19 research outputs found
Evidence for room temperature superconductivity at graphite interfaces
In the last 43 years several hints were reported suggesting the existence of
granular superconductivity above room temperature in different graphite-based
systems. In this paper some of the results are reviewed, giving special
attention to those obtained in water and n-heptane treated graphite powders,
commercial and natural bulk graphite samples with different characteristics as
well as transmission electron microscope (TEM) lamellae. The overall results
indicate that superconducting regions exist and are localized at certain
internal interfaces of the graphite structure. The existence of the
rhombohedral graphite phase in all samples with superconducting-like properties
suggests its interfaces with the Bernal phase as a possible origin for the
high-temperature superconductivity, as theoretical calculations predict. High
precision electrical resistance and magnetization measurements were used to
identify a transition at K. To check for the existence of
true zero resistance paths in the samples we used local magnetic measurements,
which results support the existence of superconducting regions at such high
temperatures.Comment: 10 pages, 9 figures, 2nd International Workshop "Towards Room
Temperature Superconductivity: Superhydrides and more", Orange California May
2017. To be published in "Quantum Studies: Mathematics and Foundations"
(Springer Nature
Identification of a possible superconducting transition above room temperature in natural graphite crystals
Measuring with high precision the electrical resistance of highly ordered
natural graphite samples from a Brazil mine, we have identified a transition at
350~K with 40~K transition width. The step-like change in
temperature of the resistance, its magnetic irreversibility and time dependence
after a field change, consistent with trapped flux and flux creep, and the
partial magnetic flux expulsion obtained by magnetization measurements, suggest
the existence of granular superconductivity below 350~K. The zero-field virgin
state can only be reached again after zero field cooling the sample from above
the transition. Paradoxically, the extraordinarily high transition temperature
we found for this and several other graphite samples is the reason why this
transition remained undetected so far. The existence of well ordered
rhombohedral graphite phase in all measured samples has been proved by x-rays
diffraction measurements, suggesting its interfaces with the Bernal phase as a
possible origin for the high-temperature superconductivity, as theoretical
studies predicted. The localization of granular superconductivity at these two
dimensional interfaces prevents the observation of a zero resistance state or
of a full Meissner state.Comment: 14 pages with 21 figure
Coupled magnetic and structural transitions in La0.7Sr0.3MnO3 films on SrTiO3
The magnetic properties of three epitaxial La0.7Sr0.3MnO3 films of
thickness 5, 15 and 40 nm grown on SrTiO3 (001) substrates were investigated.
The structural transition of the SrTiO3 substrate induces a magnetic transition
in the manganite films due to magnetoelastic coupling. Below the temperature
of the structural transition additional steps in the magnetization reversal
characteristics appear characterized by clearly defined coercive fields. These
additional coercive fields depend on the cooling history of the sample and
are related to the formation of structural domains in the La0.7Sr0.3MnO3 films
induced by the substrate
Recommended from our members
Weak electron irradiation suppresses the anomalous magnetization of N-doped diamond crystals
Several diamond bulk crystals with a concentration of electrically neutral single substitutional nitrogen atoms of ≲80 ppm, the so-called C or P1 centers, are irradiated with electrons at 10 MeV energy and low fluence. The results show a complete suppression of the irreversible behavior in field and temperature of the magnetization below 30 K, after a decrease in ≲40 ppm in the concentration of C centers produced by the electron irradiation. This result indicates that magnetic C centers are at the origin of the large hysteretic behavior found recently in nitrogen-doped diamond crystals. This is remarkable because of the relatively low density of C centers, stressing the extraordinary role of the C centers in triggering those phenomena in diamond at relatively high temperatures. After annealing the samples at high temperatures in vacuum, the hysteretic behavior is partially recovered
Coupled magnetic and structural transitions in La0.7Sr0.3MnO3 films on SrTiO3
The magnetic properties of three epitaxial La0.7Sr0.3MnO3 films of
thickness 5, 15 and 40 nm grown on SrTiO3 (001) substrates were investigated.
The structural transition of the SrTiO3 substrate induces a magnetic transition
in the manganite films due to magnetoelastic coupling. Below the temperature
of the structural transition additional steps in the magnetization reversal
characteristics appear characterized by clearly defined coercive fields. These
additional coercive fields depend on the cooling history of the sample and
are related to the formation of structural domains in the La0.7Sr0.3MnO3 films
induced by the substrate
Coupled magnetic and structural transitions in La0.7Sr0.3MnO3 films on SrTiO3
The magnetic properties of three epitaxial La0.7Sr0.3MnO3 films of
thickness 5, 15 and 40 nm grown on SrTiO3 (001) substrates were investigated.
The structural transition of the SrTiO3 substrate induces a magnetic transition
in the manganite films due to magnetoelastic coupling. Below the temperature
of the structural transition additional steps in the magnetization reversal
characteristics appear characterized by clearly defined coercive fields. These
additional coercive fields depend on the cooling history of the sample and
are related to the formation of structural domains in the La0.7Sr0.3MnO3 films
induced by the substrate
Existence of a magnetically ordered hole gas at the La
The study of spatially confined complex oxides is of wide interest, since correlated electrons at interfaces might form new states of matter. Here La0.7Sr0.3MnO3/SrRuO3 superlattices with coherently grown interfaces and layer thicknesses down to one unit cell were fabricated by pulsed laser deposition. The superlattices were studied by X-ray, HRTEM, magnetization and magnetotransport measurements. For such small thicknesses La0.7Sr0.3MnO3 films are antiferromagnetic and insulating. Despite the small layer thickness, the LaSrMnO layers in the superlattices were ferromagnetic with Curie temperatures close to room temperature. Whereas the resistivity of the superlattices showed metallic behaviour and was dominated by the conducting SrRuO3 layers, the off-diagonal resistivity showed an anomalous Hall effect with ferromagnetic loop shape even far above the Curie temperature of the SrRuO3 layers as well as a positive high field slope. This indicates the presence of a highly conducting, ferromagnetically ordered hole gas at the interfaces that might be formed by a charge-transfer process. This result opens up an alternative route for the fabrication of quasi-two-dimensional systems
Magnetic manipulation in Dy/Tb multilayer upon electron-irradiation
Manipulation and control of defects triggered by an electron beam allow us to conduct defect engineering on layered materials. We investigate topologically stable helices within a [Dy(10 nm)/Tb(10 nm)]30 multilayer subjected to MeV electron(e)-irradiation up to a maximum fluence of 9.58 × 1018 e/cm2. As electrons can go through the sample homogeneously and with high penetration depth, they produce defects without doping. Our e-irradiation results indicate defect induced magnetic manipulation, which increases the blocking/freezing temperature of spin-frustrated interfaces by 4%. This increase implies an increase in the spin-cluster volume. Consequently, the reduced uncompensated pinning centres decrease the interfacial exchange bias coupling by 45%. Direct manipulation of pinning centres would thereby allow us to tailor spintronic devices in a clean way.Fil: Paul, Amitesh. Technion - Israel Institute of Technology; IsraelFil: Esquinazi, Pablo D.. Division Of Quantum Magnetism And Superconductivity, Un; AlemaniaFil: Zandalazini, Carlos Ivan. Consejo Nacional de Investigaciones Científicas y Técnicas. Centro Científico Tecnológico Conicet - Córdoba. Instituto de Física Enrique Gaviola. Universidad Nacional de Córdoba. Instituto de Física Enrique Gaviola; Argentina. Universidad Nacional de Córdoba. Facultad de Matemática, Astronomía y Física; ArgentinaFil: Setzer, Annette. Division Of Quantum Magnetism And Superconductivity, Un; AlemaniaFil: Knolle, Wolfgang. No especifíca
