bsc/crypto/bn256/cloudflare/gfp6.go
Antoine Rondelet 2388e425f2 crypto/bn256/cloudflare: fix comments to describe the updated curve parameters (#19577)
* Removed comment section referring to Cloudflare's bn curve parameters

* Added comment to clarify the nature of the parameters

* Changed value of xi to i+9
2019-05-28 09:13:30 +03:00

214 lines
4.5 KiB
Go

package bn256
// For details of the algorithms used, see "Multiplication and Squaring on
// Pairing-Friendly Fields, Devegili et al.
// http://eprint.iacr.org/2006/471.pdf.
// gfP6 implements the field of size p⁶ as a cubic extension of gfP2 where τ³=ξ
// and ξ=i+9.
type gfP6 struct {
x, y, z gfP2 // value is xτ² + yτ + z
}
func (e *gfP6) String() string {
return "(" + e.x.String() + ", " + e.y.String() + ", " + e.z.String() + ")"
}
func (e *gfP6) Set(a *gfP6) *gfP6 {
e.x.Set(&a.x)
e.y.Set(&a.y)
e.z.Set(&a.z)
return e
}
func (e *gfP6) SetZero() *gfP6 {
e.x.SetZero()
e.y.SetZero()
e.z.SetZero()
return e
}
func (e *gfP6) SetOne() *gfP6 {
e.x.SetZero()
e.y.SetZero()
e.z.SetOne()
return e
}
func (e *gfP6) IsZero() bool {
return e.x.IsZero() && e.y.IsZero() && e.z.IsZero()
}
func (e *gfP6) IsOne() bool {
return e.x.IsZero() && e.y.IsZero() && e.z.IsOne()
}
func (e *gfP6) Neg(a *gfP6) *gfP6 {
e.x.Neg(&a.x)
e.y.Neg(&a.y)
e.z.Neg(&a.z)
return e
}
func (e *gfP6) Frobenius(a *gfP6) *gfP6 {
e.x.Conjugate(&a.x)
e.y.Conjugate(&a.y)
e.z.Conjugate(&a.z)
e.x.Mul(&e.x, xiTo2PMinus2Over3)
e.y.Mul(&e.y, xiToPMinus1Over3)
return e
}
// FrobeniusP2 computes (xτ²+yτ+z)^(p²) = xτ^(2p²) + yτ^(p²) + z
func (e *gfP6) FrobeniusP2(a *gfP6) *gfP6 {
// τ^(2p²) = τ²τ^(2p²-2) = τ²ξ^((2p²-2)/3)
e.x.MulScalar(&a.x, xiTo2PSquaredMinus2Over3)
// τ^(p²) = ττ^(p²-1) = τξ^((p²-1)/3)
e.y.MulScalar(&a.y, xiToPSquaredMinus1Over3)
e.z.Set(&a.z)
return e
}
func (e *gfP6) FrobeniusP4(a *gfP6) *gfP6 {
e.x.MulScalar(&a.x, xiToPSquaredMinus1Over3)
e.y.MulScalar(&a.y, xiTo2PSquaredMinus2Over3)
e.z.Set(&a.z)
return e
}
func (e *gfP6) Add(a, b *gfP6) *gfP6 {
e.x.Add(&a.x, &b.x)
e.y.Add(&a.y, &b.y)
e.z.Add(&a.z, &b.z)
return e
}
func (e *gfP6) Sub(a, b *gfP6) *gfP6 {
e.x.Sub(&a.x, &b.x)
e.y.Sub(&a.y, &b.y)
e.z.Sub(&a.z, &b.z)
return e
}
func (e *gfP6) Mul(a, b *gfP6) *gfP6 {
// "Multiplication and Squaring on Pairing-Friendly Fields"
// Section 4, Karatsuba method.
// http://eprint.iacr.org/2006/471.pdf
v0 := (&gfP2{}).Mul(&a.z, &b.z)
v1 := (&gfP2{}).Mul(&a.y, &b.y)
v2 := (&gfP2{}).Mul(&a.x, &b.x)
t0 := (&gfP2{}).Add(&a.x, &a.y)
t1 := (&gfP2{}).Add(&b.x, &b.y)
tz := (&gfP2{}).Mul(t0, t1)
tz.Sub(tz, v1).Sub(tz, v2).MulXi(tz).Add(tz, v0)
t0.Add(&a.y, &a.z)
t1.Add(&b.y, &b.z)
ty := (&gfP2{}).Mul(t0, t1)
t0.MulXi(v2)
ty.Sub(ty, v0).Sub(ty, v1).Add(ty, t0)
t0.Add(&a.x, &a.z)
t1.Add(&b.x, &b.z)
tx := (&gfP2{}).Mul(t0, t1)
tx.Sub(tx, v0).Add(tx, v1).Sub(tx, v2)
e.x.Set(tx)
e.y.Set(ty)
e.z.Set(tz)
return e
}
func (e *gfP6) MulScalar(a *gfP6, b *gfP2) *gfP6 {
e.x.Mul(&a.x, b)
e.y.Mul(&a.y, b)
e.z.Mul(&a.z, b)
return e
}
func (e *gfP6) MulGFP(a *gfP6, b *gfP) *gfP6 {
e.x.MulScalar(&a.x, b)
e.y.MulScalar(&a.y, b)
e.z.MulScalar(&a.z, b)
return e
}
// MulTau computes τ·(aτ²+bτ+c) = bτ²+cτ+aξ
func (e *gfP6) MulTau(a *gfP6) *gfP6 {
tz := (&gfP2{}).MulXi(&a.x)
ty := (&gfP2{}).Set(&a.y)
e.y.Set(&a.z)
e.x.Set(ty)
e.z.Set(tz)
return e
}
func (e *gfP6) Square(a *gfP6) *gfP6 {
v0 := (&gfP2{}).Square(&a.z)
v1 := (&gfP2{}).Square(&a.y)
v2 := (&gfP2{}).Square(&a.x)
c0 := (&gfP2{}).Add(&a.x, &a.y)
c0.Square(c0).Sub(c0, v1).Sub(c0, v2).MulXi(c0).Add(c0, v0)
c1 := (&gfP2{}).Add(&a.y, &a.z)
c1.Square(c1).Sub(c1, v0).Sub(c1, v1)
xiV2 := (&gfP2{}).MulXi(v2)
c1.Add(c1, xiV2)
c2 := (&gfP2{}).Add(&a.x, &a.z)
c2.Square(c2).Sub(c2, v0).Add(c2, v1).Sub(c2, v2)
e.x.Set(c2)
e.y.Set(c1)
e.z.Set(c0)
return e
}
func (e *gfP6) Invert(a *gfP6) *gfP6 {
// See "Implementing cryptographic pairings", M. Scott, section 3.2.
// ftp://136.206.11.249/pub/crypto/pairings.pdf
// Here we can give a short explanation of how it works: let j be a cubic root of
// unity in GF(p²) so that 1+j+j²=0.
// Then (xτ² + yτ + z)(xj²τ² + yjτ + z)(xjτ² + yj²τ + z)
// = (xτ² + yτ + z)(Cτ²+Bτ+A)
// = (x³ξ²+y³ξ+z³-3ξxyz) = F is an element of the base field (the norm).
//
// On the other hand (xj²τ² + yjτ + z)(xjτ² + yj²τ + z)
// = τ²(y²-ξxz) + τ(ξx²-yz) + (z²-ξxy)
//
// So that's why A = (z²-ξxy), B = (ξx²-yz), C = (y²-ξxz)
t1 := (&gfP2{}).Mul(&a.x, &a.y)
t1.MulXi(t1)
A := (&gfP2{}).Square(&a.z)
A.Sub(A, t1)
B := (&gfP2{}).Square(&a.x)
B.MulXi(B)
t1.Mul(&a.y, &a.z)
B.Sub(B, t1)
C := (&gfP2{}).Square(&a.y)
t1.Mul(&a.x, &a.z)
C.Sub(C, t1)
F := (&gfP2{}).Mul(C, &a.y)
F.MulXi(F)
t1.Mul(A, &a.z)
F.Add(F, t1)
t1.Mul(B, &a.x).MulXi(t1)
F.Add(F, t1)
F.Invert(F)
e.x.Mul(C, F)
e.y.Mul(B, F)
e.z.Mul(A, F)
return e
}