The CARS microscope system had an axial spatial resolution of about 10 μm and a lateral spatial www.selleckchem.com/screening/selective-library.html resolution of about 1 μm. Hyperspectral CARS imaging provides a method to rapidly and visually confirm the solid-state form on the surface of an oral dosage form, both pre- and post-dissolution. Hyperspectral CARS images were obtained by rapidly imaging the sample while slowly sweeping the wavelength of the OPO in discrete steps, so that each frame in the image stack corresponds to a different vibrational frequency [26]. A color look up table was then applied to the image stack, with a separate color

applied to each frame in the image. Finally, the frames were projected together, resulting in a single two-dimensional image wherein each material appears with a unique color. This process is illustrated as a diagram in Fig. 2. In this study, 512 × 512 pixel hyperspectral images were collected over a range of 100 cm−1 with each hyperspectral image taking approximately 2 min to record. CARS spectra shown in this article are pixel intensity profiles across the vibrational

frequencies and were extracted from the hyperspectral image data. Further information about the collection of CARS spectra can be found in Garbacik et al. [26]. In situ CARS images (512 × 512 pixels) covering 350 × 350 μm were recorded every 1.12 s HTS assay those (roughly 4.3 μs/pixel dwell time) for the duration of the dissolution experiments (15 min). All in situ CARS images recorded during dissolution testing were recorded at 2952 cm−1 and were false colored green. This peak has been assigned to antisymmetric C–H stretching in the methyl groups [27] and provided a strong CARS signal for both TPa and TPm. A deuterium light source (DT-MINI-2, Ocean Optics, The Netherlands) was connected by an optical fiber to a Z-shaped flow cell (FIA-Z-SMA, Ocean Optics, The Netherlands) with a 10 mm path length An optical fiber connected the Z-shaped flow

cell to a CCD spectrometer (USB2000+, Ocean Optics, The Netherlands). Open loop channel flow through intrinsic dissolution was conducted using a peristaltic pump (Reglo, ISMATEC, Germany), which pumped dissolution medium (distilled water or methyl cellulose 0.45% w/v) through the custom built CARS microscopy dissolution flow cell and through the Z-shaped UV flow cell at a rate of 5 mL/min. UV spectra were collected at 290 nm every 30 s. Dissolution was conducted multiple times on each sample to check for consistency. CARS spectra of the C–H stretch region were collected prior to dissolution experiments on pure TPa and TPm to identify an appropriate vibrational frequency at which to record CARS images during dissolution experiments and for comparison to the before and after dissolution hyperspectral scans of the compacts.