John Bowman, Recent Talks

  • Bounds on the Global Attractor of 2D Incompressible Turbulence in the palenstrophy-enstrophy-energy space, AMS Fall Western Virtual Sectional Meeting (October 25, 2020).*
  • FFTW++: A Hybrid OpenMP/MPI Implementation of FFTs and Implicitly Dealiased Convolutions, SIAM Conference on Parallel Processing for Scientific Computing, Seattle, Washington (February 14, 2020).*
  • How to Design an Efficient Pseudospectral Code, Canadian Applied and Industrial Mathematics Society Meeting, Whistler, British Columbia (June 11, 2019).*
  • A New Technique for Constructing Exponential Integrators, Canadian Applied and Industrial Mathematics Society Meeting, Whistler, British Columbia (June 10, 2019).*
  • Exponential Integrators, Canadian Mathematical Society Meeting Vancouver, British Columbia (December 8, 2018).*
  • On the Global Attractor of 2D Incompressible Turbulence with Random Forcing and Friction, American Mathematical Society Meeting, Fayetteville, Arkansas (November 3, 2018).*
  • On the Global Attractor of 2D Incompressible Turbulence with Random Forcing and Friction, Canadian Applied and Industrial Mathematics Society Meeting, Toronto, Ontario (June 5, 2018).*
  • On the Global Attractor of 2D Incompressible Turbulence with Random Forcing, University of Texas at Austin, Austin, Texas (March 23, 2018).*
  • On the Global Attractor of 2D Incompressible Turbulence with Random Forcing, Princeton University, Princeton, New Jersey (February 19, 2018).*
  • What Is Missing in High School Mathematics Education? High School Professional Development Day, Edmonton, Alberta (November 27, 2017).*
  • On the Global Attractor of 2D Incompressible Turbulence with Random Forcing, Indiana University, Bloomington, Indiana (October 25, 2017).*
  • Pseudospectral methods for investigating the global attractor of 2D turbulence, Americas XI Conference on Differential Equations and Nonlinear Analysis, Edmonton, Alberta (August 19, 2017).
  • On the Global Attractor of 2D Incompressible Turbulence with Random Forcing, Mathematical Congress of the Americas, Montreal, Quebec (July 27, 2017).*
  • The Partial Fourier Transform, Canadian Applied and Industrial Mathematics Society Meeting, Halifax, Nova Scotia (July 19, 2017).*
  • What Is Missing in High School Mathematics Education? Alberta Mathematics Dialog, Edmonton, Alberta (May 5, 2017).*
  • What Is Missing in High School Mathematics Education? Alberta Education Mathematics Expert Working Group, Edmonton, Alberta (January 13, 2017).*
  • Implicitly Dealiased Convolutions on Shared-Memory and Distributed-Memory Parallel Processors, Canadian Applied and Industrial Mathematics Society Meeting, Edmonton, Alberta (June 29, 2016).*
  • Using Partial Fourier Transforms to Study Kolmogorov's Inertial-Range Flux, Canadian Applied and Industrial Mathematics Society Meeting, Edmonton, Alberta (June 28, 2016).*
  • Recent Advances in the Pseudospectral Method, Challenges in Nonequilibrium Statistical Physics and Fluid Dynamics Provo, Utah (May 24, 2016).*
  • Adaptive Transpose Algorithms for Distributed Multicore Processors, SIAM Conference on Parallel Processing for Scientific Computing, Paris, France (April 15, 2016).
  • Recent Advances in the Pseudospectral Method, SIAM Conference on Analysis of Partial Differential Equations, Scottsdale, Arizona (December 8, 2015).*
  • Adaptive Matrix Transpose Algorithms for Distributed Multicore Processors, Canadian Association of Physicists Meeting, Edmonton, Alberta (June 16, 2015).
  • Implicitly Padded Convolutions on Hybrid Parallel Architectures", Canadian Applied and Industrial Mathematics Society Meeting, Waterloo, Ontario (June 8, 2015).*
  • How Important is Dealiasing for Turbulence Simulations? UCLA Institute for Pure and Applied Mathematics, Los Angeles, California (September 30, 2014).*
  • Adaptive Matrix Transpose Algorithms for Distributed Multicore Processors, Canadian Applied and Industrial Mathematics Society Meeting, Saskatoon, Saskatchewan (June 25, 2014).*
  • What Is Missing in High School Mathematics Education? Alberta Mathematics Dialogue, Camrose, Alberta (May 1, 2014).*
  • Adaptive Matrix Transpose Algorithms for Distributed Multicore Processors, International Interdisciplinary Conference on Applied Mathematics, Modeling and Computational Science, Waterloo, Ontario (August 30, 2013).
  • Pseudospectral Reduction of Incompressible Two-Dimensional Turbulence, Mathematical Congress of the Americas, Guanajuato, Mexico (August 5, 2013).*
  • How Important is Dealiasing for Turbulence Simulations? Canadian Applied and Industrial Mathematics Society Meeting, Quebec, Quebec (June 19, 2013).*
  • Implicit Dealiasing of Convolutions over Distributed Memory, Canadian Applied and Industrial Mathematics Society Meeting, Quebec, Quebec (June 17, 2013).*
  • Pseudospectral Reduction of Incompressible Two-Dimensional Turbulence, Euromech Colloqium 542: Progress in Statistical Theory and Pseudospectral DNS, Lyon, France (January 18, 2013).*
  • Turbulence, Scientific Computing, and Visualization, Graduate Research Day, Department of Mathematical and Statistical Sciences, University of Alberta Edmonton, Alberta (October 25, 2012).
  • Pseudospectral Reduction of Incompressible Two-Dimensional Turbulence, Canadian Applied and Industrial Mathematics Society Meeting, Toronto, Ontario (June 25, 2012).*
  • Structure-Preserving and Exponential Discretizations of Initial-Value Problems, Condensed Matter Physics Seminar, Edmonton, Alberta (March 29, 2012).*
  • Pseudospectral Reduction of Incompressible Two-Dimensional Turbulence, Canadian Mathematical Society Meeting, Toronto, Ontario (December 12, 2011).*
  • Casimir Cascades in Two-Dimensional Turbulence, SIAM Conference on Analysis of Partial Differential Equations, San Diego, California (November 17, 2011).*
  • Pseudospectral Reduction of Incompressible Two-Dimensional Turbulence, SIAM Conference on Analysis of Partial Differential Equations, San Diego, California (November 15, 2011).*
  • Pseudospectral Reduction of Incompressible Two-Dimensional Turbulence , Geophysical Fluid Dynamics Program, Woods Hole Oceanographic Institute Woods Hole, MA (July 21, 2011).*
  • Casimir Cascades in Two-Dimensional Turbulence, Canadian Mathematical Society Meeting, Edmonton, Alberta (June 4, 2011).*
  • Casimir Cascades in 2D Turbulence, Kavli Institute for Theoretical Physics: The Nature of Turbulence, Santa Barbara, California (March 23, 2011).*
  • The Pseudospectral Method: Recent Advances and Prospects, Part II, Kavli Institute for Theoretical Physics: The Nature of Turbulence, Santa Barbara, California (March 18, 2011).*
  • The Pseudospectral Method: Recent Advances and Prospects, Part I, Kavli Institute for Theoretical Physics: The Nature of Turbulence, Santa Barbara, California (March 14, 2011).*
  • Reduced Order Modeling for Turbulent Flows, Kavli Institute for Theoretical Physics: The Nature of Turbulence, Santa Barbara, California (February 23, 2011).*
  • Open Problems in Turbulence, Kavli Institute for Theoretical Physics: The Nature of Turbulence, Santa Barbara, California (February 9, 2011).*
  • Casimir Cascades in Two-Dimensional Turbulence, Physics Colloquium, Edmonton, Alberta (September 24, 2010).*
  • Dealiased Convolutions without the Padding, Canadian Applied and Industrial Mathematics Society Meeting, St. John's, Newfoundland (June 20, 2010).*
  • Interactive TeX-Aware 3D Vector Graphics, TeX Users Group 2010, San Francisco, California (June 30, 2010).*
  • Dealiased Convolutions without the Padding, Waves Phenomena IV Edmonton, Alberta (June 15, 2010).
  • The Fastest Convolution in the West, Applied Mathematics Institute Seminar, Edmonton, Alberta (April 13, 2010).*
  • Casimir Cascades in Two-Dimensional Turbulence, Fluids Seminar, Edmonton, Alberta (February 24, 2010).*
  • To Infinity and Beyond! Last Lecture on Earth Series, University of Alberta, Edmonton, Alberta (January 27, 2010).*
  • Casimir Cascades in Two-Dimensional Turbulence, 1051st American Mathematical Society Meeting, Waco, Texas (October 17, 2009).*
  • The Multispectral Method: Progress and Prospects, 12th EUROMECH European Turbulence Conference, Marburg, Germany (September 9, 2009).
  • Casimir Cascades in Two-Dimensional Turbulence, 12th EUROMECH European Turbulence Conference, Marburg, Germany (September 8, 2009).
  • Exponential Integrators, Canadian Applied and Industrial Mathematics Society Meeting, London, Ontario (June 11, 2009).
  • A Fully Lagrangian Advection Scheme, Canadian Mathematical Society, St. John's, Newfoundland (June 8, 2009).*
  • A Fully Lagrangian Advection Scheme, Canadian Mathematical Society, Ottawa, Ontario (December 6, 2008).*
  • Casimir Cascades in Two-Dimensional Turbulence, The 18th Canadian Symposium on Fluid Dynamics, Montreal, Quebec (June 4, 2008).*
  • Casimir Cascades in Two-Dimensional Turbulence, The 32nd SIAM Southeastern-Atlantic Section Conference, Orlando, Florida (March 14, 2008).*
  • Casimir Cascades in Two-Dimensional Turbulence, 1032nd American Mathematical Society Meeting, Albuquerque, New Mexico (October 13, 2007).*
  • Asymptote: The Vector Graphics Language, Philipps-Universität Marburg, Marburg, Germany (August 16, 2007).*
  • The 3D Asymptote Generalization of the MetaPost Bezier Interpolation Algorithms, International Congress on Industrial and Applied Mathematics, Zurich, Switzerland (July 16, 2007).
  • Exponential Integrators, Canadian Applied and Industrial Mathematics Society Meeting, Banff, Alberta (May 22, 2007).*
  • Asymptote: The Vector Graphics Language, Workshop on Two-Dimensional Turbulence, Lorentz Center, Leiden University, The Netherlands (March 22, 2007).*
  • Asymptote: The Vector Graphics Language, University of Texas at Austin, Austin, Texas (February 22, 2007).*
  • Links between dissipation, intermittency, and helicity in the GOY shell model, University of Texas at Austin, Austin, Texas (February 22, 2007).*
  • Links between dissipation, intermittency, and helicity in the GOY shell model, 17th Canadian Symposium on Fluid Dynamics, Toronto, Ontario (June 17-19, 2006).*
  • A Fully Lagrangian Advection Scheme, Fifth International Conference on Scientific Computing and Applications, Banff, Alberta (May 18-21, 2006).
  • Structure-Preserving and Exponential Discretizations of Initial-Value Problems, 26th MidWest-Pacific Differential Equations Conference, Edmonton, Alberta (October 15, 2005).
  • Mode Reduction Schemes and Subgrid Models for Homogeneous Turbulence, Workshop on Representing Unresolved Degrees of Freedom for the Atmosphere and Ocean, Montreal, Quebec (March 3, 2005).*
  • Turbulent Cascades: What Length Scale Enters the Intermittency Correction? Theoretical Physics Institute Symposium, Banff, Alberta (September, 2004).*
  • Local vs. Nonlocal Enstrophy Flux in Two-Dimensional Turbulence, 5th International Conference on Dynamical Systems and Differential Equations, Pomona, California (June, 2004).*
  • Spectral Reduction of the GOY Shell Turbulence Model, Canadian Applied and Industrial Mathematics Society Meeting, Halifax, Canada (June, 2004).*
  • Structure-Preserving Discretizations of Initial-Value Problems, Oldenburg Universität, Oldenburg, Germany (February, 2004).*
  • Spectral Reduction: A Statistical Description of Turbulence, Philipps-Universität Marburg, Marburg, Germany (October, 2003).*
  • The Dual Cascade in Bounded and Unbounded Two-Dimensional Fluids, Canadian Mathematical Society, Edmonton, Alberta (June, 2003).*
  • Realizable Markovian Closures, Stochastic Modeling of Geophysical Flows Workshop, National Center for Atmospheric Research, Boulder, Colorado (March, 2003).*
  • *=invited talk

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