ライフサイエンスコーパス: magnetic anisotropy

1 ich correlates with the stress dependence of magnetic anisotropy.

2 in inversion, achieved through a large axial magnetic anisotropy.

3 reases with increasing ground-state spin and magnetic anisotropy.

4 d antiferromagnetic films with perpendicular magnetic anisotropy.

5 e magnetic exchange coupling and introducing magnetic anisotropy.

6 n configurations are defined by altering the magnetic anisotropy.

7 oxide tunes the disorder, exchange field and magnetic anisotropy.

8 thermal fluctuations can be counteracted by magnetic anisotropy.

9 film due to thermal effects that modify its magnetic anisotropy.

10 ey information for the full understanding of magnetic anisotropy.

11 40B20/MgO/TiO2 structures with perpendicular magnetic anisotropy.

12 sistent with voltage-induced modification of magnetic anisotropy.

13 e the BaFe12O19 layer exhibits perpendicular magnetic anisotropy.

14 nduced Dzyaloshinskii-Moriya interaction and magnetic anisotropy.

15 diate layer showed an improved perpendicular magnetic anisotropy.

16 l increase and decrease of the perpendicular magnetic anisotropy.

17 eld of the azido ligand and its influence on magnetic anisotropy.

18 veal the presence of an interfacial uniaxial magnetic anisotropy.

19 oated ferromagnetic layer with perpendicular magnetic anisotropy.

20 uced surface charge doping that modifies the magnetic anisotropy.

21 at exchange coupling can strongly modify the magnetic anisotropy.

22 ombine large hyperfine NMR shifts with large magnetic anisotropies.

23 ss high-spin ground states, but insufficient magnetic anisotropies.

24 Magnetic anisotropy allows magnets to maintain their dir

25 We report an observation of uniaxial magnetic anisotropy along the [100] crystallographic dir

26 The magnetic anisotropies and orientation of the magnetic ax

27 tunnel barrier, where a large perpendicular magnetic anisotropy and a sizable tunnelling magnetoresi

28 ps of R provide an experimental probe of the magnetic anisotropy and aromaticity of the C18 ring thro

29 Large magnetic anisotropy and coercivity are key properties of

30 athway can be used to in situ manipulate the magnetic anisotropy and enable non-volatile FMR tuning i

31 Magnetic anisotropy and highly anisotropic electrical tr

32 t film, leading to nonvolatile modulation of magnetic anisotropy and magnetization reversal character

33 This allows the magnetic anisotropy and microwave resonant frequency to

34 , that a 90 degrees in-plane rotation of the magnetic anisotropy and propagation of magnetic domains

35 ctions arising from the combination of large magnetic anisotropy and spin-delocalization from metal t

36 Here we show an extreme, uniaxial magnetic anisotropy and the emergence of magnetic hyster

37 ntil now, it has proved very hard to predict magnetic anisotropy, and as a consequence, most syntheti

38 Comparison of iron spin relaxivity, magnetic anisotropy, and magnetic susceptibilities argue

39 roton chemical shifts, deltaOrn delta-proton magnetic anisotropy, and NOE cross-peaks that establish

40 The effects of surface and bulk magnetic anisotropies are corroborated with those of the

41 hich have proven their capability to predict magnetic anisotropy, are described.

42 lane compressive strain and shows a stronger magnetic anisotropy as well as cation site-exchange.

43 Experimental and theoretical magnetic anisotropy axes perfectly match and lie along t

44 The magnetic anisotropy axis of 14 low-symmetry monometallic

45 been synthesized to probe the origin of the magnetic anisotropy barrier in the one-dimensional coord

46 n the basis of these shapes, the size of the magnetic anisotropy barrier in the polyradical, originat

47 Reaction of the high-magnetic anisotropy building unit [ReCl(4)(CN)(2)](2-) w

48 Sr(5)Co(4)O(12) exhibits strong magnetic anisotropy but no long-range magnetic order.

49 Lanthanide SMMs exhibit large magnetic anisotropies, but building high-spin ground sta

50 Molecules that exhibit a high degree of magnetic anisotropy can behave as individual nanomagnets

51 strain-induced changes in the perpendicular magnetic anisotropy can modify the coercive field and do

52 The magnetic anisotropy change as response to the gating vol

53 n resonances is largely accounted for by the magnetic anisotropy changes.

54 ultrathin magnetic films with perpendicular magnetic anisotropy combined with ferroelectric substrat

55 in para-tolanes, whereas in ortho-analogues magnetic anisotropy complicates the analysis making (13)

56 phase transitions into a state with striking magnetic anisotropy, consistent with the breaking of the

57 (2) ground state with significantly enhanced magnetic anisotropy (D = -0.33 cm(-1) and E = -0.018 cm(

58 zation measurements reveal a strong uniaxial magnetic anisotropy (D = -39.6 cm(-1)) acting on the S =

59 the quantitative determination of the axial magnetic anisotropy, Deltachi(ax) = -2.50 x 10(-8) m(3)/

60 these stable states minimizes the sum of the magnetic anisotropy, demagnetization, Dzyaloshinskii-Mor

61 pectroscopy, showing easy-axis or easy-plane magnetic anisotropy depending on the choice of Ln ion.

62 is change is easily detected in the observed magnetic anisotropy despite thermal population of more t

63 s has been made in the electrical control of magnetic anisotropy, domain structure, spin polarization

64 According to solvent-induced isotope and magnetic anisotropy effects, the two duplex conformers a

65 A model including a strong magnetic anisotropy, elastic, Zeeman, Heisenberg exchang

66 The clusters are marked by low magnetic anisotropy energy (MAE) of 2.72 meV and a large

67 ayer, which we use to toggle the interfacial magnetic anisotropy energy by >0.75 erg cm(-2) at just 2

68 nterfaces are analyzed through resolving the magnetic anisotropy energy by layer and orbital.

69 es which are the primary contributors to the magnetic anisotropy energy in the low temperature struct

70 t existing methods rely on locally modifying magnetic anisotropy energy or saturation magnetization,

71 Thus far, the magnetic anisotropy energy per atom in single-molecule m

72 However, with decreasing particle size the magnetic anisotropy energy per particle responsible for

73 opy (VCMA) efficiency (change of interfacial magnetic anisotropy energy per unit electric field) lead

74 d by the exchange field resulting in a large magnetic anisotropy energy via the Dzyaloshinskii-Moriya

75 Herein, we show that pairing the axial magnetic anisotropy enforced by tetramethylcyclopentadie

76 e slower relaxation derives from the greater magnetic anisotropy enforced within the strongly donatin

77 ible functionalization that will boost their magnetic anisotropy even further.

78 The ferroelectric switching of magnetic anisotropy exhibits extensive applications in e

79 otropy field (H K) and surface perpendicular magnetic anisotropy field (H KS) in the same Pt/YIG syst

80 An extrapolated, magnetic anisotropy field of 220 T and a coercivity fiel

81 ilms on amorphous substrates, with very high magnetic anisotropy fields exceeding 7 T, making them te

82 We realized the maximum magnetic anisotropy for a 3d transition metal atom by co

83 t spin-torque oscillators with perpendicular magnetic anisotropy free layers.

84 the metal centers appears to increase axial magnetic anisotropy, giving rise to larger magnetic rela

85 h weak Dzyaloshinskii-Moriya interaction and magnetic anisotropy gradient.

86 Bleaney's long-standing theory of magnetic anisotropy has been employed with some success

87 control of ferromagnetism, magnetization and magnetic anisotropy has been explored in various magneti

88 Magnetic thin films with perpendicular magnetic anisotropy have localized excitations that corr

89 vs. low frequency conditions with respect to magnetic anisotropy, (ii) EPR spectra of non-integer (Kr

90 1), respectively, a consequence of the large magnetic anisotropies imparted by these ions.

91 elected because its characteristically large magnetic anisotropy imparts significant dipolar shifts w

92 gnetic resonance spectroscopy to measure the magnetic anisotropies in different strains of Magnetospr

93 he latter of which were used to quantify the magnetic anisotropy in both the ferric high-spin aquo an

94 ling macroscopic properties such as expected magnetic anisotropy in elongated shaped macromolecules c

95 rough interfacial strain-induced rotation of magnetic anisotropy in magnetostrictive/piezoelectric mu

96 which has been widely employed to manipulate magnetic anisotropy in spintronic devices and artificial

97 n oriented single crystals, and a very large magnetic anisotropy in the magnetic susceptibility was o

98 or magnetic fields to visualize directly the magnetic anisotropy in the uniaxial ferromagnet CeRu2Ga2

99 Magnetic anisotropy is also affected by the electric fie

100 The magnetic anisotropy is axial and oriented by the axial F

101 Designing systems with large magnetic anisotropy is critical to realize nanoscopic ma

102 The massive magnetic anisotropy is due to bis-trans-disposed tert-bu

103 Furthermore, we show that the magnetic anisotropy is equally well predicted in a selec

104 garnet (YIG) system and its association with magnetic anisotropy is essential towards optimization of

105 Magnetic anisotropy is the property that confers to the

106 The perpendicular magnetic anisotropy K(eff), magnetization reversal, and

107 opatterns by crafting, at the nanoscale, the magnetic anisotropy landscape of a ferromagnetic layer e

108 Magnetic anisotropy (MA) is one of the most important ma

109 etic-dipole-induced aggregation, while their magnetic anisotropy makes them responsive to an external

110 cal quantity depends on the magnitude of the magnetic anisotropy of a complex and the size of its spi

111 tic skyrmion by modulating the perpendicular magnetic anisotropy of a nanomagnet with an electric fie

112 el systems with which to harness the maximum magnetic anisotropy of Dy(III) ions.

113 ctrostatic method, capable of predicting the magnetic anisotropy of dysprosium(III) complexes, even i

114 te disorder as well as variations of the net magnetic anisotropy of FM nuclei.

115 La0.08Zr0.52Ti0.48O3 (PLZT) films, where the magnetic anisotropy of NiFe can be electrically modified

116 The results show how synergizing the strong magnetic anisotropy of terbium(III) with the effective e

117 le for the strong positive axial and rhombic magnetic anisotropy of the high-spin Co(II) ion (D = +98

118 This changes the magnetic anisotropy of the Yb(III) ground state from eas

119 d pulse can be used to 'set' and 'reset' the magnetic anisotropy orientation and resistive state in t

120 scillator, with the energy of the easy-plane magnetic anisotropy playing the role of the Josephson en

121 rove its thermal stability and perpendicular magnetic anisotropy (PMA).

122 io as well as a large value of perpendicular magnetic anisotropy (PMA).

123 cularity on an underlayer with perpendicular magnetic anisotropy (PMA).

124 tion between the exchange interaction and 4f magnetic anisotropy present in the system.

125 Magnetic anisotropy removes this restriction, however, a

126 netic domain configuration due to an induced magnetic anisotropy resulting from the inverse magnetost

127 Significant magnetic anisotropy results from this orbital degeneracy

128 relaxation and a preliminary estimate of the magnetic anisotropy, reveal a chi that is axially anisot

129 conversion by correcting for the effects of magnetic anisotropy reveals a very substantial change in

130 ly, demonstrating that the strength of axial magnetic anisotropy scales with increasing ligand field

131 In materials with the gradient of magnetic anisotropy, spin-orbit-torque-induced magnetiza

132 The magnetic anisotropy symmetry reversibly switches from a

133 endipitous processes in the search for large magnetic anisotropy systems.

134 lbert-Slonczewski equation in the absence of magnetic anisotropy terms is described by a Mobius trans

135 quantum limit, signalling a reversal of the magnetic anisotropy that can be directly attributed to t

136 ion due to lithographic patterning induces a magnetic anisotropy that competes with the magnetocrysta

137 rder to optimize this system with respect to magnetic anisotropy, the triplesalophen ligand system ha

138 e guests report their positions by imparting magnetic anisotropy to the capsule components.

139 s, the room temperature TC, and the in-plane magnetic anisotropy together in a single layer VX2, this

140 A reversible change of magnetic anisotropy up to 219 Oe is achieved with a low

141 d, non-volatile manipulation of out-of-plane magnetic anisotropy up to 40 Oe is demonstrated and conf

142 utorial is dedicated to the investigation of magnetic anisotropy using both electron paramagnetic res

143 all motion in materials with the gradient of magnetic anisotropy using the CCM remains lack of invest

144 The voltage-controlled magnetic anisotropy (VCMA) effect, which manifests itsel

145 MeRAM devices is the low voltage-controlled magnetic anisotropy (VCMA) efficiency (change of interfa

146 uctures which exhibit low voltage-controlled magnetic anisotropy (VCMA) efficiency.

147 titative determination of voltage-controlled magnetic anisotropy (VCMA) in Au/[DEME](+) [TFSI](-) /Co

148 The molecule's spin states and magnetic anisotropy were manipulated in the absence of a

149 nel junctions with interfacial perpendicular magnetic anisotropy, where the coercivity, the magnetic

150 dentify a novel magnetic phase with enhanced magnetic anisotropy which is a candidate for rare-earth

151 ntiferromagnetic spin correlations and local magnetic anisotropy, which allows it to be indirectly ob

152 gnetic frustration has a clear in-plane (ab) magnetic anisotropy, which is maintained up to temperatu

153 a single crystal of 1 shows a giant uniaxial magnetic anisotropy with an experimental D(expt) value (

154 Significant magnetic anisotropy with the easy axis along the [101] d

155 evices in which piezoelectrically controlled magnetic anisotropy yields up to 500% mobility variation