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用量子计算机模拟金融期权定价的非厄米动力学。

Simulating the non-Hermitian dynamics of financial option pricing with quantum computers.

作者信息

Kumar Swagat, Wilmott Colin Michael

机构信息

Department of Mathematics, Nottingham Trent University, Nottingham, NG11 8NS, UK.

INSAIT, Sofia University "St. Kliment Ohridski", Sofia, Bulgaria.

出版信息

Sci Rep. 2025 Apr 17;15(1):13268. doi: 10.1038/s41598-025-97245-3.

Abstract

The Schrödinger equation describes how quantum states evolve according to the Hamiltonian of the system. For physical systems, we have it that the Hamiltonian must be a Hermitian operator to ensure unitary dynamics. For anti-Hermitian Hamiltonians, the Schrödinger equation instead models the evolution of quantum states in imaginary time. This process of imaginary time evolution has been used successfully to calculate the ground state of a quantum system. Although imaginary time evolution is non-unitary, the normalised dynamics of this evolution can be simulated on a quantum computer using the quantum imaginary time evolution (QITE) algorithm. In this paper, we broaden the scope of QITE by removing its restriction to anti-Hermitian Hamiltonians, which allows us to solve any partial differential equation (PDE) that is equivalent to the Schrödinger equation with an arbitrary, non-Hermitian Hamiltonian. An example of such a PDE is the famous Black-Scholes equation that models the price of financial derivatives. We will demonstrate how our generalised QITE methodology offers a feasible approach for real-world applications by using it to price various European option contracts modelled according to the Black-Scholes equation.

摘要

薛定谔方程描述了量子态如何根据系统的哈密顿量演化。对于物理系统,我们知道哈密顿量必须是一个厄米算符,以确保幺正动力学。对于反厄米哈密顿量,薛定谔方程反而描述了量子态在虚时间中的演化。这种虚时间演化过程已成功用于计算量子系统的基态。尽管虚时间演化是非幺正的,但这种演化的归一化动力学可以使用量子虚时间演化(QITE)算法在量子计算机上进行模拟。在本文中,我们通过消除QITE对反厄米哈密顿量的限制来拓宽其范围,这使我们能够求解任何与具有任意非厄米哈密顿量的薛定谔方程等效的偏微分方程(PDE)。这样一个PDE的例子是著名的用于对金融衍生品价格进行建模的布莱克-斯科尔斯方程。我们将通过使用我们的广义QITE方法对根据布莱克-斯科尔斯方程建模的各种欧式期权合约进行定价,来展示它如何为实际应用提供一种可行的方法。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8fb7/12006387/b1e5d9cc1c51/41598_2025_97245_Fig1_HTML.jpg

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