ライフサイエンスコーパス: Overhauser

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

19 76-92 display negative 1H-15N heteronuclear Overhauser enhancements showing they are flexible.

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

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

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

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

24 A large Overhauser coupling between the electron spin accumulati

25 Nuclear Overhauser effect (NOE) spectroscopy experiments and ana

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

27 Nuclear Overhauser effect analysis, fluorescence spectroscopy, a

28 Nuclear Overhauser effect crosspeak intensity provided interprot

29 Nuclear Overhauser effect measurements and computational results

30 Nuclear Overhauser effect spectroscopy (NOESY) experiments have

31 Nuclear Overhauser effect spectroscopy allowed for the derivatio

32 Nuclear Overhauser effect spectroscopy and molecular modeling su

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

34 Nuclear Overhauser effect spectroscopy revealed a number of inte

35 Nuclear Overhauser effects arising from the interactions of spin

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

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

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

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

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

41 on mark1H inverted question mark-15N nuclear Overhauser effects were measured for the backbone amide

42 19F nuclear Overhauser effects (NOEs) between fluorine labels on the

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

64 heir relaxation, dipolar shifts, and nuclear Overhauser effects to adjacent residues used to place th

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

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

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

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

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

70 been determined using time-averaged nuclear Overhauser effects.

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

87 Homonuclear two-dimensional nuclear Overhauser effect spectroscopy and double quantum-filter

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

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

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

91 dynamics using interproton distance (nuclear Overhauser enhancement) and furanose ring torsion angle

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

107 er distance constraints derived from nuclear Overhauser effects (NOE) and 314 dihedral angle constrai

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

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

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

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

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

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

114 Large variations in the (15)N-(1)H nuclear Overhauser effects for individual amino acids correlate

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

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

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

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

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

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

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

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

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

124 spersion, and negative heteronuclear nuclear Overhauser effects.

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

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

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

128 OE patterns and 1H-15N heteronuclear nuclear Overhauser enhancements suggest that this region of the

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

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

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

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

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

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

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

136 Strong and positive intermolecular nuclear Overhauser effect (NOE) cross-peaks define a specific co

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

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

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

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

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

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

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

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

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

146 as defined through 37 intermolecular nuclear Overhauser effects.

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

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

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

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

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

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

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

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

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

156 itate assignment of the intersubunit nuclear Overhauser effect interactions.

157 ed through inter- and intramolecular nuclear Overhauser enhancements.

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

159 Intraresidue nuclear Overhauser effect spectroscopy cross peaks were observed

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

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

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

163 stion mark-HN inverted question mark nuclear Overhauser effect (NOE) values of vMIP-II, determined th

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

187 distance restraints derived from NMR nuclear Overhauser enhancements (NOE) were incorporated in the r

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

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

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

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

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

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

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

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

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

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

198 nd were confirmed by measurements of nuclear Overhauser effects.

199 Measurement of nuclear Overhauser enhancement spectroscopy cross-relaxation rat

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

217 (1)H correlation and (15)N-separated nuclear Overhauser effect (NOE) spectroscopy experiments were us

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

235 p inverse distance dependence of the nuclear Overhauser effect (NOE), from which the distance constra

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

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

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

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

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

241 ization between these nuclei via the nuclear Overhauser effect.

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

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

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

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

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

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

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

249 ous work, we found using transferred nuclear Overhauser effect (trNOE) analysis that two 13 amino aci

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

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

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

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

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

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

256 itative information from transferred nuclear Overhauser effect experiments.

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

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

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

260 ave used two-dimensional transferred nuclear Overhauser effect spectroscopy to determine the conforma

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

262 he recombinant ECD using transferred nuclear Overhauser effect spectroscopy.

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

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

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

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

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

268 Here, we used transferred nuclear Overhauser effects to study the interaction in solution

269 sequential and mid-range transferred nuclear Overhauser effects.

270 Transferred nuclear Overhauser enhancement spectroscopy was used to determin

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

272 etermined using exchange-transferred nuclear Overhauser NMR spectroscopy.

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

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

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