Second Order Corrections to Mean Field Evolution for Weakly Interacting Bosons in The Case of Three-body Interactions

In this paper, we consider the Hamiltonian evolution of N weakly interacting bosons. Assuming triple collisions, its mean field approximation is given by a quintic Hartree equation. We construct a second order correction to the mean field approximation using a kernel k ( t , x , y ) and derive an ev...

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Published inArchive for rational mechanics and analysis Vol. 203; no. 2; pp. 455 - 497
Main Author Chen, Xuwen
Format Journal Article
LanguageEnglish
Published Berlin/Heidelberg Springer-Verlag 01.02.2012
Springer Nature B.V
Subjects
Online AccessGet full text
ISSN0003-9527
1432-0673
DOI10.1007/s00205-011-0453-8

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Abstract In this paper, we consider the Hamiltonian evolution of N weakly interacting bosons. Assuming triple collisions, its mean field approximation is given by a quintic Hartree equation. We construct a second order correction to the mean field approximation using a kernel k ( t , x , y ) and derive an evolution equation for k . We show global existence for the resulting evolution equation for the correction and establish an a priori estimate comparing the approximation to the exact Hamiltonian evolution. Our error estimate is global and uniform in time. Comparing with the work of R odnianski and S chlein (Commun Math Phys 291:31–61, 2009 ), and G rillakis , M achedon and M argetis (Commun Math Phys 294:273–301, 2010 ; Adv Math 288:1788–1815, 2011 ), where the error estimate grows in time, our approximation tracks the exact dynamics for all time with an error of the order
AbstractList In this paper, we consider the Hamiltonian evolution of N weakly interacting bosons. Assuming triple collisions, its mean field approximation is given by a quintic Hartree equation. We construct a second order correction to the mean field approximation using a kernel k(t, x, y) and derive an evolution equation for k. We show global existence for the resulting evolution equation for the correction and establish an a priori estimate comparing the approximation to the exact Hamiltonian evolution. Our error estimate is global and uniform in time. Comparing with the work of Rodnianski and Schlein (Commun Math Phys 291:31-61, 2009), and Grillakis, Machedon and Margetis (Commun Math Phys 294:273-301, 2010; Adv Math 288:1788-1815, 2011), where the error estimate grows in time, our approximation tracks the exact dynamics for all time with an error of the order O ( 1 / N ) . [PUBLICATION ABSTRACT]
In this paper, we consider the Hamiltonian evolution of N weakly interacting bosons. Assuming triple collisions, its mean field approximation is given by a quintic Hartree equation. We construct a second order correction to the mean field approximation using a kernel k ( t , x , y ) and derive an evolution equation for k . We show global existence for the resulting evolution equation for the correction and establish an a priori estimate comparing the approximation to the exact Hamiltonian evolution. Our error estimate is global and uniform in time. Comparing with the work of R odnianski and S chlein (Commun Math Phys 291:31–61, 2009 ), and G rillakis , M achedon and M argetis (Commun Math Phys 294:273–301, 2010 ; Adv Math 288:1788–1815, 2011 ), where the error estimate grows in time, our approximation tracks the exact dynamics for all time with an error of the order
Author Chen, Xuwen
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Metaplectic Representation
Hartree Equation
Order Correction
Endpoint Strichartz Estimate
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Snippet In this paper, we consider the Hamiltonian evolution of N weakly interacting bosons. Assuming triple collisions, its mean field approximation is given by a...
In this paper, we consider the Hamiltonian evolution of N weakly interacting bosons. Assuming triple collisions, its mean field approximation is given by a...
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SubjectTerms Classical Mechanics
Complex Systems
Fluid- and Aerodynamics
Mathematical and Computational Physics
Physics
Physics and Astronomy
Theoretical
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Title Second Order Corrections to Mean Field Evolution for Weakly Interacting Bosons in The Case of Three-body Interactions
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