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Published byRoderick Merritt Modified over 6 years ago
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Perturbation Theory Lecture 1 Books Recommended:
Quantum Mechanics, concept and applications by Nouredine Zetili Introduction to Quantum Mechanics by D.J. Griffiths Cohen Tanudouji, Quantum Mechanics II Introductory Quantum Mechanics, Rechard L. Liboff
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Approximate Methods: Approximate methods for stationary states corresponds to time independent Hamiltonian. Examples: perturbation theory, variational method, and the WKB method. Perturbation theory: Exactly solvable part + small correction In case we are not able to reduce the Hamiltonian of the problem to exactly solvable part+ small correction then we use variation method or WKB method
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Time independent perturbation theory
is splited into two parts, exactly solvable part and small perturbative part (1) Small perturbative part can be written as (2) From (1) -----(3)
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Non-degenerate perturbation theory
We have (4) Perturbed Eigen value and Eigen state is expanded as ------(5) ------(6) For λ = 0 we get unperturbed part.
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Use (5) and (6) in (3), we get ----(7) Now we compare powers of λ on both sides
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Zero power of λ ----(8) 1st power of λ ----(9) 2nd power of λ ----(10)
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Now we have to find eigen values and eigen functions
not much different from ----(11) Using (6) in (11), we get ----(12) Coefficients of various powers of λ vanishes ----(13)
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First order correction to :
Multiplying both sides of (9) by (14) Where we used = 0 and Thus, from (5), using (14) (15)
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Expand in terms of basis:
------(16) From (9), multiplying by (17)
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Using (17) in (16), we get ----(18) We have (19)
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Second order correction:
Multiply both sides by (20) Where we used Using (18) in (20) ----(21)
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Thus En upto 2nd order Validity :
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