Cited by 461Photorefractive and Nonlinear OpticsTerahertz technology and applicationsLaser-Matter Interactions and Applications

Detectors and sources for ultrabroadband electro-optic sampling: Experiment and theory

Leitenstorfer, A., Hunsche, S., Shah, J., Nuss, M. C., Knox, W. H.·1999·Applied Physics Letters

Abstract

A detailed calculation of the amplitude and phase response of ultrathin ZnTe and GaP electro-optic sensors is presented. We demonstrate that the inclusion of the dispersion of the second-order nonlinearity is essential. Significant structures in experimental data can be explained by the theoretical response function. Correcting for the detector characteristics, we determine the precise shape of electromagnetic transients with a time resolution of 20 fs. In addition, we show that ultrafast transport of photocarriers in semiconductors can act as an efficient source for coherent electromagnetic radiation covering the entire far-to-mid-infrared regime.

Integrity signals

Registry

Crossref · 10.1063/1.123601

Cites

14 of 14 references verified0 citation errors · 0 not checkable

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  • Leitenstorfer et al. reported ultrabroadband amplitude and phase spectra from p-i-n diodes, with complex phase that decreased from 3rad at low frequency to 1rad at 3THz, before remaining relatively flat up to the LO-phonon frequency of InP, where it varied rapidly.

    “Leitenstorfer et al. [31] reported ultrabroadband amplitude and phase spectra from p -i -n diodes, with complex phase that decreased from 3rad at low frequency to 1rad at 3THz, before remaining relatively flat up to the LO-phonon frequency of InP, where it varied rapidly.”
  • The increase in spectral phase at high frequencies can be understood as a result of the electro-optic sampling process: the measured electro-optic signal does not have exactly the same temporal shape as the true electric field of the THz pulse incident on the detection crystal.

    “This can be understood as a result of the electro-optic sampling process: the measured electro-optic signal does not have exactly the same temporal shape as the true electric field of the THz pulse incident on the detection crystal [31, 36].”
  • The response function includes the velocity mismatch between the THz and probe pulse as a result of the detection crystal's frequency-dependent refractive index, as well as the variation in the electro-optic coefficient r41(ω) with frequency.

    “This response function includes the velocity mismatch between the THz and probe pulse as a result of the detection crystal's frequency-dependent refractive index [36], as well as the variation in the electro-optic coefficient r 41 (ω) with frequency [31].”

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Authors
Leitenstorfer, A., Hunsche, S., Shah, J., Nuss, M. C., & Knox, W. H.
Affiliations
Alcatel-Lucent (France) (FR)
Venue
Applied Physics Letters
Published
1999-03-15
Volume
74
Issue
11
Pages
1516-1518
ISSN
  • 0003-6951 (ISSN-L)
  • 1077-3118
OpenAlex
W2047943165
Cited by
461
References
14
Citations by year
2026: 12 · 2025: 17 · 2024: 19 · 2023: 37 · 2022: 29 · 2021: 27 · 2020: 22 · 2019: 22 · 2018: 22 · 2017: 17 · 2016: 12 · 2015: 9 · 2014: 10 · 2013: 6 · 2012: 12
FWCI
10.52
Type
journal article
Language
en
Open access
closed
Locations
Applied Physics Letters (publishedVersion)
Topics
  • Physical Sciences › Physics and Astronomy › Atomic and Molecular Physics, and Optics › Photorefractive and Nonlinear Optics
  • Physical Sciences › Engineering › Electrical and Electronic Engineering › Terahertz technology and applications
  • Physical Sciences › Physics and Astronomy › Atomic and Molecular Physics, and Optics › Laser-Matter Interactions and Applications
Keywords
electro-optic sampling, ZnTe, GaP, amplitude and phase response, femtosecond time resolution, photocarrier transport, far-infrared radiation, mid-infrared, coherent radiation sources

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