Granted Patent B2

US 12,626,833 · App. 18/320,708 · Granted May 12, 2026

Inventors: Mikhail D. Lukin (Cambridge, MA); Vladan Vuletic (Cambridge, MA); Markus Greiner (Cambridge, MA); Ruben Verresen (Cambridge, MA); Ashvin Vishwanath (Cambridge, MA); Alexander Keesling Contreras (Cambridge, MA); Harry Jay Levine (Cambridge, MA); Giulia Semeghini (Cambridge, MA); Tout Taotao Wang (Cambridge, MA); Ahmed Omran (Cambridge, MA); Dolev Bluvstein (Cambridge, MA); Sepehr Ebadi (Cambridge, MA)

Assignees: President and Fellows of Harvard College; Massachusetts Institute of Technology

G21K1/003G06N10/20G06N10/40G06N10/70

Abstract

Claims (132)

1 . A device, comprising:

a two-dimensional array of particles,

each particle disposed at a vertex of a ruby lattice having a parameter ρ greater than

1

2

;

each particle having a first state and an excited state;

each particle that belongs to at least three unit cells of the ruby lattice having a blockade radius, when in the excited state, sufficient to form a blockade of each of at least six nearest neighboring particles in the ruby lattice from transitioning from its first state to its excited state,

and wherein the two-dimensional array has at least one outer edge configured to be in a first boundary condition.

2 . The device of claim 1 , wherein each particle is an atom, an ion, or a molecule.

3 . The device of claim 1 , wherein the blockade is a dipole blockade.

4 . The device of claim 1 , wherein the blockade is a Rydberg blockade.

5 . The device of claim 1 wherein each particle is an atom, the first state is ground state, and the blockade is a Rydberg blockade.

6 . The device of claim 1 , wherein the two-dimensional array comprises at least a first outer edge and a third outer edge, each being in the first boundary condition, and at least a second outer edge and a fourth outer edge, each being in a second boundary condition, different from the first boundary condition.

7 . The device of claim 1 , wherein the two-dimensional array has a plurality of outer edges, each outer edge being either in the first boundary condition or a second boundary condition, each outer edge being in a different boundary condition than any adjacent outer edge.

8 . The device of claim 6 , wherein the outer edges configured to be in the first boundary condition are e-condensed, and the outer edges configured to be in the second boundary condition are m-condensed.

9 . The device of claim 7 , wherein the two-dimensional array comprises at least one interior edge.

10 . The device of claim 9 , wherein each vertex enclosed by the at least one interior edge is not particle-occupied.

11 . The device of claim 10 , wherein the at least one interior edge is at a same boundary condition as at least one outer edge of the plurality of outer edges.

12 . The device of claim 9 , wherein the at least one interior edge encloses at least four vertices.

13 . The device of claim 9 , wherein the at least one interior edge encloses particle-occupied vertices.

14 . The device of claim 13 , wherein the at least one interior edge is in the first boundary condition, different from at least one outer edge of the plurality of outer edges.

15 . The device of claim 9 , wherein the two-dimensional array has a plurality of interior edges, each interior edge enclosing a corresponding plurality of vertices, each of which is not particle-occupied.

16 . The device of claim 9 , wherein the two-dimensional array has a plurality of interior edges, each interior edge enclosing a corresponding plurality of vertices, wherein at least one enclosed vertex is particle-occupied.

17 . The device of claim 16 , wherein an interior edge enclosing the at least one enclosed vertex that is particle-occupied is at a boundary condition different from at least one outer edge of the plurality of outer edges.

18 . The device of claim 17 , wherein edges configured to be at different boundary conditions are selected from e-condensed or m-condensed edges.

19 . The device of claim 1 , wherein the two-dimensional array comprises at least 96 particles.

20 . The device of claim 1 , wherein the two-dimensional array comprises at least 200 particles.

21 . A system comprising:

a confinement system for arranging particles in a two-dimensional array, wherein:

each particle is disposed at a vertex of a ruby lattice;

each particle has a first state and an excited state;

each particle that belongs to at least three unit cells of the ruby lattice has a blockade radius, when in the excited state, sufficient to blockade each of at least six nearest neighboring particles in the ruby lattice from transitioning from its first state to its excited state, and wherein two-dimensional the array has at least one outer edge configured to be at a first boundary condition;

the confinement system comprising:

a laser source arranged to create a plurality of confinement regions;

a source of an atom cloud, the atom cloud capable of being positioned to at least partially overlap with the plurality of confinement regions; and

an excitation source for exciting at least some of the particles from the first state to the excited state.

22 . The system of claim 21 , wherein the particles are atoms, and wherein the excitation source is configured to excite at least some of the atoms into a Rydberg state.

23 . The system of claim 21 , wherein the two-dimensional array comprises at least 96 particles.

24 . The system of claim 21 , wherein the two-dimensional array comprises at least 200 particles.

25 . A method of making a 2 Quantum Spin Liquid ( 2 QSL), comprising:

arranging a two-dimensional array of particles, wherein:

each particle is disposed at a vertex of a ruby lattice having a parameter ρ greater than

1

2

;

each particle has a first state and an excited state;

the two-dimensional array has at least one outer edge;

exciting about 25% of the particles into the excited state, thereby causing each particle in the excited state that belongs to at least three unit cells of the ruby lattice to have a blockade radius sufficient to blockade at least six nearest neighboring particles in the ruby lattice; and

optionally, imposing a first boundary condition on the at least one outer edge.

26 . The method of claim 25 , wherein the particles are atoms and the excited state is a Rydberg state.

27 . A method of encoding a topological qubit in a 2 Quantum Spin Liquid ( 2 QSL), comprising:

preparing a 2 QSL according to the method of claim 25 , wherein the two-dimensional array comprises at least a first outer edge, a second outer edge, a third outer edge, and a fourth outer edge;

imposing a first boundary condition on the first and third outer edges and imposing a second boundary condition on the second and fourth outer edges.

28 . The method of claim 27 , wherein the two-dimensional array has a plurality of outer edges, the method further comprising imposing either the first boundary condition or the second boundary condition on each outer edge, each outer edge having a different boundary condition than any adjacent outer edge.

29 . The method of claim 27 , wherein the outer edges configured to be in the first boundary condition are e-condensed, and the outer edges configured to be in the second boundary condition are m-condensed.

30 . A method of encoding a topological qubit in a 2 Quantum Spin Liquid ( 2 QSL), comprising:

preparing a 2 QSL according to the method of claim 25 , wherein the two-dimensional array comprises at least one interior edge.

31 . The method of claim 30 , wherein each vertex enclosed by the at least one interior edge is not particle-occupied.

32 . The method of claim 31 , wherein the at least one interior edge encloses at least four vertices.

33 . The method of claim 30 , wherein the at least one interior edge encloses particle-occupied vertices.

34 . The method of claim 33 , further comprising imposing on the at least one interior edge a boundary condition that is different from the boundary condition of the at least one outer edge.

35 . The method of claim 33 , further comprising imposing on the at least one interior edge a boundary condition that is a same boundary condition as that of the at least one outer edge.

36 . The method of claim 30 , wherein the two-dimensional array has a plurality of interior edges, each interior edge enclosing a corresponding plurality of vertices, wherein at least one enclosed vertex is particle-occupied.

37 . The method of claim 36 , further comprising imposing a boundary condition on an interior edge of the plurality of interior edges and enclosing the at least one particle-occupied vertex that is different from the boundary condition of the at least one outer edge.

38 . The method of claim 37 , wherein the interior edge configured to be at a different boundary condition is selected from e-condensed or m-condensed edges.

39 . A method of reading a state of a topological qubit encoded in a 2 Quantum Spin Liquid ( 2 QSL), the method comprising:

receiving an indication of a state of each particle of a two-dimensional array of particles,

each particle disposed at a vertex of a ruby lattice;

each particle having a first state and an excited state;

each particle that belongs to at least three unit cells of the ruby lattice having a blockade radius, when in the excited state, sufficient to blockade each of at least six nearest neighboring particles in the ruby lattice from transitioning from its first state to its excited state,

and wherein the two-dimensional array has a plurality of outer edges, each outer edge being either in a first boundary condition or in a second boundary condition, each outer edge being in a different boundary condition than any adjacent outer edge;

determining a first path through the two-dimensional array from a first outer edge of the plurality of outer edges having the first boundary condition to a second outer edge of the plurality of outer edges having the first boundary condition via a first plurality of vertices of the ruby lattice having thereat a first plurality of particles;

assigning a first value to the first path based on the state of each of the first plurality of particles;

based on the first value, determining the state of a first topological qubit.

40 . The method of claim 39 , wherein, prior to determining the first path, a basis rotation is applied to the first topological qubit.

41 . The method of claim 39 , further comprising

determining a second path through the two-dimensional array from the first outer edge of the plurality of outer edges to the second outer edge of the plurality of outer edges via a second plurality of vertices of the ruby lattice having thereat a second plurality of particles;

assigning a second value to the second path based on the state of each of the second plurality of particles; and

based on the first and second values, determining the state of the first topological qubit.

42 . The method of claim 41 , further comprising:

determining a third path through the two-dimensional array from the first outer edge of the plurality of outer edges to a third outer edge of the plurality of outer edges having the first boundary condition, via a third plurality of vertices of the ruby lattice having thereat a third plurality of particles;

assigning a third value to the third path based on the state of each of the third plurality of particles; and

based on the third value, determining the state of a second topological qubit.

43 . A method of reading a state of a topological qubit encoded in a 2 Quantum Spin Liquid ( 2 QSL), the method comprising:

receiving an indication of a state of each particle of a two-dimensional array of particles,

each particle disposed at a vertex of a ruby lattice;

each particle having a first state, and an excited state;

each particle that belongs to at least three unit cells of the ruby lattice having a blockade radius, when in the excited state, sufficient to blockade each of at least six nearest neighboring particles in the ruby lattice from transitioning from its first state to its excited state,

and wherein the two-dimensional array comprises at least one outer edge and at least one interior edge;

determining a first path through the two-dimensional array from the at least one interior edge to the at least one outer edge via a first plurality of vertices of the ruby lattice having thereat a first plurality of particles;

assigning a first value to the first path based on the state of each of the first plurality of particles;

based on the first value, determining the state of a first topological qubit.

44 . The method of claim 43 , further comprising:

determining a second path through the two-dimensional array from the at least one interior edge to the at least one outer edge via a second plurality of vertices of the ruby lattice having thereat a second plurality of particles;

assigning a second value to the first path based on the state of each of the second plurality of particles;

based on the first and second values, determining the state of the first topological qubit.

45 . The method of claim 43 , wherein the two-dimensional array has at least a second interior edge, the method further comprising:

determining a third path through the two-dimensional array from the second interior edge to the at least one outer edge via a third plurality of vertices of the ruby lattice having thereat a third plurality of particles;

assigning a third value to the third path based on the state of each of the third plurality of particles;

based on the third value, determining the state of a second topological qubit.

46 . The method of claim 39 , wherein determining the first path comprises:

assembling the path piecewise from a plurality of segments, each segment extending between two vertices in the ruby lattice wherein each segment either:

extends between two vertices in a triangular portion of a unit cell of the ruby lattice, or

extends between two vertices in different unit cells of the ruby lattice without crossing any unit cells of the ruby lattice.

47 . The method of claim 39 , wherein determining the first path comprises:

assembling the first path piecewise from a plurality of segments, each segment extending between two vertices in the ruby lattice wherein each segment:

extends between two vertices in a quadrilateral portion of a unit cell of the ruby lattice.

48 . A method of operating on a topological qubit, comprising:

preparing a topological qubit according to the method of claim 27 , wherein the first boundary condition is an e-boundary condition;

creating a first and a second e-anyon in the two-dimensional array;

removing the first e-anyon from the two-dimensional array via the first outer edge and removing the second e-anyon from the two-dimensional array via the third outer edge.

49 . A method of operating on a topological qubit, comprising:

preparing a topological qubit according to the method of claim 30 ,

creating a first and a second e-anyon in the two-dimensional array;

pinning the first e-anyon; and

moving the second e-anyon along a circular path circumscribing the at least one interior edge and having an end point at a position of the first e-anyon, thereby destroying the first and the second e-anyons.

50 . A method of encoding a first and a second topological qubit in a 2 Quantum Spin Liquid ( 2 QSL), comprising:

preparing a 2 QSL according to the method of claim 25 , wherein

the two-dimensional array comprises a first interior edge and a second interior edge, the first interior edge having a first boundary condition and the second interior edge having a second boundary condition different from the first boundary condition, the first topological qubit corresponding to the first interior edge and the second topological qubit corresponding to the second interior edge,

the two-dimensional array comprises a first outer edge, the first outer edge having the first boundary condition,

the two-dimensional array comprises an additional edge, the additional edge having the second boundary condition and being either an interior edge or an outer edge.

51 . A method of operating on a first and second topological qubit, comprising: encoding the first and second topological qubit according to the method of claim 50 ;

moving the first interior edge along a closed continuous path circumscribing the second interior edge.

52 . The method of claim 50 , wherein either (i) the first boundary condition is m-condensed and the second boundary condition is e-condensed, or (ii) the first boundary condition is e-condensed and the second boundary condition is m-condensed.

53 . The method of claim 43 , wherein determining the first path comprises:

assembling the first path piecewise from a plurality of segments, each segment extending between two vertices in the ruby lattice wherein each segment either:

extends between two vertices in a triangular portion of a unit cell of the ruby lattice, or

extends between two vertices in different unit cells of the ruby lattice without crossing any unit cells of the ruby lattice.

54 . The method of claim 43 , wherein determining the first path comprises:

assembling the first path piecewise from a plurality of segments, each segment extending between two vertices in the ruby lattice wherein each segment:

extends between two vertices in a quadrilateral portion of a unit cell of the ruby lattice.

Assignments (2)

Continuity (4)

References Cited (206)