Abstract: A qubit structure includes a substrate; a first planar metal portion residing on the substrate; a second planar metal portion residing on the substrate; a plurality of candidate tunnel junctions, a first end of each candidate tunnel junction coupled to the first planar metal portion; and a plurality of pads, each pad coupled to a second end of each candidate tunnel junction.

Abstract: An N-dimensional scan of a set of bias voltages is performed, each bias voltage defining a voltage of a corresponding electrode of a set of electrodes, the electrodes being proximate to a given qubit. A sensitivity of a performance of the given qubit to an electronic field generated by each of the electrodes is determined. A probable location of at least one two-level system (TLS) is extrapolated based on the determined sensitivities. An effect of the two-level system (TLS) on the given qubit is mitigated based on the extrapolated location.

Abstract: Field effect transistors include a stack of nanowires of vertically arranged channel layers. A source and drain region is disposed at respective ends of the vertically arranged channel layers. A gate stack is formed over, around, and between the vertically arranged channel layers. Internal spacers are each formed between the gate stack and a respective source or drain region, with at least one pair of spacers being positioned above an uppermost channel layer.

Abstract: A system comprises a memory that stores and a processor that executes computer executable components stored in the memory, wherein the computer executable components comprise an identification component that identifies a target partition definition for a quantum processor comprising a plurality of qubits, and a mapping component that directs a controller of a quantum system, comprising the quantum processor, to apply the target partition definition to control electronics at the quantum system for subsequent of an operation at the quantum processor, wherein the target partition definition corresponds to a quantum system resource, of the quantum system, associated with a target qubit of the plurality of qubits.

Abstract: Systems, computer-implemented methods, and/or computer program products that can facilitate target qubit decoupling in an echoed cross-resonance gate are provided. According to an embodiment, a computer-implemented method can comprise receiving, by a system operatively coupled to a processor, both a cross-resonance pulse and a decoupling pulse at a target qubit. The cross-resonance pulse propagates to the target qubit via a control qubit. The computer-implemented method can further comprise receiving, by the system, a state inversion pulse at the control qubit. The computer-implemented method can further comprise receiving, by the system, both a phase-inverted cross-resonance pulse and a phase-inverted decoupling pulse at the target qubit. The phase-inverted cross-resonance pulse propagates to the target qubit via the control qubit.

Abstract: An insulator region is fabricated in a semiconductor substrate of a wafer and a metal layer is fabricated on the semiconductor substrate. Test circuitry is fabricated on a first portion of the metal layer, the first portion residing at least partially over the insulator region. Quantum circuitry is fabricated on a second portion of the metal layer.

Abstract: A method, system and computer program product for calibrating a quantum operation. Layers of two qubit gates that operate in parallel are defined. A gate length for each two qubit gate in a layer of the defined layers is calibrated to correspond to the same gate length, such as the gate length of the two qubit gate in that layer with the slowest operation speed. A portion of the quantum operation is performed by the two qubit gates in the layer with the calibrated gate length. In this manner, two qubit gates that operate in parallel are effectively calibrated in a manner that results in better gate fidelities, fewer frequency collisions and fewer undesirable transitions.

Abstract: One or more systems, devices, computer program products and/or computer-implemented methods of use provided herein relate to buffers for streaming in quantum-centric supercomputing. A system can comprise a memory that can store computer-executable components. The system can further comprise a processor that executes at least one of the computer executable components that can execute a quantum circuit to obtain measurements of a qubit. The at least one of the computer executable components can further modulate, via a control two-level system (TLS) knob, a TLS landscape of a quantum processor between successive executions of the quantum circuit.

Abstract: A method, system and computer program product for calibrating a quantum operation. Layers of two qubit gates that operate in parallel are defined. A gate length for each two qubit gate in a layer of the defined layers is calibrated to correspond to the same gate length, such as the gate length of the two qubit gate in that layer with the slowest operation speed. A portion of the quantum operation is performed by the two qubit gates in the layer with the calibrated gate length. In this manner, two qubit gates that operate in parallel are effectively calibrated in a manner that results in better gate fidelities, fewer frequency collisions and fewer undesirable transitions.

Abstract: Techniques regarding an embedded microstrip transmission line implemented in one more superconducting microwave electronic devices are provided. For example, one or more embodiments described herein can comprise an apparatus, which can include a superconducting material layer positioned on a raised portion of a dielectric substrate. The raised portion can extend from a surface of the dielectric substrate. The apparatus can also comprise a dielectric film that covers at least a portion of the superconducting material layer and the raised portion of the dielectric substrate.

Abstract: A field effect transistor (FET) includes a substrate; a channel material located on the substrate, the channel material comprising one of graphene or a nanostructure; a gate located on a first portion of the channel material; and a contact aligned to the gate, the contact comprising one of a metal silicide, a metal carbide, and a metal, the contact being located over a source region and a drain region of the FET, the source region and the drain region comprising a second portion of the channel material.

Abstract: Techniques for using stark tone pulses to mitigate cross-resonance collision in qubits are presented. A tone management component can control application of pulses to qubits by a tone generator component to mitigate undesirable frequency collisions between qubits. The tone generator component (TGC) can apply an off-resonant tone pulse to a qubit during a gate to induce a stark shift. TGC can apply a cross-resonance tone pulse to a control qubit at a frequency associated with the qubit, wherein the frequency can be stark shifted based on the off-resonant tone pulse. The qubit can be a target qubit, the control qubit itself, or a spectator qubit that can be coupled to the target qubit or the control qubit. The gate can be a cross-resonance gate, a two-qubit gate, or a measurement gate that can utilize an echo sequence, a target rotary, or active cancellation.

Abstract: Devices, systems, methods, and/or computer-implemented methods that can facilitate a qubit device comprising a superconducting circuit provided on an encapsulated vacuum cavity are provided. According to an embodiment, a device can comprise a substrate having an encapsulated vacuum cavity provided on the substrate. The device can further comprise a superconducting circuit provided on the encapsulated vacuum cavity.

Abstract: Systems, computer-implemented methods, and/or computer program products that can facilitate target qubit decoupling in an echoed cross-resonance gate are provided. According to an embodiment, a computer-implemented method can comprise receiving, by a system operatively coupled to a processor, both a cross-resonance pulse and a decoupling pulse at a target qubit. The cross-resonance pulse propagates to the target qubit via a control qubit. The computer-implemented method can further comprise receiving, by the system, a state inversion pulse at the control qubit. The computer-implemented method can further comprise receiving, by the system, both a phase-inverted cross-resonance pulse and a phase-inverted decoupling pulse at the target qubit. The phase-inverted cross-resonance pulse propagates to the target qubit via the control qubit.

Abstract: Techniques for using stark tone pulses to mitigate cross-resonance collision in qubits are presented. A tone management component can control application of pulses to qubits by a tone generator component to mitigate undesirable frequency collisions between qubits. The tone generator component (TGC) can apply an off-resonant tone pulse to a qubit during a gate to induce a stark shift. TGC can apply a cross-resonance tone pulse to a control qubit at a frequency associated with the qubit, wherein the frequency can be stark shifted based on the off-resonant tone pulse. The qubit can be a target qubit, the control qubit itself, or a spectator qubit that can be coupled to the target qubit or the control qubit. The gate can be a cross-resonance gate, a two-qubit gate, or a measurement gate that can utilize an echo sequence, a target rotary, or active cancellation.

Abstract: Techniques for using stark tone pulses to mitigate cross-resonance collision in qubits are presented. A tone management component can control application of pulses to qubits by a tone generator component to mitigate undesirable frequency collisions between qubits. The tone generator component (TGC) can apply an off-resonant tone pulse to a qubit during a gate to induce a stark shift. TGC can apply a cross-resonance tone pulse to a control qubit at a frequency associated with the qubit, wherein the frequency can be stark shifted based on the off-resonant tone pulse. The qubit can be a target qubit, the control qubit itself, or a spectator qubit that can be coupled to the target qubit or the control qubit. The gate can be a cross-resonance gate, a two-qubit gate, or a measurement gate that can utilize an echo sequence, a target rotary, or active cancellation.

Abstract: Systems and techniques that facilitate mapping a heavy-hex qubit connection topology to a rectilinear physical qubit layout are provided. In various embodiments, a device can comprise a qubit lattice on a substrate. In various aspects, the qubit lattice can comprise one or more first qubit tiles. In various cases, the one or more first qubit tiles can have a first shape. In various instances, the qubit lattice can further comprise one or more second qubit tiles. In various cases, the one or more second qubit tiles can have a second shape. In various aspects, the one or more first qubit tiles can be tessellated with the one or more second qubit tiles.

Abstract: Systems, computer-implemented methods, and/or computer program products that can facilitate target qubit decoupling in an echoed cross-resonance gate are provided. According to an embodiment, a computer-implemented method can comprise receiving, by a system operatively coupled to a processor, both a cross-resonance pulse and a decoupling pulse at a target qubit. The cross-resonance pulse propagates to the target qubit via a control qubit. The computer-implemented method can further comprise receiving, by the system, a state inversion pulse at the control qubit. The computer-implemented method can further comprise receiving, by the system, both a phase-inverted cross-resonance pulse and a phase-inverted decoupling pulse at the target qubit. The phase-inverted cross-resonance pulse propagates to the target qubit via the control qubit.

Abstract: Devices, systems, methods, and/or computer-implemented methods that can facilitate a qubit device comprising a vacuum encapsulated Josephson junction are provided. According to an embodiment, a device can comprise a substrate having an encapsulated vacuum cavity provided on the substrate. The device can further comprise one or more superconducting components of a superconducting circuit provided inside the encapsulated vacuum cavity.

Abstract: Techniques for using stark tone pulses to mitigate cross-resonance collision in qubits are presented. A tone management component can control application of pulses to qubits by a tone generator component to mitigate undesirable frequency collisions between qubits. The tone generator component (TGC) can apply an off-resonant tone pulse to a qubit during a gate to induce a stark shift. TGC can apply a cross-resonance tone pulse to a control qubit at a frequency associated with the qubit, wherein the frequency can be stark shifted based on the off-resonant tone pulse. The qubit can be a target qubit, the control qubit itself, or a spectator qubit that can be coupled to the target qubit or the control qubit. The gate can be a cross-resonance gate, a two-qubit gate, or a measurement gate that can utilize an echo sequence, a target rotary, or active cancellation.