deg2(Af)โคdeg2(f)-1. When we use {+1,-1}as the range,then the derivative changes to Ag(x)=g(x)g(x+t). 3.Quantum Fourier transform For a function f:{0,1)n{+1,-1),one can define an n-qubit quantum state If one applies Hadamard gates,one on each qubit,then the state becomes Verify this๏ผ 4.XOR functions XOR functions are the class of functions F(x,y)=f(x+y)for some n-bit function f.We sometimes denote such function F by f The class contains interesting functions such as Equality and Hamming Distance.It also has an intimate connection to Fourier analysis because the rank of the communication matrix Me is nothing but the Fourier sparsity of f,i.e.the number of nonzero Fourier coefficients. Exercise.rank(M)= A lower bound for the quantum communication complexity for XOR functions is the following.First, let's define a variant of the Fourier 1-norm. lfl1e=minllgll1:lf(x)-g(xlโคe,xโ{0,1 Theorem([LS09)).Qe(f)=(logllflle). It was considered to be pretty tight,but it has lacked rigorous argument.Recently,the following bound was shown,which implies that the above lower bound is tight for low degree polynomials. Theorem([Z14])Qe(f)=o(2dlogllflle)where d=deg2(f)deg2 (ฮ๐ก๐) โค deg2 (๐) โ 1. When we use {+1,โ1} as the range, then the derivative changes to ๐ฅ๐ก๐(๐ฅ) = ๐(๐ฅ)๐(๐ฅ + ๐ก). 3. Quantum Fourier transform For a function ๐:{0,1} ๐ โ {+1,โ1}, one can define an n-qubit quantum state 1 โ๐ โ๐(๐ฅ)|๐ฅโช ๐ฅ If one applies Hadamard gates, one on each qubit, then the state becomes 1 โ๐ โ๐ฬ(๐ผ)|๐ผโช ๐ผ Verify this! 4. XOR functions XOR functions are the class of functions ๐น(๐ฅ,๐ฆ) = ๐(๐ฅ + ๐ฆ) for some ๐-bit function ๐. We sometimes denote such function ๐น by ๐ โโ The class contains interesting functions such as Equality and Hamming Distance. It also has an intimate connection to Fourier analysis because the rank of the communication matrix ๐๐น is nothing but the Fourier sparsity of ๐, i.e. the number of nonzero Fourier coefficients. Exercise. rank(๐๐โโ) = โ๐ฬโ 0 . A lower bound for the quantum communication complexity for XOR functions is the following. First, letโs define a variant of the Fourier 1-norm. โ๐โ1,๐ = min{โ๐โ1 :|๐(๐ฅ) โ ๐(๐ฅ)| โค ๐, โ๐ฅ โ {0,1} ๐} Theorem ([LS09]). ๐๐ (๐ โโ) = ฮฉ(logโ๐โ1,๐ ). It was considered to be pretty tight, but it has lacked rigorous argument. Recently, the following bound was shown, which implies that the above lower bound is tight for low degree polynomials. Theorem ([Z14]) ๐๐ (๐ โโ) = ๐(2 ๐ logโ๐โ1,๐ ) where ๐ = deg2(๐)