H10N60/85

PHONONIC MATERIAL AND METHOD FOR PRODUCING SAME
20230051884 · 2023-02-16 ·

[Problem] To provide a phononic material that exhibits a voltage-current characteristic to make current flow even when there is no potential gradient, and a method for producing the same. [Solution] A phononic material 1 has a periodic structure body 2′ in which structures 3 are periodically and regularly disposed in a constituent 2, and the periodic structure body 2′ exhibits a voltage-current characteristic to make current flow even when a potential gradient is 0 V. A method for producing the phononic material 1 has such an outline as to carry out a heat treatment to cool and warm the periodic structure body after applying a current with a magnitude to make an electrical resistance characteristic disappear to the periodic structure body 2′ having the electrical resistance characteristic that exhibits an electrical resistance value of 0Ω or less.

PHONONIC MATERIAL AND METHOD FOR PRODUCING SAME
20230044423 · 2023-02-09 ·

[Problem] To provide a phononic material that exhibits an electrical resistance characteristic less than or equal to 0Ω, a precursor of the same, and a method for producing these. [Solution] A phononic material 1 has a periodic structure body 2′ in which structures 3 are periodically and regularly disposed in a constituent 2. The periodic structure body 2′ exhibits an electrical resistance characteristic less than or equal to 0Ω, and has a temperature region that exhibits the electrical resistance characteristic in a temperature range exceeding a superconducting transition temperature when the constituent 2 has the superconducting transition temperature. A method for producing a precursor of the phononic material 1 includes a pretreatment process to obtain the precursor by carrying out a heat treatment to warm the periodic structure body after cooling the periodic structure body in a state of applying a unidirectional current to the periodic structure body 2′.

METHOD OF FABRICATING A HOLLOW WALL FOR CONTROLLING DIRECTIONAL DEPOSITION OF MATERIAL

A method of fabricating a hollow wall for controlling directional deposition of material comprises: forming a layer of resist on a substrate; removing a portion of the resist selectively to form a channel in the resist; forming a layer of an amorphous dielectric material in the channel; and removing the resist to form the hollow wall. The channel has a front surface configured to prevent bending of a corresponding front face of the hollow wall. The hollow wall is useful for controlling deposition of material when fabricating semiconductor-superconductor hybrid devices, for example. By configuring the channel appropriately, bending of the hollow wall can be prevented, allowing for more precise deposition of material. Also provided is a further method of fabricating a hollow wall; and a method of fabricating a device using the hollow walls.

Superconducting bilayers of two-dimensional materials with integrated Josephson junctions

Josephson junctions (JJ) based on bilayers of azimuthally misaligned two-dimensional materials having superconducting states are provided. Also provided are electronic devices and circuits incorporating the JJs as active components and methods of using the electronic devices and circuits. The JJs are formed from bilayers composed of azimuthally misaligned two-dimensional materials having a first superconducting segment and a second superconducting segment separated by a weak-link region that is integrated into the bilayer.

Superconducting bilayers of two-dimensional materials with integrated Josephson junctions

Josephson junctions (JJ) based on bilayers of azimuthally misaligned two-dimensional materials having superconducting states are provided. Also provided are electronic devices and circuits incorporating the JJs as active components and methods of using the electronic devices and circuits. The JJs are formed from bilayers composed of azimuthally misaligned two-dimensional materials having a first superconducting segment and a second superconducting segment separated by a weak-link region that is integrated into the bilayer.

Above room temperature type II superconductor
11710584 · 2023-07-25 · ·

A Type II superconductor includes a perforated carbonaceous material with an activating material on at least one surface. The activating material a non-polar liquid that does not incorporate Pi-bonding in its structure. The superconductor is manufactured by perforating a carbonaceous material to produce voids and coating at least one surface of the carbonaceous material with the activating material. A superconductive cable includes wires with a perforated carbonaceous material wetted with the activating material on a non-conductive substrate interspersed with non-conducting spacers and surrounded by an insulation layer. The superconductor conducts current at room temperature and above.

Above room temperature type II superconductor
11710584 · 2023-07-25 · ·

A Type II superconductor includes a perforated carbonaceous material with an activating material on at least one surface. The activating material a non-polar liquid that does not incorporate Pi-bonding in its structure. The superconductor is manufactured by perforating a carbonaceous material to produce voids and coating at least one surface of the carbonaceous material with the activating material. A superconductive cable includes wires with a perforated carbonaceous material wetted with the activating material on a non-conductive substrate interspersed with non-conducting spacers and surrounded by an insulation layer. The superconductor conducts current at room temperature and above.

QUANTUM COMPUTING DEVICE

Provided is a quantum computing device comprising a carbon nanotube, a superconducting substrate in quantum proximity to the nanotube and being in a superconducting state having a pairing correlation matrix with a substantial spin-triplet component in a direction perpendicular to the nanotube, and a magnet arranged to provide a longitudinal magnetic field along a longitudinal axis of the nanotube. Further provided is a quantum computing device comprising at least three substrates made of a superconductor material and each in a superconducting state, and a non-superconducting structure made of a material in which the electrons' closed trajectories experience strong spin-orbit coupling interactions and being in quantum proximity to the substrates. The sum of the phase differences between the order parameters of all of the substrates is at least π.

Nanostructured biomimetic protein superconductive devices of making and its multiple applications thereto
11708595 · 2023-07-25 ·

A multiple functioning superconductive device was invented based on Toroidal Josephson Junction (FFTJJ) array with 3D-cage structure self-assembled organo-metallic superlattice membrane. The device not only mimics the structure and function of an activated Matrix Metalloproteinase-2 (MMP-2) protein, but also mimics the cylinder structure of the Heat Shock Protein (HSP60) protein, that works at room temperature under a normal atmosphere, and without external electromagnetic power applied. The device enabled direct rapid real-time monitoring atto-molarity concentration ATP in biological specimens and was able to define the anti-inflammatory and pro-inflammatory status revealed a transitional range of ATP concentration under antibody-free, tracer-free and label-free conditions.

ELECTRONIC DEVICE INTENDED TO CONNECT A FIRST ELECTRONIC COMPONENT TO A SECOND ELECTRONIC COMPONENT, SYSTEM COMPRISING SUCH A DEVICE AND METHODS MAKING IT POSSIBLE TO OBTAIN SUCH A DEVICE
20230017631 · 2023-01-19 ·

An electronic device includes a first surface and a second surface opposite the first surface and intended to connect a first electronic component to a second electronic component located on the first surface by at least one conductor track, the conductor track including a plurality of sections disposed one after the other in such a way as to form the conductor track, each section being constituted of a superconducting material chosen in such a way as to form with the section that follows it, if such a section exists, and the section that precedes it, if such a section exists, an acoustic mismatching interface (or Kapitza interface).