ライフサイエンスコーパス: hyperfine

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

2 Hyperfine and quadrupole tensors are obtained by pulsed

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

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

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

6 ation (DNP) at or near room temperature, but hyperfine broadening, susceptibility to magnetic field h

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

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

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

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

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

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

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

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

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

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

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

18 14N ESEEM from a hyperfine-coupled protein nitrogen in wild type is absen

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

35 The hyperfine coupling constants are consistent with a struc

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

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

38 an S = 3 ground state with isotropic (55)Mn hyperfine coupling constants of -75, -88, -91, and 66 MH

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

40 A comparison of g tensors and (1)H hyperfine coupling constants of the PTB7-type oligomers

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

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

43 troxides which exhibit a change in their EPR hyperfine coupling constants upon enzymatic activity and

44 erved radicals, muon, proton, and phosphorus hyperfine coupling constants were determined by muSR and

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

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

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

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

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

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

51 py at X-band allowed the measurement of (1)H hyperfine coupling constants.

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

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

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

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

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

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

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

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

60 The hyperfine coupling of other protein nitrogens with the s

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

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

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

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

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

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

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

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

69 Hyperfine coupling parameters computed from DFT calculat

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

71 ination intensity, frequency sweep rate, and hyperfine coupling strength leads to efficient, sweep-di

72 The strong anisotropy of the hyperfine coupling tensor with the central carbon of a (

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

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

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

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

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

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

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

80 irectly sensitive to the order parameter via hyperfine coupling to the electronic spin degrees of fre

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

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

83 The hyperfine coupling to the terminal hydride ligand of the

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

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

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

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

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

89 motion induced by isotropic and anisotropic hyperfine coupling.

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

91 e enhanced relaxivity is a contribution from hyperfine coupling.

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

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

94 An unusual correlation of dispersion of hyperfine couplings and strength of the binding mode(s)

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

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

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

98 wed for the measurement of the corresponding hyperfine couplings associated with spin delocalization

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

116 These hyperfine couplings reflect a distribution of the unpair

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

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

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

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

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

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

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

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

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

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

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

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

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

130 cated nuclear spins with particularly strong hyperfine couplings.

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

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

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

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

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

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

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

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

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

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

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

142 reased sensitivity to certain changes in the hyperfine field direction compared to non-mixing transit

143 The local hyperfine field obtained by fitting is in excellent agre

144 The magnetic hyperfine field of [Dy(Cy(3) PO)(2) (H(2) O)(5) ]Br(3) .

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

146 netic moment and a remarkably large internal hyperfine field.

147 expected out-of-plane components of magnetic hyperfine fields and non-zero electric field gradients i

148 ng evidence that dynamical coupling with the hyperfine fields bring the electronic spins associated w

149 parameters within a working OLED: the local hyperfine fields for electron and hole in Alq(3): B(hf1)

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

151 However, since reducing hyperfine fields sharpens the Zeeman peak at the cost of

152 lay between the zero-field feature and local hyperfine fields.

153 The (1)H-hyperfine for (Ar)P(3)(B)Fe(NNH) derived from the presen

154 of molecules occupying their rotational and hyperfine ground state is best described by second-order

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

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

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

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

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

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

161 that the RISC process is not governed by the hyperfine interaction as thought previously, but proceed

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

163 n metal-oxide-semiconductor quantum dots the hyperfine interaction is sufficient to initialize, read

164 ENDOR protocol ("PESTRE") to obtain absolute hyperfine interaction signs.

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 nto magnetic fields via the electron-nuclear hyperfine interaction, which severely affects nuclear co

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

176 field, demonstrating a negligible hole spin hyperfine interaction.

177 electronic qubit states through the contact hyperfine interaction.

178 their locations through the electron-nuclear hyperfine interaction.

179 n additional broad signal with no resolvable hyperfine interaction.

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

181 ) 2.00592, and g(z) 2.00230 and with altered hyperfine interactions (apparent triplet collapsed to a

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

183 m indicate two species, one containing two N hyperfine interactions and an additional broad signal wi

184 Unfortunately, hyperfine interactions are typically too weak to address

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

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

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

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

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

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

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

192 ontext of a model that involves exchange and hyperfine interactions in the spin triplet exciplex.

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

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

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

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

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

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

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

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

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

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

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

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

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

206 alues for the polaron pair decay rate, local hyperfine magnetic field and triplet contribution to dis

207 for microscopic quantities such as the local hyperfine magnetic field, we have carried out actual fit

208 Moreover, GaAs hyperfine material constants are measured here experimen

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

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

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

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

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

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

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

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

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

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

219 as a highly compact g(z) area and small A(z) hyperfine principal value with g and A tensors that rese

220 tes, is well studied, but their influence on hyperfine quenching in a reactant molecule is not known.

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

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

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

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

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

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

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

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

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

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

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

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

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

234 s with large magnetic anisotropies and small hyperfine shifts, (7)Li shifts for typical LiFePO(4) mor

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

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

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

238 -fidelity single-shot optical readout of the hyperfine spin state of single (171)Yb(3+) ions coupled

239 ecules and atoms prepared in their stretched hyperfine spin states.

240 The transitions between the hyperfine split levels show an untypically high E2/M1 mu

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

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

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

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

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

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

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

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

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

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

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

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

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

256 ng an S = 1/2 signal with clearly observable hyperfine splittings originated from the coupling of the

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

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

259 d [Formula: see text] ion, controlled on its hyperfine state.

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

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

262 OH with Sr atoms leading to quenching of OH hyperfine states.

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

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

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

266 netic dipole and nuclear electric quadrupole hyperfine structure constants and level isotope shifts o

267 al and isotope shifts, while disagreement of hyperfine structure constants indicates an increased imp

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

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

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

271 er such phenomena persist in the presence of hyperfine structure, as exhibited by most quantum emitte

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

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

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

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

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

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

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

298 tion of different factors to the anisotropic hyperfine tensors.

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

300 rotational manifold(1), a few gigahertz for hyperfine transitions, a few terahertz for rotational tr