Two flavour boson term

2026-08-17 07:59:36 +01:00 · 2026-08-12 12:50:32 -04:00
parent 02fdff674c
commit 1c19389ba6
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+/*************************************************************************************
+
+    Grid physics library, www.github.com/paboyle/Grid
+
+    Source file: ./lib/qcd/action/pseudofermion/TwoFlavourBosonPseudoFermion.h
+
+    Copyright (C) 2026
+
+Author: Peter Boyle <pboyle@bnl.gov>
+
+    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.
+
+    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 General Public License along
+    with this program; if not, write to the Free Software Foundation, Inc.,
+    51 Franklin Street, Fifth Floor, Boston, MA 02110-1301 USA.
+
+    See the full license in the file "LICENSE" in the top level distribution directory
+*************************************************************************************/
+/*  END LEGAL */
+#pragma once
+
+NAMESPACE_BEGIN(Grid);
+
+///////////////////////////////////////////////////////////////////////////////
+// Two flavour BOSON (wrong-sign) pseudofermion for any FermionOperator B:
+//
+//    S2 = chi^dag Bdag B chi = |B chi|^2
+//
+//    integral  ==>  det( Bdag B )^-1 = |det B|^-2
+//
+// A compensator monomial: supplies an INVERSE determinant with NO solve in
+// the force or the action -- both are matrix multiplies.  The only solve is
+// the heatbath  chi = B^-1 eta,  once per trajectory (for B = the
+// Pauli-Villars operator this is a mass-one solve, trivially cheap).
+//
+// Primary use: two instances with B = PV cancel the |det PV|^2 excess of
+// TwoFlavourPVdagMPseudoFermionAction down to the DWF quotient
+// |det M|^2/|det PV|^2 (two unsquared instances rather than one squared
+// kernel: first powers of PV in the force, milder).  Being generic in B it
+// also serves Hasenbusch-chain compensation at intermediate masses, or any
+// future inverse-det bookkeeping.  (Sibling of the domain-decomposed boson
+// in DomainDecomposedBoundaryTwoFlavourBosonPseudoFermion.h, without the
+// boundary machinery.)
+//
+// Heatbath exact by construction: S2 after refresh = |B B^-1 eta|^2 = |eta|^2.
+///////////////////////////////////////////////////////////////////////////////
+template<class Impl>
+class TwoFlavourBosonPseudoFermionAction : public Action<typename Impl::GaugeField> {
+public:
+  INHERIT_IMPL_TYPES(Impl);
+
+private:
+  FermionOperator<Impl> & BOp;  // the operator whose |det|^-2 is supplied
+
+  LinearFunction<FermionField> &HeatbathSolver; // b -> B^-1 b (heatbath only)
+
+  FermionField Chi; // the pseudo fermion field for this trajectory
+
+public:
+  TwoFlavourBosonPseudoFermionAction(FermionOperator<Impl>  &_BOp,
+				     LinearFunction<FermionField> & HS
+				     ) : BOp(_BOp),
+					 HeatbathSolver(HS),
+					 Chi(_BOp.FermionGrid())
+  {};
+
+  virtual std::string action_name(){return "TwoFlavourBosonPseudoFermionAction";}
+
+  virtual std::string LogParameters(){
+    std::stringstream sstream;
+    sstream << GridLogMessage << "["<<action_name()<<"] has no parameters" << std::endl;
+    return sstream.str();
+  }
+
+  virtual void refresh(const GaugeField &U, GridSerialRNG &sRNG, GridParallelRNG& pRNG) {
+    // P(chi) = e^{- chi^dag BdagB chi} ; chi = B^-1 eta ; P(eta) = e^{-eta^dag eta}
+    // e^{-x^2/2 sig^2} => sig^2 = 0.5 ; eta enters with width 1/sqrt(2).
+    RealD scale = std::sqrt(0.5);
+    FermionField eta(BOp.FermionGrid());
+    gaussian(pRNG,eta);
+    eta = eta * scale;
+    refresh(U,eta);
+  }
+
+  // Deterministic-noise variant (test hook):
+  // after this,  S(U) == norm2(eta)  exactly (to solver tolerance).
+  void refresh(const GaugeField &U, const FermionField &eta) {
+    BOp.ImportGauge(U);
+    Chi = Zero();
+    HeatbathSolver(eta,Chi);       // Chi = B^-1 eta : the ONLY solve
+    std::cout << GridLogMessage << action_name() << " refresh |Chi|^2 = "<< norm2(Chi)<<std::endl;
+  }
+
+  //////////////////////////////////////////////////////
+  // S2 = |B chi|^2  -- matrix multiply only
+  //////////////////////////////////////////////////////
+  virtual RealD S(const GaugeField &U) {
+    BOp.ImportGauge(U);
+
+    FermionField w(BOp.FermionGrid());
+    BOp.M(Chi,w);                  // w = B chi
+    RealD action = norm2(w);
+    return action;
+  }
+
+  //////////////////////////////////////////////////////
+  // dS2 = chi^dag dBdag w + w^dag dB chi ,   w = B chi
+  // NO solves.
+  //////////////////////////////////////////////////////
+  virtual void deriv(const GaugeField &U,GaugeField & dSdU) {
+    BOp.ImportGauge(U);
+
+    FermionField w(BOp.FermionGrid());
+    GaugeField force(BOp.GaugeGrid());
+
+    BOp.M(Chi,w);                  // w = B chi
+
+    BOp.MDeriv(force, Chi, w, DaggerYes); dSdU =      force;
+    BOp.MDeriv(force, w, Chi, DaggerNo ); dSdU = dSdU+force;
+
+    dSdU *= -1.0;  // Grid action sign convention (cf TwoFlavourRatio.h)
+  };
+};
+
+NAMESPACE_END(Grid);