Table of Contents Table of Contents
Previous Page  45 / 168 Next Page
Information
Show Menu
Previous Page 45 / 168 Next Page
Page Background

Abstracts

I2.1

Non-isothermal Physico-Chemical Processes in Superfluid Helium

Haley R. P.

Lancaster University

Coherent condensates appear as emergent phenomena in many systems, sharing

the characteristic feature of an energy gap separating the lowest excitations from

the condensate ground state. An object moving with high enough velocity that

the excitation spectrum becomes gapless can create excitations at no energy

cost and initiate the breakdown of the condensate. This limit is the well-known

Landau velocity. For the neutral Fermionic superfluid

3

He-B in the T=0 limit,

flow around an oscillating body displays a very clear critical velocity for the

onset of dissipation. However, to our considerable surprise, we have found that

for uniform linear motion there is no discontinuity whatsoever in the dissipation

as the Landau critical velocity is passed and exceeded.

I2.2

Visualizing Textural Domain Walls in Superfluid

3

He by Magnetic

Resonance Imaging

Kasai Jun(1), Okamoto Yohei(1), Nishioka Keishi(1),Takagi Takeo(2), and Sasaki

Yutaka(1,3)

1) Dept. of Physics, Kyoto University, Kyoto, JAPAN.

2) Dept. of Applied Physics, Univ. of Fukui, Fukui, JAPAN.

3) LTM Center, Kyoto University, Kyoto, JAPAN.

A real space image of textural domain walls inside a single 100 micrometer

thickness slab of superfluid

3

He-A was MRI-imaged. Straight lines, which

appeared in between large domains of uniform textures, were textural domain

walls (solitons) with particularly important feature. The observed NMR properties

suggest that the domain wall has almost dipole-locked soliton structure inside

the wall, which connects two regions of uniform

d

=

l

texture with different

chirality, namely

d

,

l

and –

d

,

l

. This soliton is accompanied with two surface

chiral domain walls located back to back on both side of the slab surface. The

surface chiral domain walls anchor the dipole-locked soliton in its place.

45