The Fröhlich polaron at strong coupling: Part II — Energy-momentum relation and effective mass

We study the Fröhlich polaron model in <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msup> <mml:mi>𝐑</mml:mi> <mml:mn>3</mml:mn> </mml:msup> </mml:math> , and prove a lower bound on its ground state energy as a function of the total momentum. The bound is asymptotically sharp at large coupling. In combination with a corresponding upper bound proved earlier (Mitrouskas et al. in Forum Math. Sigma 11:1–52, 2023), it shows that the energy is approximately parabolic below the continuum threshold, and that the polaron’s effective mass (defined as the semi-latus rectum of the parabola) is given by the celebrated Landau–Pekar formula. In particular, it diverges as <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msup> <mml:mi>α</mml:mi> <mml:mn>4</mml:mn> </mml:msup> </mml:math> for large coupling constant <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mi>α</mml:mi> </mml:math> .

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Publication Details

Journal
Publications mathématiques de l IHÉS
Published
2024-08-26
DOI
https://doi.org/10.1007/s10240-024-00150-0
Citations
2
Primary Topic
Cold Atom Physics and Bose-Einstein Condensates
Type
article
Field-Weighted Citation Impact
0.68
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article

The Fröhlich polaron at strong coupling: Part II — Energy-momentum relation and effective mass

Morris Brooks, Robert Seiringer
2 citations
Publications mathématiques de l IHÉS
Cold Atom Physics and Bose-Einstein Condensates
0.68
article

The Fröhlich polaron at strong coupling: Part II — Energy-momentum relation and effective mass

Morris Brooks, Robert Seiringer
article en
2 citations

Abstract

We study the Fröhlich polaron model in <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msup> <mml:mi>𝐑</mml:mi> <mml:mn>3</mml:mn> </mml:msup> </mml:math> , and prove a lower bound on its ground state energy as a function of the total momentum. The bound is asymptotically sharp at large coupling. In combination with a corresponding upper bound proved earlier (Mitrouskas et al. in Forum Math. Sigma 11:1–52, 2023), it shows that the energy is approximately parabolic below the continuum threshold, and that the polaron’s effective mass (defined as the semi-latus rectum of the parabola) is given by the celebrated Landau–Pekar formula. In particular, it diverges as <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msup> <mml:mi>α</mml:mi> <mml:mn>4</mml:mn> </mml:msup> </mml:math> for large coupling constant <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mi>α</mml:mi> </mml:math> .

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Cold Atom Physics and Bose-Einstein Condensates
0.68
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