2011
DOI: 10.4236/jqis.2011.11002
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Application of Scale Relativity (ScR) Theory to the Problem of a Particle in a Finite One-Dimensional Square Well (FODSW) Potential

Abstract: In the present work, and along the lines of Hermann, ScR theory is applied to a finite one-dimensional square well potential problem. The aim is to show that scale relativity theory can reproduce quantum mechanical results without employing the Schrödinger equation. Some mathematical difficulties that arise when obtaining the solution to this problem were overcome by utilizing a novel mathematical connection between ScR theory and the well-known Riccati equation. Computer programs were written using the standa… Show more

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Cited by 10 publications
(8 citation statements)
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“…The validity of SR not restricted to the cases by Hermann [14] and Alrashid [18] [19] [20]. Besides, such applications are expected to reveal some novel concepts, such as the connection between SR and the Riccati equation [21] [22] [23] as revealed in the present work.…”
Section: Introductionmentioning
confidence: 83%
See 1 more Smart Citation
“…The validity of SR not restricted to the cases by Hermann [14] and Alrashid [18] [19] [20]. Besides, such applications are expected to reveal some novel concepts, such as the connection between SR and the Riccati equation [21] [22] [23] as revealed in the present work.…”
Section: Introductionmentioning
confidence: 83%
“…Similarly, Al-Rashid [18] [19] [20], applied SR to the finite one-dimensional square well potential and special case in a double oscillator problems.…”
Section: Introductionmentioning
confidence: 99%
“…Dividing the real and imaginary parts in Equation ( U is the imaginary part of W ) one gets {centerDnormalΔitalicU()UU=ucentertU=08.75emwhich (first equation) may be rewritten for a 1‐D path as a Riccati equation (Al‐Rashid et al ., ), c being a constant and y(x) an arbitrary function of x : xUx=mU2x+2uxcm 2x2yx=2m2uxcmyx=0…”
Section: The Quantum Mechanical Picturementioning
confidence: 99%
“…As in Al‐Rashid et al . (), the first equation of system () for a 1‐D domain assumes the form of a Riccati equation: ditalicdxUx=mscriptℏU2x+2scriptℏuxcmwhere c is a case‐dependent constant of integration. Defining y ( x ) as an arbitrary function of x , the first equation in system () may be also written as (Al‐Rashid et al ., ) d2dx2yx2m2uxcmyx=0…”
Section: Single Particle Scale Relativity Theory Trajectorymentioning
confidence: 99%