1996
DOI: 10.1007/978-94-017-2830-0
|View full text |Cite
|
Sign up to set email alerts
|

Quantum Mechanics on Phase Space

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

0
148
0

Year Published

2000
2000
2018
2018

Publication Types

Select...
5
5

Relationship

0
10

Authors

Journals

citations
Cited by 136 publications
(149 citation statements)
references
References 0 publications
0
148
0
Order By: Relevance
“…Let, say, X be a tight frame for H , let Y be a subsystem of X and M(Y ) = x∈Y ·, x x. Then the mapping M, defined on the family of all subsystems of X , is a simple example of a positive operator valued measure, a notion playing a major role in quantum information theory, describing generalized measurements [104]. In general, M(Y ) is not an orthogonal projection.…”
Section: Proposition 23mentioning
confidence: 99%
“…Let, say, X be a tight frame for H , let Y be a subsystem of X and M(Y ) = x∈Y ·, x x. Then the mapping M, defined on the family of all subsystems of X , is a simple example of a positive operator valued measure, a notion playing a major role in quantum information theory, describing generalized measurements [104]. In general, M(Y ) is not an orthogonal projection.…”
Section: Proposition 23mentioning
confidence: 99%
“…Such applications have been well established for the continuum theory of phase space; see, for instance, [11,19,25,29,31,34]. A satisfactory discrete version of the theory would also be expected to have such applications.…”
Section: Introductionmentioning
confidence: 99%
“…With coworkers he has proposed a wide class of alternative wave equations which overcome these shortcomings [36,[40][41][42]. For the spinless non-relativistic case the phase-space wave function is written as [36] If for each p held fixed the functions ( , ; ) ψ t q p satisfy the regularity conditions of Theorem 1 then each these currents will all be non-radiating.…”
Section: Proofmentioning
confidence: 99%