1978
DOI: 10.1107/s0021889878013904
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Neutron small-angle scattering study of phase decomposition in Au–Pt

Abstract: Isothermal decomposition of a Au‐60 at.% Pt alloy, quenched from the solid as well as the liquid state, has been studied with the D11 neutron small‐angle scattering spectrometer at ILL, Grenoble. An incident neutron wavelength of 6.7 Å was used and measurements were carried out in the range of scattering vector [β = 4πsin θ/λ] from 2.8 × 10−2 to 21 × 10−2Å−1. The preliminary results indicate that decomposition of this alloy at 550°C takes place by a spinodal mode, although deviations were observed from linear … Show more

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Cited by 32 publications
(7 citation statements)
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“…Reproduced with permission. Spinodal decomposition has been studied in many materials systems, including Al-Zn, [80] Au-Pt, [81] Cu-Ti, [82] VO 2 -TiO 2 , [83] SiO 2 -TiO 2 , [83] SiO 2 -ZnO. C) Arrays of gold nanoparticles directed by lithographically confined DNA origami.…”
Section: Wwwadvopticalmatdementioning
confidence: 99%
See 1 more Smart Citation
“…Reproduced with permission. Spinodal decomposition has been studied in many materials systems, including Al-Zn, [80] Au-Pt, [81] Cu-Ti, [82] VO 2 -TiO 2 , [83] SiO 2 -TiO 2 , [83] SiO 2 -ZnO. C) Arrays of gold nanoparticles directed by lithographically confined DNA origami.…”
Section: Wwwadvopticalmatdementioning
confidence: 99%
“…[75][76][77][78][79] In this process, phase separation occurs through diffusion in the direction of increasing concentration due to the second derivative of the free energy with respect to composition having a negative sign. Spinodal decomposition has been studied in many materials systems, including Al-Zn, [80] Au-Pt, [81] Cu-Ti, [82] VO 2 -TiO 2 , [83] SiO 2 -TiO 2 , [83] SiO 2 -ZnO. [83] These material systems have a potential to exhibit unique optical properties arising from the combination of the two constituent phases.…”
Section: Wwwadvopticalmatdementioning
confidence: 99%
“…In the Tokuyama, Enomoto & Kawasaki (1987); HF: ; FL: Fratzl & Lebowitz (1989). e: Pt-40 at.% Au (Singhal, Herman & Kostorz, 1978); t~: AI-5-3, -6.8 at.% Zn (Hennion, Ronzaud & Guyot, 1982); o: AI-6"8, -10 at.% Zn(Mg) (Komura, Osamura, Fuji & Takeda, 1985); V: A1-12-1 at.% Zn (Guyot & Simon, 1982); A: AI-22 at.% Zn(Mg) (Forouhi & de Fontaine, 1987); ~: Al-12, -22, -32 at.% Zn ; ~: AI-4, -6-8at.% Zn(Mg) (Komura, Takeda, Osamura, & Okuda, 1988); I1: Cu-33at.% Mn (Gaulin, Spooner & Morii, 1987); II': Fe-34 at.% Cr (Katano & Iizumi, 1984); A: A1-Li (see . two-phase model including interparticle interference, these authors determine a size-distribution function for spherical particles by fitting a linear combination of cubic splines to reproduce the scattering curves for Q> Qm (Magnani, Puliti & Stefanon, 1988).…”
Section: I(qt)/ I( T) = L 3( T)s[q L( T)t]mentioning
confidence: 99%
“…The observed width of the structure function in CuRh is even somewhat larger than that measured in a melt-spun AuPt alloy where the finite grain size inhibits the formation of a long range modulated structure. 18,25 Furthermore, satellite intensities near fundamental matrix reflections are likewise found in CuRh. The intensity distribution of the satellites is similar to the intensity distribution observed in the small-angle scattering experiment, i.e., the scaled intensity distributions obtained from the small-angle scattering experiment and from the satellite intensities can be represented by the same curve.…”
Section: Discussionmentioning
confidence: 80%