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Matrix Samplers and Quantum-Proof Extractors: Their Correspondence and Almost-Optimal Constructions

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Abstract

We establish an equivalence between matrix samplers and quantum-proof randomness extractors. The classical sampler–extractor equivalence is established by a seminal work of Zuckerman (Random Structures & Algorithms, 1997). Using this equivalence, we construct explicit strong matrix samplers with optimal randomness overhead and near-optimal sample complexity via constructing quantum-proof extractors. Specifically for matrix dimension DD, accuracy ε\varepsilon and failure probability δ≤εδ\leq\varepsilon, our matrix sampler uses m+Oα(log⁡(D/δ))m+O_α(\log(D/δ)) random bits and Oα(ε−2−αlog⁡1+α(D/δ))O_α(\varepsilon^{-2-α}\log^{1+α}(D/δ)) samples, for any constant α>0α>0. Compared with the matrix sampler of Xun and Zuckerman (CCC 2025), our construction has improvements in two aspects. Under the same optimal random seed length, we can replace the poly⁡D\operatorname{poly} D dependence in the number of samples by O(log⁡1−γD)O(\log^{1-γ} D). Under the same scale of sample size, we can remove their log⁡log⁡D\log\log D factor in the length of the random seed. Our underlying strong quantum-proof extractor has output length n−Oα(a+log⁡(1/η))n-O_α(a+\log(1/η)) and seed length at most (1+α)log⁡a+(2+α)log⁡(1/η)+Oα(1)(1+α)\log a+(2+α)\log(1/η)+O_α(1) for nn-bit sources with conditional min-entropy n−an-a and error ηη. We also obtain strong quantum-proof extractors for every constant entropy rate, for any error as small as 2−Ω(n)2^{-Ω(n)}, having optimal seed length O(log⁡(n/η))O(\log(n/η)) and output length Ω(n)Ω(n), improving previous constructions.

Introduction

Sampling estimates the average of a function from its values at a small number of points. Independent samples give sharp concentration bounds, but require fresh random bits for every evaluation. A randomness-efficient sampler seeks the same accuracy and confidence using samples generated from a much shorter random string. A challenge is to reduce the randomness without substantially increasing the number of samples.

From scalar to matrix sampling. For 0<ε,δ≤1/20 < \varepsilon, \delta\le1/2, consider a function f:{0,1}m→[0,1]f : \{0,1\}^{m} \to[0,1] whose mean we wish to estimate to within additive error ε\varepsilon, by a randomized procedure with failure probability at most δ\delta. The Chernoff bound shows that O(ε−2log⁡(1/δ))O(\varepsilon^{-2}\log(1/\delta)) independent uniform samples suffice. Generating these samples independently, however, costs mm random bits per sample. An averaging sampler can replace independent samples with correlated samples whose empirical average satisfies the same guarantee [8, 21].1

Definition 1.1 (Averaging samplers [8]). Let Samp⁡:{0,1}r×[t]→{0,1}m\operatorname{Samp} : \{0,1\}^{r} \times[t] \to\{0,1\}^{m}, where [t]={1,…,t}[t] = \{1,\ldots,t\}. Let RR be uniform on {0,1}r\{0,1\}^{r}, and let ZZ be uniform on {0,1}m\{0,1\}^{m}. The map Samp⁡\operatorname{Samp} is a (δ,ε)(\delta,\varepsilon) averaging sampler if, for every f:{0,1}m→[0,1]f : \{0,1\}^{m} \to[0,1],

Pr⁡R[∣1t∑i=1tf(Samp⁡(R,i))−EZf(Z)∣>ε]≤δ.\Pr_{R}\left[\left|\frac{1}{t}\sum_{i=1}^{t}f(\operatorname{Samp}(R,i))-\mathbb{E}_{Z}f(Z)\right|>\varepsilon\right]\leq\delta.

The main parameters here are the randomness complexity rr and the sample complexity tt. Classical approaches include limited independence, expander walks, and iterated sampling [11, 1, 27, 18, 25, 8]. Goldreich’s survey [21] gives an account of these methods and distinguishes averaging samplers from general samplers, such as median-of-averages constructions [7], that may use a different estimator; see also Canetti, Even, and Goldreich [9] for lower bounds. Zuckerman [Zuc97] and Reingold, Vadhan, and Wigderson [42] used the connection to extractors to approach optimal randomness complexity. More recently, for δ<ε\delta< \varepsilon, Xun and Zuckerman [XZ25] achieved m+O(log⁡(1/δ))m + O(\log(1/\delta)) random bits with sample count Oα((ε−2log⁡(1/δ))1+α)O_{\alpha}((\varepsilon^{-2}\log(1/\delta))^{1+\alpha}) for every fixed α>0\alpha> 0.

There is a matrix analogue of the sampling task for estimating scalar functions. Specifically the matrix analogue asks us to estimate the mean of a function f:{0,1}m→CD×Df : \{0,1\}^{m} \to\mathbb{C}^{D\times D}, where ∥f(z)∥≤1\|f(z)\| \leq1, and to measure the error in operator norm, ∥A∥=max⁡∥v∥2=1∥Av∥2\|A\| = \max_{\|v\|_{2}=1}\|Av\|_{2}. Thus the approximation must be accurate in every direction simultaneously. Matrix concentration inequalities, applied through Hermitian dilation for general complex matrices, show that O(ε−2log⁡(2D/δ))O(\varepsilon^{-2}\log(2D/\delta)) independent samples suffice, so the dimension enters only logarithmically [2, 49]. Such bounds are basic tools in spectral graph theory, numerical linear algebra, and quantum information. Their derandomization motivates the study of matrix (averaging) samplers [WX08, GLSS18, XZ25].

Definition 1.2 (Matrix (Averaging) samplers [XZ25]). Let Samp⁡:{0,1}r×[t]→{0,1}m\operatorname{Samp} : \{0,1\}^{r} \times[t] \to\{0,1\}^{m}. Let RR be uniform on {0,1}r\{0,1\}^{r}, and let ZZ be uniform on {0,1}m\{0,1\}^{m}.

The map Samp⁡\operatorname{Samp} is a DD-dimensional (δ,ε)(\delta,\varepsilon) matrix sampler if, for every f:{0,1}m→CD×Df : \{0,1\}^{m} \to\mathbb{C}^{D\times D} satisfying ∥f(z)∥≤1\|f(z)\| \leq1 for every zz,

Pr⁡R[∥1t∑i=1tf(Samp⁡(R,i))−EZf(Z)∥>ε]≤δ.\Pr_{R}\left[\left\|\frac{1}{t}\sum_{i=1}^{t}f(\operatorname{Samp}(R,i))-\mathbb{E}_{Z}f(Z)\right\|>\varepsilon\right]\leq\delta.

The map Samp⁡\operatorname{Samp} is a strong DD-dimensional (δ,ε)(\delta,\varepsilon) matrix sampler if, for every sequence f1,…,ft:{0,1}m→CD×Df_{1},\ldots,f_{t} : \{0,1\}^{m} \to\mathbb{C}^{D\times D} satisfying ∥fi(z)∥≤1\|f_i(z)\| \leq1 for every i,zi,z,

Pr⁡R[∥1t∑i=1t(fi(Samp⁡(R,i))−EZfi(Z))∥>ε]≤δ.\Pr_{R}\left[\left\|\frac{1}{t}\sum_{i=1}^{t}\left(f_i(\operatorname{Samp}(R,i))-\mathbb{E}_{Z}f_i(Z)\right)\right\|>\varepsilon\right]\leq\delta.

We sometimes use the term ordinary matrix sampler to distinguish a matrix sampler from a strong matrix sampler.

We call Samp⁡\operatorname{Samp} explicit if the map R↦(Samp⁡(R,1),…,Samp⁡(R,t))R \mapsto(\operatorname{Samp}(R,1),\ldots,\operatorname{Samp}(R,t)) is computable in time polynomial in r+mtr+mt. The strong version allows the test to depend on the sample position. The challenge is to satisfy this requirement while keeping both the randomness complexity and the sample complexity small.

The matrix problem has developed along two complementary lines. Garg, Lee, Song, and Srivastava [20] established a matrix Chernoff bound for expander walks, resolving the conjecture arising from the work of Wigderson and Xiao [WX08]. Subsequent extensions cover finite Markov chains [36] and time-dependent matrix observables on general state spaces [33]. Song’s recent work [45] sharpens the Hoeffding and Bernstein constants, including in the expander-walk setting. For a stationary walk on a fixed-degree expander with constant absolute spectral gap, these bounds give sample count t=O(ε−2log⁡(2D/δ))t = O(\varepsilon^{-2}\log(2D/\delta)), matching the independent-sampling bound. Generating the standard walk uses m+Θ(t)m+\Theta(t) random bits, so this construction retains an ε−2\varepsilon^{-2} factor in its randomness overhead.

The other line seeks to reduce this overhead directly. Applying a scalar sampler entry by entry gives good randomness complexity, but introduces a polynomial dependence on DD in the sample count [XZ25]. In the regime δ≤ε\delta\le\varepsilon, Xun and Zuckerman [XZ25] substantially improved the tradeoff through sampler composition: their constructions offer either nearly optimal sample complexity with an additional dimension-dependent randomness cost, or randomness overhead O(log⁡(D/δ))O(\log(D/\delta)) with a polynomial dependence on DD in the sample count. Their constructions also satisfy the strong sampling requirement [XZ25, Remark 9].

Randomness extraction and quantum side information. As shown by Zuckerman [Zuc97], there is a correspondence between averaging samplers and randomness extractors. A seeded extractor converts a weak random source into nearly uniform bits with the help of a short independent random seed. We measure the randomness of a source XX by its min-entropy H∞(X)=−log⁡2max⁡xPr⁡[X=x]H_\infty(X)=-\log_2\max_x\Pr[X=x]. Write UjU_j for the uniform distribution on jj bits and Δ(P,Q)=12∑z∣P(z)−Q(z)∣\Delta(P,Q)=\frac{1}{2}\sum_z\lvert P(z)-Q(z)\rvert for total variation distance.

Definition 1.3 (Seeded extractors [35]). A function Ext⁡:{0,1}n×{0,1}d→{0,1}m\operatorname{Ext}:\{0,1\}^n\times\{0,1\}^d\to\{0,1\}^m is a (k,η)(k,\eta) extractor if, for every distribution XX on {0,1}n\{0,1\}^n with H∞(X)≥kH_\infty(X)\ge k and an independent uniform seed Y∼UdY\sim U_d,

Δ(Ext⁡(X,Y),Um)≤η.\Delta(\operatorname{Ext}(X,Y),U_m)\le\eta.

The map Ext⁡\operatorname{Ext} is strong if, for every XX with H∞(X)≥kH_\infty(X)\ge k,

Δ((Ext⁡(X,Y),Y),Um+d)≤η.\Delta((\operatorname{Ext}(X,Y),Y),U_{m+d})\le\eta.

The classical goal is to maximize the output while minimizing the seed length, subject to the lower bounds of Radhakrishnan and Ta-Shma [41]. Universal hashing achieves entropy loss O(log⁡(1/η))O(\log(1/\eta)), but standard hash families can require a seed linear in the input length [5, 26, 27]. Trevisan [48] connected extraction to pseudorandom generators and error-correcting codes. Lu, Reingold, Vadhan, and Wigderson [32] obtained parameters optimal up to constant factors for constant error. Guruswami, Umans, and Vadhan [22] gave a condenser-based construction with seed length O(log⁡(n/η))O(\log(n/\eta)) and output length at least (1−γ)k(1-\gamma)k for every fixed γ>0\gamma>0.

Further developments include hashing and block-source methods [10, 35 WZ99, 46, 24], error reduction and improving output length [38, 39], mergers and condensers [34, 40 TSUZ07, TSU06, 17 DKS13, TSU12, 31], and extraction in low-depth circuit classes [GWW15, CJL18, CWV24]. The surveys of Shaltiel [43] and Vadhan [Vad12] provide background on classical extractors and their connections to pseudorandomness.

For sampling, the relevant connection is particularly simple to describe: for a fixed source string xx, enumerate all seeds yy and use the outputs Ext⁡(x,y)\operatorname{Ext}(x,y) as the sample points. A uniformly chosen source string becomes the sampler’s random input, and a dd-bit extractor seed gives 2d2^d samples. Zuckerman’s correspondence [Zuc97] makes this relationship precise in both directions. Additional connections to list-decodable codes and entropy sampling appear in [TSZ04, NZ96, Vad04]. As matrix sampler is a natural extension of samplers, the classic extractor–sampler correspondence [Zuc97] suggests a structural question about matrix sampling:

What type of randomness extractor corresponds to a matrix sampler?

On the other hand, quantum side information changes the extraction problem. In randomness extraction, the extracted string must be nearly uniform even to an adversary who has partial information about the source [5, 4]. If this information is stored in a quantum system, security must hold against measurements of that system [37, 51]. Although the extractor itself is a classical function, classical security does not in general imply quantum security [19].

We describe the source XX and the adversary’s register EE by a classical–quantum (cq) state ρXE\rho_{XE}. There are two relevant models. The bounded-storage model places a lower bound on H∞(X)H_\infty(X) and an upper bound on dim⁡E\dim E. The more general conditional min-entropy model directly bounds the uncertainty remaining about XX given EE: Hmin⁡(X∣E)=−log⁡2pguess(X∣E)H_{\min}(X \mid E)=-\log_2 p_{\mathrm{guess}}(X \mid E), where pguess(X∣E)p_{\mathrm{guess}}(X \mid E) is the optimal probability of guessing XX by measuring EE [29]. We measure error in trace distance, Δ(ρ,σ)=12∥ρ−σ∥1\Delta(\rho,\sigma)=\frac{1}{2}\lVert\rho-\sigma\rVert_1, and write τj=2−jI2j\tau_j=2^{-j}I_{2^j} for the uniform state on jj bits.

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