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@PHDTHESIS{Mehta:1026467,
author = {Mehta, Vrinda},
title = {{Q}uantum annealing and its variants: {A}pplication to
quadratic unconstrained binary optimization},
volume = {59},
school = {RWTH Aachen University},
type = {Dissertation},
address = {Jülich},
publisher = {Forschungszentrum Jülich GmbH Zentralbibliothek, Verlag},
reportid = {FZJ-2024-03411},
isbn = {978-3-95806-755-4},
series = {Schriften des Forschungszentrums Jülich IAS Series},
pages = {iii, 152},
year = {2024},
note = {Dissertation, RWTH Aachen University, 2023},
abstract = {In this thesis, we study the performance of the numerical
implementation of quantum annealing, as well as of physical
quantum annealing systems from D-Wave Quantum Systems Inc.,
for solving 2-Satisfiability (2-SAT) and other quadratic
unconstrained binaryoptimization (QUBO) problems. For
gauging the suitability of quantum annealing for solving
these problems, we use three main metrics: the probability
of the algorithm to solve the problem, its ability to find
all the solutions to the problem if the problem has more
than one solution, and the scaling of the time to solution
as a function of the problem size. In doing so, we compare
the performance of the numerically simulated ideal quantum
annealing with its actual physical realization. We find that
the ideal, standard quantum annealing algorithm can solve
the sets of 2-SAT problems considered in this work, even if
with a low success probability for hard problems, and can
sample the degenerate ground states of the 2-SAT problems
with multiple satisfying assignments in accordance with
perturbation theory. However, in the long annealing time
limit, the ideal standard annealing algorithm leads to a
scaling of the time to solution that is worse compared to
even the simple enumeration of all the possible states. On
the other hand, we find noise and temperature effects to
play an active role in the evolution of the state of the
system on the D-Wave quantum annealers. These systems can
solve a majority of the studied problems with a relatively
large success probability, and the scaling of the time to
solution, though still growing exponentially in the system
size, is significantly improved. Next, by means of
simulations, we introduce two modifications in the standard
quantum annealing algorithm, and gauge the performance of
the modified algorithms. These modifications are the
addition of a trigger Hamiltonian to the standard quantum
annealing Hamiltonian, or a change in the initial
Hamiltonian of the annealing Hamiltonian. We choose the
trigger Hamiltonian to have either ferromagnetic or
antiferromagnetic transverse couplings, while the additional
higher-order couplings added to the typically chosen initial
Hamiltonian are ferromagnetic. We find that these
modifications can lead to significant improvements in the
performance of the annealing algorithm, even if the scaling
behavior is still exponential.},
cin = {JSC},
cid = {I:(DE-Juel1)JSC-20090406},
pnm = {5111 - Domain-Specific Simulation $\&$ Data Life Cycle Labs
(SDLs) and Research Groups (POF4-511)},
pid = {G:(DE-HGF)POF4-5111},
typ = {PUB:(DE-HGF)3 / PUB:(DE-HGF)11},
urn = {urn:nbn:de:0001-20241209125135062-9549579-4},
doi = {10.34734/FZJ-2024-03411},
url = {https://juser.fz-juelich.de/record/1026467},
}