ライフサイエンスコーパス: magnetic material

1 ns, in particular as spin probes and organic magnetic materials.

2 structures, and introducing magnetism in non-magnetic materials.

3 er the system parameters than is possible in magnetic materials.

4 etization state of conducting and insulating magnetic materials.

5 ials, including polymers, semiconductors and magnetic materials.

6 near magnetostructural phase transitions in magnetic materials.

7 g and selective physical vapor deposition of magnetic materials.

8 ake it imperative to explore rare earth free magnetic materials.

9 radicals is important for the development of magnetic materials.

10 otential as novel, rare-earth free permanent magnetic materials.

11 etism allowed light to be used as a probe of magnetic materials.

12 ipulation of the magnetization in engineered magnetic materials.

13 is responsible for a variety of phenomena in magnetic materials.

14 a feasible new route in realizing functional magnetic materials.

15 atures and also a basis for novel functional magnetic materials.

16 een developed by combining ferroelectric and magnetic materials.

17 ey to this new generation of multifunctional magnetic materials.

18 thereby improving our understanding of real magnetic materials.

19 such as water ice, spin ice, and frustrated magnetic materials.

20 associated with external magnetic fields or magnetic materials.

21 the directed synthesis of semiconducting and magnetic materials.

22 organizing nanowires from semiconducting and magnetic materials.

23 transition metal--containing electronic and magnetic materials.

24 These devices are now smaller, with less magnetic material and improved electromagnetic interfere

25 ich is a record for a rare earth- or Pt-free magnetic material and retain values as high as 17.1 MGOe

26 coercivity are key properties of functional magnetic materials and are generally associated with rar

27 stals composed of metals, semiconductors, or magnetic materials and capped with various MCC ligands c

28 w opportunities in drug delivery, as well as magnetic materials and devices.

29 , making them ideal building blocks in novel magnetic materials and devices.

30 This is essential for the design of new bulk magnetic materials and for diminishing processes such as

31 -reversal symmetry, typically achieved using magnetic materials and more recently using the quantum H

32 ans of modulating the magnetic hystereses of magnetic materials and their heterostructures.

33 ce planarity but also the homogeneity of the magnetic materials, and our method is likely to find imm

34 nt magnetocaloric effects in a wide range of magnetic materials, and the parallel development of nano

35 Ferroelectric and magnetic materials are a time-honoured subject of study

36 Novel nanostructured Zr2 Co11 -based magnetic materials are fabricated in a single step proce

37 Nanostructured magnetic materials are important for many advanced appli

38 Frustrated magnetic materials are promising candidates for new stat

39 Magnetic materials are usually divided into two classes:

40 oxide, to prepare designed test platforms of magnetic materials at nanometer length scales.

41 alization of topological semimetal states in magnetic materials at room temperature, but also suggest

42 le very efficient electrical manipulation of magnetic materials at room temperature, for memory and l

43 to cobalt introduces potential new routes to magnetic materials based on strongly coupled, triangular

44 to create an effective magnetic field in the magnetic material being probed, which makes it possible

45 etic anisotropy has been explored in various magnetic materials, but the efficient electric-field con

46 lver chalcogenides, Ag2Se and Ag2Te, are non-magnetic materials, but their electrical resistance can

47 s been the method of choice to magnetize non-magnetic materials, but they are difficult to focus.

48 g-standing goal to create magnetism in a non-magnetic material by manipulating its structure at the n

49 ddition improves the performance of the hard-magnetic material by mitigating Brown's paradox in magne

50 iated tissue preparation, cells that contain magnetic material by their rotational behavior.

51 ular, geometrical frustration among spins in magnetic materials can lead to exotic low-temperature st

52 ructures that combine natural and artificial magnetic materials, can play a key role in terahertz dev

53 torage and separation, optical, electric and magnetic materials, chemical sensing, catalysis, and bio

54 e as building blocks for obtaining molecular magnetic materials exhibiting an additional and useful p

55 interest in the discovery and design of new magnetic materials exhibiting magnetoresistance.

56 esis of colloidal nanostructures combining a magnetic material (FePt) with a narrow-gap semiconductor

57 which in turn expands the base of available magnetic materials for devices with properties that cann

58 ticles (including metals, semiconductors and magnetic materials) form stable colloids in various molt

59 The intended use of a magnetic material, from information storage to power con

60 cond-order magnetic phase transition in soft magnetic material, gadolinium, was employed to obtain me

61 gh unconventional methods without the use of magnetic material has recently become a subject of great

62 Low-damping magnetic materials have been widely used in microwave an

63 Magnetic materials having competing, i.e., frustrated, i

64 ow that by embedding nanoparticles of a soft magnetic material in a thermoelectric matrix we achieve

65 ice is mimicked by Dy2Ti2O7, a site-ordered magnetic material in which the spins reside on a lattice

66 coupling self-assembly to the generation of magnetic materials in a simple, straight-forward manner

67 Nonreciprocal optical elements often require magnetic materials in order to break time-reversal symme

68 Simulating magnetic materials in the vicinity of a quantum phase tr

69 The only molecular-based magnetic materials in which this phenomenon has been obs

70 ration and is readily implementable to other magnetic materials independent of their size and shape a

71 nical exchange coupling between Fe and Ni in magnetic materials influences magnetic switching dynamic

72 One currently active area of research in magnetic materials involves compounds in which long-rang

73 Our finding shows that optical control of magnetic materials is a much more general phenomenon tha

74 ization of two members of a family of porous magnetic materials is described.

75 The existence of NRM in homogenous magnetic materials is still in debate, mainly due to the

76 conversion of charge-to-spin currents in non-magnetic materials, is of considerable debate.

77 fect, extraordinarily strong among other non-magnetic materials, is traced back to the specific Dirac

78 The magnetic material KCuF3 realizes an array of weakly coup

79 As the oldest known magnetic material, magnetite (Fe3O4) has fascinated mank

80 spin-dependent thermoelectric properties of magnetic materials, novel means of generating spin curre

81 Palladium doped iron rhodium is a magnetic material of significant interest for it's close

82 temperature for any metal boride and for any magnetic material of the vast 122 family of layered stru

83 Here, we show that a new magnetic material offers novel possibilities for guiding

84 angement of spins at interfaces in a layered magnetic material often has an important effect on the p

85 superconductors with strongly spin-polarized magnetic materials opens the possibility to discover new

86 Similarly, the interaction of X-rays with magnetic materials provides unique element-specific cont

87 These results suggest that a magnetic material's microstructure can be engineered to

88 Among the frustrated magnetic materials, spin-ice stands out as a particularl

89 hniques to characterize other nanostructured magnetic materials, such as nanoparticles, is also revis

90 quest for a novel low-dimensional metal-free magnetic material that would exhibit magnetism at a high

91 have revealed extraordinary spin dynamics in magnetic materials that equilibrium descriptions of magn

92 In magnetic materials, the Pauli exclusion principle typica

93 When interacting with magnetic materials, the wavefunctions of such electrons

94 nual disassembly allows in principle for all magnetic material to be recovered, shredding leads to ve

95 fficient spin detection without the need for magnetic materials, which could lead to useful spintroni

96 nt with arbitrary polarization using typical magnetic materials will benefit the development of magne

97 other hand, disordered freezing of spins in magnetic materials with decreasing temperature, the so-c

98 The FePt/ferritin assemblies are integrated magnetic materials with ferritin providing added magneti

99 ent important case studies in the pursuit of magnetic materials with inherently larger magnetic momen

100 y accomplished through the use of inherently magnetic materials with large magnetic permeability, suc

101 Results indicate that inclusion of magnetic materials with low magnetocrystalline anisotrop

102 The integration of magnetic materials with semiconductors will lead to the

103 ociation reported here of the assembled soft magnetic materials with tuneable sizes could be interest

104 by integrating monolithic ferroelectric and magnetic materials, with interfacial coupling between el