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Core spectroscopy of molecules and clusters. Svante Svensson Department of Physics Uppsala University. Outline. RAS-PES-XPS Resonant and non-resonant processes Born-Oppenheimer approximation Interference quenching Clusters . N2. A. X. B. Resonant photoexcitation.
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Core spectroscopy of molecules and clusters Svante Svensson Department of Physics Uppsala University
Outline • RAS-PES-XPS • Resonant and non-resonant processes • Born-Oppenheimer approximation • Interference quenching • Clusters
N2 A X B
Resonant photoexcitation • Resonant excitation of electronic states • state selective • element selective • vibrational level selective • control of time scale • time information (fs)
Bound and dissociative electronic states for di-atomic molecules - Non resonant excitation
Vibrational mapping Excite to a discrete vibrational level Vibrational wave packet propagates, 5 fs period Decay to final ionic state maps wave packet Time information mirrored in PES
Born Oppenheimer approximation The wavefunction develops on ONE potential curve
40 35 Avoided crossing 2 + 4 S 30 Potential energy (eV) 1h 2h1p 25 2 + 3 S F-C Region 20 1 R 2 3 4 5 6 0 Distance H-Cl(Å) Expected Franck-Condon projection (Adiabatic approximation) Potential curves in literature (f2) Binding Energy (eV) (4s)-1 (5s)-2(6s)1 (f1) M.Hiyama, S.Iwata, Chem. Phys. Lett.210,187(1993)
Direct photoionization using hn=64eV BL I411 at MAX-lab PES of “4s” for HCl+ and DCl+
Theory Born-Oppenheimer approx. no longer valid. SE equation must take two potential curves into account
DCl latest results BESSY Spring 2002 lower photon energy available at Bl U125/2 Less Doppler broadening Ca 10 meV resolution
Cluster source Can be rotated around SR beam
Depth profiling of Ar clusters using variation of excitation energy
Xe-Ar mixed clusters Atom, surface, bulk components
surface atomic bulk Xe-Ar mixed clusters Xe XPS Ar XPS Ar %
”One phonon approximation Rc=1.1511 for -500 meV detuning