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Physical Review Letters

Blackbody source and detector of ballistic quasiparticles in B3 : Emission angle from a wire moving at supercritical velocity

S. N. Fisher, A. M. Guénault, C. J. Kennedy, G. R. Pickett

Published Aug 17, 1992• 128 citations
Publisher

Abstract

Using a new quasiparticle detector and source consisting of a blackbody radiator, we have made the first measurements of the divergence of a beam of quasiparticles produced by a vibrating-wire resonator moving at supercritical velocities in superfluid $^{3}\mathit{B}$ at the zero-temperature limit. At velocities just above the critical velocity of \ensuremath{\Delta}/3${\mathit{p}}_{\mathit{F}}$ we see a very narrow beam directed along the direction of motion of the wire. As the maximum wire velocity increases the beam spreads to saturate at a half-angle divergence of approximately 55\ifmmode^\circ\else\textdegree\fi{} at a maximum velocity of order \ensuremath{\Delta}/${\mathit{p}}_{\mathit{F}}$.

DOI
10.1103/physrevlett.69.1073

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Using a new quasiparticle detector and source consisting of a blackbody radiator, we have made the first measurements of the divergence of a beam of quasiparticles produced by a vibrating-wire resonator moving at supercritical velocities in superfluid 3B^{3}\mathit{B}3B at the zero-temperature limit. At velocities just above the critical velocity of \ensuremath{\Delta}/3pF{\mathit{p}}_{\mathit{F}}pF​ we see a very narrow beam directed along the direction of motion of the wire. As the maximum wire velocity increases the beam spreads to saturate at a half-angle divergence of approximately 55\ifmmode^\circ\else\textdegree\fi{} at a maximum velocity of order \ensuremath{\Delta}/pF{\mathit{p}}_{\mathit{F}}pF​.
This thesis details experiments in the ballistic regime of superfluid 3He-B at temperatures around 100 ➭K. In this thesis, the quasiparticle beam profile from a Black-Body radiator and a vibrating wire resonator is measured using a quasiparticle camera which consists of 25 tuning forks. The vibrating wire resonator is found to have a very thinly spread beam at velocities slightly higher than the pair-breaking critical velocity which spreads out at higher velocities. At 21 mm/s the vibrating resonator is found to have a more focused beam than the Black-Body radiator where both beam profiles are found to be focused around the centre of the quasiparticle camera. A theoretical model is created in order to model the spread and intensity of the experimental beam profile from the Black-Body radiator. In this thesis, the response of some of the probes to thermal damping is measured in the form of the geometrical constants γ and λ. The geometrical constant λ is related to the velocity dependence of the probe to thermal damping and is found for two wires of varying diameter, a tuning fork and its overtone mode in which all the values of λ were close to unity. The geometrical constant γ is related to the sensitivity of a probe to thermal damping. This is found for a Black-Body radiator and then used to derive the sensitivity for other wires in the cell in thermal equilibrium with it. Two resonant modes of a small tuning fork are used to do a Black-Body radiator calibration on the area around the tuning fork which is used to find the sensitivity of 25 tuning forks (pixels) in the quasiparticle camera.
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We have observed that the motion of a vibrating-wire resonator in superfluid 3B^{3}\mathit{B}3B at temperatures below Tc{\mathrm{T}}_{\mathrm{c}}Tc​/8 is associated with a sharp critical velocity, vc{\mathrm{v}}_{\mathrm{c}}vc​, above which very high dissipation sets in. We identify this velocity with the Landau critical velocity for pair breaking. That the observed value of vc{\mathrm{v}}_{\mathrm{c}}vc​ is a factor of 2 lower than the critical velocity expected from the BCS value of the gap we take as evidence that the gap is suppressed by about 50% of its bulk value near a moving boundary.
The resistance to motion of a wire in superfluid 3B^{3}\mathit{B}3B has three contributions: that due to the internal friction of the resonator; that due to pair breaking; and that due to the quasiparticle gas. We have been able to separate quasiparticle contribution and find that it is highly nonlinear with velocity on the scale of the Landau velocity, \ensuremath{\Delta}/pF{\mathrm{p}}_{\mathrm{F}}pF​, and falls with increasing velocity. This indicates that the quasiparticle resistance is also governed by the condensate, almost certainly through Andreev reflection in the flow field around the wire.
We report the first observation of quantized circulation in superfluid 3B^{3}\mathit{B}3B. The apparatus consists of a straight vibrating wire immersed in liquid 3He^{3}\mathrm{He}3He, which is cooled by a rotating nuclear demagnetization cryostat. The experiment is carried out at about 250 \ensuremath{\mu}K. The superfluid at this temperature is in the ballistic quasiparticle regime. Circulation around the wire is found to be stable only when it takes on the values -h/2m3{\mathit{m}}_{3}m3​, 0, and +h/2m3{\mathit{m}}_{3}m3​, where h is Planck's constant and m3{\mathit{m}}_{3}m3​ is the mass of the 3He^{3}\mathrm{He}3He atom. This experiment confirms that superfluid 3B^{3}\mathit{B}3B is a Cooper-paired superfluid with a macroscopic quantum wave function.
We have observed the distortion of the gap and associated excitation spectrum in superfluid 3B^{3}\mathit{B}3B with increasing magnetic field up to the first-order transition to the A phase at a temperature of Tc{\mathit{T}}_{\mathit{c}}Tc​/T of about 7 (\ensuremath{\le}140 \ensuremath{\mu}K at P=0). The pair-breaking critical velocity of a vibrating-wire resonator is monitored as a function of field. By plotting the critical velocity we can follow changes in the B-phase excitation spectrum with increasing magnetic field, which are in excellent agreement with the calculations of Ashida and Nagai. The sudden transition to the A phase at the critical field is clearly seen.