ライフサイエンスコーパス: magnetic domain

1 nested FS portions, which vary for different magnetic domains.

2 f spins from the interior of the neighboring magnetic domains.

3 d magnons by antiphase boundaries coupled to magnetic domains.

4 ntum correlated, yet spatially disconnected, magnetic domains.

5 de AFM combined with selective modulation of magnetic domains.

6 olution of this technique enables imaging of magnetic domains and allows to locate the sites of defec

7 face but also lay the groundwork for imaging magnetic domains and domain boundaries at the magnetic T

8 rol, we achieve non-volatile manipulation of magnetic domains and domain walls in AF CrSBr bilayers,

9 gnetometry, we directly visualized nanoscale magnetic domains and periodic patterns, a signature of m

10 port spin defect-based wide-field imaging of magnetic domains and spin fluctuations in twisted double

11 essential to explore the rich properties of magnetic domains and spin textures.

12 robe to unambiguously prove the existence of magnetic domains and study their dynamics in atomically

13 The role of magnetic domains (and the walls between domains) in dete

14 magnetoplasmon at the interface of opposite magnetic domains, and demonstrate the existence of zero-

15 Magnetic domains, and the boundaries that separate them

16 The garnet film had maze-shaped magnetic domains, and the domain walls disappeared when

17 The magnetite crystals were all single magnetic domains, and the magnetization directions of sm

18 ization promoted OER already occurs on these magnetic domains, and thus the enhancement should have b

19 microscopy (AFM) is demonstrated for mapping magnetic domains at size regimes below 100 nm.

20 periments thus indicate that the presence of magnetic domains at the transition starkly increases dis

21 ission microscopy technique, we imaged small magnetic domains at very low fields in these multilayers

22 A magnetic domain boundary on the surface of a three-dimen

23 re and detected a chiral edge current at the magnetic domain boundary.

24 Manipulation of the magnetic domains by E field is directly visualized at ro

25 g-energy magnonic devices and circuits where magnetic domains can be efficiently reconfigured by magn

26 that, apart from trivial 180(o) commensurate magnetic domains, can be described by ferromagnetic and

27 ge region has a significant influence on the magnetic domain configuration due to an induced magnetic

28 recorded and numerically inverted to map its magnetic domain configuration.

29 at serves as a 'fingerprint' of a particular magnetic domain configuration.

30 netotactic bacterium that synthesises single-magnetic domain crystals which are incorporated into mag

31 Particularly, the Ouchden fault delineates a magnetic domain divide between the ancient High Atlas an

32 imensional ferromagnetism with a complicated magnetic domain dynamic.

33 -probe-type experiments can even investigate magnetic domain dynamics.

34 tting the magnetization vector of individual magnetic domains either 'up' or 'down'.

35 across antiphase boundaries support multiple magnetic domains even in particles as small as 12-14 nm.

36 By controlling the magnetic domain evolution as a function of magnetic fiel

37 ctuations induce the formation of metastable magnetic domains evolving into a single macroscopic magn

38 Understanding how magnetic domains form in the presence of disorder and th

39 Here we demonstrate laser-induced magnetic domain formation and all-optical switching in t

40 Magnetic domain formation is observed through both in si

41 cur within the finite-size regime, where the magnetic domain growth is limited due to physical defect

42 position, we demonstrate that the pinning of magnetic domains, imaged by nanoscale magnetic induction

43 s to a wide range of research areas, such as magnetic domains imaging and element specific investigat

44 Under illumination, the magnetic domains in [Co/Pd] produce a speckle pattern, a

45 observations of how tensile strain modifies magnetic domains in a ferromagnetic Ni thin plate using

46 Magnetic domains in adjacent cobalt layers can be manipu

47 Recent observations of switching of magnetic domains in ferromagnetic metals by circularly p

48 -scale ferrimagnetic structure and nanoscale magnetic domains in Ho(Co,Fe)(3) was revealed via in sit

49 momentum-conserving tunneling of ICPs across magnetic domains in the barrier.

50 c boundary, or domain wall, between opposing magnetic domains in the magnetization reversal process.

51 n permeability are observed by switching the magnetic domains in the wire and measuring the modificat

52 The confusion is that each magnetic domain is a small magnet and theoretically the

53 The magnitude and frequency of abrupt magnetic domain jumps observed in the stripe phase are d

54 Magnetic domain memory (MDM), that is, the tendency for

55 vity across vdW layers may be used to obtain magnetic domain memory behaviour, even after exposure to

56 ical lattice, and with a correlation length (magnetic domain) of 6.7(4) A.

57 x (x = 0, 1, 2, 3) microwires, including the magnetic domain period (d) and surface roughness (Rq) as

58 Magnetic domains play a fundamental role in physics of m

59 Vectorial imaging of magnetic domains reveals an unusually gradual thickness-

60 ay microscopy, with electric-field dependent magnetic domain reversal showing that the energy barrier

61 udy has found that topologically non-trivial magnetic domains separated by a complex network of domai

62 devices, compounds that allow a tailoring of magnetic domain shapes and sizes are essential.

63 The thickness-dependent magnetic domain size follows Kittel's law.

64 s, and their interference to capture the two magnetic domain states.

65 The surface magnetic domain structure (SMDS) parameters of 45 mum di

66 Magnetic domain structure and spin-dependent reflectivit

67 of finite size and strain relaxation on the magnetic domain structure is also discussed.

68 s in SrTiO3 leads to dramatic changes of the magnetic domain structure of a neighboring magnetic laye

69 Magnetization leads to the evolution of the magnetic domain structure, from a multi-domain one to a

70 of a ferromagnetic material only changes its magnetic domain structure.

71 el-type skyrmion lattice and the stripe-like magnetic domain structures as well.

72 A lack of comprehensive understanding of magnetic domain structures carrying remanence has, until

73 rate the visualization and reconstruction of magnetic domain structures in a 3D curved magnetic thin

74 tational advances allow detailed analysis of magnetic domain structures in iron particles as a functi

75 red, in addition to the observation of clear magnetic domain structures in these films.

76 it torque gives rise to instabilities of the magnetic domain structures that are reminiscent of Rayle

77 n be used to control others by reconfiguring magnetic domain structures.

78 be used to electrically pattern non-volatile magnetic-domain structures hosting chiral edge states, w

79 and the field-free altermagnetic SST-driven magnetic domain switching of the recording layer is dire

80 ens the door to future applications based on magnetic domain tailoring.

81 in wall motion and the dynamics of a uniform magnetic domain that is attributed to variations in the

82 idges the nanowire and minimizes complicated magnetic domains that otherwise compromise the magnetic

83 ses differentiated the study area into three magnetic domains: the eastern Ouzellarh block, character

84 main memory (MDM), that is, the tendency for magnetic domains to repeat the same pattern during field

85 nucleated vortex states into larger complex magnetic domains, until it is in a fully-FM state.

86 metric GdRu(2)Si(2) by selectively measuring magnetic domains using angle-resolved photoemission spec

87 s and open exciting opportunities to control magnetic domains via topological quasiparticles.

88 The interaction between a magnetic domain wall and a pinning site is explored in a

89 eport observations of the motion of a single magnetic domain wall at the scale of the individual peak

90 pagating chiral interface channels along the magnetic domain wall at zero magnetic field.

91 functionalities in chip-based devices using magnetic domain wall conduits.

92 surfactant films, and of metal surfaces, and magnetic domain wall fluctuations in antiferromagnets.

93 that encode information in the position of a magnetic domain wall in a ferromagnetic wire.

94 This prototype demonstration shows that magnetic domain wall logic devices have the necessary ch

95 ith LIFT characteristics by manipulating the magnetic domain wall motion in a synthetic antiferromagn

96 on behaviours microscopically originate from magnetic domain wall motion, which can be precisely depi

97 We present quantitative measurements of magnetic domain wall structure and its transformations a

98 dies have revealed that the disappearance of magnetic domain wall upon magnetization is responsible f

99 re for passively resetting the position of a magnetic domain wall.

100 teristics such as device switching times and magnetic domain-wall velocities depend critically on the

101 y effect has considered ideal junctions with magnetic domain walls (DW) at the interfaces, in practic

102 The current-induced motion of magnetic domain walls (DWs) confined to nanostructures i

103 complex chiral spin textures such as chiral magnetic domain walls (DWs), spin spirals, and magnetic

104 rise to spin transfer torques that can drive magnetic domain walls along nanowires.

105 Magnetic domain walls are boundaries between regions wit

106 Although two types of magnetic domain walls are known to exist in magnetic thi

107 Chiral magnetic domain walls are of great interest because lift

108 Magnetic domain walls are often referred to as solitons

109 Magnetic domain walls are topological solitons whose int

110 ale neuromorphic devices in which individual magnetic domain walls are used to perform complex data a

111 used to tailor the texture and handedness of magnetic domain walls by interface engineering.

112 , in turn, be used to change the position of magnetic domain walls by means of the spin-transfer torq

113 perimentally demonstrate that nanometer-wide magnetic domain walls can be applied to manipulate the p

114 gnet-superconductor (F/S) hybrid structures, magnetic domain walls can be used to spatially confine t

115 Here we show that magnetic domain walls can modulate spin-wave transport i

116 The current-induced motion of magnetic domain walls confined to nanostructures is of i

117 y of left- and right-handed spin textures in magnetic domain walls enables fast current-driven domain

118 pating spin polarized currents to manipulate magnetic domain walls has limited the development of suc

119 tion storage and logical processing based on magnetic domain walls have great potential for implement

120 we report the discovery of highly conductive magnetic domain walls in a magnetic insulator, Nd2Ir2O7,

121 step towards the practical implementation of magnetic domain walls in energy efficient computing.

122 y of which rely on efficient manipulation of magnetic domain walls in ferromagnetic nanowires.

123 Magnetic domain walls in magnetic tracks produce strong

124 Head-to-head and tail-to-tail magnetic domain walls in nanowires behave as free magnet

125 and and control the edge states predicted at magnetic domain walls in quantum anomalous Hall insulato

126 esult from large fringing fields surrounding magnetic domain walls in the magnetically soft layer.

127 The microscopic magnetization variation in magnetic domain walls in thin films is a crucial propert

128 The motion of magnetic domain walls induced by spin-polarized current

129 Current-driven motion of magnetic domain walls is one of the key technologies for

130 The rich internal degrees of freedom of magnetic domain walls make them an attractive complement

131 is mutual interaction between spin waves and magnetic domain walls opens up the possibility of realiz

132 ation of strain-induced periodic 180 degrees magnetic domain walls perpendicular to the strain axis.

133 But the roughness and mobility of the magnetic domain walls prevents closer packing of the mag

134 Magnetic domain walls show considerable potential as mag

135 The possibility of controlling magnetic domain walls using voltages offers an energy ef

136 isorder such as vortices in superconductors, magnetic domain walls, and charge density wave materials

137 Magnetic domain walls, in which the magnetization direct

138 Magnetic domain walls, which separate regions of opposin

139 s (less than 0.01%) can be used to propagate magnetic domain walls.

140 , which are locked to both ferroelectric and magnetic domain walls.

141 be a crossover from pinning to depinning of magnetic domain walls.

142 ging the magnetic field and the evolution of magnetic domains, we observe the macroscopic magnetic tr

143 EPR measurements show the presence of magnetic domains well above Tc , as expected for a ferro

144 f the magnetic anisotropy and propagation of magnetic domains with low applied electric fields under

145 of magnetism in GdRu(2)Si(2) by manipulating magnetic domains with magnetic field and temperature cyc

146 Non-uniform magnetic domains with non-trivial topology, such as vort

147 We are able to image magnetic domains with widths of 25 nm, and demonstrate a