Reichenbach’s Common Cause Principle in Algebraic Quantum Field Theory with Locally Finite Degrees of Freedom
In the paper it will be shown that Reichenbach’s Weak Common Cause Principle is not valid in algebraic quantum field theory with locally finite degrees of freedom in general. Namely, for any pair of projections A , B supported in spacelike separated double cones and , respectively, a correlating sta...
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Published in | Foundations of physics Vol. 42; no. 2; pp. 241 - 255 |
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Main Authors | , |
Format | Journal Article |
Language | English |
Published |
Boston
Springer US
01.02.2012
|
Subjects | |
Online Access | Get full text |
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Summary: | In the paper it will be shown that Reichenbach’s Weak Common Cause Principle is
not
valid in algebraic quantum field theory with locally finite degrees of freedom in general. Namely, for any pair of projections
A
,
B
supported in spacelike separated double cones
and
, respectively, a correlating state can be given for which there is no nontrivial common cause (system) located in the
union
of the backward light cones of
and
and commuting with the both
A
and
B
. Since noncommuting common cause solutions are presented in these states the abandonment of commutativity can modulate this result: noncommutative Common Cause Principles might survive in these models. |
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ISSN: | 0015-9018 1572-9516 |
DOI: | 10.1007/s10701-011-9594-8 |