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Upconversion of a relativistic Coulomb field terahertz pulse to the near infrared

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Upconversion of a relativistic Coulomb field terahertz pulse to the near infrared. / Jamison, S.P.; Berden, G.; Phillips, P.J.; Gillespie, W.A.; MacLeod, A.M.

In: Applied Physics Letters, Vol. 96, No. 23, 231114, 2010.

Research output: Contribution to journalJournal article

Harvard

Jamison, SP, Berden, G, Phillips, PJ, Gillespie, WA & MacLeod, AM 2010, 'Upconversion of a relativistic Coulomb field terahertz pulse to the near infrared', Applied Physics Letters, vol. 96, no. 23, 231114. https://doi.org/10.1063/1.3449132

APA

Jamison, S. P., Berden, G., Phillips, P. J., Gillespie, W. A., & MacLeod, A. M. (2010). Upconversion of a relativistic Coulomb field terahertz pulse to the near infrared. Applied Physics Letters, 96(23), [231114]. https://doi.org/10.1063/1.3449132

Vancouver

Jamison SP, Berden G, Phillips PJ, Gillespie WA, MacLeod AM. Upconversion of a relativistic Coulomb field terahertz pulse to the near infrared. Applied Physics Letters. 2010;96(23). 231114. https://doi.org/10.1063/1.3449132

Author

Jamison, S.P. ; Berden, G. ; Phillips, P.J. ; Gillespie, W.A. ; MacLeod, A.M. / Upconversion of a relativistic Coulomb field terahertz pulse to the near infrared. In: Applied Physics Letters. 2010 ; Vol. 96, No. 23.

Bibtex

@article{3f1eee2e68da4e3d8ac1fcf199aa1a1c,
title = "Upconversion of a relativistic Coulomb field terahertz pulse to the near infrared",
abstract = "We demonstrate the spectral upconversion of a unipolar subpicosecond terahertz (THz) pulse, where the THz pulse is the Coulomb field of a single relativistic electron bunch. The upconversion to the optical allows remotely located detection of long wavelength and nonpropagating components of the THz spectrum, as required for ultrafast electron bunch diagnostics. The upconversion of quasimonochromatic THz radiation has also been demonstrated, allowing the observation of distinct sum- and difference-frequency mixing components in the spectrum. Polarization dependence of first and second order sidebands at ωopt±ωTHz, and ωopt±2ωTHz, respectively, confirms the χ(2) frequency mixing mechanism.",
author = "S.P. Jamison and G. Berden and P.J. Phillips and W.A. Gillespie and A.M. MacLeod",
year = "2010",
doi = "10.1063/1.3449132",
language = "English",
volume = "96",
journal = "Applied Physics Letters",
issn = "0003-6951",
publisher = "American Institute of Physics Inc.",
number = "23",

}

RIS

TY - JOUR

T1 - Upconversion of a relativistic Coulomb field terahertz pulse to the near infrared

AU - Jamison, S.P.

AU - Berden, G.

AU - Phillips, P.J.

AU - Gillespie, W.A.

AU - MacLeod, A.M.

PY - 2010

Y1 - 2010

N2 - We demonstrate the spectral upconversion of a unipolar subpicosecond terahertz (THz) pulse, where the THz pulse is the Coulomb field of a single relativistic electron bunch. The upconversion to the optical allows remotely located detection of long wavelength and nonpropagating components of the THz spectrum, as required for ultrafast electron bunch diagnostics. The upconversion of quasimonochromatic THz radiation has also been demonstrated, allowing the observation of distinct sum- and difference-frequency mixing components in the spectrum. Polarization dependence of first and second order sidebands at ωopt±ωTHz, and ωopt±2ωTHz, respectively, confirms the χ(2) frequency mixing mechanism.

AB - We demonstrate the spectral upconversion of a unipolar subpicosecond terahertz (THz) pulse, where the THz pulse is the Coulomb field of a single relativistic electron bunch. The upconversion to the optical allows remotely located detection of long wavelength and nonpropagating components of the THz spectrum, as required for ultrafast electron bunch diagnostics. The upconversion of quasimonochromatic THz radiation has also been demonstrated, allowing the observation of distinct sum- and difference-frequency mixing components in the spectrum. Polarization dependence of first and second order sidebands at ωopt±ωTHz, and ωopt±2ωTHz, respectively, confirms the χ(2) frequency mixing mechanism.

U2 - 10.1063/1.3449132

DO - 10.1063/1.3449132

M3 - Journal article

VL - 96

JO - Applied Physics Letters

JF - Applied Physics Letters

SN - 0003-6951

IS - 23

M1 - 231114

ER -