Optical microcavities can be designed to take advantage of total internal reflection, which results in resonators supporting whispering-gallery modes (WGMs) with a high-quality factor (Q factor). One of the crucial problems of these devices for practical applications such as designing microcavity lasers, however, is that their emission is nondirectional due to their radial symmetry, in addition to their inefficient power output coupling. Here we report the design of elliptical resonators with a wavelength-size notch at the boundary, which support in-plane highly unidirectional laser emission from WGMs. The notch acts as a small scatterer such that the Q factor of the WGMs is still very high. Using midinfrared (λ ∼ 10 μm) injection quantum cascade lasers as a model system, an in-plane beam divergence as small as 6 deg with a peak optical power of ∼5 mW at room temperature has been demonstrated. The beam divergence is insensitive to the pumping current and to the notch geometry, demonstrating the robustness of this resonator design. The latter is scalable to the visible and the near infrared, thus opening the door to very low-threshold, highly unidirectional microcavity diode lasers.F ollowing the first description of the whispering-gallery mode (WGM) phenomenon in the acoustic regime by Lord Rayleigh in London's St Paul's Cathedral (1) and its subsequent analysis in terms of guided surface waves by Raman and Sutherland (2), its study was later extended to the radiofrequency (3) and optical domains (4) through the investigation of the ionosphere and solid spheres, respectively. WGMs were later investigated in liquid droplets (5) and microdisk diode lasers (6), opening a previously undescribed direction in photonics technology. WGM resonators offer great promise for investigation in the physical sciences (6-8), and applications of these devices have spanned a wide range from unique laser sources (9) and dynamic filters in communications (10) to sensors (11). One drawback, however, is that, in rotationally symmetric cavities (6, 12), WGMs can only be coupled out inefficiently and isotropically through scattering of evanescent waves by surface roughness or diffraction losses when the radius of curvature is comparable to the wavelength (9).Previously, this problem was addressed through evanescent coupling using prisms (13), in-plane waveguide (14), or tapered fibers (15). The technique of using tapered waveguide (16) for coupling high Q WGMs out of cavities is quite successful for the study of fundamental cavity physics; however, it requires careful alignment and the devices are relatively sensitive to mechanical vibrations or other variations in the surrounding environment, which limit its usage for practical applications such as achieving microcavity lasers with directional emission. Another approach is to break the rotational symmetry by using deformed optical microcavities to increase the directionality of emission and power collection efficiency (17, 18), which has the advantage of easy and robust fabrication. Th...