📄 simple.cc
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// Simple harmonic oscillator, one trajectory.#include <math.h>#include <stdio.h>#include <iostream.h>#include <fstream.h>#include "ACG.h"#include "Traject.h"#include "State.h"#include "Operator.h"#include "FieldOp.h"#include "Complex.h"main(){ // Basic operators AnnihilationOperator A; NumberOperator N; Operator Ac = A.hc(); // The Hamiltonian double omega = 1.0; Operator H = omega*Ac*A; // The Lindblad operators double gamma = 1.0; const int nOfLindblads = 1; Operator L1 = gamma*A; Operator L[nOfLindblads] = {L1}; // The initial state int dim = 100; // cutoff Hilbert space dimension int n = 5; Complex alpha(1.4,-0.4); State psi(dim,n); // number state |n> // State psi(dim,alpha); // coherent state |alpha> // The random number generator int seed = 74298; ACG gen(seed,55); ComplexNormal rand1(&gen); // Stepsize and integration time double dt=0.01; // basic time step int numdts=10; // time interval between outputs = numdts*dt int numsteps=100; // total integration time = numsteps*numdts*dt double accuracy = 0.000001; AdaptiveStep theStepper(psi,H,nOfLindblads,L,accuracy); // deterministic part: adaptive stepsize 4th/5th order Runge Kutta // stochastic part: fixed stepsize Euler// AdaptiveStochStep theStepper(psi,H,nOfLindblads,L,accuracy); // deterministic part: adaptive stepsize 4th/5th order Runge Kutta // stochastic part: Euler, same (variable) stepsize as deterministic part Trajectory theTraject(psi,dt,theStepper,&rand1); // Output const int nOfOut = 2; Operator outlist[nOfOut] = {A,N}; // Operators to output char *flist[nOfOut] = {"A.out","N.out"}; // Output files int pipe[4] = {1,2,5,7}; // Standard output: // t,Re<A>,Im<A>,<N>,<N^2>-<N>^2,dim,steps // where `t' is time, `dim' is the effective dimension of Hilbert space, // and steps is the number of adaptive steps taken. // Start integration theTraject.plotExp(nOfOut,outlist,flist,pipe,numdts,numsteps);}
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