ライフサイエンスコーパス: relativistic

1 Relativistic (60-MeV) electrons are energy-modulated ove

2 both on clusters and on periodic structures, relativistic ab initio wave function calculations that i

3 erived from the total energies obtained from relativistic and parameter-free density-functional theor

4 om classical electromagnetism to quantum and relativistic aspects.

5 Based on fully relativistic band structure calculations on respective c

6 ons can be seen as further validation of the relativistic beaming theory.

7 ated over the binary orbital period owing to relativistic beaming.

8 by the recent demonstration of laser-driven relativistic beams of monoenergetic electrons.

9 network of cosmological tests show that the relativistic Big Bang theory is a good description of ou

10 ing laser-plasma-accelerators, we reproduced relativistic, broadband radiation belt flux in the labor

11 e-density plasma wave is excited by an ultra-relativistic bunch of charged particles (the drive bunch

12 fields is driven by the passage of an ultra-relativistic bunch of charged particles (the drive bunch

13 by reverse shock emission cogenerated in the relativistic burst ejecta as it collides with surroundin

14 State-of-the-art four-component relativistic calculations of the chemical shift tensors

15 This observation is also made in fully relativistic calculations.

16 Recently, two 'relativistic' candidate tidal disruption events were dis

17 r observations are therefore consistent with relativistic causality and help to resolve the controver

18 Violation of this principle of relativistic causality leads to paradoxes, such as that

19 In the context of Electromagnetics, the relativistic causality limits the upper bound of the vel

20 However, as a consequence of the relativistic character of the charge carriers, the integ

21 are the charge carriers' two-dimensional and relativistic character.

22 by an intense laser pulse or an ultra-short relativistic charged particle beam.

23 ms of the exponential integral function with relativistic co-ordinate transform, allowing application

24 uggest that breakout of a wide-angle, mildly relativistic cocoon engulfing the jet explains the low-l

25 on: a narrow (5 degrees opening angle) ultra-relativistic component responsible for the gamma-rays an

26 rays and early afterglow, and a wide, mildly relativistic component that produces the radio and optic

27 s led to the emergence of a new paradigm of 'relativistic' condensed-matter physics, where quantum re

28 ding feature of the dioxazole moiety and the relativistic contraction of the Ir(V), which affords muc

29 u3Ge, with vec = 9, derives from significant relativistic contribution of the Au 5d(10) states to the

30 Scalar relativistic corrections and zero-point vibrational ener

31 By measuring relativistic corrections to the Keplerian description of

32 ed with and embedded in non-baryonic and non-relativistic dark matter, which dominates the total mass

33 Using relativistic density functional calculations, we found t

34 7 K, based on agreement between observed and relativistic density functional theory (DFT) calculated

35 a photoelectron spectroscopy (PES) and quasi-relativistic density functional theory (DFT) study of Au

36 azido (N(3)(-)) complexes are studied using relativistic density functional theory (DFT).

37 A relativistic density functional theory description of th

38 bed on the R (or S) enantiomer of Au40 using relativistic density functional theory.

39 cating a striking universality of the pseudo-relativistic description of the Kane fermions in HgCdTe.

40 Relativistic DFT calculations are used to explain the di

41 Relativistic DFT calculations provide an insight into th

42 Using relativistic DFT calculations, we elucidate and discuss

43 meters of [Mo 17O(SPh)4]- predicted by quasi-relativistic DFT calculations, were in good agreement wi

44 Experimental measurements are supported by relativistic DFT calculations, which confirm the presenc

45 eans of DFT calculations, which show how the relativistic differences between Au and Ag are manifeste

46 tum matter with a bulk gap and odd number of relativistic Dirac fermions on the surface.

47 he Talbot effect should exist in the case of relativistic Dirac fermions with nonzero mass.

48 lations are calibrated against all-electron, relativistic Dirac-Hartree-Fock, and coupled-cluster wit

49 Relativistic distortion of the line makes it sensitive t

50 light curve of PG 1302-102 can be fitted by relativistic Doppler boosting of emission from a compact

51 3-millisecond pulsar J0737-3039A in a highly relativistic double neutron star system, allowing unprec

52 ead to quasiparticles mimicking the massless relativistic dynamics of high-energy particle physics, a

53 Using hybrid DFT calculations with relativistic effective core potentials, the electronic s

54 nzerhof density functional and the Stuttgart relativistic effective-core-potential basis sets.

55 ists of disordered magnetic moments with all relativistic effects and explicit orbital-orbital correl

56 the context of theoretical studies on gold; relativistic effects are especially helpful in rationali

57 LMTO-ASA calculations show that scalar relativistic effects are particularly important for Hg 5

58 the theory of condensed matter, but quantum relativistic effects are usually minute in the known exp

59 h in the neutral and charged adducts without relativistic effects becomes Cu > Ag > Au.

60 However, relativistic effects couple the spin and orbital motion,

61 ater-type basis set with inclusion of scalar relativistic effects gives geometrical parameters and vi

62 at dynamical effects of Xe motion as well as relativistic effects have significant contributions to t

63 the closed-shell nature of the d states and relativistic effects in gold.

64 gular approximation (ZORA) in order to treat relativistic effects on the Pt shielding tensors.

65 This reaction mechanism is a consequence of relativistic effects that lower the energies of the merc

66 ormed to high precision, taking into account relativistic effects that scale approximately as the squ

67 racter in the Au-C bonding due to the strong relativistic effects was revealed in Au(CN)(2)(-), consi

68 ore-valence effects, a correction for scalar relativistic effects, a correction for first-order atomi

69 -order regular approximation (ZORA) to treat relativistic effects, and Born-Oppenheimer molecular dyn

70 this unusual property of Hg is attributed to relativistic effects, Zn, which is much less massive tha

71 -art in quantum accelerometers by exploiting relativistic effects.

72 This suggests that the production of relativistic ejecta is the key physical distinction betw

73 ering the burst, the properties of the ultra-relativistic ejecta of the explosion, and the ejecta's i

74 the presence of 10(48) erg coupled to mildly relativistic ejecta, along with a central engine (an acc

75 jet, viewed off-axis, or a cocoon of mildly relativistic ejecta.

76 rators based on wakefields, where an intense relativistic electron beam radiates the demanded fields

77 by measuring changes of the kinetic state of relativistic electron beams.

78 a wakefield accelerator cavity produced by a relativistic electron bunch can be mapped using the bunc

79 This method uses a few femtoseconds long relativistic electron bunch to probe the wake produced i

80 n superradiant enhancement of radiation from relativistic electron bunches in a compact electron acce

81 cceleration scheme for generating ultradense relativistic electron bunches in helical motions and hen

82 rgy and angular distribution of the observed relativistic electron flux increase.

83 t earthward 0.3 Earth radii and enhanced the relativistic electron fluxes by up to one order of magni

84 nt loss of ultra-relativistic electrons, the relativistic electron population is almost unaffected.

85 t EMIC waves may account for the loss of the relativistic electron population.

86 reservoirs, single Dirac fermion emission in relativistic electron quantum optics and read-out of spi

87 s with pseudospin, a lattice analogue of the relativistic electron spin, whereas the multilayer struc

88 All-electron relativistic electronic structure calculations can predi

89 he phenomenon with large anisotropies in the relativistic electronic structure.

90 If a second bunch of relativistic electrons (the trailing bunch) with suffici

91 multiples of photon quanta (nhomega) by the relativistic electrons accelerated to 200 keV.

92 radiation is generated by the separation of relativistic electrons and positrons in the geomagnetic

93 er that describes coupling between light and relativistic electrons and that is traditionally associa

94 Here we show that although relativistic electrons are enhanced, ultra-relativistic

95 Relativistic electrons are generated through the breakin

96 h relativistic electrons are enhanced, ultra-relativistic electrons become depleted and distributions

97 X-rays radiated by relativistic electrons driven by well-controlled high-po

98 es, rely on bunching of relativistic or near-relativistic electrons in vacuum.

99 Here we report measurements of relativistic electrons near the inner edge of the inner

100 nusual butterfly pitch angle distribution of relativistic electrons occurred within 5 Earth radii dur

101 optical analogue of Klein tunneling for the relativistic electrons passing across a potential barrie

102 The transport of hot, relativistic electrons produced by the interaction of an

103 Van Allen radiation belts consist of relativistic electrons trapped by Earth's magnetic field

104 ditions--it is possible to generate beams of relativistic electrons with low divergence and a small e

105 mmonly used for accelerating and collimating relativistic electrons, or to manipulate intense laser p

106 o exist in conventional materials harbouring relativistic electrons, such as graphene or bismuth.

107 esponsible for the significant loss of ultra-relativistic electrons, the relativistic electron popula

108 emtosecond laser pulses by a solid unleashes relativistic electrons, thereby creating a regime of rel

109 ism of wave-driven butterfly distribution of relativistic electrons.

110 e for the radial diffusion of radiation belt relativistic electrons.

111 teristic of synchrotron radiation, requiring relativistic electrons.

112 waves mainly contribute to the loss of ultra-relativistic electrons.

113 , including charge carriers that mimic ultra-relativistic elementary particles.

114 provide the dominant loss mechanism at ultra-relativistic energies and produce a profound dropout of

115 or acceleration of lower-energy electrons to relativistic energies in situ in the heart of the radiat

116 radiation belt electrons are accelerated to relativistic energies remains an unanswered question.

117 field) distribution of electrons up to ultra-relativistic energies.

118 ying interaction between forward currents of relativistic energy "hot" electrons created by the laser

119 ransport is essentially governed by Dirac's (relativistic) equation.

120 ear spin configurations and is driven by non-relativistic exchange-strictive mechanisms.

121 collapse also powers an even more brilliant relativistic explosion known as a long-duration gamma-ra

122 flux observed is close to the value at which relativistic feedback processes become important, with a

123 -yMn1-zSb2 (y, z < 0.1) with nearly massless relativistic fermion behaviour (m( *) = 0.04 - 0.05m0, w

124 The combination of relativistic fermion behaviour and ferromagnetism in Sr1

125 Weyl particles are elusive relativistic fermionic particles with vanishing mass.

126 Under magnetic fields, relativistic fermions acquire Berry phase of pi in cyclo

127 rtunity to investigate the interplay between relativistic fermions and spontaneous TRS breaking.

128 tunities to explore the exotic properties of relativistic fermions in condensed matter.

129 Relativistic fermions in topological quantum materials a

130 te a condensed-matter realization of massive relativistic fermions in two dimensions.

131 This charge-neutral plasma of quasi-relativistic fermions is expected to exhibit a substanti

132 possible to realize two-dimensional gases of relativistic fermions with unprecedented transport prope

133 ation (a theoretical description of massless relativistic fermions).

134 ac Hamiltonian, which successfully describes relativistic fermions, applies equally well to electrons

135 in a strongly out of equilibrium gas of hot relativistic fermions, characterized by a surprisingly l

136 at the crossing point, a signature unique to relativistic fermions.

137 nism itself remain enigmatic because, once a relativistic fireball is created, the physics of the aft

138 e show that the burst is powered by the same relativistic fireball mechanism as long GRBs, with the e

139 rature scanning tunnelling spectroscopy, and relativistic first-principles calculations.

140 best indirect evidence being the unseen fast relativistic flow inferred to energize slower components

141 is the 'internal shock model', in which the relativistic flow is unsteady.

142 Our hydrodynamic theory consists of relativistic fluids at each Weyl node, coupled together

143 nctional theory (DFT) with the semiempirical relativistic force field (RFF) method of Kutateladze and

144 to the data, calculated as the ratio of the relativistic form factors of the phantom material and bo

145 e spin density in the MSOs calculated at the relativistic four-component DFT level are discussed and

146 in 10(18) enables new timing applications in relativistic geodesy, enhanced Earth- and space-based na

147 e clocks for inertial navigation systems and relativistic geodesy.

148 The Shapiro delay is a general-relativistic increase in light travel time through the c

149 of femtosecond optical laser pulses, E, with relativistic intensities I > 10(21) W/cm(2) is efficient

150 At relativistic intensities, the focus has been mainly on i

151 gineering light-matter interactions at ultra-relativistic intensities.

152 ields created in an overdense, hot plasma by relativistic intensity (10(18) W/cm(2)) femtosecond lase

153 ds the role of J x B absorption mechanism at relativistic intensity.

154 rtz (THz) source based on the interaction of relativistic-intensity femtosecond lasers with aligned c

155 conclude that we have captured the onset of relativistic jet activity from a supermassive black hole

156 X-ray and radio emission is due to an ultra-relativistic jet being launched during the merger (and s

157 ed hypothesis is that they are produced by a relativistic jet created by the merger of two compact st

158 ay spectral shape are consistent with beamed relativistic jet emission from an accreting stellar blac

159 sources; the radio emission originates in a relativistic jet thought to be launched from the innermo

160 interpreted as the onset of emission from a relativistic jet.

161 s a rare opportunity to study the birth of a relativistic jet.

162 clear, as is the mechanism for launching the relativistic jets and their composition.

163 Such relativistic jets are not expected to be launched from w

164 Relativistic jets are not expected to be produced by sou

165 The formation of relativistic jets by an accreting compact object is one

166 theory is poorly understood, observations of relativistic jets from systems known as microquasars (co

167 Thus the unexpected presence of relativistic jets in a ULS challenges canonical theories

168 logical distances, thought to originate from relativistic jets launched at the deaths of massive star

169 Numerical simulations imply that the relativistic jets often seen from accreting black holes

170 to central supermassive black holes, produce relativistic jets with lifetimes of at least one million

171 Stellar-mass black holes with relativistic jets, also known as microquasars, mimic the

172 Accreting black holes are known to power relativistic jets, both in stellar-mass binary systems a

173 sion in galaxy cores and to the formation of relativistic jets, but no observations to date have been

174 (BHs) produce intense radiation and powerful relativistic jets, which are affected by the BH's spin m

175 mately 10% of active galactic nuclei exhibit relativistic jets, which are powered by the accretion of

176 Black holes generate collimated, relativistic jets, which have been observed in gamma-ray

177 complex microphysics of realistic shocks in relativistic jets.

178 es could then also have a broad influence on relativistic laser-matter interactions.

179 er platform for studying quasiparticles with relativistic-like features.

180 ed by these gauge fields can be taken to the relativistic magnetic quantum limit, which has so far be

181 ults from global, three-dimensional, general-relativistic magnetohydrodynamic turbulence simulations.

182 We used fully three-dimensional general relativistic magnetohydrodynamical simulations to study

183 ns cannot be achieved using state-of-the-art relativistic many-body calculations that include quantum

184 Specifically, we show that the general relativistic mass-energy equivalence implies gravitation

185 dispersion of electrons on demand, enabling relativistic massless Dirac quasiparticles, and thus ind

186 A major complication is that the relativistic massless electrons in pristine graphene exh

187 the low energy excitations behave like ultra-relativistic massless particles with linear energy dispe

188 gy-momentum relations that resemble those of relativistic massless particles.

189 quantum Fisher information we determine how relativistic motion modifies the ultimate bound in the p

190 We show how to use relativistic motion to generate continuous variable Gaus

191 ssible to tune with ultrafast light pulses a relativistic nanoscale Schottky barrier, in a way that i

192 takes on its full significance whenever its relativistic nature, in the short- and long terms, is ta

193 The total pressure due to the relativistic, non-thermal population of electrons can be

194 However, the general relativistic notion of time is recovered in the classica

195 event such as a supernova or coalescence of relativistic objects.

196 e coherent potential approximation and fully relativistic one-step-model photoemission calculations i

197 icles to intense laser light is intrinsic to relativistic optics, the development of compact laser-dr

198 stic electrons, thereby creating a regime of relativistic optics.

199 lasers and vacuum tubes, rely on bunching of relativistic or near-relativistic electrons in vacuum.

200 e separated by 0.007-0.017 parsecs, implying relativistic orbital speeds.

201 9A and B) were recently discovered in highly relativistic orbits around one another.

202 mpt emission to internal shocks in the ultra-relativistic outflow generated by the internal engine; e

203 A relativistic outflow is not predicted in this situation,

204 he production of an energetic and collimated relativistic outflow powered by a central engine (an acc

205 Ibc SN 2009bb, which requires a substantial relativistic outflow powered by a central engine.

206 ingle physical region, implying an extremely relativistic outflow that propagates within the narrow i

207 There is evidence for a mildly relativistic outflow, jet collimation, and a spectrum ch

208 e conclude that we are seeing a newly formed relativistic outflow, launched by transient accretion on

209 istent with curvature effects arising in the relativistic outflow.

210 RBs) are most probably powered by collimated relativistic outflows (jets) from accreting black holes

211 radio searches for type Ibc supernovae with relativistic outflows.

212 ynchrotron emission indicative of shocks and relativistic particle acceleration, thereby pinpointing

213 This has enabled exciting applications of relativistic particle beams and coherent X-ray radiation

214 has been proposed that the powerful jets of relativistic particles (such as electrons) launched by s

215 nvolt gamma-ray wavelengths, suggesting that relativistic particles are accelerated by strong shocks

216 to their close resemblance to elusive ultra-relativistic particles as well as their potential for fu

217 and holes in this material closely resemble relativistic particles with a non-zero rest mass.

218 ions-charge carriers that behave as massless relativistic particles with an intrinsic angular momentu

219 The charge carriers in graphene mimic relativistic particles with zero rest mass and have an e

220 anks to charge carriers which mimic massless relativistic particles, and (iii) it has promise for a n

221 anks to charge carriers which mimic massless relativistic particles, and (iii) it has promise for a n

222 Electrons therein behave as massless relativistic particles, giving rise to strikingly unconv

223 The requirement for relativistic particles, however, makes Cerenkov emission

224 ne, where charge carriers behave as massless relativistic particles, it has been predicted that highl

225 Like massless relativistic particles, they have linear dispersion and

226 oduce 'jets'--collimated bipolar outflows of relativistic particles.

227 ant flare in the form of magnetic fields and relativistic particles.

228 e fermions, cannot be described by any other relativistic particles.

229 lation (HYSCORE), and IR fingerprints, using relativistic Pauli and ZORA-SOMF/B3LYP methods.

230 The relativistic periastron advance for the two eccentric sy

231 or spintronics explores spin-related quantum relativistic phenomena in solid-state systems.

232 tic' condensed-matter physics, where quantum relativistic phenomena, some of which are unobservable i

233 It plays a crucial role in relativistic phenomena, such as Klein tunneling, but it

234 The long-sought relativistic phenomenon of massless Dirac fermions, know

235 Cerenkov radiation, a relativistic physical phenomenon that was discovered 70

236 We recently demonstrated that a relativistic plasma aperture produced in an ultra-thin f

237 a massive black hole is believed to feed the relativistic plasma jets found in many active galactic n

238 ated through the breaking of large-amplitude relativistic plasma waves created in the wake of the las

239 al galaxies, through inflation of bubbles of relativistic plasma.

240 We discuss how such general relativistic positional information (GRPI) can guide sys

241 addition, we can estimate the mass using the relativistic precession model, from which we get a value

242 ct values of E(G) different from the general relativistic prediction because, in these theories, the

243 f megaparsecs, in agreement with the general relativistic prediction of E(G) approximately 0.4.

244 We investigate relativistic quantum AB rings threaded by a magnetic flu

245 By using matrix infrared spectroscopy and relativistic quantum chemistry calculations, we have sho

246 um computation, our results pave the way for relativistic quantum computation schemes.

247 gent fermionic quasiparticles not present in relativistic quantum field theory.

248 However, relativistic quantum mechanics allows for generating cur

249 Relativistic quantum mechanics predicts that when the ch

250 In non-relativistic quantum mechanics, these are independent, r

251 h emergent electronic properties governed by relativistic quantum mechanics.

252 We present a framework for relativistic quantum metrology that is useful for both E

253 graphene, with its charge carriers mimicking relativistic quantum particles and its formidable potent

254 equation, which allows the investigation of relativistic quantum phenomena in a benchtop experiment.

255 e SPCs can be attributed to a robust type of relativistic quantum states, i.e., Dirac whispering gall

256 Our discovery of WGMs in relativistic quantum systems is remarkable because, alth

257 be applied to develop a novel generation of relativistic quantum technologies for gravimeters, clock

258 n potentially be the base for a new class of relativistic qubit systems.

259 and produce a profound dropout of the ultra-relativistic radiation belt fluxes.

260 Here using a relativistic Rankine-Hugoniot-like analysis, we show for

261 spin of black holes is through the study of relativistic reflection features from the inner accretio

262 as hitherto been no significant detection of relativistic reflection features in a moderate-redshift

263 the existence of a binary black hole in the relativistic regime.

264 Measurements suggest the presence of relativistic runaway electron avalanches (RREA), the sam

265 conventional dielectric breakdown or involve relativistic runaway electron processes.

266 We developed a quantum algorithm to compute relativistic scattering probabilities in a massive quant

267 that can be described accurately by the non-relativistic Schrodinger equation.

268 dynamics, one relative to the other, using 'relativistic' sets of residual dipolar couplings (RDCs).

269 ted that particles are accelerated at mildly relativistic shocks generated by the collisions of mater

270 ine our understanding of GRB progenitors and relativistic shocks, gamma-ray observations alone have n

271 a fundamental property of electrons with the relativistic spectrum found in graphene and topological

272 positive temperature is that they have a non-relativistic speed of sound that is infinite.

273 This persistent wind is expelled at relativistic speeds from the inner accretion disk, and i

274 Electrons at relativistic speeds, diffusing in magnetic fields, cause

275 le, and if the baryons can be accelerated to relativistic speeds, the jets should be strong sources o

276 lines, characteristic of baryonic jets with relativistic speeds.

277 izing a large number of charged particles to relativistic speeds.

278 Recently discovered relativistic spin torques induced by a lateral current a

279 rceived two model physical mechanisms of the relativistic spin torques, one driven by the spin-Hall e

280 a HOMO-LUMO gap, the Jahn-Teller effect and relativistic spin-orbit coupling.

281 ues for these parameters were computed using relativistic spin-orbit density functional theory with a

282 magnons into high-frequency currents via the relativistic spin-orbit interaction.

283 Recent experiments have demonstrated that relativistic spin-orbit torques can provide the means fo

284 These single valley relativistic states, massless Kane fermions, cannot be d

285 Independently, a second mildly relativistic supernova has been reported.

286 ometres per second, believed to originate in relativistic (that is, near the speed of light) disk win

287 moment of the electron, inspired Schwinger's relativistic theory of quantum electrodynamics and gave

288 Since relativistic thermodynamics is a topic that can be treat

289 The construction of a relativistic thermodynamics theory is still controversia

290 we present a review of the main theories of relativistic thermodynamics, with an special emphasis on

291 s HgCdTe offer another realization of pseudo-relativistic three-dimensional particles in condensed ma

292 e date there is no agreement on which set of relativistic transformations of thermodynamic quantities

293 We also present a set of relativistic transformations that we have derived by ass

294 ibutions to the total NMR chemical shifts, a relativistic two-component DFT approach was used.

295 Jets of highly energized plasma with relativistic velocities are associated with black holes

296 very high-energy, heavy ions accelerated to relativistic velocities, to stabilize a high-pressure ph

297 a powerful accretion-disk wind with a mildly relativistic velocity (a quarter that of light) in the X

298 derived directly from the linearized general relativistic wave equation alone, for an arbitrary gauge

299 radio data require the existence of a mildly relativistic wide-angle outflow moving towards us.

300 e aiMD trajectories, using the two-component relativistic zeroth-order regular approximation (ZORA) i