ライフサイエンスコーパス: magic-angle spinning

1 proton CSAs in fully protonated solids under magic angle spinning.

2 asing of individual spinning sidebands under magic angle spinning.

3 (13)C-(1)H residual dipolar couplings under magic-angle spinning.

4 he use of highly deuterated samples and fast magic-angle spinning.

5 observed by 13C solid-state NMR even without magic-angle spinning.

6 cho double-resonance (REDOR) technique under magic-angle spinning.

7 s virus (MeV) nucleocapsids under ultra-fast magic-angle spinning.

8 r burn trauma; and ex vivo, high-resolution, magic angle spinning (1)H NMR on intact excised mouse mu

9 spectroscopy, powder X-ray diffraction, and magic-angle spinning (1)H-decoupled (13)C NMR.

10 Proton high-resolution magic angle spinning ((1)H HR-MAS) nuclear magnetic reso

11 Cross-polarization magic angle spinning (13)C NMR spectra showed that CO2 b

12 to the hydrophobic milieu, we carried out 2D magic-angle spinning (13)C NMR experiments on the water-

13 ymer analysis was conducted using melt-state magic-angle spinning (13)C NMR spectroscopy of both line

14 te were determined via VT cross-polarization magic-angle spinning (13)C NMR spectroscopy.

15 diffraction, solid-state cross-polarization/magic-angle spinning (13)C NMR, and Bloch-decay (13)C NM

16 l (2D) and three-dimensional high-resolution magic-angle-spinning (13)C solid-state nuclear magnetic

17 SpSEEKFLRRIGRFG) are studied using deuterium magic angle spinning ((2)H MAS) line shape and spin-latt

18 Two-dimensional magic-angle spinning (2D MAS) exchange and constant-time

19 inositide/phosphatidylcholine vesicles using magic angle spinning (31)P NMR spectroscopy.

20 and cholesterol was studied with static and magic angle spinning (31)P NMR spectroscopy.

21 gin unit, were investigated with solid-state magic angle spinning (51)V NMR, FT-IR, in situ Raman, in

22 lysis of the (77)Se{(1)H} cross-polarization magic angle spinning and (77)Se spin-echo solid-state NM

23 Using magic-angle spinning and cross-polarization techniques t

24 gh-quality membrane protein samples for both magic-angle spinning and oriented-sample solid-state NMR

25 Cross-polarization magic-angle spinning and rotational-echo double resonanc

26 ratio for solid-state NMR experiments under magic-angle spinning and static conditions, respectively

27 rho) measurements, direct polarization with magic-angle spinning, and static CP of the hydrated and

28 Magic angle spinning at kHz frequencies restored resolut

29 Using low-power schemes under magic-angle spinning at 40 kHz, we obtained two-dimensio

30 The tensor orientation is obtained under magic angle spinning by modulating a recoupled chemical

31 We have adapted it to broad spectra and fast magic-angle spinning by accounting for long pulses (comp

32 ange materials for data storage, even 22-kHz magic-angle spinning cannot resolve the center- and side

33 res and correlated them with (13)C and (15)N magic angle spinning chemical shift data.

34 (31)P NMR under magic angle spinning conditions resolves the SM and DOPC

35 atic liquid crystalline alignment, and under magic angle spinning conditions where alignment relative

36 R1rho rates, which were measured under fast magic angle spinning conditions, vary by an order of mag

37 D (13)C-(13)C correlation spectroscopy under magic angle spinning conditions.

38 The measurements are carried out under magic-angle spinning conditions, using the constant-time

39 investigate membrane protein topology under magic-angle spinning conditions.

40 experiment in liquids, is robust under fast magic-angle-spinning conditions and in the presence of d

41 troscopy (ATR FT-IR), and cross polarization magic angle spinning (CP MAS) NMR spectroscopy.

42 Using (19)F-->(1)H cross-polarization magic angle spinning (CP-MAS) nuclear magnetic resonance

43 olar dephasing, and (15)N cross-polarization/magic angle spinning (CP/MAS).

44 e line (2)H NMR and (13)C cross-polarization magic-angle spinning (CP-MAS) NMR spectra of Ala-PLB and

45 ructural investigation by cross-polarization magic-angle spinning (CP-MAS) NMR.

46 RD) and solid-state (13)C cross-polarization magic-angle-spinning (CP-MAS) NMR.

47 various methods, such as cross-polarization magic angle spinning (CPMAS) (13)C NMR and single crysta

48 ontact times were used in cross-polarization magic angle spinning (CPMAS) NMR, CP rotational-echo dou

49 ta yielded orientational restraints, whereas magic-angle spinning data yielded interhelical distance

50 We describe the use of magic angle spinning deuterium NMR to establish the stru

51 luded quantitative (13)C direct polarization/magic angle spinning (DP/MAS) and DP/MAS with recoupled

52 amically hyperpolarized (1)H to (13)C during magic-angle spinning dynamic nuclear polarization (DNP)

53 From a suite of two-dimensional and 3D magic-angle spinning experiments, (13)C and (15)N chemic

54 ing sPREs in practically the entire range of magic angle spinning frequencies used for biomolecular s

55 application of (1)H-detected experiments at magic-angle spinning frequencies of >50 kHz enables the

56 The impact of the sample temperature and magic angle spinning frequency on epsilon is investigate

57 ments (17.6, 20.0, and 23.5 T) and ultrafast magic angle spinning (>60 kHz), high-quality spectra wer

58 High Resolution Magic Angle Spinning (HR-MAS) is an NMR technique that c

59 changes during storage, (1)H high resolution-magic angle spinning (HR-MAS) NMR spectroscopy of apple

60 The feasibility of (1)H-High Resolution-Magic Angle Spinning (HR-MAS) nuclear magnetic resonance

61 In the present study a high-resolution magic angle spinning (HR-MAS) proton ((1)H) NMR spectros

62 The utility of high-resolution magic-angle spinning (HR-MAS) NMR for studying drug deli

63 High-resolution magic-angle spinning (HR-MAS) NMR was developed in late

64 High-resolution magic-angle spinning (HR-MAS) nuclear magnetic resonance

65 of C. elegans based on (1)H high-resolution magic-angle spinning (HR-MAS) nuclear magnetic resonance

66 t tissue samples by means of high-resolution magic-angle-spinning (HR-MAS) NMR spectroscopy and we pr

67 and metabolite analysis, by high-resolution magic angle spinning (HRMAS) (1)H NMR spectroscopy, in B

68 nd subsequent application of high-resolution magic angle spinning (HRMAS) (1)H nuclear magnetic reson

69 r metabolism was analyzed by high-resolution magic angle spinning (HRMAS) nuclear magnetic resonance

70 his paper describes a proton high resolution magic angle spinning (HRMAS) nuclear magnetic resonance

71 The new result for DOPC from magic angle spinning is consistent with x-ray results.

72 Here, we used high-resolution magic angle spinning magnetic resonance mass spectroscop

73 al, immunohistochemistry and high resolution magic angle spinning magnetic resonance spectroscopy (MR

74 We investigated if magic angle spinning (MAS) 1H NMR can be used as a tool

75 First, calcium-43 magic angle spinning (MAS) and static NMR spectra of a (

76 ptophan's interfacial preference by using 1H magic angle spinning (MAS) chemical shift measurements,

77 or all three compounds under both static and magic angle spinning (MAS) conditions at 21.1 T, allowin

78 designed 3D (2)H-(13)C-(13)C solid-state NMR magic angle spinning (MAS) experiment is presented and d

79 ancements of up to 23 have been obtained for magic angle spinning (MAS) experiments at 5 T and 85-90

80 H-(113)Cd and (1)H-(77)Se cross-polarization magic angle spinning (MAS) experiments, which demonstrat

81 We employ a combination of (13)C/(15)N magic angle spinning (MAS) NMR and (2)H NMR to study the

82 dard addition of water is combined with (1)H magic angle spinning (MAS) NMR detection, absolute quant

83 We describe a new magic angle spinning (MAS) NMR experiment for obtaining

84 We introduce a family of two-dimensional magic angle spinning (MAS) NMR experiments for structura

85 st demonstration of natural-abundance (43)Ca magic angle spinning (MAS) NMR experiments on bone, usin

86 e we report atomic-level characterization by magic angle spinning (MAS) NMR of the muscle isoform of

87 Magic angle spinning (MAS) NMR spectra of labeled rhodop

88 es in the 17O high-resolution triple-quantum magic angle spinning (MAS) NMR spectra were resolved and

89 d examined their (13)C-(13)C and (13)C-(15)N magic angle spinning (MAS) NMR spectra.

90 reviously we have demonstrated the use of 1H magic angle spinning (MAS) NMR spectroscopy for the topo

91 Protein magic angle spinning (MAS) NMR spectroscopy has generate

92 Magic Angle Spinning (MAS) NMR spectroscopy is a powerfu

93 Fast magic angle spinning (MAS) NMR spectroscopy is becoming

94 High-resolution (19)F magic angle spinning (MAS) NMR spectroscopy is used to s

95 otopic substitution (NDIS) techniques, (6)Li Magic Angle Spinning (MAS) NMR spectroscopy, and for the

96 and the CA-SP1 maturation intermediate using magic angle spinning (MAS) NMR spectroscopy.

97 We report a magic angle spinning (MAS) NMR structure of the drug-res

98 Magic angle spinning (MAS) NMR studies of amyloid and me

99 the fibril formation process in vitro, and a magic angle spinning (MAS) NMR study of the fibrils form

100 pic labeling strategies and multidimensional magic angle spinning (MAS) NMR techniques at high magnet

101 Nonetheless, recent developments in magic angle spinning (MAS) NMR technology have made it p

102 a membrane protein using dipolar recoupling magic angle spinning (MAS) NMR.

103 al characterization of GNNQQNY fibrils using magic angle spinning (MAS) NMR.

104 Silicon-29 magic angle spinning (MAS) nuclear magnetic resonance (N

105 (6)Li magic angle spinning (MAS) nuclear magnetic resonance (N

106 absorption fine structure (EXAFS) and (27)Al magic angle spinning (MAS) nuclear magnetic resonance (N

107 ce-specific backbone resonance assignment of magic angle spinning (MAS) nuclear magnetic resonance (N

108 cy driven dipolar recoupling (RFDR) and (1)H magic angle spinning (MAS) nuclear Overhauser effect spe

109 nhancements increase rapidly with increasing magic angle spinning (MAS) rates.

110 Although magic angle spinning (MAS) solid-state NMR is a powerful

111 Multidimensional magic angle spinning (MAS) solid-state NMR of uniformly

112 of oriented sample (OS) solid-state NMR and magic angle spinning (MAS) solid-state NMR techniques to

113 We introduce a labeling scheme for magic angle spinning (MAS) solid-state NMR that is based

114 ctural forms and examined the specimens with magic angle spinning (MAS) solid-state nuclear magnetic

115 13)C(alpha) dipolar coupling, stationary and magic angle spinning (MAS) spectra with and without (15)

116 We applied rapid (60 kilohertz) magic angle spinning (MAS) to obtain high-resolution hyd

117 vity on natural abundance samples using fast magic angle spinning (MAS), indirect detection of low-ga

118 ce (NMR) with (1)H detection under ultrafast magic angle spinning (MAS).

119 o-dimensional NOESY 1H NMR spectroscopy with magic angle spinning (MAS).

120 field of dynamic nuclear polarization under magic angle spinning (MAS-DNP) could be used to dramatic

121 The 2D NMR spectra were acquired under fast magic-angle spinning (MAS) and dipolar-assisted rotation

122 )C dynamic nuclear polarization at 5 T under magic-angle spinning (MAS) at 82 K using a mixture of mo

123 We have used static in situ and magic-angle spinning (MAS) ex situ (13)C nuclear magneti

124 NMR spectroscopy, including both static and magic-angle spinning (MAS) experiments.

125 peptides or proteins by measuring RDCs using magic-angle spinning (MAS) in combination with dipolar r

126 rphs by a combination of stationary and fast magic-angle spinning (MAS) methods at high magnetic fiel

127 blies in the escape from CypA dependence, by magic-angle spinning (MAS) NMR and molecular dynamics (M

128 powder XRD, (1)H double-quantum solid-state magic-angle spinning (MAS) NMR and small-angle neutron s

129 Utilizing (17)O magic-angle spinning (MAS) NMR at multiple magnetic fiel

130 Heteronuclear solid-state magic-angle spinning (MAS) NMR experiments for probing (

131 nt 3D 15N-13C-13C-15N dipolar-chemical shift magic-angle spinning (MAS) NMR experiments.

132 n structure determination by proton-detected magic-angle spinning (MAS) NMR has focused on highly deu

133 Fluorescence and 31P magic-angle spinning (MAS) NMR measurements indicated th

134 ic reaction centers (RCs) as modification of magic-angle spinning (MAS) NMR signal intensity under il

135 ique that enhances the signal intensities in magic-angle spinning (MAS) NMR spectra.

136 Subsequently, magic-angle spinning (MAS) NMR spectroscopy with sensiti

137 e compared structurally using (13)C and (1)H magic-angle spinning (MAS) NMR.

138 (13)C solid-state magic-angle spinning (MAS) nuclear magnetic resonance (N

139 y depends on their dynamics, and solid-state magic-angle spinning (MAS) nuclear magnetic resonance (N

140 Additionally, fast (25 kHz) magic-angle spinning (MAS) provides optimal sensitivity

141 ere we report sample preparation and initial magic-angle spinning (MAS) solid-state NMR (SSNMR) of CY

142 Dynamic nuclear polarization (DNP) magic-angle spinning (MAS) solid-state NMR (ssNMR) spect

143 Magic-angle spinning (MAS) solid-state NMR (SSNMR) techn

144 Here we present magic-angle spinning (MAS) solid-state NMR studies of un

145 ation of 1H, 13C, and 15N chemical shifts by magic-angle spinning (MAS) solid-state NMR with first-pr

146 I3-SH3 in amyloid fibril form as revealed by magic-angle spinning (MAS) solid-state nuclear magnetic

147 Nevertheless, DNP-enhanced magic-angle spinning (MAS) spectra recorded at 5 T and 9

148 P23-144 amyloid by using 2D J-coupling-based magic-angle spinning (MAS) SSNMR techniques.

149 Magic-angle spinning (MAS) was used to obtain high-resol

150 ion of 13C and 15N NMR chemical shifts under magic-angle spinning (MAS), effects of local mobility on

151 sensitivity and high-resolution under sample magic-angle spinning (MAS).

152 rse protonation or with approximately 30 kHz magic-angle spinning (MAS).

153 nhancement of 110 was obtained in high-field magic-angle-spinning (MAS) NMR experiments.

154 S31N mutant of M2(18-60) determined using 3D magic-angle-spinning (MAS) NMR spectra acquired with a (

155 High-resolution (1)H magic-angle-spinning (MAS) NMR spectroscopy has been app

156 Here we apply magic-angle-spinning (MAS) NMR to examine the structure

157 Magic-angle-spinning (MAS) solid-state NMR (ssNMR) spect

158 Using magic-angle-spinning (MAS) solid-state NMR spectroscopy,

159 ng (R(3)) combined with the multiple-quantum magic-angle spinning (MQMAS) in a three-dimensional (3D)

160 , based on a series of temperature-dependent magic-angle spinning multinuclear nuclear-magnetic-reson

161 Solid-state magic angle spinning NMR analyses and SEM microscopy hav

162 ound to end-binding protein EB1 and free, by magic angle spinning NMR and molecular dynamics simulati

163 Here we applied magic angle spinning NMR and selective Arg isotope enric

164 th solid-state wide-line and high resolution magic angle spinning NMR as well as with fluorescence co

165 We demonstrate a novel 3D NNC magic angle spinning NMR experiment that generates (15)N

166 We describe three-dimensional magic angle spinning NMR experiments that enable simulta

167 We present solid-state magic angle spinning NMR measurements of rhodopsin and t

168 version by solid state (13)C cross-polarized magic angle spinning NMR reveals that solid heptacene ha

169 A microautoclave magic angle spinning NMR rotor is developed enabling in

170 rovided by analysis of 2D rotor-synchronized magic angle spinning NMR spectra of doubly 13C carbonyl

171 We report solid-state deuterium magic angle spinning NMR spectra of perdeuterated adaman

172 We report magic angle spinning NMR spectra of POPC and DPhPC membr

173 uctural constraints obtained from high field magic angle spinning NMR spectra.

174 NMR crystallography approach based on (51)V magic angle spinning NMR spectroscopy and Density Functi

175 e to detailed structural characterization by magic angle spinning NMR spectroscopy and that solid-sta

176 omplementation, determined using solid-state magic angle spinning NMR spectroscopy at 17.6 T.

177 nts of vanadium have been addressed by (51)V magic angle spinning NMR spectroscopy of six-coordinated

178 nge interhelical distance measurements using magic angle spinning NMR spectroscopy provide high-resol

179 Here, we use magic angle spinning NMR spectroscopy to obtain the (13)

180 Here, we use solid-state magic angle spinning NMR spectroscopy to probe the chang

181 (13)C cross-polarization magic angle spinning NMR spectroscopy was used to charac

182 ransgenic mouse model using a combination of magic angle spinning NMR spectroscopy, in silico predict

183 HO(*) was determined using calibrated (19)F magic angle spinning NMR spectroscopy.

184 e magnetic moments have been examined by 31P magic angle spinning NMR spectroscopy.

185 5-115), in its fibrillar form, determined by magic angle spinning NMR spectroscopy.

186 n motor on polymeric microtubules, solved by magic angle spinning NMR spectroscopy.

187 lycine-rich) domain of mammalian dynactin by magic angle spinning NMR spectroscopy.

188 In addition, 1H high-resolution magic angle spinning NMR techniques were employed to col

189 We confirm with (1)H magic angle spinning NMR that the increased hydration is

190 We used high resolution magic angle spinning NMR to establish the location of MA

191 In particular, we employ magic angle spinning NMR to examine a structural phase t

192 ol) in monounsaturated model membranes using magic angle spinning NMR to measure these interactions t

193 Here, we apply magic angle spinning NMR to the two parent states follow

194 dividual bilayer lipids was studied by (31)P magic angle spinning NMR, and toxin-induced changes in b

195 eled agonist CP-55,940-d(6) measured by (2)H magic angle spinning NMR, as well as by activation of G

196 an array of approaches (limited proteolysis, magic angle spinning NMR, Fourier transform infrared spe

197 ng this protocol, proteoliposome samples for magic-angle spinning NMR and uniformly aligned samples (

198 We describe a magic-angle spinning NMR experiment for selective (13)C-

199 1)H-(15)N-(13)C-(1)H dipolar chemical shift, magic-angle spinning NMR experiments.

200 mensional (2D) solid-state (29)Si and (27)Al magic-angle spinning NMR methodologies, including T(1)-r

201 High-resolution magic-angle spinning NMR of high-Z spin-1/2 nuclei such

202 Crosspolarization magic-angle spinning NMR showed that chemical shifts of

203 NMR experiments that enhance sensitivity in magic-angle spinning NMR spectra of cryo-trapped photocy

204 We also present one-dimensional (13)C magic-angle spinning NMR spectra of the labeled A beta(1

205 two-dimensional (13)C-(13)C and (15)N-(13)C magic-angle spinning NMR spectra.

206 Solid-state (13)C magic-angle spinning NMR spectroscopy at natural isotopi

207 This approach combining oriented-sample and magic-angle spinning NMR spectroscopy in native-like lip

208 lved spectrum, obtained from high-resolution magic-angle spinning NMR spectroscopy of liver tissues,

209 Using (15)N cross polarization magic-angle spinning NMR spectroscopy, the protonation o

210 The (13) C cross-polarization magic-angle spinning NMR spectroscopy, X-ray diffraction

211 study provides, to our knowledge, the first magic-angle spinning NMR structure of an intact filament

212 es of CP-55,940 and POPC were measured by 1H magic-angle spinning NMR with pulsed magnetic field grad

213 Magic-angle spinning NMR, often in combination with phot

214 e been observed by performing double-quantum magic-angle-spinning NMR at low temperature in the prese

215 We describe three-dimensional magic-angle-spinning NMR experiments for the simultaneou

216 shift anisotropy (CSA) tensors, recorded in magic-angle-spinning NMR experiments, provide direct res

217 (13)C magic-angle-spinning NMR methods were applied to investi

218 Magic-angle-spinning NMR reveals that fibrillar exon1 ha

219 microscopy and circular dichroism and (11)B magic-angle-spinning NMR spectroscopy, is stable in wate

220 Using (19) F magic-angle-spinning NMR spectroscopy, we obtained detai

221 ling experiments in conjunction with DNP and magic-angle-spinning NMR spectroscopy.

222 ir distribution function (PDF) analysis, and magic-angle-spinning NMR spectroscopy.

223 We used high-resolution magic-angle-spinning NMR studies on site-specific isotop

224 We propose a 19F spin diffusion magic-angle-spinning NMR technique to determine the olig

225 bility of dynamic nuclear polarization (DNP) magic-angle-spinning NMR techniques, along with a judici

226 y induced dynamic nuclear polarization) MAS (magic angle spinning) NMR demonstrates that indeed the p

227 at low temperature and high viscosity) MAS (magic angle spinning) NMR that both populations are pres

228 tion of solid-state (13)C-cross-polarization magic angle spinning nuclear magnetic resonance ((13)C-C

229 spectroscopy (XAS), (13)C Cross polarization-magic angle spinning nuclear magnetic resonance (CP-MAS

230 We show that high-resolution 17O magic angle spinning nuclear magnetic resonance (MAS NMR

231 mography, complemented with (27)Al and (31)P magic angle spinning nuclear magnetic resonance (MAS NMR

232 ration of multilamellar lipid vesicles using magic angle spinning nuclear magnetic resonance has been

233 9 kDa paramagnetic enzyme, using solid-state magic angle spinning nuclear magnetic resonance methods.

234 rphism based on sideband analyses of the 31P magic angle spinning nuclear magnetic resonance spectra.

235 ders of magnitude in length scale--including magic angle spinning nuclear magnetic resonance spectros

236 ructure of Nafion 211 using calibrated (19)F magic angle spinning nuclear magnetic resonance spectros

237 e matrix were investigated using solid-state magic angle spinning nuclear magnetic resonance spectros

238 (1)H HRMAS-NMR (High Resolution Magic Angle Spinning Nuclear Magnetic Resonance) spectro

239 ing a variety of techniques, including (31)P magic angle spinning nuclear magnetic resonance, and are

240 aracterized by solid-state (27)Al and (63)Cu magic angle spinning nuclear magnetic resonance.

241 Metabonomic analysis using 1H Magic Angle Spinning Nuclear Magnetic Resonsance (MAS-NM

242 we utilized state-of-the-art high-resolution magic-angle spinning nuclear magnetic resonance (HRMAS N

243 )3 NASICON series has been analyzed by (31)P magic-angle spinning nuclear magnetic resonance (MAS NMR

244 P dipolar heteronuclear correlation (HETCOR) magic-angle spinning nuclear magnetic resonance (NMR) is

245 Magic-angle spinning nuclear magnetic resonance is well

246 ion of ultrahigh magnetic field, solid-state magic-angle spinning nuclear magnetic resonance spectros

247 esicles were studied using (31)P solid-state magic-angle-spinning nuclear magnetic resonance spectros

248 (1)H High Resolution Magic Angle Spinning-Nuclear Magnetic Resonance (HRMAS-N

249 lies that are stable and are not affected by magic angle spinning of the samples at frequencies betwe

250 mellar liposomes using pulsed field gradient magic-angle spinning (PFG-MAS) (1)H NMR.

251 f the protein in combination with high-speed magic angle spinning produces (1)H resonances averaging

252 tatectomy were analyzed with high-resolution magic angle spinning proton magnetic resonance spectrosc

253 tate NMR measurements at very fast (100 kHz) magic-angle spinning rates and at high (23.5 T) magnetic

254 inescent scaffolds, (13)C cross-polarization magic angle spinning solid-state (CP-MAS) NMR spectrosco

255 In this study, we present a combined magic angle spinning solid-state and solution NMR study

256 Magic angle spinning solid-state NMR (MAS SSNMR) methods

257 We employ magic angle spinning solid-state NMR and other methods t

258 In addition, magic angle spinning solid-state NMR experiments carried

259 shift data and interhelical cross peaks from magic angle spinning solid-state NMR of a liposomal prep

260 is, FT-IR, UV-vis diffuse reflectance, (31)P magic angle spinning solid-state NMR spectroscopy, and p

261 Here, we describe (1)H-detected magic angle spinning solid-state NMR studies of monomeri

262 Here we present a magic angle spinning solid-state NMR study demonstrating

263 By using magic angle spinning solid-state NMR to investigate stab

264 t with dynamic nuclear polarization enhanced magic angle spinning solid-state NMR to study this chall

265 Raman spectroscopy, 31P magic angle spinning solid-state NMR, and pair distribut

266 Using advanced magic angle spinning solid-state NMR, we directly probe

267 g pulse sequences are of great importance in magic angle spinning solid-state NMR.

268 Magic-angle spinning solid-state NMR (SSNMR) studies of

269 guided by structure restraints obtained from magic-angle spinning solid-state NMR experimental data.

270 or dual data acquisition of multidimensional magic-angle spinning solid-state NMR experiments is pres

271 eled octasaccharide heparin analogue enabled magic-angle spinning solid-state NMR of the GAG bound to

272 ignments are presented for resonances in the magic-angle spinning solid-state NMR spectra of the majo

273 ntroduce an iterative approach that combines magic-angle spinning solid-state NMR spectroscopy and at

274 Here, we have used magic-angle spinning solid-state NMR spectroscopy to pro

275 oid fibrils in vitro, has been determined by magic-angle spinning solid-state NMR spectroscopy.

276 mical shift assignments of large proteins by magic-angle spinning solid-state NMR, using the 21-kDa d

277 studying its interactions with the capsid by magic-angle spinning solid-state NMR.

278 rotein structure determination methods using magic-angle spinning solid-state nuclear magnetic resona

279 itates rapid acquisition of multidimensional magic-angle spinning solid-state nuclear magnetic resona

280 n function (PDF) analysis and ex situ (23)Na magic-angle spinning solid-state nuclear magnetic resona

281 We present magic-angle-spinning solid-state NMR results of Ser31 an

282 We report magic-angle-spinning solid-state NMR results of the memb

283 Here we show that by using (7)Li magic-angle-spinning solid-state NMR spectroscopy, inclu

284 Using magic-angle-spinning solid-state NMR spectroscopy, we sh

285 Here we report on magic-angle-spinning solid-state NMR studies of the amyl

286 We used magic-angle-spinning solid-state NMR to determine the co

287 Magic-angle-spinning solid-state nuclear magnetic resona

288 stationary amides and "solution-like" (13)C magic angle spinning spectra at 75 degrees C, at which t

289 nding through comparative cross polarization magic-angle spinning spectra was also observed.

290 e-bound RTD-1 exhibits narrow line widths in magic-angle spinning spectra, but the sideband intensiti

291 re investigated using proton high-resolution magic angle spinning spectroscopy ((1)H HR-MAS).

292 IDH1-mutated tumors by (31)P high-resolution magic angle spinning spectroscopy.

293 e-dimensional CPMAS (cross-polarization with magic angle spinning) techniques, including spectral edi

294 we demonstrate through (13)C high-resolution magic-angle-spinning that (13)C acetate from fermentatio

295 with one being performed at high-resolution magic-angle spinning to obtain pure J-couplings without

296 bservable with single pulse excitation using magic angle spinning until the sample temperature reache

297 al shift anisotropy (CSA) is recoupled under magic-angle spinning using the SUPER technique to yield

298 onsidered essentially as a solid-state, slow-magic-angle-spinning version of the distortionless enhan

299 sional heteronuclear NMR in conjunction with magic-angle spinning, we have identified chemical bondin

300 (13)C chemical shift spectra obtained under magic-angle spinning were used evaluate the dehydration-