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 ed in a fully protonated sample with 100 kHz magic-angle spinning.

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

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

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

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

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

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

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

11 High-resolution magic-angle-spinning (1)H NMR spectroscopy (HR-MAS NMR)

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

27 Magic angle spinning at kHz frequencies restored resolut

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

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

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

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

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

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

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

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

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

37 opy and solid-state (13)C cross-polarization magic angle spinning (CP-MAS) NMR spectroscopy of the fr

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

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

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

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

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

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

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

45 solid-state NMR by (13)C cross-polarization magic angle spinning (CPMAS).

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

47 utilizing (13)C and (19)F cross-polarization magic-angle-spinning data are evaluated.

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

49 Gd(III) complex, [Gd(tpatcn)], doubling the magic-angle-spinning DNP enhancement of the previous sta

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

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

52 The development of magic-angle spinning dynamic nuclear polarization (MAS D

53 In recent years magic angle spinning-dynamic nuclear polarization (MAS-D

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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 A new in situ magic angle spinning (MAS) (7)Li nuclear magnetic resona

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

76 We demonstrate the performance of TIDE for magic angle spinning (MAS) [(13)C,(13)C]-DARR NMR spectr

77 proton-detected NMR spectroscopy under fast magic angle spinning (MAS) and dynamic nuclear polarizat

78 (1)H and (19)F afforded by 60 kHz ultrafast magic angle spinning (MAS) and enable the analysis of mi

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

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

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

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

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

84 longitudinal relaxation time (T(1e) ) during magic angle spinning (MAS) NMR by observation of DNP-enh

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

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

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

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

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

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

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

92 ombine solid-state (17)O, (27)Al, and (71)Ga magic angle spinning (MAS) NMR spectroscopy and density-

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

113 ons are supported by data from phosphorus-31 magic angle spinning (MAS) solid state NMR spectroscopy,

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

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

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

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

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

119 in (19)F dynamic nuclear polarization (DNP) magic angle spinning (MAS) spectra at 14.1 T on HIV-1 ca

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

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

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

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

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

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

126 By using solid-state NMR with fast magic-angle spinning (MAS) at high magnetic fields ((1)H

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

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

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

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

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

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

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

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

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

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

137 lear polarization (DNP)-enhanced solid-state magic-angle spinning (MAS) NMR in combination with light

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

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

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

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

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

143 loprotein from a powder sample, by combining magic-angle spinning (MAS) nuclear magnetic resonance (N

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

159 ovative combination of high-resolution (11)B magic-angle-spinning (MAS) and (105)Pd static solid-stat

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

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

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

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

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

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

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

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

168 ts were obtained by (1)H, (13)C, and (207)Pb magic angle spinning NMR and (14)N static NMR.

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

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

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

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

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

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

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

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

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

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

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

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

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

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

183 We employed solution and magic angle spinning NMR spectroscopy to characterize th

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

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

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

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

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

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

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

191 5-115), in its fibrillar form, determined by magic angle spinning NMR spectroscopy.

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

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

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

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

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

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

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

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

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

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

202 of capsid protein (CA) tubes, determined by magic-angle spinning NMR and data-guided molecular dynam

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

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

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

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

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

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

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

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

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

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

213 C) and pressures (79-89 bar) using operando magic-angle spinning NMR spectroscopy.

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

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

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

217 ture information obtained from near-complete magic-angle-spinning NMR assignments of the 39 kDa-large

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

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

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

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

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

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

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

225 gle X-ray scattering, and solid-state (19) F magic-angle-spinning NMR spectroscopy.

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

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

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

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

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

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

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

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

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

235 9 kDa paramagnetic enzyme, using solid-state magic angle spinning nuclear magnetic resonance methods.

236 (1)H high-resolution magic angle spinning nuclear magnetic resonance spectra

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

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

239 ric brain tumours using (1)H-High-Resolution Magic Angle Spinning nuclear magnetic resonance spectros

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

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

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

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

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

245 (31)P magic-angle spinning nuclear magnetic resonance (MAS NMR

246 )3 NASICON series has been analyzed by (31)P magic-angle spinning nuclear magnetic resonance (MAS NMR

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

248 Magic-angle spinning nuclear magnetic resonance is well

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

250 al shifts (CS) from solution and solid state magic-angle-spinning nuclear magnetic resonance (NMR) sp

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

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

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

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

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

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

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

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

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

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

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

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

263 sorption experiments, infrared spectroscopy, magic angle spinning solid-state NMR spectroscopy, and v

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

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

266 Here, we use multi-dimensional magic angle spinning solid-state NMR to characterize the

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

299 BMS) leads to broadening of resonances under magic angle spinning, we show that for monodisperse and

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