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On Fractional Schrödinger Equation and Its Application International Journal of Scientific & Engineering Research Volume 4, Issue 2, February-2013 1 ISSN 2229-5518 On Fractional Schrödinger Equation and Its Application Avik Kumar Mahata Abstract— In the note, recent efforts to derive fractional quantum mechanics are recalled. Time-space fractional Schrödinger equation with and without a Non Local term also been discussed. Applications of a fractional approach to the Schrödinger equation for free electron and potential well are discussed as well. Index Terms— Caputo Fractional Derivative, Fractional Calculus, Fractional Schrödinger Equation, Space Time Fractional Schrödinger Equation, Time- Space fractional Schrödinger like equation, Free Electron, Potential Well. 1. INTRODUCTION Specifically, they present the model of a hydrogen- The fractality concept in Quantum Mechanics like fractional atom called “fractional Bohr atom.” developed throughout the last decade. The term fractional Quantum Mechanics was first introduced Recently Herrmann has applied the fractional by Laskin [1]. The path integrals over the Lévy mechanical approach to several particular problems paths are defined and fractional quantum and statistical mechanics have been developed via new [7-12]. Some other cases of the fractional fractional path integrals approach. A fractional Schrödinger equation were discussed by Naber [13] generalization of the Schrödinger equation, new and Ben Adda & Cresson [14]. relation between the energy and the momentum of non-relativistic fractional quantum-mechanical particle has been established [1]. The concept of 2. FRACTIONAL CALCULUS fractional calculus, originated from Leibniz, has gained increasing interest during last two decades (see e.g. [2] and activity of the Fracalmo research Fractional Calculus is a field of mathematic group [3]). But the concept of fractional calculus was study that grows out of the traditional definitions of originally introduced by Leibniz, which has gained special interest in recent time. Later Laskin [4] the calculus integral and derivative operators in studied the properties of the fractional Schrödinger much the same way fractional exponents is an equation. outgrowth of exponents with integer value. Since Hermiticity of the fractional Hamilton operator the appearance of the idea of differentiation and was proved and also established the parity conservation law for fractional quantum mechanics. integration of arbitrary (not necessary integer) order As physical applications of the fractional there was not any acceptable geometric and physical Schrödinger equation he found the energy spectra of a hydrogenlike atom (fractional “Bohr atom”) and interpretation of these operations for more than 300 of a fractional oscillator in the semiclassical year. In [15], it is shown that geometric approximation. An equation for the fractional probability current density is developed and interpretation of fractional integration is”‘Shadows discussed and also discussed the relationships on the walls”’ and its Physical interpretation is” between the fractional and standard Schrödinger ‘Shadows of the past”’. I will discuss different equations. Later E.Ahmed et al. studied on the order of fractional Schrödinger equation [5]. Muslih & definition of fractional differentiation and Agrawal [6] studied the Schrödinger equation is integration below, studied in a fractional space. ———————————————— 2.1 Different Definition Avik Kumar Mahata is currently pursuing masters degree program in Material Science and Engineering in National Institute of Technology, Trichy, Tamilnadu, INDIA, PH- i) L. Euler (1730) +919786177547, E-mail: [email protected] Euler generalized the formula IJSER © 2013 http://www.ijser.org International Journal of Scientific & Engineering Research Volume 4, Issue 2, February-2013 2 ISSN 2229-5518 The popular definition of fractional calculus = ( − 1) … … ( − + 1)() is this which shows joining of the above two definitions, By using the following property of Gamma 1 () () = ( ) function, ( − ) ( − ) ( ) ( ) ( + 1 = − 1 … … − + vi) The Caputo fractional 1) ( − + 1) derivative The Caputo definition of the fractional derivative To obtain; follows the inverted sequence of operations. An ( + 1) = () ordinary differentiation is followed by the fractional ( − + 1) integration, Gamma function is defined as follows, () = ∫ () , Re(z) >0 1 ()() ( ) = () , ( − ) ( − ) ii) J.B.J Fourier (1820-22) ( − 1 ≤ < ) . By means of integral representation, vii) The fractional Schrödinger equation. 1 () = () cos(px − pz)dp The most general fractional Schrödinger equation 2 He wrote, may be obtained when, () → → = ∫ () ∫ cos px − pz + dp However, special care need to be undertaken in order to introduce canonically conjugate iii) J.Liovilli (1832-1855) observables and . The third definition of Liovilli includes 3. Space Time Fractional Schrödinger Fractional Derivative, Equation ( ) The Feynman path integral formulation of quantum () = (() ( + ℎ) + mechanics is based on a path integral over ( ) ( + 2ℎ) − ⋯ ) Brownian paths. In diffusion theory, this can also be . done to generate the standard diffusion equation; however, there are examples of many phenomena iv) G.F.B Riemann that are only properly described when non- Brownian paths are considered. When this is done, His definition of fractional integral is, the resulting diffusion equation has factional derivatives [16,17]. Due to the strong similarity () = ∫ ( − )()() + between the Schrödinger equation and the standard () diffusion equation one might expect modifications () to the Schrödinger equation generated by considering non-Brownian paths in the path integral v) Riemann-Liovilli definition derivation. This gives the time-factional, space- IJSER © 2013 http://www.ijser.org International Journal of Scientific & Engineering Research Volume 4, Issue 2, February-2013 3 ISSN 2229-5518 fractional and space–time-factional Schrödinger 4. Time-Space fractional Schrödinger equation [4, 19, and 20]. like equation In Quantum Mechanics the famous Schrödinger Lenzi and Oliveira et al. [25] analyze the is given by (in one dimension), following integer Schrödinger equation with a nonlocal term, (,) ℏ (,) ℏ = − + (, )(, ) (,) ℏ (,) ℏ = + ∫ ̅ ∫ ̅( − where ψ(x, t) and V (x, t) denote the wave function ̅, − )̅ (̅, ) (4) and the potential function, respectively. Feynman and Hibbs [21] reformulated the Schrödinger where the last term represents a nonlocal term equation by use of a path integral approach acting on the system and the kernel U(x, t). considering the Gaussian probability distribution. According to literatures [22] and [25], when a Later the time space fractional Schrödinger nonlocal term act on the fractional quantum system equation [22] obtained by Dong and Xu equation (1) can be written as the following, (in one dimension); ℏ ( ) ( ) / ( ) (ℏ) (, ) = ℏ , , = (−ℏ ∆) , + , ℏ / ℏ (,) ℏ(,) ℏ (−ℏ ∆) (, ) + (, ) (1) ( ) ̅ , + ∫ ∫ ̅( − ̅, − )(,) (5) where (, ) and (, ) are wave function and potential energy respectively, = is 5. Solution of simple system by Time “fractional quantum diffusion coefficient” with Fractional Schrodinger Equation physical dimension, 5.1 Free Electron 1− = × × = for = 2 The time fractional Schrödinger equation for And , a free particle is given by, ℏ ℏ ℏ = , = , = , = () = − (6) (2) To solve this equation, apply a Fourier transform on the spatial coordinate, are Plank length, time, mass and energy. And G and c are Gravitational constant and speed of light ((, ) = (, ) respectively and Caputo Fractional , and (−ℏ∆)/ Derivative of order is () () = (7) quantum Riesz fractional derivative [see 23,24] defined by the following, The resulting equation can be rearranged and the results of the second appendix can be used. Namely, (−ℏ∆)/(, ) = ∫ () ℏ || × ℏ the identity for the Mittag-Leffler (26,27) function ℏ ( ) with a complex argument, ∫ , , (1<α≤2) (3) IJSER © 2013 http://www.ijser.org International Journal of Scientific & Engineering Research Volume 4, Issue 2, February-2013 4 ISSN 2229-5518 () = (8) () The interesting result is when time goes to infinity. And we get, / (∞) = ℏ / (14) = { − (−) , } (9) This is the same energy spectrum that is obtained for the non-fractional Schrödinger () equation except for the factor of 1/ and the where = In Eq.(9) the first term is exponent of 1/ . Since is less than one the spacing oscillatory, and the second is decay in the time between energy levels is greater than that given by variable. Inverse Fourier transforming gives the the non-fractional Schrödinger equation. In fact the final solution, smaller the value of the greater the difference (, ) = (, ) = between energy levels. And at t = 0 the spacing between the energy levels is that same as that of the ∫ { − (−), } non-fractional Schrödinger equation. (10) This can be broken into two parts, a Schrödinger like piece divided by , and a decay term that 6. Conclusion goes to zero as time goes to infinity. Note that as goes to one the decay term goes to zero and the Complex systems (CS) are frequent in nature. Schrödinger like term becomes the non-fractional Mathematical methods can be helpful in Schrödinger term. may be chosen so that the understanding them. Motivated by the properties of initial probability is one. Due to the decay term in CS we concluded that Fractional order systems are the solution one may ask what happens
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