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arXiv:0909.3392

On the communication complexity of XOR functions

Ashley Montanaro, Tobias Osborne

Published Sep 18, 2009• 44 citations
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Abstract

An XOR function is a function of the form g(x,y) = f(x + y), for some boolean function f on n bits. We study the quantum and classical communication complexity of XOR functions. In the case of exact protocols, we completely characterise one-way communication complexity for all f. We also show that, when f is monotone, g's quantum and classical complexities are quadratically related, and that when f is a linear threshold function, g's quantum complexity is Theta(n). More generally, we make a structural conjecture about the Fourier spectra of boolean functions which, if true, would imply that the quantum and classical exact communication complexities of all XOR functions are asymptotically equivalent. We give two randomised classical protocols for general XOR functions which are efficient for certain functions, and a third protocol for linear threshold functions with high margin. These protocols operate in the symmetric message passing model with shared randomness.

DOI
10.48550/arxiv.0909.3392

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An XOR function is a function of the form g(x,y) = f(x + y), for some boolean function f on n bits. We study the quantum and classical communication complexity of XOR functions. In the case of exact protocols, we completely characterise one-way communication complexity for all f. We also show that, when f is monotone, g's quantum and classical complexities are quadratically related, and that when f is a linear threshold function, g's quantum complexity is Theta(n). More generally, we make a structural conjecture about the Fourier spectra of boolean functions which, if true, would imply that the quantum and classical exact communication complexities of all XOR functions are asymptotically equivalent. We give two randomised classical protocols for general XOR functions which are efficient for certain functions, and a third protocol for linear threshold functions with high margin. These protocols operate in the symmetric message passing model with shared randomness.
Boolean function F(x,y)F(x,y)F(x,y) for x,y∈{0,1}nx,y \in \{0,1\}^nx,y∈{0,1}n is an XOR function if F(x,y)=f(x⊕y)F(x,y)=f(x\oplus y)F(x,y)=f(x⊕y) for some function fff on nnn input bits, where ⊕\oplus⊕ is a bit-wise XOR. XOR functions are relevant in communication complexity, partially for allowing Fourier analytic technique. For total XOR functions it is known that deterministic communication complexity of FFF is closely related to parity decision tree complexity of fff. Montanaro and Osbourne (2009) observed that one-sided communication complexity Dcc→(F)D_{cc}^{\rightarrow}(F)Dcc→​(F) of FFF is exactly equal to nonadaptive parity decision tree complexity NADT⊕(f)NADT^{\oplus}(f)NADT⊕(f) of fff. Hatami et al. (2018) showed that unrestricted communication complexity of FFF is polynomially related to parity decision tree complexity of fff. We initiate the studies of a similar connection for partial functions. We show that in case of one-sided communication complexity whether these measures are equal, depends on the number of undefined inputs of fff. On the one hand, if Dcc→(F)=tD_{cc}^{\rightarrow}(F)=tDcc→​(F)=t and fff is undefined on at most O(2n−tn−t)O(\frac{2^{n-t}}{\sqrt{n-t}})O(n−t​2n−t​), then NADT⊕(f)=tNADT^{\oplus}(f)=tNADT⊕(f)=t. On the other hand, for a wide range of values of Dcc→(F)D_{cc}^{\rightarrow}(F)Dcc→​(F) and NADT⊕(f)NADT^{\oplus}(f)NADT⊕(f) (from constant to n−2n-2n−2) we provide partial functions for which Dcc→(F)<NADT⊕(f)D_{cc}^{\rightarrow}(F) < NADT^{\oplus}(f)Dcc→​(F)<NADT⊕(f). In particular, we provide a function with an exponential gap between the two measures. Our separation results translate to the case of two-sided communication complexity as well, in particular showing that the result of Hatami et al. (2018) cannot be generalized to partial functions. Previous results for total functions heavily rely on Boolean Fourier analysis and the technique does not translate to partial functions. For the proofs of our results we build a linear algebraic framework instead. Separation results are proved through the reduction to covering codes.
Boolean function F(x,y) for x,y ∈ {0,1}ⁿ is an XOR function if F(x,y) = f(x⊕ y) for some function f on n input bits, where ⊕ is a bit-wise XOR. XOR functions are relevant in communication complexity, partially for allowing the Fourier analytic technique. For total XOR functions, it is known that deterministic communication complexity of F is closely related to parity decision tree complexity of f. Montanaro and Osbourne (2009) observed that one-way communication complexity D_{cc}^{→}(F) of F is exactly equal to non-adaptive parity decision tree complexity NADT^{⊕}(f) of f. Hatami et al. (2018) showed that unrestricted communication complexity of F is polynomially related to parity decision tree complexity of f. We initiate the study of a similar connection for partial functions. We show that in the case of one-way communication complexity whether these measures are equal, depends on the number of undefined inputs of f. More precisely, if D_{cc}^{→}(F) = t and f is undefined on at most O((2^{n-t})/(√{n-t})) inputs, then NADT^{⊕}(f) = t. We also provide stronger bounds in extreme cases of small and large complexity. We show that the restriction on the number of undefined inputs in these results is unavoidable. That is, for a wide range of values of D_{cc}^{→}(F) and NADT^{⊕}(f) (from constant to n-2) we provide partial functions (with more than Ω((2^{n-t})/(√{n-t})) undefined inputs, where t = D_{cc}^{→}) for which D_{cc}^{→}(F) < NADT^{⊕}(f). In particular, we provide a function with an exponential gap between the two measures. Our separation results translate to the case of two-way communication complexity as well, in particular showing that the result of Hatami et al. (2018) cannot be generalized to partial functions. Previous results for total functions heavily rely on the Boolean Fourier analysis and thus, the technique does not translate to partial functions. For the proofs of our results we build a linear algebraic framework instead. Separation results are proved through the reduction to covering codes.
A major open problem in communication complexity is whether or not quantum protocols can be exponentially more efficient than classical ones for computing a {\em total} Boolean function in the two-party interactive model. Razborov's result ({\em Izvestiya: Mathematics}, 67(1):145--159, 2002) implies the conjectured negative answer for functions FFF of the following form: F(x,y)=fn(x1⋅y1,x2⋅y2,...,xn⋅yn)F(x, y)=f_n(x_1\cdot y_1, x_2\cdot y_2, ..., x_n\cdot y_n)F(x,y)=fn​(x1​⋅y1​,x2​⋅y2​,...,xn​⋅yn​), where fnf_nfn​ is a {\em symmetric} Boolean function on nnn Boolean inputs, and xix_ixi​, yiy_iyi​ are the iii'th bit of xxx and yyy, respectively. His proof critically depends on the symmetry of fnf_nfn​. We develop a lower-bound method that does not require symmetry and prove the conjecture for a broader class of functions. Each of those functions FFF is the ``block-composition'' of a ``building block'' gk:{0,1}k×{0,1}k→{0,1}g_k : \{0, 1\}^k \times \{0, 1\}^k \rightarrow \{0, 1\}gk​:{0,1}k×{0,1}k→{0,1}, and an fn:{0,1}n→{0,1}f_n : \{0, 1\}^n \rightarrow \{0, 1\}fn​:{0,1}n→{0,1}, such that F(x,y)=fn(gk(x1,y1),gk(x2,y2),...,gk(xn,yn))F(x, y) = f_n( g_k(x_1, y_1), g_k(x_2, y_2), ..., g_k(x_n, y_n) )F(x,y)=fn​(gk​(x1​,y1​),gk​(x2​,y2​),...,gk​(xn​,yn​)), where xix_ixi​ and yiy_iyi​ are the iii'th kkk-bit block of x,y∈{0,1}nkx, y\in\{0, 1\}^{nk}x,y∈{0,1}nk, respectively. We show that as long as g_k itself is "hard'' enough, its block-composition with an arbitrary f_n has polynomially related quantum and classical communication complexities. For example, when g_k is the Inner Product function with k=\Omega(\log n), the deterministic communication complexity of its block-composition with any f_n is asymptotically at most the quantum complexity to the power of 7.
A major open problem in quantum communication complexity is whether quantum protocols can be exponentially more efficient than classical protocols for computing total Boolean functions; the prevailing conjecture is that they cannot be so. In a seminal work, Razborov (2002) resolved this question for AND-functions of the form F(x,y)=f(x1∧y1,…,xn∧yn), F(x,y) = f(x_1 \land y_1, \ldots, x_n \land y_n), F(x,y)=f(x1​∧y1​,…,xn​∧yn​), when the outer function fff is symmetric, by proving that their bounded-error quantum and classical communication complexities are polynomially related. Since then, extending this result to all AND-functions has remained open and has been posed by several authors. In this work, we settle this problem in a strong way. We show that for every Boolean function fff, the bounded-error quantum and classical deterministic communication complexities of the function f∘AND2f \circ \mathrm{AND}_2f∘AND2​ are polynomially related, up to polylogarithmic factors in nnn. We prove this by showing that both are characterized--up to polynomial loss--by the logarithm of the De Morgan sparsity of fff. Our results build on the recent work of Chattopadhyay, Dahiya, and Lovett (2025) on structural characterizations of non-sparse Boolean functions, which we extend to resolve the conjecture for general AND-functions.
We show that for any Boolean function f : {0,1}n → {0,1}, the bounded-error quantum communication complexity Q∊(f ○ ⊕) of XOR functions f(x ⊕ y) satisfies that where d = deg2(f) is the ℱ2-degree of f, and ‖ ‖1,∊ = ming:‖f–g‖∞≤∊ ‖ĝ‖1. This implies that the previous lower bound Q∊(f ○ ⊕) = Ω(log ‖ ‖1,∊) by Lee and Shraibman [LS09] is tight for f with low 2-degree. The result also confirms the quantum version of the Log-rank Conjecture for low-degree XOR functions. In addition, we show that the exact quantum communication complexity satisfies where ‖ ‖0 is the number of nonzero Fourier coefficients of f. This matches the previous lower bound QE(f(x, y)) = Ω(logrank(Mf)) by Buhrman and de Wolf [BdW01] for low-degree XOR functions.
We study a model of communication complexity that encompasses many well-studied problems, including classical and quantum communication complexity, the complexity of simulating distributions arising from bipartite measurements of shared quantum states, and XOR games. In this model, Alice gets an input xxx, Bob gets an input yyy, and their goal is to each produce an output a,ba,ba,b distributed according to some pre-specified joint distribution p(a,b∣x,y)p(a,b|x,y)p(a,b∣x,y). Our results apply to any non-signaling distribution, that is, those where Alice's marginal distribution does not depend on Bob's input, and vice versa.~~~By taking a geometric view of the non-signaling distributions, we introduce a simple new technique based on affine combinations of lower-complexity distributions, and we give the first general technique to apply to all these settings, with elementary proofs and very intuitive interpretations. Specifically, we introduce two complexity measures, one which gives lower bounds on classical communication, and one for quantum communication. These measures can be expressed as convex optimization problems. We show that the dual formulations have a striking interpretation, since they coincide with maximum violations of Bell and Tsirelson inequalities. The dual expressions are closely related to the winning probability of XOR games. Despite their apparent simplicity, these lower bounds subsume many known communication complexity lower bound methods, most notably the recent lower bounds of Linial and Shraibman for the special case of Boolean functions. We show that as in the case of Boolean functions, the gap between the quantum and classical lower bounds is at most linear in the size of the support of the distribution, and does not depend on the size of the inputs. This translates into a bound on the gap between maximal Bell and Tsirelson inequality violations, which was previously known only for the case of distributions with Boolean outcomes and uniform marginals. It also allows us to show that for some distributions, information theoretic methods are necessary to prove strong lower bounds. ~~~ Finally, we give an exponential upper bound on quantum and classical communication complexity in the simultaneous messages model, for any non-signaling distribution. One consequence of this is a simple proof that any quantum distribution can be approximated with a constant number of bits of communication.