We propose a frustration-free model for the Moore-Read quantum Hall state on sufficiently thin cylinders with circumferences $\lesssim 7$ magnetic lengths. While the Moore-Read Hamiltonian involves complicated long-range interactions between triplets of electrons in a Landau level, our effective model is a simpler one-dimensional chain of qubits with deformed Fredkin gates. We show that the ground state of the Fredkin model has high overlap with the Moore-Read wave function and accurately reproduces the latter's entanglement properties. Moreover, we demonstrate that the model captures the dynamical response of the Moore-Read state to a geometric quench, induced by suddenly changing the anisotropy of the system. We elucidate the underlying m...
Bilayer graphene exhibits a rich phase diagram in the quantum Hall regime, arising from a multitude ...
A 2D Fock-state lattice (FSL is constructed from the many-body states of two interacting two-mode qu...
Quantum simulation advantage over classical memory limitations would allow compact quantum circuits ...
Intermediate-scale quantum technologies provide new opportunities for scientific discovery, yet they...
We study the entanglement dynamics of thermofield double (TFD) states in integrable spin chains and ...
The emergence of a collective behavior in a many-body system is responsible of the quantum criticali...
We introduce an exactly solvable fermion chain that describes a ν=1/3 fractional quantum Hall (FQH) ...
The Moore-Read state is one the most well known non-Abelian fractional quantum Hall states. It suppo...
Inspired by current research on measurement-induced quantum phase transitions, we analyze the nonuni...
A complete understanding of the the ν = 5/2 fractional quantum hall effect (FQHE) continues to be am...
The quantum Hall effect occuring in two-dimensional electron gases was first explained by Laughlin, ...
We use the dynamical structure factors of the quantum Hall states at $\nu=1/3$ and $\nu=1/2$ in the ...
We introduce a quench of the geometry of Landau level orbitals as a probe of nonequilibrium dynamics...
We show that the model wave functions used to describe the fractional quantum Hall effect have exact...
We present a microscopic model for a singly charged quantum dot (QD) ensemble to reveal the origin o...
Bilayer graphene exhibits a rich phase diagram in the quantum Hall regime, arising from a multitude ...
A 2D Fock-state lattice (FSL is constructed from the many-body states of two interacting two-mode qu...
Quantum simulation advantage over classical memory limitations would allow compact quantum circuits ...
Intermediate-scale quantum technologies provide new opportunities for scientific discovery, yet they...
We study the entanglement dynamics of thermofield double (TFD) states in integrable spin chains and ...
The emergence of a collective behavior in a many-body system is responsible of the quantum criticali...
We introduce an exactly solvable fermion chain that describes a ν=1/3 fractional quantum Hall (FQH) ...
The Moore-Read state is one the most well known non-Abelian fractional quantum Hall states. It suppo...
Inspired by current research on measurement-induced quantum phase transitions, we analyze the nonuni...
A complete understanding of the the ν = 5/2 fractional quantum hall effect (FQHE) continues to be am...
The quantum Hall effect occuring in two-dimensional electron gases was first explained by Laughlin, ...
We use the dynamical structure factors of the quantum Hall states at $\nu=1/3$ and $\nu=1/2$ in the ...
We introduce a quench of the geometry of Landau level orbitals as a probe of nonequilibrium dynamics...
We show that the model wave functions used to describe the fractional quantum Hall effect have exact...
We present a microscopic model for a singly charged quantum dot (QD) ensemble to reveal the origin o...
Bilayer graphene exhibits a rich phase diagram in the quantum Hall regime, arising from a multitude ...
A 2D Fock-state lattice (FSL is constructed from the many-body states of two interacting two-mode qu...
Quantum simulation advantage over classical memory limitations would allow compact quantum circuits ...