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Optical ray tracing for crossed beam photothermal deflection spectroscopy
Applied Optics
|May 11, 2010
Summary
This study uses geometrical optics to model laser beam paths in pulsed photothermal deflection spectroscopy (PDS). Maximum signal occurs at the end of the pump pulse, with analytical models accurate for short pulses.
Area of Science:
- Optical Physics
- Spectroscopy
- Laser-Matter Interactions
Background:
- Pulsed photothermal deflection spectroscopy (PDS) is a sensitive technique for analyzing gas properties.
- Accurate modeling of probe beam behavior is crucial for interpreting PDS signals.
- Previous analytical models may not fully account for thermal diffusion effects in PDS.
Purpose of the Study:
- To develop and apply a geometrical algorithm for tracing probe laser beam trajectories in pulsed PDS.
- To investigate the influence of various parameters on ray trajectories and signal deflection.
- To compare geometrical ray tracing results with analytical calculations and experimental observations.
Main Methods:
- Implementation of a geometrical algorithm for optical ray tracing of probe laser beams.
- Simulation of ray trajectories under varying conditions: time, pump beam energy, radius, and pulse duration.
- Computation and comparison of probe beam exit angles with analytical deflection angles.
Main Results:
- Excellent agreement between geometrical ray tracing and analytical calculations for short pump pulse durations (shorter than thermal diffusion time).
- Analytical model inaccuracy for long pump pulse durations due to neglected thermal diffusion.
- Observed signal saturation at high absorbed pump beam energy attributed to excessive absorber heating.
- Maximum probe beam deflection occurs at the end of the pump pulse duration.
Conclusions:
- Geometrical ray tracing provides an accurate method for modeling probe beam behavior in pulsed PDS.
- The timing of deflection measurement is critical, with the end of the pump pulse yielding maximum deflection.
- Understanding thermal diffusion effects is essential for accurate analytical modeling in PDS, especially for longer pulses.

