Abstract
Demonstration of substrate-emitting quantum cascade lasers (QCLs) with a distributed Bragg reflector (DBR) used for wavelength selection and a second-order outcoupler spectrally detuned from the reflector is reported. A 40-stage QCL structure with the gain spectrum centered at 4.1 μm was processed into 20 μm-wide ridge-waveguide devices with a 4 mm-long gain section, a 0.5 mm-long first-order DBR section with 644 nm period, and a 1.5 mm-long second-order outcoupler with 1100 nm period. Etch depth and duty cycle were 900 nm and 45%, respectively, for both gratings. The three sections shared the same electrical contact and were, therefore, pumped at the same current density. A device with a high-reflection coated back facet and anti-reflection coated front facet and substrate side delivered a peak power of 0.6 W from the substrate into a single-lobed beam with ∼1° × 18° angular full width at half maximum (FWHM). Due to the spectral detuning, the beam was extracted from the device at an angle of ∼−34° relative to the growth direction. The measured spectrum had a FWHM of 3 cm−1, and its peak was centered at 4.07 μm, close to the design value of 4.10 μm. The detuning between the two gratings allows for independent optimization of grating profiles to significantly improve the overall laser performance, which will be the focus of future work.
Highlights
quantum cascade lasers (QCLs) optical power can be effectively scaled with the cavity length.7 The optimal facet reflectivity for long-cavity (5–10 mm)
Even a short grating can provide sufficient optical feedback required for lasing, leaving most of the laser waveguide unperturbed. This can be leveraged in the design of surface-emitting QCLs by combining a long gain section to achieve high optical power with a short firstorder distributed Bragg reflector (DBR) used for wavelength selection and a second-order outcoupler for increasing emission aperture size (Fig. 1)
Since both the effective reflectivity for the first-order DBR section and outcoupling efficiency for the second-order section strongly depend on a grating profile, it would be beneficial to spectrally detune the two gratings from each other, which would allow for their independent optimization to improve the overall laser performance
Summary
QCL optical power can be effectively scaled with the cavity length.7 The optimal facet reflectivity for long-cavity (5–10 mm). Output optical power for QCLs in the surface-emitting configuration is extracted perpendicular to the optical cavity utilizing a second-order diffraction grating etched into the upper cladding layers of the laser waveguide.
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