// Checks if any errors occur while building Hamiltonian for both index conventions.
        public void BuildFermionHamiltonian()
        {
            var sourceHamiltonian = new OrbitalIntegralHamiltonian();

            sourceHamiltonian.Add(orbitalIntegrals);

            var targetHamiltonian0 = sourceHamiltonian.ToFermionHamiltonian(IndexConvention.HalfUp);

            var targetHamiltonian1 = sourceHamiltonian.ToFermionHamiltonian(IndexConvention.UpDown);
        }
コード例 #2
0
        static void SimulateHubbardHamiltonianTest()
        {
            //////////////////////////////////////////////////////////////////////////
            // Introduction //////////////////////////////////////////////////////////
            //////////////////////////////////////////////////////////////////////////

            // In this example, we will estimate the ground state energy of
            // 1D Hubbard Hamiltonian using the quantum chemistry library.

            // The 1D Hubbard model has `n` sites. Let `i` be the site index,
            // `s` = 1,0 be the spin index, where 0 is up and 1 is down, `t` be the
            // hopping coefficient, `u` the repulsion coefficient, and aᵢₛ the fermionic
            // annihilation operator on the fermion indexed by `(i,s)`. The Hamiltonian
            // of this model is
            //
            //     H ≔ - t Σᵢ (a†ᵢₛ aᵢ₊₁ₛ + a†ᵢ₊₁ₛ aᵢₛ) + u Σᵢ a†ᵢ₀ a†ᵢ₁ aᵢ₁ aᵢ₀
            //
            // Note that we use closed boundary conditions.

            #region Building the Hubbard Hamiltonian through orbital integrals

            var t      = 0.2; // hopping coefficient
            var u      = 1.0; // repulsion coefficient
            var nSites = 6;   // number of sites;
            // Construct Hubbard Hamiltonian
            var hubbardOrbitalIntegralHamiltonian = new OrbitalIntegralHamiltonian();

            foreach (var i in Enumerable.Range(0, nSites))
            {
                hubbardOrbitalIntegralHamiltonian.Add(new OrbitalIntegral(new[] { i, (i + 1) % nSites }, -t));
                hubbardOrbitalIntegralHamiltonian.Add(new OrbitalIntegral(new[] { i, i, i, i }, u));
            }

            // Create fermion representation of Hamiltonian
            // In this case, we use the spin-orbital to integer
            // indexing convention `x = orbitalIdx + spin * nSites`; as it
            // minimizes the length of Jordan–Wigner strings
            var hubbardFermionHamiltonian = hubbardOrbitalIntegralHamiltonian.ToFermionHamiltonian(IndexConvention.HalfUp);

            #endregion


            #region Estimating energies by simulating quantum phase estimation
            // Create Jordan–Wigner representation of Hamiltonian
            var jordanWignerEncoding = hubbardFermionHamiltonian.ToPauliHamiltonian();

            // Create data structure to pass to QSharp.
            var qSharpData = jordanWignerEncoding.ToQSharpFormat().Pad();

            Console.WriteLine($"Estimate Hubbard Hamiltonian energy:");

            #endregion
        }
コード例 #3
0
        /// <summary>
        /// Sample implementation of end-to-end electronic structure problem simulation.
        /// </summary>
        /// <param name="filename"></param>
        public static void SampleWorkflow(
            string filename,
            string wavefunctionLabel,
            IndexConvention indexConvention
            )
        {
            // Deserialize Broombridge from file.
            Data broombridge = Deserializers.DeserializeBroombridge(filename);

            // A single file can contain multiple problem descriptions. Let us pick the first one.
            var problemData = broombridge.ProblemDescriptions.First();

            #region Create electronic structure Hamiltonian
            // Electronic structure Hamiltonians are usually represented compactly by orbital integrals. Let us construct
            // such a Hamiltonian from broombridge.
            OrbitalIntegralHamiltonian orbitalIntegralHamiltonian = problemData.OrbitalIntegralHamiltonian;

            // We can obtain the full fermion Hamiltonian from the more compact orbital integral representation.
            // This transformation requires us to pick a convention for converting a spin-orbital index to a single integer.
            // Let us pick one according to the formula `integer = 2 * orbitalIndex + spinIndex`.
            FermionHamiltonian fermionHamiltonian = orbitalIntegralHamiltonian.ToFermionHamiltonian(indexConvention);

            // We target a qubit quantum computer, which requires a Pauli representation of the fermion Hamiltonian.
            // A number of mappings from fermions to qubits are possible. Let us choose the Jordan–Wigner encoding.
            PauliHamiltonian pauliHamiltonian = fermionHamiltonian.ToPauliHamiltonian(QubitEncoding.JordanWigner);
            #endregion

            #region Create wavefunction Ansatzes
            // A list of trial wavefunctions can be provided in the Broombridge file. For instance, the wavefunction
            // may be a single-reference Hartree--Fock state, a multi-reference state, or a unitary coupled-cluster state.
            // In this case, Broombridge indexes the fermion operators with spin-orbitals instead of integers.
            Dictionary <string, FermionWavefunction <SpinOrbital> > inputStates = problemData.Wavefunctions ?? new Dictionary <string, FermionWavefunction <SpinOrbital> >();

            // If no states are provided, use the Hartree--Fock state.
            // As fermion operators the fermion Hamiltonian are already indexed by, we now apply the desired
            // spin-orbital -> integer indexing convention.
            FermionWavefunction <int> inputState = inputStates.ContainsKey(wavefunctionLabel)
                ? inputStates[wavefunctionLabel].ToIndexing(indexConvention)
                : fermionHamiltonian.CreateHartreeFockState(problemData.NElectrons);
            #endregion

            #region Pipe to QSharp and simulate
            // We now convert this Hamiltonian and a selected state to a format that than be passed onto the QSharp component
            // of the library that implements quantum simulation algorithms.
            var qSharpHamiltonian  = pauliHamiltonian.ToQSharpFormat();
            var qSharpWavefunction = inputState.ToQSharpFormat();
            var qSharpData         = QSharpFormat.Convert.ToQSharpFormat(qSharpHamiltonian, qSharpWavefunction);
            #endregion
        }
コード例 #4
0
        public void JsonEncoding()
        {
            var  filename    = "Broombridge/broombridge_v0.2.yaml";
            Data broombridge = Deserializers.DeserializeBroombridge(filename);
            var  problemData = broombridge.ProblemDescriptions.First();

            OrbitalIntegralHamiltonian orbitalIntegralHamiltonian = problemData.OrbitalIntegralHamiltonian;
            FermionHamiltonian         original = orbitalIntegralHamiltonian.ToFermionHamiltonian(IndexConvention.HalfUp);

            var json = JsonConvert.SerializeObject(original);

            File.WriteAllText("fermion.original.json", json);

            var serialized = JsonConvert.DeserializeObject <FermionHamiltonian>(json);

            File.WriteAllText("fermion.serialized.json", JsonConvert.SerializeObject(serialized));

            Assert.Equal(original.SystemIndices.Count, serialized.SystemIndices.Count);
            Assert.Equal(original.Terms.Count, serialized.Terms.Count);
            Assert.Equal(original.Norm(), serialized.Norm());
            Assert.Equal(original.ToString(), serialized.ToString());
        }
コード例 #5
0
        /// <summary>
        /// Loads a FermionHamiltonian from either a .yaml file with a Broombridge definition,
        /// or from a ProblemDescription.
        /// If the fileName is specified, that will be used and the problemDescription will be ignored.
        /// </summary>
        public Task <ExecutionResult> Run(string input, IChannel channel)
        {
            if (string.IsNullOrWhiteSpace(input))
            {
                channel.Stderr("Please provide the name of a Broombridge file or a problem description to load the fermion Hamiltonian from.");
                return(Task.FromResult(ExecuteStatus.Error.ToExecutionResult()));
            }

            // Identify the ProblemDescription with the hamiltonian from the arguments.
            var args        = JsonConvert.DeserializeObject <Arguments>(input);
            var problemData = SelectProblemDescription(args);

            // Electronic structure Hamiltonians are usually represented compactly by orbital integrals. Let us construct
            // such a Hamiltonian from broombridge.
            OrbitalIntegralHamiltonian orbitalIntegralHamiltonian = problemData.OrbitalIntegralHamiltonian;

            // We can obtain the full fermion Hamiltonian from the more compact orbital integral representation.
            // This transformation requires us to pick a convention for converting a spin-orbital index to a single integer.
            // Let us pick one according to the formula `integer = 2 * orbitalIndex + spinIndex`.
            FermionHamiltonian fermionHamiltonian = orbitalIntegralHamiltonian.ToFermionHamiltonian(args.IndexConvention);

            return(Task.FromResult(fermionHamiltonian.ToExecutionResult()));
        }
コード例 #6
0
ファイル: Program.cs プロジェクト: ziqi-ma/Quantum
        static void Main(string[] args)
        {
            //////////////////////////////////////////////////////////////////////////
            // Introduction //////////////////////////////////////////////////////////
            //////////////////////////////////////////////////////////////////////////

            // In this example, we will estimate the ground state energy of
            // 1D Hubbard Hamiltonian using the quantum chemistry library.

            // The 1D Hubbard model has `n` sites. Let `i` be the site index,
            // `s` = 1,0 be the spin index, where 0 is up and 1 is down, `t` be the
            // hopping coefficient, `u` the repulsion coefficient, and aᵢₛ the fermionic
            // annihilation operator on the fermion indexed by `(i,s)`. The Hamiltonian
            // of this model is
            //
            //     H ≔ - t Σᵢ (a†ᵢₛ aᵢ₊₁ₛ + a†ᵢ₊₁ₛ aᵢₛ) + u Σᵢ a†ᵢ₀ a†ᵢ₁ aᵢ₁ aᵢ₀
            //
            // Note that we use closed boundary conditions.

            #region Building the Hubbard Hamiltonian through orbital integrals

            var t      = 0.2; // hopping coefficient
            var u      = 1.0; // repulsion coefficient
            var nSites = 6;   // number of sites;
            // Construct Hubbard Hamiltonian
            var hubbardOrbitalIntegralHamiltonian = new OrbitalIntegralHamiltonian();

            foreach (var i in Enumerable.Range(0, nSites))
            {
                hubbardOrbitalIntegralHamiltonian.Add(new OrbitalIntegral(new[] { i, (i + 1) % nSites }, -t));
                hubbardOrbitalIntegralHamiltonian.Add(new OrbitalIntegral(new[] { i, i, i, i }, u));
            }

            // Create fermion representation of Hamiltonian
            // In this case, we use the spin-orbital to integer
            // indexing convention `x = orbitalIdx + spin * nSites`; as it
            // minimizes the length of Jordan–Wigner strings
            var hubbardFermionHamiltonian = hubbardOrbitalIntegralHamiltonian.ToFermionHamiltonian(IndexConvention.HalfUp);

            #endregion


            #region Estimating energies by simulating quantum phase estimation
            // Create Jordan–Wigner representation of Hamiltonian
            var jordanWignerEncoding = hubbardFermionHamiltonian.ToPauliHamiltonian();

            // Create data structure to pass to QSharp.
            var qSharpData = jordanWignerEncoding.ToQSharpFormat().Pad();

            Console.WriteLine($"Estimate Hubbard Hamiltonian energy:");
            // Bits of precision in phase estimation.
            var bits = 7;

            // Repetitions to find minimum energy.
            var reps = 5;

            // Trotter step size
            var trotterStep = 0.5;

            using (var qsim = new QuantumSimulator())
            {
                for (int i = 0; i < reps; i++)
                {
                    // EstimateEnergyByTrotterization
                    // Name should make clear that it does it by trotterized
                    var(phaseEst, energyEst) = GetEnergy.Run(qsim, qSharpData, bits, trotterStep).Result;

                    Console.WriteLine($"Rep #{i}: Energy estimate: {energyEst}; Phase estimate: {phaseEst}");
                }
            }

            Console.WriteLine("Press Enter to continue...");
            if (System.Diagnostics.Debugger.IsAttached)
            {
                Console.ReadLine();
            }
            #endregion
        }