We investigate the orthogonality catastrophe and quantum speed limit in the Creutz model for dynamical quantum phase transitions. We demonstrate that exact zeros of the Loschmidt echo can exist in finite-size systems for specific discrete values. We highlight the role of the zero-energy mode when analyzing quench dynamics near the critical point. We also examine the behavior of the time for the first exact zeros of the Loschmidt echo and the corresponding quantum speed limit time as the system size increases. While the bound is not tight, it can be attributed to the scaling properties of the band gap and energy variance with respect to system size. As such, we establish a relation between the orthogonality catastrophe and quantum speed limi...
The Loschmidt echo is a purely quantum-mechanical quantity whose determination for large quantum man...
Quantum speed limits such as the Mandelstam-Tamm or Margolus-Levitin bounds offer a quantitative for...
The minimal evolution time between two distinguishable states is of fundamental interest in quantum ...
The dynamical quantum phase transition is characterized by the emergence of nonanalytic behaviors in...
A remarkable feature of quantum many-body systems is the orthogonality catastrophe that describes th...
In this work we develop the theory of the Loschmidt echo and dynamical phase transitions in non-inte...
We show that non-Hermitian biorthogonal many-body phase transitions can be characterized by the enha...
Quantum speed limits (QSLs) provide an upper bound for the speed of evolution of quantum states in a...
Quantum critical states exhibit strong quantum fluctuations and are therefore highly susceptible to ...
We unveil the role of the long time average of Loschmidt echo in the characterization of nonequilibr...
Quantum coherence will undoubtedly play a fundamental role in understanding the dynamics of quantum ...
We uncover a novel dynamical quantum phase transition, using random matrix theory and its associated...
In most lattice models, the closing of a band gap typically occurs at high-symmetry points in the Br...
We present an alternative protocol allowing for the preparation of critical states that instead of s...
We study the slow quenching dynamics (characterized by an inverse rate τ−1) of a one-dimensional tra...
The Loschmidt echo is a purely quantum-mechanical quantity whose determination for large quantum man...
Quantum speed limits such as the Mandelstam-Tamm or Margolus-Levitin bounds offer a quantitative for...
The minimal evolution time between two distinguishable states is of fundamental interest in quantum ...
The dynamical quantum phase transition is characterized by the emergence of nonanalytic behaviors in...
A remarkable feature of quantum many-body systems is the orthogonality catastrophe that describes th...
In this work we develop the theory of the Loschmidt echo and dynamical phase transitions in non-inte...
We show that non-Hermitian biorthogonal many-body phase transitions can be characterized by the enha...
Quantum speed limits (QSLs) provide an upper bound for the speed of evolution of quantum states in a...
Quantum critical states exhibit strong quantum fluctuations and are therefore highly susceptible to ...
We unveil the role of the long time average of Loschmidt echo in the characterization of nonequilibr...
Quantum coherence will undoubtedly play a fundamental role in understanding the dynamics of quantum ...
We uncover a novel dynamical quantum phase transition, using random matrix theory and its associated...
In most lattice models, the closing of a band gap typically occurs at high-symmetry points in the Br...
We present an alternative protocol allowing for the preparation of critical states that instead of s...
We study the slow quenching dynamics (characterized by an inverse rate τ−1) of a one-dimensional tra...
The Loschmidt echo is a purely quantum-mechanical quantity whose determination for large quantum man...
Quantum speed limits such as the Mandelstam-Tamm or Margolus-Levitin bounds offer a quantitative for...
The minimal evolution time between two distinguishable states is of fundamental interest in quantum ...