The product formula for regularized Fredholm determinants
By Thomas Britz, Alan Carey, Fritz Gesztesy, Roger Nichols, Fedor Sukochev, and Dmitriy Zanin
Abstract
For trace class operators $A, B \in \mathcal{B}_1(\mathcal{H})$($\mathcal{H}$ a complex, separable Hilbert space), the product formula for Fredholm determinants holds in the familiar form
When trace class operators are replaced by Hilbert–Schmidt operators $A, B \in \mathcal{B}_2(\mathcal{H})$ and the Fredholm determinant ${\det }_{\mathcal{H}}(I_{\mathcal{H}} - A)$,$A \in \mathcal{B}_1(\mathcal{H})$, by the 2nd regularized Fredholm determinant ${\det }_{\mathcal{H},2}(I_{\mathcal{H}} - A) = {\det }_{\mathcal{H}} ((I_{\mathcal{H}} - A) \exp (A))$,$A \in \mathcal{B}_2(\mathcal{H})$, the product formula must be replaced by
$$\begin{align*} {\det }_{\mathcal{H},2} ((I_{\mathcal{H}} - A) (I_{\mathcal{H}} - B)) &= {\det }_{\mathcal{H},2} (I_{\mathcal{H}} - A) {\det }_{\mathcal{H},2} (I_{\mathcal{H}} - B) \\ & \quad \times \exp (- \operatorname {tr}_{\mathcal{H}}(AB)). \end{align*}$$
The product formula for the case of higher regularized Fredholm determinants ${\det }_{\mathcal{H},k}(I_{\mathcal{H}} - A)$,$A \in \mathcal{B}_k(\mathcal{H})$,$k \in \mathbb{N}$,$k \geqslant 2$, does not seem to be easily accessible and hence this note aims at filling this gap in the literature.
1. Introduction
The purpose of this note is to prove a product formula for regularized (modified) Fredholm determinants extending the well-known Hilbert–Schmidt case.
To set the stage, we recall that if $A \in \mathcal{B}_1(\mathcal{H})$ is a trace class operator on the complex, separable Hilbert space $\mathcal{H}$, that is, the sequence of (necessarily nonnegative) eigenvalues $\lambda _j\big ((A^*A)^{1/2}\big )$,$j \in \mathbb{N}_0 = \mathbb{N} \cup \{0\}$, of $|A| = (A^*A)^{1/2}$ (the singular values of $A$), ordered in nonincreasing magnitude and counted according to their multiplicity, lies in $\ell ^1(\mathbb{N}_0)$, the Fredholm determinant ${\det }_{\mathcal{H}}(I_{\mathcal{H}} - A)$ associated with $I_{\mathcal{H}} - A$,$A \in \mathcal{B}_1(\mathcal{H})$, is given by the absolutely convergent infinite product
where $\lambda _j(A)$,$j \in \mathbb{N}_0$, are the (generally, complex) eigenvalues of $A$ ordered again with respect to nonincreasing absolute value and now counted according to their algebraic multiplicity.
A celebrated property of ${\det }_{\mathcal{H}}(I_{\mathcal{H}} - \,\cdot \,)$ that (like the analog of Equation 1.1) is shared with the case where $\mathcal{H}$ is finite-dimensional, is the product formula
$$\begin{equation} {\det }_{\mathcal{H}} ((I_{\mathcal{H}} - A) (I_{\mathcal{H}} - B)) = {\det }_{\mathcal{H}} (I_{\mathcal{H}} - A) {\det }_{\mathcal{H}} (I_{\mathcal{H}} - B), \quad A, B \in \mathcal{B}_1(\mathcal{H}) \cssId{texmlid3}{\tag{1.2}} \end{equation}$$
When extending these considerations to operators $A \in \mathcal{B}_p(\mathcal{H})$, with $\mathcal{B}_p(\mathcal{H})$,$p \in [1,\infty )$, the $\ell ^p(\mathbb{N}_0)$-based trace ideals (i.e., the eigenvalues $\lambda _j\big ((A^*A)^{1/2}\big )$,$j \in \mathbb{N}_0$, of $(A^*A)^{1/2}$ now lie in $\ell ^p(\mathbb{N}_0)$, see, e.g., Reference 4, Sect. III.7), the $k$th regularized Fredholm determinant ${\det }_{\mathcal{H},k}(I_{\mathcal{H}} - A)$,$k \in \mathbb{N}$,$k \geqslant p$, associated with $I_{\mathcal{H}} - A$,$A \in \mathcal{B}_k(\mathcal{H})$, is given by
We note that ${\det }_{\mathcal{H},k}(I_{\mathcal{H}} - \,\cdot \,)$ is continuous on $\mathcal{B}_{\ell }(\mathcal{H})$ for $1 \leqslant \ell \leqslant k$, and
$$\begin{equation} {\det }_{\mathcal{H},k} (I_{\mathcal{H}} - AB) = {\det }_{\mathcal{H},k} (I_{\mathcal{H}} - BA), \quad A, B \in \mathcal{B}(\mathcal{H}), \; AB, BA \in \mathcal{B}_k(\mathcal{H}) \cssId{texmlid14}{\tag{1.4}} \end{equation}$$
(this extends to the case where $A$ maps between different Hilbert spaces $\mathcal{H}_2$ and $\mathcal{H}_1$ and $B$ from $\mathcal{H}_1$ to $\mathcal{H}_2$, etc.).
The analog of the simple product formula Equation 1.2 no longer holds for $k \geqslant 2$ and it is well-known in the special Hilbert–Schmidt case $k=2$ that Equation 1.2 must be replaced by
$$\begin{align} {\det }_{\mathcal{H},2} ((I_{\mathcal{H}} - A) (I_{\mathcal{H}} - B)) &= {\det }_{\mathcal{H},2} (I_{\mathcal{H}} - A) {\det }_{\mathcal{H},2} (I_{\mathcal{H}} - B) \\ & \quad \times \exp (- \operatorname {tr}_{\mathcal{H}}(AB)), \quad A, B \in \mathcal{B}_2(\mathcal{H}) \cssId{texmlid4}{\tag{1.5}} \end{align}$$
More precisely, we were interested in a product formula for ${\det }_{\mathcal{H},k} ((I_{\mathcal{H}} - A) (I_{\mathcal{H}} - B))$ for $A,B \in \mathcal{B}_k(\mathcal{H})$ in terms of ${\det }_{\mathcal{H},k} (I_{\mathcal{H}} - A)$ and ${\det }_{\mathcal{H},k} (I_{\mathcal{H}} - B)$,$k \in \mathbb{N}$,$k \geqslant 3$. As kindly pointed out to us by Rupert Frank, the particular case where $A$ is a finite rank operator, denoted by $F$, and $B \in \mathcal{B}_k(\mathcal{H})$ was considered in Reference 5, Lemma 1.5.10 (see also, Reference 6, Proposition 4.8 $(ii)$), and the result
with $p_n(\,\cdot \,,\,\cdot \,)$ a polynomial in two variables and of finite rank, was derived. An extension of this formula to three factors, that is,
We present the proof of a quantitative version of Theorem 1.1 in two parts. In the next section we prove an algebraic result, Lemma 2.4, that is the key to the analytic part of the argument appearing in the final section on regularized determinants.
2. The commutator subspace in the algebra of noncommutative polynomials
To prove a quantitative version of Theorem 1.1 and hence derive a formula for $X_k(A,B)$, we first need to recall some facts on the commutator subspace of an algebra of noncommutative polynomials.
Let ${\mathrm{ Pol_2}}$ be the free polynomial algebra in $2$ (noncommuting) variables, $A$ and $B$. Let $W$ be the set of noncommutative monomials (words in the alphabet $\{A,B\}$). (We recall that the set $W$ is a semigroup with respect to concatenation, $1$ is the neutral element of this semigroup, that is, $1$ is an empty word in this alphabet.) Every $x\in {\mathrm{ Pol_2}}$ can be written as a sum
Here the coefficients $\widehat{x}(w)$ vanish for all but finitely many $w\in W$.
Let $[{\mathrm{ Pol_2}},{\mathrm{ Pol_2}}]$ be the commutator subspace of ${\mathrm{ Pol_2}}$, that is, the linear span of commutators $[x_1,x_2]$,$x_1,x_2\in {\mathrm{ Pol_2}}$.
Next, we need some notation. Let $k_1,k_2 \in \mathbb{N}_0 = \mathbb{N} \cup \{0\}$, and set
Here, $S_j$ is the set of all partitions of the set $\{1,\cdots ,j\}$,$1 \leqslant j \leqslant k_1 + k_2$. (The symbol $|\,\cdot \,|$ abbreviating the cardinality of a subset of $\mathbb{Z}$.) The condition $|\pi |=3$ means that $\pi$ breaks the set $\{1,\cdots ,j\}$ into exactly $3$ pieces denoted by $\pi _1$,$\pi _2$, and $\pi _3$ (some of them can be empty). The element $z_{\pi }$ denotes the product
(with $A^c = \{1,\dots ,j\} \backslash \mathcal{A}$ the complement of $\mathcal{A}$ in $\{1,\dots ,j\}$).
Using this notation we can now state the following fact:
3. The product formula for $k$th modified Fredholm determinants
After these preparations we are ready to return to the product formula for regularized determinants and specialize the preceding algebraic considerations to the context of Theorem 1.1.
since for $1 \leqslant j \leqslant k-1$,$L(y_{\mathcal{A}}) = j+|\mathcal{A}| \geqslant k$, and hence one obtains the inequality
$$\begin{equation} \|x_k\|_{\mathcal{B}_1(\mathcal{H})}\leqslant c_k\max _{\substack{0\leqslant k_1,k_2<k\\ k_1+k_2\geqslant k}} \|A\|_{\mathcal{B}_k(\mathcal{H})}^{k_1}\|B\|_{\mathcal{B}_k(\mathcal{H})}^{k_2}, \quad k \in \mathbb{N}, \; k \geqslant 2, \tag{3.2} \end{equation}$$
for some $c_k > 0$,$k \geqslant 2$. We also set (cf. Equation 2.22) $X_1(A,B) = 0$.
Acknowledgments
We are indebted to Galina Levitina for very helpful remarks on a first draft of this paper and to Rupert Frank for kindly pointing out references Reference 3 and Reference 5 to us. We are particularly indebted to the anonymous referee for a very careful reading of our manuscript and for making excellent suggestions for improvements.
A. Carey, F. Gesztesy, G. Levitina, R. Nichols, F. Sukochev, and D. Zanin, On the limiting absorption principle for massless Dirac operators and properties of spectral shift functions, preprint, 2020.
Reference [2]
Nelson Dunford and Jacob T. Schwartz, Linear operators. Part II: Spectral theory. Selfadjoint operators in Hilbert space; With the assistance of William G. Bade and Robert G. Bartle; Reprint of the 1963 original; A Wiley-Interscience Publication, Wiley Classics Library, John Wiley & Sons, Inc., New York, 1988. MR1009163, Show rawAMSref\bib{DS88}{book}{
author={Dunford, Nelson},
author={Schwartz, Jacob T.},
title={Linear operators. Part II},
series={Wiley Classics Library},
subtitle={Spectral theory. Selfadjoint operators in Hilbert space; With the assistance of William G. Bade and Robert G. Bartle; Reprint of the 1963 original; A Wiley-Interscience Publication},
publisher={John Wiley \& Sons, Inc., New York},
date={1988},
pages={i--x, 859--1923 and 1--7},
isbn={0-471-60847-5},
review={\MR {1009163}},
}
Reference [3]
Rupert L. Frank, Eigenvalue bounds for Schrödinger operators with complex potentials. III, Trans. Amer. Math. Soc. 370 (2018), no. 1, 219–240, DOI 10.1090/tran/6936. MR3717979, Show rawAMSref\bib{Fr17}{article}{
author={Frank, Rupert L.},
title={Eigenvalue bounds for Schr\"{o}dinger operators with complex potentials. III},
journal={Trans. Amer. Math. Soc.},
volume={370},
date={2018},
number={1},
pages={219--240},
issn={0002-9947},
review={\MR {3717979}},
doi={10.1090/tran/6936},
}
Reference [4]
I. C. Gohberg and M. G. Kreĭn, Introduction to the theory of linear nonselfadjoint operators, Translated from the Russian by A. Feinstein. Translations of Mathematical Monographs, Vol. 18, American Mathematical Society, Providence, R.I., 1969. MR0246142, Show rawAMSref\bib{GK69}{book}{
author={Gohberg, I. C.},
author={Kre\u {\i }n, M. G.},
title={Introduction to the theory of linear nonselfadjoint operators},
series={Translated from the Russian by A. Feinstein. Translations of Mathematical Monographs, Vol. 18},
publisher={American Mathematical Society, Providence, R.I.},
date={1969},
pages={xv+378},
review={\MR {0246142}},
}
Reference [5]
M. Hansmann, On the discrete spectrum of linear operators in Hilbert spaces, Ph.D. Thesis, Technical University of Clausthal, Germany, 2005.
Reference [6]
Marcel Hansmann, Perturbation determinants in Banach spaces—with an application to eigenvalue estimates for perturbed operators, Math. Nachr. 289 (2016), no. 13, 1606–1625, DOI 10.1002/mana.201500315. MR3549372, Show rawAMSref\bib{Ha16}{article}{
author={Hansmann, Marcel},
title={Perturbation determinants in Banach spaces---with an application to eigenvalue estimates for perturbed operators},
journal={Math. Nachr.},
volume={289},
date={2016},
number={13},
pages={1606--1625},
issn={0025-584X},
review={\MR {3549372}},
doi={10.1002/mana.201500315},
}
Reference [7]
A. I. Markushevich, Theory of functions of a complex variable. Vol. I, II, III, Second English edition, Chelsea Publishing Co., New York, 1977. Translated and edited by Richard A. Silverman. MR0444912, Show rawAMSref\bib{Ma85}{book}{
author={Markushevich, A. I.},
title={Theory of functions of a complex variable. Vol. I, II, III},
edition={Second English edition},
note={Translated and edited by Richard A. Silverman},
publisher={Chelsea Publishing Co., New York},
date={1977},
pages={xxii+1238 pp. (three volumes in one; not consecutively paged) ISBN 0-8284-0296-5},
review={\MR {0444912}},
}
Reference [8]
Michael Reed and Barry Simon, Methods of modern mathematical physics. IV. Analysis of operators, Academic Press [Harcourt Brace Jovanovich, Publishers], New York-London, 1978. MR0493421, Show rawAMSref\bib{RS78}{book}{
author={Reed, Michael},
author={Simon, Barry},
title={Methods of modern mathematical physics. IV. Analysis of operators},
publisher={Academic Press [Harcourt Brace Jovanovich, Publishers], New York-London},
date={1978},
pages={xv+396},
isbn={0-12-585004-2},
review={\MR {0493421}},
}
Reference [9]
Barry Simon, Notes on infinite determinants of Hilbert space operators, Advances in Math. 24 (1977), no. 3, 244–273, DOI 10.1016/0001-8708(77)90057-3. MR482328, Show rawAMSref\bib{Si77}{article}{
author={Simon, Barry},
title={Notes on infinite determinants of Hilbert space operators},
journal={Advances in Math.},
volume={24},
date={1977},
number={3},
pages={244--273},
issn={0001-8708},
review={\MR {482328}},
doi={10.1016/0001-8708(77)90057-3},
}
Reference [10]
Barry Simon, Trace ideals and their applications, 2nd ed., Mathematical Surveys and Monographs, vol. 120, American Mathematical Society, Providence, RI, 2005, DOI 10.1090/surv/120. MR2154153, Show rawAMSref\bib{Si05}{book}{
author={Simon, Barry},
title={Trace ideals and their applications},
series={Mathematical Surveys and Monographs},
volume={120},
edition={2},
publisher={American Mathematical Society, Providence, RI},
date={2005},
pages={viii+150},
isbn={0-8218-3581-5},
review={\MR {2154153}},
doi={10.1090/surv/120},
}
Reference [11]
Barry Simon, Operator theory, A Comprehensive Course in Analysis, Part 4, American Mathematical Society, Providence, RI, 2015, DOI 10.1090/simon/004. MR3364494, Show rawAMSref\bib{Si15}{book}{
author={Simon, Barry},
title={Operator theory},
series={A Comprehensive Course in Analysis, Part 4},
publisher={American Mathematical Society, Providence, RI},
date={2015},
pages={xviii+749},
isbn={978-1-4704-1103-9},
review={\MR {3364494}},
doi={10.1090/simon/004},
}
Reference [12]
D. R. Yafaev, Mathematical scattering theory, Translations of Mathematical Monographs, vol. 105, American Mathematical Society, Providence, RI, 1992. General theory; Translated from the Russian by J. R. Schulenberger, DOI 10.1090/mmono/105. MR1180965, Show rawAMSref\bib{Ya92}{book}{
author={Yafaev, D. R.},
title={Mathematical scattering theory},
series={Translations of Mathematical Monographs},
volume={105},
note={General theory; Translated from the Russian by J. R. Schulenberger},
publisher={American Mathematical Society, Providence, RI},
date={1992},
pages={x+341},
isbn={0-8218-4558-6},
review={\MR {1180965}},
doi={10.1090/mmono/105},
}
Mathematical Sciences Institute, Australian National University, Kingsley Street, Canberra, ACT 0200, Australia; and School of Mathematics and Applied Statistics, University of Wollongong, NSW, Australia, 2522
Note. To explore an equation, focus it (e.g., by clicking on it) and use the arrow keys to navigate its structure. Screenreader users should be advised that enabling speech synthesis will lead to duplicate aural rendering.