ライフサイエンスコーパス: inelastic

1 ible to increases in price (i.e., were more "inelastic").

2 More than half the nurses applying the inelastic (38 [56%]) and elastic (36 [53%]) bandages obt

3 which corresponds to mainly physiologically inelastic A-band part of the protein, and for a proteoly

4 Here, we show that an inelastic aerogel made of single-walled carbon nanotubes

5 during holidays when SSB demand may be more inelastic, and 2) aggregated posttax time points to addr

6 The main aspects of stereodynamics in inelastic atom-molecule collisions can often be understo

7 pressures ranged from 11 mm Hg exerted by an inelastic bandage to 80 mm Hg exerted by a 2-component b

8 dage, and 27 of 68 nurses (40%) applying the inelastic bandage.

9 ternal stress fields, are fundamental to the inelastic behavior of solids.

10 dispersion of the acoustic-like branch from inelastic (Brillouin) light scattering experiments under

11 his effect indicates a low contribution from inelastic carrier-impurity or phonon-impurity scattering

12 systems of spherical particles due either to inelastic clustering or persistent density inhomogeneity

13 cited states up to approximately 20 meV, and inelastic co-tunnelling.

14 it treatment of the elasticity of the limbs, inelastic collision between a soft body and rigid surfac

15 we show here that in the simplest case of an inelastic collision between an atom and a nearly homonuc

16 ses have been limited to the modification of inelastic collisions and chemical reactions.

17 gration emerges spontaneously as a result of inelastic collisions between neighboring cells: collisio

18 served in such systems when agitation causes inelastic collisions between particles.

19 al potential energy surface (PES) that HF-HF inelastic collisions do not obey the energy and angular

20 Inelastic collisions involving molecular species are key

21 -that, in part, they result from stochastic, inelastic collisions of ejecta and coalescence of partia

22 imulations, fully incorporating friction and inelastic collisions, are designed to reproduce experime

23 the stented limbs indicates that elastic or inelastic compression support of the successfully stente

24 An inelastic cross-section of 60.3 +/- 2.1 mb is measured f

25 a unified theoretical framework that bridges inelastic crystalline defects and elastic deformations o

26 These simulations predict that non-uniform inelastic deformation over larger areas and increased en

27 ks slide relative to each other, propagating inelastic deformation over millimeter length scales.

28 The relative resistance to inelastic deformation, measured via the ratio of nanoind

29 es invading non-altruistic populations under inelastic density regulation.

30 y was examined between choices classified as inelastic, elastic, and suppressed demand, operationaliz

31 The method can also be applied to inelastic electron or neutron scattering.

32 oltage, indicative of vibrational heating by inelastic electron scattering.

33 ory G protein-coupled receptors occurs by an inelastic electron tunneling mechanism that is mediated

34 s increased by vibrational excitation via an inelastic electron tunneling process.

35 between the two proteins in conductance and inelastic electron tunneling spectra at <|0.5 V| bias vo

36 Inelastic electron tunneling spectroscopy (IETS) and cur

37 Inelastic electron tunneling spectroscopy (IETS) has bec

38 Inelastic electron tunneling spectroscopy (IETS) has bee

39 molecular vibrations provides the basis for inelastic electron tunneling spectroscopy.

40 ectra of these structures were measured with inelastic electron tunneling spectroscopy.

41 e thermally activated motion is nondirected, inelastic electron tunneling triggers rotations, where t

42 attering, neutrons, low-energy electrons and inelastic electron tunnelling are powerful techniques th

43 this technique, current-voltage analysis and inelastic electron tunnelling spectroscopy (IETS) demons

44 and conductance-voltage characteristics, and inelastic electron tunnelling spectroscopy, we attribute

45 wise or anticlockwise direction by selective inelastic electron tunnelling through different subunits

46 laser pulse, and exploit the sensitivity of inelastic electron-light scattering to changes in the ma

47 all superhelices show elastic, plastic, and inelastic elongation regimes and undergo a dynamic trans

48 oped a method to capture the electron-phonon inelastic energy exchange in real time and have used it

49 show that a colossal synergy occurs between inelastic energy loss and pre-existing atomic defects cr

50 ions with solids is well known to result in inelastic energy loss to electrons and elastic energy lo

51 y-Rideal reaction mechanism and accounts for inelastic energy losses commensurate with surface re-ion

52 This phenomenon is explained with an inelastic excitation mechanism, whereby hydrogen atoms i

53 al-organic complexes were formed by means of inelastic excitations in a scanning tunneling microscope

54 e characterized by singlet-triplet spin-flip inelastic excitations with an effective exchange couplin

55 and farm prices rise sharply in the face of inelastic food demands.

56 ing is universally observed in vibrationally inelastic H + D(2) collisions over a broad range of cond

57 We present elastic and inelastic incoherent neutron scattering data from a seri

58 Here we describe the first inelastic incoherent neutron scattering spectroscopy stu

59 We have previously used inelastic incoherent neutron scattering spectroscopy to

60 features are presumably attributable to the inelastic inter-band electron-electron scattering origin

61 ures for different dissipation mechanisms of inelastic inter-particle collisions.

62 electron system of SiC by energetic ions via inelastic ionization can effectively anneal pre-existing

63 leigh/Mie), while the second channel detects inelastic light scattering (Raman) or fluorescence.

64 e of Zeeman energies, and appear in resonant inelastic light scattering experiments as well-defined r

65 Inelastic light scattering spectroscopy has, since its f

66 e have a crucial role as quantum pathways in inelastic light scattering, and this is exemplified by r

67 In the quantum mechanical picture of inelastic light scattering, incident photons first excit

68 s hot luminescence, which is another form of inelastic light scattering, results from excited-state r

69 portunities to probe, manipulate and utilize inelastic light scattering.

70 Resonant inelastic light-scattering spectra reveal low-lying tran

71 atomic gases in the lattice by measuring the inelastic loss of doublons.

72 ree- and four-body features are found in the inelastic-loss spectrum.

73 Inelastic losses in molecular collisions(2-5), however,

74 Here we report inelastic magnetic neutron-scattering measurements that

75 This scenario fully explains the observed inelastic magnetic response of alpha-RuCl3 and reveals t

76 d uncertainties that remain in regard to the inelastic mean free path of photoelectrons in aqueous me

77 alculated photoionization cross sections and inelastic mean free paths or experimentally.

78 ray photon energies and thus larger electron inelastic mean-free paths should provide a more accurate

79 Cells are wrapped in inelastic membranes, yet they can sustain large mechanic

80 ind a lower bound on the ratio of elastic to inelastic molecule-atom collisions that is greater than

81 e converted into protons through elastic and inelastic (n,p) interactions.

82 low-energy spin fluctuations is revealed by inelastic neutron measurements.

83 The lattice dynamics has been studied by inelastic neutron or X-ray scattering.

84 ies reported include: magnetic measurements, inelastic neutron scattering (including single crystal m

85 distribution function (PDF) (100-503 K) and inelastic neutron scattering (INS) (5-450 K), respective

86 Inelastic neutron scattering (INS) is uniquely sensitive

87 Inelastic neutron scattering (INS) studies on complex 1

88 Inelastic neutron scattering (INS) studies reveal that t

89 R), near-ambient pressure XPS (NAP-XPS), and inelastic neutron scattering (INS)) were applied to dete

90 ies, including magnetic measurements, powder inelastic neutron scattering (INS), and DFT calculations

91 h both spin-excitations in PLCCO measured by inelastic neutron scattering (resonance mode) and a low-

92 Inelastic neutron scattering and DFT calculations confir

93 desorption spectroscopy, Raman measurements, inelastic neutron scattering and first principles calcul

94 In addition, inelastic neutron scattering and frequency-domain Fourie

95 ts dispersion curves as measured by coherent inelastic neutron scattering and inelastic X-ray scatter

96 otational degrees of freedom, as revealed by inelastic neutron scattering and infrared spectroscopy.

97 on chemical shifts and demonstrate that deep inelastic neutron scattering and solid-state nuclear mag

98 ements of the low-frequency vibrations using inelastic neutron scattering and terahertz time-domain s

99 Quasi-elastic and inelastic neutron scattering are used to probe the dynam

100 response RNA are also used to backcalculate inelastic neutron scattering data that match previous in

101 Here we show that four-dimensional inelastic neutron scattering enables us to portray entan

102 arity to natural hydrates is confirmed using inelastic neutron scattering experiments and synchrotron

103 High-resolution inelastic neutron scattering experiments on the cyanobac

104 ns of single crystal neutron diffraction and inelastic neutron scattering experiments we shed light o

105 been achieved, using neutron diffraction and inelastic neutron scattering experiments, coupled with d

106 ned experimentally (3.1 kcal mol(-)(1)) from inelastic neutron scattering experiments, is in reasonab

107 Ideal probes of these excitations are inelastic neutron scattering experiments.

108 in conjunction with neutron diffraction and inelastic neutron scattering instruments allowing in sit

109 vibrational dynamics of water as measured by inelastic neutron scattering is presented.

110 including electrical transport measurements, inelastic neutron scattering measurement, and first-prin

111 Using a combination of inelastic neutron scattering measurements and first-prin

112 itu synchrotron X-ray diffuse scattering and inelastic neutron scattering measurements from a prototy

113 -resolution time-of-flight quasi-elastic and inelastic neutron scattering measurements in a wide ener

114 Here, by performing inelastic neutron scattering measurements on a supercond

115 We present inelastic neutron scattering measurements on hydrogen in

116 neutron scattering data that match previous inelastic neutron scattering measurements on larger and

117 Here we report inelastic neutron scattering observations of a magnetic

118 Here we report inelastic neutron scattering results for HgBa(2)CuO(4+de

119 Inelastic neutron scattering results reveal that a large

120 Two-magnon Raman scattering and inelastic neutron scattering reveal a superexchange cons

121 In situ neutron diffraction and inelastic neutron scattering revealed that confined nick

122 erms, temperature programmed desorption, and inelastic neutron scattering spectroscopy show the exist

123 upon H2 dissociation over ceria via in situ inelastic neutron scattering spectroscopy.

124 Neutron diffraction and inelastic neutron scattering studies enable the direct o

125 In situ powder X-ray diffraction and inelastic neutron scattering studies, combined with mode

126 By a thorough single-crystal inelastic neutron scattering study, we demonstrate that

127 oride Cs2AgF4, using magnetic susceptometry, inelastic neutron scattering techniques and both X-ray a

128 Using both neutron powder diffraction and inelastic neutron scattering techniques, we find that MI

129 Here we employ state-of-the-art inelastic neutron scattering to comprehend the full thre

130 Here we use inelastic neutron scattering to demonstrate that the res

131 e we exploit state-of-the-art single-crystal inelastic neutron scattering to directly measure for the

132 MOF-8, IRMOF-11, and MOF-177 were studied by inelastic neutron scattering to gain information on the

133 Here, we use inelastic neutron scattering to show that low-energy spi

134 Here we use inelastic neutron scattering to study magnetic fluctuati

135 High-resolution inelastic neutron scattering was used to identify major

136 By using inelastic neutron scattering we have collected a complet

137 rthermore, vibrational spectra (infrared and inelastic neutron scattering) were recorded and compared

138 Single-crystal neutron diffraction, inelastic neutron scattering, and density functional cal

139 try, specific heat measurements, elastic and inelastic neutron scattering, and density functional the

140 agnetization and specific heat measurements, inelastic neutron scattering, and electron paramagnetic

141 Inelastic neutron scattering, density functional theory,

142 Inelastic neutron scattering, far-infrared spectroscopy,

143 nsition in SnS and SnSe are investigated via inelastic neutron scattering, high-resolution Raman spec

144 luding powder X-ray and neutron diffraction, inelastic neutron scattering, infrared spectroscopy, and

145 Novel experimental techniques, such as deep inelastic neutron scattering, now provide a detailed vie

146 metal rings, using magnetic measurements and inelastic neutron scattering, supported by density funct

147 Combining contrast matching approaches with inelastic neutron scattering, we isolate the bending mod

148 hed for electron-phonon anomalies in LSNO by inelastic neutron scattering.

149 OH was confirmed using X-ray diffraction and inelastic neutron scattering.

150 e-stripe correlations, in La2-xSrxNiO4 using inelastic neutron scattering.

151 2), which have been successfully revealed by inelastic neutron scattering.

152 stent with dipolar interactions, as seen for inelastic neutron scattering.

153 prediction can be tested experimentally via inelastic neutron scattering.

154 accessing the cellular water dynamics using inelastic neutron scattering.

155 ate binding interactions have been probed by inelastic neutron scattering.

156 investigate uranyl fluoride (UO(2)F(2)) with inelastic neutron scattering.

157 Here we employ inelastic neutron scatting measurements and density func

158 Combining in situ neutron diffraction, inelastic neutron spectroscopy, density functional theor

159 ervation has been confirmed unambiguously by inelastic neutron spectroscopy.

160 Inelastic neutron-scattering data reveal that the intens

161 Here we report inelastic neutron-scattering experiments that reveal bot

162 integral and differential cross sections for inelastic NO-He collisions in the 0.2 to 8.5 centimeter(

163 the determination of spectral parameters in inelastic optical scattering.

164 d opens a door to detailed investigations of inelastic or reactive processes.

165 in principle that the setup can be used for inelastic phonon line-width measurements.

166 appropriate vibrational state to accept the inelastic portion of the tunneling electron's energy.

167 sonic beam, we have studied the rotationally inelastic process wherein deuterium hydride (HD) (v = 1,

168 During eruptions, inelastic processes including magma mush erosion and the

169 nable dipolar interactions dominate over all inelastic processes.

170 Here we present the first measurement of the inelastic proton-proton interaction cross-section at a c

171 ering resonance features in both elastic and inelastic rate coefficients at collision energies below

172 and holes generated by plasmon decay, before inelastic relaxation, using a quantized plasmon model wi

173 deformable to large elastic strains without inelastic relaxation.

174 g elastic response ([Formula: see text] ns), inelastic reorganization ([Formula: see text] ns), and s

175 The elastic and inelastic response of [001] oriented silicon to laser co

176 h rapid assays, however, we observe that the inelastic response shows significant changes and can be

177 Moreover, a near-isotropic inelastic response was observed when we analyzed indenta

178 ineered blood vessels have largely relied on inelastic scaffolds or biological solutions with uncerta

179 ligand binding has been monitored by Nuclear Inelastic Scattering (NIS), also called Nuclear Resonant

180 condensed history scheme, i.e., catastrophic inelastic scattering and Bremsstrahlung events are simul

181 is due to unfavourable ratios of elastic to inelastic scattering and impractically slow thermalizati

182 ta were collected to resolve the elastic and inelastic scattering components in the diffuse scatterin

183 eV, and therefore we conclude that increased inelastic scattering counteracts increased amplitude con

184 Here, we show through neutron inelastic scattering experiments that the PNRs can also

185 ndependently-occurs nonlocally upon resonant inelastic scattering from single atomic defects at graph

186 Vibrationally inelastic scattering is a fundamental collision process

187 Inelastic scattering is a fundamental collisional proces

188 = 3, j') products suggest that vibrationally inelastic scattering is the result of a frustrated react

189 Elastic and inelastic scattering measurements reveal the quantum mec

190 Nuclear inelastic scattering of (57)Fe labeled [NiFe] hydrogenas

191 We consider inelastic scattering of Gaussian wave packets with param

192 By measuring the inelastic scattering of light, Raman spectroscopy is abl

193 erential cross-sections for the rotationally inelastic scattering of NO(X2Pi1/2, v=0, j=0.5, f) by Ar

194 ional nondispersing intensity comes from the inelastic scattering of the outgoing photoelectron.

195 lying spectroscopic effect is the incoherent inelastic scattering of two photons on the vibrational q

196 neutral-neutral collisions: we find that the inelastic scattering process H + D(2)(v = 0, j = 0, 2) -

197 cross sections (DCSs) for the vibrationally inelastic scattering process H + o-D(2)(v = 0, j = 0,2)

198 with diminished kinetic energy; that is, the inelastic scattering process is essentially a frustrated

199 dence long-range static ferromagnetic order, inelastic scattering shows that short-range correlated a

200 simulations of the momentum- and real-space inelastic scattering signals from a linear cyanotetracet

201 Photon and neutron inelastic scattering spectrometers are microscopes for i

202 Elastic and inelastic scattering spectroscopy and electromagnetic si

203 th gate-modulated and laser-energy dependent inelastic scattering spectroscopy.

204 e rotational and parity states of v = 10 for inelastic scattering studies.

205 and magnetic correlations using elastic and inelastic scattering techniques.

206 ciated with low KE electrons, very low or no inelastic scattering, and effective pumping and the desi

207 by a strong transient signal in small-angle inelastic scattering, and nuclear structural changes (ri

208 energy distribution, as measured by neutron inelastic scattering, is only slightly altered.

209 anthracene-based emitters in the MOF through inelastic scattering, leading to efficient generation of

210 conventional quasiparticle dynamics, such as inelastic scattering, or hydrodynamic collective motion

211 ase at a higher rate than phase contrast and inelastic scattering.

212 advances have taken place is in rotationally inelastic scattering.

213 amorphous-crystal interfaces exhibit unique inelastic shear (slip) transfer characteristics, fundame

214 , long-stretch, single-component bandage; an inelastic, short-stretch, single-component bandage; and

215 rowth and developmental delay and redundant, inelastic skin, is caused by mutations in the a2 subunit

216 n characterized by redundant, pendulous, and inelastic skin.

217 n characterized by redundant, pendulous, and inelastic skin.

218 Thermodynamics, and realized here using an 'inelastic thermal collimator' element.

219 creasing rotation angle, but the elastic and inelastic torsion stiffnesses are remarkably different.

220 al in achieving high efficiency or power via inelastic transport and without relying on heavy-element

221 n be improved by nanostructures that exploit inelastic transport processes.

222 duced by applying an electric field or using inelastic tunneling electrons from a scanning tunneling

223 Here we use the inelastic tunneling probe (itProbe) to acquire real-spac

224 We constructed an inelastic tunneling probe based on the scanning tunnelin

225 An application of the inelastic tunneling probe reveals the sharing of hydroge

226 The relative intensities of the inelastic tunneling processes are consistent with dipola

227 Combining inelastic tunneling spectroscopy, UV photoelectron spect

228 We show that inelastic tunnelling leads to the characteristic dip-hum

229 ical results on the selection of altruism in inelastic viscous homogeneous populations, namely that n

230 We have performed inelastic X-ray and neutron scattering experiments that

231 ultrafast dynamics in condensed matter using inelastic X-ray scattering (IXS) is described.

232 Here, we use causality-inverted inelastic x-ray scattering (IXS) to image the charge-tra

233 nation of X-ray absorption and 1s3p resonant inelastic X-ray scattering (Kbeta RIXS) allows Co(IV) to

234 pic technique, namely core-level nonresonant inelastic X-ray scattering (NIXS).

235 Operando nuclear resonant inelastic X-ray scattering (NRIXS) and X-ray absorption

236 We report nonresonant inelastic X-ray scattering (NRIXS) measurement of core-s

237 es comparing spectra measured by nonresonant inelastic X-ray scattering (NRIXS), a bulk-sensitive tec

238 Valence-to-core resonant inelastic X-ray scattering (RIXS) and high energy resolu

239 Recent resonant inelastic X-ray scattering (RIXS) experiments in hole-do

240 Here, we carry out resonant inelastic x-ray scattering (RIXS) experiments on Gd x Sc

241 Data from Kalpha resonant inelastic X-ray scattering (RIXS) have been used to extr

242 Time-resolved resonant inelastic X-ray scattering (RIXS) is one of the developi

243 Resonant inelastic X-ray scattering (RIXS) measurements at the ac

244 pairing for superconductivity; and resonant inelastic X-ray scattering (RIXS) provides a considerabl

245 ere we combine X-ray absorption and resonant inelastic X-ray scattering (RIXS) spectroscopies to reso

246 bility of indirect K -edge bimagnon resonant inelastic X-ray scattering (RIXS) spectrum as a viable e

247 orption spectroscopy (XAS) and 1s2p resonant inelastic X-ray scattering (RIXS) to study oxyhemoglobin

248 Resonant inelastic X-ray scattering (RIXS) was used to collect Mn

249 the realization of high resolution resonant inelastic X-ray scattering (RIXS) with a stable ultrasho

250 ray emission spectroscopy (XES) and resonant inelastic X-ray scattering (RIXS).

251 tain L-edge like data through 1s2p resonance inelastic X-ray scattering (RIXS).

252 ray emission spectroscopy (XES) and resonant inelastic X-ray scattering (RIXS).

253 measurements made at room temperature using inelastic X-ray scattering and neutron scattering techni

254 opy, X-ray absorption spectroscopy, resonant inelastic X-ray scattering and neutron scattering to dem

255 The technique, based on inelastic X-ray scattering and the principle of detailed

256 ) alloy using in situ high-energy resolution inelastic X-ray scattering and X-ray diffraction.

257 Here, we implement magnetic resonant inelastic X-ray scattering at a free-electron laser to d

258 ts ultrafast dynamics accessed with resonant inelastic X-ray scattering at the N 1s level using synch

259 8 by means of excitation spectra of resonant inelastic X-ray scattering at the Ta L3 and L2 edges.

260 Using inelastic X-ray scattering beyond the dipole limit and h

261 th neutron diffraction and then via resonant inelastic X-ray scattering determine the salient electro

262 ed in aqueous solution using high-resolution inelastic x-ray scattering down to molecular length-scal

263 In this paper we present inelastic X-ray scattering experiments in a diamond anvi

264 We performed inelastic x-ray scattering experiments on crystals of gr

265 GeO2 at ambient temperature was measured by inelastic x-ray scattering from ambient pressure up to p

266 temperatures up to 1700 kelvin with nuclear inelastic x-ray scattering in a laser-heated diamond anv

267 by coherent inelastic neutron scattering and inelastic X-ray scattering in different thermodynamic co

268 Synchrotron inelastic x-ray scattering measurements of oxygen K-edge

269 city of liquid Fe84C16 up to 70 GPa based on inelastic X-ray scattering measurements.

270 Here we use resonant inelastic X-ray scattering over a wide temperature range

271 Inelastic X-ray scattering permitted the first quantitat

272 the spectral and momentum resolution of the inelastic X-ray scattering spectrometers along with a ma

273 combination of x-ray absorption and resonant inelastic x-ray scattering spectroscopy, how the Coulomb

274 soft X-ray absorption spectroscopy, resonant inelastic X-ray scattering spectroscopy, X-ray absorptio

275 Here we report a high resolution inelastic X-ray scattering study of the in-plane phonon

276 both structures using the momentum-dependent inelastic X-ray scattering technique.

277 ture-dependent X-ray absorption and resonant inelastic X-ray scattering techniques.

278 Here the authors use resonant inelastic X-ray scattering to demonstrate that the theor

279 Here we use resonant inelastic X-ray scattering to follow the evolution of ch

280 Using inelastic X-ray scattering to probe the boron and nitrog

281 We used inelastic x-ray scattering to probe the phonon dispersio

282 Combining resonant inelastic X-ray scattering with detailed modelling, we d

283 Inelastic X-ray scattering with meV energy resolution (I

284 In addition, resonant inelastic X-ray scattering with unprecedented energy res

285 he oxygen K-edge, metal L-edge, and resonant inelastic X-ray scattering, are discussed.

286 agnetic excitation gap, measured by resonant inelastic x-ray scattering, is quite different between t

287 e combine three spectroscopic tools-resonant inelastic X-ray scattering, photoluminescence and optica

288 Here we demonstrate, using resonant inelastic X-ray scattering, that optimally hole-doped su

289 y diffraction, a phase-sensitive analogue to inelastic X-ray scattering, to measure the corresponding

290 determined previously using nuclear resonant inelastic X-ray scattering, were used to calculate the s

291 Here we use resonant inelastic X-ray scattering, which is sensitive to comple

292 evaluated for the first time by nonresonant inelastic X-ray scattering, X-ray absorption spectroscop

293 died a highly stoichiometric magnetite using inelastic X-ray scattering, X-ray diffraction and emissi

294 y absorption spectroscopy, and 1s2p resonant inelastic X-ray scattering.

295 d the nature of pre-edge lines identified by inelastic X-ray scattering.

296 alpha-plutonium and find good agreement with inelastic x-ray scattering.

297 erved from optical spectroscopy and resonant inelastic X-ray scattering.

298 sample at an X-Ray free electron laser using inelastic X-ray scattering.

299 ion conditions using (57)Fe nuclear resonant inelastic X-ray scattering.

300 ith XANES, soft X-ray spectroscopy, resonant inelastic X-ray spectroscopy, and Raman spectroscopy.