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Optical and NIR Photodetachment Spectroscopy in External Fields Charlotte Chapter of the OSA March 15, 2001. John Yukich Davidson College Department of Physics. -. -. -. +. -. -. -. -. -. +. -. -. Negative Ion Formation. Short-range attractive potential ( ~ 2 eV by a few Å )
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Optical and NIRPhotodetachment Spectroscopy inExternal FieldsCharlotte Chapter of the OSAMarch 15, 2001 John Yukich Davidson College Department of Physics
- - - + - - - - - + - - Negative Ion Formation • Short-range attractive potential ( ~ 2 eV by a few Å ) • Electron correlation effects – responsible for covalent bonds • Only one or two stable, boundstates of the ion
- - - - + - - Photodetachment - - + - - • X- + photon X + e- • ½ of electron-atom collision • minimum photon energy necessary is known • as the “electron affinity” • Why study photodetachment in fields?
Photodetachment with B-Fields • departing electron executes cyclotron motion in field • motion in plane perpendicular to B is quantized to cyclotron or Landau levels separated by the cyclotron frequency ω = eB/me • motion along axis of field is continuous, non-quantized • for typical B = 1.0 Tesla, ω ≈ 30 GHz, period = 36 ps • quantized Landau levels add structure to detachment cross section
Optical Apparatus Diode seed Diode amplifier MOPA: 250 mW single-mode tunable Wavemeter to 0.02 cm-1 Spectrum Analyzer 8 GHz FSR Ion trap
Time-domain spectroscopy • Short pulse excites multiple cyclotron levels simultaneously. • Wave packet of cyclotron states orbits atomic core with uniform cyclotron frequency. • Subsequent short pulse probes the detached portion of the electron wave function • Alternately: second pulse creates additional wave packet
Multiple path interferometry • Phase information of first pulse is stored in the ions • Phase information of second pulse is then compared with that of first pulse • Optical memory! What about electric fields?