We present a framework, compliant with the general canonical principle of statistical mechanics, to define measures on the set of pure Gaussian states of continuous variable systems. Within such a framework, we define two specific measures, referred to as ‘micro-canonical’ and ‘canonical’, and apply them to study systematically the statistical properties of the bipartite entanglement of n -mode pure Gaussian states at, respectively, given maximal energy and given temperature. We prove the ‘concentration of measure’ around a finite average, occurring for the entanglement in the thermodynamical limit in both the canonical and the micro-canonical approach. For finite n , we determine analytically the average and standard deviation of the entanglement (as quantified by the reduced purity) between one mode and all the other modes. Furthermore, we numerically investigate more general situations, clearly showing that the onset of the concentration of measure already occurs at relatively small n .We present a framework, compliant with the general canonical principle of statistical mechanics, to define measures on the set of pure Gaussian states of continuous variable systems. Within such a framework, we define two specific measures, referred to as ‘micro-canonical’ and ‘canonical’, and apply them to study systematically the statistical properties of the bipartite entanglement of n -mode pure Gaussian states at, respectively, given maximal energy and given temperature. We prove the ‘concentration of measure’ around a finite average, occurring for the entanglement in the thermodynamical limit in both the canonical and the micro-canonical approach. For finite n , we determine analytically the average and standard deviation of the entanglement (as quantified by the reduced purity) between one mode and all the other modes. Furthermore, we numerically investigate more general situations, clearly showing that the onset of the concentration of measure already occurs at relatively small n .

arXiv:quant-ph/0701051Journal of Physics A Mathematical and TheoreticalJul 19, 200725 citations

The Principles of Canonical Mechanics

Springer eBooksNov 20, 20050 citations

Canonical Transformations for Quantum Systems

WORLD SCIENTIFIC eBooksAug 17, 20150 citations

Hamilton-Jacobi quantization of the finite dimensional systems with constraints

Dumitru Bǎleanu, Yurdahan Güler

The Hamiltonian treatment of constrained systems in $G\ddot{u}ler's$ formalism leads us to the total differential equations in many variables. These equations are integrable if the corresponding system of partial differential equations is a Jacobi system. The main aim of this paper is to investigate the quantization of the finite dimensional systems with constraints using the canonical formalism introduced by $G\ddot{u}ler$ . This approach is applied for two systems with constraints and the results are in agreement with those obtained by Dirac's canonical quatization method and path integral quantization method.The Hamiltonian treatment of constrained systems in $G\ddot{u}ler's$ formalism leads us to the total differential equations in many variables. These equations are integrable if the corresponding system of partial differential equations is a Jacobi system. The main aim of this paper is to investigate the quantization of the finite dimensional systems with constraints using the canonical formalism introduced by $G\ddot{u}ler$. This approach is applied for two systems with constraints and the results are in agreement with those obtained by Dirac's canonical quatization method and path integral quantization method.

arXiv:hep-th/9901083Il Nuovo Cimento BJan 19, 19990 citations

The Hamiltonian treatment of constrained systems in

G\ddot{u}ler's

formalism leads us to the total differential equations in many variables. These equations are integrable if the corresponding system of partial differential equations is a Jacobi system. The main aim of this paper is to investigate the quantization of the finite dimensional systems with constraints using the canonical formalism introduced by

G\ddot{u}ler

. This approach is applied for two systems with constraints and the results are in agreement with those obtained by Dirac's canonical quatization method and path integral quantization method.