Granted Patent B2

US 12,572,834 · App. 17/899,291 · Granted Mar 10, 2026

Inventors: Andrei Ruskuc (Pasadena, CA); Joonhee Choi (Pasadena, CA); Chun-Ju Wu (Pasadena, CA); Andrei Faraon (La Canada Flintridge, CA)

Assignee: CALIFORNIA INSTITUTE OF TECHNOLOGY

G06N10/40G06N10/20

Abstract

Claims (91)

1 . A device for coupling a qubit to a register, comprising:

a circuit for controlling application of one or more cycles of a protocol comprising a sequence of pulses synchronized with an RF field, a timing, a phase, and a duration of each of the pulses, and a period and amplitude of the RF field, wherein:

the application of the one or more cycles of the protocol controls a coherent spin exchange interaction between a register and a qubit having a zero magnetic dipole moment;

the qubit comprises a first spin state and a second spin state both of which have the zero magnetic dipole moment;

the register comprises multiple register spins having an energy level structure;

the register spins are indistinguishable so as to be configurable in basis states including a superposition state used for storing a quantum state of the qubit; and

the pulses each comprise an electromagnetic field tuned to excite a transition between the first spin state and the second spin state.

2 . The device of claim 1 , wherein the protocol is configured to:

suppress or cancel one or more non-exchange interactions between the register and the qubit,

suppress or cancel noise coupled to the qubit and causing decoherence of the quantum state of the qubit,

enable the coherent spin exchange interaction that performs a quantum logic gate,

coherently transferring the quantum state of the qubit between the register and the qubit.

3 . The device of claim 1 , wherein the circuit controls:

application of a period of the protocol within a time period shorter than a rate of change of a magnetic noise, so that the magnetic noise is quasistatic during the application of the period of the protocol, wherein the magnetic noise causes qubit decoherence and induces a second order interaction (incoherent interaction) between the qubit and the register; and

at least one of the phase, the duration, or time spacing of the pulses in the period so that:

the spin-exchange interactions induced by the RF field are preserved or maintained across the period;

one or more non-exchange interactions induced by the RF field are cancelled across the period;

any exchange interactions and any non-exchange interactions induced by the magnetic noise are cancelled across the period; and

the qubit decoherence induced by the magnetic noise is cancelled over the period; and

the RF field toggling between two values of equal magnitude and opposite polarity such that:

the period is associated with a frequency of a precession of each of the multiple register spins about a predetermined quantization axis; and

the amplitude is selected for a predetermined magnitude of the coherent spin exchange interaction between the register spins and the qubit, and

so as to form the coherent spin exchange interaction.

4 . The device of claim 3 , wherein the protocol comprises the sequence of single qubit gates, each of the single qubit gates comprising one of the pulses having the frequency and duration tuned to drive the transition between the first spin state and the second spin state.

5 . The device of claim 1 comprising a quantum memory, wherein the circuit:

controls application of a number of cycles of the protocol in combination with an initialization of the qubit so as to configure the register spins in a polarized state;

controls application of one or more of the pulses to set the quantum state of the qubit; and

controls application of a number of cycles of the protocol so as to apply a first swap gate (two qubit gate) transferring the quantum state of the qubit from the qubit to the register, thereby changing the polarized state to a corresponding state of the register spins corresponding to the quantum state; and

controls application of a number of cycles of the protocol so as to apply a second swap gate retrieving the quantum state in the qubit from the register, thereby changing the corresponding state of the register spins to the polarized state.

6 . The device of claim 5 , wherein configuring the register spins in the polarized state comprises polarizing the register, which is initially in an unpolarized state comprising any configuration of excitations of the register spins, by:

(a) initializing the qubit in the first spin state by controlling application of one or more initialization pulses of an initialization electromagnetic field having a frequency tuned to initialize the quantum state of the qubit in the first spin state;

(b) applying one or more cycles of the protocol transferring a spin excitation from the register spins to the qubit; and

(c) repeating steps (a) and (b) until all the excitations of the register spins are transferred from the register to the qubit and the register spins are initialized in the polarized state, as characterized by a measurement of the qubit remaining in the first spin state after step (b).

7 . The device of claim 5 , wherein the circuit controls application of the protocol so as to apply the first swap gate mapping (via the coherent spin exchange interaction) between the qubit and the register, such that:

if the qubit is in the first spin state, the corresponding state of the register is the polarized state,

if the qubit is in the second spin state, the corresponding state of the register is a W state, and

if the qubit is in a superposition of the first spin state and the second spin state, the corresponding state of the register is a superposition of the polarized state and the W state, and

wherein the W state is a superposition of all single spin excitation states of the register spins.

8 . The device of claim 1 , wherein the circuit:

controls application of one or more cycles of the protocol in combination with an initialization of the qubit so as to configure the register spins in a polarized state;

controls application of one or more of the pulses to set the quantum state of the qubit;

controls application of one or more cycles of the protocol so as to apply a first square root of swap gate entangling the qubit with the register so as to form a Bell state; and

controls application of one or more cycles of the protocol so as to apply a second square root of swap gate interacting with the Bell state so as to perform a measurement of the Bell state.

9 . A repeater in a quantum network comprising the device of claim 8 .

10 . The repeater of claim 9 , further comprising:

a photonic cavity coupled to a solid state material comprising the qubit and the register;

one or more microwave sources coupled to the qubit via a microwave waveguide, the microwave sources outputting one or more first microwave pulses and/or one or more second microwave pulses;

a radio frequency source outputting the RF field; and

one or more laser sources outputting one or more laser pulses coupled to the qubit through the photonic cavity; and wherein:

the circuit controls the one or more laser sources and the one or more microwave sources so as to:

output initialization pulses comprising at least one of the one or more laser pulses or the one or more first microwave pulses having initialization frequencies for exciting one or more transitions initializing the qubit;

apply the protocol comprising the single qubit gates comprising the second microwave pulses in synchronization with the RF field; and

output one or more readout electromagnetic fields having a readout frequency for exciting a readout transition from the second spin state to a readout state, so as to stimulate output of third pulses from the readout state.

11 . The device of claim 1 , wherein:

the pulses each comprise a pi pulse or a pi/2 pulse having at least one phase selected from +x −x, +y, or −y, and

the circuit controls:

the sequence such that the period of the RF field is 2τ and a spacing of the pulses is τ/4, and

for a given magnitude of the spin exchange interaction determined by the amplitude of the RF field, a number of repeats or cycles of the protocol that applies at least one of a swap gate transferring a quantum state between the qubit and the register, a square root of a swap gate for forming or measuring a Bell state, or that can be used to polarize the spins into a polarized state in combination with an initialization of the qubit.

12 . The device of claim 1 wherein the circuit selects the duration and the timing of each of the pulses and a toggling of the RF field to engineer the coherent spin-exchange interaction comprising:

{circumflex over ( {tilde over (S)} )} + Î − +{circumflex over ( {tilde over (S)} )} − Î + ,

where {circumflex over (Ĩ)} + =|↑ ↓|, {circumflex over (Ĩ)} − =|↓ ↑| are the raising and lowering operators in an effective nuclear two-level manifold of the multiple spins in the register and {circumflex over ({tilde over (S)})} + are similarly defined for the qubit.

13 . The device of claim 1 , wherein the RF field comprises a square wave and the sequence of pulses comprise:

in a first half period τ of the square wave a sequence of the second pulses comprising:

a first pi/2 pulse having a phase +Y followed by a first pi pulse having a phase +Y, the beginning of the first pi/2 pulse and the center of the first pi pulse separated in time by τ/4;

a second pi/2 pulse immediately followed by a third pi/2 pulse, the end of the second pi/2 pulse separated in time from the center of the first pi pulse by τ/4, wherein the second pi/2 pulse has a phase −Y and the third pi/2 pulse has a phase −X;

a second pi pulse having a phase −X and following the third pi/2 pulse, a center of the second pi pulse separated in time from the center of the first pi pulse by τ/2; and

a fourth pi/2 pulse having a phase −X, wherein the end of the fourth pi/2 pulse is separated in time from center of the second pi pulse by τ/4; and

in a second half period τ of the square wave, a repeat of the sequence of second pulses but wherein the first pi/2 pulse, the first pi pulse, and the second pi/2 pulse have opposite phase as compared to the first pi/2 pulse, the first pi pulse, and the second pi/2 pulse in the first half period, respectively.

14 . The device of claim 1 , wherein the protocol de-couples the qubit from decoherence noise and random interactions caused by a nuclear Overhauser field generated by a host lattice in which the qubit is located.

15 . A system for implementing a quantum register comprising the device of claim 1 coupled to:

a spin carrying defect in a host lattice, wherein the spin carrying defect comprises the qubit and the host lattice comprises the register, or

a quantum dot in a host lattice, wherein the quantum dot comprises the qubit and the host lattice comprises the register.

16 . The system of claim 15 , wherein the spin carrying defect is a qubit ion comprising the qubit and the register comprises a lattice of register ions surrounding the qubit ion.

17 . The device of claim 1 , wherein the multiple spins in the register comprise nuclear spins and the first spin state and the second spin state comprise electron spin states.

18 . A method for coupling a qubit to a quantum register, comprising:

obtaining a protocol comprising a sequence of pulses synchronized with an RF field, the protocol further comprising a timing, a phase, and a duration of each of the pulses comprising a single qubit gate, and a period and amplitude of the RF field, wherein application of the protocol controls a coherent spin exchange interaction between a register and a qubit; and

applying one or more cycles of the protocol to the qubit, so as to modulate the coherent spin exchange interaction transferring a spin excitation between the qubit and the register; and

wherein:

the qubit comprises a first spin state and a second spin state both having a zero magnetic dipole moment;

the register spins are indistinguishable so as to be configurable in basis states including a superposition state used for storing a quantum state of the qubit; and

the pulses comprise an electromagnetic field tuned to excite a transition between the first spin state and the second spin state.

19 . The method of claim 18 , further comprising applying a number of cycles of the protocol so as transfer quantum information between the qubit and the register, comprising:

applying a first number of the cycles of the protocol to the qubit in combination with an initialization of the qubit so as to configure the register spins in a polarized state;

applying one or more of the pulses to the qubit to set the quantum state of the qubit;

applying a second number of the cycles of the protocol to the qubit so as to apply a first swap gate (two qubit gate) transferring the quantum state of the qubit from the qubit to the register, thereby changing the polarized state to a corresponding state of the register spins corresponding to the quantum state; and

applying one or more cycles of the protocol to the qubit so as to apply a second swap gate retrieving the quantum state in the qubit from the register, thereby changing the corresponding state of the register spins to the polarized state.

20 . The method of claim 18 , further comprising a number of the cycles of the protocol so as to form and measurement of a Bell state, comprising:

applying a first number of the cycles of the protocol in combination with an initialization of the qubit so as to configure the register spins in a polarized state;

applying one or more of the pulses to the qubit to set the quantum state of the qubit;

applying a second number of the cycles of the protocol to the qubit so as to apply a first square root of swap gate entangling the qubit with the register so as to form a Bell state; and

applying one or more cycles of the protocol to the qubit so as to apply a second square root of swap gate interacting with the Bell state so as to perform a measurement of the Bell state.

Assignments (2)

Continuity (2)

References Cited (38)