ライフサイエンスコーパス: applied magnetic field

1 ased ion acceleration with a kilotesla-level applied magnetic field.

2 eloped that enables graft retrieval under an applied magnetic field.

3 duced inside the superconducting state by an applied magnetic field.

4 phase gradients created in the leads by the applied magnetic field.

5 sotropy and fast magnetic relaxation in zero applied magnetic field.

6 ization imprint that are both actuated by an applied magnetic field.

7 lectrical current that is proportional to an applied magnetic field.

8 high-Tc superconductor in the presence of an applied magnetic field.

9 conductor La(2-x)Sr(x)CuO4 (x = 0.163) in an applied magnetic field.

10 g coupling regime via the orientation of the applied magnetic field.

11 quantum mechanics can be tuned by varying an applied magnetic field.

12 rt is spin-valley polarized, even without an applied magnetic field.

13 ate a topological Chern insulator without an applied magnetic field.

14 plet radical-pair states made possible by an applied magnetic field.

15 highly unusual thermal Hall effect under an applied magnetic field.

16 t of magnetic entropy present below 1 K in 0-applied magnetic field.

17 polarization that is an even function of the applied magnetic field.

18 known to connect molecular chirality with an applied magnetic field.

19 terial might be significantly retarded by an applied magnetic field.

20 e magnetization away from the c-axis with an applied magnetic field.

21 suppression is not present in the absence of applied magnetic field.

22 he primary axisymmetric flow modified by the applied magnetic field.

23 ia through an artificial pore space under an applied magnetic field.

24 -2/3 and v = -3/5 ferromagnetic states with applied magnetic field.

25 the crystal orientation with respect to the applied magnetic field.

26 n of the state in the filling factor with an applied magnetic field.

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

28 ble high sensitivity of the structure to the applied magnetic field.

29 lation using injected current rather than an applied magnetic field.

30 al symmetry has been broken by an externally applied magnetic field.

31 netic state as a function of temperature and applied magnetic field.

32 mplexes are sensitive to external stress and applied magnetic field.

33 ion electron microscopy as a function of the applied magnetic field.

34 changes to the Fermi surface induced by the applied magnetic field.

35 ich trap superconducting vortices induced by applied magnetic field.

36 ns depends on the magnitude and direction of applied magnetic field.

37 collective directions for the Fe moments by applied magnetic field.

38 he sensitivity of the yield of (3)*TPD to an applied magnetic field.

39 al's electrical resistance in response to an applied magnetic field.

40 tion of the magnitude and orientation of the applied magnetic field.

41 an be fine-tuned by the exchange-bias and an applied magnetic field.

42 en repeatable magnetization reversal with no applied magnetic field.

43 on signal exhibits a sharp dependence on the applied magnetic field.

44 lly aligned parallel to the direction of the applied magnetic field.

45 olecule magnet behavior in the absence of an applied magnetic field.

46 ariation in the electrical resistivity under applied magnetic field.

47 far in bilayer graphene in the absence of an applied magnetic field.

48 eaks in the density of states produced by an applied magnetic field.

49 s were investigated both with and without an applied magnetic field.

50 tic gradient concentrators for an externally applied magnetic field.

51 s transport properties in the presence of an applied magnetic field.

52 hown by variable-temperature measurements in applied magnetic field.

53 rage alignment of each helix relative to the applied magnetic field.

54 high engineering critical current density in applied magnetic fields.

55 n-magnetic semiconductors, in the absence of applied magnetic fields.

56 e cooling weakens the plasma response to the applied magnetic fields.

57 atent heats are traditionally accessed using applied magnetic fields.

58 bbles rising in a liquid metal under varying applied magnetic fields.

59 by the quantum metric and can be tuned with applied magnetic fields.

60 utral and charged excitonic resonances under applied magnetic fields.

61 of the electrical transport measurements at applied magnetic fields.

62 and easily manipulated using temperature and applied magnetic fields.

63 Precession frequencies exceed 2 THz in applied magnetic fields.

64 with various optical responses to externally applied magnetic fields.

65 eaus, and exotic spin states with increasing applied magnetic fields.

66 miconductor band structure in the absence of applied magnetic fields.

67 Here, we report that an applied magnetic field (0-1 T) can be used control the c

68 130 K when the material was exposed to weak applied magnetic fields (10 Oe) and a distinct "half-lev

69 eels assemble into swarms that, depending on applied magnetic field actuation patterns, can be design

70 that specific variations of temperature and applied magnetic fields allow us to make FDy parallel to

71 measured as a function of orientation of the applied magnetic field allowed us to quantify the magnit

72 wall senses and that can be measured by the applied magnetic field amplitude along the nanowire wher

73 Using an applied magnetic field and an advancing oxygen gradient,

74 ch requires zero electrical resistance in an applied magnetic field and depends on vortex dynamics, a

75 n be mutually controlled by the direction of applied magnetic field and linear polarization of the la

76 pling strength can be tuned by modifying the applied magnetic field and spin current.

77 relationship between the drift velocity and applied magnetic field and the value of the maximum drif

78 For a constant applied magnetic field and under the same driving condit

79 rational in the presence of large externally applied magnetic fields and functions even for electroni

80 ise to a record magnetocaloric effect at low applied magnetic fields and low temperatures.

81 nabling largely tunable optical responses to applied magnetic fields and magnons.

82 our detection method requires no externally applied magnetic fields and the associated fabrication i

83 , the resistance increases in response to an applied magnetic field) and only weakly temperature-depe

84 on-linear response to the orientation of the applied magnetic field, and extract a spin-orbit gap E 5

85 evolution with changing electron density and applied magnetic field, and present two possible models

86 pid excursions, opposite the direction of an applied magnetic field, and slower returns along the dir

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

88 this quantum many-body effect induced by an applied magnetic field are rare.

89 nce peaks aligned along the direction of the applied magnetic field, as expected for a pair of Majora

90 ements of the magnetization as a function of applied magnetic field at 2 K for Na4MnU6F30 confirmed t

91 Increasing the strength of the applied magnetic field brings all spinwave modes to high

92 rature, pressure, impurity concentration and applied magnetic field, but, surprisingly, there have be

93 liably moved over 15-20 um distances at zero applied magnetic field by a magnon spin current excited

94 etic materials, ordered phases induced by an applied magnetic field can be described as the Bose-Eins

95 etection limits and decrease assay times, an applied magnetic field can be used to promote target bin

96 We demonstrate that a locally applied magnetic field can enhance the cellular entry of

97 th and spatial confinement controlled by the applied magnetic field direction.

98 present in radical polymer thin films under applied magnetic fields due to the presence of impurity

99 Under applied magnetic field, electrons and holes couple acros

100 Light irradiation under an applied magnetic field enables fully reversible switchin

101 erconductivity is a rare phenomenon where an applied magnetic field enhances or induces superconducti

102 tic hyperfine structure in the absence of an applied magnetic field, excluding the possibility that i

103 At zero applied magnetic field, extremely rapid (300-600 GHz) sp

104 photoluminescence patterns as a function of applied magnetic field for select quantum emitters in h-

105 sure electric conductance measurements in an applied magnetic field for the sample quenched from high

106 Bp, these resonances are insensitive to the applied magnetic field; for fields in excess of Bp, the

107 , for instance, through a slight tilt of the applied magnetic field from the normal of the nanopillar

108 ere, we show that in UTe(2) crystals extreme applied magnetic fields give rise to an unprecedented hi

109 is typically dictated by the strength of the applied magnetic field gradients, resulting in hard reso

110 el vector reorientation in the absence of an applied magnetic field, H.

111 ical current density (J(c)) as a function of applied magnetic field has been studied from magnetic is

112 for the colossal change in resistance under applied magnetic field, has prevented an atomistic-level

113 ity of manipulating magnetic systems without applied magnetic fields have attracted growing attention

114 d increase of the intrinsic noise at certain applied magnetic fields heralds the spontaneous prolifer

115 sport exhibits asymmetry with respect to the applied magnetic field, i.e., an exchange-bias behavior.

116 By controlling an applied magnetic field in a laser produced plasma, we ha

117 try-breaking electronic orders tunable by an applied magnetic field in a model Kagome magnet FeSn con

118 ing the axis of rotation with respect to the applied magnetic field in a spinning liquid crystalline

119 is established at room temperature and zero applied magnetic field in light-emitting diodes(2-7), th

120 der of (H/2) x 10(11) cm(-2), where H is the applied magnetic field in tesla.

121 The Kitaev model with an applied magnetic field in the [Formula: see text] direct

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

123 e electronic states in the vortex halo in an applied magnetic field, in strong field that suppresses

124 quencies as a function of the inverse of the applied magnetic field, incommensurate order leads to th

125 ductive object, which then interact with the applied magnetic field, inducing force and torque on the

126 y with a nitrogen-vacancy defect using small applied magnetic fields, inducing significant nitrogen-v

127 Under certain conditions, an applied magnetic field is expected to stabilize an unusu

128 the pair's recombination is enhanced as the applied magnetic field is reduced.

129 rature and lose their magnetization when the applied magnetic field is removed.

130 f cobalt nanocontacts as the direction of an applied magnetic field is varied.

131 reaction of Kramers-degenerate states to an applied magnetic field, is of increasing importance in t

132 Fe(Te0:9Se0:1) are remarkably insensitive to applied magnetic field, leading to predictions of upper

133 The lifting of this protection by the applied magnetic field leads to a very large magnetoresi

134 An analysis of the data obtained in applied magnetic fields leads to the assignment of the s

135 ngth scales, and can be modulated in situ by applied magnetic fields <250 mT, resulting in an enhance

136 Magnetic, wild-type cells swimming in an applied magnetic field more quickly migrate away from th

137 Variable temperature magnetization and applied magnetic field Mossbauer spectroscopy studies re

138 10(5) A/cm2 to 2 x 10(6) A/cm2 at 5 K in an applied magnetic field of 10 kilooersteds (1 oersted = 8

139 Neutron diffraction has shown that an applied magnetic field of 5 T is sufficient to induce sa

140 it was measured by magnetometry at 5 K in an applied magnetic field of 5 T.

141 on-local magnetoresistance of >90,000% in an applied magnetic field of 9 T at 300 K in few-layer grap

142 covery of novel multiple sign changes versus applied magnetic field of the MR in the cubic intermetal

143 We predict that the direction of a modest applied magnetic field of u(0)H 1 to 2 T can tune betwee

144 c structure in GdPd3 is highly fragile since applied magnetic fields of moderate strength significant

145 This study examines the effect of externally applied magnetic field on particle deposition patterns.

146 We combine tunable uniaxial stress and applied magnetic field on the ferromagnetic superconduct

147 The effects of applied magnetic fields on the photochemistry of purifie

148 The effects of applied magnetic fields on the traveling wave formed by

149 micrometre-distance displacement without an applied magnetic field or any other external stimuli can

150 They exhibit large tunability under an applied magnetic field or gate voltage, and clear signat

151 s spin polarization can be achieved using an applied magnetic field or polarized ferromagnetic contac

152 field flow fractionation, which utilizes an applied magnetic field oriented orthogonal to the capill

153 The range in pressure, temperature and applied magnetic field over which we observe an anomalou

154 lations, indicates that the direction of the applied magnetic field promotes the formation of suspend

155 t excitations of a quantum spin ladder in an applied magnetic field provide a supersymmetric analogue

156 eversal magnetic field effect (MFE) when the applied magnetic field range is reduced to the sub-milli

157 a field-induced spin disordered state in an applied magnetic field range of 7.5 T < B ( b-axis) < 10

158 We varied the direction of an applied magnetic field relative to the crystal axes, and

159 ges as high as 5.6% under only 1.3 T, or 3 T applied magnetic fields, respectively.

160 nt perpendicular to the heat current and the applied magnetic field, resulting in the thermal Hall ef

161 magnetocaloric effect (MCE) as a function of applied magnetic field reveals isothermal entropy change

162 iferromagnetic Kitaev model in an externally applied magnetic field, sandwiched between the well-know

163 ing of the fourfold degeneracy in very large applied magnetic fields, separating the quartet into int

164 oto detector signal vs. the frequency of the applied magnetic field show a characteristic peak due to

165 Studies in applied magnetic fields show that the spins of sites a a

166 diffraction efficiency as a function of the applied magnetic field, showing potential for wirelessly

167 The dependence of the (3.)PDI yield on an applied magnetic field shows a resonance, which gives th

168 ter/unit Tesla, K(NAA) in the absence of any applied magnetic field strength would be 32.

169 at improvement is equivalent to doubling the applied magnetic field strength, without loss in signal-

170 tor, in which the control over an externally applied magnetic field suffices to create and manipulate

171 Under an applied magnetic field, superparamagnetic Fe(3) O(4) nan

172 ransforms into a transverse conical state in applied magnetic field, supporting a significant THE sig

173 a temperature gradient in a perpendicularly applied magnetic field, termed the Nernst effect, has pr

174 large-amplitude modulation of the externally applied magnetic field that is suitable for non-magnetic

175 by thermal fluctuations can be studied using applied magnetic fields that are sufficiently strong to

176 abatic temperature following a change in the applied magnetic field, that is, the magnetocaloric effe

177 ure-dependent resistance with and without an applied magnetic field, the magnetization (M) versus mag

178 current is then reduced towards zero in the applied magnetic field, the magnetization can reliably f

179 In contrast to a superconductor in a uniform applied magnetic field, the nucleation of the supercondu

180 2 clusters are paramagnetic, but in external applied magnetic fields they exhibit exalted diamagnetis

181 nodiscs were shown to align in an externally applied magnetic field, they can also be used to measure

182 raphically patterned magnetic dipoles and an applied magnetic field to drive an assembly process simi

183 el the ESR spectra observed in an externally applied magnetic field to enable dc magnetometry in solu

184 by the fully developed COC combines with the applied magnetic field to exert the greatly enhanced tra

185 computing by modulating the amplitude of the applied magnetic field to inject time-multiplexed input

186 oscopy at temperatures as low as 10 mK in an applied magnetic field to study the top layer of multila

187 wheels) and manipulated under the control of applied magnetic fields to enable rapid thrombolysis of

188 s of tuning parameters, such as pressure and applied magnetic field, to exactly suppress a continuous

189 on suppression of superconductivity by high applied magnetic fields, together with complementary spe

190 1.X, were recorded between 4.2 and 200 K in applied magnetic fields up to 8.0 T.

191 to reorient the antiferromagnet spin-axis in applied magnetic fields via the exchange spring effect.

192 Using neutron scattering in an applied magnetic field, we observe spontaneous decay bet

193 Under an applied magnetic field, we observe that the helical grou

194 Probing the charged excitons in applied magnetic fields, we observe large gyromagnetic r

195 Magnetic labels magnetized by a homogeneous applied magnetic field weaken and strengthen the applied

196 ow rate and the strength and gradient of the applied magnetic field were the key parameters in contro

197 excellent retention of this current in high applied magnetic fields were achieved in the thick films

198 (0.5)Fe(1.5)O(4) (MAFO) thin films near zero applied magnetic field where the sample forms a multi-do

199 This crossover is destroyed by an applied magnetic field which suggests a magnetic origin

200 loading forces by adjusting the magnitude of applied magnetic field, which is very important for stud

201 the suppression of magnetic scattering in an applied magnetic field, which is well-described by consi

202 ed through either current/voltage pulsing or applied magnetic field, which represents a promising ste

203 the optical rotation that do not respond to applied magnetic fields, while the spontaneous Kerr sign

204 lso show magnetic correlations shifting with applied magnetic field with a degree of missing entropy

205 All features shift linearly versus applied magnetic field with slopes matching the correspo

206 Taken together, the data show that applied magnetic fields with magnetic nanoparticles can

207 rotation from an in-plane to an out-of-plane applied magnetic field, with the greatest suppression ob

208 isplays a large, nearly linear increase with applied magnetic field without saturation to the highest

209 ulsive to attractive by tuning an externally applied magnetic field yields detailed information on th