ライフサイエンスコーパス: antiferromagnetism

1 te connection between its insulating gap and antiferromagnetism.

2 ntaneous spin Hall effect and momentum space antiferromagnetism.

3 endent evidence for a local moment origin of antiferromagnetism.

4 (2) octahedra and exhibits characteristic 2D antiferromagnetism.

5 structure that we associate with metastable antiferromagnetism.

6 to rivers of charge that separate regions of antiferromagnetism.

7 ere the lattice symmetry is preserved by the antiferromagnetism.

8 o induce switching between paramagnetism and antiferromagnetism.

9 lay of multiple degenerate nodal physics and antiferromagnetism.

10 mation for the microscopic origin of layered antiferromagnetism(14-18).

11 tertwined with other forms of order, such as antiferromagnetism(5-7) or charge-density-wave order(8),

12 ent metallic state that preserves long-range antiferromagnetism, a phase that cannot be reached by si

13 ndeed, it is the suppression of commensurate antiferromagnetism (AF) that usually allows this type of

14 d a work function of 5.08 eV, harboring both antiferromagnetism (AFM) and strong red photoluminescenc

15 tivity in a narrow region near the border to antiferromagnetism (AFM) as a function of pressure or do

16 on-Fermi liquid (NFL) behavior and collinear antiferromagnetism (AFM) in V(1/3)NbS(2).

17 mpeting types of electronic order, including antiferromagnetism and charge density waves.

18 t and a broad low-doped region of coexisting antiferromagnetism and d-wave pairing with a triplet p c

19 avevector [Formula: see text] induced by the antiferromagnetism and d-wave pairing.

20 rom an SO(5) symmetry principle that unifies antiferromagnetism and d-wave superconductivity.

21 e tetragonal forms exhibit only an incipient antiferromagnetism and experimentally show superconducti

22 n internal, magnetoelectric coupling between antiferromagnetism and ferroelectricity in the BiFeO(3)

23 to-optical microscopy measurements by canted antiferromagnetism and find a number of Weyl points.

24 The competition between antiferromagnetism and hole motion in two-dimensional Mo

25 erroelectricity, piezoelectricity, ferro and antiferromagnetism and so on that have the potential for

26 Our results establish the combination of antiferromagnetism and superconductivity as a novel rout

27 distinct possibility that genuine long-range antiferromagnetism and superconductivity do not coexist.

28 ritical line separates a phase of coexisting antiferromagnetism and superconductivity from a purely u

29 ced, possibly due to a microscopic mixing of antiferromagnetism and superconductivity, suggesting tha

30 h to the study of CO and its relationship to antiferromagnetism and superconductivity.

31 ides that have been doped to the boundary of antiferromagnetism and superconductivity.

32 ground states, including superconductivity, antiferromagnetism, and heavy-fermion behaviour.

33 ng (the cluster glassy state) and the canted antiferromagnetism, and then the direct interaction amon

34 ssive) strain, including unusual interfacial antiferromagnetism arising d-orbital occupations, and bo

35 We show that incommensurate orbital antiferromagnetism, associated with circulating currents

36 at exhibits both ferroelectricity and canted antiferromagnetism at room temperature, making it a uniq

37 )CoIn(5) in magnetic fields near the edge of antiferromagnetism at the critical doping x(c) ~ 0.03.

38 spin states and coupling schemes (ferro- vs. antiferromagnetism) based on DFT calculations, Mossbauer

39 ts reveal that this material exhibits canted antiferromagnetism below 15.5 K.

40 Magnetic measurements reveal easy-axis antiferromagnetism below 168 K.

41 energy gap in the visible spectrum, and weak antiferromagnetism between the planes, suggesting possib

42 Recent results, however, indicate that antiferromagnetism can appear in the superconducting sta

43 Antiferromagnetism, characterized by alternating magneti

44 n scattering to show that ferromagnetism and antiferromagnetism coexist in the low T state of the pyr

45 If 2D antiferromagnetism could be converted to 2D ferromagneti

46 In contrast to antiferromagnetism, demonstration of ferromagnetic coupl

47 that demonstrates a subtle form of itinerant antiferromagnetism formally equivalent to the Bardeen-Co

48 by the application of a magnetic field, and antiferromagnetism has been observed in hole-doped mater

49 Antiferromagnetism has been theoretically predicted to b

50 universal low-energy theory for the onset of antiferromagnetism in a metal can be realized in lattice

51 report the electrical detection of colinear antiferromagnetism in all-epitaxial RuO(2)/MgO/RuO(2) tu

52 especially focusing on ferroelectricity and antiferromagnetism in chemically modified BiFeO(3), a co

53 in- and charge-density waves associated with antiferromagnetism in elemental chromium.

54 The quantum theory of antiferromagnetism in metals is necessary for our unders

55 Emerging antiferromagnetism in the anisotropic structure is studi

56 Establishing the relation between ubiquitous antiferromagnetism in the parent compounds of unconventi

57 ken C 4 symmetry, while suppressing the Neel antiferromagnetism in the SrVO3 layers.

58 Conventional antiferromagnetism in these compounds is dominated by fe

59 lar, atomically thin CrI(3) exhibits layered antiferromagnetism, in which adjacent ferromagnetic mono

60 scattering shows that short-range correlated antiferromagnetism is also present.

61 Antiferromagnetism is established as the competing order

62 gh-field spin wave measurements confirm that antiferromagnetism is metastable within the otherwise fe

63 Layered antiferromagnetism is the spatial arrangement of ferroma

64 quantum entanglement-not the destruction of antiferromagnetism-is the common driver of the varied be

65 To assess the role of antiferromagnetism, it is essential to understand the do

66 Formula: see text] (hole-doped) region shows antiferromagnetism limited to very low doping, stripes m

67 of the vortex and it has been suggested that antiferromagnetism might develop there.

68 pends on vortex dynamics, and the underlying antiferromagnetism of the cuprates.

69 e charge carriers enter the CuO2 layers, the antiferromagnetism of the parent insulators, where each

70 te relaxation of the inherent frustration of antiferromagnetism on a hexagonal close-packed lattice.

71 The breakdown of itinerant antiferromagnetism only comes clearly into view in the c

72 her symmetry-breaking ground states, such as antiferromagnetism or charge-density-wave (CDW) order.

73 sually high-temperature magnetic order, with antiferromagnetism persisting to at least 500 K, and ref

74 hain magnet behavior hidden below the canted antiferromagnetism (T(N) = 5.8 K) already evidenced by d

75 ns evolve from participation in large moment antiferromagnetism to superconductivity in these systems

76 Far from the usual destruction of antiferromagnetism via spin polarization, the high-field

77 For c/a > 0.99, hidden antiferromagnetism was revealed and the magnetisation ve

78 scenario of Fermi surface reconstruction by antiferromagnetism, where an anti-correlation is commonl

79 A symptom of this localization is antiferromagnetism, where the spins of localized electro

80 ive long-range exchange coupling mediated by antiferromagnetism, which significantly enhances the mag

81 ntly limited understanding of weak itinerant antiferromagnetism, while providing insights into the ef

82 ng of ferroelectricity, ferroelasticity, and antiferromagnetism with controllable spin directions via

83 m becomes superconducting in the presence of antiferromagnetism, with the weight continuously shiftin

84 surements reveal a continuous evolution from antiferromagnetism (x = 0) to a spin-glass state (0 < x