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Fredholm determinant properties for trace-class operators

Statement

Assume the Axiom of Choice. Let H be a complex Hilbert space and T∈S1(H). The function DT(z)=det⁡H(I+zT) is entire and, locally uniformly in z,

DT(z)=∏j(1+zλj(T)),

where all nonzero eigenvalues are listed with their finite algebraic multiplicities, and ∑j∣λj(T)∣≤∥T∥1. It satisfies

DT(0)=1,DT′(0)=tr⁡H(T), ∣DT(z)∣≤∏j(1+∣z∣sj(T))≤e∣z∣∥T∥1,

and for every ε>0 there is Cε such that ∣DT(z)∣≤Cεeε∣z∣. For trace-class A,B, ∣DA(z)−DB(z)∣≤∣z∣∥A−B∥1e1+∣z∣∥A∥1+∣z∣∥B∥1, and

det⁡H(I+A+B+AB)=det⁡H(I+A)det⁡H(I+B).

Moreover DT(z)=0 exactly when I+zT is not boundedly invertible, and the zero at −1/λ has the algebraic multiplicity of λ≠0.

If finite-rank Tn converge to T in trace norm, their ordinary finite-dimensional determinants converge to DT locally uniformly. Where I+zT is invertible,

DT′(z)=DT(z)tr⁡H(T(I+zT)−1).

All assertions include H={0}, finite eigenvalue lists and the empty list.

Facts & Assumptions

Given: The Axiom of Choice, a complex Hilbert space H, and the displayed trace-class operators.

[F1]

The determinant is defined through a separable reducing support; its value is independent of the support, entire and normalized, and equals the locally uniform product over the nonzero eigenvalues with algebraic multiplicity. Finite-rank values are ordinary finite-dimensional determinants (Fredholm determinant of a trace-class operator, Arbitrary-Hilbert Fredholm determinant from a separable reducing support).

[F2]

On a separable complex Hilbert space the local determinant satisfies DS′(0)=tr⁡(S) (Local separable trace-class determinant construction).

[F3]

On a separable complex Hilbert space the eigenvalue absolute sum is at most the trace norm, with algebraic multiplicities (Weyl product and sum inequalities for compact operators).

[F4]

On a separable complex Hilbert space the local determinant satisfies the singular-value product and exponential bounds, minimal exponential type, the displayed trace-norm continuity estimate, multiplicativity at z=1, and locally uniform convergence of finite-rank determinants in trace norm (Trace-norm continuity, growth and multiplicativity of the local determinant).

[F5]

On a separable complex Hilbert space, the local determinant vanishes exactly when I+zS is not boundedly invertible, and its zero at −1/λ has order malg(λ;S) (Zeros of the local Fredholm determinant).

[F6]

On a separable complex Hilbert space, at every invertibility point, DS′(z)=DS(z)tr⁡(S(I+zS)−1) (Logarithmic derivative of the local Fredholm determinant).

[F7]

Trace-class operators form a linear two-sided ideal, their trace norm is a norm, and singular values are the positive eigenvalues of ∣T∣ (Trace class is a two sided Banach operator ideal, Absolute value and singular values of a compact operator).

[F8]

The trace is basis-independent and agrees with every nuclear trace sum (Trace is absolutely convergent and basis independent).

Proof

technique · direct
1.1F1F7F8given

Choose a nuclear support M from [F1] and write H=M⊕M⊥ and T=S⊕0. The nuclear trace formula gives tr⁡H(T)=tr⁡M(S): the same nuclear vectors lie in M, so their scalar inner products are unchanged. The block identity T∗T=S∗S⊕0 and uniqueness of the compact positive square root, as established in Fredholm determinant of a trace-class operator, give ∣T∣=∣S∣⊕0. Thus T and S have the same nonzero singular values, including multiplicity, and ∥T∥1=∥S∥1. For each λ≠0, (T−λI)r=(S−λIM)r⊕(−λ)rIM⊥; hence their nonzero eigenvalues and algebraic multiplicities agree.

2.1F1F2F3F4step 1.1

By [F1], DT=DS is entire, normalized, and has the stated locally uniform spectral product. Applying [F3] to S and step 1.1 gives ∑j∣λj(T)∣≤∥T∥1. Applying [F2] gives DT′(0)=DS′(0)=tr⁡M(S)=tr⁡H(T). The singular-value product, exponential bound and minimal exponential type in [F4] transfer from S using the same singular-value list and trace norm. This also covers finite and empty lists.

2.2F1F5F6F8step 1.1

For each z, I+zT=(IM+zS)⊕IM⊥. It has a bounded inverse exactly when IM+zS does, because the inverse of a block diagonal operator is the block inverse and restriction of a bounded inverse to the reducing summand is bounded. The generalized kernels in step 1.1 preserve algebraic multiplicity. Hence [F5] gives both directions of the stated zero criterion and the exact zero order at −1/λ. If I+zT is invertible, its inverse is (IM+zS)−1⊕IM⊥; consequently T(I+zT)−1=S(IM+zS)−1⊕0. The same nuclear trace formula as step 1.1 equates these traces, so [F6] gives the displayed logarithmic derivative.

2.3F1F4F7step 1.1

For trace-class A,B on H, take nuclear representations for both and let N be the closed span of all their input and output vectors. The finite union of the two countable vector lists has a countable dense set of finite Gaussian-rational combinations; the support proof in [F1] shows N is separable and reduces both operators, with A=AN⊕0 and B=BN⊕0. By [F7], C:=A+B+AB is trace class and C=(AN+BN+ANBN)⊕0; the same N supports A−B. The block singular-value argument of step 1.1 gives ∥A−B∥1=∥AN−BN∥1 and ∥A∥1=∥AN∥1, ∥B∥1=∥BN∥1. Apply the separable continuity estimate and multiplicativity in [F4] on N, and use support independence in [F1] for all three determinants. These are exactly the displayed arbitrary-space formulas, including the same numerical exponential constant.

2.4F1F4step 1.1

Suppose finite-rank Tn→T in trace norm. AC chooses nuclear representations for T and the countable family (Tn); taking the closed span of every input and output vector gives one separable reducing support N for all of them. Their restrictions Sn,S obey ∥Sn−S∥1=∥Tn−T∥1→0 by the block singular-value argument of step 1.1. Apply the locally uniform finite-rank approximation in [F4] on N. By [F1], DSn=DTn and each is the ordinary determinant on any finite-dimensional subspace containing ran⁡Tn; the same support lemma shows independence of that subspace. Therefore those ordinary determinants converge locally uniformly to DS=DT.

3.1F1F2F4F5F6step 2.1step 2.2step 2.4∎

If H={0} or T=0, [F1] gives DT≡1, its derivative and trace are zero, and the product and singular-value lists are empty. For z=0, normalization holds, and the logarithmic-derivative formula follows from step 2.1. A finite-rank operator is covered by [F1] and step 2.4. Full AC supplies the separable-support and AC-qualified spectral suppliers and permits the countable family of nuclear representations in step 2.4; its Countable Choice consequence supplies [F2], [F4] and [F6]. Both directions of the zero criterion were established in step 2.2.

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