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 apping, (3) contrast generation, as in turbo spin echo.

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

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

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

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

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

9 ate free precession (SSFP), single-shot fast spin-echo, 2D and 3D T1-weighted spoiled gradient-echo (

10 corresponding conventional morphologic turbo spin-echo 3-T sequences by three readers in consecutive

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

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

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

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

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

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

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

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

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

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

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

22 mpare our approach to ESPIRiT and SAKE using spin-echo and gradient echo MRI data from the human head

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

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

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

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

27 n groups 1-4, respectively) with T1-weighted spin-echo and T1 and T2 mapping to determine visual sign

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

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

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

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

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

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

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

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

36 pproximate duration, 3 minutes; five slices; spin-echo cardiac diffusion acquisition; b values, 0 and

37 phenomenon experimentally and also show that spin echo codes can be used for quantification.

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

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

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

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

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

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

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

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

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

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

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

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

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

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 measurements wer

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

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

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

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

57 Conclusion Gradient-echo spin-echo echo-planar imaging sequence provided quantita

58 Both were rated higher than the standard spin-echo echo-planar imaging.

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

63 Our X-ray absorption and electron spin echo envelope modulation (ESEEM) analyses strongly

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

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

66 Electron spin echo envelope modulation (ESEEM) experiments sugges

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

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

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

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

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

72 r, we observe a strong out-of-phase electron spin echo envelope modulation (OOP-ESEEM) signal from th

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

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

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

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

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

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

79 Electron spin echo envelope modulation spectroscopy establishes t

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

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

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

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

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

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

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

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

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

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

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

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

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

93 that set signal evolution during a train of spin echoes, especially with nonuniform echo spacing app

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

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

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

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

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

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

100 s described, based on the use of a modulated spin echo for the initial excitation.

101 Conclusion Both three-dimensional (3D) fast spin-echo (FSE) and 3D gradient-echo (GRE) sequences had

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

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

104 es, whereas all studies after 2011 used fast spin-echo (FSE) sequences.

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

106 e the cardiac application of a gradient-echo spin-echo (GESE) echo-planar imaging sequence for dynami

107 nducted at 1.5 T or 3.0 T using gradient and spin-echo (GRASE) or T2-prepared balanced steady-state f

108 2 half-Fourier acquisition single-shot turbo spin-echo (HASTE), spectrally attenuated inversion recov

109 Spin echoes have also been researched in dynamic decoupl

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

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

112 95 +/- 0.22; 164 slices; P<0.01), whereas T1 spin echo images showed no significant change.

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

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

115 5 degrees ) and T2-weighted single-shot fast spin-echo images (1501/80) were acquired.

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

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

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

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

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

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

122 nsverse relaxation were generated using fast spin echo imaging.

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

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

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

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

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

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

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

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

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

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

133 and a higher percentage of DPA+ voxels in T1 spin-echo lesions (odds ratio, 1.06; P = 0.036) were sig

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

135 We present in-situ neutron spin echo measurements on an entangled polydimethylsilox

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

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

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

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

140 ne of the real space measurement techniques, spin echo modulated small angle neutron scattering (SEMS

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

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

143 5-T single-slab three-dimensional (3D) turbo spin-echo MR image (1200/271) at the level of the right

144 5-T single-slab three-dimensional (3D) turbo spin-echo MR image (1200/271) at the level of the right

145 rresponding axial 1.5-T single-slab 3D turbo spin-echo MR image at the level of the left internal aud

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

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

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

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

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

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

152 9 years) underwent nine dynamic T1-weighted, spin-echo MR imaging studies, using intravenous, gadolin

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

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

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

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

157 assessed on ex vivo gradient echo and turbo spin echo MRI sequences and compared to findings on avai

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

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

160 luorescence spectroscopy and pulsed gradient spin echo NMR.

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

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

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

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

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

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

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

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

169 g a comprehensive approach-combining neutron spin-echo (NSE) spectroscopy, solid-state deuterium NMR

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

188 0.813), followed by TOF (r = 0.745) and fast spin-echo (r = 0.497) imaging.

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

190 : (a) Coronal T2-weighted fat-saturated fast spin-echo (repetition time msec/echo time msec, 2220/57;

191 : (a) Coronal T2-weighted fat-saturated fast spin-echo (repetition time msec/echo time msec, 2220/57;

192 : (a) Coronal T2-weighted fat-saturated fast spin-echo (repetition time msec/echo time msec, 2220/57;

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

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

195 g and monitoring breast cancer, but standard spin-echo (SE) echo-planar DWI methods often have poor i

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

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

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

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

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

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

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

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

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

205 y method for labeling and a single-shot fast spin echo sequence for image readout.

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

207 rearm, thigh, and calf were generated from a spin-echo sequence (repetition time msec/echo time msec,

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

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

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

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

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

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

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

215 using a black-blood T2-weighted radial fast spin-echo sequence in participants with CF.

216 C NMR spectra were acquired using a z-stored spin-echo sequence to achieve higher spectral quality, w

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

218 mpared with the T2-weighted single-shot fast spin-echo sequence, as established by quantitative and q

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

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

221 l shift-encoded Dixon sequence and multiecho spin-echo sequence.

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

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

224 I protocol including T2-weighted radial fast spin-echo sequence.

225 uorocarbon by using a three-dimensional fast spin-echo sequence.

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

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

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

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

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

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

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

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

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

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

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

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

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

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

240 with those obtained with conventional turbo spin-echo sequences.

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

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

243 Ramsey fringes and spin echo signals allow us to understand and improve qua

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

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

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

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

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

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

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

251 Using Neutron Spin Echo Spectroscopy (NSE), we have investigated the u

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

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

254 h temporal and spatial resolution of neutron spin echo spectroscopy to investigate the large-scale dy

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

256 ing, tracer-based microrheology, and neutron spin echo spectroscopy.

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

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

259 By combining helium spin-echo spectroscopy and density functional theory cal

260 yoglobin has been investigated using neutron spin-echo spectroscopy in different states: native-like,

261 Neutron spin-echo spectroscopy measurements revealed a large con

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

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

264 ination between T2-weighted single-shot fast spin-echo (SSFSE) and echo-planar imaging (EPI) fluid-at

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

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

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

268 ensive complementary neutron small-angle and spin-echo study directly showing the presence of signifi

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

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

271 Figure 2a: (a) Axial fast spin-echo T1-weighted MRI (496/8) and (b) axial reconstr

272 Figure 2b: (a) Axial fast spin-echo T1-weighted MRI (496/8) and (b) axial reconstr

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

274 eference standard single-section single-echo spin-echo T2 mapping sequences by using a Bland-Altman p

275 me msec, 11 000/125) MRI and (b) axial turbo spin-echo T2-weighted (3000/80) MRI of the brain through

276 me msec, 11 000/125) MRI and (b) axial turbo spin-echo T2-weighted (3000/80) MRI of the brain through

277 me msec, 11 000/125) MRI and (b) axial turbo spin-echo T2-weighted (3000/80) MRI of the brain through

278 me msec, 11 000/125) MRI and (b) axial turbo spin-echo T2-weighted (3000/80) MRI of the brain through

279 recovery (6000/120) MRI and (d) axial turbo spin-echo T2-weighted (5545/100) MRI through the same le

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

281 Figure 1c: (a) Coronal and (b, c) axial fast spin-echo T2-weighted MR images of the pelvis, with b be

282 Figure 1a: (a) Coronal and (b, c) axial fast spin-echo T2-weighted MR images of the pelvis, with b be

283 Figure 1b: (a) Coronal and (b, c) axial fast spin-echo T2-weighted MR images of the pelvis, with b be

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

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

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

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

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 (