Nanometre fcc clusters versus bulk bcc alloy: the structure of Cu-Pd catalysts

Authors
Citation
V. Shah et Lq. Yang, Nanometre fcc clusters versus bulk bcc alloy: the structure of Cu-Pd catalysts, PHIL MAG A, 79(8), 1999, pp. 2025-2049
Citations number
38
Categorie Soggetti
Apllied Physucs/Condensed Matter/Materiales Science
Journal title
PHILOSOPHICAL MAGAZINE A-PHYSICS OF CONDENSED MATTER STRUCTURE DEFECTS ANDMECHANICAL PROPERTIES
ISSN journal
13642804 → ACNP
Volume
79
Issue
8
Year of publication
1999
Pages
2025 - 2049
Database
ISI
SICI code
1364-2804(199908)79:8<2025:NFCVBB>2.0.ZU;2-7
Abstract
We present a simple method to improve the accuracy of the calculated heat o f mixing for the Cu-Pd alloy within the formalism of the molecular dynamics /Monte Carlo-corrected effective medium (MD/MC-CEM) theory by adding a fitt ed Morse potential to the pair interaction between Cu and Pd atoms. This le ads to a much better agreement between the theoretical and experimental Val ues of heats of mixing for five different compositions of the Cu-Pd alloy i n the bulk phases. Using this newly fitted model, we have performed simulat ions on CuPd clusters consisting of 50-10 000 atoms with fee and bce struct ures. Our calculations show that in the range of cluster sizes of several t housand atoms, the fee structure is energetically favoured over the bcc str ucture. We estimate an approximate size for the fcc to bcc (CsCl, known bul k structure for CuPd) transition in these clusters to be around 10 000 atom s. Additionally, we have also performed calculations of the X-ray diffracti on patterns of a variety of cluster geometries and sizes. The calculated X- ray diffraction pattern of a slightly distorted fee cluster exhibits the ma in features observed in the available experimental diffraction patterns of colloidal bimetallic catalysts of CuPd. The calculated diffraction patterns of bcc clusters are quite different from the experimental data.