ライフサイエンスコーパス: orbit

1 eir location near critical structures in the orbit.

2 a pi Berry phase accumulated along cyclotron orbit.

3 described: HAS-BLED, ATRIA, HEMORR2HAGES and ORBIT.

4 and a palpable mass in the left superonasal orbit.

5 RI) to evaluate postsurgical findings in the orbit.

6 xpressed on selected vascular lesions of the orbit.

7 on orbit in the surface states known as Weyl orbit.

8 t of a cellular function in real time and on orbit.

9 ins that are preferentially aligned with the orbit.

10 be related to the quantized version of Weyl orbits.

11 t, in turn, pushed them onto planet-crossing orbits.

12 magnetic breakdown tunnelling to additional orbits.

13 points and periodic and aperiodic molecular orbits.

14 onfiguration relative to exceptionally large orbits.

15 s of pulley displacements were modeled using Orbit 1.8 (Eidactics, San Francisco, CA) computational s

16 gically confirmed tumor recurrences (3 of 55 orbits, 5.5%) were correctly judged as "definitive tumor

17 numerical experiments of a water-rich planet orbiting a double star.

18 n into a low-dimensional, periodic, decaying orbit - a spiral - in which it behaved as a true attract

19 stent with the theoretically predicted 'Weyl orbits', a kind of cyclotron motion that weaves together

20 9-0.64] for HAS-BLED vs 0.68 [0.65-0.70] for ORBIT; ABC-bleeding vs HAS-BLED p<0.0001 and ABC-bleedin

21 METHODS AND Using data from ORBIT-AF (Outcomes Registry for Better Informed Treatmen

22 ohort study included 9,749 patients from the ORBIT-AF (Outcomes Registry for Better Informed Treatmen

23 ed 5,738 patients treated with a NOAC at 242 ORBIT-AF II (Outcomes Registry for Better Informed Treat

24 nformed Treatment of Atrial Fibrillation II [ORBIT-AF II]; NCT01701817).

25 ame orbit when evoked, and returning to that orbit after transient perturbation.

26 Spin-orbit alignment can be measured when the planet transits

27 oscillations associated with various closed orbits also emerge sequentially with increasing density.

28 Vascular lesions of the orbit, although not malignant, can cause morbidity becau

29 and high-risk patients appropriately, whilst ORBIT and ATRIA categorised most major bleeds into their

30 Earth's orbit and axial tilt imprint a strong seasonal cycle on

31 Neuroimaging of the orbit and brain and a biopsy of the affected muscles sho

32 e define the relative importance of the spin-orbit and crystal field interactions, and explain the ex

33 turally owing to aging changes in each eye's orbit and extra-ocular muscles, or in oculomotor dysfunc

34 Adding 'labile INR' to ATRIA, ORBIT and HEMORR2HAGES improved their predictive value f

35 bile INR' criteria (i.e. TTR <65%) to ATRIA, ORBIT and HEMORR2HAGES increased their ability of discri

36 ng risk was assessed by the HAS-BLED, ATRIA, ORBIT and HEMORR2HAGES scores.

37 se of multi-band Mott physics including spin-orbit and Hund's coupling is realized in Ca2RuO4.

38 mplimentary hydrodynamic mechanisms, Jeffrey Orbit and shear-induced flagella unbundling, are respons

39 Variations in the Earth's orbit and spin vector are a primary control on insolatio

40 cts the contours of the cheeks, temples, and orbits and may negatively affect patients' adherence to

41 supernova explosions of young stars on large orbits), and some models also predict it to contribute s

42 (although tidally modulated) throughout each orbit, and since the 2005 discovery of the plumes.

43 Adding TTR to ORBIT, ATRIA and HEMORR2HAGES led to improved predictive

44 Adding 'labile INR' (TTR < 65%) to ORBIT, ATRIA and HEMORR2HAGES significantly improved the

45 ent a key step in understanding surface spin-orbit band electronic transport.

46 trations of these behaviours in surface spin-orbit bands exist.

47 tars are expected to be on circular, aligned orbits because of strong tidal interactions with the ste

48 Yet the secular evolution of the planetary orbits beyond 50 million years ago remains highly uncert

49 s. 86%, respectively; p < 0.0001) and higher ORBIT bleeding scores (25% and 31% >4 vs. 11%, respectiv

50 The density varied between orbits by up to two orders of magnitude.

51 Spaceborne measurements by NASA's Orbiting Carbon Observatory-2 (OCO-2) at the kilometer s

52 NASA's Orbiting Carbon Observatory-2 (OCO-2) mission was motiva

53 Orbiting Carbon Observatory-2 (OCO-2)'s SIF data acquisi

54 bservations of carbon dioxide (CO2) from the Orbiting Carbon Observatory-2 are used to characterize t

55 inconsistencies may be due to NOAA satellite orbit changes and MODIS sensor degradation.

56 Exoplanets orbiting close to cool stars are expected to be on circu

57 The Rosetta spacecraft spent 2 years orbiting comet 67P/Churyumov-Gerasimenko, most of it at

58 xperimental detection of these CPP planetary orbit complexes.

59 a measurement environment is close to the in-orbit conditions and it can satisfy the stringent requir

60 ators that are predicted to be strongly spin-orbit coupled analogues of the parent state of cuprate h

61 our proposal in real materials, such as spin-orbit coupled graphene and crystal Bismuth.

62 idths give a potential tool to identify spin-orbit coupled states, and show measurement of U(V)...U(V

63 ogical phases of two-dimensional Rashba spin-orbit coupled superconductors.

64 esent in a near-zero temperature spin-1 spin-orbit-coupled atomic Bose gas and the quantum phase tran

65 tates and quasi-momenta, and to produce spin-orbit-coupled dynamics.

66 Here we demonstrate that spin-orbit-coupled fermions can be engineered to occur natura

67 -films is similar to that of Jeff = 1/2 spin-orbit-coupled Mott insulator Sr2IrO4 and Ba2IrO4, with t

68 amics, by focusing on a one-dimensional spin-orbit-coupled nanowire quantum dot.

69 er, spontaneous emission in alkali-atom spin-orbit-coupled systems is hindered by heating, limiting t

70 function calculations that incorporate spin-orbit coupling (CASSCF), and by a full-model Hamiltonian

71 We investigated curvature-enhanced spin-orbit coupling (SOC) and spinterface effect in carbon-ba

72 ideration has been given to the role of spin-orbit coupling (SOC) in 5d oxides, particularly on the f

73 Engineered spin-orbit coupling (SOC) in cold-atom systems can enable the

74 The splittings are attributed to spin-orbit coupling (SOC) in the ECX(*) radicals.

75 ge, using d-wave superfluid with Rashba spin-orbit coupling (SOC) interactions.

76 It is well-established that high spin-orbit coupling (SOC) materials convert a charge current

77 Owing to the inherently weak spin-orbit coupling (SOC) of OSECs, their inverse spin Hall e

78 The influence of spin-orbit coupling (SOC) on the physical properties of the 5

79 of strong electronic correlations with spin-orbit coupling (SOC) represents a central issue in quant

80 density of state, orbital overlap, and spin-orbit coupling (SOC) strength in the FePt film, leading

81 covered their Fermiology evolution with spin-orbit coupling (SOC) strength.

82 cs requires understanding the molecular spin-orbit coupling (SOC), and a means to tune its strength.

83 s show that the QSH phase arises from a spin-orbit coupling (SOC)-induced s-p band inversion or p-p b

84 ing nonmagnetic 5d TMOs with pronounced spin-orbit coupling (SOC).

85 Due to the combination of a substantial spin-orbit coupling and correlation effects, iridium oxides h

86 omplex interplay between Dirac physics, spin-orbit coupling and externally applied fields.

87 o identical valleys as a consequence of spin-orbit coupling and inversion symmetry breaking, leading

88 asurements confirm the requisite strong spin-orbit coupling and low-temperature magnetic order matchi

89 ), and by a full-model Hamiltonian with spin-orbit coupling and Slater-Condon parameters (CONDON).

90 feature tightly bound excitons, strong spin-orbit coupling and spin-valley degrees of freedom.

91 SrSi2 is a Weyl semimetal even without spin-orbit coupling and that, after the inclusion of spin-orb

92 ures which are mainly induced by strong spin-orbit coupling and the inversion symmetry breaking in th

93 Strong oscillations in spin-orbit coupling and the involvement of higher-lying quart

94 symmetries in solid-state systems with spin-orbit coupling and time-reversal symmetry.

95 Strong Coulomb repulsion and spin-orbit coupling are known to give rise to exotic physical

96 Bose-Einstein condensates with spin-orbit coupling are predicted to possess a stripe phase w

97 ceptor charge transfer molecules, where spin-orbit coupling between singlet and triplet states is med

98 e and conduction band along with strong spin-orbit coupling can be realized in correlated materials.

99 ossing point calculations predict small spin-orbit coupling constants making the spin state change fr

100 chanical calculations, it is clear that spin-orbit coupling contributes significantly to berkelium's

101 lectronic repulsion, crystal field, and spin-orbit coupling effects can be of similar magnitude.

102 ificant MLCT character, enabling strong spin-orbit coupling for highly efficient intersystem-crossing

103 cture calculations which reveal a large spin-orbit coupling gap of epsilonso = 0.21 eV.

104 The inclusion of spin-orbit coupling gives rise to Weyl nodes, whose momentum

105 imensional heterostructures with strong spin-orbit coupling have direct relevance to topological quan

106 lities of correlated metals with strong spin-orbit coupling have only recently begun to be explored.

107 na in [Pb2BiS3][AuTe2], a new 2D strong spin-orbit coupling heterostructure system.

108 ther with the large g-factor and Rashba spin-orbit coupling in In0.75 Ga0.25 As quantum wells, which

109 resent a formulation of electromagnetic spin-orbit coupling in magneto-optic media, and propose an al

110 ture and the interplay between spin and spin-orbit coupling in materials.

111 tic interactions, superconductivity and spin-orbit coupling in the same q2DES makes the LaAlO3/EuTiO3

112 n efficient spin texture induced by the spin-orbit coupling in the topological surface states that re

113 icrostates that are not solely spin up, spin-orbit coupling induced mixing of low-lying excited state

114 en a semiconductor nanowire with strong spin-orbit coupling is brought into contact with a supercondu

115 t magnetization-induced electromagnetic spin-orbit coupling is possible, and that it leads to unequal

116 he magnitude of such asymmetric part of spin-orbit coupling is worthwhile, as they account for spin-o

117 Strong spin-orbit coupling lifts the degeneracy of t 2g orbitals in

118 band electronic correlations and strong spin-orbit coupling may conspire in selecting a rather unusua

119 properties of graphene with the strong spin-orbit coupling of MoS2 and allows switching of the spin

120 Spin-orbit torques arising from the spin-orbit coupling of non-magnetic heavy metals allow electr

121 s becomes controlled by the full atomic spin-orbit coupling of the 3d and 4d transition metals, resul

122 iya interaction originating from strong spin-orbit coupling of Yb 4f is a key ingredient to explain m

123 igand motion have a greater effect than spin-orbit coupling on determining the forward and reverse is

124 We also discuss the role of spin-orbit coupling on the competition between covalency and

125 veal the effect of stacking orders with spin-orbit coupling on the electronic properties of few-layer

126 stood only as the consequence of strong spin-orbit coupling that, together with substrate-induced inv

127 a, and propose an alternative source of spin-orbit coupling to non-paraxial optics vortices.

128 ons, vibronic activity, and the role of spin-orbit coupling under charge-transfer perturbations.

129 larized phases, which are stabilized by spin-orbit coupling's explicit locking between spin and motio

130 ds, superconducting systems with strong spin-orbit coupling, and paired states of interacting composi

131 pological phases in systems with strong spin-orbit coupling, and ultra-manipulable materials platform

132 etic and heavy metal layers with strong spin-orbit coupling, but details of the interaction remain to

133 lculations show that, in the absence of spin-orbit coupling, Co2TiX features three topological nodal

134 ronic localization effect due to strong spin-orbit coupling, implying that heavily Nb-doped Sr(Nb0.2T

135 urrent flows in a heavy metal film with spin-orbit coupling, it produces a torque on and thereby swit

136 related systems and, given their strong spin-orbit coupling, present a natural setting to make progre

137 ffect in normal metals (NM) with strong spin-orbit coupling, such as Pt or Ta.

138 ng the group IVA element, the degree of spin-orbit coupling, the functionalization chemistry or the s

139 In the absence of spin-orbit coupling, the predicted reaction mechanism is qual

140 tructural symmetry, stacking orders and spin-orbit coupling, transitional metal dichalcogenides have

141 upling and that, after the inclusion of spin-orbit coupling, two Weyl fermions stick together forming

142 nated host molecules leads to increased spin-orbit coupling, which in turn enhances intersystem cross

143 nel with "spin momentum locking" due to spin-orbit coupling.

144 he Abrikosov-Gorkov model due to strong spin-orbit coupling.

145 s commonly observed in channels without spin-orbit coupling.

146 using the hybrid functional B3PW91 with spin-orbit coupling.

147 ferromagnetic materials with very large spin-orbit coupling.

148 ters the ratio of Rashba to Dresselhaus spin-orbit coupling.

149 her layered structures with interfacial spin-orbit coupling.

150 5.16muB) likely due to a high degree of spin-orbit coupling.

151 osymmetric compound PbTaSe2 with strong spin-orbit coupling.

152 nd semiconducting layers with intrinsic spin-orbit coupling.

153 to orbital mixing induced by pronounced spin-orbit coupling.

154 ing a phase-coherent system with strong spin-orbit coupling.

155 -atomic 4f-4f Coulomb interactions, and spin-orbit coupling.

156 hich is allowed only in the presence of spin-orbit coupling.

157 imensional systems in conventional, low-spin-orbit-coupling semiconductors.

158 ers, such as the Rashba and Dresselhaus spin-orbit-coupling strengths, as well as the Lande factor.

159 cause, owing to Lorentz forces, spiral modes orbit decreases in diameter pulling the charge carriers

160 The discovery of planets orbiting double stars at close distances has sparked inc

161 nal allows to detect the decay of the binary orbit due to gravitational wave emission by observing tw

162 ll be unable to escape each other; they will orbit each other for a time, ultimately undergoing a low

163 The atmospheres of orbiting Earth-sized planets are observationally accessi

164 The spin-orbit effective fields due to the spin Hall effect were

165 Here we demonstrate the presence of spin-orbit effects near the NM/FM interface that exhibit a ve

166 (FM) bilayer interface, the symmetry of spin-orbit effects requires that the spin current, charge cur

167 Here the authors demonstrate spin-orbit effects with a different symmetry, which could hel

168 nctional theory calculations, including spin-orbit effects, are in excellent agreement with these exp

169 hese findings show that low dimensional spin-orbit entangled 3d-5d interfaces provide an avenue to un

170 These spin-orbit entangled states can host exotic quantum phases su

171 torques may play an important part in binary orbit evolution.

172 mperatures, we observed caustics of skipping orbits extending over hundreds of superlattice periods,

173 ntrol it electrically via an artificial spin-orbit field from a micromagnet.

174 These orbits form stable spatially periodic patterns, the unit

175 Two orbits from 2 children rated as "suspicious of tumor" re

176 th HAS-BLED (HR: 1.62;95% CI: 1.06-2.48) and ORBIT (HR: 1.83;95% CI: 1.08-3.09) 'high-risk' categorie

177 on MRI as a potential screening tool for the orbit in children with retinoblastoma to exclude tumor r

178 c semimetals exhibit a new type of cyclotron orbit in the surface states known as Weyl orbit.

179 sufficient gas to form new stars if they had orbited in their host galaxies' gaseous disks throughout

180 tence of short, moderately unstable periodic orbits in the perturbed system.

181 HEMORR2HAGES, Shireman, HAS-BLED, ATRIA and ORBIT) in a large cohort of Chinese inpatients with AF.

182 um eigenstates resembling classical periodic orbits, in two-dimensional quantum wells perturbed by lo

183 states that change topology through the spin-orbit-induced band inversion.

184 The high-Z bcc metals with large spin-orbit-induced bandgaps are discussed as candidates for t

185 t these cannot be older than Phobos' current orbit inside Mars' Roche limit.

186 aterials which takes into account both, spin-orbit interaction and electronic nematicity.

187 hout time-reversal symmetry breaking or spin-orbit interaction and provide quantized low-temperature

188 the interface resulting from the large spin-orbit interaction and the spin-momentum locking of the t

189 epresents a way of implementing coupled spin-orbit interaction between electrons and photons and may

190 The spin-orbit interaction enables interconversion between a char

191 n an external magnetic field and Rashba spin-orbit interaction in semiconductor nanostructures.

192 is an optical analogous of Rashba like spin-orbit interaction parameter present in quantum waves, in

193 geometric phase phenomenon arising from spin-orbit interaction provides a route to implement photonic

194 coupling a 2D electron gas with strong spin-orbit interaction to an s-wave superconductor.

195 tem has strong correlations and a large spin-orbit interaction, it often exhibits a plethora of mutua

196 c inversion of bulk bands driven by the spin-orbit interaction.

197 is results from a combination of strong spin-orbit interactions and local inversion symmetry breaking

198 f non-magnetic heavy metals with strong spin-orbit interactions and transition-metal ferromagnetic la

199 re notably, our ability to engineer the spin-orbit interactions enables us to simultaneously manipula

200 onverting charge to spin currents using spin-orbit interactions has useful applications in spintronic

201 ation corrections to conductance due to spin-orbit interactions, and linear positive magnetoresistanc

202 curvature effects, together with strong spin-orbit interactions, can generate unconventional Landau l

203 n-symmetry breaking, when combined with spin-orbit interactions, can mediate Rashba-like spin splitti

204 ermionic atoms with laser field induced spin orbit interactions.

205 perties due to opposing dependencies on spin-orbit interactions.

206 example of first-class moment (Mn) and spin-orbit (Ir) combination.

207 The circular orbit is unlikely to be the result of tides and therefor

208 nce of a large population of unbound or wide-orbit Jupiter-mass planets (reported to be almost twice

209 e, (2) astronauts who flew only in low Earth orbit (LEO), and (3) Apollo lunar astronauts, the only h

210 We present a spin-orbit logic gate that performs a universal logic operati

211 Here, we show that spin-orbit materials possess an intrinsic basis for the execu

212 sensitivity to gravity, through real-time on orbit measurements and by using an experimental system,

213 ature superconductor-related materials, spin-orbit Mott insulators, frustrated magnets, and dilute ma

214 (n = 27 of 36; 75%), and involvement of the orbit (n = 32 of 55; 58%).

215 w that the solar perturbations on the Moon's orbit naturally induce a large lunar inclination and rem

216 Remarkably, the spin-orbit nodal lines in PbTaSe2 are not only protected by t

217 a, choroid, ciliary body, lacrimal gland, or orbit (OA-uveal lymphoma) were included.

218 fibroblast accumulation, and scarring in the orbit of affected individuals.

219 ion acquired during cruise phase outside the orbit of Jupiter, and find a statistical upper limit on

220 es are randomly oriented with respect to the orbit of the binary system), whereas those that formed f

221 seasonal changes induced by the rotation and orbit of the comet.

222 We find that the eccentric orbit of the Neptune-mass exoplanet GJ 436b is nearly pe

223 aotic behavior as the radius of the circular orbit of the point mass increases (other parameters bein

224 tems containing super-Earths and Neptunes in orbits of a few days to a few months.

225 ion associated with interactions between the orbits of Mars and the Earth, using an integrated radioi

226 be responsible for establishing the current orbits of the four giant planets in the Solar System by

227 es of planetesimals that accreted beyond the orbits of the gas giants.

228 ing vs HAS-BLED p<0.0001 and ABC-bleeding vs ORBIT p=0.0008).

229 ing vs HAS-BLED p<0.0001 and ABC-bleeding vs ORBIT p=0.0016).

230 k categories for the HAS-BLED (p = 0.023) or ORBIT (p = 0.022) scores, respectively, conferred signif

231 do localization plays a similar role to spin-orbit pair breaking in making WHH fits to the data.

232 ology Assessment Committee Oculoplastics and Orbit Panel reviewed for relevancy.

233 rm neurofibromas (PNs) involving the eyelid, orbit, periorbital, and facial structures (orbital-perio

234 quency of Jupiter-mass free-floating or wide-orbit planets of 0.25 planets per main-sequence star.

235 ra of host stars induced by the influence of orbiting planets.

236 A temperate planet has been discovered orbiting Proxima Centauri, the closest M dwarf, but it p

237 and caused to move in a prescribed circular orbit relative to the shell.

238 he Maki parameter, require an effective spin-orbit relaxation parameter of order unity.

239 Our data suggest that 11 orbits remain possible for the third planet, the most li

240 led abducens nerve bundles did not reach the orbit, resulting in secondary aberrant misinnervation of

241 plasma core, mainly due to the large FRC ion orbits, resulting in near-classical thermal ion confinem

242 er than the focusing length (that is, of the orbit scale), the beam transit through the atmosphere in

243 ing score performed better than HAS-BLED and ORBIT scores and should be useful as decision support on

244 than the conventional HAS-BLED and the newer ORBIT scores for major bleeding in both the derivation c

245 learance) also outperformed the HAS-BLED and ORBIT scores.

246 Variations in Earth's orbit (so called 'Milankovitch cycles') have driven cycl

247 aAs/GaMnAs structure by current-induced spin-orbit (SO) magnetic field.

248 Juno's capture orbit spanned the jovian magnetosphere from bow shock to

249 The direct band gap character and large spin-orbit splitting of the valence band edges (at the K and

250 perature dependence of the band gap and spin-orbit splitting of the valence band.

251 mechanics has revealed that an asteroid may orbit stably in the same region as a planet, despite rev

252 diated through the emergence of a novel spin-orbit state within the nominally paramagnetic SIO.

253 We use orbit superposition models to determine that the black h

254 nters with cometary debris in Earth-crossing orbits (Taurid Complex) that was generated by fragmentat

255 t that numerous asteroids should be found on orbits that closely approach the Sun, but few have been

256 recently discovered system of seven planets orbiting the ultracool dwarf star TRAPPIST-1 and find th

257 li) are too small to trap BV in hydrodynamic orbit, the prey are also susceptible to their own hydrod

258 During a series of dedicated low-altitude orbits, the Rosetta Orbiter Spectrometer for Ion and Neu

259 undetected population of terrestrial planets orbiting them--ranging from metal-rich Mercury-sized pla

260 In contrast to conventional cyclotron orbits, this motion is driven by the transfer of chirali

261 ut with too much uncertainty in its measured orbit to establish whether it was such a retrograde co-o

262 h is based on an alternative mechanism, spin orbit torque (SOT) driven chiral DW motions.

263 This spin-orbit torque (SOT) has been widely used to manipulate th

264 the efficient electric-field control of spin-orbit torque (SOT) still remains elusive.

265 Such spin-orbit torque (SOT)-induced switching has been studied ex

266 FeB/MgO heterostructures in presence of spin-orbit torque and thermal noise can be harnessed to enabl

267 ling is worthwhile, as they account for spin-orbit torque in spintronic devices of ferromagnets witho

268 ield is found to generate an additional spin-orbit torque on the CoNiCo magnets, which is confirmed b

269 etic skyrmions can be controlled by the spin-orbit torque on the nanosecond time scale, which points

270 Here we demonstrate that sub-nanosecond spin-orbit torque pulses can generate single skyrmions at cus

271 is a modification proposed for the high spin-orbit torque strength Pt/Co/Ta stack, to improve its the

272 Methods based on the spin-orbit torque switching in heavy metal/ferromagnet struct

273 th the gradient of magnetic anisotropy, spin-orbit-torque-induced magnetization behaviour has attract

274 equations to quantitatively depict the spin-orbit-torque-induced motion of domain walls in a Ta/CoFe

275 Current-induced spin-orbit torques (SOTs) in structurally asymmetric multilay

276 al skyrmions, whose motion is driven by spin-orbit torques and is deterministic, which makes systems

277 Spin-orbit torques arising from the spin-orbit coupling of no

278 nts have demonstrated that relativistic spin-orbit torques can provide the means for an efficient ele

279 s shown to simultaneously reproduce the spin-orbit torques generated using the spin Hall effect, spin

280 materials is tungsten, for which large spin-orbit torques have been found in thin films that are sta

281 analytical formulas are derived for the spin-orbit torques in a heavy metal/ferromagnet bilayer geome

282 Here we report sizeable spin-orbit torques in IrMn/CoFeB/MgO structures.

283 operties of the films suggests that the spin-orbit torques in this system may originate dominantly fr

284 Although spin-orbit torques led to domain nucleation in continuous fil

285 rent induced magnetization switching by spin-orbit torques offers an energy-efficient means of writin

286 skyrmions, triggered by current-induced spin-orbit torques, can be reliably tuned by changing the mag

287 Together with sizeable spin-orbit torques, these features make antiferromagnets a pr

288 hand, if antiferromagnets can generate spin-orbit torques, they may enable all-electrical determinis

289 The origin of spin-orbit torques, which are generated by the conversion of

290 ably tuned by changing the magnitude of spin-orbit torques.

291 which magnetic resonance (MR) imaging of the orbits was subsequently performed ( Fig 1 ).

292 as a true attractor, converging to the same orbit when evoked, and returning to that orbit after tra

293 d small eccentricities of Earth's elliptical orbit, whereas the warmest configuration occurs at minim

294 essures in the subarachnoid space within the orbit, which impinges on the optic nerve and/or eye in a

295 arged particles are bound to their cyclotron orbits, while the neutral exciton-polaritons move freely

296 d venous pressure produces congestion in the orbit with resultant transudation of fluid and increased

297 near-infrared wavelengths, but when in close orbits with less dense stars, white dwarfs can strip mat

298 pplied force and can even exhibit elliptical orbits with nonzero orbital angular momentum.

299 could predict motor output directly from its orbit, yet individual neurons' participation changed acr

300 protoplanetary disks, disks of gas and dust orbiting young stars.