ライフサイエンスコーパス: angular momentum

1 tate atoms (atoms with zero internal orbital angular momentum).

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

3 the splitting of superatom orbitals of high angular momentum.

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

5 indices for light fields possessing orbital angular momentum.

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

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

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

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

10 ut which the fluid circulates with quantized angular momentum.

11 in-polarized current and the electrons' spin angular momentum.

12 taking advantage of Anderson localization in angular momentum.

13 hibit elliptical orbits with nonzero orbital angular momentum.

14 used to monitor protein motion at zero-total angular momentum.

15 the handedness (helicity) of the electronic angular momentum.

16 gely controlled by variations in atmospheric angular momentum.

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

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

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

20 fronts such as vortex beams carrying orbital angular momentum.

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

22 etermined by conservation of energy and spin angular momentum.

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

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

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

26 tum nondemolition measurement of atomic spin-angular momentum allowed us to influence the quantum sta

27 The outward transfer of angular momentum allows the star to contract without bre

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

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

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

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

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

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

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

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

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

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

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

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

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

41 Angular-momentum arguments show that the pi-electron-ric

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

43 t overall rotation is possible at zero-total angular momentum as a result of flexibility.

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

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

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

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

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

49 Such orbital angular momentum based multiplexing can potentially incr

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

67 tions from Neptune, so that the transport of angular momentum by density waves can result in orbital

68 gas from rotating equatorial disks and shed angular momentum by ejecting gas in bipolar outflows.

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

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

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

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

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

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

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

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

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

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

79 Angular momentum conservation follows immediately.

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

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

82 the S(N)2 reaction are discussed, including angular momentum constraints, orientational effects, and

83 orientation and size are constrained by the angular momentum contained in both the Earth's spin and

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

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

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

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

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

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

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

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

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

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

94 0 degrees] to specifically reveal rotational angular-momentum directions for scattered molecules.

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

134 herical atoms with non-zero internal orbital angular momentum) is thought to proceed rapidly.

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

165 The close similarity of axial oceanic angular momentum (OAM) results from two independent OGCM

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

185 poor Moon, as well as the current masses and angular momentum of the Earth-Moon system.

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

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

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

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

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

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

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

193 ferromagnet, through direct transfer of spin angular momentum, offers the possibility of manipulating

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

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

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

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

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

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

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

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

202 nge in a reasonable way with increase in the angular momentum quantum number J and with change in the

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

204 he moment of inertia with increase in J, the angular-momentum quantum number, many of the lanthanon g

205 s from values K approximately 82-104 for the angular-momentum quantum number, that the moment of iner

206 forming the Moon with an appropriate impact angular momentum required the impact to occur when the E

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

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

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

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

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

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

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

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

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

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

217 We find that the fraction of a projectile's angular momentum that is retained by a target asteroid i

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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