The confinement of an annealed branched polymer by a potential well

The Lifshitz equation for the confinement of a linear polymer in a spherical cavity of radius R has the form of the Schrödinger equation for a quantum particle trapped in a potential well with flat bottom and infinite walls at radius R. We show that the Lifshitz equation of a confined annealed branc...

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Published in:Физика низких температур
Date:2017
Main Authors: Grosberg, A.Y., Kelly, Joshua, Bruinsma, Robijn
Format: Article
Language:English
Published: Фізико-технічний інститут низьких температур ім. Б.І. Вєркіна НАН України 2017
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Online Access:https://nasplib.isofts.kiev.ua/handle/123456789/129359
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Journal Title:Digital Library of Periodicals of National Academy of Sciences of Ukraine
Cite this:The confinement of an annealed branched polymer by a potential well / Alexander Y. Grosberg, Joshua Kelly, Robijn Bruinsma // Физика низких температур. — 2017. — Т. 43, № 1. — С. 122-131. — Бібліогр.: 20 назв. — англ.

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Digital Library of Periodicals of National Academy of Sciences of Ukraine
id nasplib_isofts_kiev_ua-123456789-129359
record_format dspace
spelling Grosberg, A.Y.
Kelly, Joshua
Bruinsma, Robijn
2018-01-19T14:04:46Z
2018-01-19T14:04:46Z
2017
The confinement of an annealed branched polymer by a potential well / Alexander Y. Grosberg, Joshua Kelly, Robijn Bruinsma // Физика низких температур. — 2017. — Т. 43, № 1. — С. 122-131. — Бібліогр.: 20 назв. — англ.
0132-6414
PACS: 36.20.–r, 87.15.H–
https://nasplib.isofts.kiev.ua/handle/123456789/129359
The Lifshitz equation for the confinement of a linear polymer in a spherical cavity of radius R has the form of the Schrödinger equation for a quantum particle trapped in a potential well with flat bottom and infinite walls at radius R. We show that the Lifshitz equation of a confined annealed branched polymer has the form of the Schrödinger equation for a quantum harmonic oscillator. The harmonic oscillator potential results from the repulsion of the many branches from the potential walls. Mathematically, it must be obtained from the solution of the equation of motion of a second, now classical, particle in a non-linear potential that depends self-consistently on the eigenvalue of the quantum oscillator. The resulting confinement energy has a 1/R⁴ dependence on the confinement radius R, in agreement with scaling arguments. We discuss the application of this result to the problem of the confinement of single-stranded RNA molecules inside spherical capsids.
en
Фізико-технічний інститут низьких температур ім. Б.І. Вєркіна НАН України
Физика низких температур
К 100-летию со дня рождения И.М. Лифшица
The confinement of an annealed branched polymer by a potential well
Article
published earlier
institution Digital Library of Periodicals of National Academy of Sciences of Ukraine
collection DSpace DC
title The confinement of an annealed branched polymer by a potential well
spellingShingle The confinement of an annealed branched polymer by a potential well
Grosberg, A.Y.
Kelly, Joshua
Bruinsma, Robijn
К 100-летию со дня рождения И.М. Лифшица
title_short The confinement of an annealed branched polymer by a potential well
title_full The confinement of an annealed branched polymer by a potential well
title_fullStr The confinement of an annealed branched polymer by a potential well
title_full_unstemmed The confinement of an annealed branched polymer by a potential well
title_sort confinement of an annealed branched polymer by a potential well
author Grosberg, A.Y.
Kelly, Joshua
Bruinsma, Robijn
author_facet Grosberg, A.Y.
Kelly, Joshua
Bruinsma, Robijn
topic К 100-летию со дня рождения И.М. Лифшица
topic_facet К 100-летию со дня рождения И.М. Лифшица
publishDate 2017
language English
container_title Физика низких температур
publisher Фізико-технічний інститут низьких температур ім. Б.І. Вєркіна НАН України
format Article
description The Lifshitz equation for the confinement of a linear polymer in a spherical cavity of radius R has the form of the Schrödinger equation for a quantum particle trapped in a potential well with flat bottom and infinite walls at radius R. We show that the Lifshitz equation of a confined annealed branched polymer has the form of the Schrödinger equation for a quantum harmonic oscillator. The harmonic oscillator potential results from the repulsion of the many branches from the potential walls. Mathematically, it must be obtained from the solution of the equation of motion of a second, now classical, particle in a non-linear potential that depends self-consistently on the eigenvalue of the quantum oscillator. The resulting confinement energy has a 1/R⁴ dependence on the confinement radius R, in agreement with scaling arguments. We discuss the application of this result to the problem of the confinement of single-stranded RNA molecules inside spherical capsids.
issn 0132-6414
url https://nasplib.isofts.kiev.ua/handle/123456789/129359
citation_txt The confinement of an annealed branched polymer by a potential well / Alexander Y. Grosberg, Joshua Kelly, Robijn Bruinsma // Физика низких температур. — 2017. — Т. 43, № 1. — С. 122-131. — Бібліогр.: 20 назв. — англ.
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first_indexed 2025-12-07T17:18:40Z
last_indexed 2025-12-07T17:18:40Z
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