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The Photoelectron Angular Distribution as a Probe of Energetically Indistinguishable Channels in Photodetachment Matthew Van Duzor, Richard Mabbs, Foster.

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Presentation on theme: "The Photoelectron Angular Distribution as a Probe of Energetically Indistinguishable Channels in Photodetachment Matthew Van Duzor, Richard Mabbs, Foster."— Presentation transcript:

1 The Photoelectron Angular Distribution as a Probe of Energetically Indistinguishable Channels in Photodetachment Matthew Van Duzor, Richard Mabbs, Foster Mbaiwa and Jie Wei OSU International Symposium on Molecular Spectroscopy 6/24/10

2 Outline Background: Experiment: Results & Interpretation:
I− • CH3CN Photodetachment and dipole bound state (DBS) Experiment: Photoelectron Imaging of I− • CH3X (X=CN, I, Br, Cl). Results & Interpretation: Evidence of autodetachment in photoelectron angular distributions (PADs)

3 I−CH3CN Cluster Anion 2P3/2 SO splitting 0.94 eV eBE = 3.54 eV (0.48 eV > I−) Transitions referred to as “2P3/2”, “2P1/2” throughout Both I−, I−CH3CN display prominent spectral feature I−, 273 nm 2P1/2 I− • CH3CN, 273 nm

4 I−CH3CN Photoelectron Images
Evolution on the 2P3/2 angular distribution is focus of present work 2P3/2 2P1/2 ε θ Transitions are fit to I(θ) ∝ C{1+βP2(cosθ)} where θ is defined with respect to the linearly polarized electric (ε) field of the detachment laser I− • CH3CN, 273 nm

5 CH3CN− Dipole Bound Anion
The I− • CH3CN cluster anion is a well known precursor of the CH3CN− dipole-bound state (DBS) CH3CN μ = 3.92 D (μcritical ≥ 2.0 D) photoneutral action spectrum I−(1S0) • CH3CN I(2P3/2) + CH3CN− 355 nm VDE Intensity peaks ~18 meV below 2P3/2 threshold C.G. Bailey, C.E.H. Dessent, M.A. Johnson, K. H. Bowen, J. Chem. Phys. 104, 6976 (1996). C.E.H. Dessent, C.G. Bailey, and M.A. Johnson, J. Chem. Phys. 103, 2006 (1995).

6 Total Cross Section: Near 2P1/2 Threshold
Cross section displays enhancement below the 2P1/2 channel opening Measured position of peak ~17 meV below 2P1/2 Suggests DBS excitation similar to that below 2P3/2 channel 2P1/2 channel opening

7 Energetically equivalent!
Experimental Scheme I(2P1/2) • CH3CN I(2P1/2) • CH3CN− 355 nm Excitation near “2P3/2”: I(2P3/2) • CH3CN− 279 nm Excitation near “2P1/2”: I(2P1/2) • CH3CN− I(2P3/2) • CH3CN + e− (~0.92 eV) Energetically equivalent! I(2P3/2) • CH3CN + e− (~0.92 eV) Relaxation, autodetachment I(2P3/2) • CH3CN I(2P3/2) • CH3CN− I−(1S0) • CH3CN

8 I−CH3CN, I−: 2P3/2 Channel 2P1/2 channel opening “Peak” β value occurs ~25 meV prior to 2P1/2 channel opening I− and I− • CH3CN images were collected at photodetachment wavelengths from nm, β values extracted I− • CH3CN I−

9 Detail: Near 2P1/2 Threshold
279 nm 278 nm Evolution of PAD from λ = 288 to 275 nm (~200 meV) 277 nm 280 nm 283 nm 281 nm 276 nm 275 nm 288 nm 285 nm 2P1/2 channel opening

10 Interpretation Calculation of DBS illustrates spatial overlap of 2P1/2 excited I and DB orbital e− localized long enough to allow SO relaxation I(2P1/2)−•CH3X → I(2P3/2)•CH3CN + e− aug-cc-pvdz/CRENBL

11 Sub-Critical μ: I−CH3X (X=I, Br, Cl)
2P3/2 I−, 280 nm eBE=3.06 2P1/2 Molecular dipoles are in all cases <2 D. I− • CH3X (X=1, Br, Cl) spectra display 2 prominent features Splitting = 0.94 eV, consistent with I− I− • CH3Cl, 280 nm eBE=3.41, μ = 1.89 D I− • CH3Br, 280 nm eBE=3.42, μ = 1.82 D I− • CH3I, 280 nm eBE=3.43, μ = 1.62 D

12 I−CH3X (X=I, Br, Cl): 2P3/2 Channel
I−CH3CN β “peak” Change in position (eKE) and relative magnitude compared to I−CH3CN I− and I−CH3X (X=I, Br, Cl) images were collected at λ= nm, β values extracted 2P1/2 channel opening For all clusters, “peaks” appear near 2P1/2 channel opening I− • CH3I I− • CH3Br I− • CH3Cl I−

13 Detail: Near I−CH3X (X=I, Br, Cl) 2P1/2 Threshold
Peak positions coincident with 2P1/2 channel opening Suggests that threshold e− are “delayed” long enough to allow competition by autodetahcment 2P1/2 channel opening

14 Conclusions Photoelectron angular distributions were extracted over a eV (eKE) range for I− • CH3CN, I− • CH3I, I− • CH3Br, I− • CH3Cl and I−. Rapid variation in the I− • CH3X (X=CN, I, Br, Cl) β parameter at eKEs consistent with 2P3/2 photodetachment was observed at energies near the 2P1/2 channel opening These features were attributed to autodetachment associated with the 2P1/2 excited state of the I moiety General feature of I− • X clusters studied (X= polar molecule).

15 Foster Mbaiwa, Jie Wei and Richard Mabbs
Acknowledgements Foster Mbaiwa, Jie Wei and Richard Mabbs Funding:


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