1,920 research outputs found
Signatures of quantum criticality in the thermopower of Ba(Fe(1-x)Co(x))2As2
We demonstrate that the thermopower (S) can be used to probe the spin
fluctuations (SFs) in proximity to the quantum critical point (QCP) in Fe-based
superconductors. The sensitivity of S to the entropy of charge carriers allows
us to observe an increase of S/T in Ba(Fe(1-x)Co(x))2As2 close to the
spin-density-wave (SDW) QCP. This behavior is due to the coupling of low-energy
conduction electrons to two-dimensional SFs, similar to heavy-fermion systems.
The low-temperature enhancement of S/T in the Co substitution range 0.02 < x <
0.1 is bordered by two Lifshitz transitions, and it corresponds to the
superconducting region, where a similarity between the electron and
non-reconstructed hole pockets exists. The maximal S/T is observed in proximity
to the commensurate-to-incommensurate SDW transition, for critical x_c ~ 0.05,
close to the highest superconducting T_c. This analysis indicates that low-T
thermopower is influenced by critical spin fluctuations which are important for
the superconducting mechanism
Research on applied bioelectrochemistry First quarterly progress report, 14 Mar. - 30 Jun. 1963
Optimum use of human waste as electrochemical fuels by urea bacterial organism conversion
Interplay between superconductivity and itinerant magnetism in underdoped BaKFeAs ( 0.2) probed by the response to controlled point-like disorder
The response of superconductors to controlled introduction of point-like
disorder is an important tool to probe their microscopic electronic collective
behavior. In the case of iron-based superconductors (IBS), magnetic
fluctuations presumably play an important role in inducing high temperature
superconductivity. In some cases, these two seemingly incompatible orders
coexist microscopically. Therefore, understanding how this unique coexistence
state is affected by disorder can provide important information about the
microscopic mechanisms involved. In one of the most studied pnictide family,
hole-doped BaKFeAs (BaK122), this coexistence occurs over a
wide range of doping levels, 0.16~~0.25. We used
relativistic 2.5 MeV electrons to induce vacancy-interstitial (Frenkel) pairs
that act as efficient point-like scattering centers. Upon increasing dose of
irradiation, the superconducting transition temperature decreases
dramatically. In the absence of nodes in the order parameter this provides a
strong support for a sign-changing pairing. Simultaneously, in the
normal state, there is a strong violation of the Matthiessen's rule and a
decrease (surprisingly, at the same rate as ) of the magnetic transition
temperature , which indicates the itinerant nature of the long-range
magnetic order. Comparison of the hole-doped BaK122 with electron-doped
Ba(FeCo)As (FeCo122) with similar 110~K,
0.02, reveals significant differences in the normal states, with no
apparent Matthiessen's rule violation above on the electron-doped
side. We interpret these results in terms of the distinct impact of impurity
scattering on the competing itinerant antiferromagnetic and
superconducting orders
Ferromagnetism or slow paramagnetic relaxation in Fe-doped LiN?
We report on isothermal magnetization, M\"ossbauer spectroscopy, and
magnetostriction as well as temperature-dependent alternating-current (ac)
susceptibility, specific heat, and thermal expansion of single crystalline and
polycrstalline Li(LiFe)N with and .
Magnetic hysteresis emerges at temperatures below K with
coercivity fields of up to T at K and magnetic
anisotropy energies of K (meV). The ac susceptibility is strongly
frequency dependent (--Hz) and reveals an effective energy
barrier for spin reversal of K. The relaxation times
follow Arrhenius behavior for K. For K, however, the
relaxation times of s are only weakly
temperature-dependent indicating the relevance of a quantum tunneling process
instead of thermal excitations. The magnetic entropy amounts to more than
J molK which significantly exceeds ln2, the
value expected for the entropy of a ground state doublet. Thermal expansion and
magnetostriction indicate a weak magneto-elastic coupling in accordance with
slow relaxation of the magnetization. The classification of
Li(LiFe)N as ferromagnet is stressed and contrasted with highly
anisotropic and slowly relaxing paramagnetic behavior.Comment: 12 pages, 10 figure
Anisotropy Reversal of the Upper Critical Field at Low Temperatures and Spin-Locked Superconductivity in K2Cr3As3
We report the first measurements of the anisotropic upper critical field
for KCrAs single crystals up to 60 T and K. Our results show that the upper critical field parallel to the Cr
chains, , exhibits a paramagnetically-limited behavior,
whereas the shape of the curve (perpendicular to the Cr
chains) has no evidence of paramagnetic effects. As a result, the curves
and cross at K, so that
the anisotropy parameter
increases from near to at 0.6 K. This behavior of is inconsistent with triplet
superconductivity but suggests a form of singlet superconductivity with the
electron spins locked onto the direction of Cr chains
Epilogue: Superconducting Materials Past, Present and Future
Experimental contributors to the field of Superconducting Materials share
their informal views on the subject.Comment: Epilogue to Physica C Special Issue on Superconducting Materials,
Volume 514 (2015
Systematic effects of carbon doping on the superconducting properties of Mg(BC)
The upper critical field, , of Mg(BC) has been
measured in order to probe the maximum magnetic field range for
superconductivity that can be attained by C doping. Carbon doped boron
filaments are prepared by CVD techniques, and then these fibers are then
exposed to Mg vapor to form the superconducting compound. The transition
temperatures are depressed about C and rises at about C. This means that 3.5% C will depress from to and
raise from to . Higher fields are probably
attainable in the region of 5% C to 7% C. These rises in are
accompanied by a rise in resistivity at from about
to about . Given that the samples are polycrystalline wire
segments, the experimentally determined curves represent the upper
manifold associated with
Remarkably robust and correlated coherence and antiferromagnetism in (CeLa)CuGe
We present magnetic susceptibility, resistivity, specific heat, and
thermoelectric power measurements on (CeLa)CuGe single
crystals (0 1). With La substitution, the antiferromagnetic
temperature is suppressed in an almost linear fashion and moves below
0.36 K, the base temperature of our measurements for 0.8. Surprisingly, in
addition to robust antiferromagnetism, the system also shows low temperature
coherent scattering below up to 0.9 of La, indicating a small
percolation limit 9 of Ce that separates a coherent regime from a
single-ion Kondo impurity regime. as a function of magnetic field was
found to have different behavior for 0.9. Remarkably,
at = 0 was found to be linearly proportional to . The
jump in the magnetic specific heat at as a function of
for (CeLa)CuGe follows the theoretical prediction
based on the molecular field calculation for the = 1/2 resonant level
model
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