ライフサイエンスコーパス: tetragonal

1 n to a cubic phase with higher symmetry than tetragonal.

2 ate-Cu interaction and the site becomes less tetragonal.

3 onal block copolymer morphologies, including tetragonal and helical structures, from a combination of

4 rical transport studies reveal that both the tetragonal and hexagonal CoSe nanoplates show strong thi

5 of DAPAL from Escherichia coli (EcDAPAL) in tetragonal and monoclinic forms at 2.0 and 2.2 A resolut

6 and controlled crystal phases (e.g., cubic, tetragonal and multi-phase).

7 to show that there is a coexistence of both tetragonal and orthorhombic phases through the low-tempe

8 the pure tetragonal phase into a mixture of tetragonal and orthorhombic phases), the electrical cond

9 n are calculated to be 50 and 27 meV for the tetragonal and orthorhombic phases, respectively, which

10 est refined with a model containing both the tetragonal and orthorhombic phases.

11 intermediate strain regime takes place, with tetragonal and orthorhombic structural phases coexisting

12 This material occurs in two crystal forms, tetragonal and orthorhombic, both with a band gap much s

13 The equilibrium between the tetragonal and pentagonal prism followed a linear free-e

14 getically competitive potential phases, four tetragonal and two monoclinic structures.

15 rent occurrence of structural (monoclinic to tetragonal) and electrical (insulator to the conductor)

16 nic compounds (3-D Pm3n cubic, 3-D P4(2)/mnm tetragonal, and a crystallographically forbidden 12-fold

17 s are found, and three phases (orthorhombic, tetragonal, and collapsed tetragonal) coexist between TS

18 nd AB13 stoichiometry with cubic, hexagonal, tetragonal, and orthorhombic symmetries have been identi

19 ns result from moving the boundaries between tetragonal- and rhombohedral-like phases, which changes

20 They crystallize in the tetragonal anti-PbO structure, which is composed of laye

21 ogenous protein oxygen ligand in a distorted tetragonal array.

22 f bulk SrTiO3(STO) transitions from cubic to tetragonal at around 105 K.

23 the boron icosahedra and 2b sites in a alpha-tetragonal B(52) base structure.

24 (Isotypic SrHg(2)Tl(2) also exists.) The tetragonal barium structure (P4(2)/mnm, a = 10.606 A, c

25 age-displayed peptide library via binding to tetragonal BaTiO3 powder.

26 ze and consist of a mixture of body centered tetragonal (bct) and body centered cubic (bcc) structure

27 ork, we report the presence of body-centered tetragonal (bct) and body-centered orthorhombic (bco) ph

28 ubic (FCC) through a series of body-centered tetragonal (BCT) intermediate phases.

29 structure was found to show a body-centered tetragonal (BCT) type.

30 es--body-centered cubic (bcc), body-centered tetragonal (bct), and face-centered cubic (fcc)--as conf

31 on vacancy in nonintercalated FeSe (PbO-type tetragonal beta-Fe1-xSe).

32 rom the cubic alpha-phase (Pm3 m, #221) to a tetragonal beta-phase (P4/mbm, #127) at around 285 K, fo

33 cysteines are at loops L1 and L3 and form a tetragonal binding site for a zinc ion.

34 f uniform anatase NCs based on the truncated tetragonal bipyramidal geometry.

35 or superconductivity in U compounds with the tetragonal body-centered [Formula: see text] structure.

36 embly of single-crystal FeGe2 nanowires with tetragonal C16 crystal structure shows anisotropic magne

37 measurements demonstrate the presence of the tetragonal Cd(3)As(2) crystal phase in studied films.

38 studies revealed that it crystallizes in the tetragonal CeCr(2)Si(2)C structure.

39 The structure is monoclinic, with a pseudo-tetragonal cell that favors multiple twinning on a scale

40 cation exchange, extracts sulfur to produce tetragonal chalcocite (Cu(2)S).

41 structural differences between digenite and tetragonal chalcocite are believed to influence the acce

42 es undergo a spontaneous phase transition to tetragonal chalcocite in situ, prior to the onset of cat

43 sence of the BT2 peptide exhibiting the most tetragonal character.

44 ses (orthorhombic, tetragonal, and collapsed tetragonal) coexist between TS=95 K and 45 K.

45 lloidal superstructures, including cubic and tetragonal colloidal crystals, with no known atomic anal

46 We show that Cu(2+)-Abeta(11-40) forms a tetragonal complex with a 34 +/- 5 fm dissociation const

47 the growth temperature, ultrathin 2D layered tetragonal CoSe nanoplates and nonlayered hexagonal CoSe

48 ction of external dopants, and therefore the tetragonal crystal structure and carrier mobility of CuB

49 ay diffraction patterns yielded good fits to tetragonal crystal structures, with the BaTiO3 formed in

50 The tetragonal crystal system is conserved during this trans

51 we show that common garnet with a non-cubic (tetragonal) crystal structure is much more widespread th

52 Tetragonal crystals are obtained with improved diffracti

53 nt pressure: PI with a nonmagnetic collapsed tetragonal (cT) phase at low temperature and PII with an

54 onal (T), orthorhombic (O) and the collapsed-tetragonal (cT) phases in the structural phase diagram o

55 /Ala analogues suggest a dynamic view of the tetragonal Cu(2+) complex, with axial as well as equator

56 The data are consistent with a tetragonal Cu(II) site with nitrogen and oxygen ligands.

57 one, two, or three dimensions (orthorhombic, tetragonal, cubic).

58 mantle discontinuities can be explained by a tetragonal-cubic phase transition in Ti-bearing CaSiO(3)

59 The synthesis of monodisperse chalcopyrite (tetragonal) CuInSe(2) nanocrystals is reported.

60 ing in a CuMnAs/Fe bilayer, we conclude that tetragonal CuMnAs films are suitable candidate materials

61 Tetragonal CuMnAs is an antiferromagnetic material with

62 upling between an epitaxial antiferromagnet, tetragonal CuMnAs, and an Fe surface layer.

63 mine the spin axis and magnetic structure in tetragonal CuMnAs, and reveal the presence of an interfa

64 high-temperature antiferromagnetic material, tetragonal CuMnAs, which exhibits excellent crystal qual

65 The tetragonal cuprate HgBa(2)CuO(4+delta), with only one Cu

66 pair of Cr(III) ions occupying edge-sharing tetragonal distorted octahedral sites generated by forma

67 ure (TC) and the substrate induced (pseudo-) tetragonal distortion (ratio of out-of-plane to in-plane

68 in volume, but only a very small increase in tetragonal distortion at Hc.

69 nd leads to a structural instability towards tetragonal distortion at low temperatures.

70 st that the non-monotonicity arises from the tetragonal distortion under large biaxial strain.

71 minishes the energy gain associated with the tetragonal distortion, allowing the cubic phase to be st

72 terface to be comparable to that of a single tetragonal domain of STO, the anisotropy of interfacial

73 conductivity is strongly modified by the STO tetragonal domain structure.

74 Both the tetragonal elongation of the CoO(4)S(2) polyhedron and t

75 systems are shown to correlate well with the tetragonal elongation of the coordination environment.

76 A tetragonal, end-on superoxide structure is proposed base

77 cannot support a terminal oxido ligand in a tetragonal environment.

78 generated in solution (ESI-MS, m/z = 565.15; tetragonal EPR) by reacting *NO(g) with superoxo complex

79 tructure to chemically ordered face-centered tetragonal (fct) structure, and further promotes formic

80 onal intermetallic [denoted as face centered tetragonal (fct)] structure.

81 rimentally investigated in thin films of the tetragonal ferroelectric PbZr(0.2) Ti(0.8) O(3) .

82 Finally, a phase diagram of tetragonal FeS as functions of pressure and temperature

83 FDMFT) scheme to comprehensively explain why tetragonal FeS shows both semiconducting and metallic re

84 he superconducting transition temperature of tetragonal FeS was gradually depressed by pressure, diff

85 S3-like complex associated with mackinawite (tetragonal FeS) rather than as a discrete As2S3 phase.

86 hypothesis that nanocrystalline mackinawite (tetragonal FeS), which is abundant in sediments where Hg

87 ucting and metallic responses in contrast to tetragonal FeSe which is a pseudogaped metal above the s

88 ssed by pressure, different from the case in tetragonal FeSe.

89 Structure of the enzyme in the tetragonal form had PLP bound at the active site, wherea

90 ystals and the {110} faces of the non-native tetragonal form.

91 While the tetragonal forms exhibit only an incipient antiferromagn

92 h {100} and {110} faces of the hexagonal and tetragonal forms, respectively.

93 s FeS, FeSe and FeTe with their better known tetragonal forms.

94 the sodium disorder and showing that a local tetragonal framework more accurately describes the struc

95 ust phenazine linkage into a two-dimensional tetragonal framework that is stable under boiling water,

96 K, followed by a first-order transition to a tetragonal gamma-phase (retaining P4/mbm, #127) at 140 K

97 ise to two mononuclear Cu(II) complexes with tetragonal geometry.

98 ities and the second-order elastic moduli of tetragonal hen egg-white lysozyme crystals were determin

99 tes a series of sp(2) carbon frameworks with tetragonal, hexagonal, and kagome topologies.

100 a solid oxide reaction method resulting in a tetragonal hollandite structure (space group I4/m).

101 accompanied by a structural distortion from tetragonal I4/m symmetry to monoclinic I2/m symmetry, wh

102 temperature, with the symmetry lowered from tetragonal I4/mmm to orthorhombic Immm and the size of t

103 )TiO(4) spinel transforms to a high pressure tetragonal (I4(1)/amd, No.141) phase at 14.7 GPa.

104 dopts a non-centrosymmetric structure in the tetragonal I42m space group with unit cell parameters a=

105 At 295 K, (NH(4))(3)Cr(O(2))(4) is tetragonal (I42m), with the NH(4)(+) ions occupying two

106 The perforation obeys a tetragonal instead of hexagonal symmetry.

107 d as face centered cubic (fcc)] structure to tetragonal intermetallic [denoted as face centered tetra

108 Transport properties of tetragonal iron monosulfide, mackinawite, show a range o

109 More importantly, tetragonal iron(V)-nitrido and -oxo complexes 1-3 and 5

110 dd excitons of the Fe(2+) sites arise from a tetragonal Jahn-Teller active polaronic distortion of th

111 n the out-of-plane thermal conductivities of tetragonal L10 FePt (001) easy-axis and cubic A1 FePt th

112 ar phase transformed first to a new phase of tetragonal lattice (T-phase) over a narrow range of rela

113 The c-parameter in the tetragonal lattice is observed to expand up to 0.5% for

114 CaM41/75 crystallized in a tetragonal lattice with the Ca2+ bound in all four EF-ha

115 crystalline order were obtained, adopting a tetragonal lattice.

116 from the initial monoclinic structure to the tetragonal lattice.

117 Fs with the expected body-centered (cubic or tetragonal) lattice arrangements.

118 dendrimers that self-organize into cubic and tetragonal lattices.

119 In the tetragonal ligand field, these electrons populate an orb

120 y giving local structures that are cubic and tetragonal like from the point of view of the PbI(3) fra

121 of a piezomagnetic coupling to the adjacent tetragonal-like phase and the epitaxial constraint.

122 Electric field-dependent studies show that a tetragonal-like phase can be reversibly converted into a

123 atically templated by a nanoscale anion, the tetragonal Lindqvist polyoxometalate Mo6O19(2-).

124 Further in-depth analyses suggested that tetragonal low spin iron(V)-nitrido and -oxo complexes f

125 ment with experiments on the growth rates of tetragonal lysozyme crystals as a function of pH, salt c

126 ctive self-assembly could be used to prepare tetragonal (M8L12), pentagonal (M10L15), and hexagonal (

127 nm diameter skyrmions in the centrosymmetric tetragonal magnet GdRu(2)Si(2) without a geometrically f

128 A baromagnetic effect in a novel tetragonal magnetic structure is introduced by vacancies

129 e mechanism that leads to the sudden drop of tetragonal magnetostriction at x ~ 19, a long-standing p

130 e thermal expansion in the a-b plane of this tetragonal material.

131 at around 338 K between a high-temperature, tetragonal, metallic state (T) and a low-temperature, mo

132 ce of solar cells made with HaPs, especially tetragonal methylammonium lead triiodide (MAPbI3).

133 runeisen parameters (gamma(th)) of cubic and tetragonal Mg(2)TiO(4) phases are 1.01 and 0.63.

134 we develop three-dimensional silicon-coated tetragonal microlattices that transform into sinusoidal

135 on in a strain-driven rhombohedral and super-tetragonal mixed phase of BiFeO(3).

136 the large geometric misfit between adjacent tetragonal Mn(3)O(4) grains results in tilt boundaries a

137 Unlike previously reported, tetragonal Mn(V) nitrides with a d(2), nonmagnetic S = 0

138 oes anionic persulfide reduction to form the tetragonal Mo(VI) complex [MoOS3](2-).

139 discovery and synthesis of a novel Cl-doped tetragonal Na3PS4 (t-Na3-xPS4-xClx) solid electrolyte wi

140 The six exposed facets of this tetragonal nanocrystal give rise to six pieces of "nanoS

141 induce the rapid formation of ferroelectric (tetragonal) nanocrystalline BaTiO3 at room temperature f

142 ct the bulk two-dimensional SAMs and various tetragonal nanocrystals.

143 realize the coexistence of rhombohedral and tetragonal nanodomains embedded in a cubic matrix.

144 p to 3.9 x 10(7) A cm(-2) , while the square tetragonal nanoplates show considerably lower conductivi

145 on temperature (Tc) and unit cell metrics of tetragonal (NH3)yCs0.4FeSe were investigated in high pre

146 For Co(II)(OEP) doped into tetragonal Ni(II)(OEP) (which displays a very large g( p

147 yz)(5)](SbF(6))(2) (2) crystallize in either tetragonal or orthorhombic space groups; their structure

148 ed polycrystals of materials that are either tetragonal or rhombohedral cannot switch; yet polycrysta

149 The former can be ascribed to the tetragonal-orthorhombic structural phase transition, and

150 ni-axial phase transformation mechanism, the tetragonal/orthorhombic-to-collapsed-tetragonal phase tr

151 lly cubic transition occurs from the ambient tetragonal P4 mm structure in pure PbTiO(3); whereas the

152 12(1)) is nonsuperconducting and undergoes a tetragonal (P4/nmm) to monoclinic (P2(1)/m) structural t

153 adjacent unit cells, is best described by a tetragonal P4mm space group.

154 e average structure is orthorhombic Amm2 and tetragonal P4mm, was best described by the rhombohedral

155 tely 12 times larger than the stoichiometric tetragonal parent phase of CeNbO4 as a result of the hel

156 It is found that superconductor FeS (tetragonal) partly transforms to a hexagonal structure a

157 In the stability field of tetragonal PbTiO3 we observed pressure-induced reversals

158 t the nanoscale ferroelectric switching of a tetragonal PbZr(0.2)Ti(0.8)O(3) thin film under an appli

159 We report a novel observation of the tetragonal perforated layer structures in a series of ro

160 ic change in the BCP morphology, and uniform tetragonal perforations were observed at f(PMPCS) approx

161 chiral spheres self-organize into cubic and tetragonal periodic arrays and into a quasiperiodic 12-f

162 ith the inversion-asymmetry parameter in the tetragonal perovskites, evaluate anisotropic g-factors f

163 eventually to a high pressure body-centered tetragonal phase (SG: I4/mmm).

164 ilms on NSTO100 coexist a commensurate [001]-tetragonal phase and two incommensurate [010]-monoclinic

165 ion of approximately 1/8, where a new pseudo-tetragonal phase appears and the electric modulation of

166 s stabilizes the high-temperature disordered tetragonal phase at a much lower temperature.

167 perature, the spinel phase coexists with the tetragonal phase between 14.7 and 24.3 GPa.

168 s for pseudorhombohedral compositions near a tetragonal phase boundary.

169 We observe the ferroelectric tetragonal phase even for the smallest particles at 26 n

170 por transport and found to maintain the same tetragonal phase in ambient air for at least 197 d.

171 res from the initial monoclinic to the final tetragonal phase in crystalline vanadium dioxide; the ch

172 This tetragonal phase in P4/mcc space group, along with the d

173 peak width and splitting reminiscent of the tetragonal phase in single crystals.

174 n the crystal structure (i.e., from the pure tetragonal phase into a mixture of tetragonal and orthor

175 the volume reduction on change from cubic to tetragonal phase is about 9%.

176 e is recoverable to ambient pressure and the tetragonal phase is at least partially recoverable.

177 isothermal bulk modulus of the high-pressure tetragonal phase is calculated to be 209(2) GPa and V(0)

178 Here we report that a stable body-centred tetragonal phase is observed in silver nanoparticles wit

179 tric cubic phase, although the ferroelectric tetragonal phase is partly retained even in ca. 7 nm nan

180 phases, Ag(2)Se is obtained in a metastable tetragonal phase not observed in the bulk.

181 In the paramagnetic tetragonal phase of BaFe(2-x)T(x)As2 (where T is Co or N

182 rystals, while successful in stabilizing the tetragonal phase of isomorphous ZrO2, has produced nanor

183 with the structural domain formation in the tetragonal phase of STO.

184 The body-centered tetragonal phase originates from the distortion of cubic

185 Rather, it stays in the tetragonal phase over a wide temperature range of 110 to

186 resulting from recrystallizing the original tetragonal phase reported by Lis in acetonitrile and tol

187 s widely accepted that in a classic cubic-to-tetragonal phase transformation, with only three tetrago

188 sm, the tetragonal/orthorhombic-to-collapsed-tetragonal phase transformation.

189 The orthorhombic-to-tetragonal phase transition in perovskite can significan

190 nt mobility confirm that the orthorhombic-to-tetragonal phase transition is a first-order phase trans

191 associated with the reported orthorhombic-to-tetragonal phase transition of La2NiO4+delta.

192 dynamics of a tip bias-induced rhombohedral-tetragonal phase transition of strained (001)-BiFeO3 (rh

193 gation of the size-dependent orthorhombic-to-tetragonal phase transition using a combined temperature

194 suggests a possible tetragonal to collapsed tetragonal phase transition.

195 fraction studies revealed that the films had tetragonal phase with (001) orientation.

196 as-synthesized nanomaterials possess a pure tetragonal phase with variable morphologies from shuttle

197 calculations identify softer bonding in the tetragonal phase, relative to the monoclinic phase, as t

198 r scattering, and gamma = 0.5 +/- 0.1 in the tetragonal phase, suggesting another dominant mechanism,

199 rystals at low temperature (still within the tetragonal phase, which is stable at room temperature).

200 es on the magnetic field as the conventional tetragonal phase.

201 cubic phases transformed to a body-centered tetragonal phase.

202 a dominant factor for destabilization of the tetragonal phase.

203 hase, Si-VIII and two of our other predicted tetragonal phases are highly likely within laser-affecte

204 e also observed coexistence of the cubic and tetragonal phases over a range of temperature in all cas

205 Upon cooling further, all the tetragonal phases transformed into a low temperature ort

206 n two slightly different non-superconducting tetragonal phases, PI and PII, through thermal treatment

207 ound to be similar to bulk yttria-stabilized tetragonal polycrystals of the same relative density but

208 The tetragonal polymorph determined at ambient pressure tran

209 a grain of stishovite (from the interior), a tetragonal polymorph of silica that only occurs at ultra

210 The dynamic adaptability of tetragonal prismatic nanocapsule 1(8+) in the selective

211 an emissive poly(ethylene glycol)-decorated tetragonal prismatic platinum(II) cage was prepared and

212 These tetragonal prismatic SCCs are self-assembled on mixing a

213 0 degrees platinum metal complex (3) affords tetragonal prisms (4) as single products.

214 been tested on the assembly of trigonal and tetragonal prisms from the biphenyl rod, [Ph2P(CH2)3PPh2

215 ynthesis of stable 3-D metallosupramolecular tetragonal prisms in which multicomponent coordination-d

216 he giant strain originates from rhombohedral-tetragonal (R-T) phase transition under electric-filed,

217 We observe a new tetragonal rectangular crystal (TRX) phase possessing (q

218 nder electric-filed, and is recoverable from tetragonal-rhombohedral (T-R) phase transition by compre

219 complex non-centrosymmetric structure in the tetragonal space group I4 2m was solved by means of sing

220 Im network (alpha-phase) crystallizes in the tetragonal space group I4(1)cd (a = 23.5028(4) A, c = 12

221 e of Sr(3)Co(2)O(4)Cl(2) is described in the tetragonal space group I4/mmm [a = 4.007(1) A, c = 22.28

222 neutron diffraction data and belongs to the tetragonal space group P4/m (no.

223 These compounds crystallize in tetragonal space group P4/mnc with the Sc2Fe3Si5-type st

224 stals, the gammaN308K crystals belonged to a tetragonal space group with an unusually long unit cell

225 The majority phase was found to be tetragonal (space group I4/mmm) with lattice parameters

226 tion below 155 K, changing the symmetry from tetragonal (space group P4/nmm) to monoclinic (space gro

227 2)-Ac), which also crystallizes in an axial (tetragonal) space group but which now is recognized to c

228 ermined by single-crystal X-ray diffraction: tetragonal, space group I4(1)/acd, a = 19.102(2), b = 19

229 At first sight, the quenched tetragonal spinel CuMn(2)O(4) can be formulated with Cu(

230 Epitaxial tetragonal SrTiN2 films have been successfully prepared

231 , in this paper, for the first time a unique tetragonal star-like morphology of polyaniline was appli

232 he transformation from twinned-monoclinic to tetragonal, starting at a twin boundary and propagating

233 strained BiFeO3 films transition into a true tetragonal state at 430 degrees C but remain polar to mu

234 lar to neat AB, that is, the orthorhombic-to-tetragonal structural phase transition is observed at 22

235 ed on thermal cycling above the STO cubic-to-tetragonal structural transition temperature, implying t

236 n orthorhombic structure (Pnma, no. 62) to a tetragonal structure (P4/mbm, no. 127) is found around 2

237 rom a face-centered cubic to a body-centered tetragonal structure after failure.

238 matrix by 2.35%, forcing it to maintain its tetragonal structure and resulting in the highest BaTiO(

239 The single crystals of tetragonal structure are easy to cleave into perfect squ

240 nium into CaSiO(3) perovskite stabilizes the tetragonal structure at higher temperatures, and that th

241 k-like orthorhombically distorted phase to a tetragonal structure by shifting the oxygen octahedra ro

242 This tetragonal structure has a 1:1 order of cations on both

243 A crucial feature of the tetragonal structure is that the methylammonium ions do

244 rystalline domains with the long axis of the tetragonal structure oriented perpendicular to the subst

245 ansformation of the cubic Mg(2)TiO(4) to the tetragonal structure was complete by 29.2 GPa, ~5 GPa hi

246 structural measurements reveal a persistent tetragonal structure with smooth changes in the atomic d

247 Larger nanocrystals adopt the beta-Sn tetragonal structure, while smaller nanocrystals show st

248 taxial Ca2IrO4 thin-films are of K2NiF4-type tetragonal structure.

249 ce-centred-cubic structure to a body-centred-tetragonal structure.

250 of optically isotropic cubic phase into the tetragonal structure.

251 , the Bi2Se3 crystallizes into body-centered tetragonal structures rather than the recently reported

252 uperlattices, simple-cubic and body-centered-tetragonal structures, has been achieved using a home-bu

253 to growth of BiFeO3 thin films on cubic and tetragonal substrates involving high levels of tensile s

254 In Sr(2)RuO(4) films deposited on tetragonal substrates the highest-conductivity direction

255 is a superstructure of the infinite-layered tetragonal superconducting phase of SrCuO2 and is not st

256 As a demonstration, we realize the tetragonal superlattice of octagonal gold nanorods, brea

257 es the superlattice symmetry, leading to the tetragonal superlattice that becomes energetically favor

258 Surprisingly, such sparse tetragonal superstructure exhibits much higher thermosta

259 disordered Na(x)V(2)(PO(4))(2)F(3) phase of tetragonal symmetry (I4/mmm space group).

260 e are revealed to break the room-temperature tetragonal symmetry in Ba(Fe1-x Cox)2 As2.

261 till higher levels of lithium intercalation, tetragonal symmetry is regained: Li(1.52(5))Y(2)Ti(2)O(5

262 The tetragonal symmetry of the dianionic template creates a

263 um intercalation into Y(2)Ti(2)O(5)S(2), the tetragonal symmetry of the host is retained: Li(0.30(5))

264 Rather, cation inversion creates a local tetragonal symmetry that extends over sub-nanometer doma

265 rly all mononuclear Mn(V)-oxo complexes have tetragonal symmetry, producing low-spin species.

266 ment, and B = boron) exhibit orthorhombic or tetragonal symmetry, with the only exception being hexag

267 , as these couple together to break the same tetragonal symmetry.

268 rization switching in prototypical BaTiO3 of tetragonal symmetry.

269 single-molecule magnet (SMM) in truly axial (tetragonal) symmetry.

270 piezoelectric d33 coefficient appears at the tetragonal (T) - orthorhombic (O) phase boundary rather

271 that Ca122 can be stabilized in two distinct tetragonal (T) phases at room temperature and ambient pr

272 perature range of 300 K-1.5 K, but induces a tetragonal (T) to an orthorhombic (OR) phase transition

273 tified the phase transition curves among the tetragonal (T), orthorhombic (O) and the collapsed-tetra

274 re-entant isotropic (I(re)), and a novel 3D tetragonal (Tet) phases.

275 Hexagonal hexaminophenyl benzene, tetragonal tetrakis(4-aminophenyl) ethane, and trigonal

276 very thin and epitaxially constrained to be tetragonal (that is, with four-fold symmetry), so one ex

277 We report a liquid crystal (LC) phase with a tetragonal three-dimensional unit cell containing 30 glo

278 structure and superconductivity in cubic and tetragonal TiH2.

279 This suggests a possible tetragonal to collapsed tetragonal phase transition.

280 factor causing the phase transition from the tetragonal to cubic phase near T(C) is a change in the s

281 ine the mechanism of the transition from the tetragonal to cubic phase.

282 I) induced a change of crystal symmetry from tetragonal to monlclinic, which could lead to an increas

283 y is suppressed and the lattice changes from tetragonal to monoclinic on cooling.

284 ion of paramagnetic to antiferromagnetic and tetragonal to orthorhombic structural transitions of "12

285 gap exists close to the transition from the tetragonal to orthorhombic structures (0.6 < x < 0.8).

286 ell parameters upon K content as well as the tetragonal to orthorhombic transition at low temperature

287 It is found that the tetragonal-to-cubic phase transition in YSZ at T > 900 d

288 BaTiO(3) to at least 330 degrees C, and the tetragonal-to-cubic structural transition temperature to

289 llic compound [Formula: see text] exhibits a tetragonal-to-orthorhombic phase transition consistent w

290 in-domains without uniaxial strain below the tetragonal-to-orthorhombic structural (nematic) transiti

291 ides, these competing phases are marked by a tetragonal-to-orthorhombic structural transition and a c

292 n equilibrium phase characterized by a large tetragonal unit cell containing 30 microphase-separated

293 complex phase is characterized by a gigantic tetragonal unit cell, in which 30 sub-2-nm quasispherica

294 n a and a 5% decrease in c parameters of the tetragonal unit cells, which results in disintegration o

295 agonal phase transformation, with only three tetragonal variants having only six twin systems, tuning

296 mation of an HfO2 nanorod from monoclinic to tetragonal, with a transformation temperature suppressed

297 ther compressed, undergoes a transition to a tetragonal Xe(N2)2-II phase at 14 GPa; this phase appear

298 Y-TZP (yttria-stabilized tetragonal zirconia polycrystal) is the most widely used

299 thacrylate-based resins to yttria-stabilized tetragonal zirconia polycrystals (Y-TZP) and further inv

300 etic semiconductor (Ba,K)F(Zn,Mn)As with the tetragonal ZrCuSiAs-type structure which is identical to