ライフサイエンスコーパス: tetragonal

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

2 near or trigonal, whereas CuII prefers to be tetragonal.

3 The family of ten isomorphous tetragonal A-DNA octamers provides a unique opportunity

4 .1 GPa) and 45 +/- 5 GPa for Xe clathrate B (tetragonal, a = 8.320 +/- 0.004 A, c = 10.287 +/- 0.007

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

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

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 it may influence the equilibrium between the tetragonal and the orthorhombic forms of isocitrate dehy

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

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 Therefore, the tetragonal arrangement of MIP observed in both plasma me

22 ogenous protein oxygen ligand in a distorted tetragonal array.

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

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

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

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

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

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

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

34 y crystallography for 1 reveals the shortest tetragonal C-S bond on record (1.771 A).

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

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

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

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

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

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

41 dyl termini, meant to be used as trigonal or tetragonal connectors for the construction of large mole

42 ovalent attachment of the heme and its fixed tetragonal coordination geometry, cytochrome c folding c

43 stroms in diameter, and ASU-32, based on the tetragonal CrB4 network, contains channels with a minimu

44 ion anisotropy for V(3+) ion residing in the tetragonal crystal field.

45 tructure was first solved to 3.4 A using the tetragonal crystal form and a three-wavelength Se-Met mu

46 here has been determined from monoclinic and tetragonal crystal forms.

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

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

49 The tetragonal crystal system is conserved during this trans

50 Tetragonal crystals are obtained with improved diffracti

51 Tetragonal crystals contained a pentamer of dimers in th

52 -g-g-c-g-c-c-3') and crystallized, producing tetragonal crystals that diffract to 2.3 A resolution.

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 e spherical beads having a range of lattices-tetragonal, cubic, and hexagonal-using hierarchical self

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

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

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

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

69 metric parameters, including the presence of tetragonal distortion in the FdI cluster common to this

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 ibes a new approach for making face-centered tetragonal (fct) FePt nanoparticles with a diameter of 1

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

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

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 bacteria forms from nonmagnetic mackinawite (tetragonal FeS) and possibly from cubic FeS.

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

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

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

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

90 ed and compared to the previously determined tetragonal form (space group P43212).

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

92 between the two substrates reported for the tetragonal form indicates that it is probably not in an

93 genase is related to the previously reported tetragonal form largely by an approximately 16 degrees s

94 P), the triclinic B form of Ni(II)(OEP), the tetragonal form of Ni(II)(OEP) and Zn(II)(OEP); five-coo

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

96 olume increase by 2% relative to the dimeric tetragonal form.

97 While the tetragonal forms exhibit only an incipient antiferromagn

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

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

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

101 X-ray structure of 2 reveals a 6-coordinate, tetragonal geometry with one nitrogen donor of an asymme

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

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

104 de ions, present in the crystal structure of tetragonal hen egg-white lysozyme through the substituti

105 Using solely a native crystal of tetragonal hen egg-white lysozyme, a protein of 14 kDa m

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

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

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

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

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

111 The perforation obeys a tetragonal instead of hexagonal symmetry.

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

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

114 -isopropylmalate dehydrogenase than does the tetragonal isocitrate dehydrogenase conformation.

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

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

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

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

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

120 from the initial monoclinic structure to the tetragonal lattice.

121 crystalline order were obtained, adopting a tetragonal lattice.

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

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

124 e microstructure of the specimens containing tetragonal leucite was characterized by twinned leucite

125 -CD(3)-labeled samples are consistent with a tetragonal ligand environment of three nitrogens and one

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

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

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

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

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

131 emperature, and pH on the nucleation rate of tetragonal lysozyme crystals.

132 acidic solutions that lead to the growth of tetragonal lysozyme crystals.

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

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

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

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

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

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

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

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

141 the most open of the three models while the tetragonal model is the most closed.

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

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

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

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

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

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

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

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

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

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

152 1,2,2-tetrachloroethane) crystallizes in the tetragonal P4/n space group and the structure has been s

153 12(1)) is nonsuperconducting and undergoes a tetragonal (P4/nmm) to monoclinic (P2(1)/m) structural t

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

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 hase to the chemically ordered face-centered tetragonal phase and transforms the nanoparticle superla

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

191 suggests a possible tetragonal to collapsed tetragonal phase transition.

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

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

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

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

196 a dominant factor for destabilization of the tetragonal phase.

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

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

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

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

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

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

203 The tetragonal polymorph determined at ambient pressure tran

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

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

206 0 degrees platinum metal complex (3) affords tetragonal prisms (4) as single products.

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

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

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

210 porphyrins, bringing the layers into strict tetragonal register.

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

212 ormed at 6 degrees C on bipyramidally tipped tetragonal rod-shaped NPL crystals revealed large micron

213 and firing, leucite transformed into either tetragonal rubidium leucite or cubic cesium leucite.

214 The diskettes are determined to be tetragonal SnO structure (P4/nmm), with their flat surfa

215 nchrotron radiation source, a crystal with a tetragonal space group diffracted to a resolution of 2.6

216 e group P1, monoclinic space group C2/c, and tetragonal space group I4(1)/a, respectively.

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

218 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

219 The protein crystallized in the tetragonal space group P4(1)2(1)2, with one molecule per

220 isomorphous to the all IC counterpart in the tetragonal space group P4(1)22 (a = b = 28.03 A, c = 58.

221 The RNA duplex crystallized in the tetragonal space group P4(1)22 with two independent mole

222 They belonged to the tetragonal space group P4(2)2(1)2, with cell parameters:

223 space group P2(1), and 2 crystallized in the tetragonal space group P4(3).

224 eviously characterized crystal belong to the tetragonal space group P4(3)2(1)2 (a = b = 88.6 A, c = 1

225 The crystals belong to the tetragonal space group P4(3)2(1)2, with unit cell dimens

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

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

228 The crystals belong to the tetragonal space group P42212 and have large unit cell d

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

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

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

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

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

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

235 Epitaxial tetragonal SrTiN2 films have been successfully prepared

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

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

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

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

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

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

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

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

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

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

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

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

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

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

250 of optically isotropic cubic phase into the tetragonal structure.

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

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

253 eveal a trimeric oligomer as observed in the tetragonal structure; this appears to be a unique featur

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

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

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

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

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

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

260 Surprisingly, such sparse tetragonal superstructure exhibits much higher thermosta

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

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

263 The pure protein OlpA, has a tetragonal symmetry of its morphological subunits.

264 The tetragonal symmetry of the dianionic template creates a

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

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

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

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

269 rization switching in prototypical BaTiO3 of tetragonal symmetry.

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

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

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

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

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

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

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

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

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

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

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

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

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

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

288 Tetragonal UCSB-8 has an unusually large cage built from

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

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

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

292 Outside the active site cleft a tetragonal volume of density was identified as a sulfate

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

294 mesophase transformation (from hexagonal to tetragonal) within the film.

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

296 h the I-band to their anchoring sites in the tetragonal Z-band lattice.

297 ss-infiltrated alumina and yttria-stabilized tetragonal zirconia polycrystal (Y-TZP).

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