Journal article
Symmetry breaking: a classic example of quantum interference captured by mixed quantum/classical theory
- Abstract:
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The phenomena of propensity and inverse propensity are explored using time-dependent mixed quantum classical theory, MQCT, in which the rotational motion of the molecule is treated quantum mechanically, whereas the scattering process is described classically. Good agreement with the results of accurate full-quantum calculations is reported for a closed shell approximation to the NO + Ar system. It is shown that MQCT reproduces both phenomena in a broad range of the final states of the molecule and for various initial rotational states, offering a unique time-dependent insight. It permits seeing that both propensity and inverse propensity occur due to efficient depopulation of some states at the early postcollisional stage of the scattering process, when the molecule exists in a coherent superposition of many excited states that span a very broad range of angular momentum quantum numbers, populated by an efficient stepladder process of many consecutive transitions with small Δj.
- Publication status:
- Published
- Peer review status:
- Peer reviewed
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Access Document
- Files:
-
-
(Preview, Accepted manuscript, pdf, 1.2MB, Terms of use)
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- Publisher copy:
- 10.1021/acs.jpclett.3c02887
Authors
- Publisher:
- American Chemical Society
- Journal:
- Journal of Physical Chemistry Letters More from this journal
- Volume:
- 14
- Issue:
- 47
- Pages:
- 10617-10623
- Publication date:
- 2023-11-20
- Acceptance date:
- 2023-11-17
- DOI:
- EISSN:
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1948-7185
- Pmid:
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37982682
- Language:
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English
- Keywords:
- Pubs id:
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1570701
- Local pid:
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pubs:1570701
- Deposit date:
-
2024-01-02
Terms of use
- Copyright holder:
- American Chemical Society
- Copyright date:
- 2023
- Rights statement:
- Copyright © 2023 American Chemical Society
- Notes:
- This is the accepted manuscript version of the article. The final version is available online from American Chemical Society at https://dx.doi.org/10.1021/acs.jpclett.3c02887
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