Nanoparticle transport in conical-shaped nanopores.

This report presents a fundamental study of nanoparticle transport phenomena in conical-shaped pores contained within glass membranes. The electrophoretic translocation of charged polystyrene (PS) nanoparticles (80- and 160-nm-radius) was investigated using the Coulter counter principle (or "resistive-pulse" method) in which the time-dependent nanopore current is recorded as the nanoparticle is driven across the membrane. Particle translocation through the conical-shaped nanopore results in a direction-dependent and asymmetric triangular-shaped resistive pulse. Because the sensing zone of conical-shaped nanopores is localized at the orifice, the translocation of nanoparticles through this zone is very rapid, resulting in pulse widths of ~200 μs for the nanopores used in this study. A linear dependence between translocation rate and nanoparticle concentration was observed from 10(7) to 10(11) particles/mL for both 80- and 160-nm-radius particles, and the magnitude of the resistive pulse scaled approximately in proportion to the particle volume. A finite-element simulation based on continuum theory to compute ion fluxes was combined with a dynamic electric force-based nanoparticle trajectory calculation to compute the position- and time-dependent nanoparticle velocity as the nanoparticle translocates through the conical-shaped nanopore. The computational results were used to compute the resistive pulse current-time response for conical-shaped pores, allowing comparison between experimental and simulated pulse heights and translocation times. The simulation and experimental results indicate that nanoparticle size can be differentiated based on pulse height, and to a lesser extent based on translocation time.

[1]  J. Reiner,et al.  Theory for polymer analysis using nanopore-based single-molecule mass spectrometry , 2010, Proceedings of the National Academy of Sciences.

[2]  Richard M Crooks,et al.  A carbon nanotube-based coulter nanoparticle counter. , 2004, Accounts of chemical research.

[3]  Charles R. Martin,et al.  Nanomaterials: A Membrane-Based Synthetic Approach , 1994, Science.

[4]  Demonstration of Coulter counting through a cylindrical solid state nanopore , 2008 .

[5]  Richard M. Crooks,et al.  Single Carbon Nanotube Membranes: A Well-Defined Model for Studying Mass Transport through Nanoporous Materials , 2000 .

[6]  J. P. Guerrette,et al.  Scan-rate-dependent current rectification of cone-shaped silica nanopores in quartz nanopipettes. , 2010, Journal of the American Chemical Society.

[7]  Chuen Ho,et al.  Electrolytic transport through a synthetic nanometer-diameter pore. , 2005, Proceedings of the National Academy of Sciences of the United States of America.

[8]  Susan Daniel,et al.  Single ion-channel recordings using glass nanopore membranes. , 2007, Journal of the American Chemical Society.

[9]  D. Branton,et al.  Characterization of individual polynucleotide molecules using a membrane channel. , 1996, Proceedings of the National Academy of Sciences of the United States of America.

[10]  Henry S White,et al.  Resistive Pulse Analysis of Microgel Deformation During Nanopore Translocation. , 2011, The journal of physical chemistry. C, Nanomaterials and interfaces.

[11]  C. Martin,et al.  Highly sensitive methods for electroanalytical chemistry based on nanotubule membranes. , 1999, Analytical chemistry.

[12]  C. R. Martin,et al.  Electrophoretic protein transport in gold nanotube membranes. , 2003, Analytical chemistry.

[13]  Stephen W. Feldberg,et al.  Current Rectification at Quartz Nanopipet Electrodes , 1997 .

[14]  R. Crooks,et al.  Comparison of nanoparticle size and electrophoretic mobility measurements using a carbon-nanotube-based coulter counter, dynamic light scattering, transmission electron microscopy, and phase analysis light scattering. , 2004, Langmuir : the ACS journal of surfaces and colloids.

[15]  C. P. Bean,et al.  Counting and Sizing of Submicron Particles by the Resistive Pulse Technique , 1970 .

[16]  Lydia L. Sohn,et al.  Direct detection of antibody–antigen binding using an on-chip artificial pore , 2003, Proceedings of the National Academy of Sciences of the United States of America.

[17]  R. Kawano,et al.  Quartz nanopore membranes for suspended bilayer ion channel recordings. , 2010, Analytical Chemistry.

[18]  Javier Cervera,et al.  Ionic conduction, rectification, and selectivity in single conical nanopores. , 2006, The Journal of chemical physics.

[19]  C. R. Martin,et al.  Conical nanopore membranes. Preparation and transport properties. , 2004, Analytical chemistry.

[20]  R W DeBlois,et al.  Sizes and concentrations of several type C oncornaviruses and bacteriophage T2 by the resistive-pulse technique , 1977, Journal of virology.

[21]  Sean Conlan,et al.  Stochastic sensing of organic analytes by a pore-forming protein containing a molecular adapter , 1999, Nature.

[22]  K. Rubinson,et al.  Single-molecule mass spectrometry in solution using a solitary nanopore , 2007, Proceedings of the National Academy of Sciences.

[23]  H. White,et al.  Steady-state voltammetric response of the nanopore electrode. , 2006, Analytical chemistry.

[24]  R. Crooks,et al.  Observation of DNA transport through a single carbon nanotube channel using fluorescence microscopy. , 2003, Chemical communications.

[25]  A. Bund,et al.  Mechanism of electrostatic gating at conical glass nanopore electrodes. , 2008, Langmuir : the ACS journal of surfaces and colloids.

[26]  Charles R. Martin,et al.  Resistive-Pulse SensingFrom Microbes to Molecules , 2000 .

[27]  H. White,et al.  The nanopore electrode. , 2004, Analytical chemistry.

[28]  Andreas Bund,et al.  Ion current rectification at nanopores in glass membranes. , 2008, Langmuir : the ACS journal of surfaces and colloids.

[29]  Richard M Crooks,et al.  Simultaneous determination of the size and surface charge of individual nanoparticles using a carbon nanotube-based Coulter counter. , 2003, Analytical chemistry.

[30]  B. Schiedt,et al.  A Poisson/Nernst-Planck model for ionic transport through synthetic conical nanopores , 2005 .

[31]  A. Fadeev,et al.  Trialkylsilane Monolayers Covalently Attached to Silicon Surfaces: Wettability Studies Indicating that Molecular Topography Contributes to Contact Angle Hysteresis , 1999 .

[32]  J. Reiner,et al.  Changes in ion channel geometry resolved to sub-ångström precision via single molecule mass spectrometry , 2010, Journal of physics. Condensed matter : an Institute of Physics journal.

[33]  Ryan J. White,et al.  Bench-top method for fabricating glass-sealed nanodisk electrodes, glass nanopore electrodes, and glass nanopore membranes of controlled size. , 2007, Analytical chemistry.

[34]  Richard M Crooks,et al.  The resurgence of Coulter counting for analyzing nanoscale objects. , 2004, The Analyst.

[35]  Z. Siwy,et al.  Ion‐Current Rectification in Nanopores and Nanotubes with Broken Symmetry , 2006 .

[36]  Lydia L. Sohn,et al.  Quantitative sensing of nanoscale colloids using a microchip Coulter counter , 2001 .

[37]  Susan Daniel,et al.  Ionic conductivity of the aqueous layer separating a lipid bilayer membrane and a glass support. , 2006, Langmuir : the ACS journal of surfaces and colloids.

[38]  David G. Grier,et al.  The charge of glass and silica surfaces , 2001 .

[39]  Royce W Murray,et al.  Nanoelectrochemistry: metal nanoparticles, nanoelectrodes, and nanopores. , 2008, Chemical reviews.

[40]  Z. Siwy,et al.  Conical-nanotube ion-current rectifiers: the role of surface charge. , 2004, Journal of the American Chemical Society.

[41]  M. Wood,et al.  A silica nanochannel and its applications in sensing and molecular transport. , 2009, Analytical chemistry.