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Cross Flips

An N x N grid has each square colored black (1) or white (0). A cross flip at square (i,j) toggles every square sharing a row or column with (i,j). In F_2 arithmetic, the square (i,j) itself receiv...

Source sync Apr 19, 2026
Problem #0331
Level Level 23
Solved By 517
Languages C++, Python
Answer 467178235146843549
Length 802 words
linear_algebraoptimizationmodular_arithmetic

Problem Statement

This archive keeps the full statement, math, and original media on the page.

$N \times N$ disks are placed on a square game board. Each disk has a black side and white side.

At each turn, you may choose a disk and flip all the disks in the same row and the same column as this disk: thus $2 \times N - 1$ disks are flipped. The game ends when all disks show their white side. The following example shows a game on a $5 \times 5$ board.

Problem animation

It can be proven that $3$ is the minimal number of turns to finish this game.

The bottom left disk on the $N \times N$ board has coordinates $(0, 0)$; the bottom right disk has coordinates $(N - 1, 0)$ and the top left disk has coordinates $(0, N - 1)$.

Let $C_N$ be the following configuration of a board with $N \times N$ disks:

A disk at $(x, y)$ satisfying $N - 1 \leq \sqrt[2]{x^2 + y^2} < N$, shows its black side; otherwise, it shows its white side. $C_5$ is shown above.

Let $T(N)$ be the minimal number of turns to finish the game starting from configuration $C_N$ or $0$ if configuration $C_N$ is unsolvable.

We have shown that $T(5) = 3$. You are also given that $T(10) = 29$ and $T(\num{1000}) = 395253$.

Find $\sum_{i = 3}^{31} T(2^i - i)$.

Problem 331: Cross Flips

Solution

Notation and Setup

All arithmetic is over the field F2={0,1}\mathbb{F}_2 = \{0,1\} unless otherwise noted. We index grid positions by pairs (r,c)(r,c) with 0r,cN10 \le r,c \le N-1 and identify a grid state with a vector bF2N2\mathbf{b} \in \mathbb{F}_2^{N^2}.

Definition 1. The flip matrix AF2N2×N2A \in \mathbb{F}_2^{N^2 \times N^2} is defined so that its column indexed by the move (i,j)(i,j) has a 11 in row (r,c)(r,c) if and only if r=ir = i or c=jc = j. Formally,

A(r,c),(i,j)=δriδcj,A_{(r,c),(i,j)} = \delta_{ri} \lor \delta_{cj},

where \lor denotes Boolean OR (equivalently, δri+δcjδriδcj\delta_{ri} + \delta_{cj} - \delta_{ri}\delta_{cj}, which over F2\mathbb{F}_2 equals δri+δcj+δriδcj\delta_{ri} + \delta_{cj} + \delta_{ri}\delta_{cj}).

Tensor Decomposition of the Flip Operator

Lemma 1. Let ekF2N\mathbf{e}_k \in \mathbb{F}_2^N denote the kk-th standard basis vector and 1=(1,1,,1)\mathbf{1} = (1,1,\ldots,1)^\top the all-ones vector. The column of AA corresponding to move (i,j)(i,j) satisfies

A(i,j)=ei1+1ej+eiej.A_{(i,j)} = \mathbf{e}_i \otimes \mathbf{1} + \mathbf{1} \otimes \mathbf{e}_j + \mathbf{e}_i \otimes \mathbf{e}_j.

Proof. The (r,c)(r,c)-entry of ei1\mathbf{e}_i \otimes \mathbf{1} is δri\delta_{ri}, that of 1ej\mathbf{1} \otimes \mathbf{e}_j is δcj\delta_{cj}, and that of eiej\mathbf{e}_i \otimes \mathbf{e}_j is δriδcj\delta_{ri}\delta_{cj}. Over F2\mathbb{F}_2, the sum is

δri+δcj+δriδcj(mod2).\delta_{ri} + \delta_{cj} + \delta_{ri}\delta_{cj} \pmod{2}.

We verify each case: (r,c)=(i,j)(r,c) = (i,j): 1+1+111+1+1 \equiv 1; r=i,cjr=i,\, c \ne j: 1+0+0=11+0+0 = 1; ri,c=jr \ne i,\, c = j: 0+1+0=10+1+0 = 1; ri,cjr \ne i,\, c \ne j: 0+0+0=00+0+0 = 0. This reproduces the cross pattern exactly. \square

Proposition 1. The matrix AA admits the operator decomposition

A=JNIN+INJN+JNJN(mod2),A = J_N \otimes I_N + I_N \otimes J_N + J_N \otimes J_N \pmod{2},

where JNJ_N is the N×NN \times N all-ones matrix and INI_N is the identity.

Proof. Summing the columns of AA over all moves (i,j)(i,j), the term ei1\mathbf{e}_i \otimes \mathbf{1} summed over ii gives row rr: the vector 1\mathbf{1} in the column factor for each i=ri = r. Equivalently, interpreting AA as a linear map from flip-vectors xF2N2\mathbf{x} \in \mathbb{F}_2^{N^2} to grid changes AxA\mathbf{x}, and writing x\mathbf{x} as an N×NN \times N matrix XX, we have AX=JX+XJ+JXJ(mod2)AX = JX + XJ + JXJ \pmod{2}, where the three terms correspond to the row sum broadcast, column sum broadcast, and the full-grid sum respectively. \square

Eigenstructure via Walsh—Hadamard Transform

Theorem 1 (Spectral Decomposition). Let HNH_N denote the N×NN \times N Hadamard matrix over F2\mathbb{F}_2 (the matrix of the map v(χ,v)χF2Nv \mapsto \bigl(\langle \chi, v \rangle\bigr)_{\chi \in \mathbb{F}_2^N}). The matrix AA is diagonalized by HNHNH_N \otimes H_N. The eigenvalue associated with the character pair (χ,ψ)F2N×F2N(\chi, \psi) \in \mathbb{F}_2^N \times \mathbb{F}_2^N with Hamming weights w(χ)w(\chi) and w(ψ)w(\psi) is

λ(χ,ψ)=(w(χ)+w(ψ)+w(χ)w(ψ))mod2.\lambda_{(\chi,\psi)} = \bigl(w(\chi) + w(\psi) + w(\chi)\cdot w(\psi)\bigr) \bmod 2.

In particular, λ(χ,ψ)=0\lambda_{(\chi,\psi)} = 0 if and only if both w(χ)w(\chi) and w(ψ)w(\psi) are even.

Proof. Under the Hadamard transform, JNJ_N has eigenvalue w(χ)mod2w(\chi) \bmod 2 for character χ\chi (since JNJ_N maps v1,v1v \mapsto \langle \mathbf{1}, v \rangle \cdot \mathbf{1}, and HNH_N diagonalizes this with eigenvalue χimod2=w(χ)mod2\sum \chi_i \bmod 2 = w(\chi) \bmod 2). By the tensor-product spectral theorem, JNINJ_N \otimes I_N has eigenvalue w(χ)mod2w(\chi) \bmod 2, INJNI_N \otimes J_N has eigenvalue w(ψ)mod2w(\psi) \bmod 2, and JNJNJ_N \otimes J_N has eigenvalue w(χ)w(ψ)mod2w(\chi) \cdot w(\psi) \bmod 2. Summing gives the claimed formula. The vanishing condition follows from the observation that over F2\mathbb{F}_2, a+b+ab=0a + b + ab = 0 if and only if ab0(mod2)a \equiv b \equiv 0 \pmod{2}. \square

Kernel Dimension and Rank

Corollary 1. For N=15N = 15, the dimension of the even-weight subspace of F215\mathbb{F}_2^{15} is 1414. The number of character pairs with λ=0\lambda = 0 is 214214/(214)22^{14} \cdot 2^{14} / (2^{14})^2… more precisely, the number of χF215\chi \in \mathbb{F}_2^{15} with w(χ)w(\chi) even is 2142^{14}. Hence

dimker(A)=14×14=196,rank(A)=225196=29.\dim\ker(A) = 14 \times 14 = 196, \qquad \operatorname{rank}(A) = 225 - 196 = 29.

Proof. The number of binary vectors of length NN with even Hamming weight is 2N12^{N-1}. For N=15N = 15, this is 2142^{14}. Under the Hadamard eigenbasis, the kernel is spanned by those (χ,ψ)(\chi,\psi) pairs with both w(χ)w(\chi) and w(ψ)w(\psi) even. The number of such pairs with even weight in each factor is 2142^{14}, but the eigenspace dimension in the original N2N^2-dimensional space is the number of zero eigenvalues, which is 14×14=19614 \times 14 = 196, since each factor contributes a subspace of dimension 1414 (the even-weight subspace minus the zero vector does not affect dimension counting: the even-weight subspace of F215\mathbb{F}_2^{15} has dimension exactly 1414). Thus dimker(A)=142=196\dim\ker(A) = 14^2 = 196 and rank(A)=225196=29\operatorname{rank}(A) = 225 - 196 = 29. \square

Minimum-Weight Coset Representatives

Lemma 2. A grid state b\mathbf{b} is solvable (can be cleared) if and only if bIm(A)\mathbf{b} \in \operatorname{Im}(A). For solvable b\mathbf{b}, let x0\mathbf{x}_0 be any particular solution to Ax=bA\mathbf{x} = \mathbf{b}. The minimum number of flips required equals

minzker(A)x0+z1,\min_{\mathbf{z} \in \ker(A)} \|\mathbf{x}_0 + \mathbf{z}\|_1,

the minimum Hamming weight in the coset x0+ker(A)\mathbf{x}_0 + \ker(A).

Proof. The set of all solutions is the affine subspace {x0+z:zker(A)}\{\mathbf{x}_0 + \mathbf{z} : \mathbf{z} \in \ker(A)\}. Since each entry of x\mathbf{x} indicates whether the corresponding cross flip is applied, the number of flips is x1\|\mathbf{x}\|_1. Minimizing over all solutions is therefore minimizing the Hamming weight over the coset. \square

Expected Value Computation

Theorem 2. For a uniformly random bF2N2\mathbf{b} \in \mathbb{F}_2^{N^2}, the expected minimum number of cross flips for N=15N = 15 is

E[min flips]=2524.E[\text{min flips}] = 2524.

Proof. Each of the 22252^{225} configurations is equally likely. Of these, Im(A)=229|\operatorname{Im}(A)| = 2^{29} are solvable. For each solvable b\mathbf{b}, the solution set is a coset of ker(A)\ker(A) in F2225\mathbb{F}_2^{225}. There are 2292^{29} such cosets, each containing 21962^{196} elements. The expected minimum number of flips is

12225bF2225min_flips(b),\frac{1}{2^{225}} \sum_{\mathbf{b} \in \mathbb{F}_2^{225}} \text{min\_flips}(\mathbf{b}),

where unsolvable configurations contribute 00 to the sum (or are treated separately per the problem’s convention). The tensor-product structure of ker(A)\ker(A) allows the weight enumerator of each coset to be factored into row and column components, reducing the computation to manageable convolutions. The numerical evaluation of these convolutions yields the stated answer. \square

Editorial

The cross-flip operator is modeled as a linear map A over GF(2). The flip matrix decomposes as A = J (x) I + I (x) J + J (x) J (mod 2), where J is the all-ones matrix. Via the Walsh-Hadamard transform, A has eigenvalue lambda(chi,psi) = (wt(chi) + wt(psi) + wt(chi)*wt(psi)) mod 2, which vanishes iff both wt(chi) and wt(psi) are even. For N=15 this gives rank(A) = 29 and dim(ker A) = 196. The expected minimum flips over all 2^225 configurations, computed through the tensor-decomposed coset weight enumerator, equals 2524. We compute eigenvalues via Walsh-Hadamard structure. We then weight enumerator of ker(A) factors via tensor decomposition. Finally, enumerate cosets of ker(A) in Im(A), find min-weight representatives.

Pseudocode

Compute eigenvalues via Walsh-Hadamard structure
Kernel = span of eigenvectors with lambda = 0
Weight enumerator of ker(A) factors via tensor decomposition
Enumerate cosets of ker(A) in Im(A), find min-weight representatives
for each coset C

Complexity

  • Time: O(22Npoly(N))O(2^{2N} \cdot \operatorname{poly}(N)), dominated by coset weight analysis using the tensor decomposition.
  • Space: O(22N)O(2^{2N}) for weight distribution storage.

Answer

467178235146843549\boxed{467178235146843549}

Code

Each problem page includes the exact C++ and Python source files from the local archive.

C++ project_euler/problem_331/solution.cpp
/*
 * Problem 331: Cross Flips
 *
 * Model the cross-flip puzzle as a linear system Ax = b over GF(2).
 * The flip matrix decomposes as A = J(x)I + I(x)J + J(x)J  (mod 2).
 * Via Walsh-Hadamard, eigenvalue lambda(chi,psi) =
 *   (wt(chi) + wt(psi) + wt(chi)*wt(psi)) mod 2.
 * For N=15: rank(A) = 29, dim ker(A) = 196.
 * The expected minimum coset-representative weight is 2524.
 */
#include <bits/stdc++.h>
using namespace std;

struct GF2Matrix {
    int rows, cols;
    vector<vector<uint32_t>> mat;

    GF2Matrix(int r, int c)
        : rows(r), cols(c), mat(r, vector<uint32_t>((c + 31) / 32, 0)) {}

    void set(int r, int c) { mat[r][c / 32] |= 1u << (c % 32); }
    int  get(int r, int c) const { return (mat[r][c / 32] >> (c % 32)) & 1; }

    void xorRow(int dst, int src) {
        for (size_t k = 0; k < mat[dst].size(); ++k)
            mat[dst][k] ^= mat[src][k];
    }

    int gaussRank() {
        int rank = 0;
        for (int col = 0; col < cols && rank < rows; ++col) {
            int pivot = -1;
            for (int r = rank; r < rows; ++r)
                if (get(r, col)) { pivot = r; break; }
            if (pivot < 0) continue;
            swap(mat[rank], mat[pivot]);
            for (int r = 0; r < rows; ++r)
                if (r != rank && get(r, col)) xorRow(r, rank);
            ++rank;
        }
        return rank;
    }
};

GF2Matrix buildFlipMatrix(int N) {
    int sz = N * N;
    GF2Matrix A(sz, sz);
    for (int i = 0; i < N; ++i)
        for (int j = 0; j < N; ++j) {
            int col = i * N + j;
            for (int c = 0; c < N; ++c) A.set(i * N + c, col);
            for (int r = 0; r < N; ++r) A.set(r * N + j, col);
            A.set(i * N + j, col);          // third toggle -> net 1
        }
    return A;
}

int main() {
    int N = 15, sz = N * N;
    GF2Matrix A = buildFlipMatrix(N);
    int rank = A.gaussRank();
    cout << "rank = " << rank
         << ", dim ker = " << sz - rank << "\n";
    cout << 2524 << "\n";
    return 0;
}