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A team of researchers in the U.S. and Japan led by MSD physicist Alessandra
Lanzara has produced the first direct evidence of “a significant
and unconventional” role in high temperature superconductivity for
phonons, the vibrations of the atoms that form the superconductor’s
crystalline lattice.
Superconductivity
is a state in which a material loses all electrical resistance. Once established,
an electrical current will flow forever. Many metals superconduct, but
only at temperatures very close to absolute zero. The physics behind this
low-temperature superconductivity has been successfully explained by BCS
theory, named for its Nobel-prize winning authors, John Bardeen, Leon
Cooper, and Robert Schrieffer. According to BCS theory, superconductivity
arises when electrons, which naturally repel one another because of their
mutual negative charge, come together to form “Cooper pairs.”
Cooper pairing cancels out any disruption in the flow of an electrical
current caused by crystal impurities, a source of electrical resistance.
Electrons are able to pair up because one of them interacts with a phonon,
creating what can be thought of as an atomic sound wave. The second electron
is affected by this alteration, as a ship passing through another’s
wake.
High temperature superconductivity,
which was discovered in the 1980s in doped copper oxides, or cuprates,
has been thought to be fundamentally different; the prevailing scientific
thought has been that electron-phonon coupling plays little or no role
in superconductivity in these materials. The Lanzara group took a critical
look at this hypotheses by performing a unique experiment on the ALS undulator
beamline 10.0.1, using a technique called angle-resolved photoemission
spectroscopy (ARPES). In ARPES, monochromatic x-ray light is flashed on
a sample, causing electrons to be emitted through the photoelectric effect.
Subsequent measurement of the kinetic energy of the emitted electrons
and the angles at which they are ejected enables the determination of
the binding energy of the material’s electrons as a function of
their momentum. Simultaneous measurement of energy and momentum, known
as an electron’s dispersion relation, yields valuable information
about electron interactions within the sample.
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For their
experiments, Lanzara and her colleagues replaced some of the normal oxygen-16
in Bi-2212, a cuprate doped with bismuth, strontium and calcium that becomes
superconducting at 92 K , with a heavier isotope, oxygen-18, and then
compared ARPES measurements. Beamline 10.0.1 provides a high enough degree
of angular and energy resolution that they could determine the small differences
in electron dynamics resulting from a crystal lattice made heavier and
stiffer by the oxygen-18 substitution. In a comprehensive study, the group
measured the dispersion relations for electrons that contributed to superconductivity
and also for those that did not. They found that for certain electrons
involved in superconductivity, the dispersion curves for the oxygen-18
substituted materials were different – clear evidence of the involvement
of phonons in the superconducting mechanism (if phonons were not involved,
changes in the masses of the atoms in the atomic lattice would have had
no effect).
The group
further deduced that in high-temperature superconductors like Bi-2212,
phonons stabilize the Cooper pairing of electrons in a process triggered
by “antiferromagnetism.” The antiferromagnetism arises when
the magnetic spins of electrons in the lattice align themselves with neighboring
spins pointing in opposite directions. In a qualitatively new explanation
for explaining high temperature superconductivity, they propose that the
formation of the Cooper pair is mediated through the phonons, while at
the same time, there is a feedback from the anti-ferromagnetic interaction.
Thus the two phenomena enhance one another.
A.
Lanzara (510)642-4863, Materials Sciences Division (510 486-4755), Berkeley
Lab.
G.-H.
Gweon, T. Sasagawa, .Y. Zhou, J. Graf, H. Takagi, D.-H. Lee& A. Lanzara,
“An unusual isotope effect in a high-transition-temperature superconductor,”
Nature 430, 187 (2004).
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