Files

425 lines
20 KiB
C
Raw Permalink Blame History

This file contains ambiguous Unicode characters
This file contains Unicode characters that might be confused with other characters. If you think that this is intentional, you can safely ignore this warning. Use the Escape button to reveal them.
#ifdef INTELLISENSE_DIRECTIVES
# include "gen/macs.h"
# include "gen/offsets.h"
# include "gte.h"
# include "gp.h"
# include "tape.h"
# include "math.atom.h"
#endif
ATOM_FILE_DEBUGGER_LINE_MARKER(gte_atom_c);
#pragma region MACs (Mips Atom Components)
/* Words: 3; Loads 3 S2 indices from the face array */
FI_ Slice_MipsCode ac_load_tri_indices(AtomBuilder_R ab, U4 r_face_cusor, U4 r_i0, U4 r_i1, U4 r_i2)
atom_dbg_skip MipsAtomComp_Proc_(ab, {
load_half_u(r_i0, r_face_cusor, 0 * S_(S2)),
load_half_u(r_i1, r_face_cusor, 1 * S_(S2)),
load_half_u(r_i2, r_face_cusor, 2 * S_(S2)),
})
FI_ Slice_MipsCode ac_gte_mv_to_cr_diag_v3s4(AtomBuilder_R ab, Reg_(V3_S4) v) MipsAtomComp_Proc_(ab, {
gte_mv_to_ctrl_r(v.y, gte_cr_RT13),
gte_mv_to_ctrl_r(v.z, gte_cr_RT22),
gte_mv_to_ctrl_r(v.x, gte_cr_RT11),
})
FI_ Slice_MipsCode ac_gte_ld_ir123_v3s4(AtomBuilder_R ab, Reg_(V3_S4) v) MipsAtomComp_Proc_(ab, {
gte_mv_to_data_r(v.x, C2_IR1),
gte_mv_to_data_r(v.y, C2_IR2),
gte_mv_to_data_r(v.z, C2_IR3),
})
/* ─── GTE OP cross product (a × b → a) ───
* Sets up RT diagonal from a.xyz, IR1/2/3 from b.xyz, fires OP,
* reads MAC1/2/3, shifts right 12 (S12.20 → S12.0 OuterProduct12), writes back to a.xyz.
* Composes the three sub-primitives (RT-load, IR-load, OP, MAC-read, shift)
* into one component for use by atoms that need the cross product inline.
*
* Output gpr (a) aliases source-A gpr; MAC read clobbers source-A's load targets,
* but by that point the RT load is complete and source A is dead.
* Pipeline: clobbers IR1..3, MAC1..3, RT11..33.
*
* The CPU→COP2 transfer chains (3 ctc2, 3 mtc2) require a 2-slot retirement gap,
* and the MFC2→GPR chain (3 mfc2) requires a 1-slot retirement gap, before the GPR can be read.
* The hazard nops are inlined below — same convention as ac_gte_gpf_scale — so any atom body inlining this component inherits them.
*
* Words: 18 (3 ctc2 + 2 nop + 3 mtc2 + 2 nop + 1 op + 3 mfc2 + 1 nop + 3 sra).
*/
FI_ Slice_MipsCode ac_gte_op_cross_v3s4(AtomBuilder_R ab, Reg_(V3_S4) a, Reg_(V3_S4) b) atom_dbg_skip MipsAtomComp_Proc_(ab, {
mac_gte_mv_to_cr_diag_v3s4(a), GteDelay_ /* RT diagonal: D1 = a.x, D2 = a.y, D3 = a.z */
mac_gte_ld_ir123_v3s4(b), GteDelay_ /* IR: second operand (b.xyz) */
gte_cmdw_cross, /* OP: MAC1/2/3 = a × b (S12.20) */
mac_gte_mv_from_mac123_v3s4(a), GteDelay_ /* Read MAC1/2/3 → a.xyz (overwrites source-A's load targets) */
mac_shift_aright_v3s4_self(a, 12), /* Right-shift MAC by 12 (S12.20 → S12.0 OuterProduct12) */
})
/* Words: 3; Stores the 3 transformed (V2_S2 screen) vertices to the F3.
* PIPELINE: post-RTPT (SXY0=v0.screen, SXY1=v1.screen, SXY2=v2.screen). */
FI_ Slice_MipsCode ac_gte_store_f3(AtomBuilder_R ab, U4 r_primitive_cursor) atom_dbg_skip MipsAtomComp_Proc_(ab, {
gte_sw(C2_SXY0, r_primitive_cursor, O_(Poly_F3,p0)),
gte_sw(C2_SXY1, r_primitive_cursor, O_(Poly_F3,p1)),
gte_sw(C2_SXY2, r_primitive_cursor, O_(Poly_F3,p2)),
})
/* Words: 18; Translates indices to vertex addresses and pushes them to GTE */
I_ Slice_MipsCode ac_gte_load_tri_verts(AtomBuilder_R ab, Reg vbase, Reg v0, Reg v1, Reg v2) atom_dbg_skip MipsAtomComp_Proc_(ab, {
shift_lleft(R_AT, v0, v3s2_byteoff), add_u_self(R_AT, vbase), load_word(R_V0, R_AT, O_(V3_S2,x)), load_word(R_V1, R_AT, O_(V3_S2,z)), LdSlot_ gte_mv_to_data_r(R_V0, C2_VXY0), gte_mv_to_data_r(R_V1, C2_VZ0),
shift_lleft(R_AT, v1, v3s2_byteoff), add_u_self(R_AT, vbase), load_word(R_V0, R_AT, O_(V3_S2,x)), load_word(R_V1, R_AT, O_(V3_S2,z)), LdSlot_ gte_mv_to_data_r(R_V0, C2_VXY1), gte_mv_to_data_r(R_V1, C2_VZ1),
shift_lleft(R_AT, v2, v3s2_byteoff), add_u_self(R_AT, vbase), load_word(R_V0, R_AT, O_(V3_S2,x)), load_word(R_V1, R_AT, O_(V3_S2,z)), LdSlot_ gte_mv_to_data_r(R_V0, C2_VXY2), gte_mv_to_data_r(R_V1, C2_VZ2),
})
/* Words: 3; Stores the 3 transformed (V2_S2 screen) vertices of the
* G4 triangle portion to p0/p1/p2.
* PIPELINE: post-RTPT, pre-RTPS (SXY0=v0.screen, SXY1=v1.screen, SXY2=v2.screen).
* MUST be called BEFORE V3-RTPS, otherwise SXY0/1/2 get overwritten with v3
* (RTPS writes only to SXY2, but to keep the three registers aligned with v0/v1/v2 you must store before RTPS). */
FI_ Slice_MipsCode ac_gte_store_g4_p012(AtomBuilder_R ab, Reg r_primitive_cursor) atom_dbg_skip MipsAtomComp_Proc_(ab, {
gte_sw(C2_SXY0, r_primitive_cursor, O_(Poly_G4,p0)),
gte_sw(C2_SXY1, r_primitive_cursor, O_(Poly_G4,p1)),
gte_sw(C2_SXY2, r_primitive_cursor, O_(Poly_G4,p2)),
})
/* Words: 1; Stores the V3 screen coord to the G4's p3 slot.
* PIPELINE: post-RTPS (SXY2 holds v3.screen because RTPS writes its single-vertex result to SXY2;
* SXY0 still holds v0.screen from the earlier RTPT.
*/
FI_ Slice_MipsCode ac_gte_store_g4_p3(AtomBuilder_R ab, U4 r_primitive_cursor) atom_dbg_skip MipsAtomComp_Proc_(ab, { gte_sw(C2_SXY2, r_primitive_cursor, O_(Poly_G4,p3)) })
/* ─── STAGE 1 of normalize: SQR + mfc2 MAC1/2/3 ───
* Emits squared magnitude per component (in MAC1/2/3) into caller-provided scratch regs. */
FI_ Slice_MipsCode ac_gte_sqr_v3(AtomBuilder_R ab, U4 r_sx, U4 r_sy, U4 r_sz, U4 r_sq_x, U4 r_sq_y, U4 r_sq_z) atom_dbg_skip MipsAtomComp_Proc_(ab, {
mac_gte_sqr_v3s4(r_sx, r_sy, r_sz, nop),
gte_mv_from_data_r(r_sq_x, C2_MAC1),
gte_mv_from_data_r(r_sq_y, C2_MAC2),
gte_mv_from_data_r(r_sq_z, C2_MAC3),
})
/* ─── SQR FIRE — mtc2 3 GPRs into IR1/IR2/IR3, then fire SQR. ─── */
FI_ Slice_MipsCode ac_gte_sqr_v3s4(AtomBuilder_R ab, Reg sx, Reg sy, Reg sz, MipsCode delay_slot)
atom_dbg_skip MipsAtomComp_Proc_(ab, {
gte_mv_to_data_r(sx, C2_IR1),
gte_mv_to_data_r(sy, C2_IR2),
gte_mv_to_data_r(sz, C2_IR3),
delay_slot, gte_cmdw_sqr,
})
/* ─── STAGE 4 of normalize: mtc2 IR0..3 + GPF + mfc2 MAC + srav finalize ───
* Reusable standalone — given an IR0 = 1/|v| estimate (typically from a sqrtbl lookup) and a shift count
* (typically (31 - LZCR)/2), multiplies IR0*IR[i] via GPF and shifts right to produce the normalized output.
* Used standalone for "scale vector by scalar".
* Words: 11. Clobbers: IR0..3, MAC1..3. Uses gte_cmdw_gpf (sf=0, lm=0). */
FI_ Slice_MipsCode ac_gte_gpf_scale(AtomBuilder_R ab,
U4 r_sx, U4 r_sy, U4 r_sz,
U4 r_recip_est, U4 r_shift,
U4 r_dx, U4 r_dy, U4 r_dz)
atom_dbg_skip MipsAtomComp_Proc_(ab, {
gte_mv_to_data_r(r_recip_est, C2_IR0),
gte_mv_to_data_r(r_sx, C2_IR1),
gte_mv_to_data_r(r_sy, C2_IR2),
gte_mv_to_data_r(r_sz, C2_IR3),
GteDelay_ nop2, /* retire IR0..IR3 → GPF input pre-fill (matches libgte 0x80016134..0x80016138) */
gte_cmdw_gpf,
gte_mv_from_data_r(r_dx, C2_MAC1),
gte_mv_from_data_r(r_dy, C2_MAC2),
gte_mv_from_data_r(r_dz, C2_MAC3),
shift_aright_var(r_dx, r_dx, r_shift),
shift_aright_var(r_dy, r_dy, r_shift),
shift_aright_var(r_dz, r_dz, r_shift),
})
/* ─── TRANS MATRIX (libgte TransMatrix port) ───
* Atom component — auto-generates mac_trans_matrix Mac composer macro.
* m->t = v (struct copy; libgte's TransMatrix at 0x8001a540 is just 3 store_words, no GTE, no add).
* Uses 1 GPR (r_t1 = off value) per axis; per-axis load-delay-slot pattern.
* Words: 9. Clobbers: r_t1. */
FI_ Slice_MipsCode ac_trans_mt3s3s4(AtomBuilder_R ab
, U4 r_mtx, U4 r_off
, U4 r_t0, U4 r_t1, U4 r_t2
) MipsAtomComp_Proc_(ab, {
load_word( r_t0, r_off, O_(V3_S4,x)),
load_word( r_t1, r_off, O_(V3_S4,y)),
load_word( r_t2, r_off, O_(V3_S4,z)),
store_word(r_t0, r_mtx, O_(MT3_S2S4,t[0])),
store_word(r_t1, r_mtx, O_(MT3_S2S4,t[1])),
store_word(r_t2, r_mtx, O_(MT3_S2S4,t[2])),
})
/* ─── LZCR ROUND EVEN + HALF-SHIFT ───
* Takes the raw LZCR leading-zero/ones count (from mfc2 C2_LZCR, range 1..32 per PSX-SPX cop2r31) and the |v|² sum (in r_mag_sq from the MAC1+MAC2+MAC3 add).
* Produces:
* r_shift ← LZCR rounded down to even (clear bit 0)
* r_mag_sq_copy ← |v|² sum (moved out of r_mag_sq before it's overwritten)
* r_mag_sq ← (31 - even_LZCR) / 2 = the final srav/GPF shift amount
*
* Rounding to even ensures (31 - LZCR) is always odd, so the >> 1 division is consistent — no 0.5 loss.
* The caller branches on LZCR < 24 to decide left-shift vs right-shift of r_mag_sq_copy, then saves the shift count.
*
* Note: C2_LZCR (cop2r31) is a fixed read-only C2 data register — the caller must read it via mfc2 from C2_LZCR;
* there is no register choice at the hardware level. Only the GPR that holds the result is caller-determined. */
FI_ Slice_MipsCode ac_lzcr_round_even_half_shift(AtomBuilder_R ab, Reg shift, Reg mag_sq, Reg mag_sq_copy)
atom_dbg_skip MipsAtomComp_Proc_(ab, {
and_i(shift, shift, gte_lzcr_even_mask),
or_u(mag_sq_copy, mag_sq, 0),
li_s( mag_sq, 31),
sub_s( mag_sq, mag_sq, shift),
shift_aright(mag_sq, mag_sq, 1),
})
FI_ Slice_MipsCode ac_gte_general_purpose_interopolation(AtomBuilder_R ab
, Reg to_ir0, Reg to_ir1, Reg to_ir2, Reg to_ir3
, Reg fr_mac1, Reg fr_mac2, Reg fr_mac3
, MipsCode nop_slot1, MipsCode nop_slot2)
MipsAtomComp_Proc_(ab, {
gte_mv_to_data_r(to_ir0, C2_IR0),
gte_mv_to_data_r(to_ir1, C2_IR1), /* IR1 = src.x (preserved in r_tmp — r_mac2_scratch was clobbered to MAC2 in stage 1.5) */
gte_mv_to_data_r(to_ir2, C2_IR2),
gte_mv_to_data_r(to_ir3, C2_IR3), /* IR3 = src.z (reloaded) */
GteDelay_ nop_slot1,
GteDelay_ nop_slot2,
gte_cmdw_gpf,
gte_mv_from_data_r(fr_mac1, C2_MAC1),
gte_mv_from_data_r(fr_mac2, C2_MAC2),
gte_mv_from_data_r(fr_mac3, C2_MAC3),
})
FI_ Slice_MipsCode ac_gte_mv_from_data_r_mac123(AtomBuilder_R ab, Reg fr_mac1, Reg fr_mac2, Reg fr_mac3)
MipsAtomComp_Proc_(ab, {
gte_mv_from_data_r(fr_mac1, C2_MAC1),
gte_mv_from_data_r(fr_mac2, C2_MAC2),
gte_mv_from_data_r(fr_mac3, C2_MAC3),
})
FI_ Slice_MipsCode ac_gte_mv_from_mac123_v3s4(AtomBuilder_R ab, Reg_(V3_S4) v) MipsAtomComp_ProcMap_(ab, mac_gte_mv_from_data_r_mac123(v.x, v.y, v.z))
#pragma endregion MACs (Mips Atom Components)
#pragma region Atom Procs
/* Normalize V3_S4 using the PSYQ/libgte reciprocal-sqrt method:
* |v|² = x² + y² + z²
* LZCR determines the exponent of |v|².
* Round that exponent even and shift |v|² into [1, 4).
* sqrtbl approximates 1/sqrt(mantissa).
* GPF multiplies v by that reciprocal-sqrt mantissa.
* srav_shift restores the exponent scale.
* Effectively: v_normalized = v * (1 / sqrt(|v|²)).
*
* ─── Local port of PSYQ's sqrtbl (1/sqrt lookup table for VectorNormal). ───
* Source: PSYQ 4.7 libgte sqrtbl at 0x800185B4 in hello_camera.elf.
* objdump -s --start-address=0x800185B4 --stop-address=0x800185F4 hello_camera.elf -> 192 entries x 16-bit signed, stored in 1.12 fixed point.
* Data is identical to the libgte original (byte-for-byte verified).
*
* ─── Table semantics ───
* For table index i in [0, 192):
* x = 1 + i / 64
* tbl[i] = floor(4096 / sqrt(x))
* Thus the table uniformly samples 1/sqrt(x) over:
* x in [1.0, 4.0)
* at steps of 1/64, with the result represented in 1.12 fixed point (0x1000 = 1.0).
*
* Representative entries:
* [ 0] 0x1000 = 1.000000 ; 1 / sqrt(1.000000)
* [ 16] 0x0e4f = 0.894287 ; 1 / sqrt(1.250000)
* [ 32] 0x0d10 = 0.816406 ; 1 / sqrt(1.500000)
* [ 48] 0x0c18 = 0.755859 ; 1 / sqrt(1.750000)
* [ 64] 0x0b50 = 0.707031 ; 1 / sqrt(2.000000)
* [128] 0x093c = 0.577148 ; 1 / sqrt(3.000000)
* [191] 0x0804 = 0.500977 ; 1 / sqrt(3.984375)
*
* ─── How VectorNormal indexes it ───
* Let:
* mag_sq = x*x + y*y + z*z
* lzcr = leading-zero count of mag_sq
* For a non-zero magnitude, libgte first rounds LZCR down to an even number:
* lzcr_even = lzcr & ~1
*
* It then shifts mag_sq so that its significant bits land in one of two
* adjacent normalized ranges:
* if lzcr_even >= 24:
* aligned = mag_sq << (lzcr_even - 24)
* else:
* aligned = mag_sq >> (24 - lzcr_even)
*
* Because lzcr_even differs from the true LZCR by at most one bit:
* raw LZCR even -> aligned in [0x80, 0x100)
* raw LZCR odd -> aligned in [0x40, 0x080)
* therefore:
* aligned in [0x40, 0x100)
*
* Dividing this normalized integer by 64 gives exactly the table domain:
* x = aligned / 64
* x in [1.0, 4.0)
*
* The lookup is therefore:
* index = aligned - 0x40
* byte_offset = index * sizeof(S2)
* inv_len = sqrtbl[index]
* or equivalently, matching the libgte instructions:
* addi aligned, -64
* sll aligned, 1
* lh inv_len, sqrtbl + aligned
*
* ─── Why the domain spans [1, 4) instead of [1, 2) ───
* Square-root scaling depends on the parity of the exponent.
* Rounding LZCR to even absorbs exponent changes in pairs of bits, leaving the lookup mantissa normalized over a factor-of-four interval [1, 4).
*
* The corresponding exponent correction is retained separately as:
* srav_shift = (31 - lzcr_even) >> 1
*
* After GPF multiplies the original vector components by the table's reciprocal-square-root coefficient,
* this shift restores the exponent scale and yields the normalized vector.
*
* Reproduced verbatim from libgte; also matches PSn00bSDK VectorNormalS _norm_table (24 rows x 8 halfwords, final entry 0x0804).
**/
internal S2 const gte_normalize_sqr_tbl[192] align_(2) = {
0x1000, 0x0fe0, 0x0fc1, 0x0fa3, 0x0f85, 0x0f68, 0x0f4c, 0x0f30,
0x0f15, 0x0efb, 0x0ee1, 0x0ec7, 0x0eae, 0x0e96, 0x0e7e, 0x0e66,
0x0e4f, 0x0e38, 0x0e22, 0x0e0c, 0x0df7, 0x0de2, 0x0dcd, 0x0db9,
0x0da5, 0x0d91, 0x0d7e, 0x0d6b, 0x0d58, 0x0d45, 0x0d33, 0x0d21,
0x0d10, 0x0cff, 0x0cee, 0x0cdd, 0x0ccc, 0x0cbc, 0x0cac, 0x0c9c,
0x0c8d, 0x0c7d, 0x0c6e, 0x0c5f, 0x0c51, 0x0c42, 0x0c34, 0x0c26,
0x0c18, 0x0c0a, 0x0bfd, 0x0bef, 0x0be2, 0x0bd5, 0x0bc8, 0x0bbb,
0x0baf, 0x0ba2, 0x0b96, 0x0b8a, 0x0b7e, 0x0b72, 0x0b67, 0x0b5b,
0x0b50, 0x0b45, 0x0b39, 0x0b2e, 0x0b24, 0x0b19, 0x0b0e, 0x0b04,
0x0af9, 0x0aef, 0x0ae5, 0x0adb, 0x0ad1, 0x0ac7, 0x0abd, 0x0ab4,
0x0aaa, 0x0aa1, 0x0a97, 0x0a8e, 0x0a85, 0x0a7c, 0x0a73, 0x0a6a,
0x0a61, 0x0a59, 0x0a50, 0x0a47, 0x0a3f, 0x0a37, 0x0a2e, 0x0a26,
0x0a1e, 0x0a16, 0x0a0e, 0x0a06, 0x09fe, 0x09f6, 0x09ef, 0x09e7,
0x09e0, 0x09d8, 0x09d1, 0x09c9, 0x09c2, 0x09bb, 0x09b4, 0x09ad,
0x09a5, 0x099e, 0x0998, 0x0991, 0x098a, 0x0983, 0x097c, 0x0976,
0x096f, 0x0969, 0x0962, 0x095c, 0x0955, 0x094f, 0x0949, 0x0943,
0x093c, 0x0936, 0x0930, 0x092a, 0x0924, 0x091e, 0x0918, 0x0912,
0x090d, 0x0907, 0x0901, 0x08fb, 0x08f6, 0x08f0, 0x08eb, 0x08e5,
0x08e0, 0x08da, 0x08d5, 0x08cf, 0x08ca, 0x08c5, 0x08bf, 0x08ba,
0x08b5, 0x08b0, 0x08ab, 0x08a6, 0x08a1, 0x089c, 0x0897, 0x0892,
0x088d, 0x0888, 0x0883, 0x087e, 0x087a, 0x0875, 0x0870, 0x086b,
0x0867, 0x0862, 0x085e, 0x0859, 0x0855, 0x0850, 0x084c, 0x0847,
0x0843, 0x083e, 0x083a, 0x0836, 0x0831, 0x082d, 0x0829, 0x0824,
0x0820, 0x081c, 0x0818, 0x0814, 0x0810, 0x080c, 0x0808, 0x0804,
};
typedef Struct_(Binds_normalize_v3s4) { U2 src_offset; U2 dst_offset; };
typedef Struct_(RegUse_normalize_v3s4) {
union { Reg_(V3_S4) res, src; };
union { Reg r0, src_ptr, mac2; };
union { Reg r1, dst_ptr; };
union { Reg r2, dst_offset, mac1, v_sqr_aligned, sqrtbl_byte_offset; };
union { Reg r3, src_offset, align_delta, shift_count, sqrtbl_lookup; };
union { Reg r4, mac3, v_sqr_sum, srav_shift; };
union { Reg r5, lzcr_raw, lzcr_even, inv_len; };
};
/* ─── Full normalize (all 4 stages inline) ───
* Generic 4-stage GTE normalize (SQR → sum+LZCR → align+sqrtbl → GPF+srav). */
internal MipsAtom* normalize_v3s4(AtomArena_R aa, RegUse_normalize_v3s4 r)
MipsAtom_Proc_(aa, {
load_half(r.src_offset, R_TapePtr, O_(Binds_normalize_v3s4, src_offset)),
load_half(r.dst_offset, R_TapePtr, O_(Binds_normalize_v3s4, dst_offset)),
LdSlot_ add_u(r.src_ptr, R_ScratchBase, r.src_offset),
LdSlot_ add_u(r.dst_ptr, R_ScratchBase, r.dst_offset),
LdSlot_ add_ui_self(R_TapePtr, S_(Binds_normalize_v3s4)),
mac_load_v3s4(r.src, r.src_ptr, 0),
/* Stage 1: mtc2 src → IR1/2/3, SQR fires. */
LdSlot_ mac_gte_sqr_v3s4(r.src.x, r.src.y, r.src.z, LdSlot_ nop),
/* Stage 2: mfc2 MAC1/2/3, sum, mtc2 LZCS. src_ptr is dead; reuse as mac2. */
mac_gte_mv_from_data_r_mac123(r.mac1, r.mac2, r.mac3), LdSlot_ nop,
add_u_self( r.v_sqr_sum, r.mac1),
add_u_self( r.v_sqr_sum, r.mac2),
gte_mv_to_data_r( r.v_sqr_sum, C2_LZCS), GteDelay_ nop2,
gte_mv_from_data_r(r.lzcr_raw, C2_LZCR), GteDelay_ nop,
/* Stage 3: even(LZCR), half-shift, align |v|² to bit 24. */
mac_lzcr_round_even_half_shift(r.lzcr_raw, r.v_sqr_sum, r.v_sqr_aligned),
add_si( r.align_delta, r.lzcr_even, -24),
branch_lt_zero(r.align_delta, atom_offset(aligned_done, srav_path)), BdSlot_ nop, /* bltz → srav_path (LZCR < 24 path) */
jump_rel(atom_offset(srav_path, aligned_done)), /* b → aligned_done (LZCR >= 24 path) */
BdSlot_ shift_lleft_var(r.v_sqr_aligned, r.v_sqr_aligned, r.align_delta),
atom_label(srav_path)
li_s( r.shift_count, 24),
sub_s(r.shift_count, r.shift_count, r.lzcr_even),
shift_aright_var(r.v_sqr_aligned, r.v_sqr_aligned, r.shift_count),
atom_label(aligned_done)
add_si( r.sqrtbl_byte_offset, r.v_sqr_aligned, -64),
shift_lleft(r.sqrtbl_byte_offset, r.sqrtbl_byte_offset, 1),
mac_load_word_imm(r.sqrtbl_lookup, & gte_normalize_sqr_tbl), add_u_self(r.sqrtbl_lookup, r.sqrtbl_byte_offset),
load_half(r.inv_len, r.sqrtbl_lookup, 0),
LdSlot_ nop,
mac_gte_general_purpose_interopolation(r.inv_len,
r.src.x, r.src.y, r.src.z,
r.res.x, r.res.y, r.res.z,
GteDelay_ load_word(R_AtomJmp, R_TapePtr, 0), LdSlot_ // ac_yield: word 1
GteDelay_ add_ui_self( R_TapePtr, S_(MipsCode)) // ac_yield: word
),
mac_shift_aright_var_v3s4_self(r.res, r.srav_shift),
mac_store_v3s4(r.res, r.dst_ptr, 0),
jump_reg(R_AtomJmp), BdSlot_ nop // ac_yield: word 3-4
})
/* ─── GTE OP cross product (a × b → out) ───
* Generalized V3_S4 cross product via GTE OP (OuterProduct12 libpsyx convention).
* The >> 12 shift converts S12.20 → S12.0 OuterProduct12. */
typedef Struct_(Binds_gte_cross_v3s4) { V3_S4* src_a; V3_S4* src_b; V3_S4* out; };
typedef Struct_(RegUse_gte_cross_v3s4) {
Reg_(V3_S4) a;
Reg_(V3_S4) b;
Reg out;
Reg src_a;
Reg src_b;
};
internal MipsAtom* gte_cross_v3s4(AtomArena_R aa, RegUse_gte_cross_v3s4 r)
atom_info(atom_bind(Binds_gte_cross_v3s4)) MipsAtom_Proc_(aa, {
load_word(r.src_a, R_TapePtr, O_(Binds_gte_cross_v3s4,src_a)),
load_word(r.src_b, R_TapePtr, O_(Binds_gte_cross_v3s4,src_b)),
load_word(r.out, R_TapePtr, O_(Binds_gte_cross_v3s4,out)),
LdSlot_ add_ui_self(R_TapePtr, S_(Binds_gte_cross_v3s4)),
mac_load_v3s4(r.a, r.src_a, 0), LdSlot_
mac_load_v3s4(r.b, r.src_b, 0), LdSlot_
mac_gte_op_cross_v3s4(r.a, r.b), /* RT diagonal + IR + OP + MAC read + shift */
mac_store_v3s4(r.a, r.out, 0),
mac_yield()
})
#pragma endregion Atom Procs
#pragma region Baked Atoms
typedef Struct_(Binds_SetGteMT3S2S4) {
MT3_S2S4* transform;
};
internal MipsAtom_(set_gte_mt3s2s4) atom_info(
atom_bind(Binds_SetGteMT3S2S4)
, atom_reads(R_TapePtr)
){
/* Pop matrix address from tape into R_T3 ($11) */
load_word(R_T3, R_TapePtr, O_(Binds_SetGteMT3S2S4,transform)),
add_ui_self( R_TapePtr, S_(Binds_SetGteMT3S2S4)),
/* Load 3x3 Rotation + 3x1 Translation from R_T3 into GTE CONTROL Regs (ctc2) */
load_word(R_T0, R_T3, 0),
load_word(R_T1, R_T3, 4),
gte_mv_to_ctrl_r(R_T0, gte_cr_RT11),
gte_mv_to_ctrl_r(R_T1, gte_cr_RT12),
load_word(R_T0, R_T3, 8),
load_word(R_T1, R_T3, 12),
load_word(R_T2, R_T3, 16),
gte_mv_to_ctrl_r(R_T0, gte_cr_RT13),
gte_mv_to_ctrl_r(R_T1, gte_cr_RT21),
gte_mv_to_ctrl_r(R_T2, gte_cr_RT22),
load_word(R_T0, R_T3, 20),
load_word(R_T1, R_T3, 24),
load_word(R_T2, R_T3, 28),
gte_mv_to_ctrl_r(R_T0, gte_cr_TRX),
gte_mv_to_ctrl_r(R_T1, gte_cr_TRY),
gte_mv_to_ctrl_r(R_T2, gte_cr_TRZ),
mac_yield()
};
#pragma endregion Baked Atoms