Temperature superconductor
Ramping turn-to-turn loss and magnetization loss of a No-Insulation (RE)Ba2Cu3Ox high temperature superconductor pancake coil
... This paper is to study ramping turn-to-turn loss and magnetization loss of a no-insulation (NI) high temperature superconductor (HTS) pancake coil wound with (RE)Ba2Cu3Ox (REBCO) conductors. For insulated ...
27
Construction and Operation of an Internal Coil Device, RT-1, with a High-Temperature Superconductor
... An internal coil device called Ring Trap-1 (RT-1) has been constructed to explore an innovative concept for a high-beta plasma based on a new relaxation theory. A high-temperature superconductor (HTS) ...
8
Uniaxial pressure control of competing orders in a high temperature superconductor
... Abstract: Cuprates exhibit antiferromagnetic, charge-density-wave (CDW), and high-temperature superconducting ground states that can be tuned by doping and external magnetic fields. However, disorder generated by ...
17
Theory and Applications of High Temperature Superconductor
... Cuprates and iron based superconductors are similar in occurrence of unusual normal state properties which are outside the framework of Fermi liquid theory. The tetragonal- to- orthorhombic phase transition study in the ...
27
Diffraction studies of the structural phase transition in the high temperature superconductor YBCO
... According to a number of previous studies, at high temperature >400'C the T/01 phase transition in YBCO is second order and it has been shown by a sharp boundary between the tetragonal a[r] ...
210
A study of the high temperature superconductor YBa₂Cu₃O₇ 𝛿 and its cobalt doped derivative
... Abstract Static nuclear magnetic resonance NMR techniques have been used to study the magnetic hyperfine interactions of 63Cu and 89Y nuclei in the superconducting T=1.5K.. and normal T=[r] ...
322
Enhanced magnetic field sensing using planar high-temperature superconductor shields
... In Fig. 6 is plotted SF for the one-side planar shield as the function the distance between the shield and the Hall probe at 20 Hz and magnetic field of 21 mT for shields with 1 - 4 layers. The measured shielding factor ...
5
Charge trapping and super-Poissonian noise centers in a cuprate high-temperature superconductor
... high temperature superconductors in their normal state are very two-dimensional: while transport in the ab plane is perfectly metallic, it is insulating along the c-axis, with ratios between the two exceeding 10 4 ...
12
Platinum in High Temperature Superconductor Technology2-9
... Although there have been many reports of single crystal strontium titanate and magnesium oxide substrates being used, thin films of these materials on amorphous substrate[r] ...
8
A Simplified Approach to the Problems of Room Temperature Superconductivity
... An attempt to simplify the approach to the problems of room-temperature superconductors was done. The key factor has been highlighted—a giant spin-orbit interaction as a result of specific geo- metry of crystal. ...
7
Attenuation in a Cylindrical Left Handed Material (LHM) Wave Guide Structure
... with 0 ≤ x ≤ 0.65. R.D Black et al. [20]. It describes a high-temperature superconducting-receiver system for use in nuclear magnetic resonance (NMR) microscopy. The implementation of thin-film YBCO receiver coils ...
8
Superconductor Hybrids Electronic Paths to Quantum Computing
... Second, research has focussed on creating systems that mimic the behavior of the p -wave superconductor setup described above. This mimicking includes several possible suggestions of systems which all need to have ...
17
Complex spectral evolution in a BCS superconductor, ZrB12
... of Lifschitz transition. The spectral lineshape near the Fermi level in the high resolution spectra exhibit deviation from typical Fermi liquid behavior. A dip at the Fermi level emerges above the super- conducting ...
7
Superconductor derived from a topological insulator heterostructure
... to the lowest temperature of our SQUID magnetometer, 1.8 K. The result is shown in Fig. S4, where one can see that there is no visible Curie behavior in neither of the field directions. If the Schottky anomaly was ...
12
Quantum point contact as a probe of a topological superconductor
... nontrivial phase. In contrast, the plateaux are at the usual integer multiples in the topologically trivial phase. Disorder destroys all plateaux except the first, which remains precisely quantized, consistent with ...
11
Modified Atomic Theory Identifies Formation of Superconductor
... I propose Modified Atomic Structure, because nobody ascertains clear idea about the nucleus so far i.e. the distribution of protons and neutrons in the nucleus of an atom. If the protons are staying side by side, then a ...
7
Superconductor derived from a topological insulator heterostructure
... a superconductor synthesized by intercalating Cu into a naturally formed topological insulator (TI) heterostructure consisting of Bi 2 Se 3 TI units separated by ...
5
Upper critical field of the noncentrosymmetric superconductor BiPd
... noncentrosymmetric superconductor of which crystals may be grown and cleaved, enabling surface-sensitive ...s-wave superconductor, and we report its superconducting parameters as drawn from the bulk upper ...
7
SUPERCONDUCTING MATERIALS AND ITS APPLICATIONS
... Superconducting is a phenomenon of exactly zero electrical resistance and expulsion of magnetic flux fields occurring in certain materials called superconductors when cooled below a characteristic critical ...
6
Andreev-Bragg reflection from an Amperian superconductor
... Amperian superconductor [12], but since Andreev reflection is a local process we expect the predicted experimental signature of the 2k F pairing to be robust and ...
5