/
bls12_381_hash_to_G2.circom
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bls12_381_hash_to_G2.circom
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pragma circom 2.0.3;
include "bigint.circom";
include "bigint_func.circom";
include "fp.circom";
include "fp2.circom";
include "curve.circom";
include "curve_fp2.circom";
include "bls12_381_func.circom";
/*
implementation of optimized simplified SWU map to BLS12-381 G2
following Wahby-Boneh: Section 4.2 of https://eprint.iacr.org/2019/403.pdf
Python reference code: https://github.com/algorand/bls_sigs_ref/blob/master/python-impl/opt_swu_g2.py
Additional exposition: https://hackmd.io/@benjaminion/bls12-381#Simplified-SWU-map
E2 is y^2 = x^3 + 4(1+u) over Fp2
E2' is a curve of form y^2 = x^3 + a x + b that is 3-isogenous to E2
Constants are a = 240 u, b = 1012 + 1012 u where u = sqrt(-1)
*/
// Simplified SWU map, optimized and adapted to E2'
// in = t: 2 x k array, element of Fp2
// out: 2 x 2 x k array, point (out[0], out[1]) on curve E2'
//
// This is osswu2_help(t) in Python reference code
// See Section 4.2 of Wahby-Boneh: https://eprint.iacr.org/2019/403.pdf
// circom implementation is slightly different since sqrt and inversion are cheap
template OptSimpleSWU2(n, k){
signal input in[2][k];
signal output out[2][2][k];
//signal output isInfinity; optimized simple SWU should never return point at infinity, exceptional case still returns a normal point
var p[50] = get_BLS12_381_prime(n, k);
var a[2] = [0, 240];
var b[2] = [1012, 1012];
// distinguished non-square in Fp2 for SWU map: xi = -2 - u
// this is Z in the suite 8.8.2 of https://datatracker.ietf.org/doc/html/draft-irtf-cfrg-hash-to-curve-14#section-10
var xi[2] = [-2, -1];
var LOGK = log_ceil(k);
// in = t, compute t^2, t^3
component t_sq = SignedFp2MultiplyNoCarryCompress(n, k, p, n, 3*n + 2*LOGK + 1 );
for(var i=0; i<2; i++)for(var idx=0; idx<k; idx++){
t_sq.a[i][idx] <== in[i][idx];
t_sq.b[i][idx] <== in[i][idx];
}
// compute xi * t^2
component xi_t_sq = SignedFp2CarryModP(n, k, 3*n + 2*LOGK + 3, p);
for(var idx=0; idx<k; idx++){
xi_t_sq.in[0][idx] <== xi[0] * t_sq.out[0][idx] - xi[1] * t_sq.out[1][idx];
xi_t_sq.in[1][idx] <== xi[0] * t_sq.out[1][idx] + xi[1] * t_sq.out[0][idx];
}
// xi^2 * t^4
component xi2t4 = SignedFp2MultiplyNoCarryCompress(n, k, p, n, 3*n + 2*LOGK + 1);
for(var i=0; i<2; i++)for(var idx=0; idx<k; idx++){
xi2t4.a[i][idx] <== xi_t_sq.out[i][idx];
xi2t4.b[i][idx] <== xi_t_sq.out[i][idx];
}
// xi^2 * t^4 + xi * t^2
var num_den_common[2][k];
for(var i=0; i<2; i++)for(var idx=0; idx<k; idx++)
num_den_common[i][idx] = xi2t4.out[i][idx] + xi_t_sq.out[i][idx];
// X0(t) = b (xi^2 * t^4 + xi * t^2 + 1) / (-a * (xi^2 * t^4 + xi * t^2))
component X0_den = SignedFp2CarryModP(n, k, 3*n + 2*LOGK + 2 + 9, p);
for(var idx=0; idx<k; idx++){
X0_den.in[0][idx] <== -a[0] * num_den_common[0][idx] + a[1] * num_den_common[1][idx];
X0_den.in[1][idx] <== -a[0] * num_den_common[1][idx] - a[1] * num_den_common[0][idx];
}
// if X0_den = 0, replace with X1_den = a * xi; this way X1(t) = X0_num / X1_den = b / (xi * a)
// X1_den = a * xi = 240 - 480 i
assert( n == 55 && k == 7 );
var X1_den[2][k];
if( n == 55 && k == 7 ){
X1_den = [[240,0,0,0,0,0,0],
[35747322042230987,36025922209447795,1084959616957103,7925923977987733,16551456537884751,23443114579904617,1829881462546425]];
}
// Exception if X0_den = 0:
component exception = Fp2IsZero(n, k, p);
for(var i=0; i<2; i++)for(var idx=0; idx<k; idx++)
exception.in[i][idx] <== X0_den.out[i][idx];
//isInfinity <== exception.out;
num_den_common[0][0]++;
component X0_num = SignedFp2CarryModP(n, k, 3*n + 2*LOGK + 2 + 11, p);
for(var idx=0; idx<k; idx++){
X0_num.in[0][idx] <== b[0] * num_den_common[0][idx] - b[1] * num_den_common[1][idx];
X0_num.in[1][idx] <== b[0] * num_den_common[1][idx] + b[1] * num_den_common[0][idx];
}
// division is same cost/constraints as multiplication, so we will compute X0 and avoid using projective coordinates
component X0 = SignedFp2Divide(n, k, n, n, p);
for(var i=0; i<2; i++)for(var idx=0; idx<k; idx++){
X0.a[i][idx] <== X0_num.out[i][idx];
X0.b[i][idx] <== X0_den.out[i][idx] + exception.out * (X1_den[i][idx] - X0_den.out[i][idx]);
}
// g(x) = x^3 + a x + b
// Compute g(X0(t))
component gX0 = EllipticCurveFunction(n, k, a, b, p);
// X1(t) = xi * t^2 * X0(t)
component X1 = Fp2Multiply(n, k, p);
for(var i=0; i<2; i++)for(var idx=0; idx<k; idx++){
gX0.in[i][idx] <== X0.out[i][idx];
X1.a[i][idx] <== xi_t_sq.out[i][idx];
X1.b[i][idx] <== X0.out[i][idx];
}
component xi3t6 = Fp2MultiplyThree(n, k, p); // shares a hidden component with xi2t4; I'll let compiler optimize that out for readability
for(var i=0; i<2; i++)for(var idx=0; idx<k; idx++){
xi3t6.a[i][idx] <== xi_t_sq.out[i][idx];
xi3t6.b[i][idx] <== xi_t_sq.out[i][idx];
xi3t6.c[i][idx] <== xi_t_sq.out[i][idx];
}
// g(X1(t)) = xi^3 * t^6 * g(X0(t))
component gX1 = Fp2Multiply(n, k, p);
for(var i=0; i<2; i++)for(var idx=0; idx<k; idx++){
gX1.a[i][idx] <== xi3t6.out[i][idx];
gX1.b[i][idx] <== gX0.out[i][idx];
}
/*
xi^3 is not a square, so one of gX0, gX1 must be a square
isSquare = 1 if gX0 is a square, = 0 if gX1 is a square
sqrt = sqrt(gX0) if isSquare = 1, sqrt = sqrt(gX1) if isSquare = 0
Implementation is special to p^2 = 9 mod 16
References:
p. 9 of https://eprint.iacr.org/2019/403.pdf
F.2.1.1 for general version for any field: https://datatracker.ietf.org/doc/html/draft-irtf-cfrg-hash-to-curve-14#appendix-F.2.1.1
I do not use the trick for combining division and sqrt from Section 5 of
Bernstein, Duif, Lange, Schwabe, and Yang, "High-speed high-security signatures",
since division is cheap in circom
*/
signal isSquare;
// Precompute sqrt_candidate = gX0^{(p^2 + 7) / 16}
// p^2 + 7
var c1[50] = long_add_unequal(n, 2*k, 1, prod(n, k, p, p), [7]);
// (p^2 + 7) // 16
var c2[2][50] = long_div2(n, 1, 2*k-1, c1, [16]);
assert( c2[1][0] == 0 ); // assert p^2 + 7 is divisible by 16
var sqrt_candidate[2][50] = find_Fp2_exp(n, k, gX0.out, p, c2[0]);
// if gX0 is a square, square root must be sqrt_candidate * (8th-root of unity)
// -1 is a square in Fp2 (because p^2 - 1 is even) so we only need to check half of the 8th roots of unity
var roots[4][2][50] = get_roots_of_unity(n, k);
var sqrt_witness[2][2][50];
for(var i=0; i<2; i++)for(var j=0; j<2; j++)for(var idx=0; idx<k; idx++)
sqrt_witness[i][j][idx] = 0;
var is_square = 0;
for(var i=0; i<4; i++){
var sqrt_tmp[2][50] = find_Fp2_product(n, k, sqrt_candidate, roots[i], p);
if(is_equal_Fp2(n, k, find_Fp2_product(n, k, sqrt_tmp, sqrt_tmp, p), gX0.out) == 1){
is_square = 1;
sqrt_witness[0] = sqrt_tmp;
}
}
isSquare <-- is_square;
isSquare * (1-isSquare) === 0;
var is_square1 = 0;
var etas[4][2][50] = get_etas(n, k);
// find square root of gX1
// square root of gX1 must be = sqrt_candidate * t^3 * eta
// for one of four precomputed values of eta
// eta determined by eta^2 = xi^3 * (-1)^{-1/4}
var t_cu[2][50] = find_Fp2_product(n, k, find_Fp2_product(n, k, in, in, p), in, p);
sqrt_candidate = find_Fp2_product(n, k, sqrt_candidate, t_cu, p);
for(var i=0; i<4; i++){
var sqrt_tmp[2][50] = find_Fp2_product(n, k, sqrt_candidate, etas[i], p);
if(is_equal_Fp2(n, k, find_Fp2_product(n, k, sqrt_tmp, sqrt_tmp, p), gX1.out) == 1){
is_square1 = 1;
sqrt_witness[1] = sqrt_tmp;
}
}
assert(is_square == 1 || is_square1 == 1); // one of gX0 or gX1 must be a square!
// X = out[0] = X0 if isSquare == 1, else X = X1
for(var i=0; i<2; i++)for(var idx=0; idx<k; idx++)
out[0][i][idx] <== isSquare * (X0.out[i][idx] - X1.out[i][idx]) + X1.out[i][idx];
// sgn0(t)
component sgn_in = Fp2Sgn0(n, k, p);
for(var i=0; i<2; i++)for(var idx=0; idx<k; idx++)
sgn_in.in[i][idx] <== in[i][idx];
var Y[2][50];
for(var i=0; i<2; i++)for(var idx=0; idx<k; idx++)
Y[i][idx] = is_square * sqrt_witness[0][i][idx] + (1-is_square) * sqrt_witness[1][i][idx];
// Y = out[1] = +- sqrt_witness; sign determined by sgn0(Y) = sgn0(t)
if(get_fp2_sgn0(k, Y) != sgn_in.out){
Y[0] = long_sub(n, k, p, Y[0]);
Y[1] = long_sub(n, k, p, Y[1]);
}
component Y_sq = Fp2Multiply(n, k, p);
// Y^2 == g(X)
for(var i=0; i<2; i++)for(var idx=0; idx<k; idx++){
out[1][i][idx] <-- Y[i][idx];
Y_sq.a[i][idx] <== out[1][i][idx];
Y_sq.b[i][idx] <== out[1][i][idx];
}
for(var i=0; i<2; i++)for(var idx=0; idx<k; idx++){
Y_sq.out[i][idx] === isSquare * (gX0.out[i][idx] - gX1.out[i][idx]) + gX1.out[i][idx];
}
// sgn0(Y) == sgn0(t)
component sgn_Y = Fp2Sgn0(n, k, p);
for(var i=0; i<2; i++)for(var idx=0; idx<k; idx++)
sgn_Y.in[i][idx] <== out[1][i][idx];
sgn_Y.out === sgn_in.out;
}
/*
3-Isogeny from E2' to E2
References:
Appendix E.3 of https://datatracker.ietf.org/doc/html/draft-irtf-cfrg-hash-to-curve-14#appendix-E.3
Section 4.3 of Wahby-Boneh: https://eprint.iacr.org/2019/403.pdf
iso3(P) in Python reference code: https://github.com/algorand/bls_sigs_ref/blob/master/python-impl/opt_swu_g2.py
*/
// Input:
// in = (x', y') point on E2' assumed to not be point at infinity
// inIsInfinity = 1 if input is point at infinity on E2' (in which case x', y' are arbitrary)
// Output:
// out = (x, y) is point on E2 after applying 3-isogeny to in
// isInfinity = 1 if one of exceptional cases occurs and output should be point at infinity
// Exceptions:
// inIsInfinity = 1
// input is a pole of the isogeny, i.e., x_den or y_den = 0
template Iso3Map(n, k){
signal input in[2][2][k];
//signal input inIsInfinity;
signal output out[2][2][k];
signal output isInfinity;
var p[50] = get_BLS12_381_prime(n, k);
// load coefficients of the isogeny (precomputed)
var coeffs[4][4][2][50] = get_iso3_coeffs(n, k);
// x = x_num / x_den
// y = y' * y_num / y_den
// x_num = sum_{i=0}^3 coeffs[0][i] * x'^i
// x_den = x'^2 + coeffs[1][1] * x' + coeffs[1][0]
// y_num = sum_{i=0}^3 coeffs[2][i] * x'^i
// y_den = x'^3 + sum_{i=0}^2 coeffs[3][i] * x'^i
var LOGK = log_ceil(k);
component xp2_nocarry = SignedFp2MultiplyNoCarry(n, k, 2*n + LOGK + 1);
component xp2 = SignedFp2CompressCarry(n, k, k-1, 2*n+LOGK+1, p);
component xp3_nocarry = SignedFp2MultiplyNoCarryUnequal(n, 2*k-1, k, 3*n + 2*LOGK + 2);
component xp3 = SignedFp2CompressCarry(n, k, 2*k-2, 3*n+2*LOGK+2, p);
for(var i=0; i<2; i++)for(var idx=0; idx<k; idx++){
xp2_nocarry.a[i][idx] <== in[0][i][idx];
xp2_nocarry.b[i][idx] <== in[0][i][idx];
xp3_nocarry.b[i][idx] <== in[0][i][idx];
}
for(var i=0; i<2; i++)for(var idx=0; idx<2*k-1; idx++){
xp3_nocarry.a[i][idx] <== xp2_nocarry.out[i][idx];
xp2.in[i][idx] <== xp2_nocarry.out[i][idx];
}
for(var i=0; i<2; i++)for(var idx=0; idx<3*k-2; idx++)
xp3.in[i][idx] <== xp3_nocarry.out[i][idx];
signal xp_pow[3][2][k];
for(var i=0; i<2; i++)for(var idx=0; idx<k; idx++){
xp_pow[0][i][idx] <== in[0][i][idx];
xp_pow[1][i][idx] <== xp2.out[i][idx];
xp_pow[2][i][idx] <== xp3.out[i][idx];
}
component coeffs_xp[4][3];
var deg[4] = [3, 1, 3, 2];
for(var i=0; i<4; i++)for(var j=0; j<deg[i]; j++){
coeffs_xp[i][j] = SignedFp2MultiplyNoCarry(n, k, 2*n + LOGK + 1);
for(var l=0; l<2; l++)for(var idx=0; idx<k; idx++){
coeffs_xp[i][j].a[l][idx] <== coeffs[i][j+1][l][idx];
coeffs_xp[i][j].b[l][idx] <== xp_pow[j][l][idx];
}
}
var x_frac[4][2][50];
for(var i=0; i<4; i++){
for(var l=0; l<2; l++)for(var idx=0; idx<2*k-1; idx++){
if(idx<k)
x_frac[i][l][idx] = coeffs[i][0][l][idx];
else
x_frac[i][l][idx] = 0;
}
for(var j=0; j<deg[i]; j++)for(var l=0; l<2; l++)for(var idx=0; idx<2*k-1; idx++)
x_frac[i][l][idx] += coeffs_xp[i][j].out[l][idx];
}
for(var l=0; l<2; l++)for(var idx=0; idx<k; idx++){
x_frac[1][l][idx] += xp2.out[l][idx];
x_frac[3][l][idx] += xp3.out[l][idx];
}
// carry the denominators since we need to check whether they are 0
component den[2];
component den_is_zero[2];
for(var i=0; i<2; i++){
den[i] = SignedFp2CompressCarry(n, k, k-1, 2*n + LOGK + 3, p);
for(var l=0; l<2; l++)for(var idx=0; idx<2*k-1; idx++)
den[i].in[l][idx] <== x_frac[2*i+1][l][idx];
den_is_zero[i] = Fp2IsZero(n, k, p);
for(var l=0; l<2; l++)for(var idx=0; idx<k; idx++)
den_is_zero[i].in[l][idx] <== den[i].out[l][idx];
}
//component exception = IsZero();
//exception.in <== inIsInfinity + den_is_zero[0].out + den_is_zero[1].out;
isInfinity <== den_is_zero[0].out + den_is_zero[1].out - den_is_zero[0].out * den_is_zero[1].out; // OR gate: if either denominator is 0, output point at infinity
component num[2];
for(var i=0; i<2; i++){
num[i] = Fp2Compress(n, k, k-1, p, 3*n + 2*LOGK + 3);
for(var l=0; l<2; l++)for(var idx=0; idx<2*k-1; idx++)
num[i].in[l][idx] <== x_frac[2*i][l][idx];
}
component x[2];
// num / den if den != 0, else num / 1
for(var i=0; i<2; i++){
x[i] = SignedFp2Divide(n, k, 3*n + 2*LOGK + 3, n, p);
for(var l=0; l<2; l++)for(var idx=0; idx<k; idx++){
x[i].a[l][idx] <== num[i].out[l][idx];
if(l==0 && idx==0)
x[i].b[l][idx] <== isInfinity * (1 - den[i].out[l][idx]) + den[i].out[l][idx];
else
x[i].b[l][idx] <== -isInfinity * den[i].out[l][idx] + den[i].out[l][idx];
}
}
component y = Fp2Multiply(n, k, p);
for(var i=0; i<2; i++)for(var idx=0; idx<k; idx++){
y.a[i][idx] <== in[1][i][idx];
y.b[i][idx] <== x[1].out[i][idx];
}
for(var i=0; i<2; i++)for(var idx=0; idx<k; idx++){
out[0][i][idx] <== x[0].out[i][idx];
out[1][i][idx] <== y.out[i][idx];
}
}
/*
Cofactor Clearing for BLS12-381 G2
Implementation below follows Appendix G.3 of https://datatracker.ietf.org/doc/html/draft-irtf-cfrg-hash-to-curve-14#appendix-G.3
References:
The endomorphism psi of Budroni-Pintore: https://eprint.iacr.org/2017/419.pdf
BLS For the Rest of Us: https://hackmd.io/@benjaminion/bls12-381#Cofactor-clearing
*/
// Input: in, a point on the curve E2 : y^2 = x^3 + 4(1+u)
// coordinates of in are in "proper" representation
// Output: out = psi(in), a point on the same curve.
template EndomorphismPsi(n, k, p){
signal input in[2][2][k];
signal output out[2][2][k];
var c[2][2][k];
// Constants:
// c0 = 1 / (1 + I)^((p - 1) / 3) # in GF(p^2)
// c1 = 1 / (1 + I)^((p - 1) / 2) # in GF(p^2)
assert( n == 55 && k == 7 );
if( n == 55 && k == 7 ){
c = [[[0, 0, 0, 0, 0, 0, 0],
[35184372088875693,
22472499736345367,
5698637743850064,
21300661132716363,
21929049149954008,
23430044241153146,
1829881462546425]],
[[31097504852074146,
21847832108733923,
11215546103677201,
1564033941097252,
9796175148277139,
23041766052141807,
1359550313685033],
[4649817190157321,
14178090100713872,
25898210532243870,
6361890036890480,
6755281389607612,
401348527762810,
470331148861392]]];
}
component frob[2];
component qx[2];
for(var i=0; i<2; i++){
frob[i] = Fp2FrobeniusMap(n, k, 1, p);
for(var j=0; j<2; j++)for(var idx=0; idx<k; idx++)
frob[i].in[j][idx] <== in[i][j][idx];
qx[i] = Fp2Multiply(n, k, p);
for(var j=0; j<2; j++)for(var idx=0; idx<k; idx++){
qx[i].a[j][idx] <== c[i][j][idx];
qx[i].b[j][idx] <== frob[i].out[j][idx];
}
}
for(var j=0; j<2; j++)for(var idx=0; idx<k; idx++){
out[0][j][idx] <== qx[0].out[j][idx];
out[1][j][idx] <== qx[1].out[j][idx];
}
}
// Input: in, a point on the curve E2 : y^2 = x^3 + 4(1+u)
// coordinates of in are in "proper" representation
// Output: out = psi(psi(in)), a point on the same curve.
template EndomorphismPsi2(n, k, p){
signal input in[2][2][k];
signal output out[2][2][k];
var c[k];
// Third root of unity:
// c = 1 / 2^((p - 1) / 3) # in GF(p)
assert( n == 55 && k == 7 );
if( n == 55 && k == 7 ){
c = [35184372088875692,
22472499736345367,
5698637743850064,
21300661132716363,
21929049149954008,
23430044241153146,
1829881462546425];
}
component qx[2];
component qy[2];
for(var i=0; i<2; i++){
qx[i] = FpMultiply(n, k, p);
for(var idx=0; idx<k; idx++){
qx[i].a[idx] <== c[idx];
qx[i].b[idx] <== in[0][i][idx];
}
qy[i] = BigSub(n, k);
for(var idx=0; idx<k; idx++){
qy[i].a[idx] <== p[idx];
qy[i].b[idx] <== in[1][i][idx];
}
}
for(var i=0; i<2; i++)for(var idx=0; idx<k; idx++){
out[0][i][idx] <== qx[i].out[idx];
out[1][i][idx] <== qy[i].out[idx];
}
}
// in = P, a point on curve E2
// out = [x^2 - x - 1]P + [x-1]*psi(P) + psi2(2*P)
// where x = -15132376222941642752 is the parameter for BLS12-381
template ClearCofactorG2(n, k){
signal input in[2][2][k];
signal input inIsInfinity;
signal output out[2][2][k];
signal output isInfinity;
var p[50] = get_BLS12_381_prime(n, k);
var x_abs = get_BLS12_381_parameter(); // this is abs(x). remember x is negative!
var a[2] = [0,0];
var b[2] = [4,4];
var dummy_point[2][2][50] = get_generator_G2(n, k);
// Output: [|x|^2 + |x| - 1]*P + [-|x|-1]*psi(P) + psi2(2*P)
// = |x| * (|x|*P + P - psi(P)) - P -psi(P) + psi2(2*P)
// replace `in` with dummy_point if inIsInfinity = 1 to ensure P is on the curve
signal P[2][2][k];
component xP = EllipticCurveScalarMultiplyFp2(n, k, b, x_abs, p);
component psiP = EndomorphismPsi(n, k, p);
component neg_Py = Fp2Negate(n, k, p);
component neg_psiPy = Fp2Negate(n, k, p);
component doubP = EllipticCurveDoubleFp2(n, k, a, b, p);
xP.inIsInfinity <== inIsInfinity;
for(var i=0; i<2; i++)for(var j=0; j<2; j++)for(var idx=0; idx<k; idx++){
P[i][j][idx] <== in[i][j][idx] + inIsInfinity * (dummy_point[i][j][idx] - in[i][j][idx]);
xP.in[i][j][idx] <== P[i][j][idx];
psiP.in[i][j][idx] <== P[i][j][idx];
doubP.in[i][j][idx] <== P[i][j][idx];
}
for(var j=0; j<2; j++)for(var idx=0; idx<k; idx++){
neg_Py.in[j][idx] <== P[1][j][idx];
neg_psiPy.in[j][idx] <== psiP.out[1][j][idx];
}
component psi22P = EndomorphismPsi2(n, k, p);
component add[5];
for(var i=0; i<5; i++)
add[i] = EllipticCurveAddFp2(n, k, a, b, p);
for(var i=0; i<2; i++)for(var j=0; j<2; j++)for(var idx=0; idx<k; idx++){
psi22P.in[i][j][idx] <== doubP.out[i][j][idx];
add[0].a[i][j][idx] <== xP.out[i][j][idx];
add[0].b[i][j][idx] <== P[i][j][idx];
}
add[0].aIsInfinity <== xP.isInfinity;
add[0].bIsInfinity <== inIsInfinity;
for(var i=0; i<2; i++)for(var j=0; j<2; j++)for(var idx=0; idx<k; idx++){
add[1].a[i][j][idx] <== add[0].out[i][j][idx];
if(i==0)
add[1].b[i][j][idx] <== psiP.out[i][j][idx];
else
add[1].b[i][j][idx] <== neg_psiPy.out[j][idx];
}
add[1].aIsInfinity <== add[0].isInfinity;
add[1].bIsInfinity <== inIsInfinity;
component xadd1 = EllipticCurveScalarMultiplyFp2(n, k, b, x_abs, p);
for(var i=0; i<2; i++)for(var j=0; j<2; j++)for(var idx=0; idx<k; idx++)
xadd1.in[i][j][idx] <== add[1].out[i][j][idx];
xadd1.inIsInfinity <== add[1].isInfinity;
for(var i=0; i<2; i++)for(var j=0; j<2; j++)for(var idx=0; idx<k; idx++){
add[2].a[i][j][idx] <== xadd1.out[i][j][idx];
if(i==0)
add[2].b[i][j][idx] <== P[i][j][idx];
else
add[2].b[i][j][idx] <== neg_Py.out[j][idx];
}
add[2].aIsInfinity <== xadd1.isInfinity;
add[2].bIsInfinity <== inIsInfinity;
for(var i=0; i<2; i++)for(var j=0; j<2; j++)for(var idx=0; idx<k; idx++){
add[3].a[i][j][idx] <== add[2].out[i][j][idx];
if(i==0)
add[3].b[i][j][idx] <== psiP.out[i][j][idx];
else
add[3].b[i][j][idx] <== neg_psiPy.out[j][idx];
}
add[3].aIsInfinity <== add[2].isInfinity;
add[3].bIsInfinity <== inIsInfinity;
for(var i=0; i<2; i++)for(var j=0; j<2; j++)for(var idx=0; idx<k; idx++){
add[4].a[i][j][idx] <== add[3].out[i][j][idx];
add[4].b[i][j][idx] <== psi22P.out[i][j][idx];
}
add[4].aIsInfinity <== add[3].isInfinity;
add[4].bIsInfinity <== inIsInfinity;
// isInfinity = add[4].isInfinity or inIsInfinity (if starting point was O, output must be O)
isInfinity <== add[4].isInfinity + inIsInfinity - inIsInfinity * add[4].isInfinity;
for(var i=0; i<2; i++)for(var j=0; j<2; j++)for(var idx=0; idx<k; idx++)
out[i][j][idx] <== add[4].out[i][j][idx] + isInfinity * (dummy_point[i][j][idx] - add[4].out[i][j][idx]);
}
// `in` is 2 x 2 x k representing two field elements in Fp2
// `out` is 2 x 2 x k representing a point in subgroup G2 of E2(Fp2) twisted curve for BLS12-381
// isInfinity = 1 if `out` is point at infinity
// Implements steps 2-6 of hash_to_curve as specified in https://datatracker.ietf.org/doc/html/draft-irtf-cfrg-hash-to-curve-14#section-3
// In practice `in` = hash_to_field(msg, 2) for an arbitrary-length byte string, in which case `out` = hash_to_curve(msg)
template MapToG2(n, k){
signal input in[2][2][k];
signal output out[2][2][k];
signal output isInfinity;
var p[50] = get_BLS12_381_prime(n, k);
component Qp[2];
for(var i=0; i<2; i++){
Qp[i] = OptSimpleSWU2(n, k);
for(var j=0; j<2; j++)for(var idx=0; idx<k; idx++)
Qp[i].in[j][idx] <== in[i][j][idx];
}
// There is a small optimization we can do: Iso3Map is a group homomorphism, so we can add first and then apply isogeny. This uses EllipticCurveAdd on E2'
component Rp = EllipticCurveAddFp2(n, k, [0, 240], [1012, 1012], p);
for(var i=0; i<2; i++)for(var j=0; j<2; j++)for(var idx=0; idx<k; idx++){
Rp.a[i][j][idx] <== Qp[0].out[i][j][idx];
Rp.b[i][j][idx] <== Qp[1].out[i][j][idx];
}
Rp.aIsInfinity <== 0;
Rp.bIsInfinity <== 0;
component R = Iso3Map(n, k);
for(var i=0; i<2; i++)for(var j=0; j<2; j++)for(var idx=0; idx<k; idx++)
R.in[i][j][idx] <== Rp.out[i][j][idx];
component P = ClearCofactorG2(n, k);
for(var i=0; i<2; i++)for(var j=0; j<2; j++)for(var idx=0; idx<k; idx++)
P.in[i][j][idx] <== R.out[i][j][idx];
P.inIsInfinity <== R.isInfinity + Rp.isInfinity - R.isInfinity * Rp.isInfinity;
isInfinity <== P.isInfinity;
for(var i=0; i<2; i++)for(var j=0; j<2; j++)for(var idx=0; idx<k; idx++)
out[i][j][idx] <== P.out[i][j][idx];
}
/*
Subgroup checks for G1, G2:
use the latest methods by Scott: https://eprint.iacr.org/2021/1130.pdf
Other references:
Bowe: https://eprint.iacr.org/2019/814.pdf
El Housni: https://hackmd.io/@yelhousni/bls12_subgroup_check
*/
// `in` = P is 2 x 2 x k, pair of Fp2 elements
// check P is on curve twist E2(Fp2)
// check psi(P) = [x]P where x is parameter for BLS12-381
template SubgroupCheckG2(n, k){
signal input in[2][2][k];
var p[50] = get_BLS12_381_prime(n, k);
var x_abs = get_BLS12_381_parameter();
component is_on_curve = PointOnCurveFp2(n, k, [0,0], [4,4], p);
for(var i=0; i<2; i++)for(var j=0; j<2; j++)for(var idx=0; idx<k; idx++)
is_on_curve.in[i][j][idx] <== in[i][j][idx];
component psiP = EndomorphismPsi(n, k, p);
component negP = Fp2Negate(n, k, p);
component xP = EllipticCurveScalarMultiplyUnequalFp2(n, k, [4, 4], x_abs, p);
for(var j=0; j<2; j++)for(var idx=0; idx<k; idx++)
negP.in[j][idx] <== in[1][j][idx];
for(var j=0; j<2; j++)for(var idx=0; idx<k; idx++){
psiP.in[0][j][idx] <== in[0][j][idx];
psiP.in[1][j][idx] <== in[1][j][idx];
xP.in[0][j][idx] <== in[0][j][idx];
xP.in[1][j][idx] <== negP.out[j][idx];
}
// psi(P) == [x]P
component is_eq[2];
for(var i=0; i<2; i++){
is_eq[i] = Fp2IsEqual(n, k, p);
for(var j=0; j<2; j++)for(var idx=0; idx<k; idx++){
is_eq[i].a[j][idx] <== psiP.out[i][j][idx];
is_eq[i].b[j][idx] <== xP.out[i][j][idx];
}
}
is_eq[0].out === 1;
is_eq[1].out === 1;
}
// `in` = P is 2 x k, pair of Fp elements
// check P is on curve E(Fp)
// check phi(P) == [-x^2] P where phi(x,y) = (omega * x, y) where omega is a cube root of unity in Fp
template SubgroupCheckG1(n, k){
signal input in[2][k];
var p[50] = get_BLS12_381_prime(n, k);
var x_abs = get_BLS12_381_parameter();
var b = 4;
component is_on_curve = PointOnCurve(n, k, 0, b, p);
for(var i=0; i<2; i++)for(var idx=0; idx<k; idx++)
is_on_curve.in[i][idx] <== in[i][idx];
var omega[k];
// Third root of unity:
// omega = 2^((p - 1) / 3) # in GF(p)
assert( n == 55 && k == 7 );
if( n == 55 && k == 7 ){
omega = [562949953355774,
13553422473102428,
31415118892071007,
22654059864235337,
30651204406894710,
13070338751470,
0];
}
component phiPx = FpMultiply(n, k, p);
for(var idx=0; idx<k; idx++){
phiPx.a[idx] <== omega[idx];
phiPx.b[idx] <== in[0][idx];
}
component phiPy_neg = BigSub(n, k);
for(var idx=0; idx<k; idx++){
phiPy_neg.a[idx] <== p[idx];
phiPy_neg.b[idx] <== in[1][idx];
}
// x has hamming weight 6 while x^2 has hamming weight 17 so better to do double-and-add on x twice
component xP = EllipticCurveScalarMultiplyUnequal(n, k, b, x_abs, p);
component x2P = EllipticCurveScalarMultiplyUnequal(n, k, b, x_abs, p);
for(var i=0; i<2; i++)for(var idx=0; idx<k; idx++)
xP.in[i][idx] <== in[i][idx];
for(var i=0; i<2; i++)for(var idx=0; idx<k; idx++)
x2P.in[i][idx] <== xP.out[i][idx];
// check -phi(P) == [x^2]P
component is_eq = Fp2IsEqual(n, k, p); // using Fp2IsEqual to check two Fp points are equal
for(var idx=0; idx<k; idx++){
is_eq.a[0][idx] <== phiPx.out[idx];
is_eq.a[1][idx] <== phiPy_neg.out[idx];
is_eq.b[0][idx] <== x2P.out[0][idx];
is_eq.b[1][idx] <== x2P.out[1][idx];
}
is_eq.out === 1;
}
template SubgroupCheckG1WithValidX(n, k){
signal input in[2][k];
var p[50] = get_BLS12_381_prime(n, k);
var x_abs = get_BLS12_381_parameter();
var b = 4;
component is_on_curve = PointOnCurve(n, k, 0, b, p);
for(var i=0; i<2; i++)for(var idx=0; idx<k; idx++)
is_on_curve.in[i][idx] <== in[i][idx];
}