USA As Represented by Secretary of the Navy

Other

Susan Anne Elizabeth Berggren

Benjamin J Taylor

Anna Leese De Escobar

Robert Lewis Fagaly

Marcio Calixto De Andrade

Teresa H Emery

Nicholas Biagio Ferrante

Oleg A Mukhanov

Visarath In

Patrick Longhini

Antonio Palacios

Sergio A Montoya

Thomas Sheffield

James J Collins

Erica L Daly

Georgy Prokopenko

Daniel Hallman

Rachel Mae Hobbs

A platform provides precise thermal regulation of cryogenic electronic circuits. The platform includes a cold distribution plate, cold blades, heaters, and a thermal regulator. The cold distribution plate couples to a cryogenic cooler for cooling the cold distribution plate. The cold blades contact and extend from a periphery of the cold distribution plate. The cold blades support and cool the cryogenic electronic circuits, which include a respective cryogenic electronic circuit disposed on each of the cold blades. The heaters heat the cold blades, with the heaters including a respective heater disposed at each of the cold blades. The thermal regulator controls the heaters to maintain a predetermined temperature at each of the cryogenic electronic circuits.

Platform for precise thermal regulation of cryogenic electronic circuits

A superconducting quantum interference apparatus comprising a planar array of loops where each loop constitutes a superconducting quantum interference device, and a magnetic shield disposed over part of one of the loops so to protect the covered part of the loop from exposure to a magnetic field.

High temperature superconductor bi-superconducting quantum interference device

A superconducting quantum interference device (SQUID) array (SQA) includes at least one row each including SQUIDs. The SQUIDs in each row are connected in parallel and include junctions, such as Josephson junctions, shared among the SQUIDs. The SQUIDs have respective inductance parameters and the junctions have respective critical currents. The respective inductance parameters of the SQUIDs and respective critical currents of the junctions both vary in a predetermined pattern across the row. This improves performance including improved linearity and improved sensitivity.

Superconducting quantum interference device (SQUID) array (SQA) having predetermined pattern across each row

A superconducting electronic circuit includes at least two SQUID elements, an array of at least three Josephson Junctions, and a magnetic source element. Each SQUID element has no shared Josephson Junctions or at least one shared Josephson Junction with another SQUID element and at least one exclusive Josephson Junction. The array of at least three Josephson Junctions are connected in one, two, or three-dimensions. The magnetic source element has an electrically-tunable spatially non-uniform magnetic field.

Superconducting electronic circuit

A system is provided for detecting a radio frequency signal. The system includes a dielectric platform, a first SQUID array, a second array of SQUIDs and a processing component. The dielectric platform has a first planar surface and a second planar surface that is disposed at an angle relative to the first planar surface. The first array of SQUIDs is disposed on the first planar surface and can output a first detection signal based on the radio frequency signal. The second array of SQUIDs is disposed on the second planar surface and can output a second detection signal based on the radio frequency signal. The processing component can determine a first plane from which the radio frequency signal is transmitting based on the first detection signal and the second detection signal.

Orthogonal SQUID arrays on a baseline with rotation

A device is disclosed that includes a substrate, a first superconducting quantum interference device (SQUID), a second SQUID and a third SQUID. The first SQUID is disposed on the substrate and has a first feature dimension, a second feature dimension and a first effective geometric magnetic inductance parameter value, &#x3b2;. The second SQUID is disposed on the substrate and has the first feature dimension, a third feature dimension and a second effective geometric magnetic inductance parameter value, &#x3b2;. The third SQUID is disposed on the substrate and has the first feature dimension, a fourth feature dimension and a third effective geometric magnetic inductance parameter value, &#x3b2;, wherein &#x3b2;&#x3c;&#x3b2;&#x3c;&#x3b2;.

Method for producing SQUID arrays composed of SQUID elements having large spread in magnetic inductance values and comparable internal dimensions

A superconducting quantum interference device (SQUID) for mobile magnetic sensing applications comprising: at least two Josephson junction electrically connected to a superconducting loop; and a resistive element connected in series with one of the Josephson junctions in the superconducting loop. The resistive element is disposed in the same superconducting loop as the at least two Josephson junctions.

SQUID having integrated resistive element

A superconducting quantum interference device (SQUID) for mobile applications comprising: a superconducting flux transformer having a pickup coil and an input coil, wherein the input coil is inductively coupled to a Josephson junction; a resistive element connected in series between the pickup coil and the input coil so as to function as a high pass filter such that direct current (DC) bias current is prevented from flowing through the input coil; and a flux bias circuit electrically connected in parallel to the superconducting flux transformer between the pickup coil and the input coil so as to reduce motion-induced noise.

Magnetic sensor with combined high pass flux concentrator and flux biasing circuit

First and second superconductive sensors receive an electromagnetic signal. The first and second superconductive sensors are spaced apart such that there is a phase difference between the electromagnetic signal as received at the first and second superconductive sensors. The first and second superconductive sensors output respective first and second voltage signals corresponding to the electromagnetic signal as received by the first and second superconductive sensors. A nonlinear detector detects a voltage difference between the first and second voltage signals and provides an output signal representing the detected voltage difference. The output signal corresponds to the phase difference between the electromagnetic signal as received at the first and second superconductive sensors.

Electromagnetic signal phase discrimination using superconductive sensors and a nonlinear detector

A system includes a substrate having a high-temperature superconductor compound film disposed thereon. A first superconducting region is formed within the film and has a first stabilized oxygen content. A second superconducting region is also formed within the film and is located adjacent to the first superconducting region. The second superconducting region has a second stabilized oxygen content. A boundary region is formed within the film and separates the first superconducting region from the second superconducting region. A voltage source is connected to the first superconducting region and the second superconducting region. The boundary region emits electromagnetic radiation responsive to an applied voltage from the voltage source to one of the first superconducting region and the second superconducting region. A current flows from the first superconducting region to the second superconducting region, or vice versa, responsive to the applied voltage.

High-temperature superconductor teraherz emitting diode

An intrinsic superconducting gradiometer comprising: a first array having at least two superconducting devices, wherein the first array has upper and lower terminals located on opposite sides of the first array, wherein the upper terminal is configured to receive a bias signal; and a second array that is identical to, oriented the same as, and located in close proximity to the first array, wherein the second array's upper terminal is grounded and its lower terminal is electrically connected to the first array's lower terminal such that a measured voltage difference between the first array's upper terminal and the second array's upper terminal represents a net current generated by a gradient magnetic field where near-field measurements are cancelled, and wherein the intrinsic superconducting gradiometer is designed to provide the measured voltage difference that is directly proportional to the magnetic field gradient without being connected to any external coils or flux transducers.

SQUID array planar and axial gradiometer

The transfer function of a sensing device including a plurality of sensors is automatically adjusted based on a power level of an incident electromagnetic signal detected by the plurality of sensors. Each of the plurality of sensors is associated with a unique transfer function. An output from one of the plurality of sensors associated with a particular transfer function is automatically selected based on a power level of the detected incident electromagnetic signal. Responsive to a change in the power level of the detected electromagnetic signal, another output from a different one of the plurality of sensors associated with a different transfer function is selected. The transfer function is adjusted over time by automatically selecting outputs from different ones of the plurality of sensors based on changes in the power level of the detected incident electromagnetic signal.

Methods, devices, and integrated circuits for automatically adjusting a transfer function of a sensing device based on a power level of an incident electromagnetic signal

A device in accordance with several embodiments can include a plurality of N Superconducting Quantum Interference Devices (SQUIDs), which can be divided into a plurality of sub-blocks of SQUIDs. The SQUIDs in the sub-blocks can be RF SQUIDs, DC SQUIDs or bi-SQUIDs. The sub-blocks can be arranged in a plurality of X tiers, with each Ttier having a different number of sub-blocks of SQUIDs than an immediately adjacent Ttier. Each Ttier can have the same total bias current; and can have SQUIDs with different critical currents and loop sizes, with the different loop sizes on each tier having a Gaussian distribution of between 0.5 and 1.5 (or a random distribution). Additionally, the Arrays can be configured as three independent planar arrays of SQUIDs. The three planar arrays can be triangular when viewed in top plan, and can be arranged so that they are orthogonal to each other.

Tiered superconducting quantum interference device (SQUID) array

An antenna includes a plurality of superconducting quantum interference device (SQUID) arrays on a chip, and a printed circuit board (PCB) formed with a cutout for receiving the chip. The PCB is formed with a set of coplanar transmission lines, and the chip is inserted into the cutout so that each said transmission line connects to a respective SQUID array. A cryogenic system can cool the chip to a temperature that causes a transition to superconductivity for the SQUID arrays. A thermal radome can be placed around the chip, the PCB and the cryogenic system to maintain the temperature. A DC bias can be applied to the SQUID arrays to facilitate RF detection. The SQUID array, chip and CPW transmission lines can cooperate to allow for both detection of said RF energy and conversion of said RF energy to a signal without requiring the use of a conductive antenna dish.

System and method for broadband far and near field radio frequency radiation detection using superconducting quantum detector arrays

A High Temperature Superconducting (HTS) Superconducting Quantum Interference Device and methods for fabrication can include at least one bi-Superconducting Quantum Interference Device. The bi-SQUID can include an HTS substrate that can be formed with a step edge. A superconducting loop of YBCO can be deposited on the step edge to establish two Josephson Junctions. A superconducting path that bi-sects the superconducting loop path can also be deposited onto the substrate. In some embodiments, the bisecting path can cross the step edge twice, and the bisecting path can be ion milled at one of the crossing points to round the bisecting path and thereby remove the fourth Josephson Junction at the other crossing point. In still other embodiments, the bisecting path can be completely on the upper shelf (or the lower shelf), and the bisecting path can be ion damaged, ion damaged, or particle damaged, to establish the third Josephson Junction.

Growing community of inventors

San Diego, CA, United States of America

Susan Anne Elizabeth Berggren