"Veil of Hadronization": Pion Entropy & PSD at RHIC
... 1. The source-averaged pion phase space density f is very high, in the low momentum region roughly 2 that observed at the CERN SPS for Pb+Pb at Snn=17 GeV. 2. The pion entropy per particle Sp/Np is very low, implying a significant pion chemical potential (p~63 MeV) at freeze out. 3. For central ...
... 1. The source-averaged pion phase space density f is very high, in the low momentum region roughly 2 that observed at the CERN SPS for Pb+Pb at Snn=17 GeV. 2. The pion entropy per particle Sp/Np is very low, implying a significant pion chemical potential (p~63 MeV) at freeze out. 3. For central ...
Testing the Dimension of Hilbert Spaces
... scenario. When dealing with fundamental issues, for instance, it can be relevant to estimate the dimension of a quantum system without any distinction between classical and quantum resources. The motivation is that if nature is indeed described by quantum theory, classical degrees of freedom have al ...
... scenario. When dealing with fundamental issues, for instance, it can be relevant to estimate the dimension of a quantum system without any distinction between classical and quantum resources. The motivation is that if nature is indeed described by quantum theory, classical degrees of freedom have al ...
quantum algorithms - Computer Engineering
... In our usual computers, a bit is either 0 or 1 at a particular time. As a direct consequence of this, a group (register) of n bits can contain only one of 2n different numbers at a given time. A quantum bit (qubit), on the other hand, can be in a weighted combination (superposition) of both 0 and 1 ...
... In our usual computers, a bit is either 0 or 1 at a particular time. As a direct consequence of this, a group (register) of n bits can contain only one of 2n different numbers at a given time. A quantum bit (qubit), on the other hand, can be in a weighted combination (superposition) of both 0 and 1 ...
An Introduction to Quantum Computation
... These two states are important in their own right. We denote them as |+i and |−i, respectively. For later use, we note that if we apply a Hadamard gate again, we will return to our original qubit. That is, H|+i = 0, and H|−i = 1. Notice that these two states have identical probabilities but differe ...
... These two states are important in their own right. We denote them as |+i and |−i, respectively. For later use, we note that if we apply a Hadamard gate again, we will return to our original qubit. That is, H|+i = 0, and H|−i = 1. Notice that these two states have identical probabilities but differe ...
Document
... NB1: CB neutrinos do not oscillates (by assumption) NB2: CB violates both lepton number and helicity and CB contains a calculable lepton neutrino condensate. NB3: A similar story holds for supernova neutrinos (they are believed to be approximately thermalised). NB4: Can construct a diagonal therm ...
... NB1: CB neutrinos do not oscillates (by assumption) NB2: CB violates both lepton number and helicity and CB contains a calculable lepton neutrino condensate. NB3: A similar story holds for supernova neutrinos (they are believed to be approximately thermalised). NB4: Can construct a diagonal therm ...
Quantum Computers Can Search Rapidly by Using Almost
... be microscopic— however, it is extremely difficult to exert precise control over microscopic individual entities. As a result, a serious problem in implementing quantum mechanical computers is their extreme sensitivity to perturbations. This paper synthesizes algorithms in terms of unitary matrices— ...
... be microscopic— however, it is extremely difficult to exert precise control over microscopic individual entities. As a result, a serious problem in implementing quantum mechanical computers is their extreme sensitivity to perturbations. This paper synthesizes algorithms in terms of unitary matrices— ...
