Reactive and Nonreactive Scattering of Modulated Molecular Beams from Well Characterized Platinum Single Crystal Surfaces. [Mechanism, Rainbow Scattering, Angular Distribution].

Reactive and Nonreactive Scattering of Modulated Molecular Beams from Well Characterized Platinum Single Crystal Surfaces. [Mechanism, Rainbow Scattering, Angular Distribution]. PDF Author:
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Languages : en
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Reactive and nonreactive gas-surface interactions were studied by modulated molecular beam mass spectrometry on Pt(111) and stepped Pt(111) surfaces under ultra-high vacuum conditions. The angular distribution of helium atoms scattered from the stepped Pt(553) surface was measured as a function of the angle of incidence (polar, theta, and azimuthal, Phi). Rainbow scattering was observed indicating that the ordered array of steps and terraces exhibits a strongly periodic surface potential. In contrast, from the Pt(111) surface, the angular distribution of scattered helium atoms exhibits a sharp peak at the specular angle, characteristic of a smooth and well ordered surface. The interaction of hydrogen with platinum was investigated by studying the H2-D2 exchange reaction on the Pt(111) and the two stepped surfaces, Pt(553) and Pt(332). The production of HD was monitored. The mechanism of the H2-D2 exchange reaction was investigated on the Pt(111) and stepped Pt(332) surfaces. The dependence of the apparent reaction probability on surface temperature also indicates that the adsorption of hydrogen is an activated process on the Pt(111) surface, but not on the stepped Pt(332) surface. The energy barrier for hydrogen adsorption on Pt(111) deduced from this type of experiment is approx. 1.5 kcal/mole. On both surfaces, the mechanism of the recombination of adsorbed H and D atoms to form HD consists of a branched process at high crystal temperatures, with one of the branches connected in series with another reaction step at low temperatures. The process that isoperative over the entire temperature range studied, 25 to 800°C, has an activation energy and an apparent pre-exponential factor of E1 = 13.0 +- 0.4 kcal/mole and A1 = (8 +- 3) x 104 sec−1 for the Pt(332) surface and E1 = 15.6 +- 0.5 kcal/mole and A1 = (2.7 +- 1) x 105 sec −1 for the Pt(111) surface.

Reactive and Nonreactive Scattering of Modulated Molecular Beams from Well Characterized Platinum Single Crystal Surfaces. [Mechanism, Rainbow Scattering, Angular Distribution].

Reactive and Nonreactive Scattering of Modulated Molecular Beams from Well Characterized Platinum Single Crystal Surfaces. [Mechanism, Rainbow Scattering, Angular Distribution]. PDF Author:
Publisher:
ISBN:
Category :
Languages : en
Pages :

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Book Description
Reactive and nonreactive gas-surface interactions were studied by modulated molecular beam mass spectrometry on Pt(111) and stepped Pt(111) surfaces under ultra-high vacuum conditions. The angular distribution of helium atoms scattered from the stepped Pt(553) surface was measured as a function of the angle of incidence (polar, theta, and azimuthal, Phi). Rainbow scattering was observed indicating that the ordered array of steps and terraces exhibits a strongly periodic surface potential. In contrast, from the Pt(111) surface, the angular distribution of scattered helium atoms exhibits a sharp peak at the specular angle, characteristic of a smooth and well ordered surface. The interaction of hydrogen with platinum was investigated by studying the H2-D2 exchange reaction on the Pt(111) and the two stepped surfaces, Pt(553) and Pt(332). The production of HD was monitored. The mechanism of the H2-D2 exchange reaction was investigated on the Pt(111) and stepped Pt(332) surfaces. The dependence of the apparent reaction probability on surface temperature also indicates that the adsorption of hydrogen is an activated process on the Pt(111) surface, but not on the stepped Pt(332) surface. The energy barrier for hydrogen adsorption on Pt(111) deduced from this type of experiment is approx. 1.5 kcal/mole. On both surfaces, the mechanism of the recombination of adsorbed H and D atoms to form HD consists of a branched process at high crystal temperatures, with one of the branches connected in series with another reaction step at low temperatures. The process that isoperative over the entire temperature range studied, 25 to 800°C, has an activation energy and an apparent pre-exponential factor of E1 = 13.0 +- 0.4 kcal/mole and A1 = (8 +- 3) x 104 sec−1 for the Pt(332) surface and E1 = 15.6 +- 0.5 kcal/mole and A1 = (2.7 +- 1) x 105 sec −1 for the Pt(111) surface.

Energy Research Abstracts

Energy Research Abstracts PDF Author:
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Category : Power resources
Languages : en
Pages : 428

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INIS Atomindex

INIS Atomindex PDF Author:
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Category : Nuclear energy
Languages : en
Pages : 1440

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Physics Briefs

Physics Briefs PDF Author:
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Category : Physics
Languages : en
Pages : 742

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Dissertation Abstracts International

Dissertation Abstracts International PDF Author:
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Category : Dissertations, Academic
Languages : en
Pages : 776

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State-to-state Inelastic and Reactive Molecular Beam Scattering from Surfaces

State-to-state Inelastic and Reactive Molecular Beam Scattering from Surfaces PDF Author:
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Languages : en
Pages : 12

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Resonantly enhanced multiphoton ionization (REMPI) laser spectroscopic and molecular beam-surface scattering techniques are coupled to study inelastic and reactive gas-surface scattering with state-to-state specificity. Rotational, vibrational, translational and angular distributions have been measured for the inelastic scattering of HCI and N 2 from Au(111). In both cases the scattering is direct-inelastic in nature and exhibits interesting dynamical features such as rotational rainbow scattering. In an effort to elucidate the dynamics of chemical reactions occurring on surfaces we have extended our quantum-resolved scattering studies to include the reactive scattering of a beam of gas phase H-atoms from a chlorinated metal surface M-CI. The nascent rotational and vibrational distributions of the HCI product are determined using REMPI. The thermochemistry for this reaction on Au indicates that the product formation proceeding through chemisorbed H-atoms is slightly endothermic while direct reaction of a has phase H-atom with M-CI is highly exothermic (ca. 50 kcal/mole). Details of the experimental techniques, results and implications regarding the scattering dynamics are discussed. 55 ref., 8 fig.

Atomic and Molecular Beam Scattering from Silver (III).

Atomic and Molecular Beam Scattering from Silver (III). PDF Author: Radhesyam Sau
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Category :
Languages : en
Pages : 350

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Product Excitation in Reactive Scattering of Molecular Beams

Product Excitation in Reactive Scattering of Molecular Beams PDF Author: John Horton Birley
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Category :
Languages : en
Pages : 0

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Molecular Beam Measurements of the Rotaional State Distribution of RbBr Produced in Reactive Scattering of Rb on Br 2

Molecular Beam Measurements of the Rotaional State Distribution of RbBr Produced in Reactive Scattering of Rb on Br 2 PDF Author: Jens-Egon Mosch
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Category :
Languages : en
Pages : 27

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Out-of-plane Scattering of an Argon Molecular Beam by Heated Platinum

Out-of-plane Scattering of an Argon Molecular Beam by Heated Platinum PDF Author: Arthur Robert Rudnicki (Jr)
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Category :
Languages : en
Pages : 160

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