2021
DOI: 10.1007/s10762-021-00789-4
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Analysis of Subcycle Electro-Optic Sampling Without Background

Abstract: We explore background-free options to detect mid-infrared (MIR) electric transients. The MIR field and a near-infrared probe interact via sum- (SFG) and difference-frequency generation (DFG) in an electro-optic crystal. An intuitive picture based on a phasor representation and rigorous numerical calculations are used for analysis. It turns out that separating photons generated either by SFG or DFG from the local oscillator via spectral filtering leads to a signal purely proportional the MIR intensity envelope.… Show more

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Cited by 4 publications
(3 citation statements)
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“…As the complete interference between the sum and difference frequencies is only possible at the center of the gate spectrum, the suppression of the background relies on polarization filtering of the gate pulses (figure 7(b)). Employing this technique allows for the complete retrieval of the sample pulse with high detection sensitivity, but with sign ambiguity [121]. The region with spectral overlap between the newly generated frequencies and the gate pulse are spectrally isolated.…”
Section: Field Sampling Based On Short Optical Gate Pulsesmentioning
confidence: 99%
“…As the complete interference between the sum and difference frequencies is only possible at the center of the gate spectrum, the suppression of the background relies on polarization filtering of the gate pulses (figure 7(b)). Employing this technique allows for the complete retrieval of the sample pulse with high detection sensitivity, but with sign ambiguity [121]. The region with spectral overlap between the newly generated frequencies and the gate pulse are spectrally isolated.…”
Section: Field Sampling Based On Short Optical Gate Pulsesmentioning
confidence: 99%
“…This can be achieved, e.g., through insertion of high-and low-pass filters before the photodetectors, as in the experiments performed in Refs. [50,51] (see Appendix F for more details). The (filtered) ν-polarization-photon number operator, N ω;ν ¼ R ωþΔω=2 ω−Δω=2 dω â0 † ω;ν â0 ω;ν , can be shown to be proportional to û½1 ω to leading order in the probe amplitude α.…”
Section: B First-order Unitary Evolution In a Nonlinear Crystalmentioning
confidence: 99%
“…To the right, the spectral phase of 3-mm-thick fused silica was added to the Fouriertransform limited pulse. For all gate pulses, the spectral intensity of the sum -and difference frequency components shows a periodic modulation with twice the frequency of the detected field, which allows for a determination of the square of the field amplitude [122]. This is caused by interference of the two contributions, that are generated with equal strength in the thin crystal, with their relative phase varying with the gate pulse delay.…”
Section: Wavelength-dependent Eos Signal For Thick Detection Crystalsmentioning
confidence: 99%