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authorJason Ekstrand <[email protected]>2016-03-25 12:12:38 -0700
committerJason Ekstrand <[email protected]>2016-04-13 15:44:19 -0700
commit4455bfa9a0cc53a3c7e3c171b022cbe6d6dcdff8 (patch)
tree1ff121fe95cd27affd8d148dfe222b9a5f7be607 /src/compiler/nir/nir_opt_algebraic.py
parent765dd6534937e125b95c7998862b1a4ec76a22d8 (diff)
nir/algebraic: Add lowering for ldexp
The algorithm used is different from both the naive suggestion from the GLSL spec and the one used in GLSL IR today. Unfortunately, the GLSL IR implementation that we have today doesn't handle denormals (for those that care) or the case where the float source is +-inf. Reviewed-by: Matt Turner <[email protected]>
Diffstat (limited to 'src/compiler/nir/nir_opt_algebraic.py')
-rw-r--r--src/compiler/nir/nir_opt_algebraic.py31
1 files changed, 31 insertions, 0 deletions
diff --git a/src/compiler/nir/nir_opt_algebraic.py b/src/compiler/nir/nir_opt_algebraic.py
index 2749b06aa69..8f08e6b1341 100644
--- a/src/compiler/nir/nir_opt_algebraic.py
+++ b/src/compiler/nir/nir_opt_algebraic.py
@@ -371,6 +371,37 @@ optimizations = [
'options->lower_unpack_snorm_4x8'),
]
+def fexp2i(exp):
+ # We assume that exp is already in the range [-126, 127].
+ return ('ishl', ('iadd', exp, 127), 23)
+
+def ldexp32(f, exp):
+ # First, we clamp exp to a reasonable range. The maximum possible range
+ # for a normal exponent is [-126, 127] and, throwing in denormals, you get
+ # a maximum range of [-149, 127]. This means that we can potentially have
+ # a swing of +-276. If you start with FLT_MAX, you actually have to do
+ # ldexp(FLT_MAX, -278) to get it to flush all the way to zero. The GLSL
+ # spec, on the other hand, only requires that we handle an exponent value
+ # in the range [-126, 128]. This implementation is *mostly* correct; it
+ # handles a range on exp of [-252, 254] which allows you to create any
+ # value (including denorms if the hardware supports it) and to adjust the
+ # exponent of any normal value to anything you want.
+ exp = ('imin', ('imax', exp, -252), 254)
+
+ # Now we compute two powers of 2, one for exp/2 and one for exp-exp/2.
+ # (We use ishr which isn't the same for -1, but the -1 case still works
+ # since we use exp-exp/2 as the second exponent.) While the spec
+ # technically defines ldexp as f * 2.0^exp, simply multiplying once doesn't
+ # work with denormals and doesn't allow for the full swing in exponents
+ # that you can get with normalized values. Instead, we create two powers
+ # of two and multiply by them each in turn. That way the effective range
+ # of our exponent is doubled.
+ pow2_1 = fexp2i(('ishr', exp, 1))
+ pow2_2 = fexp2i(('isub', exp, ('ishr', exp, 1)))
+ return ('fmul', ('fmul', f, pow2_1), pow2_2)
+
+optimizations += [(('ldexp', 'x', 'exp'), ldexp32('x', 'exp'))]
+
# Unreal Engine 4 demo applications open-codes bitfieldReverse()
def bitfield_reverse(u):
step1 = ('ior', ('ishl', u, 16), ('ushr', u, 16))