Translational invariance and energy-momentum conservation law for unstable particles

Author:

Lukierski J.

Publisher

Springer Science and Business Media LLC

Subject

General Medicine

Reference6 articles.

1. R. E. Peierls:Proc. of the 1954 Glasgow Conference (London, 1955), p. 296.

2. H. Kita andY. Kawai:Progr. Theor. Phys.,31, 269 (1964).

3. L. A. Chalfin:Dokl. Akad. Nauk,165, 541 (1965).

4. The operatorsF should form an algebra, We do not specify this algebra.

5. We should assume also thatx 0 does not depend onx. If this condition is not satisfied, eq. (10) gets changed, but the decay factor can be simplified. For example, if we assume thatx μ−x μ 0 is parallel topμ, the decay factor depends only on the differencet−t 0.

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1. Observations on unstable quantons, hyperplane dependence and quantum fields;Studies in History and Philosophy of Science Part B: Studies in History and Philosophy of Modern Physics;2011-05

2. The four-dimensional position operator in theories with broken conformal symmetry;Il Nuovo Cimento A;1976-03

3. Field Theory Describing Arbitrary Two-Body Scattering Amplitude as a Born Term;Fortschritte der Physik;1973

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5. Nonuniqueness of the canonical formalism in the presence of an indefinite metric;Il Nuovo Cimento A;1968-04

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