ライフサイエンスコーパス: magnetic field

1 acceleration with a kilotesla-level applied magnetic field.

2 s could be captured under the influence of a magnetic field.

3 photothermal conversion by simply applying a magnetic field.

4 ntial of coupled phonons with applied static magnetic field.

5 ts to temperatures of several kelvin at zero magnetic field.

6 se local control of actuation using a simple magnetic field.

7 uspended in a medium exposed to a stationary magnetic field.

8 etotactic bacteria is rendered unstable by a magnetic field.

9 he resonance frequency and H is the external magnetic field.

10 on advantages by the application of external magnetic field.

11 ectly linked to solar activity and the earth magnetic field.

12 emperature by measuring the associated stray magnetic field.

13 to the photo-excitation in the absence of a magnetic field.

14 transmission measurements in an oscillating magnetic field.

15 are sensitive to external stress and applied magnetic field.

16 a second one with the same, lower, or higher magnetic field.

17 bust plateau in the extreme quantum limit of magnetic field.

18 ferromagnetic to ferromagnetic at a critical magnetic field.

19 oylglycine) (PNAG) showed a good response to magnetic field.

20 spatial and temporal changes in the coronal magnetic field.

21 with complex hopping parameters even at zero magnetic field.

22 xciton-phonon interaction under a quantizing magnetic field.

23 precisely quantized Hall resistance at zero magnetic field.

24 e to sustain a ring current when placed in a magnetic field.

25 ilm layer, allowing steering under a uniform magnetic field.

26 tterned in response to a brief exposure to a magnetic field.

27 ting in a time-dependent change in the local magnetic field.

28 with a 100% on/off ratio under zero remnant magnetic field.

29 ease stepwise under a programmed alternating magnetic field.

30 lying an electric field in the presence of a magnetic field.

31 cles allowed movement of the structures in a magnetic field.

32 rly in the ground state in the presence of a magnetic field.

33 heir magnetism may contribute to its present magnetic field.

34 initial nuclear spin states with an external magnetic field.

35 ton source (SPS) in 3D space via an external magnetic field.

36 TRPV1, a non-selective cation channel, in a magnetic field.

37 g an insulator that can be extinguished by a magnetic field.

38 plane-of-sky component of the global coronal magnetic field.

39 is and a large anomalous Hall signal at zero magnetic field.

40 n be re-aligned upon change of a programming magnetic field.

41 sualized using MRI, and are retrievable in a magnetic field.

42 ot included any effects caused by their self-magnetic field.

43 hat enables graft retrieval under an applied magnetic field.

44 and reversible shape change under actuation magnetic fields.

45 hat operate without the need for oscillating magnetic fields.

46 ysics and applications in terms of ultrahigh magnetic fields.

47 erromagnetic/ferromagnetic domains at finite magnetic fields.

48 ice and static, gradient, and radiofrequency magnetic fields.

49 deep cryogenic temperatures and under strong magnetic fields.

50 e magnetic medium, which relies on effective magnetic fields.

51 se laser pulses is used to produce ultrahigh magnetic fields.

52 ing modification of the electron spectrum in magnetic fields.

53 roxide radical cosolutes, at multiple static magnetic fields.

54 , respectively, and are stabilized by modest magnetic fields.

55 tens of nm size, generating megatesla-order magnetic fields.

56 Chern insulators that are stabilized by weak magnetic fields.

57 romagnetic VSe(2) film subject to applied DC magnetic fields.

58 ibility broadening is negligible at ultralow magnetic fields.

59 uation through the combined use of light and magnetic fields.

60 norods could be collectively regulated using magnetic fields.

61 Hall effect of a single electron band at low magnetic fields.

62 with fast magic-angle spinning (MAS) at high magnetic fields ((1)H Larmor frequency of 800-1000 MHz),

63 mostly limited to those realized in intense magnetic fields(1).

64 resulting in a periodically modulated pseudo-magnetic field(10-14), which in turn creates a 'post-gra

65 With increasing parallel magnetic field, a discrete sub-gap state in the island i

66 o opposing magnets to create a gradient of a magnetic field, a glass capillary channel to retain the

67 of a general connection between rotation and magnetic field: a magnetic field naturally arises along

68 If the DW displaces under a magnetic field above the Walker limit, the oscillatory m

69 s into the magnetic layer, while an external magnetic field along the electric current direction is g

70 es of topological excitations under external magnetic field also provide crucial information for expe

71 Strong magnetic fields also suppress the AFM order at a field-i

72 oton-hyperpolarized molecules in the Earth's magnetic field (ALTADENA condition) or in a high magneti

73 in cancer cells under programmed alternating magnetic field (AMF) similar to the neutrophil activator

74 In the presence of an alternating magnetic field (AMF), a superparamagnetic iron oxide nan

75 urce of heat generation under an alternating magnetic field (AMF).

76 to form growing chains under an alternating magnetic field (AMF).

77 ch thin flakes, a combination of an in-plane magnetic field and a charge current flowing through Ta-a

78 ia array can move in response to an external magnetic field and can be locally actuated by targeted i

79 both tuning of the resistance hysteresis by magnetic field and electric-field switching of magnetiza

80 n empirically, little is known about how the magnetic field and magnetic properties of a solution aff

81 e of its optical response on an out-of-plane magnetic field and on the gate-tuned carrier density.

82 as well as the information of exchange rate, magnetic field and radio-frequency transmission inhomoge

83 to study YBa(2)Cu(3)O(6.67) as a function of magnetic field and temperature.

84 depending on the relative orientation of the magnetic field and the light wavevector and on the absol

85 interaction energy of charged particles in a magnetic field and underlies the fractional quantum Hall

86 ould be moved through a constriction under a magnetic field and, at a second temperature, could grip

87 We apply an external in-plane magnetic field and, thereby, achieve continuous tuning o

88 view, the response of inductive materials to magnetic fields and spin-polarized currents is essential

89 sample is field-cooled under an out-of-plane magnetic field, and an exchange spring-like magnetic dep

90 he relative alignments of the magnetization, magnetic field, and electrical current, we experimentall

91 inct Landau quantization on application of a magnetic field, and the quantized Landau fan structure f

92 e caused by a short exposure to pulsed 20-mT magnetic fields, and future work may examine greater mag

93 es of organic molecules can be influenced by magnetic fields, and these magnetic field effects are di

94 The TISF is attributed to the magnetic-field- and temperature-dependent flipping of th

95 valenol (NIV) in alcoholic fermentation with magnetic field application (MF).

96 olution of the Raman spectra with increasing magnetic field applied perpendicular to the atomic layer

97 behavior above the spin-flop transition for magnetic fields applied along two orthogonal in-plane di

98 anomalous Josephson effect in the vectorial magnetic field are in agreement with our theoretical mod

99 atomic magnetometry to map the weak induced magnetic fields around Li-ion battery cells in a magneti

100 antiferromagnetic domain structures at zero magnetic field as well as antiferromagnetic/ferromagneti

101 l switching dynamics of the pre-polarisation magnetic field as well as the energy requirements, mecha

102 s aligned along the direction of the applied magnetic field, as expected for a pair of Majorana zero

103 irable orientations in a bimorph actuator by magnetic-field-assisted lithography, the bending of the

104 tion orientation is consistent with reversed magnetic field at the time of impact, the study of the P

105 derivative of the longitudinal resistance on magnetic field at the transition point follows a charact

106 demonstrate high performance in a few-Tesla magnetic field at which the sensors exhibit the quantum

107 n magnetars as a ferromagnetic liquid with a magnetic field B(S) = 10(12+/-1) T.

108 rk nugget in a ferromagnetic state with core magnetic field B(surface) = 10(12+/-1) T.

109 In a magnetic field B, fluxoid quantization generates a perio

110 omogeneous broadening of the oscillations in magnetic field B.

111 HgTe 3D topological insulator are studied in magnetic fields B tilted by angle theta from the normal

112 h can be regarded as a small effective local magnetic field (B(loc)).

113 is is typically achieved through an external magnetic field (B), which is practically cumbersome.

114 emperature T (MI) ~ 28 K is observed at zero magnetic fields (B).

115 ed with thermal fluctuations and/or external magnetic fields (B).

116 provide insights into the interplay between magnetic field, band structure and many-body interaction

117 in the magnetization loop with out-of-plane magnetic fields become more prominent.

118 tuned over two-wavelength cycles by moderate magnetic fields below 0.8 T.

119 combined presence of spin-orbit coupling and magnetic field breaks these symmetries and can lead to a

120 Increasing the strength of the applied magnetic field brings all spinwave modes to higher frequ

121 nction in a limited range of temperature and magnetic field, but Hall sensors in principle operate ov

122 onsive shape-morphing behaviors induced by a magnetic field can be digitally and repeatedly reprogram

123 fined to their lowest Landau level in a high magnetic field can form a variety of correlated states,

124 e results indicate that the application of a magnetic field can improve performance in a molecular se

125 erimentally that the often neglected optical magnetic field can nevertheless play an important role i

126 interaction revealed the presence of strong magnetic fields characteristic of Weibel Instability, an

127 e need to address the nuclei via oscillating magnetic fields complicates their integration in multi-s

128 tic field range of +/- 500 uT with the earth magnetic field components cancelled.

129 treme variations in the direction of Earth's magnetic field contain important information regarding t

130 line anisotropy, meaning that small external magnetic fields could reverse the direction of their mag

131 the lowest Landau level owing to a synthetic magnetic field created by Floquet engineering(18) a twis

132 r observable features, such as luminosity or magnetic field, crucially depends on the poorly known he

133 In a magnetic field, cubic Fe(3) O(4) nanoparticles exhibit a

134 egion, corresponding to the strongest static magnetic fields currently available.

135 Measurement of the in-plane magnetic field dependence of the chemical potential near

136 T (MI) demonstrates anisotropic magnetic field dependence with the preferred orientation

137 We find that the temperature and magnetic field dependences of the resistivity of LNO at

138 compounds and their aggregates display clear magnetic field dependences up to 25 T, with the aggregat

139 agnetoresistance emerges, resulting from the magnetic field-dependent MI transition.

140 nt density functional theory calculations of magnetic field-dependent phthalocyanine monomer and dime

141 of inequivalent Co(2+) sublattices generate magnetic-field-dependent ferroelectric polarization with

142 The levitation height of particles in the magnetic field depends on the magnetic susceptibility an

143 We optimize the magnetic field detection limit under different condition

144 apability of imaging spectroscopy in coronal magnetic field diagnostics.

145 spin Hall angle(7-9), and when flipping the magnetic-field direction, reversing the magnon chirality

146 On the other hand, magnetic fields do not suffer these losses, which has le

147 A magnetic-field-driven quantum phase transition from a QA

148 n the insulating limit, the application of a magnetic field drives a quantum phase transition to an e

149 we find magnetism to strengthen under strong magnetic fields due to suppression of the Kondo effect.

150 re chemical shift dispersion due to the high magnetic field, eddy currents caused by the pulsed magne

151 )(CH(2))(3)NH(3)), and 3D MAPbI(3) using the magnetic field effect (MFE) on conductivity and electrol

152 itting diode (OLED) displays a sign reversal magnetic field effect (MFE) when the applied magnetic fi

153 A pervasive magnetic field effect on an aromatic molecule is the aro

154 e zero-field peak results from a quasistatic magnetic-field effect of the RF radiation for periods co

155 be influenced by magnetic fields, and these magnetic field effects are diverse.

156 asis we predict the feasibility of observing magnetic field effects under experimentally relevant con

157 to investigate the radical-pair mechanism of magnetic-field effects in photochemical reactions, allow

158 MNPs) by non-heating extremely low frequency magnetic field (ELF MF) is explored as a tool for non-in

159 paradigm has been developed that allows the magnetic field emissions generated by the electrical act

160 epitaxial strain, layer thickness, electric, magnetic fields, etc.

161 on the electron), which implies C = 2, for a magnetic field exceeding 0.4 tesla.

162 Pulsed magnetic field exposure of human breast cancer cells tha

163 nsitions that are first-order insensitive to magnetic field fluctuations, enabling optical linewidths

164 Application of a magnetic field for 90 s via a magnetically assisted retr

165 articles are responsive to both electric and magnetic fields for practical applications.

166 ys have been proposed to generate switchable magnetic fields for pre-polarisation in Ultra-Low Field

167 charged particles are trapped by the Earth's magnetic field, forming the Van Allen radiation belts.

168 The built-in magnetic field gradient reduces the reliance on high-pow

169 y a magnetic device that generates a uniform magnetic field gradient within a space that is sufficien

170 ic field, eddy currents caused by the pulsed magnetic field gradients, and possible mechanical instab

171 In quantizing magnetic fields, graphene superlattices exhibit a comple

172 The Fermi energy-magnetic field-Hall conductivity (E(F)-B(z)-sigma(xy)) a

173 The Earth's magnetic field has operated for at least 3.4 billion yea

174 However, the QAH effect at zero magnetic field has so far been realized only for C = 1.

175 High magnetic fields have revealed a surprisingly small Fermi

176 Measurements under large magnetic fields have revealed an unusual Landau level (L

177 s of quark nuggets have assumed no intrinsic magnetic field; however, Tatsumi found that quark nugget

178 e, parahydrogen bubbling within a microtesla magnetic field (i.e. under conditions of SABRE in shield

179 te the band topology modification via a weak magnetic field in a ferromagnetic Weyl semimetal candida

180 s can be assessed by rheo-microMRI at a high magnetic field in a noninvasive, quantitative, and real-

181 new way for generating long-lived in-medium magnetic field in heavy ion collisions.

182 toresistance effect that appears around zero magnetic field in high mobility GaAs/AlGaAs 2DES (~10(7)

183 The bend distortion is analog to the magnetic field in metals and penetrates in the frustrate

184 polaritons up to 200 kelvin without external magnetic field in monolayer WS(2) excitons coupled to a

185 However, direct measurements of the magnetic field in the Sun's corona are difficult to obta

186 Magnetars have surface magnetic fields in excess of 10(14) gauss, the decay of

187 ic basis for possible applications of pulsed magnetic fields in novel anticancer strategies.

188 The observation of the magnetic field-independent magnetoresistance at low temp

189 At temperature T < ~17 K, the state of near-magnetic field-independent resistance, which is due to s

190 bserved enhanced VZS arises from an internal magnetic field induced by the tridopant clusters, which

191 CoMn(1-x)Fe(x)Ge demonstrated larger magnetic field-induced entropy changes and giant magneto

192 The most striking result was the large magnetic field-induced membrane deformation allowing to

193 ging, addressing image distortion because of magnetic field inhomogeneities, reproducible quantitativ

194 This organism has a similar response to magnetic field inversions as MTB.

195 A two-dimensional electron gas in a magnetic field is a model system where optical transitio

196 on of magnetic levitation in non-homogeneous magnetic field is also demonstrated.

197 FT ICR mass spectrometers with an ultrahigh magnetic field is eliminated.

198 A large out-of-plane magnetic field is expected to modify the exciton-phonon

199 Earth's magnetic field is presently characterized by a large and

200 y lateral spin-orbit torque in zero external magnetic field is reported.

201 zigzag chains (frustrated spin ladder) in a magnetic field is still lacking.

202 in a paramagnetic liquid under a nonuniform magnetic field, is a powerful tool for determining densi

203 cle distance and crystal symmetry, while the magnetic field leads to anisotropic crystal growth.

204 e electrons form a beam collimated along the magnetic-field lines.

205 ource in the presence of spatially diverging magnetic-field lines.

206 magnetic resonance in the regime of very low magnetic fields (<1 mT).

207 Finite-magnetic-field measurements further reveal weak antiloca

208 he dayside aurora is closely associated with magnetic field merging at the dayside magnetopause.

209 iggered by an exogenous circularly polarized magnetic field (MF) to enhance ferroptosis-like cell-dea

210 ash photolysis corroborated with an external magnetic field (MF), we have detected the transient gemi

211 ed meteorite samples with the ultrasensitive magnetic field modulated microwave spectroscopy (MFMMS)

212 ction between rotation and magnetic field: a magnetic field naturally arises along the fluid vorticit

213 es and their relaxation can be used to sense magnetic field noise at gigahertz frequencies.

214 hat multiple magnons participate in creating magnetic field noise below the ferromagnetic gap frequen

215 eld of up to 9 tesla, with an upper critical magnetic field of about 62 tesla according to the Ginzbu

216 We image the dynamic response to a 500 MHz magnetic field of the complex three-dimensional magnetiz

217 d electron cyclotron oscillations inside the magnetic field of the objective lens.

218 the transition temperature under an external magnetic field of up to 9 tesla, with an upper critical

219 f-filling can reappear in small out-of-plane magnetic fields of 0.4 tesla, giving rise to quantized H

220 in pO(2) sensitivity was observed at higher magnetic fields of 7 T and 9.4 T for HMDSO and OMTSO.

221 than 10 million at m/q = 1000 with moderate magnetic fields of about 7 T.

222 The dipole magnetic fields of the NV-resonant magnons couple to and

223 Alternatively, colour control by magnetic field offers contactless, non-invasive and ener

224 By pre-seeding uniform magnetic fields on the kilotesla order, the Lorenz force

225 rnal forces are applied on the fluid and the magnetic field only exerts an external torque aligning m

226 device's miniaturization, material, and zero-magnetic-field operation are important advances for rare

227 tunable through applying either an external magnetic field or hydrostatic pressure.

228 hat are predicted to give rise, under modest magnetic fields or strain, to topological semimetallic b

229 w that this phenomenon is not limited to low magnetic fields or the use of resonators with high-quali

230 rmi acceleration due to transport across the magnetic field, or if a combination of both mechanisms i

231 ining the behavior at the highest accessible magnetic fields, our results imply a different origin fo

232 etic field (ALTADENA condition) or in a high magnetic field (PASADENA condition) to induce RASER with

233 specific absorption rate (SAR) and change in magnetic field per unit time (dB/dt), maximum specific e

234 t of pai-electrons upon the application of a magnetic field perpendicular to the pai-system of the mo

235 The obtained strain-magnetic field phase diagram reveals that C(4) -symmetry

236 Using variable magnetic field PL spectroscopy, we resolved emission int

237 e mean free path of ions with the increasing magnetic field power.

238 le possibilities to achieve cilia actuation, magnetic fields present an opportunity given their quick

239 Due to its novel feature, this new magnetic field provides a nontrivial explanation to the

240 cetate-1-(13)C, resulting from zero-crossing magnetic field ramps of various durations, amplitudes, a

241 magnetic field effect (MFE) when the applied magnetic field range is reduced to the sub-milliTesla ra

242 ine)aluminium-based (Alq(3)) OLED within the magnetic field range of +/- 500 uT with the earth magnet

243 htside aurora, which is controlled mainly by magnetic field reconnection in the magnetotail, the days

244 tic Lagrangian (E and B are the electric and magnetic field, respectively).

245 102 kOe measured using static or pulsed high magnetic fields, respectively.

246 two-dimensional electron systems in a strong magnetic field revealed the quantum Hall effect(1), a to

247 nian and shed new light on metrology and bio-magnetic field sensing.

248 ion measurement is demonstrated through weak magnetic-field sensing.

249 T, with the aggregates showing more drastic magnetic field sensitivities depending on the intermolec

250 Solid-state magnetic field sensors are important for applications in

251 Most magnetic field sensors function in a limited range of te

252 discovery of a C = 2 Chern insulator at zero magnetic field should open up opportunities for discover

253 tion efficiency as a function of the applied magnetic field, showing potential for wirelessly control

254 The application of a strong magnetic field significantly and beneficially alters she

255 ical hypotheses, a weak 7 MHz radiofrequency magnetic field significantly reduces the biological resp

256 t junctions, in combination with an external magnetic field, significantly enhanced both DOX-EDT-IONP

257 cs, including effective spin-orbit coupling, magnetic fields, spin-momentum locking, a Meissner-to-vo

258 nal magnetic resonance imaging (MRI) at high magnetic field strength (7-tesla).

259 ct quantitative measurements of the evolving magnetic field strength are required to test this.

260 quires the acquisition of images at variable magnetic field strength as provided by fast field cyclin

261 The results herein communicate the highest magnetic field strength data on active zeolite catalyst

262 Higher magnetic field strength improves all performance charact

263 ds the threshold for dynamo activity and the magnetic field strength is similar to that observed in t

264 spectrometers with different configurations (magnetic field strength, manufacturer, age).

265 and dynamic range improve quadratically with magnetic field strength.

266 relationship between the Deltag(lum) and the magnetic field strength.

267 t to be produced by the decay of the coronal magnetic field strength.

268 hese insulator states increase with in-plane magnetic field, suggesting a ferromagnetic order.

269 e accurately predicted by changes in Earth's magnetic field, suggesting that these birds rely on a ge

270 The response of these correlated states to magnetic fields suggests evidence of spin-polarized grou

271 al strategy incorporating pulse-programmable magnetic field sweeping and in situ detection has been d

272 cterize the tunneling magnetoresistance, the magnetic field switching, and the current-induced switch

273 elimagnet occurs only over a very restricted magnetic field-temperature phase space and often in the

274 In zero magnetic field, the direction of the deterministic curre

275 When exposed to an alternating magnetic field, the flexible magnetic cantilevers vertic

276 In the presence of an external magnetic field, the surface plasmon polariton that exist

277 Under strong magnetic fields, the topological properties of Dirac/Wey

278 rticle trajectories, accurate values for the magnetic field through which charged species traverse ar

279 he violation of time-reversal symmetry via a magnetic field; thus establishing CPA beyond its initial

280 An increase in the magnetic field to 21 T did not show a proportional incre

281 omyocytes and applying a short-term external magnetic field to orient the cells along the applied fie

282 SPS in the devices is driven by the external magnetic field to perform different movements in a 3D fl

283 Application of magnetic field tunes this capacitance affecting its reso

284 From the behavior under external magnetic fields, two independent mechanisms giving rise

285 u[Formula: see text]PO[Formula: see text] in magnetic fields up to 45 T, revealing a field-induced sp

286 larized even at zero fields, preserves under magnetic fields up to B = 9 T.

287 ence Devices (SQUIDs) for measurement of the magnetic field vector, highly sensitive Superconducting

288 relied on transducing electric signals into magnetic fields via the electron-nuclear hyperfine inter

289 lls to sequential 50- and 385-Hz oscillating magnetic fields was sufficient to induce intracellular p

290 model with Heisenberg XY interactions and no magnetic field, we observe an anomaly in quantum phases

291 ividual layer magnetization in CrI(3) with a magnetic field, we show that the spin-dependent charge t

292 By perturbing with external magnetic fields, we show the robustness of these meron p

293 vanishing longitudinal resistance under zero magnetic field (where h is the Planck constant, e is the

294 in the real space by applying a local pulsed magnetic field, which causes their motion in the opposit

295 ignment of nuclear spins with applied static magnetic field, which is called nuclear spin polarizatio

296 sensitive to the presence of a perpendicular magnetic field, which strongly modifies the spectroscopi

297 is observed to oscillate in a perpendicular magnetic field with a flux period of h/e (h is Planck's

298 We applied a pulsed 20-millitesla (mT) magnetic field with rate of rise (dB/dt) in the msec ran

299 rforming rheo-microMRI velocimetry at a high magnetic field with strong pulsed field gradients has cl

300 Taken together, the data show that applied magnetic fields with magnetic nanoparticles can be delib