Study of Adaptative Derivative-Assemble Pseudo-Trotter Ansatzes in VQE through qiskit API Max Alteg Baptiste Chevalier Octave MestoudjianJohan-Luca Rossi

2025-05-02 0 0 1.48MB 34 页 10玖币
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Study of Adaptative Derivative-Assemble
Pseudo-Trotter Ansatzes in VQE through qiskit API
Max Alteg, Baptiste Chevalier, Octave Mestoudjian,Johan-Luca Rossi
April 2022
arXiv:2210.15438v1 [quant-ph] 25 Oct 2022
Contents
1 Theoretical Background 5
1.1 QuantumChemistry .............................. 5
1.1.1 Hamiltonian and Born-Oppenheimer approximation . . . . . . . . . 5
1.1.2 Spin-orbital and Slater determinant . . . . . . . . . . . . . . . . . . 6
1.1.3 First and Second Quantization of the Hamiltonian . . . . . . . . . . 6
1.1.4 Mapping................................. 7
1.2 Ansatzes..................................... 8
1.2.1 Introduction : Variational Method . . . . . . . . . . . . . . . . . . 8
1.2.2 Hardware Efficient Ansatz . . . . . . . . . . . . . . . . . . . . . . . 9
1.2.3 Unitary-Coupled Cluster Ansatz . . . . . . . . . . . . . . . . . . . . 11
1.2.4 ADAPT-VQE.............................. 14
1.3 OtheraspectsofVQE ............................. 16
1.3.1 Classical Optimisers . . . . . . . . . . . . . . . . . . . . . . . . . . 16
1.3.2 BarrenPlateau ............................. 18
2 Implementation 19
2.1 Qiskit general framework . . . . . . . . . . . . . . . . . . . . . . . . . . . . 20
2.1.1 Hamiltonian Mapping . . . . . . . . . . . . . . . . . . . . . . . . . 20
2.1.2 Operators representation . . . . . . . . . . . . . . . . . . . . . . . . 20
2.1.3 Aersimulator .............................. 21
2.1.4 VQE................................... 21
2.2 Pre-existingAnsatz............................... 21
2.2.1 HardwareEcient ........................... 21
2.2.2 UCCSD ................................. 21
2.3 ADAPT-VQE development . . . . . . . . . . . . . . . . . . . . . . . . . . . 21
2.3.1 Fermionic-ADAPT-VQE . . . . . . . . . . . . . . . . . . . . . . . . 22
2.3.2 Qubit-ADAPT-VQE . . . . . . . . . . . . . . . . . . . . . . . . . . 22
2.3.3 QEB-ADAPT-VQE........................... 23
3 Results and discussion 24
3.1 Comparison of various HEA . . . . . . . . . . . . . . . . . . . . . . . . . . 24
3.2 Evaluation of the accuracy of UCCSD . . . . . . . . . . . . . . . . . . . . . 26
1
3.3 Comparison of ADAPT-VQE Methods . . . . . . . . . . . . . . . . . . . . 28
3.3.1 Results for H2.............................. 28
3.3.2 Results for LiH ............................. 29
2
Introduction
The solution of the time-independent Schrodinger equation for molecular systems allows
for the prediction of chemical properties. Quantum Computers are expected to make
possible the simulation of quantum systems more efficiently and accurately than classical
ones, including the simulation of molecules. This is due to the exponential size of the
Hilbert Space.
The first algorithm which has been proposed to solve the problem of simulating elec-
tronic structure on a Quantum Computer is well-known as the Phase Estimation Algo-
rithm (PEA). Despite that PEA gives the exact ground state for a given problem, the long
circuit and the complex gates used in this algorithm make it impractical on any current
or near-term Quantum Hardware referred as NISQ (Noisy intermediate Scale Quantum)
devices.
In order to answer the problem of NISQ era and allows one to outperform classical comput-
ers, Variational Quantum Algorithms (VQAs) were designed. VQAs are hybrid classical-
quantum algorithms due to the fact that there are using a quantum hardware for com-
putation while using a classical optimizer for optimization. In this way, VQA algorithms
allows the creation of shallower circuits and are thus much more noise resilient. The VQA
algorithm we are interested in is the so-called Variational Quantum Eigensolver (VQE)
algorithm and was originally designed to simulate electronic structures and to compute
the ground state of a given molecule.
VQE is made of two main components. First, an ansatz which has several tunable param-
eters and his associated quantum circuit. The ansatz is run on the quantum device and
aim to simulate the wavefunction, the parameters of the ansatz will be optimize until the
expectation value is minimum meaning that one has found the ground state. The second
component is then the classical optimizer, it is run on a classical computer and is the often
the same as the one used in Machine Learning. At this point, it is clear that if there is a
limiting factor for VQE it can only be the ansatz.
The very first ansatz that has originally been used is called UCCSD and it is based on
Coupled Cluster Theory truncated at single and double excitations. One other way that
has been investigated alongside is the Hardware efficient ansatz (HEA) which was de-
signed to be efficiently implemented on NISQ devices but is not as efficient as UCCSD.
3
The main issue considering UCCSD is the large amount of parameters to optimize and
this leads us to the introduction of Adaptive Derivative-Assembled Pseudo-Trotter ansatz
VQE (ADAPT-VQE) which determines a quasi-optimal ansatz with a minimal number of
parameters.
Unlike ansatzes introduced above, the key point of ADAPT-VQE is to grow the ansatz at
every step, by adding operators chosen from a pre-determined pool of operators one-at-a-
time, assuring that the maximal amount of correlation energy is recovered at each step.
There exists different kind of ADAPT-VQE depending on the starting pool of operators as
the fermionic-ADAPT, the qubit-ADAPT or even the qubit excitation based (QEB).
The goal of this project is to implement the different types of ADAPT-VQE mentioned
before. After being sure to understand the theoretical background under all of these
concepts, we will implement each algorithm using quiskit. We will also compare all of
these algorithms on different criterions such as the number of parameters, the accuracy
or the number of CNOT gate used on H2and LiH molecules. Then we will have a small
discussion about the results we obtained.
4
摘要:

StudyofAdaptativeDerivative-AssemblePseudo-TrotterAnsatzesinVQEthroughqiskitAPIMaxAlteg,BaptisteChevalier,OctaveMestoudjian,Johan-LucaRossiApril2022Contents1TheoreticalBackground51.1QuantumChemistry..............................51.1.1HamiltonianandBorn-Oppenheimerapproximation.........51.1.2Spin-orb...

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