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Letter from Dyson to Pauli
Letter-1081 · Unidad documental simple · 1950/02/15
Parte de Archives of Wolfgang Pauli

Dyson explains why the symmetrical treatment of the radiation field gives the right answer in Schwinger's theory. The letter contains information about experimental results of Powell on fast Pi-mesons and a discussion of the question longitudinal photons.

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Letter from Pauli to Källén
Letter-1082 · Unidad documental simple · 1950/02/16
Parte de Archives of Wolfgang Pauli

Pauli thanks Källén for his manuscript and letter. He makes a comparison of Källén's and Yang's results. He talks about results by Rohrlich for the case of charged scalar mesons in interaction with the quantized electromagnetic field. He also talks about results by Peasler and Kiroshita and about nu mber for charged vector mesons.

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Letter from Pauli to Wentzel
Letter-1086 · Unidad documental simple · 1950/02/26
Parte de Archives of Wolfgang Pauli

Pauli writes about the renormalization method which does not work so well for general interaction in quantized field theory as in the case of positron-quantum electrodynamics.

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Letter from Pauli to Fierz
Letter-1091 · Unidad documental simple · 1950/03/20
Parte de Archives of Wolfgang Pauli

Pauli writes about the talk he had with the German physicist M. Knoll on extra sensory perception (ESP), on different classes of synchronistic phenomena, spontaneous and induced events and on the analogy of a discovery of a law of nature and the induced synchronicity.

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Letter from Heisenberg to Pauli
Letter-1093 · Unidad documental simple · 1950/03/25
Parte de Archives of Wolfgang Pauli

Heisenberg explains his ideas about the "Vertauschungsrelationen" (interchange relations) in his paper. The real problem arises after the introduction of an interaction. This belongs to the general question: which invariance conditions are fullfilled by the interaction energy? He is not as pessimistic as Pauli, the whole question boils down to the problem of finding suitable expressions for interaction out of combinations of wavefunctions which obey regular interchange relations. One has to begin by forming models for unitary theories which afterwards will split up in theories for single particles. The postulate of "hermiticity" is connected with the conservation law for nucleons.

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