Optimal Control of One Dimensional Quantum Harmonic Oscillator Under an External Field With Quadratic Dipole Function and Penalty on Momentum: Construction of the Linearised Field Amplitude Integral Equation

A. Kurşunlu, İrem Yaman, Metin Demiralp
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引用次数: 8

Abstract

In this work, the optimal control of an harmonic oscillator is considered. The external field is assumed to be weak and hence is represented by only dipole interaction. The dipole function is taken as a second degree polynomial in spatial coordinate. The objective term is composed of the expectation value of algebraic position operator. Penalty term related operator is taken as momentum. Some specific structures for spatial dependence is assumed and temporal equations are obtained for unknowns. The equations represent forward and backward evolution. The connection is provided by an algebraic equation coming from field amplitude related equation. The key unknown is the field amplitude since its determination leads us to evaluate all unknowns without remarkable difficulty. The purpose is not to determine field amplitude at the most general case but to construct an equation which involves this unknown only. The equation obtained via the linearisation of the field amplitude dependence is shown to be a linear integral equation. We do not attempt to solve it but discuss how to use appropriate methods for the solution. The equation is analytically solved at the zero interaction time limit. The real comprehensive implementation is left for future work. (© 2004 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim)

具有二次偶极子函数和动量惩罚的外场下一维量子谐振子的最优控制:线性化场振幅积分方程的构造
本文研究了谐振子的最优控制问题。假定外场很弱,因此只用偶极相互作用来表示。将偶极子函数作为空间坐标中的二次多项式。目标项由代数位置算子的期望值组成。将罚项相关算子作为动量。假设了空间依赖的一些特定结构,并对未知数得到了时间方程。方程表示向前和向后的演化。这种联系是由场振幅相关方程导出的代数方程提供的。关键的未知数是场振幅,因为它的确定使我们可以毫不费力地评估所有的未知数。目的不是在最一般的情况下确定场振幅,而是构造一个只涉及这个未知的方程。通过场振幅相关性的线性化得到的方程是一个线性积分方程。我们不试图解决它,而是讨论如何使用适当的方法来解决它。方程在零相互作用时间极限处解析求解。真正的全面落实留给今后的工作。(©2004 WILEY-VCH Verlag GmbH &KGaA公司,Weinheim)
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