ライフサイエンスコーパス: hyperfine

1 bserved for the N-O...H-C interaction (13CH3 hyperfine, a/h=0.66 MHz) in the CH3CN/TEMPO system, wher

2 5)N(-)) and extracted accurate values of the hyperfine and quadrupole couplings of both CN(-) and adt

3 unlabeled forms of the hydrazido ligand, the hyperfine and quadrupole parameters of the -N-NH2 moiety

4 Hyperfine and quadrupole tensors are obtained by pulsed

5 spectroscopy, including relaxation-filtered hyperfine and single-matched resonance transfer (SMART)

6 The larger isotropic NO hyperfine and the smaller maximal g-value of the R127A m

7 nced by a reorientation of its unique (55)Mn hyperfine axis.

8 In the current study, hyperfine broadening of the homogeneous S = 3/2 EPR spec

9 We have compared these assignments with hyperfine chemical shifts calculated from available X-ra

10 hown to be fast on the time scale of the 14N hyperfine clock ( approximately 220 ns), remains fast on

11 ), remains fast on the time scale of the 13C hyperfine clock ( approximately 50 ns).

12 The (203)Tl/(205)Tl hyperfine clock strategy is applied to a series of seven

13 Herein, the hyperfine-clock strategy is applied to dyads of dihydrop

14 ific (13)C-labels, which serve as additional hyperfine clocks.

15 ein, it is demonstrated that (203)Tl/(205)Tl hyperfine "clocks" are greatly superior to those provide

16 osition, wherein (1)H and (14)N serve as the hyperfine "clocks", and in arrays containing site-specif

17 The isotropic hyperfine constant (((17)O)A(iso) = -16.8 MHz) was deriv

18 rly equal population, one nearly axial, with hyperfine constant A parallel = 98 x 10(-4) cm(-1), and

19 experiments allowed the determination of the hyperfine constants ((17)O)A(z) = 10 MHz for [Fe(IV)H(3)

20 brid DFT calculations providing the separate hyperfine contributions of all distinct Mn-O-P and Fe-O-

21 in-orbit mechanism that is usually masked by hyperfine contributions.

22 14N ESEEM from a hyperfine-coupled protein nitrogen in wild type is absen

23 ver the whole chain on the time scale of the hyperfine coupling (ca. 100 ns).

24 The calculated 12.3-17.9 MHz (14)N hyperfine coupling (HFC) for the Fe4-bound Cys20 backbon

25 FT calculations demonstrate that the lithium hyperfine coupling A((7)Li) in [Li(+){(+/-)-1(*-)}] is v

26 Based on the anisotropy of the hyperfine coupling and of the optical polarization mecha

27 m which (17)O ENDOR showed a smaller 3.8 MHz hyperfine coupling and possible quadrupole splittings, i

28 using density functional theory of the (14)N hyperfine coupling and quadrupole coupling constants rep

29 relaxation and longitudinal DeltaHFC-Deltag (hyperfine coupling anisotropy--g-tensor anisotropy) cros

30 y large gzz value of 2.44 and a small copper hyperfine coupling Azz of 40 x 10(-4) cm(-1) (120 MHz).

31 gely a type 1 copper protein at low pH (with hyperfine coupling constant A( parallel) = 54 x 10(-4) c

32 rongly coupled nonexchangeable proton with a hyperfine coupling constant of 50 MHz.

33 isotropic signal with a g value of 2.003 and hyperfine coupling constant of 8 x 10(-4) cm(-1) to the

34 The hyperfine coupling constant of the g = 2 signal in the E

35 t polarity constant E(T)(N) and the nitrogen hyperfine coupling constant of the released nitroxide a(

36 Assuming a free-ion value for the Pu(4+) hyperfine coupling constant, we estimated a bare (239)ga

37 indicate that electron spin resonance (ESR) hyperfine coupling constants (aH values) computed at the

38 The hyperfine coupling constants (HFCs) determined from the

39 The (13)C hyperfine coupling constants also provide an independent

40 The hyperfine coupling constants and geometry of the NH(2) m

41 ons of molecular spin-orbitals (MSOs) to the hyperfine coupling constants and the spatial distributio

42 The hyperfine coupling constants are consistent with a struc

43 C isotope shifts in the IR spectra and (13)C hyperfine coupling constants in the EPR spectra exhibit

44 pectroscopy revealed a 9-line spectrum, with hyperfine coupling constants indicative of four almost m

45 n of the cluster is highly anisotropic, with hyperfine coupling constants of 9.1 and 2 x 33.3 G for t

46 stretching frequency and the imidazole (14)N hyperfine coupling constants show a good correlation wit

47 The Sc-based hyperfine structure with large hyperfine coupling constants shows that both oxidation a

48 Following DFT calculations, the predicted hyperfine coupling constants were used to simulate the E

49 in the ligand moiety and the (13)C isotropic hyperfine coupling constants, Aiso((13)C), for the indiv

50 agreement with the observed g values, ligand hyperfine coupling constants, and FTIR stretching freque

51 ance for predicting NMR chemical shifts, EPR hyperfine coupling constants, and low-energy transitions

52 ble-temperature magnetic susceptibility, EPR hyperfine coupling constants, and the results of X-ray c

53 et constraints on the relative amplitudes of hyperfine coupling constants, both for protons at chemic

54 ding affinity, perturb and diminish the 14NO hyperfine coupling determined by ENDOR (electron nuclear

55 In the substituted analogs, changes in hyperfine coupling due to altered metal-proton distances

56 The uniquely large isotropic hyperfine coupling for (13)C from CH(2)O led to the intr

57 ) substitution and that the isotropic (95)Mo hyperfine coupling in E(4) is a(iso) approximately 4 MHz

58 Thanks to the weak hyperfine coupling in silicon, a Ramsey decay timescale

59 Here we report the observation of a (57)Fe hyperfine coupling interaction with the paramagnetic sig

60 Furthermore, a single exchangeable proton hyperfine coupling is resolved, both by comparing the HY

61 rted again by EPR and ENDOR results (a (13)C hyperfine coupling of approximately 7 MHz), as well as l

62 The hyperfine coupling of other protein nitrogens with semiq

63 The hyperfine coupling of other protein nitrogens with the s

64 se EPR data reveal an exchangeable deuterium hyperfine coupling of strength |T| = 0.7 MHz, but no str

65 sotope incorporation and in the (17)O mu-oxo hyperfine coupling of the di-mu-oxo di-Mn(III,IV) bipyri

66 The characteristic hyperfine coupling of the I = (1/2) nucleus of Ag is evi

67 ng from a manifold of states produced by the hyperfine coupling of the S = (1/2) electron spin and I

68 ganic semiconductors have been attributed to hyperfine coupling of the spins of the charge carriers a

69 EPR spectroscopy on Li[1] reveals hyperfine coupling of the unpaired electron to two magne

70 uster exerts an appreciable electron nuclear hyperfine coupling on the charge transfer dynamics.

71 experiments showing the influence of nuclear hyperfine coupling on transport properties.

72 Hyperfine coupling parameters computed from DFT calculat

73 dues, enabled assignments based on predicted hyperfine coupling parameters.

74 n going from high pH to low pH, a seven-line hyperfine coupling pattern associated with complete delo

75 s recorded at 9 GHz (X-band) reveal distinct hyperfine coupling patterns for the two flavins.

76 These results show that the hyperfine coupling provides a sensitive probe of weak hy

77 measured across the EPR line shape, showed a hyperfine coupling range from 36 to 44 MHz for 14NO and

78 The proton hyperfine coupling that was significantly altered was co

79 The signal also exhibits hyperfine coupling to at least two solvent-exchangeable

80 ermediate with a g = 2 EPR signal that shows hyperfine coupling to both 55Mn and 57Fe accumulates alm

81 ic Cr(III), EPR (HYSCORE) spectroscopy shows hyperfine coupling to nitrogen only when the amide precu

82 amid relative to the other with strong super hyperfine coupling to one PMe3 and weak SHFC to the othe

83 by CO, with greater g anisotropy and larger hyperfine coupling to the active site (63,65)Cu.

84 tributed over the two iron atoms with strong hyperfine coupling to the bridging hydride (A(iso) = -75

85 ation, while the observation of an isotropic hyperfine coupling to the cation by ENDOR measurements e

86 Notably, the isotropic (1)H/(2)H hyperfine coupling to the diatomic of Co-H2 is nearly 4-

87 ce revealed further splitting into a pentet (hyperfine coupling to the four methine protons).

88 enters, as indicated by the magnitude of the hyperfine coupling to the phosphine ligands trans to the

89 intermediate having a g-value of 2.0025 with hyperfine coupling to two spin 1/2 nuclei, each with a s

90 ar characteristics, i.e. a large anisotropic hyperfine coupling together with an almost zero isotropi

91 tion and pi back-donation, whereas the (13)C hyperfine coupling was rationalized by incongruent alpha

92 lope modulations of the Mn(2+) signal due to hyperfine coupling with protons outside the quantum dots

93 howed a (17)O hyperfine signal with a 11 MHz hyperfine coupling, tentatively assigned as mu-oxo-(17)O

94 (17)O exchange was detected with a 13.0 MHz hyperfine coupling.

95 e enhanced relaxivity is a contribution from hyperfine coupling.

96 motion induced by isotropic and anisotropic hyperfine coupling.

97 d REcovery (PESTRE) protocol for determining hyperfine-coupling signs; and Raw-DATA (RD)-PESTRE, a PE

98 The observed (15)N (I = 1/2) hyperfine couplings (A) arise from two distinct classes

99 Analysis of NO and Cu hyperfine couplings and comparison to couplings of inorg

100 accessible spin states, and (55)Mn isotropic hyperfine couplings are computed with quantum chemical m

101 The (14)N hyperfine couplings are conclusive evidence that Fe(4) i

102 C owing to the fact that the (203)Tl/(205)Tl hyperfine couplings are much larger (15-25 G) than those

103 X-band HYSCORE spectroscopy shows two (14)N hyperfine couplings attributed to one conformer.

104 tions of these three substrates by measuring hyperfine couplings between substrate deuterium atoms an

105 The experimental hyperfine couplings between the electron and the H2 gues

106 n polarization pattern and pronounced methyl hyperfine couplings characteristic of asymmetric H-bondi

107 However, by calculating hyperfine couplings for both scenarios we show that wate

108 The experimentally observed hyperfine couplings for C2'* and C3'* match well with th

109 determination of the signed isotropic (57)Fe hyperfine couplings for five of the seven iron sites of

110 mplementary similarity between the isotropic hyperfine couplings for the bridging hydrides in 3 and E

111 ble information about (1)H, (15)N, and (13)C hyperfine couplings for the Q(H) site and to describe th

112 The hyperfine couplings from Nepsilon and Np demonstrate the

113 mponents from two anisotropic beta-2'-F-atom hyperfine couplings identify the C3'* formation in one-e

114 Analysis of the proton hyperfine couplings in linear oligomers with more than t

115 tem crossing driven by the greater number of hyperfine couplings in the assembly.

116 ith phylloquinone, but the absence of methyl hyperfine couplings in the quinone contribution to the P

117 or the study of the (13)C methyl and methoxy hyperfine couplings in the semiquinone generated in the

118 mparison between calculated and experimental hyperfine couplings is performed where good agreement is

119 Comparison of the large 14N hyperfine couplings measured here with that of a hydrazi

120 he TEMPO/CH3CONH2 system yield 13CH3 and 15N hyperfine couplings of a/h=0.16 and -0.50 MHz, respectiv

121 denced by (1)H, (2)H, and (13)C ENDOR, where hyperfine couplings of approximately 6 MHz for (13)C and

122 Hyperfine couplings of coordinating (17)O (I = 5/2) nucl

123 These hyperfine couplings reflect a distribution of the unpair

124 One of the two non-exchangeable proton hyperfine couplings resolved in hyperfine sublevel corre

125 parameter D were observed, while the proton hyperfine couplings show no change in the extent of trip

126 s employed to clearly discriminate the (17)O hyperfine couplings that overlap with (14)N (I = 1) sign

127 samples (35 GHz, 77 K) showed several H-bond hyperfine couplings that were similar to those for QB-*

128 Direct measurement of the hyperfine couplings through electron-nuclear double reso

129 nuclear double resonance data reveal similar hyperfine couplings to those of other Mn(IV) species, in

130 In contrast, one set of hyperfine couplings were not observed in the dark frozen

131 plitting parameter D and much smaller proton hyperfine couplings with respect to the monomeric unit,

132 In addition, weaker hyperfine couplings with the side-chain nitrogens from a

133 owed us for the first time to determine weak hyperfine couplings with the side-chain nitrogens from a

134 with auxotrophs was used to characterize the hyperfine couplings with the side-chain nitrogens from r

135 provide quantitative characteristics of the hyperfine couplings with these nitrogens, which can be u

136 Exchangeable proton/deuteron hyperfine couplings, consistent with terminal water liga

137 The proton and nitrogen hyperfine couplings, determined using electron nuclear d

138 tate delocalization can be obtained from the hyperfine couplings, while interpretation of the zero-fi

139 perimental data for (13)C and (17)O carbonyl hyperfine couplings.

140 nal theory calculated (14)N, (17)O, and (1)H hyperfine couplings.

141 he four nitrogen and 121 proton methyl group hyperfine couplings.

142 f zero-field splitting parameters and proton hyperfine couplings.

143 cated nuclear spins with particularly strong hyperfine couplings.

144 t of EPR parameters including (1)H and (31)P hyperfine couplings.

145 ctra with partially resolved lines caused by hyperfine couplings; the differences between the couplin

146 Here, we used hyperfine electron paramagnetic resonance (EPR) spectros

147 (85)Rb) according to the placement of their hyperfine energy states in a two-dimensional spectrum.

148 spin probe exhibits a splitting of the outer hyperfine extrema (2A'(zz)) significantly smaller than t

149 a high-field EPR spectrum with well-resolved hyperfine features devoid of zero-field splitting, chara

150 rise to characteristic (14)NO and (15)NO EPR hyperfine features indicating NO involvement, and enrich

151 nterstitial) can be assigned on the basis of hyperfine (Fermi contact) shifts and quadrupolar nutatio

152 these solutions which serves to modulate the hyperfine (Fermi-contact) interaction with nitrogen nucl

153 exhibits at 4.2 K a large, positive magnetic hyperfine field, Bint = +68.1 T, and an effective g valu

154 acteristics that affect the electron-nuclear hyperfine field, the metallic shift, and magnetic order.

155 netic moment and a remarkably large internal hyperfine field.

156 spin-singlet and spin-triplet states due to hyperfine fields is suppressed by microwave driving.

157 In previous studies, hyperfine ground states of single atoms or atomic ensemb

158 when the spin-orbit contribution exceeds the hyperfine, in agreement with a theoretical model.

159 nless nuclear, the materials have negligible hyperfine interaction (HFI) and the same intrinsic SOC,

160 Although the hyperfine interaction (HFI) has been foreseen to have an

161 To obtain information about the hyperfine interaction (hfi) of 33S with Mo(V), continuou

162 der a small magnetic field due to their weak hyperfine interaction and slight difference of g-factor

163 s of both the spin-orbit interaction and the hyperfine interaction are estimated.

164 However, this advantage is offset by the hyperfine interaction between the electron spin and the

165 n echo envelope modulation (ESEEM) from (2)H-hyperfine interaction with D2O is determined for stearic

166 MCR red2a state exhibits a very large proton hyperfine interaction with principal values A((1)H) = [-

167 he effective magnetic noise arising from the hyperfine interaction with uncontrolled nuclear spins in

168 C coupling as resulting from a "transannular hyperfine interaction".

169 ity in the 4f shell, manifest in the (171)Yb hyperfine interaction, and (iv) the principal values of

170 ulti-spin-qubit state under the influence of hyperfine interaction, and clearly demonstrate that the

171 r, as measured via the isotropic NN nitrogen hyperfine interaction, and the strength of the D --> A i

172 ho techniques have been used to mitigate the hyperfine interaction, but completely cancelling the eff

173 ted by the lattice nuclear spins through the hyperfine interaction, while the dynamics of the single

174 ative of poly(phenylene-vinylene) with small hyperfine interaction.

175 electronic qubit states through the contact hyperfine interaction.

176 peak is insensitive to cupric A(x) and A(y) hyperfine interaction.

177 field, demonstrating a negligible hole spin hyperfine interaction.

178 their locations through the electron-nuclear hyperfine interaction.

179 These signals are broadened significantly by hyperfine interactions (A((17)O) approximately 180 MHz).

180 ) 2.00592, and g(z) 2.00230 and with altered hyperfine interactions (apparent triplet collapsed to a

181 coordinates predict experimentally observed hyperfine interactions and a shift in g values away from

182 The hyperfine interactions associated with the (19)F nucleus

183 We investigate the effect of variations in hyperfine interactions between different copies of simpl

184 Moreover, (13)C hyperfine interactions between the radical and the methy

185 DFT analysis of the (57) Fe electric hyperfine interactions deduced from the Mossbauer analys

186 observe that the size of the spin-orbit and hyperfine interactions depends on the magnitude and dire

187 The ratio of the isotropic (13)C hyperfine interactions for the two CN(-) ligands-a repor

188 d samples, we have specifically assigned the hyperfine interactions in a reaction intermediate.

189 es of Hg lamp experiments is not a result of hyperfine interactions making predissociation of (17)O c

190 tetrapyrrolic arrays entails analysis of the hyperfine interactions observed in the electron paramagn

191 etrapyrrolic array relies on analysis of the hyperfine interactions observed in the EPR spectrum of t

192 The large (203)Tl/(205)Tl hyperfine interactions permit accurate simulations of th

193 ctron spins in these materials is limited by hyperfine interactions with nuclear spins.

194 omparison of the experimental (1)H and (17)O hyperfine interactions with those calculated using DFT h

195 -spin density at ligand nuclei (via the weak hyperfine interactions) in molecular thorium(III) and ur

196 e meso-13C label provides a "clock" (via the hyperfine interactions) that allows investigation of a t

197 To probe these protein-derived carboxylate hyperfine interactions, which give direct bonding inform

198 f (14)N, (11)B, and (10)B nuclear quadrupole hyperfine interactions.

199 tion being much stronger than the Zeeman and hyperfine interactions.

200 A significant scalar contact hyperfine is observed for the N-O...H-C interaction (13C

201 (14)N-hyperfine is observed on gz, confirming the addition of

202 These observations suggest that each pair of hyperfine levels hosted within [V(C8S8)3](2-) are candid

203 d by the EPR spectra, which exhibit multiple hyperfine lines due to the coupling of the unpaired elec

204 d (31)P (I = 1/2) nuclei leading to multiple hyperfine lines.

205 Moreover, GaAs hyperfine material constants are measured here experimen

206 nents prevent the specific identification of hyperfine molecular information of different substances,

207 l small paramagnetic complexes combine large hyperfine NMR shifts with large magnetic anisotropies.

208 ectronic structure driving the variations in hyperfine parameters across the range of materials.

209 itrite, and an analysis of the resulting EPR hyperfine parameters confirms that mARC is remarkably si

210 Mossbauer hyperfine parameters for Fe(II)-reacted NAu-1 at pH 7.5

211 upporting evidence for the assignment of the hyperfine parameters to Fe(II) bound to basal planes and

212 ive S = 1 signal at g = 4.01 with a six-line hyperfine pattern having A(z) = 113 MHz.

213 he low pH form and reveal that its four-line hyperfine pattern results from the large EPR spectral ef

214 Spectra exhibit distinct hyperfine patterns that clearly identify the DMPO(*)-OH

215 Here we show that the ground state hyperfine populations of bismuth can be read out using t

216 the observation of a signal with a large 7Li hyperfine shift in the 7Li MAS NMR spectrum.

217 The 1H NMR hyperfine shift pattern for the substrate and axial His

218 verhauser effect spectroscopy cross-peak and hyperfine shift patterns.

219 gned to LiMn6-TM(tet) sites, specifically, a hyperfine shift related to a small fraction of re-entran

220 e required to reproduce the experimental NMR hyperfine shift results, the best theory vs experiment p

221 Co(II)-Bc in DMSO shows relatively sharper hyperfine-shifted (1)H NMR signals compared with the spe

222 Previous analysis of the hyperfine-shifted (1)H NMR signals of Co(II)-Bc A(1) rev

223 o carry out comprehensive assignments of the hyperfine-shifted (13)C and (15)N signals of the rubredo

224 n as a quantum register and demonstrate that hyperfine-shifted resonances can be separated upon prope

225 DFT has been used to predict the NMR hyperfine shifts and electron paramagnetic resonance (EP

226 on the basis of the correlations between Li hyperfine shifts and Li local structures, and two differ

227 stal helices, together with the magnitude of hyperfine shifts and paramagnetic relaxation, establish

228 so find interesting correlations between the hyperfine shifts and the bond and ring critical point pr

229 as well as the mean low-field bias of methyl hyperfine shifts and their paramagnetic relaxivity relat

230 The axial His25 CbetaH hyperfine shifts are shown to serve as independent probe

231 olecules theory, in addition to finding that hyperfine shifts can be well-predicted by using an empir

232 is indicates that the pattern of heme methyl hyperfine shifts cannot be used alone to determine the i

233 st quantum chemical investigations of 1H NMR hyperfine shifts in the blue copper proteins (BCPs): ami

234 )C and (1)H nuclear magnetic resonance (NMR) hyperfine shifts of heme aided by density functional the

235 pretation of the pattern of substrate methyl hyperfine shifts, however, indicates substrate rotations

236 ents to provide both the H-bond strength and hyperfine shifts, the latter of which were used to quant

237 an individual AlGaAs/GaAs heterojunction via hyperfine shifts.

238 ltihour (17)O exchange, which showed a (17)O hyperfine signal with a 11 MHz hyperfine coupling, tenta

239 The hyperfine spectra of these spins are a unique chemical i

240 dipolar broadened), and a localized Mn site (hyperfine-split).

241 an S = (1)/(2) EPR signal exhibiting (59)Co hyperfine splitting (A = 24 G) typical of a low-spin Co(

242 siological range from 6 to 8, the phosphorus hyperfine splitting acting as a convenient and highly se

243 The nuclear hyperfine splitting between the C3 hydrogen and the unpa

244 Resolved 13C hyperfine splitting in EPR spectra of samples prepared w

245 The appearance of 59Co hyperfine splitting in the EPR signals and the positions

246 calculated from the orientational-dependent hyperfine splitting in the EPR spectra, and (3) EPR spec

247 nd at 427 nm and the typical nine line (14)N hyperfine splitting in the EPR spectrum.

248 susceptibility data and by the appearance of hyperfine splitting in the zero-field (5)(7)Fe Mossbauer

249 There is good agreement between the hyperfine splitting parameters obtained for BMPO-OOH by

250 a well-resolved (59)Co (I = 7/2) eight-line hyperfine splitting pattern.

251 orientation of the principal axes of the 13C hyperfine splitting tensor shows that the long axis of t

252 d exchange interactions as well as the 1-13C hyperfine splitting tensor were analyzed via spectral si

253 oublet radical signal with an 11 G principal hyperfine splitting was detected within the first millis

254 bismuth, has a large zero-field ground state hyperfine splitting, comparable to that of rubidium, upo

255 agnetic-field-independent measurement of the hyperfine splitting.

256 pling interaction of TN biradicals, their g, hyperfine-splitting, and zero-field-splitting interactio

257 e peptide can be easily calculated using the hyperfine splittings gleaned from the orientational depe

258 k absorption near 800 nm and narrow parallel hyperfine splittings in electron paramagnetic resonance

259 he so-called specific difference between the hyperfine splittings in hydrogen-like and lithium-like b

260 The g-values and 14N/15N-hyperfine splittings obtained from the spectra are consi

261 The corresponding EPR spectra revealed hyperfine splittings that were highly dependent on the m

262 equation was developed for relating nuclear hyperfine splittings to electron spin distributions in f

263 rong pH-induced changes to the corresponding hyperfine splittings, Delta hfs approximately (300-1000)

264 esults is the use of different pairs of 9Be+ hyperfine states for robust qubit storage, readout, and

265 uantum gas experiments, typically two atomic hyperfine states were chosen as pseudospins.

266 The 12 G wide radical has minimal hyperfine structure and can be fit using parameters uniq

267 The 46 G wide radical has extensive hyperfine structure and can be fit with parameters consi

268 ESR spectra of the ion radicals have a rich hyperfine structure caused by two pairs of equivalent Sc

269 The observation of hyperfine structure in atomic hydrogen by Rabi and co-wo

270 ve been developed that enable studies of the hyperfine structure of antihydrogen-the antimatter count

271 The Sc-based hyperfine structure with large hyperfine coupling consta

272 assign radical location on the basis of EPR hyperfine structure.

273 by ESR spectroscopy, revealing their (45)Sc hyperfine structure.

274 eable proton hyperfine couplings resolved in hyperfine sublevel correlation (HYSCORE) spectra of the

275 lectron-nuclear double resonance (ENDOR) and hyperfine sublevel correlation (HYSCORE) spectroscopies

276 on spin echo envelope modulation (ESEEM) and hyperfine sublevel correlation (HYSCORE) spectroscopy cl

277 Two-dimensional hyperfine sublevel correlation (HYSCORE) spectroscopy re

278 Here, we used hyperfine sublevel correlation (HYSCORE) spectroscopy, i

279 Using hyperfine sublevel correlation (HYSCORE) spectroscopy, w

280 n a bidentate fashion, which is confirmed by Hyperfine Sublevel Correlation (HYSCORE) spectroscopy.

281 ectron-nuclear double resonance (ENDOR), and hyperfine sublevel correlation (HYSCORE)) electron param

282 ve electron paramagnetic resonance (CW-EPR), hyperfine sublevel correlation (HYSCORE), and IR fingerp

283 UV-visible, electron paramagnetic resonance, hyperfine sublevel correlation (HYSCORE), and Mossbauer

284 Hyperfine sublevel correlation spectroscopy (HYSCORE) sp

285 We utilize high-resolution two-dimensional hyperfine sublevel correlation spectroscopy to directly

286 We apply the hyperfine sublevel correlation technique to quantify the

287 or ultracold atoms through the 'dressing' of hyperfine sublevels of the atomic ground state, where th

288 rincipal values and orientations of both the hyperfine tensor ((14)N, A(iso) = -6.25 MHz, T = -0.94 M

289 ear spin coupled to the FeMo cofactor with a hyperfine tensor A = [0.9, 1.4, 0.45] MHz establishing t

290 or two exchangeable protons with anisotropic hyperfine tensor components, T, both in the range 4.6-5.

291 ition, (19)F chemical shift measurements and hyperfine tensor measurements of biocatalyst formulation

292 bridge hyperfine tensor to the (14)N((15)N) hyperfine tensor of the D1-His332 ligand suggests that t

293 entation of the putative (17)O mu-oxo bridge hyperfine tensor to the (14)N((15)N) hyperfine tensor of

294 fferent spin density distributions and g and hyperfine tensors for different protonation states.

295 Analysis of the metal hyperfine tensors in combination with density functional

296 roscopy, the g tensor of the radical and the hyperfine tensors of several N and H nuclei in the radic

297 ata allow a detailed analysis of the dipolar hyperfine tensors of two of the four symmetry distinct p

298 is of the zero-field splittings and magnetic hyperfine tensors suggests that the dihedral O horizonta

299 tion of different factors to the anisotropic hyperfine tensors.

300 easurements were performed on a ground-state hyperfine transition of europium ion dopants in yttrium