ライフサイエンスコーパス: metallic

1 r non-polymeric beads (i.e., glass, ceramic, metallic).

2 ly eliminated when defects render the system metallic.

3 d that the solution is truly homogeneous and metallic.

4 rkable observation, given that the liquid is metallic.

5 d to the high electrical conductivity of the metallic 1T phase of MoS2 nanosheets, the elastic modulu

6 ue to the complete transformation of MoS2 to metallic 1T phase, high porosity and stabilization effec

7 The metallic 1T-MoS2 has attracted considerable attention as

8 n evolution reaction than the edge sites and metallic 1T-phase of MoS2 catalysts.

9 ify the fundamental electronic properties of metallic (1T phase) nanosheets of molybdenum disulfide (

10 s persisted due to the unavoidable fact that metallic absorption intrinsically scales with field conf

11 work, wheat plants were exposed to pristine metallic (Ag-NPs) and sulfidized (Ag2S-NPs) silver nanop

12 ed in distinguishing silver ion release from metallic AgNPs in biological media.

13 alysis of scattering data from ten different metallic alloy liquids, we show that stronger liquids ha

14 a liquid-to-liquid phase transition in this metallic alloy supercooled melt.

15 ned and the effect demonstrated in a complex metallic alloy, even though the electronegativity differ

16 sity function analysis we find that Zr-based metallic alloy, heated to the supercooled liquid state u

17 microstructures and mechanical properties of metallic alloys lies in designing and using athermal pha

18 design concept may be applied to many other metallic alloys.

19 Germanium telluride (GeTe) is both polar and metallic, an unusual combination of properties in any ma

20 and less active in comparison to as-prepared metallic and electrochemically pretreated (E-Ir) analogu

21 ave substandard electrochemistry relative to metallic and glassy carbon electrodes.

22 to arise are the spatial phase separation of metallic and insulating regions during the MIT and the c

23 nction together with suitable nanoparticles: metallic and metal oxides, including magnetic ones, carb

24 e semiconducting at P = 1 atm, and some form metallic and superconducting symmetrically bonded AuHAu

25 Rechargeable batteries based on metallic anodes are of interest for fundamental and appl

26 he Bragg-plasmon mode supported by an organo-metallic array and molecular excitons in the form of J-a

27 no longer visible after the introduction of metallic artifacts.

28 and Sr, the materials are already marginally metallic at P = 1 atm and the combination of high and lo

29 ayered semiconductor MoSe2 exhibit parabolic metallic bands.

30 these results represent the first report of metallic behavior and permanent porosity coexisting with

31 lso the smallest gold nanocrystal to exhibit metallic behavior, with a surface plasmon resonance band

32 the extremes of electrolytic through to true metallic behavior.

33 Patients with a metallic biliary Wallstent, epilepsy, or ventricular arr

34 materials in both aerospace development and metallic biomaterials.

35 class of bulk amorphous NiFeP materials with metallic bonds from the viewpoint of electrode design.

36 In a heavily overdoped, metallic but non-superconducting LSCO (x = 0.35) film, t

37 Proton adsorption on metallic catalysts is a prerequisite for efficient hydro

38 h is characterized by low symmetry having 1D metallic chains within the planes and extremely weak int

39 -tunable reversible oxidation of a thin-film metallic channel is demonstrated.

40 identify a spectroscopic fingerprint of bulk metallic character and ferromagnetism versus depth.

41 The metallic character of (MA)PbI3 above 60 GPa was confirme

42 dband saturable absorber applications due to metallic characteristics, which agrees well with the exp

43 coordinated Co(2+) forming at the expense of metallic Co((0)).

44 e of N-doped carbon by using chloride, while metallic cobalt nanoparticles encased in protective grap

45 Nearly 90 per cent of service failures of metallic components and structures are caused by fatigue

46 While the low energy conductivity of the metallic compound is barely frequency dependent, the for

47 The conductivity data of the metallic compound show the signature of the pseudogap th

48 electronic-structure supporting the complex metallic conductivity of the material.

49 entally observed MOF that exhibits band-like metallic conductivity.

50 erahertz and mid-infrared ranges, with lower metallic conductivity.

51 ey are infinitely deformable while retaining metallic conductivity.

52 g direct tribochemical reactions between the metallic contact surface with oxygen to form an oxide in

53 nds play a key role in the immobilization of metallic contaminants.

54 An interconnected framework of ultrathin metallic copper formed provides a high conductivity back

55 to address all the limitations of permanent metallic coronary stents, such as the risks of target le

56 rrier between the nanodots and an underlying metallic Cr layer.

57 Nanoscale metallic crystals have been shown to follow a 'smaller i

58 imple way of controlling plastic flow in non-metallic crystals, enabling materials with a greater oxi

59 that two distinct mechanisms are operable on metallic Cu electrodes in acidic electrolytes: (i) elect

60 electric coating that, when wrapped around a metallic cylinder, mimics the scattering from a predefin

61 to semiconductors with tunable gaps, to semi-metallic, depending on the substrate, chemical functiona

62 e frequent and intense with the BVS than the metallic DES and could be determined by patient baseline

63 icon nanowire junction-less transistors with metallic doping densities which demonstrate clear 1D ele

64 g patterns after either Absorb BVS or Xience metallic drug-eluting stent (DES) implantation (Abbott V

65 and mechanical support functions similar to metallic drug-eluting stents (DES), followed by complete

66 results equivalent to those of conventional metallic drug-eluting stents in the early years after im

67 randomly assigned to Absorb BVS (n=3261) or metallic EES (n=2322) and followed up for 2 years.

68 and Drug Administration-approved BVS versus metallic EES in patients undergoing percutaneous coronar

69 Compared with metallic EES, risk of target lesion failure (9.6% vs. 7.

70 Compared with metallic EES, the BVS appears to be associated with both

71 k interactions between aryl moieties and the metallic electrodes are responsible for the observed phe

72 O for the synthesis of dimethyl carbonate on metallic electrodes at low overpotentials.

73 developed for homogeneous liquid mercury or metallic electrodes, are difficult to adapt to the spati

74 nsity wave-like Fermi surface instability in metallic electron doped Sr3Ir2O7 at temperatures (TDW) c

75 has been believed that lithium, the simplest metallic element, has a complicated ground-state crystal

76 Maillard browning induced in the presence of metallic elements.

77 for monitoring an object surrounded inside a metallic enclosure.

78 o predict the time-dependent accumulation of metallic engineered nanomaterials (ENMs) across environm

79 ogress in assessing the fate and toxicity of metallic engineered nanomaterials in the soil environmen

80 assigned to everolimus-eluting Absorb BVS or metallic everolimus-eluting stents (EES) and followed up

81 ss of thrombotic complications compared with metallic everolimus-eluting stents (EES).

82 In the reaction zone, there are metallic Fe and Fe-Si beads, aluminous spinel rinds on t

83 2-61.7 GPa, where a mixed semiconducting and metallic feature is observed due to the coexisting low-

84 Spin Seebeck effect (SSE) measured for metallic ferromagnetic thin films in commonly used longi

85 g theories of light-material interactions in metallic ferromagnets and multilayers.

86 ons.Owing to their conductivity, low-damping metallic ferromagnets are preferred to insulating ferrom

87 This record low damping for metallic ferromagnets offers new opportunities for charg

88 e analyse the mechanical interaction between metallic fibre networks under magnetic actuation and a m

89 in SP resonances supported by a 20-nm-thick metallic film of indium tin oxide (ITO), a plasmonic mat

90 Even well-annealed single-grain metallic films contain dislocation densities of about 10

91 nic and thermal transport properties of this metallic fluid are of fundamental interest to understand

92 wires were synthesized by a novel method of metallic-flux nanonucleation.

93 r precious metal ions from solution in their metallic form, which are immobilized on the liquid metal

94 during plastic deformation of Zr-based bulk metallic glass (BMG).

95 allization phenomena at the nanoscale, using metallic glass (MG) nanorods and in situ transmission el

96 we deposit a 200 nm-thick Zr-based thin-film metallic glass (TFMG), which acts as an effective diffus

97 rphic transition in La32Ce32Al16Ni5Cu15 bulk metallic glass and can shed new light on the mechanisms

98 g method to join Pd43Cu27Ni10P20 (at.%) bulk metallic glass and characterized the properties of the j

99 strates some structural homology between the metallic glass and its high temperature crystalline phas

100 Pressure-induced polyamorphism in Ce-based metallic glass has attracted significant interest in con

101 The Yb62.5Zn15Mg17.5Cu5 metallic glass is investigated using synchrotron x-ray t

102 calorimetry has been reported in a number of metallic glass materials in which a broad exothermal pea

103 0Ni5 target, and finally resulted in ordered metallic glass nanotube (MGNT) arrays after removal of t

104 complex size effects from one such class of metallic glass nanowires prepared by casting using molec

105 combined with the previous reports on other metallic glass systems, demonstrates that pressure induc

106 Molecular processes of creep in metallic glass thin films are simulated at experimental

107 This discovery in Yb-based metallic glass, combined with the previous reports on ot

108 dict the evolution of macroscopic state in a metallic glass, such as ageing and rejuvenation, through

109 he polyamorphism of La32Ce32Al16Ni5Cu15 bulk metallic glass, the acoustic velocities, measured up to

110 Bulk metallic glasses (BMGs) and nanocrystalline metals (NMs)

111 ructural responses of neutron irradiation in metallic glasses (MGs) have been investigated by making

112 The glass forming ability (GFA) of metallic glasses (MGs) is quantified by the critical coo

113 All metallic glasses (MGs), irrespective of their compositio

114 over fractal models of packing structure in metallic glasses (MGs).

115 parate systems - granular materials and bulk metallic glasses - we show evidence that not only the st

116 he full time evolution of avalanches in bulk metallic glasses and granular materials, we uncover a re

117 rance of shear bands of the type observed in metallic glasses deforming under mechanical stress.

118 ping, weakening and inertial effects in bulk metallic glasses have strikingly similar effects on the

119 Fluctuation electron microscopy of bulk metallic glasses of CuZrAl(Ag) demonstrates that medium-

120 ate the structure and hence the stability of metallic glasses through heat treatment.

121 of polyamorphism and structural evolution in metallic glasses under pressure.

122 ized by four decades long studies of Pd-Ni-P metallic glasses, arguably the best glass-forming alloys

123 eneral behavior for typical lanthanide based metallic glasses.

124 vides a practical viable method to join bulk metallic glasses.

125 ligands for functionalizing and stabilizing metallic gold in the form of planar gold surfaces and go

126 r, which are in contrast to the behaviour of metallic gold nanoparticles.

127 n a marked contrast with previously-explored metallic gratings, we observe the emergence of a much st

128 ers, providing more flexible tunability than metallic gratings.

129 A bioresorbable metallic heater was patterned directly on the nanofibrou

130 A bioresorbable metallic helical stent was explored as a new device oppo

131 Liquid metallic hydrogen (LMH) is the most abundant form of con

132 ation of the Wigner-Huntington transition to metallic hydrogen (MH).

133 ation of the Wigner-Huntington transition to metallic hydrogen at 495 gigapascals.

134 ch are close to predictions for solid atomic metallic hydrogen at these pressures.

135 Producing metallic hydrogen has been a great challenge in condense

136 Huntington dissociative transition to atomic metallic hydrogen in the laboratory.

137 Metallic hydrogen may be a room-temperature superconduct

138 is thus the closest analogue to solid atomic metallic hydrogen yet to be synthesized and characterize

139 ine the optical conductivity of LMH and find metallic hydrogen's static electrical conductivity to be

140 zhkin present comments on our observation of metallic hydrogen.

141 n larger, highly (18)F-FDG-avid lesions, the metallic implants had only a limited effect.

142 icial signal voids in the AC map to simulate metallic implants in standard anatomic areas.

143 ffect of susceptibility artifacts related to metallic implants on adjacent metabolically active lesio

144 method for thermal destruction of biofilm on metallic implants using high-frequency (>100 kHz) altern

145 ating the attenuation map in the presence of metallic implants, to be used for whole-body attenuation

146 ested on 11 subjects presenting 13 different metallic implants, who underwent CT and PET/MR scans.

147 and linear attenuation coefficient (LAC) of metallic implants.

148 onal theory calculations show that Ti3 CN is metallic, in contrast to other 2D saturable absorber mat

149 techniques is presented, such as inserting a metallic interlayer, a molecular self-assembled monolaye

150 o this is whether the distribution of mobile metallic ions is random or not.

151 shell is determined by the concentration of metallic ions used in the solution during the galvanic r

152 architecture of an iridium oxide shell on a metallic iridium core, formed through the fast dealloyin

153 match seismic data, implying the presence of metallic iron in an isochemical mantle.

154 binding studies and never without synthetic metallic labels.

155 This avoids formation of metallic Lewis adducts and confers the Au(I)/Pt(0) pair

156 several decades because of safety concerns, metallic Li is now ready for a revival, thanks to the de

157 The use of metallic Li is one of the most favoured choices for next

158 acial behavior of garnet SSE in contact with metallic Li through in situ monitoring of Li plating-str

159 We attribute the metallic-like edge conductance to a nontrivial topology

160 ing theoretical models that LMH is an atomic metallic liquid.

161 alent liquids, but has not been observed for metallic liquids.

162 al that the oxide coating enables wetting of metallic lithium in contact with the garnet electrolyte

163 rier to ion transport, comparable to that of metallic magnesium.

164 Thus, there is a need for a metallic material system that can overcome these perform

165 may alleviate radiation damage in irradiated metallic materials as free surface are defect sinks.

166 the design of radiation-tolerant nanoporous metallic materials for advanced nuclear reactor applicat

167 long-standing strength-ductility tradeoff of metallic materials in general.

168 servations show that texturally equilibrated metallic melt does not wet the silicate grain boundaries

169 Evidence for the percolation of metallic melt is provided by X-ray microtomography of pr

170 with the ability to bind to a wide range of metallic, metal oxide, mineral, and polymer substrates.

171 ory, for a compacted dimension realized in a metallic metasurface periodically structured in the form

172 Metallic microparticles can acquire remarkable nanoscale

173 y moving the height of the nanowires above a metallic mirror.

174 a parallel bundle of sub-nanometer-diameter metallic Mo6 Te6 nanowires (NWs) driven by catalyzer-fre

175 With metallic MoB, the introduction of n-type semiconductive

176 lly exfoliated nanosheets of two-dimensional metallic molybdenum disulfide (MoS2) on thin plastic sub

177 he electronic properties of the 2D MoS2 with metallic MoS2 showing high responsivity and the semicond

178 itation of dipolar and CTP resonant modes in metallic nanodimers bridged by phase-change material (PC

179 chieved for the atomic-level manipulation of metallic nanomaterials.

180 ity even under the resonant condition of the metallic nanoparticle.

181 EM) analysis confirmed the presence of small metallic nanoparticles (5.4 +/- 1.4 nm for long axis / 3

182 cing hybrid random antenna arrays with small metallic nanoparticles and ultra-thin nonlinear optical

183 erent nanomaterials such as nanochannels and metallic nanoparticles for the development of innovative

184 of reports are limited to the replacement of metallic nanoparticles or metal surfaces.

185 ks, as well as careful control of the dopant metallic nanoparticles or semiconductors, are believed t

186 ally robust and can act as templates to host metallic nanoparticles such as gold and silver.

187 ght of around 125 nm are used, which utilize metallic nanoparticles to create a hotspot where fluores

188 rality of NPCs can be adaptively imparted to metallic nanoparticles, covering them to generate struct

189 lution as an ionic species and does not form metallic nanoparticles.

190 ounts due to the formation of self-nucleated metallic nanoparticles.

191 optical control of the gigahertz response of metallic nanostructures, opening the door to new optomec

192 deep subdiffraction confinement assisted by metallic nanostructures.

193 ucing agent that can be generalized in other metallic nanowire syntheses.

194 s are attributed to the mixed covalent/ionic/metallic nature of the bonding.

195 The functional groups preserve the metallic nature of the MoS2 nanosheets, inhibiting conve

196 thography to fabricate electrical wires from metallic NCs.

197 ites are successfully developed by embedding metallic Ni nanowires within an insulating poly(vinylide

198 o a continuous aqueous phase with the use of metallic nickel (Ni) nanoparticles (NPs) under condition

199 n a maximization of the amount of accessible metallic nickel in the form of small nanoparticles while

200 oxygen electrocatalyst consisting of porous metallic nickel-iron nitride (Ni3 FeN) supporting ordere

201 chanism to afford synthesis of group 3-based metallic nitride clusterfullerenes.

202 cal seafloor imaging allows quantifying poly-metallic nodule abundance at spatial scales from centime

203 Poly-metallic nodules are a marine resource considered for de

204 The metallic NWs can act as an efficient hole injection laye

205 he presence of a small band-gap and thus non-metallic or molecular-like behaviour.

206 bility of untethered communication through a metallic or nonmetallic barrier.

207 er fashion, biomolecules and nanostructures (metallic or not) may amplify the SPR signal and improve

208 ation processes on commercially pure Mg with metallic or oxidized surfaces and on MgY alloy with oxid

209 of organic/inorganic hybrid perovskites with metallic or semiconducting phases of 2D MoS2 nanosheets

210 Recently, powders of a metallic oxide (Sr1-xNbO3, 0.03<x<0.20) were reported to

211 Metallic palladium surfaces are highly selective in prom

212 small organic molecules, the authors prepare metallic paper electrodes for supercapacitors with high

213 rt the insulating paper to the highly porous metallic paper with large surface areas that can functio

214 The maximum power and energy density of the metallic paper-based supercapacitors are estimated to be

215 al and pseudocapacitive nanoparticles on the metallic papers can remarkably increase the areal capaci

216 Adding magnetic and/or metallic particles to cement mixes changes the propertie

217 ingle-atom catalysts but often also comprise metallic particles.

218 ayered black phosphorus (BP) transistor with metallic PGex contacts formed by rapid thermal annealing

219 TaS2 is driven by coupling to the metastable metallic phase coexisting within the Mott commensurate C

220 cesses however, tracking the early stages of metallic phase nucleation is challenging.

221 t is slightly worse compared to the pristine metallic phase of MoS2.

222 veal a transition from a semiconducting to a metallic phase with decreasing temperature, which is unp

223 ses, probes the subsequent relaxation in the metallic phase, and measures the phase-transition dynami

224 When VO2 is in the metallic phase, Fabry-Perot type of resonance occurs and

225 For both the insulating and the metallic phase, the formation of the transient configura

226 ion from an antiferromagnetic insulator to a metallic phase.

227 xcitation process in both the insulating and metallic phases, probes the subsequent relaxation in the

228 characterize its paramagnetic insulating and metallic phases, showing the proximity of mackinawite to

229 .g. quantum efficiency (QE) in grating-based metallic photocathodes.

230 Here we discuss inorganic, metallic, polymeric, and carbon-based NEs for their outs

231 Metallic powder bed additive manufacturing is capable of

232 asma sintering (SPS) using ZrO2 and lamellar metallic powders of tantalum or niobium (20 vol.%) as st

233 an on-off ratio 5), in contrast to the pure metallic pristine sample.

234 a multipolar nematic phase of matter in the metallic pyrochlore Cd2Re2O7 using spatially resolved se

235 itional possibility for the phase diagram of metallic quantum ferromagnets.The study of phase transit

236 iform current steps are indicative of NPs of metallic radii in agreement with those determined by tra

237 ionally simple conditions without the aid of metallic reagents and toxic oxidants.

238 S substantial changes would be seen when the metallic regime was tuned towards an electronic state th

239 tegration of VO2 structures and conventional metallic resonating components can enable a class of hig

240 tetragonal FeS shows both semiconducting and metallic responses in contrast to tetragonal FeSe which

241 netic moment of 2D Ti-based TMDs toward half-metallic room-temperature ferromagnetism character.

242 on of 3-indoxylphosphate and silver nitrate, metallic silver is determined by anodic stripping voltam

243 ere 18-24% lower than the nominal density of metallic silver, with an overall mean value of 7900 +/-

244 effects distinct from delivered particulate metallic silver.

245 (CO and H2S) that may interact with embedded metallic sites.

246 Modern planar inductors consist of metallic spirals that consume significant chip area, res

247 ecord pressure nor the phase transition to a metallic state are supported by data and that the data c

248 uctance counter-intuitively decreases in the metallic state relative to the insulating state.The deve

249 erconductivity and appears upon entering the metallic state with the dynamical Jahn-Teller effect as

250 within the traditionally thermally unstable metallic state.

251 he charge gap between the Mott insulator and metallic states can be closed near 6 GPa.

252 Prominent examples are ill-understood metallic states in d- and f-band compounds near Mott-lik

253 Unusual metallic states involving breakdown of the standard Ferm

254 Semiconductive behavior and proximity to metallic states with nodal superconductivity mark this d

255 rbable vascular scaffold (924 patients) or a metallic stent (921 patients).

256 A 1-year follow-up, polymer-free metallic stent coated with biolimus-A9 followed by 1-mon

257 sorbable scaffold with an everolimus-eluting metallic stent in the context of routine clinical practi

258 gher incidence of device thrombosis than the metallic stent through 2 years of follow-up.

259 ble scaffold and the patients who received a metallic stent.

260 trials comparing BVS with everolimus-eluting metallic stents (EES) raised concerns about BVS safety.

261 tenting (PTBS) with uncovered selfexpandable metallic stents (SEMS), and to identify predictors of su

262 vascular scaffold (BVS), no comparison with metallic stents has been conducted in a randomized fashi

263 ound to have expansion properties similar to metallic stents, utilizing materials which are typically

264 interstitial TWIP-TRIP-HEA thus unifies all metallic strengthening mechanisms in one material, leadi

265 Herein, a half-metallic structure of TMDs is successfully developed by

266 This is achieved by fabricating a floating metallic structure that concentrates the pyroelectric ch

267 In the second case, a multi-metallic structure was fabricated via laser 3D printing

268 lied to explore a new Ti6Al4V to SS316 multi-metallic structure.

269 ted by combining active media with patterned metallic structures.

270 ectric ridge between a dielectric slab and a metallic substrate, a hybrid dielectric-loaded nanoridge

271 MA is placed at a nanometric distance from a metallic substrate, the strong and coherent interaction

272 on errors induced by the interaction between metallic substrates and single fluorophores.

273 tic moment and electronic spin in underlying metallic substrates.

274 optical resonators consisting of an array of metallic subwavelength nanowires on a transparent substr

275 ased the mass loss for the same alloy with a metallic surface (surface oxides were removed).

276 Nanoparticles attached just above a flat metallic surface can trap optical fields in the nanoscal

277 both enhanced at the borders of oxidized and metallic surface regions.

278 These findings show that the metallic surface states in topological insulators can ex

279 Topological crystalline insulators possess metallic surface states protected by crystalline symmetr

280 insulating bulk and topologically protected metallic surface states.

281 Thus, characterizing metallic surface structures under reaction conditions at

282 re reactive than the corresponding O-covered metallic surfaces under similar conditions, although sti

283 ngle-wall CNTs (SWCNT) films with controlled metallic SWCNT concentrations and doping degree and (2)

284 Strong electron interactions can drive metallic systems toward a variety of well-known symmetry

285 bounded between a resonant metasurface and a metallic thin-film reflector.

286 y, (Sb1-x Bi x )2Te3 was introduced as a non-metallic TI whose carrier type can be tuned from n to p

287 rance of such iridescent films, ranging from metallic to pixelated or matt textures, paving the way f

288 underlying band structure is tuned from the metallic to the insulating side of the gap opening.

289 ses, emerging percolating clusters support a metallic transport across the entire film.

290 tron spectroscopy showed that the surface is metallic under reaction conditions.

291 We demonstrate a useful yield of 24% for metallic uranium.

292 mperatures ranging from 240 to 340 kelvin in metallic vanadium dioxide in the vicinity of its metal-i

293 the thermal conductance of gold and platinum metallic wires down to single-atom junctions.

294 rphs, collectively tagged borophene, are all metallic with high free charge carrier concentration, po

295 ressure of 495 gigapascals, hydrogen becomes metallic, with reflectivity as high as 0.91.

296 338 longhorned beetles (Cerambycidae) and 38 metallic wood boring beetles (Buprestidae) intercepted i

297 Thus, the novel metallic wood composite boasts an extraordinary anisotro

298 The anisotropic functionality of the metallic wood enables it to be used for thermal manageme

299 The highly anisotropic metallic wood serves as an example for further anisotrop

300 Here, a metallic wood with metal continuously filling the wood v