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Linear Trace-Deficit Decay for Permanents of Positive Semidefinite Contractions

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Abstract

Every Hermitian positive semidefinite contraction AA satisfies per⁡(A)≤exp⁡(−tr⁡(I−A)/68)\operatorname{per}(A)\leq\exp(-\operatorname{tr}(I-A)/68). This proves the linear trace-deficit bound conjectured by Ebrahimnejad, Nagda, and Oveis Gharan, whose estimate had quadratic dependence on the normalized deficit. The proof combines a size-biased complex Gaussian representation, a block version of Hanson–Wright decoupling, and a rational Loewner majorant. The constant is uniform in the dimension and is not optimized.

Introduction

Background and the source problem

For A=(Aij)∈Cn×nA=(A_{ij})\in\mathbb{C}^{n\times n}, its permanent is

per⁡(A)=∑σ∈Sn∏i=1nAi,σ(i).\operatorname{per}(A)=\sum_{\sigma\in S_n}\prod_{i=1}^{n}A_{i,\sigma(i)}.

When AA is Hermitian positive semidefinite, the permanent is nonnegative and admits a useful complex Gaussian representation. The permanent of a positive semidefinite matrix is also monotone in the Loewner order; both facts will be proved below.

There are two related questions: how accurately a permanent can be approximated, and how small it must be when the matrix falls below the identity. For the first, Anari, Gurvits, Oveis Gharan, and Saberi [3 Theorem 1 and Definition 1] obtained a deterministic e(γ+1)ne^{(\gamma+1)n}-approximation through a diagonal-majorant relaxation; here γ\gamma is Euler’s constant. Yuan and Parrilo [4 Corollary 1.2] sharpened the guarantee for that relaxation using its connection with products of linear forms and low-rank solutions. Ebrahimnejad, Nagda, and Oveis Gharan [1 Theorems 1.1–1.2] subsequently improved the approximation exponent below γ+1\gamma+1 and established hardness below γ\gamma. Anari and Ebrahimnejad [2 Theorem 1] have now obtained the optimal e(γ+o(1))ne^{(\gamma+o(1))n} exponent. The present paper concerns the second question, a structural inequality for each individual matrix.

In their work on approximating positive semidefinite permanents, Ebrahimnejad, Nagda, and Oveis Gharan established the following trace-sensitive estimate.

Theorem 1.1 (Ebrahimnejad–Nagda–Oveis Gharan [1 Lemma 1.3]). Let 0≤ε≤10\le\varepsilon\le1, and let A∈Cn×nA\in\mathbb{C}^{n\times n} be Hermitian with

0⪯A⪯Inandtr⁡(A)≤(1−ε)n.0\preceq A\preceq I_n \qquad\text{and} \qquad\operatorname{tr}(A)\le(1-\varepsilon)n.

Then

per⁡(A)≤(1−ε220)n.\operatorname{per}(A)\le\left(1-\frac{\varepsilon^2}{20}\right)^n.

In Section 1.4 of [1], the authors identify the O(ε2)O(\varepsilon^2) dependence in Theorem 1.1 as the bottleneck to a better approximation ratio and conjecture that it can be improved to O(ε)O(\varepsilon). Since the estimate in Theorem 1.1 is expressed through its base, the corresponding quantitative target is the following.

Conjectural target 1.2 (Linear form of the source-paper target [1 Section 1.4]). There is a universal constant c>0c > 0 such that, for every 0≤ε≤10 \le\varepsilon\le1 and every Hermitian matrix AA satisfying

0⪯A⪯In,tr⁡(A)≤(1−ε)n,0 \preceq A \preceq I_n,\qquad\operatorname{tr}(A) \le(1-\varepsilon)n,

one has

per⁡(A)≤(1−cε)n.\operatorname{per}(A) \le(1-c\varepsilon)^n.

Contribution

The main result establishes Conjecture 1.2 through an exponential estimate in the actual trace deficit.

Theorem 1.3 (Trace-deficit decay). For every n≥1n \ge1 and every Hermitian matrix A∈Cn×nA \in\mathbb{C}^{n \times n} with 0⪯A⪯In0 \preceq A \preceq I_n,

per⁡(A)≤exp⁡(−168tr⁡(In−A)).(1)\operatorname{per}(A) \le\exp\left(-\frac{1}{68}\operatorname{tr}(I_n-A)\right). \tag*{(1)}

Corollary 1.4 (Linear dependence on ε\varepsilon). Under the hypotheses of Conjecture 1.2,

per⁡(A)≤e−εn/68≤(1−cε)n,c=1−e−1/68>0.\operatorname{per}(A) \le e^{-\varepsilon n/68} \le(1-c\varepsilon)^n,\qquad c=1-e^{-1/68}>0.

The proof has two principal components.

  1. The local estimate in Theorem 4.1 shows that, for K⪰0K \succeq0 of sufficiently small operator norm,

log⁡per⁡((In+K)−1)≤−tr⁡(K)+17tr⁡(K2).\log\operatorname{per}((I_n+K)^{-1}) \le-\operatorname{tr}(K)+17\operatorname{tr}(K^2).

Its linear term comes from an exact Gaussian density calculation, while Lemma 3.1 keeps the quadratic error proportional to tr⁡(K2)\operatorname{tr}(K^2), rather than to (tr⁡K)2(\operatorname{tr}K)^2.

  1. Lemma 5.2 compares a general contraction A=In−DA=I_n-D to the rational majorant (In+θD)−1(I_n+\theta D)^{-1} in Loewner order. Taking θ=1/34\theta=1/34, applying Theorem 4.1, and using D2⪯DD^2\preceq D yields Theorem 1.3.

Intuition and related methods

For a diagonal contraction, the scalar inequality a≤e−(1−a)a\le e^{-(1-a)} immediately gives per⁡(A)≤e−tr⁡(I−A)\operatorname{per}(A)\le e^{-\operatorname{tr}(I-A)}. Off-diagonal entries introduce additional permutation terms, and Example 6.2 shows that this constant cannot hold for all contractions. Nevertheless, the total spectral deficit remains the right quantity. The spectral cutoff in the proof of [1 Lemma 1.3] first finds sufficiently many eigenvalues a sufficient distance below one. Both quantities cost a factor of the normalized deficit. The rational majorant above instead shrinks every deficit by the same fixed factor and retains their entire sum.

The local calculation explains why this is possible. Gaussian Wick identities for PSD permanents are standard; see [1 Lemma 2.9]. Barvinok [5] uses such an integral representation for an approximation scheme when the eigenvalues lie in [1,2][1,2], and [1 Lemma 3.2] uses it to bound permanents by determinants. Here a change of density absorbs the product of squared coordinates into independent size-biased complex Gaussian variables. Their expected quadratic form is 2tr⁡K2\operatorname{tr}K, whereas the determinant factor contributes at most tr⁡K\operatorname{tr}K. This leaves a negative linear term. The essential estimate is that its fluctuation costs only O(tr⁡K2)O(\operatorname{tr}K^2).

The random partition and Gaussian linearization used to control that fluctuation follow the proof strategy of Rudelson and Vershynin [6], proof of Theorem 1.1, Steps 2–4. The auxiliary-Gaussian comparison also appears in Hsu, Kakade, and Zhang [7, Theorem 1 and Remark 2]. These are precedents for the method, rather than statements of the permanent inequality. Each complex coordinate here gives an independent two-dimensional real block; its real and imaginary parts are dependent after size biasing. Lemma 3.1 therefore gives the block argument explicitly, with constants sufficient for the application. The exact Gamma transform handles the diagonal part separately.

Corollary 1.4 provides the replacement requested in [1 Section 1.4]. It is not needed to claim the current best approximation ratio, which is already supplied by [2]. The entropic upper certificate in [2 Eq. (4) and Theorem 7] does not by itself give trace-deficit decay: on A=aInA=aI_n, a>0a>0, it equals (4a/e)n(4a/e)^n. Indeed, its logarithm is the maximum of

nlog⁡a+∑ilog⁡Xii+log⁡det⁡X−tr⁡X+n(X≻0).n\log a+\sum_i \log X_{ii}+\log\det X-\operatorname{tr}X+n \qquad(X\succ0).

Hadamard’s determinant inequality bounds this by nlog⁡a+∑i(2log⁡Xii−Xii+1)n\log a+\sum_i(2\log X_{ii}-X_{ii}+1). Each summand is maximized at Xii=2X_{ii}=2, and X=2InX=2I_n attains equality. Thus this certificate exceeds one for e/4<a<1e/4<a<1, even though the trace deficit is positive. Theorem 1.3 supplies a direct pointwise estimate; its constant is not asserted to be optimal.

Another algorithmic upper bound is the permanent process of Laddha and Pittu [8, Algorithm 1 and Theorem 1.3], valid for real PSD matrices as well as nonnegative matrices. Its elimination-type certificate need not decay on contractions: on the rank-one projection Jn/nJ_n/n, where JnJ_n is the all-ones matrix, each step doubles all entries of the remaining submatrix. The product of its pivots is therefore 2n(n−1)/2/nn2^{n(n-1)/2}/n^n, which already exceeds one at n=7n=7. Yi’s recent deterministic approximation scheme [9, Theorem 1.1(b)] instead treats nonnegative matrices with dense support and nonzero entries in a fixed positive interval. That input regime differs from arbitrary complex PSD contractions.

Gaussian preliminaries

We write X∗X^* for the conjugate transpose of a complex matrix XX. The symbols ∥⋅∥op⁡\lVert\cdot\rVert_{\operatorname{op}} and ∥⋅∥F\lVert\cdot\rVert_F denote the operator and Frobenius norms. A standard circular complex Gaussian random variable has density

dγ(w)=1πe−∣w∣2 d2w(w∈C).d\gamma(w)=\frac{1}{\pi}e^{-\lvert w\rvert^2}\,d^2w \qquad(w\in\mathbb{C}).

Equivalently, W=(G1+iG2)/2W=(G_1+iG_2)/\sqrt{2}, where G1,G2G_1,G_2 are independent standard real Gaussian variables.

Wick's formula

The following representation is the complex version of Wick’s formula. It also appears as Lemma 2.9 in [1].

Lemma 2.1 (Complex Gaussian representation). Let B∈Cn×nB\in\mathbb{C}^{n\times n} be Hermitian positive semidefinite, and let ZZ be a centered circular complex Gaussian vector with covariance E[ZZ∗]=B\mathbb{E}[ZZ^*]=B. Then

per⁡(B)=E∏i=1n∣Zi∣2.(2)\operatorname{per}(B)=\mathbb{E}\prod_{i=1}^{n}\lvert Z_i\rvert^2. \tag*{(2)}

Proof. For a circular complex Gaussian vector, the only nonzero pairings in the mixed moment

E[Z1⋯ZnZ1‾⋯Zn‾]\mathbb{E}[Z_1\cdots Z_n\overline{Z_1}\cdots\overline{Z_n}]

pair each unbarred coordinate with a barred coordinate. Such a pairing is specified by a permutation σ∈Sn\sigma\in S_n, and its contribution is

∏i=1nE[ZiZσ(i)‾]=∏i=1nBi,σ(i).\prod_{i=1}^{n}\mathbb{E}[Z_i\overline{Z_{\sigma(i)}}]=\prod_{i=1}^{n}B_{i,\sigma(i)}.

Summing over all σ∈Sn\sigma\in S_n gives (2). A singular covariance follows either from the same moment identity or by approximation with B+δInB+\delta I_n.

A size-biased complex Gaussian law

Define a probability measure ν1\nu_1 on C\mathbb{C} by

dν1(w)=1π∣w∣2e−∣w∣2 d2w.(3)d\nu_1(w)=\frac{1}{\pi}|w|^2e^{-|w|^2}\,d^2w. \tag*{(3)}

It is normalized because Eγ∣W∣2=1\mathbb{E}_{\gamma}|W|^2=1. The next lemma records both a subgaussian estimate in real coordinates and the exact radial Laplace transform.

Lemma 2.2 (Size-biased Gaussian identities). Let WW have law ν1\nu_1, and set

ξ=(2 ℜW,2 ℑW)∈R2.\xi=(\sqrt{2}\,\Re W,\sqrt{2}\,\Im W)\in\mathbb{R}^2.

Then, for every u∈R2u\in\mathbb{R}^2,

EeuTξ=(1+∥u∥222)e∥u∥22/2≤e∥u∥22.(4)\mathbb{E}e^{u^{\mathsf{T}}\xi}=\left(1+\frac{\lVert u\rVert_2^2}{2}\right)e^{\lVert u\rVert_2^2/2}\leq e^{\lVert u\rVert_2^2}. \tag*{(4)}

Moreover, R=∣W∣2R=|W|^2 has the Gamma(2,1)(2,1) density xe−xxe^{-x} on [0,∞)[0,\infty), and therefore

Ee−aR=(1+a)−2,ER=2(a≥0).(5)\mathbb{E}e^{-aR}=(1+a)^{-2},\qquad\mathbb{E}R=2\qquad(a\geq0). \tag*{(5)}

Proof. Under the untilted law γ\gamma, the vector (2 ℜW,2 ℑW)(\sqrt{2}\,\Re W,\sqrt{2}\,\Im W) is a standard real Gaussian vector G=(G1,G2)G=(G_1,G_2), while ∣W∣2=(G12+G22)/2|W|^2=(G_1^2+G_2^2)/2. Hence, for every nonnegative measurable function ff,

Eν1f(ξ)=12E[(G12+G22)f(G)].\mathbb{E}_{\nu_1}f(\xi)=\frac{1}{2}\mathbb{E}\left[(G_1^2+G_2^2)f(G)\right].

Differentiating the standard Gaussian moment-generating function gives

E[Gj2euTG]=(1+uj2)e∥u∥22/2.\mathbb{E}\left[G_j^2e^{u^{\mathsf{T}}G}\right]=(1+u_j^2)e^{\lVert u\rVert_2^2/2}.

Summing over j=1,2j=1,2 and dividing by 2 yields the equality in (4). Its inequality follows from 1+t/2≤et/21+t/2\leq e^{t/2} for t≥0t\geq0.

Under γ\gamma, the variable ∣W∣2|W|^2 has density e−xe^{-x} on [0,∞)[0,\infty). The size bias in (3) changes this to xe−xxe^{-x}. Direct integration gives

∫0∞xe−(1+a)x dx=(1+a)−2,\int_0^\infty xe^{-(1+a)x}\,dx=(1+a)^{-2},

and differentiating at a=0a=0 gives ER=2\mathbb{E}R=2.

Corollary 2.3 (Product-block linear MGF). Let ξ1,…,ξn\xi_1,\ldots,\xi_n be independent copies of the vector in Lemma 2.2, and put Ξ=(ξ1,…,ξn)∈R2n\Xi=(\xi_1,\ldots,\xi_n)\in\mathbb{R}^{2n}. Then

EevTΞ≤e∥v∥22for every v∈R2n.\mathbb{E}e^{v^{\mathsf{T}}\Xi}\leq e^{\lVert v\rVert_2^2}\qquad\text{for every }v\in\mathbb{R}^{2n}.

Proof. Apply (4) to each two-dimensional block of vv and multiply the resulting estimates.

An off-diagonal quadratic MGF estimate

The local permanent estimate will separate the diagonal and off-diagonal parts of a quadratic form. The diagonal transform is explicit by (5). The following dimension-free estimate controls the off-diagonal part.

Lemma 3.1 (Block-off-diagonal quadratic estimate). Let Ξ=(ξ1,…,ξn)\Xi=(\xi_1,\ldots,\xi_n) be as in Corollary 2.3. Let RR be a real symmetric 2n×2n2n \times2n matrix whose diagonal 2×22 \times2 blocks vanish. If

64s2∥R∥op2≤12,(6)64s^2\lVert R\rVert_{\mathrm{op}}^2 \le\frac{1}{2}, \tag*{(6)}

then

log⁡EesΞTRΞ≤32s2∥R∥F2.(7)\log\mathbb{E}e^{s\Xi^{\mathsf{T}}R\Xi} \le32s^2\lVert R\rVert_{\mathrm{F}}^2. \tag*{(7)}

Proof. Choose a random set Λ⊂{1,…,n}\Lambda\subset\{1,\ldots,n\} by including each block index independently with probability 1/21/2, and define

XΛ=∑i∈Λj∉ΛξiTRijξj.X_\Lambda=\sum_{\substack{i\in\Lambda\\j\notin\Lambda}}\xi_i^{\mathsf{T}}R_{ij}\xi_j.

Because the diagonal blocks of RR vanish, every ordered pair (i,j)(i,j) with i≠ji\ne j occurs in this sum with probability 1/41/4. Consequently,

ΞTRΞ=4EΛXΛ.(8)\Xi^{\mathsf{T}}R\Xi=4\mathbb{E}_\Lambda X_\Lambda. \tag*{(8)}

For every fixed value of Ξ\Xi, convexity of the exponential gives

esΞTRΞ≤EΛe4sXΛ.(9)e^{s\Xi^{\mathsf{T}}R\Xi}\le\mathbb{E}_\Lambda e^{4sX_\Lambda}. \tag*{(9)}

Fix Λ\Lambda. Write a=ΞΛa=\Xi_\Lambda and b=ΞΛcb=\Xi_{\Lambda^c}, and let TΛT_\Lambda be the rectangular cross-cut block of RR for which

XΛ=bTTΛa.X_\Lambda=b^{\mathsf{T}}T_\Lambda a.

For u∈Ru\in\mathbb{R}, conditioning on aa and applying Corollary 2.3 to the independent blocks in bb yields

Eb[euXΛ∣a]≤exp⁡(u2∥TΛa∥22).(10)\mathbb{E}_b[e^{uX_\Lambda}\mid a]\le\exp\left(u^2\lVert T_\Lambda a\rVert_2^2\right). \tag*{(10)}

Let gg be a standard real Gaussian vector of the row dimension of TΛT_\Lambda, independent of all other variables. Gaussian linearization and another use of Corollary 2.3 give

eu2∥TΛa∥22=Ege2∣u∣gTTΛa,(11)e^{u^2\lVert T_\Lambda a\rVert_2^2}=\mathbb{E}_g e^{\sqrt{2}|u|g^{\mathsf{T}}T_\Lambda a}, \tag*{(11)}
Eae2∣u∣gTTΛa≤exp⁡(2u2∥TΛTg∥22).(12)\mathbb{E}_a e^{\sqrt{2}|u|g^{\mathsf{T}}T_\Lambda a}\le\exp\left(2u^2\lVert T_\Lambda^{\mathsf{T}}g\rVert_2^2\right). \tag*{(12)}

Combining (10)–(12), and denoting the singular values of TΛT_\Lambda by σ1,…,σm\sigma_1,\ldots,\sigma_m, gives

EeuXΛ≤∏r=1m(1−4u2σr2)−1/2,(13)\mathbb{E}e^{uX_\Lambda}\le\prod_{r=1}^{m}(1-4u^2\sigma_r^2)^{-1/2}, \tag*{(13)}

provided 4u2∥TΛ∥op2<14u^2\lVert T_\Lambda\rVert_{\mathrm{op}}^2<1. For 0≤x≤1/20\le x\le1/2, the elementary inequality −12log⁡(1−x)≤x-\frac{1}{2}\log(1-x)\le x holds. It follows from (13) that, whenever 4u2∥TΛ∥op2≤1/24u^2\lVert T_\Lambda\rVert_{\mathrm{op}}^2\le1/2,

log⁡EeuXΛ≤4u2∥TΛ∥F2.(14)\log\mathbb{E}e^{uX_\Lambda}\le4u^2\lVert T_\Lambda\rVert_{\mathrm{F}}^2. \tag*{(14)}

The cross-cut block is a rectangular compression of RR, so

∥TΛ∥op≤∥R∥op.\lVert T_\Lambda\rVert_{\mathrm{op}}\le\lVert R\rVert_{\mathrm{op}}.

In the decomposition into the coordinates indexed by Λ\Lambda and Λc\Lambda^{c}, the two cross-cut blocks of the symmetric matrix RR are TΛT_{\Lambda} and TΛTT_{\Lambda}^{\mathsf{T}}. Thus

2∥TΛ∥F2≤∥R∥F2.(15)2\lVert T_{\Lambda}\rVert_{\mathrm{F}}^{2}\leq\lVert R\rVert_{\mathrm{F}}^{2}. \tag*{(15)}

Set u=4su=4s. The hypothesis (6) implies the condition for (14), and hence

log⁡Ee4sXΛ≤64s2∥TΛ∥F2≤32s2∥R∥F2.\log\mathbb{E}e^{4sX_{\Lambda}}\leq64s^{2}\lVert T_{\Lambda}\rVert_{\mathrm{F}}^{2}\leq32s^{2}\lVert R\rVert_{\mathrm{F}}^{2}.

This bound is uniform in Λ\Lambda. Taking expectations in (9) and then applying the uniform bound proves (7).

Local stability near the identity

We now combine the exact radial transform and Lemma 3.1. The resulting estimate is local only in operator norm and has no dependence on the dimension.

Theorem 4.1 (Local permanent stability). Let K∈Cn×nK\in\mathbb{C}^{n\times n} be Hermitian positive semidefinite and satisfy

∥K∥op≤217.\lVert K\rVert_{\mathrm{op}}\leq\frac{\sqrt{2}}{17}.

Then

log⁡per⁡((In+K)−1)≤−tr⁡(K)+17tr⁡(K2).(16)\log\operatorname{per}\left((I_n+K)^{-1}\right)\leq-\operatorname{tr}(K)+17\operatorname{tr}(K^{2}). \tag*{(16)}

Proof. Put B=(In+K)−1B=(I_n+K)^{-1}. The matrix BB is positive definite. If ZZ is circular complex Gaussian with covariance BB, then Lemma 2.1 and the Gaussian density give

per⁡(B)=1πndet⁡B∫Cn(∏i=1n∣zi∣2)e−z∗B−1z d2nz=det⁡(In+K)Eνe−W∗KW.(17)\operatorname{per}(B)=\frac{1}{\pi^{n}\det B}\int_{\mathbb{C}^{n}}\left(\prod_{i=1}^{n}|z_i|^{2}\right)e^{-z^{*}B^{-1}z}\,d^{2n}z =\det(I_n+K)\mathbb{E}_{\nu}e^{-W^{*}KW}. \tag*{(17)}

where ν=ν1⊗n\nu=\nu_1^{\otimes n} and the coordinates W1,…,WnW_1,\ldots,W_n are independent with the density (3). Write ki=Kii≥0k_i=K_{ii}\geq0 and decompose the real random variable

Q=W∗KW=Qd+Qo,Q=W^{*}KW=Q_{\mathrm{d}}+Q_{\mathrm{o}},

where

Qd=∑i=1nki∣Wi∣2,Qo=∑i≠jWi‾KijWj.Q_{\mathrm{d}}=\sum_{i=1}^{n}k_i|W_i|^{2},\qquad Q_{\mathrm{o}}=\sum_{i\neq j}\overline{W_i}K_{ij}W_j.

By (5),

EνQd=2tr⁡(K),EνQo=0.\mathbb{E}_{\nu}Q_{\mathrm{d}}=2\operatorname{tr}(K),\qquad\mathbb{E}_{\nu}Q_{\mathrm{o}}=0.

Set Ud=Qd−2tr⁡(K)U_{\mathrm{d}}=Q_{\mathrm{d}}-2\operatorname{tr}(K), and choose the conjugate Hölder exponents

p=17,q=1716.p=17,\qquad q=\frac{17}{16}.

Hölder’s inequality yields

Eνe−(Q−2tr⁡K)≤(Eνe−pUd)1/p(Eνe−qQo)1/q.(18)\mathbb{E}_{\nu}e^{-(Q-2\operatorname{tr}K)} \leq\left(\mathbb{E}_{\nu}e^{-pU_{\mathrm{d}}}\right)^{1/p} \left(\mathbb{E}_{\nu}e^{-qQ_{\mathrm{o}}}\right)^{1/q}. \tag*{(18)}

For the diagonal factor, the exact transform (5) gives

Ee−pki(∣Wi∣2−2)=e2pki(1+pki)−2.\mathbb{E}e^{-pk_i(|W_i|^{2}-2)}=e^{2pk_i}(1+pk_i)^{-2}.

Independence therefore implies

1plog⁡Eνe−pUd=∑i=1n(2ki−2plog⁡(1+pki)).(19)\frac{1}{p}\log\mathbb{E}_{\nu}e^{-pU_d}=\sum_{i=1}^{n}\left(2k_i-\frac{2}{p}\log(1+pk_i)\right). \tag*{(19)}

The elementary inequality log⁡(1+x)≥x−x2/2\log(1+x)\ge x-x^2/2 for x≥0x\ge0 turns (19) into

1plog⁡Eνe−pUd≤17∑i=1nki2.(20)\frac{1}{p}\log\mathbb{E}_{\nu}e^{-pU_d}\le17\sum_{i=1}^{n}k_i^2. \tag*{(20)}

It remains to control the off-diagonal factor. Write K=P+iSK=P+iS, where PP is real symmetric and SS is real skew-symmetric. Its realification is

R(K)=(P−SSP).\mathcal{R}(K)=\begin{pmatrix}P&-S\\S&P\end{pmatrix}.

For ξi=(2 ℜWi,2 ℑWi)\xi_i=(\sqrt{2}\,\Re W_i,\sqrt{2}\,\Im W_i) and Ξ=(ξ1,…,ξn)\Xi=(\xi_1,\ldots,\xi_n), after the harmless orthogonal permutation that groups coordinates by ii, one has

W∗KW=ΞTMΞ,M=12R(K).W^{*}KW=\Xi^{\mathsf T}M\Xi,\qquad M=\frac{1}{2}\mathcal{R}(K).

Let H=K−diag⁡(K)H=K-\operatorname{diag}(K), and let MoM_o be obtained from MM by deleting its diagonal 2×22\times2 blocks. Then

Qo=ΞTMoΞ,Mo=12R(H)Q_o=\Xi^{\mathsf T}M_o\Xi,\qquad M_o=\frac{1}{2}\mathcal{R}(H)

up to the same coordinate permutation. The realification identities give

∥Mo∥op⁡=12∥H∥op⁡,∥Mo∥F2=12∥H∥F2.(21)\lVert M_o\rVert_{\operatorname{op}}=\frac{1}{2}\lVert H\rVert_{\operatorname{op}},\qquad\lVert M_o\rVert_{\mathrm F}^{2}=\frac{1}{2}\lVert H\rVert_{\mathrm F}^{2}. \tag*{(21)}

Since K⪰0K\succeq0,

∥diag⁡(K)∥op⁡=max⁡iki≤∥K∥op⁡.\lVert\operatorname{diag}(K)\rVert_{\operatorname{op}}=\max_i k_i\le\lVert K\rVert_{\operatorname{op}}.

It follows from (21) that

∥Mo∥op⁡≤12(∥K∥op⁡+∥diag⁡(K)∥op⁡)≤∥K∥op⁡.(22)\lVert M_o\rVert_{\operatorname{op}}\le\frac{1}{2}\left(\lVert K\rVert_{\operatorname{op}}+\lVert\operatorname{diag}(K)\rVert_{\operatorname{op}}\right)\le\lVert K\rVert_{\operatorname{op}}. \tag*{(22)}

The norm hypothesis and q=17/16q=17/16 now give the exact threshold

64q2∥Mo∥op⁡2≤64(1716)2(217)2=12.64q^2\lVert M_o\rVert_{\operatorname{op}}^2\le64\left(\frac{17}{16}\right)^2\left(\frac{\sqrt{2}}{17}\right)^2=\frac{1}{2}.

Lemma 3.1, applied with R=MoR=M_o and s=−qs=-q, therefore yields

log⁡Eνe−qQo≤32q2∥Mo∥F2.\log\mathbb{E}_{\nu}e^{-qQ_o}\le32q^2\lVert M_o\rVert_{\mathrm F}^2.

Because HH is Hermitian with zero diagonal,

∥Mo∥F2=12∥H∥F2=∑i<j∣Kij∣2.\lVert M_o\rVert_{\mathrm F}^2=\frac{1}{2}\lVert H\rVert_{\mathrm F}^2=\sum_{i<j}|K_{ij}|^2.

Since 32q=3432q=34, we obtain

1qlog⁡Eνe−qQo≤34∑i<j∣Kij∣2.(23)\frac{1}{q}\log\mathbb{E}_{\nu}e^{-qQ_o}\le34\sum_{i<j}|K_{ij}|^2. \tag*{(23)}

Combining (18), (20), and (23), and using

tr⁡(K2)=∑iki2+2∑i<j∣Kij∣2,\operatorname{tr}(K^2)=\sum_i k_i^2+2\sum_{i<j}|K_{ij}|^2,

gives

log⁡Eνe−(Q−2tr⁡K)≤17tr⁡(K2).(24)\log\mathbb{E}_{\nu}e^{-(Q-2\operatorname{tr}K)}\leq17\operatorname{tr}(K^2). \tag*{(24)}

Equivalently,

log⁡Eνe−Q≤−2tr⁡(K)+17tr⁡(K2).\log\mathbb{E}_{\nu}e^{-Q}\leq-2\operatorname{tr}(K)+17\operatorname{tr}(K^2).

Finally, applying log⁡(1+x)≤x\log(1+x)\leq x to the eigenvalues of KK gives log⁡det⁡(In+K)≤tr⁡(K)\log\det(I_n+K)\leq\operatorname{tr}(K). Together with (17), this implies

log⁡per⁡(B)≤−tr⁡(K)+17tr⁡(K2),\log\operatorname{per}(B)\leq-\operatorname{tr}(K)+17\operatorname{tr}(K^2),

which is (16).

Loewner comparison and the global estimate

For completeness, we first prove the monotonicity used in the source paper as Lemma 2.8 [1].

Lemma 5.1 (Loewner monotonicity). If 0⪯A⪯B0\preceq A\preceq B are Hermitian n×nn\times n matrices, then

per⁡(A)≤per⁡(B).\operatorname{per}(A)\leq\operatorname{per}(B).

Proof. In (Cn)⊗n(\mathbb{C}^{n})^{\otimes n}, define

v=1n!∑σ∈Sneσ(1)⊗⋯⊗eσ(n).v=\frac{1}{\sqrt{n!}}\sum_{\sigma\in S_n}e_{\sigma(1)}\otimes\cdots\otimes e_{\sigma(n)}.

Expanding the matrix coefficient and grouping pairs of permutations by their relative permutation gives

⟨v,A⊗nv⟩=per⁡(A).(25)\langle v,A^{\otimes n}v\rangle=\operatorname{per}(A). \tag*{(25)}

Moreover, the telescoping identity

B⊗n−A⊗n=∑j=1nA⊗(j−1)⊗(B−A)⊗B⊗(n−j)B^{\otimes n}-A^{\otimes n}=\sum_{j=1}^{n}A^{\otimes(j-1)}\otimes(B-A)\otimes B^{\otimes(n-j)}

expresses the difference as a sum of positive semidefinite matrices. Hence A⊗n⪯B⊗nA^{\otimes n}\preceq B^{\otimes n}. Taking the matrix coefficient at vv and using (25) proves the claim.

Lemma 5.2 (Rational Loewner majorant). Let 0⪯A⪯In0\preceq A\preceq I_n, put D=In−AD=I_n-A, and let 0≤θ≤10\leq\theta\leq1. Then

A⪯(In+θD)−1.A\preceq(I_n+\theta D)^{-1}.

Proof. For every d∈[0,1]d\in[0,1],

11+θd−(1−d)=d(1−θ+θd)1+θd≥0.(26)\frac{1}{1+\theta d}-(1-d)=\frac{d(1-\theta+\theta d)}{1+\theta d}\geq0. \tag*{(26)}

Since the spectrum of DD is contained in [0,1][0,1], applying (26) through functional calculus gives

In−D⪯(In+θD)−1.I_n-D\preceq(I_n+\theta D)^{-1}.

Proof of Theorem 1.3. Set D=In−AD=I_n-A, so that 0⪯D⪯In0\preceq D\preceq I_n, and choose

θ=134,K=θD,B=(In+K)−1.\theta=\frac{1}{34},\qquad K=\theta D,\qquad B=(I_n+K)^{-1}.

Lemma 5.2 gives A⪯BA\preceq B. Furthermore,

∥K∥op⁡≤134≤217.\lVert K\rVert_{\operatorname{op}}\le\frac{1}{34}\le\frac{\sqrt{2}}{17}.

so Theorem 4.1 applies. Since D2⪯DD^2\preceq D,

tr⁡(K)=θtr⁡(D),tr⁡(K2)=θ2tr⁡(D2)≤θ2tr⁡(D).\operatorname{tr}(K)=\theta\operatorname{tr}(D),\qquad\operatorname{tr}(K^2)=\theta^2\operatorname{tr}(D^2)\le\theta^2\operatorname{tr}(D).

Therefore,

log⁡per⁡(B)≤−tr⁡(K)+17tr⁡(K2)≤−(θ−17θ2)tr⁡(D)=−168tr⁡(D).\begin{aligned} \log\operatorname{per}(B)&\le-\operatorname{tr}(K)+17\operatorname{tr}(K^2)\\ &\le-(\theta-17\theta^2)\operatorname{tr}(D)=-\frac{1}{68}\operatorname{tr}(D). \end{aligned}

By Lemma 5.1,

per⁡(A)≤per⁡(B)≤exp⁡(−168tr⁡(In−A)).\operatorname{per}(A)\le\operatorname{per}(B)\le\exp\left(-\frac{1}{68}\operatorname{tr}(I_n-A)\right).

Proof of Corollary 1.4. The trace hypothesis gives tr⁡(In−A)≥εn\operatorname{tr}(I_n-A)\ge\varepsilon n, so Theorem 1.3 implies

per⁡(A)≤e−εn/68.\operatorname{per}(A)\le e^{-\varepsilon n/68}.

The function x↦e−x/68x\mapsto e^{-x/68} is convex. On [0,1][0,1], it therefore lies below the chord joining its endpoint values:

e−ε/68≤(1−ε)+εe−1/68=1−(1−e−1/68)ε.e^{-\varepsilon/68}\le(1-\varepsilon)+\varepsilon e^{-1/68}=1-(1-e^{-1/68})\varepsilon.

Raising this scalar inequality to the nnth power proves the result.

Examples and remarks

Example 6.1 (Diagonal contractions). For A=diag⁡(a1,…,an)A=\operatorname{diag}(a_1,\ldots,a_n) with 0≤ai≤10\le a_i\le1,

per⁡(A)=∏i=1nai≤exp⁡(−∑i=1n(1−ai))=e−tr⁡(In−A).\operatorname{per}(A)=\prod_{i=1}^{n}a_i\le\exp\left(-\sum_{i=1}^{n}(1-a_i)\right)=e^{-\operatorname{tr}(I_n-A)}.

Here the first inequality is the scalar bound log⁡a≤a−1\log a\le a-1, with the case a=0a=0 understood by continuity. Thus the trace deficit is the natural first-order quantity already in the diagonal case, although the universal constant furnished by the noncommutative argument is smaller.

Example 6.2 (A restriction on the universal constant). The rank-one projection

P=12(1111)P=\frac{1}{2}\begin{pmatrix}1&1\\1&1\end{pmatrix}

has eigenvalues zero and one, per⁡(P)=1/4+1/4=1/2\operatorname{per}(P)=1/4+1/4=1/2, and tr⁡(I2−P)=1\operatorname{tr}(I_2-P)=1. For the block diagonal contraction consisting of mm copies of PP, a nonzero permutation term must preserve each block. The permanent is therefore 2−m2^{-m}, while the trace deficit is mm. Consequently any universal inequality per⁡(A)≤e−κtr⁡(I−A)\operatorname{per}(A)\le e^{-\kappa\operatorname{tr}(I-A)} must have κ≤log⁡2\kappa\le\log2. In particular, the diagonal-case constant one does not extend to all PSD contractions.

Remark 6.3 (Where the dimension-free error enters). The key feature of Lemma 3.1 is its Frobenius-norm error. After realification, this becomes the off-diagonal part of tr⁡(K2)\operatorname{tr}(K^2). Together with the exact Gamma transform of the diagonal part, the entire second-order error in Theorem 4.1 is 17tr⁡(K2)17\operatorname{tr}(K^2). For K=θDK=\theta D and 0⪯D⪯In0\preceq D\preceq I_n, this is at most 17θ2tr⁡(D)17\theta^2\operatorname{tr}(D), which can be absorbed into the linear term uniformly in nn.

Remark 6.4 (Constants). The choices p=17p=17, q=17/16q=17/16, and θ=1/34\theta=1/34 were made to keep the threshold arithmetic transparent. They are not expected to be optimal. The purpose of the estimate is the linear dependence on tr⁡(In−A)\operatorname{tr}(I_n-A), which is exactly what converts the quadratic ε\varepsilon-dependence in Theorem 1.1 into the linear dependence requested in [1 Section 1.4].

References

  1. [1]F. Ebrahimnejad, A. Nagda, and S. Oveis Gharan, On approximability of the permanent of PSD matrices, STOC 2025, 625–630. Numbered references use the full version, arXiv:2404.10959v1, 2024. https://arxiv.org/abs/2404.10959.
  2. [2]N. Anari and F. Ebrahimnejad, Optimal e^{(γ+o(1))n}-Approximation of the Permanent of Positive Semidefinite Matrices, arXiv:2605.21946, 2026. https://arxiv.org/abs/2605.21946.
  3. [3]N. Anari, L. Gurvits, S. Oveis Gharan, and A. Saberi, Simply exponential approximation of the permanent of positive semidefinite matrices, FOCS 2017, 914–925. https://arxiv.org/abs/1704.03486.
  4. [4]C. Yuan and P. A. Parrilo, Maximizing products of linear forms, and the permanent of positive semidefinite matrices, Mathematical Programming 193 (2022), 499–510. https://doi.org/10.1007/s10107-021-01616-3.
  5. [5]A. Barvinok, A remark on approximating permanents of positive definite matrices, arXiv:2005.06344, 2020. https://arxiv.org/abs/2005.06344.
  6. [6]M. Rudelson and R. Vershynin, Hanson–Wright inequality and sub-Gaussian concentration, Electronic Communications in Probability 18 (2013), no. 82, 1–9. https://arxiv.org/abs/1306.2872.

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