ライフサイエンスコーパス: orbit

1 paced by obliquity, under a low-eccentricity orbit.

2 d to a third super-Earth in a more temperate orbit.

3 andidate passing in front of the star in its orbit.

4 play of computed tomography (CT) data of the orbit.

5 aunches and debris accumulation in low-Earth orbit.

6 llets in the chest, abdomen, limbs, face and orbit.

7 utoimmune inflammatory disease affecting the orbit.

8 thickness) to the quantum phase of the Weyl orbit.

9 , implying an origin from a highly eccentric orbit.

10 derwent diffusion-weighted MR imaging of the orbit.

11 a small host star, and an eccentric 204-day orbit.

12 itude, one can precisely control the spinner orbit.

13 ded from superior temporal side of the right orbit.

14 d from bone marrow, can be identified in the orbit.

15 ology confirmed a pleomorphic adenoma of the orbit.

16 over long timescales of [Formula: see text] orbits.

17 r forming wide-separation planets on oblique orbits.

18 wider differential diagnosis with MRI of the orbits.

19 ified Lifshitz-Onsager relation for the Weyl orbits.

20 ses and consequently the conductivities from orbit 288 to 292.

21 sis populations consisted of 278 patients in ORBIT-3 (183 patients received at least one dose of ARD-

22 nd Aug 19, 2015, we screened 514 patients in ORBIT-3 and 533 patients in ORBIT-4.

23 ORBIT-3 and ORBIT-4 were international, randomised, doub

24 In a pooled analysis of data from both ORBIT-3 and ORBIT-4, the median time to first pulmonary

25 dverse events were similar in both groups in ORBIT-3 and ORBIT-4.

26 compared with placebo in ORBIT-4, but not in ORBIT-3 or the pooled analysis.

27 In ORBIT-3, the median time to first pulmonary exacerbation

28 and 95 received placebo) and 304 patients in ORBIT-4 (206 patients received at least one dose of ARD-

29 ORBIT-3 and ORBIT-4 were international, randomised, double-blind, pl

30 monary exacerbation compared with placebo in ORBIT-4, but not in ORBIT-3 or the pooled analysis.

31 In ORBIT-4, the median time to first pulmonary exacerbation

32 ooled analysis of data from both ORBIT-3 and ORBIT-4, the median time to first pulmonary exacerbation

33 514 patients in ORBIT-3 and 533 patients in ORBIT-4.

34 s were similar in both groups in ORBIT-3 and ORBIT-4.

35 ich extends to the innermost stable circular orbit(6,7).

36 A giant planet orbiting a hot white dwarf with a semi-major axis of aro

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

38 ce origami-rotor-based imaging and tracking (ORBIT), a method that uses fluorescently labelled DNA or

39 F patients from 80 US sites participating in ORBIT-AF from June 2010 to August 2011.

40 d at baseline and 1 year in a subset of 1347 ORBIT-AF patients from 80 US sites participating in ORBI

41 r Informed Treatment of Atrial Fibrillation (ORBIT-AF) registry, a United States-based outpatient atr

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

43 We use data obtained from the orbiting Akatsuki spacecraft to investigate how the supe

44 New observations from spacecraft in orbit allowed an estimation of gross carbon fluxes, phot

45 Notably, these animals were sacrificed on-orbit and exposed to varying spaceflight durations (i.e.

46 olvement is even rarer, mostly involving the orbit and eyelids, although marginal corneal ulcers, uve

47 en that these animals were not sacrificed on-orbit and instead returned live to earth, it is unclear

48 or radiological signs of involvement of the orbit and intracranium is rare and carries a high morbid

49 ammatory orbital involvement, imaging of the orbit and paranasal sinuses should be considered early.

50 nt with complications commonly involving the orbit and the intracranial space.

51 higher-frequency spinner occupies the inner orbit and the lower-frequency one circles on the outer o

52 with the black hole stretches them along the orbit) and they show both thermal dust emission and line

53 riments in space, enables sample recovery on-orbit, and avoids triggering standard indices of chronic

54 the magnetic flux density at geosynchronous orbit, and the solar wind dynamic pressure and IMF flux

55 tems: fixed points, recurrent sets, periodic orbits, and limit cycles.

56 e geometry, based on the hexagonal cyclotron orbits appearing in this material.

57 cal and nondetected in the infrared, and its orbit appears to cross the debris ring around the star w

58 yzer are trapped around the middle plane and orbit around the central axis perpendicular to the middl

59 In this setting, E. coli and Enterobacteria orbit around the dispersed particles.

60 3844b, a 1.3-Earth-radii world in an 11-hour orbit around the small nearby star LHS 3844.

61 planets can survive this phase and remain in orbit around the white dwarf(3,4).

62 stable patterns, e.g., triangles or squares, orbiting around the center of the cell.

63 planets might also find their way into tight orbits around white dwarfs, but it is unclear whether th

64 o intact planets have been detected in close orbits around white dwarfs.

65 scopically detectable giant planets in close orbits around white dwarfs.

66 ehavior in that they executed cyclotron-like orbits associated with the underlying topology.

67 The slight improvement noted in both orbits at 12 months may be the result of natural remissi

68 Belt, a class of small bodies in undisturbed orbits beyond Neptune, is composed of primitive objects

69 t of the lobes indicates that they were a co-orbiting binary that experienced angular momentum loss a

70 dio pulsars in short-period eccentric binary orbits can be used to study both gravitational dynamics

71 Hippocamp orbits close to Proteus, the outermost and largest of th

72 Our results imply that most rocky exoplanets orbiting closer to their star than the habitable zone th

73 The Weyl orbits consist of Fermi arcs (open arc-like surface stat

74 mately 60% compared to a geostationary Earth orbit constellation with similar coverage over typical s

75 Satellites launched into orbit contribute to-and risk damage from-a growing build

76 prepare neutron beams with lattices of spin-orbit correlations, as demonstrated by their spin-depend

77 ellations with significantly reduced mass-to-orbit costs and increased design life.

78 etic one-way spin switch device using a spin-orbit coupled Bose-Einstein condensate subjected to a mo

79 eractions can be tailored and probed in spin-orbit coupled heterostructures by engineering subtle str

80 at a nonmagnetic impurity can introduce spin-orbit coupled magnetic resonance in topological magnets.

81 rating the pseudo-Jahn-Teller effect of spin-orbit-coupled complex oxides.

82 owever, quantum materials hosting ideal spin-orbit-coupled kagome lattices with strong out-of-plane m

83 %, the metamagnetic transition field of spin-orbit-coupled Mott insulator Sr(2) IrO(4) can be in situ

84 tacts (QPCs) in the presence of lateral spin-orbit coupling (LSOC) is studied using a number of QPCs

85 Understanding the effects of spin-orbit coupling (SOC) and many-body interactions on spin

86 s a strong driving force from efficient spin-orbit coupling (SOC) between the singlet and triplet wav

87 ials based on band inversion induced by spin-orbit coupling (SOC) effect.

88 spinor Kohn-Sham orbitals (SKSOs) with spin-orbit coupling (SOC) interaction as a basis to compute e

89 Spin-orbit coupling (SOC) is the key to realizing time-revers

90 ayer of a magnetic insulator and a high spin-orbit coupling (SOC) metal coated over a non-magnetic su

91 ra-atomic interaction parameter (U) and spin-orbit coupling (SOC) were not properly accounted for in

92 , when combined with colossal intrinsic spin-orbit coupling (SOC), theoretically give rise to giant R

93 metry breaking combined with the strong spin-orbit coupling (SOC).

94 ters are well-known to suffer from weak spin-orbit coupling and a high reorganization energy upon pho

95 T) based wavefunctions with and without spin-orbit coupling and compute the 'spin-orbit-spillage' as

96 py induced by the combination of strong spin-orbit coupling and crystal field splitting.

97 demonstrate how the combined action of spin-orbit coupling and exchange interaction induces a strong

98 novel properties, such as large Rashba spin-orbit coupling and formation of strongly correlated elec

99 c effects and phenomena associated with spin-orbit coupling and intrinsic symmetry breaking are of im

100 However, the combined presence of spin-orbit coupling and magnetic field breaks these symmetrie

101 e classes of compounds is influenced by spin-orbit coupling and their temperature-dependent behavior

102 n temperature, together with the strong spin-orbit coupling and van der Waals structure, underlines t

103 semiconductor quantum wells with large spin-orbit coupling are capable of hosting topological superc

104 While in metallic systems, spin-orbit coupling arises from a proximate heavy metal, we s

105 cs in magnetic systems with anisotropic spin-orbit coupling as well as perspectives for the ultrafast

106 m crossing is achieved by combining the spin-orbit coupling associated to Br heavy atoms in 1,3,5,8-t

107 wing to inversion symmetry breaking and spin-orbit coupling by a heavy metal such as Pt.

108 that two-dimensional magnets with weak spin-orbit coupling can be a promising family for realizing m

109 ntum behavior mediated via effects like spin-orbit coupling can be effectively achieved by systematic

110 ounds using abundant elements with high spin-orbit coupling for sustainable electroluminescent device

111 al magnetism gives rise to an intrinsic spin-orbit coupling generating interfacial DMI at mirror symm

112 , emerges as a general result of strong spin-orbit coupling in a 2D electron system.

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

114 in Fe(3)Sn(2) are subject to intrinsic spin-orbit coupling in the d electron sector which is likely

115 ensity of InAs, we are able to tune the spin-orbit coupling in the Josephson junction.

116 study uncovers the role of anisotropic spin-orbit coupling in the spin dynamics in a half-metallic L

117 d spin-valley symmetry, consistent with spin-orbit coupling induced in the TBG via its proximity to W

118 Spin-orbit coupling is a fundamental mechanism that connects

119 optical domain, an analogous synthetic spin-orbit coupling is accessible by engineering optical anis

120 w 0.1 eV our data are best explained if spin-orbit coupling is included, suggesting that at these ene

121 While the spin-orbit coupling is known to play a pivotal role in the ul

122 near T(N)/T(s), and such effects due to spin-orbit coupling must be taken into account to unveil the

123 Spin-orbit coupling of light has come to the fore in nanoopti

124 ant copper requires overcoming the weak spin-orbit coupling of the light metal as well as limiting th

125 onic transitions most influenced by the spin-orbit coupling of the Mn(III) ion.

126 , we systematically study the effect of spin-orbit coupling on dipole-dipole energy transfer in MOFs

127 tization, the effect of the anisotropic spin-orbit coupling on the transient magnetization remains an

128 Spin-orbit coupling opens a large gap of 80 meV at the quadra

129 cs, also introduce scope for tuning the spin-orbit coupling properties and metal-ligand covalency in

130 ana zero modes in materials with strong spin-orbit coupling proximity coupled to superconductors.

131 avy atoms in 2D-PEPI contribute a large spin-orbit coupling that influences the electronic band struc

132 d, although due to the relatively large spin-orbit coupling these materials may show great promise fo

133 ashba(12) effects, which originate from spin-orbit coupling within the NM layer and at the FM/NM inte

134 olaritons) that are subject to photonic spin-orbit coupling(11) from which Dirac cones emerge(12), an

135 ly controlled through heavy-metal-based spin-orbit coupling(9-11) or tuning of the singlet-triplet en

136 The presence of strong spin-orbit coupling, allied with symmetry breaking ensured by

137 f 1D ultracold atoms with Raman-induced spin-orbit coupling, establishing this system as a platform f

138 state with Bogoliubov Fermi surfaces if spin-orbit coupling, interband pairing and time reversal symm

139 variety of physics, including effective spin-orbit coupling, magnetic fields, spin-momentum locking,

140 n heavy atoms are present due to strong spin-orbit coupling, or when strongly bound long-lived comple

141 al time-reversal invariant systems with spin-orbit coupling, thus serving as a direct probe of the tr

142 trong spin-independent interactions and spin-orbit coupling, we show that the spinor Bose liquid conf

143 asurements show an electrically tunable spin-orbit coupling, with a spin-orbit length similar to that

144 th nontrivial topology if combined with spin-orbit coupling.

145 he broken inversion symmetry and strong spin-orbit coupling.

146 xed states arising from the anisotropic spin-orbit coupling.

147 e inversion (PT) symmetry and with weak spin-orbit coupling.

148 chiral spin textures enforced by strong spin-orbit coupling.

149 e properties of a 1D system with strong spin-orbit coupling.

150 antage of a sizable band gap and strong spin-orbit coupling.

151 n mode in the presence of an artificial spin-orbit coupling.

152 Galilean invariance in the presence of spin-orbit coupling.

153 f the conduction and valence bands, and spin-orbit coupling.

154 ong light-matter interactions and large spin-orbit coupling.

155 of its intrinsic superconductivity and spin-orbit-coupling.

156 tance, as direct consequences of strong spin-orbit couplings.

157 or their orbits; graphlet degree or graphlet orbit degree vectors, the latter being compatible with O

158 The widely varying orbits derived for the six G objects demonstrate that th

159 ogress in magnetoelectric switching and spin-orbit detection of state, and show that in comparison wi

160 s last seen in 1989, and provide astrometry, orbit determinations and size estimates for all the inne

161 rified models, we propose deeply scaled spin-orbit devices exhibiting high-speed deterministic switch

162 to reliably switch at room temperature, spin-orbit devices should be large to reduce thermal fluctuat

163 sign rules that lead to deeply scalable spin-orbit devices.

164 izes complex defect configurations, in which orbiting dynamics couples to thermodynamic chirality to

165 rk collectively demonstrates the strong spin-orbit effect of the single-atomic impurity at the quantu

166 Spin-orbit electronics (spin-orbitronics) has been widely dis

167 The discovery of the spin-orbit-entangled exciton in antiferromagnetic NiPS(3) int

168 Here we show that a spin-orbit-entangled exciton state appears below the Neel tem

169 ing four orders of magnitude for FFR of spin-orbit excited molecular ions with merged beam and electr

170 The apparent detection of an exoplanet orbiting Fomalhaut was announced in 2008.

171 Earth to ISS, video images were acquired on orbit from 16- and 32-week-old female mice.

172 s forms: distributions of graphlets or their orbits; graphlet degree or graphlet orbit degree vectors

173 sensed data, including those from satellites orbiting >700 km from the surface of Earth, can offer va

174 stems, with particular emphasis on the "spin-orbit heavy-atom effect on the light-atom" NMR shift (SO

175 to-orbital angular momentum conversion, spin-orbit hybrid entanglement, particle manipulation and tra

176 d to investigate transfers among the bounded orbits in different altitudes.

177 w type of quantum Hall effect, based on Weyl orbits in nanostructures of the three-dimensional topolo

178 algorithm correctly predicts other planetary orbits, including parabolic and hyperbolic escaping orbi

179 Recently, spin-orbit-induced spin transport phenomena have been realize

180 and show how the forces confine spinners to orbit inside the same-sign vortex cells of the wave-driv

181 ies, but they become coupled by light's spin-orbit interaction (SOI) in certain exotic geometries and

182 he interplay between superconductivity, spin-orbit interaction and magnetism.

183 These plasmonic fields undergo spin-orbit interaction and their superposition generates an a

184 The energy gap induced by spin-orbit interaction at the Dirac cone of out-of-plane orbi

185 ealize an artificial Rashba-Dresselhaus spin-orbit interaction in a liquid crystal-filled optical cav

186 Such states are enforced by very strong spin-orbit interaction in solids composed of heavy elements.

187 n detected and attributed to the strong spin-orbit interaction in this iridate.

188 , by exploiting the inherent and stable spin-orbit interaction of orbital angular momentum fiber mode

189 llows the exploration of unconventional spin-orbit interaction of phonons in this circuit platform, w

190 ometric phase derived from the photonic spin-orbit interaction provides an integrated strategy.

191 served in photonic lattices where pseudospin-orbit interaction takes place, we generalize the theory

192 theory analysis proves that under weak spin-orbit interaction, a band inversion occurs.

193 perties of total momentum conservation, spin-orbit interaction, and optical non-Hermitian symmetry br

194 ecently is the role of the relativistic spin-orbit interaction.

195 with neighboring Rh atoms with a large spin-orbit interaction.

196 aggered magnetization enabled by strong spin-orbit interaction.

197 Spin-orbit interactions lead to distinctive functionalities i

198 mon-envelope evolution, wherein the original orbit is enveloped during the red giant phase and shrink

199 s to show that the precession of the earth's orbit is the primary control on monsoon intensity.

200 The collapse of the defect orbits is punctuated by another boundary-localized nucle

201 The raised orbits, lateral line canals and weakly ossified postcran

202 lly tunable spin-orbit coupling, with a spin-orbit length similar to that of III-V materials.

203 , that have anomalously large radii, or that orbit less active stars.

204 Mice were euthanized on-orbit, livers and spleens dissected, and remaining tissu

205 ecular-weight atmospheres on warm exoplanets orbiting M-stars, we should target worlds that formed H(

206 l properties in the non-centrosymmetric spin-orbit magnet PrAlGe by combining spectroscopy and transp

207 on a high-affinity DNA sequence using freely orbiting magnetic tweezers.

208 The coupling of insulating AFMs to spin-orbit materials(3-7) enables spin transport via AFM magn

209 lecule corresponding to vibrational and spin-orbit motion, respectively.

210 The orbit of the planet is most probably the result of gravi

211 l of rod-shape bacteria is validated against orbiting of immotile bacteria in shear flows.

212 2016 and April 2017 during the ring-grazing orbits of the Cassini mission.

213 cle radiation environment over the first two orbits of the probe.

214 including parabolic and hyperbolic escaping orbits, of the solar system without learning or knowing

215 We reviewed 804 MRI studies of the orbit or brain.

216 es reveal that the gap states experience the orbit-orbit interaction through Coulomb polarization to

217 ties, strongly suggesting that their extreme orbits originate from environmental perturbations rather

218 During the red giant phase, any close-orbiting planets will be engulfed by the star(2), but mo

219 s, we report the discovery of localized spin-orbit polarons (SOPs) with three-fold rotation symmetry

220 Cassini's Grand Finale orbits provided for the first time in-situ measurements

221 correlated quantum phases in the strong spin-orbit regime in graphene heterostructures.

222 Bose-Einstein condensates (BECs) in an Earth-orbiting research laboratory, the Cold Atom Lab.

223 nt and Lense-Thirring (LT) precession of the orbit resulting from rapid rotation of the WD.

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

225 nusual objects have been found to be closely orbiting Sagittarius A*: the so-called G sources, G1 and

226 ndex (NDVI), from moderate resolution, polar-orbiting satellite sensors have widely been used for ana

227 meter Suite (VIIRS), one of the latest polar-orbiting satellite sensors.

228 n has been challenging to measure from polar orbiting satellites.

229 ace of Saturn's planet-sized moon Titan, and orbited Saturn for the next 13 years.

230 es for the Maki parameter alpha and the spin-orbit scattering constant lambda(SO).

231 Theory predicts that spin-orbit scattering leads to a Dzyaloshinskii-Moriya type e

232 field theory from a set of data of planetary orbits similar to what Kepler inherited from Tycho Brahe

233 Most known terrestrial planets orbit small stars with radii less than 60 per cent of th

234 cal predictions that hot terrestrial planets orbiting small stars may not retain substantial atmosphe

235 This system has an orbit so compact that the entire binary could fit within

236 The electron affinities (EA), spin-orbit (SO) splittings, and "symmetric"/"asymmetric" stre

237 Planetary orbit, specifically the condition of perpetual free-fall

238 ut spin-orbit coupling and compute the 'spin-orbit-spillage' as a measure of band-inversion.

239 ([Formula: see text]) and valence band spin-orbit splitting energy (Delta(SO)).

240 ized orbitals, exhibiting an intriguing spin-orbit splitting, analogous to the splitting of the topol

241 s outside the Solar System(1), most of which orbit stars that will eventually evolve into red giants

242 al intersection between (3)Q(0)/(1)Q(1) spin-orbit states is revealed by ultrafast XUV transient abso

243 nges that a human sees when viewing the spin-orbit states is shown to be equal to the number (N) of r

244 le to perceive and discriminate optical spin-orbit states.

245 Saturn-orbiting streams of material impact the F ring.

246 Results from the ORBIT study demonstrate that treatment with ocriplasmin

247 to atmospheric loss than their counterparts orbiting Sun-like stars(3-6).

248 Engineering of spin-orbit synthetic Hamiltonians in optical cavities opens t

249 cal description of a complex electronic spin-orbit system and synthetic Hamiltonians derived for the

250 several gravitationally bound particles that orbited temporarily in the Bennu environment.

251 ennu is a dark asteroid on an Earth-crossing orbit that is thought to have assembled from the fragmen

252 and proptosis improved slightly more in the orbit that was treated first.

253 of pebble-sized objects on dynamically cold orbits that enhanced the Earth's gravitational focusing

254 While only the masses of the planets orbiting the brightest stars can be determined by ground

255 multiplanet system of super-Earth exoplanets orbiting the nearby red dwarf star GJ 887.

256 e dwarf star G29-38 and transits from debris orbiting the white dwarf WD 1145+017 (ref.

257 he frequency offset as the Earth rotates and orbits the Sun.

258 From its pole-to-pole orbit, the Juno spacecraft discovered arrays of cyclonic

259 irlons, formed by groups of active particles orbiting their common center of mass.

260 ntegrations of the first [Formula: see text] orbits, thus achieving speed-ups of up to [Formula: see

261 We used ORBIT to track the DNA rotations that result from unwind

262 absence, to aberrant projections within the orbit, to a normal trajectory.

263 t of the AHE that we term the anomalous spin-orbit torque (ASOT), wherein an electric current paralle

264 rent-induced magnetization switching by spin-orbit torque (SOT) holds considerable promise for next g

265 gical insulators (TIs) can exert strong spin-orbit torque (SOT) on adjacent magnetization, offering g

266 Utilizing spin-orbit torque (SOT) to switch a magnetic moment provides

267 Magnetization switching by spin-orbit torque (SOT) via spin Hall effect represents as a

268 , initialized to their hard axes by the spin orbit torque from a heavy metal under-layer utilizing th

269 full magnetization switching by lateral spin-orbit torque in zero external magnetic field is reported

270 In this work, by studying the spin-orbit torque induced switching in the Heusler alloy Mn(2

271 n of this diffusive spin torque and the spin-orbit torque results in skyrmion motion which helps to e

272 hts that current densities required for spin-orbit torque switching of Cr(2) Ge(2) Te(6) are about tw

273 ination with magnetic fields(7) or Neel spin-orbit torque(8) is used for the information writing proc

274 n spin-structure design for controlling spin-orbit torque, enabling high-efficient antiferromagnetic

275 rromagnetic layer and components of the spin-orbit torque, we derive design rules that lead to deeply

276 Spin-orbit torques (SOTs) in multilayers of ferromagnetic (FM

277 t tool that can be leveraged to control spin-orbit torques (SOTs).

278 ostructures can generate unconventional spin-orbit torques at room temperature corresponding to out-o

279 nown that skyrmions can be driven using spin-orbit torques due to the spin-Hall effect.

280 In most cases, generation of spin-orbit torques has relied on an external injection of out

281 n into consideration when investigating spin-orbit torques in ferromagnetic/non-magnetic bilayers.

282 to the magnetization generates opposite spin-orbit torques on the surfaces of the magnetic film.

283 stable antiferromagnetic Neel vector by spin-orbit torques.

284 intronic logic device that operates via spin-orbit transduction (the coupling of an electron's angula

285 Here, we use graphlet-orbit transitions (GoTs), a different graphlet-based mea

286 plasmin Research to Better Inform Treatment (ORBIT) trial (NCT02079883) was a Phase IV multicenter, p

287 n topological magnets which can feature spin-orbit tunability.

288 atmospheres(5), in warm debris disks(6-9) or orbiting very closely(10-12), which has been interpreted

289 difference between the treated and untreated orbit was observed in any of the main outcome measures a

290 One randomly selected orbit was treated with 20 Gy of external beam therapy; s

291 imaged six small moons of Neptune, all with orbits well interior to that of the large, retrograde mo

292 zyme activity levels in tissues recovered on-orbit were of acceptable quality.

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

294 the lower-frequency one circles on the outer orbit, while the orbital motions of both spinners are sy

295 We envisage that ORBIT will enable studies of a wide range of interaction

296 on and exploration of space beyond low-Earth orbit will require small crews to live in isolation and

297 eveloped to perform experiments in low earth orbit with on-board sample recovery, thereby avoiding co

298 ons were associated with rubbing the eye and orbit with the back of the hand or wrist, rather than th

299 stem in a five-hour, low-eccentricity (0.09) orbit, with an orbital separation of 1.8 solar radii(7),

300 s from 1995-2017, which cover S0-2's 16-year orbit, with measurements from March to September 2018, w

301 at giant planets can be scattered into tight orbits without being tidally disrupted, motivating the s