ライフサイエンスコーパス: ferromagnet

1 ed electrons from the La(0.66)Sr(0.33)MnO(3) ferromagnet.

2 metal or the Rashba-Edelstein effect in the ferromagnet.

3 superconductor upon entering the neighboring ferromagnet.

4 ements show that F4BImNN acts as a quasi-1-D ferromagnet.

5 hysteresis loops reminiscent of a classical ferromagnet.

6 h the reversal of magnetic field in an Ising ferromagnet.

7 ase transition is the transverse field Ising ferromagnet.

8 oscillations in ensemble-averaged spins of a ferromagnet.

9 peculiar kind of constrained two-dimensional ferromagnet.

10 governed by an antiferromagnet instead of a ferromagnet.

11 etal and spin transfer torque in an in-plane ferromagnet.

12 um processing with spin-transport effects in ferromagnets.

13 s for writing and reading the information in ferromagnets.

14 with properties that cannot be achieved with ferromagnets.

15 st common spin ensembles in nature: spins in ferromagnets.

16 DW if grown between non-co-linearly aligned ferromagnets.

17 could assist or accomplish the switching of ferromagnets.

18 ls that are as large as the highest seen for ferromagnets.

19 han the macroscopic scales characteristic of ferromagnets.

20 previously observed only using half-metallic ferromagnets.

21 materials such as electrical conductors and ferromagnets.

22 ced magnetoresistance in low-carrier-density ferromagnets.

23 litatively similar to the classic d-electron ferromagnets.

24 to manipulate the magnetization in metallic ferromagnets.

25 these antiferromagnetic materials to become ferromagnets.

26 ty that makes antiferromagnets distinct from ferromagnets.

27 e writing magnetic field angle, analogous to ferromagnets.

28 rt lifetime of these excitations in metallic ferromagnets.

29 perconductor interface with an inhomogeneous ferromagnet, a gapless odd frequency superconducting sta

30 unctional, yielding a room-temperature Fe-Pt ferromagnet, a superconducting sample of Ag2Pd3S (Tc = 1

31 hase transition from an antiferromagnet to a ferromagnet above room temperature (Tr approximately 370

32 oxides, polycrystalline ferroelectrics, and ferromagnets alike.

33 The easily measured properties of the ferromagnet allow access to the internal magnetic degree

34 In a ferromagnet, an applied electric field E invariably prod

35 an antiferromagnet and those in an adjacent ferromagnet, an effect first discovered in 1956 and refe

36 ferent Prussian blue analogues, where A is a ferromagnet and B is a photoinducible ferrimagnet, have

37 higher than those of any known ferroelectric ferromagnet and rival the best materials that are solely

38 is a nearly ideal two-dimensional Heisenberg ferromagnet and so will be useful for studying fundament

39 ar coupling between the magnetization in the ferromagnet and the projection of the antiferromagnetic

40 ing the local excitations of systems such as ferromagnets and antiferromagnets, skyrmions, atomically

41 s of light-material interactions in metallic ferromagnets and multilayers.

42 to the coercivity mechanism of Nd-based bulk ferromagnets and provide a new idea to design prospectiv

43 f over 11 T at 2 K outperform all known hard ferromagnets and single-molecular magnets.

44 carriers acquire spin-polarization from the ferromagnet, and dynamically polarize these nuclear spin

45 ining effects associated with a conventional ferromagnet/antiferromagnet system.

46 One particularly simple system is a ferromagnet approaching its Curie temperature, T(C), whe

47 ng landscape when the superconductor and the ferromagnet are electron ically coupled or insulated by

48 Ferromagnets are commonly magnetized by either external

49 Meanwhile, low-damping metallic ferromagnets are desired for charge-based spintronic dev

50 Ferroelectric ferromagnets are exceedingly rare, fundamentally interes

51 to their conductivity, low-damping metallic ferromagnets are preferred to insulating ferromagnets in

52 La(0.7)Sr(0.3)MnO(3) is a conducting ferromagnet at room temperature.

53 to induce efficient spin-torque switching of ferromagnets at room temperature.

54 The feasibility of a single-domain ferromagnet based on uniaxial magnetic ions was examined

55 er cooling, the compounds become canted weak ferromagnets below 40 K.

56 for the spin-orbit torques in a heavy metal/ferromagnet bilayer geometry, showing in general both fi

57 that uses current passing through a tantalum-ferromagnet bilayer to switch a nanomagnet, with a magne

58 that spin-orbit interactions in heavy-metal/ferromagnet bilayers can produce strong current-driven t

59 ological insulator (TI) is in contact with a ferromagnet, both time-reversal and inversion symmetries

60 nce domain wall motion in ultrathin metallic ferromagnets, but the effects have been relatively modes

61 recently resulted in room-temperature polar ferromagnets, but the electrical polarization has not be

62 c films deposited on electrically insulating ferromagnets, but the films' high resistance limits ther

63 ormed from spin-frustrated semiconductors to ferromagnets by doping with either electrons or holes, p

64 in the magnetization behaviour of thin-film ferromagnets by three distinct mechanisms that can each

65 ar near magnetization inhomogeneities in the ferromagnet, called bifurcations.

66 n current applied to a nanoscale region of a ferromagnet can act as negative magnetic damping and the

67 The fact that ferromagnets can be studied easily and with high precisi

68 cyanoethylene) magnetically orders as a weak ferromagnet (canted antiferromagnet) below 21.0 +/- 0.1

69 ctly the magnetic anisotropy in the uniaxial ferromagnet CeRu2Ga2B.

70 ange interactions at the interface between a ferromagnet (Co(0.9)Fe(0.1)) and the antiferromagnet.

71 elds to tune the quasi-one-dimensional Ising ferromagnet CoNb2O6 (cobalt niobate) through its critica

72 Studies to date on ferromagnet/d-wave superconductor heterostructures focus

73 c insulators (e.g. EuO, GdN) or halfmetallic ferromagnets (e.g. CrO2, LCMO).

74 Our hybrid device has a ferromagnet electrode as a spin injector and a spin Hall

75 per pairs, which arise in superconductor (S)-ferromagnet (F) heterostructures with magnetic inhomogen

76 gnetic inhomogeneity at a superconductor (S)-ferromagnet (F) interface converts spin-singlet Cooper p

77 d phases, such as a superconductor (S) and a ferromagnet (F), is driving new fundamental physics and

78 l the flow of electrons by ferromagnets in a ferromagnet (F1)/normal metal (N)/ferromagnet (F2) spin

79 gnets in a ferromagnet (F1)/normal metal (N)/ferromagnet (F2) spin valve, where F1 acts as the polari

80 Although the strong interactions in a ferromagnet favour the excitation of extended collective

81 As the ferromagnet Fe becomes more noble in the FePt compound,

82 is considered to arise from the bulk of the ferromagnet (FM) and the proximity-induced FM boundary l

83 the magnetisation dynamics of an insulating ferromagnet (FM) deposited on the surface of a three-dim

84 Recent discoveries from superconductor (S)/ferromagnet (FM) heterostructures include pi-junctions,

85 means of writing information in heavy metal/ferromagnet (FM) multilayer systems.

86 neration (SHG) to study a ferroelectric (FE)/ferromagnet (FM) oxide heterostructure.

87 lm, accompanying an antiferromagnet (AFM) to ferromagnet (FM) phase transition.

88 e it exerts a unidirectional anisotropy to a ferromagnet (FM) when coupled to an antiferromagnet (AFM

89 onary topological solitons in a fluid chiral ferromagnet formed by colloidal dispersions of magnetic

90 5) in some insulating ferromagnets, metallic ferromagnets generally have larger damping due to magnon

91 Depending on the ferromagnet geometry and material parameters, this asymm

92 of a single classical spin (e.g. monodomain ferromagnet) governed by the Landau-Lifshitz-Gilbert-Slo

93 ces that, rather than reorienting spins in a ferromagnet, harness direct control of a materials intri

94 ts.The study of phase transitions in quantum ferromagnets has shown that the approach to a continuous

95 Therefore, Sr4Ru3O10, a T C = 105 K ferromagnet, has attracted much attention in recent year

96 tional superconductors coupled with metallic ferromagnets; however it is still less known for oxide m

97 of exchange bias with unusual features of a ferromagnet in contact with a spin glass, demonstrating

98 fields from both, the superconductor and the ferromagnet in hybrid magnetic nano-devices based on hig

99 nifested in heterostructures consisting of a ferromagnet in intimate contact with the multiferroic Bi

100 ntronics to control the flow of electrons by ferromagnets in a ferromagnet (F1)/normal metal (N)/ferr

101 lic ferromagnets are preferred to insulating ferromagnets in charge-based spintronic devices, but are

102 The ferromagnets in question are disordered, low-carrier-den

103 erial is well described as a two-dimensional ferromagnet, in sharp contrast to the high-T(C) cuprates

104 ng of ferromagnetic/nonmagnetic systems, the ferromagnet-induced magnetic moment in the adjacent nonm

105 ons, we explain why the Co chalcogenides are ferromagnets instead of superconductors as in their iron

106 we report a study of spin pumping at the TI-ferromagnet interface, investigating spin transfer dynam

107 pin-Hall-effect-driven antidamping torque in ferromagnets interfaced with paramagnets with strong int

108 ephson junctions in which the superconductor/ferromagnet interfaces (S/F) are magnetically inhomogene

109 effect at complex-oxide-based superconductor/ferromagnet interfaces is not so clear.

110 as the hysteresis-loop shift observed when a ferromagnet is in contact with an antiferromagnet.

111 al control of the magnetization switching in ferromagnets is highly desired for future spintronic app

112 m that drives the magnetisation switching in ferromagnets is unclear.

113 magnetization of a model disordered uniaxial ferromagnet, is an isothermal regulator of domain pinnin

114 ffect, discovered more than 150 years ago in ferromagnets, is also present in AFMs.

115 d that when an ultrafast laser impinges on a ferromagnet, its spin moment undergoes a dramatic change

116 2Cu3O7 (YBCO) and colossal magnetoresistance ferromagnet La0.67Ca0.33MnO3 (LCMO).

117 Here we show that the ferromagnet La2-2xSr1+2xMn2O7 (x = 0.38) possesses minor

118 on by interfacial coupling to the insulating ferromagnet LaMnO3, and used to generate interlayer magn

119 e target spin separation is smaller than the ferromagnet lateral dimensions; typically about a tenth

120 ultrafast demagnetization of a perpendicular ferromagnet leads to spin accumulation in a normal metal

121 dict that Fe-doped CaZnOS is a single-domain ferromagnet like a bar magnet, and find the probable cau

122 in a bulk semiconductor without the need for ferromagnets, lithographic patterning techniques, or qua

123 hous paramagnetic layer through proximity to ferromagnets, mediating both exchange-spring magnet beha

124 an reach 10(-4) to 10(-5) in some insulating ferromagnets, metallic ferromagnets generally have large

125 tronic structure and lattice dynamics in the ferromagnet MnBi using first-principles calculations and

126 le AHE is rather well-understood in metallic ferromagnets, much less is known about the relevance of

127 NaFe4Sb12 is a known ferromagnet near a quantum critical point.

128 this is possible in composites of conducting ferromagnets (Ni or MnBi) containing metallic nanopartic

129 Although now a ubiquitous observation in ferromagnets, obvious flux-closure patterns have been so

130 register between perpendicularly magnetized ferromagnets of subnanometre thickness, similar to the l

131 This record low damping for metallic ferromagnets offers new opportunities for charge-based a

132 f anisotropy of a thin layer of a conductive ferromagnet on a dielectric substrate under the influenc

133 agnetic devices results from the torque on a ferromagnet owing to its interaction with a spin-polariz

134 easurements of magnetic noise emanating from ferromagnets owing to domain motion were first carried o

135 The ferromagnet/oxide interface is key to developing emergin

136 in torques induced by a lateral current at a ferromagnet/paramagnet interface are a candidate spintro

137 e presence of two-channel Kondo physics in a ferromagnet, pointing to considerable robustness of the

138 The bistability of ordered spin states in ferromagnets provides the basis for magnetic memory func

139 d state switches between antiferromagnet and ferromagnet, providing an additional tuning parameter in

140 The superconductor-ferromagnet proximity effect describes the fast decay of

141 tion of charge pumping in which a precessing ferromagnet pumps a charge current, demonstrating direct

142 nuclear polarization (DNP) in a quantum Hall ferromagnet (QHF) is a highly sensitive method for the d

143 an arise by a different mechanism in certain ferromagnets--quantum interference effects rather than s

144 Spin selectivity in a ferromagnet results from a difference in the density of

145 tion of the magnetic field in superconductor/ferromagnet (S/F) hybrids.

146 ow well established that at a superconductor/ferromagnet (S/F) interface an unconventional supercondu

147 polarized nuclear spins that align along the ferromagnet's magnetization.

148 stinguishing feature of spin accumulation in ferromagnet-semiconductor devices is its precession in a

149 ues in a prepared epitaxial transition-metal ferromagnet/semiconductor-paramagnet single-crystal stru

150 e spin-orbit torque switching in heavy metal/ferromagnet structures have been proposed with magnetic

151 While the energy scales of the rare earth ferromagnet studied here restrict the effects to cryogen

152 structure phase diagram as seen in itinerant ferromagnets such as ZrZn2 and UGe2.

153 Owing to strong magnetic coupling with the ferromagnet, such independent switching of an adsorbed m

154 In magnetically coupled, planar ferromagnet-superconductor (F/S) hybrid structures, magn

155 ensitivity is practically unchanged when the ferromagnet surface to the target spin separation is sma

156 ploited, it does not extend to semiconductor/ferromagnet systems, because the effect is too weak for

157 nerated by the magnetization dynamics of the ferromagnet that also forms at the same interface, which

158 ty for the phase diagram of metallic quantum ferromagnets.The study of phase transitions in quantum f

159 c exchange interaction with the surface of a ferromagnet; the device shows an unexpected interfacial

160 rison with those of useful ferroelectrics or ferromagnets: their spontaneous polarizations or magneti

161 zewski-like torque inversely scales with the ferromagnet thickness, and the field-like torque has a t

162 trical current can apply a large torque to a ferromagnet, through direct transfer of spin angular mom

163 involving the change of the magnetic state (ferromagnet to antiferromagnet) has been proposed.

164 rent, which can be injected into an adjacent ferromagnet to exert a torque.

165 duces a two serial magnetic transitions from ferromagnet to non-magnet state at room temperature.

166 ere that by forcing the magnetization in the ferromagnet to precess at resonance instead of relying o

167 ept may eventually reduce the sensitivity of ferromagnets to magnetic field perturbations to being a

168 intronics depends on the spin sensitivity of ferromagnets to the spin of the equal spin-triplet Coope

169 viding evidence of a spin selectivity of the ferromagnets to the spin of the triplet Cooper pairs.

170 he pioneering S/FI (where FI is a insulating ferromagnet) tunneling experiments of Meservey and Tedro

171 detail required for the characterization of ferromagnets used in fields ranging from spintronics to

172 a of spin Hall material into a small area of ferromagnet using a normal metal with large spin diffusi

173 omagnetic are transformed into ferroelectric ferromagnets using a single control parameter, strain.

174 ently, however, a new route to ferroelectric ferromagnets was proposed by which magnetically ordered

175 etically soft, two-dimensional van der Waals ferromagnet, we achieve unprecedented control of the tra

176 0 < or = x < or = 2) phases are not ordinary ferromagnets where all the magnetic spins are parallel a

177 ntiferromagnet film is exchange coupled to a ferromagnet, which allows us to reorient the antiferroma

178 ween an antiferromagnet or ferrimagnet and a ferromagnet, which has been widely employed to manipulat

179 c quantum phenomenon is spin tunnelling in a ferromagnet, which may be formulated in terms of domain

180 hod is to investigate macroscopic disordered ferromagnets, whose dynamics are dominated by domain wal

181 system comes from the fact that it is a hard ferromagnet with a large coercive field (Hc > 1.0 T) and

182 olayer chromium triiodide (CrI3) is an Ising ferromagnet with out-of-plane spin orientation.

183 CoSe and CoS are found to be weak itinerant ferromagnets with Curie temperatures close to 10 K.

184 romagnets can improve the functionalities of ferromagnets with higher response times, and having the

185 om temperature in ultrathin transition metal ferromagnets with magnetic transmission soft X-ray micro

186 le to existing classes of highly anisotropic ferromagnets with ordering at room temperature or above.

187 The switching of ferromagnets with perpendicular magnetization is of part

188 work demonstrates that in spin-orbit-coupled ferromagnets with weak extrinsic domain wall pinning, th

189 r spin-orbit torque in spintronic devices of ferromagnets without inversion symmetry.

190 iscovered several decades ago, the itinerant ferromagnets ZrZn2 and Sc3In, the understanding of their