Exact density-matrix solutions for relativistic scalar-field CSL show collapse to single clump but with dominant particle production that violates experimental bounds.
However, t he usual annihilation operator is a = 1√ 2 [ ˆX + i ˆP ] whereas the one used here is a = [ ˆX + i 1 2 ˆP ]
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On the CSL Scalar Field Relativistic Collapse Model
Exact density-matrix solutions for relativistic scalar-field CSL show collapse to single clump but with dominant particle production that violates experimental bounds.