Energies of dilute Fermi gases and universalities in BCS theory (Record no. 768047)

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000 -LEADER
fixed length control field 04207ntm a22004217a 4500
003 - CONTROL NUMBER IDENTIFIER
control field AT-ISTA
005 - DATE AND TIME OF LATEST TRANSACTION
control field 20250911132645.0
008 - FIXED-LENGTH DATA ELEMENTS--GENERAL INFORMATION
fixed length control field 250911s2024 au ||||| m||| 00| 0 eng d
040 ## - CATALOGING SOURCE
Transcribing agency ISTA
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Personal name Lauritsen, Asbjorn Baekgaard
9 (RLIN) 1084211
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Title Energies of dilute Fermi gases and universalities in BCS theory
260 ## - PUBLICATION, DISTRIBUTION, ETC. (IMPRINT)
Name of publisher, distributor, etc. Institute of Science and Technology Austria
Date of publication, distribution, etc. 2024
500 ## - GENERAL NOTE
General note Thesis
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Formatted contents note Abstract
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Formatted contents note Acknowledgements
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Formatted contents note About the Author
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Formatted contents note List of Publications
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Formatted contents note Table of Contents
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Formatted contents note List of Figures
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Formatted contents note Preface
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Formatted contents note I Energies of Dilute Fermi Gases
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Formatted contents note 1 Introduction to the theory of dilute quantum gases
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Formatted contents note 2 Pair of particles in an
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Formatted contents note 3 Ground state energy of the dilute spin-polarized Fermi gas: Upper bound via cluster expansion
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Formatted contents note 4 Ground state energy of the dilute spin-polarized Fermi gas: Lower bound
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Formatted contents note 5 Almost optimal upper bound for the ground state energy of a dilute Fermi gas via cluster expansion
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Formatted contents note 6 Pressure of a dilute spin-polarized Fermi gas: Lower bound
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Formatted contents note 7 Pressure of a dilute spin-polarized Fermi gas: Upper bound
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Formatted contents note II Universalities in BCS Theory
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Formatted contents note 8 Brief introduction to the BCS theory of superconductivity
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Formatted contents note 9 Universality in low-dimensional BCS theory
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Formatted contents note 10 The BCS energy gap at high density
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Formatted contents note 11 Universal behaviour of the BCS energy gap
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Formatted contents note Bibliography
520 ## - SUMMARY, ETC.
Summary, etc. This thesis consists of two separate parts. In the first part we consider a dilute Fermi gas interacting through a repulsive interaction in dimensions $d=1,2,3$. Our focus is mostly on the physically most relevant dimension $d=3$ and the setting of a spin-polarized (equivalently spinless) gas, where the Pauli exclusion principle plays a key role. We show that, at zero temperature, the ground state energy density of the interacting spin-polarized gas differs (to leading order) from that of the free (i.e. non-interacting) gas by a term of order $a_p^d\rho^{2+2/d}$ with $a_p$ the $p$-wave scattering length of the repulsive interaction and $\rho$ the density. Further, we extend this to positive temperature and show that the pressure of an interacting spin-polarized gas differs from that of the free gas by a now temperature dependent term, again of order $a_p^d\rho^{2+2/d}$. Lastly, we consider the setting of a spin-$\frac{1}{2}$ Fermi gas in $d=3$ dimensions and show that here, as an upper bound, the ground state energy density differs from that of the free system by a term of order $a_s \rho^2$ with an error smaller than $a_s \rho^2 (a_s\rho^{1/3})^{1-\eps}$ for any $\eps > 0$, where $a_s$ is the $s$-wave scattering length of the repulsive interaction. These asymptotic formulas complement the similar formulas in the literature for the dilute Bose and spin-$\frac{1}{2}$ Fermi gas, where the ground state energies or pressures differ from that of the corresponding free systems by a term of order $a_s \rho^2$ in dimension $d=3$. In the spin-polarized setting, the corrections, of order $a_p^3\rho^{8/3}$ in dimension $d=3$, are thus much smaller and requires a more delicate analysis. In the second part of the thesis we consider the Bardeen--Cooper--Schrieffer (BCS) theory of superconductivity and in particular its associated critical temperature and energy gap. We prove that the ratio of the zero-temperature energy gap and critical temperature $\Xi(T=0)/T_c$ approaches a universal constant $\pi e^{-\gamma}\approx 1.76$ in both the limit of high density in dimension $d=3$ and in the limit of weak coupling in dimensions $d=1,2$. This complements the proofs in the literature of this universal behaviour in the limit of weak coupling or low density in dimension $d=3$. Secondly, we prove that the ratio of the energy gap at positive temperature and critical temperature $\Xi(T)/T_c$ approaches a universal function of the relative temperature $T/T_c$ in the limit of weak coupling in dimensions $d=1,2,3$.
856 ## - ELECTRONIC LOCATION AND ACCESS
Uniform Resource Identifier <a href="https://doi.org/10.15479/at:ista:18135">https://doi.org/10.15479/at:ista:18135</a>
942 ## - ADDED ENTRY ELEMENTS (KOHA)
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  Not Lost Dewey Decimal Classification     Library Library 11/09/2025   Quiet Room AT-ISTA#003298 16/09/2025 11/09/2025 Book

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