We demonstrate a system for the phase-resolved epi-detection of coherent anti-Stokes Raman scattering (CARS) signals in highly scattering and/or thick samples. With this setup, we measure the complex vibrational responses of multiple components in a thick, highly-scattering pharmaceutical tablet in real time and verify that the epi-and forward-detected information are in very good agreement. Coherent anti-Stokes Raman scattering (CARS) has matured in recent years into an imaging and spectroscopy technique that is finding applications in a range of disciplines including biology [1][2][3][4], remote sensing [5,6], and pharmaceutics [7,8]. The high spatial and spectral resolutions of CARS, combined with its capabilities for imaging in both transmission and reflection [9,10] at speeds up to video rate [11], have led to work specifically aimed at bringing down costs and complexity [12] to enable its use by non-specialists. However, this technique is not without problems. In particular, a strong, frequencyindependent non-resonant background interferes with the resonant signal of interest, reducing contrast and creating imaging and spectral artifacts that can be difficult to interpret. In order to remove, suppress, or extract this non-resonant background, a number of specialized methods have been developed that exploit polarization [9,13,14], spectral [15], time [16][17][18], and/or phase [19][20][21] dependencies of the CARS process. This last feature is of particular interest because it can be used to determine the full complex vibrational response of an arbitrary sample [22]. We previously introduced a method known as vibrational phase contrast CARS (VPC-CARS) to measure the pure vibrational phase of a sample [23], and used it to measure the full vibrational responses of multiple materials in both heterogeneous and homogeneous mixtures [24]. Heterodyne CARS measurements, in which an external local oscillator is interfered with the CARS emission, contain information about both the vibrational phase of the molecular oscillators and the relative local phases of the optical excitation fields. The local excitation phase is subject to disturbances from the variations in the relative phases of the pump, Stokes, and local oscillator beams, which can come from refractive index differences in the sample, interferometric instabilities, and field-of-view curvature resulting from dispersion in the focusing objective lens. To remove these effects a separate measurement is made in which only the local excitation phase is detected. The difference of the heterodyne and local excitation phases is the pure vibrational phase of the molecular oscillators. In previous experiments, heterodyne and local excitation phase measurements were performed in series on a pixel-by-pixel basis, with the local oscillator at nanowatt levels for the heterodyne process and at multi-millwatt powers for the local excitation phase detection. The exact power of the heterodyne local oscillator was a critical parameter for obtaining shot-noise-limited measurem...