We perform electromagnetic wave simulations of fully three-dimensional optical Limaçon-microcavities, one basis for their future applications in microlasers and photonic devices. The analysis of the three-dimensional modes and far-fields reveals an increase of the quality factors as compared to the two-dimensional case. The structure of the far-field in the third dimension shows pronounced maxima in the emission directionality inclined to the resonator plane which may be exploited for coupling the resonator modes to the environment. This triggers ideas for technical applications, like the suggested sensor that can detect small changes in the environment based on changes in the emission profile. [14,15] which confine light in whispering gallery modes with high quality factors Q. The first microdisk-based microlasers had the drawback of isotropic light emission because of rotational symmetry. In order to observe a directional laser emission, deformed microcavities were investigated [16][17][18]. A promising shape to combine directional emission and high quality factors is the Limaçon-shape [19]. Here, ray and wave calculations based on a two-dimensional model system agree very well with the experimentally observed far-field characteristics [20][21][22][23].In reality, however, microcavities are three-dimensional (3D) objects with finite heights. This third dimension will be especially important when the cavity sizes are further reduced and both cavity height h and radius R become comparable to the wavelength [24,25]. Here, we systematically study 3D microcavities of Limaçon-shape, see left inset of FIG. 1. Its cross section in the x-y-plane is given in polar coordinates (r, φ), cf. FIG. 1, bywith mean Radius R and deformation parameter δ. We set δ = 0.43, a value known [19] to yield a highly directional far-field emission for two-dimensional (2D) cavities with refractive index n = 3.3 embedded in vacuum (n 0 = 1) as used here. We first discuss modes and farfields of 3D Limaçon cavities of varying height to radius ratio h/R, followed by outlining a sensor application based on the 3D character of the far field and its extreme sensitivity to tiny changes in the refractive index. Using MEEP [26], a free finite-difference time-domain (FDTD) software package, 3D electromagnetic wave simulations have been performed to calculate the normalized frequencies Ω = kR = Re(ω)R/c, with ω being a complex frequency and c the speed of light, the quality factors Q = −0.5Re(ω)/Im(ω), the distributions of the electric field component E z (x, y, z) (modes) and the farfield intensity I(φ, θ). As our focus is on wavelength-scale cavities, kR ranges from 1.9 up to 10.7, with k = 2π/λ being the wave number and λ the wavelength in vacuum. We use a E z -point-dipole source to excite the modes and focus on the study of TM-polarized modes.We first discuss the analogies between the structures of modes of the 2D and 3D Limaçon cavity, respectively. An example of a 2D mode and the (x, y)-cross section of a 3D mode are shown in FIG. 2 (a) and (b)...