552 research outputs found
Effect of the particle-hole channel on BCS--Bose-Einstein condensation crossover in atomic Fermi gases
BCS--Bose-Einstein condensation (BEC) crossover is effected by increasing
pairing strength between fermions from weak to strong in the particle-particle
channel. Here we study the effect of the particle-hole channel on the zero
gap , superfluid transition temperature and the
pseudogap at , as well as the mean-field ratio
, from BCS through BEC regimes, in the
framework of a pairing fluctuation theory which includes self-consistently the
contributions of finite-momentum pairs. These pairs necessarily lead to a
pseudogap in single particle excitation spectrum above and below
. We sum over the infinite particle-hole ladder diagrams so that
the particle-particle and particle-hole -matrices are entangled with each
other. We find that the particle-hole susceptibility has a complex dynamical
structure, with strong momentum and frequency dependencies, and is sensitive to
temperature, gap size and interaction strength. We conclude that neglecting the
self-energy feedback causes a serious over-estimate of the particle-hole
susceptibility. In the BCS limit, the particle-hole channel effect may be
approximated by the same reduction in the overall pairing strength so that the
ratio is unaffected, in agreement with Gor'kov
\textit{et al.} to the leading order. However, the effect becomes more complex
and pronounced in the crossover regime, where the particle-hole susceptibility
is reduced by both a smaller Fermi surface and a big (pseudo)gap. Deep in the
BEC regime, the particle-hole channel contributions drop to zero. We propose
that precision measurements of the magnetic field for Feshbach resonance at low
temperatures as a function of density can be used to quantify the particle-hole
susceptibility and test different theories.Comment: Substantial rewriting of the theory section and the discussion of
Tc/E_F at unitarit
Investigation of Diamond Nucleation under Very Low Pressure in Chemical Vapor Deposition
Diamond nucleation under very low pressure (0.1-1.0 torr) was obtained at
very high nucleation densities and very rapid rates using hot-filament chemical
vapor deposition (HFCVD). The density on mirror-polished silicon was as high as
10^10 - 10^11 cm^{-2}, equivalent to the highest density in a microwave-plasma
CVD system. That on scratched silicon substrates was up to 10^9 cm^{-2}, 1-2
orders of magnitude higher than that obtained under conventionally low pressure
(tens of torr, 10^7 - 10^8 cm^{-2}). Also, the density on scratched titanium
substrates was as high as 10^10 cm^{-2}. The samples were characterized using
scanning electron microscopy (SEM) and Raman spectroscopy. The mechanism is
investigated in detail, revealing that, under very low pressure, very long mean
free path of the gas species, strong electron emission from the hot filament,
and high efficiency of decomposition of hydrocarbon species by the filament
greatly increase the concentration of reactive hydrocarbon radicals and atomic
hydrogen on the substrate surface, and therefore, dramatically enhance the
nucleation eventually. This work has great practical applications and
theoretical significance.Comment: 8 pages, 8 figures in JPEG compressed form, containing 10 photos,
REVTeX, in publication forma
Population of closed-channel molecules in trapped Fermi gases with broad Feshbach resonances
We compute the fraction of closed-channel molecules in trapped atomic Fermi
gases, over the entire range of accessible fields and temperatures. We use a
two-channel model of BCS--Bose-Einstein condensation (BEC) crossover theory at
general temperature , and show that this fraction provides a measure of the
dependent pairing gap. Our calculations, containing no free parameters, are
in good quantitative agreement with recent low measurements in Li. We
present readily testable predictions for the dependencies of the closed-channel
fraction on temperature and Fermi momentum.Comment: 4 pages, 3 figures, published in PR
Pseudogap phenomena in ultracold atomic Fermi gases
The pairing and superfluid phenomena in a two-component ultracold atomic
Fermi gas is an analogue of Cooper pairing and superconductivity in an electron
system, in particular, the high superconductors. Owing to the various
tunable parameters that have been made accessible experimentally in recent
years, atomic Fermi gases can be explored as a prototype or quantum simulator
of superconductors. It is hoped that, utilizing such an analogy, the study of
atomic Fermi gases may shed light to the mysteries of high
superconductivity. One obstacle to the ultimate understanding of high
superconductivity, from day one of its discovery, is the anomalous yet
widespread pseudogap phenomena, for which a consensus is yet to be reached
within the physics community, after over 27 years of intensive research
efforts. In this article, we shall review the progress in the study of
pseudogap phenomena in atomic Fermi gases in terms of both theoretical
understanding and experimental observations. We show that there is strong,
unambiguous evidence for the existence of a pseudogap in strongly interacting
Fermi gases. In this context, we shall present a pairing fluctuation theory of
the pseudogap physics and show that it is indeed a strong candidate theory for
high superconductivity.Comment: Invited review article, 32 Figures, 29 page
Finite Temperature Effects in Ultracold Fermi Gases
This article is written as a Lecture given in the 2006 Varenna Summer School
on "Ultracold Fermi Gases". Here we present a review of BCS--Bose Einstein
condensation (BEC) crossover theory with emphasis on finite temperature
effects. We discuss the role of temperature as it enters a theoretical
formalism which is based on the standard BCS-Leggett ground state. We also
discuss the role of temperature in the context of experiments ranging from
thermometric issues to signatures of superfluidity. Particularly important to
this discussion is the novel normal state associated with the crossover regime,
intermediate between BCS and BEC. The experimental evidence for this unusual
normal state (associated with pre-formed pairs) and its counterpart below
(associated with non-condensed pairs) is presented in the context of different
experiments. We end with a discussion of finite temperature effects in spin
polarized superfluids, where is found to play a crucial role in both theory
and experiment.Comment: Lecture given at the International School of Physics "Enrico Fermi"
-- the 2006 Varenna Summer School on "Ultracold Fermi Gases", 27 pages, 17
figure
Mechanism of Diamond Nucleation on Titanium Substrate under Very Low Pressure
Nucleation and its mechanism of diamond on titanium substrates under very low
pressure was studied using hot-filament chemical vapor deposition. Very high
nucleation rates and densities (10^8-10^{10} cm^{-2}) were obtained under 1
torr, which were 1-3 orders of magnitude higher than the counterpart (10^7
cm^{-2}) under conventionally low pressure (tens of torr). The effects of
substrate temperature and methane concentration under very low pressure were
also investigated, revealing that, overly high substrate temperature leads to a
relatively low nucleation density, and that higher CH_4 concentration gives
rise to a higher density and a higher rate. The nucleation mechanism is
discussed in detail. While a large amount of atomic hydrogen creates nucleating
sites, sufficient supersaturation of carbon and/or hydrocarbon species on/near
the substrate surface is the key factor for nucleation, in competition against
the rapid formation of carbide. Very low pressure leads to long mean free path
and other benefiting effects, and hence, is critical for rapid, high-density
nucleation. Effects of substrate temperature and CH_4 concentration are also
important. This further implies that C_2H_x (x<6) and CH_4 also contribute to
nucleation, but CH_{1-3} dominates under very low pressure. The
very-low-pressure method seems to be the only candidate to make diamond
deposition on titanium films applicable. It also sheds light on how to increase
the diamond growth rate.Comment: 8 pages (REVTeX) plus 4 (PostScript) figures with 14 photos,
Ghostscript 4.02 or higher may be needed to view the PS files. But they print
OK; Resubmit to fix the HTML tags in the abstract fiel
What can ultracold Fermi gases teach us about high superconductors and vice versa?
We review recent developments in the field of ultracold atomic Fermi gases.
As the cold atom system evolves from BCS to Bose-Einstein condensation (BEC),
the behavior of the thermodynamics, and the particle density profiles evolves
smoothly in a way which can be well understood theoretically. In the
interesting "unitary" regime, we show that these and other data necessarily
requires the introduction of a pseudogap in the fermionic spectrum which
exhibits many striking similarities to its counterpart in underdoped high
superconductors. We emphasize these similarities, giving an overview of the
experimental tools and key issues of common interest in both systems.Comment: 4 pages, 6 figures, to appear in a special issue of Physica C for the
M2S-HTSC VIII Conference Proceeding
Particle Density Distributions in Fermi Gas Superfluids: Molecular Boson Effects
We show how to describe the behavior associated with the usual
BCS- Bose Einstein condensation (BEC) crossover ground state. We confine our
attention here to the BEC and near-BEC regime where analytical calculations are
possible. At finite , non-condensed fermion pairs must be included, although
they have been generally ignored in the literature. Within this BEC regime we
compute the equations of state for the one and two channel models; these two
cases correspond to whether Feshbach resonance effects are omitted or included.
Differences between these two cases can be traced to differences between the
nature of a Cooper pair and bosonic condensate. Our results are also compared
with the Gross Pitaevskii equations of state for true bosons. Differences found
here are associated with the underlying fermionic character of the system.
Finally, the particle density distribution functions for a trap containing
superfluid fermionic atoms are computed using a Thomas-Fermi approach. The one
and two channel behavior is found to be very different; we find a narrowing of
the density profile as a result of Feshbach resonance effects. Importantly, we
infer that the ratio between bosonic and fermionic scattering lengths depends
on the magnetic detuning and is generally smaller than 2. Future experiments
will be required to determine to what extent this ratio varies with magnetic
fields.Comment: 8 pages, 2 figure, Revtex 4, submitted to PRA; manuscript expanded,
figure adde
Reentrant Superfluidity and Pair Density Wave in Single Component Dipolar Fermi Gases
We study the superfluidity of single component dipolar Fermi gases in three
dimensions within a pairing fluctuation theory. The transition temperature
for the dominant wave superfluidity exhibits a remarkable
re-entrant behavior as a function of the pairing strength induced by the
dipole-dipole interaction (DDI), which leads to an anisotropic pair dispersion.
The anisotropy and the long range nature of the DDI cause to vanish for a
narrow range of intermediate interaction strengths, where a pair density wave
state emerges as the ground state. The superfluid density and thermodynamics
below , along with the density profiles in a harmonic trap, are
investigated as well, throughout the BCS-BEC crossover. Implications for
experiments are discussed.Comment: 6 pages, 6 color figures; replaced with the final published versio
Applying BCS-BEC Crossover Theory To High Temperature Superconductors and Ultracold Atomic Fermi Gases
This review is written at the time of the twentieth anniversary of the
discovery of high temperature superconductors, which, nearly coincides with the
important discovery of the superfluid phases of ultracold trapped fermionic
atoms. We show how these two subjects have much in common. Both have been
addressed from the perspective of the BCS-Bose Einstein condensation (BEC)
crossover scenario, which is designed to treat short coherence length
superfluids with transition temperatures which are "high", with respect to the
Fermi energy. A generalized mean field treatment of BCS-BEC crossover at
general temperatures , based on the BCS-Leggett ground state, has met with
remarkable success in the fermionic atomic systems. Here we summarize this
success in the context of four different cold atom experiments, all of which
provide indications, direct or indirect, for the existence of a pseudogap. This
scenario also provides a physical picture of the pseudogap phase in the
underdoped cuprates which is a central focus of high research. We
summarize successful applications of BCS-BEC crossover to key experiments in
high systems including the phase diagram, specific heat, and vortex core
STM data, along with the Nernst effect, and exciting recent data on the
superfluid density in very underdoped samples,Comment: Review article for the 20th anniversary of high Tc superconductivity,
20 pages, 25 figures, to appear in J Low Temp Phy
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