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For use as a terahertz detector, the switch consists of the same geometry but without the applied bias voltage. Instead, the incident terahertz pulse itself provides the bias field for the charge carriers during the interval when the switch is activated by the (much shorter) laser pulse. The induced
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pulses is focused on the gap, it excites charge carriers into the semiconductor's conduction band, which are subsequently accelerated by the bias voltage. The induced acceleration from the photocurrent causes the charge carriers to radiate in terahertz frequencies, generating a pulse lasting several
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An Auston switch consists of a transmission line antenna with a gap that is bridged by a semiconductor. For terahertz generation, a DC bias voltage is applied across the antenna. When light from a
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photocurrent can then be amplified and measured. To map the entire span of the terahertz pulse, the time delay between the femtosecond pulses at generation and detection can be varied.
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Schmuttenmaer, Charles A. (April 2004). "Exploring
Dynamics in the Far-Infrared with Terahertz Spectroscopy".
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Typical time response of a photocurrent generated with an Auston switch using a femtosecond laser pulse.
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that is commonly used in the generation and detection of pulsed
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Bartolo, edited by
Baldassare Di; Forte, Ottavio (2006).
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IEEE Transactions on
Terahertz Science and Technology
91:Advances in spectroscopy for lasers and sensing
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226:Nuss, Martin C.; Orenstein, Joseph (1998).
35:radiation. It is named after the physicist
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136:"Terahertz Pioneer: David H. Auston"
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294:Terahertz technology
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