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D. Gagnon

Publications and source records attributed to D. Gagnon.

4 recordsLinked to original sources

Undulatory swimming in viscoelastic fluids under confinement

Low Reynolds number swimmers frequently move near boundaries, such as spirochetes moving through porous tissues and sperm navigating the reproductive tract. Furthermore, these microorganisms must often navigate non-Newtonian fluids such as mucus, which are typically shear-thinning and viscoelastic. Here, we experimentally investigate such a system using the model biological organism \textit{C. elegans} swimming through microfluidic channels containing viscous Newtonian fluids and viscoelastic fluids. Swimmer kinematics and resulting flow fields are measured as a function of channel width and therefore the strength of confinement. Results show that, for viscoelastic fluids, weak or moderate confinement can lead to enhancement in propulsion speed but for strong confinement this enhancement is lost and the swimming speed is slower than for an unconfined nematode. We use theory developed for bending elastic filaments in viscoelastic fluids to show that while (weak) confinement leads to increases in swimming speed there is a, $De-$ dependent, $Wi$ (Weissenberg number) number transition from a linear stress response regime to a nonlinear (or exponential) stress response regime. The experimentally obtained velocity fields are used to calculate a Weissenberg number to show that the decrease in swimming speed with confinement is likely related to growth in elastic stresses around the swimmer.

physics.flu-dyn

Carrier-envelope phase effects in graphene

We numerically study the interaction of a terahertz pulse with monolayer graphene. We observe that the electron momentum density is affected by the carrier-envelope phase (CEP) of the single- to few-cycle terahertz laser pulse that induces the electron dynamics. In particular, we see strong asymmetric electron momentum distributions for non-zero values of the CEP. We explain the origin of the asymmetry within the adiabatic-impulse model by finding conditions to reach minimal adiabatic gap between the valence band and the conduction band. We discuss how these conditions and the interference pattern, emanating from successive non-adiabatic transitions at this minimal gap, affect the electron momentum density and how they are modified by the CEP. This opens the door to control fundamental time-dependent electron dynamics in the tunneling regime in Dirac materials. Also, this control suggests a way to measure the CEP of a terahertz laser pulse when it interacts with condensed matter systems.

cond-mat.mes-hall

Numerical computation of dynamical Schwinger-like pair production in graphene

The density of electron-hole pairs produced in a graphene sample immersed in a homogeneous time-dependent electrical field is evaluated. Because low energy charge carriers in graphene are described by relativistic quantum mechanics, the calculation is performed within the strong field quantum electrodynamics formalism, requiring a solution of the Dirac equation in momentum space. The latter is solved using a split-operator numerical scheme on parallel computers, allowing for the investigation of several field configurations. The strength of the method is illustrated by computing the electron momentum density generated from a realistic laser pulse model. We observe quantum interference patterns reminiscent of Landau-Zener-Stückelberg interferometry.

cond-mat.mes-hall

Time-domain quantum interference in graphene

The electron momentum density obtained from the Schwinger-like mechanism is evaluated for a graphene sample immersed in a homogeneous time-dependent electric field. Based on the analogy between graphene low-energy electrons and quantum electrodynamics (QED), numerical techniques borrowed from strong field QED are employed and compared to approximate analytical approaches. It is demonstrated that for some range of experimentally accessible parameters, the pair production proceeds by sequences of adiabatic evolutions followed by non-adiabatic Landau-Zener transitions, reminiscent of the Kibble-Zurek mechanism describing topological defect density in second order phase transitions. For some field configurations, this yields interference patterns in momentum space which are explained in terms of the adiabatic-impulse model and the Landau-Zener-Stückelberg interferometry.

cond-mat.mes-hall