High-fidelity measurement of bosonic modes
High-fidelity measurements of qubits are achieved by increasing a number of measurements taken by use of a swap operation and a readout qubit, deflating a bosonic qubit for which measurement outcomes are affected by single photon/phonon loss events, deflating a bosonic qubit enabling readout in other basis, and evolving the qubit under a Hamiltonian that couples a mode to be measured to another mode where the Hamiltonian is selected from a three wave mixing interaction, and/or a combination of these techniques.
1. A method of measuring an ancilla qubit in a context of error correction of stored quantum information, wherein a set of one or more error correction gates are applied between one or more data qubits storing the quantum information and the ancilla qubit to entangle the ancilla qubit with the one or more data qubits, the method comprising:
transferring an excitation of the ancilla qubit to an additional readout qubit using a SWAP gate or other sequence of one or more gates that perform a swap function;
performing one or more measurements of the readout qubit; and
applying another set of one or more error correction gates between the one or more data qubits storing the quantum information and the ancilla qubit concurrently with performing at least some of the one or more measurements of the readout qubit.
2. The method of claim 1 , wherein the data qubits, the ancilla qubit, and the readout qubit are implemented using mechanical resonators.
3. The method of claim 2 , wherein the swap gate is mediated by an asymmetrically threaded superconducting quantum interference device (ATS).
4. The method of claim 1 , wherein the data qubits, the ancilla qubit, and the readout qubit are implemented using bosonic modes.
5. The method of claim 1 , wherein an amount of time during which the one or more data qubits idle while performing the swap gate is less than an amount of time required to perform the one or more measurements of the readout qubit.
6. The method of claim 5 , wherein the one or more measurements of the readout qubit:
comprise a plurality of repeated measurements taken subsequent to performing the swap gate or other gates that perform the swap function; and
are repeated up until an approximate time when a swap gate operation is performed for a next round of error correction, wherein the swap gate operation of the next round of error correction is performed subsequent to applying the other set of one or more error correction gates.
7. The method of claim 6 , wherein the plurality of repeated measurements of the readout qubit comprise repeated QND (quantum non demolition) parity measurements of the readout qubit.
8. The method of claim 5 , wherein the readout qubit is a higher mode of an ancilla oscillator for the ancilla qubit.
9. The method of claim 8 , wherein the ancilla oscillator is a λ/2 oscillator, and wherein the readout qubit has a mode that is twice a base mode of the ancilla oscillator.
10. A method of performing a measurement of quantum information in a cat qubit, the method comprising:
evolving under a Hamiltonian which couples the phase of α of the cat qubit (an “a” mode) to a measurable property of another bosonic mode (a “b” mode) wherein the Hamiltonian is achieved via a three wave or higher mixing Hamiltonian; and
performing homodyne, heterodyne, or photo detection of the “b” mode to determine a state of the “a” mode,
wherein the cat qubit is implemented using a system comprising:
mechanical resonators; and
a control circuit comprising an asymmetrically-threaded superconducting quantum interference device (ATS) coupled with the mechanical resonators,
wherein the control circuit is configured to stabilize an arbitrary coherent state superposition (cat state) of the mechanical resonators to store quantum information, wherein to stabilize the arbitrary cat-state, the control circuit is configured to:
excite phonons in the mechanical resonators by driving respective storage modes of the mechanical resonators; and
dissipate phonons via an open transmission line coupled to the control circuit configured to absorb photons from a dump mode of the control circuit.
11. The method of claim 10 , wherein:
the Hamiltonian is derived from a three wave mixing Hamiltonian mediated by an ATS;
the “a” mode is implemented via a mechanical storage resonator; and
the “b” mode is implemented via an electromagnetic resonator.
12. The method of claim 11 , wherein a Hamiltonian for the readout comprises:
g ( a+a † )( b+b † );
ig ( a+a † )( b−b † ); or
g ( ab † +a † b ).