/usr/include/libint2/boys.h is in libint2-dev 2.1.0~beta2-2.
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* This file is a part of Libint.
* Copyright (C) 2004-2014 Edward F. Valeev
*
* This program is free software: you can redistribute it and/or modify
* it under the terms of the GNU Library General Public License, version 2,
* as published by the Free Software Foundation.
*
* This program is distributed in the hope that it will be useful,
* but WITHOUT ANY WARRANTY; without even the implied warranty of
* MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the
* GNU General Public License for more details.
*
* You should have received a copy of the GNU Library General Public License
* along with this program. If not, see http://www.gnu.org/licenses/.
*
*/
// prototype for the Boys function engines (Boys function = Fm(T))
// the Chebyshev extrapolation code is based on that by Frank Neese
#ifndef _libint2_src_lib_libint_boys_h_
#define _libint2_src_lib_libint_boys_h_
#if defined(__cplusplus)
#include <iostream>
#include <cstdlib>
#include <cmath>
#include <stdexcept>
#include <libint2/vector.h>
#include <cassert>
#include <vector>
#include <algorithm>
// some features require at least C++11
#if __cplusplus > 199711L
#include <memory>
#endif
#if HAVE_LAPACK // use F77-type interface for now, switch to LAPACKE later
extern "C" void dgesv_(const int* n,
const int* nrhs, double* A, const int* lda,
int* ipiv, double* b, const int* ldb,
int* info);
#endif
namespace libint2 {
/// holds tables of expensive quantities
template<typename Real>
class ExpensiveNumbers {
public:
ExpensiveNumbers(int ifac = -1, int idf = -1, int ibc = -1) {
if (ifac >= 0) {
fac.resize(ifac + 1);
fac[0] = 1.0;
for (int i = 1; i <= ifac; i++) {
fac[i] = i * fac[i - 1];
}
}
if (idf >= 0) {
df.resize(idf + 1);
/* df[i] gives (i-1)!!, so that (-1)!! is defined... */
df[0] = 1.0;
if (idf >= 1)
df[1] = 1.0;
if (idf >= 2)
df[2] = 1.0;
for (int i = 3; i <= idf; i++) {
df[i] = (i - 1) * df[i - 2];
}
}
if (ibc >= 0) {
bc_.resize((ibc+1)*(ibc+1));
std::fill(bc_.begin(), bc_.end(), Real(0));
bc.resize(ibc+1);
bc[0] = &bc_[0];
for(int i=1; i<=ibc; ++i)
bc[i] = bc[i-1] + (ibc+1);
for(int i=0; i<=ibc; i++)
bc[i][0] = 1.0;
for(int i=0; i<=ibc; i++)
for(int j=1; j<=i; ++j)
bc[i][j] = bc[i][j-1] * Real(i-j+1) / Real(j);
}
for (int i = 0; i < 128; i++) {
twoi1[i] = 1.0 / (Real(2.0) * i + Real(1.0));
ihalf[i] = Real(i) - Real(0.5);
}
}
~ExpensiveNumbers() {
}
std::vector<Real> fac;
std::vector<Real> df;
std::vector<Real*> bc;
// these quantitites are needed with indices <= mmax
// 64 is sufficient to handle up to 4 center integrals with up to L=15 basis functions
// but need higher values for Yukawa integrals ...
Real twoi1[128]; /* 1/(2 i + 1); needed for downward recursion */
Real ihalf[128]; /* i - 0.5, needed for upward recursion */
private:
std::vector<Real> bc_;
};
#define _local_min_macro(a,b) ((a) > (b) ? (a) : (b))
/** Computes the Boys function, \f$ F_m (T) = \int_0^1 u^{2m} \exp(-T u^2) \, {\rm d}u \f$,
* using single algorithm (asymptotic expansion). Slow for the sake of precision control.
* Useful in two cases:
* <ul>
* <li> for reference purposes, if \c Real supports high/arbitrary precision, and </li>
* <li> for moderate values of \f$ T \f$, if \c Real is a low-precision floating-point type.
* N.B. FmEval_Reference2 , which can compute for all practical values of \f$ T \f$ and \f$ m \f$, is recommended
* with standard \c Real types (\c double and \c float). </li>
* </ul>
*
* \note Precision is controlled heuristically, i.e. cannot be guaranteed mathematically;
* will stop if absolute precision is reached, or precision of \c Real is exhausted.
* It is important that \c std::numeric_limits<Real> is defined appropriately.
*
* @tparam Real the type to use for all floating-point computations.
* Must be able to compute logarithm and exponential, i.e.
* log(x) and exp(x), where x is Real, must be valid expressions.
*/
template<typename Real>
struct FmEval_Reference {
/// computes a single value of \f$ F_m(T) \f$ using MacLaurin series.
static Real eval(Real T, size_t m, Real absolute_precision) {
assert(m < 100);
static const Real T_crit = std::numeric_limits<Real>::is_bounded == true ? -log( std::numeric_limits<Real>::min() * 100.5 / 2. ) : Real(0) ;
if (std::numeric_limits<Real>::is_bounded && T > T_crit)
throw std::overflow_error("FmEval_Reference<Real>::eval: Real lacks precision for the given value of argument T");
Real denom = (m + 0.5);
Real term = 0.5 * exp(-T) / denom;
Real old_term = 0.0;
Real sum = term;
//Real rel_error;
Real epsilon;
const Real relative_zero = std::numeric_limits<Real>::epsilon();
const Real absolute_precision_o_1000 = absolute_precision * 0.001;
do {
denom += 1.0;
old_term = term;
term = old_term * T / denom;
sum += term;
//rel_error = term / sum;
// stop if adding a term smaller or equal to absolute_precision/1000 and smaller than relative_zero * sum
// When sum is small in absolute value, the second threshold is more important
epsilon = _local_min_macro(absolute_precision_o_1000, sum*relative_zero);
} while (term > epsilon || old_term < term);
return sum;
}
/// fills up an array of Fm(T) for m in [0,mmax]
/// @param[out] Fm array to be filled in with the Boys function values, must be at least mmax+1 elements long
/// @param[in] T the Boys function argument
/// @param[in] mmax the maximum value of m for which Boys function will be computed;
/// @param[in] absolute_precision the absolute precision to which to compute the result
static void eval(Real* Fm, Real T, size_t mmax, Real absolute_precision) {
// evaluate for mmax using MacLaurin series
// it converges fastest for the largest m -> use it to compute Fmmax(T)
// see JPC 94, 5564 (1990).
for(size_t m=0; m<=mmax; ++m)
Fm[m] = eval(T, m, absolute_precision);
return;
/** downward recursion does not maintain absolute precision, only relative precision, and cannot be used for T > 10
if (mmax > 0) {
const Real T2 = 2.0 * T;
const Real exp_T = exp(-T);
for (int m = mmax - 1; m >= 0; m--)
Fm[m] = (Fm[m + 1] * T2 + exp_T) / (2 * m + 1);
}
*/
}
};
/** Computes the Boys function, \$ F_m (T) = \int_0^1 u^{2m} \exp(-T u^2) \, {\rm d}u \$,
* using multi-algorithm approach (upward precision for T>=30, and asymptotic summation for T<30).
* This is slow and should be used for reference purposes, e.g. computing the interpolation tables.
* Precision is not always guaranteed as it is limited by the precision of \c Real type.
* When \c Real is \c double, can maintain 1e-14 precision for up to m=38 and 0<=T<=1e9 .
*
* @tparam Real the type to use for all floating-point computations.
* Must be able to compute logarithm, exponential, square root, and error function, i.e.
* log(x), exp(x), sqrt(x), and erf(x), where x is Real, must be valid expressions.
*/
template<typename Real>
struct FmEval_Reference2 {
/// fills up an array of Fm(T) for m in [0,mmax]
/// @param[out] Fm array to be filled in with the Boys function values, must be at least mmax+1 elements long
/// @param[in] t the Boys function argument
/// @param[in] mmax the maximum value of m for which Boys function will be computed;
/// @param[in] absolute_precision the absolute precision to which to compute the result
static void eval(Real* Fm, Real t, size_t mmax, Real absolute_precision) {
if (t < Real(30)) {
FmEval_Reference<Real>::eval(Fm,t,mmax,absolute_precision);
}
else {
const Real two_over_sqrt_pi{1.128379167095512573896158903121545171688101258657997713688171443421284936882986828973487320404214727};
const Real K = 1.0/two_over_sqrt_pi;
auto t2 = 2*t;
auto et = exp(-t);
auto sqrt_t = sqrt(t);
Fm[0] = K*erf(sqrt_t)/sqrt_t;
if (mmax > 0)
for(size_t m=0; m<=mmax-1; m++) {
Fm[m+1] = ((2*m + 1)*Fm[m] - et)/(t2);
}
}
}
};
/** Computes the Boys function, \$ F_m (T) = \int_0^1 u^{2m} \exp(-T u^2) \, {\rm d}u \$,
* using Chebyshev interpolation.
* based on the code from ORCA by Dr. Frank Neese.
*/
template <typename Real = double>
class FmEval_Chebyshev3 {
static const int NGRID = 4096; //!< number of grid points
static const int INTERPOLATION_ORDER = 4; //!< interpolation order + 1
static const bool INTERPOLATION_AND_RECURSION = false; //!< compute F_lmax(T) and then iterate down to F_0(T)? Else use interpolation only
const Real T_crit; //!< critical value of T above which safe to use upward recusion
const Real delta; //!< grid size
const Real one_over_delta; //! 1/delta
int mmax; //!< the maximum m that is tabulated
ExpensiveNumbers<double> numbers_;
Real *c; /* the Chebyshev coefficients table, NGRID by mmax*interpolation_order */
public:
/// \param m_max maximum value of the Boys function index; set to -1 to skip initialization
/// \param precision the desired precision
FmEval_Chebyshev3(int m_max, double = 0.0) :
T_crit(30.0), // this translates in appr. 1e-15 error in upward recursion, see the note below
delta(T_crit / (NGRID - 1)),
one_over_delta(1.0 / delta),
mmax(m_max), numbers_(14, 0) {
assert(mmax <= 63);
if (m_max >= 0)
init();
}
~FmEval_Chebyshev3() {
if (mmax >= 0) {
free(c);
}
}
// some features require at least C++11
#if __cplusplus > 199711L
/// Singleton interface allows to manage the lone instance; adjusts max m values as needed in thread-safe fashion
static const std::shared_ptr<FmEval_Chebyshev3>& instance(int m_max, double = 0.0) {
// thread-safe per C++11 standard [6.7.4]
static std::shared_ptr<FmEval_Chebyshev3> instance_ = 0;
const bool need_new_instance = !instance_ || (instance_ && instance_->max_m() < m_max);
if (need_new_instance) {
auto new_instance = std::make_shared<FmEval_Chebyshev3>(m_max);
instance_ = new_instance; // thread-safe
}
return instance_;
}
#endif
/// @return the maximum value of m for which the Boys function can be computed with this object
int max_m() const { return mmax; }
/// fills in Fm with computed Boys function values for m in [0,mmax]
/// @param[out] Fm array to be filled in with the Boys function values, must be at least mmax+1 elements long
/// @param[in] x the Boys function argument
/// @param[in] mmax the maximum value of m for which Boys function will be computed; mmax must be <= the value returned by max_m
inline void eval(Real* Fm, Real x, int m_max) const {
// large T => use upward recursion
// cost = 1 div + 1 sqrt + (1 + 2*(m-1)) muls
if (x > T_crit) {
const double one_over_x = 1.0/x;
Fm[0] = 0.88622692545275801365 * sqrt(one_over_x); // see Eq. (9.8.9) in Helgaker-Jorgensen-Olsen
if (m_max == 0)
return;
// this upward recursion formula omits - e^(-x)/(2x), which for x>T_crit is <1e-15
for (int i = 1; i <= m_max; i++)
Fm[i] = Fm[i - 1] * numbers_.ihalf[i] * one_over_x; // see Eq. (9.8.13)
return;
}
// ---------------------------------------------
// small and intermediate arguments => interpolate Fm and (optional) downward recursion
// ---------------------------------------------
// about which point on the grid to interpolate?
const double xd = x * one_over_delta;
const int iv = int(xd); // the interval
// INTERPOLATION_AND_RECURSION== true? evaluate by interpolation for LARGEST m only
// INTERPOLATION_AND_RECURSION==false? evaluate by interpolation for ALL m
const int m_min = INTERPOLATION_AND_RECURSION ? m_max : 0;
#if defined(__AVX__) || defined(__SSE2__)
const auto x2 = xd*xd;
const auto x3 = x2*xd;
# if defined (__AVX__)
libint2::simd::VectorAVXDouble xvec(1., xd, x2, x3);
# else // defined(__SSE2__)
libint2::simd::VectorSSEDouble x0vec(1., xd);
libint2::simd::VectorSSEDouble x1vec(x2, x3);
# endif
#endif // SSE2 || AVX
const Real *d = c + INTERPOLATION_ORDER * (iv * (mmax+1) + m_min); // ptr to the interpolation data for m=mmin
int m = m_min;
#if defined(__AVX__)
if (m_max-m >=3) {
const int unroll_size = 4;
const int m_fence = (m_max + 2 - unroll_size);
for(; m<m_fence; m+=unroll_size, d+=INTERPOLATION_ORDER*unroll_size) {
libint2::simd::VectorAVXDouble d0v, d1v, d2v, d3v;
d0v.load_aligned(d);
d1v.load_aligned(d+INTERPOLATION_ORDER);
d2v.load_aligned(d+2*INTERPOLATION_ORDER);
d3v.load_aligned(d+3*INTERPOLATION_ORDER);
libint2::simd::VectorAVXDouble fm0 = d0v * xvec;
libint2::simd::VectorAVXDouble fm1 = d1v * xvec;
libint2::simd::VectorAVXDouble fm2 = d2v * xvec;
libint2::simd::VectorAVXDouble fm3 = d3v * xvec;
libint2::simd::VectorAVXDouble sum0123 = horizontal_add(fm0, fm1, fm2, fm3);
sum0123.convert(&Fm[m]);
}
} // unroll_size=4
if (m_max-m >=1) {
const int unroll_size = 2;
const int m_fence = (m_max + 2 - unroll_size);
for(; m<m_fence; m+=unroll_size, d+=INTERPOLATION_ORDER*unroll_size) {
libint2::simd::VectorAVXDouble d0v, d1v;
d0v.load_aligned(d);
d1v.load_aligned(d+INTERPOLATION_ORDER);
libint2::simd::VectorAVXDouble fm0 = d0v * xvec;
libint2::simd::VectorAVXDouble fm1 = d1v * xvec;
libint2::simd::VectorSSEDouble sum01 = horizontal_add(fm0, fm1);
sum01.convert(&Fm[m]);
}
} // unroll_size=2
{ // no unrolling
for(; m<=m_max; ++m, d+=INTERPOLATION_ORDER) {
libint2::simd::VectorAVXDouble dvec;
dvec.load_aligned(d);
libint2::simd::VectorAVXDouble fm_prereduce = dvec * xvec;
Fm[m] = horizontal_add(fm_prereduce);
}
}
#elif defined(__SSE2__)
if (m_max-m >=1) {
const int unroll_size = 2;
const int m_fence = (m_max + 2 - unroll_size);
for(; m<m_fence; m+=unroll_size, d+=INTERPOLATION_ORDER*unroll_size) {
libint2::simd::VectorSSEDouble d00v, d01v, d10v, d11v;
d00v.load_aligned(d);
d01v.load_aligned(d+2);
d10v.load_aligned(d+4); // d + INTERPOLATION_ORDER
d11v.load_aligned(d+6);
libint2::simd::VectorSSEDouble fm00 = d00v * x0vec;
libint2::simd::VectorSSEDouble fm01 = d01v * x1vec;
libint2::simd::VectorSSEDouble fm10 = d10v * x0vec;
libint2::simd::VectorSSEDouble fm11 = d11v * x1vec;
libint2::simd::VectorSSEDouble sum01 = horizontal_add(fm00, fm10) + horizontal_add(fm01, fm11);
sum01.convert(&Fm[m]);
}
} // unroll_size=2
{ // no unrolling
for(; m<=m_max; ++m, d+=INTERPOLATION_ORDER) {
libint2::simd::VectorSSEDouble d0vec, d1vec;
d0vec.load_aligned(d);
d1vec.load_aligned(d+2);
Fm[m] = horizontal_add(d0vec * x0vec + d1vec * x1vec);
}
}
#else // not SSE2 nor AVX available
for(int m=m_min; m<=m_max; ++m, d+=INTERPOLATION_ORDER) {
Fm[m] = d[0]
+ xd * (d[1] + xd * (d[2] + xd * d[3]));
// // check against the reference value
// if (false) {
// double refvalue = FmEval_Reference2<double>::eval(x, m, 1e-15); // compute F(T)
// if (abs(refvalue - Fm[m]) > 1e-10) {
// std::cout << "T = " << x << " m = " << m << " cheb = "
// << Fm[m] << " ref = " << refvalue << std::endl;
// }
// }
}
#endif
// use downward recursion (Eq. (9.8.14) in HJO)
// WARNING: do not turn this on ... on modern CPU exp is very slow
if (INTERPOLATION_AND_RECURSION && m_max > 0) {
const bool INTERPOLATION_AND_RECURSION_is_slow_on_modern_CPU = false;
assert(INTERPOLATION_AND_RECURSION_is_slow_on_modern_CPU);
const Real x2 = 2.0 * x;
const Real exp_x = exp(-x);
for (int m = m_max - 1; m >= 0; m--)
Fm[m] = (Fm[m + 1] * x2 + exp_x) * numbers_.twoi1[m];
}
}
private:
/* ----------------------------------------------------------------------------
This function here creates the expansion coefficients for a single interval
ON INPUT a,b : the interval boundaries
cc : a pointer to the appropriate place in
the coefficient table
m : the F[m] to generate
ON OUTPUT cc : cc[0]-cc[3] hold the coefficients
---------------------------------------------------------------------------- */
void MakeCoeffs(double a, double b, Real *cc, int m) {
int k, j;
double f[128], ac[128], Fm[128];
double sum;
// characterize the interval
double TwoDelta = b - a;
double Delta = 0.5 * TwoDelta;
double HalfDelta = 0.5 * Delta;
double XXX = a + Delta;
const double absolute_precision = 1e-100; // compute as precisely as possible
FmEval_Reference2<double>::eval(Fm, XXX, m + INTERPOLATION_ORDER + 20,
absolute_precision);
for (k = 0; k <= INTERPOLATION_ORDER + 20; k++) {
if ((k % 2) == 0)
f[k] = Fm[k + m];
else
f[k] = -Fm[k + m];
}
// calculate the coefficients a
double fac;
for (j = 0; j < INTERPOLATION_ORDER; j++) {
if (j == 0)
fac = 1.0;
else
fac = 2.0 * pow(HalfDelta, (double) j);
sum = 0.0;
for (k = 0; k < 10; k++)
sum += f[j + 2 * k] * pow(HalfDelta, (double) (2 * k)) / numbers_.fac[k]
/ numbers_.fac[k + j];
ac[j] = fac * sum;
}
// calculate the coefficients c that are Gill's f's
double arg = -XXX / Delta;
double arg2 = arg * arg;
double arg3 = arg2 * arg;
auto cc0 = (ac[0] - ac[2]) + (ac[1] - 3.0 * ac[3]) * arg
+ 2.0 * ac[2] * arg2 + 4.0 * ac[3] * arg3;
auto cc1 = (2.0 * ac[1] - 6.0 * ac[3]) + 8.0 * ac[2] * arg
+ 24.0 * ac[3] * arg2;
auto cc2 = 8.0 * ac[2] + 48.0 * ac[3] * arg;
auto cc3 = 32.0 * ac[3];
cc[0] = cc0;
cc[1] = cc1;
cc[2] = cc2;
cc[3] = cc3;
}
/* ----------------------------------------------------------------------------
This function makes the expansion coefficients for all intervals
ON INPUT m : the highest F[m] to generate
ON OUTPUT c : the coefficients c[m][i] are generated
---------------------------------------------------------------------------- */
void init() {
int iv, im;
// get memory
void* result;
posix_memalign(&result, 4*sizeof(Real), (mmax + 1) * NGRID * INTERPOLATION_ORDER * sizeof(Real));
c = static_cast<Real*>(result);
// make expansion coefficients for each grid value of T
for (iv = 0; iv < NGRID; iv++) {
const auto a = iv * delta;
const auto b = a + delta;
// loop over all m values and make the coefficients
for (im = 0; im <= mmax; im++) {
MakeCoeffs(a, b, c + (iv * (mmax+1) + im) * INTERPOLATION_ORDER, im);
}
}
}
};
#ifndef STATIC_OON
#define STATIC_OON
namespace {
const double oon[] = {0.0, 1.0, 1.0/2.0, 1.0/3.0, 1.0/4.0, 1.0/5.0, 1.0/6.0, 1.0/7.0, 1.0/8.0, 1.0/9.0, 1.0/10.0, 1.0/11.0};
}
#endif
/** Computes the Boys function, \$ F_m (T) = \int_0^1 u^{2m} \exp(-T u^2) \, {\rm d}u \$,
* using Taylor interpolation of up to 8-th order.
* @tparam Real the type to use for all floating-point computations. Must support std::exp, std::pow, std::fabs, std::max, and std::floor.
* @tparam INTERPOLATION_ORDER the interpolation order. The higher the order the less memory this object will need, but the computational cost will increase (usually very slightly)
*/
template<typename Real = double, int INTERPOLATION_ORDER = 7>
class FmEval_Taylor {
public:
static const int max_interp_order = 8;
static const bool INTERPOLATION_AND_RECURSION = false; // compute F_lmax(T) and then iterate down to F_0(T)? Else use interpolation only
const double soft_zero_;
/// Constructs the object to be able to compute Boys funcion for m in [0,mmax], with relative \c precision
FmEval_Taylor(unsigned int mmax, Real precision) :
soft_zero_(1e-6), cutoff_(precision), numbers_(
INTERPOLATION_ORDER + 1, 2 * (mmax + INTERPOLATION_ORDER - 1)) {
assert(mmax <= 63);
const double sqrt_pi = std::sqrt(M_PI);
/*---------------------------------------
We are doing Taylor interpolation with
n=TAYLOR_ORDER terms here:
error <= delT^n/(n+1)!
---------------------------------------*/
delT_ = 2.0
* std::pow(cutoff_ * numbers_.fac[INTERPOLATION_ORDER + 1],
1.0 / INTERPOLATION_ORDER);
oodelT_ = 1.0 / delT_;
max_m_ = mmax + INTERPOLATION_ORDER - 1;
T_crit_ = new Real[max_m_ + 1]; /*--- m=0 is included! ---*/
max_T_ = 0;
/*--- Figure out T_crit for each m and put into the T_crit ---*/
for (int m = max_m_; m >= 0; --m) {
/*------------------------------------------
Damped Newton-Raphson method to solve
T^{m-0.5}*exp(-T) = epsilon*Gamma(m+0.5)
The solution is the max T for which to do
the interpolation
------------------------------------------*/
double T = -log(cutoff_);
const double egamma = cutoff_ * sqrt_pi * numbers_.df[2 * m]
/ std::pow(2.0, m);
double T_new = T;
double func;
do {
const double damping_factor = 0.2;
T = T_new;
/* f(T) = the difference between LHS and RHS of the equation above */
func = std::pow(T, m - 0.5) * std::exp(-T) - egamma;
const double dfuncdT = ((m - 0.5) * std::pow(T, m - 1.5)
- std::pow(T, m - 0.5)) * std::exp(-T);
/* f(T) has 2 roots and has a maximum in between. If f'(T) > 0 we are to the left of the hump. Make a big step to the right. */
if (dfuncdT > 0.0) {
T_new *= 2.0;
} else {
/* damp the step */
double deltaT = -func / dfuncdT;
const double sign_deltaT = (deltaT > 0.0) ? 1.0 : -1.0;
const double max_deltaT = damping_factor * T;
if (std::fabs(deltaT) > max_deltaT)
deltaT = sign_deltaT * max_deltaT;
T_new = T + deltaT;
}
if (T_new <= 0.0) {
T_new = T / 2.0;
}
} while (std::fabs(func / egamma) >= soft_zero_);
T_crit_[m] = T_new;
const int T_idx = (int) std::floor(T_new / delT_);
max_T_ = std::max(max_T_, T_idx);
}
// allocate the grid (see the comments below)
{
const int nrow = max_T_ + 1;
const int ncol = max_m_ + 1;
grid_ = new Real*[nrow];
grid_[0] = new Real[nrow * ncol];
//std::cout << "Allocated interpolation table of " << nrow * ncol << " reals" << std::endl;
for (int r = 1; r < nrow; ++r)
grid_[r] = grid_[r - 1] + ncol;
}
/*-------------------------------------------------------
Tabulate the gamma function from t=delT to T_crit[m]:
1) include T=0 though the table is empty for T=0 since
Fm(0) is simple to compute
-------------------------------------------------------*/
/*--- do the mmax first ---*/
for (int T_idx = max_T_; T_idx >= 0; --T_idx) {
const double T = T_idx * delT_;
libint2::FmEval_Reference2<double>::eval(grid_[T_idx], T, max_m_, 1e-100);
}
}
~FmEval_Taylor() {
delete[] T_crit_;
delete[] grid_[0];
delete[] grid_;
}
// some features require at least C++11
#if __cplusplus > 199711L
/// Singleton interface allows to manage the lone instance;
/// adjusts max m and precision values as needed in thread-safe fashion
static const std::shared_ptr<FmEval_Taylor>& instance(unsigned int mmax, Real precision) {
// thread-safe per C++11 standard [6.7.4]
static std::shared_ptr<FmEval_Taylor> instance_ = 0;
const bool need_new_instance = !instance_ ||
(instance_ && (instance_->max_m() < mmax ||
instance_->precision() > precision));
if (need_new_instance) {
auto new_instance = std::make_shared<FmEval_Taylor>(mmax, precision);
instance_ = new_instance; // thread-safe
}
return instance_;
}
#endif
/// @return the maximum value of m for which this object can compute the Boys function
int max_m() const { return max_m_ - INTERPOLATION_ORDER + 1; }
/// @return the precision with which this object can compute the Boys function
Real precision() const { return cutoff_; }
/// computes Boys function values with m index in range [0,mmax]
/// @param[out] Fm array to be filled in with the Boys function values, must be at least mmax+1 elements long
/// @param[in] x the Boys function argument
/// @param[in] mmax the maximum value of m for which Boys function will be computed;
/// it must be <= the value returned by max_m() (this is not checked)
void eval(Real* Fm, Real T, int mmax) const {
const double sqrt_pio2 = 1.2533141373155002512;
const double two_T = 2.0 * T;
// stop recursion at mmin
const int mmin = INTERPOLATION_AND_RECURSION ? mmax : 0;
/*-------------------------------------
Compute Fm(T) from mmax down to mmin
-------------------------------------*/
const bool use_upward_recursion = true;
if (use_upward_recursion) {
// if (T > 30.0) {
if (T > T_crit_[0]) {
const double one_over_x = 1.0/T;
Fm[0] = 0.88622692545275801365 * sqrt(one_over_x); // see Eq. (9.8.9) in Helgaker-Jorgensen-Olsen
if (mmax == 0)
return;
// this upward recursion formula omits - e^(-x)/(2x), which for x>T_crit is <1e-15
for (int i = 1; i <= mmax; i++)
Fm[i] = Fm[i - 1] * numbers_.ihalf[i] * one_over_x; // see Eq. (9.8.13)
return;
}
}
// since Tcrit grows with mmax, this condition only needs to be determined once
if (T > T_crit_[mmax]) {
double pow_two_T_to_minusjp05 = std::pow(two_T, -mmax - 0.5);
for (int m = mmax; m >= mmin; --m) {
/*--- Asymptotic formula ---*/
Fm[m] = numbers_.df[2 * m] * sqrt_pio2 * pow_two_T_to_minusjp05;
pow_two_T_to_minusjp05 *= two_T;
}
}
else
{
const int T_ind = (int) (0.5 + T * oodelT_);
const Real h = T_ind * delT_ - T;
const Real* F_row = grid_[T_ind] + mmin;
#if defined (__AVX__)
libint2::simd::VectorAVXDouble h0123, h4567;
if (INTERPOLATION_ORDER == 3 || INTERPOLATION_ORDER == 7) {
const double h2 = h*h*oon[2];
const double h3 = h2*h*oon[3];
h0123 = libint2::simd::VectorAVXDouble (1.0, h, h2, h3);
if (INTERPOLATION_ORDER == 7) {
const double h4 = h3*h*oon[4];
const double h5 = h4*h*oon[5];
const double h6 = h5*h*oon[6];
const double h7 = h6*h*oon[7];
h4567 = libint2::simd::VectorAVXDouble (h4, h5, h6, h7);
}
}
// libint2::simd::VectorAVXDouble h0123(1.0);
// libint2::simd::VectorAVXDouble h4567(1.0);
#endif
int m = mmin;
if (mmax-m >=1) {
const int unroll_size = 2;
const int m_fence = (mmax + 2 - unroll_size);
for(; m<m_fence; m+=unroll_size, F_row+=unroll_size) {
#if defined(__AVX__)
if (INTERPOLATION_ORDER == 3 || INTERPOLATION_ORDER == 7) {
libint2::simd::VectorAVXDouble fr0_0123; fr0_0123.load(F_row);
libint2::simd::VectorAVXDouble fr1_0123; fr1_0123.load(F_row+1);
libint2::simd::VectorSSEDouble fm01 = horizontal_add(fr0_0123*h0123, fr1_0123*h0123);
if (INTERPOLATION_ORDER == 7) {
libint2::simd::VectorAVXDouble fr0_4567; fr0_4567.load(F_row+4);
libint2::simd::VectorAVXDouble fr1_4567; fr1_4567.load(F_row+5);
fm01 += horizontal_add(fr0_4567*h4567, fr1_4567*h4567);
}
fm01.convert(&Fm[m]);
}
else {
#endif
Real total0 = 0.0, total1 = 0.0;
for(int i=INTERPOLATION_ORDER; i>=1; --i) {
total0 = oon[i]*h*(F_row[i] + total0);
total1 = oon[i]*h*(F_row[i+1] + total1);
}
Fm[m] = F_row[0] + total0;
Fm[m+1] = F_row[1] + total1;
#if defined(__AVX__)
}
#endif
}
} // unroll_size = 2
if (m<=mmax) { // unroll_size = 1
#if defined(__AVX__)
if (INTERPOLATION_ORDER == 3 || INTERPOLATION_ORDER == 7) {
libint2::simd::VectorAVXDouble fr0123; fr0123.load(F_row);
if (INTERPOLATION_ORDER == 7) {
libint2::simd::VectorAVXDouble fr4567; fr4567.load(F_row+4);
libint2::simd::VectorSSEDouble fm = horizontal_add(fr0123*h0123, fr4567*h4567);
Fm[m] = horizontal_add(fm);
}
else { // INTERPOLATION_ORDER == 3
Fm[m] = horizontal_add(fr0123*h0123);
}
}
else {
#endif
Real total = 0.0;
for(int i=INTERPOLATION_ORDER; i>=1; --i) {
total = oon[i]*h*(F_row[i] + total);
}
Fm[m] = F_row[0] + total;
#if defined(__AVX__)
}
#endif
} // unroll_size = 1
// check against the reference value
// if (false) {
// double refvalue = FmEval_Reference2<double>::eval(T, mmax, 1e-15); // compute F(T) with m=mmax
// if (abs(refvalue - Fm[mmax]) > 1e-14) {
// std::cout << "T = " << T << " m = " << mmax << " cheb = "
// << Fm[mmax] << " ref = " << refvalue << std::endl;
// }
// }
} // if T < T_crit
/*------------------------------------
And then do downward recursion in j
------------------------------------*/
if (INTERPOLATION_AND_RECURSION && mmin > 0) {
const Real exp_mT = std::exp(-T);
for (int m = mmin - 1; m >= 0; --m) {
Fm[m] = (exp_mT + two_T * Fm[m+1]) * numbers_.twoi1[m];
}
}
}
private:
Real **grid_; /* Table of "exact" Fm(T) values. Row index corresponds to
values of T (max_T+1 rows), column index to values
of m (max_m+1 columns) */
Real delT_; /* The step size for T, depends on cutoff */
Real oodelT_; /* 1.0 / delT_, see above */
Real cutoff_; /* Tolerance cutoff used in all computations of Fm(T) */
int max_m_; /* Maximum value of m in the table, depends on cutoff
and the number of terms in Taylor interpolation */
int max_T_; /* Maximum index of T in the table, depends on cutoff
and m */
Real *T_crit_; /* Maximum T for each row, depends on cutoff;
for a given m and T_idx <= max_T_idx[m] use Taylor interpolation,
for a given m and T_idx > max_T_idx[m] use the asymptotic formula */
ExpensiveNumbers<double> numbers_;
/**
* Power series estimate of the error introduced by replacing
* \f$ F_m(T) = \int_0^1 \exp(-T t^2) t^{2 m} \, \mathrm{d} t \f$ with analytically
* integrable \f$ \int_0^\infty \exp(-T t^2) t^{2 m} \, \mathrm{d} t = \frac{(2m-1)!!}{2^{m+1}} \sqrt{\frac{\pi}{T^{2m+1}}} \f$
* @param m
* @param T
* @return the error estimate
*/
static double truncation_error(unsigned int m, double T) {
const double m2= m * m;
const double m3= m2 * m;
const double m4= m2 * m2;
const double T2= T * T;
const double T3= T2 * T;
const double T4= T2 * T2;
const double T5= T2 * T3;
const double result = exp(-T) * (105 + 16*m4 + 16*m3*(T - 8) - 30*T + 12*T2
- 8*T3 + 16*T4 + 8*m2*(43 - 9*T + 2*T2) +
4*m*(-88 + 23*T - 8*T2 + 4*T3))/(32*T5);
return result;
}
/**
* Leading-order estimate of the error introduced by replacing
* \f$ F_m(T) = \int_0^1 \exp(-T t^2) t^{2 m} \, \mathrm{d} t \f$ with analytically
* integrable \f$ \int_0^\infty \exp(-T t^2) t^{2 m} \, \mathrm{d} t = \frac{(2m-1)!!}{2^{m+1}} \sqrt{\frac{\pi}{T^{2m+1}}} \f$
* @param m
* @param T
* @return the error estimate
*/
static double truncation_error(double T) {
const double result = exp(-T) /(2*T);
return result;
}
};
//////////////////////////////////////////////////////////
/// core integral for Yukawa and exponential interactions
//////////////////////////////////////////////////////////
#if 0
/**
* Evaluates core integral for the Yukawa potential \f$ \exp(- \zeta r) / r \f$
* @tparam Real real type
*/
template<typename Real>
struct YukawaGmEval {
static const int mmin = -1;
///
YukawaGmEval(unsigned int mmax, Real precision) :
mmax_(mmax), precision_(precision),
numbers_(),
Gm_0_U_(256) // should be enough to hold up to G_{255}(0,U)
{ }
unsigned int max_m() const { return mmax; }
/// @return the precision with which this object can compute the result
Real precision() const { return precision_; }
///
void eval_yukawa(Real* Gm, Real T, Real U, size_t mmax, Real absolute_precision) {
assert(false); // not yet implemented
}
///
void eval_slater(Real* Gm, Real T, Real U, size_t mmax, Real absolute_precision) {
assert(false); // not yet implemented
}
/// Scheme 1 of Ten-no: upward recursion from \f$ G_{-1} (T,U) \f$ and \f$ G_0 (T,U) \f$
/// T must be non-zero!
/// @param[out] Gm \f$ G_m(T,U), m=-1..mmax \f$
static void eval_yukawa_s1(Real* Gm, Real T, Real U, size_t mmax) {
Real G_m1;
const Real sqrt_U = sqrt(U);
const Real sqrt_T = sqrt(T);
const Real oo_sqrt_T = 1 / sqrt_T;
const Real oo_sqrt_U = 1 / sqrt_U;
const Real exp_mT = exp(-T);
const Real kappa = sqrt_U - sqrt_T;
const Real lambda = sqrt_U + sqrt_T;
const Real sqrtPi_over_4(0.44311346272637900682454187083528629569938736403060);
const Real pfac = sqrtPi_over_4 * exp_mT;
const Real erfc_k = exp(kappa*kappa) * (1 - erf(kappa));
const Real erfc_l = exp(lambda*lambda) * (1 - erf(lambda));
Gm[0] = pfac * (erfc_k + erfc_l) * oo_sqrt_U;
Gm[1] = pfac * (erfc_k - erfc_l) * oo_sqrt_T;
if (mmax > 0) {
// first application of URR
const Real oo_two_T = 0.5 / T;
const Real two_U = 2.0 * U;
for(unsigned int m=1, two_m_minus_1=1; m<=mmax; ++m, two_m_minus_1+=2) {
Gm[m+1] = oo_two_T * ( two_m_minus_1 * Gm[m] + two_U * Gm[m-1] - exp_mT);
}
}
return;
}
/// Scheme 2 of Ten-no:
/// - evaluate G_m(0,U) for m = mmax ... mmax+n, where n is the number of terms in Maclaurin expansion
/// how? see eval_yukawa_Gm0U
/// - then MacLaurin expansion for \f$ G_{m_{\rm max}}(T,U) \f$ and \f$ G_{m_{\rm max}-1}(T,U) \f$
/// - then downward recursion
/// @param[out] Gm \f$ G_m(T,U), m=-1..mmax \f$
void eval_yukawa_s2(Real* Gm, Real T, Real U, size_t mmax) {
// TODO estimate the number of expansion terms for the given precision
const int expansion_order = 60;
eval_yukawa_Gm0U(Gm_0_U_, U, mmax - 1 + expansion_order);
// Maclaurin
// downward recursion
//Gm[m + 1] = 1/(2 U) (E^-T - (2 m + 3) Gm[[m + 2]] + 2 T Gm[[m + 3]])
const Real one_over_twoU = 0.5 / U;
const Real one_over_twoU = 2.0 * T;
const Real exp_mT = exp(-T);
for(int m=mmax-2; m>=-1; --m)
Gm[m] = one_over_twoU (exp_mT - numbers_.twoi1[m+1] * Gm[m+1] + twoT Gm[m+2])
// testing ...
std::copy(Gm_0_U_.begin()+1, Gm_0_U_.begin()+mmax+2, Gm);
return;
}
/// Scheme 3 of Ten-no:
/// - evaluate G_m(0,U) for m = 0 ... mmax+n, where n is the max order of terms in Maclaurin expansion
/// how? see eval_yukawa_Gm0U
/// - then MacLaurin expansion for \f$ G_{m}(T,U) \f$ for m = 0 ... mmax
/// @param[out] Gm \f$ G_m(T,U), m=-1..mmax \f$
void eval_yukawa_s3(Real* Gm, Real T, Real U, size_t mmax) {
// Ten-no's prescription:
//
assert(false);
// testing ...
std::copy(Gm_0_U_.begin()+1, Gm_0_U_.begin()+mmax+2, Gm);
return;
}
/**
* computes prerequisites for MacLaurin expansion of Gm(T,U)
* for m in [-1,mmax); uses Ten-no's prescription, i.e.
*
*
* @param[out] Gm0U
* @param[in] U
* @param[in] mmax
*/
void eval_yukawa_Gm0U(Real* Gm0U, Real U, int mmax, int mmin = -1) {
// Ten-no's prescription:
// start with Gm*(0,T)
// 1) for U < 5, m* = -1
// 2) for U > 5, m* = min(U,mmax)
int mstar;
// G_{-1} (0,U) is easy
if (U < 5.0) {
mstar = -1;
const Real sqrt_U = sqrt(U);
const Real exp_U = exp(U);
const Real oo_sqrt_U = 1 / sqrt_U;
const Real sqrtPi_over_2(
0.88622692545275801364908374167057259139877472806119);
const Real pfac = sqrtPi_over_2 * exp_U;
const Real erfc_sqrt_U = 1.0 - erf(sqrt_U);
Gm_0_U_[0] = pfac * exp_U * oo_sqrt_U * erfc_sqrt_U;
// can get G0 for "free"
// this is the l'Hopital-transformed expression for G_0 (0,T)
// const Real sqrtPi(
// 1.7724538509055160272981674833411451827975494561224);
// Gm_0_U_[1] = 1.0 - exp_U * sqrtPi * sqrt_U * erfc_sqrt_U;
}
else { // use continued fraction for m*
mstar = std::min((size_t)U,(size_t)mmax);
const bool implemented = false;
assert(implemented == true);
}
{ // use recursion if needed
const Real two_U = 2.0 * U;
// simplified URR
if (mmax > mstar) {
for(int m=mstar+1; m<=mmax; ++m) {
Gm_0_U_[m+1] = numbers_.twoi1[m] * (1.0 - two_U * Gm_0_U_[m]);
}
}
// simplified DRR
if (mstar > mmin) { // instead of -1 because we trigger this only for U > 5
const Real one_over_U = 2.0 / two_U;
for(int m=mstar-1; m>=mmin; --m) {
Gm_0_U_[m+1] = one_over_U * ( 0.5 - numbers_.ihalf[m+2] * Gm_0_U_[m+2]);
}
}
}
// testing ...
std::copy(Gm_0_U_.begin()+1, Gm_0_U_.begin()+mmax+2, Gm0U);
return;
}
/// computes a single value of G_{-1}(T,U)
static Real eval_Gm1(Real T, Real U) {
const Real sqrt_U = sqrt(U);
const Real sqrt_T = sqrt(T);
const Real exp_mT = exp(-T);
const Real kappa = sqrt_U - sqrt_T;
const Real lambda = sqrt_U + sqrt_T;
const Real sqrtPi_over_4(0.44311346272637900682454187083528629569938736403060);
const Real result = sqrtPi_over_4 * exp_mT *
(exp(kappa*kappa) * (1 - erf(kappa)) + exp(lambda*lambda) * (1 - erf(lambda))) / sqrt_U;
return result;
}
/// computes a single value of G_0(T,U)
static Real eval_G0(Real T, Real U) {
const Real sqrt_U = sqrt(U);
const Real sqrt_T = sqrt(T);
const Real exp_mT = exp(-T);
const Real kappa = sqrt_U - sqrt_T;
const Real lambda = sqrt_U + sqrt_T;
const Real sqrtPi_over_4(0.44311346272637900682454187083528629569938736403060);
const Real result = sqrtPi_over_4 * exp_mT *
(exp(kappa*kappa) * (1 - erf(kappa)) - exp(lambda*lambda) * (1 - erf(lambda))) / sqrt_T;
return result;
}
/// computes \f$ G_{-1}(T,U) \f$ and \f$ G_{0}(T,U) \f$ , both are needed for Yukawa and Slater integrals
/// @param[out] result result[0] contains \f$ G_{-1}(T,U) \f$, result[1] contains \f$ G_{0}(T,U) \f$
static void eval_G_m1_0(Real* result, Real T, Real U) {
const Real sqrt_U = sqrt(U);
const Real sqrt_T = sqrt(T);
const Real oo_sqrt_U = 1 / sqrt_U;
const Real oo_sqrt_T = 1 / sqrt_T;
const Real exp_mT = exp(-T);
const Real kappa = sqrt_U - sqrt_T;
const Real lambda = sqrt_U + sqrt_T;
const Real sqrtPi_over_4(0.44311346272637900682454187083528629569938736403060);
const Real pfac = sqrtPi_over_4 * exp_mT;
const Real erfc_k = exp(kappa*kappa) * (1 - erf(kappa));
const Real erfc_l = exp(lambda*lambda) * (1 - erf(lambda));
result[0] = pfac * (erfc_k + erfc_l) * oo_sqrt_U;
result[1] = pfac * (erfc_k - erfc_l) * oo_sqrt_T;
}
/// computes a single value of G(T,U) using MacLaurin series.
static Real eval_MacLaurinT(Real T, Real U, size_t m, Real absolute_precision) {
assert(false); // not yet implemented
return 0.0;
}
private:
std::vector<Real> Gm_0_U_; // used for MacLaurin expansion
unsigned int mmax_;
Real precision_;
ExpensiveNumbers<Real> numbers_;
// since evaluation may involve several functions, will store some intermediate constants here
// to avoid the cost of extra parameters
//Real exp_U_;
//Real exp_mT_;
size_t count_tenno_algorithm_branches[3]; // counts the number of times each branch Ten-no algorithm
// was picked
};
#endif
//////////////////////////////////////////////////////////
/// core integrals r12^k \sum_i \exp(- a_i r_12^2)
//////////////////////////////////////////////////////////
/// each thread needs its own scratch if k==-1
template <typename Real, int k> struct GaussianGmEvalScratch;
/// create this object for each thread that needs to use GaussianGmEval<Real,-1>
template <typename Real>
struct GaussianGmEvalScratch<Real, -1> {
std::vector<Real> Fm_;
std::vector<Real> g_i;
std::vector<Real> r_i;
std::vector<Real> oorhog_i;
GaussianGmEvalScratch() {}
GaussianGmEvalScratch(int mmax) {
init(mmax);
}
void init(int mmax) {
Fm_.resize(mmax+1);
g_i.resize(mmax+1);
r_i.resize(mmax+1);
oorhog_i.resize(mmax+1);
g_i[0] = 1.0;
r_i[0] = 1.0;
}
};
/**
* Evaluates core integral \$ G_m(\rho, T) = \left( - \frac{\partial}{\partial T} \right)^n G_0(\rho,T) \f$,
* \f$ G_0(\rho,T) = \int \exp(-\rho |\vec{r} - \vec{P} + \vec{Q}|^2) g(r) \, {\rm d}\vec{r} \f$
* over a general contracted
* Gaussian geminal \f$ g(r_{12}) = r_{12}^k \sum_i c_i \exp(- a_i r_{12}^2), \quad k = -1, 0, 2 \f$ .
* The integrals are needed in R12/F12 methods with STG-nG correlation factors.
* Specifically, for a correlation factor \f$ f(r_{12}) = \sum_i c_i \exp(- a_i r_{12}^2) \f$
* integrals with the following kernels are needed:
* <ul>
* <li> \f$ f(r_{12}) \f$ (k=0) </li>
* <li> \f$ f(r_{12}) / r_{12} \f$ (k=-1) </li>
* <li> \f$ f(r_{12})^2 \f$ (k=0, @sa GaussianGmEval::eval ) </li>
* <li> \f$ [f(r_{12}), [\hat{T}_1, f(r_{12})]] \f$ (k=2, @sa GaussianGmEval::eval ) </li>
* </ul>
*
* N.B. ``Asymmetric'' kernels, \f$ f(r_{12}) g(r_{12}) \f$ and
* \f$ [f(r_{12}), [\hat{T}_1, g(r_{12})]] \f$, where f and g are two different geminals,
* can also be handled straightforwardly.
*
* \note for more details see DOI: 10.1039/b605188j
*/
template<typename Real, int k>
struct GaussianGmEval {
/**
* @param[in] mmax the evaluator will be used to compute Gm(T) for 0 <= m <= mmax
*/
GaussianGmEval(int mmax, Real precision) : mmax_(mmax),
precision_(precision), fm_eval_(0),
numbers_(-1,-1,mmax) {
assert(k == -1 || k == 0 || k == 2);
// for k=-1 need to evaluate the Boys function
if (k == -1) {
fm_eval_ = new FmEval_Taylor<Real>(mmax_, precision_);
// fm_eval_ = new FmEval_Chebyshev3(mmax_);
scratch_.init(mmax_);
}
}
~GaussianGmEval() {
delete fm_eval_;
fm_eval_ = 0;
}
// some features require at least C++11
#if __cplusplus > 199711L
/// Singleton interface allows to manage the lone instance;
/// adjusts max m and precision values as needed in thread-safe fashion
static const std::shared_ptr<GaussianGmEval>& instance(unsigned int mmax, Real precision) {
// thread-safe per C++11 standard [6.7.4]
static std::shared_ptr<GaussianGmEval> instance_ = 0;
const bool need_new_instance = !instance_ ||
(instance_ && (instance_->max_m() < mmax ||
instance_->precision() > precision));
if (need_new_instance) {
auto new_instance = std::make_shared<GaussianGmEval>(mmax, precision);
instance_ = new_instance; // thread-safe
}
return instance_;
}
#endif
/// @return the maximum value of m for which the \f$ G_m(\rho, T) \f$ can be computed with this object
int max_m() const { return mmax_; }
/// @return the precision with which this object can compute the Boys function
Real precision() const { return precision_; }
/** computes \f$ G_m(\rho, T) \f$ using downward recursion.
*
* @warning NOT reentrant if \c k == -1 and C++11 is not available
*
* @param[out] Gm array to be filled in with the \f$ Gm(\rho, T) \f$ values, must be at least mmax+1 elements long
* @param[in] rho
* @param[in] T
* @param[in] mmax mmax the maximum value of m for which Boys function will be computed;
* it must be <= the value returned by max_m() (this is not checked)
* @param[in] geminal the Gaussian geminal for which the core integral \f$ Gm(\rho, T) \f$ is computed
* @param[in] scr if \c k ==-1 and need this to be reentrant, must provide ptr to the per-thread \c GaussianGmEvalScratch<Real,-1> object;
* no need to specify \c scr otherwise
*/
template <typename AnyReal>
void eval(Real* Gm, Real rho, Real T, size_t mmax,
const std::vector<std::pair<AnyReal, AnyReal> >& geminal,
void* scr = 0) {
std::fill(Gm, Gm+mmax+1, Real(0));
const double sqrt_rho = sqrt(rho);
const double oo_sqrt_rho = 1.0/sqrt_rho;
if (k == -1) {
GaussianGmEvalScratch<Real, -1>& scratch = (scr == 0) ? scratch_ : *(reinterpret_cast<GaussianGmEvalScratch<Real, -1>*>(scr));
for(int i=1; i<=mmax; i++) {
scratch.r_i[i] = scratch.r_i[i-1] * rho;
}
}
typedef typename std::vector<std::pair<AnyReal, AnyReal> >::const_iterator citer;
const citer gend = geminal.end();
for(citer i=geminal.begin(); i!= gend; ++i) {
const double gamma = i->first;
const double gcoef = i->second;
const double rhog = rho + gamma;
const double oorhog = 1.0/rhog;
const double gorg = gamma * oorhog;
const double rorg = rho * oorhog;
const double sqrt_rho_org = sqrt_rho * oorhog;
const double sqrt_rhog = sqrt(rhog);
const double sqrt_rorg = sqrt_rho_org * sqrt_rhog;
/// (ss|g12|ss)
const Real const_SQRTPI_2(0.88622692545275801364908374167057259139877472806119); /* sqrt(pi)/2 */
const double SS_K0G12_SS = gcoef * oo_sqrt_rho * const_SQRTPI_2 * rorg * sqrt_rorg * exp(-gorg*T);
if (k == -1) {
GaussianGmEvalScratch<Real, -1>& scratch = (scr == 0) ? scratch_ : *(reinterpret_cast<GaussianGmEvalScratch<Real, -1>*>(scr));
const double rorgT = rorg * T;
fm_eval_->eval(&scratch.Fm_[0], rorgT, mmax);
#if 1
const Real const_2_SQRTPI(1.12837916709551257389615890312154517); /* 2/sqrt(pi) */
const Real pfac = const_2_SQRTPI * sqrt_rhog * SS_K0G12_SS;
scratch.oorhog_i[0] = pfac;
for(int i=1; i<=mmax; i++) {
scratch.g_i[i] = scratch.g_i[i-1] * gamma;
scratch.oorhog_i[i] = scratch.oorhog_i[i-1] * oorhog;
}
for(int m=0; m<=mmax; m++) {
Real ssss = 0.0;
Real* bcm = numbers_.bc[m];
for(int n=0; n<=m; n++) {
ssss += bcm[n] * scratch.r_i[n] * scratch.g_i[m-n] * scratch.Fm_[n];
}
Gm[m] += ssss * scratch.oorhog_i[m];
}
#endif
}
if (k == 0) {
double ss_oper_ss_m = SS_K0G12_SS;
Gm[0] += ss_oper_ss_m;
for(int m=1; m<=mmax; ++m) {
ss_oper_ss_m *= gorg;
Gm[m] += ss_oper_ss_m;
}
}
if (k == 2) {
/// (ss|g12*r12^2|ss)
const double rorgT = rorg * T;
const double SS_K2G12_SS_0 = (1.5 + rorgT) * (SS_K0G12_SS * oorhog);
const double SS_K2G12_SS_m1 = rorg * (SS_K0G12_SS * oorhog);
double SS_K2G12_SS_gorg_m = SS_K2G12_SS_0 ;
double SS_K2G12_SS_gorg_m1 = SS_K2G12_SS_m1;
Gm[0] += SS_K2G12_SS_gorg_m;
for(int m=1; m<=mmax; ++m) {
SS_K2G12_SS_gorg_m *= gorg;
Gm[m] += SS_K2G12_SS_gorg_m - m * SS_K2G12_SS_gorg_m1;
SS_K2G12_SS_gorg_m1 *= gorg;
}
}
}
}
private:
int mmax_;
Real precision_; //< absolute precision
FmEval_Taylor<Real>* fm_eval_;
// FmEval_Chebyshev3* fm_eval_;
GaussianGmEvalScratch <Real, -1> scratch_; // only used in serial if k==-1
ExpensiveNumbers<Real> numbers_;
};
/*
* Slater geminal fitting is available only if have LAPACK
*/
#if HAVE_LAPACK
/*
f[x_] := - Exp[-\[Zeta] x] / \[Zeta];
ff[cc_, aa_, x_] := Sum[cc[[i]]*Exp[-aa[[i]] x^2], {i, 1, n}];
*/
template <typename Real>
Real
fstg(Real zeta,
Real x) {
return -std::exp(-zeta*x)/zeta;
}
template <typename Real>
Real
fngtg(const std::vector<Real>& cc,
const std::vector<Real>& aa,
Real x) {
Real value = 0.0;
const Real x2 = x * x;
const unsigned int n = cc.size();
for(unsigned int i=0; i<n; ++i)
value += cc[i] * std::exp(- aa[i] * x2);
return value;
}
// --- weighting functions ---
// L2 error is weighted by ww(x)
// hence error is weighted by sqrt(ww(x))
template <typename Real>
Real
wwtewklopper(Real x) {
const Real x2 = x * x;
return x2 * std::exp(-2 * x2);
}
template <typename Real>
Real
wwcusp(Real x) {
const Real x2 = x * x;
const Real x6 = x2 * x2 * x2;
return std::exp(-0.005 * x6);
}
// default is Tew-Klopper
template <typename Real>
Real
ww(Real x) {
//return wwtewklopper(x);
return wwcusp(x);
}
template <typename Real>
Real
norm(const std::vector<Real>& vec) {
Real value = 0.0;
const unsigned int n = vec.size();
for(unsigned int i=0; i<n; ++i)
value += vec[i] * vec[i];
return value;
}
template <typename Real>
void LinearSolveDamped(const std::vector<Real>& A,
const std::vector<Real>& b,
Real lambda,
std::vector<Real>& x) {
const size_t n = b.size();
std::vector<Real> Acopy(A);
for(size_t m=0; m<n; ++m) Acopy[m*n + m] *= (1 + lambda);
std::vector<Real> e(b);
//int info = LAPACKE_dgesv( LAPACK_ROW_MAJOR, n, 1, &Acopy[0], n, &ipiv[0], &e[0], n );
{
std::vector<int> ipiv(n);
int n = b.size();
int one = 1;
int info;
dgesv_(&n, &one, &Acopy[0], &n, &ipiv[0], &e[0], &n, &info);
assert (info == 0);
}
x = e;
}
/**
* computes a least-squares fit of \f$ -exp(-\zeta r_{12})/\zeta = \sum_{i=1}^n c_i exp(-a_i r_{12}^2) \f$
* on \f$ r_{12} \in [0, x_{\rm max}] \f$ discretized to npts.
* @param[in] n
* @param[in] zeta
* @param[out] geminal
* @param[in] xmin
* @param[in] xmax
* @param[in] npts
*/
template <typename Real>
void stg_ng_fit(unsigned int n,
Real zeta,
std::vector< std::pair<Real, Real> >& geminal,
Real xmin = 0.0,
Real xmax = 10.0,
unsigned int npts = 1001) {
// initial guess
std::vector<Real> cc(n, 1.0); // coefficients
std::vector<Real> aa(n); // exponents
for(unsigned int i=0; i<n; ++i)
aa[i] = std::pow(3.0, (i + 2 - (n + 1)/2.0));
// first rescale cc for ff[x] to match the norm of f[x]
Real ffnormfac = 0.0;
for(unsigned int i=0; i<n; ++i)
for(unsigned int j=0; j<n; ++j)
ffnormfac += cc[i] * cc[j]/std::sqrt(aa[i] + aa[j]);
const Real Nf = std::sqrt(2.0 * zeta) * zeta;
const Real Nff = std::sqrt(2.0) / (std::sqrt(ffnormfac) *
std::sqrt(std::sqrt(M_PI)));
for(unsigned int i=0; i<n; ++i) cc[i] *= -Nff/Nf;
Real lambda0 = 1000; // damping factor is initially set to 1000, eventually should end up at 0
const Real nu = 3.0; // increase/decrease the damping factor scale it by this
const Real epsilon = 1e-15; // convergence
const unsigned int maxniter = 200;
// grid points on which we will fit
std::vector<Real> xi(npts);
for(unsigned int i=0; i<npts; ++i) xi[i] = xmin + (xmax - xmin)*i/(npts - 1);
std::vector<Real> err(npts);
const size_t nparams = 2*n; // params = expansion coefficients + gaussian exponents
std::vector<Real> J( npts * nparams );
std::vector<Real> delta(nparams);
// std::cout << "iteration 0" << std::endl;
// for(unsigned int i=0; i<n; ++i)
// std::cout << cc[i] << " " << aa[i] << std::endl;
Real errnormI;
Real errnormIm1 = 1e3;
bool converged = false;
unsigned int iter = 0;
while (!converged && iter < maxniter) {
// std::cout << "Iteration " << ++iter << ": lambda = " << lambda0/nu << std::endl;
for(unsigned int i=0; i<npts; ++i) {
const Real x = xi[i];
err[i] = (fstg(zeta, x) - fngtg(cc, aa, x)) * std::sqrt(ww(x));
}
errnormI = norm(err)/std::sqrt((Real)npts);
// std::cout << "|err|=" << errnormI << std::endl;
converged = std::abs((errnormI - errnormIm1)/errnormIm1) <= epsilon;
if (converged) break;
errnormIm1 = errnormI;
for(unsigned int i=0; i<npts; ++i) {
const Real x2 = xi[i] * xi[i];
const Real sqrt_ww_x = std::sqrt(ww(xi[i]));
const unsigned int ioffset = i * nparams;
for(unsigned int j=0; j<n; ++j)
J[ioffset+j] = (std::exp(-aa[j] * x2)) * sqrt_ww_x;
const unsigned int ioffsetn = ioffset+n;
for(unsigned int j=0; j<n; ++j)
J[ioffsetn+j] = - sqrt_ww_x * x2 * cc[j] * std::exp(-aa[j] * x2);
}
std::vector<Real> A( nparams * nparams);
for(size_t r=0, rc=0; r<nparams; ++r) {
for(size_t c=0; c<nparams; ++c, ++rc) {
double Arc = 0.0;
for(size_t i=0, ir=r, ic=c; i<npts; ++i, ir+=nparams, ic+=nparams)
Arc += J[ir] * J[ic];
A[rc] = Arc;
}
}
std::vector<Real> b( nparams );
for(size_t r=0; r<nparams; ++r) {
Real br = 0.0;
for(size_t i=0, ir=r; i<npts; ++i, ir+=nparams)
br += J[ir] * err[i];
b[r] = br;
}
// try decreasing damping first
// if not successful try increasing damping until it results in a decrease in the error
lambda0 /= nu;
for(int l=-1; l<1000; ++l) {
LinearSolveDamped(A, b, lambda0, delta );
std::vector<double> cc_0(cc); for(unsigned int i=0; i<n; ++i) cc_0[i] += delta[i];
std::vector<double> aa_0(aa); for(unsigned int i=0; i<n; ++i) aa_0[i] += delta[i+n];
// if any of the exponents are negative the step is too large and need to increase damping
bool step_too_large = false;
for(unsigned int i=0; i<n; ++i)
if (aa_0[i] < 0.0) {
step_too_large = true;
break;
}
if (!step_too_large) {
std::vector<double> err_0(npts);
for(unsigned int i=0; i<npts; ++i) {
const double x = xi[i];
err_0[i] = (fstg(zeta, x) - fngtg(cc_0, aa_0, x)) * std::sqrt(ww(x));
}
const double errnorm_0 = norm(err_0)/std::sqrt((double)npts);
if (errnorm_0 < errnormI) {
cc = cc_0;
aa = aa_0;
break;
}
else // step lead to increase of the error -- try dampening a bit more
lambda0 *= nu;
}
else // too large of a step
lambda0 *= nu;
} // done adjusting the damping factor
} // end of iterative minimization
// if reached max # of iterations throw if the error is too terrible
assert(not (iter == maxniter && errnormI > 1e-10));
for(unsigned int i=0; i<n; ++i)
geminal[i] = std::make_pair(aa[i], cc[i]);
}
#endif
} // end of namespace libint2
#endif // C++ only
#endif // header guard
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