recent experiments in low-energy electron-molecule collisions

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1 t Experiments in Low-Energy Electron-Molecule Colli - valence * shape resonances - diffuse dipole- (& polarizability-) bound resonances - vibrational Feshbach resonances - doorway states - molecules - with dipole moment: HF, HCl, HBr - without dipole moment: CO 2 , N 2 O, CH 4 - large molecules: - nitromethane - chlorobenzene - pyrrole - ethylene carbonate Threshold phenomena lectron collisions with a radical: NO ·

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Recent Experiments in Low-Energy Electron-Molecule Collisions. Threshold phenomena. - valence s * shape resonances - diffuse dipole- (& polarizability-) bound resonances - vibrational Feshbach resonances - doorway states - molecules - with dipole moment: HF, HCl, HBr - PowerPoint PPT Presentation

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Page 1: Recent Experiments in Low-Energy Electron-Molecule Collisions

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Recent Experiments in Low-Energy Electron-Molecule Collisions

- valence * shape resonances- diffuse dipole- (& polarizability-) bound resonances- vibrational Feshbach resonances- doorway states- molecules

- with dipole moment: HF, HCl, HBr- without dipole moment: CO2, N2O, CH4

- large molecules: - nitromethane- chlorobenzene- pyrrole- ethylene carbonate

Threshold phenomena

Electron collisions with a radical: NO·

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Sample Elastic Cross Sections

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Sample Elastic Cross Sections

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Differential cross sections in N2O

Marinković B, Szmytkowski C, Pejčev V, Filipović D and Vuškoviš L,J. Phys. B 19 2365 (1986)

Johnstone W M and Newell W R, J. Phys. B 26 129 (1993)

Kitajima M, Sakamoto Y, Gulley R J, Hoshino M, Gibson J C, Tanaka H and Buckman S J, J. Phys. B 33 1687 (2000)

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Vibrational excitation in hydrogen fluoride: experiment and theory

Martin Čížek, Jiří Horáček, Michael Allan and Wolfgang Domcke 2003

= 1.83 D

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HF: Spectra and Potential Curves

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HCl

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Čížek Horáček Sergenton Popović Allan Domcke Leininger Gadea, Phys. Rev. A 2000

HBr and DBr red: experiment

blue: nonlocal resonance model = 0.82 D

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Generic potential curves

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CO2

bending

= 0.0 D

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N2O - Elastic & Vibrational Excitation

elastic and fundamental vibrations overtone vibrations

= 0.16 D

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N2O - Dissociative Attachment

Bound anion calculation: Kryachko et al., J. Chem. Phys. 2001

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Ethylene Carbonate = 5.3 D

Dissociative Electron Attachment in Cyclopentanone, -Butyrolactone, Ethylene Carbonate and Ethylene Carbonate-d4: Role of Dipole-Bound ResonancesM. Stepanović, Y. Pariat and M. AllanJ. Chem. Phys. 110 (1999) 11376

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Nitromethane CH3NO2

= 3.46 D

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Nitromethane: Elastic DCS

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Selectivity of vibrational excitation in chlorobenzene

= 1.54 D

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Pyrrole

= 1.77 D

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Methane: Energy-Loss Spectrum

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Methane: DCS overview

B. H. Lengsfield III, T. N. Rescigno, C. W. McCurdy, Phys. Rev. A 44 (1991) 4296

W. Sohn, K.-H. Kochem, K.-M. Scheuerlein, K. Jung, H. Ehrhardt J. Phys. B 19 (1986) 3625

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Methane: detail

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Conclusions I

- often interaction diffuse state ↔ valence state

- diabatic vs adiabatic potential surfaces

- vibrational Feshbach resonances (VFR)

- outer well resonances

- (*) shape resonances

- doorway states

Threshold phenomena

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Diffuse and Valence States of Anions

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NO: Potential Curves

initial NO final NONO– resonance

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NO: transitions between electronic fine structure states

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NO: transitions between electronic fine structure states

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NO: vibrational transitions

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Comparison of NO and O2

NO O2

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NO: angular dependence

elastic Vibrational excitation

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Conclusions II

NO·: transitions between electronic fine structure states

- gigantic resonant cross section, elastic

- resonance parentage

- elastic cross sections not equal?