ライフサイエンスコーパス: solid state

1 near-infrared to visible frequencies in the solid state.

2 ion maxima ranging from 474 to 495 nm in the solid state.

3 dicating the formation of a unique amorphous solid state.

4 d charge-transfer-dynamic modulations in the solid state.

5 en-bond-acceptor molecule synthesized in the solid state.

6 erties are observed in MeCN solution and the solid state.

7 ation of Fe(3+) at the alkylated site in the solid state.

8 ds in solution and fluoresce strongly in the solid state.

9 rly all relevant decoherence channels in the solid state.

10 ed mechanism, modulated electrochemically in solid-state.

11 single-crystal and powder XRD, IR, TGA, and solid-state (1) H and (13) C NMR spectroscopy, 2) in sol

12 ng-dependent TFT properties; high-resolution solid-state (1)H, (71)Ga, and (115)In NMR spectroscopy;

13 orientations on membranes were determined by solid-state (15)N NMR data.

14 Using solid-state (15)N NMR spectroscopy, the cis/trans isomer

15 idate its binding mode using two-dimensional solid-state (19)F NMR spectroscopy in conjunction with d

16 single-crystal X-ray diffraction, 1D and 2D solid-state (19)F NMR spectroscopy supported by ab initi

17 By dynamic solid state (2)H NMR measurements, using deuterium-label

18 lations are oriented on glass substrates and solid-state (31) P NMR spectroscopy is shown to be highl

19 yelectrolytes as anion-exchange membranes in solid-state alkaline fuel cells.

20 A solid-state analogy of solvation is polaron formation, b

21 rameworks are highly luminescent even in the solid state and exhibit topology-dependent pai transmiss

22 eterocycles are blue fluorescent in both the solid state and in solution with ca. 2700-8400 cm(-1) St

23 ew receptor forms inclusion complexes in the solid state and in solution, showing a dependence of the

24 y restricted two-layer structure both in the solid state and in solution.

25 r long lifetime and diffusion length in both solid-state and solution phase systems, and to their app

26 dicals, and these species exhibit remarkable solid-state and solution stability.

27 d 2 (no interaction) < 1 < 3 < 4 both in the solid-state and solution.

28 dynamic equilibria occur easily, even in the solid state, and are sensitive to electronic and steric

29 However, leading solid-state approaches function only at temperatures bel

30 Optically-interfaced spins in the solid state are a promising platform for quantum technol

31 Activation energies for bond exchange in the solid state are lower for networks incorporating flexibl

32 of the pyrimidines in both solution and the solid state are reported, along with computational model

33 ded ample evidence for the importance of the solid-state arrangement on the porosity and analyte upta

34 r centres in diamond have emerged as leading solid-state 'artificial atom' qubits(2,3) because they e

35 tion of a derivatized ferrocene anion in the solid state as part of an isostructural family of 3d met

36 Finally, the solid-state associations were also stabilized by multice

37 B(NDippCH)(2) }](2) , which is stable in the solid state at room temperature for extended periods (48

38 one adducts show red-shifted emission in the solid state, attributable to the charge-transfer charact

39 We instead employed a solid-state avalanche photodiode (APD)-based detector fo

40 remendous progress in the development of all-solid-state batteries (ASSBs).

41 e particles for electrochemical reactions in solid-state batteries and provides crucial insights into

42 Solid-state batteries are a proposed route to safely ach

43 Solid-state batteries enabled by solid-state polymer ele

44 tes (SSEs) as the most critical component in solid-state batteries largely lead the future battery de

45 of the initial discrete interfacial contact, solid-state batteries may still display homogeneous lith

46 Solid-state batteries with desirable advantages, includi

47 gies: Na-ion batteries, K-ion batteries, all-solid-state batteries, and multivalent batteries.

48 Interfacial issues commonly exist in solid-state batteries, and the microstructural complexit

49 onductors are critical to the development of solid-state batteries.

50 omising inorganic solid electrolytes for all-solid-state batteries.

51 des a new design strategy for other types of solid-state batteries.

52 garnet-type solid-state electrolytes and all solid-state batteries.

53 ndidate as the anode for high-energy-density solid-state batteries.

54 -state polymer electrolytes for high-voltage solid-state batteries.

55 lasses are promising electrolytes for use in solid-state batteries.

56 ufacturing and applications of sulfide-based solid-state batteries.

57 the application of a lithium metal anode in solid-state batteries.

58 rtion at electrode/electrolyte interfaces in solid-state batteries.

59 future development of solid electrolytes and solid-state batteries.

60 ign and manufacturing of high energy density solid-state batteries.

61 lyte and its application in various types of solid-state battery concepts (e.g., Li-ion, Li-S, and Li

62 compounds were fully characterized 1) in the solid state by single-crystal and powder XRD, IR, TGA, a

63 d by comparing in vivo results for a digital solid-state cadmium-zinc-telluride SPECT/CT system with

64 measurements using (99m)Tc-tetrofosmin and a solid-state cardiac camera.

65 utilised to analyse dendritic growth in all-solid-state cells.

66 Solid state chemical analysis of pharmaceutical inhalati

67 ts related to solids from the viewpoint of a solid-state chemist, summarizes techniques for growing s

68 This review briefly describes the solid state chemistry of many of these materials.

69 topic encompassing condensed matter physics, solid state chemistry, and materials science.

70 , which is a unique structural phenomenon in solid state chemistry.

71 ls science discipline at the intersection of solid-state chemistry and mechanical engineering that ex

72 Basic science research, involving solid-state chemistry and physics, has been at the cente

73 ociated phenomena lie at the intersection of solid-state chemistry, condensed matter physics, and mat

74 als represent a new frontier in the field of solid-state chemistry.

75 ere, we present a general approach to access solid-state CNT mimic structures via the self-assembly o

76 The FRET in the solid-state coaxial heterojunctions with an inner PDHF c

77 tion interactions in solution, the resulting solid-state compounds, and behavior and properties that

78 und that both solution-phase aggregation and solid-state crystallinity of these acceptor polymers are

79 This eutectoid microstructure is a result of solid-state decomposition of the FCC matrix and therefor

80 ization of larger-scale quantum systems with solid-state defects will require high-fidelity control o

81 ization and readout mechanisms, analogous to solid-state defects, molecules could be integrated into

82 s work with laser-cooled atoms and ions, and solid-state defects, spin readout is accomplished using

83 mation science, as has been demonstrated for solid-state defects.

84 The measurements were also supported using solid-state density functional theory simulations of the

85 rlonic state, we observe gaseous, liquid and solid states, depending on the inter-particle and self-d

86 PECT) is feasible using cardiac cameras with solid-state detectors.

87 bining neutron spin-echo (NSE) spectroscopy, solid-state deuterium NMR ((2)H NMR) spectroscopy, and m

88 duced cyclophane and this 1:1 complex in the solid state deviate from the analogous (super)structures

89 So far, experimental studies with solid-state devices in the giant-atom regime have been l

90 y complicate the integration of TTA in other solid-state devices.

91 arily high electrochemical activity and fast solid-state diffusion.

92 ecent developments in SPECT hardware include solid-state digital systems with higher sensitivity and

93 oexisting with topological surface states in solid-state Dirac semimetals, we introduce and layer a s

94 The nanowires with both solid-state donor and acceptor blocks exhibit Forster re

95 Here we present an all-solid-state, electrically tunable and reflective metasur

96 Here we report an all-solid-state electrochemical CO(2)RR system for continuou

97 Solid-state electrochromic devices often need appropriat

98 ganic electronics and in polythiophene-based solid-state electrochromic devices to understand and val

99 he functionality of the perovskite towards a solid-state electrolyte with electrochemical stability u

100 Among the current SSEs, composite solid-state electrolytes (CSSEs) with multiple phases ha

101 Solid-state electrolytes (SSEs) as the most critical com

102 The discovery of new solid-state electrolytes (SSEs) can be guided by computa

103 The recent discovery of highly conductive solid-state electrolytes (SSEs) has led to tremendous pr

104 As the key component in ASSLBs, solid-state electrolytes (SSEs) with non-flammability an

105 g interest in the development of garnet-type solid-state electrolytes and all solid-state batteries.

106 ered one of the most promising and important solid-state electrolytes for batteries with potential be

107 The coupling of solid-state electrolytes with a Li-metal anode and state

108 and applications, including advancements in solid-state electrolytes, multicomponent structures, and

109 concentrated solvent-in-salt electrolytes to solid-state electrolytes, the current research realm of

110 Among all solid-state electrolytes, the sulfide electrolytes have

111 Solid-state emitters(5), such as quantum dots and defect

112 Solid-state fermentation (SSF) by Aspergillus spp. and M

113 The effects of solid-state fermentation (SSF) with Aspergillus sojae, A

114 This polarization is comparable to that of solid state ferroelectrics and is close to the average v

115 ntitatively produces an exceptionally stable solid-state FK A15 phase through a rapid and irreversibl

116 but virtual properties of all molecular and solid state formations.

117 e existing metal halide perovskites in their solid state have severely limited their practical applic

118 trinuclear complexes that undergo reversible solid-state inter-molecular rearrangements to produce di

119 Note that traditional solid-state ISE electrodes are rigid ion-to-electron tra

120 backscattered reflectometry, together with a solid-state laser diode operating at 980 nm.

121 layed over the last two decades in realizing solid-state laser refrigeration is discussed.

122 t have recently been proposed to realize the solid-state laser refrigeration of semiconducting materi

123 In conclusion, novel materials for solid-state laser refrigeration, including color centers

124 equent development of advanced materials for solid-state laser refrigeration.

125 s, and the development of radiation-balanced solid-state lasers.

126 In a broad class of all-solid-state Li batteries, one approach to suppress Li de

127 Solid-state Li-ion batteries (SSLIBs) have recently attr

128 g solid electrolytes for next-generation all-solid-state Li-ion battery applications due to their hig

129 All-solid-state Li-metal cells with these composite electrol

130 All-solid-state Li||Li cells can operate at very demanding c

131 ework (COF-TRO) as cathode materials for all-solid-state LIBs.

132 for applications related to photocatalysis, solid-state light emitters, and chemical sensing will be

133 practical, large-scale applications such as solid-state lighting and displays.

134 e variety of high-power and high-temperature solid-state lighting, lasing, and display devices that h

135 n electrolyte, the C/S cathode experiences a solid-state lithiation/delithiation reaction after the f

136 All-solid-state lithium batteries (ASSLBs) are considered as

137 All-solid-state lithium ion batteries (ASSLBs) are considere

138 hosphorus oxynitride (LiPON) is an amorphous solid-state lithium ion conductor displaying exemplary c

139 sues with the metal-electrolyte interface in solid-state lithium metal batteries can be overcome usin

140 Solid-state lithium metal batteries require accommodatio

141 te and opens up new possibilities for future solid-state lithium-metal batteries and structural energ

142 Solid-state lithium-metal batteries with solid electroly

143 Solid-state lithium-sulfur batteries (SSLSBs) with high

144 Quasi-solid-state LSBs, where sulfur is encapsulated in the mi

145 ental chemical shifts (CS) from solution and solid state magic-angle-spinning nuclear magnetic resona

146 stal X-ray diffraction studies, solution and solid-state magnetic studies, and (57)Fe Mossbauer spect

147 thods, including electrospray ionization and solid state MALDI, as well as MS methods using multiplex

148 mulating and exploring the band structure of solid-state materials in clean and controlled experiment

149 of the full potential of nitrogen-containing solid-state materials is limited by the inert and gaseou

150 eractions as an attractive means to generate solid-state materials that mimic carbon nanotubes, impor

151 electromagnetic waves and free electrons in solid-state materials(1), has yet to be put to large-sca

152 ld-driven photocurrents in various nanoscale solid-state materials, little has been done in examining

153 is predetermined by the intrinsic nature of solid-state materials, which cannot be easily modified w

154 (1-3), have directed fundamental research in solid-state materials.

155 Host-guest complex solid state molecular motion is a critical but underexpl

156 To reduce the mass and mechanical complexity solid-state morphing materials are desirable but are typ

157 derable promise and paves the way for stiff, solid-state morphing materials.

158 A close examination of the solid-state morphologies reveals that the locked superst

159 ne of nanohoops, enables the manipulation of solid-state morphology without significantly changing th

160 The observed dynamic behavior in the solid state moves as a yellow wavefront through the oran

161 obial fuel cell and microbial battery with a solid-state NaFe(II)Fe(III)(CN)(6) (Prussian Blue) catho

162 Solid-state nanopores have broad applications from singl

163 -5 kbp double-stranded DNA molecules through solid-state nanopores in the presence of tangential flui

164 inetic translocation of biomolecules through solid-state nanopores represents a label-free single-mol

165 nematic liquid crystalline phase, leading to solid-state nanostructured colored films upon solvent ev

166 better targeting, design and optimization of solid-state natural food bio-preservatives.

167 The solid-state NCM || Li metal batteries exhibit enhanced s

168 ure was established through a combination of solid-state NMR (SSNMR) experiments, including J-resolve

169 We report solid-state NMR (ssNMR) measurements on spherical virus-

170 Multidimensional solid-state NMR (SSNMR) spectroscopy experiments reveal

171 Using solid-state NMR and deprotonation energy calculations, t

172 recedented two-step process as elucidated by solid-state NMR and molecular dynamics simulation.

173 Advanced solid-state NMR and quantum-chemical methods allow us to

174 hNM dynamics was determined by solid-state NMR and revealed that the lamellar gel-to-fl

175 X-ray diffraction, and variable-temperature solid-state NMR by (13)C cross-polarization magic angle

176 imulations accurately predicted our previous solid-state NMR data and newly acquired electron paramag

177 Using a combination of solution and solid-state NMR experiments, cosedimentation assays, dif

178 lear polarization enhanced (27)Al and (29)Si solid-state NMR experiments.

179 rization of materials for which conventional solid-state NMR is impractical due to the lack of sensit

180 We present solid-state NMR measurements of beta-strand secondary st

181 We present solid-state NMR measurements of this open mutant at neut

182 idimetry, cryogenic electron microscopy, and solid-state NMR measurements.

183 In oriented-sample (OS) solid-state NMR of membrane proteins, the angular-depend

184 identify the challenges and devise a (119)Sn solid-state NMR protocol for the determination of the lo

185 Conventional and DNP-enhanced solid-state NMR provides a molecular-level understanding

186 Li solid-state NMR results show an increase in Li(+) ions (

187 tions and the concentrated conditions of the solid-state NMR samples, we found substantial amounts of

188 Solid-state NMR shows that Asp is sparsely occluded with

189 Solid-state NMR spectra and optimized structures obtaine

190 Surface-selective (133)Cs solid-state NMR spectra show the presence of an addition

191 1-42 and 69-77, which are visible in the MAS solid-state NMR spectra, show (13)Calpha chemical shifts

192 rve resolution approach (MCR), to denoise 2D solid-state NMR spectra, yielding a substantial S/N rati

193 Herein, we demonstrate that solid-state NMR spectroscopy allows the unambiguous assi

194 amma-Al(2)O(3) by using two-dimensional (2D) solid-state NMR spectroscopy at high field.

195 In the last few years, solid-state NMR spectroscopy enabled the determination o

196 lts highlight the utility of high-resolution solid-state NMR spectroscopy for studying ligand binding

197 ecular correlation times obtained from (13)C solid-state NMR spectroscopy measurements establish the

198 sed transmission EM, biochemical assays, and solid-state NMR spectroscopy of representative isolates

199 Herein, we demonstrate the application of solid-state NMR spectroscopy on native, heterogeneous th

200 Here, we employ nondestructive (31)P solid-state NMR spectroscopy to investigate the chemical

201 Fourier transform infrared spectroscopy and solid-state NMR spectroscopy validate the N-H(2) group a

202 ation lifetime spectroscopy (PALS), FTIR and solid-state NMR spectroscopy) to demonstrate how a hiera

203 Using (11) B solid-state NMR spectroscopy, we show that the majority

204 transmembrane domain (ETM), determined using solid-state NMR spectroscopy.

205 g density functional theory calculations and solid-state NMR spectroscopy.

206 Dye binding and solid-state NMR studies reveal changes in fibril surface

207 Solid-state NMR supports these predictions and reveals p

208 art experimental methods including extensive solid-state NMR techniques and HAADF-STEM imaging.

209 e use multi-dimensional magic angle spinning solid-state NMR to characterize the sorghum secondary ce

210 Here, we use solid-state NMR to determine the 3D structure of the amy

211 cal monomeric composition as demonstrated by solid-state NMR, complemented by spectroscopic, thermal,

212 of teixobactins in cellular membranes using solid-state NMR, microscopy, and affinity assays.

213 e of spectroscopic methods, including (23)Na solid-state NMR, Mossbauer, and X-ray photoelectron spec

214 Using MAS solid-state NMR, we studied the fibril structure of a re

215 man hormone beta-endorphin was determined by solid-state NMR.

216 Presented here is a new solid-state-NMR-based quantification method for componen

217 Hence, we demonstrate the advantage of using solid-state nuclear magnetic resonance (NMR) spectroscop

218 ple mutants of the Kir channel KirBac1.1 via solid-state nuclear magnetic resonance (SSNMR) spectrosc

219 tions, dynamic nuclear polarization-enhanced solid-state nuclear magnetic resonance and cryo-electron

220 This interaction has been elucidated by solid-state nuclear magnetic resonance and density funct

221 nction, isothermal titration calorimetry and solid-state nuclear magnetic resonance spectroscopy as w

222 ation of high-resolution imaging and in situ solid-state nuclear magnetic resonance spectroscopy, we

223 in ZIF glasses using ultrahigh-field zinc-67 solid-state nuclear magnetic resonance spectroscopy.

224 This template-directed solid-state nucleation pathway is enabled by the large i

225 tive organic compounds working either in the solid state or in solution for aqueous or nonaqueous ele

226 ed approaches for the design of heterocyclic solid-state organic ionic conductors (SOICs) in flexible

227 Solid-state packing plays a defining role in the propert

228 In the solid state, pai-pai stacking suppresses their emission,

229 y, we reveal the underlying mechanism of the solid-state phase transformation of these amorphous nano

230 ur synthetic route features a stereospecific solid-state photodecarbonylation reaction to introduce t

231 quality are at the frontier of contemporary solid state physics.

232 lations in physical-chemistry and atomic and solid-state physics.

233 cognition of an order-disorder transition in solid-state physics/chemistry and geophysics.

234 Our results establish a new solid-state platform based on moire superlattices that c

235 These results showcase a solid-state platform based on single coherent rare-earth

236 OLEDs offer an alternative solid-state platform to investigate the radical-pair mec

237 for CRE detection is translated into an all-solid-state platform, in which the enzyme is immobilized

238 Among these systems, solid-state point defect spins are known for being long-

239 rfluid helium(27), or coupled atomic(28) and solid-state polariton(29) condensates.

240 ization inside electrochemical cells to form solid-state polymer batteries with good interfacial char

241 Solid-state batteries enabled by solid-state polymer electrolytes (SPEs) are under active

242 This work offers an important pathway toward solid-state polymer electrolytes for high-voltage solid-

243 Many phase transformations associated with solid-state precipitation look structurally simple, yet,

244 reby gain an extra level of control over the solid state properties of organic optoelectronic materia

245 Synthetic control over the solid state properties of organic optoelectronic materia

246 The solid-state properties of organic radicals depend on rad

247 known to exhibit notably different trends in solid-state properties; a well-known illustration is the

248 interfaces between photons and a variety of solid-state QIP platforms.

249 Solid-state quantum acoustodynamic (QAD) systems provide

250 Solid-state quantum coherent devices are quickly progres

251 r spins also featured in early proposals for solid-state quantum computers(1) and demonstrations of q

252 Many solid-state quantum devices operate at millikelvin tempe

253 ctor microcavities using exciton-polaritons, solid-state quasi-particles with a light mass and sizeab

254 um interfaces between mechanical systems and solid-state qubit processors, this paves the way for mec

255 of polarons which is best suited for in situ solid-state Raman spectroelectrochemistry.

256 Solid-state reactions between micrometer-size powders ar

257 rated with various protein mediators, become solid-state reactors that can localize at the critical i

258 The reversible solid-state rearrangement, confirmed in situ using powde

259 nt a detailed study of the intercalation and solid state reduction of metallic and semiconducting enr

260 egrees of freedom, central pillars of future solid state science.

261 racterization, comparison of properties, and solid-state self-assembly of the compounds are discussed

262 oups to be characterized in solution and the solid state, several of which are too weak - or are disf

263 the chiral moiety, shows a propensity for a solid-state sorting phenomenon.

264 s with the lower-energy (177)Lu energy peak, solid-state SPECT/CT imaging provided an accuracy to wit

265 Solid-state spin defects are a promising platform for qu

266 Here we use a single solid-state spin memory integrated in a nanophotonic dia

267 ed analogue exhibits remarkable solution and solid-state stability.

268 High-yield synthesis, spectroscopic and solid-state structural proof of the lactam-embedded smal

269 The solid state structure, UV-visible spectroscopy, magnetom

270 Its solid-state structure and density functional theory (DFT

271 The solid-state structure of the (+)-5-methyllithium complex

272 In this rare example, we could determine the solid-state structure of the 100% dimerized product and

273 Solid state structures thus show in both cases a stabili

274 act as "crystal modulators" to modulate the solid-state structures and properties.

275 his technique facilitated the elucidation of solid-state structures of all five compounds with <1.1 a

276 Solution- and solid-state studies of the dimerization of this new cong

277 output under complex deformations for an all-solid-state supercapacitor.

278 X-ray diffraction analysis reveals that the solid-state superstructure of the 1:1 complex constitute

279 chemical modification of RNA structure using solid-state synthesis or enzymatic transformations.

280 Here we describe a solid state system that operates on the basis of complex

281 of passive, dynamic thermal regulation in a solid-state system with temperature-dependent thermal em

282 However, triplet pairing is rare in solid-state systems and has not been unambiguously ident

283 er, the reported performance of TTA in rigid solid-state systems is substantially inferior, which may

284 d-state TTA comparable to solution-processed solid-state systems.

285 ers a circa 70 % drop in conductivity in the solid state that can be recovered upon subsequent irradi

286 base pair which is a stable formation in the solid state that has previously not even been suggested.

287 iral assemblies in nonpolar solution and the solid state through double-helical intermolecular and tr

288 at undergo nanoscale phase separation in the solid state to produce sub-10 nm surface features.

289 We have exploited our recently reported solid-state topochemical polymerization/cyclization-arom

290 n of highly hydrated amorphous particles and solid-state transformation of a protein-rich amorphous p

291 r rearrangement into crystalline domains via solid-state transformation.

292 is the first demonstration of dry-processed solid-state TTA comparable to solution-processed solid-s

293 ffer a route to achieving higher-performance solid-state TTA upconversion devices that are compatible

294 ds, such as electron paramagnetic resonance, solid-state ultraviolet-visible spectroscopy, and all-at

295 Solid-state UV-vis spectroscopy reveals that azobenzene

296 uctural elucidation of these newly developed solid-state white-light emitting HDP materials.

297 cycle adopts a columnar packing motif in the solid state with large void spaces between pentacene uni

298 ll adopt butterfly-like conformations in the solid state with the P-organyl substituents adopting mut

299 Solid-state zinc ion sensor is developed with high enoug

300 e as a freestanding air cathode for flexible solid-state Zn-air batteries without the use of carbon p