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Advanced Diagnostics Navigation

• Atomic and molecular species, positive and negative ions
  • Laser-Induced Fluorescence (LIF) and Two-Photon Absorption LIF (TALIF)
    • Nanosecond LIF/TALIF
    • Femtosecond TALIF
    • CW LIF for measurements of Ar and Xe ion and atom VDFs
  • Radar Resonant Enhanced Multi-Photon Ionization (Radar REMPI)
• Characterization of plasma, chemical composition and dynamic behavior
  • Optical Emission Spectroscopy (OES)
  • Fourier Transform Infrared Spectrometry
  • Fast Imaging
  • Electrostatic Quadrupole Mass Spectrometer and Energy Analyzer
  • Electrostatic probes
• Electron velocity distribution function, gas flow velocity and temperature
  • Thomson, Raman, and Rayleigh scattering
  • Hybrid Coherent Anti-Stokes Raman Scattering (Hybrid CARS)
  • Femtosecond Laser Electronic Excitation Tagging (FLEET)
• Electric field and space potential
  • Electric Field-Induced Second Harmonic Generation (E-FISH)
  • Electrostatic probes
• Nanoparticle Diagnostics
  • Laser-Induced Incandescence (LII)
  • Laser-Induced Breakdown Spectroscopy (LIBS)
  • Coherent Rayleigh-Brillouin Scattering (CRBS)
• Surface Diagnostics
  • Surface Second Harmonic Generation (SHG)
  • Electron-induced Secondary Electron Emission and Surface Charging Measurements
  • Surface Potential Measurements with the Kelvin Probe Diagnostic

Femtosecond Two-photon LIF (FS TALIF)

Absolute and relative species density measurements

1-D and 2-D mapping of species spatial distribution with ~100μm resolution

Temporal dynamics of species with 200ps resolution

Species densities as low as 10¹¹ cm^-3

Laser-induced fluorescence (LIF) allows mapping the density of atoms and molecules in gases and plasmas. Absolute densities can also be determined with appropriate calibration. Many atomic species of interest, however, require excitation in the vacuum ultraviolet (VUV) spectral range. Two-photon LIF (or TALIF) allows excitation using visible of UV laser pulses which can be used in atmosphere. In order to efficiently pump the excited states using a two-photon transition, short laser pulses are required. The fs and ps lasers are particularly useful for measuring the effective lifetimes of the excited levels in highly collisional environments. Coupled with detection by fast iCCD with minimal exposure times 0.2 ns this allows measuring sub-nanosecond lifetimes of excited levels subject to fast collisional quenching. Effective lifetimes are used to determine the dominant collisional partners. Finally, the fs pulse excitation is necessary in liquid where the lifetime of the excited levels is expected to be very short < 0.2 ns. With fs lasers we expect to induce excitation on a timescale faster than quenching de-excitation, permitting for fluorescence to be detected. The fs excitation is thus necessary to measure the penetration of species into the liquid phase. In the cases where the two-photon absorption transition of the species to be excited is energetically separated from other species, or if the species of interest is the majority species, another advantage of using fs TALIF is the use of the non-degenerate sum-frequency mixing. This not only makes the two-photon absorption to be very efficient, but it also allows for excitation without the need for precise wavelength tuning.

1. Kulatilaka et al., Opt. Lett. 37, 3051 (2012).

  This capability is located at the Princeton University Dept. of Mechanical and Aerospace Engineering.