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 that behaves as a spring; some sections are inelastic and do not take part in the development of pas

6 quasi-particle diffusion coefficient and the inelastic and elastic scattering rates.

7 however, that the pyranose ring structure is inelastic and locked into a chair-like conformation.

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

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

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

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

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

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

14 ling opens up an electronically nonadiabatic inelastic channel, which competes substantially with rea

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

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

17 the energy range from 50 to 500 eV exhibited inelastic collision mean free paths of the order of a fe

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

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

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

21 Rotationally inelastic collisions of nitric oxide (NO) molecules with

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

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

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

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

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

27 For epoxy polymer, inelastic deformations also contributed heavily to measu

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

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

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

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

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

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

34 Inelastic electron tunneling spectra for an isolated ace

35 Inelastic electron tunneling spectroscopy (IETS) and cur

36 Inelastic electron tunneling spectroscopy (IETS) and OMT

37 Inelastic electron tunneling spectroscopy (IETS) has bec

38 Inelastic electron tunneling spectroscopy (IETS) has bee

39 ere observed with the aid of single-molecule inelastic electron tunneling spectroscopy (STM-IETS).

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

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

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 I propose that the detection mechanism is inelastic electron tunnelling.

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

55 ns (the 'atoms' of the system) interact with inelastic forces and enduring contacts.

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 stems over a range of hydration states using inelastic incoherent neutron scattering.

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

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 Inelastic light scattering by low-energy spin-excitation

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

66 Inelastic light scattering spectroscopy has, since its f

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

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

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

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

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

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

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

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

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

82 temperature programmed desorption (TPD), and inelastic neutron scattering (INS) measurements.

83 code has been applied to the analysis of the inelastic neutron scattering (INS) spectrum of an ionic

84 Inelastic neutron scattering (INS) studies on complex 1

85 Inelastic neutron scattering (INS) studies reveal that t

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

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

88 Inelastic neutron scattering and DFT calculations confir

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

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

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

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

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

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

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

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

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

98 High-resolution inelastic neutron scattering experiments on the cyanobac

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

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

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

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

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

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

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

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

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

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

109 Here we report inelastic neutron scattering observations of a magnetic

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

111 Inelastic neutron scattering results reveal that a large

112 Inelastic neutron scattering spectroscopy of the rotatio

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

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

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

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

117 A comprehensive inelastic neutron scattering study of magnetic excitatio

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

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

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

121 Here we use inelastic neutron scattering to characterize possible me

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

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

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

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

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

127 Inelastic neutron scattering was used to study the wave

128 By using inelastic neutron scattering we have collected a complet

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

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

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

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

133 Inelastic neutron scattering, density functional theory,

134 Inelastic neutron scattering, far-infrared spectroscopy,

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

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

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

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

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

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

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

142 prediction can be tested experimentally via inelastic neutron scattering.

143 a measurement of the magnetic form factor by inelastic neutron scattering; the data show that neutron

144 Here we employ inelastic neutron scatting measurements and density func

145 ervation has been confirmed unambiguously by inelastic neutron spectroscopy.

146 Inelastic neutron-scattering data reveal that the intens

147 omparison to available x-ray diffraction and inelastic neutron-scattering data shows that current gen

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

165 Body fat measurements by neutron inelastic scattering have shown a significant increase o

166 Vibrationally inelastic scattering is a fundamental collision process

167 Inelastic scattering is a fundamental collisional proces

168 = 3, j') products suggest that vibrationally inelastic scattering is the result of a frustrated react

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

170 We consider inelastic scattering of Gaussian wave packets with param

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

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

173 The dependence of vibrationally elastic and inelastic scattering on oxygen coverage strongly suggest

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

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

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

177 onic potential and in agreement with neutron inelastic scattering results.

178 ectroscopy of carbon using synchrotron x-ray inelastic scattering reveals that half of the pi-bonds b

179 Photon and neutron inelastic scattering spectrometers are microscopes for i

180 Elastic and inelastic scattering spectroscopy and electromagnetic si

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

182 idence in favour of long (10 micros or more) inelastic scattering times in nearly isolated dots.

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

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

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

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

187 ody potassium (TBK) measurements and neutron inelastic scattering.

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

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

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

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

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

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

194 l cells showed instances of both elastic and inelastic strain transmission, suggesting a role in obse

195 een growing muscle fibers and the relatively inelastic synaptic terminals that adhere to them causes

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

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

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

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

200 that, at long distances, the phonon-modified inelastic tunneling always dominates over the convention

201 ional microscopy from spatial imaging of the inelastic tunneling channels yielded additional data to

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

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

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

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

206 Combining inelastic tunneling spectroscopy, UV photoelectron spect

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

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

209 ement of normal mode calculations to nuclear inelastic x-ray absorption data from (nitrosyl)iron(II)t

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

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

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

213 We investigated the application of inelastic x-ray scattering (IXS) to lipid bilayers.

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

234 8 by means of excitation spectra of resonant inelastic X-ray scattering at the Ta L3 and L2 edges.

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

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

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

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

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

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

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

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

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

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

245 Inelastic X-ray scattering permitted the first quantitat

246 High-resolution resonant inelastic x-ray scattering revealed dispersive charge ex

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

248 Inelastic x-ray scattering spectroscopy can provide quan

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

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

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

252 s (DOS) of iron measured by nuclear resonant inelastic x-ray scattering to 153 gigapascals and calcul

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

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

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

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

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

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

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

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

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

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

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

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

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

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

267 ning a containerless sample environment with inelastic x-ray scattering.

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

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

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