ライフサイエンスコーパス: canted

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

23 3 manifest a distortion in which one smif is canted in the plane perpendicular to the other.

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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