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arXiv:2610.41657

Mathematical foundations of second quantization: an introduction through spin-boson models

Davide Lonigro

math-phquant-phSubmitted Oct 30, 2026• Announced Nov 2, 2026
arXivHTMLPDF

Abstract

These lecture notes originate from a one-semester course on the mathematical foundations of second quantization, first given at the Department of Physics of the Friedrich-Alexander-Universität Erlangen-Nürnberg in the Winter Semester 2025/26 to a mixed audience of physics and mathematics students. Their guiding thread is a class of physical models: spin-boson models, describing a two-level system coupled to a boson field. After summarizing the necessary background on unbounded operators, up to the Kato-Rellich and KLMN theorems, and developing direct sums and tensor products of Hilbert spaces and of unbounded operators, we treat single-mode boson fields, constructing the ladder and number operators and characterizing their domains, before moving to Fock spaces, second quantization, bosonic and fermionic annihilation and creation operators, and the canonical (anti)commutation relations. Throughout, spin-boson models provide both the motivation and the test bench for the formalism: we rigorously establish their self-adjointness, solve the pure dephasing and Jaynes-Cummings models explicitly, deriving their spectra and the qubit channels they induce, show how their multimode counterparts display irreversible decoherence and decay, and, in an appendix, prove the rotating-wave approximation for the quantum Rabi model with an explicit error bound. Finally, we use the KLMN theorem to construct spin-boson models with non-normalizable form factors, and briefly discuss stronger ultraviolet divergences and the need for renormalization. Exercises with full solutions are included.

AI Summary

These lecture notes address how to formulate second quantization and spin–boson dynamics rigorously, including operator domains, self-adjointness, and the justification of approximations. Intended for readers with basic functional analysis and quantum mechanics, they develop direct sums and tensor products of unbounded operators, single-mode ladder operators, Fock spaces, second quantization, and bosonic and fermionic canonical relations. Spin–boson models organize the applications. Kato–Rellich perturbation theory establishes self-adjointness for regular couplings. The single-mode pure-dephasing and Jaynes–Cummings models are solved explicitly, including spectra, eigenvectors, and reduced qubit channels; multimode versions illustrate irreversible decoherence and decay. An appendix proves the rotating-wave approximation for the quantum Rabi model with an explicit error bound. Exercises and full solutions accompany the development. For non-square-integrable form factors satisfying $\omega^{-1/2}f\in\mathfrak h$, annihilation operators remain controlled on the free-energy form domain, while creation terms are interpreted as forms. The KLMN theorem constructs a semibounded self-adjoint Hamiltonian and yields ultraviolet-cutoff convergence in norm resolvent, with error bounded by $2\sqrt{2}\|B\|\|\omega^{-1/2}(f-f_\Lambda)\|$ at a specified negative spectral parameter. The notes explicitly claim neither originality nor completeness. Stronger ultraviolet singularities require renormalization methods only briefly surveyed, and the form-sum construction generally does not identify the operator domain. Multimode exponential decay is ordinarily approximate; exact all-time exponential decay requires idealized singular spectral densities, with a Hamiltonian unbounded below in the spontaneous-emission example.

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131 pages. Lecture notes with exercises

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These lecture notes originate from a one-semester course on the mathematical foundations of second quantization, first given at the Department of Physics of the Friedrich-Alexander-Universität Erlangen-Nürnberg in the Winter Semester 2025/26 to a mixed audience of physics and mathematics students. Their guiding thread is a class of physical models: spin-boson models, describing a two-level system coupled to a boson field. After summarizing the necessary background on unbounded operators, up to the Kato-Rellich and KLMN theorems, and developing direct sums and tensor products of Hilbert spaces and of unbounded operators, we treat single-mode boson fields, constructing the ladder and number operators and characterizing their domains, before moving to Fock spaces, second quantization, bosonic and fermionic annihilation and creation operators, and the canonical (anti)commutation relations. Throughout, spin-boson models provide both the motivation and the test bench for the formalism: we rigorously establish their self-adjointness, solve the pure dephasing and Jaynes-Cummings models explicitly, deriving their spectra and the qubit channels they induce, show how their multimode counterparts display irreversible decoherence and decay, and, in an appendix, prove the rotating-wave approximation for the quantum Rabi model with an explicit error bound. Finally, we use the KLMN theorem to construct spin-boson models with non-normalizable form factors, and briefly discuss stronger ultraviolet divergences and the need for renormalization. Exercises with full solutions are included.
These lecture notes address how to formulate second quantization and spin–boson dynamics rigorously, including operator domains, self-adjointness, and the justification of approximations. Intended for readers with basic functional analysis and quantum mechanics, they develop direct sums and tensor products of unbounded operators, single-mode ladder operators, Fock spaces, second quantization, and bosonic and fermionic canonical relations.
Spin–boson models organize the applications. Kato–Rellich perturbation theory establishes self-adjointness for regular couplings. The single-mode pure-dephasing and Jaynes–Cummings models are solved explicitly, including spectra, eigenvectors, and reduced qubit channels; multimode versions illustrate irreversible decoherence and decay. An appendix proves the rotating-wave approximation for the quantum Rabi model with an explicit error bound. Exercises and full solutions accompany the development.
For non-square-integrable form factors satisfying ω−1/2f∈h\omega^{-1/2}f\in\mathfrak hω−1/2f∈h, annihilation operators remain controlled on the free-energy form domain, while creation terms are interpreted as forms. The KLMN theorem constructs a semibounded self-adjoint Hamiltonian and yields ultraviolet-cutoff convergence in norm resolvent, with error bounded by 22∥B∥∥ω−1/2(f−fΛ)∥2\sqrt{2}\|B\|\|\omega^{-1/2}(f-f_\Lambda)\|22​∥B∥∥ω−1/2(f−fΛ​)∥ at a specified negative spectral parameter.
The notes explicitly claim neither originality nor completeness. Stronger ultraviolet singularities require renormalization methods only briefly surveyed, and the form-sum construction generally does not identify the operator domain. Multimode exponential decay is ordinarily approximate; exact all-time exponential decay requires idealized singular spectral densities, with a Hamiltonian unbounded below in the spontaneous-emission example.
In this chapter we describe a technique to deal with identical particles that is called second quantization . Despite being a technique, second quantization helps a lot in understanding physics. One can learn and endlessly repeat newspaper-style statements particles are fields , fields are particles without grasping their meaning. Second quantization brings these concepts to an operational level. Since the procedure of second quantization is slightly different for fermions and bosons, we have to treat the two cases separately. We start with considering a system of identical bosons, and introduce creation and annihilation operators (CAPs) that change the number of particles in a given many-particle state, thereby connecting different states in Fock space. We show how to express occupation numbers in terms of CAPs, and then get to the heart of the second quantization: the commutation relations for the bosonic CAPs. As a next step, we construct field operators out of the CAPs and spend quite some time (and energy) presenting the physics of the particles in terms of these field operators. Only afterward, do we explain why all this activity has been called second quantization. In Section 3.4 we then present the same procedure for fermions, and we mainly focus on what is different as compared to bosons. The formalism of second quantization is summarized in Table 3.1.
This is a self-contained and hopefully readable account on the method of creation and annihilation operators (also known as the Fock space representation or the "second quantization" formalism) for non-relativistic quantum mechanics of many particles. Assuming knowledge only on conventional quantum mechanics in the wave function formalism, we define the creation and annihilation operators, discuss their properties, and introduce corresponding representations of states and operators of many-particle systems. As the title of the note suggests, we cover most topics treated in sections 6.7 and 6.8 of Feynman's "Statistical Mechanics: A Set of Lectures". As a preliminary, we also carefully discuss the symmetry of wave functions describing indistinguishable particles. We note that all the contents of the present note are completely standard, and the definitions and the derivations presented here have been known to many. Although the style of the present note may be slightly more mathematical than standard physics literatures, we do not try to achieve full mathematical rigor.(Note to experts: In particular we here DERIVE the (anti)commutation relations of the creation and annihilation operators, rather than simply declaring them. In this sense our approach is quite close to that of Feynman's. But we here focus on the action of creation/annihilation operators on general NNN body wave functions, while Feynman makes a heavy use of Slater-determinant-type states from the beginning. We hope that our presentation provides a better perspective on the formalism.)
The first volume (General Theory) differs from most textbooks as it emphasizes the mathematical structure and mathematical rigor, while being adapted to the teaching the first semester of an advanced course in Quantum Mechanics (the content of the book are the lectures of courses actually delivered.). It differs also from the very few texts in Quantum Mechanics that give emphasis to the mathematical aspects because this book, being written as Lecture Notes, has the structure of lectures delivered in a course, namely introduction of the problem, outline of the relevant points, mathematical tools needed, theorems, proofs. This makes this book particularly useful for self-study and for instructors in the preparation of a second course in Quantum Mechanics (after a first basic course). With some minor additions it can be used also as a basis of a first course in Quantum Mechanics for students in mathematics curricula. The second part (Selected Topics) are lecture notes of a more advanced course aimed at giving the basic notions necessary to do research in several areas of mathematical physics connected with quantum mechanics, from solid state to singular interactions, many body theory, semi-classical analysis, quantum statistical mechanics. The structure of this book is suitable for a second-semester course, in which the lectures are meant to provide, in addition to theorems and proofs, an overview of a more specific subject and hints to the direction of research. In this respect and for the width of subjects this second volume differs from other monographs on Quantum Mechanics. The second volume can be useful for students who want to have a basic preparation for doing research and for instructors who may want to use it as a basis for the presentation of selected topics.
Abstract Chapter 2 provides a review of pertinent aspects of the quantum mechanics of systems composed of many particles. It focuses on the foundations of quantum many-particle physics, the many-particle Hilbert spaces to describe large assemblies of interacting systems composed of Bosons or Fermions, which lead to the versatile formalism of second quantization as a convenient and eminently practical language ubiquitous in the mathematical formulation of the theory of many-particle systems of quantum matter. The main objects in which the formalism of second quantization is expressed are the Bosonic or Fermionic creation and annihilation operators that become, in the position basis, the quantum field operators.
Written for a two-semester graduate course in Quantum Mechanics, this comprehensive text helps develop the tools and formalism of Quantum Mechanics and its applications to physical systems. It suits students who have taken some introductory Quantum Mechanics and Modern Physics courses at undergraduate level, but it is self-contained and does not assume any specific background knowledge beyond appropriate fluency in mathematics. The text takes a modern logical approach rather than a historical one and it covers standard material, such as the hydrogen atom and the harmonic oscillator, the WKB approximations and Bohr-Sommerfeld quantization. Important modern topics and examples are also described, including Berry phase, quantum information, complexity and chaos, decoherence and thermalization, nonstandard statistics, as well as more advanced material such as path integrals, scattering theory, multiparticles and Fock space. Readers will gain a broad overview of Quantum Mechanics, as solid preparation for further study or research.
Written for a two-semester graduate course in Quantum Mechanics, this comprehensive text helps develop the tools and formalism of Quantum Mechanics and its applications to physical systems. It suits students who have taken some introductory Quantum Mechanics and Modern Physics courses at undergraduate level, but it is self-contained and does not assume any specific background knowledge beyond appropriate fluency in mathematics. The text takes a modern logical approach rather than a historical one and it covers standard material, such as the hydrogen atom and the harmonic oscillator, the WKB approximations and Bohr-Sommerfeld quantization. Important modern topics and examples are also described, including Berry phase, quantum information, complexity and chaos, decoherence and thermalization, nonstandard statistics, as well as more advanced material such as path integrals, scattering theory, multiparticles and Fock space. Readers will gain a broad overview of Quantum Mechanics, as solid preparation for further study or research.