ライフサイエンスコーパス: charge transfer

1 donor or acceptor, thereby accelerating the charge transfer.

2 and large surface area that can support the charge transfer.

3 hese polymers owing to additional interchain charge transfer.

4 nd-alignments conducive to the phenomenon of charge transfer.

5 to play important roles in facilitating this charge transfer.

6 aterials due to the effect of intramolecular charge transfer.

7 and sufficient orbital overlap for efficient charge transfer.

8 ponse deactivation time course and increased charge transfer.

9 e, suggesting a mechanism of phonon-assisted charge transfer.

10 erties is based on the concept of electronic charge transfer.

11 ains large due to the lack of intramolecular charge transfer.

12 12) and blue for YB(12)-can be attributed to charge-transfer.

13 ing to the low driving force for interfacial charge-transfer.

14 in ~50 ns via a series of pairwise interdot charge transfers.

15 s have potential implications for long-range charge transfers.

16 The unconventional doublet ligand-to-metal charge transfer ((2)LMCT) photoactive excited state exhi

17 te insulation layers are used to inhibit the charge transfer(5,6) or when off-resonance excitations a

18 ism which is based on directly affecting the charge transfer ability of the metal separately by cyste

19 the DFT-calculated charge density reveals no charge transfer/accumulation at the interface, indicatin

20 n the acceptor compartment, by accepting the charge transfer across the SLM, which enabled the applic

21 tructure, the partial density of states, and charge transfer analysis.

22 investigation of their relationship with the charge transfer and adsorption process in the HER.

23 pai-conjugated structure, which facilitates charge transfer and consequently offers good capacitance

24 aled linear encoding of PC rates in synaptic charge transfer and DCN spiking activity.

25 reas (up to 1165 m(2).g(-1)) allow efficient charge transfer and diffusion.

26 atomic distances of 0.6-0.7 and possess both charge transfer and electrostatic characteristics.

27 EFs along the reaction axis can control this charge transfer and impart electrostatic catalysis.

28 .92 quantum yield ascribed to intramolecular charge transfer and intramolecular through-space conjuga

29 ow and observe that the relative energies of charge transfer and locally excited triplet states influ

30 the electrode and electrolyte to facilitate charge transfer and mass transport, plays a vital role i

31 Magnetic field signals tracking the charge transfer and optical Geostationary Lightning Mapp

32 ising from mismatching between photo-induced charge transfer and optical image movements.

33 sting and conversion, but their insufficient charge transfer and rapid charge recombination impede th

34 efect structure: ionic charges contribute to charge transfer and screening at oxide interfaces, trigg

35 Charge transfer and separation are important processes g

36 ion-state changes do not necessarily reflect charge transfer and that the concept of polar mismatch i

37 solvent polarity, affect the outcome of the charge-transfer and corresponding rate constants.

38 d excited states for enhanced mixing between charge-transfer and locally excited states.

39 densates mature via pervasive intermolecular charge-transfer and persistent backbone interactions dri

40 induced process, which couples intermetallic charge-transfer and spin transition, has been debated fo

41 nism involving metal-substrate complexation, charge transfer, and aerobic turnover, involving high-va

42 ctate function, such as vibrational modes or charge transfer, and are limited to room-temperature sam

43 t on the interplay between light absorption, charge transfer, and catalytic activity at molecular-cat

44 This approach to modulate the optical, charge transfer, and catalytic properties of conjugated

45 l heating, light-induced hot electron-driven charge transfer, and direct electron shuttling under dar

46 Different charge-separation, charge-transfer, and charge-recombination routes have be

47 nic coupling matrix elements between ground, charge-transfer, and locally excited states were determi

48 njugation and intramolecular "through-space" charge transfers are molecular phenomena that have been

49 ine would have a few effects: intramolecular charge transfer, aromaticity reversal, rotation, and ste

50 d polyacenes which either favour or prohibit charge transfer as the triplet acceptors.

51 toms and K-PHI is partially originating from charge transfer, as disclosed by our energy decompositio

52 ical transitions are based on intramolecular charge transfer, as shown by solvatochromic measurements

53 tant heteromeric GlyRs is expected to reduce charge transfer at the synapse, despite the high equilib

54 to-fragmentation processes: (a) ligand-metal charge transfer, (b) CF(3) elimination, and (c) C-C bond

55 The TBPCExBox(4+) complex displays a charge transfer band at 450 nm and an exciplex emission

56 this phenomenon to be nested in the smaller charge transfer band gap of the Ni-based compounds compa

57 ious inherent properties like intramolecular charge-transfer band and redox behavior.

58 r-energy Br 4p for Cl 3p orbitals lowers the charge-transfer band gap of the perovskite by 0.9 eV.

59 a step towards understanding and controlling charge-transfer-based functions using light.

60 Charge-transfer-based materials with intramolecular dono

61 addition of 1-5 muM Fe(II) leads to dynamic charge transfer between dissolved and adsorbed species a

62 s exquisitely sensitive to the nature of the charge transfer between F4TCNQ and its matrix.

63 Furthermore, there is an obvious charge transfer between oil and PTFE, which further conf

64 steps revealed details of the structure and charge transfer between the material encapsulated and th

65 netic field, we show that the spin-dependent charge transfer between WSe(2) and CrI(3) is dominated b

66 The energy and charge transfers between adjacent organic and inorganic

67 for spatially separating bond activation and charge transfer by exploiting mixed electron-proton cond

68 d states reveals that efficient photoinduced charge transfer can be achieved in the complexes with pa

69 scenarios, it is an interesting question, if charge transfer can be coupled with RNA function.

70 Its reaction center chromophores, where the charge transfer cascade is initiated, are arranged symme

71 Establishing highly effective charge transfer channels in carbon nitride (C(3) N(4) )

72 s, thus forming both in-plane and interlayer charge transfer channels.

73 onally (TD-DFT calculations), the pronounced charge transfer character of the longest wavelength abso

74 eds through a transition state with moderate charge transfer character.

75 sion in the solid state, attributable to the charge-transfer character of these inclusion complexes.

76 ndicate that this absorption has significant charge-transfer character.

77 Considering their superior charge-transfer characteristics, easy tenability of ener

78 Kinetic parameters such as charge transfer coefficient (0.52 and 0.44 for AT and VC

79 charge transfer rate constant, k(0), and the charge transfer coefficient, alpha) and nonfaradaic term

80 Here, we report our findings on the charge transfer collisions of cold [Formula: see text] i

81 dinated Ti sites, forming the stable dopa-Ti charge transfer complex and thus generating enhanced ano

82 oquinodimethane (F4TCNQ), is of interest for charge transfer complex formation and as a p-dopant in o

83 of SQOR proceeds via formation of an intense charge transfer complex that subsequently decays to elim

84 ovides the first example of a boron-to-metal charge-transfer complex and evidence of a pai-aromatic B

85 eta-FAD at a rate of 920 s(-1), yielding the charge-transfer complex NAD(+):beta-FADH(-) with an abso

86 tation of a rare high-order enzyme-templated charge-transfer complex that forms between an alkene, al

87 species is accessed by photoexcitation of a charge-transfer complex that forms between flavin and su

88 lained by the formation of the anion-solvent charge-transfer complex, which we study for 16 anion-sol

89 PH, probably representing the formation of a charge-transfer complex.

90 ing, S-H...pai, C-H...pai, pai-pai stacking, charge-transfer complexation, etc.

91 ronic properties are summarized, focusing on charge transfer, conductivity, and electronic structure.

92 m of |T(A)|(2), consideration of mixing with charge-transfer configurations and of excitonic interact

93 trochemical models, we find that interfacial charge transfer contributes non-negligibly to this inter

94 on selectively enhances the Fe(2+) -> Fe(3+) charge-transfer contribution in the spin-up channel, str

95 te that an unusual cascade of intermolecular charge-transfer coupled with a multitude of transient no

96 p-stacked molecular geometries and increased charge-transfer couplings.

97 electrochemical properties and energies for charge transfer (CT) absorption and emission compounds a

98 A remarkable charge transfer (CT) band is described in the bifurcatin

99 The charge transfer (CT) character of the exciplexes (88-97%

100 excited MOF (i.e., NU-1000*) to TPPZn and a charge transfer (CT) from excited porphyrin (i.e., TPPZn

101 tance between nucleobases, so that a similar charge transfer (CT) mechanism governs the photophysics

102 the HE states, and the other concerned with charge transfer (CT) to the adsorbate antibonding sigma*

103 empts on the theoretical description of this charge transfer (CT)-IT system have considered the Nerns

104 o identify a precursor electronic state with charge-transfer (CT) character that precedes polaron for

105 between the lowest excited state, which has charge-transfer (CT) character, and the ground state.

106 Six new binary charge-transfer (CT) cocrystals have been synthesized by

107 Herein, we report the creation of a charge-transfer (CT) fluorophore and the discovery that

108 in-filtering effect during an intramolecular charge-transfer (CT) process.

109 ic solar cells, this involves intermolecular charge-transfer (CT) states whose energies set the maxim

110 suffer typically from femtosecond timescale charge-transfer (CT)-state quenching by low-lying nonrea

111 [M(pdms)(2) ] (M=Co, Zn) allow for multiple charge transfers (CTs) between the SIM donor [M(pdms)(2)

112 ganization energy, an important parameter in charge transfer, decreases as n is increased.

113 igh optical activity study reveals important charge-transfer differences within the aromatic oligomer

114 let transitions consistently showing shorter charge transfer distances.

115 nsfer with an electron acceptor/donor (i.e., charge transfer doping) or through introduction of defec

116 ing strategies, including heteroatom doping, charge-transfer doping, and defective doping, have now b

117 he Bingel reaction leads to the formation of charge-transfer dyads, which can operate in organic phot

118 The design of these intramolecular charge-transfer dyes is based on the concept of spirocon

119 zing Marcus theory framework, we explain why charge-transfer-dynamic modulations can only be unveiled

120 engineered to optically trigger photoinduced charge-transfer-dynamic modulations in the solid state.

121 ake advantage of optical fields for tuneable charge-transfer-dynamic remote actuators, opens the path

122 nd recombination dynamics, along with linear charge-transfer-dynamic variations with the optical-fiel

123 ant NP-assembled electrodes through improved charge transfer efficiency.

124 y (DeltaE(ox) ~ 200 mV) and by Inter-Valence Charge Transfer electronic excitations in the near IR.

125 he ability to switch between extremes of the charge transfer energy continuum is without precedent in

126 rd metallization despite the seemingly large charge-transfer energy scale.

127 hibit panchromatic absorption and nanosecond charge-transfer excited state lifetimes, enabled by the

128 inium iodide, provides an early outer-sphere charge-transfer excited state that reports on solvent po

129 Long-lived charge-transfer excited states that undergo redox reacti

130 sky-blue to deep-blue photoluminescence from charge-transfer excited states.

131 sphere, halide-to-metal, and metal-to-ligand charge-transfer excited states.

132 ter is dominated by the coupling between the charge-transfer exciton at 1.96 eV and a longitudinal op

133 The dimer N levels include local and charge transfer excitons within each dimer.

134 Charge-transfer excitons (CTEs) immensely enrich propert

135 ent Ir-B bonding and weak ionic bonding with charge transfer from B(3) to Ir, and can be viewed as an

136 s strongly correlated with the extent of the charge transfer from the alkene (hydrogen acceptor) to t

137 The reaction proceeds via intramolecular charge transfer from the donor to acceptor, thereby enha

138 optimal driving force, the rate constant for charge transfer from the triplet state is surprisingly s

139 tron, proton, and ion transfer in biological charge transfer have focused primarily on the nano- and

140 ultaneously investigated at the prototypical charge-transfer heterointerface, LaAlO(3) /SrTiO(3) .

141 The proposed model confirms the gating charge transfer hypothesis with the movement of the S4 s

142 digo 6 and 7 exhibit a strong intramolecular charge transfer (ICT) absorption band in the near IR reg

143 ai* transitions are dominant, intramolecular charge transfer (ICT) also contributes in the excited st

144 Here, we report an intramolecular charge transfer (ICT) dye, DMNDC, as an alternative to t

145 for their ability to act as modular internal charge transfer (ICT) fluorescent probes or donor/accept

146 d electron transfer (PET) and intramolecular charge transfer (ICT) properties.

147 cence lifetime, and effective intramolecular charge transfer (ICT) properties.

148 ligand charge transfer (MLCT) to interligand charge transfer (ICT) with increasing electron-donating

149 ed that the polymer undergoes intramolecular charge transfer (ICT).

150 substitution, they feature an intramolecular charge-transfer (ICT) character in the excited state.

151 he photophysical data and the intramolecular charge-transfer (ICT) processes of the synthesized dyes.

152 mainly attributable to the enhanced mass and charge transfer imparted by nano- and micro-confinement

153 Leveraging spin-dependent charge transfer in the device, we demonstrate spin selec

154 vely low polarity solvents result in partial charge transfer in the host donor-guest acceptor complex

155 Markedly, evidence of the charge transfer in the hybrid material was demonstrated

156 Its application to the antiferromagnetic charge transfer insulator YBa(2)Cu(3)O(6.1) revealed rap

157 ies were no longer coupled via a covalent or charge transfer interaction as in typical DSORs.

158 PT) was used as a guest to study host-guest, charge transfer interaction with CB[7,8] in water.

159 chemiresistive response of the MOFs involves charge transfer interactions triggered by the analytes a

160 include hydrogen bonding, pai-pai stacking, charge transfer interactions, electrostatic interactions

161 Due to very small charge transfer interactions, He gas adsorption saturate

162 Benefiting from intermolecular charge transfer interactions, the two co-crystals posses

163 ct correlation can be attributed to enhanced charge-transfer interactions at host/dopant interface wi

164 rption, charge separation and transport, and charge transfer is a key challenge, which has attracted

165 y under oxygen ambient, ionic and electronic charge transfer is deconvoluted in response to the oxyge

166 ects could play an explicit role even if the charge transfer is inhibited(8).

167 Photoinduced charge-transfer is an important process in nature and te

168 extending the IDT core to promote interchain charge transfer, is a logical strategy toward high-mobil

169 separation of electrons and holes with high charge transfer kinetics.

170 Furthermore, received wisdom suggests slower charge-transfer kinetics for semiconductors than for met

171 described a systematic analysis to separate charge-transfer kinetics from diode effects and interact

172 Our results show that both ligand-to-metal charge transfer (LMCT) and photogenerated superoxide (O(

173 nding of excited states with ligand-to-metal charge transfer (LMCT) character is paramount to account

174 -on" of aurophilicity, where ligand to metal charge transfer (LMCT) induces the aurophilic bonding.

175 apid charge separation by a cascade Z-scheme charge transfer mechanism formed by the dimension-matche

176 r other metal ions which was attributed to a charge transfer mechanism.

177 ve site tyrosine is part of a "hole-hopping" charge-transfer mechanism formed of a pathway of conserv

178 istics of CPs, including bio-electrochemical charge-transfer mechanisms, and contrast them with natur

179 g and thereby contributes to the lowering of charge-transfer-mediated coupling even at shorter interc

180 ligible long-range Coulombic and short-range charge-transfer-mediated couplings in the null aggregate

181 The metal-to-ligand charge transfer (MLCT) excited states of Ru polypyridyl

182 ifetimes of the redox-active metal-to-ligand charge transfer (MLCT) excited states typically encounte

183 deactivation of the initial metal-to-ligand charge transfer (MLCT) state to low-lying (d,d) states l

184 omputationally assigned as a metal-to-ligand charge transfer (MLCT) state with an energy of 1.6 eV (3

185 lexes changes character from metal-to-ligand charge transfer (MLCT) to interligand charge transfer (I

186 Direct singlet-to-triplet metal-to-ligand charge transfer (MLCT) transitions are evident in the 55

187 oexcitation by the virtue of metal-to-ligand charge transfer (MLCT), and subsequent redox trans-metal

188 lived electronically excited metal-to-ligand charge-transfer (MLCT) states, but these species suffer

189 ard electronegative O atoms in the intuitive charge-transfer model.

190 attribute this to spin-dependent interlayer charge transfer occurring on timescales between the exci

191 anism with increasing bias, and photoinduced charge transfer occurs at femtosecond timescale (~50 fs)

192 Charge transfer occurs between microbial cells and the M

193 Intervalence charge transfer occurs between the Rh centers, as eviden

194 easurements indicate that the intermolecular charge-transfer occurs with forming electric dipoles (D(

195 st plot provides an insight into the rate of charge transfer on the electrode/electrolyte interface.

196 alloys, which was attributed to the ease of charge transfer on the surface.

197 f their 2H phase via external means, such as charge transfer or high electric field, allows the conve

198 four-coordinated nickel atom is able to form charge-transfer orbitals through delocalization of elect

199 By application of the charge-transfer paradigm, it is shown that the emergence

200 (<=-0.3V) exhibited slower growth but higher charge transfer parameters.

201 from the perspective of various interfacial charge-transfer phenomena and reaction mechanisms.

202 of the electronic and ionic roles regarding charge-transfer phenomena poses a central challenge.

203 The ultrafast charge transfer probed at high electron donor concentrat

204 e forward reaction and catalyzed by a single charge-transfer process for the reverse switching.

205 ent absorption spectroscopy indicates a fast charge-transfer process within 20 ps of photoexcitation.

206 f the fundamental properties, especially the charge-transfer process, electron-phonon interactions, a

207 f particular importance when the bimolecular charge transfer processes are not limited by the intrins

208 Ultrafast charge transfer processes in polymer/fullerene blends ha

209 In this work, the energy and charge transfer processes in PSI complexes isolated from

210 ode) works in self-powered mode and triggers charge transfer processes in the second ("sensing") bipo

211 Photoinduced bimolecular charge transfer processes involving the iron(III) N-hete

212 process expands the current perspectives of charge-transfer processes and will inspire future applic

213 deeper understanding of homoconjugation and charge-transfer processes of triptycenes.

214 dge of the working principle of such coupled charge-transfer processes remains, however, fragmentary

215 eened dipole interactions and suppression of charge-transfer processes.

216 ical properties with enhanced chemical-based charge-transfer processes.

217 provement in Au nanoparticle and interfacial charge transfer promotion at the TiO(2)/substrate interf

218 ndicate enhanced surface coverage and better charge transfer properties of the proposed electrochemic

219 ogy, oxidation states, functional groups and charge transfer property of POC/MWCNTs electrode, the re

220 The intermolecular charge transfer property of PT-TPA forms a stabilized re

221 potential, E(0), the standard heterogeneous charge transfer rate constant, k(0), and the charge tran

222 ce can be minimized without jeopardizing the charge-transfer rate and without concerns about a curren

223 The first studies towards estimation of charge transfer rates as a function of acceptor stacking

224 n transport and determines the heterogeneous charge transfer rates by controlling the nature and degr

225 Here, we disentangle the intrinsic charge-transfer rates from morphology-dependent exciton

226 n sheath promote their intermolecular proton/charge transfer reactions, which dictates the properties

227 tion and the factors that control asymmetric charge transfer remaining under investigation.

228 e higher surface area (97.895 m(2)/g), lower charge transfer resistance (16.2 kOmega) for the ZCNT 0.

229 dies observed that L-MT sample performed low charge transfer resistance (336.7 Omega cm(2)) that prom

230 tion principle was based on the variation of charge transfer resistance (DeltaR(ct)) relative to the

231 A detailed impedimetric analysis shows low charge transfer resistance (R(CT)) and solution resistan

232 tion on the biosensor but also decreases the charge transfer resistance (R(ct)) of the screen-printed

233 y UV-A radiation by following the changes in charge transfer resistance (R(ct)).

234 cific surface area, which contributed to low charge transfer resistance and high transduction activit

235 y towards the reduction of triiodide and low charge transfer resistance at the electrode-electrolyte

236 s prepared on polyolefin films exhibit a low charge transfer resistance of about 20 Omega, high sensi

237 ites show almost an order-of-magnitude lower charge transfer resistance than CPE-K alone, supporting

238 The estimated charge transfer resistance value of 300 Omega cm(2) obta

239 hage on the cytosensor surface increased the charge transfer resistance, enabling detection of colifo

240 SA to the second one leads to changes in the charge transfer resistance, which correlate to the amoun

241 The Tafel plots indicate remarkably low charge transfer resistance-Tafel slopes of 35 and 38 mV

242 ifferent RBP4 concentrations plotted against charge transfer resistance.

243 surface area, lower particle size and lower charge transfer resistance.

244 cuit elements of solution resistance (R(s)), charge-transfer resistance (R(ct)), double-layer capacit

245 ls present in water samples by measuring the charge-transfer resistance changes of the electrode with

246 ter that is altered by target binding is the charge-transfer resistance.

247 ation-controlled nanosheets to possess lower charge-transfer resistances, leading to more complete ph

248 ncement (~10(6)) due to its strong broadband charge-transfer resonance, but also extraordinarily high

249 rption spectroscopy reveal symmetry-breaking charge transfer/separation and recombination dynamics wi

250 A charge transfer signal revealed an intriguing interplay

251 at the formation of a twisted intramolecular charge-transfer species enables the population of higher

252 etracyanobutadiene (TPA-TCBD), a high-energy charge-transfer species, are linked to a near-IR sensiti

253 s mobility correlates with the presence of a charge transfer state, while their ratio is a function o

254 xing between its singlet excited state and a charge transfer state, yielding an excimer-like state, w

255 Specifically, an underlying zwitterionic charge-transfer state is required to explain its sensiti

256 This strongly affects the charge-transfer state of the compound as well as its pol

257 d also be mediated by a high-energy, virtual charge-transfer state.

258 re a match for previously identified exciton-charge transfer states (Chl(D1) (+)Phe(D1) (-))* and (P(

259 its enhanced catalytic activity arising from charge transfer states (CTSs) between its two chromophor

260 Remarkably, no low-energy charge transfer states are located within the "special p

261 ility enables direct excitation of low-lying charge transfer states by far-red light.

262 ates from reduced recombination of localized charge transfer states.

263 terplay between emissive singlet and triplet charge-transfer states and amide-localized triplet state

264 lectron-hole encounters at later times, both charge-transfer states and emissive excitons are regener

265 setting up an equilibrium between excitons, charge-transfer states and free charges.

266 promotes the formation of hybridised exciton/charge-transfer states at the interface, dissociating ef

267 he formation of long-lived and disorder-free charge-transfer states in these systems enables them to

268 xes, the SOC generated by the intermolecular charge-transfer states shows large and small values (ref

269 rmally activated dissociation of interfacial charge-transfer states that occurs over hundreds of pico

270 apsulating "arms" results in the creation of charge-transfer states which modify the excited state pr

271 ime, we confirm the presence of two adjacent charge-transfer states, a C(60)-ZnP(*-)-Fc(*+) intermedi

272 Intramolecular charge-transfer states, involving hemiquinhydrones are p

273 separating the critical bond activation and charge transfer steps of electrocatalysis.

274 del with well-known rate expressions for the charge-transfer steps in the pathways.

275 We describe herein a novel charge transfer system designed with BiVO(4) as a protot

276 mplications for the design of more effective charge-transfer systems.

277 otein matrix renders the Chl(D1) -> Pheo(D1) charge-transfer the lowest energy excitation globally wi

278 absorption, ideal morphology, and efficient charge transfer, the devices based on the PBDB-T-F/Y1-4F

279 The few available data report on charge transfer through RNA duplex structures mainly com

280 ere demonstrate distance-dependent reductive charge transfer through RNA duplexes and through the non

281 el, which is slow to form, to allow a larger charge transfer through the open channel that closes mor

282 MABN forms an excited twisted intramolecular charge-transfer (TICT) state that emits with a distincti

283 Distinct from twisted intramolecular charge-transfer (TICT) states, experiment-supported dens

284 We demonstrate that charge-transfer timescales remain at a few hundred femto

285 ine both rapid reductive quenching and rapid charge transfer to a metal-based cocatalyst.

286 In contrast, charge transfer to naphthalene is energetically unfavour

287 in a more active conformation and amplifying charge transfer to result in a greater reduction in impe

288 well as the model complexes, is a result of charge transfer to the pyridyl groups, in contrast to th

289 olve RS(-) -> Fe-O(2)(*-) and O(2)(*-) -> Fe charge transfer transitions.

290 They dictate the charge transfer/transport from the perovskite layer to t

291 clean interfaces with minimum losses during charge transfer/transport.

292 interfaces to ensure enhanced photoactivated charge transfer under visible light.

293 sed, the latter originating from chromophore charge transfer upon excitation.

294 (OAc)(4) (1) undergoes metal-metal to ligand charge transfer upon visible light irradiation, which is

295 Cascade charge transfer was realized by a H-bond linked zinc pht

296 gh KO CFs evoked larger amplitude EPSCs, the charge transfer was the same as wild-type as a result of

297 ecular orbital distributions for facilitated charge transfer, which make 2D CCP-Th a promising candid

298 charge modulation can be achieved via direct charge transfer with an electron acceptor/donor (i.e., c

299 ive to their propensity for complexation and charge transfer with Fe(3+).

300 involve ligand-to-metal and metal-to-ligand charge transfer with intermediate structural reconfigura

301 is this that drives the subsequent Fe-to-Co charge-transfer within ~200 fs.