ライフサイエンスコーパス: antiferromagnetic

1 ing order and can be either ferromagnetic or antiferromagnetic.

2 entropy-stabilized oxides considered here is antiferromagnetic.

3 ns between nearest-neighbor Mn(2+) atoms are antiferromagnetic.

4 agnetic states: +/-ferromagnetic (FM) and +/-antiferromagnetic (A-FM).

5 While its neutral form mediates a weak antiferromagnetic (AF) coupling between the two S = 1 Ni

6 es of the system, it is known to enhance the antiferromagnetic (AF) ordering temperature T(N) ( < T(s

7 rgoes a magnetostructural transition from an antiferromagnetic (AF) to a ferromagnetic (FM) phase bet

8 interest due its highly unusual first-order antiferromagnetic (AF) to ferromagnetic (FM) phase trans

9 the other hand, manipulation of magnetism in antiferromagnetic (AFM) based nanojunctions by purely el

10 d-order non-reciprocal optical effects(8) in antiferromagnetic (AFM) bilayers.

11 i-layer of a heavy metal (Pt) and a bi-axial antiferromagnetic (AFM) dielectric (NiO) can be a source

12 tributed to competing ferromagnetic (FM) and antiferromagnetic (AFM) exchange interactions for Eu- an

13 her is from a ferromagnetic (FM) metal to an antiferromagnetic (AFM) insulator at [Formula: see text]

14 rt the observation of ferromagnetic (FM) and antiferromagnetic (AFM) interlayer exchange coupling (IE

15 because neutron scattering suggests that the antiferromagnetic (AFM) long-range order, which is belie

16 Spintronic devices based on antiferromagnetic (AFM) materials hold the promise of fa

17 ion system: Pressure suppresses local-moment antiferromagnetic (AFM) order and induces superconductiv

18 While the control of antiferromagnetic (AFM) orders has been realized by vari

19 structure near the Fermi level emerge in the antiferromagnetic (AFM) phase.

20 nostructures, an opportunity of manipulating antiferromagnetic (AFM) states should offer another rout

21 e show that it is ferromagnetic in plane but antiferromagnetic along the c axis with an out-of-plane

22 Simulations of a quantum magnet with antiferromagnetic and dimerized ground states confirm th

23 ion or the growth axial direction, with both antiferromagnetic and ferromagnetic orders.

24 e magnets, the coexistence of third-neighbor antiferromagnetic and nearest-neighbor ferromagnetic exc

25 d tricritical point separating paramagnetic, antiferromagnetic, and metamagnetic phases in the compou

26 to demonstrate a smoothly varying zero-field antiferromagnetic anisotropic magnetoresistance (AMR) wi

27 the observed magnetic phase transition, from antiferromagnetic at 5 unit cells (ucs) of LMO or below

28 accompanied by corresponding rotation of the antiferromagnetic axis as well, thus maintaining the rig

29 edicted to form around charged dopants in an antiferromagnetic background in the low-doping regime, c

30 ring of "wrong" spins that mismatch with the antiferromagnetic background.

31 of correlation effects in nonsuperconducting antiferromagnetic BaCr2As2 by means of angle-resolved ph

32 re we demonstrate experimentally that canted antiferromagnetic BaMnSb2 is a 3D Weyl semimetal with a

33 ervation of these effects remains elusive in antiferromagnetic-based devices.

34 toms, which leads to either ferromagnetic or antiferromagnetic behavior.

35 h are highly sensitive to the interaction of antiferromagnetic Bi(0.9)La(0.1)FeO(3) with ionic conduc

36 This state forms antiferromagnetic bilayers separated by null spin bilaye

37 icroelectronic circuitry, we implemented the antiferromagnetic bit cell in a standard printed circuit

38 ically and form a one-dimensional Heisenberg antiferromagnetic chain along the a-axis of the crystal.

39 pentahydrate, CN), an alternating Heisenberg antiferromagnetic chain model material, is performed wit

40 The fundamental excitations in an antiferromagnetic chain of spins-1/2 are spinons, de-con

41 Its application to the antiferromagnetic charge transfer insulator YBa(2)Cu(3)O

42 resonance can transmit coherently across an antiferromagnetic CoO insulating layer to drive a cohere

43 ex pseudo-ordering gives rise to short-range antiferromagnetic correlation within an insulating state

44 creation of artificial Mott insulators where antiferromagnetic correlations between spins and orbital

45 Antiferromagnetic correlations have been argued to be th

46 ere, we report site-resolved observations of antiferromagnetic correlations in a two-dimensional, Hub

47 Due to electronic repulsion, the antiferromagnetic correlations of the impurity lattice a

48 solved measurements, we revealed anisotropic antiferromagnetic correlations, a precursor to long-rang

49 e high-pressure synthesis of a new polar and antiferromagnetic corundum derivative Mn2MnWO6, which ad

50 e-stable memory device in epitaxial MnTe, an antiferromagnetic counterpart of common II-VI semiconduc

51 (2) and S 3p(z) orbitals results in a strong antiferromagnetic coupling (computed J = -1516.9 cm(-1))

52 ty measurements rationalize an unprecedented antiferromagnetic coupling between a magnetic U(4+) site

53 DFT calculations further support the strong antiferromagnetic coupling between Co(II) ions and bptz

54 sign of EB is related to the frustration of antiferromagnetic coupling between the ferromagnetic reg

55 ameworks, a transition from ferromagnetic to antiferromagnetic coupling between the metal binding sit

56 both compounds, the experimentally observed antiferromagnetic coupling can be quantitatively explain

57 The intrachain antiferromagnetic coupling in 2 is by far strongest amon

58 ctional theory calculations, we describe the antiferromagnetic coupling in this system that occurs in

59 1) chain of organic radicals with intrachain antiferromagnetic coupling of J'/ k = -14 K, which is as

60 two independent U(V) 5f (1) centers, with no antiferromagnetic coupling present.

61 the [Formula: see text] planes could have an antiferromagnetic coupling that matches or surpasses the

62 uare lattice and with a record high in-plane antiferromagnetic coupling.

63 stem reflect an S = 1/2 paramagnet with weak antiferromagnetic coupling.

64 an unusual molecule stabilized by d-orbital antiferromagnetic coupling.

65 in pumping in heterostructures of a uniaxial antiferromagnetic Cr(2)O(3) crystal and a heavy metal (P

66 ronic state transition in highly crystalline antiferromagnetic CrN films with strain and reduced dime

67 heterostructures exhibiting Neel order in an antiferromagnetic CrSb and ferromagnetic order in Cr-dop

68 l switching between stable configurations in antiferromagnetic CuMnAs thin-film devices by applied cu

69 and, we observe a Mott insulating state with antiferromagnetic Curie-Weiss behaviour, as expected for

70 A practical realization of these antiferromagnetic devices is limited by the requirement

71 The antiferromagnetic dipnictide USb(2) has been of recent i

72 sensitive magnetic sensor to map out layered antiferromagnetic domain structures at zero magnetic fie

73 theories indeed predicted faster dynamics of antiferromagnetic domain walls (DWs) than ferromagnetic

74 The scale-free distribution of antiferromagnetic domains and its non-integral dimension

75 olution to directly visualize the texture of antiferromagnetic domains in NdNiO(3).

76 The intrinsic high frequencies of antiferromagnetic dynamics represent another property th

77 A model for an antiferromagnetic effective exchange interaction based o

78 itive to disturbing magnetic fields, and the antiferromagnetic element would not magnetically affect

79 an S=4 spin system with strong cobalt-ligand antiferromagnetic exchange and J approximately -290 cm(-

80 The interplay between antiferromagnetic exchange and magnetic anisotropy ampli

81 ulations, demonstrate the presence of strong antiferromagnetic exchange between spin centers, with a

82 lculations demonstrate that a unique form of antiferromagnetic exchange coupling appears at the inter

83 The antiferromagnetic exchange coupling between the layers l

84 directly proportional to the strength of the antiferromagnetic exchange coupling between the two sub-

85 and superlattices, we demonstrate the use of antiferromagnetic exchange coupling in manipulating the

86 oth perpendicular to the film plane, a large antiferromagnetic exchange interaction induces a high fr

87 When the value of antiferromagnetic exchange interaction is one and a half

88 ation of pairwise Mn(III)2 ferromagnetic and antiferromagnetic exchange interactions, and the resulta

89 .4 K and fields up to 35 T, reveal competing antiferromagnetic exchange interactions; DFT calculation

90 ertain level compared to the other competing antiferromagnetic exchange pathways can the correspondin

91 Quantum Monte Carlo simulations reveal antiferromagnetic exchange-coupling constants with an av

92 s of Ti atoms interacting with each other in antiferromagnetic fashion to lower the total energy of t

93 rk opens pathways toward a new generation of antiferromagnetic - ferromagnetic interactions for spint

94 structures at zero magnetic field as well as antiferromagnetic/ferromagnetic domains at finite magnet

95 Also, while bulk SmMnO(3) is antiferromagnetic, ferromagnetism was induced in the com

96 rmation in a bilayer system of ferromagnetic/antiferromagnetic (FM/AFM) films, in which the bulk DMI

97 erromagnetic state to Mott insulating G-type antiferromagnetic (G-AFM) state was found in Ca3(Ru(1-x)

98 ion from ferromagnetic [Gd(2)C](2+).2e(-) to antiferromagnetic Gd(2)CCl caused by attenuating interat

99 ger ferromagnetic spin alignments within the antiferromagnetic [Gd(2)C](2+) lattice framework.

100 O3, the new double perovskite oxides have an antiferromagnetic ground state and around room temperatu

101 relative stability of the ferromagnetic and antiferromagnetic ground states, arising from its atomic

102 While the former have insulating and antiferromagnetic ground states, LNO remains metallic an

103 Kitaev interactions, while a second-neighbor antiferromagnetic Heisenberg exchange drives the ground

104 ing it to a problem of quantum magnetism, an antiferromagnetic Heisenberg model in an external magnet

105 A class of antiferromagnetic honeycomb lattices compounds, A(4)B(2)

106 etism in MnPt films, although it is robustly antiferromagnetic in bulk.

107 t LNO is a strange metal, on the verge of an antiferromagnetic instability.

108 scovery of spin current transmission through antiferromagnetic insulating materials opens up vast opp

109 = K, Rb, Cs), the presence of an intergrown antiferromagnetic insulating phase makes the study of th

110 tectable metamagnetic switching, despite the antiferromagnetic insulating state.

111 iCo(2) O(4) from ferrimagnetic metallic into antiferromagnetic insulating with protonation at elevate

112 illerite SrCoO2.5 that is a room-temperature antiferromagnetic insulator (AFM-I) and the perovskite S

113 urrent can ever keep its coherence inside an antiferromagnetic insulator and so drive the spin preces

114 lly-doped topological insulator grown on the antiferromagnetic insulator Cr(2) O(3) .

115 dide (CrI(3)) has been shown to be a layered antiferromagnetic insulator in its few-layer form(1), op

116 mechanism by showing that even the simplest antiferromagnetic insulator like MnO, could display a ma

117 that the interfacial coupling between the 3d antiferromagnetic insulator SrMnO3 and the 5d paramagnet

118 which we attribute to the evolution from an antiferromagnetic insulator to a metallic phase.

119 is a ferromagnetic metal, and SrCoO2.5 is an antiferromagnetic insulator-enable an unusual form of ma

120 tors arise from doping a strongly correlated antiferromagnetic insulator.

121 These results identify antiferromagnetic insulators as suitable candidates for

122 ibits real space Fe and Cu ordering, and are antiferromagnetic insulators with the insulating behavio

123 Four weakly antiferromagnetic interacting biradicals of benzo[1,2- b

124 though solid-state magnetometry indicates an antiferromagnetic interaction between the two iron cente

125 Strong antiferromagnetic interactions across antiphase boundari

126 rate singlet-triplet ground states with weak antiferromagnetic interactions evaluated by magnetometry

127 eraction in the former (2J=14.4 cm(-1) ) and antiferromagnetic interactions in 1O at low temperatures

128 The cubes display weakened antiferromagnetic interactions in the form of a spin-flo

129 l arrangements, which interact via isotropic antiferromagnetic interactions, can generate such a frus

130 UID magnetometry, reveal weak intramolecular antiferromagnetic interactions.

131 a competition between the Zeeman energy and antiferromagnetic interfacial exchange coupling energy.

132 ative and positive exchange bias, as well as antiferromagnetic interlayer coupling are observed in di

133 ial arrangement of ferromagnetic layers with antiferromagnetic interlayer coupling.

134 ults highlight an enhancement of the CrCl(3) antiferromagnetic interlayer interaction that appears to

135 The antiferromagnetic IrMn layer also supplies an in-plane e

136 gether with an excess of La can stabilize an antiferromagnetic LaMnO3-type phase at the interface reg

137 sign alternates with the periodicity of the antiferromagnetic lattice.

138 dicates that these structural defects in the antiferromagnetic layer are behind the resulting large v

139 a ferromagnetic layer exchange-coupled to an antiferromagnetic layer.

140 the transport properties exclusively in the antiferromagnetic layer.

141 both the hidden-order (HO) and large-moment antiferromagnetic (LMAFM) phases and established the 3D

142 both the hidden-order (HO) and large-moment antiferromagnetic (LMAFM) regions of the phase diagram.

143 The antiferromagnetic long-range order manifests through the

144 ing this topic is: whether and how could THz antiferromagnetic magnons mediate a GHz spin current?

145 cooling through the Neel temperature of the antiferromagnetic material in the presence of a magnetic

146 he ability to represent information using an antiferromagnetic material is attractive for future anti

147 Tetragonal CuMnAs is an antiferromagnetic material with favourable properties fo

148 eraction that couples a ferromagnetic and an antiferromagnetic material, resulting in a unidirectiona

149 k on integrating topological insulators with antiferromagnetic materials and unveils new avenues towa

150 Antiferromagnetic materials are internally magnetic, but

151 ) has a general consequence of causing these antiferromagnetic materials to become ferromagnets.

152 studies have focussed on the utilization of antiferromagnetic materials with biaxial magnetic anisot

153 arge can anisotropic magnetoresistance be in antiferromagnetic materials with very large spin-orbit c

154 romagnetic islands nucleate in an insulating antiferromagnetic matrix.

155 r the electrical read-out of multiple-stable antiferromagnetic memory states, which we set by heat-as

156 In spintronics, the antiferromagnetic metal IrMn has been used as the pinnin

157 Magnetic studies reveal strong antiferromagnetic metal...radical coupling with coupling

158 othermal magnetotransport measurements in an antiferromagnetic-metal(IrMn)/ferromagnetic-insulator th

159 s have been realized using fully compensated antiferromagnetic metals.

160 Whereas we find antiferromagnetic Mn-Mn coupling along the chain, the in

161 ompeting ferromagnetic (Mn(2+) -Mn(3+) ) and antiferromagnetic (Mn(2+) -Mn(2) , Mn(3+) -Mn(3+) ) inte

162 Moreover, highly ordered antiferromagnetic MnPt films exhibit superiorly large ex

163 This implies that information stored in antiferromagnetic moments would be invisible to common m

164 e means for an efficient electric control of antiferromagnetic moments.

165 heoretical evidence of the realization of an antiferromagnetic Mott insulating phase in 2D pai-conjug

166 a quantum phase transition (QPT) between an antiferromagnetic Mott insulating state and a paramagnet

167 cuprate high-temperature superconductors, an antiferromagnetic Mott insulating state can be destabili

168 enon at the LaMnO3/SrTiO3 interface where an antiferromagnetic Mott insulator abruptly transforms int

169 e-doping to the parent compound, which is an antiferromagnetic Mott insulator, has been predicted to

170 tion process in superfluid helium due to the antiferromagnetic nature of chromium.

171 weak disorder and quantum fluctuations of an antiferromagnetic nature.

172 reversible switching of the thermally-stable antiferromagnetic Neel vector by spin-orbit torques.

173 overy of the spin-orbit-entangled exciton in antiferromagnetic NiPS(3) introduces van der Waals magne

174 en the nonmagnetic metallic cT phase and the antiferromagnetic O phase.

175 single-phase multiferroics remain limited by antiferromagnetic or weak ferromagnetic alignments, by a

176 Direct coupling between BiFeO3 antiferromagnetic order and Co magnetization is observed

177 ron-based superconductivity develops near an antiferromagnetic order and out of a bad-metal normal st

178 ven by the X-ray-induced modification of the antiferromagnetic order and the corresponding exchange b

179 candidate Na(2)BaCo(PO(4))(2), which has an antiferromagnetic order at very low temperature (T(N) ~

180 Additionally, BaMnSb2 also exhibits a G-type antiferromagnetic order below 283 K.

181 By exploiting the fact that the antiferromagnetic order can be reconfigured by local the

182 We show here that an induced antiferromagnetic order can be stabilized in the [111] d

183 particular, we demonstrate the emergence of antiferromagnetic order in a system which is initially i

184 xtremely high magnetic fields to destroy the antiferromagnetic order in gamma-lithium iridate and rev

185 The manipulation of antiferromagnetic order in magnetoelectric Cr(2)O(3) usi

186 The smooth disappearance of antiferromagnetic order in strongly correlated metals co

187 Antiferromagnetic order occurs below a Neel temperature

188 Upon increasing the P-content, the antiferromagnetic order of the Ce-4f moment is suppresse

189 l strong interfacial interaction between the antiferromagnetic order of the Cr(2) O(3) and the magnet

190 e towards large-amplitude modulations of the antiferromagnetic order parameter.

191 of Bi(3+) at around 135 K, and a long-range antiferromagnetic order related to the Cr(3+) spins arou

192 The data reveal the development of nuclear antiferromagnetic order slightly above 2 mK and of heavy

193 The onset temperature T CDW takes over the antiferromagnetic order temperature T N beyond a critica

194 ate is usually electronically frozen with an antiferromagnetic order that resists external control.

195 BiFeO3, as well as exchange coupling of its antiferromagnetic order to a ferromagnetic overlayer.

196 ate instead of the more traditional ferro or antiferromagnetic order to couple to electric properties

197 ic order for 304 K < T < 565 K, but a canted antiferromagnetic order with a ferromagnetic component f

198 tion functions reveals a hidden finite-range antiferromagnetic order, a direct consequence of spin-ch

199 anied by short-range, quasi-one-dimensional, antiferromagnetic order, and provides a natural explanat

200 eminiscent of a transition into a phase with antiferromagnetic order, but evidence for an associated

201 g these fields, which couple strongly to the antiferromagnetic order, we demonstrate room-temperature

202 iprocal SHG originates only from the layered antiferromagnetic order, which breaks both the spatial-i

203 the vicinity of the onset of the short-range antiferromagnetic order.

204 and reaches a coherent state assisted by the antiferromagnetic order.

205 c structure of ferromagnetic and spin-canted antiferromagnetic ordered materials as well as an unders

206 On decreasing x from 0.5, the antiferromagnetic-ordered moment continuously decreases,

207 (ferromagnetic ordering in the ab plane and antiferromagnetic ordering along the c axis below 286 K)

208 (22)As(32), and Eu(3)Ga(6)As(8) and indicate antiferromagnetic ordering below 10 K.

209 Powder neutron diffraction confirms antiferromagnetic ordering below TN approximately 175 K,

210 he coexistence between superconductivity and antiferromagnetic ordering in the same CuO(2) sheet.

211 The antiferromagnetic ordering that MnBi(2)Te(4) shows makes

212 strong magnetic correlations persist at the antiferromagnetic ordering vector up to dopings of about

213 ombic) phase transition at Ts = 90 K without antiferromagnetic ordering-by neutron scattering, findin

214 ainly from the B-site Fe exhibiting a G-type antiferromagnetic ordering.

215 The complex antiferromagnetic orders observed in the honeycomb irida

216 ghest attainable magnetic fields.The complex antiferromagnetic orders observed in the honeycomb irida

217 gnetic scattering shows predominately c-axis antiferromagnetic orientation of the magnetic moments fo

218 cT) phase at low temperature and PII with an antiferromagnetic orthorhombic (O) phase at low temperat

219 gnments that are found within the 3-D C-type antiferromagnetic perovskites.

220 se transition taking place at ~400 K from an antiferromagnetic phase at room temperature to a high te

221 e planes of Fe and Rh atoms in the nominally antiferromagnetic phase at room temperature.

222 (7) superconductors at the point where their antiferromagnetic phase comes to an end.

223 The activation volume of the antiferromagnetic phase is more than two orders of magni

224 upt transition from the ferromagnetic to the antiferromagnetic phase, while the reverse transition re

225 ilms designed so that both ferromagnetic and antiferromagnetic phases are bistable at room temperatur

226 nomena and highlight their importance in the antiferromagnetic phases of Kondo lattices.

227 O3:NiO films, which can be attributed to the antiferromagnetic properties of the Co3O4 phase.

228 3R-MoN(2) also shows weak antiferromagnetic properties, which probably originates

229 face between a spin ice and an isostructural antiferromagnetic pyrochlore iridate and whose monopole

230 h magnets with high intrinsic coercivity and antiferromagnetic pyrochlores with strongly-pinned ferro

231 Kondo lattice systems in the vicinity of an antiferromagnetic QCP.

232 ls with unconventional superconductivity and antiferromagnetic QCPs(1-4) has led to the belief that t

233 LNO is a quantum critical metal, close to an antiferromagnetic quantum critical point (QCP).

234 duced state in the vicinity of a field-tuned antiferromagnetic quantum critical point at Hc approxima

235 results underline that fluctuations from the antiferromagnetic quantum criticality promote unconventi

236 However, spin-current generation via antiferromagnetic resonance and simultaneous electrical

237 At 0.240 terahertz, the antiferromagnetic resonance in Cr(2)O(3) occurs at about

238 Although the antiferromagnetic response in the pseudogap state has be

239 Peripentacene dimers exhibit an antiferromagnetic (S=0) singlet ground state.

240 ies of CrSBr are reported, an air-stable vdW antiferromagnetic semiconductor that readily cleaves per

241 se transition between stable 1D metal and an antiferromagnetic semiconductor, with the phase boundary

242 g large U/t ratio drives these COFs into the antiferromagnetic side of the phase diagram.

243 Carlo simulations, we show that a fractional antiferromagnetic skyrmion lattice is stabilized in MnSc

244 d that the skyrmion Hall effect vanishes for antiferromagnetic skyrmions because their fictitious mag

245 demonstrates that the theoretically proposed antiferromagnetic skyrmions can be stabilized in real ma

246 Such antiferromagnetic skyrmions may allow more flexible cont

247 ayed growth of spin fluctuations and develop antiferromagnetic spatial correlations resulting from th

248 er is a consequence of the interplay between antiferromagnetic spin correlations and local magnetic a

249 Antiferromagnetic spin correlations are maximal at half-

250 play between local many-body excitations and antiferromagnetic spin correlations.

251 ding allows us to investigate the physics of antiferromagnetic spin dynamics and highlights the impor

252 y high velocities can be attained due to the antiferromagnetic spin dynamics associated with ferrimag

253 s remarkable enhancement is a consequence of antiferromagnetic spin dynamics at TA.

254 However, experimental investigations of antiferromagnetic spin dynamics have remained unexplored

255 al motivation towards this direction is that antiferromagnetic spin dynamics is expected to be much f

256 Here we show that fast field-driven antiferromagnetic spin dynamics is realized in ferrimagn

257 Antiferromagnetic spin motion at terahertz (THz) frequen

258 an in-plane oriented diagonal double-stripe antiferromagnetic spin structure.

259 ibility of digital data processing utilizing antiferromagnetic spin waves and enable the direct proje

260 quency mode is accounted for as an effective antiferromagnetic spin-wave mode.

261 romagnetic material is attractive for future antiferromagnetic spintronic devices.

262 The field of antiferromagnetic spintronics can also be viewed from th

263 Antiferromagnetic spintronics is an emerging field; anti

264 Antiferromagnetic spintronics is an emerging research fi

265 e demonstrates the ultrafast readout for the antiferromagnetic spintronics using Mn(3)Sn, and will al

266 g spin-orbit torque, enabling high-efficient antiferromagnetic spintronics.

267 ena and they became crucial for the field of antiferromagnetic spintronics.

268 avenues towards dissipationless topological antiferromagnetic spintronics.

269 tlook of future research and applications of antiferromagnetic spintronics.

270 s the ultrafast manipulation of magnetism in antiferromagnetic spintronics.

271 the potential of polycrystalline metals for antiferromagnetic spintronics.

272 lane ferromagnetic ground state, an in-plane antiferromagnetic state appears at temperatures above 90

273 A phase transition from metallic AFM-b antiferromagnetic state to Mott insulating G-type antife

274 Starting with the film in a uniform antiferromagnetic state, the ability to write arbitrary

275 und reveals the asymmetry is enhanced in the antiferromagnetic state.

276 e propose detection schemes for implementing antiferromagnetic states and density waves.

277 rial is characterized by a 3-k non-collinear antiferromagnetic structure and multidomain Jahn-Teller

278 d, we find that Sr2MgOsO6 orders in a type I antiferromagnetic structure at the remarkably high tempe

279 mergence of a ((1/4),(1/4),(1/4))-wavevector antiferromagnetic structure in LaNiO3 and the presence o

280 magnetic state of Eu evolves from the canted antiferromagnetic structure in the ground state, via a p

281 temperatures, we trace modifications of the antiferromagnetic structure of the compound.

282 ediate pressure, finally to an "unconfirmed" antiferromagnetic structure under the high pressure.

283 , T(N) = 132 +/- 1 K, CrSBr adopts an A-type antiferromagnetic structure with each individual layer f

284 on between ferromagnetic double-exchange and antiferromagnetic super-exchange.

285 illations corresponds to the strength of the antiferromagnetic superexchange interaction in NiO and t

286 ther demonstrate that MnBi(4)Te(7) is a Z(2) antiferromagnetic TI with two types of surface states as

287 This goal is achieved by coupling spins in antiferromagnetic TmFeO(3) (thulium orthoferrite) with t

288 a possible quantum phase transition from an antiferromagnetic to a weak ferromagnetic state at filli

289 ted to the interlayer ordering changing from antiferromagnetic to ferromagnetic at a critical magneti

290 by ~50% and that the transition from layered antiferromagnetic to ferromagnetic order tunes the spect

291 tures, electronic reconstruction leads to an antiferromagnetic to ferromagnetic transition, making th

292 xperimental techniques the realization of an antiferromagnetic topological insulator in the layered v

293 magnetic susceptibility measurements find an antiferromagnetic transition at [Formula: see text] K.

294 We demonstrate detection of antiferromagnetic transition in ultra-thin CoO films via

295 rmed by the TN values of the paramagnetic to antiferromagnetic transition.

296 emained challenging to excite and manipulate antiferromagnetic-type propagating spin waves.

297 Antiferromagnetic-type spin waves are innately high-spee

298 eel temperature of 150 kelvin in NiPS(3), an antiferromagnetic van der Waals material.

299 tionship between ferroelectric polarization, antiferromagnetic vector and the Dzyaloshinskii-Moriya v

300 exchange coupling within the [Fe8 ] core is antiferromagnetic which is attenuated upon reduction to