Complex-Valued Hough Transforms for Circles.
... every point, we look for the wavelet of maximum magnitude Vjx0 (x0 ) = maxj Vj (x0 ) (j is the orientation index), and use only the points x0 such that Vjx0 (x0 ) > Γ (an empirically defined threshold). Let m(x0 ) = Vjx0 (x0 ), and τx0 be the unit vector perpendicular to the direction of Vjx0 . In t ...
... every point, we look for the wavelet of maximum magnitude Vjx0 (x0 ) = maxj Vj (x0 ) (j is the orientation index), and use only the points x0 such that Vjx0 (x0 ) > Γ (an empirically defined threshold). Let m(x0 ) = Vjx0 (x0 ), and τx0 be the unit vector perpendicular to the direction of Vjx0 . In t ...
![arXiv:1606.09570v1 [physics.gen-ph] 29 Jun 2016](http://s1.studyres.com/store/data/017089913_1-b139408de069e5e90b03e592a6592573-300x300.png)
arXiv:1606.09570v1 [physics.gen-ph] 29 Jun 2016
... After it was established experimentally that baryons contain three quarks there were intense efforts to identify a satisfactory taxonomy for a variety of baryons. This goal was satisfactorily achieved in the seventies [1, 2], by employing electric charge as well as the concepts of isospin and strang ...
... After it was established experimentally that baryons contain three quarks there were intense efforts to identify a satisfactory taxonomy for a variety of baryons. This goal was satisfactorily achieved in the seventies [1, 2], by employing electric charge as well as the concepts of isospin and strang ...
wu.pdf
... space-time noncommutativity. In this talk I am restricted only to the case of Eq. (1).) There are two ways of interpreting these commutation relations. The first way is to interpret xi as operators in a Hilbert space satisfying Eq. (1). In this interpretation, the noncommutative space can be mathemat ...
... space-time noncommutativity. In this talk I am restricted only to the case of Eq. (1).) There are two ways of interpreting these commutation relations. The first way is to interpret xi as operators in a Hilbert space satisfying Eq. (1). In this interpretation, the noncommutative space can be mathemat ...
1 Time evolution of a spin an an external magnetic field and Spin
... where to simplify notation I set δ = 21 − φΦ0 . The boundary condition of the problem is that at t = 0 the system is in the spin down effective state (or m = 0 state in the original picture) and we are asked to evaluate the probability that it appears in the spin up state after some time T . This sp ...
... where to simplify notation I set δ = 21 − φΦ0 . The boundary condition of the problem is that at t = 0 the system is in the spin down effective state (or m = 0 state in the original picture) and we are asked to evaluate the probability that it appears in the spin up state after some time T . This sp ...
Abstract book - Nonequilibrim Phenomena in Quantum Systems
... the realization of novel states of matter. In this talk, we will discuss how it can lead to the generation of time-evolving states that are eigenstates of emergent local Hamiltonians, not trivially related to the ones dictating the time evolution. We study geometric quenches in interacting fermionic ...
... the realization of novel states of matter. In this talk, we will discuss how it can lead to the generation of time-evolving states that are eigenstates of emergent local Hamiltonians, not trivially related to the ones dictating the time evolution. We study geometric quenches in interacting fermionic ...
... nearby « @4,5#. The other generalization has been to incorporate effects from orbits that start at a node of the wave function and therefore should have zero strength in R(Ŝ) ~in the simple implementation of closed-orbit theory! @6#. Our present results are for m51 and 2 spectra in H, K, and Cs; m\ ...
