ライフサイエンスコーパス: nuclear Overhauser effect

1 of polarization between these nuclei via the nuclear Overhauser effect.

2 en determined using the exchange-transferred nuclear Overhauser effect.

3 ner similar to the spin-polarization induced nuclear Overhauser effect.

4 GCG) has been determined using time-averaged nuclear Overhauser effects.

5 shift dispersion, and negative heteronuclear nuclear Overhauser effects.

6 rsion, and negative (1)H-(15)N heteronuclear nuclear Overhauser effects.

7 eristic sequential and mid-range transferred nuclear Overhauser effects.

8 e relaxation rates and amide nitrogen-proton nuclear Overhauser effects.

9 nd tert-butyl groups was readily detected by nuclear Overhauser effects.

10 shifts and were confirmed by measurements of nuclear Overhauser effects.

11 pocket was defined through 37 intermolecular nuclear Overhauser effects.

12 relaxation times, T1 and T2, and the 1H-15N nuclear Overhauser effect (1H-15N NOE) indicates that mo

13 ls, was determined utilizing two-dimensional nuclear Overhauser effect (2D NOE) and double-quantum-fi

14 duplex have been made using two-dimensional nuclear Overhauser effect (2D NOE) spectra, at three dif

15 nothiazine and detection of isotope-filtered nuclear Overhauser effects allowed identification of dru

16 Nuclear Overhauser effect analysis, fluorescence spectro

17 resonance techniques using 1290 experimental nuclear Overhauser effect and dipolar coupling constrain

18 spectroscopy in D2O (NOESY (two-dimensional nuclear Overhauser effect and exchange spectroscopy) at

19 nd proton cross-peaks were well dispersed in nuclear Overhauser effect and heteronuclear single quant

20 A structure calculated by using nuclear Overhauser effect and other NMR constraints reve

21 The structure was refined using nuclear Overhauser effect and residual dipolar coupling

22 Solution NMR-based nuclear Overhauser effect and scalar J-coupling constant

23 nstraints based on the observed magnitude of nuclear Overhauser effects and 58 torsion angle restrain

24 Sequential Nuclear Overhauser Effects and double-quantum-filtered c

25 e conformations responsible for the observed nuclear Overhauser effects and inter-nuclear coupling.

26 ined structure as indicated by the number of nuclear Overhauser effects and is shown to play a critic

27 tion structure of recombinant FH1-3 based on nuclear Overhauser effects and RDCs.

28 ular modeling and NMR spectroscopy including nuclear Overhauser effects and residual dipolar coupling

29 ith aliphatic resonances in [Ca(2+)](4)-CaM (nuclear Overhauser effect) and increases the Ca(2+) affi

30 h-affinity complexes using (15)N R(1), R(2), nuclear Overhauser effect, and chemical-shift anisotropy

31 d D-LDH, such as the chemical shift changes, nuclear Overhauser effect, and solvent-induced isotopic

32 ere chemical shift assignments, (15)N-edited nuclear Overhauser effects, and (1)H-(15)N residual dipo

33 Sequential NMR assignments, intramonomer nuclear Overhauser effects, and circular dichroism spect

34 ts has been obtained using NMR spectrometry, nuclear Overhauser effects, and density functional theor

35 ents using (15)N-(13)C-labeled protein, (1)H nuclear Overhauser effects, and longitudinal relaxation

36 netic relaxation enhancement, intermolecular nuclear Overhauser effects, and targeted mutagenesis con

37 First, short-range nuclear Overhauser effects are detected between the arom

38 of a native-like partial core; no non-native nuclear Overhauser effects are observed.

39 Chemical shifts and nuclear Overhauser effects are similar to those of nativ

40 Nuclear Overhauser effects arising from the interactions

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

42 inal and transverse 13C relaxation rates and nuclear Overhauser effects at both 500 and 600 MHz (prot

43 The method is based on the nuclear Overhauser effect between bound anesthetic proto

44 n firmly assigned through (a) measurement of nuclear Overhauser effect connectivities, (b) prediction

45 dence of these H3(+) resonance; and observed nuclear Overhauser effects consistent with Hoogsteen and

46 ogram CYANA to build a network of interchain nuclear Overhauser effect constraints that can be used t

47 acetylated peptide and by weak medium-range nuclear Overhauser effect contacts indicative of alpha-h

48 ymmetric dimer interface, 172 intermolecular nuclear Overhauser effect correlations (NOEs) define the

49 ents Using Satisfiability (MAUS), leveraging Nuclear Overhauser Effect cross-peak data, peak residue

50 the membrane, as supported by intermolecular nuclear Overhauser effect cross-peaks between the peptid

51 Nuclear Overhauser effect crosspeak intensity provided i

52 Using 1H NMR spectroscopy, we observe nuclear Overhauser effect crosspeaks consistent with pro

53 were modeled using experimental transferred nuclear Overhauser effect data derived upon binding R*.

54 he conformational ensemble obtained by using nuclear Overhauser effect data in structure calculations

55 r proteins in solution from experimental NMR nuclear Overhauser effect data only and with minimal ass

56 Chemical shift index analysis and nuclear Overhauser effect data show that PrP(29-231) con

57 Heteronuclear (15)N-(1)H nuclear Overhauser effect data showed that the non-helic

58 In addition, the chemical shift and nuclear Overhauser effect data suggest that amino acids

59 cture was solved based on homonuclear proton nuclear Overhauser effect data using complete relaxation

60 ion of the two domains is not defined by the nuclear Overhauser effect data.

61 sidual dipolar coupling and inter-domain NOE nuclear Overhauser effect data.

62 Analysis of inter-residue nuclear Overhauser effects demonstrates that a native-li

63 In total, 3354 nuclear Overhauser effect-derived distance constraints,

64 a-helical membrane proteins >15 kDa in size, Nuclear-Overhauser effect-derived distance restraints ar

65 of the resulting alkenes were established by nuclear Overhauser effect difference NMR spectroscopy.

66 lex with the RA-GEF2 peptide using the exact nuclear Overhauser effect (eNOE) method.

67 istate structures were calculated from exact nuclear Overhauser effect (eNOE).

68 Furthermore, (13)C-edited nuclear Overhauser effects establish transient formation

69 Heteronuclear nuclear Overhauser effect experiments show that the new

70 ted average of the two is detected in NMR by nuclear Overhauser effect experiments.

71 NMR chemical shift trends and proton-proton nuclear Overhauser effect experiments.

72 in quantitative information from transferred nuclear Overhauser effect experiments.

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

74 d question mark1H inverted question mark-15N nuclear Overhauser effects for the 15N nuclear spins usi

75 emporal resolution of minutes, using relayed nuclear Overhauser effect (glycoNOE) MRI.

76 Intermolecular nuclear Overhauser effects have been used to investigate

77 in conformation as determined by transferred nuclear Overhauser effects in NMR spectra.

78 and (iii) selective detection of (19)F-(19)F nuclear Overhauser effects in the Escherichia coli pepti

79 ies done by using the heteronuclear [1H]-15N nuclear Overhauser effect indicate that almost half of P

80 Steady-state {(1)H}-(15)N heteronuclear nuclear Overhauser effects indicate that the protein's c

81 Distances derived from nuclear Overhauser effects indicate that the three Ser r

82 agnetic resonance spectroscopy, based on 905 nuclear Overhauser effect inter-proton distance restrain

83 to facilitate assignment of the intersubunit nuclear Overhauser effect interactions.

84 The pattern of observed peptide-lipid nuclear Overhauser effects is consistent with a parallel

85 contact zone derived from the intermolecular nuclear Overhauser effects is in agreement with recent b

86 ntify small molecules in complex mixtures by nuclear Overhauser effect magnetization transfer.

87 Nuclear Overhauser effect measurements and computational

88 R2) and steady state heteronuclear 15N [1H] nuclear Overhauser effect measurements at 500 and 600 MH

89 ic resonance line-broadening and transferred nuclear Overhauser effect measurements to identify the m

90 Furthermore, based on exchange-transferred nuclear Overhauser effect measurements, we established t

91 unds were verified by NMR spectroscopy using nuclear Overhauser effect methodology.

92 hermal titration calorimetry, intermolecular nuclear Overhauser effects, mutagenesis, and protection

93 ts derived from a combination of transferred nuclear Overhauser effect NMR experiments and molecular

94 Two-dimensional nuclear Overhauser effect NMR spectra demonstrate that t

95 en determined by two-dimensional transferred nuclear Overhauser effect NMR spectroscopy at 600 MHz.

96 have been studied in aqueous solutions using nuclear Overhauser effect (NOE) and transferred NOE NMR

97 ore region as evidenced by an intermolecular nuclear Overhauser effect (NOE) between each metallopept

98 Analyses of NMR chemical shifts and backbone nuclear Overhauser effect (NOE) connectivities showed th

99 ent was based on 2778 unambiguously assigned nuclear Overhauser effect (NOE) connectivities, 297 ambi

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

101 Strong and positive intermolecular nuclear Overhauser effect (NOE) cross-peaks define a spe

102 Long-range nuclear Overhauser effect (NOE) cross-peaks showed the t

103 Distance bounds, calculated from the nuclear Overhauser effect (NOE) crosspeak intensities vi

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

105 ted protein from unassigned experimental NMR nuclear Overhauser effect (NOE) data only.

106 ts, and distance restraints derived from the nuclear Overhauser effect (NOE) data were used to calcul

107 We also calculated the nuclear Overhauser effect (NOE) distances from the molec

108 Unwanted sample heating and nuclear Overhauser effect (NOE) enhancements are the two

109 l and transverse relaxation rates and 15N-1H nuclear Overhauser effect (NOE) enhancements were measur

110 ) detection of intermolecular contacts using nuclear Overhauser effect (NOE) experiments; (iv) struct

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

112 in relaxation rate (R(2)), and heteronuclear nuclear Overhauser effect (NOE) have been carried out at

113 we support these assignments with sequential nuclear Overhauser effect (NOE) information obtained fro

114 between different (1)H environments via the nuclear Overhauser effect (NOE) is included in the NMR p

115 relaxation times made it impractical to use nuclear Overhauser effect (NOE) measurements for assignm

116 Experimental NMR nuclear Overhauser effect (NOE) measurements of an asymm

117 cytochrome b5 were quantified using {1H}-15N nuclear Overhauser effect (nOe) measurements, which char

118 heavily on distance restraints derived from nuclear Overhauser effect (NOE) measurements.

119 he 13C relaxation data, T1, and steady-state nuclear Overhauser effect (NOE) obtained at two differen

120 geous when classical NMR parameters like the nuclear Overhauser effect (NOE) or J-couplings fail.

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

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

123 tative distance restraints, analogous to the nuclear Overhauser effect (NOE) routinely used in soluti

124 emical shift, T1 values, and one-dimensional nuclear Overhauser effect (nOe) saturation transfer expe

125 omplete relaxation matrix methods to analyze nuclear Overhauser effect (NOE) spectroscopic cross-peak

126 ermining resonance assignments, interpreting nuclear Overhauser effect (NOE) spectroscopy (NOESY) spe

127 Nuclear Overhauser effect (NOE) spectroscopy experiments

128 C-(13)C-(1)H correlation and (15)N-separated nuclear Overhauser effect (NOE) spectroscopy experiments

129 Nuclear Overhauser effect (NOE) spectroscopy revealed a

130 A total of 1159 useful nuclear Overhauser effect (NOE) upper distance constrain

131 rted question mark-HN inverted question mark nuclear Overhauser effect (NOE) values of vMIP-II, deter

132 The resulting process is equal to the nuclear Overhauser effect (NOE) where typically continuo

133 the steep inverse distance dependence of the nuclear Overhauser effect (NOE), from which the distance

134 ng a novel combination of chemical shift and nuclear Overhauser effect (NOE)-based methods.

135 (r.m.s.d.) = 1.2 A] was determined from 475 nuclear Overhauser effect (NOE)-derived distance restrai

136 On the basis of 951 nuclear Overhauser effect (NOE)-derived distance restrai

137 angstrom2 were generated with a total of 500 nuclear Overhauser effect (NOE)-derived distance restrai

138 m the human RBCC protein, MID1) based on 670 nuclear Overhauser effect (NOE)-derived distance restrai

139 ed interactions and violated very few of the nuclear Overhauser effect (NOE)-derived distances used i

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

141 s to enhance connectivities revealed via the nuclear Overhauser effect (NOE).

142 se sensitivity for observing the intraligand nuclear Overhauser effect (NOE).

143 erse relaxation rate (R2), and heteronuclear nuclear Overhauser effect (NOE)] measured at two tempera

144 Nuclear Overhauser effects (nOe's) observed by two-dimen

145 876 upper distance constraints derived from nuclear Overhauser effects (NOE) and 173 dihedral angle

146 1878 upper distance constraints derived from nuclear Overhauser effects (NOE) and 314 dihedral angle

147 pendent on the observation of intermolecular nuclear Overhauser effects (NOE) and their assignments,

148 Chemical shift indices and nuclear Overhauser effects (NOE) confirmed helices in th

149 on rate constants (RN(Nx,y)=1/T2) and 1H-15N nuclear Overhauser effects (NOE) were obtained for 143 o

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

151 Long-range nuclear Overhauser effects (NOE) within this subdomain a

152 chemical shifts and the pattern of midrange nuclear Overhauser effects (NOE).

153 (T(2)) measurements as well as [(1)H]-(15)N nuclear Overhauser effects (NOE).

154 data such as complexation-induced shifts and nuclear Overhauser effects (nOe).

155 The PBEs, in combination with HN-HN nuclear Overhauser effects (NOEs) and chemical shift ind

156 domain without an inhibitor is based on 2813 nuclear Overhauser effects (NOEs) and has an average RMS

157 ossibly differences in homonuclear (1)H-(1)H nuclear Overhauser effects (NOEs) and heteronuclear (1)H

158 structure was determined on the basis of the nuclear Overhauser effects (NOEs) and the hydrogen bond

159 intensity of both sequential and long-range nuclear Overhauser effects (NOEs) between backbone amide

160 19F nuclear Overhauser effects (NOEs) between fluorine label

161 Intermolecular nuclear Overhauser effects (NOEs) between protein and wa

162 Observation of several interbase nuclear Overhauser effects (NOEs) clearly indicates a st

163 easure (13)C T(1), T(1rho) and heteronuclear nuclear Overhauser effects (NOEs) for sugar and base nuc

164 ns and nitrogens, and (1)H-(1)H interresidue nuclear Overhauser effects (NOEs) for the two mutants wi

165 to DNA chemical shifts and 24 intermolecular nuclear Overhauser effects (NOEs) identify the 5'-ApG an

166 g, chemical shift mapping and intermolecular nuclear Overhauser effects (NOEs) indicate the presence

167 It retains most of its solution nuclear Overhauser effects (NOEs) upon binding to either

168 stance and angular restraints based on 1H-1H nuclear Overhauser effects (NOEs), hydrogen-bonding netw

169 Based on 1H intermolecular nuclear Overhauser effects (NOEs), the THF rings of all

170 Using paramagnetic probes and protein-DPC nuclear Overhauser effects (NOEs), we define portions of

171 rom assigned intra-ligand and protein-ligand nuclear Overhauser effects (NOEs).

172 he backbone resonances and measure H(N)-H(N) nuclear Overhauser effects (NOEs).

173 t be defined because there are no long-range nuclear Overhauser effects (NOEs).

174 n distances were estimated from the observed nuclear Overhauser effects (NOEs).

175 R) rely on distance restraints also known as Nuclear Overhauser effects (NOEs).

176 J couplings, isotropic chemical shifts, and nuclear Overhauser effects (NOEs)/rotational frame nucle

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

178 ifts (CSs), intensities of NOESY crosspeaks [nuclear Overhauser effects (NOEs)], and residual dipolar

179 of r-K2 (1)H-NMR signals and two-dimensional nuclear Overhauser effect (NOESY) experiments in the pre

180 peaks with minor conformation in (19)F-(19)F nuclear Overhauser effect (NOESY) spectra.

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

182 degrees), the set of medium- and short-range nuclear Overhauser effects observed for the active N-ter

183 The simulated nuclear Overhauser effect pair distances are in excellen

184 usion rates, the NH chemical shifts, and the nuclear Overhauser effect patterns provided a coherent p

185 ntribution of conformational exchange to the nuclear Overhauser effect peak intensity, we applied inf

186 sonance assignments and detailed analysis of nuclear Overhauser effects permit the direct comparison

187 ts, coupling constants, relaxation rates and nuclear Overhauser effect prediction applied to the thre

188 Using a nuclear Overhauser effect ratio strategy to define the a

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

190 Spin-lattice, spin-spin, and heteronuclear nuclear Overhauser effect relaxation data for backbone a

191 NMR experiments (correlated chemical shifts, nuclear Overhauser effects, residual dipolar couplings)

192 ust and has a high tolerance for misassigned nuclear Overhauser effect restraints, greatly simplifyin

193 r Overhauser effects (NOEs)/rotational frame nuclear Overhauser effects (ROEs).

194 conformational analysis from rotating angle nuclear Overhauser effect (ROESY) data.

195 ion matrix simulation of the two-dimensional nuclear Overhauser effect spectra at various mixing time

196 Multidimensional nuclear Overhauser effect spectra, X-filtered spectra an

197 hanges upon Zn(2+) binding were supported by nuclear Overhauser effect spectrometry (NOESY) studies.

198 centers was assigned through two-dimensional nuclear Overhauser effect spectroscopic analysis coupled

199 evertheless, structure calculations based on nuclear Overhauser effect spectroscopic data combined wi

200 The two distinct structures are derived from nuclear Overhauser effect spectroscopic distance restrai

201 Two-dimensional rotating-frame nuclear Overhauser effect spectroscopy (2D ROESY) (1)H N

202 cal shift measurements, two-dimensional (2D) nuclear Overhauser effect spectroscopy (2D-NOESY) 1H MAS

203 Heteronuclear (1)H-(15)N nuclear Overhauser effect spectroscopy (NOESY) and heter

204 This is accomplished by utilizing nuclear Overhauser effect spectroscopy (NOESY) at subzer

205 thiol (PTs)] were isolated and identified by nuclear Overhauser effect spectroscopy (NOESY) correlati

206 ance (NMR) experiments, and (5) NMR transfer nuclear Overhauser effect spectroscopy (NOESY) experimen

207 ized by variable temperature NMR studies and nuclear Overhauser effect spectroscopy (NOESY) experimen

208 Nuclear Overhauser effect spectroscopy (NOESY) experimen

209 methyl groups that is based on methyl-methyl nuclear Overhauser effect spectroscopy (NOESY) peak list

210 This, in combination with two-dimensional nuclear Overhauser effect spectroscopy (NOESY) results,

211 cts versus their free components, whereas 2D nuclear Overhauser effect spectroscopy (NOESY) spectra s

212 molecule tend to correlate together in a 2D nuclear Overhauser effect spectroscopy (NOESY) spectrum,

213 thin the same molecule may correlate in a 2D nuclear Overhauser effect spectroscopy (NOESY) spectrum,

214 g (RFDR) and (1)H magic angle spinning (MAS) nuclear Overhauser effect spectroscopy (NOESY) technique

215 MAS-assisted two-dimensional nuclear Overhauser effect spectroscopy (NOESY) was condu

216 combination of (1)H NMR and two-dimensional Nuclear Overhauser Effect Spectroscopy (NOESY) which rev

217 SY), total correlation spectroscopy (TOCSY), nuclear Overhauser effect spectroscopy (NOESY), and rota

218 To this end, we have used nuclear Overhauser effect spectroscopy (NOESY)-based dis

219 )C relaxation parameters, and rotating-frame nuclear Overhauser effect spectroscopy (ROESY) crosspeak

220 ect spectroscopy (NOESY), and rotating frame nuclear Overhauser effect spectroscopy (ROESY) data were

221 re determined by transferred two-dimensional nuclear Overhauser effect spectroscopy (TRNOESY) measure

222 n the present work, we have used transferred nuclear Overhauser effect spectroscopy (TRNOESY) to dete

223 The NMR method of transferred nuclear Overhauser effect spectroscopy (TRNOESY) was use

224 We used transferred nuclear Overhauser effect spectroscopy (TrNOESY), which

225 Nuclear Overhauser effect spectroscopy allowed for the d

226 Homonuclear two-dimensional nuclear Overhauser effect spectroscopy and double quantu

227 ion-ordered spectroscopy, and rotating-frame nuclear Overhauser effect spectroscopy and high-resoluti

228 esidues near Trp191, as shown by transferred nuclear Overhauser effect spectroscopy and hydrogen/deut

229 Nuclear Overhauser effect spectroscopy and molecular mod

230 Transferred nuclear Overhauser effect spectroscopy and rotating fram

231 VSD-phospholipid micelle interactions using nuclear Overhauser effect spectroscopy and showed that t

232 Nuclear Overhauser effect spectroscopy confirms the spat

233 Intraresidue nuclear Overhauser effect spectroscopy cross peaks were

234 site as reflected in optical spectra and NMR nuclear Overhauser effect spectroscopy cross-peak and hy

235 tion matrix analysis of sets of experimental nuclear Overhauser effect spectroscopy crosspeaks.

236 Nuclear Overhauser effect spectroscopy experiments of th

237 itionally, NMR(2) relies on isotope-filtered nuclear Overhauser effect spectroscopy experiments requi

238 no-7-iminoindolizin-1-ones) were rejected by nuclear Overhauser effect spectroscopy experiments.

239 ucture of the two isomers is determined with nuclear Overhauser effect spectroscopy NMR and single-cr

240 Quantum mechanics calculations and nuclear Overhauser effect spectroscopy NMR studies sugge

241 Analysis by two-dimensional transfer nuclear Overhauser effect spectroscopy of the induced so

242 This method includes the acquisition of nuclear Overhauser effect spectroscopy one-dimensional a

243 Nuclear Overhauser effect spectroscopy revealed a number

244 Detailed analysis of the nuclear Overhauser effect spectroscopy spectra of the pr

245 trad-bound guanine can be extracted from the nuclear Overhauser effect spectroscopy spectrum based on

246 Two-dimensional transferred nuclear Overhauser effect spectroscopy studies of bound

247 Two-dimensional nuclear Overhauser effect spectroscopy suggests that the

248 ct, we have used two-dimensional transferred nuclear Overhauser effect spectroscopy to determine the

249 version recovery method, and the transferred nuclear Overhauser effect spectroscopy was used to study

250 0) IKENLKDCGLF was determined by transferred nuclear Overhauser effect spectroscopy while it was boun

251 d annealing using structural restraints from nuclear Overhauser effect spectroscopy, and scalar and r

252 Characterized by NMR studies and nuclear Overhauser effect spectroscopy, complex 7 is a d

253 R spectra, total correlated spectroscopy and nuclear Overhauser effect spectroscopy, show that the mo

254 ation, which is confirmed by two-dimensional nuclear Overhauser effect spectroscopy, the crystal stru

255 (K(a) up to 19,000 M(-1)), and is shown--by nuclear Overhauser effect spectroscopy--to adopt the thr

256 und to the recombinant ECD using transferred nuclear Overhauser effect spectroscopy.

257 to Galpha(s), was determined by transferred nuclear Overhauser effect spectroscopy.

258 upon binding, as demonstrated by transferred nuclear Overhauser effect spectroscopy.

259 ronic acid group at position 4', as shown by nuclear Overhauser effect spectroscopy.

260 of the products by X-ray crystallography and nuclear Overhauser effect spectroscopy.

261 as measured by NMR experiments of (1)H-(15)N nuclear Overhauser effect, spin-lattice relaxation, and

262 The spin polarization-induced nuclear Overhauser effect (SPINOE), particularly at low

263 NMR-filtered nuclear Overhauser effect studies confirmed these observ

264 internally inconsistent group of long range nuclear Overhauser effects suggest a close proximity of

265 axation-dispersion experiments, and filtered nuclear Overhauser effects suggest that CCL27 does not a

266 R1) or heteronuclear cross relaxation rates (nuclear Overhauser effect), suggesting that the 14-38 di

267 exhibits fewer helix-related and long range nuclear Overhauser effects than does the d-Ser(B8) analo

268 As monitored by two-dimensional (19)F-(19)F nuclear Overhauser effect, the distance between two phen

269 Contributions of the nuclear Overhauser effect to exchange rates measured wit

270 d, and their relaxation, dipolar shifts, and nuclear Overhauser effects to adjacent residues used to

271 an NMR experiment that allows one to exploit nuclear Overhauser effects to determine internuclear dis

272 gion of the talin rod and use intermolecular nuclear Overhauser effects to determine the structure of

273 Here, we used transferred nuclear Overhauser effects to study the interaction in s

274 ositioned in the heme cavity on the basis of nuclear Overhauser effects to the heme and each other, d

275 l shift perturbation and the inter-molecular nuclear Overhauser effects to the RNA.

276 Nuclear Overhauser effects to urea for these segments ar

277 In previous work, we found using transferred nuclear Overhauser effect (trNOE) analysis that two 13 a

278 ectroscopy experiments, inducing transferred nuclear Overhauser effect (trNOE) and saturation transfe

279 This transferred nuclear Overhauser effect (trNOE) disrupts the observed

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

281 Previous transferred nuclear Overhauser effect (trNOE) studies with peptides

282 d nucleotide was determined from transferred nuclear Overhauser effects (trnOe) experiments to determ

283 contact surfaces are studied by transferred nuclear Overhauser effects (trNOEs) and saturation trans

284 Traditionally, transferred nuclear Overhauser effects (trNOEs), measured from NMR s

285 e geometry calculations based on transferred nuclear Overhauser effects (TRNOEs).

286 re determined by two-dimensional transferred nuclear Overhauser effect (TRNOESY) measurements combine

287 re determined by two-dimensional transferred nuclear Overhauser effect (TRNOESY) measurements combine

288 Long-range inter-residue nuclear Overhauser effects unequivocally confirmed the f

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

290 turation, and reduced heteronuclear (1H-15N) nuclear Overhauser effect values.

291 The transferred nuclear Overhauser effect was used to characterize confo

292 relaxation data and steady-state (1)H- (15)N nuclear Overhauser effects were analyzed using model-fre

293 frame relaxation rates and the heteronuclear nuclear Overhauser effects were carried out on a uniform

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

295 d question mark1H inverted question mark-15N nuclear Overhauser effects were measured for the backbon

296 Intermolecular (1)H(19)F and (1)H(1)H nuclear Overhauser effects were used to explore interact

297 y arising from changes in creatine level and nuclear overhauser effects, which were not found using c

298 The distance relation of nuclear Overhauser effects with a factor of r(-6) is emp

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