Fast 8 MHz polarization modulation
coupled with analytical modeling,
fast beam-scanning, and synchronous digitization (SD) have enabled
simultaneous nonlinear optical Stokes ellipsometry (NOSE) and polarized
laser transmittance imaging with image acquisition rates up to video
rate. In contrast to polarimetry, in which the polarization state
of the exiting beam is recorded, NOSE enables recovery of the complex-valued
Jones tensor of the sample that describes all polarization-dependent
observables of the measurement. Every video-rate scan produces a set
of 30 images (10 for each detector with three detectors operating
in parallel), each of which corresponds to a different polarization-dependent
result. Linear fitting of this image set contracts it down to a set
of five parameters for each detector in second harmonic generation
(SHG) and three parameters for the transmittance of the incident beam.
These parameters can in turn be used to recover the Jones tensor elements
of the sample. Following validation of the approach using z-cut quartz,
NOSE microscopy was performed for microcrystals of both naproxen and
glucose isomerase. When weighted by the measurement time, NOSE microscopy
was found to provide a substantial (>7 decades) improvement in
the
signal-to-noise ratio relative to our previous measurements based
on the rotation of optical elements and a 3-fold improvement relative
to previous single-point NOSE approaches.
Here we demonstrate the use of second harmonic generation (SHG) microscopy-guided synchrotron powder X-ray diffraction (PXRD) for the detection of trace crystalline active pharmaceutical ingredients in a common polymer blend. The combined instrument is capable of detecting 100 ppm crystalline ritonavir in an amorphous hydroxypropyl methylcellulose matrix with a high signal-to-noise ratio (>5000). The high spatial resolution afforded by SHG microscopy allows for the use of a minibeam collimator to reduce the total volume of material probed by synchrotron PXRD. The reduction in probed volume results in reduced background from amorphous material. The ability to detect low crystalline loading has the potential to improve measurements in the formulation pipeline for pharmaceutical solid dispersions, for which even trace quantities of crystalline active ingredients can negatively impact the stability and bioavailability of the final drug product.
Second harmonic generation (SHG) microscopy was used to rapidly identify regions of interest for localized confocal Raman spectroscopy measurements in order to quantify crystallinity within lyophilized Abraxane powder (protein bound paclitaxel for injectable suspension). Water insoluble noncentrosymmetric crystalline particles ranging from ∼1 to 120 μm were identified by SHG, with wide variability in crystal size and frequency observed between several batches of Abraxane. By targeting the Raman analysis to these localized regions identified by SHG, the required measurement time was decreased over 2 orders of magnitude, from 8 h to 2 s. Experimental Raman spectra of SHG active domains in Abraxane were in good agreement with experimental spectra of pure crystalline paclitaxel. These collective results are consistent with up to 30% of the active ingredient being present as poorly soluble crystalline particulates in some batches of Abraxane.
Nonlinear optical Stokes ellipsometric (NOSE) microscopy was demonstrated for the analysis of collagen-rich biological tissues. NOSE is based on polarization-dependent second harmonic generation imaging. NOSE was used to access the molecular-level distribution of collagen fibril orientation relative to the local fiber axis at every position within the field of view. Fibril tilt-angle distribution was investigated by combining the NOSE measurements with ab initio calculations of the predicted molecular nonlinear optical response of a single collagen triple helix. The results were compared with results obtained previously by scanning electron microscopy, nuclear magnetic resonance imaging, and electron tomography. These results were enabled by first measuring the laboratory-frame Jones nonlinear susceptibility tensor, then extending to the local-frame tensor through pixel-by-pixel corrections based on local orientation.
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