J. M. Parpia

Chiral Superfluid Helium-3 in the Quasi-Two-Dimensional Limit

Supercooling of the A phase of ³He.

Observation of suppressed viscosity in the normal state of ³He due to superfluid fluctuations.

Observation of suppressed viscosity in the normal state of 3He due to superfluid fluctuations

Conversion Between $$^3$$He Melting Curve Scales Below 100 mK

Supercooling of the A phase of 3He}

Fragility of surface states in topological superfluid ³He.

Path-Dependent Supercooling of the <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mmultiscripts><mml:mrow><mml:mi>He</mml:mi></mml:mrow><mml:mprescripts/><mml:none/><mml:mrow><mml:mn>3</mml:mn></mml:mrow></mml:mmultiscripts></mml:mrow></mml:math> Superfluid <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mstyle mathvariant="italic"><mml:mrow><mml:mi>A</mml:mi></mml:mrow></mml:mstyle><mml:mo>−</mml:mo><mml:mstyl

Anomalous Inferred Viscosity and Normal Density Near the $$^3$$He $$T_{\mathrm{c}}$$ in a Torsion Pendulum

Thermal transport of helium-3 in a strongly confining channel.

Tunable phonon-cavity coupling in graphene membranes

Control of the Graphene–Protein Interface Is Required To Preserve Adsorbed Protein Function

Phase Diagram of the Topological Superfluid ³ He Confined in a Nanoscale Slab Geometry

Photothermal Self-Oscillation and Laser Cooling of Graphene Optomechanical Systems