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The described procedure results in aerogels containing viable cyt. c. As specified at the end of the introduction, cyt. c can be encapsulated from aqueous buffer solutions that range from 4.4 to 70 mM phosphate. Examples of cyt. c-silica (cyt. c-SiO2) aerogels made from solutions containing different buffer concentrations are shown in Figure 4. All gels are relatively translucent, with the gels made from 70 mM buffer the most opaque.
A comparison of the spectroscopy of cyt. c under different conditions is shown in Figure 5. A typical spectrum (Figure 5c) shows the large Soret peak around 408 nm for cyt. c-SiO2 aerogels and is very similar to the spectrum of cyt. c in solution (Figure 5a). In addition, a spectrum of cyt. c encapsulated within aerogels with metal nanoparticles is also shown (Figure 5b) and the cyt. c-SiO2 aerogel spectrum is similar to this spectrum as well. When the cyt. c-SiO2 aerogel is exposed to nitric oxide, a typical shifting of the Soret peak is observed (Figure 5d).
The UV-vis spectra for gels made from cyt. c solutions in varying buffer concentrations are shown in Figure 6. All of these gels show characteristic UV-visible spectroscopic features indicating that cyt. c is not in a denatured state within the gels. However, the decreased translucency of the gels made from 70 mM buffer results in a lower signal-to-noise ratio for these spectra.
The CD spectra of cyt. c-SiO2 aerogels are similar to the spectra of cyt. c encapsulated within aerogels with metal nanoparticles, while both types of aerogel spectra differ from a spectrum of cyt. c in buffered solution (Figure 7).
Figure 8 shows a typical nitric oxide monitoring response for cyt. c-SiO2 aerogels and corresponding aerogels that also contain metal nanoparticles in addition to cyt. c. The difference between the absorbance at 414 nm and that at 408 nm is seen to increase and then decrease when the gels are exposed to nitric oxide and then nitrogen respectively in succession.
If the supercritical carbon dioxide is not released at a slow enough rate, the viability of the cyt. c within the formed aerogels will be compromised. This is revealed by comparing resulting UV-visible spectra after forming gels by releasing the carbon dioxide at different rates (Figure 9).

Figure 1: Critical point drying apparatus. The critical point drying apparatus shown from the (A) front and (B) back with the transfer boat and apparatus door shown next to the back of the apparatus.

Figure 2: Cardboard platform. The assembled cardboard platform for holding an aerogel in the path of an instrument's beam.

Figure 3: Nitric oxide sensing set-up. The nitric oxide sensing set-up is shown including (A) the fume hood enclosed 10% nitric oxide, 90% nitrogen cylinder, tubing, and T-valve, and (B) the cuvette with inserted needles.

Figure 4: Sample cyt. c-SiO2 aerogels. Aerogels encapsulating 15 μM cyt. c in 4.4 mM, 40 mM, and 70 mM potassium phosphate buffer are shown in comparison to a dime from left to right. These aerogels are approximately 0.2-0.5-cm high. Reprinted with permission9.

Figure 5: Cyt. c-SiO2 aerogel spectroscopy. Visible spectra of 15 μM cytochrome c in (a) 50 mM phosphate buffer solution; (b) Au(5-nm)~cyt. c-SiO2 aerogel; (c) cyt. c–SiO2 aerogel (exposed to air); (d) cyt. c-SiO2 aerogel (exposed to nitric oxide for 3.5 min). These representative spectra of each type of gel are offset for clarity, and the dashed line denotes the position of the Soret peak of cyt. c in buffer. While each spectrum is of 15 μM cyt. c, the gel thicknesses (or heights) are only 0.2-0.5-cm compared to the 1-cm solution cuvet resulting in a higher solution absorbance. Reprinted with permission9.

Figure 6: Aerogel spectroscopy as encapsulated buffer concentration is varied. Averaged UV-visible spectral absorbance of aerogels divided by gel path length for gels encapsulating 15 μM cyt. c in 70 mM (black) (average of 4 spectra), 40 mM (red, dotted) (average of 8 spectra), and 4.4 mM (green, dashed) (average of 9 spectra) potassium phosphate buffer. Reprinted with permission9.

Figure 7: Aerogel circular dichroism spectroscopy. Circular dichroism spectra of cyt. c in sodium phosphate buffered solution (solid), two representative spectra of cyt. c-SiO2 aerogels (dashed), and two representative spectra of Au(5-nm)~cyt. cSiO-2 aerogels (dotted). Reprinted with permission9.

Figure 8: Nitric oxide detection with cyt. c-SiO2 aerogels. Monitoring the shift (ΔA = A414 nm - A408 nm) in the Soret intensity of cyt. c (solid red) and Au~cyt. c (dashed blue) encapsulated in SiO2 composite aerogel nanoarchitectures as gas flow is toggled between nitrogen (where Soret peak maximum is at ~408 nm) and nitric oxide (where Soret peak maximum is at ~414 nm). Each curve is an average of 3-4 trials, with two of the cyt. c-SiO2 trials monitored at ΔA = A414 nm - A407 nm since the initial Soret peak maximum was at 407 nm for these trials. Reprinted with permission9.

Figure 9: Effect of supercritical fluid release time. Averaged UV-visible spectral absorbance divided by gel path length for cyt. c-SiO2 aerogels encapsulating 10 μM cyt. c in 50 mM phosphate buffer in which the supercritically dried aerogels were made by either releasing supercritical carbon dioxide over 45 min (solid, black (average of 9 spectra)) or 7 min (dashed, red (average of 4 spectra)). Reprinted with permission9.