1987
DOI: 10.1016/0001-6160(87)90071-x
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Spinodal ordering beyond the lifshitz point in Cu3Pd observed by high voltage electron microscopy

Abstract: Cu-Pd samples of compositions varying from 16 to 26 at.% Pd were irradiated in situ in the 1.5 MeV electron microscope at various temperatures.Low-temperature (-180·C) irradiation produced completely disordered solid solutions, room-temperature irradiation produced steady-state short-range order (SRO), and high-temperature irradiation tended to produce the expected equilibrium long-range order. In particular, the 18 and 20% samples irradiated at room temperature exhibited steady-state modulated SRO although on… Show more

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Cited by 28 publications
(5 citation statements)
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“…Previous studies (e.g. [2,19,20]) that obtained L1 2 as the ground state at ≈18% referred to the ANNNI Ising model, or performed an electronic mean field approach [8]. However, negligence of S1 in the first-principles input [11] will favour interactions that are 'blind' for S1.…”
mentioning
confidence: 99%
“…Previous studies (e.g. [2,19,20]) that obtained L1 2 as the ground state at ≈18% referred to the ANNNI Ising model, or performed an electronic mean field approach [8]. However, negligence of S1 in the first-principles input [11] will favour interactions that are 'blind' for S1.…”
mentioning
confidence: 99%
“…The other possible process is spinodal decomposition, 10) which is definable under electron irradiation conditions. [38][39][40] In this process, when the mean concentration of surface vacancies, which increases at a constant rate q with irradiation time t, exceeds a critical value C nu above which d 2 F=dðqtÞ 2 < 0 (F is the free energy in the binary system), the concentration wave of surface vacancies with a specific wave number k max preferentially grows and an ordered array of vacancy agglomerates with the spacings of l nn $ 2=k max is formed. According to a simple decomposition model, 41) k max can be estimated by solving…”
Section: Discussionmentioning
confidence: 99%
“…29. It consists of the sum of the terms proportional to the Fourier transforms of ⌽ R 1 ,R 2 ,R 3 (3) and ⌽ R 1 ,R 2 ,R 3 ,R 4 (4) . In the present paper, we assume that X k is negligible, i.e., X k Ϸ0, so that the contribution from this high-order term is comparatively small.…”
Section: ͑3͒mentioning
confidence: 99%