ライフサイエンスコーパス: spin-echo

1 quences (including the benchmark multi-pulse spin echo).

2 concentrated solutions of mAbs using neutron spin echo.

3 lation double resonance) and heteronuclear J-spin-echoes.

4 imes higher than that with conventional fast spin-echo (0.12) and gradient-echo (0.19) MR imaging.

5 ly identify the same potential biomarkers as spin-echo (1)H NMR spectra in which broad lines are supp

6 oth T1- and T2-weighted spin-echo images (T1 spin echo, 20 axial slices per animal; T2 spin echo, 28

7 T1 spin echo, 20 axial slices per animal; T2 spin echo, 28 slices per animal).

8 s based on the acquisition of stimulated and spin echo 3D EPI images and was originally developed at

9 tion, myocardial edema (multiecho short-axis spin-echo acquisition), and myocardial fibrosis (Look-Lo

10 hnique with background suppression and turbo-spin-echo acquisition.

11 out degrading temporal resolution, ultrafast spin-echo acquisitions were implemented.

12 Fast spin-echo anatomic images were obtained, followed by seq

13 using Philips Achieva 1.5T device, including spin echo and gradient echo sequences with T1-, T2- and

14 um, the PET/MR protocol included T1-weighted spin echo and proton-density fat-saturated sequences in

15 We used T2-weighted two-dimensional fast spin echo and T1-weighted three-dimensional magnetizatio

16 Using a combination of electron spin echoes and proton spin manipulation, we showed that

17 th-hold coronal T2-weighted single-shot fast spin-echo and breath-hold coronal 3D T1-weighted spoiled

18 e and coronal half-Fourier single-shot turbo spin-echo and breath-hold oblique coronal heavily T2-wei

19 axial) structural imaging (T2-weighted turbo spin-echo and diffusion-weighted imaging), acquired with

20 freehand MR guidance predominantly with fast spin-echo and gradient-echo sequences.

21 rametric relaxation maps were generated from spin-echo and gradient-recalled-echo sequences.

22 mens, and investigated with T2-weighted fast spin-echo and multiecho spin-echo sequences on a 3.0-T M

23 other scattering frameworks such as neutron spin-echo and Raman spectroscopy.

24 ere imaged with endovaginal T2-weighted fast spin-echo and single-shot DW echo-planar MR imaging of t

25 images (including intermediate-weighted fast spin-echo and T2 mapping sequences), and the Physical Ac

26 d via water-saturation efficiency using fast spin-echo and T2-weighted images.

27 red RAGE sequence, as compared with the fast spin-echo and TOF sequences, demonstrated higher diagnos

28 wo-dimensional ) turbo spin-echo ( TSE turbo spin echo ) and 3D three-dimensional fast low-angle shot

29 quilibrium -prepared multicontrast TSE turbo spin echo , and 3D three-dimensional MSDE motion-sensiti

30 ton echoes, the orbital analogue of the Hahn spin echo, and Rabi oscillations familiar from magnetic

31 , spin-lock multiple gradient-echo, multiple spin-echo, and multiple gradient-echo sequences.

32 enuated inversion recovery, T2-weighted fast spin-echo, and T2*-weighted gradient-echo sequences.

33 PAI and T2-weighted spin-echo-based BOLD MR imaging were performed to assess

34 ual self-assembled InGaAs/GaAs quantum dots: spin-echo coherence times in the range 1.2-4.5 ms are fo

35 Magnetic resonance imaging included spin-echo coronal and sagittal imaging for meniscal scor

36 ) and Mo(*) maps were also created from fast spin echo data in a subset of pigs (n=5) to help charact

37 The CP-MAS and spin-echo data indicate discrete surface and core (77)Se

38 Using neutron spin-echo data up to a very high momentum transfer q ( a

39 sion of the Knight shift and the linear-in-T spin echo decay that increases with doping.

40 The spin echo decay time is ~40 mus, both with one and four

41 labeled on a single cysteine residue display spin-echo decays with a single phase-memory time T2M and

42 sonance (EPR) line shapes and nonexponential spin-echo decays, which undergo a transition to homogene

43 The observation of Rabi oscillations of the spin echo demonstrates the possibility to coherently man

44 dimethyls in commonly used nitroxides causes spin echo dephasing times (Tm) to be too short to perfor

45 Low-temperature spin-echo-detected EPR spectra of yeast Y* reveal an EPR

46 rease about 50-fold as indicated by electron spin-echo detection.

47 tant determined from a quantitative 1D (15N) spin-echo difference experiment for the C15/A27 interact

48 Using a 1H-205Tl spin-echo difference experiment we show that, in the Tl+

49 splanted kidneys were monitored by obtaining spin-echo diffusion-weighted MR images and gradient-echo

50 s infused in six normal rats and a series of spin-echo diffusion-weighted MR images was obtained at f

51 al ADC maps can be obtained in rats by using spin-echo diffusion-weighted MR imaging at 7 T.

52 Spin-echo diffusion-weighted MR imaging may have potenti

53 Spin-echo diffusion-weighted MR imaging measurements wer

54 thods, namely, the Carr-Purcell-Meiboom-Gill spin-echo, diffusion editing, and skyline projection of

55 ic resonance (MR) imaging protocol (sagittal spin-echo Dixon T2-weighted fat-only and water-only imag

56 protocol (sagittal spin-echo T1-weighted and spin-echo Dixon T2-weighted water-only imaging).

57 d rapid gradient echo T1-weighted, and turbo spin echo, dual-echo (proton density and T2 weighted) se

58 Precontrast single-shot spin-echo echo-planar diffusion-weighted images were obt

59 ADCs were measured with a spin-echo echo-planar sequence at five b values ranging

60 Electron spin echo electron paramagnetic resonance (ESE-EPR) spec

61 in membranous Na,K-ATPase is investigated by spin-echo electron paramagnetic resonance.

62 n spin-echo envelope modulation and electron spin-echo-electron nuclear double resonance to the struc

63 These data together with data from electron spin echo envelope modulation (ESEEM) allowed to model t

64 Two- and four-pulse electron spin echo envelope modulation (ESEEM) and four-pulse two

65 resonance (ESR) experiments such as electron spin echo envelope modulation (ESEEM) and hyperfine subl

66 oides have been characterized using electron spin echo envelope modulation (ESEEM) and hyperfine subl

67 on paramagnetic resonance (EPR) and electron spin echo envelope modulation (ESEEM) experiments have b

68 The standardized intensity of the electron spin echo envelope modulation (ESEEM) from (2)H-hyperfin

69 pair [P700+ A1-] and the associated electron spin echo envelope modulation (ESEEM) have been studied

70 Electron spin echo envelope modulation (ESEEM) spectral results i

71 oxygenase (TauD) was measured using electron spin echo envelope modulation (ESEEM) spectroscopy.

72 Variable-frequency electron spin echo envelope modulation (ESEEM) studies of this sp

73 The three-pulse electron spin echo envelope modulation (ESEEM) technique was used

74 pin interactions using out-of-phase electron spin echo envelope modulation (OOP-ESEEM).

75 two magnetic resonance techniques: electron-spin echo envelope modulation and Overhauser dynamic nuc

76 nt (RIDME) technique to measure the electron spin echo envelope modulation caused by the dipole inter

77 Two-dimensional electron spin echo envelope modulation has been applied to explor

78 ed nitrogens determined from S-band electron spin echo envelope modulation spectra identify them as N

79 The two-dimensional electron spin echo envelope modulation spectra of uniformly 15N-l

80 Electron spin echo envelope modulation spectroscopy establishes t

81 Mn2+ by using a rapid freeze-quench-electron spin echo envelope modulation technique.

82 environment through two-dimensional electron spin echo envelope modulation, and characterized functio

83 We also observe electron spin echo envelope modulations of the Mn(2+) signal due

84 cilitate its assignment, the C-band electron spin-echo envelope modulation (ESEEM) spectra of lpH SO

85 on paramagnetic resonance (EPR) and electron spin-echo envelope modulation (ESEEM) spectroscopic prop

86 uclear double resonance (ENDOR) and electron spin-echo envelope modulation (ESEEM) spectroscopies, ca

87 terized by using X-band three-pulse electron spin-echo envelope modulation (ESEEM) spectroscopy in th

88 acterized by using X-band two-pulse electron spin-echo envelope modulation (ESEEM) spectroscopy in th

89 Electron spin-echo envelope modulation (ESEEM) spectroscopy is a

90 is explored with (87)Sr three-pulse electron spin-echo envelope modulation (ESEEM) spectroscopy.

91 clear double resonance (ENDOR), and electron spin-echo envelope modulation (ESEEM) studies on the Cu(

92 Electron spin-echo envelope modulation (ESEEM) was used to search

93 nd multitechnique (continuous-wave, electron spin-echo envelope modulation (ESEEM), pulsed electron-n

94 pply the pulsed EPR technologies of electron spin-echo envelope modulation and electron spin-echo-ele

95 Results from electron spin-echo envelope modulation and electron-nuclear doubl

96 stem II has been investigated using electron spin-echo envelope modulation spectroscopy in the presen

97 l of Mn2+ in this site using ESEEM (electron spin-echo envelope modulation) spectroscopy.

98 we have conducted an EPR and ESEEM (electron spin-echo envelope modulation) study of D1-D170H PSII pa

99 the manganese cluster, measured by electron spin-echo envelope modulation, prompted us to examine wh

100 in the coherent spin precession observed in spin-echo envelope modulation.

101 tion by X-band EPR, S-band EPR, and electron spin-echo envelope spectroscopy, demonstrates coordinati

102 paramagnetic resonance techniques [electron-spin-echo (ESE)-EPR/electron nuclear double resonance/ES

103 btained in a heteronuclear and a homonuclear spin-echo experiment, S(Q)(tau) = S(HET)(tau)/S(HOM)(tau

104 d (13)C signal in a heteronuclear (1)H/(13)C spin-echo experiment.

105 gnature of the 1 MHz defect in a time-domain spin-echo experiment.

106 (19)F spin echo experiments using the Carr-Purcell-Meiboom-Gil

107 easily by using amplitude-modulated 1D (1)H spin-echo experiments with selective inversion of the (1

108 ngth and time regimes appropriate to neutron spin-echo experiments, the results of Zilman and Granek

109 nerves were imaged with a fat-saturated fast spin echo (FSE) sequence and a magnetization transfer se

110 al fat-suppressed intermediate-weighted fast spin-echo (FSE) (repetition time msec/echo time [TE] mse

111 ow-SAR optimized three-dimensional (3D) fast spin-echo (FSE) and fluid-attenuated inversion-recovery

112 ted gradient-echo (GRE) and T2-weighted fast spin-echo (FSE) MR imaging before and after SPIO enhance

113 a new isotropic three-dimensional (3D) fast spin-echo (FSE) pulse sequence with parallel imaging and

114 aging by using morphologic (T1-weighted fast spin-echo [FSE], T2-weighted FSE, proton density [PD]-we

115 Spin echoes have also been researched in dynamic decoupl

116 In contrast, the helium-3 spin-echo (HeSE) technique achieves spatial and time res

117 those conditions presenting with T1 weighted spin echo hyperintensity within the central nervous syst

118 95 +/- 0.22; 164 slices; P<0.01), whereas T1 spin echo images showed no significant change.

119 Abdominal MRI scans (axial T1-weighted spin echo images) were taken, from which adipose tissue

120 ensity-weighted 2D two-dimensional TSE turbo spin echo images, as well as T1-weighted 3D three-dimens

121 5 degrees ) and T2-weighted single-shot fast spin-echo images (1501/80) were acquired.

122 abdominal aortas on both T1- and T2-weighted spin-echo images (T1 spin echo, 20 axial slices per anim

123 was measured on T2-weighted single-shot fast spin-echo images by one of six radiologists (1-3 years o

124 Measurements were made on single-shot fast spin-echo images by tracing free-form regions of interes

125 by using sagittal two-dimensional multiecho spin-echo images of the right knee.

126 fusion-weighted, and multiecho gradient-echo/spin-echo images were acquired; cerebral blood flow and

127 rsion recovery, T2-weighted, and T1-weighted spin-echo images.

128 lanced fast field-echo and T2-weighted turbo spin-echo images.

129 , and respiratory-triggered T2-weighted fast spin-echo images.

130 gradient-recalled echo and T2-weighted fast spin-echo images.

131 T1- and T2-weighted (W) black blood spin echo imaging was performed in 1 axial slice, and th

132 nsverse relaxation were generated using fast spin echo imaging.

133 llel lines with enhanced reconstruction fast spin-echo imaging (T2 method), and gradient-echo imaging

134 cluded thick- and thin-slab single-shot fast spin-echo imaging and transverse fast spin-echo imaging.

135 bust, but visualization of myocardial fat by spin-echo imaging is less reliable.

136 using T1- and T2-weighted and proton-density spin-echo imaging sequences.

137 Spin-echo imaging was used to define contrast-enhanced r

138 re evaluated by using ultrashort-TE imaging, spin-echo imaging, histopathologic analysis, and PLM, wi

139 t fast spin-echo imaging and transverse fast spin-echo imaging.

140 ed RAGE imaging; 70%, 92%, and 0.63 for fast spin-echo imaging; and 56%, 96%, and 0.57 for TOF imagin

141 al MR sequences: unenhanced T2-weighted fast spin-echo imaging; unenhanced diffusion-weighted imaging

142 agnitude of signal intensity reduction on T2 spin echo in vivo images further correlated with macroph

143 etermined from the temperature dependence of spin-echo intensities at a pulse spacing of 200 ns agree

144 MR imaging was fat suppressed fast spin echo intermediate or T2 weighted (repetition time m

145 emization were followed by selective, double spin-echo inversion-recovery (1)H NMR spectroscopy over

146 zation-prepared RAGE (kappa = 0.53) and fast spin-echo (kappa = 0.42) sequences yielded moderate agre

147 hically gated variable flip angle (VFA) fast spin-echo magnetic resonance (MR) angiography technique

148 al-enhanced, double inversion-recovery, fast spin-echo magnetic resonance (MR) images were acquired t

149 Three-dimensional fast spin-echo magnetic resonance images were acquired at 7 T

150 rates between approximately 30-140 K, and by spin-echo measurements of the enhancement of spin-spin r

151 ouble-quantum (DQ) (19)F MAS NMR spectra and spin-echo measurements provided additional information a

152 f imager type (ANCOVA F value=1.4, P=.24) or spin-echo method (P=.67, Wilcoxon test) on number of les

153 cardiographically gated partial-Fourier fast spin-echo methods and balanced steady-state free precess

154 et al.--from pixel-by-pixel fittings of the spin-echo modulation for the 2D correlation peaks due to

155 entation as phylloquinone, and out-of-phase, spin-echo modulation spectroscopy shows the same P700(+)

156 to that of the wild type, and out-of-phase, spin-echo modulation spectroscopy shows the same P700(+)

157 A fast recovery fast spin echo MR sequence was selected for high RF power, an

158 ow-signal-intensity structure on T1-weighted spin-echo MR and MR arthrographic images.

159 Black-blood fast spin-echo MR images allow morphologic assessment of the

160 loss of signal intensity on T2-weighted fast spin-echo MR images obtained with fat saturation compare

161 Sequential T1-weighted spin-echo MR images were acquired in 10 rats to assess l

162 ties (n = 126) on intermediate-weighted fast spin-echo MR images were categorized into four subgrades

163 With use of sagittal single-shot fast spin-echo MR images, the cecal tilt angle was calculated

164 was correlated only with fat-saturated fast spin-echo MR imaging (r = 0.76, P < .01); the relative s

165 T1-weighted spin-echo MR imaging and MR arthrography in standard ima

166 ative least squares algorithm from multiecho spin-echo MR imaging data.

167 T1-weighted spin-echo MR imaging of 48 lesser MTP joints of 12 cadav

168 9 years) underwent nine dynamic T1-weighted, spin-echo MR imaging studies, using intravenous, gadolin

169 ccurately quantified with fat-saturated fast spin-echo MR imaging than with out-of-phase gradient-ech

170 r fat quantification with fat-saturated fast spin-echo MR imaging was significantly better than it wa

171 After 24 hours, Gadomer-enhanced T1-weighted spin-echo MR imaging was used to define microvascular ob

172 Spin-echo MR imaging was used to monitor changes in myoc

173 ho and triple-dose post-contrast T1-weighted spin echo MRI scans.

174 S who were scanned with STIR and T1-weighted spin-echo MRI of the whole spine.

175 ion mass spectrometry, pulsed field gradient spin echo NMR measurements, electrochemical analysis, an

176 luorescence spectroscopy and pulsed gradient spin echo NMR.

177 asurements obtained by pulsed field gradient spin-echo NMR and chronoamperometry, the backfolded dend

178 amolecules was determined by pulsed-gradient spin-echo NMR and modeled with molecular force field sim

179 Pulsed gradient spin-echo NMR experiments show that the clusters remain

180 Pulsed-gradient spin-echo NMR is often the method of choice because it m

181 ned by a variable-temperature solid-state 2D spin-echo NMR spectroscopic study.

182 Pulsed gradient spin-echo NMR spectroscopy was used in place of the prev

183 X-ray scattering), PGSE-NMR (pulsed-gradient spin-echo NMR), fluorescence quenching, and electrospray

184 ing, surface tensiometry, and pulse-gradient spin-echo NMR.

185 s comparable to that using Neutron Resonance Spin Echo (NRSE) coils.

186 -angle neutron scattering (SANS) and neutron spin echo (NSE) spectroscopy were used to measure the te

187 a new approach based on Oscillating Gradient Spin-Echo (OGSE) MRI methods that can differentiate the

188 ave analyzed a series of MAS 1H NMR spectra (spin-echo, one-dimensional, and diffusion-edited) and 31

189 area); (ii) optic nerve proton density fast spin-echo (optic nerve proton density-lesion length); (i

190 Pulsed gradient spin echo (PGSE) is a well-known NMR technique for deter

191 with those obtained from the pulse gradient spin echo (PGSE) NMR method.

192 ious water, and was shown by pulsed gradient spin-echo (PGSE) NMR experiments to adopt a dinuclear st

193 cence spectroscopy and pulsed field gradient spin-echo (PGSE) NMR spectroscopy in combination with so

194 e glass transition, display heterogeneity in spin-echo phase-memory time and a stronger inhomogeneous

195 men by using highly resolved proton-density (spin-echo proton density) and gradient-recalled-echo (GR

196 Whole-brain 3D fast spin-echo pseudocontinuous ASL images were acquired at 3

197 rformed using noncontrast (T2-weighted turbo spin echo pulse sequence) and gadolinium-diethylene tria

198 ho-weighted images were obtained with a fast spin-echo pulse sequence for comparison.

199 with a standard T1-weighted two-dimensional spin-echo pulse sequence of the brain at 1.5 T.

200 d from images acquired by using a mixed fast spin-echo pulse sequence that was implemented with respi

201 tic resonance (MR) imaging with a mixed fast spin-echo pulse sequence were assessed.

202 modified three-dimensional fast large-angle spin-echo pulse sequence.

203 ance frequency of 200 MHz (4.7 T) using a 3D spin-echo pulse sequence.

204 -electron spin states were demonstrated, and spin-echo pulse sequences were used to suppress hyperfin

205 imaging system, intermediate-weighted turbo spin-echo pulse sequences, and MR-conditional needles, d

206 ained--using the REINE (REfocused INADEQUATE spin-Echo) pulse sequence presented by Cadars et al.--fr

207 0.813), followed by TOF (r = 0.745) and fast spin-echo (r = 0.497) imaging.

208 ation was performed with localized adiabatic spin-echo refocusing (LASER) by using adiabatic gradient

209 Thick-slab single-shot fast spin-echo (repetition time msec/echo time msec, 4,500/94

210 Sequential T1-weighted spin echo sagittal and axial sections were obtained and

211 h the following pulse sequences: T1-weighted spin echo (SE), intermediate-weighted fast SE, fat-suppr

212 state (SPGR), and two-dimensional (2D) fast spin echo (SE)-for evaluating articular cartilage in the

213 T1-weighted spin-echo (SE) and fat-suppressed gradient-echo (GE) seq

214 large vessel contribution using the improved spin-echo (SE) BOLD method but with overall decreased se

215 nal (2D) gradient-recalled echo (GRE) and 2D spin-echo (SE) echo-planar imaging (EPI) magnetic resona

216 C), and on-resonance water-suppression turbo spin-echo (SE) images with PC were obtained before and a

217 Purpose To (a) evaluate modified spin-echo (SE) magnetic resonance (MR) elastographic seq

218 Ventricular wall thickening was measured on spin-echo (SE) MR images.

219 D) single- and multisection black-blood fast spin-echo (SE) sequences.

220 l noncontiguous T2-weighted single-shot fast spin-echo (SE) sequences; transverse fat-suppressed T2-w

221 and different inversion times and a multiple spin-echo (SE) technique with different echo times to me

222 T1-weighted fast spin-echo (SE), fat-suppressed T2-weighted fast SE, in-

223 was performed before injection (T1-weighted spin-echo [SE] and T2-weighted fast SE acquisitions) and

224 nsional [2D] gradient-echo [GRE] imaging, 2D spin-echo [SE] echo-planar imaging, and three-dimensiona

225 ing sequences (an intermediate-weighted fast spin-echo [SE] sequence and a spoiled gradient-echo [GRE

226 ghted turbo gradient-echo, T1-weighted turbo spin-echo [SE], and T2-weighted single-shot SE sequences

227 were scanned with a diffusion-weighted fast spin echo sequence at 78 mum isotropic voxels.

228 of the needle tip was confirmed with a fast spin-echo sequence (1904/4.5, 36-cm field of view).

229 T, T2 mapping was performed with a multiecho spin-echo sequence (repetition time msec/echo times msec

230 onance (MR) imaging and a diffusion-weighted spin-echo sequence (spatial resolution, 50 x 100 x 800 m

231 ere acquired with a standard pulsed-gradient spin-echo sequence (Stejskal-Tanner) in a clinical 3-T s

232 The fast spin-echo sequence and the fat-saturated SPGR sequence a

233 ndwidth were applied by using the warp turbo-spin-echo sequence at 1.5 T.

234 a water excitation SPGR sequence, and a fast spin-echo sequence at 3.0 T and a fat-saturated SPGR seq

235 A double gated (respiration and cardiac) spin-echo sequence at 9.4T was used to evaluate whole lu

236 R imaging at 3 T, including a dual-echo fast spin-echo sequence, a T1-weighted volume sequence, and a

237 f half Fourier acquisition single-shot turbo spin-echo sequence, cine, and T2-weighted images as well

238 ancement by Carr-Purcell-Meiboom-Gill (CPMG) spin-echo sequence.

239 e and T2 mapping using a hybrid gradient and spin-echo sequence.

240 surface coil and a dynamic single-shot fast spin-echo sequence.

241 rated, T2-weighted (T2w) and dual echo turbo spin echo sequences as well as a 3D T2-weighted, fat-sat

242 Arterial spin labeling and asymmetric spin echo sequences measured CBF and OEF, respectively,

243 , using three-dimensional T(2)-weighted fast-spin echo sequences, before doing invasive autopsy.

244 sonance (MR) imaging has been performed with spin-echo sequences and spoiled gradient-echo sequences.

245 ter excitation, fat-saturated SPGR, and fast spin-echo sequences at 3.0 T and the fat-saturated SPGR

246 ance (MR) imaging unit with T2-weighted fast spin-echo sequences immediately after, as well as 2 and

247 ith T2-weighted fast spin-echo and multiecho spin-echo sequences on a 3.0-T MR imaging unit.

248 e imaging (MRI) according to the acquisition Spin-Echo sequences T1 and T2.

249 ld oblique coronal heavily T2-weighted turbo spin-echo sequences were performed.

250 R examinations consisted of multiplanar fast spin-echo sequences with similar tissue contrast at 1.5

251 l half-Fourier acquisition single-shot turbo spin-echo sequences, balanced steady-state free precessi

252 d spoiled gradient-echo and T2-weighted fast spin-echo sequences, three-dimensional very short TE seq

253 ired by this search we introduce a family of spin-echo sequences, which can still detect site-specifi

254 rse and coronal T2-weighted single-shot fast spin-echo sequences.

255 overy, and sagittal T1- and T2-weighted fast spin-echo sequences.

256 limitations) by using five single-shot turbo spin-echo sequences.

257 ne were within 5% for both gradient-echo and spin-echo sequences.

258 roton-density-weighted two dimensional turbo-spin-echo sequences; voxel size: 0.4 x 0.3 x 3.5 mm(3) )

259 We observed hundreds of spin echo signals lasting for more than 600 milliseconds

260 years) were obtained with diffusion-weighted spin-echo single-shot echo-planar MR imaging.

261 Quadrupolar spin-echo solid-state (2)H NMR spectroscopy, in combinat

262 polarization magic angle spinning and (77)Se spin-echo solid-state NMR for Cd(77)Se quantum dots.

263 methods demonstrating the compressibility of spin-echo spectra are presented for several measurements

264 in previously presented 2D z-filtered (31)P spin-echo spectra.

265 ct surface dynamical processes with a helium spin-echo spectrometer for the first time.

266 n parameters using Grazing Incidence Neutron Spin Echo Spectroscopy (GINSES), where an evanescent neu

267 Using neutron spin echo spectroscopy (NSE), we show salt-concentration

268 We report a measurement by neutron spin echo spectroscopy of the diffusion of hemoglobin in

269 Using Neutron Spin Echo Spectroscopy we observed fragment motion on a

270 Using neutron spin-echo spectroscopy (NSE), normal mode analysis, and

271 ns in proteins is the application of neutron spin-echo spectroscopy (NSE).

272 Neutron spin-echo spectroscopy measurements revealed a large con

273 Neutron spin-echo spectroscopy provides a means to study membran

274 Neutron spin-echo spectroscopy was used to study structural fluc

275 tion of heavily T2-weighted single-shot fast spin-echo (SSFSE) images and three-dimensional (3D) grad

276 and speed improvements for single-shot fast spin-echo (SSFSE) with variable refocusing flip angles a

277 ily T2-weighted [TR 2000 ms; TE-200 ms] fast spin echo study in coronal and sagittal planes.

278 to that with the standard protocol (sagittal spin-echo T1-weighted and spin-echo Dixon T2-weighted wa

279 urated (FS) and non-fat-saturated (NFS) fast spin-echo T1-weighted imaging (T1 method), FS and NFS T2

280 lts, we show that the angular information in spin-echo T2 is consistent with this model.

281 by using axial and coronal single-shot fast spin-echo T2-weighted images obtained at 1.5 T.

282 phased-array MR imaging (ie, unenhanced fast spin-echo T2-weighted imaging and gradient-echo T1-weigh

283 The imaging protocol included fast spin-echo T2-weighted MR imaging, breath-hold DW echo-pl

284 fibrosis using semiquantitative T2-weighted spin echo, T2 mapping, and T1 mapping before and 3 and 1

285 vise a space-time analogue of the well-known spin echo technique, yielding insight into decoherence m

286 materials at atomic sized resolution and the spin-echo technique opens up the possibility of compress

287 aches that use the recently developed helium spin-echo technique to measure surface potential energy

288 interferometric beam modulation utilizing a spin-echo technique.

289 Spin-echo techniques have been used to mitigate the hype

290 d MR imaging, including two-dimensional fast spin-echo, three-dimensional time-of-flight (TOF), and t

291 Two-dimensional ( 2D two-dimensional ) turbo spin-echo ( TSE turbo spin echo ) and 3D three-dimension

292 recovery gradient echo (IR-GRE), T(1)-turbo spin echo (TSE), and T(2)-TSE images were acquired befor

293 ormed at 1.5T and included T2-weighted turbo spin-echo (TSE) and diffusion-weighted (DW) images acqui

294 e precession (SSFP) cine sequences and turbo spin-echo (TSE) black-blood (BB) sequences was evaluated

295 ated (FS) proton density (PD)-weighted turbo spin-echo (TSE) imaging in the detection of bone marrow

296 and an unenhanced coronal T1-weighted turbo spin-echo (TSE) sequence for bone analysis.

297 sing-flip-angle three-dimensional (3D) turbo spin-echo (TSE) sequence was modified to acquire both in

298 electron spin coherence time without use of 'spin echo'-type techniques.

299 ially available sequences (gradient echo and spin echo) were acquired during quiet breathing in six p

300 iplicative acceleration factor from multiple spin echoes (x32) and compressed sensing (CS) sampling (