ライフサイエンスコーパス: antiferromagnetism

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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 to rivers of charge that separate regions of antiferromagnetism.

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

23 Antiferromagnetism has been theoretically predicted to b

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

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

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

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

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

29 Antiferromagnetism is established as the competing order

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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