added os-specific defines from cmake required by memtestG80

[gromacs/qmmm-gamess-us.git] / src / mdlib / coupling.c

/* -*- mode: c; tab-width: 4; indent-tabs-mode: nil; c-basic-offset: 4; c-file-style: "stroustrup"; -*-
 * 
 *                This source code is part of
 * 
 *                 G   R   O   M   A   C   S
 * 
 *          GROningen MAchine for Chemical Simulations
 * 
 *                        VERSION 3.2.0
 * Written by David van der Spoel, Erik Lindahl, Berk Hess, and others.
 * Copyright (c) 1991-2000, University of Groningen, The Netherlands.
 * Copyright (c) 2001-2004, The GROMACS development team,
 * check out http://www.gromacs.org for more information.

 * This program is free software; you can redistribute it and/or
 * modify it under the terms of the GNU General Public License
 * as published by the Free Software Foundation; either version 2
 * of the License, or (at your option) any later version.
 * 
 * If you want to redistribute modifications, please consider that
 * scientific software is very special. Version control is crucial -
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 */
#ifdef HAVE_CONFIG_H
#include <config.h>
#endif

#include "typedefs.h"
#include "smalloc.h"
#include "update.h"
#include "vec.h"
#include "macros.h"
#include "physics.h"
#include "names.h"
#include "gmx_fatal.h"
#include "txtdump.h"
#include "nrnb.h"
#include "gmx_random.h"

#define NTROTTERCALLS 5
#define NTROTTERPARTS 3

/* these integration routines are only references inside this file */
static void NHC_trotter(t_grpopts *opts,int nvar, gmx_ekindata_t *ekind,real dtfull,
                        double xi[],double vxi[], double scalefac[], real *veta, t_extmass *MassQ, bool bEkinAveVel)

{
    /* general routine for both barostat and thermostat nose hoover chains */

    int   i,j,mi,mj,jmax,nd;
    double Ekin,Efac,reft,kT;
    double dt;
    t_grp_tcstat *tcstat;
    double *ivxi,*ixi;
    double *iQinv;
    double *GQ;
    bool bBarostat;
    int mstepsi, mstepsj;
    int ns = SUZUKI_YOSHIDA_NUM;  /* set the degree of integration in the types/state.h file */
    int nh = opts->nhchainlength;
    
    snew(GQ,nh);
    mstepsi = mstepsj = ns;

/* if scalefac is NULL, we are doing the NHC of the barostat */
    
    bBarostat = FALSE;
    if (scalefac == NULL) {
        bBarostat = TRUE;
    }

    for (i=0; i<nvar; i++) 
    {
    
        /* make it easier to iterate by selecting 
           out the sub-array that corresponds to this T group */
        
        ivxi = &vxi[i*nh];
        ixi = &xi[i*nh];
        if (bBarostat) {
            iQinv = &(MassQ->QPinv[i*nh]); 
            nd = 1; /* THIS WILL CHANGE IF NOT ISOTROPIC */
            reft = max(0.0,opts->ref_t[0]);
            Ekin = sqr(*veta)/MassQ->Winv;
        } else {
            iQinv = &(MassQ->Qinv[i*nh]);  
            tcstat = &ekind->tcstat[i];
            nd = opts->nrdf[i];
            reft = max(0.0,opts->ref_t[i]);
            if (bEkinAveVel) 
            {
                Ekin = 2*trace(tcstat->ekinf)*tcstat->ekinscalef_nhc;
            } else {
                Ekin = 2*trace(tcstat->ekinh)*tcstat->ekinscaleh_nhc;
            }
        }
        kT = BOLTZ*reft;

        for(mi=0;mi<mstepsi;mi++) 
        {
            for(mj=0;mj<mstepsj;mj++)
            { 
                /* weighting for this step using Suzuki-Yoshida integration - fixed at 5 */
                dt = sy_const[ns][mj] * dtfull / mstepsi;
                
                /* compute the thermal forces */
                GQ[0] = iQinv[0]*(Ekin - nd*kT);
                
                for (j=0;j<nh-1;j++) 
                {       
                    if (iQinv[j+1] > 0) {
                        /* we actually don't need to update here if we save the 
                           state of the GQ, but it's easier to just recompute*/
                        GQ[j+1] = iQinv[j+1]*((sqr(ivxi[j])/iQinv[j])-kT);        
                    } else {
                        GQ[j+1] = 0;
                    }
                }
                
                ivxi[nh-1] += 0.25*dt*GQ[nh-1];
                for (j=nh-1;j>0;j--) 
                { 
                    Efac = exp(-0.125*dt*ivxi[j]);
                    ivxi[j-1] = Efac*(ivxi[j-1]*Efac + 0.25*dt*GQ[j-1]);
                }
                
                Efac = exp(-0.5*dt*ivxi[0]);
                if (bBarostat) {
                    *veta *= Efac;                
                } else {
                    scalefac[i] *= Efac;
                }
                Ekin *= (Efac*Efac);
                
                /* Issue - if the KE is an average of the last and the current temperatures, then we might not be
                   able to scale the kinetic energy directly with this factor.  Might take more bookkeeping -- have to
                   think about this a bit more . . . */

                GQ[0] = iQinv[0]*(Ekin - nd*kT);
                
                /* update thermostat positions */
                for (j=0;j<nh;j++) 
                { 
                    ixi[j] += 0.5*dt*ivxi[j];
                }
                
                for (j=0;j<nh-1;j++) 
                { 
                    Efac = exp(-0.125*dt*ivxi[j+1]);
                    ivxi[j] = Efac*(ivxi[j]*Efac + 0.25*dt*GQ[j]);
                    if (iQinv[j+1] > 0) {
                        GQ[j+1] = iQinv[j+1]*((sqr(ivxi[j])/iQinv[j])-kT);  
                    } else {
                        GQ[j+1] = 0;
                    }
                }
                ivxi[nh-1] += 0.25*dt*GQ[nh-1];
            }
        }
    }
    sfree(GQ);
}

static void boxv_trotter(t_inputrec *ir, real *veta, real dt, tensor box, 
                         gmx_ekindata_t *ekind, tensor vir, real pcorr, real ecorr, t_extmass *MassQ)
{

    real  pscal;
    double alpha;
    int   i,j,d,n,nwall;
    real  T,GW,vol;
    tensor Winvm,ekinmod,localpres;
    
    /* The heat bath is coupled to a separate barostat, the last temperature group.  In the 
       2006 Tuckerman et al paper., the order is iL_{T_baro} iL {T_part}
    */
    
    if (ir->epct==epctSEMIISOTROPIC) 
    {
        nwall = 2;
    } 
    else 
    {
        nwall = 3;
    }

    /* eta is in pure units.  veta is in units of ps^-1. GW is in 
       units of ps^-2.  However, eta has a reference of 1 nm^3, so care must be 
       taken to use only RATIOS of eta in updating the volume. */
    
    /* we take the partial pressure tensors, modify the 
       kinetic energy tensor, and recovert to pressure */
    
    if (ir->opts.nrdf[0]==0) 
    { 
        gmx_fatal(FARGS,"Barostat is coupled to a T-group with no degrees of freedom\n");    
    } 
    /* alpha factor for phase space volume, then multiply by the ekin scaling factor.  */
    alpha = 1.0 + DIM/((double)ir->opts.nrdf[0]);
    alpha *= ekind->tcstat[0].ekinscalef_nhc;
    msmul(ekind->ekin,alpha,ekinmod);  
    
    /* for now, we use Elr = 0, because if you want to get it right, you
       really should be using PME. Maybe print a warning? */
    
    pscal   = calc_pres(ir->ePBC,nwall,box,ekinmod,vir,localpres,0.0) + pcorr;
    
    vol = det(box);
    GW = (vol*(MassQ->Winv/PRESFAC))*(DIM*pscal - trace(ir->ref_p));   /* W is in ps^2 * bar * nm^3 */
    
    *veta += 0.5*dt*GW;   
}

/* 
 * This file implements temperature and pressure coupling algorithms:
 * For now only the Weak coupling and the modified weak coupling.
 *
 * Furthermore computation of pressure and temperature is done here
 *
 */

real calc_pres(int ePBC,int nwall,matrix box,tensor ekin,tensor vir,
               tensor pres,real Elr)
{
    int  n,m;
    real fac,Plr;
    
    if (ePBC==epbcNONE || (ePBC==epbcXY && nwall!=2))
        clear_mat(pres);
    else {
        /* Uitzoeken welke ekin hier van toepassing is, zie Evans & Morris - E. 
         * Wrs. moet de druktensor gecorrigeerd worden voor de netto stroom in  
         * het systeem...       
         */
        
        /* Long range correction for periodic systems, see
         * Neumann et al. JCP
         * divide by 6 because it is multiplied by fac later on.
         * If Elr = 0, no correction is made.
         */
        
        /* This formula should not be used with Ewald or PME, 
         * where the full long-range virial is calculated. EL 990823
         */
        Plr = Elr/6.0;
        
        fac=PRESFAC*2.0/det(box);
        for(n=0; (n<DIM); n++)
            for(m=0; (m<DIM); m++)
                pres[n][m]=(ekin[n][m]-vir[n][m]+Plr)*fac;
        
        if (debug) {
            pr_rvecs(debug,0,"PC: pres",pres,DIM);
            pr_rvecs(debug,0,"PC: ekin",ekin,DIM);
            pr_rvecs(debug,0,"PC: vir ",vir, DIM);
            pr_rvecs(debug,0,"PC: box ",box, DIM);
        }
    }
    return trace(pres)/DIM;
}

real calc_temp(real ekin,real nrdf)
{
    if (nrdf > 0)
        return (2.0*ekin)/(nrdf*BOLTZ);
    else
        return 0;
}

void parrinellorahman_pcoupl(FILE *fplog,gmx_large_int_t step,
                             t_inputrec *ir,real dt,tensor pres,
                             tensor box,tensor box_rel,tensor boxv,
                             tensor M,matrix mu,bool bFirstStep)
{
  /* This doesn't do any coordinate updating. It just
   * integrates the box vector equations from the calculated
   * acceleration due to pressure difference. We also compute
   * the tensor M which is used in update to couple the particle
   * coordinates to the box vectors.
   *
   * In Nose and Klein (Mol.Phys 50 (1983) no 5., p 1055) this is
   * given as
   *            -1    .           .     -1
   * M_nk = (h')   * (h' * h + h' h) * h
   *
   * with the dots denoting time derivatives and h is the transformation from
   * the scaled frame to the real frame, i.e. the TRANSPOSE of the box. 
   * This also goes for the pressure and M tensors - they are transposed relative
   * to ours. Our equation thus becomes:
   *
   *                  -1       .    .           -1
   * M_gmx = M_nk' = b  * (b * b' + b * b') * b'
   * 
   * where b is the gromacs box matrix.                       
   * Our box accelerations are given by
   *   ..                                    ..
   *   b = vol/W inv(box') * (P-ref_P)     (=h')
   */
  
  int    d,n;
  tensor winv;
  real   vol=box[XX][XX]*box[YY][YY]*box[ZZ][ZZ];
  real   atot,arel,change,maxchange,xy_pressure;
  tensor invbox,pdiff,t1,t2;

  real maxl;

  m_inv_ur0(box,invbox);

  if (!bFirstStep) {
    /* Note that PRESFAC does not occur here.
     * The pressure and compressibility always occur as a product,
     * therefore the pressure unit drops out.
     */
    maxl=max(box[XX][XX],box[YY][YY]);
    maxl=max(maxl,box[ZZ][ZZ]);
    for(d=0;d<DIM;d++)
      for(n=0;n<DIM;n++)
        winv[d][n]=
          (4*M_PI*M_PI*ir->compress[d][n])/(3*ir->tau_p*ir->tau_p*maxl);
    
    m_sub(pres,ir->ref_p,pdiff);
    
    if(ir->epct==epctSURFACETENSION) {
      /* Unlike Berendsen coupling it might not be trivial to include a z
       * pressure correction here? On the other hand we don't scale the
       * box momentarily, but change accelerations, so it might not be crucial.
       */
      xy_pressure=0.5*(pres[XX][XX]+pres[YY][YY]);
      for(d=0;d<ZZ;d++)
        pdiff[d][d]=(xy_pressure-(pres[ZZ][ZZ]-ir->ref_p[d][d]/box[d][d]));
    }
    
    tmmul(invbox,pdiff,t1);
    /* Move the off-diagonal elements of the 'force' to one side to ensure
     * that we obey the box constraints.
     */
    for(d=0;d<DIM;d++) {
      for(n=0;n<d;n++) {
        t1[d][n] += t1[n][d];
        t1[n][d] = 0;
      }
    }
    
    switch (ir->epct) {
    case epctANISOTROPIC:
      for(d=0;d<DIM;d++) 
        for(n=0;n<=d;n++)
          t1[d][n] *= winv[d][n]*vol;
      break;
    case epctISOTROPIC:
      /* calculate total volume acceleration */
      atot=box[XX][XX]*box[YY][YY]*t1[ZZ][ZZ]+
        box[XX][XX]*t1[YY][YY]*box[ZZ][ZZ]+
        t1[XX][XX]*box[YY][YY]*box[ZZ][ZZ];
      arel=atot/(3*vol);
      /* set all RELATIVE box accelerations equal, and maintain total V
       * change speed */
      for(d=0;d<DIM;d++)
        for(n=0;n<=d;n++)
          t1[d][n] = winv[0][0]*vol*arel*box[d][n];    
      break;
    case epctSEMIISOTROPIC:
    case epctSURFACETENSION:
      /* Note the correction to pdiff above for surftens. coupling  */
      
      /* calculate total XY volume acceleration */
      atot=box[XX][XX]*t1[YY][YY]+t1[XX][XX]*box[YY][YY];
      arel=atot/(2*box[XX][XX]*box[YY][YY]);
      /* set RELATIVE XY box accelerations equal, and maintain total V
       * change speed. Dont change the third box vector accelerations */
      for(d=0;d<ZZ;d++)
        for(n=0;n<=d;n++)
          t1[d][n] = winv[d][n]*vol*arel*box[d][n];
      for(n=0;n<DIM;n++)
        t1[ZZ][n] *= winv[d][n]*vol;
      break;
    default:
      gmx_fatal(FARGS,"Parrinello-Rahman pressure coupling type %s "
                  "not supported yet\n",EPCOUPLTYPETYPE(ir->epct));
      break;
    }
    
    maxchange=0;
    for(d=0;d<DIM;d++)
      for(n=0;n<=d;n++) {
        boxv[d][n] += dt*t1[d][n];
        
        /* We do NOT update the box vectors themselves here, since
         * we need them for shifting later. It is instead done last
         * in the update() routine.
         */
        
        /* Calculate the change relative to diagonal elements-
           since it's perfectly ok for the off-diagonal ones to
           be zero it doesn't make sense to check the change relative
           to its current size.
        */
        
        change=fabs(dt*boxv[d][n]/box[d][d]);
        
        if (change>maxchange)
          maxchange=change;
      }
    
    if (maxchange > 0.01 && fplog) {
      char buf[22];
      fprintf(fplog,"\nStep %s  Warning: Pressure scaling more than 1%%.\n",
              gmx_step_str(step,buf));
    }
  }
  
  preserve_box_shape(ir,box_rel,boxv);

  mtmul(boxv,box,t1);       /* t1=boxv * b' */
  mmul(invbox,t1,t2);
  mtmul(t2,invbox,M);

  /* Determine the scaling matrix mu for the coordinates */
  for(d=0;d<DIM;d++)
    for(n=0;n<=d;n++)
      t1[d][n] = box[d][n] + dt*boxv[d][n];
  preserve_box_shape(ir,box_rel,t1);
  /* t1 is the box at t+dt, determine mu as the relative change */
  mmul_ur0(invbox,t1,mu);
}

void berendsen_pcoupl(FILE *fplog,gmx_large_int_t step, 
                      t_inputrec *ir,real dt, tensor pres,matrix box,
                      matrix mu)
{
  int    d,n;
  real   scalar_pressure, xy_pressure, p_corr_z;
  char   *ptr,buf[STRLEN];

  /*
   *  Calculate the scaling matrix mu
   */
  scalar_pressure=0;
  xy_pressure=0;
  for(d=0; d<DIM; d++) {
    scalar_pressure += pres[d][d]/DIM;
    if (d != ZZ)
      xy_pressure += pres[d][d]/(DIM-1);
  }
  /* Pressure is now in bar, everywhere. */
#define factor(d,m) (ir->compress[d][m]*dt/ir->tau_p)
  
  /* mu has been changed from pow(1+...,1/3) to 1+.../3, since this is
   * necessary for triclinic scaling
   */
  clear_mat(mu);
  switch (ir->epct) {
  case epctISOTROPIC:
    for(d=0; d<DIM; d++) 
      {
        mu[d][d] = 1.0 - factor(d,d)*(ir->ref_p[d][d] - scalar_pressure) /DIM;
      }
    break;
  case epctSEMIISOTROPIC:
    for(d=0; d<ZZ; d++)
      mu[d][d] = 1.0 - factor(d,d)*(ir->ref_p[d][d]-xy_pressure)/DIM;
    mu[ZZ][ZZ] = 
      1.0 - factor(ZZ,ZZ)*(ir->ref_p[ZZ][ZZ] - pres[ZZ][ZZ])/DIM;
    break;
  case epctANISOTROPIC:
    for(d=0; d<DIM; d++)
      for(n=0; n<DIM; n++)
        mu[d][n] = (d==n ? 1.0 : 0.0) 
          -factor(d,n)*(ir->ref_p[d][n] - pres[d][n])/DIM;
    break;
  case epctSURFACETENSION:
    /* ir->ref_p[0/1] is the reference surface-tension times *
     * the number of surfaces                                */
    if (ir->compress[ZZ][ZZ])
      p_corr_z = dt/ir->tau_p*(ir->ref_p[ZZ][ZZ] - pres[ZZ][ZZ]);
    else
      /* when the compressibity is zero, set the pressure correction   *
       * in the z-direction to zero to get the correct surface tension */
      p_corr_z = 0;
    mu[ZZ][ZZ] = 1.0 - ir->compress[ZZ][ZZ]*p_corr_z;
    for(d=0; d<DIM-1; d++)
      mu[d][d] = 1.0 + factor(d,d)*(ir->ref_p[d][d]/(mu[ZZ][ZZ]*box[ZZ][ZZ])
                                    - (pres[ZZ][ZZ]+p_corr_z - xy_pressure))/(DIM-1);
    break;
  default:
    gmx_fatal(FARGS,"Berendsen pressure coupling type %s not supported yet\n",
                EPCOUPLTYPETYPE(ir->epct));
    break;
  }
  /* To fullfill the orientation restrictions on triclinic boxes
   * we will set mu_yx, mu_zx and mu_zy to 0 and correct
   * the other elements of mu to first order.
   */
  mu[YY][XX] += mu[XX][YY];
  mu[ZZ][XX] += mu[XX][ZZ];
  mu[ZZ][YY] += mu[YY][ZZ];
  mu[XX][YY] = 0;
  mu[XX][ZZ] = 0;
  mu[YY][ZZ] = 0;

  if (debug) {
    pr_rvecs(debug,0,"PC: pres ",pres,3);
    pr_rvecs(debug,0,"PC: mu   ",mu,3);
  }
  
  if (mu[XX][XX]<0.99 || mu[XX][XX]>1.01 ||
      mu[YY][YY]<0.99 || mu[YY][YY]>1.01 ||
      mu[ZZ][ZZ]<0.99 || mu[ZZ][ZZ]>1.01) {
    char buf2[22];
    sprintf(buf,"\nStep %s  Warning: pressure scaling more than 1%%, "
            "mu: %g %g %g\n",
            gmx_step_str(step,buf2),mu[XX][XX],mu[YY][YY],mu[ZZ][ZZ]);
    if (fplog)
      fprintf(fplog,"%s",buf);
    fprintf(stderr,"%s",buf);
  }
}

void berendsen_pscale(t_inputrec *ir,matrix mu,
                      matrix box,matrix box_rel,
                      int start,int nr_atoms,
                      rvec x[],unsigned short cFREEZE[],
                      t_nrnb *nrnb)
{
  ivec   *nFreeze=ir->opts.nFreeze;
  int    n,d,g=0;
      
  /* Scale the positions */
  for (n=start; n<start+nr_atoms; n++) {
    if (cFREEZE)
      g = cFREEZE[n];
    
    if (!nFreeze[g][XX])
      x[n][XX] = mu[XX][XX]*x[n][XX]+mu[YY][XX]*x[n][YY]+mu[ZZ][XX]*x[n][ZZ];
    if (!nFreeze[g][YY])
      x[n][YY] = mu[YY][YY]*x[n][YY]+mu[ZZ][YY]*x[n][ZZ];
    if (!nFreeze[g][ZZ])
      x[n][ZZ] = mu[ZZ][ZZ]*x[n][ZZ];
  }
  /* compute final boxlengths */
  for (d=0; d<DIM; d++) {
    box[d][XX] = mu[XX][XX]*box[d][XX]+mu[YY][XX]*box[d][YY]+mu[ZZ][XX]*box[d][ZZ];
    box[d][YY] = mu[YY][YY]*box[d][YY]+mu[ZZ][YY]*box[d][ZZ];
    box[d][ZZ] = mu[ZZ][ZZ]*box[d][ZZ];
  }      

  preserve_box_shape(ir,box_rel,box);
  
  /* (un)shifting should NOT be done after this,
   * since the box vectors might have changed
   */
  inc_nrnb(nrnb,eNR_PCOUPL,nr_atoms);
}

void berendsen_tcoupl(t_grpopts *opts,gmx_ekindata_t *ekind,real dt)
{
  int    i;
  
  real   T,reft=0,lll; 

  for(i=0; (i<opts->ngtc); i++) {
    T = ekind->tcstat[i].Th;
    
    if ((opts->tau_t[i] > 0) && (T > 0.0)) {
 
      reft = max(0.0,opts->ref_t[i]);
      lll  = sqrt(1.0 + (dt/opts->tau_t[i])*(reft/T-1.0));
      ekind->tcstat[i].lambda = max(min(lll,1.25),0.8);
    }
    else {
       ekind->tcstat[i].lambda = 1.0;
    }

    if (debug)
      fprintf(debug,"TC: group %d: T: %g, Lambda: %g\n",
              i,T,ekind->tcstat[i].lambda);
  }
}

void nosehoover_tcoupl(t_grpopts *opts,gmx_ekindata_t *ekind,real dt,
                       double xi[],double vxi[], t_extmass *MassQ)
{
    int   i;
    real  reft,oldvxi;
    
    /* note that this routine does not include Nose-hoover chains yet. Should be easy to add. */
    
    for(i=0; (i<opts->ngtc); i++) {
        reft = max(0.0,opts->ref_t[i]);
        oldvxi = vxi[i];
        vxi[i]  += dt*MassQ->Qinv[i]*(ekind->tcstat[i].Th - reft);
        xi[i] += dt*(oldvxi + vxi[i])*0.5;
    }
}

t_state *init_bufstate(const t_state *template_state) 
{
    t_state *state;
    int nc = template_state->nhchainlength;
    snew(state,1);
    snew(state->nosehoover_xi,nc*template_state->ngtc);
    snew(state->nosehoover_vxi,nc*template_state->ngtc);
    snew(state->therm_integral,template_state->ngtc);
    snew(state->nhpres_xi,nc*template_state->nnhpres);
    snew(state->nhpres_vxi,nc*template_state->nnhpres);

    return state;
}  

void destroy_bufstate(t_state *state) 
{
    sfree(state->x);
    sfree(state->v);
    sfree(state->nosehoover_xi);
    sfree(state->nosehoover_vxi);
    sfree(state->therm_integral);
    sfree(state->nhpres_xi);
    sfree(state->nhpres_vxi);
    sfree(state);
}  

void trotter_update(t_inputrec *ir,gmx_ekindata_t *ekind, 
                    gmx_enerdata_t *enerd, t_state *state, 
                    tensor vir, t_mdatoms *md, 
                    t_extmass *MassQ, int *trotter_seq) 
{
    
    int n,i,j,d,ntgrp,ngtc,gc=0;
    t_grp_tcstat *tcstat;
    t_grpopts *opts;
    real ecorr,pcorr,dvdlcorr;
    real bmass,qmass,reft,kT,dt,nd;
    tensor dumpres,dumvir;
    double *scalefac;
    rvec sumv,consk;

    /* signal we are returning if nothing is going to be done in this routine */
    if (trotter_seq[0] == etrtSKIPALL) 
    {
        return;
    }
    opts = &(ir->opts); /* just for ease of referencing */
    ngtc = opts->ngtc;
    snew(scalefac,opts->ngtc);
    for (i=0;i<ngtc;i++) 
    {
        scalefac[i] = 1;
    }
    /* execute the series of trotter updates specified in the trotterpart array */
    
    for (i=0;i<NTROTTERPARTS;i++){
        /* allow for doubled intgrators by doubling dt instead of making 2 calls */
        if ((trotter_seq[i] == etrtBAROV2) || (trotter_seq[i] == etrtBARONHC2) || (trotter_seq[i] == etrtNHC2))
        {
            dt = 2 * ir->delta_t;
        }
        else 
        {
            dt = ir->delta_t;
        }
            
        switch (trotter_seq[i])
        {
        case etrtBAROV:
        case etrtBAROV2:
            boxv_trotter(ir,&(state->veta),dt,state->box,ekind,vir,
                         enerd->term[F_PDISPCORR],enerd->term[F_DISPCORR],MassQ);
            break;
        case etrtBARONHC:
        case etrtBARONHC2:
            NHC_trotter(opts,state->nnhpres,ekind,dt,state->nhpres_xi,
                        state->nhpres_vxi,NULL,&(state->veta),MassQ,FALSE);      
            break;
        case etrtNHC:
        case etrtNHC2:
            NHC_trotter(opts,opts->ngtc,ekind,dt,state->nosehoover_xi,
                        state->nosehoover_vxi,scalefac,NULL,MassQ,(ir->eI==eiVV));
            /* need to rescale the kinetic energies and velocities here.  Could 
               scale the velocities later, but we need them scaled in order to 
               produce the correct outputs, so we'll scale them here. */
            
            for (i=0; i<ngtc;i++) 
            {
                tcstat = &ekind->tcstat[i];
                tcstat->vscale_nhc = scalefac[i]; 
                tcstat->ekinscaleh_nhc *= (scalefac[i]*scalefac[i]); 
                tcstat->ekinscalef_nhc *= (scalefac[i]*scalefac[i]); 
            }
            /* now that we've scaled the groupwise velocities, we can add them up to get the total */
            /* but do we actually need the total? */
            
            /* modify the velocities as well */
            for (n=md->start;n<md->start+md->homenr;n++) 
            {
                if (md->cTC) 
                { 
                    gc = md->cTC[n];
                }
                for (d=0;d<DIM;d++) 
                {
                    state->v[n][d] *= scalefac[gc];
                }
                
                if (debug) 
                {
                    for (d=0;d<DIM;d++) 
                    {
                        sumv[d] += (state->v[n][d])/md->invmass[n];
                    }
                }
            }          
            break;
        default:
            break;
        }
    }
    /* check for conserved momentum -- worth looking at this again eventually, but not working right now.*/  
#if 0
    if (debug) 
    {
        if (bFirstHalf) 
        {
            for (d=0;d<DIM;d++) 
            {
                consk[d] = sumv[d]*exp((1 + 1.0/opts->nrdf[0])*((1.0/DIM)*log(det(state->box)/state->vol0)) + state->nosehoover_xi[0]); 
            }
            fprintf(debug,"Conserved kappa: %15.8f %15.8f %15.8f\n",consk[0],consk[1],consk[2]);    
        }
    }
#endif
    sfree(scalefac);
}

int **init_npt_vars(t_inputrec *ir, t_state *state, t_extmass *MassQ, bool bTrotter) 
{
    int n,i,j,d,ntgrp,ngtc,nnhpres,nh,gc=0;
    t_grp_tcstat *tcstat;
    t_grpopts *opts;
    real ecorr,pcorr,dvdlcorr;
    real bmass,qmass,reft,kT,dt,ndj,nd;
    tensor dumpres,dumvir;
    int **trotter_seq;

    opts = &(ir->opts); /* just for ease of referencing */
    ngtc = state->ngtc;
    nnhpres = state->nnhpres;
    nh = state->nhchainlength; 

    if (ir->eI == eiMD) {
        snew(MassQ->Qinv,ngtc);
        for(i=0; (i<ngtc); i++) 
        { 
            if ((opts->tau_t[i] > 0) && (opts->ref_t[i] > 0)) 
            {
                MassQ->Qinv[i]=1.0/(sqr(opts->tau_t[i]/M_2PI)*opts->ref_t[i]);
            } 
            else 
            {
                MassQ->Qinv[i]=0.0;     
            }
        }
    }
    else if (EI_VV(ir->eI))
    {
    /* Set pressure variables */
        
        if (state->vol0 == 0) 
        {
            state->vol0 = det(state->box); /* because we start by defining a fixed compressibility, 
                                              we need the volume at this compressibility to solve the problem */ 
        }

        /* units are nm^3 * ns^2 / (nm^3 * bar / kJ/mol) = kJ/mol  */
        /* Investigate this more -- is this the right mass to make it? */
        MassQ->Winv = (PRESFAC*trace(ir->compress)*BOLTZ*opts->ref_t[0])/(DIM*state->vol0*sqr(ir->tau_p/M_2PI));
        /* An alternate mass definition, from Tuckerman et al. */ 
        /* MassQ->Winv = 1.0/(sqr(ir->tau_p/M_2PI)*(opts->nrdf[0]+DIM)*BOLTZ*opts->ref_t[0]); */
        for (d=0;d<DIM;d++) 
        {
            for (n=0;n<DIM;n++) 
            {
                MassQ->Winvm[d][n]= PRESFAC*ir->compress[d][n]/(state->vol0*sqr(ir->tau_p/M_2PI)); 
                /* not clear this is correct yet for the anisotropic case*/
            } 
        }           
        /* Allocate space for thermostat variables */
        snew(MassQ->Qinv,ngtc*nh);
        
        /* now, set temperature variables */
        for(i=0; i<ngtc; i++) 
        {
            if ((opts->tau_t[i] > 0) && (opts->ref_t[i] > 0)) 
            {
                reft = max(0.0,opts->ref_t[i]);
                nd = opts->nrdf[i];
                kT = BOLTZ*reft;
                for (j=0;j<nh;j++) 
                {
                    if (j==0) 
                    {
                        ndj = nd;
                    } 
                    else 
                    {
                        ndj = 1;
                    }
                    MassQ->Qinv[i*nh+j]   = 1.0/(sqr(opts->tau_t[i]/M_2PI)*ndj*kT);
                }
            }
            else 
            {
                reft=0.0;
                for (j=0;j<nh;j++) 
                {
                    MassQ->Qinv[i*nh+j] = 0.0;
                }
            }
        }
    }
    
    /* first, initialize clear all the trotter calls */
    snew(trotter_seq,NTROTTERCALLS);
    for (i=0;i<NTROTTERCALLS;i++) 
    {
        snew(trotter_seq[i],NTROTTERPARTS);
        for (j=0;j<NTROTTERPARTS;j++) {
            trotter_seq[i][j] = etrtNONE;
        }
        trotter_seq[i][0] = etrtSKIPALL;
    }
    
    if (!bTrotter) 
    {
        /* no trotter calls, so we never use the values in the array.
         * We access them (so we need to define them, but ignore
         * then.*/

        return trotter_seq;
    }

    /* compute the kinetic energy by using the half step velocities or
     * the kinetic energies, depending on the order of the trotter calls */

    if (ir->eI==eiVV)
    {
        if (IR_NPT_TROTTER(ir)) 
        {
            /* This is the complicated version - there are 4 possible calls, depending on ordering.
               We start with the initial one. */
            /* first, a round that estimates veta. */
            trotter_seq[0][0] = etrtBAROV; 
            
            /* trotter_seq[1] is etrtNHC for 1/2 step velocities - leave zero */
            
            /* The first half trotter update */
            trotter_seq[2][0] = etrtBAROV;
            trotter_seq[2][1] = etrtNHC;
            trotter_seq[2][2] = etrtBARONHC;
            
            /* The second half trotter update */
            trotter_seq[3][0] = etrtBARONHC;
            trotter_seq[3][1] = etrtNHC;
            trotter_seq[3][2] = etrtBAROV;

            /* trotter_seq[4] is etrtNHC for second 1/2 step velocities - leave zero */

        } 
        else 
        {
            if (IR_NVT_TROTTER(ir)) 
            {
                /* This is the easy version - there are only two calls, both the same. 
                   Otherwise, even easier -- no calls  */
                trotter_seq[2][0] = etrtNHC;
                trotter_seq[3][0] = etrtNHC;
            }
        }
    } else if (ir->eI==eiVVAK) {
        if (IR_NPT_TROTTER(ir)) 
        {
            /* This is the complicated version - there are 4 possible calls, depending on ordering.
               We start with the initial one. */
            /* first, a round that estimates veta. */
            trotter_seq[0][0] = etrtBAROV; 
            
            /* The first half trotter update, part 1 -- double update, because it commutes */
            trotter_seq[1][0] = etrtNHC;

            /* The first half trotter update, part 2 */
            trotter_seq[2][0] = etrtBAROV;
            trotter_seq[2][1] = etrtBARONHC;
            
            /* The second half trotter update, part 1 */
            trotter_seq[3][0] = etrtBARONHC;
            trotter_seq[3][1] = etrtBAROV;

            /* The second half trotter update -- blank for now */
            trotter_seq[4][0] = etrtNHC;
        } 
        else 
        {
            if (IR_NVT_TROTTER(ir)) 
            {
                /* This is the easy version - there is only one call, both the same. 
                   Otherwise, even easier -- no calls  */
                trotter_seq[1][0] = etrtNHC;
                trotter_seq[4][0] = etrtNHC;
            }
        }
    }

    switch (ir->epct) 
    {
    case epctISOTROPIC:  
    default:
        bmass = DIM*DIM;  /* recommended mass parameters for isotropic barostat */
    }    

    snew(MassQ->QPinv,nnhpres*opts->nhchainlength);

    /* barostat temperature */
    if ((ir->tau_p > 0) && (opts->ref_t[0] > 0)) 
    {
        reft = max(0.0,opts->ref_t[0]);
        kT = BOLTZ*reft;
        for (i=0;i<nnhpres;i++) {
            for (j=0;j<nh;j++) 
            {
                if (j==0) {
                    qmass = bmass;
                } 
                else 
                {
                    qmass = 1;
                }
                MassQ->QPinv[i*opts->nhchainlength+j]   = 1.0/(sqr(opts->tau_t[0]/M_2PI)*qmass*kT);
            }
        }
    }
    else 
    {
        for (i=0;i<nnhpres;i++) {
            for (j=0;j<nh;j++) 
            {
                MassQ->QPinv[i*nh+j]=0.0;
            }
        }
    }    
    return trotter_seq;
}

real NPT_energy(t_inputrec *ir, t_state *state, t_extmass *MassQ)
{
    int  i,j,nd,ndj,bmass,qmass,ngtcall;
    real ener_npt,reft,eta,kT,tau;
    double *ivxi, *ixi;
    double *iQinv;
    real vol,dbaro,W,Q;
    int nh = state->nhchainlength;

    ener_npt = 0;
    
    /* now we compute the contribution of the pressure to the conserved quantity*/
    
    if (ir->epc==epcMTTK) 
    {
        /* find the volume, and the kinetic energy of the volume */
        
        switch (ir->epct) {
            
        case epctISOTROPIC:
            /* contribution from the pressure momenenta */
            ener_npt += 0.5*sqr(state->veta)/MassQ->Winv;
            
            /* contribution from the PV term */
            vol = det(state->box);
            ener_npt += vol*trace(ir->ref_p)/(DIM*PRESFAC);

            break;
        case epctANISOTROPIC:
            
            break;
            
        case epctSURFACETENSION:
            
            break;
        case epctSEMIISOTROPIC:
            
            break;
        default:
            break;
        }
    }
    
    if (IR_NPT_TROTTER(ir)) 
    {
        /* add the energy from the barostat thermostat chain */
        for (i=0;i<state->nnhpres;i++) {

            /* note -- assumes only one degree of freedom that is thermostatted in barostat */
            ivxi = &state->nhpres_vxi[i*nh];
            ixi = &state->nhpres_xi[i*nh];
            iQinv = &(MassQ->QPinv[i*nh]);
            reft = max(ir->opts.ref_t[0],0); /* using 'System' temperature */
            kT = BOLTZ * reft;
        
            for (j=0;j<nh;j++) 
            {
                ener_npt += 0.5*sqr(ivxi[j])/iQinv[j];
                /* contribution from the thermal variable of the NH chain */
                ener_npt += ixi[j]*kT;
                if (debug) 
                {
                    fprintf(debug,"P-T-group: %10d Chain %4d ThermV: %15.8f ThermX: %15.8f",i,j,ivxi[j],ixi[j]);
                }
            }
        }
    }
        
    if (ir->etc) 
    {
        for(i=0; i<ir->opts.ngtc; i++) 
        {
            ixi = &state->nosehoover_xi[i*nh];
            ivxi = &state->nosehoover_vxi[i*nh];
            iQinv = &(MassQ->Qinv[i*nh]);
            
            nd = ir->opts.nrdf[i];
            reft = max(ir->opts.ref_t[i],0);
            kT = BOLTZ * reft;
            
            if (nd > 0) 
            {
                if (IR_NVT_TROTTER(ir))
                {
                    /* contribution from the thermal momenta of the NH chain */
                    for (j=0;j<nh;j++) 
                    {
                        ener_npt += 0.5*sqr(ivxi[j])/iQinv[j];
                        /* contribution from the thermal variable of the NH chain */
                        if (j==0) {
                            ndj = nd;
                        } 
                        else 
                        {
                            ndj = 1;
                        } 
                        ener_npt += ndj*ixi[j]*kT;
                    }
                }
                else  /* Other non Trotter temperature NH control  -- no chains yet. */
                { 
                    ener_npt += 0.5*BOLTZ*nd*sqr(ivxi[0])/iQinv[0];
                    ener_npt += nd*ixi[0]*kT;
                }
            }
        }
    }
    return ener_npt;
}

static real vrescale_gamdev(int ia, gmx_rng_t rng)
/* Gamma distribution, adapted from numerical recipes */
{
  int j;
  real am,e,s,v1,v2,x,y;
  
  if (ia < 6) {
    x = 1.0;
    for(j=1; j<=ia; j++) {
      x *= gmx_rng_uniform_real(rng);
    }
    x = -log(x);
  } else {
    do {
      do {
        do {
          v1 = gmx_rng_uniform_real(rng);
          v2 = 2.0*gmx_rng_uniform_real(rng)-1.0;
        } while (v1*v1 + v2*v2 > 1.0);
        y = v2/v1;
        am = ia - 1;
        s = sqrt(2.0*am + 1.0);
        x = s*y + am;
      } while (x <= 0.0);
      e = (1.0 + y*y)*exp(am*log(x/am) - s*y);
    } while (gmx_rng_uniform_real(rng) > e);
  }

  return x;
}

static real vrescale_sumnoises(int nn,gmx_rng_t rng)
{
/*
 * Returns the sum of n independent gaussian noises squared
 * (i.e. equivalent to summing the square of the return values
 * of nn calls to gmx_rng_gaussian_real).xs
 */
  real rr;

  if (nn == 0) {
    return 0.0;
  } else if (nn == 1) {
    rr = gmx_rng_gaussian_real(rng);
    return rr*rr;
  } else if (nn % 2 == 0) {
    return 2.0*vrescale_gamdev(nn/2,rng);
  } else {
    rr = gmx_rng_gaussian_real(rng);
    return 2.0*vrescale_gamdev((nn-1)/2,rng) + rr*rr;
  }
}

static real vrescale_resamplekin(real kk,real sigma, int ndeg, real taut,
                                 gmx_rng_t rng)
{
/*
 * Generates a new value for the kinetic energy,
 * according to Bussi et al JCP (2007), Eq. (A7)
 * kk:    present value of the kinetic energy of the atoms to be thermalized (in arbitrary units)
 * sigma: target average value of the kinetic energy (ndeg k_b T/2)  (in the same units as kk)
 * ndeg:  number of degrees of freedom of the atoms to be thermalized
 * taut:  relaxation time of the thermostat, in units of 'how often this routine is called'
 */
  real factor,rr;

  if (taut > 0.1) {
    factor = exp(-1.0/taut);
  } else {
    factor = 0.0;
  }
  rr = gmx_rng_gaussian_real(rng);
  return
    kk +
    (1.0 - factor)*(sigma*(vrescale_sumnoises(ndeg-1,rng) + rr*rr)/ndeg - kk) +
    2.0*rr*sqrt(kk*sigma/ndeg*(1.0 - factor)*factor);
}

void vrescale_tcoupl(t_grpopts *opts,gmx_ekindata_t *ekind,real dt,
                     double therm_integral[],gmx_rng_t rng)
{
  int    i;
  real   Ek,Ek_ref1,Ek_ref,Ek_new; 

  for(i=0; (i<opts->ngtc); i++) {
    Ek = trace(ekind->tcstat[i].ekinh);
    
    if (opts->tau_t[i] >= 0 && opts->nrdf[i] > 0 && Ek > 0) {
      Ek_ref1   = 0.5*opts->ref_t[i]*BOLTZ;
      Ek_ref    = Ek_ref1*opts->nrdf[i];

      Ek_new =
        vrescale_resamplekin(Ek,Ek_ref,opts->nrdf[i],opts->tau_t[i]/dt,rng);

      /* Analytically Ek_new>=0, but we check for rounding errors */
      if (Ek_new <= 0) {
        ekind->tcstat[i].lambda = 0.0;
      } else {
        ekind->tcstat[i].lambda = sqrt(Ek_new/Ek);
      }
      therm_integral[i] -= Ek_new - Ek;

      if (debug) {
        fprintf(debug,"TC: group %d: Ekr %g, Ek %g, Ek_new %g, Lambda: %g\n",
                i,Ek_ref,Ek,Ek_new,ekind->tcstat[i].lambda);
      }
    } else {
       ekind->tcstat[i].lambda = 1.0;
    }
  }
}

real vrescale_energy(t_grpopts *opts,double therm_integral[])
{
  int i;
  real ener;

  ener = 0;
  for(i=0; i<opts->ngtc; i++) {
    ener += therm_integral[i];
  }
  
  return ener;
}

/* set target temperatures if we are annealing */
void update_annealing_target_temp(t_grpopts *opts,real t)
{
  int i,j,n,npoints;
  real pert,thist=0,x;

  for(i=0;i<opts->ngtc;i++) {
    npoints = opts->anneal_npoints[i];
    switch (opts->annealing[i]) {
    case eannNO:
      continue;
    case  eannPERIODIC:
      /* calculate time modulo the period */
      pert  = opts->anneal_time[i][npoints-1];
      n     = t / pert;
      thist = t - n*pert; /* modulo time */
      /* Make sure rounding didn't get us outside the interval */
      if (fabs(thist-pert) < GMX_REAL_EPS*100)
        thist=0;
      break;
    case eannSINGLE:
      thist = t;
      break;
    default:
      gmx_fatal(FARGS,"Death horror in update_annealing_target_temp (i=%d/%d npoints=%d)",i,opts->ngtc,npoints);
    }
    /* We are doing annealing for this group if we got here, 
     * and we have the (relative) time as thist.
     * calculate target temp */
    j=0;
    while ((j < npoints-1) && (thist>(opts->anneal_time[i][j+1])))
      j++;
    if (j < npoints-1) {
      /* Found our position between points j and j+1. 
       * Interpolate: x is the amount from j+1, (1-x) from point j 
       * First treat possible jumps in temperature as a special case.
       */
      if ((opts->anneal_time[i][j+1]-opts->anneal_time[i][j]) < GMX_REAL_EPS*100)
        opts->ref_t[i]=opts->anneal_temp[i][j+1];
      else {
        x = ((thist-opts->anneal_time[i][j])/
             (opts->anneal_time[i][j+1]-opts->anneal_time[i][j]));
        opts->ref_t[i] = x*opts->anneal_temp[i][j+1]+(1-x)*opts->anneal_temp[i][j];
      }
    }
    else {
      opts->ref_t[i] = opts->anneal_temp[i][npoints-1];
    }
  }
}