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1 ion, using novel collimator designs based on tungsten.
2 ce and Fermi-velocity distribution vF(kF) of tungsten.
3 roximately -0.5 by incorporating oxygen into tungsten.
4 , such as arsenic, antimony, molybdenum, and tungsten.
5 ation mechanism in nanoscale crystals of BCC tungsten.
6 igh-pressure helium bubbles in plasma-facing tungsten.
7 roughening were observed in the cold rolled tungsten.
8 or two different grades of ultrafine-grained tungsten.
9 balt (0.5-6 nM), molybdenum (10-5600 nM) and tungsten (0.3-8 nM) in Hydrate Ridge sediment porewaters
11 terium Geobacter metallireducens harboring 4 tungsten, 4 zinc, 2 selenocysteines, 6 FAD, and >50 FeS
12 ion, we assessed functional neurotoxicity of tungsten, a common microelectrode material, and two cond
13 dynamic stability and magnetic properties of tungsten adsorbed tri-vacancy fluorinated (TVF) graphene
19 vide a lower bound to the coherence time for tungsten analogues due to a destructive interference fro
20 lium antimonide cell paired with a broadband tungsten and a radiatively-optimized Drude radiator are
22 ments used in high-temperature alloys (e.g., tungsten and molybdenum), to vulnerability to supply res
23 is of pi/pi* orbital energy matching between tungsten and organic PE fragments and the introduction o
24 igands within complexes based on molybdenum, tungsten and ruthenium has led to reactivity and selecti
28 al physiological function (chromium, nickel, tungsten, and vanadium), and 12 with known toxicity (ant
36 The key limiting factors for the Drude- and tungsten-based devices are respectively the recombinatio
38 eous thermal plasmon emission, we engineer a tungsten-based thermal emitter, fabricated in an industr
40 The optical properties of particularly the tungsten-based transition-metal dichalcogenides are stro
41 s into a polyoxometalate cage, a new type of tungsten-based unconventional Dawson-like cluster, [W18O
42 d graphene (G) sandwiched between beta-phase tungsten (beta-W) films of 15, 30 and 40 nm thickness.
43 bunit of this complex harbors an active site tungsten-bis-pyranopterin cofactor with the metal being
44 pening process was efficiently promoted by a tungsten/bis(hydroxamic acid) catalytic system, furnishi
47 ent experiments reveal that micro-structured tungsten can exhibit significant deviation from the blac
48 sted that non-3d high-valency metals such as tungsten can modulate 3d metal oxides, providing near-op
51 pported tungsten carbide (WC) and molybdenum tungsten carbide (Mo(x)W(1-x)C) nanoparticles are highly
53 s of three different metallic nanoparticles, tungsten carbide (WC), silver (Ag) and copper (Cu), in c
57 n plastic blocks, cured and sectioned with a tungsten carbide knife to obtain mineralized bone sectio
59 drawn nanowires can be alleviated by adding tungsten carbide nanoparticles to the metal core to arri
63 have solved this challenge and now report a tungsten catalyst supported by a tetraanionic pincer lig
64 n-to-air atmosphere between a solid pin type tungsten cathode and a liquid drop placed on a graphite
66 ish benzene ring reduction at an active-site tungsten cofactor; however, the mechanism and components
69 nyl isocyanide (CNdipp) have been developed; tungsten complexes incorporating these oligoarylisocyani
70 of the valley polarization as a function of tungsten concentration, where 40% tungsten incorporation
71 ions of climbing prismatic loops in iron and tungsten, confirming that this novel form of vacancy-fre
72 y a member of the TF family, named TaoR (for tungsten-containing aldehyde oxidoreductase regulator).
73 acterial genes for molybdenum-containing and tungsten-containing enzymes are often differentially reg
75 t work, we conclude that all molybdenum- and tungsten-containing formate dehydrogenases and related e
76 lectively, and efficiently interconverted by tungsten-containing formate dehydrogenases that surpass
77 x chemistry, and excited-state properties of tungsten-containing oligo-phenylene-ethynylenes (OPEs) o
78 aspect to its redox metabolism, involving a tungsten-containing oxidoreductase of unknown function.
79 for solid solutions of tungsten in ReB2 with tungsten content up to a surprisingly large limit of nea
80 along both the a- and c-axes with increasing tungsten content, as evaluated by powder X-ray and neutr
81 th and resistivity are compared to isotropic tungsten-copper composites fabricated by standard powder
82 s, we demonstrate on the specific example of tungsten-copper composites the effect of anisotropy on t
87 olarized emission in a molybdenum diselenide/tungsten diselenide (MoSe(2)/WSe(2)) heterobilayer with
88 nterfaces, in tungsten disulfide (WS(2)) and tungsten diselenide (WSe(2)) contacted with indium alloy
89 ed spirals of tungsten disulfide (WS(2)) and tungsten diselenide (WSe(2)) draped over nanoparticles n
93 leveraging the atomically thin semiconductor tungsten diselenide (WSe2) as a host for quantum dot-lik
94 ily such as molybdenum disulphide (MoS2) and tungsten diselenide (WSe2), as well as other emerging tw
95 operties of mono and few-layer TMDs, such as tungsten diselenide (WSe2), by controlling the defects,
98 show that the Type-II band-alignment between tungsten diselenide and chromium triiodide can be exploi
100 ic arrays of hundreds of quantum emitters in tungsten diselenide and tungsten disulphide monolayers,
102 monic sideband (HSB) generation in monolayer tungsten diselenide creates distinct electronic interfer
103 mitters in atomically thin materials such as tungsten diselenide have been demonstrated to host optic
104 alley-polaritons by embedding a monolayer of tungsten diselenide in a monolithic dielectric cavity.
105 e probed the momentum state of excitons in a tungsten diselenide monolayer by photoemitting their con
106 y thin crystalline semiconductor--that is, a tungsten diselenide monolayer--is non-destructively and
108 illars to coordinate the spatial location of tungsten diselenide quantum emitters, we uncover the pos
109 ron-hole pairs in the layered dichalcogenide tungsten diselenide while a strong terahertz field accel
110 ical to this second approach is to interface tungsten diselenide with other van der Waals materials w
114 tion of moire superlattice exciton states in tungsten diselenide/tungsten disulfide (WSe(2)/WS(2)) he
115 insulating states at fractional fillings of tungsten diselenide/tungsten disulfide moire superlattic
117 onstrated by growing supertwisted spirals of tungsten disulfide (WS(2)) and tungsten diselenide (WSe(
118 ts, indicative of defect-free interfaces, in tungsten disulfide (WS(2)) and tungsten diselenide (WSe(
119 operates at room temperature using monolayer tungsten disulfide (WS(2)) as the emissive material.
120 ensurate molybdenum diselenide (MoSe(2)) and tungsten disulfide (WS(2)) monolayers, we demonstrate th
123 s of biosurfactant stabilized/functionalized tungsten disulfide (WS(2)-B) quantum dots (QDs) and its
124 Here, the growth of oxidation-resistant tungsten disulfide (WS2 ) monolayers on graphene is demo
125 MDs) such as molybdenum disulfide (MoS2) and tungsten disulfide (WS2) are envisioned to present unpre
128 nally large Bloch-Siegert shift in monolayer tungsten disulfide (WS2) under infrared optical driving.
129 attice exciton states in tungsten diselenide/tungsten disulfide (WSe(2)/WS(2)) heterostructures in wh
130 also demonstrate that optical properties of tungsten disulfide can be effectively tuned by carriers
133 tion of light guiding in an atomically thick tungsten disulfide membrane patterned as a photonic crys
135 nsfer at a 2D/0D heterostructure composed of tungsten disulfide monolayers (2D-WS2) and a single laye
139 nergy of oxygen molecules on graphene and 2D tungsten disulfide using temperature-programmed terahert
144 quantum emitters in tungsten diselenide and tungsten disulphide monolayers, emitting across a range
146 f monolayer molybdenum disulphide (MoS2) and tungsten disulphide, grown directly on insulating SiO2 s
149 study, we designed a photodetector based on tungsten ditelluride (WTe(2)) with carefully fabricated
153 The structure is based on thin films of tungsten-doped vanadium dioxide where the tungsten fract
154 s from pairs of sensilla impaled by the same tungsten electrode to demonstrate that direct electrical
155 delivery of a high-voltage nsEP to cells by tungsten electrodes creates a multitude of biophysical p
156 tanium ethoxide and dopant concentrations of tungsten ethoxide at 500 degrees C from a toluene soluti
157 ntation of transformed Escherichia coli with tungsten facilitated the replacement of molybdenum in re
158 Here, we show that a plain incandescent tungsten filament (3,000 K) surrounded by a cold-side na
159 While the incorporation of oxygen into the tungsten films leads to significant changes in their mic
160 he results show that graphene inserted among tungsten films plays a dominant role in reducing radiati
161 energy landscape for self climb in iron and tungsten, finding a simple, material independent energy
163 One of the most interesting materials is tungsten, for which large spin-orbit torques have been f
164 of tungsten-doped vanadium dioxide where the tungsten fraction is judiciously graded across a thickne
166 ient photochemical vapor generation (PVG) of tungsten has been achieved for the first time using a 19
167 , promethium, and samarium), cobalt, silver, tungsten, heavy rare earth elements (yttrium, europium,
171 of helium gas bubble superlattices within a tungsten host matrix to uncover mechanistic insight into
172 n transfer (PCET) was studied in a series of tungsten hydride complexes with pendant pyridyl arms ([(
173 f zirconium hydride, probably facilitated by tungsten hydride which was formed at this temperature.
174 d oxidative addition of the Si-H bond to the tungsten(II) center, there is strong experimental and NM
175 -H bond is heterolytically cleaved to form a tungsten(II) hydride and a silylium ion, which is stabil
176 ure can be maintained for solid solutions of tungsten in ReB2 with tungsten content up to a surprisin
177 nt equations of state of gold, platinum, and tungsten in static experiments up to 500 gigapascals.
178 unction of tungsten concentration, where 40% tungsten incorporation is sufficient to achieve valley p
179 nolytic cleavage of epothilone B followed by tungsten-induced deoxygenation of the epoxide moiety.
180 ntity of the sixth ligand of the active-site tungsten ion together with the interplay of the electron
182 udies reveal a synergistic interplay between tungsten, iron, and cobalt in producing a favorable loca
193 nt tungsten-to-oxygen silyl migration in the tungsten(IV) silyl hydride is also energetically feasibl
195 to dramatically affect the microstructure of tungsten, leading to bubble growth, blistering, and/or t
198 photocathodes are synthesized by evaporating tungsten metal in an ambient of ethylene gas to form tun
201 ms are addressed by introducing a mixture of tungsten microparticles dispersed within a LM matrix (LM
202 assette was introduced into callus cells via tungsten microparticles, and stable transformants were s
206 In this article, we fabricate chromium and tungsten nano-antennas and demonstrate that they can han
208 cribed, which applies high voltage between a tungsten nanotip and a metal plate to generate a plasma
210 strate the synthesis of Pt shell on titanium tungsten nitride core nanoparticles (Pt/TiWN) by high te
212 the superhard metals, the highest boride of tungsten--often referred to as WB4 and sometimes as W(1-
213 ns of aromatic ligands eta(2)-coordinated to tungsten or molybdenum and the use of these reactions in
214 ith 1T' structure, namely, 1T'-MX2 with M = (tungsten or molybdenum) and X = (tellurium, selenium, or
216 ue by studying Li-ion insertion in hexagonal tungsten oxide (h-WO(3)) nanorods during chronoamperomet
220 by a porous shell growing at the surface of tungsten oxide and shielding the wire surface from flowi
221 is article, we study three different niobium-tungsten oxide crystallographic shear phases (Nb(12)WO(3
223 the fabrication of thick, vertically aligned tungsten oxide nanochannel layers, with pore diameter of
225 important structural promotional effect that tungsten oxide offers for the SCR reaction by V(2) O(5)
232 contrast to what happens in materials (like tungsten oxide) susceptible to ionic electromigration an
234 e report an approach to synthesize molecular tungsten-oxide-based pentagonal building blocks, in a ne
236 Treating 3 with acid chlorides provides the tungsten oxo chloride species [CF3-ONO]W(O)Cl (4) and di
238 Despite the importance of the heterogeneous tungsten-oxo-based olefin metathesis catalyst (WO(3)/SiO
239 ious carbonyl-containing substrates provides tungsten-oxo-vinyl complexes upon oxygen atom transfer.
240 We report the colloidal synthesis of an ~3 tungsten-oxygen (W-O) layer thick (~1 nm), two-dimension
242 Furthermore, the performance of different tungsten period-thicknesses in radiation tolerance is sy
243 ompare thermal radiation from a micro-cavity/tungsten photonic crystal (W-PC) and a blackbody, which
244 ardment under tokamak-relevant conditions on tungsten plasma-facing materials in a magnetic fusion en
245 in characterizing the mechanical behavior of tungsten polycrystalline samples with ion-irradiated sur
249 allium (Ptrend = 0.13), 2.18 (1.51-3.15) for tungsten (Ptrend < 0.01), and 1.46 (1.09-1.96) for urani
250 tion with the Drude radiator outperforms the tungsten radiator, dominated by frustrated modes, only f
251 nium-182 in mantle domains with high hafnium/tungsten ratios, were created during the first ~50 milli
253 itation to collect particles on the tip of a Tungsten rod, and subsequently, by flowing liquid over t
254 s in stereoretentive olefin metathesis using tungsten, ruthenium, and molybdenum catalysts are presen
255 metal in an ambient of ethylene gas to form tungsten semicarbide (W2C) thin films on top of p-type s
256 able materials (e.g., magnesium, molybdenum, tungsten, silicon, germanium, silicon dioxide, silicon n
257 ost promising elemental materials, including tungsten, silicon, graphite, diamond and graphene, for p
259 of aldehyde oxidoreductase aor and represses tungsten-specific ABC-type transporter tupABC genes unde
262 n ultra-thin bilayer of copper and amorphous tungsten suboxide, which derives its remarkable optical
264 cused attention on the supply chains of tin, tungsten, tantalum, and gold (3TG), specifically those o
265 The model estimates the upper bound of tin, tungsten, tantalum, and gold use within ICT products to
271 , nanochannels, nanopores) on metals such as tungsten that up to now were regarded as very difficult
273 ions of irradiated water targets showed that tungsten thicker than 1.4 mm resulted in fewer photons a
278 the spin texture in iron/nickel bilayers on tungsten to show that chiral domain walls of mixed Bloch
279 sisting of oxidative addition and subsequent tungsten-to-oxygen silyl migration in the tungsten(IV) s
280 the structural and electronic properties of tungsten trioxide (WO3) surfaces interfaced with an IrO2
281 classical but inert transition metal oxide, tungsten trioxide, to be an efficient electrocatalyst fo
282 on of ultrafine- and nanocrystalline-grained tungsten under conditions similar to those in a reactor,
288 ray photoelectron spectroscopy, the as-grown tungsten(VI) sub-oxide was identified as monoclinic W18O
290 ly tested on short-lived molybdenum (Mo) and tungsten (W) isotopes to the preparation of a carbonyl c
291 lds on previous studies on military-relevant tungsten (W) to more thoroughly explore environmental pa
294 a recent study on 3000 appm helium-implanted tungsten (W-3000He), we hypothesized helium-induced irra
298 phological transformations of the surface of tungsten wires in a specially designed electrochemical c
299 nd bis-terphenyl complexes of molybdenum and tungsten with general composition M2(Ar')(O2CR)3 and M2(