Granted Patent B2

US 12,475,402 · App. 18/246,673 · Granted Nov 18, 2025

Inventors: Théau Peronnin (Paris, FR); Benjamin Huard (Lyons, FR); Sébastien Jezouin (Paris, FR); Antoine Marquet (Lyons, FR)

Assignees: CENTRE NATIONAL DE LA RECHERCHE SCIENTIFIQUE (CNRS); ECOLE NORMALE SUPERIEURE DE LYON; UNIVERSITE CLAUDE BERNARD LYON 1

G06N10/70G06N10/40

Abstract

Claims (31)

1 . A system ( 200 ) for autonomous stabilization of quantum states comprising:

a quantum harmonic oscillator ( 202 ) configured to carry information encoded in states of the oscillator having a predetermined parity of a number of bosons comprised in the harmonic oscillator ( 202 ),

an auxiliary device ( 201 ) configured to be in a ground state |g> or in an excited state |f> among a plurality of excited states, the device ( 201 ) being dispersively coupled to the oscillator ( 202 ), so that a frequency difference between the ground state |g> and the excited state |f> depends linearly on a frequency shift χ and on the number of bosons,

a dissipator ( 203 ) configured to switch from an excited state |1> to a ground state |0>,

an exciter ( 204 ) configured to generate first ( 205 , 405 ) and second ( 206 , 406 ) frequency combs, intended to be sent to at least one of the quantum harmonic oscillator ( 202 ), the auxiliary device ( 201 ) and the dissipator ( 203 ) so as to add a boson in the harmonic oscillator ( 202 ) if the number of bosons does not have the predetermined parity, characterized in that a first frequency difference separating two successive lines of the first frequency comb ( 205 , 405 ) is equal to twice the frequency shift χ and is equal to twice a second frequency difference separating two successive lines of the second comb ( 206 , 406 ).

2 . The system according to claim 1 , wherein the first and second combs have peaks in the time domain, the peaks of the first comb being time-shifted relative to the peaks of the second comb.

3 . The system according to claim 1 or 2 , further configured to be, for each integer k of a set of integers, in:

a first level ( 401 ) defined by a first number of bosons equal to the integer k, the ground state |g> and the ground state |0>,

a second level ( 402 ) defined by a second number of bosons equal to the integer k+1, the excited state |g> and the ground state |0>,

a third level ( 403 ) in which the auxiliary device is in the excited state |f> and the dissipator is in the stable state |0>,

a fourth level ( 404 ) in which the auxiliary device is in the ground state |g> and the dissipator is in the excited state |1>, the exciter ( 204 ) being configured to couple, for each integer k, the first, third and fourth levels if the integer k does not have the predetermined parity, so as to switch the system from the first level ( 401 ) to the second level ( 402 ), the exciter ( 204 ) being configured to generate the first and second frequency combs so that, for each integer k:

the first comb ( 405 ) comprises a first line if the integer k does not have the predetermined parity, the first line having a frequency equal to a transition frequency between the first and third levels, and

the second comb ( 406 ) comprises a second line having a frequency equal to a transition frequency between the third and fourth levels.

4 . The system according to claim 3 , wherein the harmonic oscillator ( 202 ) comprises the second number of bosons equal to the integer k+1 in the fourth level ( 402 ).

5 . The system according to claim 3 , wherein the information is encoded in states of the oscillator corresponding to a number of bosons comprised between a floor integer k min having the predetermined parity and a ceiling integer k max having the predetermined parity, the set of integers being equal to the integers included between the integers k min −1 and k max −1.

6 . The system according to claim 1 , wherein the quantum harmonic oscillator ( 202 ) is a first superconducting microwave resonator, the auxiliary system ( 201 ) is a transmon, the dissipator ( 203 ) is a second superconducting microwave resonator having a quality factor lower than a quality factor of the first superconducting microwave resonator.

7 . The system according to claim 1 , wherein an amplitude of the lines of the first frequency comb and of the second frequency comb is characterized by a coupling frequency, the coupling frequency being lower than the quarter of the second frequency difference.

8 . A method for autonomous stabilization of quantum states comprising the following steps:

encoding information in states of a quantum harmonic oscillator, the states having a predetermined parity of a number of bosons comprised in the harmonic oscillator,

dispersively coupling the harmonic oscillator to an auxiliary device, so that a frequency difference between a ground state |g> of the auxiliary device and an excited state |f> of the auxiliary device depends linearly on a frequency shift χ and the number of bosons,

coupling the auxiliary device to a dissipator configured to switch from an excited state |1> to a ground state |0>,

generating first and second frequency combs, a first frequency difference separating two successive lines of the first frequency comb being equal to twice the frequency shift χ and equal to twice a second frequency difference separating two successive lines of the second comb, and

sending the first and second frequency combs to at least one amongst the quantum harmonic oscillator, the auxiliary device and the dissipator so as to add a boson in the harmonic oscillator if the number of bosons does not have the predetermined parity.

9 . The method according to claim 8 , further comprising an optimization of the amplitude of the lines of the first and second frequency combs, the amplitude of the lines being characterized by a coupling frequency, comprising the following steps:

selecting a coupling frequency value lower than the quarter of the second frequency difference,

measuring a lifetime of the states having a number of bosons of the predetermined parity, and

modifying the value of the coupling frequency based on the lifetime measured according to an optimization algorithm of the lifetime so as to identify an optimal value of the coupling frequency corresponding to a maximum of the lifetime.

10 . The method according to claim 8 , further comprising an optimization of a de-energization rate γ dis equal to the probability of switching from the level |1> into the level |0> per unit of time, comprising the following steps:

selecting a value of the de-energization rate lower than the second frequency difference,

measuring a lifetime of the states having a number of bosons of the predetermined parity, and

modifying the value of the de-energization rate based on the lifetime measured according to an optimization algorithm of the lifetime so as to identify an optimal value of the de-energization rate corresponding to a maximum of the lifetime.

Assignments (3)

Priority Claims (1)

Continuity (1)

References Cited (9)