Complexified phase spaces, initial value representations, and the accuracy of semiclassical propagation
Using phase-space complexification, an Initial Value Representation (IVR) for the semiclassical propagator in position space is obtained as a composition of inverse Segal-Bargmann (S-B) transforms of the semiclassical coherent state propagator. The result is shown to be free of caustic singularities...
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creator | Lando, Gabriel M |
description | Using phase-space complexification, an Initial Value Representation (IVR) for
the semiclassical propagator in position space is obtained as a composition of
inverse Segal-Bargmann (S-B) transforms of the semiclassical coherent state
propagator. The result is shown to be free of caustic singularities and
identical to the Herman-Kluk (H-K) propagator, found ubiquitously in physical
and chemical applications. We contrast the theoretical aspects of this
particular IVR with the van Vleck-Gutzwiller (vV-G) propagator and one of its
IVRs, often employed in order to evade the non-linear "root-search" for
trajectories required by vV-G. We demonstrate that bypassing the root-search
comes at the price of serious numerical instability for all IVRs except the H-K
propagator. We back up our theoretical arguments with comprehensive numerical
calculations performed using the homogeneous Kerr system, about which we also
unveil some unexpected new phenomena, namely: (1) the observation of a clear
mark of half the Ehrenfest's time in semiclassical dynamics; and (2) the
accumulation of trajectories around caustics as a function of increasing time
(dubbed "caustic stickiness"). We expect these phenomena to be more general
than for the Kerr system alone. |
doi_str_mv | 10.48550/arxiv.2006.13902 |
format | Article |
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the semiclassical propagator in position space is obtained as a composition of
inverse Segal-Bargmann (S-B) transforms of the semiclassical coherent state
propagator. The result is shown to be free of caustic singularities and
identical to the Herman-Kluk (H-K) propagator, found ubiquitously in physical
and chemical applications. We contrast the theoretical aspects of this
particular IVR with the van Vleck-Gutzwiller (vV-G) propagator and one of its
IVRs, often employed in order to evade the non-linear "root-search" for
trajectories required by vV-G. We demonstrate that bypassing the root-search
comes at the price of serious numerical instability for all IVRs except the H-K
propagator. We back up our theoretical arguments with comprehensive numerical
calculations performed using the homogeneous Kerr system, about which we also
unveil some unexpected new phenomena, namely: (1) the observation of a clear
mark of half the Ehrenfest's time in semiclassical dynamics; and (2) the
accumulation of trajectories around caustics as a function of increasing time
(dubbed "caustic stickiness"). We expect these phenomena to be more general
than for the Kerr system alone.</description><identifier>DOI: 10.48550/arxiv.2006.13902</identifier><language>eng</language><subject>Physics - Quantum Physics</subject><creationdate>2020-06</creationdate><rights>http://arxiv.org/licenses/nonexclusive-distrib/1.0</rights><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>228,230,776,881</link.rule.ids><linktorsrc>$$Uhttps://arxiv.org/abs/2006.13902$$EView_record_in_Cornell_University$$FView_record_in_$$GCornell_University$$Hfree_for_read</linktorsrc><backlink>$$Uhttps://doi.org/10.48550/arXiv.2006.13902$$DView paper in arXiv$$Hfree_for_read</backlink></links><search><creatorcontrib>Lando, Gabriel M</creatorcontrib><title>Complexified phase spaces, initial value representations, and the accuracy of semiclassical propagation</title><description>Using phase-space complexification, an Initial Value Representation (IVR) for
the semiclassical propagator in position space is obtained as a composition of
inverse Segal-Bargmann (S-B) transforms of the semiclassical coherent state
propagator. The result is shown to be free of caustic singularities and
identical to the Herman-Kluk (H-K) propagator, found ubiquitously in physical
and chemical applications. We contrast the theoretical aspects of this
particular IVR with the van Vleck-Gutzwiller (vV-G) propagator and one of its
IVRs, often employed in order to evade the non-linear "root-search" for
trajectories required by vV-G. We demonstrate that bypassing the root-search
comes at the price of serious numerical instability for all IVRs except the H-K
propagator. We back up our theoretical arguments with comprehensive numerical
calculations performed using the homogeneous Kerr system, about which we also
unveil some unexpected new phenomena, namely: (1) the observation of a clear
mark of half the Ehrenfest's time in semiclassical dynamics; and (2) the
accumulation of trajectories around caustics as a function of increasing time
(dubbed "caustic stickiness"). We expect these phenomena to be more general
than for the Kerr system alone.</description><subject>Physics - Quantum Physics</subject><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2020</creationdate><recordtype>article</recordtype><sourceid>GOX</sourceid><recordid>eNotj7luwzAQRNmkCJx8QKrwAyKF4iFKZSDkAgy4cS-sVkubgA6ClA377-MoqaaYeQM8xp4KkevKGPEK8eLPuRSizAtVC3nPDs08hoEu3nnqeThCIp4CIKUX7ie_eBj4GYYT8UghUqJpgcXP062GqefLkTggniLglc-OJxo9DpCSxxsY4hzgsO4f2J2DIdHjf27Y_uN933xl293nd_O2zaC0Muuphs71VpsKC6PJ1NoWFiwaiZ10qnJdWUqJlRLKWCxtJayzyvadRiwQ1YY9_92upm2IfoR4bX-N29VY_QAyElMR</recordid><startdate>20200624</startdate><enddate>20200624</enddate><creator>Lando, Gabriel M</creator><scope>GOX</scope></search><sort><creationdate>20200624</creationdate><title>Complexified phase spaces, initial value representations, and the accuracy of semiclassical propagation</title><author>Lando, Gabriel M</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a672-de9abfd7458c154e594717a7c52cb2f38fb6622c830357c67807f737db4cc1cc3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2020</creationdate><topic>Physics - Quantum Physics</topic><toplevel>online_resources</toplevel><creatorcontrib>Lando, Gabriel M</creatorcontrib><collection>arXiv.org</collection></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext_linktorsrc</fulltext></delivery><addata><au>Lando, Gabriel M</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Complexified phase spaces, initial value representations, and the accuracy of semiclassical propagation</atitle><date>2020-06-24</date><risdate>2020</risdate><abstract>Using phase-space complexification, an Initial Value Representation (IVR) for
the semiclassical propagator in position space is obtained as a composition of
inverse Segal-Bargmann (S-B) transforms of the semiclassical coherent state
propagator. The result is shown to be free of caustic singularities and
identical to the Herman-Kluk (H-K) propagator, found ubiquitously in physical
and chemical applications. We contrast the theoretical aspects of this
particular IVR with the van Vleck-Gutzwiller (vV-G) propagator and one of its
IVRs, often employed in order to evade the non-linear "root-search" for
trajectories required by vV-G. We demonstrate that bypassing the root-search
comes at the price of serious numerical instability for all IVRs except the H-K
propagator. We back up our theoretical arguments with comprehensive numerical
calculations performed using the homogeneous Kerr system, about which we also
unveil some unexpected new phenomena, namely: (1) the observation of a clear
mark of half the Ehrenfest's time in semiclassical dynamics; and (2) the
accumulation of trajectories around caustics as a function of increasing time
(dubbed "caustic stickiness"). We expect these phenomena to be more general
than for the Kerr system alone.</abstract><doi>10.48550/arxiv.2006.13902</doi><oa>free_for_read</oa></addata></record> |
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title | Complexified phase spaces, initial value representations, and the accuracy of semiclassical propagation |
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