I’ve been gathering data for a paper using my microporous MgF2 nanomembranes so here are some sample figures for such a paper.
Herein, we are trying to create a porous, Raman-compatible substrate for use in cell culture. Researchers have used Raman microspectroscopy to perform quantitative non-invasive measurements of biomolecules in cells. It’s a very exciting technique. While silicon based substrates have excellent properties for cell culture, they have strong Raman background signals and absorb a lot of laser power at the illumination wavelengths we would like to use. MgF2, Quartz, and CaF2 are considered Raman-compatible for their substantially weaker backgrounds. Researchers currently deposit or culture cells on non-permeable coverglasses made of these materials. However, we have known that cells sometimes require a permeable substrate to adopt morphologies that are more consistent with in vivo studies of morphology. So using our microporous nitride substrates, we wish to create a substrate that will have both the permeability and the Raman-compatibility necessary to facilitate more accurate Raman studies of those types of cells.
Figure 1. MgF2 nanomembrane material properties. (a)-(b) MgF2 relief pattern transfer, with cartoon crossections of microporous films (not to scale). Beginning with a freestanding film of microporous silicon nitride (a), MgF2 is evaporated onto the substrate (200 nm, 0.1-0.3 nm/sec, 250 °C, Platen Rotation), coating the porous substrate, resulting in a hybrid material. (b) The substrate is then inverted and purified using RIE (90% CHF3, 10% Oxygen, 75 mTorr, 100 W), releasing a freestanding nanoporous film of MgF2. (c) A SEM image normal to the membrane plane shows the infilling effect of the direct evaporation process, as the template pores narrow from their designed 500 nm diameters to approximately 325 nm. (d) SEM crossection of a partially etched MgF2 nanomembrane (with some template backing remaining), showing film thickness close to the targeted 200 nm.
EDS measurement of the composition of the freestanding membrane. While the Mg and F signals are preserved across the freestanding region, the Si signal is not. The membranes are >85% MgF2 in the freestanding region. As a side note, there was some sample drift, so the image is blurred. This is a 30kX image.
Before Etch
After Etch
Previous Figure with 50 nm thick nanoporous MgF2. Here the burst pressure for the 200 nm microporous MgF2 is about 7 PSI, over a 5-slot structure instead of a square window.
20X Live/Dead stain image of P6 HUVECS (Day 7) on fabricated microporous MgF2 grown in MCDB131 media. Eventually, we will use ARPE-19 Cells with tight junction staining which have a characteristic response to permeable substrates.
We will have to reestabilish the Raman background of the membranes, but the material composition looks to be the same as with my nanoporous material. HUVECS seem to stick ok without using any additional coatings.
Hi all, recently we improved cell tracking with the use of SiR-DNA label (see highlights below). random migration: A. Representative cell tracking from three independent migration experiments, color-coded by the color bars to the left in red, green, and blue. B. Distributions of motility parameters (persistence time, instantaneous speed, average speed, pathlength, and displacement)…
We ordered quantum dots from Invitrogen. These QDs have a PEG coating that terminates in COOH and should cause the dots to be negatively charged. They are about 12.6 nm in diameter: They exhibit a -40mV zeta potential by zetasizer measurements, however the particles appear to aggregate a great deal (under microscope and visibly turn…
Since I’m now back pretty much full time on the filter project, I’ll give a quick update about where we stand and where I’m going with it, as well as some (negative) results from this week. On the membrane transfer side of things, we finally have a tool that can produce fine enough vapor…
It was speculated that the rate of diffusion through a charged membrane had a direct relationship with pressure – as pressure increases, the kinetic energy of the charged particles is more likely to overcome the electrostatic repulsion of the membrane, until at a high enough pressure the repulsive force is small enough to be ignored….
This is the final post (hopefully) summarizing my simulation results I did to model Endohm system. Barrett used endohm cup system to do the coculture of bEnd3 and glial cells for his BBB studies. The resistance values obtained while using pncSi and uniformly porous membrane for cell growth were drastically different, and it was not very…
In my earlier posts, as well as in Josh’s NPN paper and Tom’s ACS nano paper, we’ve talked a lot about the resolutions of nanoparticle separations. What we mean by it is how well the membrane is able to discriminate between two similarly sized particles. For instance, we predict that a series of gold nanoparticle filtrations…