ライフサイエンスコーパス: single crystal

1 sized crystals, as a ceramic, and even as a single crystal.

2 ng a second-order phase transition in a bulk single crystal.

3 bserved by EPR using a slurry of small-sized single crystals.

4 that all shells in the heterostructures are single crystals.

5 imes the largest reported values in BaTiO(3) single crystals.

6 ng from 469 nm to 583 nm from ten individual single crystals.

7 challenging to grow n-type Mg(3) (Sb,Bi)(2) single crystals.

8 magnitude greater than that in high-quality single crystals.

9 ethod at room temperature to form inch sized single crystals.

10 rgence of superconductivity in undoped Ca122 single crystals.

11 imes the largest reported values in BaTiO(3) single crystals.

12 xist in both CH(3)NH(3)PbI(3) thin films and single crystals.

13 in solution, this compound forms homochiral single crystals.

14 re trianglimine macrocyclic host from gel to single crystals.

15 y networks of PBAs is the inaccessibility of single crystals(16).

16 The nanoribbons are atomically flat single crystals, aligned exclusively in the zigzag cryst

17 non has been explained on the basis of X-ray single-crystal analysis.

18 of monolayer high islands on the respective single crystal and (ii) to modify the step sites for ads

19 ropic kappa(L) value of the Cs(2)PbI(2)Cl(2) single crystal and observed an ultralow kappa(L) value o

20 technique, we harvest some centimeter-sized single crystals and achieved high device performance.

21 iplet annihilation in high-quality pentacene single crystals and anthradithiophene (diF-TES-ADT) thin

22 ng and visualising mosaicity within metallic single crystals and provides the foundation for post-mor

23 moreflectance measurements were performed on single crystals and thin films, and theoretical predicti

24 PTE and electron microscopy measurements of single-crystal and bicrystal gold microscale devices.

25 their crystal structures were determined by single-crystal and powder X-ray diffraction (space group

26 a combination of high-resolution synchrotron single-crystal and powder X-ray diffraction techniques.

27 e temperatures and which is characterized by single-crystal and powder X-ray diffraction.

28 fully characterized 1) in the solid state by single-crystal and powder XRD, IR, TGA, and solid-state

29 neration, we study structure and symmetry of single-crystal and thin-film samples.

30 e chemist, summarizes techniques for growing single crystals, and describes basic physical property m

31 anosheets, nano- or microplates, thin films, single crystals, and polycrystalline bulks), and advance

32 e-component MOF superlattices, binary MOF-Au single crystals, and two-dimensional MOF nanorod assembl

33 Flexible organic single crystals are evolving as new materials for optica

34 e high electronic and optical quality of the single crystals are required.

35 red up to 2.1 GPa in a diamond anvil cell on single crystals, are in excellent agreement, correlating

36 50 K, which compared diffraction data from a single crystal as Pb or after irradiation with blue ligh

37 e, we report the synthesis and structures of single-crystal (BA)(2)(A)Pb(2)I(7) where BA = butylammon

38 f a quenched FeRh thin film (25 nm) grown on single crystal barium titanate (BTO).

39 ere, a photoluminescence (PL) measurement of single-crystal BAs at different temperatures and pressur

40 ivity in a hexagonal perovskite chalcogenide single crystal, BaTiS(3), despite its highly symmetric a

41 graphene crystals for large area, that is, a single-crystal bilayer, and (AB-stacked) few-layer graph

42 conductivity exceeding 1000 W m(-1) K(-1) in single-crystal boron arsenide (BAs) has led to interest

43 r packing of Y6 not only exists in molecular single crystals but also in thin films.

44 anic frameworks (COFs) can be synthesized as single crystals by preparing COF particles as colloidal

45 rs, they were recently grown as micron-sized single crystals by temporally resolving the growth and n

46 Here we show that these alkali metals-as single crystals-can grow out of and retract inside the t

47 vely regulates the performance fade issue of single-crystal cathode and provides new insights for imp

48 Single-crystal cathode materials for lithium-ion batteri

49 For example, single-crystal CdTe and CdZnTe films that would take sev

50 to investigate bulk mosaicity within as-cast single crystal CMSX-4 and CMSX-10 Ni-base superalloys.

51 Ferroelectric domain walls in single-crystal complex oxide thin films are found to be

52 Single-crystal conductivity data are consistent with cha

53 To address the aforementioned issue, a single-crystal core-shell-shell "sandwich" structured UC

54 gnetic properties of thin (less than 100 nm) single crystal Cr(2)O(3) films on epitaxial V(2)O(3) buf

55 Single-crystal cryogenic X-ray diffraction at 6 K, elect

56 Here, we report the growth of freestanding single crystal CsPbBr(3) SCHPFs with thickness less than

57 uctural signatures: a distinct transition to single-crystal Cu(2)O cubes upon air exposure, low cryst

58 ve as the templates for producing high-index single-crystal Cu-based alloys.

59 Detailed mechanistic investigation from the single-crystal data indicates that the strain generated

60 ethod to determine the bulk temperature of a single crystal diamond sample at an X-Ray free electron

61 Furthermore, single crystal diffraction data obtained from oxidation

62 ombination of in situ synchrotron powder and single-crystal diffraction, infrared spectroscopy and mo

63 an example, thin films with millimeter-sized single-crystal domains and pure crystallographic orienta

64 y can be used practically, ranging from bulk single crystals (e.g., in gamma and X-ray detectors) to

65 tion of CO molecules at well-defined Pt(hkl) single-crystal electrode surfaces is a key step towards

66 ferroelastic transition of TIPS-P, flexible single-crystal electronic devices were obtained that can

67 s application is the difficulty in growing a single-crystal epitaxial film of cuprous halides.

68 We first demonstrate the single crystal epitaxy of high quality cuprous iodide (C

69 nvestigation of agostic interactions through single-crystal EPR spectroscopy.

70 ctrical conductivity and carrier mobility of single crystals exhibit a metallic behavior with a typic

71 The as-obtained ultrathin antimony oxide single crystals exhibit high dielectric constant (~100)

72 , and this enables fabrication of perovskite single-crystal FETs with high mobility of up to ~15 cm(2

73 ct on the growth rate of ultrathin CsPbBr(3) single-crystal film.

74 ificantly reduce the leakage of 300 nm thick single crystal films.

75 ion-controlled growth of epitaxial Sr(3) SnO single-crystal films by molecular-beam epitaxy (MBE).

76 ly small amount of precursor to render large single-crystal flakes, which usually causes low coverage

77 been synthesized in both polycrystalline and single crystal form, and their structural and magnetic p

78 offers a practical means to keep 3D-printed single crystals from cracking due to unrelieved residual

79 (mutau) product, tunable bandgap and simple single crystal growth from low-cost solution processes.

80 Through a combination of single crystal growth, experiments involving in situ dep

81 bservations that, in the formation of 2D COF single crystals, growth dominates over nucleation when m

82 It is extremely challenging to grow single-crystal halide perovskite films (SCHPFs) with not

83 conduction along different directions of the single crystal has the potential to impact a broad range

84 Thus, a reliable way of growing single-crystal hBN films directly on wafers would contri

85 Recent studies have shown the growth of single-crystal hBN films on molten gold surfaces(4) or b

86 we report the successful epitaxial growth of single-crystal hBN monolayers on a Cu (111) thin film ac

87 Growing single-crystal hBN on such high-symmetry surface planes

88 s reliable approach to producing wafer-scale single-crystal hBN paves the way to future 2D electronic

89 The obtained single-crystal hBN, incorporated as an interface layer b

90 The transferred single-crystal hybrid perovskites are of comparable qual

91 l-growth-and-transfer method for fabricating single-crystal hybrid perovskites on arbitrary substrate

92 hes focus on polycrystalline materials(5-7), single-crystal hybrid perovskites show improved carrier

93 Devices based on these single-crystal hybrid perovskites show not only high sta

94 However, the fabrication of single-crystal hybrid perovskites, and controlling their

95 a challenge to prepare large-area high-index single crystals in a controllable and cost-efficient man

96 Here we exploit state-of-the-art single-crystal inelastic neutron scattering to directly

97 The nucleation and growth of macroscopic single crystals is demonstrated by using the Debye scree

98 tion in MAPbI(3) , MAPbBr(3) , and FAPbBr(3) single crystals, is proven through D/H NMR quantificatio

99 , (110), and (111) orientation, deposited on single crystal LaAlO(3) substrates, were investigated us

100 we report a facile method to disassemble vdW single crystals layer by layer into monolayers with near

101 We demonstrate the growth of single-crystal layers of hexagonal boron nitride (BN) an

102 ven in high-quality, electrically insulating single crystals, leading to anomalous transport properti

103 Here, we present methods to deposit single-crystal material at rates 2-3 orders of magnitude

104 , after being cycled at high voltages, these single-crystal materials exhibit severe structural insta

105 a promising path to engage the fiber-shaped single-crystal materials in applications from 1D fiber d

106 Previous theoretical studies predict that single crystals Mg(3) (Sb,Bi)(2) can exhibit higher ther

107 can be used to reshape, resize and relocate single-crystal microwaveguides in order to attain spatia

108 ng molecular-beam epitaxy (MBE), a series of single crystal Mn(x) Fe(3-) (x) O(4) thin films with con

109 Here, 2D ultrathin single-crystal molybdenum oxide (MoO(2) ) flakes that ex

110 f high-throughput techniques for exfoliating single-crystal monolayers with sufficient size and high

111 olidification conditions on the variation in single crystal mosaicity was investigated.

112 the electrical transport of Fe(4+delta)Se(5) single-crystal nanowires exhibiting 5 x 5 Fe-vacancy ord

113 Hydride positions in 1 were confirmed by single-crystal neutron diffraction.

114 Single crystal Ni-based superalloys have long been an es

115 f only 3 wt.% Re in the second generation of single crystal Ni-based superalloys which almost doubled

116 Single crystals obtained from the sol state show that na

117 ttice thermal conductivity (kappa(L)) in the single crystal of all-inorganic layered Ruddlesden-Poppe

118 e study of vortex dynamics in a high-quality single crystal of HgBa(2)CuO(4+delta), a highly anisotro

119 tudies the cathodic corrosion of a spherical single crystal of platinum in an aqueous alkaline electr

120 scattering measurements on a superconducting single crystal of Sr(0.1)Bi(2)Se(3), a prime candidate f

121 Large single crystals of a constitutionally isomeric COF (BP-C

122 efore, uniaxial pressure necessary to detwin single crystals of BaFe(2)As(2) actually rotates the eas

123 microscale were space-filling, comparable to single crystals of geologic aragonite.

124 Here, growth of large single crystals of metal-free halide perovskite DABCO-NH

125 asily detachable template molecule, yielding single crystals of MUV-3.

126 al flux as a synthetic route to high quality single crystals of novel intermetallic subchalcogenides

127 flux to synthesize large (millimeter scale) single crystals of novel subchalcogenide materials.

128 Like silicon, single crystals of organic semiconductors are pursued to

129 ave recently been synthesized by irradiating single crystals of suitably packed monomers.

130 Electric measurements of single crystals of the MV salts show a semiconducting be

131 When exposed to UV light, single crystals of the vinyl azides 3-azido-1-phenylprop

132 Here we report the growth of single crystals of various PBAs and the measurement and

133 Single crystals of Znby were produced, providing the fir

134 yclic voltammetry, transient absorption, and single-crystal OFET measurements.

135 e the way for high-performance ultraflexible single-crystal organic electronics for sensors, memories

136 s employed to recrystallize the SnSe core to single-crystal over the entire fiber.

137 2PA-PL spatial mappings over large areas of single crystal platelets demonstrate the co-existence of

138 repair, restore, and reshape any superalloy single-crystal product.

139 ion, anhydrous atmosphere proton-conduction, single-crystal proton-conduction, and including MOF-base

140 impurity scattering in Te-doped Mg(3) Sb(2) single crystals proves that the thermally activated mobi

141 size high-quality Cs(3)Bi(2)I(9) perovskite single crystals (PSCs).

142 uinone, proceeding through single-crystal-to-single-crystal reactions.

143 nating this grain boundary resistance in the single crystals results in a large enhancement of the we

144 Single-crystal results demonstrate that the crystals obt

145 nd experimental studies demonstrate that the single-crystal rock-salt SnSe fibers possess high thermo

146 0.8% for a powder sample and 98% for a large single crystal sample is achieved.

147 solvate, AcMe@G(2) BDS, by single-crystal-to-single-crystal (SC-SC) desolvation, and exhibits a Type

148 n the gray area of a clean single-crystal-to-single-crystal (SCSC) transformation and violent PS effe

149 eed of 4155 m s(-1), comparable to GaAs, but single crystals show very low lattice thermal conductivi

150 We achieve this stress by bending single-crystal silicon microbeams using an in situ therm

151 method is demonstrated to achieve ultralong single-crystal SnSe wire with rock-salt structure and hi

152 4) ], was synthesized by a single-crystal to single-crystal solid/gas hydrogenation from a norbornadi

153 crystallographic orientation mapping of bulk single crystal specimens with good spatial resolution.

154 The single-crystal SrTiO(3) (001) has two different surface

155 and its crystal structure was determined via single crystal structural analysis.

156 IR, mass, and elemental analyses, including single-crystal structural studies.

157 polymorphs of the benchmark compound ROY as single crystals structurally characterized by X-ray diff

158 The single crystal structure of the CAM-Ag nanofibers is sol

159 The dehydrated single-crystal structure of Mg-CUK-1L confirms retention

160 The fabricated silver nanorods show single-crystal structure with a low resistivity of 8.58

161 all display negative curvature according to single crystal structures.

162 An analysis of the single-crystal structures reveals that the incorporation

163 Photophysical studies, single-crystal structures, and theoretical calculations

164 wn on SrRuO(3) (SRO) buffered SrTiO(3) (STO) single crystal substrate by optimized pulsed laser depos

165 epitaxial V(2)O(3) buffered Al(2)O(3) (0001) single crystal substrates.

166 ns is that very slow deposition on expensive single-crystal substrates yields high crystalline qualit

167 a mechanical deformation of plastic organic single crystals such as bending results in a small yet s

168 Studies using single crystals suggest a polycrystalline surface should

169 lecules by immersion in hot melts, providing single crystals suitable for X-ray diffraction.

170 (MCTPQT(6+) ) were prepared and their X-ray single-crystal (super)structures reveal intricate three-

171 Three X-ray single-crystal superstructures-KAu(CN)(2)Calpha-cyclodex

172 more detailed studies on single molecules or single crystal surfaces.

173 N), up to 25 and 30 GPa, respectively, using single-crystal synchrotron X-ray diffraction, infrared s

174 ons was observed for the first time based on single-crystal synchrotron X-ray experiments (100-450 K)

175 A comprehensive study using a combination of single crystal/synchrotron powder X-ray diffraction, sol

176 ic properties of n-type Te-doped Mg(3) Sb(2) single crystals, synthesized by a combination of Sb-flux

177 is difficult to elucidate in the absence of single crystals that are suitable for X-ray diffraction.

178 plied to the Y(1-x)Pr(x)Ba(2)Cu(3)O(7-delta) single crystal, the pseudogap increases as dlnDelta*/dP

179 on(14-20), NdNiO(2) and Nd(0.8)Sr(0.2)NiO(2) single-crystal thin films are synthesized by reducing th

180 rained epitaxial growth of halide perovskite single-crystal thin films on lattice-mismatched halide p

181 Single-crystal tin selenide (SnSe), a record holder of h

182 to TiO(2) surfaces (either nanostructured or single-crystal TiO(2)(110)) was found to be highly depen

183 ilor the size and shape of peptide-based MOF single crystals to specific applications.

184 bornane)][BAr(F) (4) ], was synthesized by a single-crystal to single-crystal solid/gas hydrogenation

185 PCH(2) PCy(2) )(NBD)][BAr(F) (4) ] occurs in single-crystal to single-crystal transformations.

186 g N(2)-released structures were observed via single-crystal-to-crystal transformation, suggesting for

187 from its acetone solvate, AcMe@G(2) BDS, by single-crystal-to-single-crystal (SC-SC) desolvation, an

188 is example falls in the gray area of a clean single-crystal-to-single-crystal (SCSC) transformation a

189 ichloro-1,4-benzoquinone, proceeding through single-crystal-to-single-crystal reactions.

190 the crystals can undergo guest exchange in a single-crystal-to-single-crystal transformation generati

191 ization of the bridging DTE ligand induces a single-crystal-to-single-crystal transformation that can

192 The phototriggered guest release occurs in a single-crystal-to-single-crystal transformation that is

193 HEP-7, which upon heating in air undergoes a single-crystal-to-single-crystal transformation to gener

194 al Li-ion insertion and extraction to induce single-crystal-to-single-crystal transformations in a tu

195 ndergo guest exchange in a single-crystal-to-single-crystal transformation generating a series of iso

196 dging DTE ligand induces a single-crystal-to-single-crystal transformation that can be monitored usin

197 guest release occurs in a single-crystal-to-single-crystal transformation that is in the absence por

198 heating in air undergoes a single-crystal-to-single-crystal transformation to generate Gd-IHEP-8.

199 n and extraction to induce single-crystal-to-single-crystal transformations in a tunnel-structured V(

200 D)][BAr(F) (4) ] occurs in single-crystal to single-crystal transformations.

201 Moreover, we identify vapor-induced single crystal transitions that are reversible and respo

202 The repair of damaged Ni-based superalloy single-crystal turbine blades has been a long-standing c

203 centimeter-sized layered [Formula: see text] single crystals under high oxygen pressures of 120-150 b

204 ferroelectric phase in a Y-type hexaferrite single crystal up to 450 K, and demonstrated the reversa

205 a comprehensive structural study of the PFWO single crystals using a combination of synchrotron X-ray

206 e have studied the spin splitting in 2D-PEPI single crystals using the circular photogalvanic effect

207 The trap densities in single crystals varied by five orders of magnitude, with

208 hesize high-quality ultrathin antimony oxide single crystals via a substrate-buffer-controlled chemic

209 behaviour of two types of lead-iodide based single crystals, we here highlight the extrinsic origin

210 e-correlated single photon counting to study single crystals, we show that the white-light emission d

211 crystal created different domains inside the single crystal, which multiplied the already developed s

212 ehind a damage-free and residual-stress-free single crystal with uniform gamma ' precipitates indisti

213 e Cu foils are successfully transformed into single crystals with a series of high-index facets, rely

214 lar, we demonstrate formation of the largest single crystals with controlled nonequilibrium shapes of

215 The method can prepare macroscopic bulk single crystals with other block copolymer systems, sugg

216 Single crystal X-ray crystallography showed that in some

217 Single crystal X-ray crystallography shows that the mono

218 , (Py)Cn(*), and 1.1/2MeOH were confirmed by single crystal X-ray crystallography, EPR spectroscopy,

219 Single crystal X-ray diffraction analysis and micro Rama

220 Single crystal X-ray diffraction analysis of the metal-o

221 nal space group I4 2m was solved by means of single crystal X-ray diffraction as a 6-component twin d

222 The article will show that single crystal X-ray diffraction based on both Bragg and

223 Single crystal X-ray diffraction studies indicate that Z

224 se solid-state structures were elucidated by single crystal X-ray diffraction studies.

225 e complexes (1 and 2) was substantiated with single crystal X-ray diffraction study.

226 NMR, FT-IR, UV-vis, MALDI-TOF spectral data, single crystal X-ray diffraction, and CHN elemental anal

227 nuclear NMR spectroscopy, mass spectrometry, single crystal X-ray diffraction, and DFT studies.

228 e structure of GTUB5 was characterized using single crystal X-ray diffraction.

229 this pentametallic assembly was confirmed by single crystal X-ray investigation.

230 3-dipolar cycloadditions, were elucidated by single crystal X-ray, visible-near infrared (vis-NIR) sp

231 material was confirmed by powder (PXRD) and single-crystal X-ray (SC-XRD) diffraction.

232 us stereocenters is observed on the basis of single-crystal X-ray analyses of the intermediates and d

233 Single-crystal X-ray analyses on MOF-1 showed that Cu(+2

234 Single-crystal X-ray analysis indicated that POP-oNH(2)

235 Single-crystal X-ray analysis shows that the finely arra

236 In addition, single-crystal X-ray analysis was used to elucidate the

237 the two product types was corroborated by a single-crystal X-ray analysis.

238 ese compounds was unambiguously confirmed by single-crystal X-ray analysis.

239 ructures determined through a combination of single-crystal X-ray and neutron diffraction reveal an A

240 Detailed insights from single-crystal X-ray and solution structures of Hby have

241 Single-crystal X-ray crystallographic analysis shows tha

242 solute configuration of 1 was established by single-crystal X-ray crystallographic analysis using Cu

243 e fully characterized using a combination of single-crystal X-ray crystallography and paramagnetic (1

244 Its structure, determined using single-crystal X-ray crystallography, shows that quantum

245 molecular structures are fully elucidated by single-crystal X-ray crystallography.

246 product was obtained, which was confirmed by single-crystal X-ray crystallography.

247 spectroscopically and, in many cases, using single-crystal X-ray crystallography.

248 Synchrotron single-crystal X-ray data (100 K) allowed the resolution

249 Single-crystal X-ray diffraction analyses reveal planar

250 y radiation damage, especially as Pg, during single-crystal X-ray diffraction analyses, which could c

251 -allene was determined for the first time by single-crystal X-ray diffraction analysis and nOe NMR ex

252 spectroscopic techniques in conjunction with single-crystal X-ray diffraction analysis.

253 Like recently reported SrB(3) C(3) ,([1]) single-crystal X-ray diffraction and computational model

254 The structure, solved using high-temperature single-crystal X-ray diffraction and confirmed by high-t

255 Single-crystal X-ray diffraction and gas chromatography

256 The compounds have been characterized by single-crystal X-ray diffraction and have the formulas [

257 Single-crystal X-ray diffraction and resonant ultrasound

258 complex, which has been characterized using single-crystal X-ray diffraction and X-ray absorption, N

259 Here single-crystal X-ray diffraction and X-ray pair distribu

260 In this work, NMR crystallography and single-crystal X-ray diffraction are combined for the co

261 ced helicene 1(2-) has been characterized by single-crystal X-ray diffraction as a solvent-separated

262 graphically refined crystal structures using single-crystal X-ray diffraction data reveal that the di

263 rystallised and their structure confirmed by single-crystal X-ray diffraction determination, as well

264 High-pressure single-crystal X-ray diffraction has been used to trap b

265 Single-crystal x-ray diffraction of 2 and 3 revealed fou

266 Single-crystal X-ray diffraction reveals that the MA, FA

267 Single-crystal X-ray diffraction reveals that Y6 molecul

268 Single-crystal X-ray diffraction studies reveal that the

269 Herein, based on results of in situ single-crystal X-ray diffraction studies up to 27 GPa, w

270 A combination of single-crystal X-ray diffraction studies, solution and s

271 mation of the imine product was achieved via single-crystal X-ray diffraction studies.

272 Here we present a single-crystal X-ray diffraction study of solid hydrogen

273 ystal structure has been also obtained using single-crystal X-ray diffraction techniques.

274 erando powder X-ray diffraction, we leverage single-crystal X-ray diffraction to identify the sequenc

275 3gamma -> 3delta transitions are reversible (single-crystal X-ray diffraction), and the 3gamma -> 3de

276 After framework identification by single-crystal X-ray diffraction, 1D and 2D solid-state

277 Single-crystal X-ray diffraction, alongside in situ fluo

278 was probed by multinuclear NMR spectroscopy, single-crystal X-ray diffraction, and DFT computations.

279 = 7), and confirm the crystal structure with single-crystal X-ray diffraction, and provide indirect e

280 s were characterized by NMR in solution, MS, single-crystal X-ray diffraction, and variable-temperatu

281 elded microcrystals that were unsuitable for single-crystal X-ray diffraction, but ideal for MicroED.

282 A combination of gas adsorption analysis, single-crystal X-ray diffraction, magnetic susceptibilit

283 bicenes were comprehensively investigated by single-crystal X-ray diffraction, NMR spectroscopy, UV-v

284 ted and characterized by elemental analysis, single-crystal X-ray diffraction, UV/Vis absorption, cyc

285 nd is structurally characterized by means of single-crystal X-ray diffraction, which reveals the pres

286 hemical oxidant and fully characterized with single-crystal X-ray diffraction, X-ray absorption spect

287 to be an orthorhombic space group (Pbam) by single-crystal X-ray diffraction.

288 s from atomic-level structures obtained with single-crystal X-ray diffraction.

289 f (1)H and (13)C NMR spectrometry as well as single-crystal X-ray diffraction.

290 d spectroscopy, X-ray powder diffraction and single-crystal X-ray diffraction.

291 ation by (15) N NMR and IR spectroscopy, and single-crystal X-ray diffraction.

292 sly established by both NMR spectroscopy and single-crystal X-ray diffraction.

293 Despite its unusual molecular size, single-crystal X-ray structural analysis (resolution 0.9

294 phortriamide co-crystal is described and its single-crystal X-ray structure shows short HaBs between

295 Single-crystal X-ray structures of Re[Cl(8)TpCF(3)PC](O)

296 s of solution phase isomer distributions and single-crystal X-ray structures reveals that isomer pref

297 Single-crystal X-ray structures were determined for all

298 A set of techniques such as single-crystal X-ray, dynamic light scattering (DLS), el

299 leates has been unambiguously established by single-crystal XRD studies.

300 remely bright-50 times brighter than that of single-crystal ZnO, a direct-gap semiconductor that has