Francis M. Gasparini
Professor of Physics
- Office : 132 Fronczak Hall ; Labs : 137 & 139 Fronczak Hall.
- Phone : (716)645-2005
- Fax : (716)645-2507
- email : fmg@acsu.buffalo.edu
- See also: Low Temperature Physics Group Home Page
- Ph.D (Minnesota, 1970)
- Experimental Low Temperature Physics
QUANTUM FLUIDS AND PHASE TRANSITIONS
Experiments in our laboratory center on the behavior of the quantum liquids,
He4 and He3, at low temperatures. The quantum refers to the
fact that the zero point motion plays a crucial role in the phase behavior of
these liquids. This is responsible for the fact that the liquid phase
persists to absolute zero. The experiments which we have done most
recently all involve the behavior of these systems in a lower dimension.
That is, in a situation where the helium is constrained in some way so
that, for instance, it behaves as a two-dimensional thermodynamic system
rather than three dimensional. This is the case for films consisting of
one or two atomic layers.
Liquid He4 undergoes a phase transition into a superfluid state at
2.18K. This is analogous in many ways to the superconducting transition
in the case of electrons. This transition in He4 is of considerable
interest from the point of view of critical phenomena. The transition has
been studied most extensively in order to verify theoretical predictions of
critical behavior. An important aspect of this, which is still ongoing,
is the behavior at the transition when the helium is not in the
thermodynamic limit. That is, when a spatial dimension is imposed which
limits the critical fluctuations which are responsible for the
thermodynamic singularities.
We have recently developed a technique whereby we are able to space two
silicon wafers at a uniform separation which can be as small as 1000
Angstroms over the full area of the wafers. This involves lithography and
a bonding process in a microclean chamber. The bonded wafers allow us to
confine the helium in a geometry which leads to a behavior which changes
from 3-dimensional to 2-dimensional as the transition is approached. We
have measured the superfluid fraction in this geometry by using a torsional
oscillator technique and, we are currently measuring the heat capacity using
an AC technique. Future work will involve geometries where, near the
transition, the behavior will change to 1-dimension and 0-dimension.
Another area in which we are currently interested is the helium-fullerite
system. One issue involved here is the possibility of intercalating helium
atoms inside a crystal made of fullerene molecules. These molecules are
spheroids made of carbon atoms. The most popular is C60, this has 60
carbon atoms arranged in a molecule which resembles a soccer ball. Another
issue of interest, apart from intercalation, is the nature of the monolayer
which adsorbs on crystals of these molecules. The interaction potential for
helium and the C60 crystal has been calculated recently. It appears that
some interesting new phases of helium could exist in the near-monolayer
adsorption region.
References
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"Heat capacity of mixtures of 3He-4He confined to coupled 1um boxes."
Mark O. Kimball and F. M. Gasparini
Sumitted to the editors of the LT23 conference in Hiroshima, Japan.
PDF of paper (148k)
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"Surprising behavior of the superfluid fraction for 4He and
3He-4He mixtures in 18.5 nm channels."
Mark O. Kimball, Manuel Diaz-Avila, and F. M. Gasparini
Sumitted to the editors of the LT23 conference in Hiroshima, Japan.
PDF of paper (133k)
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"4He confined to 1um3 boxes, 0D crossover, surface and edge effects."
Mark O. Kimball, Manuel Diaz-Avila, and F. M. Gasparini
Sumitted to the editors of the LT23 conference in Hiroshima, Japan.
PDF of paper (127k)
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"Critical Behavior and Scaling of Confined 3He-4He Mixtures"
Mark O. Kimball and F. M. Gasparini
J. Low Temp. Phys. 126, Nos. 1/2, 103-108 (2002)
PDF of paper (359k)
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"Van der Waals effects at the superfluid transition of confined 4He"
K. P. Mooney and F. M. Gasparini
J. Low Temp. Phys. 126, Nos. 1/2, 247-253 (2002)
PDF of paper (141k)
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"The Superfluid Transition of 4He, a Test Case for Finite-Size Scaling at a Second Order Phase Transition"
F. M. Gasparini, M. O. Kimball, and K. P. Mooney
J. Phys. Condens. Matter 13, 4871 (2001)
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"Superfluid Fraction of 3He - 4He Mixtures Confined at 0.0483 um between Silicon Wafers"
M. O. Kimball and F. M. Gasparini
Phys. Rev. Lett. 86, 1558 (2001)
PDF of paper (291k)
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"Specific Heat Near the Superfluid Transition of a 0.9869 micron
4He Film."
M. O. Kimball, S. Mehta, and F. M. Gasparini
J. Low Temp. Phys. Vol 121, Nos. 1/2, 29 (2000).
PDF of paper (2607k)
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"Specific Heat of 4He Confined to 9869A Planar Geometry."
M. O. Kimball and F. M. Gasparini
Physica B (2000) 284-288 47-48
PDF of paper (123k)
PS of paper (407k)
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"Superfluid Density of Confined 3He-4He Using
Adiabatic Fountain Resonance"
F. M. Gasparini and M. O. Kimball
Physica B 284-288 (2000) 317-318
PDF of paper (189k)
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"Superfluid Transition of 4He for Two-Dimensional Crossover, Heat Capacity, and Finite Size Scaling"
S. Mehta, M. O. Kimball and F. M. Gasparini
J. Low Temp. Phys. Vol. 114, Nos. 5/6, 467 (1999).
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"4He Confined in 0.0483 um Planar Geometry, Specific Heat and Scaling Near Tlambda"
S. Mehta, M. O. Kimball and F. M. Gasparini
J. Low Temp. Phys. Vol. 113, Nos. 3/4, 435 (1998).
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"Specific Heat and Scaling of 4He Confined in a Planar
Geometry"
S. Mehta and F. M. Gasparini
Phys. Rev. Lett. Vol. 78, Nos. 13, 2596 (1997).
PDF of paper (179k)