Single Photon-Induced Symmetry Breaking of H 2 Dissociation
H 2 , the smallest and most abundant molecule in the universe, has a perfectly symmetric ground state. What does it take to break this symmetry? We found that the inversion symmetry can be broken by absorption of a linearly polarized photon, which itself has inversion symmetry. In particular, the em...
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Veröffentlicht in: | Science (American Association for the Advancement of Science) 2007-02, Vol.315 (5812), p.629-633 |
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creator | Martín, F. Fernández, J. Havermeier, T. Foucar, L. Weber, Th Kreidi, K. Schöffler, M. Schmidt, L. Jahnke, T. Jagutzki, O. Czasch, A. Benis, E. P. Osipov, T. Landers, A. L. Belkacem, A. Prior, M. H. Schmidt-Böcking, H. Cocke, C. L. Dörner, R. |
description | H
2
, the smallest and most abundant molecule in the universe, has a perfectly symmetric ground state. What does it take to break this symmetry? We found that the inversion symmetry can be broken by absorption of a linearly polarized photon, which itself has inversion symmetry. In particular, the emission of a photoelectron with subsequent dissociation of the remaining H
+
2
fragment shows no symmetry with respect to the ionic H
+
and neutral H atomic fragments. This lack of symmetry results from the entanglement between symmetric and antisymmetric H
+
2
states that is caused by autoionization. The mechanisms behind this symmetry breaking are general for all molecules. |
doi_str_mv | 10.1126/science.1136598 |
format | Article |
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2
, the smallest and most abundant molecule in the universe, has a perfectly symmetric ground state. What does it take to break this symmetry? We found that the inversion symmetry can be broken by absorption of a linearly polarized photon, which itself has inversion symmetry. In particular, the emission of a photoelectron with subsequent dissociation of the remaining H
+
2
fragment shows no symmetry with respect to the ionic H
+
and neutral H atomic fragments. This lack of symmetry results from the entanglement between symmetric and antisymmetric H
+
2
states that is caused by autoionization. The mechanisms behind this symmetry breaking are general for all molecules.</description><identifier>ISSN: 0036-8075</identifier><identifier>EISSN: 1095-9203</identifier><identifier>DOI: 10.1126/science.1136598</identifier><language>eng</language><ispartof>Science (American Association for the Advancement of Science), 2007-02, Vol.315 (5812), p.629-633</ispartof><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c212t-9d00cc5fbcf50971719c674feee162b8c92a46eec184e7f32af3c022af328b33</citedby><cites>FETCH-LOGICAL-c212t-9d00cc5fbcf50971719c674feee162b8c92a46eec184e7f32af3c022af328b33</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,776,780,2871,2872,27901,27902</link.rule.ids></links><search><creatorcontrib>Martín, F.</creatorcontrib><creatorcontrib>Fernández, J.</creatorcontrib><creatorcontrib>Havermeier, T.</creatorcontrib><creatorcontrib>Foucar, L.</creatorcontrib><creatorcontrib>Weber, Th</creatorcontrib><creatorcontrib>Kreidi, K.</creatorcontrib><creatorcontrib>Schöffler, M.</creatorcontrib><creatorcontrib>Schmidt, L.</creatorcontrib><creatorcontrib>Jahnke, T.</creatorcontrib><creatorcontrib>Jagutzki, O.</creatorcontrib><creatorcontrib>Czasch, A.</creatorcontrib><creatorcontrib>Benis, E. P.</creatorcontrib><creatorcontrib>Osipov, T.</creatorcontrib><creatorcontrib>Landers, A. L.</creatorcontrib><creatorcontrib>Belkacem, A.</creatorcontrib><creatorcontrib>Prior, M. H.</creatorcontrib><creatorcontrib>Schmidt-Böcking, H.</creatorcontrib><creatorcontrib>Cocke, C. L.</creatorcontrib><creatorcontrib>Dörner, R.</creatorcontrib><title>Single Photon-Induced Symmetry Breaking of H 2 Dissociation</title><title>Science (American Association for the Advancement of Science)</title><description>H
2
, the smallest and most abundant molecule in the universe, has a perfectly symmetric ground state. What does it take to break this symmetry? We found that the inversion symmetry can be broken by absorption of a linearly polarized photon, which itself has inversion symmetry. In particular, the emission of a photoelectron with subsequent dissociation of the remaining H
+
2
fragment shows no symmetry with respect to the ionic H
+
and neutral H atomic fragments. This lack of symmetry results from the entanglement between symmetric and antisymmetric H
+
2
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2
, the smallest and most abundant molecule in the universe, has a perfectly symmetric ground state. What does it take to break this symmetry? We found that the inversion symmetry can be broken by absorption of a linearly polarized photon, which itself has inversion symmetry. In particular, the emission of a photoelectron with subsequent dissociation of the remaining H
+
2
fragment shows no symmetry with respect to the ionic H
+
and neutral H atomic fragments. This lack of symmetry results from the entanglement between symmetric and antisymmetric H
+
2
states that is caused by autoionization. The mechanisms behind this symmetry breaking are general for all molecules.</abstract><doi>10.1126/science.1136598</doi><tpages>5</tpages><oa>free_for_read</oa></addata></record> |
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source | American Association for the Advancement of Science; Jstor Complete Legacy |
title | Single Photon-Induced Symmetry Breaking of H 2 Dissociation |
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