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 functional-theory (DFT) model, that is fully relativistic and accounts for orbital-orbital coupling (

4 FRBs may be highly relativistic and geometrically beamed, or FRB-like event

5 We detected a combination of special relativistic and gravitational redshift, quantified usin

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

7 om classical electromagnetism to quantum and relativistic aspects.

8 These quasi-relativistic atomic orbitals may be used for improving a

9 Based on fully relativistic band structure calculations on respective c

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

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

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

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

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

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

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

17 This observation is also made in fully relativistic calculations.

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

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

20 ol of an EM field generating media including relativistic charge particle beams.

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

22 Due to the resultant collective motion of relativistic charged particles around the central axis,

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 atter interactions that take place under non-relativistic conditions.

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

27 of a radial-node in the valence-orbital and relativistic contraction/expansion of the valence/semico

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

29 e results are compared to calculations using relativistic coupled-cluster theory.

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

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

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

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

34 Relativistic DFT calculations are used to explain the di

35 Relativistic DFT calculations provide an insight into th

36 Using relativistic DFT calculations, we elucidate and discuss

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

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

39 are rooted in the underlying physics of the relativistic Dirac equation that describes the low energ

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

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

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

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

44 Hence these metamaterials mimic a relativistic effect without the need for any actual mate

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

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

47 Relativistic effects caused by the presence of an atom o

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

49 In this paper, we study the relativistic effects in a three-body bound state.

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

51 Our calculations show that the relativistic effects lead to a roughly 2% reduction in t

52 However, in groups 11 and 12, the relativistic effects maximize spatial-coincidence in the

53 A fundamental understanding of such relativistic effects on NMR shifts is important in many

54 The relativistic effects on three-body binding energy are ca

55 of very high-energy electrons (VHEEs) due to relativistic effects reduces scattering and enables irra

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

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

58 The role of relativistic effects was examined, and the analysis is e

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

60 -art in quantum accelerometers by exploiting relativistic effects.

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

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

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

64 icle accelerators capable of producing ultra-relativistic electron beams.

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

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

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

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

69 ons near the bulk of the laser target, these relativistic electron currents are subject to plasma ins

70 Here we use crystallographic measurements by relativistic electron diffraction to demonstrate that te

71 their optimization requires knowledge of the relativistic electron dynamics and the fields they produ

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

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

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

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

76 subsequent outward radial diffusion of ultra-relativistic electron populations.

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

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

79 All-electron relativistic electronic structure calculations can predi

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

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

82 This emission requires a population of relativistic electrons and a magnetic field located in a

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

84 These relativistic electrons are effectively collisionless, an

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

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

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

88 ations for understanding the origin of ultra-relativistic electrons in Earth's radiation belts, as we

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

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

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

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

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

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

95 , Dirac proposed a wave equation to describe relativistic electrons(1).

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

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

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

99 teristic of synchrotron radiation, requiring relativistic electrons.

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

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

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

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

104 ten involve the acceleration of particles to relativistic energies and the generation of high-intensi

105 However, whether electrons at these ultra-relativistic energies are locally accelerated, arise fro

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

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

108 ated from a few kiloelectronvolts up to near-relativistic energies via at least two processes: 'impul

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

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

111 which shows an excellent agreement with the relativistic energy eigenvalue.

112 we envisage the use of these ligands for the relativistic enhancement of radiative deactivation rate

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

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

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

116 The combination of relativistic fermion behaviour and ferromagnetism in Sr1

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

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

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

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

121 Relativistic fermions in topological quantum materials a

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

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

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

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

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

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

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

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

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

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

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

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

134 For this purpose, the relativistic form of the Faddeev equations is solved in

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

136 LT precession, an effect of relativistic frame dragging, is a prediction of general

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

138 e clocks for inertial navigation systems and relativistic geodesy.

139 d thin foil targets, but generally describes relativistic harmonic generation, including at normal in

140 retical work the ultimate efficiency of this relativistic high-order-harmonic generation remains uncl

141 -velocity features originate from the mildly relativistic hot cocoon that is generated by an ultra-re

142 nd nonzero total momenta, a manifestation of relativistic hydrodynamics.

143 In particular, when a relativistic intense laser focus interacts with a thin s

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

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

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

147 magnetic components of light at modest (non-relativistic) intensities.

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

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

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

151 tself, are believed to originate in an ultra-relativistic jet breaking out from a massive stellar env

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

153 on may have been produced by either a narrow relativistic jet or an isotropic outflow.

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

155 tic hot cocoon that is generated by an ultra-relativistic jet within the gamma-ray burst expanding an

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

157 alculations, of photospheric emission from a relativistic jet.

158 dicating that GW170817 produced a structured relativistic jet.

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

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

161 Relativistic jets are not expected to be produced by sou

162 Powerful relativistic jets are one of the main ways in which accr

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

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

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

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

167 gamma-ray bursts (GRBs) originate from ultra-relativistic jets launched from the collapsing cores of

168 in some active galactic nuclei (AGN) drives relativistic jets of plasma, which dissipate a significa

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

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

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

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

173 complex microphysics of realistic shocks in relativistic jets.

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

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

176 magnon group velocity serves as an analogous relativistic limit for the speed of magnetic solitons.

177 of 4300 meters per second-within ~10% of the relativistic limit-and we observe key signatures of rela

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

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

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

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

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

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

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

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

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

187 istic limit-and we observe key signatures of relativistic motion associated with Lorentz contraction,

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

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

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

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

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

193 e infrared sources will open up new areas of relativistic nonlinear optics of plasmas, impulse IR spe

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

195 uon fluid (the "subatomic swirl") created in relativistic nuclear collisions.

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 istent with curvature effects arising in the relativistic outflow.

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

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

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

205 A relativistic particle undergoing successive boosts which

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

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

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

209 , and is in turn the principal source of the relativistic particles required to power the synchrotron

210 cks constructed from the internal degrees of relativistic particles that move through curved spacetim

211 energy release leading to the production of relativistic particles that now populate huge cavities o

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

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

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

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

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

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

218 may reaccelerate a preexisting population of relativistic particles, producing emission at radio wave

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

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

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

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

223 s rotation of coordinate axes is caused by a relativistic phenomenon called Thomas Rotation.

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

225 lling and a manifestation of the underlying 'relativistic' physics of a proximity-induced superconduc

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

227 Relativistic plasma mirrors generate broadband power-law

228 expected to behave like a quantum-critical, relativistic plasma-the "Dirac fluid"-in which massless

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

230 and inexpensive source of high-quality ultra-relativistic positrons for laser-driven and particle-dri

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

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

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

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

235 This result is compared to state-of-the-art relativistic quantum mechanical calculations that incorp

236 Exact solutions of a novel quasi-relativistic quantum mechanical wave equation are found

237 However, relativistic quantum mechanics allows for generating cur

238 we see that the symmetry group relating non-relativistic quantum mechanics and special relativity vi

239 Relativistic quantum mechanics predicts that when the ch

240 h emergent electronic properties governed by relativistic quantum mechanics.

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

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

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

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

245 lids, by which a clear method for discerning relativistic quasiparticles has not yet been established

246 Detecting the spectroscopic signatures of relativistic quasiparticles in emergent topological mate

247 ethod for detecting the magnetic response of relativistic quasiparticles in topological materials.

248 om the saturating magnetic responses for non-relativistic quasiparticles, the non-saturating signals

249 and Weyl nodal materials can host low-energy relativistic quasiparticles.

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

251 of Weibel Instability, and corroborated the relativistic radial expansion of the ionization front, w

252 mum) resolution shadowgraphy video capturing relativistic radial ionization front expansion and the a

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

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

255 o a supermassive black hole should exhibit a relativistic redshift.

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

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

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

259 uantities like electromagnetic fields in the relativistic regime.

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

261 conventional dielectric breakdown or involve relativistic runaway electron processes.

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

263 nd the light transmitted due to the onset of relativistic self-induced transparency.

264 s invoke neutron star magnetospheres(3-5) or relativistic shocks far from the central energy source(6

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

266 ct objects (neutron stars or black holes) or relativistic shocks launched from such objects have been

267 and disfavours the radiation models invoking relativistic shocks.

268 y accessible experimental framework to study relativistic solitonic physics.

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

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

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

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

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

274 lines, characteristic of baryonic jets with relativistic speeds.

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

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

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

278 h as the calculation of frequency shifts for relativistic spin-1/2 particles undergoing Larmor preces

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

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

281 cance relatively recently is the role of the relativistic spin-orbit interaction.

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

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

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

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

286 Since relativistic thermodynamics is a topic that can be treat

287 The construction of a relativistic thermodynamics theory is still controversia

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

289 ddeev components in the normalization of the relativistic three-body wave function is studied in deta

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

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

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

293 t-pulse laser to accelerate deuterons in the relativistic transparency regime.

294 We constrain the relativistic treatment of the pulsar polarization model

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

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

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 ls are crystalline solids that host emergent relativistic Weyl fermions and have characteristic surfa

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