Accurate computation of scaled complementary error function, erfcx()
The (exponentially) scaled complementary error function, commonly designated by erfcx , is defined mathematically as erfcx(x) := ex2 erfc(x). It frequently occurs in diffusion problems in physics as well as chemistry. While some mathematical environments, such as MATLAB and GNU Octave, provide this function, it is absent from the C standard math library, which only provides erf() and erfc() .
While it is possible to implement one's own erfcx() based directly on the mathematical definition, this only works over a limited input domain, because in the positive half-plane erfc() underflows for arguments of moderate magnitude, while exp() overflows, as noted in this question, for example.
For use with C, one could adapt some erfcx() open-source implementations such as the one in the Faadeeva package, as pointed to in responses to this question. However, these implementations typically do not provide full accuracy for a given floating-point format. For example, tests with 232 test vectors show the maximum error of erfcx() as provided by the Faadeeva package to be 8.41 ulps in the positive half-plane and 511.68 ulps in the negative half-plane.
A reasonable bound for an accurate implementation would be 4 ulps, corresponding to the accuracy bound of the math functions in the LA profile of Intel's Vector Math library, which I have found to be a reasonable bound for non-trivial math function implementations that require both good accuracy and good performance.
How could erfcx() , and the corresponding single-precision version, erfcxf() , be implemented accurately, while using only the C standard math library, and requiring no external libraries? We can assume that C's float nad double types are mapped to IEEE 754-2008 binary32 and binary64 floating-point types. Hardware support for the fused multiply-add operation (FMA) can be assumed, as this is supported by all major processor architectures at this time.
The best approach for an erfcx() implementation I have found so far is based on the following paper:
MM Shepherd and JG Laframboise, "Chebyshev Approximation of (1 + 2 x) exp(x2) erfc x in 0 ≤ x < ∞." Mathematics of Computation, Volume 36, No. 153, January 1981, pp. 249-253 (online)
The paper proposes clever transformations that map the scaled complementary error function to a tightly bounded helper function that is amenable to straightforward polynomial approximation. I have experimented with variations of the transformations for the sake of performance, but all of these have had negative impact on accuracy. The choice of the constant K in the transformation (x - K) / (x + K) has a non-obvious relationship with the accuracy of the core approximation. I empirically determined "optimal" values, which differ from the paper.
The transformations for the arguments to the core approximation and the intermediate results back into into erfcx results incur additional rounding errors. To mitigate their impact on accuracy, we need to apply compensation steps, which I outlined in some detail in my earlier question & answer regarding erfcf . The availability of FMA greatly simplifies this task.
The resulting single-precision code looks as follows:
/*
* Based on: M. M. Shepherd and J. G. Laframboise, "Chebyshev Approximation of
* (1+2x)exp(x^2)erfc x in 0 <= x < INF", Mathematics of Computation, Vol. 36,
* No. 153, January 1981, pp. 249-253.
*
*/
float my_erfcxf (float x)
{
float a, d, e, m, p, q, r, s, t;
a = fmaxf (x, 0.0f - x); // NaN-preserving absolute value computation
/* Compute q = (a-2)/(a+2) accurately. [0,INF) -> [-1,1] */
m = a - 2.0f;
p = a + 2.0f;
#if FAST_RCP_SSE
r = fast_recipf_sse (p);
#else
r = 1.0f / p;
#endif
q = m * r;
t = fmaf (q + 1.0f, -2.0f, a);
e = fmaf (q, -a, t);
q = fmaf (r, e, q);
/* Approximate (1+2*a)*exp(a*a)*erfc(a) as p(q)+1 for q in [-1,1] */
p = 0x1.f10000p-15f; // 5.92470169e-5
p = fmaf (p, q, 0x1.521cc6p-13f); // 1.61224554e-4
p = fmaf (p, q, -0x1.6b4ffep-12f); // -3.46481771e-4
p = fmaf (p, q, -0x1.6e2a7cp-10f); // -1.39681227e-3
p = fmaf (p, q, 0x1.3c1d7ep-10f); // 1.20588380e-3
p = fmaf (p, q, 0x1.1cc236p-07f); // 8.69014394e-3
p = fmaf (p, q, -0x1.069940p-07f); // -8.01387429e-3
p = fmaf (p, q, -0x1.bc1b6cp-05f); // -5.42122945e-2
p = fmaf (p, q, 0x1.4ff8acp-03f); // 1.64048523e-1
p = fmaf (p, q, -0x1.54081ap-03f); // -1.66031078e-1
p = fmaf (p, q, -0x1.7bf5cep-04f); // -9.27637145e-2
p = fmaf (p, q, 0x1.1ba03ap-02f); // 2.76978403e-1
/* Divide (1+p) by (1+2*a) ==> exp(a*a)*erfc(a) */
d = a + 0.5f;
#if FAST_RCP_SSE
r = fast_recipf_sse (d);
#else
r = 1.0f / d;
#endif
r = r * 0.5f;
q = fmaf (p, r, r); // q = (p+1)/(1+2*a)
t = q + q;
e = (p - q) + fmaf (t, -a, 1.0f); // residual: (p+1)-q*(1+2*a)
r = fmaf (e, r, q);
if (a > 0x1.fffffep127f) r = 0.0f; // 3.40282347e+38 // handle INF argument
/* Handle negative arguments: erfcx(x) = 2*exp(x*x) - erfcx(|x|) */
if (x < 0.0f) {
s = x * x;
d = fmaf (x, x, -s);
e = expf (s);
r = e - r;
r = fmaf (e, d + d, r);
r = r + e;
if (e > 0x1.fffffep127f) r = e; // 3.40282347e+38 // avoid creating NaN
}
return r;
}
The maximum error of this implementation in the negative half-plane will depend on the accuracy of the standard math library's implementation of expf() . Using the Intel compiler, version 13.1.3.198, and compiling with /fp:strict I observed a maximum error of 2.00450 ulps in the positive half-plane and 2.38412 ulps in the negative half-plane in an exhaustive test. Best I can tell at this time, a faithfully-rounded implementation of expf() will result in a maximum error of less than 2.5 ulps.
Note that while the code contains two divisions, which are potentially slow operations, they occur in the special form of reciprocals, and are thus amenable to the use of fast reciprocal approximations on many platforms. As long as the reciprocal approximation is faithfully rounded, the impact on erfcxf() accuracy seems to be negligible, based on experiments. Even slightly larger errors, such as in the fast SSE version (with maximum error < 2.0 ulps) appear to have only a minor impact.
/* Fast reciprocal approximation. HW approximation plus Newton iteration */
float fast_recipf_sse (float a)
{
__m128 t;
float e, r;
t = _mm_set_ss (a);
t = _mm_rcp_ss (t);
_mm_store_ss (&r, t);
e = fmaf (0.0f - a, r, 1.0f);
r = fmaf (e, r, r);
return r;
}
Double-precision version erfcx() is structurally identical to the single-precision version erfcxf() , but requires a minimax polynomial approximation with many more terms. This presents a challenge when optimizing the core approximation, as many heuristics will break down when the search space is very large. The coefficients below represent my best solution to date, and there is definitely room for improvement. Building with the Intel compiler and /fp:strict , and using 232 random test vectors, the maximum error observed was 2.83788 ulps in the positive half-plane and 2.77856 ulps in the negative half-plane.
double my_erfcx (double x)
{
double a, d, e, m, p, q, r, s, t;
a = fmax (x, 0.0 - x); // NaN preserving absolute value computation
/* Compute q = (a-4)/(a+4) accurately. [0,INF) -> [-1,1] */
m = a - 4.0;
p = a + 4.0;
r = 1.0 / p;
q = m * r;
t = fma (q + 1.0, -4.0, a);
e = fma (q, -a, t);
q = fma (r, e, q);
/* Approximate (1+2*a)*exp(a*a)*erfc(a) as p(q)+1 for q in [-1,1] */
p = 0x1.edcad78fc8044p-31; // 8.9820305531190140e-10
p = fma (p, q, 0x1.b1548f14735d1p-30); // 1.5764464777959401e-09
p = fma (p, q, -0x1.a1ad2e6c4a7a8p-27); // -1.2155985739342269e-08
p = fma (p, q, -0x1.1985b48f08574p-26); // -1.6386753783877791e-08
p = fma (p, q, 0x1.c6a8093ac4f83p-24); // 1.0585794011876720e-07
p = fma (p, q, 0x1.31c2b2b44b731p-24); // 7.1190423171700940e-08
p = fma (p, q, -0x1.b87373facb29fp-21); // -8.2040389712752056e-07
p = fma (p, q, 0x1.3fef1358803b7p-22); // 2.9796165315625938e-07
p = fma (p, q, 0x1.7eec072bb0be3p-18); // 5.7059822144459833e-06
p = fma (p, q, -0x1.78a680a741c4ap-17); // -1.1225056665965572e-05
p = fma (p, q, -0x1.9951f39295cf4p-16); // -2.4397380523258482e-05
p = fma (p, q, 0x1.3be1255ce180bp-13); // 1.5062307184282616e-04
p = fma (p, q, -0x1.a1df71176b791p-13); // -1.9925728768782324e-04
p = fma (p, q, -0x1.8d4aaa0099bc8p-11); // -7.5777369791018515e-04
p = fma (p, q, 0x1.49c673066c831p-8); // 5.0319701025945277e-03
p = fma (p, q, -0x1.0962386ea02b7p-6); // -1.6197733983519948e-02
p = fma (p, q, 0x1.3079edf465cc3p-5); // 3.7167515521269866e-02
p = fma (p, q, -0x1.0fb06dfedc4ccp-4); // -6.6330365820039094e-02
p = fma (p, q, 0x1.7fee004e266dfp-4); // 9.3732834999538536e-02
p = fma (p, q, -0x1.9ddb23c3e14d2p-4); // -1.0103906603588378e-01
p = fma (p, q, 0x1.16ecefcfa4865p-4); // 6.8097054254651804e-02
p = fma (p, q, 0x1.f7f5df66fc349p-7); // 1.5379652102610957e-02
p = fma (p, q, -0x1.1df1ad154a27fp-3); // -1.3962111684056208e-01
p = fma (p, q, 0x1.dd2c8b74febf6p-3); // 2.3299511862555250e-01
/* Divide (1+p) by (1+2*a) ==> exp(a*a)*erfc(a) */
d = a + 0.5;
r = 1.0 / d;
r = r * 0.5;
q = fma (p, r, r); // q = (p+1)/(1+2*a)
t = q + q;
e = (p - q) + fma (t, -a, 1.0); // residual: (p+1)-q*(1+2*a)
r = fma (e, r, q);
/* Handle argument of infinity */
if (a > 0x1.fffffffffffffp1023) r = 0.0;
/* Handle negative arguments: erfcx(x) = 2*exp(x*x) - erfcx(|x|) */
if (x < 0.0) {
s = x * x;
d = fma (x, x, -s);
e = exp (s);
r = e - r;
r = fma (e, d + d, r);
r = r + e;
if (e > 0x1.fffffffffffffp1023) r = e; // avoid creating NaN
}
return r;
}
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