2016
DOI: 10.1364/oe.24.021059
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Optical generation of single-cycle 10 MW peak power 100 GHz waves

Abstract: We demonstrate the generation of 100 GHz single-cycle pulses with up to 10 MW of peak power using optical rectification and broadband phase matching via the tilted pulse front (TPF) technique in lithium niobate. The optical driver is a cryogenically cooled Yb:YAG amplifier providing tens of mJ energy, ~5 ps long laser pulses. We obtain a high THz pulse energy up to 65 µJ with 31.6 MV/m peak electric field when focused close to its diffraction limit of 2.5 mm diameter. A high optical-to-THz energy conversion ef… Show more

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Cited by 13 publications
(6 citation statements)
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“…The third spatial dimension (y) maybe ignored since diffraction effects of both terahertz and pump waves in this direction are negligible for large beams. The model accounts for various spatio-temporal distortions of the optical pulse such as angular dispersion and spatial chirp, which enables accurate quantitative predictions as verified by prior experiments [382,383].…”
Section: Single-cycle Thz Generationmentioning
confidence: 74%
“…The third spatial dimension (y) maybe ignored since diffraction effects of both terahertz and pump waves in this direction are negligible for large beams. The model accounts for various spatio-temporal distortions of the optical pulse such as angular dispersion and spatial chirp, which enables accurate quantitative predictions as verified by prior experiments [382,383].…”
Section: Single-cycle Thz Generationmentioning
confidence: 74%
“…[38] Such a saturation phenomenon is unusual compared to our previous THz generation implementations, which utilized ultrashort-pulse laser-pumped lithium niobate crystals without vertically focusing the laser spot beam. [42][43][44] However, this behavior was observed when a tightly focused method was employed. [41] As shown in Figure 3a, we hypothesize that other competitive nonlinear phenomena, such as the SPM effect, occur in the crystals owing to the high-intensity pump, degrading the pump spectrum and lowering the THz radiation efficiency.…”
Section: Room-temperature High-energy Thz Generationmentioning
confidence: 99%
“…Most setups utilize a single lens for imaging the tilted-pulse front into the crystal whereas others rely on a telescope for imaging. One advantage of the single-lens setup is, that the magnification and thus both the pulse-front-tilt angle and the angle of the image can be tuned via adjusting the grating-lens and lens-crystal distances, often used as optimization procedure in experiments 34,35,38,58,60 . However, it is harder to decouple effects due to a change in pump fluence from effects caused by the altered angles of pulse-front tilt and image plane during this optimization procedure and determine a global optimum of the THz efficiency since all three parameters are simultaneously changed.…”
Section: Setup Design: a Practical View On Choosing A Proper Imaging Setup For The Optimization Proceduresmentioning
confidence: 99%