ライフサイエンスコーパス: Overhauser

1 2), and Pi using a single contrast agent and Overhauser-enhanced magnetic resonance imaging technique

2 r with electron spin-resonance lineshape and Overhauser dynamic nuclear polarization analysis to cons

3 : electron-spin echo envelope modulation and Overhauser dynamic nuclear polarization.

4 ed into heterogeneous regions of the PEM and Overhauser dynamic nuclear polarization relaxometry, thi

5 in B12 were studied using MD simulations and Overhauser DNP-enhanced NMR.

6 by using a hyperpolarized (1)H-MRI, known as Overhauser enhanced MRI (OMRI), and an oxygen-sensitive

7 ilic lipid vesicle surfaces were measured by Overhauser dynamic nuclear polarization (ODNP).

8 This structure, proposed by Overhauser in 1984, has been questioned repeatedly but h

9 rface, is analyzed by the recently developed Overhauser dynamic nuclear polarization (ODNP) technique

10 The emerging Overhauser effect dynamic nuclear polarization (ODNP) te

11 In this study, we employ Overhauser dynamic nuclear polarization (ODNP) to probe

12 n distances obtained from the rotating frame Overhauser effect spectroscopy (ROESY) NMR experiment, w

13 tion spectroscopy (TOCSY) and rotating frame Overhauser enhancement spectroscopy (ROESY) spectra of t

14 ward this end, we have used a rotating-frame Overhauser effect spectroscopy-type NMR pulse sequence w

15 Rotating-frame Overhauser effects were used to infer the site residency

16 etermined in solution by (1)H rotating-frame Overhauser enhancement spectroscopy experiments.

17 vely transferring the spin polarization from Overhauser dynamic nuclear polarization (ODNP)-enhanced

18 hydration water using an emerging tool, (1)H Overhauser dynamic nuclear polarization (ODNP)-enhanced

19 eta turn that, from a [1H]-15N heteronuclear Overhauser effect experiment, appears to enjoy substanti

20 relaxation rates and [1H]-15N heteronuclear Overhauser effects of the backbone amides of the free an

21 76-92 display negative 1H-15N heteronuclear Overhauser enhancements showing they are flexible.

22 ed NMR spectroscopy as well as heteronuclear Overhauser enhancement NMR spectroscopy.

23 verified by either (19)F-(1)H heteronuclear Overhauser spectroscopy (HOESY) or X-ray crystallography

24 Proton-nitrogen heteronuclear Overhauser enhancement measurements revealed that the ad

25 to each other as demonstrated by interligand Overhauser effects between ubiquinone-1 and DBMIB or 2-n

26 A large Overhauser coupling between the electron spin accumulati

27 Nuclear Overhauser effect (NOE) spectroscopy experiments and ana

28 Nuclear Overhauser effect (NOE) spectroscopy revealed a number o

29 Nuclear Overhauser effect analysis, fluorescence spectroscopy, a

30 Nuclear Overhauser effect crosspeak intensity provided interprot

31 Nuclear Overhauser effect measurements and computational results

32 Nuclear Overhauser effect spectroscopy (NOESY) experiments have

33 Nuclear Overhauser effect spectroscopy allowed for the derivatio

34 Nuclear Overhauser effect spectroscopy and molecular modeling su

35 Nuclear Overhauser effect spectroscopy experiments of the 13C-la

36 Nuclear Overhauser effect spectroscopy revealed a number of inte

37 Nuclear Overhauser effects arising from the interactions of spin

38 Nuclear Overhauser effects to urea for these segments are also c

39 Nuclear Overhauser enhancement (NOE) data indicate that, while F

40 Nuclear Overhauser enhancement cross-peaks between Co(NH(3))(6)(

41 me b5 were quantified using {1H}-15N nuclear Overhauser effect (nOe) measurements, which characterize

42 ion measurements as well as [1H]-15N nuclear Overhauser effects at 500 and 600 MHz.

43 19F nuclear Overhauser effects (NOEs) between fluorine labels on the

44 mics are primarily conducted with 1D nuclear Overhauser enhancement spectroscopy (NOESY) presat for w

45 nd angular restraints based on 1H-1H nuclear Overhauser effects (NOEs), hydrogen-bonding networks, 3J

46 ty complexes using (15)N R(1), R(2), nuclear Overhauser effect, and chemical-shift anisotropy dipolar

47 ithout an inhibitor is based on 2813 nuclear Overhauser effects (NOEs) and has an average RMSD to the

48 us their free components, whereas 2D nuclear Overhauser effect spectroscopy (NOESY) spectra suggest c

49 e tend to correlate together in a 2D nuclear Overhauser effect spectroscopy (NOESY) spectrum, thus op

50 In total, 3354 nuclear Overhauser effect-derived distance constraints, 240 dihe

51 d.) = 1.2 A] was determined from 475 nuclear Overhauser effect (NOE)-derived distance restrains, 20 r

52 man RBCC protein, MID1) based on 670 nuclear Overhauser effect (NOE)-derived distance restraints, 12

53 d hydroxyl group was assigned with a nuclear Overhauser correlated spectroscopy experiment (1 alpha-H

54 Using a nuclear Overhauser effect ratio strategy to define the alanine P

55 Rapid amide-amide nuclear Overhauser enhancement buildup points to a large alpha-h

56 Unwanted sample heating and nuclear Overhauser effect (NOE) enhancements are the two main dr

57 NMR chemical shifts and nuclear Overhauser effect (NOE) patterns of Ca(2+)-bound Frq1 we

58 el combination of chemical shift and nuclear Overhauser effect (NOE)-based methods.

59 ling constants, relaxation rates and nuclear Overhauser effect prediction applied to the three levels

60 Quantum mechanics calculations and nuclear Overhauser effect spectroscopy NMR studies suggest that

61 a, total correlated spectroscopy and nuclear Overhauser effect spectroscopy, show that the molecule e

62 roducts by X-ray crystallography and nuclear Overhauser effect spectroscopy.

63 Chemical shift indices and nuclear Overhauser effects (NOE) confirmed helices in the presen

64 Chemical shift indices (CSI) and nuclear Overhauser effects (NOE) with 600 MHz NMR and CD confirm

65 ings, isotropic chemical shifts, and nuclear Overhauser effects (NOEs)/rotational frame nuclear Overh

66 s [chemical shifts, J couplings, and nuclear Overhauser effects (NOEs)] are expected.

67 Chemical shifts and nuclear Overhauser effects are similar to those of native IGF-I.

68 R1, R2 and nuclear Overhauser enhancement (NOE) values are similar in Abeta

69 nuclear single quantum coherence and nuclear Overhauser enhancement spectroscopy spectra for the trik

70 Proton decoupling and nuclear Overhauser enhancement were used to improve the spectral

71 ational analysis from rotating angle nuclear Overhauser effect (ROESY) data.

72 on distance restraints also known as Nuclear Overhauser effects (NOEs).

73 based on 2778 unambiguously assigned nuclear Overhauser effect (NOE) connectivities, 297 ambiguous NO

74 been determined using time-averaged nuclear Overhauser effects.

75 of NMR chemical shifts and backbone nuclear Overhauser effect (NOE) connectivities showed that OspA[

76 Solution NMR-based nuclear Overhauser effect and scalar J-coupling constants can pr

77 esulting alkenes were established by nuclear Overhauser effect difference NMR spectroscopy.

78 age of the two is detected in NMR by nuclear Overhauser effect experiments.

79 all molecules in complex mixtures by nuclear Overhauser effect magnetization transfer.

80 pon Zn(2+) binding were supported by nuclear Overhauser effect spectrometry (NOESY) studies.

81 p to 19,000 M(-1)), and is shown--by nuclear Overhauser effect spectroscopy--to adopt the threading g

82 id group at position 4', as shown by nuclear Overhauser effect spectroscopy.

83 ent alignment media, supplemented by nuclear Overhauser enhancement data and torsion angle restraints

84 hatic resonances in [Ca(2+)](4)-CaM (nuclear Overhauser effect) and increases the Ca(2+) affinity of

85 n this procedure, the time-consuming nuclear Overhauser enhancement (NOE)-based sequential assignment

86 s), intensities of NOESY crosspeaks [nuclear Overhauser effects (NOEs)], and residual dipolar couplin

87 Two-dimensional nuclear Overhauser effect NMR spectra demonstrate that this atom

88 was assigned through two-dimensional nuclear Overhauser effect spectroscopic analysis coupled with co

89 in combination with two-dimensional nuclear Overhauser effect spectroscopy (NOESY) results, demonstr

90 tion of (1)H NMR and two-dimensional Nuclear Overhauser Effect Spectroscopy (NOESY) which revealed fu

91 mined by transferred two-dimensional nuclear Overhauser effect spectroscopy (TRNOESY) measurements an

92 Two-dimensional nuclear Overhauser effect spectroscopy suggests that the triple

93 cular dichroism, and two-dimensional nuclear Overhauser enhancement spectra conclusively proves that

94 -relaxation rates in two-dimensional nuclear Overhauser enhancement spectroscopy NMR experiments show

95 Many drug-DNA nuclear Overhauser enhancements (NOEs) in the minor groove are i

96 paramagnetic probes and protein-DPC nuclear Overhauser effects (NOEs), we define portions of the gro

97 Furthermore, (13)C-edited nuclear Overhauser effects establish transient formation of a na

98 tructures were calculated from exact nuclear Overhauser effect (eNOE).

99 ntegration of simulations with exact nuclear Overhauser enhancements data allowed us to characterize

100 e techniques using 1290 experimental nuclear Overhauser effect and dipolar coupling constraints ( app

101 rix analysis of sets of experimental nuclear Overhauser effect spectroscopy crosspeaks.

102 th minor conformation in (19)F-(19)F nuclear Overhauser effect (NOESY) spectra.

103 tored by two-dimensional (19)F-(19)F nuclear Overhauser effect, the distance between two phenylalanin

104 ) selective detection of (19)F-(19)F nuclear Overhauser effects in the Escherichia coli peptidyl-prol

105 NMR-filtered nuclear Overhauser effect studies confirmed these observations a

106 dispersion experiments, and filtered nuclear Overhauser effects suggest that CCL27 does not adopt a d

107 Two-dimensional rotating-frame nuclear Overhauser effect spectroscopy (2D ROESY) (1)H NMR analy

108 ation parameters, and rotating-frame nuclear Overhauser effect spectroscopy (ROESY) crosspeaks that c

109 troscopy (NOESY), and rotating frame nuclear Overhauser effect spectroscopy (ROESY) data were recorde

110 red spectroscopy, and rotating-frame nuclear Overhauser effect spectroscopy and high-resolution elect

111 user effects (NOEs)/rotational frame nuclear Overhauser effects (ROEs).

112 distinct structures are derived from nuclear Overhauser effect spectroscopic distance restraints coup

113 ing using structural restraints from nuclear Overhauser effect spectroscopy, and scalar and residual

114 Distances derived from nuclear Overhauser effects indicate that the three Ser residues

115 ranslational restraints derived from nuclear Overhauser enhancement data may be limited.

116 straints (1074) were determined from nuclear Overhauser enhancements and main-chain torsion-angle con

117 ion of the cations as extracted from nuclear Overhauser experiments is in line with the preferred con

118 Heteronuclear (15)N-(1)H nuclear Overhauser effect data showed that the non-helical N-ter

119 differences in homonuclear (1)H-(1)H nuclear Overhauser effects (NOEs) and heteronuclear (1)H-(15)N N

120 ntermolecular (1)H(19)F and (1)H(1)H nuclear Overhauser effects were used to explore interaction of s

121 ng (15)N-(13)C-labeled protein, (1)H nuclear Overhauser effects, and longitudinal relaxation data ide

122 these interactions through both (1)H nuclear Overhauser enhancement (NOE) and paramagnetic relaxation

123 ation rate (R(2)), and heteronuclear nuclear Overhauser effect (NOE) have been carried out at 11.7T a

124 axation rate (R2), and heteronuclear nuclear Overhauser effect (NOE)] measured at two temperatures (2

125 Heteronuclear nuclear Overhauser effect experiments show that the new linker r

126 attice, spin-spin, and heteronuclear nuclear Overhauser effect relaxation data for backbone amide (15

127 13)C T(1), T(1rho) and heteronuclear nuclear Overhauser effects (NOEs) for sugar and base nuclei, as

128 ady-state {(1)H}-(15)N heteronuclear nuclear Overhauser effects indicate that the protein's core is r

129 spersion, and negative heteronuclear nuclear Overhauser effects.

130 nd negative (1)H-(15)N heteronuclear nuclear Overhauser effects.

131 nfirmed by T1, T2, and heteronuclear nuclear Overhauser enhancement (NOE) measurements.

132 ion NMR experiments of heteronuclear nuclear Overhauser enhancement (NOE), spin-lattice (R(1)), and s

133 The PBEs, in combination with HN-HN nuclear Overhauser effects (NOEs) and chemical shift index (CSI)

134 (15)N-T(1), (15)N-T(2), (15)N-{(1)H} nuclear Overhauser effect, reduced spectral density, and general

135 n cross-peaks were well dispersed in nuclear Overhauser effect and heteronuclear single quantum coher

136 eling and NMR spectroscopy including nuclear Overhauser effects and residual dipolar coupling of a sa

137 lar to the spin-polarization induced nuclear Overhauser effect.

138 ANA to build a network of interchain nuclear Overhauser effect constraints that can be used to accura

139 on as evidenced by an intermolecular nuclear Overhauser effect (NOE) between each metallopeptide His

140 rane, as supported by intermolecular nuclear Overhauser effect cross-peaks between the peptide and sh

141 on the observation of intermolecular nuclear Overhauser effects (NOE) and their assignments, which ar

142 Intermolecular nuclear Overhauser effects (NOEs) between protein and water prov

143 hemical shifts and 24 intermolecular nuclear Overhauser effects (NOEs) identify the 5'-ApG and 5'-GpT

144 cal shift mapping and intermolecular nuclear Overhauser effects (NOEs) indicate the presence of at le

145 Intermolecular nuclear Overhauser effects have been used to investigate the int

146 zone derived from the intermolecular nuclear Overhauser effects is in agreement with recent biochemic

147 the talin rod and use intermolecular nuclear Overhauser effects to determine the structure of the com

148 itration calorimetry, intermolecular nuclear Overhauser effects, mutagenesis, and protection from par

149 as defined through 37 intermolecular nuclear Overhauser effects.

150 aling on the basis of intermolecular nuclear Overhauser enhancement data and residual dipolar couplin

151 translational (i.e., intermolecular nuclear Overhauser enhancement, NOE, data) and orientational (i.

152 generated a number of intermolecular nuclear Overhauser enhancements (NOEs) and chemical shift pertur

153 perimentally resolved intermolecular nuclear Overhauser enhancements (NOEs) are extremely weak; most

154 produced a number of intermolecular nuclear Overhauser enhancements (NOEs) to residues in TMs 6 and

155 resonance assignments, interpreting nuclear Overhauser effect (NOE) spectroscopy (NOESY) spectra, an

156 itrogens, and (1)H-(1)H interresidue nuclear Overhauser effects (NOEs) for the two mutants with those

157 A large number of interresidue Nuclear Overhauser enhancements (NOEs) augmented by stereospecif

158 e to a dense network of interresidue nuclear Overhauser enhancements.

159 itate assignment of the intersubunit nuclear Overhauser effect interactions.

160 tivity for observing the intraligand nuclear Overhauser effect (NOE).

161 ed through inter- and intramolecular nuclear Overhauser enhancements.

162 ential NMR assignments, intramonomer nuclear Overhauser effects, and circular dichroism spectra are c

163 Intraresidue nuclear Overhauser effect spectroscopy cross peaks were observed

164 gned intra-ligand and protein-ligand nuclear Overhauser effects (NOEs).

165 enhancement of multiple native-like nuclear Overhauser effects within the tethered protein.

166 he pattern of observed peptide-lipid nuclear Overhauser effects is consistent with a parallel orienta

167 and (1)H magic angle spinning (MAS) nuclear Overhauser effect spectroscopy (NOESY) techniques, we sh

168 roups that is based on methyl-methyl nuclear Overhauser effect spectroscopy (NOESY) peak lists.

169 l shifts and the pattern of midrange nuclear Overhauser effects (NOE).

170 has a high tolerance for misassigned nuclear Overhauser effect restraints, greatly simplifying NMR st

171 perturbation and the inter-molecular nuclear Overhauser effects to the RNA.

172 Multidimensional nuclear Overhauser effect spectra, X-filtered spectra and (3)J(H

173 s interpretation of multidimensional nuclear Overhauser spectra for high-resolution structure determi

174 m-range alphaN(i,i+2) of each mutant nuclear Overhauser enhancements were observed in the urea-unfold

175 Similar chemical shifts and (15)N nuclear Overhauser effect (NOE) patterns of the peptide in compl

176 Heteronuclear (1)H-(15)N nuclear Overhauser effect spectroscopy (NOESY) and heteronuclear

177 T(1), T(2), and (1)H/(15)N nuclear Overhauser effect values measured for the amide backbone

178 red by NMR experiments of (1)H-(15)N nuclear Overhauser effect, spin-lattice relaxation, and spin-spi

179 measurements as well as [(1)H]-(15)N nuclear Overhauser effects (NOE).

180 on data and steady-state (1)H- (15)N nuclear Overhauser effects were analyzed using model-free formal

181 elaxation times and the {(1)H}-(15)N nuclear Overhauser enhancement (nOe) of uniformly (15)N-enriched

182 Heteronuclear (1)H-(15)N nuclear Overhauser enhancement measurements revealed very limite

183 acterized using isotope-edited (15)N nuclear Overhauser enhancement spectroscopy heteronuclear single

184 C) domain (as probed by {(1)H}-(15)N nuclear Overhauser enhancements) is progressively less ordered.

185 one resonances and measure H(N)-H(N) nuclear Overhauser effects (NOEs).

186 ive-like partial core; no non-native nuclear Overhauser effects are observed.

187 ein from unassigned experimental NMR nuclear Overhauser effect (NOE) data only.

188 Experimental NMR nuclear Overhauser effect (NOE) measurements of an asymmetricall

189 ns in solution from experimental NMR nuclear Overhauser effect data only and with minimal assignments

190 reflected in optical spectra and NMR nuclear Overhauser effect spectroscopy cross-peak and hyperfine

191 distance restraints derived from NMR nuclear Overhauser enhancement (NOE) data to predict protein str

192 A combination of FT-IR, (1)H NMR, nuclear Overhauser effect (NOESY), and diffusion-ordered (DOSY)

193 ton of one of the G.A base-pairs, no nuclear Overhauser enhancement cross-peaks between the cobalt li

194 ipolar coupling and inter-domain NOE nuclear Overhauser effect data.

195 mations responsible for the observed nuclear Overhauser effects and inter-nuclear coupling.

196 these H3(+) resonance; and observed nuclear Overhauser effects consistent with Hoogsteen and Watson-

197 assigned through (a) measurement of nuclear Overhauser effect connectivities, (b) prediction of the

198 s method includes the acquisition of nuclear Overhauser effect spectroscopy one-dimensional and J-res

199 ucture as indicated by the number of nuclear Overhauser effects and is shown to play a critical role

200 assignments and detailed analysis of nuclear Overhauser effects permit the direct comparison of the f

201 The distance relation of nuclear Overhauser effects with a factor of r(-6) is employed to

202 nd were confirmed by measurements of nuclear Overhauser effects.

203 Measurement of nuclear Overhauser enhancement spectroscopy cross-relaxation rat

204 ess, structure calculations based on nuclear Overhauser effect spectroscopic data combined with (15)N

205 ucture of recombinant FH1-3 based on nuclear Overhauser effects and RDCs.

206 d tissue is enhanced by a (1)H-(31)P nuclear Overhauser effect (NOE).

207 mical shift trends and proton-proton nuclear Overhauser effect experiments.

208 shifts and 78 unambiguous long-range nuclear Overhauser effect (NOE) constraints.

209 ted peptide and by weak medium-range nuclear Overhauser effect contacts indicative of alpha-helical c

210 ty of both sequential and long-range nuclear Overhauser effects (NOEs) between backbone amide protons

211 First, short-range nuclear Overhauser effects are detected between the aromatic sid

212 lly inconsistent group of long range nuclear Overhauser effects suggest a close proximity of the heli

213 s fewer helix-related and long range nuclear Overhauser effects than does the d-Ser(B8) analog or nat

214 tra-chain H(N)-H(N) and medium-range nuclear Overhauser enhancements (NOEs).

215 Medium-range nuclear Overhauser enhancements were detected in segments corres

216 eteronuclear cross relaxation rates (nuclear Overhauser effect), suggesting that the 14-38 disulfide

217 Analysis of inter-residue nuclear Overhauser effects demonstrates that a native-like fold

218 ng range (|i - j| > or = 5 residues) nuclear Overhauser enhancement restraints were derived exclusive

219 d ligand-protein NOEs, respectively (nuclear Overhauser enhancements).

220 ions lead to attenuation of selected nuclear Overhauser enhancements and accelerated amide proton exc

221 rt these assignments with sequential nuclear Overhauser effect (NOE) information obtained from a two-

222 Sequential Nuclear Overhauser Effects and double-quantum-filtered correlati

223 riments (correlated chemical shifts, nuclear Overhauser effects, residual dipolar couplings) to predi

224 In contrast, no significant nuclear Overhauser enhancement signals arising from the C-ring,

225 The simulated nuclear Overhauser effect pair distances are in excellent agreem

226 experiments with the through-space (nuclear Overhauser enhancement spectroscopy, NOESY) experiment.

227 tal NMR chemical shifts, plus sparse nuclear Overhauser effect (NOE) data if available.

228 old could be determined using sparse nuclear Overhauser enhancement (NOE) distance restraints involvi

229 een obtained using NMR spectrometry, nuclear Overhauser effects, and density functional theory to det

230 elaxation data, T1, and steady-state nuclear Overhauser effect (NOE) obtained at two different magnet

231 ), T(2), T(1)(rho), and steady-state nuclear Overhauser effects were measured at 500 and 600 MHz.

232 Distance bounds, calculated from the nuclear Overhauser effect (NOE) crosspeak intensities via a comp

233 distance restraints derived from the nuclear Overhauser effect (NOE) data were used to calculate the

234 We also calculated the nuclear Overhauser effect (NOE) distances from the molecular dyn

235 The nuclear Overhauser effect (NOE) has long been used as a selectiv

236 different (1)H environments via the nuclear Overhauser effect (NOE) is included in the NMR pulse seq

237 istance restraints, analogous to the nuclear Overhauser effect (NOE) routinely used in solution NMR.

238 he resulting process is equal to the nuclear Overhauser effect (NOE) where typically continuous satur

239 The method is based on the nuclear Overhauser effect between bound anesthetic protons and a

240 he two domains is not defined by the nuclear Overhauser effect data.

241 on of conformational exchange to the nuclear Overhauser effect peak intensity, we applied inferential

242 nd guanine can be extracted from the nuclear Overhauser effect spectroscopy spectrum based on the clo

243 Contributions of the nuclear Overhauser effect to exchange rates measured with invers

244 ization between these nuclei via the nuclear Overhauser effect.

245 e was determined on the basis of the nuclear Overhauser effects (NOEs) and the hydrogen bond restrain

246 Analysis of the nuclear Overhauser enhancement (NOE) and the alphaH NMR chemical

247 ycogen and water protons through the nuclear Overhauser enhancement (NOE).

248 Moreover, the simulation of the nuclear Overhauser enhancement spectra suggests that it is most

249 ods, using a model-based approach to nuclear Overhauser enhancement spectroscopy peak assignment.

250 al correlation spectroscopy (TOCSY), nuclear Overhauser effect spectroscopy (NOESY), and rotating fra

251 R) experiments, and (5) NMR transfer nuclear Overhauser effect spectroscopy (NOESY) experiments that

252 Analysis by two-dimensional transfer nuclear Overhauser effect spectroscopy of the induced solution s

253 py experiments, inducing transferred nuclear Overhauser effect (trNOE) and saturation transfer differ

254 This transferred nuclear Overhauser effect (trNOE) disrupts the observed signal d

255 of G(t)alpha derived by transferred nuclear Overhauser effect (TrNOE) NMR.

256 mined by two-dimensional transferred nuclear Overhauser effect (TRNOESY) measurements combined with m

257 mined by two-dimensional transferred nuclear Overhauser effect (TRNOESY) measurements combined with m

258 deled using experimental transferred nuclear Overhauser effect data derived upon binding R*.

259 rmore, based on exchange-transferred nuclear Overhauser effect measurements, we established that MBM1

260 ed from a combination of transferred nuclear Overhauser effect NMR experiments and molecular dynamics

261 We used transferred nuclear Overhauser effect spectroscopy (TrNOESY), which can be u

262 recovery method, and the transferred nuclear Overhauser effect spectroscopy was used to study the bin

263 he recombinant ECD using transferred nuclear Overhauser effect spectroscopy.

264 ha(s), was determined by transferred nuclear Overhauser effect spectroscopy.

265 ding, as demonstrated by transferred nuclear Overhauser effect spectroscopy.

266 tide was determined from transferred nuclear Overhauser effects (trnOe) experiments to determine inte

267 surfaces are studied by transferred nuclear Overhauser effects (trNOEs) and saturation transfer diff

268 Traditionally, transferred nuclear Overhauser effects (trNOEs), measured from NMR spectra o

269 Transferred nuclear Overhauser enhancement spectroscopy was used to determin

270 Transferred nuclear Overhauser experiments revealed that the h-region and pa

271 etermined using exchange-transferred nuclear Overhauser NMR spectroscopy.

272 ion times made it impractical to use nuclear Overhauser effect (NOE) measurements for assignment purp

273 To this end, we have used nuclear Overhauser effect spectroscopy (NOESY)-based distance re

274 ion of intermolecular contacts using nuclear Overhauser effect (NOE) experiments; (iv) structure dete

275 A structure calculated by using nuclear Overhauser effect and other NMR constraints reveals that

276 The structure was refined using nuclear Overhauser effect and residual dipolar coupling data.

277 rmational ensemble obtained by using nuclear Overhauser effect data in structure calculations reveale

278 e verified by NMR spectroscopy using nuclear Overhauser effect methodology.

279 spholipid micelle interactions using nuclear Overhauser effect spectroscopy and showed that the micel

280 membrane proteins in nanodiscs using nuclear Overhauser enhancement spectroscopy (NOESY) spectroscopy

281 ritical internuclear distances using nuclear Overhauser enhancement spectroscopy.

282 This is accomplished by utilizing nuclear Overhauser effect spectroscopy (NOESY) at subzero temper

283 s simulations were in agreement with nuclear Overhauser cross-peak intensities.

284 l membrane proteins >15 kDa in size, Nuclear-Overhauser effect-derived distance restraints are diffic

285 e width of 2.1 G allowing for an increase of Overhauser enhancements and reduction in rf power deposi

286 Water was hyperpolarized by means of Overhauser DNP in the 0.35-T fringe field of a 1.5-T MR

287 The methodology is based on Overhauser enhanced magnetic resonance imaging (OMRI), a

288 le-temperature NMR studies and 2D rotational Overhauser effect spectroscopy NMR experiments have show

289 couplings, (15)N chemical shifts, rotational Overhauser effects, and residual dipolar couplings were

290 provided by the site-specific and selective Overhauser dynamic nuclear polarization of solvent molec

291 Here we report solid-state Overhauser effect DNP enhancements of over 100 at 18.8 T

292 Our results demonstrate that Overhauser DNP at high field provides efficient polariza

293 sample, the spin noise spectrum revealed the Overhauser field created by optically oriented nuclei an

294 Here, we demonstrate that the Overhauser effect, a proton-electron polarization transf

295 l by up to 2 orders of magnitude through the Overhauser effect under ambient conditions at 0.35 tesla

296 conditions can be achieved by utilizing the Overhauser effect.

297 continuous in situ hyperpolarization via the Overhauser mechanism, in combination with the excellent

298 ethod to obtain local water dynamics through Overhauser dynamic nuclear polarization (DNP).

299 Using Overhauser dynamic nuclear polarization relaxometry, we

300 led SOS-NMR for structural information using Overhauser effects and selective labeling and is validat