
Rapid readout of a register of qubits using open loop... Joshua Combes , Aaron Denney , and Howard M. Wiseman
... FIG. 2: To gain some intuition about the measurement process in a register we illustrate the effect of measurement on the eigenvalues of ρ by plotting them on a Hamming cube. A Hamming cube is a way of depicting the distance between n bit binary strings. The distance between two strings is given by ...
... FIG. 2: To gain some intuition about the measurement process in a register we illustrate the effect of measurement on the eigenvalues of ρ by plotting them on a Hamming cube. A Hamming cube is a way of depicting the distance between n bit binary strings. The distance between two strings is given by ...
Lecture Notes for the 2014 HEP Summer School for Experimental
... which we recognise as the total energy of the system. From the definition of the Hamiltonian one may derive (problem 1.1) ∂H ∂H = −ṗi , = ẋi , ∂qi ∂pi which constitute Hamilton’s equations. These are useful in proving the relation between symmetries and conserved quantities. For example, one readi ...
... which we recognise as the total energy of the system. From the definition of the Hamiltonian one may derive (problem 1.1) ∂H ∂H = −ṗi , = ẋi , ∂qi ∂pi which constitute Hamilton’s equations. These are useful in proving the relation between symmetries and conserved quantities. For example, one readi ...
1 The Fourier Transform
... This is the time-dependent Schrödinger equation for a free particle, i.e., where V = 0, written in the position representation. This shows that plane waves exp(ikx − iωt) are eigenfunctions of the free particle Hamiltonian. The probability of finding a particle at position x is proportional to the ...
... This is the time-dependent Schrödinger equation for a free particle, i.e., where V = 0, written in the position representation. This shows that plane waves exp(ikx − iωt) are eigenfunctions of the free particle Hamiltonian. The probability of finding a particle at position x is proportional to the ...
Classical continuum theory of the dipole-forbidden collective excitations in quantum... W. L. Schaich M. R. Geller and G. Vignale
... grating as a flat 2D conductor whose ~local! resistivity varies periodically in the y direction. To enhance the signal strength and simplify the analysis, we assume that the single wire studied before has been periodically repeated in the y direction with the same period d.2W that the grating has. T ...
... grating as a flat 2D conductor whose ~local! resistivity varies periodically in the y direction. To enhance the signal strength and simplify the analysis, we assume that the single wire studied before has been periodically repeated in the y direction with the same period d.2W that the grating has. T ...
arXiv:math/0609622v2 [math.CO] 9 Jul 2007
... graph such that a 180 degree rotation R2 about the origin maps G to itself and the length of a path between v and R2 (v) is even. In particular, if the graph is embedded in a square grid, if you rotate the graph by 180 degrees, you get the same graph back, AND the center of rotation is not the cente ...
... graph such that a 180 degree rotation R2 about the origin maps G to itself and the length of a path between v and R2 (v) is even. In particular, if the graph is embedded in a square grid, if you rotate the graph by 180 degrees, you get the same graph back, AND the center of rotation is not the cente ...
Electronic Structure According to the Orbital Approximation
... Atomic orbitals are classified according to so-called “good” quantum numbers of stationary observables, measurable properties of the system that are mathematically expressed as Hermitian operators. Probability densities corresponding to the states of good quantum numbers are independent of time [2]. ...
... Atomic orbitals are classified according to so-called “good” quantum numbers of stationary observables, measurable properties of the system that are mathematically expressed as Hermitian operators. Probability densities corresponding to the states of good quantum numbers are independent of time [2]. ...
Limits of time in cosmology
... or 2) rudiments (cores) of clocks with a well-defined duration should, in principle, be present (time-clock relation). Clearly, the first possibility is not an option in the very early universe where no actual clocks, let alone observers and measurements, are available. As we shall see below, the vi ...
... or 2) rudiments (cores) of clocks with a well-defined duration should, in principle, be present (time-clock relation). Clearly, the first possibility is not an option in the very early universe where no actual clocks, let alone observers and measurements, are available. As we shall see below, the vi ...