The final public oral examination of Yayu Wang
will take place on
Friday, June 18, 2004 at 10:30 a.m. in Room 202. The examining
committee will consist of Professors N. P. Ong, P. Anderson, D.
Huse, M. Z. Hasan and C. Nappi. Any other members of the
University wishing to attend the examination may do so.
The thesis of Yayu Wang, entitled
"Nernst effect in high temperature superconductors", has been placed on deposit.
Any member of the University wishing to read the thesis may do
so. Any objections should be submitted to me in writing.
The
principal advisor for this work was N.P. Ong.
ABSTRACT
This thesis presents a study of the Nernst effect in high
temperature
superconductors. The vortex Nernst measurements have been carried
out on a
variety of high Tc cuprates to very high magnetic fields. These
results provide vital information about the properties and
relations of
the pseudogap phase and superconducting phase in high
Tc
superconductors.
Our first result is the existence of vortex-like excitations at
temperatures much higher than Tc0, the zero filed transition
temperature, in the cuprates. This anomalous behavior is most
dramatic in
the underdoped regime (0.10 < x < 0.12) where vortex-like signal
persists
to more than 100 K above Tc0. This finding suggests that in
the
putative normal state of cuprates, although bulk Meissner effect
is absent
and resistivity looks normal, the amplitude of the Cooper pairing
is still
sizable. The transition at Tc0 is driven by the loss of long
range phase coherence rather than the disappearance of
superconducting
condensate.
The high field Nernst effect offers a reliable way to determine
the upper
critical field Hc2 of high Tc cuprates and many unusual
properties
are uncovered. For cuprates with relatively large hole density (x> 0.15),
we found that Hc2 is almost temperature independent
for T < Tc0.
This is in strong contrast to the Hc2-T relation of
conventional
superconductors. Moreover, using a scaling analysis, we have
demonstrated
that Hc2 increases with decreasing hole density x in this
doping
range, implying a stronger pairing potential at lower doping.
Both of
these findings are in excellent agreement with the gap amplitude \Delta
measured by ARPES and STM.
In the severely underdoped regime (x < 0.12), some new features
become
apparent and they imply that the vortex Nernst signal is
comprised of two
distinct contributions. The first is from coherent regions with
long range
phase coherence and relatively low upper critical field, more
like the
superconducting phase; the second is from phase incoherent
regions with
much larger field scales, indicative of the pseudogap phase.
Analysis of
our data shows that with rising temperature, the superconducting
phase
gives weight to the pseudogap phase. The conversion between these
two
phases strongly suggests that they are closely related to each
other
rather than being competing orders. Moreover, the upper critical
field
Hc2 of the superconducting phase scales with the onset
temperature
T^{\nu}_{onset} of the vortx-like excitations.
Daniel Marlow
Chair, Dept. of Physics