Joseph E. Reiner

Nanoscopic Porous Sensors

There are thousands of different nanometer-scale pores in biology, many of which act as sensors for specific chemical agents. Recent work suggests that protein and solid-state nanopores have many potential uses in a wide variety of analytical applications. In this review we survey this field of research and discuss the prospects for advances that could be made in the near future.

Disease Detection and Management via Single Nanopore-Based Sensors

Sensors Joseph E. Reiner,*,† Arvind Balijepalli,‡,§ Joseph W. F. Robertson,‡ Jason Campbell,‡ John Suehle,‡ and John J. Kasianowicz‡ †Department of Physics, Virginia Commonwealth University, 701 W. Grace Street, Richmond, Virginia 23284, United States ‡Physical Measurement Laboratory, National Institute of Standards and Technology, Gaithersburg, Maryland 20899-8120, United States Laboratory of Computational Biology, National Heart Lung and Blood Institute, Rockville, Maryland 20852, United States

Theory for polymer analysis using nanopore-based single-molecule mass spectrometry

Nanometer-scale pores have demonstrated potential for the electrical detection, quantification, and characterization of molecules for biomedical applications and the chemical analysis of polymers. Despite extensive research in the nanopore sensing field, there is a paucity of theoretical models that incorporate the interactions between chemicals (i.e., solute, solvent, analyte, and nanopore). Here, we develop a model that simultaneously describes both the current blockade depth and residence times caused by individual poly(ethylene glycol) (PEG) molecules in a single α-hemolysin ion channel. Modeling polymer-cation binding leads to a description of two significant effects: a reduction in the mobile cation concentration inside the pore and an increase in the affinity between the polymer and the pore. The model was used to estimate the free energy of formation for K+-PEG inside the nanopore (≈-49.7 meV) and the free energy of PEG partitioning into the nanopore (≈0.76 meV per ethylene glycol monomer). The results suggest that rational, physical models for the analysis of analyte-nanopore interactions will develop the full potential of nanopore-based sensing for chemical and biological applications.

Capture and release of a conditional state of a cavity QED system by quantum feedback

Detection of a single photon escaping an optical cavity QED system prepares a nonclassical state of the electromagnetic field. The evolution of the state can be modified by changing the drive of the cavity. For the appropriate feedback, the conditional state can be captured (stabilized) and then released. This is observed by a conditional intensity measurement that shows suppression of vacuum Rabi oscillations for the length of the feedback pulse and their subsequent return.

Temperature Sculpting in Yoctoliter Volumes

The ability to perturb large ensembles of molecules from equilibrium led to major advances in understanding reaction mechanisms in chemistry and biology. Here, we demonstrate the ability to control, measure, and make use of rapid temperature changes in fluid volumes that are commensurate with the size of single molecules. The method is based on attaching gold nanoparticles to a single nanometer-scale pore formed by a protein ion channel. Visible laser light incident on the nanoparticles causes a rapid and large increase of the adjacent solution temperature, which is estimated from the change in the nanopore ionic conductance. The temperature shift also affects the ability of individual molecules to enter into and interact with the nanopore. This technique could significantly improve sensor systems and force measurements based on single nanopores, thereby enabling a method for single molecule thermodynamics and kinetics.

Theory of Polymer-Nanopore Interactions Refined Using Molecular Dynamics Simulations

Molecular dynamics simulations were used to refine a theoretical model that describes the interaction of single polyethylene glycol (PEG) molecules with α-hemolysin (αHL) nanopores. The simulations support the underlying assumptions of the model, that PEG decreases the pore conductance by binding cations (which reduces the number of mobile ions in the pore) and by volume exclusion, and provide bounds for fits to new experimental data. Estimation of cation binding indicates that four monomers coordinate a single K(+) in a crown-ether-like structure, with, on average, 1.5 cations bound to a PEG 29-mer at a bulk electrolyte concentration of 4 M KCl. Additionally, PEG is more cylindrical and has a larger cross-section area in the pore than in solution, although its volume is similar. Two key experimental quantities of PEG are described by the model: the ratio of single channel current in the presence of PEG to that in the polymers absence (blockade depth) and the mean residence time of PEG in the pore. The refined theoretical model is simultaneously fit to the experimentally determined current blockade depth and the mean residence times for PEGs with 15 to 45 monomers, at applied transmembrane potentials of -40 to -80 mV and for three electrolyte concentrations. The model estimates the free energy of the PEG-cation complexes to be -5.3 kBT. Finally the entropic penalty of confining PEG to the pore is found to be inversely proportional to the electrolyte concentration.

Optically trapped aqueous droplets for single molecule studies

We demonstrate a technique for creating, manipulating, and combining femtoliter volume chemical containers. The containers are surfactant-stabilized aqueous droplets in a low index-of-refraction fluorocarbon medium. The index-of-refraction mismatch between the container and fluorocarbon is such that individual droplets can be optically trapped by single focus laser beams, i.e., optical tweezers. Here, we trap and manipulate individual droplets, detect the fluorescence from single dye and red fluorescent protein molecules encapsulated in droplets, and observe fluorescence resonance energy transfer from a single dye pair on a deoxyribonucleic acid molecule encapsulated in a droplet.

Changes in ion channel geometry resolved to sub-ångström precision via single molecule mass spectrometry

The ion channel formed by Staphylococcus aureus alpha-hemolysin switches between multiple open conducting states. We describe a method for precisely estimating the changes in the ion channel geometry that correspond to these different states. Experimentally, we observed that the permeability of a single channel to differently sized poly(ethylene glycol) molecules depends on the magnitude of the open state conductance. A simple theory is proposed for determining changes in channel length of 4.2% and in cross-sectional area of -0.4%.

Stable and robust polymer nanotubes stretched from polymersomes.

We create long polymer nanotubes by directly pulling on the membrane of polymersomes using either optical tweezers or a micropipette. The polymersomes are composed of amphiphilic diblock copolymers, and the nanotubes formed have an aqueous core connected to the aqueous interior of the polymersome. We stabilize the pulled nanotubes by subsequent chemical cross-linking. The cross-linked nanotubes are extremely robust and can be moved to another medium for use elsewhere. We demonstrate the ability to form networks of polymer nanotubes and polymersomes by optical manipulation. The aqueous core of the polymer nanotubes together with their robust character makes them interesting candidates for nanofluidics and other applications in biotechnology.

Generation and mixing of subfemtoliter aqueous droplets on demand.

We describe a novel method of generating monodisperse subfemtoliter aqueous droplets on demand by means of piezoelectric injection. Droplets with volumes down to 200 aL are generated by this technique. The droplets are injected into a low refractive index perfluorocarbon so that they can be optically trapped. We demonstrate the use of optical tweezers to manipulate and mix droplets. For example, using optical tweezers we bring two droplets, one containing a calcium sensitive dye and the other calcium chloride, into contact. The droplets coalesce with a resulting reaction time of about 1 ms. The monodispersity, manipulability, repeatability, small size, and fast mixing afforded by this system offer many opportunities for nanochemistry and observation of chemical reactions on a molecule-by-molecule basis.