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Program and Abstract Book - SRON

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19 th International Symposium on Space Terahertz Technology<br />

Invited presentation 7-2<br />

Experiences with QCL local oscillators<br />

H.-W. Hübers<br />

German Aerospace Center<br />

Institute of Planetary Research<br />

Rutherfordstr. 2, 12489 Berlin, Germany<br />

In 2001 the first THz quantum cascade laser (QCL) has been demonstrated. Since then<br />

rapid progress has been made. Attractive features, which have been demonstrated for<br />

lasers operating in cw mode are emission between 1.2 THz <strong>and</strong> 4.9 THz, operation above<br />

the temperature of liquid nitrogen, output power beyond 100 mW, narrow linewidth of<br />

less than 10 kHz, <strong>and</strong> single mode operation by use of a distributed feedback structure.<br />

These features make QCLs promising devices for use as local oscillator in heterodyne<br />

receivers such as GREAT on SOFIA or future spaceborne heterodyne receivers. Initial<br />

experiments with a QCL as local oscillator <strong>and</strong> a hot electron bolometric mixer have been<br />

performed in 2005 for the first time. The noise temperature as well as the Allan time were<br />

the same as measured with a gas laser local oscillator. A major issue is the quality of the<br />

beam profile. Since the dimensions of the outcoupling facet of a QCL are in the order of<br />

or even less than the emission wavelength, diffraction degrades the beam profile.<br />

Nevertheless the output profile of a QCL with a surface plasmon waveguide can be<br />

transformed into an almost Gaussian profile with appropriate optics. With such a profile<br />

it was shown that 10 µW power in front of the cryostat window is sufficient for pumping<br />

the HEB mixer. Also, frequency-locking to a gas laser emission line, Doppler limited<br />

high resolution molecular spectroscopy, <strong>and</strong> frequency tuning with an external cavity<br />

resonator have been demonstrated. In this presentation the state-of-the-art of QCL local<br />

oscillator development will be reviewed <strong>and</strong> remaining challenges for implementation in<br />

a heterodyne receiver will be discussed.<br />

63

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