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Multichannel Quantum Defect Theory -The Brief Introduction - Department of Chemistry Kim Ji-Hyun
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1.What is a channel ? Any possible grouping of elementary or composite particles corresponding to a particular final state Elastic and Inelastic scatterings Above threshold : open Below threshold : closed
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Particles : a, b, c Bound states : (bc), (bc) , (ac) ☞ channel 0, 1, 2, 3 a + (bc) → a + b + c (breakup) → a + (bc) (elastic scattering) → a + (bc) (excitation) → b + (ac) (rearrangement)
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2. Quantum Defect For a hydrogenic atom, E n = E ∞ - 1/n 2 For an alkaline or alkaline-earth atom, E n = E ∞ – 1/(n – ) 2 n = n – : effective quantum number : quantum defect ☞ from short-range interactions with a core
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3. Division of Region ☞ system = ionic core + a Rydberg electron 1) The inner region(R ≤ R 0 ) the existence of strong short-range interactions besides a long-range potential spanned by regular solutions obtained from solving the close-coupled equation
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2) The outer region (R ≥ R 0 ) Channels are decoupled. spanned by regular and irregular solutions obtained from solving the ordinary second- order differential equation ※ the most famous base pair ⇒ Coulomb functions
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4. Boundary conditions For standing wave channel basis, the continuity conditions at the matching radius R 0 For fragmentation eigenchannels, the condition imposing on their asymptotic forms The divergence terms must disappears in asymptotic regions.
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5. The power in experiments From the compatibility equation, Lu-Fano plot : graphical determination of discrete levels From cross sections, Reproduction of complex spectra with the short-range K matrix and the long-range quantum defect parameters and
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<References> Ch. Jungen, Molecular Application of Quantum Defect Theory (Institute of Physics Publishing, Bristol, 1996) John R. Taylor, Scattering theory(John Wiley & Sons, New York, 1972) C. –W. Lee, submitted to Phys. Rev. A
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