ライフサイエンスコーパス: angular momentum

1 hibit elliptical orbits with nonzero orbital angular momentum.

2 e beam diffraction and from the beam orbital angular momentum.

3 iple electrons, which can also carry orbital angular momentum.

4 ses a helical wave front and carries orbital angular momentum.

5 fronts such as vortex beams carrying orbital angular momentum.

6 tation vanes can provide the air inflow with angular momentum.

7 etermined by conservation of energy and spin angular momentum.

8 ith a novel energy dependence on the orbital angular momentum.

9 the splitting of superatom orbitals of high angular momentum.

10 tate vector in the discrete basis of orbital angular momentum.

11 indices for light fields possessing orbital angular momentum.

12 n to induce a range of perturbations in body angular momentum.

13 hat are retrograde with respect to the total angular momentum.

14 ing spin angular momentum to flow to orbital angular momentum.

15 n the opposite direction to the flow of spin angular momentum.

16 ut which the fluid circulates with quantized angular momentum.

17 neutron beams with coupled spin and orbital angular momentum.

18 signed with strong chirality induced orbital angular momentum.

19 often further constrained by the rotational angular momentum.

20 ) there is no polarization and hence no spin angular momentum.

21 iginate from the chirality-dependent orbital angular momentum.

22 shifting the source location and introducing angular momentum.

23 rganize to avoid each other while conserving angular momentum.

24 Waves can carry both linear and angular momentum.

25 e-and the details of the required removal of angular momentum.

26 igh-dimensionally entangled in their orbital angular momentum.

27 to transmit spins because of their vanishing angular momentum(9-11).

28 We computed changes in whole-body motion and angular momentum across the two conditions.

29 ious Moon-formation studies assumed that the angular momentum after the impact was similar to that of

30 ing of its tail induces the most rapid, zero-angular momentum air-righting response yet measured.

31 These particles have their spin, or internal angular momentum, aligned either parallel or antiparalle

32 nts, such as vortex beams that carry orbital angular momentum, also known as topological charge.

33 f the plasmonic vortex are determined by the angular momentum (AM) of the light, and the geometrical

34 generally independent of the electron's spin angular momentum, an internal degree of freedom possesse

35 isted Laguerre-Gaussian lasers, with orbital angular momentum and characterized by doughnut-shaped in

36 gineer their bond length, vibrational state, angular momentum and orientation in a small electric fie

37 from the entanglement of the optical orbital angular momentum and radial profile degrees of freedom p

38 ique for the generation of broadband orbital angular momentum and radially polarized beams.

39 er-spinning early Earth-Moon system can lose angular momentum and reach the present state through an

40 question our understanding of how stars lose angular momentum and spin down as they age(12-14).

41 Through weak measurements of orbital angular momentum and strong measurements of angular posi

42 The discrete nature of orbital angular momentum and the continuous but periodic nature

43 in accordance with the conservation of spin angular momentum, and high thermal stability owing to th

44 ams with helical wavefronts carrying orbital angular momentum are expected to provide new capabilitie

45 ate number, and beams with different orbital angular momentum are orthogonal.

46 densates (whose atoms have non-zero internal angular momentum) are quantum fluids that simultaneously

47 n acts to homogenize the distribution of the angular momentum around the rotational axis.

48 onductors has identified the electron's spin angular momentum as a new state variable that should be

49 andmark experiment(1) demonstrating that the angular momentum associated with aligned electron spins

50 momentum can be characterised by the "spin" angular momentum associated with circular polarisation,

51 ange that scatters states of finite relative angular momentum at collision energies where only s-wave

52 sic and extrinsic components of the photon's angular momentum at short-wavelengths.

53 tonomous spinning units injecting energy and angular momentum at the microscopic level represent a pr

54 e addition, and extraction of usable orbital angular momentum at the single-photon level, is further

55 collisions arising from tunneling through an angular momentum barrier followed by a short-range chemi

56 y six independent parameters including mass, angular momentum, baryon fraction, age and size, as well

57 ep central dark-matter profiles, because low-angular-momentum baryons and dark matter sink to the cen

58 Such orbital angular momentum based multiplexing can potentially incr

59 city-dependent focusing and imaging devices, angular-momentum-based quantum information processing an

60 In general, orbital angular momentum beams are generated using free-space bu

61 s(-1) Hz(-1) using four independent orbital-angular momentum beams on each of two polarizations.

62 an 8-Gbit s(-1) link containing two orbital angular momentum beams on each of two polarizations.

63 reover, we show that Bessel-Gaussian orbital-angular-momentum beams are more tolerant to obstructions

64 rant to obstructions than non-Bessel orbital-angular-momentum beams.

65 l phenomenon, resulting from the transfer of angular momentum between interacting light and matter in

66 t of dipolar-interaction-induced transfer of angular momentum between the J=0 and J=1 internal partic

67 ternal tidal torques, or from an exchange of angular momentum between the solid Earth and its fluid c

68 and is consistent with seasonal exchange of angular momentum between the surface and Titan's dense s

69 Resonant exchange of rotational angular momentum between two molecules realizes a spin-e

70 The resulting angular momentum bias splits the ring's azimuthal resona

71 n acoustic nonreciprocal circulator based on angular-momentum bias, time-reversal symmetry is broken

72 ow that these limitations may be overcome by angular momentum-biased metamaterials, in which a proper

73 Further analysis of Earth's angular momentum budget and NASA's Apollo Landing Mirror

74 that not only does the beam contain orbital angular momentum but can trivially be converted to a rad

75 topology favours long-range order of orbital angular momentum but the spins are thought to remain dis

76 nd disk winds can both in principle transfer angular momentum, but hitherto we lacked evidence that e

77 ull many-body dynamics of the acquisition of angular momentum by a gas of ultracold bosons in two dim

78 The onset of quenching of orbital angular momentum by ligand fields is observed to occur a

79 a ferromagnet can be converted to mechanical angular momentum by reversing the direction of magnetiza

80 ther fundamental particles have an intrinsic angular momentum called spin.

81 hen the wave is transverse (e.g. light), the angular momentum can be characterised by the "spin" angu

82 V(TCNE)(x) is demonstrated and show that the angular momentum carried by microwave-excited coherent s

83 All eight orbital angular momentum channels are recovered with bit-error r

84 de demultiplexer to demultiplex four orbital angular momentum channels with crosstalk less than -12.5

85 f multiplexing up to 200 independent orbital angular momentum channels.

86 d highlights the importance of tuning of the angular momentum compensation point of ferrimagnets, whi

87 dynamics is realized in ferrimagnets at the angular momentum compensation point TA.

88 ce, the skyrmion Hall effect vanishes at the angular momentum compensation temperature where the net

89 e show that pseudospin can turn into orbital angular momentum completely, thus upholding the belief t

90 With planetary perturbers, the inner orbit's angular momentum component parallel to the total angular

91 The spin angular momentum components of linearly polarized light

92 onic transitions, term energies, and orbital angular momentum components of the bound electronic stat

93 a two-dimensional decomposition into orbital angular momentum components, or indeed any discrete basi

94 r and the relative phase between its orbital-angular-momentum components.

95 Angular momentum conservation follows immediately.

96 s easily explained within the context of the angular momentum conservation model, this relatively sim

97 based on Wigner's original ideas concerning angular momentum conservation to interpret the photo-ind

98 se values suggest a significant spin orbital angular momentum contribution that leads to a magnetic m

99 r-wave plate devices empower spin to orbital angular momentum conversion and vector polarization form

100 and that it leads to unequal spin to orbital angular momentum conversion in magneto-optic media evane

101 With that hindsight, here orbital angular momentum conversion of optical vortices through

102 sing applications related to spin-to-orbital angular momentum conversion, spin-orbit hybrid entanglem

103 ing, focusing/defocusing and spin-to-orbital angular momentum conversion.

104 is minimized through the formation of higher angular momentum Cooper pairs, with Fermi surface nodes

105 t these photons avoid each other and exhibit angular momentum correlations, the hallmarks of Laughlin

106 ndent scattering calculations, within a full angular momentum coupling formulation, were performed fo

107 We show that transverse-spin to orbital angular momentum coupling into magneto-optic waveguide m

108 tperforms previous methods based on systems' angular momentum deficit, chaos indicators, and parametr

109 to transfer the entanglement to the orbital angular momentum degree of freedom.

110 odes with entangled polarisation and orbital angular momentum degrees of freedom.

111 formulation of nonreciprocal transverse-spin angular-momentum-density shifts for evanescent waves in

112 Furthermore, the emitted photons carry spin angular momentum determined by the chirality of the spir

113 0 degrees] to specifically reveal rotational angular-momentum directions for scattered molecules.

114 t that hydrodynamic instabilities adjust the angular-momentum distribution at mid-latitudes.

115 st rotation is the result of conservation of angular momentum during the collapse of a rotating stell

116 cs and are likely to be crucial for removing angular momentum during the collapse.

117 they can be turbulent and thereby transport angular momentum effectively is controversial.

118 we estimate that the distribution of orbital angular momentum entanglement over more than 100 km of f

119 echanisms of rotational excitation, based on angular momentum exchange between the molecule and eithe

120 imescales, the dominant contribution is from angular momentum exchange between the solid mantle and f

121 and stable spin-orbit interaction of orbital angular momentum fiber modes, giant, scalable optical ac

122 It leads to spontaneous generation of angular momentum, finite Chern numbers and topologically

123 tably designed resonator lattice biased with angular momentum, forming the acoustic analogue of a mag

124 cosecond driven by the non-local transfer of angular momentum from larger adjacent Fe-rich nanoregion

125 henomena, for example the shedding of excess angular momentum from protostars by twisting of field li

126 cient control over the conversion of optical angular momentum from spin to orbital form in a metasurf

127 Such impacts require subsequent removal of angular momentum from the Earth-Moon system through a re

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

129 their tails in a measured manner to redirect angular momentum from their bodies to their tails, stabi

130 They can acquire mass and angular momentum from their companions, to be spun up to

131 lastic collisions do not obey the energy and angular momentum gap laws.

132 Strong outflows from supernovae remove low-angular-momentum gas, which inhibits the formation of bu

133 on model, but supports the high-energy, high-angular-momentum giant impact model for the origin of th

134 r tidal evolution model supports recent high-angular-momentum, giant-impact scenarios to explain the

135 hotly debated, the key question of where the angular momentum goes on these femtosecond timescales re

136 abolic cost) rather than balance (whole-body angular momentum, H), and are typically constrained to p

137 Thus far, orbital angular momentum holography has been achieved using phas

138 Here, we demonstrate an orbital angular momentum holography technology that is capable o

139 ant impact and therefore a high-energy, high-angular-momentum impact.

140 ron propagating through a solid carries spin angular momentum in addition to its mass and charge.

141 down the disk rotation by carrying away its angular momentum in an outflow and determine the directi

142 However, the true dynamics of angular momentum in finite, interacting many-body system

143 y then smoothly and sequentially transferred angular momentum in four stages between the jointed abdo

144 Moreover, the orbital angular momentum in helical chiral nanowire structures c

145 ve key questions such as the conservation of angular momentum in highly nonlinear light-matter intera

146 investigate the conservation of the orbital angular momentum in necklace and elliptical rotating bea

147 rs, the generation and conversion of orbital angular momentum in nonlinear optical media has found ma

148 Accretion disks must transfer angular momentum in order for matter to travel radially

149 Vortices are essential to angular momentum in quantum systems such as ultracold at

150 imply different mechanisms for transporting angular momentum in the disks of actively accreting youn

151 avenues for exciting applications of orbital angular momentum in the nanoworld.

152 wave-like transport of both energy and spin angular momentum, in a quasi-equilibrium gas of magnons

153 We conclude that only angular momentum induced optically by the inverse Farada

154 reconfiguration of the orbital and internal angular momentum into a high spin ([Formula: see text])

155 e conversion of plasmonic vortices with zero angular momentum into plasmonic vortices with arbitrary

156 These flows are thought to deposit gas and angular momentum into the circumgalactic medium, creatin

157 Conservation of angular momentum is a familiar tenet in science but has

158 The orbital angular momentum is a unique property for organic chiral

159 Sufficient angular momentum is deposited on the proto-neutron star

160 echanisms of vortex nucleation and show that angular momentum is hidden in phantom vortices modes whi

161 entum into plasmonic vortices with arbitrary angular momentum is illustrated in several particular ca

162 articles nor that of the excitation; rather, angular momentum is introduced by the particle's interac

163 version which persists even in systems where angular momentum is not conserved, unveiling its topolog

164 The wave angular momentum is transferred to floating micro-partic

165 curs in central-spin systems when electronic angular momentum is transferred to nuclear spins and is

166 their ground state, labelled by their total angular momentum J and parity pai.

167 tructure associated with the effective total angular momentum J(eff) = 1/2 Mott state remains robust

168 ollision-induced transitions in energy E and angular momentum J.

169 entangled state, identified by the effective angular momentum jeff, can host novel quantum phases.

170 be revealed by the regulation of whole-body angular momentum (L) during walking.

171 y were a co-orbiting binary that experienced angular momentum loss and subsequent merger, possibly be

172 d X-ray diffraction to show that most of the angular momentum lost from the spin system upon laser-in

173 important instrument for the removal of high-angular-momentum material from the accretion disk, there

174 ts suggest that angular position and orbital angular momentum may find important applications in quan

175 onfirm that, for the entanglement of orbital angular momentum, measurement in the Bessel basis is mor

176 on, we demonstrate a millimetre-wave orbital angular momentum mode demultiplexer to demultiplex four

177 On-off keying and orbital angular momentum mode switching are achieved at rates of

178 bits-per-second data transmission using four angular momentum modes at a single wavelength, and 1.6 t

179 he ability to rapidly switch between orbital angular momentum modes of light has important implicatio

180 Here, we show the transmission of orbital angular momentum modes of light over a distance of 143 k

181 by Fourier transform using different orbital angular momentum modes of light, allowing lensless recon

182 's double slit to spatial parity and orbital angular momentum modes.

183 y to actively tune between different orbital angular momentum modes.

184 with broadband and high throughput, orbital-angular-momentum multiplexing at a high spectral efficie

185 lar momentum component parallel to the total angular momentum need not be constant.

186 se front carry a quantized amount of orbital angular momentum (OAM) and have become important in vari

187 intrinsic properties of light, e.g., orbital angular momentum (OAM) and linear momentum (LM), with a

188 Light carries both orbital angular momentum (OAM) and spin angular momentum (SAM),

189 Electron waves that carry orbital angular momentum (OAM) are characterized by a quantized

190 red and visible light beams carrying orbital angular momentum (OAM) are currently thoroughly studied

191 ith circular polarisation, and the "orbital" angular momentum (OAM) arising from the phase cross-sect

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

193 An orbital angular momentum (OAM) carrying beam has the ability to

194 These elements-SAM-to-orbital angular momentum (OAM) converters-are based on the geome

195 Electromagnetic waves carrying orbital angular momentum (OAM) have been used for mode division

196 generation and propagation based on orbital angular momentum (OAM) have recently gained significant

197 Exact eigen modes with orbital angular momentum (OAM) in the complex media of unmagneti

198 The orbital angular momentum (OAM) intrinsically carried by vortex l

199 The effective generation of orbital angular momentum (OAM) lasing, especially at a micro- an

200 ters can be realized using synthetic orbital angular momentum (OAM) lattices in degenerate cavities.

201 coding off-axis points with discrete orbital angular momentum (OAM) modes is investigated.

202 hat has received interest is that of orbital angular momentum (OAM) modes.

203 alignment is even more important for orbital angular momentum (OAM) multiplexing systems since misali

204 that by analyzing the change in the orbital angular momentum (OAM) of a tilted light beam eclipsed b

205 put communication approach using the orbital angular momentum (OAM) of acoustic vortex beams with one

206 Orbital angular momentum (OAM) of light is an attractive degree

207 Applications that use the orbital angular momentum (OAM) of light show promise for increas

208 monstrate the viability of using the orbital angular momentum (OAM) of light to create orthogonal, sp

209 The quantized orbital angular momentum (OAM) of photons offers an additional d

210 Light fields carrying orbital angular momentum (OAM) provide powerful capabilities for

211 Orbital angular momentum (OAM) state of photons offer an attract

212 light at will, while preserving its orbital angular momentum (OAM) state.

213 lable multichannel superpositions of orbital angular momentum (OAM) states with various topological c

214 The orbital angular momentum (OAM) transformation of optical vortex

215 olarization coupled to two different orbital angular momentum (OAM) values ([Formula: see text] and [

216 th arbitrary polarization states and orbital angular momentum (OAM) values along the beam propagation

217 ions based on optical beams carrying orbital angular momentum (OAM) will probably require photonic in

218 Optical vortices, which carry orbital angular momentum (OAM), can be flexibly produced and mea

219 These light beams, which carry orbital angular momentum (OAM), have been successfully utilized

220 e, in principle, unbounded amount of orbital angular momentum (OAM).

221 non-collinear light beams that carry orbital angular momentum (OAM).

222 e existing methods for measuring the orbital-angular-momentum (OAM) spectrum suffer from issues such

223 We explore the use of orbital-angular-momentum (OAM)-multiplexing to increase the capa

224 The transverse component of the spin angular momentum of evanescent waves gives rise to later

225 a Kramers doublet and quartet with effective angular momentum of J eff = 1/2 and 3/2, respectively.

226 Wavelength, polarization and orbital angular momentum of light are important degrees of freed

227 de a route for exploiting the spin and orbit angular momentum of light for information processing and

228 on, information can be stored in the orbital angular momentum of light, as this degree of freedom has

229 h devices can selectively detect the orbital angular momentum of light.

230 The resulting high angular momentum of more than 40,000h per atom (where h

231 eriments ranging from the measurement of the angular momentum of photons and the g-factor of metals t

232 cs that governs the interactions between the angular momentum of photons and the magnetic order param

233 The equations governing the angular momentum of the ball relative to the point of co

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

235 n the absence of strong coupling between the angular momentum of the disk and that of the host star,

236 In ferromagnetic metals, the spin angular momentum of the electrons results in spin-depend

237 ticity and its detection through the orbital angular momentum of the emitted light are implemented in

238 which allows them to interact with the spin angular momentum of the impinging light field.

239 y the angle of incidence and the photon spin angular momentum of the incident radiation.

240 By analyzing the orbital angular momentum of the light scattered from a spinning

241 tion frequency of the object and the orbital angular momentum of the light.

242 hat are retrograde with respect to the total angular momentum of the system.

243 ons between the angular position and orbital angular momentum of two photons created by the nonlinear

244 ation of primitive plasmon modes of the same angular momentum on its inner and outer surfaces.

245 a plethora of applications based on orbital angular momentum or vector polarization, such as optical

246 oupling in addition to its effect on orbital angular momentum (orbital reduction).

247 e fundamental attributes of light, including angular momentum, phase, or polarization.

248 nces, transverse spatial modes, like orbital angular momentum possessing Laguerre Gauss modes, are fa

249 r circling a drain, inflowing mass must lose angular momentum, presumably by vigorous turbulence in d

250 quench is designed to convert the staggered angular momentum, previously thought by experts difficul

251 a yield an experimental determination of the angular-momentum-projected final local density of states

252 ed the contributions from the three dominant angular momentum projections of the collisions.

253 creating Cooper pairs, though with spin and angular momentum properties different from those of conv

254 quantized along the anisotropy axis with an angular momentum quantum number mJ=+/-(15)/2.

255 As they become older, stars lose mass and angular momentum, resulting in an observed slowdown in s

256 Optical elements that convert the spin angular momentum (SAM) of light into vortex beams have f

257 both orbital angular momentum (OAM) and spin angular momentum (SAM), related to wavefront rotation an

258 ess relativistic particles with an intrinsic angular momentum (spin) locked to its translational mome

259 magnetic dipole aligned with their internal angular momentum (spin).

260 phase front 'twisting' indicates the orbital angular momentum state number, and beams with different

261 ies of C-points and L-lines, and the orbital angular momentum states are also measured.

262 r converting arbitrary SAM states into total angular momentum states characterized by a superposition

263 to image electronic excitation to different angular momentum states depending on sample bias.

264 te entanglement swapping of multiple orbital angular momentum states of light.

265 effect can be used for manipulating photonic angular momentum states, and the measurement technique h

266 a sudden and large increase in the energy of angular-momentum states in circular graphene p-n junctio

267 econds and corresponds to 80 per cent of the angular momentum that is lost from the spin system.

268 suggested that graphene pseudospin is a real angular momentum that might manifest itself as an observ

269 y a critical role, allowing the disk to shed angular momentum that would otherwise inhibit accretion.

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

271 broken by spin-orbit coupling, allowing spin angular momentum to flow to orbital angular momentum.

272 he neutron star or it may possess sufficient angular momentum to form a disk.

273 s hyperentangled in polarization and orbital angular momentum to implement superdense teleportation,

274 ling' Bessel-Gaussian beams carrying orbital-angular-momentum to overcome limitations in obstructed f

275 This transient creation of non-trivial spin angular momentum topology pertains to cosmological struc

276 counterclockwise in the south and transport angular momentum toward the equator, maintaining the Sun

277 ttributed to magnetic circular dichroism and angular momentum transfer between sublattices.

278 Orbital angular momentum transfer is also shown to rotate a levi

279 tions and optical data, we estimate that the angular momentum transfer occurs on a timescale of 200 f

280 e induced by an alternating current owing to angular momentum transfer.

281 lated problem concerns the timescale of this angular momentum transfer.

282 otoelectron momentum is large and the recoil angular momentum transferred to the molecule is larger w

283 nt to account for measured rates of mass and angular momentum transport in protoplanetary disks.

284 Scaled to accretion disks, rates of angular momentum transport lie far below astrophysical r

285 proposed as sources for dissipation of spin angular momentum, ultrafast spin dependent transport of

286 Beams carrying quantized amounts of orbital angular momentum (up to 100h) per electron were observed

287 l frequency shift was still present when the angular momentum vector was parallel to the observation

288 ntermediate and almost parallel to the total angular momentum vector.

289 of 'hot Neptunes' and 'super-Earths') whose angular momentum vectors are misaligned with respect to

290 ocities and the initial and final rotational angular momentum vectors of HD provides insight into the

291 d no correlation between the CO velocity and angular momentum vectors.

292 switching of the magnetisation with optical angular momentum was demonstrated recently.

293 tic domain wall through the transfer of spin angular momentum when current flows in a magnetic nanowi

294 in optical waveguides carry transverse spin angular momentum which is also locked to the propagation

295 e in-gap states possess chirality of orbital angular momentum, which is related to the chiral spin te

296 shows large unquenched ground-state orbital angular momentum, which leads to highly anisotropic elec

297 g those effects, thermal tides transport the angular momentum, which maintains the rotation peak, nea

298 generalized forms of waves carrying orbital angular momentum with inhomogeneous states-of-polarizati

299 transduction (the coupling of an electron's angular momentum with its linear momentum) combined with

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