Abstract: A terahertz difference-frequency generation quantum cascade laser source that provides monolithic, electrically-controlled tunable terahertz emission. The quantum cascade laser includes a substrate, a lower cladding layer positioned above the substrate and an active region layer with optical nonlinearity positioned on the lower cladding layer. The active region layer is arranged as a multiple quantum well structure. One or more feedback gratings are etched into spatially separated sections of the cladding layer positioned on either side of the active region. The periodicity of each grating section determines the mid-infrared lasing frequencies. The grating sections are electrically isolated from one another and biased independently. Tuning is achieved by changing a refractive index of one or all of the grating sections via a DC current bias thereby causing a shift in the mid-infrared lasing frequency. In this manner, a monolithic, electrically-pumped, tunable THz source is achieved.

Abstract: Methods and systems include generating one or more mid-infrared frequencies based at least upon electron transitions in one or more quantum cascade heterostructures. The quantum cascade heterostructures are concurrently configured with a significant second-order nonlinear susceptibility, a significant third-order nonlinear susceptibility, and an insignificant group velocity dispersion. A set of mid-infrared frequencies (that may include a frequency comb) is generated in the quantum cascade heterostructures based at least upon a four-wave mixing of the one or more mid-infrared frequencies. The four-wave mixing arises at least from the significant third-order nonlinear susceptibility and the insignificant group velocity dispersion. A set of terahertz frequencies (that may include a frequency comb) is generated in the quantum cascade heterostructures based at least upon a difference frequency generation from mid-infrared frequency pairs selected from the set of mid-infrared frequencies.

Abstract: Methods and systems include generating one or more mid-infrared frequencies based at least upon electron transitions in one or more quantum cascade heterostructures. The quantum cascade heterostructures are concurrently configured with a significant second-order nonlinear susceptibility, a significant third-order nonlinear susceptibility, and an insignificant group velocity dispersion. A set of mid-infrared frequencies (that may include a frequency comb) is generated in the quantum cascade heterostructures based at least upon a four-wave mixing of the one or more mid-infrared frequencies. The four-wave mixing arises at least from the significant third-order nonlinear susceptibility and the insignificant group velocity dispersion. A set of terahertz frequencies (that may include a frequency comb) is generated in the quantum cascade heterostructures based at least upon a difference frequency generation from mid-infrared frequency pairs selected from the set of mid-infrared frequencies.

Abstract: A broadly tunable terahertz source constructed as an external cavity system using a difference-frequency generation quantum cascade laser source. The external cavity system includes an external diffraction grating configured to tune and reflect mid-infrared emission at a first wavelength. The laser includes a mid-infrared feedback grating defined in the laser waveguide of the laser to fix mid-infrared lasing at a second wavelength. Alternatively, two external diffraction gratings may be configured to tune and reflect mid-infrared emission at a first wavelength and a second wavelength. Tunable terahertz radiation is then generated at frequency ?THz=|?1??2|, where ?1 and ?2 are the frequencies of the first and second mid-infrared lasing wavelengths.