| 685 | * @returns [sin(x/2^bits)*2^bits, cos(x/2^bits)*2^bits] |
| 686 | */ |
| 687 | export function fpsincos(x: bigint, bits: number): [bigint, bigint] { |
| 688 | const B = BigInt(bits); |
| 689 | const scale = 1n << B; |
| 690 | // sin(0) = 0, cos(0) = 1 |
| 691 | if (x === 0n) return [0n, scale]; |
| 692 | |
| 693 | const pi = fppi(bits); |
| 694 | const twoPi = 2n * pi; |
| 695 | const halfPi = pi / 2n; |
| 696 | |
| 697 | // Step 1: Reduce modulo 2π to [0, 2π) |
| 698 | // For large arguments, x % twoPi loses precision because x has many |
| 699 | // more bits than twoPi. Use extended precision for the reduction. |
| 700 | let r: bigint; |
| 701 | const absX = bigintAbs(x); |
| 702 | if (absX > scale << 30n) { |
| 703 | // Large argument: compute at extended precision. |
| 704 | // Extra guard bits: bitLength(|x/scale|) + 64. |
| 705 | const extraBits = bitLength(absX) - bits + 64; |
| 706 | const extBits = bits + extraBits; |
| 707 | const extX = x << BigInt(extraBits); |
| 708 | const extPi = fppi(extBits); |
| 709 | const extTwoPi = 2n * extPi; |
| 710 | |
| 711 | let extR = extX % extTwoPi; |
| 712 | if (extR < 0n) extR += extTwoPi; |
| 713 | |
| 714 | // Scale back |
| 715 | r = extR >> BigInt(extraBits); |
| 716 | } else { |
| 717 | r = x % twoPi; |
| 718 | } |
| 719 | if (r < 0n) r += twoPi; |
| 720 | |
| 721 | // Step 2: Quadrant reduction to [0, π/2] |
| 722 | // Determine quadrant and adjust sign |
| 723 | let sinSign = 1n; |
| 724 | let cosSign = 1n; |
| 725 | |
| 726 | if (r > 3n * halfPi) { |
| 727 | // Quadrant 4: [3π/2, 2π) → sin negative, cos positive, use 2π - r |
| 728 | r = twoPi - r; |
| 729 | sinSign = -1n; |
| 730 | } else if (r > pi) { |
| 731 | // Quadrant 3: [π, 3π/2] → sin negative, cos negative, use r - π |
| 732 | r = r - pi; |
| 733 | sinSign = -1n; |
| 734 | cosSign = -1n; |
| 735 | } else if (r > halfPi) { |
| 736 | // Quadrant 2: [π/2, π] → sin positive, cos negative, use π - r |
| 737 | r = pi - r; |
| 738 | cosSign = -1n; |
| 739 | } |
| 740 | // else Quadrant 1: [0, π/2] — no change |
| 741 | |
| 742 | // Step 3: Double-angle halving |
| 743 | // Each halving is cheap (integer divide by 2) but reconstruction costs O(M(p)). |
| 744 | // Each Taylor term also costs O(M(p)). Balance the two for O(√p) total steps. |