QuRE: The Quantum Resource Estimator Toolbox
... physical error rate, the resource requirements of topological QECCs increase much more moderately than those of concatenated codes. Consequently, for a typical real-world sized quantum algorithm, the surface code requires fewer resources than the Steane code when the physical error rate is above app ...
... physical error rate, the resource requirements of topological QECCs increase much more moderately than those of concatenated codes. Consequently, for a typical real-world sized quantum algorithm, the surface code requires fewer resources than the Steane code when the physical error rate is above app ...
Calculation of the nucleon axial charge in lattice QCD
... formulation of quarks in lattice QCD with an exact chiral symmetry even on the lattice. ...
... formulation of quarks in lattice QCD with an exact chiral symmetry even on the lattice. ...
Probability, Expectation Value and Uncertainty
... the operator represents all the possible results that could be obtained if the associated physical observable were to be measured. The eigenstates of the operator are the states of the system for which the associated eigenvalue would be, with 100% certainty, the measured result, if the observable we ...
... the operator represents all the possible results that could be obtained if the associated physical observable were to be measured. The eigenstates of the operator are the states of the system for which the associated eigenvalue would be, with 100% certainty, the measured result, if the observable we ...
Isolated-core excitations in strong electric fields. I. Theory F. Robicheaux
... ⫽ 具 ⌽ i 兩 D 兩 ⌽ i ⬘ 典 . The approximations in this equation are that the effect from the dipole operator on the Rydberg electron is not included and the projection of A onto B is only for the region outside of the core. The error in the dipole matrix element from each of these approximations will be ...
... ⫽ 具 ⌽ i 兩 D 兩 ⌽ i ⬘ 典 . The approximations in this equation are that the effect from the dipole operator on the Rydberg electron is not included and the projection of A onto B is only for the region outside of the core. The error in the dipole matrix element from each of these approximations will be ...
How Quantum Theory Helps us Explain
... it is assumed that any cause of an instance of the phenomenon bears an asymmetric relation of causal influence to it. Lewis (1986) argued that to explain a particular event is to provide information about its causal history: the event would be expected by anyone who had enough such information ahead ...
... it is assumed that any cause of an instance of the phenomenon bears an asymmetric relation of causal influence to it. Lewis (1986) argued that to explain a particular event is to provide information about its causal history: the event would be expected by anyone who had enough such information ahead ...
A Bell Theorem Without Inequalities for Two
... reality, it is a very problematical state, since two independently produced particles that have never met are suddenly thrown into an entanglement, even though they have no shared history. We will show that the situation is strange enough so that one cannot reproduce the quantum perfect correlations ...
... reality, it is a very problematical state, since two independently produced particles that have never met are suddenly thrown into an entanglement, even though they have no shared history. We will show that the situation is strange enough so that one cannot reproduce the quantum perfect correlations ...
Reflection of matter waves in potential structures
... rapidly, the different modes will not have sufficient time to experience adiabatic following. As a result, the wave packet is left in a coherent superposition where the expansion coefficients are given by projection on the new eigenstates. In the case of a sudden widening of the potential, causing t ...
... rapidly, the different modes will not have sufficient time to experience adiabatic following. As a result, the wave packet is left in a coherent superposition where the expansion coefficients are given by projection on the new eigenstates. In the case of a sudden widening of the potential, causing t ...
Photoemission studies of quantum well states in thin films
... convenient platform for experimenting with many-body effects. This paper will focus on quantum well effects in thin ®lms. A simple beginner's model for electronic motion perpendicular to the ®lm surface is that of a free electron con®ned in a one-dimensional box. Although this is a very crude model, ...
... convenient platform for experimenting with many-body effects. This paper will focus on quantum well effects in thin ®lms. A simple beginner's model for electronic motion perpendicular to the ®lm surface is that of a free electron con®ned in a one-dimensional box. Although this is a very crude model, ...
