International Business Machines Corporation

Globalfoundries Inc.

Zeon Corporation

Applied Materials, Inc.

Markus Brink

Sami Rosenblatt

Jared Barney Hertzberg

Rasit Onur Topaloglu

Dongbing Shao

Michael A Guillorn

Hsinyu Tsai

Firat Solgun

Vivekananda P Adiga

Hiroyuki Miyazoe

Benjamin B Wymore

Christian Lavoie

Salvatore Bernardo Olivadese

Martin O Sandberg

Sebastian Ulrich Engelmann

Jay Michael Gambetta

Joy Cheng

Nicholas Torleiv Bronn

Antonio Corcoles-Gonzalez

Chung-Hsun Lin

Masahiro Nakamura

Jerry M Chow

Patryk Gumann

Nicholas C M Fuller

Gregory S Doerk

Josephine B Chang

Jeng-Bang Yau

Joshua T Smith

Baleegh Abdo

Chi-Chun Liu

Eric Andrew Joseph

Jason Scott Orcutt

Daniel Sanders

Robert L Bruce

Yann A Astier

Michael F Lofaro

Gurpreet Singh

John Bruley

Alexander M Friz

Melia Tjio

Bryan D Trimm

Jeffrey W Sleight

Keith E Fogel

Arvind Kumar

Joshua M Rubin

Kafai Lai

Harry S Barowski

Eric Peter Lewandowski

Sean Hart

Mark Hoinkis

Stephen L Brown

Adam M Pyzyna

Daniela Florentina Bogorin

Oblesh Jinka

Albert Frisch

Bang N To

Hsinuyu Tsai

Sweet Jean L

Adiga Vivekananda

Bryan Trimm

A thermalization structure is formed using a cover configured with a set of pillars, the cover being a part of a cryogenic enclosure of a low temperature device (LTD). A chip including the LTD is configured with a set of cavities, a cavity in the set of cavities having a cavity profile. A pillar from the set of pillars and corresponding to the cavity has a pillar profile such that the pillar profile causes the pillar to couple with the cavity of the cavity profile within a gap tolerance to thermally couple the chip to the cover for heat dissipation in a cryogenic operation of the chip.

Cryogenic packaging for thermalization of low temperature devices

Fabrication of superconducting devices that combine or separate direct currents and microwave signals is provided. A method can comprise forming a direct current circuit that supports a direct current, a microwave circuit that supports a microwave signal, and a common circuit that supports the direct current and the microwave signal. The method can also comprise operatively coupling a first end of the direct current circuit and a first end of the microwave circuit to a first end of the common circuit. The direct current circuit can comprise a bandstop circuit and the microwave circuit can comprise a capacitor. Alternatively, the direct current circuit can comprise a bandstop circuit and the microwave circuit can comprise a bandpass circuit. Alternatively, the microwave circuit can comprise a capacitor and the direct current circuit can comprise one or more quarter-wavelength transmission lines.

Fabrication of superconducting devices that control direct currents and microwave signals

Techniques facilitating formation of amorphous superconducting alloys for superconducting circuits are provided. A device can comprise one or more superconducting components that comprise an amorphous superconducting alloy comprising two or more elements. At least one element of the two or more elements is a superconducting element.

Amorphous superconducting alloys for superconducting circuits

A method of increasing grain size of polycrystalline superconducting materials for superconducting circuits, includes forming an initial superconducting epitaxial layer lattice matched to a substrate formed of a substrate material, the initial superconducting epitaxial layer formed of a compound including the substrate material and a first metal; and forming a second layer of the first metal on the initial superconducting epitaxial layer and heating the layers to increase a thickness of the initial superconducting epitaxial layer formed of the compound.

Increasing grain size of polycrystalline superconducting materials for superconducting circuits

A technique relates to a superconducting chip. Resonant units have resonant frequencies, and the resonant units are configured as superconducting resonators. Josephson junctions are in the resonant units, and one or more of the Josephson junctions have a shorted tunnel barrier.

Qubit network non-volatile identification

Systems and techniques that facilitate spurious junction prevention via in-situ ion milling are provided. In various embodiments, a method can comprise forming a tunnel barrier of a Josephson junction on a substrate during a shadow evaporation process. In various instances, the method can further comprise etching an exposed portion of the tunnel barrier during the shadow evaporation process. In various embodiments, the shadow evaporation process can comprise patterning a resist stack onto the substrate. In various instances, the etching the exposed portion of the tunnel barrier can leave a protected portion of the tunnel barrier within a shadow of the resist stack. In various instances, the shadow of the resist stack can be based on a direction of the etching the exposed portion of the tunnel barrier. In various embodiments, the shadow evaporation process can further comprise depositing a first superconducting material on the substrate after the patterning the resist stack, oxidizing a surface of the first superconducting material to form the tunnel barrier, and depositing a second superconducting material over the protected portion of the tunnel barrier to form a Josephson junction. In various instances, the etching the exposed portion of the tunnel barrier can occur after the oxidizing the surface of the first superconducting material and before the depositing the second superconducting material.

Spurious junction prevention via in-situ ion milling

Techniques related to vertical silicon-on-metal superconducting quantum interference devices and method of fabricating the same are provided. Also provided are associated flux control and biasing circuitry. A superconductor structure can comprise a silicon-on-metal substrate that can comprise a first superconducting layer, comprising a first superconducting material, between a first crystalline silicon layer and a second crystalline silicon layer. The superconducting structure can also comprise a first via comprising a first Josephson junction and a second via comprising a second Josephson junction. The first via and the second via can be formed between the first superconducting layer and a second superconducting layer, comprising a second superconducting material. An electrical loop around a defined area of the second crystalline silicon layer can comprise the first via comprising the first Josephson junction, the second via comprising the second Josephson junction, the first superconducting layer, and the second superconducting layer.

Vertical silicon-on-metal superconducting quantum interference device

According to an embodiment of the present invention, a quantum processor includes a qubit chip. The qubit chip includes a substrate, and a plurality of qubits formed on a first surface of the substrate. The plurality of qubits are arranged in a pattern, wherein nearest-neighbor qubits in the pattern are connected. The quantum processor also includes a long-range connector configured to connect a first qubit of the plurality of qubits to a second qubit of the plurality of qubits, wherein the first and second qubits are separated by at least a third qubit in the pattern.

Highway jumper to enable long range connectivity for superconducting quantum computer chip

A superconducting circuit includes a Josephson junction device including a lower superconducting material layer formed on a substrate and a junction layer formed on the lower superconducting material layer. The superconducting circuit also includes an upper superconducting material layer formed over the junction layer. At least the lower superconducting material layer comprises grains having a size that is larger than a size of the Josephson junction.

Grain size control of superconducting materials in thin films for Josephson junctions

A system includes a first quantum circuit plane that includes a first qubit, a second qubit and a third qubit. A coupled-line bus is coupled between the first qubit and the second qubit. A second circuit plane is connected to the first quantum circuit plane, comprising a control line coupled to the third qubit. The control line and the coupled-line bus are on different planes and crossing over each other, and configured to mitigate cross-talk caused by the crossing during signal transmission.

Coupled-line bus to suppress classical crosstalk for superconducting qubits

A quantum computing device includes a first chip having a first substrate and one or more qubits disposed on the first substrate. Each of the one or more qubits has an associated resonance frequency. The quantum computing device further includes a second chip having a second substrate and at least one conductive surface disposed on the second substrate opposite the one or more qubits. The at least one conductive surface has at least one dimension configured to adjust the resonance frequency associated with at least one of the one or more qubits to a determined frequency adjustment value.

Qubit frequency tuning structures and fabrication methods for flip chip quantum computing devices

An embodiment of a qubit tuning device includes a first layer configured to generate a magnetic field, the first layer comprising a material exhibiting superconductivity in a cryogenic temperature range. In an embodiment, the qubit tuning device includes a qubit of a quantum processor chip, wherein the first layer is configured to magnetically interact with the qubit such that a first magnetic flux of the first layer causes a first change in a first resonance frequency of the qubit by a first frequency shift value.

Qubit tuning by magnetic fields in superconductors

A method of fabricating a superconductor device includes providing a first metal layer on top of the substrate. An oxidation of a top surface of the first metal layer is rejected. A second metal layer is deposited on top of the second metal layer. A superconducting alloy of the first metal layer and the second metal layer is created between the first metal layer and the second metal layer. There is no oxide layer between the superconducting alloy and the first metal layer.

Superconducting structure and device surface termination with alloy

A method of measuring contact resistance at an interface for superconducting circuits is provided. The method includes using a chain structure of superconductors to measure a contact resistance at a contact between contacting superconductor. The method further includes eliminating ohmic resistance from wire lengths in the chain structure by operating below the lowest superconducting transition temperature of all the superconductors in the chain structure. The measurement is dominated by contact resistances of the contacts between contacting superconductors in the chain.

Methods and structure to probe the metal-metal interface for superconducting circuits

An on-chip microwave filter circuit includes a substrate formed of a first material that exhibits at least a threshold level of thermal conductivity, wherein the threshold level of thermal conductivity is achieved at a cryogenic temperature range in which a quantum computing circuit operates. The filter circuit further includes a dispersive component configured to filter a plurality of frequencies in an input signal, the dispersive component including a first transmission line disposed on the substrate, the first transmission line being formed of a second material that exhibits at least a second threshold level of thermal conductivity, where the second threshold level of thermal conductivity is achieved at a cryogenic temperature range in which a quantum computing circuit operates. The dispersive component further includes a second transmission line disposed on the substrate, the second transmission line being formed of the second material.

Cryogenic on-chip microwave filter for quantum devices

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White Plains, NY, United States of America

Markus Brink