3 # Vector Operations Extension to SV
5 This extension is usually dependent on SV SUBVL being implemented. When SUBVL is set to define the length of a subvector the operations in this extension interpret the elements as a single vector.
7 Normally in SV all operations are scalar and independent, and the operations on them may inherently be independently parallelised, with the result being a vector of length exactly equal to the input vectors.
9 In this extension, the subvector itself is typically the unit, although some operations will work on scalars or standard vectors as well, or the result is a scalar that is dependent on all elements within the vector arguments.
11 However given that some of the parameters are vectors (with and without SUBVL set), and some are scalars (where SUBVL will not apply), some clear rules need to be defined as to how the operations work.
13 Examples which can require SUBVL include cross product and may in future involve complex numbers.
17 * SUBVL=2, vd, vs; SUBVL ignored on beta.
18 * VL nonzero ok. beta as scalar ok (applies across all vectors)
19 * non vector args vd, vs, or SUBVL!=2 reserved.
21 6 opcode options (fmt3):
23 * CORDIC.lin.rot vd, vs, beta
24 * CORDIC.cir.rot vd, vs, beta
25 * CORDIC.hyp.rot vd, vs, beta
26 * CORDIC.lin.vec vd, vs, beta
27 * CORDIC.cir.vec vd, vs, beta
28 * CORDIC.hyp.vec vd, vs, beta
30 CORDIC is an extremely general-purpose algorithm useful for a huge number
31 of diverse purposes. In its full form it does however require quite a
32 few parameters, one of which is a vector, making it awkward to include in
33 a standard "scalar" ISA. Additionally the coordinates can be set to circular,
34 linear or hyperbolic, producing three different modes, and the algorithm
35 may also be run in either "vector" mode or "rotation" mode. See [[discussion]]
37 CORDIC can also be used for performing DCT. See
38 <https://arxiv.org/abs/1606.02424>
40 vx, vy = CORDIC(vx, vy, coordinate\_mode, beta)
43 int iterations = 0; // Number of times to run the algorithm
44 float arctanTable[iterations]; // in Radians
45 float K = 0.6073; // K
46 float v_x,v_y; // Vector v; x and y components
48 for(i=0; i < iterations; i++) {
49 arctanTable[i] = atan(pow(2,-i));
52 float vnew_x; // To store the new value of x;
53 for(i = 0; i < iterations; i++) {
54 // If beta is negative, we need to do a counter-clockwise rotation:
56 vnew_x = v_x + (v_y*pow(2,-i));
57 v_y -= (v_x*pow(2,-i));
58 beta += arctanTable[i];
60 // If beta is positive, we need to do a clockwise rotation:
62 vnew_x = v_x - (v_y*pow(2,-i));
63 v_y += (v_x*pow(2,-i));
64 beta -= arctanTable[i];
73 * <http://www.myhdl.org/docs/examples/sinecomp/>
75 ## Vector cross product
77 SUBVL=3, all regs. VL nonzero produces multiple vd results.
81 Result is the cross product of x and y, i.e., the resulting components are, in order:
83 x[1] * y[2] - y[1] * x[2]
84 x[2] * y[0] - y[2] * x[0]
85 x[0] * y[1] - y[0] * x[1]
87 All the operands must be vectors of 3 components of a floating-point type.
91 vec3 a, b; // elements in order a.x, a.y, a.z
93 vec3 t1 = a.yzx; // produce vector [a.y, a.z, a.x]
98 vec3 cross = t1 * t2 - p;
107 fmulsub F3, F4, F7, F8
109 ## Vector dot product
111 * SUBVL ignored on rd. SUBVL=2,3,4 vs1,vs2, if all vectors, multiple results generated. If rd scalar, only first (unpredicated) SUBVector is used.
112 * rd=scalar, SUBVL=1 and vs1, vs2=vec will produce one scalar result. Predication allowed on src vectors.
116 Computes the dot product of two vectors. Internal accuracy must be
117 greater than the input vectors and the result.
119 Pseudocode in python:
121 from operator import mul
126 double dot_product(float v[], float u[], int n)
129 for (int i = 0; i < n; i++)
130 result += v[i] * u[i];
136 * rd=scalar, vs1=vec (SUBVL=1)
137 * rd=scalar, vs1=vec (SUBVL=2,3,4) only 1 (predication rules apply)
138 * rd=vec, SUBVL ignored; vs1=vec, SUBVL=2,3,4
139 * rd=vec, SUBVL ignored; vs1=vec, SUBVL=1: reserved encoding.
143 The scalar length of a vector:
145 sqrt(x[0]^2 + x[1]^2 + ...).
151 The scalar distance between two vectors. Subtracts one vector from the
152 other and returns length:
158 * VLERP rd, vs1, rs2 # SUBVL=2: vs1.v0 vs1.v1
160 Known as **fmix** in GLSL.
162 <https://en.m.wikipedia.org/wiki/Linear_interpolation>
166 // Imprecise method, which does not guarantee v = v1 when t = 1,
167 // due to floating-point arithmetic error.
168 // This form may be used when the hardware has a native fused
169 // multiply-add instruction.
170 float lerp(float v0, float v1, float t) {
171 return v0 + t * (v1 - v0);
174 // Precise method, which guarantees v = v1 when t = 1.
175 float lerp(float v0, float v1, float t) {
176 return (1 - t) * v0 + t * v1;
181 * VSLERP vd, vs1, vs2, rs3
183 Not recommended as it is not commonly used and has several trigonometric
184 functions, although CORDIC in vector rotate circular mode is designed for this purpose. Also a costly 4 arg operation.
186 <https://en.m.wikipedia.org/wiki/Slerp>
190 Quaternion slerp(Quaternion v0, Quaternion v1, double t) {
191 // Only unit quaternions are valid rotations.
192 // Normalize to avoid undefined behavior.
196 // Compute the cosine of the angle between the two vectors.
197 double dot = dot_product(v0, v1);
199 // If the dot product is negative, slerp won't take
200 // the shorter path. Note that v1 and -v1 are equivalent when
201 // the negation is applied to all four components. Fix by
202 // reversing one quaternion.
208 const double DOT_THRESHOLD = 0.9995;
209 if (dot > DOT_THRESHOLD) {
210 // If the inputs are too close for comfort, linearly interpolate
211 // and normalize the result.
213 Quaternion result = v0 + t*(v1 - v0);
218 // Since dot is in range [0, DOT_THRESHOLD], acos is safe
219 double theta_0 = acos(dot); // theta_0 = angle between input vectors
220 double theta = theta_0*t; // theta = angle between v0 and result
221 double sin_theta = sin(theta); // compute this value only once
222 double sin_theta_0 = sin(theta_0); // compute this value only once
224 double s0 = cos(theta) - dot * sin_theta / sin_theta_0; // == sin(theta_0 - theta) / sin(theta_0)
225 double s1 = sin_theta / sin_theta_0;
227 return (s0 * v0) + (s1 * v1);
230 However this algorithm does not involve transcendentals except in
231 the computation of the tables: <https://en.wikipedia.org/wiki/CORDIC#Rotation_mode>
233 function v = cordic(beta,n)
234 % This function computes v = [cos(beta), sin(beta)] (beta in radians)
235 % using n iterations. Increasing n will increase the precision.
237 if beta < -pi/2 || beta > pi/2
239 v = cordic(beta + pi, n);
241 v = cordic(beta - pi, n);
243 v = -v; % flip the sign for second or third quadrant
247 % Initialization of tables of constants used by CORDIC
248 % need a table of arctangents of negative powers of two, in radians:
249 % angles = atan(2.^-(0:27));
251 0.78539816339745 0.46364760900081
252 0.24497866312686 0.12435499454676 ...
253 0.06241880999596 0.03123983343027
254 0.01562372862048 0.00781234106010 ...
255 0.00390623013197 0.00195312251648
256 0.00097656218956 0.00048828121119 ...
257 0.00024414062015 0.00012207031189
258 0.00006103515617 0.00003051757812 ...
259 0.00001525878906 0.00000762939453
260 0.00000381469727 0.00000190734863 ...
261 0.00000095367432 0.00000047683716
262 0.00000023841858 0.00000011920929 ...
263 0.00000005960464 0.00000002980232
264 0.00000001490116 0.00000000745058 ];
265 % and a table of products of reciprocal lengths of vectors [1, 2^-2j]:
266 % Kvalues = cumprod(1./abs(1 + 1j*2.^(-(0:23))))
268 0.70710678118655 0.63245553203368
269 0.61357199107790 0.60883391251775 ...
270 0.60764825625617 0.60735177014130
271 0.60727764409353 0.60725911229889 ...
272 0.60725447933256 0.60725332108988
273 0.60725303152913 0.60725295913894 ...
274 0.60725294104140 0.60725293651701
275 0.60725293538591 0.60725293510314 ...
276 0.60725293503245 0.60725293501477
277 0.60725293501035 0.60725293500925 ...
278 0.60725293500897 0.60725293500890
279 0.60725293500889 0.60725293500888 ];
280 Kn = Kvalues(min(n, length(Kvalues)));
282 % Initialize loop variables:
283 v = [1;0]; % start with 2-vector cosine and sine of zero
294 factor = sigma * poweroftwo;
295 % Note the matrix multiplication can be done using scaling by
296 % powers of two and addition subtraction
297 R = [1, -factor; factor, 1];
298 v = R * v; % 2-by-2 matrix multiply
299 beta = beta - sigma * angle; % update the remaining angle
300 poweroftwo = poweroftwo / 2;
301 % update the angle from table, or eventually by just dividing by two
302 if j+2 > length(angles)
309 % Adjust length of output vector to be [cos(beta), sin(beta)]:
315 2x2 matrix multiply can be done with shifts and adds:
317 x = v[0] - sigma * (v[1] * 2^(-j));
318 y = sigma * (v[0] * 2^(-j)) + v[1];
321 The technique is outlined in a paper as being applicable to 3D:
322 <https://www.atlantis-press.com/proceedings/jcis2006/232>
324 # Expensive 3-operand OP32 operations
326 3-operand operations are extremely expensive in terms of OP32 encoding space. A potential idea is to embed 3 RVC register formats across two out of three 5-bit fields rs1/rs2/rd
328 Another is to overwrite one of the src registers.
336 * <http://lists.libre-riscv.org/pipermail/libre-riscv-dev/2019-September/002736.html>
337 * <http://lists.libre-riscv.org/pipermail/libre-riscv-dev/2019-September/002733.html>
338 * <http://bugs.libre-riscv.org/show_bug.cgi?id=142>