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Carrier Generation and Recombination01:22

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Carrier generation is the process by which electron-hole pairs (EHPs) are created within the semiconductor. In direct-bandgap semiconductors, such as gallium arsenide (GaAs), this occurs efficiently when energy absorption prompts valence electrons to leap into the conduction band, leaving behind holes.
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Solid-State High Harmonic Generation in Common Large Bandgap Substrate Materials.

Ezra Korican-Barlay1, Bailey R Nebgen1,2, Jacob A Spies1,2

  • 1Department of Chemistry, University of California, Berkeley, California 94720, United States.

The Journal of Physical Chemistry. A
|October 10, 2024
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Summary
This summary is machine-generated.

Substrate emissions in solid-state high harmonic generation (sHHG) spectroscopy can interfere with material analysis. This study characterizes substrate sHHG, guiding optimal substrate selection for accurate quantum material studies.

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Area of Science:

  • Ultrafast spectroscopy
  • Quantum materials science
  • Solid-state physics

Background:

  • Solid-state high harmonic generation (sHHG) spectroscopy is a powerful technique for probing electronic structure and crystal symmetries in materials.
  • Substrate-supported samples are commonly used, with the assumption that substrates do not contribute significantly to the sHHG signal.
  • This assumption may not hold, as substrates can emit sHHG signals, potentially interfering with the analysis of the target material.

Purpose of the Study:

  • To investigate and characterize the sHHG emissions from commonly used optical substrates.
  • To evaluate the influence of substrate properties (e.g., crystalline quality, orientation) on sHHG.
  • To provide guidance for selecting appropriate substrates to minimize interference in sHHG studies of novel quantum materials.

Main Methods:

  • Power-dependent and polarization angle-resolved sHHG measurements were performed.
  • Fused silica, calcium fluoride, diamond, and sapphire substrates were studied.
  • A mid-infrared (MIR) driving field was used for sHHG excitation.

Main Results:

  • Substrate sHHG emissions were observed at moderate driving field intensities.
  • The sHHG yield and angular dependence of substrates vary significantly.
  • Different crystalline qualities and orientations of the same substrate material exhibit distinct sHHG characteristics.

Conclusions:

  • Substrate contributions to sHHG must be carefully considered, especially at higher driving field intensities.
  • Optimal substrate selection is crucial for accurate interpretation of sHHG data from novel materials.
  • This work facilitates the study of a broader range of materials by minimizing substrate-related artifacts.