25 research outputs found
Chemical potential oscillations from a single nodal pocket in the underdoped high-Tc superconductor YBa2Cu3O6+x
The mystery of the normal state in the underdoped cuprates has deepened with
the use of newer and complementary experimental probes. While photoemission
studies have revealed solely `Fermi arcs' centered on nodal points in the
Brillouin zone at which holes aggregate upon doping, more recent quantum
oscillation experiments have been interpreted in terms of an ambipolar Fermi
surface, that includes sections containing electron carriers located at the
antinodal region. To address the question of whether an ambipolar Fermi surface
truly exists, here we utilize measurements of the second harmonic quantum
oscillations, which reveal that the amplitude of these oscillations arises
mainly from oscillations in the chemical potential, providing crucial
information on the nature of the Fermi surface in underdoped YBa2Cu3O6+x. In
particular, the detailed relationship between the second harmonic amplitude and
the fundamental amplitude of the quantum oscillations leads us to the
conclusion that there exists only a single underlying quasi-two dimensional
Fermi surface pocket giving rise to the multiple frequency components observed
via the effects of warping, bilayer splitting and magnetic breakdown. A range
of studies suggest that the pocket is most likely associated with states near
the nodal region of the Brillouin zone of underdoped YBa2Cu3O6+x at high
magnetic fields.Comment: 7 pages, 4 figure
High-Field Superconductivity at an Electronic Topological Transition in URhGe
The emergence of superconductivity at high magnetic fields in URhGe is
regarded as a paradigm for new state formation approaching a quantum critical
point. Until now, a divergence of the quasiparticle mass at the metamagnetic
transition was considered essential for superconductivity to survive at
magnetic fields above 30 tesla. Here we report the observation of quantum
oscillations in URhGe revealing a tiny pocket of heavy quasiparticles that
shrinks continuously with increasing magnetic field, and finally disappears at
a topological Fermi surface transition close to or at the metamagnetic field.
The quasiparticle mass decreases and remains finite, implying that the Fermi
velocity vanishes due to the collapse of the Fermi wavevector. This offers a
novel explanation for the re-emergence of superconductivity at extreme magnetic
fields and makes URhGe the first proven example of a material where magnetic
field-tuning of the Fermi surface, rather than quantum criticality alone,
governs quantum phase formation.Comment: A revised version has been accepted for publication in Nature Physic
Magnetism and its microscopic origin in iron-based high-temperature superconductors
High-temperature superconductivity in the iron-based materials emerges from,
or sometimes coexists with, their metallic or insulating parent compound
states. This is surprising since these undoped states display dramatically
different antiferromagnetic (AF) spin arrangements and Nel
temperatures. Although there is general consensus that magnetic interactions
are important for superconductivity, much is still unknown concerning the
microscopic origin of the magnetic states. In this review, progress in this
area is summarized, focusing on recent experimental and theoretical results and
discussing their microscopic implications. It is concluded that the parent
compounds are in a state that is more complex than implied by a simple Fermi
surface nesting scenario, and a dual description including both itinerant and
localized degrees of freedom is needed to properly describe these fascinating
materials.Comment: 14 pages, 4 figures, Review article, accepted for publication in
Nature Physic