ライフサイエンスコーパス: canted

1 ization, suggesting it still keeps the small canted AFM state.

2 ith Chern number C = 1 appears as the AFM to canted-AFM phase transition happens.

3 hortcoming two sensors were assembled with a canted angle similar to that employed in radar bearing l

4 age (+/-60 degrees ) based on the 30 degrees canted angle used.

5 c interactions led to magnetic ordering as a canted antiferromagnet (T(N) = 3.8 K) with a small spont

6 The unsolvated material 3a orders as a spin-canted antiferromagnet at 8 K, with a canting angle phi

7 This material is a spin canted antiferromagnet below 15.9 K with a weak ferromag

8 ization data, and a magnetic transition to a canted antiferromagnet state was found at 24.1 K.

9 pi-stacks, and the material orders as a spin-canted antiferromagnet with T(N) = 35 K, with a spontane

10 ) magnetically orders as a weak ferromagnet (canted antiferromagnet) below 21.0 +/- 0.1 K, as observe

11 rough three ordered phases: antiferromagnet, canted antiferromagnet, and ferromagnet.

12 y induced magnetic state resembles that of a canted antiferromagnet, opening an avenue toward creatin

13 thoferrite, YFeO(3), a perovskite-structured canted antiferromagnet.

14 This results in a canted antiferromagnetic arrangement in which the domina

15 Here we demonstrate experimentally that canted antiferromagnetic BaMnSb2 is a 3D Weyl semimetal

16 ographic axis giving a quasi-one-dimensional canted antiferromagnetic character, as shown by magnetic

17 ffraction near the Dy L(3) edge, we unveil a canted antiferromagnetic ground state arising from a qua

18 al phase is significantly enhanced above the canted antiferromagnetic moment in the bulk phase, as a

19 y functional theory calculations reveals the canted antiferromagnetic nature with significant spin fl

20 omagnetic order for 304 K < T < 565 K, but a canted antiferromagnetic order with a ferromagnetic comp

21 magnetic structure of ferromagnetic and spin-canted antiferromagnetic ordered materials as well as an

22 A weak ferromagnetic transition with canted antiferromagnetic spins along the a-axis is found

23 It exhibits a canted antiferromagnetic state below 35 kelvin, with mag

24 In the resulting canted antiferromagnetic state, we observe transport sig

25 the Mn(2+) centres in MnSrTa(2)O(7) adopt a canted antiferromagnetic state, with a small spontaneous

26 e, the magnetic state of Eu evolves from the canted antiferromagnetic structure in the ground state,

27 adratic) manner in the antiferroquadrupolar (canted antiferromagnetic) phase, which are attributed to

28 minority spin states of ferromagnetic, spin-canted antiferromagnetic, and fully antiferromagnetic bi

29 i(2)Te(4) is a rare platform for realizing a canted-antiferromagnetic (cAFM) Chern insulator with ele

30 ing below 50 K, Sr(3)Co(2)O(4)Cl(2) adopts a canted antiferromagnetically ordered state.

31 ingle-chain magnet behavior hidden below the canted antiferromagnetism (T(N) = 5.8 K) already evidenc

32 d magneto-optical microscopy measurements by canted antiferromagnetism and find a number of Weyl poin

33 rial that exhibits both ferroelectricity and canted antiferromagnetism at room temperature, making it

34 surements reveal that this material exhibits canted antiferromagnetism below 15.5 K.

35 ordering (the cluster glassy state) and the canted antiferromagnetism, and then the direct interacti

36 The canted antiferromagnets combine antiferromagnetic order

37 (that is, all of the effects present in the canted antiferromagnets(11,12)).

38 in which Delta-Rh intercalates in one of two canted binding conformations.

39 rically with each other and together adopt a canted conformation relative to the catalytic domains.

40 Hence, the canted directionality of the squaramide (NH)2 motif, fav

41 Here we show that a canted ferromagnetic phase which is preceded by local po

42 Commensurate antiferromagnetic layers and a canted ferromagnetic structure dominate the Si-rich part

43 plex spin-orbit torque switching observed in canted Gd(x)Co(100-x) not only provides a platform for s

44 3 manifest a distortion in which one smif is canted in the plane perpendicular to the other.

45 logical spin glass and (2) a frustrated spin-canted magnet with low-temperature exchange bias.

46 tahedral tilting, with local distortions and canted magnetic Ce(3+) order evidencing two-dimensional

47 predicted that the in-plane component of the canted magnetic moment at the CoFe/BiFeO3 interface can

48 etic anisotropy, Neel vector orientation and canted magnetism via electron injection and local distor

49 Pseudodipolar interactions lead to a net canted moment along the c-axis, while the sublattice mag

50 ield through a ~180 degrees switching of the canted moment in BiFeO3.

51 f the magnetization in the CoFe layer to the canted moment in the BiFeO3 layer.

52 deterministic reversal of the DM vector and canted moment using an electric field at room temperatur

53 magnet with T(N) = 35 K, with a spontaneous (canted) moment M(spont) = 1.4 x 10(-3) muB and a coerciv

54 two MOFs, NipymcaCl and NipymcaBr, featuring canted Ni(2+)-based moments.

55 etic correlations, a precursor to long-range canted order.

56 A peculiar canted ordering of the organic A-cation dipole moments g

57 grown on the topological insulator Bi2Te3 is canted out of the high-symmetry directions of the surfac

58 colloidal silica superballs crystallize into canted phases in the presence of depletants.

59 ounterparts, the oxidized cluster has a spin-canted, S = (1)/(2) ground state, and the reduced cluste

60 rings of PIN-acac complexes 18a and 18b were canted significantly from planarity and projected the im

61 cited in a broad class of iron oxides with a canted spin configuration.

62 omena, we demonstrate a new functionality of canted spin order for magnonics and show that it facilit

63 tivity straddles a transition between a spin-canted state with a finite in-plane magnetic moment and

64 o-solid phase transitions between square and canted structures.

65 d zero-dimensional molecule to ordered, spin-canted, three-dimensional lattice being the result of th

66 On further cooling, the compounds become canted weak ferromagnets below 40 K.

67 e vaginal lumen and penis tip were both left-canted with similar angular bends that mirrored one anot