detailed analyses incorporating molecular photophysics and semiconductor density of states measure
75 l suited for investigations of the intrinsic photophysics and spectroscopy of organic-inorganic metal
76 tification and differentiation of host-guest photophysics and stoichiometries, both in aqueous media
77                         In this Article, the photophysics and the dynamics of an efficient SPP-mediat
78 nits to the aniline nitrogens influenced the photophysics and the sensory responses of the XFs, as th
79 ate the dopant effects on both the intrinsic photophysics and their interfacial charge transfer by co
80 stimulus-dependent changes in intrinsic 2-AP photophysics and/or interactions with adjacent residues.
81 monstrate prolonged air stability, excellent photophysics, and amplified spontaneous emission and las
82                               The synthesis, photophysics, and biochemical utility of a fluorescent N
83  of instrumentation, sample preparation, and photophysics, and describe major evolving strategies for
84                        The electrochemistry, photophysics, and ECL of Ru(bpy)3(2+) in the presence of
85 ight and direct visualisation of dissipative photophysics, and illustrate this with an example based
86             The synthesis, characterization, photophysics, and oxygen sensing properties are examined
87 lity, important fundamental questions on the photophysics, and paths forward to improve the performan
88 icant implications for understanding CdSe NC photophysics, and suggest that photochemistry and short-
89 Cl-BI) chromophore allowed us to establish a photophysics-aperture relationship.
90 ased our understanding of O(2)(a(1)Delta(g)) photophysics appreciably and facilitated both spatial an
91  and emission spectra, electrochemistry, and photophysics are described.
92 also has a pronounced effect on the observed photophysics, as introduction of electron-releasing aryl
93 olecules are at the heart of photochemistry, photophysics, as well as photobiology and also play a ro
94  The recent discovery of thermally activated photophysics at CdSe nanocrystal-molecule interfaces ena
95                   By exploiting the enhanced photophysics at low temperature, angstrom precision can
96  of BA in the crystal structure can tune its photophysics between SF and SB-CS.
97 y expands the purview of thermally activated photophysics beyond what is possible using only molecule
98 ansmitters in terms of molecular energetics, photophysics, binding affinity, stability, and energy of
99 t also in applications, including catalysis, photophysics, bioorganometallic chemistry, materials, et
100 hibit size-tunable emission spectra and rich photophysics, but their atomic organization is poorly un
101 phores, demonstrating how coupled oscillator photophysics can yield organic photovoltaic device (OPV)
102 ular localized states offer within molecular photophysics/chemistry and organic electronics, we hope
103 These inorganic emitters, which exhibit rich photophysics combined with a high phosphorescence quantu
104                                 Their unique photophysics depend sensitively on the presence or absen
105 l recombination and realize nearly intrinsic photophysics-dictated device performance in 2D semicondu
106 cribe the synthesis, computational analysis, photophysics, electrochemistry and electrochemiluminesce
107                      In this work, the basic photophysics, electrochemistry, and electrogenerated che
108             In this report, we established a photophysics-electronics correlation for actinide-contai
109 hts the synergy between molecular design and photophysics for advancing theranostic applications.
110 sts that multiple triplet states mediate the photophysics for efficient light emission in delayed flu
111 nergy transfer is utilized to engineer donor photophysics for facile signal amplification and selecti
112 e amino group twisting ability in the BODIPY photophysics for nonsterically hindered and constrained
113 ography (qPAINT), works independently of dye photophysics for robust counting with high precision and
114 lassic excited-state singlet and triplet PZn photophysics for the A(His):B(Thr):(DPP)Zn protein (k(fl
115  We further show that sg-FCS can distinguish photophysics from dynamic intensity changes even if a da
116                                          The photophysics have been elucidated by intensity-dependent
117 lexes of Ru(ii) and Ir(iii), compounds whose photophysics have been studied for decades within the in
118 ds based on single-molecule localization and photophysics have brought nanoscale imaging with visible
119  have been employed to successfully describe photophysics in a variety of molecular materials.
120 ielding a comprehensive understanding of its photophysics in DNA.
121  manifestations of interesting chemistry and photophysics in N-heterocyclic coordination compounds of
122  disconnect persists between the fundamental photophysics in pristine 2D semiconductors and the pract
123 id photooxidation and for the study of their photophysics in real-world environments.
124                          To characterize 2AP photophysics in the context of a DNA strand, time-depend
125 unction are presented, along with underlying photophysics in these blends.
126 sient absorption spectroscopy to investigate photophysics in these molecules, we find that homoconjug
127 s spectacular expansion is their fascinating photophysics involving a complex interplay of carrier, l
128 ommonly associated with exciton dynamics and photophysics involving charge and energy transfer, as we
129                    Finally, the advantageous photophysics is complemented by a significant photostabi
130                           We show that their photophysics is essentially governed by the multitude of
131                                        Their photophysics is governed by the twist of lateral phenyl
132 on has been well established, the subsequent photophysics is highly sensitive to the local protein en
133  material bandgap without altering ultrafast photophysics is reported.
134          However, our understanding of their photophysics is still limited, hampering their quantitat
135                                         TADF photophysics is then quantitatively addressed in a coher
136 rade polyacenes but also it can affect their photophysics, leading to both the sensitization and quen
137   These shortcomings are a result of complex photophysics, leading to rate asynchrony between oxidati
138 r charge transfer (CT) mechanism governs the photophysics of (th)G independently of its flanking nucl
139 investigate the effect of aggregation on the photophysics of 1,4-diethynylbenzenes, we analyzed the a
140  2D devices and highlight that the intrinsic photophysics of 2D semiconductors can be used to create
141  or "d-d" states that typically dominate the photophysics of 3d metal complexes but with significant
142 centered states in analogy to the well-known photophysics of [Ru(bpy)(3)](2+).
143                           Here, we tuned the photophysics of a 9,9'-bianthracene (BA) single crystal
144 omolecular structure based on the changes in photophysics of a chromophore upon dimer formation.
145                     Here, we investigate the photophysics of a prototypical polyyne (i.e., 1D chain w
146 nce spectroscopies, we have investigated the photophysics of a series of carbon nitrides on time scal
147 synthesis, structures, electrochemistry, and photophysics of a series of facial (fac) and meridional
148 port a systematic study on the synthesis and photophysics of all possible 6,8-disubstituted luminol d
149                             We find that the photophysics of allomelanin starkly differs from that of
150 erto not been observed in the intramolecular photophysics of an isolated anion, raising questions int
151 rovides mechanistic insight into the complex photophysics of Anthozoan PCFPs and will facilitate futu
152    A key element and enduring mystery in the photophysics of azobenzenes, central to all such applica
153 rick base pair is an inadequate model of the photophysics of B-DNA.
154 iferin in the gas phase and characterize the photophysics of both keto and enol forms.
155                                          The photophysics of both the sodium salts and the ethyl este
156 ce characterisation approaches to reveal new photophysics of broadly-studied hematite devices.
157  well suited as a testbed for studies of the photophysics of carbon-based nanoscopic emitters.
158               These results suggest that the photophysics of CH3NH3SnI3 perovskite are as favorable a
159  there is less progress in understanding the photophysics of common optoacoustic contrast agents.
160 dition to detailing a process central to the photophysics of Cr(III), these results reinforce the not
161                             By examining the photophysics of CsPbBr(3) quantum dots (QDs), nanowires
162 izers but also shed general insight into the photophysics of d(3) and related Mn complexes.
163                                          The photophysics of dialkylamino- and/or pyridine-containing
164  materials and highlights new aspects in the photophysics of donor-acceptor small molecules when comp
165                 The results show the complex photophysics of efficient TADF materials and give clear
166 understanding and ultimately controlling the photophysics of energy flow in CNT-based devices.
167                        However, to date, the photophysics of excitons in carbon nanotubes is largely
168  (3)(d-d) states are commonly invoked in the photophysics of ferrocene complexes, mention of the high
169 igand field excited states that dominate the photophysics of first-row transition metal complexes.
170                                          The photophysics of flavins is highly dependent on their env
171 is also provides a new tool for studying the photophysics of fluorescent molecules and chemosensors a
172           We also provide an overview of the photophysics of fluorescent proteins, highlighting the i
173 t detailed and precise information about the photophysics of fluorescent specimens at optical resolut
174 ibution (i.e., the lattice constant) and the photophysics of fluorophores (i.e., critical radius of t
175          In addition, the role of W57 in the photophysics of GFP has been probed by mutating this res
176 phore framework used to design and interpret photophysics of iSF materials.
177 ties from blending organic orbitals with the photophysics of metal halide semiconductors.
178 w us to systematically unravel the ultrafast photophysics of molecular dyads and triads in surface ar
179 es, two of our groups previously studied the photophysics of Ni((t-Bu)bpy)(o-Tol)Cl, which is represe
180 tivated in processes that involve light, the photophysics of O(2)(a(1)Delta(g)) are equally important
181  exploited for tuning the photochemistry and photophysics of organic chromophores.
182 d by Coulomb attraction, plays a key role in photophysics of organic molecules and drives practically
183 comparison of the efficiency, stability, and photophysics of organic solar cells employing poly[(5,6-
184                               We explore the photophysics of P(NDI2OD-T2), a high-mobility and air-st
185 ta provide a unifying picture of the complex photophysics of PCFPs and RSFPs.
186 w effective synthetic strategy to tailor the photophysics of phenothiazine-based organic materials fo
187                                 Although the photophysics of QDs has been intensely studied, much les
188                                    Here, the photophysics of red fluorescent protein (dsRed) from dis
189 The effect of a methanesulfinyl group on the photophysics of several aromatic chromophores is reporte
190 ress in characterizing and understanding the photophysics of single molecules in condensed matter, mo
191                           To investigate the photophysics of special pairs independently of the compl
192 ring analysis that leverages on the blinking photophysics of specific organic dyes showed that the ma
193                      Here, we report unusual photophysics of state-of-the-art InP-based quantum dots,
194                  Then the photochemistry and photophysics of strongly coupled systems using Fabry-Per
195 onic structure theory is used to analyze the photophysics of sulfur-bridged terthiophene dimers.
196 ically coupled mechanism describes the basic photophysics of TADF.
197 ehensive investigation of the solution-phase photophysics of tetracene bis-carboxylic acid [5,12-tetr
198 ereochemical environment strongly affect the photophysics of the complexes, particularly the phosphor
199 n important role in the electrochemistry and photophysics of the complexes.
200                                          The photophysics of the cruciforms was investigated upon add
201 important temperature-related changes in the photophysics of the dyes that have been largely ignored.
202 the kinetic rates that govern the stochastic photophysics of the fluorophores to improve the predicti
203                    Here, we investigated the photophysics of the FRET-opsin GEVIs Voltron1 and Voltro
204 esults bring important new insights into the photophysics of the GFP chromophore and provide a new sc
205 , the inclusion of these dopants affects the photophysics of the host in a surprising way, generating
206 does not have a substantial influence on the photophysics of the materials.
207                                              Photophysics of the MLCT excited-state of [Ru(bpy)(tpy)(
208             We start with an overview of the photophysics of the nucleobases in the gas phase and in
209 ) from 6 to 900 has been synthesized and the photophysics of the series and monomer cyanine dye have
210 um yields were measured as well to probe the photophysics of the system.
211  a detailed and comprehensive picture of the photophysics of thermally activated delayed fluorescence
212                       Knowing the underlying photophysics of thermally activated delayed fluorescence
213              We conclude by arguing that the photophysics of these carbon nitride materials show clos
214 iding direct measurements of the spectra and photophysics of these chemically identical molecules in
215 ion mechanism, shedding light on the complex photophysics of these dyes.
216 r and delocalized or excitonic states in the photophysics of these systems and discuss the main photo
217 , there have been few studies concerning the photophysics of these systems.
218 suitable metals for this transformation, the photophysics of these trimeric molecules, as well as the
219 und by Coulomb interactions or excitons, the photophysics of thin films made of Ruddlesden-Popper per
220 l Review, we present a basic overview of the photophysics of this class of compounds with the goal of
221 scence bands adding to the complexity of the photophysics of this family of materials.
222                            Understanding the photophysics of this system is of interest to further ad
223 tical calculations help explain the specific photophysics of this system, while time-resolved EPR sho
224  knowing the defect density in understanding photophysics of TMDCs.
225  it a powerful tool for studying the complex photophysics of transition metal complexes.
226 A general approach to dissecting the complex photophysics of tryptophan is presented and used to eluc
227 en employed to investigate the excited-state photophysics of vitamin B12 (cyanocobalamin, CNCbl) and
228 ve description of the CsPbBr(3) perovskites' photophysics, offering novel insights on the light-induc
229 gs also show a substantial dependence of ANI photophysics on hydrogen bonding with the solvating medi
230 tions associated with dye photochemistry and photophysics, or the requirement for fluorescent labelin
231 iew highlights the physical interactions and photophysics properties of Mol@NT obtained by the confin
232 els are needed to rationalise the regimes of photophysics reached in these materials.
233 ations to provide a detailed analysis of the photophysics, reactivities, and unexplained stereoselect
234  Fe(II) complexes that express (3)MLCT state photophysics reminiscent of their heavy-metal analogs.
235 le of ultrafast spectroscopy and fundamental photophysics studies in advancing perovskite optoelectro
236 ield a unifying picture of the excited-state photophysics that accounts for observations in both type
237 ast decades in understanding the fundamental photophysics that governs the spectroscopic and environm
238               While caveats remain regarding photophysics, this suggests that the supertertiary confo
239 higher pulse energy enables novel regimes of photophysics to be exploited for microscopic imaging.
240                        We use a model of the photophysics to decompose the phosphorescent enhancement
241 Our results highlight the sensitivity of the photophysics to local environment, which may control the
242 ipation by leveraging the sensitivity of the photophysics to the protein structure.
243                                              Photophysics tunability through alteration of framework
244                               However, their photophysics typically suffer from slow reverse intersys
245  a universal functional form, independent of photophysics, under relatively mild assumptions.
246                          Confinement-imposed photophysics was probed for novel stimuli-responsive hyd
247  broad range of functional groups, for which photophysics were experimentally and theoretically inves
248 portunities for molecular photochemistry and photophysics, which has caused an ever-rising interest i
249 al imaging to correlate the local changes in photophysics with composition in CH3NH3PbI3 films under
250 emonstrate a new regime of intrinsic exciton photophysics with prolonged spontaneous emission times u

 
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