Quantum algorithm

Deutsch–Jozsa algorithm

The Deutsch–Jozsa algorithm solves a black-box problem that requires exponentially many queries to the black box for any deterministic classical computer, but can be done with a single query by a quantum computer. However, when comparing bounded-error classical and quantum algorithms, there is no speedup, since a classical probabilistic algorithm can solve the problem with a constant number of queries with small probability of error. The algorithm determines whether a function f is either constant (0 on all inputs or 1 on all inputs) or balanced (returns 1 for half of the input domain and 0 for the other half).

Bernstein–Vazirani algorithm

The Bernstein–Vazirani algorithm is the first quantum algorithm that solves a problem more efficiently than the best known classical algorithm. It was designed to create an oracle separation between BQP and BPP.

Simon's algorithm

Simon's algorithm solves a black-box problem exponentially faster than any classical algorithm, including bounded-error probabilistic algorithms. This algorithm, which achieves an exponential speedup over all classical algorithms that we consider efficient, was the motivation for Shor's algorithm for factoring.

Quantum phase estimation algorithm

The quantum phase estimation algorithm is used to determine the eigenphase of an eigenvector of a unitary gate, given a quantum state proportional to the eigenvector and access to the gate. The algorithm is frequently used as a subroutine in other algorithms.

Shor's algorithm

Shor's algorithm solves the discrete logarithm problem and the integer factorization problem in polynomial time,^[9] whereas the best known classical algorithms take super-polynomial time. It is unknown whether these problems are in P or NP-complete. It is also one of the few quantum algorithms that solves a non-black-box problem in polynomial time, where the best known classical algorithms run in super-polynomial time.

Hidden subgroup problem

The abelian hidden subgroup problem is a generalization of many problems that can be solved by a quantum computer, such as Simon's problem, solving Pell's equation, testing the principal ideal of a ring R and factoring. There are efficient quantum algorithms known for the Abelian hidden subgroup problem.^[10] The more general hidden subgroup problem, where the group is not necessarily abelian, is a generalization of the previously mentioned problems, as well as graph isomorphism and certain lattice problems. Efficient quantum algorithms are known for certain non-abelian groups. However, no efficient algorithms are known for the symmetric group, which would give an efficient algorithm for graph isomorphism^[11] and the dihedral group, which would solve certain lattice problems.^[12]

Estimating Gauss sums

A Gauss sum is a type of exponential sum. The best known classical algorithm for estimating these sums takes exponential time. Since the discrete logarithm problem reduces to Gauss sum estimation, an efficient classical algorithm for estimating Gauss sums would imply an efficient classical algorithm for computing discrete logarithms, which is considered unlikely. However, quantum computers can estimate Gauss sums to polynomial precision in polynomial time.^[13]

Fourier fishing and Fourier checking

Consider an oracle consisting of n random Boolean functions mapping n-bit strings to a Boolean value, with the goal of finding n n-bit strings z₁,..., z_n such that for the Hadamard-Fourier transform, at least 3/4 of the strings satisfy

${\displaystyle |{\tilde {f}}(z_{i})|\geqslant 1}$

and at least 1/4 satisfy

${\displaystyle |{\tilde {f}}(z_{i})|\geqslant 2.}$

This can be done in bounded-error quantum polynomial time (BQP).^[14]

Grover's algorithm

Grover's algorithm searches an unstructured database (or an unordered list) with N entries for a marked entry, using only ${\displaystyle O({\sqrt {N}})}$ queries instead of the ${\displaystyle O({N})}$ queries required classically.^[16] Classically, ${\displaystyle O({N})}$ queries are required even allowing bounded-error probabilistic algorithms.

Theorists have considered a hypothetical generalization of a standard quantum computer that could access the histories of the hidden variables in Bohmian mechanics. (Such a computer is completely hypothetical and would not be a standard quantum computer, or even possible under the standard theory of quantum mechanics.) Such a hypothetical computer could implement a search of an N-item database in at most ${\displaystyle O({\sqrt[{3}]{N}})}$ steps. This is slightly faster than the ${\displaystyle O({\sqrt {N}})}$ steps taken by Grover's algorithm. However, neither search method would allow either model of quantum computer to solve NP-complete problems in polynomial time.^[17]

Quantum counting

Quantum counting solves a generalization of the search problem. It solves the problem of counting the number of marked entries in an unordered list, instead of just detecting whether one exists. Specifically, it counts the number of marked entries in an ${\displaystyle N}$-element list with an error of at most ${\displaystyle \varepsilon }$ by making only ${\displaystyle \Theta \left(\varepsilon ^{-1}{\sqrt {N/k}}\right)}$ queries, where ${\displaystyle k}$ is the number of marked elements in the list.^[18][19] More precisely, the algorithm outputs an estimate ${\displaystyle k'}$ for ${\displaystyle k}$, the number of marked entries, with accuracy ${\displaystyle |k-k'|\leq \varepsilon k}$.

Boson sampling problem

The Boson Sampling Problem in an experimental configuration assumes^[23] an input of bosons (e.g., photons) of moderate number that are randomly scattered into a large number of output modes, constrained by a defined unitarity. When individual photons are used, the problem is isomorphic to a multi-photon quantum walk.^[24] The problem is then to produce a fair sample of the probability distribution of the output that depends on the input arrangement of bosons and the unitarity.^[25] Solving this problem with a classical computer algorithm requires computing the permanent of the unitary transform matrix, which may take a prohibitively long time or be outright impossible. In 2014, it was proposed^[26] that existing technology and standard probabilistic methods of generating single-photon states could be used as an input into a suitable quantum computable linear optical network and that sampling of the output probability distribution would be demonstrably superior using quantum algorithms. In 2015, investigation predicted^[27] the sampling problem had similar complexity for inputs other than Fock-state photons and identified a transition in computational complexity from classically simulable to just as hard as the Boson Sampling Problem, depending on the size of coherent amplitude inputs.

Element distinctness problem

The element distinctness problem is the problem of determining whether all the elements of a list are distinct. Classically, ${\displaystyle \Omega (N)}$ queries are required for a list of size ${\displaystyle N}$; however, it can be solved in ${\displaystyle \Theta (N^{2/3})}$ queries on a quantum computer. The optimal algorithm was put forth by Andris Ambainis,^[28] and Yaoyun Shi first proved a tight lower bound when the size of the range is sufficiently large.^[29] Ambainis^[30] and Kutin^[31] independently (and via different proofs) extended that work to obtain the lower bound for all functions.

Triangle-finding problem

The triangle-finding problem is the problem of determining whether a given graph with N vertices contains a triangle (a clique of size 3). Given oracle access to the adjacency matrix of the graph, the classical query complexity is ${\displaystyle \Theta (N^{2})}$, since for a graph with only one triangle this is the query complexity needed to find any edge at all. Meanwhile, for quantum algorithms the lower bound is ${\displaystyle \Omega (N)}$, the number of queries needed to find any edge with Grover's algorithm. However, finding any edge does not guarantee finding a triangle if there exists any. A Grover search over all ${\displaystyle \Theta (N^{3})}$ potential triangles does solve the problem, but the query complexity, O(N^3/2), can be improved upon.^[32]

While ${\displaystyle \Omega (N)}$ remains the best-known lower bound for quantum algorithms, the best algorithm known requires O(N^5/4) queries,^[33] an improvement over the previous best O(N^1.3) queries.^[22][34]

Formula evaluation

A formula is a tree with a gate at each internal node and an input bit at each leaf node. The problem is to evaluate the formula, which is the output of the root node, given oracle access to the input.

A well studied formula is the balanced binary tree with only NAND gates.^[35] This type of formula requires ${\displaystyle \Theta (N^{c})}$ queries using randomness,^[36] where ${\displaystyle c=\log _{2}(1+{\sqrt {33}})/4\approx 0.754}$. With a quantum algorithm, however, it can be solved in ${\displaystyle \Theta (N^{1/2})}$ queries. No better quantum algorithm for this case was known until one was found for the unconventional Hamiltonian oracle model.^[7] The same result for the standard setting soon followed.^[37]

Fast quantum algorithms for more complicated formulas are also known.^[38]

Group commutativity

The problem is to determine if a black-box group, given by k generators, is commutative. A black-box group is a group with an oracle function, which must be used to perform the group operations (multiplication, inversion, and comparison with identity). The interest in this context lies in the query complexity, which is the number of oracle calls needed to solve the problem. The deterministic and randomized query complexities are ${\displaystyle \Theta (k^{2})}$ and ${\displaystyle \Theta (k)}$, respectively.^[39] A quantum algorithm requires ${\displaystyle \Omega (k^{2/3})}$ queries, while the best-known classical algorithm uses ${\displaystyle O(k^{2/3}\log k)}$ queries.^[40]

Computing knot invariants

Witten had shown that the Chern-Simons topological quantum field theory (TQFT) can be solved in terms of Jones polynomials. A quantum computer can simulate a TQFT, and thereby approximate the Jones polynomial,^[42] which as far as we know, is hard to compute classically in the worst-case scenario.^{[citation needed]}

Quantum simulation

The idea that quantum computers might be more powerful than classical computers originated in Richard Feynman's observation that classical computers seem to require exponential time to simulate many-particle quantum systems, yet quantum many-body systems are able to "solve themselves."^[43] Since then, the idea that quantum computers can simulate quantum physical processes exponentially faster than classical computers has been greatly fleshed out and elaborated. Efficient (i.e., polynomial-time) quantum algorithms have been developed for simulating both Bosonic and Fermionic systems,^[44] as well as the simulation of chemical reactions beyond the capabilities of current classical supercomputers using only a few hundred qubits.^[45] Quantum computers can also efficiently simulate topological quantum field theories.^[46] In addition to its intrinsic interest, this result has led to efficient quantum algorithms for estimating quantum topological invariants such as Jones^[47] and HOMFLY polynomials,^[48] and the Turaev-Viro invariant of three-dimensional manifolds.^[49]

Solving a linear system of equations

In 2009, Aram Harrow, Avinatan Hassidim, and Seth Lloyd, formulated a quantum algorithm for solving linear systems. The algorithm estimates the result of a scalar measurement on the solution vector to a given linear system of equations.^[50]

Provided that the linear system is sparse and has a low condition number ${\displaystyle \kappa }$, and that the user is interested in the result of a scalar measurement on the solution vector (instead of the values of the solution vector itself), then the algorithm has a runtime of ${\displaystyle O(\log(N)\kappa ^{2})}$, where ${\displaystyle N}$ is the number of variables in the linear system. This offers an exponential speedup over the fastest classical algorithm, which runs in ${\displaystyle O(N\kappa )}$ (or ${\displaystyle O(N{\sqrt {\kappa }})}$ for positive semidefinite matrices).

QAOA

The quantum approximate optimization algorithm takes inspiration from quantum annealing, performing a discretized approximation of quantum annealing using a quantum circuit. It can be used to solve problems in graph theory.^[52] The algorithm makes use of classical optimization of quantum operations to maximize an "objective function."

Variational quantum eigensolver

The variational quantum eigensolver (VQE) algorithm applies classical optimization to minimize the energy expectation value of an ansatz state to find the ground state of a Hermitian operator, such as a molecule's Hamiltonian.^[53] It can also be extended to find excited energies of molecular Hamiltonians.^[54]

Contracted quantum eigensolver

The contracted quantum eigensolver (CQE) algorithm minimizes the residual of a contraction (or projection) of the Schrödinger equation onto the space of two (or more) electrons to find the ground- or excited-state energy and two-electron reduced density matrix of a molecule.^[55] It is based on classical methods for solving energies and two-electron reduced density matrices directly from the anti-Hermitian contracted Schrödinger equation.^[56]

Surveys

• Dalzell, Alexander M.; et al. (2025). Quantum Algorithms. arXiv:2310.03011. doi:10.1017/9781009639651. ISBN 978-1-009-63965-1.
• Smith, J.; Mosca, M. (2012). "Algorithms for Quantum Computers". Handbook of Natural Computing. pp. 1451–1492. arXiv:1001.0767. doi:10.1007/978-3-540-92910-9_43. ISBN 978-3-540-92909-3. S2CID 16565723.
• Childs, A. M.; Van Dam, W. (2010). "Quantum algorithms for algebraic problems". Reviews of Modern Physics. 82 (1): 1–52. arXiv:0812.0380. Bibcode:2010RvMP...82....1C. doi:10.1103/RevModPhys.82.1. S2CID 119261679.