Hill differential equation information

In mathematics, the Hill equation or Hill differential equation is the second-order linear ordinary differential equation

{\frac {d^{2}y}{dt^{2}}}+f(t)y=0,

where $f(t)$ is a periodic function with minimal period $\pi$ and average zero. By these we mean that for all $t$

f(t+\pi )=f(t),

and

\int _{0}^{\pi }f(t)\,dt=0,

and if $p$ is a number with $0<p<\pi$ , the equation $f(t+p)=f(t)$ must fail for some $t$ .^[1] It is named after George William Hill, who introduced it in 1886.^[2]

Because $f(t)$ has period $\pi$ , the Hill equation can be rewritten using the Fourier series of $f(t)$ :

{\frac {d^{2}y}{dt^{2}}}+\left(\theta _{0}+2\sum _{n=1}^{\infty }\theta _{n}\cos(2nt)+\sum _{m=1}^{\infty }\phi _{m}\sin(2mt)\right)y=0.

Important special cases of Hill's equation include the Mathieu equation (in which only the terms corresponding to n = 0, 1 are included) and the Meissner equation.

Hill's equation is an important example in the understanding of periodic differential equations. Depending on the exact shape of $f(t)$ , solutions may stay bounded for all time, or the amplitude of the oscillations in solutions may grow exponentially.^[3] The precise form of the solutions to Hill's equation is described by Floquet theory. Solutions can also be written in terms of Hill determinants.^[1]

Aside from its original application to lunar stability,^[2] the Hill equation appears in many settings including in modeling of a quadrupole mass spectrometer,^[4] as the one-dimensional Schrödinger equation of an electron in a crystal,^[5] quantum optics of two-level systems, accelerator physics and electromagnetic structures that are periodic in space^[6] and/or in time.^[7]

^ ^a ^b Magnus, W.; Winkler, S. (2013). Hill's equation. Courier. ISBN 9780486150291.
^ ^a ^b Hill, G.W. (1886). "On the Part of the Motion of Lunar Perigee Which is a Function of the Mean Motions of the Sun and Moon". Acta Math. 8 (1): 1–36. doi:10.1007/BF02417081.
^ Teschl, Gerald (2012). Ordinary Differential Equations and Dynamical Systems. Providence: American Mathematical Society. ISBN 978-0-8218-8328-0.
^ Sheretov, Ernst P. (April 2000). "Opportunities for optimization of the rf signal applied to electrodes of quadrupole mass spectrometers.: Part I. General theory". International Journal of Mass Spectrometry. 198 (1–2): 83–96. doi:10.1016/S1387-3806(00)00165-2.
^ Casperson, Lee W. (November 1984). "Solvable Hill equation". Physical Review A. 30: 2749. doi:10.1103/PhysRevA.30.2749.
^ Brillouin, L. (1946). Wave Propagation in Periodic Structures: Electric Filters and Crystal Lattices, McGraw–Hill, New York
^ Koutserimpas, Theodoros T.; Fleury, Romain (October 2018). "Electromagnetic Waves in a Time Periodic Medium With Step-Varying Refractive Index". IEEE Transactions on Antennas and Propagation. 66 (10): 5300–5307. doi:10.1109/TAP.2018.2858200.

[hill-eq-1] Magnus, W.; Winkler, S. (2013). Hill's equation. Courier. ISBN 9780486150291.

[hill1886-2] Hill, G.W. (1886). "On the Part of the Motion of Lunar Perigee Which is a Function of the Mean Motions of the Sun and Moon". Acta Math. 8 (1): 1–36. doi:10.1007/BF02417081.

[3] Teschl, Gerald (2012). Ordinary Differential Equations and Dynamical Systems. Providence: American Mathematical Society. ISBN 978-0-8218-8328-0.

[4] Sheretov, Ernst P. (April 2000). "Opportunities for optimization of the rf signal applied to electrodes of quadrupole mass spectrometers.: Part I. General theory". International Journal of Mass Spectrometry. 198 (1–2): 83–96. doi:10.1016/S1387-3806(00)00165-2.

[5] Casperson, Lee W. (November 1984). "Solvable Hill equation". Physical Review A. 30: 2749. doi:10.1103/PhysRevA.30.2749.

[6] Brillouin, L. (1946). Wave Propagation in Periodic Structures: Electric Filters and Crystal Lattices, McGraw–Hill, New York

[7] Koutserimpas, Theodoros T.; Fleury, Romain (October 2018). "Electromagnetic Waves in a Time Periodic Medium With Step-Varying Refractive Index". IEEE Transactions on Antennas and Propagation. 66 (10): 5300–5307. doi:10.1109/TAP.2018.2858200.

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