ライフサイエンスコーパス: momentum

1 cluster, should not be able to impress real momentum.

2 ctrons, which can also carry orbital angular momentum.

3 lical wave front and carries orbital angular momentum.

4 outflow tract, with consequent loss of flow momentum.

5 lutions for functional TR has gained greater momentum.

6 uch as vortex beams carrying orbital angular momentum.

7 persion as a function of electron transverse momentum.

8 , wherein electron spins are locked to their momentum.

9 exture with spin locked at right angles with momentum.

10 anes can provide the air inflow with angular momentum.

11 nucleus rotates about the principal axis of momentum.

12 ks, which do not exhibit dispersion with the momentum.

13 nd intrapocket paired state with finite pair momentum.

14 liptical orbits with nonzero orbital angular momentum.

15 us targeting systems is increasingly gaining momentum.

16 ing effect which correlates spin with linear momentum.

17 iffraction and from the beam orbital angular momentum.

18 metries in their bandgaps and offset crystal momentums.

19 The MOMENTUM 3 trial (Multicenter Study of MagLev Technology

20 In this secondary analysis of the MOMENTUM 3 trial, the HM3 LVAS demonstrated greater free

21 do-crystal geometry that equally distributes momentum across elements.

22 rticles have their spin, or internal angular momentum, aligned either parallel or antiparallel with t

23 asmonic vortex are determined by the angular momentum (AM) of the light, and the geometrical topologi

24 guerre-Gaussian lasers, with orbital angular momentum and characterized by doughnut-shaped intensity

25 t in establishing the initial conditions for momentum and energy transfer to the environment as the p

26 c states in a material as a function of both momentum and energy, providing central insights into str

27 and surface influences the transfer of mass, momentum and energy.

28 The momentum and heat transport in rarefied gas flows is kno

29 heir bond length, vibrational state, angular momentum and orientation in a small electric field.

30 entanglement of the optical orbital angular momentum and radial profile degrees of freedom possessed

31 the generation of broadband orbital angular momentum and radially polarized beams.

32 e increase of fractal dimension reduces both momentum and thermal boundary layers, meanwhile extends

33 y harmonic phonons should only carry crystal momentum and, while impinging on the cluster, should not

34 heoretical results indicate that transfer of momentum and/or heat from the bubbles to the cells are t

35 d globally, this planning process is gaining momentum, and some plans are taking early shape.

36 igh-resolution method for measuring the full momentum- and energy-resolved electronic spectral functi

37 experimental timescales, allowing subsequent momentum- and spin-resolved in situ probing of the SOC b

38 Immunotherapy is gathering momentum as a primary therapy for cancer patients.

39 Virus-based therapies have gained momentum as the next generation of treatments for a vari

40 position coordinates and three components of momentum, as continuous variables.

41 rienced a revival of interest and scientific momentum, as the pharmaceutical industry has come to app

42 extrinsic components of the photon's angular momentum at short-wavelengths.

43 from simultaneous conservation of energy and momentum at the interface to essentially evaluate GB/int

44 d retraction, the substrate imparts vertical momentum back to the droplet with a springboard effect,

45 we show that Bessel-Gaussian orbital-angular-momentum beams are more tolerant to obstructions than no

46 obstructions than non-Bessel orbital-angular-momentum beams.

47 enon, resulting from the transfer of angular momentum between interacting light and matter in which t

48 olar-interaction-induced transfer of angular momentum between the J=0 and J=1 internal particle level

49 t only does the beam contain orbital angular momentum but can trivially be converted to a radially po

50 -body dynamics of the acquisition of angular momentum by a gas of ultracold bosons in two dimensions

51 , trions can radiatively decay with non-zero momentum by kicking out an electron, resulting in an asy

52 ind stress modulates the air-sea transfer of momentum by providing a sink of mesoscale eddy energy as

53 rks (COFs) has recently gathered significant momentum by the virtue of their predictive design, contr

54 ghts the importance of tuning of the angular momentum compensation point of ferrimagnets, which could

55 s is realized in ferrimagnets at the angular momentum compensation point TA.

56 on capacity is achieved through position and momentum complementarity.

57 hat pseudospin can turn into orbital angular momentum completely, thus upholding the belief that pseu

58 distributions of the sum of the two electron momentum components along the direction of the polarizat

59 esponding to the discrete orbital and radial momentum components of the light field.

60 ergy is proposed by virtue of the energy and momentum conservation equations.

61 Angular momentum conservation follows immediately.

62 trong exciton binding may assist in parallel momentum conservation in CT exciton formation.

63 eter-scale surface deformation by exploiting momentum conservation of the interaction between laser l

64 odelled in the weakly nonlinear regime using momentum conservation of the self-collimated beams in th

65 ice which can be well explained by the quasi-momentum conservation rule.

66 The law of momentum conservation rules out many desired processes i

67 ive fluids in two spatial dimensions without momentum conservation, and growing one-dimensional inter

68 ism is an extremely tiny violation of energy-momentum conservation, which can, in principle, be detec

69 viscosity of the fluid, which is governed by momentum-conserving internal collisions.

70 late devices empower spin to orbital angular momentum conversion and vector polarization formation, w

71 it leads to unequal spin to orbital angular momentum conversion in magneto-optic media evanescent wa

72 ized through the formation of higher angular momentum Cooper pairs, with Fermi surface nodes in the p

73 The momentum correlation between the bromine ions in a three

74 We report a measurement of the transverse momentum correlation between two photons by detecting on

75 We quantify the transverse momentum correlation by analyzing the visibility of this

76 n be extremely unequal, leading to novel e-e momentum correlation spectra that can be measured experi

77 The experimentally determined momentum correlations and the isomer-resolved fragment-i

78 The induced ferromagnetic momentum couples with conduction electrons generating un

79 Here, we report the observation of a spin-momentum coupling achieved by loading a Bose-Einstein co

80 show that transverse-spin to orbital angular momentum coupling into magneto-optic waveguide media eng

81 The realization of spin-momentum coupling with lattice bands as pseudospins pave

82 The quantum emulation of spin-momentum coupling, a crucial ingredient for the emergenc

83 h entangled polarisation and orbital angular momentum degrees of freedom.

84 ion of nonreciprocal transverse-spin angular-momentum-density shifts for evanescent waves in magneto-

85 Its momentum dependence and spin texture imply an intimate c

86 whose dispersions exactly follow the energy-momentum dependence calculated by a Hubbard model with s

87 ation using the electronic structure and the momentum dependence of the -wave superconducting gap det

88 ling further drives a rich three-dimensional momentum dependence of the underlying Fermi-surface spin

89 Combining photon-energy and momentum dependent RIXS measurements with theoretical ca

90 an additional moving lattice that induces a momentum-dependent coupling between the two pseudospins,

91 es into account the shape, spin texture, and momentum-dependent propagation of the Fermi arc surface

92 ation of the Dirac fermions is locked to the momentum direction.

93 with linear energy dispersion in all (three) momentum directions.

94 ess Dirac fermions (MDFs) with linear energy-momentum dispersion (1, 2) , providing a condensed-matte

95 Electrons with a linear energy/momentum dispersion are called massless Dirac electrons

96 materials are characterized by linear energy-momentum dispersion near band crossing points.

97 e is manifested in the characteristic energy-momentum dispersion relation studied in photoluminescenc

98 ng phenomena, such as a graphene-like energy-momentum dispersion, Bloch oscillations, or the Hofstadt

99 in one direction) while maintaining a sharp momentum distribution (the hallmark of superfluid Bose-E

100 tituents is decisive and the spatial and the momentum distribution of one electron depends on those o

101 We found that the momentum distribution of the impurity exhibits character

102 A diagnostic of the momentum distribution shows that a quasi-Bragg splitter

103 lived coherent oscillations in the fermionic momentum distribution, with a period that is determined

104 e well), and was not an artifact of residual momentum during intermittent gyration.

105 istry, metal-containing polymers have gained momentum during recent decades.

106 ate that the distribution of orbital angular momentum entanglement over more than 100 km of free spac

107 plification of this latter result provides a momentum equation containing three dominant forces: (a)

108 diffusion coupled with the fluctuating fluid momentum equation result in enhanced charge transport vi

109 ions act as transistor-like, angle dependent momentum filters, whereas triangular networks act as sta

110 s can be corrected by modifying the downward momentum flux to the surface.

111 A comparison between the heat and momentum fluxes during 5 days of a dry CAP episode in Fe

112 ference of Parties (COP21) agreement renewed momentum for action against climate change, creating the

113 fore urgently needed to maintain the current momentum for control and elimination of this disease.

114 Our results provide exciting new momentum for developing mGluR1-based pharmacology to tre

115 During the scattering event, the momentum [Formula: see text] is transferred by the wave

116 ntrol over the conversion of optical angular momentum from spin to orbital form in a metasurface syst

117 a large lunar inclination and remove angular momentum from the Earth-Moon system.

118 ad, the primary cause was waves transporting momentum from the Northern Hemisphere.

119 enhancement of cultivated peanut has gained momentum from the sequenced genomes of the diploid ances

120 ated by adult stem cell therapy has gathered momentum fueled by tantalizing clues and visionary goals

121 Given the momentum gained toward polio eradication, these resource

122 , but supports the high-energy, high-angular-momentum giant impact model for the origin of the Moon.

123 evolution model supports recent high-angular-momentum, giant-impact scenarios to explain the Moon's i

124 and elimination has been achieved and policy momentum has been generated through continued bilateral,

125 energy drop as the function of reduced quasi-momentum has never been challenged in a spin-preserving

126 on laws, such as those of charge, energy and momentum, have a central role in physics.

127 n-commuting observables such as position and momentum Heisenberg's uncertainty principle limits the i

128 botic pancreatoduodenectomy (RPD) is gaining momentum; however, its impact on major outcomes, includi

129 oling times for hexagonal BN, where the high-momentum hyperbolic phonon polaritons enable efficient n

130 the genetic causes of ID has recently gained momentum, identification of pathogenic mutations that ca

131 information from the widely applied Coulomb momentum imaging method.The timescale of isomerization i

132 its Dirac-like spin texture by spin-filtered momentum imaging.

133 ct and therefore a high-energy, high-angular-momentum impact.

134 shifts and quantum weak measurements of the momentum in a vortex wavefunction.

135 However, the true dynamics of angular momentum in finite, interacting many-body systems like t

136 uestions such as the conservation of angular momentum in highly nonlinear light-matter interactions,

137 gate the conservation of the orbital angular momentum in necklace and elliptical rotating beams.

138 Vortices are essential to angular momentum in quantum systems such as ultracold atomic gas

139 The concept of hypofractionation is gaining momentum in radiation oncology centres, enabled by recen

140 for exciting applications of orbital angular momentum in the nanoworld.

141 As a result, full blood momentum in the outflow tract is used to facilitate earl

142 and treatment on quality of life have gained momentum in the past 10 years.

143 parasites of phytoplankton has been gaining momentum in the past few years.

144 the electronic mode fell to zero at nonzero momentum, indicating dynamical slowing of plasma fluctua

145 We conclude that only angular momentum induced optically by the inverse Faraday effect

146 In this work, the axial jet separator, a new momentum interface, is characterized by theory and empir

147 microcavity polariton dispersion, which has momentum intervals with positive and negative group velo

148 guration of the orbital and internal angular momentum into a high spin ([Formula: see text]) state; t

149 flows are thought to deposit gas and angular momentum into the circumgalactic medium, creating disk-

150 s of vortex nucleation and show that angular momentum is hidden in phantom vortices modes which so fa

151 nor that of the excitation; rather, angular momentum is introduced by the particle's interaction wit

152 As the probe bunch traverses the wake, its momentum is modulated by the electric field of the wake,

153 The wave angular momentum is transferred to floating micro-particles, gui

154 the propagation of a pair of electrons with momentum k and -k has a log singularity as the temperatu

155 r parallel or antiparallel with their linear momentum, labelled as left and right chirality, respecti

156 We find a nonlinear growth relation of the momentum layer, but a linear one of the thermal layer, w

157 xcite electrons to states far above the spin-momentum locked Dirac cone and the underlying mechanism

158 electronic properties because of their spin-momentum locked Dirac-cone-like band structure.

159 pabilities to study Bloch oscillations, spin-momentum locking and Van Hove singularities in the trans

160 argue that this remarkable signature of spin-momentum locking can only be observed in multi-terminal

161 s and photons can respectively have the spin-momentum locking effect which correlates spin with linea

162 tector magnetization indicate that hole spin-momentum locking follows the right-hand rule, opposite t

163 observe spin polarization arising from spin-momentum locking in both cases, with opposite signs of t

164 Spin-momentum locking in protected surface states enables eff

165 e Dirac point by electrically detecting spin-momentum locking in surface states of a p-type TI, Sb2Te

166 tion against backscattering through the spin-momentum locking mechanism.

167 he large spin-orbit interaction and the spin-momentum locking of the topological insulator surface gr

168 This spin-momentum locking property gives rise to very interesting

169 e of the spin signal is consistent with spin-momentum locking property of surface states of SmB6.

170 harge current flowing in a channel with spin-momentum locking such as topological insulator surface s

171 heory for an arbitrary 2D channel with "spin momentum locking" due to spin-orbit coupling.

172 Because of spin-momentum locking, changing light propagation direction r

173 enerates a net spin polarization due to spin-momentum locking, which is electrically detected as a vo

174 spin flow relative to the direction of spin-momentum locking.

175 ly dispersing Dirac surface states with spin-momentum locking.

176 n Hall effect-surface modes with strong spin-momentum locking.

177 ted to propagate through the bulk when their momentum matches that of the surface projections of the

178 However, the requirement of momentum matching along the metasurface sets its nontriv

179 ) transitions are designed to achieve smooth momentum matching and highly efficient spoof SPP mode co

180 radiatively inactive (dark) due to spin and momentum mismatch between the constituent electron and h

181 we show the transmission of orbital angular momentum modes of light over a distance of 143 km betwee

182 carry a quantized amount of orbital angular momentum (OAM) and have become important in various fiel

183 Electron waves that carry orbital angular momentum (OAM) are characterized by a quantized and unbo

184 visible light beams carrying orbital angular momentum (OAM) are currently thoroughly studied for thei

185 and transmitting four green orbital angular momentum (OAM) beams through a single aperture.

186 These elements-SAM-to-orbital angular momentum (OAM) converters-are based on the geometric pha

187 ectromagnetic waves carrying orbital angular momentum (OAM) have been used for mode division multiple

188 Exact eigen modes with orbital angular momentum (OAM) in the complex media of unmagnetized homo

189 The effective generation of orbital angular momentum (OAM) lasing, especially at a micro- and nanosc

190 be realized using synthetic orbital angular momentum (OAM) lattices in degenerate cavities.

191 ff-axis points with discrete orbital angular momentum (OAM) modes is investigated.

192 received interest is that of orbital angular momentum (OAM) modes.

193 t is even more important for orbital angular momentum (OAM) multiplexing systems since misalignment b

194 analyzing the change in the orbital angular momentum (OAM) of a tilted light beam eclipsed by a movi

195 unication approach using the orbital angular momentum (OAM) of acoustic vortex beams with one order e

196 ng methods for measuring the orbital-angular-momentum (OAM) spectrum suffer from issues such as poor

197 Orbital angular momentum (OAM) state of photons offer an attractive addi

198 ltichannel superpositions of orbital angular momentum (OAM) states with various topological charges.

199 ptical vortices, which carry orbital angular momentum (OAM), can be flexibly produced and measured wi

200 ese light beams, which carry orbital angular momentum (OAM), have been successfully utilized in the v

201 We explore the use of orbital-angular-momentum (OAM)-multiplexing to increase the capacity of

202 any surface is the pressure generated by the momentum of impinging photons.

203 s doublet and quartet with effective angular momentum of J eff = 1/2 and 3/2, respectively.

204 governs the interactions between the angular momentum of photons and the magnetic order parameter of

205 The equations governing the angular momentum of the ball relative to the point of contact wi

206 For example, to minimize spin (angular momentum of the body) at takeoff, plant-sucking bugs app

207 e and allow an organism to anticipate to the momentum of the day.

208 llows them to interact with the spin angular momentum of the impinging light field.

209 rs for a length of time short enough for the momentum of the incoming phonon to be conserved.

210 No phonon scattering occurs and the momentum of the phonons released by the defect is unrela

211 s released by the defect is unrelated to the momentum of the phonons that generated the excitation.

212 ora of applications based on orbital angular momentum or vector polarization, such as optical sensing

213 success of therapeutic inhibitors and gained momentum over the past few years.

214 ey move with their group velocity, with real momentum, part of which is transmitted to the adsorbate

215 an experimentally obtained anti-correlation momentum pattern at higher intensities is reproduced wit

216 ametrized by the lower limit of the electron momentum - pmin - is critical for estimating the total e

217 le, and [Formula: see text] is a microscopic momentum-preserving scattering rate.

218 theory, however, pairs can exist with finite momentum Q, thus generating a state with a spatially mod

219 nsisting of a graph-theoretic description of momentum (reciprocal) space and a complementary group-th

220 Dirac materials are characterized by energy-momentum relations that resemble those of relativistic m

221 ransport is conventionally determined by the momentum-relaxing scattering of electrons by the host so

222 on of hybrid polariton modes is evidenced in momentum resolved photoluminescence and reflectivity stu

223 Using the recently developed technique of momentum-resolved electron energy-loss spectroscopy (M-E

224 We also discuss momentum-resolved Ramsey spectroscopy methods for observ

225 ey become older, stars lose mass and angular momentum, resulting in an observed slowdown in surface r

226 tical elements that convert the spin angular momentum (SAM) of light into vortex beams have found app

227 e of FeSe and determine its exact energy and momentum scales.

228 er mobility in GNRs by affecting the carrier momentum scattering rate.

229 elative to organic thin films, thus reducing momentum scattering.

230 Momentum separators can reduce unwanted low-density gase

231 rogen compounds in the atmosphere has gained momentum since the identification of their crucial role

232 Zurek mechanism in the quantum regime in the momentum space and find the measured scaling of excitati

233 ly observe topological surface-state arcs in momentum space by near-field scanning the surface of a c

234 roken Cooper pairs, and signals an important momentum space dichotomy in the formation of Cooper pair

235 iconductor heterojunction, delocalization in momentum space due to strong exciton binding may assist

236 ct experimental observation of Fermi arcs in momentum space has been reported so far.

237 bit coupling gives rise to Weyl nodes, whose momentum space locations can be controlled as a function

238 ence of inequivalent valleys K and K' in the momentum space of 2D hexagonal lattices provides a new e

239 rgy states are squeezed to a single point in momentum space when the chemical potential mu is tuned p

240 that can be viewed as magnetic monopoles in momentum space) in the bulk and unique Fermi arcs genera

241 omic interferometer to measure Berry flux in momentum space, in analogy to an Aharonov-Bohm interfero

242 imately a few hundred T) produced by them in momentum space, our discovery lays the foundation for a

243 by a set of Landau-Zener crossings in pseudo-momentum space, that can be probed with high accuracy us

244 rmi lines or zero-dimensional Weyl points in momentum space, where the valence and conduction bands t

245 XPCS probes the dynamics in momentum space, which in the SAXS geometry reflects stru

246 exhibit gap maxima oriented orthogonally in momentum space.

247 ed by an isotropic power-law distribution in momentum space.

248 fermions by splitting the spin degeneracy in momentum space.

249 reconstruct dynamical correlations in energy-momentum space.

250 ectrically gated bilayer graphene (BLG), the momentum-space Berry curvature Omega carries opposite si

251 of how local valence fluctuations connect to momentum-space concepts such as band filling and Fermi s

252 The impact of this change on the momentum-space electronic structure is essential for und

253 Here, using (87)Rb atoms in a momentum-space lattice, we realize fully tunable condens

254 er-driven dynamics of atomic population in a momentum-space lattice.

255 Here, the authors use synthetic momentum-space lattices to engineer spatially and dynami

256 We propose that momentum-space mapping of the second-order non-linear st

257 Meanwhile, hole-doped TMDs with momentum-space-split spinless fermions remain unexplored

258 for topological superconductors out of such momentum-space-split spinless fermions.

259 ether reveal the particle's nonlocal modular momentum spatially separated from its mass.

260 single-surface phenomenon, attributed to the momentum-spin locking on each individual surface.

261 ting arbitrary SAM states into total angular momentum states characterized by a superposition of inde

262 and large increase in the energy of angular-momentum states in circular graphene p-n junction resona

263 g splitter with the occupation of mainly two momentum states is achieved in this regime.

264 glement swapping of multiple orbital angular momentum states of light.

265 ons of Li0.8Fe0.2ODFeSe, revealing analogous momentum structure and dispersion to hole-doped cuprates

266 The observed energy-dependent momentum structure and twisted dispersion of spin excita

267 the sub-optical cycle energy and transverse momentum structure imprinted on the electron beam.

268 for several decades, and it has gained fresh momentum thanks to recent community-wide blind tests aim

269 es framing decisions and describe a clinical momentum that promotes surgical intervention.

270 the energy, the wave number, and the angular momentum through the bifurcations.

271 on a picosecond time scale by deflecting the momentum-time correlated electrons in the diffraction pe

272 demonstrated to provide an effective optical momentum to bend light in arbitrary ways.

273 ssel-Gaussian beams carrying orbital-angular-momentum to overcome limitations in obstructed free-spac

274 Surprisingly, momentum transfer at the molecular scale closely resembl

275 d to magnetic circular dichroism and angular momentum transfer between sublattices.

276 emperature-dependent component appears, with momentum transfer dependence pointing toward nanoscale d

277 ed environment, probably providing efficient momentum transfer for driving turbulence.

278 While momentum transfer from active particles to their immedia

279 Orbital angular momentum transfer is also shown to rotate a levitated ob

280 the backscattering geometry at large photon momentum transfer maximizes the XRS signal at the given

281 y from one Weyl node to another, rather than momentum transfer of the Lorentz force.

282 ular structure with adequate sampling of the momentum transfer space.

283 -inspired impulsive mechanism that maximizes momentum transfer to water.

284 narrowing of the QENS signal appears between momentum transfer values Q = 0.7-1.1 A(-1) corresponding

285 dented high accuracy in an extended range of momentum transfers has allowed the derivation of detaile

286 ions to neutral atoms with little change in momentum, transform these to a bright source of MeV atom

287 The observed broadband and fast momentum transformation could promote applications such

288 The broadband momentum transformation enhances the device conversion e

289 We report broadband momentum transformations of light in asymmetric whisperi

290 the standard QBO paradigm based on vertical momentum transport.

291 equences for our understanding of energy and momentum transportation in the flare-related phenomena.

292 and peak position that differs from the zero momentum trion energy.

293 The hypothesis is often cited and has gained momentum, turning it into paradigm status.

294 le carrier distribution in different crystal momentum valleys.

295 and the initial and final rotational angular momentum vectors of HD provides insight into the strong

296 h property couples the stress-strain and the momentum-velocity relations.

297 ng of the magnetisation with optical angular momentum was demonstrated recently.

298 cal waveguides carry transverse spin angular momentum which is also locked to the propagation directi

299 This momentum will probably move strongly across stakeholder

300 Pure spin current, a flow of spin angular momentum without flow of any accompanying net charge, is