ライフサイエンスコーパス: energy transfer

1 ly uncharacterized chlorophyll-to-carotenoid energy transfer.

2 text] showing nonexpected scattering at low-energy transfer.

3 of bound ligand results in Forster resonance energy transfer.

4 , immunoblotting, and fluorescence resonance energy transfer.

5 hose of fluorescence-based Forster resonance energy transfer.

6 oprecipitation and bioluminescence resonance energy transfer.

7 cceptor, and subsequent CP Forster resonance energy transfer.

8 ; enhancing tunneling events; and optimizing energy transfer.

9 vent dye self-quenching and ensure efficient energy transfer.

10 d more n-type characteristics for sufficient energy transfer.

11 s photoredox catalytic processes and triplet energy transfer.

12 antenna followed by intramolecular-FRET/TBET energy transfers.

13 ter separation of the Mn centers and prevent energy transfer, a bulky singly protonated cation that a

14 t-matter interactions that induce charge and energy transfer across interfaces form the foundation fo

15 The mechanisms of triplet energy transfer across the inorganic nanocrystal/organic

16 de and confocal/sensitized Forster resonance energy transfer analyses revealed that these fibrils sho

17 quitin screens and in vivo Forster resonance energy transfer analyses showed that exocyst EXO70 subun

18 namics simulation and fluorescence resonance energy transfer analysis suggest that Ca(2+) binding to

19 work indicate successful triplet-to-singlet energy transfer and a sizable increase in the transfer k

20 t absorption study of FR-PSII, investigating energy transfer and charge separation processes.

21 tanding the overall energetics of excitation energy transfer and charge separation reactions in FR-PS

22 rations, thus restricting the intermolecular energy transfer and corresponding quenching phenomena.

23 entral dye, thereby explaining the efficient energy transfer and demonstrating similarity with struct

24 us emission enhancement, to plasmon-assisted energy transfer and enhancement of two-photon transition

25 ng acceptor photobleaching Forster resonance energy transfer and fluorescence cross-correlation spect

26 o DUX4 as assessed by fluorescence resonance energy transfer and fluorescence polarization techniques

27 ntegrating single-molecule Forster resonance energy transfer and hydrogen-deuterium exchange mass spe

28 mApple to quantify the effects of resonance energy transfer and incomplete maturation of mApple on b

29 n to ICD and draws the connection to related energy transfer and ionization processes.

30 super-resolution imaging, Forster resonance energy transfer and nanoscale total internal reflection

31 ing intermolecular bioluminescence resonance energy transfer and proximity ligation assays, we found

32 in nanoimaging, nanoscale light propagation, energy transfer and quantum physics.

33 molecularly imprinted sensors, ECL resonance energy transfer and ratiometric biosensors and give futu

34 reatment strategy because of the high-linear-energy transfer and short pathlength of alpha-radiation

35 the specificity of bioluminescent resonance energy transfer and the high signal intensity of HiBiT/L

36 n the confined nanospace was critical to the energy transfer and the light-harvesting efficiency.

37 ct their reactivities based on triplet state energy transfer and transition state energy feasibility.

38 esolution microscopy, fluorescence resonance energy transfer, and biochemical analysis, we observed t

39 tenna size while maintaining fast excitation energy transfer, and thus high trapping efficiency, with

40 ubtle compositional changes on intermetallic energy transfer, and thus on the resulting photophysical

41 and coupled voltage signals for the wireless energy transfer are developed, showing excellent agreeme

42 (picosecond time scale) and highly efficient energy transfer (around 90% efficiency), as evidenced by

43 namics and photophysics involving charge and energy transfer, as well as exciton dissociation and cha

44 ere assessed in a time-resolved fluorescence energy transfer assay against the full-length recombinan

45 Fast kinetic bioluminescence resonance energy transfer assays in transfected HEK cells showed t

46 bitory factor (MIF), using Forster resonance energy transfer-based approaches.

47 Using Foerster resonance energy transfer-based biosensors in patch clamp experime

48 udies coupled with bioluminescence resonance energy transfer-based cellular studies to show that STAM

49 le stability, measured via Forster resonance energy transfer-based fluorescent spectrometry, was comp

50 the-art time-resolved fluorescence resonance energy transfer-based internalization assay to directly

51 While Forster resonance energy transfer-based methods have traditionally been wi

52 Using a fluorescence resonance energy transfer-based substrate cleavage assay, we showe

53 fying single-molecule fluorescence resonance energy transfer between a first fluorescent probe in the

54 Experimentally observed energy transfer between a range of different polymer fil

55 ted by measurement of fluorescence resonance energy transfer between coexpressed fluorophore-tagged s

56 munoassay (FLFIA) depending on non-radiative energy transfer between graphene oxide and quantum dots

57 duce the use of homo-FRET (Forster resonance energy transfer between identical fluorophores) fluoresc

58 olled by host differential sensitization and energy transfer between lanthanide ions.

59 Selective vibrational energy transfer between molecules in the liquid phase, a

60 to-hopping transition for long-range triplet energy transfer between nanocrystal light absorbers and

61 opamine is assessed by quantifying resonance energy transfer between receptor and ligand.

62 nanoring was synthesized as a model for the energy transfer between the light-harvesting complex LH1

63 iting step in the exciton propagation is the energy transfer between the originally prepared excitons

64 illars confirms efficient triplet-to-triplet energy transfer between the porphyrin linkers and the mo

65 inding of CN(-) to hemicyanine inhibited the energy transfer between the two moieties, resulting in a

66 Live cell Forster resonance energy transfer biosensor imaging of cultured myocytes r

67 r activation using bioluminescence resonance energy transfer biosensors revealed a predominant effect

68 ab has developed a bioluminescence resonance energy transfer (BRET) imaging approach that directly su

69 Bioluminescence resonance energy transfer (BRET) is a sensitive optical detection

70 Galphao-betagamma bioluminescence resonance energy transfer (BRET) sensor, we found that GPR158 decr

71 Bioluminescence resonance energy transfer (BRET) technology offers new insight by

72 Using bioluminescence resonance energy transfer (BRET), HO-1 formed HO-1*P450 complexes

73 Using bioluminescence resonance energy transfer (BRET)-based and conformational fluoresc

74 he hydrogen-bonded system is less rigid, and energy transfer by chromophore relaxation is accelerated

75 se its light collection efficiency (i.e., CR energy transfer) by conjugation with multiple CR-absorbi

76 C function, as measured by Forster resonance energy transfer, Ca(2+) imaging, and electrophysiologica

77 Our findings reveal that efficient energy transfer can be achieved for thin (<=10 nm) organ

78 Resonance energy transfer can be used to constitutively or dynamic

79 on via intermolecular homo-Forster resonance energy transfer can decipher the architecture of amyloid

80 also rendered enantioselective by harnessing energy transfer catalysis to mediate selective radical g

81 alysis and single-molecule Forster Resonance Energy Transfer confirm that these mutations prevent CD4

82 plify signal via chemiluminescence resonance energy transfer (DAS-CRET) using two non-conjugated smar

83 2D layer passivating the 3D material, or in energy-transfer devices requiring controlled energy flow

84 s) residing in the antenna are important for energy transfer dynamics and yield, however, their preci

85 grees of freedom (DoF) during the excitation energy transfer (EET) dynamics of light-harvesting compl

86 Site-specific homo-Forster resonance energy transfer efficiencies measured by fluorescence de

87 This is analogous to an energy transfer efficiency and allows experiments perfor

88 Additionally, changes in energy transfer efficiency and interchromophore distance

89 y in pulse mode, and achieves over 94% total energy transfer efficiency in constant mode.

90 ocess is successfully fabricated, showing an energy transfer efficiency up to 95% and a remarkably hi

91 carotenoid-to-(bacterio)chlorophyll [(B)Chl] energy transfer efficiency.

92 The energy-transfer efficiency can be further enhanced by in

93 gineer electrochromic fluorescence resonance energy transfer (eFRET) genetically encoded voltage indi

94 or and acceptor were chosen to facilitate an energy transfer (EnT) from the excited MOF (i.e., NU-100

95 410-490 nm, lambda(max) = 465 nm) through an energy transfer (EnT) process, followed by homolytic cle

96 fforded the attainment of a highly efficient energy transfer (ET).

97 etation of single molecule Forster resonance energy transfer experiments (FRET) supported the theoret

98 Single-molecule Forster resonance energy transfer experiments confirm that the +3 RTIC is

99 ous spin-labeling and fluorescence resonance energy transfer experiments designed to monitor the posi

100 Fluorescence resonance energy transfer experiments in HEK293 cells transfected

101 g molecular modeling, fluorescence resonance energy transfer experiments on living cells, biochemical

102 Forster resonance energy transfer experiments using full-length SARAF vali

103 ination of single-molecule Forster resonance energy transfer experiments, polymer theory, and molecul

104 Time-resolved fluorescence resonance energy transfer fluorescence assays demonstrated that l-

105 rce-profile analysis (FPA) and photo-induced energy-transfer fluorescence correlation spectroscopy (P

106 ARF1*GTPs in vivo by fluorescence resonance energy transfer-fluorescence lifetime imaging microscopy

107 bsorption results obtained herein imply that energy transfer for all three compounds has near unity y

108 lasers, and adiabatic control of topological energy transfer for mode and polarization conversion.

109 Forster resonance energy transfer (FRET) and fluorescence cross-correlatio

110 In particular, we use Forster resonance energy transfer (FRET) and fluorescence intensity fluctu

111 of dynamic single-molecule Forster Resonance Energy Transfer (FRET) and kinetic Monte Carlo (kMC) sim

112 based on the principle of Forster resonance energy transfer (FRET) and using upconversion nanopartic

113 Both fluorescence resonance energy transfer (FRET) and western blotting revealed the

114 Therefore, we employed a Forster resonance energy transfer (FRET) approach using a small fluorescei

115 ding domain, we engineer a Forster resonance energy transfer (FRET) based biosensor deemed BioSTING.

116 udy, we have constructed a Forster Resonance Energy Transfer (FRET) based pH nanoprobe using upconver

117 We used Forster energy transfer (FRET) between 7AW and the flavin to est

118 Here, we show that Forster resonance energy transfer (FRET) between fluorescent dyes and betw

119 Here, we measured Forster resonance energy transfer (FRET) between fluorescent proteins fuse

120 Using a fluorescence resonance energy transfer (FRET) biosensor-based assay, a variety

121 ith fluorescent probes and Forster resonance energy transfer (FRET) biosensors to monitor the changes

122 cence quenching assays and Forster resonance energy transfer (FRET) distance measurements.

123 label and as an interbase Forster resonance energy transfer (FRET) donor.

124 ching of fluorescence in a Forster resonance energy transfer (FRET) donor/acceptor couple of antibody

125 proposed and studied novel Forster resonance energy transfer (FRET) dual DNA probes with the excimer-

126 ion spectroscopy (FCS) and Forster resonance energy transfer (FRET) enable assessment of interaction

127 n reaction is monitored by Forster resonance energy transfer (FRET) experiments both in solution and

128 Fluorescence resonance energy transfer (FRET) experiments show that the mBBC fo

129 -based intramolecular fluorescence resonance energy transfer (FRET) experiments to determine structur

130 nd acceptor blocks exhibit Forster resonance energy transfer (FRET) from the PDHF inner core to the P

131 hat performs comparably to Forster resonance energy transfer (FRET) has not yet been reported.

132 Forster resonance energy transfer (FRET) is a powerful tool to investigate

133 tassium efflux assays, and Forster resonance energy transfer (FRET) measurements.

134 has benefited greatly from Forster Resonance Energy Transfer (FRET) measurements.

135 imaging microscopy (FLIM)-Forster resonance energy transfer (FRET) microscopy data acquired in live

136 g in conjunction with fluorescence resonance energy transfer (FRET) microscopy to uncover the molecul

137 erbium-to-quantum dot (QD) Forster resonance energy transfer (FRET) nanoprobe with narrow and tunable

138 , we designed a novel fluorescence resonance energy transfer (FRET) peptide derived from a gel-based

139 nd analyses of three-color Forster resonance energy transfer (FRET) spectroscopy for probing sub-mill

140 ing TFs, and a quantum-dot Forster Resonance Energy Transfer (FRET) strategy for transducing analyte

141 sion was also confirmed by Forster resonance energy transfer (FRET) studies to show membrane blending

142 rely on the measurement of Forster resonance energy transfer (FRET) to detect changes in biosensor co

143 we employ single molecule Forster resonance energy transfer (FRET) to determine the influence of wil

144 munoprecipitation and fluorescence resonance energy transfer (FRET) to quantify micropeptide oligomer

145 yes that undergo efficient Forster Resonance Energy Transfer (FRET) to red fluorescent acceptor hybri

146 method for measurements of Forster resonance energy transfer (FRET), and for quantification of protei

147 eveloped a sensor based on Forster resonance energy transfer (FRET), which uses the principles of pol

148 e have developed a tunable Forster resonance energy transfer (FRET)-based assay to detect triplex/H-D

149 Genetically encoded Forster Resonance Energy Transfer (FRET)-based biosensors are powerful too

150 Here, we used a Forster Resonance Energy Transfer (FRET)-based cGMP biosensor combined wit

151 ve expanded the toolbox of Forster Resonance Energy Transfer (FRET)-based ERK biosensors by creating

152 FPs), we engineered an NIR Forster resonance energy transfer (FRET)-based genetically encoded calcium

153 This study utilized a Forster resonance energy transfer (FRET)-based molecular tension sensor an

154 a genetically encoded fluorescence resonance energy transfer (FRET)-based Pb(2+) biosensor, 'Met-lead

155 Fluorescence/Forster resonance energy transfer (FRET)-based probes are capable of monit

156 Using a Forster resonance energy transfer (FRET)-based screening strategy, we foun

157 Here, a new Forster resonance energy transfer (FRET)-based sensor is integrated with a

158 ton-induced processes in a Forster resonance energy transfer (FRET)-operated photochromic fluorene-di

159 a, found in a sample using Forster resonance energy transfer (FRET).

160 y, which can be studied by Forster resonance energy transfer (FRET).

161 nformational state by fluorescence resonance energy transfer (FRET).

162 using single-molecule fluorescence resonance energy transfer (FRET).

163 minimally-perturbing fluorescence-resonance-energy-transfer (FRET) biosensor (FynSensor) that reveal

164 eloped a J-aggregate-based Forster-resonance energy-transfer (FRET) method to investigate the release

165 s of oximes can be harnessed via the triplet energy transfer from a commercially available iridium ph

166 We also report functional energy transfer from a cytoplasmic fluorescent protein d

167 y be eliminated through efficient excitation energy transfer from a photoexcited polymer layer to the

168 Using transient absorption spectroscopy, energy transfer from an iridium photocatalyst to a catal

169 xperimental studies provide evidence for the energy transfer from an iridium photocatalyst to the all

170 mpromise that retains an acceptable level of energy transfer from carotenoids to (B)Chls while allowi

171 tion spectroscopy is used to confirm triplet energy transfer from CdSe to transmitter, and the format

172 Results show a rapid subpicosecond energy transfer from chlorophyll-a to the long-wavelengt

173 of photosystem II activity along with direct energy transfer from photosystem II to photosystem I pla

174 t excitons that are directly created through energy transfer from singlet oxygen molecules ((1)O(2)).

175 The complex displays efficient energy transfer from the central cyanine dye to the surr

176 ghly oriented 2D crystal films have a faster energy transfer from the high-bandgap domains to the low

177 me of 36 ps, being kinetically controlled by energy transfer from the long-wavelength chlorophyll to

178 The measurement of the secular energy transfer from the parallel electric field as a fu

179 rates catalysis triggered by triplet-triplet energy transfer from the quantum dot.

180 ructural analysis quantitatively revealed an energy transfer from W51 and W350 to trans-resveratrol w

181 al wave power, which is the transport of the energy transferred from the wind into sea-surface motion

182 On the one hand, using nonradiative energy transfer, GOMs are conceived to deactivate the ph

183 dimers quantitatively, leading to efficient energy transfer (>85 %) upon photoexcitation.

184 nt light elicits homotypic Forster resonance energy transfer (homo-FRET), in which the emitted radiat

185 color single-molecule fluorescence resonance energy transfer imaging and molecular dynamics simulatio

186 can be visualized and quantified by Cerenkov energy transfer imaging, positron-emission tomography, a

187 ed by single-molecule (SM) Forster Resonance Energy Transfer imaging.

188 the mechanisms of fluorescence quenching and energy transfer in complex DNA probes and the choice of

189 ptoelectronic applications such as efficient energy transfer in disordered condensed matter systems.

190 work contributes to the general knowledge of energy transfer in materials and provides groundwork for

191 fect of spin-orbit coupling on dipole-dipole energy transfer in MOFs using steady-state and time-reso

192 We employ Forster resonance energy transfer in order to trace intra and intermolecul

193 etinal after photoactivation and decelerates energy transfer into the protein by impairing the releas

194 ing the cavity lifetime, suggesting that the energy transfer is a polaritonic process.

195 the tumor site is maximized and efficient CR energy transfer is enabled, which maximizes the tumor-ta

196 Efficient energy transfer is particularly important for multiexcit

197 ectroscopy experiments reveal that resonance energy transfer is the mechanism responsible for the flu

198 ering three different scenarios: (a) triplet energy transfer is the rate controlling step, (b) excite

199 In addition, bioluminescent resonance energy transfer is used to quantify dynamic interactions

200 activity were monitored by Forster resonance energy transfer, L-type Ca(2+) current by whole-cell pat

201 ss vibrational energy available from triplet energy transfer leads to hot and nonstatistical dynamics

202 cal advantages of low-energy and high-linear energy transfer (LET) protons present within the Bragg p

203 ng micrometastases because of the low-linear-energy-transfer (LET) properties of high-energy beta-par

204 bserved by single-molecule Forster resonance energy transfer measurements.

205 rom the ligand triplet state is the dominant energy transfer mechanism in these photoluminescent syst

206 We envision that our study of the productive energy-transfer-mediated pathway would encourage the dev

207 otoredox conditions have unanimously invoked energy-transfer-mediated pathways.

208 gel electrophoresis, fluorescence resonance energy transfer-melting, electrospray ionization mass sp

209 molecules, phospholipid cell membranes, and energy transfer molecules such as adenosine triphosphate

210 ntagonists using a bioluminescence resonance energy transfer (NanoBRET) assay.

211 h a nanoluciferase bioluminescence resonance energy transfer (NanoBRET)-based ligand binding assay fo

212 Ps scaffold through the nanomaterial-surface energy transfer (NSET) effect, which gives an extended l

213 antage of the highly efficient non-radiative energy transfer occurring between photoexcited fluoropho

214 The use of single-molecule Forster resonance energy transfer offers a unique tool to map conformation

215 (dsDNA) samples containing Forster resonance energy transfer pairs.

216 This vibrational energy-transfer pathway opens doors for applications in

217 hown that, although there are a multitude of energy transfer pathways between distant parts of a prot

218 es have led to a map of the architecture and energy transfer pathways between LHC pigments.

219 oxidation or reduction of the tetrasulfide, energy transfer photocatalysis was particularly useful.

220 s to shift single-molecule Forster resonance energy transfer populations back toward the on-pathway c

221 tibodies with a FRET (fluorescence resonance energy transfer) probe to gauge the redox activity of th

222 We have developed a panel of cell-permeable energy transfer probes to quantify target occupancy for

223 Energy transfer proceeds in orthogonal dyads in contrast

224 nd B850 BChls a These measurements show that energy transfer proceeds with an efficiency of ~100%, pr

225 with a two-step sequential Forster resonance energy transfer process is successfully fabricated, show

226 nt dearomatization of the heterocycle via an energy transfer process promoted by an iridium-based pho

227 The energy transfer process was spectroscopically probed by

228 ion, which is initiated by a triplet-triplet energy transfer process.

229 ing diodes with broad substrate scope via an energy transfer process.

230 ox units enables us to understand the charge/energy-transfer process within these crystalline solid c

231 lasmon-induced hot electron and the resonant energy transfer processes can occur on a time scale of l

232 to the understanding of light-harvesting and energy transfer processes that occur within these molecu

233 nce lifetime upon photoisomerization-induced energy transfer processes through light irradiation.

234 mphasis on the charge (electron, proton) and energy transfer processes.

235 introduced a homogeneous quenching resonance energy transfer (QRET) assay for nucleotide binding stud

236 introduce a homogeneous quenching resonance energy transfer (QRET) for cGMP to monitor both sGC and

237 New Forster resonance energy transfer reporters were used to assay Ca(2+) and

238 Knowledge of rotational energy transfer (RET) involving carbon monoxide (CO) mol

239 Photo-induced electron/energy transfer reversible addition-fragmentation chain

240 nt porphyrin-catalyzed photoinduced electron/energy transfer-reversible addition-fragmentation chain-

241 monic effects are outlined, such as resonant energy transfer, scattering, hot electron injection, gui

242 ubcellularly targeted fluorescence resonance energy transfer sensors can precisely locate and measure

243 y detected by nonlocalized Forster resonance energy transfer sensors were induced by pacing and minim

244 Using single-molecule Forster resonance energy transfer (smFRET) and cleavage assays, we show th

245 used single molecule fluorescence resonance energy transfer (smFRET) and molecular dynamics simulati

246 reening of single-molecule Forster resonance energy transfer (smFRET) data to identify high-quality t

247 emical and single-molecule Forster resonance energy transfer (smFRET) experiments, we studied how fra

248 Single-molecule fluorescence resonance energy transfer (smFRET) has revealed that native Env on

249 le-molecule fluorescence (Forster) resonance energy transfer (smFRET) imaging to observe conformation

250 Single-molecule Forster Resonance Energy Transfer (smFRET) is a powerful technique capable

251 Single-molecule Forster resonance energy transfer (smFRET) is a powerful technique for inv

252 Single-molecule Forster Resonance energy transfer (smFRET) is an adaptable method for stud

253 udies, our single-molecule Forster resonance energy transfer (smFRET) measurements of junction dynami

254 le-molecule Forster (fluorescence) resonance energy transfer (smFRET) measurements of the amino acid

255 sis we use single molecule Forster Resonance Energy Transfer (smFRET) to measure the conformation of

256 AFM), single-molecule fluorescence resonance energy transfer (smFRET), nanopore tweezers, and hybrid

257 assay and single-molecule Forster resonance energy transfer (smFRET)-imaging, we found that acidic p

258 SAXS), and single-molecule Forster Resonance Energy Transfer (smFRET).

259 inks using single-molecule Forster Resonance Energy Transfer (smFRET).

260 hree-color single-molecule Forster resonance energy transfer spectroscopy to obtain the distribution

261 to anthracene through a single 15 ns Dexter energy transfer step with a nearly 50% yield.

262 ow direct observation of the ligand-to-metal energy transfer step, preventing a determination of the

263 s of all elementary tryptophan-to-tryptophan energy-transfer steps in picoseconds to nanoseconds, in

264 leic acid isothermal amplification utilizing energy-transfer-tagged oligonucleotide probes provides a

265 No appreciable energy transfer takes place from lutein 1 to lutein 2, c

266 The Forster resonance energy transfer technique also suggested that the same S

267 -sensitive single-molecule Forster resonance energy transfer technique we show that monomeric and oli

268 e use single-molecule fluorescence resonance energy transfer techniques to examine the conformational

269 l scanning calorimetry and Forster resonance energy transfer techniques, we observed that the SM- and

270 a direct proxy for the efficiency of triplet energy transfer (TET), as well as transient absorption m

271 plementation of time-gated Forster resonance energy transfer (TG-FRET) between terbium donors and dye

272 transition metal ion fluorescence resonance energy transfer (tmFRET).

273 e use single-molecule fluorescence resonance energy transfer to characterize the HNH domain motions o

274 ation of the carotenoids and the pathways of energy transfer to chlorophylls.

275 at funnel all excitation quanta by ultrafast energy transfer to individual light-redirecting acceptor

276 eloped an assay using fluorescence resonance energy transfer to measure SNARE complex formation in re

277 ractions determined by oxidation of TMPD and energy transfer to O(2) ((1)O(2) formation) methods.

278 In the remaining complexes (~55%), the energy transfer to P(700) occurred at ~36 ps, similar to

279 Here, we use Forster resonance energy transfer to reveal the architecture of individual

280 ed yield of the fission in tetracene and the energy transfer to silicon is around 133 per cent, estab

281 ly one is directly involved in the resonance energy transfer to sulfo-Cy3.

282 exciton states of the molecules can undergo energy transfer to the lanthanide ions with unity effici

283 Accordingly, energy transfer to the protein is achieved by chromophor

284 a sensitive time-resolved Forster resonance energy transfer (TR-FRET) detection method for PTMs of c

285 ve used time-resolved fluorescence resonance energy transfer (TR-FRET) to study structural changes in

286 chnology and time-resolved Forster resonance energy transfer (TR-FRET).

287 from single-molecule fluorescence resonance energy transfer trajectories without the need for solvin

288 or to a co-catalyst through triplet-triplet energy transfer (TT EnT).

289 Using optimized conditions, the energy transfer UC process could be observed for the fir

290 tion principle is based on Forster resonance energy transfer using gold nanoclusters as a signal repo

291 tograms of single-molecule Forster resonance energy transfer values to a sum of two Gaussians and the

292 Energy transferred via thermal radiation between two sur

293 Using single-molecule Forster resonance energy transfer, we identified functionally relevant ope

294 rmation was measured using Forster resonance energy transfer, which detects nanodomains as well as la

295 y of the quasi-2D films to achieve efficient energy transfer, which is a critical requirement for lig

296 d boosts the efficiency of Forster resonance energy transfer, which was observed experimentally by a

297 n because of their breeding strategy of high energy transfer while fasting, but we anticipate that mo

298 ed state investigations such as electron and energy transfer with electron-acceptors and -donors.

299 aling unit that engages in Forster resonance energy transfer with the indicator dye.

300 gnificant implications for the structure and energy transfer within ice giants, our results highlight