ライフサイエンスコーパス: single crystal

1 t one-kilogram sphere from a (28)Si-enriched single crystal.

2 n IrO2(110) epitaxially grown on a TiO2(110) single crystal.

3 olarization, was fabricated based on the BZA single crystal.

4 o a linearly connected zigzag pattern in the single crystal.

5 e number of silicon atoms in the core of the single crystal.

6 ply this method to characterize a CH3NH3PbI3 single crystal.

7 f layered graphitic carbon structures within single crystals.

8 3 unit cells thick and the surface of SrTiO3 single crystals.

9 rived either as a supramolecular hydrogel or single crystals.

10 e a few percent larger than that of the bulk single crystals.

11 als matches that of solid crystals, often of single crystals.

12 possess similar optoelectronic properties to single crystals.

13 rom methylammonium lead trihalide perovskite single crystals.

14 rmation of a dense forest of millimeter-long single crystals.

15 tting reminiscent of the tetragonal phase in single crystals.

16 ent of the surface energy of silicon carbide single crystals.

17 y silica gel chromatography and readily form single crystals.

18 e3 thin films grown on superconducting NbSe2 single crystals.

19 ce crystallography and chemistry of a LaAlO3 single crystal, a material mainly used as a substrate to

20 ) (PDI) self-assembled monolayer adsorbed on single-crystal Ag substrates at room temperature.

21 demonstrate that epitaxy can be used to grow single-crystal analogous materials as large-format elect

22 printed micrometer-scale polymer mounts for single crystal analysis have been prepared by photopolym

23 X-ray single-crystal analysis of four of the synthesized bipyr

24 ficiencies of approximately 20% for the bulk single crystals and 12% for the microscale crystals.

25 insulating substrates and could enable doped single crystals and crystalline substrates for a range o

26 isting of sulfur-deficient cobalt oxysulfide single crystals and nitrogen-doped graphene nanomeshes (

27 dated by reconstructing two stacked Co-Ni-Ga single crystals, and by comparison with a grain map obta

28 The obtained results promise new single crystal applications in ultrahigh-power transduce

29 ence and show that the optical properties of single crystals are almost identical to those of polycry

30 Both monomer and polymer single crystals are analyzed by X-ray diffraction, which

31 Large single crystals are grown using the vapor transport meth

32 However, for large scale applications single crystals are not suitable and it is essential to

33 free NiO prototype and NiO grown on Ni(110) single crystal as the one with defects.

34 eved by using different types of metal oxide single crystals as reference systems.

35 oelectric hysteresis from well-characterized single crystals at low temperature (still within the tet

36 annealed strontium titanate (SrTiO3, or STO) single crystals at room temperature.

37 ng process to fabricate high-quality organic single crystals, based on various semiconducting small m

38 Single-crystal-based field-effect transistor devices of

39 iaxial stress can convert polycrystalline or single-crystal benzene monomer into single-crystalline p

40 that it is indeed possible to create stable single-crystal blue-phase domains with the desired orien

41 here for preparation of stable, macroscopic single-crystal blue-phase materials.

42 allows for the formation of micrometer-scale single-crystal body-centered cubic gold nanoparticle sup

43 e ultrahard range (HV > 80 GPa) by examining single-crystal boron-doped diamond (BDD) with boron cont

44 nopatterned surfaces, leading to macroscopic single-crystal BP specimens where the dynamics of mesocr

45 Single-crystal BPs are shown to offer fertile grounds fo

46 l surfaces, especially on well-defined metal single crystals but also on other flat substrates such a

47 designated Form II, which can be isolated as single crystals, but converts very slowly at room temper

48 es of HOIPs and an inorganic perovskite (IP) single crystal by measuring nanoindentation creep and st

49 ing efficiency in hybrid perovskite with its single crystals by measuring the ratio of the re-emitted

50 EBSD measurements showed that, in principle, single crystals can be grown to unlimited lengths using

51 The emission color of the single crystals can be tuned readily from blue to red th

52 g the below-bandgap absorption of perovskite single crystals can narrow down their effective optical

53 Recent findings suggest that organic single crystals can provide spin-transport media with mu

54 eworks (MOFs): following a single-crystal to single-crystal cation metathesis, the Ca(2+) counterions

55 with irreversible microstructural damage in single-crystal, coarse-grained, ultrafine-grained and na

56 We report the successful growth of single crystals containing ferric enterobactin using rac

57 of the coefficient of thermal expansion of a single-crystal copper sample demonstrates that the metho

58 he dianion of the title compound, from which single crystals could be obtained and X-ray data acquire

59 e films are still significantly behind their single-crystal counterparts.

60 and {100} on nanocubes, are similar to their single-crystal counterparts.

61 The suitability of the 3D printed mounts for single crystal crystallography has been demonstrated thr

62 port the nontemplated colloidal synthesis of single crystal CsPbBr3 perovskite nanosheets with latera

63 echanochemical reaction produces macroscopic single crystals despite large dimensional changes caused

64 uous-breathing mechanism that was studied by single-crystal diffraction in a MOF with a diamondoid ne

65 ansition behavior of these materials through single-crystal diffraction measurements and demonstrate

66 by atomic-resolution scanning TEM (STEM) and single-crystal diffraction using synchrotron radiation.

67 Here we show single-crystal diffraction using ultrashort 90 keV HEX-

68 spectroscopy, ESI-MS spectrometry, and X-ray single-crystal diffractometry.

69 The capillary performance parameter within single crystal domain (K ij /R eff = 10(-3) to 10(-2) mi

70 Here we report single-crystal elasticity data on (Al,Fe)-bearing bridgm

71 face structure and the composition of the Cu single crystal electrodes were controlled over time.

72 These giant single crystals exhibit extraordinarily sharp photonic b

73 react under topochemical control to produce single-crystal extended solids.

74 The assembly of single-crystal FeGe2 nanowires with tetragonal C16 cryst

75 ical and physical investigations, microscale single-crystal fiber field-effect transistors were also

76 the structural and electronic properties of single crystal films.

77 We report the successful growth of a BZA single crystal for the first time in this study.

78 much weaker thermoelectric response than in single crystal form.

79 In this work, we report the fabrication of single crystal gallium phosphide thin films on transpare

80 Here we study spin injection in single-crystal gallium nitride nanowires and report robu

81 Finally, our single-crystal gallium nitride samples have a trigonal c

82 wafer-size flexible and transparent foils of single-crystal gold using silicon as a template.

83 ompleted, the IrMn layer contains very large single-crystal grains, with a large density of structura

84 readily prepared by pi-pi stacking two clean single-crystal graphene TEM grids, in which atomic-scale

85 east an order of magnitude to beyond that of single-crystal graphite.

86 oduce within glass a graded refractive index single crystal (GRISC) optically active waveguide.

87 on of chemical vapor transport (CVT), an old single-crystal growth technique, has been extended from

88 Relaxor ferroelectric single crystals have triggered revolution in electromech

89 The use of new silicon single crystals highly enriched in (28)Si recently produ

90 ve been reported for lead halide perovskites single crystals; however, ambiguities in basic propertie

91 on of super-swelled lipid bicontinuous cubic single crystals: (i) organic solvent drying speed, (ii)

92 onlinear I-V characteristics in Bi0.96Sb0.04 single crystals in the diffusive limit, which occurs onl

93 l additive became 50-300 nm, near-spherical, single crystals in the exhaust.

94 Single-crystal incremental heating provides leverage wit

95 By a thorough single-crystal inelastic neutron scattering study, we de

96 external efficiency approaching the level of single-crystal InP and CdSe.

97 he homoepitaxial growth of a metal halide on single crystals investigated with in situ reflection hig

98 We report the synthesis of single-crystal iron germanium nanowires via chemical vap

99 free-standing (BEDT-TTF)C60 charge-transfer single crystal is demonstrated.

100 t the trap density in CH3NH3PbBr3 perovskite single crystals is 10(15) cm(-3), only one order of magn

101 onductivity of Pb1-x Sn x Se (x = 0.23-0.25) single crystals is dominated by the surface states where

102 Here, the long-range order in rubrene single crystals is utilized to engineer organic-semicond

103 to a deterministic process, and to generate single-crystal joints with their c-axis orientation tail

104 questions, we have studied the behaviour of single-crystal La2-xSrxCuO4 films through which an elect

105 In this study the authors report a universal single crystal layer release process, called "3D spallin

106 rier protection mechanism by comparing three single-crystal lead bromide perovskites: CH3NH3PbBr3, CH

107 the optimal conditions for the formation of single crystal lines.

108 y is based on a controlled single-crystal to single-crystal linker exchange of 2-methylimidazole in Z

109 ng to elucidate the delithiation dynamics of single-crystal lithium iron phosphate microrods with lon

110 Here, we examine this proposal by growing single-crystal LSCO thin films with doping on both sides

111 Single-crystal magnetic hysteresis studies reveal the pr

112 ls can be transformed in a single-crystal-to-single-crystal manner.

113 ly inducing controlled defect complexes into single crystal materials.

114 Single-crystal measurements reveal opening up of the hys

115 Single-crystal, molecular orbital computations, and opti

116 By means of single crystal neutron diffraction and inelastic neutron

117 resistivity, ac magnetic susceptibility and single-crystal neutron diffraction measurements.

118 Single-crystal neutron diffraction shows that this downt

119 Time dependent plastic deformation in a single crystal nickel-base superalloy during cooling fro

120 hain charge transport based on an individual single crystal of conjugated polymers, and demonstrate t

121 magnetization measurements of a high quality single crystal of Cr1/3NbS2 over three magnetic field re

122 We used neutron scattering on single crystals of alpha-RuCl3 to reconstruct dynamical

123 scence and absorption spectra collected from single crystals of Bk(IO3)4 show evidence for doping wit

124 rmoelectric performance has been reported in single crystals of Ca3Co4O9.

125 roperties on an atomic level, we investigate single crystals of CH3NH3PbI3 with a narrow transition (

126 properties and energy absorption behavior of single crystals of four isostructural UiO-type MOFs unde

127 have investigated the electronic response of single crystals of indium selenide by means of angle-res

128 consequences, the electric field applied to single crystals of methylammonium lead bromide (CH3 NH3

129 Here, we synthesize single crystals of methylammonium lead bromide (CH3NH3Pb

130 The single crystals of tetragonal structure are easy to clea

131 Here we show that single crystals of thiolate-protected clusters can be gr

132 ein, we overcome these challenges and obtain single crystals of three zirconium phosphonates that are

133 Examination of PSE in UMCM-8 and single crystals of UiO-66 shows a similar trend, illustr

134 Here we show that single crystals of uranium dioxide subjected to strong m

135 low fields and positive at higher fields, in single crystals of VSe2.

136 , the compound undergoes a single-crystal-to-single-crystal one-electron reduction to give (Cp2Co)1.4

137 sity modulator based on Bi1:5Sb0:5Te1:8Se1:2 single crystal, one of the most insulating topological i

138 an transfer of sub-centimeter-sized graphene single crystals onto TEM grids to fabricate large-area a

139 resolution structures can be obtained from a single crystal or by merging data from multiple crystals

140 have been extensively studied in two forms: single-crystals or polycrystalline thin films.

141 bonds to each monomer and a lack of reactant single-crystal order.

142 For example, few single-crystal organic monomers react under topochemical

143 eff = 10(-3) microm), comparable to that of single crystals, overcomes hydraulic resistances through

144 ced, resulting in an efficiency of 17.8% for single crystal perovskite solar cells.

145 Single-crystal perovskite ferroelectric material is inte

146 ine the linear optical response of thin-film single-crystal perylene samples of distinct polymorphs i

147 fully dynamic atomistic simulations of bulk single-crystal plasticity in the body-centred-cubic meta

148 HMB-based single crystals prepared by simple cleaving method satis

149 amic force spectroscopy using nanoengineered single crystal probes reveals an attractive force with 6

150 A sample of a (28)Si-enriched single crystal produced to test the possibility of obtai

151 -defined, free-standing frames using polymer single crystals (PSCs) as the template.

152 films exhibited 3D growth on sapphire and 2D single-crystal quality on GaN, exhibiting substantial im

153 dow ranging from 0.0036 to 54 meV on a large single crystal sample, respectively.

154 axis) of magnetization were grown on a-plane single-crystal sapphire substrates by direct current mag

155 The single-crystal-to-single-crystal (scsc) synthesis of a 2D polymer based on

156 signals arising from the interface region of single-crystal semi-insulating GaAs that has been coated

157 Single crystal semiconductor nanomembranes (NM) are impo

158 to the outstanding electrical properties of single crystal semiconductors, there is great interest i

159 The 1D tubular ionic polymer observed in the single crystals should make it possible to understand th

160 This interferometer is fabricated from a single-crystal silicon cantilever on a transmission elec

161 When a WSe2 monolayer is placed on top of a single-crystal silver film, its emission into near-field

162 esponse of the methylammonium lead triiodide single crystal solar cells is extended to 820 nm, 20 nm

163 -crystals source and the double-nonlinearity single-crystal source, the orthogonal QPM superlattice i

164 urements were performed on URu2 - x Fe x Si2 single-crystal specimens in high magnetic fields up to 4

165 (1) H NMR spectroscopic titrations, ICP-MS, single-crystal structural analyses, and theoretical calc

166 of the uranyl(VI) ions as elucidated by the single-crystal structure of the gamma-ray irradiated mat

167 The single crystal structures of [Ir(ppy)2(L1)][PF6].1.5CH2C

168 Single crystal structures of model compounds representat

169 Single crystal structures of the high and low conducting

170 ional theory computed electronic structures, single crystal structures, and experimental lattice cohe

171 nocrystals with icosahedral, decahedral, and single-crystal structures are favored at sizes below 7 n

172 nd azimuth-dependent IRRAS data recorded for single crystal substrates has allowed for fundamental in

173 lms on large-format ( approximately 6 cm(2)) single-crystal substrates, and confirm epitaxial growth

174 liable, chemically clean approach to prepare single crystals suitable for accurate crystallographic a

175 f Pt remains uncertain, even for the Pt(111) single-crystal surface.

176 ochemistry of the triiodide anion (I3(-)) in single-crystal tetra-n-butylammonium triiodide using bro

177 tion of domains made it possible to identify single crystals that release up to three times more elec

178 lf-diffusion coefficients in natural olivine single crystals that were determined at upper mantle con

179 uctors, there is great interest in releasing single crystal thin films and fabricating flexible elect

180 be the structural and magnetic properties of single crystal thin-film YIG where the temperature depen

181 her exploration on magnetoelectric effect in single crystal/thin film specimens.

182 ere have been numerous studies of the rutile single-crystal TiO2(110) interface with water.

183 F) with tubular pores undergoes a reversible single crystal to single crystal transition between neut

184 report a dopant compensation in alloyed OIHP single crystals to overcome limitations of device noise

185 metal-organic frameworks (MOFs): following a single-crystal to single-crystal cation metathesis, the

186 The new strategy is based on a controlled single-crystal to single-crystal linker exchange of 2-me

187 The single-crystal-to-single-crystal (scsc) synthesis of a 2

188 hich these materials can be transformed in a single-crystal-to-single-crystal manner.

189 solution of Cp2Co, the compound undergoes a single-crystal-to-single-crystal one-electron reduction

190 e inserted into the superstructure through a single-crystal-to-single-crystal transformation.

191 e superstructure through a single-crystal-to-single-crystal transformation.

192 res undergoes a reversible single crystal to single crystal transition between neutral and anionic ph

193 Here, perovskite thin-single-crystal (TSC) photodetectors are fabricated with

194 less than 0.5% in CH3NH3PbI3 and CH3NH3PbBr3 single crystals under excitation intensity close to one

195 RE = Pr, Sm, Dy) compounds has been grown as single crystals via an indium flux.

196 tructures in As-doped CdTe using high-purity single crystal wafers to investigate the mechanisms that

197 A 66% spin polarization of the BZA single crystal was obtained by Andreev reflection spectr

198 of the MOF, triaxial impedance analyses on a single crystal was performed and confirmed bulk proton c

199 Studying YbMnO3 single crystals, we have confirmed that p-type conductio

200 Single crystals were efficiently grown for radical precu

201 Preformed poly(ethylene oxide) (PEO) single crystals were used as the template to direct the

202 Large ice single crystals were used to fabricate samples with the

203 2D MoS2 single crystals were utilized as the host material to em

204 in a Y-type hexaferrite Ba0.4Sr1.6Mg2Fe12O22 single crystal, which exhibits record-breaking direct an

205 migration in a model hybrid-perovskite thin single crystal, while the link with photoluminescence pr

206 junction across slightly n-type doped MAPbI3 single crystals with Au/MAPbI3/Ag configuration based on

207 of Mo2 C produces well-faceted, large-sized single crystals with low defect density, as confirmed by

208 Thin methylammonium lead triiodide single crystals with tuned thickness of tens of micromet

209 ading to the emergence of lipid bicontinuous single crystals with unprecedented swelling capacity.

210 Atomically thin single crystals, without grain boundaries and associated

211 udy, and electrical transport measurement of single crystal WSe2 in diamond anvil cells with pressure

212 Single crystal X-ray analysis revealed that these new po

213 ble tris-dentate ligand and characterized by single crystal X-ray analysis.

214 IR and NMR spectroscopic data as well as by single crystal X-ray analysis.

215 protected gold nanocrystal characterized by single crystal X-ray crystallography (sc-XRD), Au279(SPh

216 st characterization of an allenyl radical by single crystal X-ray crystallography is reported.

217 Single crystal X-ray diffraction (SC-XRD) is the princip

218 Single crystal X-ray diffraction (SCXRD) and electrospra

219 and UV-vis spectroscopies, ITC studies, and single crystal X-ray diffraction analyses.

220 /1, v/v) or dichloroethane (DCE), as well as single crystal X-ray diffraction analyses.

221 Single crystal X-ray diffraction analysis shows that hos

222 complexes were isolated and characterized by single crystal X-ray diffraction and/or NMR spectroscopy

223 2D NMR spectroscopic techniques and single crystal X-ray diffraction established the propose

224 The structures of 5 and 6 were confirmed by single crystal X-ray diffraction measurements.

225 mining the steps in the weaving process with single crystal X-ray diffraction, we find that the degre

226 , zero-field (57)Fe Mossbauer, magnetometry, single crystal X-ray diffraction, XAS, and EXAFS for 6.

227 ro-field (57)Fe Mossbauer, magnetometry, and single crystal X-ray diffraction.

228 obtained isomers were then established using single crystal X-ray diffraction.

229 as a molecular species and characterized by single crystal X-ray structure analysis.

230 The single crystal X-ray structure reveals that sodium selen

231 Single crystal X-ray structures of three of their radica

232 R spectra of all complexes as well as IR and single crystal X-ray studies were obtained to fully eluc

233 tion of the supporting phosphine ligands and single crystal X-ray/neutron diffraction are exploited i

234 e solid and solution state were confirmed by single-crystal X-ray analyses and their solution NMR and

235 rate (NaTFPB), theoretical calculations, and single-crystal X-ray analyses indicate that the conforma

236 ions in the new CD-MOF has been confirmed by single-crystal X-ray analysis by determining the vacanci

237 Single-crystal X-ray analysis of both SubPc-TCBD-aniline

238 Single-crystal X-ray analysis of the beta-heptakis(trifl

239 Single-crystal X-ray analysis revealed the nearly flat c

240 Single-crystal X-ray analysis reveals a beta-Keggin clus

241 Single-crystal X-ray analysis shows that the charged tra

242 ereochemistry of 3 was determined via 13a by single-crystal X-ray analysis.

243 Single-crystal X-ray characterization of cationic (alpha

244 by several spectroscopic methods, as well as single-crystal X-ray crystallography.

245 e oxide and two sultones were established by single-crystal X-ray crystallography.

246 Some key structures are determined using single-crystal X-ray crystallography.

247 terocyclic ring system was confirmed through single-crystal X-ray crystallography.

248 ter sorption were corroborated using in situ single-crystal X-ray diffraction (SCXRD) studies.

249 has been investigated in the solid state by single-crystal X-ray diffraction (XRD) and in solution u

250 d using a multitechnique approach, including single-crystal X-ray diffraction (XRD), gas-phase electr

251 MR, electronic circular dichroism (ECD), and single-crystal X-ray diffraction analyses.

252 Using single-crystal X-ray diffraction analysis (SCXRD), we sh

253 Both (1)H NMR spectroscopy and single-crystal X-ray diffraction analysis confirm the fo

254 Single-crystal X-ray diffraction analysis of the monomer

255 In situ single-crystal X-ray diffraction analysis was carried ou

256 omplex characterized by multinuclear NMR and single-crystal X-ray diffraction analysis.

257 racterized by different techniques including single-crystal X-ray diffraction and mass spectrometry.

258 100 GPa and temperatures over 2,500 K using single-crystal X-ray diffraction and Mossbauer spectrosc

259 Single-crystal X-ray diffraction and NMR studies support

260 We confirm its structure by single-crystal X-ray diffraction and show by (27) Al NMR

261 hallenge: Gas-phase electron diffraction and single-crystal X-ray diffraction are both established te

262 Single-crystal X-ray diffraction confirmed structures th

263 The modulated structure was refined from the single-crystal X-ray diffraction data with a superspace

264 Supported by Landau theory and single-crystal X-ray diffraction data, we re-evaluate th

265 ctural zinc frameworks obtained from in situ single-crystal X-ray diffraction experiments.

266 rized using NMR spectroscopy in solution and single-crystal X-ray diffraction in the solid state.

267 d [MS subsetm-CBPQT](4(+*)) were examined by single-crystal X-ray diffraction measurements and densit

268 Single-crystal X-ray diffraction of its tris(cobaltoceni

269 in Co2(m-dobdc) and Co2(p-dobdc) via in situ single-crystal X-ray diffraction reveal that the vast im

270 Single-crystal X-ray diffraction revealed a triclinic cr

271 Structural characterization by single-crystal X-ray diffraction reveals that these comp

272 Solid-state (13)C NMR spectra and single-crystal X-ray diffraction structures of the Zn an

273 As revealed by a single-crystal X-ray diffraction study, the first deprot

274 Both anions are characterized by single-crystal X-ray diffraction, (1)H and (13)C NMR, an

275 Single-crystal X-ray diffraction, accompanied by molecul

276 terized by UV-vis/fluorescence spectroscopy, single-crystal X-ray diffraction, and cyclic voltammetry

277 te by Raman spectroscopy and low-temperature single-crystal X-ray diffraction, and in the gas phase b

278 Using high-pressure (HP) single-crystal X-ray diffraction, density functional the

279 lysis of crystallographic data obtained from single-crystal X-ray diffraction, focusing on two featur

280 olid-state (super)structure, investigated by single-crystal X-ray diffraction, reveals the formation

281 @2gamma-CD@{Mo154} has been characterized by single-crystal X-ray diffraction, thus demonstrating the

282 tammetry, differential scanning calorimetry, single-crystal X-ray diffraction, transient absorption s

283 The structures of 3-5 are supported by single-crystal X-ray diffraction.

284 O2 (CF 3.190(9)-3.389(9) A), as confirmed by single-crystal X-ray diffraction.

285 The key structures were confirmed by single-crystal X-ray diffraction.

286 by multinuclear NMR spectroscopy as well as single-crystal X-ray diffraction.

287 d characterized by IR, UV-vis, EPR, NMR, and single-crystal X-ray diffractions.

288 V-vis-NIR absorption and MCD spectroscopies, single-crystal X-ray structure determination, vibrationa

289 Remarkably, the single-crystal X-ray structure of one atropisomer of eac

290 ing, transmission electron microscopy, and a single-crystal X-ray structure to show that heterometals

291 Knowledge of their single-crystal X-ray structures has been instrumental to

292 Single-crystal X-ray structures of 1-benzoyl-2-(perfluor

293 Single-crystal X-ray structures of complexes of the rece

294 This is a factor of 2.5 less than for single-crystal X-ray-diffraction-based structure determi

295 d on the basis of spectroscopic evidence and single crystal XRD results, indicates that the detection

296 Single-crystal XRD analysis reveals that POM:gamma-CD co

297 om the reduced symmetry in 7 as confirmed by single-crystal XRD analysis, we established that the gro

298 he hexol-type derivatives were determined by single-crystal XRD and NMR spectroscopy and confirmed th

299 the preparation method were characterized by single-crystal XRD, giving two crystal structures, a tri

300 High quality single crystal ZrSiS as a theoretically predicted Dirac