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Multichannel Quantum Defect Theory -The Brief Introduction Department of Chemistry Kim Ji-Hyun 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 Particles : a, b, c Bound states : (bc), (bc), (ac) ☞channel 0, 1, 2, 3 a + (bc) → a + b + c → a + (bc) → a + (bc) → b + (ac) (breakup) (elastic scattering) (excitation) (rearrangement) 2. Quantum Defect For a hydrogenic atom, En = E∞ - 1/n2 • For an alkaline or alkaline-earth atom, En = E∞ – 1/(n – m)2 nn = n – m : effective quantum number m : quantum defect ☞ from short-range interactions with a core 3. Division of Region ☞ system = ionic core + a Rydberg electron 1) The inner region(R ≤ R0) • the existence of strong short-range interactions besides a long-range potential • spanned by regular solutions obtained from solving the close-coupled equation 2) The outer region (R ≥ R0) • Channels are decoupled. • spanned by regular and irregular solutions obtained from solving the ordinary secondorder differential equation ※ the most famous base pair ⇒ Coulomb functions 4. Boundary conditions For standing wave channel basis, the continuity conditions at the matching radius R0 For fragmentation eigenchannels, the condition imposing on their asymptotic forms The divergence terms must disappears in asymptotic regions. 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 h and b <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