We envisage many-body systems that can be described by quantum spin-chain Hamiltonians with a trivial separable eigenstate. For generic Hamiltonians, such a state represents a quantum scar. We show that, typically, a macroscopically-entangled state naturally grows after a single projective measurement of just one spin in the trivial eigenstate; moreover, we identify a condition under which what is growing is a "Schr\"odinger's cat state". Our analysis does not reveal any particular requirement for the entangled state to develop, provided that the trivial eigenstate does not minimise/maximise a local conservation law. We study two examples explicitly: systems described by generic Hamiltonians and a model that exhibits a $U(1)$ hidden symmetr...
Atypical eigenstates in the form of quantum scars and fragmentation of Hilbert space due to conserva...
Describing non-equilibrium properties of quantum many-body systems is challenging due to high entang...
Is the Schr\"odinger equation with the Hamiltonian $\widehat{H}=-i\hbar\frac{\partial\ }{\partial\ta...
We propose a class of non-integrable quantum spin chain models that exhibit quantum many-body scars ...
Highly excited eigenstates of quantum many-body systems are typically featureless thermal states. So...
The quantum state of Schroedinger's cat is usually incorrectly described as a superposition of "dead...
We study weak ergodicity breaking in a one-dimensional, nonintegrable spin-1 XY model. We construct ...
We provide a systematic approach for constructing approximate quantum many-body scars (QMBS) startin...
Recent experimental observation of weak ergodicity breaking in Rydberg atom quantum simulators has s...
We construct a family of three-body spin-1/2 Hamiltonians with a super-extensive set of infinitely l...
In systems governed by “chaotic” local Hamiltonians, we conjecture the universality of eigenstate en...
Consider a generic quantum spin chain that can be mapped to free quadratic fermions via Jordan-Wigne...
Quantum many-body scar states are many-body states with finite energy density in non-integrable mode...
We analyze the application of the history state formalism to quantum walks. The formalism allows one...
We prove that estimating the ground state energy of a translationally-invariant, nearest-neighbour H...
Atypical eigenstates in the form of quantum scars and fragmentation of Hilbert space due to conserva...
Describing non-equilibrium properties of quantum many-body systems is challenging due to high entang...
Is the Schr\"odinger equation with the Hamiltonian $\widehat{H}=-i\hbar\frac{\partial\ }{\partial\ta...
We propose a class of non-integrable quantum spin chain models that exhibit quantum many-body scars ...
Highly excited eigenstates of quantum many-body systems are typically featureless thermal states. So...
The quantum state of Schroedinger's cat is usually incorrectly described as a superposition of "dead...
We study weak ergodicity breaking in a one-dimensional, nonintegrable spin-1 XY model. We construct ...
We provide a systematic approach for constructing approximate quantum many-body scars (QMBS) startin...
Recent experimental observation of weak ergodicity breaking in Rydberg atom quantum simulators has s...
We construct a family of three-body spin-1/2 Hamiltonians with a super-extensive set of infinitely l...
In systems governed by “chaotic” local Hamiltonians, we conjecture the universality of eigenstate en...
Consider a generic quantum spin chain that can be mapped to free quadratic fermions via Jordan-Wigne...
Quantum many-body scar states are many-body states with finite energy density in non-integrable mode...
We analyze the application of the history state formalism to quantum walks. The formalism allows one...
We prove that estimating the ground state energy of a translationally-invariant, nearest-neighbour H...
Atypical eigenstates in the form of quantum scars and fragmentation of Hilbert space due to conserva...
Describing non-equilibrium properties of quantum many-body systems is challenging due to high entang...
Is the Schr\"odinger equation with the Hamiltonian $\widehat{H}=-i\hbar\frac{\partial\ }{\partial\ta...