Quantum states of hydrogen atom motion on the Pd(111) surface and in the subsurface

We investigate the quantum states of hydrogen atom motion on Pd(111) surface and in its subsurface by calculating the wavefunctions and the eigenenergies for hydrogen atom motion within the framework of the variation method on an adiabatic potential energy surface (PES), obtained through first-princ...

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Main Authors: Ozawa, Nobuki, Arboleda, Nelson B., Jr., Roman, Tanglaw A., Nakanishi, Hiroshi, Dino, Wilson Agerico, Kasai, Hideaki
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Published: Animo Repository 2007
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Online Access:https://animorepository.dlsu.edu.ph/faculty_research/3800
https://animorepository.dlsu.edu.ph/context/faculty_research/article/4802/type/native/viewcontent/365214.html
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spelling oai:animorepository.dlsu.edu.ph:faculty_research-48022022-08-27T04:03:36Z Quantum states of hydrogen atom motion on the Pd(111) surface and in the subsurface Ozawa, Nobuki Arboleda, Nelson B., Jr. Roman, Tanglaw A. Nakanishi, Hiroshi Dino, Wilson Agerico Kasai, Hideaki We investigate the quantum states of hydrogen atom motion on Pd(111) surface and in its subsurface by calculating the wavefunctions and the eigenenergies for hydrogen atom motion within the framework of the variation method on an adiabatic potential energy surface (PES), obtained through first-principles calculations, for the hydrogen atom motion. The calculated results show that the ground-state wavefunction for the hydrogen atom motion localizes on the face-centered cubic (fcc) hollow site of the surface. The higher excited state wavefunctions are distributed between the first and second layers, and subsequently delocalized under the second atom layer. These suggest that an effective diffusion path of the hydrogen atom into the subsurface area passes through the fcc hollow site to the octahedral sites in the subsurface. Moreover, activation energies for diffusion of H and D atoms over the saddle point of the PES between the fcc hollow site and the first (second) octahedral site are estimated as 598 (882)meV and 646 (939)meV, respectively. Furthermore, the activation energies for diffusion of H and D atoms over the saddle point of the PES between the first (second) octahedral site and the fcc hollow site are estimated as 285 (483)meV and 323 (532)meV, respectively. © IOP Publishing Ltd. 2007-09-12T07:00:00Z text text/html https://animorepository.dlsu.edu.ph/faculty_research/3800 info:doi/10.1088/0953-8984/19/36/365214 https://animorepository.dlsu.edu.ph/context/faculty_research/article/4802/type/native/viewcontent/365214.html Faculty Research Work Animo Repository Hydrogen Atoms Potential energy surfaces Wave functions Palladium compounds Physics
institution De La Salle University
building De La Salle University Library
continent Asia
country Philippines
Philippines
content_provider De La Salle University Library
collection DLSU Institutional Repository
topic Hydrogen
Atoms
Potential energy surfaces
Wave functions
Palladium compounds
Physics
spellingShingle Hydrogen
Atoms
Potential energy surfaces
Wave functions
Palladium compounds
Physics
Ozawa, Nobuki
Arboleda, Nelson B., Jr.
Roman, Tanglaw A.
Nakanishi, Hiroshi
Dino, Wilson Agerico
Kasai, Hideaki
Quantum states of hydrogen atom motion on the Pd(111) surface and in the subsurface
description We investigate the quantum states of hydrogen atom motion on Pd(111) surface and in its subsurface by calculating the wavefunctions and the eigenenergies for hydrogen atom motion within the framework of the variation method on an adiabatic potential energy surface (PES), obtained through first-principles calculations, for the hydrogen atom motion. The calculated results show that the ground-state wavefunction for the hydrogen atom motion localizes on the face-centered cubic (fcc) hollow site of the surface. The higher excited state wavefunctions are distributed between the first and second layers, and subsequently delocalized under the second atom layer. These suggest that an effective diffusion path of the hydrogen atom into the subsurface area passes through the fcc hollow site to the octahedral sites in the subsurface. Moreover, activation energies for diffusion of H and D atoms over the saddle point of the PES between the fcc hollow site and the first (second) octahedral site are estimated as 598 (882)meV and 646 (939)meV, respectively. Furthermore, the activation energies for diffusion of H and D atoms over the saddle point of the PES between the first (second) octahedral site and the fcc hollow site are estimated as 285 (483)meV and 323 (532)meV, respectively. © IOP Publishing Ltd.
format text
author Ozawa, Nobuki
Arboleda, Nelson B., Jr.
Roman, Tanglaw A.
Nakanishi, Hiroshi
Dino, Wilson Agerico
Kasai, Hideaki
author_facet Ozawa, Nobuki
Arboleda, Nelson B., Jr.
Roman, Tanglaw A.
Nakanishi, Hiroshi
Dino, Wilson Agerico
Kasai, Hideaki
author_sort Ozawa, Nobuki
title Quantum states of hydrogen atom motion on the Pd(111) surface and in the subsurface
title_short Quantum states of hydrogen atom motion on the Pd(111) surface and in the subsurface
title_full Quantum states of hydrogen atom motion on the Pd(111) surface and in the subsurface
title_fullStr Quantum states of hydrogen atom motion on the Pd(111) surface and in the subsurface
title_full_unstemmed Quantum states of hydrogen atom motion on the Pd(111) surface and in the subsurface
title_sort quantum states of hydrogen atom motion on the pd(111) surface and in the subsurface
publisher Animo Repository
publishDate 2007
url https://animorepository.dlsu.edu.ph/faculty_research/3800
https://animorepository.dlsu.edu.ph/context/faculty_research/article/4802/type/native/viewcontent/365214.html
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