#TopologicalOrder

2026-02-08

It seems like the basic building blocks of a topological quantum computer were demonstrated experimentally for the first time.

arxiv.org/abs/2601.20956

The promise of topological quantum computer – which would be resistant to errors because it would encode quantum information using trajectories of weird “quasiparticles” called anyons – is one of the main motivations why people investigate topological orders like fractional quantum Hall effect or spin liquids. The catch about this study is that, as far as I understand, it lacks the required stability, which arises from the fact that the topological order is exhibited by the ground state of the system (lowest energy), and the anyons are lowest excitations (lowest energies above the ground state). Here, as far as I understand, the topologically ordered state was created inside a quantum computer, with no reference to energy. Still, this is one step closer to realizing topological quantum computation. Also, the study uses quantum gates based both on anyon braiding – “winding” their trajectories around each other – and “fusion”, i.e. merging anyons with each other. I was not aware you can use fusion in this way.

#science #physics #quantum #CondensedMatter #CondMat #QuantumComputing #TopologicalOrder #anyons

2025-03-31

Fractional quantum Hall states in atom arrays

Our second approach to create a topological order in atom arrays is to focus on a different kind of topological order: fractional quantum Hall (FQH) states. These were first discovered in condensed matter. It is possible to confine electrons to move in two-dimensions only (such as in the 2D material graphene or in so-called metal-oxide-semiconductor transistors) and then put them in a strong perpendicular magnetic fields. The electrons then move in circles (so-called “cyclotron motion”), but since they are quantum objects, only some values of radius are allowed. Thus, the energy can only take certain fixed values (we call them “Landau levels”). There are however different possibilities of an electron having the same energy, because the center of the orbit can be located in different places – we say that Landau levels are “degenerate”. And when there is degeneracy, the interaction between electrons becomes very important. Without interactions, there are many possible ways of arranging electrons within a Landau level, all with the same energy. In the presence of interactions, some arrangements become preferred – and it turns out those correspond to topological orders known as the FQH states. Such systems host anyons which look like fractions of an electron – like somehow the electron split into several parts.

[1/2]

#Physics #science #TopologicalOrder #Quantum #QuantumOptics #CondensedMatter #CondMat #cond_mat #QuantumHall

On the left: a hexagonal array of atoms (red balls with small arrows arranged in the xy plane) in a magnetic field (big arrow in the z direction). On the right: the energy levels of each atom: black bar on the bottom denoting the ground state, dashed black line denoting the frequency of atomic transition, and two bars denoting excited states: red bar below the dashed line and blue bar above the dashed line. The distance between the dashed line and each of the bar is mu*B. Each of the excited states is connected with the ground state with double-sided arrow in respective colour, denoting the fact that it can absorb and emit circularly polarized light (red and blue correspond to opposite circular polarizations).The figure comes from the following paper: https://journals.aps.org/prl/abstract/10.1103/PhysRevLett.119.023603
2025-03-10

Spin liquids in Rydberg atom arrays in cavities

What is our proposal for the realization of spin liquid?

We consider an atom array held by optical tweezers and placed in an optical cavity. The cavity consists of two mirrors placed on the opposite sides of the system. The photons which normally would escape the system (at least some of them) will bounce back and forth between the mirrors. In such a configuration, the distance between atoms becomes irrelevant and the probability of an excitation hopping between any two atoms becomes the same.

The second ingredient is that the excited state of the atoms would be a Rydberg state – a very high-energy state where the electron is far away from the nucleus. The atoms in Rydberg states interact strongly by van der Waals forces. In our case it would mean that two excitations will have much higher energy when they are at nearest-neighboring atoms than if they are far away.

This setting seems much different from usual crystals. In the typical material, the electrons are much more likely to hop between nearest-neighboring atoms than far-away ones, while in our case they would be able hop arbitrarily far with the same probability. But it turns out that there is in equivalence between such “infinite-range hopping + Rydberg” model and the Heisenberg model, commonly used to describe magnets, including the frustrated ones.
[1/2]
#Physics #Quantum #TopologicalOrder #CondMat #CondensedMatter #QuantumOptics #Science

A tweezer array in a cavity. The cavity is the two mirrors on left and right trapping a yellow beam of light between them. Inside the cavity, there are several atoms arranged in a “star of David” pattern (a small instance of the frustrated kagome lattice). The atoms are held by optical tweezers (vertical red beams of light)
2025-02-21

#Microsoft has announced that they created topological qubits.

The perspective of creating such qubits is one of the main reasons why scientists are interested in topological orders. A topological qubit will be based on the operations of braiding anyons (see my post about anyons here: fediscience.org/@quinto/113284). Such operations will be naturally protected from noise, as the exact trajectory on which the anyons move does not matter. It only matters which anyon encircles which. Adding some random noise to the trajectory would not change that.

There are, however, some reasons to be skeptical about Microsoft's claims - see here: nature.com/articles/d41586-025

#QuantumComputing #Quantum #physics #TopologicalOrder #qubits

2025-01-27

Quantum simulation of topological orders

In the previous posts, I was talking a lot about complex quantum states that we aim to study in the QUINTO project: topological orders, in particular spin liquids. Now, let us see how quantum optics can help us in this endeavour.

Topological orders can be hard to find. Not all of them – one particular class, “fractional quantum Hall states”, can be created in the lab by applying very strong magnetic field to electrons confined in two dimensions. But others, such as spin liquids, remain elusive, even though scientists proposed some materials in which spin liquids might occur.

Moreover, with solid-state materials, we don’t usually have enough control to manipulate individual anyons as precisely as we would want (even though impressive experiments were performed with tiny anyon colliders and anyon interferometers in the quantum Hall systems).

An alternative is to assemble a quantum system – a “quantum simulator” from scratch, piece by piece, precisely controlling its parameters. For example, it is possible to “catch” a single atom with a laser beam – a so-called “optical tweezer”. The radiation pressure of the beam “traps” the atom in the point where the light is strongest, i.e. where the beam is focused. Such atoms can then be arranged in arrays resembling crystals.

[1/2]
#TopologicalOrder #Physics #Science #Quantum #QuantumSimulation #QuantumPhysics #QuantumOptics

A picture taken from the following article: G. Semeghini et al., “Probing topological spin liquids on a programmable quantum simulator”, “Science” 374, 1242-1247 (2021)

Left: a fluorescence image of atoms in the array of tweezers, superimposed over kagome lattice (a ruby lattice, where the atoms are located, is formed by the middle points of the bonds of kagome lattice).

Right: A snapshot of the spin liquid state. The atoms in Rydberg state are denoted by grey ellipses. After mapping to kagome lattice, these atoms can be understood as dimers occupying bonds of the kagome lattice (something analogous to the singlet bonds discussed earlier)

Middle: a diagram showing interaction  between the atoms, as well as the energy levels of an atom: a ground state, a Ryberg level and an arrow from the ground state to somewhere above the Rydberg level, denoting the laser light driving the transitions between levels.
2025-01-13

Anyons in spin liquids

To see how anyons can arise in topological orders, one can look again on the simplified picture of the Z2 spin liquid (see the previous post: fediscience.org/@quinto/113465). Anyons can be created on the top of the spin liquid by altering the singlet pattern.

First, we can break one singlet bond into two spins, one up and one down, which can move freely throughout the pattern by rearranging the singlets. The two spins can be thought of as (quasi)particles called spinons.

By the way, spinons can also be created by flipping a spin. In a spin liquid ground state, we have as many up spins as down spins, so all of them can be paired into singlets. But if we flip one of, say, down spins, we have *two* up spins that cannot be paired – two spinons. One flipped spin somehow turns into two quasiparticles. This is known as “fractionalization”.

Secondly, we can do something more complicated. We can draw a line intersecting some bonds. Then, in the sum over all singlet configurations, we put a plus if the line intersect an even number of singlets and minus if this number is odd. The ends of the line are quasiparticles called visons. It does not matter how we draw the line – it only matters where it starts and ends.
[1/2]
#physics #science #CondensedMatter #CondMat #TopologicalOrder #Anyons

Three pictures of a triangular lattice covered by singlet bonds (blue lines). In the first picture (“spinons”), two lattice sites are not connected by any singlet bonds, instead, free spins (blue arrows) are placed there. Two such configurations are shown and a plus sign is placed between them, and a “+…” on the right side, indicating that one should add up all such configurations.

In the second picture (“visons”), also two configurations are shown. Now, each site is connected to some singlet bond. A red line is drawn through the middles of some triangles. In the first configuration, the line does not cross any singlet bond. In the second configuration, it crosses one singlet bond, marked in red. There is a red minus sign in front of the second configuration and a “+…” on its right side, indicating that one should sum all configurations, but the ones where the line crosses an odd number of singlet bonds enter the sum with a minus sign.

The third picture (“braiding”) also consists of two parts. The first part shows a configuration with two visons (a red line through the middles of triangles) and two spinons located near each other (just created by destroying one singlet bond). One of the spinons will move on a path encircling one of the visons, shown in green. The second part shows the same configuration after the spinon moved along the path. The singlet bonds within the paths are rearranged, and one more singlet bond is crossing the red line.
2024-12-11

Yesterday Charlie-Ray Mann gave a talk as a part of the "Many-Body Quantum Optics" program at KITP. Charlie is a postdoc working in the same group as me. Part of presented work (2D numerics which is not directly referenced) was done by me within the QUINTO project. You can listen to the recording of the talk here: online.kitp.ucsb.edu/online/mb

#CondensedMatter #condMat #Cond_mat #TopologicalOrder #SpinLiquid #QuantumOptics #Optics #Physics #ColdAtoms #Science

First slide of the talk. Title: "Emergence of Quantum Spin Liquids from Atom-Cavity Interactions", author: Charlie-Ray Mann. Below a schematic picture of an array of atoms held by optical tweezers (vertical laser beams) in an optical cavity (two mirrors on the left and right, and the light confined by the two mirrors). There are circles around two neighboring atoms, signifying the Rydberg blockade interaction. The slide contains also the logo of ICFO (the institute in Barcelona where our group works, as well as the logo of Marie Skłodowska-Curie Action, from which the research was financed).
2024-11-11

Spin liquid

As an example of how a topological order can look like, one can look at simplified picture of so-called Z2 spin liquid. This type of topological order is postulated to occur in some “frustrated magnets”.
#physics #TopologicalOrder #science #CondensedMatter #CondMat
[1/6]

The picture has three parts. The first explain frustration. There is a triangle on whose corners there are spins (arrows). The first spin points up, the second points down. The third is replaced by a question mark because it cannot “decide” if it points up or down.

The second part presents the singlet state, which is written as: arrow up, arrow down minus arrow down, arrow up. 

The third part presents the spin liquid. It shows a triangular lattice. On some of its “bonds” there is a blue line, which represents a singlet state. Then, next to it, there is another instance of triangular lattice with different arrangement of blue lines. There is a plus sign between them and three dots on the right, signifying that many such arrangements are possible and that the spin liquid consists of a sum of all of them.
2024-08-06

Hi!
We are conducting a research project on the intersection of quantum optics and condensed matter. We study what happens if an ordered array of atoms absorbs many photons, thus becoming a complex system of many interacting particles. We want to find and exploit analogies between such systems and so-called topological orders, and build a “bridge” between the two fields of physics.
#introduction #Physics #CondensedMatter #CondMat #QuantumOptics #TopologicalOrder #ManyBody #ColdAtoms

[1/2]

Client Info

Server: https://mastodon.social
Version: 2025.07
Repository: https://github.com/cyevgeniy/lmst