ライフサイエンスコーパス: insulate

1 me materials are metallic whereas others are insulating.

2 Abrahams, et al. that all 2D systems must be insulating.

3 e crystal and amorphous C60 are electrically insulating.

4 his is expected since diesel is electrically insulating.

5 lectron localization and makes this material insulating.

6 ust and scalable circuit performance such as insulating a gene circuit against unwanted interactions

7 erstanding of the fundamental limitations to insulating active material loading.

8 strate how this negative feedback regulation insulates alternative sigma factor activity from competi

9 Insulating aluminum oxide nanocrystals are assembled lay

10 harge order is present in La5/3Sr1/3CoO4, an insulating analogue of the copper oxide superconductors

11 keep mitosis short, constant, and temporally insulated and anticipate it might be a commonly used reg

12 ea synthesis of 1D-MoSe2 nanoribbons on both insulating and conducting substrates via molecular beam

13 internal porous domains alongside non-porous insulating and conductive materials, in highly controlle

14 paramagnetic metal LaNiO3, which can become insulating and magnetic when only a few monolayers thick

15 lows the photoexcitation process in both the insulating and metallic phases, probes the subsequent re

16 (LDA+DMFT) we characterize its paramagnetic insulating and metallic phases, showing the proximity of

17 r plasmonics research in previously untapped insulating and strongly-correlated materials.

18 For both the insulating and the metallic phase, the formation of the

19 etallic ferromagnetic islands nucleate in an insulating antiferromagnetic matrix.

20 due to correlation effect making the surface insulating as opposed to that in LAO which remains metal

21 tance at microwave frequencies despite being insulating at d.c.

22 Myelin, which ensheaths and insulates axons, is a specialized membrane highly enrich

23 In insulating BaBiO3 we observed an increase in conductivit

24 ocalized on the CuTe ribbons and that the 1D insulating band structure is also resilient to such larg

25 nd separated from two metallic reservoirs by insulating barriers.

26 nces, the substitution experimentally yields insulating behavior from a significant decrease in carri

27 a simple chemical perspective on the unusual insulating behavior of such materials, complementing the

28 ion and the resulting ferrimagnetic-metallic/insulating behavior.

29 is is often accompanied by semiconducting or insulating behavior.

30 nd are antiferromagnetic insulators with the insulating behaviour persisting above the Neel temperatu

31 -domain bilayer graphene, which shows gapped insulating behaviour under a vertical electrical field,

32 edicted properties, such as a 2D topological insulating behaviour with a very large bandgap, and the

33 7 and low buffer concentrations, the film is insulating below 0.8 (V vs SHE) but becomes conductive a

34 ct is observed in dual-gated devices of bulk-insulating Bi2-x Sb x Te3 thin films, where the field-in

35 measurements in flakes exfoliated from bulk insulating Bi2Te2Se crystals, using two outside nonmagne

36 ications without suffering any influences of insulating binders usually used to fix nanomaterials on

37 The electrical insulating BNNTs are used as the one-dimensional (1D) su

38 Here we show that the growth of electrically insulating BNNTs on graphene can enable the use of graph

39 that we attribute to defects within the bulk insulating boron nitride.

40 lerant behavior based on the ability to self-insulate breakdown faults, and we enhance fundamental un

41 ed by the unique electronic properties of an insulating bulk and metallic boundaries arising from non

42 ulators are a new class of materials with an insulating bulk and topologically protected metallic sur

43 ), a well-known Kondo insulator in which the insulating bulk arises from strong electron correlations

44 The results exhibit signature of insulating bulk electronic structure with tiny intensiti

45 nusual insulating state with an electrically insulating bulk that simultaneously yields bulk quantum

46 novel class of quantum matter with a gapped insulating bulk, yet gapless spin-helical Dirac fermion

47 onstrated topological surface states with an insulating bulk.

48 host a conducting surface juxtaposed with an insulating bulk.

49 e ferromagnet are electron ically coupled or insulated by a thin dielectric layer, with an indication

50 Nominally conductive interfaces are rendered insulating by solvent immersion, which deprotonates the

51 This relocalization insulates cells at the center from apically applied liga

52 zed core clusters of Bi2I9(3-) surrounded by insulating CH3NH3(+) was prepared via solution processin

53 in arbitrary configuration of conducting and insulating channels is investigated and the problem is r

54 uctance gets suppressed, confirming the spin-insulating character of a superfluid.

55 onstrate that, although undoped DNPs have an insulating character, they show electrochemical activity

56 icates that the epitaxial h-BN film has good insulating characteristics.

57 Architectural proteins insulate compartmental domains by reducing interaction f

58 vercome this constraint with an electrically insulating composite that exhibits an unprecedented comb

59 uctors (InP, Si, Ge, PbS, InAs and Te) in an insulating composite to tailor its infrared reflectance

60 alkali halides such as NaCl or KBr and polar insulating Cu2N terminating bulk copper.

61 sistant glycolytic reserve that functionally insulates DeltaPsim and mitochondrial ROS production fro

62 that is, robustness despite perturbation--to insulate development against environmental and genetic v

63 d (BDD) microband electrode, insulated in an insulating diamond platform for durability and integrate

64 ring particles at low volume fractions in an insulating dielectric offers a promising way to reduce r

65 low-bandgap semiconductor microinclusions in insulating dielectrics.

66 2S) is under intense study because it is the insulating discharge product of ultrahigh energy density

67 image the nanoscale formation and growth of insulating domains across the temperature-driven MIT in

68 phase is intrinsically phase separated into insulating domains with polar and nonpolar symmetries.

69 ic within band theory and presumably becomes insulating due to surface disorder or surface reconstruc

70 glia to regulate process extension so as to insulate each neuropil compartment.

71 good electron conducting path nullifying the insulating effect of MPA and also act as a proper immobi

72 d to condense into either a superfluid or an insulating electronic crystal.

73 parts of the dielectric permittivity of semi-insulating Fe-doped InP crystalline wafers in the 2-700

74 nt, is transparent in the infrared and is an insulating ferrimagnet leading to its use in optical and

75 cross a thin film of yttrium iron garnet, an insulating ferrimagnet, and forming a heterojunction wit

76 Erasable conductive domain walls in insulating ferroelectric thin films can be used for non-

77 investigate the magnetisation dynamics of an insulating ferromagnet (FM) deposited on the surface of

78 11] direction by interfacial coupling to the insulating ferromagnet LaMnO3, and used to generate inte

79 e case in the pioneering S/FI (where FI is a insulating ferromagnet) tunneling experiments of Meserve

80 al films which is comparable to conventional insulating ferromagnetic YIG films.

81 mping metallic ferromagnets are preferred to insulating ferromagnets in charge-based spintronic devic

82 hin metallic films deposited on electrically insulating ferromagnets, but the films' high resistance

83 constant can reach 10(-4) to 10(-5) in some insulating ferromagnets, metallic ferromagnets generally

84 ind applications as a robust multifunctional insulating film that can be applied in integrated photon

85 CM approach curves, allowing a comparison of insulating film thickness for the different terminations

86 ble, nonvolatile metallic phase in initially insulating films of WO3 Here, we use hard X-ray photoele

87 ition in the fluid phase between a molecular insulating fluid and a monoatomic metallic fluid has bee

88 ng hydrogen transitions from a molecular and insulating fluid to a conducting state without passing t

89 s, some resist and remain modular, seemingly insulated from extrinsic perturbations-an intriguing pos

90 ; even pathways that share components can be insulated from one another.

91 tic amines, and other amines whose charge is insulated from the aromatic ring.

92 sm by which lamellipodial actin networks are insulated from the effects of tropomyosin.

93 activated in the dark even when electrically insulated from the electrodes.

94 stream genes embedded within LRCs are highly insulated from the variation in expression of upstream g

95 Simultaneously, other mRNAs are insulated from these stress-induced changes in eIF4F ass

96 ation, suggesting that mitosis is temporally insulated from variability in earlier cell-cycle phases.

97 hydrogen atoms also can convert electrically insulating fully hydrogenated graphene back into conduct

98 tallic AFM-b antiferromagnetic state to Mott insulating G-type antiferromagnetic (G-AFM) state was fo

99 the interface region of single-crystal semi-insulating GaAs that has been coated and passivated with

100 o uncover an intimate connection between its insulating gap and antiferromagnetism.

101 of quantum matters, are characterized by an insulating gap in the bulk and a metallic state on the s

102 classes: Mott-Hubbard insulators, where the insulating gap is driven by the Coulomb repulsion U on t

103 talline ceramic had semiconductor grains and insulating grain boundaries, and that the activation ene

104 rk, a novel system including an electrically insulated graphite die for Spark Plasma Sintering (SPS)

105 e interplay between the two generates a Mott-insulating ground state with a peculiar charge-density-w

106 nsfer from Ti to Ni sites, giving rise to an insulating ground state with orbital polarization and e(

107 ct = 0.05 eV, is more consistent with a Mott insulating ground state.

108 ness of charge transfer (CT) effect and Mott insulating ground states.

109 ttice multiferroic Cu2OSeO3 became the first insulating helimagnetic material in which a long-range o

110 s (LEDs) made by stacking metallic graphene, insulating hexagonal boron nitride and various semicondu

111 are fabricated from electrically conductive, insulated, hydrophobic textiles, but the concept can be

112 ron doped diamond (BDD) microband electrode, insulated in an insulating diamond platform for durabili

113 rder whereas bulk wires, on contrary, become insulating in some region of inter-chain interaction par

114 These MWCNTs were found to be insulating in spite of their graphitic layered outer str

115 a topological insulator - material which is insulating in the bulk but conducting on its surface, al

116 described by a Bloch Hamiltonian, system is insulating in the bulk of sample throughout the quantum

117 the substrate of the hetero-couple with the insulating interface.

118 S4 has on the formation of an electronically insulating, ionically conducting solid electrolyte inter

119 ostic assay based on a reverse transcription-insulated isothermal PCR (RT-iiPCR) method for the detec

120 turbances, both of which are needed to fully insulate it from the cell cycle and give it its observed

121 In quiescent cells, the primary cilium insulates itself from contiguous dynamic membrane proces

122 The metallic interface between insulating LaAlO3 and SrTiO3 opens up the field of oxide

123 pair the functional role of the sheath as an insulating layer for proper nerve conduction.

124 ological insulators are often capped with an insulating layer since topological insulators are known

125 ack changes in the structure of the adsorbed insulating layer.

126 erately maximized, that is, in films between insulating layers.

127 de may lead to the irreversible formation of insulating Li2 CO3 , making the battery less rechargeabl

128 r and carbon dioxide in air to form a Li-ion insulating Li2 CO3 layer on the surface of the garnet pa

129 its theoretical value due to the build-up of insulating lithium peroxide (Li(2)O(2)), the battery's p

130 ol the magnetization state of conducting and insulating magnetic materials.

131 The substrate can be an insulating material or (semi)conductor, but herein, we f

132 Undoped CVD diamond is an insulating material with superior chemical stability in

133 fects in 2D-Mg(OH)2, but also offer novel 2D-insulating material with unique physical, vibrational, a

134 es, such as continuous layers or islands, of insulating material.

135 electrode mapping, as well as in studies of insulating materials as demonstrated by transient spot r

136 nitride (h-BN) is a good candidate for gate-insulating materials by minimizing interaction from subs

137 Heterostructures of insulating materials hold great promise, as confirmed by

138 However, the spectrum of good insulating materials is still very narrow.

139 Topological insulators are insulating materials that display conducting surface sta

140 ing with electric or magnetic fields, or for insulating materials where the addition of a conductive

141 wice or higher than ac breakdown strength in insulating materials, remains unclear.

142 xide semiconductors seem hard to act as high insulating materials.

143 sheets are one of the strongest electrically insulating materials.

144 Using this approach, insulating matrix and conductive electrode inks are dire

145 ent is ensheathment of axons with myelin, an insulating membrane formed by oligodendrocytes.

146 ge transport through junctions consisting of insulating molecular units is a quantum phenomenon that

147 nd indium; R1 and R2 refer to two classes of insulating molecular units-(CH2)n and (C6H4)m-that are c

148 ment is the formation of specific amounts of insulating myelin membrane on axons.

149 n result from damage or dysregulation of the insulating myelin sheath surrounding spinal motor axons,

150 tegration of semiconducting, conducting, and insulating nanomaterials together into precise intricate

151 city retention, and safety features of bulk, insulating Nb2O5 synthesized in a single step at relativ

152 ogene activation can occur via disruption of insulated neighborhood boundaries in cancer cells.

153 Insulated neighborhoods are a powerful paradigm for gene

154 letions that eliminate the boundary sites of insulated neighborhoods containing prominent T-ALL proto

155 enhancer-promoter interactions occur within insulated neighborhoods during cell state transition.

156 n occur via genetic alterations that disrupt insulated neighborhoods in malignant cells.

157 We mapped insulated neighborhoods in T cell acute lymphoblastic le

158 Here, we review evidence that insulated neighborhoods provide for specific enhancer-ge

159 enes depends on chromosome structures called insulated neighborhoods, we investigated whether proto-o

160 nd their target genes generally occur within insulated neighborhoods, which are chromosomal loop stru

161 e identified form a chromosomal framework of insulated neighborhoods, which in turn form topologicall

162 proteolipid-rich membrane that ensheaths and insulates nerve fibers, facilitates the rapid conduction

163 analysis of thick films of micrometer-sized, insulating niobia particles indicates that the capacity

164 ited on graphite electrodes modified with an insulating nitrocellulose film and is evoked after the c

165 ependence function even with minimal cytosol insulating nuclei.

166 nanoribbons with this precision directly on insulating or semiconducting substrates has not been pos

167 conductor nanocrystals (NCs), replacement of insulating organic capping ligands with chemically diver

168 tes with metal halide slabs separated by the insulating organic layers are reported to show higher st

169 ical tunneling of electrons across ultrathin insulating oxide barriers has been studied extensively f

170 ormance without nanostructuring in a complex insulating oxide expands the field for battery material

171 ing ultramicroelectrodes modified with thin, insulating oxide films where electronic tunneling betwee

172 f tunable correlated plasmons in a Mott-like insulating oxide from the Sr1-xNb1-yO3+delta family.

173 bility metal-oxide field effect transistors, insulating oxide interfaces, graphene, and MoS2 have cha

174 s (2DEG) formed at the interface between two insulating oxides have attracted great attention in the

175 s (2DEG) formed at the interface between two insulating oxides such as LaAlO3 and SrTiO3 (STO) is of

176 metal-insulator-metal (MIM) structures with insulating oxides, such as TiO(2), are limited by a lack

177 nductivity and mobility than the constituent insulating oxides.

178 This approach can convert the insulating paper to the highly porous metallic paper wit

179 lishing a rigorous engineering framework for insulating parts and modules from their context to impro

180 The insulating [Pb2BiS3] sheet inhibits interlayer charge ho

181 In our experiments, insulated percutaneous wires connect to an externally mo

182 e in holding together the myelin sheath that insulates peripheral nerves.

183 c transport properties of semiconducting and insulating perovskite oxides.

184 An insulating PH5 phase, the structure and bonding of which

185 tance property is ascribed to the introduced insulating phase at the grain boundaries.

186 ess in understanding the nature of this Mott insulating phase has been impeded by the lack of knowled

187 ally the voltage-induced breakdown of a Mott insulating phase in a system of charged classical partic

188 scanning tunnelling microscope switches the insulating phase locally into a metallic phase with irre

189 presence of an intergrown antiferromagnetic insulating phase makes the study of the underlying physi

190 scopy-the band structure of the paramagnetic insulating phase of Ca2RuO4 and show how it features sev

191 a metallic state to low temperatures in the insulating phase of epitaxially grown thin films of VO2.

192 er graphene is predicted to be a topological insulating phase protected by no-valley mixing symmetry,

193 two-dimensional electron systems exhibit an insulating phase that is understood as a form of pinned

194 2/3Ca1/3MnO3 into an emergent charge-ordered insulating phase with extreme photo-susceptibility, wher

195 When VO2 is in its insulating phase, the structure is highly reflective due

196 Here we show that, near the Mott insulating phase, the upper critical field Hc2 of the fu

197 easures the phase-transition dynamics in the insulating phase.

198 tion is shown to be essential to explain the insulating phase.

199 a simple Fermi liquid, a poorly understood "insulating" phase as indicated by a metal-"insulator" cr

200 To characterize these insulating phases of matter, we introduce a paradigm in

201 ents aligned from dipolar interactions as in insulating phases.

202 m coexistence of ferromagnetic, metallic and insulating phases.

203 a-vis to those of the corresponding backbone-insulated poly{[N,N'-bis(2-octyldodecyl)-1,4,5,8-naphtha

204 by embedding metallic Ni nanowires within an insulating poly(vinylidene fluoride) (PVDF) matrix in so

205 es offers protection against formation of an insulating polydopamine layer, while retaining the abili

206 anic and organic additives in conjugated and insulating polymer matrices are covered, as well as the

207 The use of insulating polymers as binders or matrices is proposed,

208 of conjugated small molecules and amorphous insulating polymers to produce OTFTs with consistently e

209 Tunneling contacts made of any insulating polymers, a champion technology in silicon so

210 d polymers, (2) dopants and counterions, (3) insulating polymers, and (4) conductive fillers.

211 manipulate SWNTs with the help of arrays of insulating posts in a microfluidic device around which e

212 m(-2) s(-0.5)), consistent with a thermally insulating powdered surface, is inferred.

213 Here we demonstrate that the insulating properties of atomic-layer-deposited Al2O3 th

214 In addition, the electrically insulating properties of the composite are well preserve

215 Insulated radiofrequency wires were positioned 2 to 5 mm

216 the spatial phase separation of metallic and insulating regions during the MIT and the coupling of la

217 Conductive and insulating samples have been processed, with thicknesses

218 bacteria and acted as ET pathways across the insulating SAMs on the electrode surface, resulting in a

219 Droplet interface bilayers (DIBs), flexible insulating scaffolds for such materials, can be used as

220 Attachment of a fluorescent particle to the insulating sheath of the SECM tip extends this technique

221 trol of the RG (defined as the radius of the insulating sheath over the radius of the active metal el

222 Oligodendrocytes produce myelin, an insulating sheath required for the saltatory conduction

223 The ratio of the insulating sheath to the electroactive core of the UMEs

224 structure is tuned from the metallic to the insulating side of the gap opening.

225 ed in rectangular pillars etched into a semi-insulating silicon carbide substrate.

226 few-layer graphene, and etch tracks exposing insulating SiO2 regions are integrated into nanoscale sy

227 ) and tungsten disulphide, grown directly on insulating SiO2 substrates, with excellent spatial homog

228 atteries is the formation of an electrically insulating solid layer that allows lithium ion transport

229 omparably sized, surface-bound conductive or insulating spherical NP.

230 Insulating SrTiO3 (STO) can host 2D electron systems (2D

231 n the transition between the correlated Mott insulating state and a metallic state of a transition me

232 tion (QPT) between an antiferromagnetic Mott insulating state and a paramagnetic metallic state.

233 oxides, including an interaction-driven Mott insulating state and an antiferromagnetic (AFM) state.

234 icture of the correlated metal near the Mott insulating state and rule out alternative scenarios in w

235 Controlled access to the border of the Mott insulating state by variation of control parameters offe

236 e superconductors, an antiferromagnetic Mott insulating state can be destabilized toward unconvention

237 to reality by revealing the occurrence of an insulating state close to charge neutrality in Bernal-st

238 tion from superconducting to an unusual Mott insulating state emerging with the increase of LCMO laye

239 However, such gaps rarely lead to the highly insulating state expected at low temperatures.

240 Our discovery of a Mott-insulating state in NaFe1-xCuxAs thus makes it the only

241 resembles that observed in bilayers, but the insulating state in tetralayers is visible at higher tem

242 ve case, the conventional description of the insulating state is inadequate and demonstrate a method

243 nal theory suggests that the band gap in the insulating state is reduced by pressure as a result of i

244 spin polarization, understanding AHE in the insulating state is valuable from the point of view of s

245 d's coupling that together generate the Mott insulating state of Ca2RuO4.

246 The transition into the Mott insulating state raises important fundamental questions.

247 conversion from conducting/semiconducting to insulating state through molecular dissociation and diso

248 In addition, the realization of the QAHE insulating state unveils new ways to explore quantum pha

249 ere, we report the observation of an unusual insulating state with an electrically insulating bulk th

250 tivity can be smoothly connected to the Mott-insulating state, highlighting the important role of ele

251 ange antiferromagnetic correlation within an insulating state.

252 reases in the metallic state relative to the insulating state.The development of future computation d

253 Insulating states can be topologically nontrivial, a wel

254 ature of the transition from the metallic to insulating states of a 2D system.

255 ey define macroscopic phenomena such as Mott insulating states, spontaneous spin- and charge-order, a

256 ure and magnetic field dependences of AHE in insulating, strongly-disordered two-dimensional Mn delta

257 onuniform electric fields are generated with insulating structures embedded in a microchannel.

258 o directly measure SOTs in both metallic and insulating structures.

259 energy source was demonstrated on arbitrary insulating substrate (e.g. polymer sheet/paper) by coati

260 inetically characterized from SECM toward an insulating substrate, with promising potentiality in man

261 t been observed in graphene layers on a near-insulating substrate.

262 curves, line scans, and array scans over an insulating substrate.

263 ation is unsaturatable, this mechanism could insulate substrates from crosstalk, but it would also pr

264 and non-destructive RHEED monitoring even on insulating substrates and could enable doped single crys

265 Facile, large-area transfer of GNRs onto insulating substrates and subsequent device fabrication

266 ne characterisation of graphene films on non-insulating substrates such as germanium.

267 nables direct nanopatterning and thinning on insulating substrates such as SiO2 /Si.

268 er mobility, and their large-scale growth on insulating substrates would enable the batch fabrication

269 rrole helps mitigate the negative effects of insulating sulfur, and the elastomeric matrix accommodat

270 ple for microelectrospotting of electrically insulating surface-imprinted films is made by using scop

271 t patterned ion deposition on conductive and insulating surfaces is possible.

272 ochemical microscopy (SECM) toward different insulating surfaces such as glass, silanized glass, or P

273 metallic conductivity due to the presence of insulating surfactant.

274 level can facilitate the design of maximally insulated systems featuring heterologously expressed enz

275 tration is observed in numerous electrically insulating systems, in metals it is a rare phenomenon.

276 omain walls with conducting head-to-head and insulating tail-to-tail configurations, which exhibit a

277 osphatase 2B (PP2B, calcineurin) focuses and insulates termination of local second messenger response

278 We demonstrate a method to make common insulating textile fibres conductive, by coating them wi

279 GF-betaR signaling, suggesting that TGF-beta insulates Tfh progenitor cells from IL-2-delivered mTOR

280 h(I)-enolate to a Rh(I)-heterobenzyl species insulates the resultant alpha-stereocenter from epimeriz

281 Specifically, DYRK1A inhibition insulates the self-renewing subpopulation of human pluri

282 electrolytes, and on externally heating and insulating the cells.

283 the film was depleted of holes becoming more insulating, the electric field extended throughout the f

284 are indeed highly promiscuous, how do cells insulate themselves against unwanted crosstalk?

285 the CCCTC-binding factor (CTCF) functions to insulate these adjacent yet antagonistic chromatin domai

286 To insulate these frameworks from ambient magnetic signals,

287 enient and reliable method of obtaining high insulating thin film in oxide semiconductor for the appl

288 TERS tip can be functionalized and partially insulated to be used as a microelectrode enabling electr

289 l CoV2O4, which stands at the crossover from insulating to itinerant behavior using the first princip

290 ystem that displays a temperature-controlled insulating to metal phase transition near room temperatu

291 rming the electronic properties of MOFs from insulating to semiconducting, as well as provide a bluep

292 diverse electronic properties, ranging from insulating to superconducting.

293 :5Te1:8Se1:2 single crystal, one of the most insulating topological insulators.

294 Fermi surface on the metallic side of a Mott insulating transition by high pressure quantum oscillato

295 ) electronic cooler junctions by a nanoscale insulating tunnel barrier introduced between the Sm and

296 These polyhydrides remain insulating up to 215 GPa.

297 embled heterostructure of an FeSC and a Mott-insulating vanadium oxide.

298 CNT thread partially insulated with a thin polystyrene coating to define the

299 In this work, disordered-IrMn3/insulating-Y3Fe5O12 exchange-biased bilayers are studied

300 ism of spin generation where the role of the insulating yet topologically non-trivial bulk becomes ex