Magnetically Coated Bioabsorbable Stents for Renormalization of Arterial Vessel Walls after Stent Implantation.

The insertion of a stent in diseased arteries is a common endovascular procedure that can be compromised by the development of short- and long-term inflammatory responses leading to restenosis and thrombosis, respectively. While treatment with drugs, either systemic or localized, has decreased the incidence of restenosis and thrombosis these complications persist and are associated with a high mortality in those that present with stent thrombosis. We reasoned that if stents could be made to undergo accelerated endothelialization in the deployed region, then such an approach would further decrease the occurrence of stent thrombosis and restenosis thereby improving clinical outcomes. Toward that objective, the first step necessitated efficient capture of progenitor stem cells, which eventually would become the new endothelium. To achieve this objective, we engineered intrinsic ferromagnetism within nonmagnetizable, biodegradable magnesium (Mg) bare metal stents. Mg stents were coated with biodegradable polylactide (PLA) polymer embedding magnetizable iron-platinum (FePt) alloy nanoparticles, nanomagnetic particles, nMags, which increased the surface area and hence magnetization of the stent. nMags uniformly distributed on stents enabled capture, under flow, up to 50 mL/min, of systemically injected iron-oxide-labeled (IO-labeled) progenitor stem cells. Critical parameters enhancing capture efficiency were optimized, and we demonstrated the generality of the approach by showing that nMag-coated stents can capture different cell types. Our work is a potential paradigm shift in engineering stents because implants are rendered as tissue in the body, and this "natural stealthiness" reduces or eliminates issues associated with pro-inflammatory immune responses postimplantation.

An analysis of early-stage IL-2 capture times in populations of T cells diffusively interacting in a confined environment.

This numerical analysis examines early-stage Interlukin-2 (IL-2) capture in large populations of secreting T helper (Th) and absorbing T regulatory (Treg) cells in an attempt to provide rational guidelines for when diffusive interactions can affect the Th autocrine cycle, as reflected in capture times. Autocrine and paracrine capture is calculated over a wide range of conditions: the mix of cells in a population; cell size and spacing; antigen activated IL-2 secretion and Th receptor expression rates; receptor dissociation constant; and number of resting Treg receptors. Correlations for quickly estimating IL-2 capture over these conditions are provided. This study suggests that a typical Treg can scavenge a significant amount of IL-2 without affecting autocrine capture by the Th. As a result, Treg influence on autocrine capture is shorter-ranged than previously reported. It is conjectured that high early-stage paracrine relative to autocrine capture leads to faster receptor enhancement for a Treg than a Th. The resulting enhancement time gap is considerably longer and, thus, diffusive suppression more likely, for a weakly- as opposed to strongly-activated Th. The methodology can be extended to later-stage capture to confirm this conjecture and to diffusive interactions in other cell-type populations.

Diffusive transfer between two intensely interacting cells with limited surface kinetics.

The diffusive transfer, or paracrine delivery, of chemical factors during the interaction of an emitting cell and a receiving cell is a ubiquitous cellular process that facilitates information exchange between the cells an/or to bystander cells. In the cellular immune response this exchange governs the magnitude and breadth of killing of cellular targets, inflammation or tolerance. Paracrine delivery is examined here by solving the the steady-state diffusion equation for the concentration field surrounding two intensely interacting, equi-sized cells on which surface kinetics limits the rates of factor emission and absorption. These chemical factors may be cytokines, such as Interlukins and Interferons, but the results are presented in a generic form so as to be applicable to any chemical factor and/or cell-type interaction. In addition to providing overall transfer rates and transfer efficiencies, the results also indicate that when the receiving cell is naïve, with few factor receptors on its surface, there may be a significant accumulation of factor in the synaptic region between the cells with a consequent release of factor to the medium where it can signal bystander cells. This factor accumulation may play a critical role in activating a naïve receiving cell. As the receiving cell activates and becomes more absorbent, the factor accumulation diminishes, as does potential bystander signaling.

A model for solvated ion emission from electrospray droplets.

A model is presented which shows that the energy required to emit small singly charged and large multiply charged (protein) solvated ions from electrospray droplets can be considerably lower than those predicted by earlier models. By allowing the droplet surface to distort in reaction to the emerging ion, a more nuanced picture of the ion emission mechanism appears, one that covers the range from pure ion evaporation (PIE) for small ions to what may be termed activated pseudo-Rayleigh ion release (PRIR), a mechanism that yields charge states nearly indistinguishable from the charge residue model (CRM), for large ions. Predictions based on this model are qualitatively consistent with many experimentally observed trends.

Discrete Charge Distributions in Dielectric Droplets.

The electrospray ion source has recently revolutionized mass spectrometry by allowing researchers to produce gaseous ions of very large molecular weights such as proteins and polymers. The process by which these high-molecular-weight ions are produced, however, is not very well understood. The purpose of the present work is to study the fields in the vicinity of each charge in order to shed some light on the ion formation process for charged dielectric droplets. An important feature of this work, therefore, is the treatment of the charge as discrete rather than continuous. The picture that emerges is of discrete charges in a dielectric droplet thermally oscillating around a potential well, located slightly below the droplet surface. The charges produce localized electrostatic pressures on the droplet surface that are higher (15.5 and 70% for dielectric constants of 80 and 20, respectively) than expected if the charge distribution were continuous. These high localized pressures could locally stretch the surface and result in the emission of ions or small charged droplets. The magnitude of these localized pressures is a function of the number of charges and the dielectric constant of the droplet. Copyright 1998 Academic Press.