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#REDIRECT[[Continuous-variable quantum information]]
'''Continuous Quantum Computation''' Two major motivations for studying continuous quantum computation are:
* Many scientific problems have continuous mathematical formulations. Exaples of such formulations are
** Path integration
** [[Feynman-Kac]] path integration
** [[Schrödinger]] equation
* In their standard monograph Nielsen and Chuang state "Of particular interest is a decisive answer to the problem whether quantum computers are more powerful than classical computers." To answer this question one must know the classical and quantum computationsl complexities
In the section An Example: Path Integration solving a continuous problem on a quantum computer will be discussed. Here the second motivation will be amplified. By computational complexity (complexity for brevity) is meant the '''minimal''' computational resources needed to solve a problem. Two of the most important resources for quantum computing are qubits and queries. Classical complexity has been extensively studied in [[Information-Based Complexity| informations-based complexity]]. The classical complexity of many continuous problems is known. Therefore, when the quantum complexity of these problems is obtained, the question as to whether quantum computers are more powerful than classical can be answered. Furthermore, it can be established how much more powerful. In contrast, the complexity of discrete problems is typically unknown; one has to settle for the complexity hierarchy. For example, the classical complexity of integrer factorization is unknown.
===An Example: Path Integration===
Path integration has numerous applications including quantum mechanics, quantum chemistry, statistical mechanics, and computational complexity. We want to compute an approximation to within error at most <math>\epsilon</math> with probability, say, at least 3/4. Then the following was shown by Traub and Woźniakowski:
* A quantum computer enjoys exponential speedup over the classical worst case and quadratic speedup over the classical randomized case.
* The query complexity is of order <math>\epsilon^{-1}</math>.
* The qubit complexity is of order <math>\epsilon^{-2}\log\epsilon^{-1}</math>.
Thus the qubit complexity of path integration is a second degree polynomial in <math>\epsilon^{-1}</math> That seems pretty good but we probably won't have enough qubits for a long time to do new science especially with error correction. Since this is a complexity result we can't do better by inventing a clever new algorithm. But perhaps we can do better by changing the formalrules of quantum computation.
In the standard model of quantum computation the only probabilistic nature of quantum computation only enters through measurement; the queries are deterministic. As an analogy to classica Monte Carlo Woźniakowski introduced the idea of a quantum setting with randomized queries. He showed that in this setting the qubit complexity is of order <math> \log\epsilon^{-1}</math>, thus achieving an exponential improvement over the qubit complexity in the standard quantum computing setting.
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