ライフサイエンスコーパス: alloy

1 n induced by the formation of a CuAg surface alloy.

2 y the reduced Fe restores the original Ni-Fe alloy.

3 of Ge into BP and the formation of the PGex alloy.

4 dealloying and formation of a Ni-richer NiFe alloy.

5 nt) of the two end-members of the Si1-x Ge x alloy.

6 is comparable to that of bulk InGaN ternary alloy.

7 + Al9(Co, Ni)2 + unknown phase] for the 84Al alloy.

8 tion behavior from a supersaturated quenched alloy.

9 binaries, and to a more complex Ni40Fe40Cr20 alloy.

10 ure in the prototype CoCrFeMnNi high-entropy alloy.

11 hemically leaching lithium from the Li13 Si4 alloy.

12 at 800 K for the Ti0.5 Hf0.5 NiSn0.98 Sb0.02 alloy.

13 ll lead a better swelling resistance for ODS alloy.

14 lic glasses, arguably the best glass-forming alloys.

15 f the deformation mechanisms of shape memory alloys.

16 ment for the continued study of ZnSnxGe1-xN2 alloys.

17 c properties as the conventional III-Nitride alloys.

18 microalloying enhances creep performance of alloys.

19 bic C15 Laves phases commonly found in metal alloys.

20 properties superior to those of conventional alloys.

21 radiation resistant oxide-dispersed ferritic alloys.

22 the major elements (Cu, Sn, and Pb) in these alloys.

23 ors, frustrated magnets, and dilute magnetic alloys.

24 tructured Ti1-x Hfx NiSn1-y Sby half-Heusler alloys.

25 erface between CuAl5 and stainless steel 304 alloys.

26 e the photoluminescence properties of GaAsBi alloys.

27 ep resistance compared to monolithic Ti6Al4V alloys.

28 , coupled with simulations in ZrCu amorphous alloys.

29 ct the stability of the omega-phase in these alloys.

30 gy of entropy stabilization of high-symmetry alloys.

31 ritical role in the design of multicomponent alloys.

32 oncept may be applied to many other metallic alloys.

33 n complex organic matter and nanosized Ni-Fe alloys.

34 ichment in the silicate melt surrounding the alloys.

35 h models for sensitisation in 5xxx series Al-alloys.

36 thermore, due to the band convergence of the alloyed 3% mol.

37 n, cobalt, nickel, copper, and nickel-cobalt alloy), accomplished by a facile low-temperature ammoniu

38 e in the Ti content over the range of master alloy additions, causes the grain number density to incr

39 ity aluminium with a range of Al3Ti1B master alloy additions.

40 %) ternary alloy after laser surface remelting.

41 ystallization of three multicomponent glassy alloys, Al86Y7Ni5Co1Fe0.5Pd0.5, Al85Y8Ni5Co1Fe0.5Pd0.5 a

42 tive metal, can be substantially improved by alloying, alloy stability remains a concern.

43 ment compared to that provided by the master alloy alone.

44 This alloy also exhibits compromised foreign body response (F

45 Alloying also increases the hole mobility to 560 cm(2) V

46 ure is incorporated into a prototype Heusler alloy and MgO barrier based magnetic tunnel junction, wh

47 Alloy and microstructure optimization have led to impres

48 Joining titanium alloy and stainless steel is becoming an urgent need sin

49 s are good contributions in joining titanium alloy and stainless steel.

50 h-capacity hybrid In-Li anodes that use both alloying and plating approaches for charge storage.

51 sample is further reduced to 0.7 W/m.K by Sb alloying and spark plasma sintering (SPS), which introdu

52 gy intensive manufacturing processes such as alloying and spark plasma sintering.

53 microstructural design approaches for Ti-Nb alloys and beta-stabilized Ti-alloys in general.

54 nufacturing is applicable to a wide range of alloys and can be implemented using a range of additive

55 se cobalt-based active sites, including FeCo alloys and Co4 N nanoparticles, plays a critical role in

56 on the birefringence of the dilute-As GaNAs alloys and comparison to other experimentally characteri

57 Examples are shape memory alloys and high strength steels, which together stand fo

58 es, leading to the discovery of high-entropy alloys and high-entropy oxides.

59 scopic imaging confirms the formation of TMD alloys and identifies a random distribution of the alloy

60 -oxidation reaction history between Al-Cu-Fe alloys and silicate melt.

61 [alpha-Al + compounds] for the 86Al and 85Al alloys, and [am] --> [am + alpha-Al + cubic AlxMy (M = Y

62 eads, aluminous spinel rinds on the Al-Cu-Fe alloys, and Al2O3 enrichment in the silicate melt surrou

63 rrosion) of polycrystalline nonnoble metals, alloys, and inorganic materials within confined interfac

64 iously observed in crystallization of glassy alloys, and seems to originate from instability of the m

65 foils inheriting the desirable properties of alloy anodes and pure metal anodes.

66 Alloy anodes are one promising option, but without pre-s

67 as the isotopic shifts associated with such alloying are small.

68 ns show that the active metals in the molten alloys are atomically dispersed and negatively charged.

69 ZnSnxGe1-xN2 alloys are chemically miscible semiconductor compounds w

70 Magnesium (Mg) alloys are promising materials for biodegradable implant

71 ectic Ga-In (EGaIn) and Ga-In-Sn (Galinstan) alloys are typically used due to their high conductivity

72 modulated reflectivity measurements of ZnOSe alloys are used to demonstrate a splitting of the valenc

73 lence subband offer a potential of using the alloy as an intermediate band semiconductor for solar po

74 e we show that, self-diffusion in Si1-x Ge x alloys as a function of temperature and Ge concentration

75 We used nontoxic eutectic gallium-based alloys as a reaction solvent and co-alloyed desired meta

76 demonstrate the utility of composite protein alloys as inexpensive and effective means to create dura

77 s cross-cutting lower melting-point Al-Cu-Fe alloys, as well as unambiguous evidence of a reduction-o

78 efficiency and lower emission demands use of alloys at higher operating temperatures (200 degrees C-2

79 ction and morphology transition of magnesium alloys at the atomic level.

80 n up a new avenue for further development of alloy-based anodes with high capacity and long cycle lif

81 The safety and efficacy of a novel cobalt alloy-based coronary stent with a durable elastomeric po

82 The alloying behavior between FAPbI3 and CsSnI3 perovskites

83 e obtained a comprehensive classification of alloying behavior for 813 binary alloy systems consistin

84 Besides TWIP and TRIP, such alloys benefit from massive substitutional and interstit

85 an be sufficient to completely transform the alloy between its martensitic and austenitic states if t

86 tion-dependent control of thermal history in alloys beyond the surface, and utilizes additive manufac

87 e, negative stiffness state of a martensitic alloy by its coherent integration with a compatible, sta

88 s in the periodic table, their compounds, or alloys by a one-step, scalable, low-cost, and eco-friend

89 strategy for the design of ultrastrong steel alloys by high-density nanoprecipitation with minimal la

90 order of amorphous silicon oxycarbide (SiOC) alloys by using the atomic pair-distribution function (P

91 f Al-based high-strength nanostructured bulk alloys by warm working.

92 osition and the corresponding bandgap of the alloy can be continuously tuned from ReSe2 (1.32 eV) to

93 Because they are liquid-phase, these alloys can alter the electrical and thermal properties o

94 xtraordinary creep-resistance of Mg-Nd-based alloys can be correlated to the formation of nanoscale-p

95 ctive index difference between GaN and GaNAs alloys can be engineered to be up to 0.35 in the visibl

96 range can be grown on graphene using a Mo-Cu alloy catalyst.

97 eluting stents has included use of new metal alloys, changes in stent architecture, and use of biores

98 Hierarchically structured Ni-Cu alloys composed of 3D network-like microscopic branches

99 on an Al-2Cu alloy were consistent when the alloy compositions are converted to their growth restric

100 he diffusivity of hydrogen in hcp metals and alloys, considering both thermally activated hopping and

101 The Ti1-x Hfx NiSn1-y Sby alloys containing inherent atomic-scale defect disorders

102 d in silica, through capillary breakup of an alloy-core silica-cladding fiber.

103 Crystallization of microdroplets of molten alloys could, in principle, present a number of possible

104 n the enhanced performance relative to their alloy counterparts that lack elemental ordering.

105 deformation mechanisms in the medium-entropy alloy CrCoNi that exhibits one of the highest combinatio

106 acked phase of the prototypical high-entropy alloy CrMnFeCoNi.

107 The AlN/GaN digital alloy (DA) is a superlattice-like nanostructure formed b

108 The III-Nitride digital alloy (DA) is comprehensively studied as a short-period

109 was fabricated via a facile electrochemical alloying/dealloying method.

110 Here, we show that dilute alloying decreases 1's bandgap by ca. 0.5 eV.

111 ins may be a major contributing factor to Mg alloy degradation, but are not yet fully understood.

112 y relevant mixture of proteins, on Mg and Mg alloy degradation.

113 the preferred growth directions of magnesium alloy dendrite change as the type and amount of solute e

114 ther homogeneous oxides, heterojunctions, or alloys depending on the annealing temperature and compos

115 Our results have implications for alloy design as they suggest that formation of beta1-lik

116 y provide guidance for all fatigue-resistant alloy design efforts.

117 um-based alloys as a reaction solvent and co-alloyed desired metals into the melt.

118 lution phases are a current area of focus in alloy development.

119 Alloying/doping in 2D material is important due to wide

120 Here we report on the crystallization of alloyed droplets of controlled micrometer dimensions com

121 the tensile properties of the recycled Al-Si alloys due to the presence of the Fe containing intermet

122 l changes and phase transformations of Ti-Nb alloys during heating by in situ synchrotron diffraction

123 volution in alkaline media at an Inconel 625 alloy electrocatalyst during rotation at 1600 rpm.

124 Further development of Pt alloy electrocatalysts relies on the design of architect

125 and identifies a random distribution of the alloyed elements.

126 rials change, sometimes catastrophically, as alloying elements and impurities accumulate preferential

127 To understand effects of alloying elements on irradiation-induced defect producti

128 arge defect clusters, the effect of specific alloying elements on suppression of damage accumulation

129 k, we demonstrate that a liquid gold-silicon alloy established in classical vapor-liquid-solid growth

130 he effect demonstrated in a complex metallic alloy, even though the electronegativity differences wit

131 strengths in basaltic glasses and iron-rich alloys, even at high pressure.

132 results suggest that the binary and ternary alloys exhibit higher radiation resistance than elementa

133 strained, with transition metal high-entropy alloys exhibiting only face- or body-centered cubic stru

134 This alloy exhibits high yield strength and elongation of 276

135 e fast dealloying of osmium from an Ir25Os75 alloy, exhibits an exceptional balance between oxygen ev

136 s study, we spin silk fibroin into a protein alloy fibre with whole fibronectin using wet spinning ap

137 cell viability is improved up to six fold on alloy fibres when serum is present while migration and s

138 l attachment is observed to silk-fibronectin alloy fibres without serum present while not compromisin

139 principles of radiation-tolerant structural alloys for advanced energy systems.

140 Our findings indicate the potential of GaNAs alloys for III-nitride based waveguide and photonic circ

141 structural alloys, in particular, aluminium alloys for transportation sector.

142 % Zr increased d of the base alloy from 729 to 740 nm while retaining Rq from 1 nm t

143 owing that such an NCD layer prevents the Zr alloy from directly interacting with water, we show that

144 fully tunable conductivity of ReS2x Se2(1-x) alloys from n-type to bipolar and p-type is realized.

145 the galvanic replacement of the liquid metal alloy galinstan with Ag and Au.

146 l resolution provides a key understanding of alloy growth with important industrial applications.

147 The Li-Mg alloy has low overpotential, leading to a lower interfac

148 reas dopant-compensated CH3NH3PbBr2.94Cl0.06 alloy has over tenfold improved bulk resistivity of 3.6

149 n situ experimental techniques, that Pd-Ni-P alloys have a hidden amorphous phase in the supercooled

150 ingle phase (fcc) Al0.3CoCrFeNi high-entropy alloy (HEA) was studied in the low and high strain-rate

151 High-entropy alloys (HEAs) consisting of multiple principle elements

152 High-entropy alloys (HEAs) in which interesting physical, chemical, a

153 The potential of high-entropy alloys (HEAs) to exhibit an extraordinary combination of

154 Multicomponent systems, termed High Entropy Alloys (HEAs), with predominantly single solid solution

155 tion analysis we find that Zr-based metallic alloy, heated to the supercooled liquid state under hydr

156 Alloying in 2D results in the development of new, divers

157 he structures and properties of high-entropy alloys in a manner not achievable by conventional proces

158 ing the element composition of these ternary alloys in all three spatial dimensions.

159 the amount of sulfides and potentially metal alloys in bulk rock, possibly producing redox heterogene

160 ches for Ti-Nb alloys and beta-stabilized Ti-alloys in general.

161 Successful applications of WCu alloys in high voltage electrical switches require their

162 Here we use ozone-activated silver-gold alloys in the form of nanoporous gold as a case study to

163 ed; the vast majority of the more than 5,500 alloys in use today cannot be additively manufactured be

164 the complex degradation behavior of Mg-based alloys in vivo.

165 opment of a host of high strength structural alloys, in particular, aluminium alloys for transportati

166 vidence firmly establishes that the Al-Cu-Fe alloys (including quasicrystals) formed in outer space i

167 re significantly higher than that of Ti6Al4V alloys, indicating a higher creep resistance.

168 a wide range by dopant migration toward the alloyed interface during ZnS shell passivation, which pr

169 s found that the dopant migration toward the alloyed interface of core/shell QDs is a thermodynamical

170 ter-sized particles of aluminum or magnesium alloys into alkoxide nanowires of tunable dimensions, wh

171 iber yarns; thermally activated shape-memory alloys; ionic-polymer/metal composites; dielectric-elast

172 onent AlxMy] to [am + alpha-Al] for the 84Al alloy is abnormal, not previously observed in crystalliz

173 Strengthening of this class of steel alloy is based on minimal lattice misfit to achieve maxi

174 Thus, we demonstrate that this alloy is suitable as an active component in near room te

175 evealed, ANE contribution of the isolated FM alloy is twofold, surface and bulk.

176 Here, a Nickel-Titanium alloy is used as a sensory material in order to quantita

177 Tailoring structural phase transitions using alloying is a novel idea with implications in designing

178 ngth due to addition of Cu, in Fe-rich Al-Si alloys is promising from the alloy recyclability point o

179 The composition of alloys is tuned by changing the growth temperatures.

180 dge of diffusion processes in semiconducting alloys is very important both technologically and from a

181 erarchical-precipitate-strengthened ferritic alloy, is effective in reducing the diffusional relaxati

182 the surface of three bilayer thick PbSe-SnSe alloy layers was discovered within [(Pbx Sn1-x Se)1+delt

183 ed through the use of compositionally-graded alloy libraries, which were photo-thermally heated by sc

184 ctures and mechanical properties of metallic alloys lies in designing and using athermal phase transf

185 scattering data from ten different metallic alloy liquids, we show that stronger liquids have steepe

186 d carriers with microsecond lifetimes in the alloyed material, which is very promising for photovolta

187 This metal alloy may take advantage simultaneously of the strong LS

188 e describe here innovative processing of low alloy medium-carbon steel with a duplex microstructure c

189 We report a Mg alloy Mg-2.2Nd-0.1Zn-0.4Zr (wt.%, denoted as JDBM-2) sho

190 It is found that, compared with crystalline alloys, MGs have some specific structural responses to n

191 apor deposition growth of 1T' ReS2x Se2(1-x) alloy monolayers is reported for the first time.

192 useful for polymers that form a mechanically alloyed morphology due to the high degree of miscibility

193 Here, synthesis of quaternary alloys Mox W1-x S2y Se2(1-y) is reported using chemical

194 olution synthesis of colloidal few-layer TMD alloys, MoxW1-xSe2 and WS2ySe2(1-y), exhibiting fully tu

195 se of shape memory and magnetic shape memory alloys (MSMAs) is believed to be a precursor state of th

196 post-synthesis thermal treatments for other alloy nanocatalysts as well.

197 for the future design of structured platinum alloy nanocatalysts.Core-shell platinum alloy nanopartic

198 In contrast to alloy nanocrystals with no elemental ordering, it is cha

199 certain amount of CoO to the supported Au-Pd alloy nanoparticles (NPs) to generate high-performance A

200 inum alloy nanocatalysts.Core-shell platinum alloy nanoparticles are promising catalysts for oxygen r

201 nto hollow Au nanoclusters, creating precise alloy nanoparticles atom-by-atom.

202 Shape-controlled octahedral Pt-Ni alloy nanoparticles exhibit remarkably high activities f

203 Most TMD alloy nanostructures are synthesized as films on substra

204 Three-dimensional (3D) interconnected metal alloy nanostructures possess superior catalytic performa

205 nsights into the structures of colloidal TMD alloy nanostructures that were previously only accessibl

206 High-entropy alloys, near-equiatomic solid solutions of five or more

207 In contrast to the disordered alloy NP, which is catalytically active for hydrogen evo

208 late-stripped Au and contacted by a eutectic alloy of gallium and indium top contacts.

209 esolved multicolor CsPbX3 (X = Cl, Br, I, or alloy of two halides) nanowire heterojunctions with a pi

210 gBiBr6 as host, band-gap engineering through alloying of In(III) /Sb(III) has been demonstrated in th

211 mpositions to date are multiple-cation solid alloys of formamidinium (FA), methylammonium (MA), cesiu

212 emical vapor deposition to grow monolayer 2D alloys of Re-doped MoSe2 with show composition tunable s

213 ength such as doping with fine particles and alloying often significantly decrease their conductivity

214 Here we report a dopant compensation in alloyed OIHP single crystals to overcome limitations of

215 by material and process improvements such as alloying, operating temperature reduction, and flue gas

216 n reduction activity without inducing shape, alloying or strain effects and without compromising stab

217 s high throughput, convenience for preparing alloys or series of doped nanomaterials, and its continu

218 A nickel-titanium shape memory alloy part was created with multiple shape-recovery stag

219 The alloyed perovskite described herein is the first double

220 thermodynamic parameters of the newly formed alloy phases and their crystal structures could be deter

221 of miscible and immiscible systems of binary alloys plays a critical role in the design of multicompo

222 echanical and physical properties, aluminium alloys possess wide potential in the automotive industry

223 led them onto 7075 and 6061 series aluminium alloy powders.

224 and costly wrought processes, while titanium alloys produced using low-cost powder metallurgy methods

225 0 to approximately 115 Omega cm(2) due to an alloying reaction between the Li metal and the Ge.

226 Indium coatings also undergo reversible alloying reactions with lithium ions, facilitating desig

227 n Fe-rich Al-Si alloys is promising from the alloy recyclability point of view.

228 With further temperature increase, the alloy reenters the supercooled liquid phase, which forms

229 ated that the local photoconductivity in the alloy region can be tailored and enhanced by two orders

230 e carrier diffusion and confinement into the alloy region.

231 hat are generally inherent in nanostructured alloys remains a challenge.

232 Ti-alloys represent the principal structural materials in b

233 1.4 lower than pure Ni and the 80:20 binary alloys, respectively.

234 t pressures of the retained hcp high-entropy alloy reveal that the fcc phase is a stable polymorph at

235 Zr alloy samples were coated with nanocrystalline diamond (

236 Precise control of alloying sites has long been a challenging pursuit, yet

237 molecular formula and atomically-controlled alloying sites in protecting shell.

238 action opens a door to precisely control the alloying sites in the protecting shell of bimetallic NPs

239 ABSTARCT: Shape memory alloys (SMAs) have the ability to show large recoverable

240 Single-phase concentrated solid-solution alloys (SP-CSAs) have recently gained unprecedented atte

241 , can be substantially improved by alloying, alloy stability remains a concern.

242 Phase changes are observed when the wood alloy state changes from liquid to solid.

243 Here, we demonstrate an alloying strategy to speed up the crystallization kineti

244 0.25 eletrocatalyst can be attributed to its alloyed structure with the proper Ni/Cu ratio and a larg

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

246 In the molten alloy system, the insoluble carbon floats to the surface

247 rosion and stress corrosion cracking in this alloy system.

248 fication of alloying behavior for 813 binary alloy systems consisting of transition and lanthanide me

249 hich have previously only been considered in alloy systems with four or fewer components.

250 most of the precipitation hardened aluminium alloys that are currently available can withstand maximu

251 evelop coarsening resistant high-temperature alloys that are stable in the temperature range of 250-3

252 from [Formula: see text] of dilute magnetic alloys that was ascribed to their hierarchical and fract

253 CO concentration by changing the solvent or alloying the surface.

254 erarchical-precipitate-strengthened ferritic alloy, the in-depth understanding of its high-temperatur

255 ential to widen the application window of Ti alloys, the most important structural material in aerosp

256 However, currently only a few alloys, the most relevant being AlSi10Mg, TiAl6V4, CoCr

257 In oxide-dispersed ferritic alloys, the phenomenon of irradiation-induced Cr redistr

258 It was found that for most binary magnesium alloys, the preferred growth direction of the alpha-Mg d

259 Owing to the 1T' structure of ReS2x Se2(1-x) alloys, they exhibit strong anisotropic optical, electri

260 In particular, for Mg-Al alloys, this direction changes from [Formula: see text]

261 he Al-concentration increased, and for Mg-Zn alloys, this direction changes from [Formula: see text]

262 sent a new approach in designing an Al-based alloy through solid state precipitation route that provi

263 e manufacturing of the industrially relevant alloy Ti-6Al-4V is known to create a multitude of phases

264 coil is placed on the top of a melting wood alloy to examine the changes of its inductance during so

265 ron-based hard X-ray nanotomography in Al-Cu alloys to measure kinetics of different nanoscale phases

266 contains the smallest amount of added master alloy, ultrasonics caused significant additional grain r

267 er of magnitude improvement in creep life of alloys upon adding small amounts of elements like zinc.

268 developed a new pathway for fabricating WCu alloys using spark plasma infiltrating sintering of copp

269 tation response of a high-temperature NiTiHf alloy was determined as a function of temperature.

270 those from similar experiments on an Al-2Cu alloy were consistent when the alloy compositions are co

271 vealed that these meta-magnetic shape memory alloys were capable of generating entropy changes of 14

272 Aluminum 2024 and permalloy 80 alloys were stacked together and shocked in a stainless

273 tions in NiCoMnIn meta-magnetic shape memory alloys were studied under constant and varying mechanica

274 e glass transition appears even for the 85Al alloy where the primary phase is alpha-Al.

275 local atomic distribution in ReS2x Se2(1-x) alloy, where S and Se atoms are selectively occupied at

276 duces with increasing addition of the master alloy which adds additional TiB2 particles and Ti solute

277 the mixed MAPb(ClxBr1-x)3 and MAPb(BrxI1-x)3 alloys, which we associate with symmetry breaking within

278 over CuAg bimetallic electrodes and surface alloys, which we find to be more selective for the forma

279 on, but increased the mass loss for the same alloy with a metallic surface (surface oxides were remov

280 BS reduced the mass loss of Mg-Yttrium (MgY) alloy with an oxidized surface during immersion degradat

281 found to continuously decrease in the master alloy with increasing cycles of salt-fluxing treatment,

282 ith metallic or oxidized surfaces and on MgY alloy with oxidized surfaces.

283 n metals, noble metals, and their bimetallic alloy with precisely controlled sizes ( approximately 1

284 The experiment also synthesized AlNiFe alloy with the B2 (CsCl-type) structure and the metastab

285 ystem, where we identify Au56Cu27Si17 as the alloy with the highest GFA.

286 trollable growth of monolayer ReS2x Se2(1-x) alloy with tunable bandgaps and electrical properties as

287 We fabricate a FM alloy with zero Nernst coefficient to mitigate the ANE c

288 tigate the thermoelectric properties of GeSe alloyed with AgSbSe2 , which stabilizes a new rhombohedr

289 Tungsten tetraboride alloys with a variable concentration of boron were prepa

290 ine phonon transport in nanocrystalline SiGe alloys with ab-initio electron-phonon scattering rates.

291 he optical properties of dilute-As GaN1-xAsx alloys with arsenic (As) content ranging from 0% up to 1

292 o reported for both as-cast and solutionized alloys with different amount of Cu without and with agei

293 Among three hierarchically structured Ni-Cu alloys with different Ni/Cu ratios (Ni0.25 Cu0.75 , Ni0.

294 ing approach for producing low-cost titanium alloys with exceptional fatigue strength via the hydroge

295 Traditionally, titanium alloys with satisfactory mechanical properties can only

296 ayered transition metal dichalcogenide (TMD) alloys with tunable compositions are promising candidate

297 otential of additive manufacturing to create alloys with unique microstructures and high performance

298 ore, our systematic study on dilute magnetic alloys with varying magnetic concentration exhibits cros

299 d structure of phosphorus-rich GaNxPyAs1-x-y alloys (x 0.025 and y >/= 0.6) is studied experimental

300 ering process was then applied to deposit an alloyed Zr55Cu30Al10Ni5 target, and finally resulted in