Periodic and constant solutions of matrix Riccati differential equations: n — 2. Proc. Roy. Sur 1’equation differentielle matricielle de type Riccati. Bull. Math. The qualitative study of second order linear equations originated in the classic paper . for a history of the Riccati transformation. Differentielle. (Q(t),’)’. VESSIOT, E.: “Sur quelques equations diffeYentielles ordinaires du second ordre .” Annales de (3) “Sur l’equation differentielle de Riccati du second ordre.
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Retrieved from ” https: In this paper we present a Galoisian approach of how to find explicit propagators through Liouvillian solutions for linear second order differential equations equationn to Riccati equations.
Yariv, Quantum fluctuations and noise in parametric processes: Remember me on this computer. Sometimes, we also use a cookie to keep track of your trolley contents. In fact, they present a non-periodic solution that allows us to write the propagator explicitly; the fact of the solution being non-periodic is fundamental.
Theorem 9 Galoisian approach to Idfferentielle. It follows the construction of the propagators related with these ddifferentielle conditions. This doesn’t mean that anyone who uses your computer can access your account information as we separate association what the cookie provides from authentication.
Help Center Find new research papers in: For example, at loot. We denote by G0 the connected component of the identity, thus, when G0 satisfies some property, we say that G virtually satisfies such property. The steady-state non-dynamic version of these is referred to as the algebraic Riccati equation. Morales-Ruiz for their useful comments, suggestions and great hospitality.
Now, we summarize the cases one and two of Kovacic Algorithm that will be used in Section 4. Toy models inspired by integrable Riccati equations. This is different to construct the explicit propagators know- ing apriory the solutions of the Riccatti or characteristic equation, which can open other possibilities to study propagator with special functions as characteristic equations, for example, Heun equation.
Now, we study the integrability, in Galoisian sense, of this equation through Kovacic Algorithm. Afterward, we con- struct the corresponding propagator associated to this characteristic equa- tion. The solutions obtained throgh such towers are called Liouvillian. The Hamiltonian 2 had also been considered by Angelow and Trifonov [4, 5] in order to describe the light propagation in a nonlinear anisotropic waveguide. From Wikipedia, the free encyclopedia. To access your account information you need to be authenticated, which means that you need to enter your password to confirm that you are indeed the person that the cookie claims you to be.
Thus, we mean by inte- grable whenever the differential equation has Liouvillian solutions instead of special functions solutions. Suslov, The Cauchy problem for a forced harmonic oscillatorPreprint arXiv: Differential Galois group, Green functions, propagators, Ric- cati equation.
In both cases you should know how to switch cookies back on! Propagators and Green Functions. Orszag, Quantum OpticsSpringer, Heidelberg, In virtue of Theorem 9 we can construct many Liouvillian propagators through integrable second order differential equations over a dif- ferential field as well by algebraic solutions, over such differential field, of Riccati equations. Cookies come in two flavours – persistent and transient.
If Pn does not exist, then case 2 cannot hold. The non-linear Riccati equation can always be reduced to a second order linear ordinary differential equation ODE: This Galoisian structure depends on the nature of the solutions of the differential equation; for instance, one obtains some kind of solvability virtual for the Galois group whenever one obtains Liouvillian solutions, and in this case one says that the differential equation is inte- grable.
In this section we find solutions to 4.
Theorem 2 Lie-Kolchin Theorem. Transient cookies are kept in RAM and are deleted either when you close all your browser windows, or when you reboot your computer.
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Furthermore, by Proposition 4, departing from the differential equation 17 we can arrive at the Riccati equation 15 through changes wquation variables. Galoisian Approach to Propagators In this equatio we apply the Picard-Vessiot theory in the context of propagators. Translation of differebtielle original Latin into English by Ian Bruce. Views Read Edit View history. We can see that applying by hand Kovacic Differrntielle it can be a lit- tle difficults, but thanks to has been implemented it in Maple command kovacicsols we can avoid such calculations.
The Galois theory of differential equations, also called Differential Galois Theory and Picard-Vessiot The- ory, has been developed by Picard, Vessiot, Kolchin and currently by a lot of researchers, see [2, 3, 15, 16, 17, 25, 38].
Suslov, Propagator of a charged particle with a spin in uniform magnetic and perpendicular electric fields, Lett.
This is the practical aim of this paper, which will be given in Section 4 and in Section 5. Suslov, Models of damped oscillators in quantum mechanics, Journal of Physical Mathematics 1S 16 pages. Click here to sign up.
As in , we obtain three conditions for n to get virtual solv- ability of the differential Galois group. To study Liouvillian solutions for linear second order differential equations, as well the integrability of their associated Riccati equations, we use Kovacic algorithm see  and an algebrization procedure see [1, 3].
We consider the differential Galois theory in the context of second order linear differential equations. Primary 81Q05; Secondary 12H We use the Galoisian approach to LSE, Theorem 9, to generalize examples introduced in  as well as to introduce toy examples. We present a short summary of the Hamiltonian algebrization process that will be used in Section 4. Else, case 1 cannot hold.