1. CaF: All Spectra and All Dynamics R. W. Field, J. J. Kay, S. L. Coy, V. S. Petrovic, S. N. Altunata, B. M. Wong, and Ch. Jungen NSF

2. Multichannel Quantum Defect Theory MQDT builds a complete description of something complicated, CaF, by combining complete (all states) descriptions of two isolated parts, CaF + and e -, at infinite separation. Space is divided into an infinite simple region and a compact region of complex interactions. The H eff matrix would be of infinite dimension. An e -, incident with definite ε, ℓ, scatters inelastically off of the ion-core in a definite v +,N + state. The building blocks are channels rather than individual electronic states. A channel consists of infinite number of states, with the e - in a particular mixed- ℓ form converging to a v +,N + state of the ion-core.

3. MQDT The scattering of the e - off of the ion-core is described by the “Reaction Matrix,” K, which is expressed in terms of quantum defect matrix elements: K ij = tan(πμ ij ).. The μ ij are expanded as power series in internuclear distance, R, and energy. μ ij, dμ ij /dR, and dμ ij /dε are the fitted quantities. The MQDT equations yield eigenquantum defects and eigenvectors, which may be expressed in either the Hund’s case (b) or (d) basis sets. There are many useful, a priori known transformations between basis sets.

4. Quantum defect matrix element values and derivatives obtained from fits to CaF Σ, Π, Δ, and Φ states. Uncertainties are indicated in parentheses. If no numerical value is given, the parameter has been held fixed at zero.

5. Quality of fit for vibrationally-excited levels with low-n*

6. Quality of fit in the vicinity of n* = 7.0. Vibronic states at this energy that belong to different vibrational quantum numbers are interleaved. Here, the classical period of electronic motion [proportional to (n*) 3 ] is approximately equal to the classical period of vibrational motion. Vibronic perturbations are frequent.

7. Example of a strong vibronic (homogeneous) perturbation. In the absence of the perturbation, the 7.36 ‘p’ Π v=0 and 6.36 ‘p’ Π v=1 levels are nearly degenerate. The perturbation causes a ~45 cm -1 splitting of the levels and complete mixing of the two zero-order wavefunctions.

8. Quality of fit in the n* = 16.5 – 17.5 region. Above n*  16, rotational interactions are ubiquitous and quite strong, causing the destruction of regular rotational patterns, which is evident here.

9. Nonpenetrating States: Stacked Plot for N, N + Assignment

10. Nonpenetrating States Live Near Integer n*

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12. Vibrational Autoionization: Single Channel (HLB-RWF)

13. Case (b) to Case (d) Transformation case (b)case (d) even N f Σ,Π,Δ,ΦN + =N-3,N-1,N+1,N+3 + paritydΣ,Π,ΔN + =N-2,N, N+2 [10] p Σ,Π N + =N-1,N+1 s Σ N + =N -parityf -,Π,Δ,ΦN + =N-2,N,N+2 [6] d -,Π,Δ N + =N-1,N+1 p -,Π N + =N s - N + =-

14. Multichannel Autoionization Want total autoionization rate from every n*,N,v + =1 level and fractional yields into different N + levels of CaF + v + =0. Transform the μ and dμ/dR matrices from case (b) to case (d). Solve the MQDT equations to get eigenvectors expressed in case (d). For the optically selected eigenstate, compute expectation value of [dμ/dR(d)] T dμ/dR(d). This can be broken down into individual N + contributions

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