ライフサイエンスコーパス: magnetic field

1 by external stimuli (ferroelectric field and magnetic field).

2 with a single external power source (i.e., a magnetic field).

3 s the solar wind plasma and confines Earth's magnetic field.

4 direction even in the absence of an external magnetic field.

5 in navigational information from the Earth's magnetic field.

6 resolution fMRI and TPM imaging at ultrahigh magnetic field.

7 Zeeman effect in presence of an out-of-plane magnetic field.

8 ated and controlled solely by an oscillating magnetic field.

9 s delivered into pollen in the presence of a magnetic field.

10 esistivity anisotropy induced by an in-plane magnetic field.

11 to EE +/- 1 before reversal of terrestrial magnetic field.

12 parated from the aqueous phase by applying a magnetic field.

13 unction of charge parity on the dots, and in magnetic field.

14 and accepted magnitude for Archaean earth's magnetic field.

15 the magnitude and direction of the external magnetic field.

16 state to an onion-like one under an in-plane magnetic field.

17 le energized by an external alternating (ac) magnetic field.

18 its rigidity by deflecting it with a uniform magnetic field.

19 s in water at room temperature and ultra-low magnetic field.

20 t as a ferromagnetic liquid with a 10(12)-T magnetic field.

21 e discussed as a function of temperature and magnetic field.

22 tals upon application of sufficiently strong magnetic field.

23 nisotropy, depending on the direction of the magnetic field.

24 the magnitude and direction of the external magnetic field.

25 hybrid nanorod suspension using an external magnetic field.

26 spin ice at equilibrium through a staggered magnetic field.

27 nding paradox of the duration of the induced magnetic field.

28 tiaromatic') simply by changing the external magnetic field.

29 , as such flow states depend on the external magnetic field.

30 two-dimensional system without any in-plane magnetic field.

31 rolled by the frequency and amplitude of the magnetic field.

32 erromagnetic Heisenberg model in an external magnetic field.

33 structure by current-induced spin-orbit (SO) magnetic field.

34 namics in response to an applied oscillating magnetic field.

35 les below room temperature under an external magnetic field.

36 iferromagnetic material in the presence of a magnetic field.

37 al cell disruption under an applied rotating magnetic field.

38 g Ising chain in the presence of an external magnetic field.

39 ght-circularly polarized light caused by the magnetic field.

40 s that flow without resistance, even at zero magnetic field.

41 , indicating a primary record of the Earth's magnetic field.

42 al tuning parameters such as temperature and magnetic field.

43 of the PZT-LSMO Schottky barriers on applied magnetic field.

44 NPs can be captured by applying the external magnetic field.

45 ral response is monitored after removing the magnetic field.

46 very and temporal control of mRNA sensing by magnetic field.

47 rently mobile particles in the presence of a magnetic field.

48 hard gap in the system that can be closed by magnetic fields.

49 ence in graphene at Terahertz frequencies in magnetic fields.

50 a graphene electron-hole bilayer at moderate magnetic fields.

51 the Ile, Leu, and Val residues at two static magnetic fields.

52 f valley-polarized excitons in perpendicular magnetic fields.

53 ed to certain stimuli, for instance, heat or magnetic fields.

54 001)-oriented Pb1-x Sn x Se in zero and high magnetic fields.

55 ns of heterogeneous catalysis and microtesla magnetic fields.

56 nly in the presence of parallel electric and magnetic fields.

57 laxation rates at fast (60 kHz) MAS and high magnetic field (1 GHz), we were able to describe the mot

58 O magic-angle spinning (MAS) NMR at multiple magnetic fields (17.6-35.2 T/750-1500 MHz for (1)H) the

59 ing a range of frequencies (150-375 kHz) and magnetic fields (4-44 kA/m).

60 The external field is a magnetic field acting on a superparamagnetic microbead s

61 Here we report a new strategy termed magnetic field-activated binary deoxyribozyme (MaBiDZ) s

62 e Sun is related to the evolution of coronal magnetic field activity.

63 ime, the T1 relaxation time, of protons in a magnetic field after excitation by a radiofrequency puls

64 the diffusive limit, which occurs only for a magnetic-field-aligned electric field (E parallelB).

65 stals of uranium dioxide subjected to strong magnetic fields along threefold axes in the magnetic sta

66 using high-frequency (>100 kHz) alternating magnetic fields (AMF).

67 s dissipate heat when exposed to alternating magnetic fields (AMFs), making them suitable for cancer

68 brain activity, such as shifts in sustained magnetic field amplitude, measured with magnetoencephalo

69 l dichalcogenides host a valley splitting in magnetic field analogous to the Zeeman effect.

70 nucleated by the application of an external magnetic field and are stable at zero field with a diame

71 ladder with the presence of tilted external magnetic field and four-Majorana interaction.

72 le through motion analysis of RBCs in a high magnetic field and gradient.

73 o-gap phase to disturbances like disorder or magnetic field and is shown to gap out part of the Fermi

74 However, the lifetime of the nebular magnetic field and nebula are poorly constrained.

75 lled using the interplay between an external magnetic field and Rashba spin-orbit interaction in semi

76 The MNP chains are assembled in a rotating magnetic field and stabilized by multivalent target mole

77 ed that the present method can visualize the magnetic field and temperature distribution simultaneous

78 um iron garnet thin film, and visualizes the magnetic field and temperature distributions through the

79 is obtained by controlling the direction of magnetic field and the thickness of the sample.

80 e explored the dynamics of sunspot-producing magnetic fields and discovered for the first time that b

81 in the presence of large externally applied magnetic fields and functions even for electronic system

82 lation can achieve spectroscopy of classical magnetic fields and individual quantum spins with orders

83 d a targeted location wirelessly by rotating magnetic fields and perform on-demand magnetoelectricall

84 rive positional information from the Earth's magnetic field" and that this information guides their m

85 the carrier density, layer polarization and magnetic field, and find evidence for the paired Pfaffia

86 s to exogenous stimuli, such as temperature, magnetic field, and optical light.

87 vector as a function of temperature, applied magnetic field, and varying angle in Sr4Ru3O10.

88 T(1/2) dependence, a robust independence of magnetic fields, and a close relevance to structural dis

89 cements (>100) are limited to relatively low magnetic fields, and DNP at fields higher than 9.4 T sig

90 agnetic field hardness, the absence of stray magnetic fields, and the spin-dynamics frequency scale i

91 tized by expressing TRPV1 are activated with magnetic field application.

92 critical supercurrent induced by an external magnetic field applied perpendicular to the substrate.

93 Here we use magnetic fields approaching 100 Tesla to reveal the exte

94 Since weak magnetic fields (approximately 10 mT) are adequate to co

95 antum many-body effect induced by an applied magnetic field are rare.

96 Our mobility estimates at high magnetic fields are comparable, within order of magnitud

97 of the DMI implies that no external in-plane magnetic fields are needed for this aim.

98 Moreover, although alternating current magnetic fields are the most natural choice to drive spi

99 atments would indicate an ability to use the magnetic field as a map; the compass cue(s) used by eels

100 Magnetic field assisted compaction (MC) has been employe

101 d CFO sample, Co1.2Zr0.2Fe1.6O4, prepared by magnetic field assisted compaction, have been reported i

102 Our measurements probe the structure of the magnetic field at an early stage of the jet, closer to i

103 at charge carriers experience effectively no magnetic field at simple fractions of the flux quantum p

104 f view, and the performance variations under magnetic fields at steady and nonstationary states.

105 emporally resolved measurements of megagauss magnetic fields at the rear of a 50-mum thick plastic ta

106 esonance spectroscopy at room temperature in magnetic fields below 50 mT.

107 the consideration of uniaxial anisotropy and magnetic field both perpendicular to the film plane, a l

108 ices, as they are insensitive to homogeneous magnetic fields, but interact with charge and spin curre

109 re we demonstrate that an in-plane effective magnetic field can be induced by an electric field witho

110 ost disposables and because application of a magnetic field can be used to accelerate assay kinetics.

111 Here, we show how an in-plane magnetic field can brighten the dark excitons in monolay

112 A relatively small magnetic field can confine electrons to their lowest Lan

113 ing beamed emission, but a strong multipolar magnetic field can describe its properties.

114 orientation may be controlled by an external magnetic field, can be used to map out the detailed magn

115 reshwater glass eels, and their responses to magnetic fields, can be used as a proxy for the response

116 ectrons at relativistic speeds, diffusing in magnetic fields, cause copious emission at radio frequen

117 phase can be switched on and off with small magnetic field changes on the order of 10 millitesla, po

118 here from bow shock to the planet, providing magnetic field, charged particle, and wave phenomena con

119 volves a new method of tuning by varying the magnetic field configurations in the device and the tuni

120 as generated growing interest for a possible magnetic field control of the incommensurate spin spiral

121 wo major first, young eels distinguish among magnetic fields corresponding to locations across their

122 Mesoscopic variations in magnetic field, created by microstructure, influence the

123 le shape changes upon temperature, stress or magnetic field cycling.

124 We exploit the temperature and magnetic field dependence of magnetic entropy change (De

125 ally small electric polarization, its strong magnetic field dependence, and the negative thermal expa

126 n with a characteristic spin selectivity and magnetic field dependence, being the model also for more

127 Magnetic-field-dependent photocurrent measurements of po

128 roresponse behavior, which together with the magnetic-field-dependent polarization and dielectric mea

129 monic generation effect, and corroborated by magnetic-field-dependent pyroresponse behavior, which to

130 The magnetic-field-dependent spin ordering of strained BiFeO

131 ields using a geometry easily modifiable for magnetic field detection via Faraday rotation.

132 us imaging method of the temperature and the magnetic field distributions based on the magneto optica

133 onceptually simple multiferroic in which the magnetic-field-driven flop of conical spin spirals leads

134 tional magnetoelectric couplings such as the magnetic-field-driven reversal of ferroelectric polariza

135 w that the application of a relatively small magnetic field drives the three-dimensional magnet beta-

136 thick CuMnAs layer is rotatable under small magnetic fields, due to the interlayer exchange coupling

137 We show that the prolonged magnetic field duration originates from the ultrafast op

138 g the duty cycle of alternating current (AC) magnetic field during MNFH.

139 The high magnetic field electronic structure of bilayer graphene

140 eresting the collapse can be controlled by a magnetic field even without long-range magnetic order, a

141 been tied to thermoelectrical transport in a magnetic field, even in flat space-time, suggesting that

142 energized by a uniform uniaxial alternating magnetic field exhibits dynamic arrays of self-assembled

143 lity is achieved by application of hard-axis magnetic field favoring and opposing the Dzyloshinskii-M

144 organization of the bSTC by using ultra-high magnetic field fMRI at 7 Tesla.

145 plasma deforms the topology of the external magnetic field, forming a magnetic cavity inside and com

146 magnetic colloidal particles is induced by a magnetic field [Formula: see text] At the transition fie

147 ly polarized photoluminescence is tuned with magnetic field from -37% to 37%.

148 ddressing quantitatively the effect of stray magnetic fields from both, the superconductor and the fe

149 Here, we measure the magnetic field generated by a hard-disk-drive write head

150 of strong magnetic field gradients and high magnetic fields generated by permanent magnets or superc

151 The interplay of strong interactions and magnetic fields gives rise to unusual forms of supercond

152 then exposed to laser pulses with a coaxial magnetic field gradient, resulting in high-aspect ratio

153 The use of strong magnetic field gradients and high magnetic fields genera

154 equiring only a single dot and no additional magnetic field gradients, as well as a means to interact

155 This approach does not rely on magnetic field gradients, but rather on the spatial vari

156 ally dictated by the strength of the applied magnetic field gradients, resulting in hard resolution l

157 text] increases (most likely linearly) with magnetic field H and saturates above field values rangin

158 ating power at a biological safe range of AC magnetic field (Happl .fappl < 3.0-5.0 x 10(9) A m(-1) s

159 on of properties including the radiation and magnetic field hardness, the absence of stray magnetic f

160 On the other hand, full mapping of the magnetic field has hitherto remained challenging.

161 he phase diagram of bilayer graphene at high magnetic fields has been an outstanding question, with o

162 s new sensing modality is insensitive to the magnetic field homogeneity making it more amenable to lo

163 e remained unexplored, mainly because of the magnetic field immunity of antiferromagnets.

164 Drying up a Fermi sea by magnetic field in the Brillouin zone leads to a manyfold

165 sing from the lowest Landau level under high magnetic field in type II Weyl semimetal YbMnBi2.

166 ay of studying the strength and evolution of magnetic fields in accreting white dwarfs and extends th

167 GRB radiation provides a direct probe of the magnetic fields in the collimated jets.

168 Rapid switching of applied magnetic fields in the kilohertz frequency range in the

169 sensitivity of the transition temperature to magnetic fields in the three-dimensional regime.

170 are substantially greater for inhomogeneous magnetic fields, including dynamic inhomogeneity caused

171 cascades of bifurcations as the current and magnetic field increase.

172 transitions, from which we obtain a direct, magnetic-field-independent measurement of the hyperfine

173 oscillations when subjected to out-of-plane magnetic field, indicating the dominant role of surface

174 ween these states in beta-Li2IrO3 under weak magnetic fields, indicating strongly frustrated spin int

175 throughout the quantum Hall plateau due to a magnetic field induced energy gap.

176 nderlying band gap opening occurs inside the magnetic field-induced phase, paving the way for a syste

177 upercurrent enhancement is compatible with a magnetic field-induced topological transition.

178 Magnetic field-induced, reversible martensitic transform

179 This protocol describes how to combine magnetic-field-induced mechanical stimulation with confo

180 We observe a magnetic-field-induced state in the vicinity of a field-

181 An external magnetic field induces a large splitting of the valley e

182 The magnetic field induces force on the micro-magnet causing

183 rmed our hypothesis, indicating that solving magnetic field inhomogeneity may become a powerful way t

184 also compensate for pulse imperfections and magnetic field inhomogeneity, generating an extremely na

185 When an external magnetic field is applied in a polar Kerr geometry, we o

186 perconducting dome in YBa2Cu3O y when a high magnetic field is applied perpendicular to the CuO2 plan

187 resence of a specific target mRNA and when a magnetic field is applied.

188 The sensitivity to a 50 muT magnetic field is greatly enhanced and, unlike the curre

189 resonators when a relatively small critical magnetic field is reached.

190 As the external magnetic field is swept, half-integer quantized conducta

191 ruction of all three components of nanoscale magnetic fields is possible without tilting the specimen

192 tage measurements carried out under variable magnetic field it has been found that the magneto-capaci

193 esented stimuli, e.g., early auditory evoked magnetic fields known as M100 and M200 components are at

194 similarly to a paramagnet under an external magnetic field)-lead to three kinds of thermoelectromagn

195 n the transformation characteristics and the magnetic field levels required for reversible phase tran

196 raphene flakes can respond and be aligned to magnetic field like a ferromagnetic material.

197 ween states near the Fermi level in a strong magnetic field limit.

198 ane magnetization is independent of in-plane magnetic field, linearly proportional to the in-plane cu

199 powerful electric fields directed along the magnetic field lines that connect Earth's space environm

200 n which birds exposed to weak time-dependent magnetic fields lose their ability to orient in the geom

201 emonstrating that they formed in a near-zero magnetic field (<0.6 microtesla) at 4563.5 +/- 0.1 milli

202 en shown that for the specific choice of the magnetic field magnitude and the initial polariton wave

203 burst, we present a precise 461 +/- 12 gauss magnetic field measurement in the corona.

204 Magnetic field (MF) non-ionizing radiation is widespread

205 ejection, whereby a region of highly sheared magnetic field near the solar surface becomes unstable a

206 port on the observation of another threshold magnetic field never encountered before in any other sol

207 Extreme variations of Earth's magnetic field occurred in the Levant region around 1000

208 z at zero field and reached 57.9 GHz under a magnetic field of 3 kOe, indicating that the epitaxial B

209 The methods are based on the exposure of the magnetic field of a magnetically labelled biomolecule in

210 At T = 3 K and magnetic field of Hc up to 9 Tesla, large magneto-resist

211 urtles perform impressive journeys using the magnetic field of the earth as a cue.

212 f novel multiple sign changes versus applied magnetic field of the MR in the cubic intermetallic comp

213 In about 15 per cent of these binaries, the magnetic field of the white dwarf is strong enough (at 1

214 Vice versa, these antennas sense the magnetic fields of electromagnetic waves, giving a piezo

215 ure in GdPd3 is highly fragile since applied magnetic fields of moderate strength significantly alter

216 ves the way for precision measurement of the magnetic fields of nanoscale write heads, which is impor

217 t and persist well above room temperature in magnetic fields of only a few tesla.

218 el effects of low/high frequency oscillating magnetic field on excitable cells such as neurons are we

219 a critical threshold, i.e. above a critical magnetic field or a critical current for superconductors

220 tre-distance displacement without an applied magnetic field or any other external stimuli can only oc

221 s are commonly magnetized by either external magnetic fields or spin polarized currents.

222 ectrical properties of materials by means of magnetic fields or vice versa may facilitate next-genera

223 The dependence of the magnetic field orientation on the performance of the pro

224 With increasing magnetic fields oriented along the wire axis, the wires

225 have superior critical current properties in magnetic fields over other superconductors.

226 ith the idea that a stable, globally ordered magnetic field permeates the jet at large distances from

227 Here we report the high-magnetic field phase diagram of graphite to exhibit just

228 magnetic phases in the temperature-pressure-magnetic field phase diagram of LaCrGe3.

229 ena as atmospheric structure, mass transfer, magnetic fields, photometric variability and the origin

230 that an orthogonal strain or a perpendicular magnetic field plays the role of the transverse field, t

231 We find that the magnetic field produces a magnetopause with surrounding

232 ause with surrounding plasma, as the earth's magnetic field produces a magnetopause with the solar wi

233 An annular magnetic field profile was observed 5 ps after the inte

234 ommensurate large-scale filamentation of the magnetic field profile.

235 the most decisive test of QED in the strong magnetic field regime, we find a 7-sigma discrepancy com

236 ality single crystal of Cr1/3NbS2 over three magnetic field regions.

237 Under magnetic fields, relativistic fermions acquire Berry pha

238 es, the mechanisms that animals use to sense magnetic fields remain largely mysterious.

239 0.10mugdL(-1) in the absence and presence of magnetic field, respectively, whilst for Fe@C-Fc-2 was 0

240 igh as 5.6% under only 1.3 T, or 3 T applied magnetic fields, respectively.

241 reaction recoil force and the self-generated magnetic fields result in not only trapping of a great a

242 dition, where a small change in the external magnetic field results in a drastic increase of the indu

243 In the first case, the application of a magnetic field reveals a wing-structure phase diagram as

244 electrons, parallel and antiparallel to the magnetic field, reveals a complex topology with the crea

245 used by quasi-periodic energy-exchange among magnetic fields, Rossby waves and differential rotation

246 ator sensors is described, from electric and magnetic field sensing to mechanical sensing, from singl

247 This phenomenon is utilized for magnetic field sensing.

248 The maximum magnetic field sensitivities of -100 pm/mT and -488 pm/m

249 We describe a magnetic field sensor based on a spin wave interferomete

250 angle as the eye rotated were detected by a magnetic field sensor.

251 with a complementary biomolecule bound to a magnetic field sensor.

252 ic-angle spinning rates and at high (23.5 T) magnetic field, severe sensitivity and resolution challe

253 bres in the spectroscopy voxel take with the magnetic field should be within +/-24.5 degrees .

254 ntrast, the effects of a homogeneous, static magnetic field (SMF) on Central Nervous System (CNS) gli

255 We demonstrate that transcranial static magnetic field stimulation (tSMS) over the somatosensory

256 oration (NEP) using alternating current (ac)-magnetic field stimulation.

257 are stabilized by a combination of external magnetic fields, stray field energies, higher-order exch

258 actor 2 reduction in near-Earth heliospheric magnetic field strength and solar wind speed, and up to

259 ets align progressively well with increasing magnetic field strength and that the alignment is effect

260 determine the risks associated with MRI at a magnetic field strength of 1.5 tesla for patients who ha

261 specific conditions of pH, temperature, and magnetic field strength, because changes in conditions c

262 Small pockets of low magnetic field strength, small radius of curvature, and

263 cation year, functional MR imaging paradigm, magnetic field strength, statistical threshold, and anal

264 Purpose To determine the impact of different magnetic field strengths (1, 1.5, 3, and 7 T) and the ef

265 75 cm and 20 cm respectively in the range of magnetic field strengths from 0 to 200 mT.

266 Magnetic fields suppress this superconducting dome, unve

267 n to only about 14 kelvin using a consistent magnetic field sweep rate of about 20 oersted per second

268 ransport signature is reproducible over many magnetic field sweeps and appears at different temperatu

269 Strong magnetic fields, synchrotron emission, and Compton scatt

270 These include using electric and magnetic fields, temperature, ultrasound or light to int

271 oling synchrotron radiation in a large-scale magnetic field that is advected from the black hole and

272 there has been no evidence that they have a magnetic field that is strong enough to affect the accre

273 n aromatic molecule is such as to generate a magnetic field that opposes the external field inside th

274 After isolating the sandwiches by a magnetic field, the DNAs of the probes which have been h

275 ferrofluid is subjected to a modest external magnetic field, the nanoparticles inside the ferrofluid

276 the size and speed of the emitting zone, the magnetic field, the number of emitting particles and the

277 predicted for two-dimensional electrons in a magnetic field-the Hofstadter butterfly.

278 Covalently connected carbon nanotubes create magnetic fields through graphene nanoribbons, cascading

279 controlled separately to form an asymmetric magnetic field to change the direction of laser-produced

280 MCF-7 breast cancer cells and activated by a magnetic field to fluorescently report the presence of s

281 The approach uses alternating magnetic fields to heat superparamagnetic nanoparticles

282 ramagnetic agent is used in conjunction with magnetic fields to levitate and assemble cells.

283 Approaches that utilize localized magnetic fields to manipulate magnetic particles carryin

284 Here, we utilize vector magnetic fields to visualize directly the magnetic aniso

285 We derive this result from high-magnetic-field transport measurements in La1.6-x Nd0.4Sr

286 x Fe x Si2 single-crystal specimens in high magnetic fields up to 45 T (DC fields) and 60 T (pulsed

287 electrical resistance measured in very high magnetic fields up to 67 Tesla.

288 tion (DNP) experiments decreases at the high magnetic fields used in contemporary high-resolution NMR

289 The applied external magnetic field was a factor which yielded better sensiti

290 ve to myofibres, the myofibre angle with the magnetic field was derived from the voxel orientation.

291 Without magnetic field, we find steady flow patterns, previously

292 biomolecules is decided by the direction of magnetic field where prebiotic life originated on Archae

293 This crossover is destroyed by an applied magnetic field which suggests a magnetic origin of the h

294 time-reversal-breaking effect of an in-plane magnetic field, which anisotropically lifts the protecti

295 y external perturbations such as pressure or magnetic field, which enhances the frustration.

296 control of degree of freedom in bilayer with magnetic field, which makes bilayer a promising platform

297 spins in diamond is used to sense nanoscale magnetic fields with an intrinsic frequency resolution o

298 he generation and control of fast switchable magnetic fields with large gradients on the nanoscale is

299 pable of discriminating changes to the local magnetic field, with no difference seen in approaches to

300 l information and navigate using the earth's magnetic field, yet in sharks, much remains uncertain re