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In [[theoretical physics]], the '''eikonal approximation''' ([[Greek language|Greek]] εἰκών for likeness, icon or image) is an approximative method useful in wave scattering equations which occur in [[optics]], [[quantum mechanics]], [[quantum electrodynamics]], and [[Scattering amplitude#Partial wave expansion|partial wave expansion]]. | |||
==Informal description== | |||
The main advantage the eikonal approximation offers is that the equations reduce to a [[differential equation]] in a single variable. This reduction into a single variable is the result of the straight line approximation or the eikonal approximation which allows us to choose the straight line as a special direction. | |||
==Relation to the WKB approximation== | |||
The early steps involved in the eikonal approximation in quantum mechanics are very closely related to the [[WKB approximation]]. It, like the eikonal approximation, reduces the equations into a differential equation in a single variable. But the difficulty with the WKB approximation is that this variable is described by the trajectory of the particle which, in general, is complicated. | |||
==Formal description== | |||
Making use of WKB approximation we can write the wave function of the scattered system in term of [[action (physics)|action]] ''S'': | |||
:<math>\Psi=e^{iS/{\hbar}} </math> | |||
Inserting the [[wavefunction]] Ψ in the [[Schrödinger equation]] we obtain | |||
:<math> -\frac{{\hbar}^2}{2m} {\nabla}^2 \Psi= (E-V) \Psi</math> | |||
:<math> -\frac{{\hbar}^2}{2m} {\nabla}^2 {e^{iS/{\hbar}}}=(E-V) e^{iS/{\hbar}}</math> | |||
:<math>\frac{1}{2m} {(\nabla S)}^2 - \frac{i\hbar}{2m}{\nabla}^2 S= E-V</math> | |||
We write ''S'' as a ''ħ'' [[power series]] | |||
:<math>S= S_0 + \frac {\hbar}{i} S_1 + ...</math> | |||
For the zero-th order: | |||
:<math>{(\nabla S_0)}^2= E-V</math> | |||
If we consider the one-dimensional case then <math>{\nabla}^2 \rightarrow {\delta_z}^2</math>. | |||
We obtain a [[differential equation]] with the [[Boundary value problem|boundary condition]]: | |||
:<math>\frac{S(z=z_0)}{\hbar}= k z_0</math> | |||
for ''V'' → 0, ''z'' → -∞. | |||
:<math>\frac{d}{dz}\frac{S_0}{\hbar}= \sqrt{k^2 - 2mV/{\hbar}^2}</math> | |||
:<math>\frac{S_0(z)}{\hbar}= kz - \frac{m}{{\hbar}^2 k} \int_{-\infty}^{Z}{V dz'} </math> | |||
==See also== | |||
* [[Eikonal equation]] | |||
* [[Correspondence principle]] | |||
* [[Principle of least action]] | |||
==References== | |||
===Notes=== | |||
* [http://www.nhn.ou.edu/~shajesh/eikonal/sp.pdf]''Eikonal Approximation'' K. V. Shajesh Department of Physics and Astronomy, University of Oklahoma | |||
===Further reading=== | |||
* {{cite book|title=Comparison of exact solution with Eikonal approximation for elastic heavy ion scattering|edition=3rd|author=R.R. Dubey|location=|publisher=NASA|year=1995 |isbn=|url = http://books.google.co.uk/books?id=NwgVAQAAIAAJ&q=Eikonal+approximation&dq=Eikonal+approximation&hl=en&sa=X&ei=LCnkUOP8HfDa0QW-34GIBA&ved=0CDwQ6AEwAQ}} | |||
* {{cite book|title=Eikonal approximation in partial wave version|edition=3rd|author=W. Qian, H. Narumi, N. Daigaku. P. Kenkyūjo|location=Nagoya|publisher=|year=1989|isbn=|url = http://books.google.co.uk/books?id=5RdRAAAAMAAJ&q=Eikonal+approximation&dq=Eikonal+approximation&hl=en&sa=X&ei=LCnkUOP8HfDa0QW-34GIBA&ved=0CDYQ6AEwAA}} | |||
*{{cite article | |||
| author = M. Lévy, J. Sucher | |||
| year = 1969 | |||
| location = Maryland, USA | |||
| publisher = | |||
| journal = Phys. Rev | |||
| title = Eikonal Approximation in Quantum Field Theory | |||
| arxiv = | |||
| url = http://prola.aps.org/abstract/PR/v186/i5/p1656_1 | |||
| doi = 10.1103/PhysRev.186.1656 | |||
}} | |||
*{{cite article | |||
| author = I. T. Todorov | |||
| year = 1970 | |||
| location = New Jersey, USA | |||
| publisher = | |||
| journal = Phys. Rev D | |||
| title = Quasipotential Equation Corresponding to the Relativistic Eikonal Approximation | |||
| arxiv = | |||
| url = http://prd.aps.org/abstract/PRD/v3/i10/p2351_1 | |||
| doi = 10.1103/PhysRevD.3.2351 | |||
}} | |||
*{{cite article | |||
| author = D.R. Harrington | |||
| year = 1969 | |||
| location = New Jersey, USA | |||
| publisher = | |||
| journal = Phys. Rev | |||
| title = Multiple Scattering, the Glauber Approximation, and the Off-Shell Eikonal Approximation | |||
| arxiv = | |||
| url = http://prola.aps.org/abstract/PR/v184/i5/p1745_1 | |||
| doi = 10.1103/PhysRev.184.1745 | |||
}} | |||
[[Category:Theoretical physics]] | |||
[[Category:Mathematical analysis]] | |||
{{applied-math-stub}} | |||
{{Quantum-stub}} |
Revision as of 02:10, 4 February 2014
In theoretical physics, the eikonal approximation (Greek εἰκών for likeness, icon or image) is an approximative method useful in wave scattering equations which occur in optics, quantum mechanics, quantum electrodynamics, and partial wave expansion.
Informal description
The main advantage the eikonal approximation offers is that the equations reduce to a differential equation in a single variable. This reduction into a single variable is the result of the straight line approximation or the eikonal approximation which allows us to choose the straight line as a special direction.
Relation to the WKB approximation
The early steps involved in the eikonal approximation in quantum mechanics are very closely related to the WKB approximation. It, like the eikonal approximation, reduces the equations into a differential equation in a single variable. But the difficulty with the WKB approximation is that this variable is described by the trajectory of the particle which, in general, is complicated.
Formal description
Making use of WKB approximation we can write the wave function of the scattered system in term of action S:
Inserting the wavefunction Ψ in the Schrödinger equation we obtain
We write S as a ħ power series
For the zero-th order:
If we consider the one-dimensional case then .
We obtain a differential equation with the boundary condition:
for V → 0, z → -∞.
See also
References
Notes
- [1]Eikonal Approximation K. V. Shajesh Department of Physics and Astronomy, University of Oklahoma
Further reading
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