Derivation of Pauli Equation and its Bipartite Form based on Budiyono-Rohrlich Ontic Extension and Epistemic Restriction of Statistical Model of Quantum Mechanics

Author(s):  
Husin Alatas ◽  
Ahmad N. Aziz ◽  
Hendradi Hardhienata
Entropy ◽  
2020 ◽  
Vol 22 (11) ◽  
pp. 1197
Author(s):  
Sholeh Razavian ◽  
Matteo G. A. Paris ◽  
Marco G. Genoni

The estimation of more than one parameter in quantum mechanics is a fundamental problem with relevant practical applications. In fact, the ultimate limits in the achievable estimation precision are ultimately linked with the non-commutativity of different observables, a peculiar property of quantum mechanics. We here consider several estimation problems for qubit systems and evaluate the corresponding quantumnessR, a measure that has been recently introduced in order to quantify how incompatible the parameters to be estimated are. In particular, R is an upper bound for the renormalized difference between the (asymptotically achievable) Holevo bound and the SLD Cramér-Rao bound (i.e., the matrix generalization of the single-parameter quantum Cramér-Rao bound). For all the estimation problems considered, we evaluate the quantumness R and, in order to better understand its usefulness in characterizing a multiparameter quantum statistical model, we compare it with the renormalized difference between the Holevo and the SLD-bound. Our results give evidence that R is a useful quantity to characterize multiparameter estimation problems, as for several quantum statistical model, it is equal to the difference between the bounds and, in general, their behavior qualitatively coincide. On the other hand, we also find evidence that, for certain quantum statistical models, the bound is not in tight, and thus R may overestimate the degree of quantum incompatibility between parameters.


1995 ◽  
Vol 10 (09) ◽  
pp. 1269-1280 ◽  
Author(s):  
N. FLEURY ◽  
M. RAUSCH DE TRAUBENBERG ◽  
R.M. YAMALEEV

Using para-Grassmann, or generalized Grassmann algebras, we define rational power of annihilation and creation operators, in order to extend supersymmetric quantum mechanics. This extension can be replaced, under some assumptions, in para-Grassmann quantum mechanics. We then apply this method to the construction of an equation which generalizes the (2+1)D Pauli equation to a particle of arbitrary spin s. This is done by means of a Hamiltonian defined as a sum of 2s monomials of degree 2s+1.


1989 ◽  
Vol 46 (1) ◽  
pp. 524-533
Author(s):  
V. P. Maslov

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