ライフサイエンスコーパス: spin

1 responsivity and anxiety throughout the life span.

2 nt number, power, duration, and/or frequency span.

3 and fibrinogen- varied across the adult age span.

4 antized harmonic fluctuations of the ordered spins.

5 electrons and robust storage in the nuclear spins.

6 After a 3 minute spin, 100% of samples were undetectable using either ass

7 The activation energies of the process span 135 kJ/mol to 226 kJ/mol, and 188 kJ/mol to 268 kJ/

8 Over the 10-y span, 56 US dental institutions received approximately $

9 The experiments we review span a range of methodological techniques, including neu

10 ion energy and its component parts, and they span a very broad range from 20 kBT to 150 kBT, dependin

11 Estimated fluxes span a wide range due to the range of diffusivity measur

12 king, institutions that enable management to span across administrative boundaries, adaptive manageme

13 the isomerization and associated ISC on the (spin) adiabatic ground potential energy surface.

14 to a 90% increase in potential ferromagnetic spin alignments in the central layer and this could be s

15 bsorb a photon to produce a singlet exciton, spin-allowed singlet fission may produce two triplet exc

16 ity that is in steady state at a longer time span and is less dependent on neurovascular coupling.

17 nic devices that rely on optical steering of spin and charge currents.

18 ations of material properties such as atomic spin and orbital magnetic moments and local magnetocryst

19 light propagation direction reverses photon spin and thus the direction of the photocurrent.

20 ange interaction between conducting electron spins and local magnetic moments.

21 OS under different coupling strength between spins and the thermal bath in the macroscopic Fockker-Pl

22 rs which have five orders of magnitude fewer spins and which require resonant optical excitations to

23 ess the flip-flop rate of the neighbour bath spins and yield a specific environment spectral density

24 Here, by using spin- and angle-resolved photoemission spectroscopy, we

25 Optical elements that convert the spin angular momentum (SAM) of light into vortex beams h

26 of moderate strength significantly alter the spin arrangement within the system-a behavior that manif

27 Use of molecular electron spins as qubits for quantum computing will depend on the

28 ure with an unexpected partially delocalized spin, as evidenced by electron paramagnetic resonance sp

29 For spin-based computing to become widespread, however, ener

30 Also, whereas the previous proposals for spin-based logic require extra devices in each individua

31 loited for long-term data storage or nuclear-spin-based quantum memory.

32 Toward this end, embedding electronic-spin-based qubits within the framework of a crystalline

33 n essential ingredient in many proposals for spin-based technologies because it would enable both of

34 future device concepts in optoelectronic and spin-based technologies.

35 ignificant differences were observed in life span between genders, where females survived longer than

36 of nuclear spins relative to the electronic spin center affects decoherence.

37 The exchange interaction, J, between two spin centres is a convenient measure of through bond ele

38 show that the exchange coupling between two spin centres is increased by a factor of 4.5 in the ring

39 based approach to simulate the dynamics of a spin chain and maximise the entanglement generation.

40 iples calculations, we reveal explicitly the spin chain scenario in CN by displaying the calculated e

41 In particular, simulating Dyson's original spin chain with the most memory-efficient classical algo

42 (1.2 x 1012GC), exhibited an increased life span, characterized by delayed weight loss and diminishe

43 ons in Cd2Os2O7 and that it exhibits complex spin-charge-lattice coupling.

44 ed cells and three types of scaffolds (i.e., spun coat, large microfiber, and medium microfiber).

45 ilm is fabricated by a low-cost and scalable spin coating process using ink solution with a truly sol

46 The one-step spin-coating process of perovskites is investigated in s

47 ng nuclear notch filtering, we demonstrate a spin coherence time (T2) of 0.87 ms, five orders of magn

48 ubstrate, and without degrading the electron spin coherence time.

49 rface unit cell resulting in a perpendicular spin component, keeping the diagonal double-stripe order

50 ral recent studies of the miscibility of the spin components of such a condensate, the presence of st

51 lator at [Formula: see text]21 GPa whose AFM spin configuration is different from the AFM state near

52 elation spectroscopy (TOCSY) provides unique spin connectivity information for the analysis of a larg

53 aching 100 Tesla to reveal the extent of the spin correlations in gamma-lithium iridate.

54 derstood in terms of stabilization caused by spin-coupling augmented by dispersion, polarization, and

55 findings, supported by theory, show how the spin crossover transition can be manipulated reversibly

56 ve room temperature; that is, well above the spin crossover transition temperature for the pristine p

57 er fluorine atoms in [Fe(dftpy)2](2+) enable spin crossover with a T1/2 of 220 K and a mixture of low

58 spin torque oscillator device driven by pure spin current arising from thermal gradient across an Y3F

59 sults imply that a perpendicularly polarized spin current can be generated with an in-plane charge cu

60 The manipulation of magnetization by spin-current occurs through the spin-transfer-torque eff

61 agnetic fields, but interact with charge and spin currents, allowing this moment to be manipulated pu

62 hertz and optical devices controlled by pure spin currents.

63 r THz and optical devices controlled by pure spin currents: a low-dissipation flow of electronic spin

64 eoretically, it has been known that breaking spin degeneracy and effectively realizing spinless fermi

65 o far focused on the control of the electron spin degree of freedom (DOF) in materials such as multif

66 rther, the many-body states possess a pseudo-spin degree of freedom that corresponds with the two dir

67 , critical phenomena, anharmonicity, and the spin degree of freedom.

68 rrelation technique to quantify the electron-spin density at ligand nuclei (via the weak hyperfine in

69 is a 1-hole (i.e., 3Cu(I)Cu(II)) state with spin density delocalized evenly over CuI and CuIV.

70 ula and parabolic barrier approximation) and spin-dependent drift-diffusion model.

71 sition(s) may be used as a predictor for the spin-dependent electron transfer, indicating that chiral

72 to control these states can provide enhanced spin-dependent readout and long-term charge stability.

73 e development of pultrusion-based biomimetic spinning devices.The natural production of silks remains

74 hemical shift correlations via proton driven spin diffusion provided distance constraints to characte

75 lved scanning tunnelling microscopy that the spin direction at the surfaces of bulk Fe1+yTe and thin

76 al structures in natural silks and serves as spinning dope.

77 ess in developing multifunctional materials, spin-driven ferroelectrics featuring both spontaneous ma

78 We show that the donor nuclear spin drives coherent rotations between the electronic qu

79 erized by a periodic inversion of the active spin during the real-time acquisition.

80 followed by the control of their individual spin dynamics has recently emerged as an essential ingre

81 how that fast field-driven antiferromagnetic spin dynamics is realized in ferrimagnets at the angular

82 resents a fundamental step to understand the spin dynamics of potential molecular quantum bits, and e

83 Spin dynamics, zero-field splitting constants, and elect

84 s comparable to that using Neutron Resonance Spin Echo (NRSE) coils.

85 sion of the Knight shift and the linear-in-T spin echo decay that increases with doping.

86 A fast recovery fast spin echo MR sequence was selected for high RF power, an

87 We report a measurement by neutron spin echo spectroscopy of the diffusion of hemoglobin in

88 ated (FS) proton density (PD)-weighted turbo spin-echo (TSE) imaging in the detection of bone marrow

89 axial) structural imaging (T2-weighted turbo spin-echo and diffusion-weighted imaging), acquired with

90 tic resonance (MR) imaging with a mixed fast spin-echo pulse sequence were assessed.

91 imaging system, intermediate-weighted turbo spin-echo pulse sequences, and MR-conditional needles, d

92 e longest living rodent, with a maximum life span exceeding 30 years, and found that injury responses

93 As the energy increased, the spin excitations assumed a diamond shape, and they dispe

94 Systems hybridising collective spin excitations with microwave photons have recently at

95 ators, we drive Rabi oscillations on nuclear spins exclusively using electric fields by employing the

96 ther was due to [Fe4S4](2+) clusters and low-spin Fe(II) hemes, most of which were associated with mi

97 This species is a low-spin Fe(iii) d(5) complex, and emission occurs from a lo

98 ers are typically derived from polymers, gel spun fibers, modified carbon fibers, carbon-nanotube fib

99 Spin fluctuations are a leading candidate for the pairin

100 The spatial separation of electron spins followed by the control of their individual spin d

101 ardiovascular disease are multifactorial and span from the individual level to the social environment

102 the theoretically predicted crossover into a spin-frozen state.

103 ion between Mott and Slater physics, where a spin-frustrated state emerges at the crossover.

104 ferroelectric polarization with no change of spin-helicity, and present a phenomenological theory tha

105 nature and comparative reactivity of two low-spin heme-peroxo-Cu complexes, LS-4DCHIm, [(DCHIm)F8Fe(I

106 RNA sequencing (RNA-seq) experiments now span hundreds to thousands of samples.

107 rangements of nanoelements called artificial spin ice can lead to specific collective behaviour, incl

108 phase', is shown to occur experimentally in spin ice, a dipolar lattice system.

109 tations, for example the magnetic charges in spin ices, also called monopoles.

110 ong fluctuations, including spin liquids and spin ices.

111 expression of shared target genes, and whose span in many cases coincides with topologically associat

112 aday rotation induced by a single electronic spin in a single-sided optical microcavity.

113 e constraint of having to polarize the (13)C spins in a dedicated apparatus nearby but separated from

114 ure the interaction between two inequivalent spins in a hybrid rotaxane molecule.

115 e ensembles down to approximately 30 nuclear spins in atomically thin hexagonal boron nitride (h-BN).

116 quantum processor based on electron-nuclear spins in silicon, with electrical control and coupling s

117 ent resonantly driven CNOT gate for electron spins in silicon.

118 imes or T2, due to interactions with nuclear spins in the local environment.

119 ultispin effects (with n being the number of spins in the system).

120 netic fields, indicating strongly frustrated spin interactions.

121 m since the presence of SOC implies that the spin is not a good quantum number.

122 alidation, our results indicate that natural spinning is achieved, not by extruding the feedstock, bu

123 an alternative sequence in which a nitroxide spin label attached to cysteine has been introduced at i

124 Spin-labeled double-cysteine mutants of VcSiaP were anal

125 paramagnetic resonance (EPR) of biomolecules spin-labeled with nitroxides can offer uniquely sensitiv

126 ical magnetic resonance scans using arterial spin labeling (ASL) were performed to study the haemodyn

127 performed using velocity-selective arterial spin labeling (VSASL) and 3D image acquisition with whol

128 amate (Glu) and glutamine (Gln) and arterial spin labeling evaluation for rCBF.

129 mages and perfusion images by using arterial spin labeling were obtained for comparison.

130 images and to perfusion images from arterial spin labeling.

131 ctive insights into these processes, but new spin-labeling strategies are needed.

132 idual magnetic molecules, nanostructures and spin-labelled biomolecules.

133 which serve as models in the search for new spin labels for DEER distance measurement at room temper

134 Nitroxide spin labels, introduced specifically at three individual

135 Wide-field amacrine cells span large segments of the retina, making them uniquely

136 Variable-temperature (1)H NMR spin-lattice relaxation (VT (1)H T1) data revealed rotat

137 agram and find a stable photo-induced chiral spin liquid near the equilibrium state.

138 c phases with strong fluctuations, including spin liquids and spin ices.

139 a route to study unconventional superfluids, spin liquids, Berezinskii-Kosterlitz-Thouless phase tran

140 tically prepared chemical exchange-sensitive spin-lock imaging was performed with a 7.0-T whole-body

141 proteins by measuring RDCs using magic-angle spinning (MAS) in combination with dipolar recoupling me

142 n of water is combined with (1)H magic angle spinning (MAS) NMR detection, absolute quantification of

143 Additionally, fast (25 kHz) magic-angle spinning (MAS) provides optimal sensitivity and resoluti

144 cale spatial resolution in remote sensing of spins may ultimately allow the structural imaging of ind

145 c thin film materials that are promising for spin-mechanical devices.

146 t signaling and mediates dermatosis in Ptpn6(spin) mice.

147 Because of spin-momentum locking, changing light propagation direct

148 We apply this method to two examples that span movement networks that vary considerably in size an

149 other platforms to generate trimers that now span multiple subtypes.

150 Reduced Lpp protein was observed in spin mutant tissues.

151 versal NV-based sensor device records single-spin NMR spectra with 13 Hz resolution at room temperatu

152 olid state (13)C cross-polarized magic angle spinning NMR reveals that solid heptacene has a half-lif

153 nsaturated model membranes using magic angle spinning NMR to measure these interactions through both

154 studied using (31)P solid-state magic-angle-spinning nuclear magnetic resonance spectroscopy and dif

155 the hydrodynamics of fluids composed of self-spinning objects such as chiral grains or colloidal part

156 on patterns of 376 million users over a time span of 6 y (January 2010 to December 2015).

157 2,000 years, to multiple tsunamis within the span of a century.

158 MHC-class I on recipient DCs during the life span of a skin graft.

159 causes a severe decline of replicative life span of daughter cells.

160 stasis of MDA-MB-231 cells and prolongs life span of mice injected with these cells.

161 We capitalized on wide geographic span of our sampling to address intriguing question abou

162 ust model systems that recapitulate the full span of thymopoiesis, from hematopoietic stem and progen

163 dC+dT delayed disease onset, prolonged life span of Tk2-deficient mice and restored mtDNA copy numbe

164 ue of Rabi oscillations in ensemble-averaged spins of a ferromagnet.

165 The qubits are represented by the spins of trapped ions, which can be prepared in various

166 Bose-Einstein condensates with spin-orbit coupling are predicted to possess a stripe ph

167 together with the large g-factor and Rashba spin-orbit coupling in In0.75 Ga0.25 As quantum wells, w

168 ice represents a way of implementing coupled spin-orbit interaction between electrons and photons and

169 ric field is found to generate an additional spin-orbit torque on the CoNiCo magnets, which is confir

170 Here we demonstrate that sub-nanosecond spin-orbit torque pulses can generate single skyrmions a

171 ochiral skyrmions, whose motion is driven by spin-orbit torques and is deterministic, which makes sys

172 nic states and quasi-momenta, and to produce spin-orbit-coupled dynamics.

173 Here we demonstrate that spin-orbit-coupled fermions can be engineered to occur n

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

175 ls with the gradient of magnetic anisotropy, spin-orbit-torque-induced magnetization behaviour has at

176 Strong spin orbital interaction (SOI) can induce unique quantum

177 rconductivity appears in the cuprates when a spin order is destroyed, while the role of charge is les

178 y waves (CDWs) without any obviously related spin order.

179 formation of microscopic domains of opposite spin orientations is observed.

180 rovided a set of constitutive promoters that span over four logs of strength without detectable fitne

181 ng of electron transport, as reported values span over three orders of magnitude.

182 h are associated with a longer maternal life span (P 1.4 x 10-3).

183 s featuring multiply and singly bonded boron spin pairs.

184 Controlling the spin-phonon coupling through ligand design thus appears

185 ptoelectronics, and the optical detection of spin physics in these materials.Carbon-based molecules c

186 A 66% spin polarization of the BZA single crystal was obtained

187 bbard model as a function of both doping and spin polarization, for which many open questions remain.

188 hich require resonant optical excitations to spin-polarize the ensemble.

189 etized by either external magnetic fields or spin polarized currents.

190 Here, progress on efficient spin-polarized carrier injection into organic semiconduc

191 particular, these would support valley- and spin-polarized chiral edge states in the quantum Hall re

192 of magnetically active N-doped graphene with spin-polarized conductive behavior.

193 Sr0.3MnO3 heterojunctions and discover a new spin-polarized current injection induced interface magne

194 rconductor (e.g. Nb, Al) and either strongly spin-polarized ferromagnetic insulators (e.g. EuO, GdN)

195 provide unique information on the extent of spin-polarized hybridization between 5f and 6d electroni

196 report the observation of fully valley- and spin-polarized LLs in high-quality WSe2 monolayers achie

197 Parallel field measurement confirms the spin-polarized nature of the ground state, which is cons

198 over a picosecond recombination time of the spin-polarized photo-carriers that only leads to a defor

199 s in a Bi2Se3 layer generates a directional, spin-polarized photocurrent.

200 Motivated by the recent derivation of spin-polarized quasiclassical boundary conditions capabl

201 Dy-free Nd30.0Fe61.8Co5.8Ga0.6Al0.1B0.9 melt spun powder (MQU-F, neo Magnequench).

202 chemical shifts and coupling constants among spins provides a much richer feature set for a compound

203 halcogenides are characterized by valley and spin quantum degrees of freedom, making it possible to e

204 imum number required by their total electron spin quantum number.

205 ere layer polarization maps to the valley or spin quantum numbers.The phase diagram of bilayer graphe

206 Spin qubits exist in specific charge states of these def

207 gate this charge state control for two major spin qubits in 4H-SiC, the divacancy and silicon vacancy

208 and a mixture of low-spin (singlet) and high-spin (quintet) populations at room temperature.

209 We demonstrate that the spin recipe for the monolayer formation can be represent

210 ing of precisely how the position of nuclear spins relative to the electronic spin center affects dec

211 Spin relaxation however limits the maximum experimental

212 e report the design, synthesis, and electron spin relaxation properties of hydrophilic tetracarboxyla

213 Here we show by spin-resolved scanning tunnelling microscopy that the sp

214 diate catalytic centers revealed by electron spin resonance (ESR) measurements and recent knowledge o

215 di teeth with combined U-series and electron spin resonance (US-ESR) dating.

216 Electron spin resonance measurement elucidates the ferromagnetic

217 In our previous electron spin resonance spectroscopic studies, the membrane-order

218 oborated by the combined results of electron spin resonance, UV-vis-NIR, and ultraviolet photoelectro

219 or atoms, exhibits a large energy barrier to spin reversal (770.8 K) and magnetic blocking (14 K).

220 to be non-chiral, we show that right-handed spin rotations are strongly favoured in this system, due

221 Complex 3 is a rare example of a high-spin (S = 1) {FeNO}(8) and is the first example, to our

222 tic condition, entropic factors, rather than spin-selection rules, are the source of the reduced Arrh

223 We impose spin-selectivity by coating the anode with chiral organi

224 near-transfer WM tests (Digit-Span, Spatial-Span), self-reported executive functioning, and function

225 ies (size, shape, density and porosity) that span several spatial scales.

226 er with a T1/2 of 220 K and a mixture of low-spin (singlet) and high-spin (quintet) populations at ro

227 conventional Debye relaxation expected for a spin solid, a state with long range order.

228 s crossovers among the two glassy states and spin solid.

229 anifest through mechanisms and features that span spatial and temporal scales.

230 Nontrained near-transfer WM tests (Digit-Span, Spatial-Span), self-reported executive functioning

231 ic studies and technologies wherein only one spin species could be handled at a time.

232 gies because it would enable both of the two spin species to be simultaneously utilized, distinct fro

233 oposed to describe the interplay between the spin speed and solution concentration.

234 high-mobility spiral surface modes based on spin-split bands.

235 ucting PtSe2 film without the characteristic spin splitting in conventional Rashba effect (R-1).

236 A remarkably high-spin-stabilizing effect through encapsulation of C70 was

237 electronic state characteristic of the high spin state at temperatures of 200 K to above room temper

238 Of crucial interest is the effect of spin state of the Fe(IV)(O) unit.

239 tively fast decay time of the hyperpolarized spin state together with the constraint of having to pol

240 that identifies the experimentally reactive spin state.

241 r, revealing a bistable, strongly correlated spin state.

242 otein stability, heme iron coordination, and spin state.

243 nion influences the reactivity more than the spin state.

244 which neighbouring iron(ii) sites undergo a spin-state transition above a threshold CO pressure, the

245 cteristic of light- or X-ray-induced excited-spin-state trapping.

246 [(PyTACN)Fe(O)(X)](+) generated in different spin states and bearing different anionic ligands X reve

247 vail of reaction pathways involving multiple spin states having little or no barrier.

248 s work examines the relative energies of the spin states of O atom, Fe(2+) ion, and FeF2 and characte

249 on, and FeF2 and characterizes their excited spin states.

250 D(+*)-A-R(-), but its yield is controlled by spin statistics of the uncorrelated A(-*)-R(*) radical p

251 Interestingly, different canting spin stripes along three 120 degree propagation directio

252 a magnetic phase, attesting that the canting spin stripes are three-fold degenerate states akin to he

253 to helices and the multiple state of canting spin stripes is a circular configuration with zero skyrm

254 the system, the development of a peak in the spin structure factor and a staggered magnetization that

255 The formation and resolution of the internal spin structure of room temperature skyrmions without a s

256 trieval methods allow us to map the internal spin structure of the skyrmion core, identifying a 25 nm

257 zero-field splitting constants, and electron-spin structures of the excited triplet states for the me

258 ground to explore interactions involving two spin sublattices and the emergent effects they may drive

259 actions between the central ion and the bath spins suppress the flip-flop rate of the neighbour bath

260 on appearance of a distinct resonance in the spin susceptibility across the cuprates, iron-based supe

261 A spin system matrix that parametrizes chemical shifts and

262 urring in spin-transfer torque-driven linear spin systems as a transition between hyperbolic and loxo

263 oscopy, we report the observation of helical spin texture in monolayer, centrosymmetric and semicondu

264 tructed sequential deletions in regions that span the 530 bps.

265 and ZF11 are not visible, while ZF8 and ZF9 span the backbone of the DNA duplex, conferring no seque

266 ese pumps form multi-protein assemblies that span the cell envelope.

267 mbinant fragments (60-79 aa), which together span the entire length of tropomyosin, were weak secreta

268 netic zone spans a ZII+/- pair: the HA zones span the P5+/- and P7+/- ZII stripe pairs, whereas the V

269 PqiB create channels of sufficient length to span the periplasmic space.

270 erize the maturation kinetics of 50 FPs that span the visible spectrum at two different temperatures

271 include high-resolution marine records that span the YD.

272 iaturized quarter-wave plate devices empower spin to orbital angular momentum conversion and vector p

273 raction confirmed structures that resemble a spinning top on a tripod and revealed that the two XB co

274 Here the authors demonstrate a spin torque oscillator device driven by pure spin curren

275 An important property of spin-torque nano-oscillators (STNOs) is their ability to

276 The optical spin-transfer torque acts over a picosecond recombinatio

277 y the same in Fe, Ni and Co, but the optical spin-transfer torque is strongly enhanced by adding a Pt

278 metry-breaking phase transition occurring in spin-transfer torque-driven linear spin systems as a tra

279 etization by spin-current occurs through the spin-transfer-torque effect, which is applied, for examp

280 he combination of a conventional cooperative spin transition and ligand-driven magnetic changes can p

281 On heating, this compound exhibits a spin transition between a LS ground state and an ordered

282 In addition, efforts to realize long spin transport in single-crystalline organic semiconduct

283 l and biologically active compounds, used as spin-trap reagents and therapeutic agents.

284 paper will help researchers to better design spin trapping experiments for food matrices.

285 dentified by electron paramagnetic resonance spin trapping, immunospin trapping, and MS analysis afte

286 allacyclobutane intermediate, leading to the spin-triplet 12-electron complex (SIMes)RuCl2 ((3)R21, S

287 a suitable physical system to realize these spin units is an active area of research.

288 ithout lifting the valley degeneracy, due to spin-valley-layer coupling.

289 ecent observation of a large superconducting spin-valve effect with a T c change 1 K in superconduct

290 tic exchange interactions, and the resultant spin vector alignments that are found within the 3-D C-t

291 his concept of bending strain engineering of spins via topological nanomechanical architecture afford

292 tocrystalline anisotropy, opening up a large spin-wave excitation gap.

293 er poor due to the difficulty of controlling spin waves in the input junction of the waveguides.

294 conventional charge-based devices have made spin waves or magnon spintronics a promising candidate f

295 purpose signal processors can be realized by spin-waves.

296 ic properties with a ground-state electronic spin, which can be read out optically.

297 rrents: a low-dissipation flow of electronic spins with no net charge displacement.

298 sical magnetic fields and individual quantum spins with orders of magnitude finer frequency resolutio

299 tant knockin LRRK2 mice over half their life span, with observable and measurable phenotype, is inval

300 e some systems exhibit stripes of charge and spin, with a locked periodicity, others host charge dens

301 actions of space and number through the life span, yet propose a theory with several weaknesses.