In quantum computing, the quantum Fourier transform (for short: QFT) is a linear transformation on quantum bits, and is the quantum analogue of the discrete Fourier transform. The quantum Fourier transform is a part of many quantum algorithms, notably Shor's algorithm for factoring and computing the discrete logarithm, the quantum phase estimation algorithm for estimating the eigenvalues of a unitary operator, and algorithms for the hidden subgroup problem.
The quantum Fourier transform can be performed efficiently on a quantum computer, with a particular decomposition into a product of simpler unitary matrices. Using a simple decomposition, the discrete Fourier transform on amplitudes can be implemented as a quantum circuit consisting of only Hadamard gates and controlled phase shift gates, where is the number of qubits. This can be compared with the classical discrete Fourier transform, which takes gates (where is the number of bits), which is exponentially more than . However, the quantum Fourier transform acts on a quantum state, whereas the classical Fourier transform acts on a vector, so not every task that uses the classical Fourier transform can take advantage of this exponential speedup.
The best quantum Fourier transform algorithms known (as of late 2000) require only gates to achieve an efficient approximation.
The quantum Fourier transform is the classical discrete Fourier transform applied to the vector of amplitudes of a quantum state, where we usually consider vectors of length . The classical Fourier transform acts on a vector and maps it to the vector according to the formula
where is a Nthroot of unity.
Similarly, the quantum Fourier transform acts on a quantum state and maps it to a quantum state according to the formula:
with defined as above.
In case that is a pure state, this can also be expressed as the map
Equivalently, the quantum Fourier transform can be viewed as a unitary matrix (or a quantum gate, similar to a boolean logic gate for classical computers) acting on quantum state vectors, where the unitary matrix is given by
Since and is a primitive Nthroot of unity, we get, for example, in the case of and phase the transformation matrix
Most of the properties of the quantum Fourier transform follow from the fact that it is a unitary transformation. This can be checked by performing matrix multiplication and ensuring that the relation holds, where is the Hermitian adjoint of . Alternately, one can check that orthogonal vectors of norm 1 get mapped to orthogonal vectors of norm 1.
From the unitary property it follows that the inverse of the quantum Fourier transform is the Hermitian adjoint of the Fourier matrix, thus . Since there is an efficient quantum circuit implementing the quantum Fourier transform, the circuit can be run in reverse to perform the inverse quantum Fourier transform. Thus both transforms can be efficiently performed on a quantum computer.
The quantum gates used in the circuit are the Hadamard gate and the controlled phase gate , here in terms of
with the -th root of unity.
The quantum Fourier transform can be approximately implemented for any N; however, the implementation for the case where N is a power of 2 is much simpler. As already stated, we assume . We have the orthonormal basis consisting of the vectors
The basis states enumerate all the possible states of the qubits:
where, with tensor product notation , indicates that qubit is in state , with either 0 or 1. By convention, the basis state index orders the possible states of the qubits lexicographically, i.e., by converting from binary to decimal in this way:
It is also useful to borrow fractional binary notation:
For instance, and
With this notation, the action of the quantum Fourier transform can be expressed in a compact manner:
As can be seen, the output qubit 1 is in a superposition of state and , and so on for the other qubits (take a second look at the sketch of the circuit above).
In other words, the discrete Fourier transform, an operation on n-qubits, can be factored into the tensor product of n single-qubit operations, suggesting it is easily represented as a quantum circuit (ignoring the reverse order of outputs). In fact, each of those single-qubit operations can be implemented efficiently using a Hadamard gate and controlled phase gates. The first term requires one Hadamard gate and (n-1) controlled phase gates, the next one requires a Hadamard gate and (n-2) controlled phase gate, and each following term requires one controlled phase gate less. Summing up the number of gates gives gates, which is quadratic polynomial in the number of qubits.
Consider the quantum Fourier transform on 3 qubits. It is the following transformation:
where is a primitive eighth root of unity satisfying (since ).
For short, setting , the matrix representing of this transformation on 3 qubits is
The 3-qubit quantum Fourier transform can be rewritten as:
In case that we use the circuit we obtain the factorization in reverse order, namely
In the following sketch we have the respective circuit for and (without normalization and with wrong order of output qubits with respect to the proper QFT).
As calculated above, the number of gates used is which is equal to , for .
Moreover, the following link shows the situation for 1-, 2- and 3-qubit case: Sketch and simulator for 1-, 2- and 3-qubit QFT
- ^ Michael Nielsen and Isaac Chuang (2000). Quantum Computation and Quantum Information. Cambridge: Cambridge University Press. ISBN 0-521-63503-9. OCLC 174527496.
- ^ L. Hales, S. Hallgren, An improved quantum Fourier transform algorithm and applications, Proceedings of the 41st Annual Symposium on Foundations of Computer Science, p. 515, November 12-14, 2000 (pdf)
- K. R. Parthasarathy, Lectures on Quantum Computation and Quantum Error Correcting Codes (Indian Statistical Institute, Delhi Center, June 2001)
- John Preskill, Lecture Notes for Physics 229: Quantum Information and Computation (CIT, September 1998)