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Notes for the paper on the influence of archetypes in Kepler's theory. Kepler: Harmonia Mundi. Latin quotations. Fludd: Replicatio. Frisch: Apologica.

Notes.Notes

Notes by Pauli for the conference on Rydberg.Notes

Notes and calculations on Yang-Feldmann's formalism.Notes

On calculations by Yang-Feldman for spin 0 particles.Calculations

Pauli's withdrawal of "On the Isospingroup in the Theory of Elementary Particles". Renounce to publish a common paper with Heisenberg on the subject.Manuscript

Pauli's withdrawal of "On the Isospingroup in the Theory of Elementary Particles". Renounce to publish a common paper with Heisenberg on the subject.Manuscript

Calculations on transveral actions in S Matrix.Calculations

Proportional multi-wire chamber. Multi-wire detectors contain layers of positively and negatively charged wires enclosed in a chamber full of gas. A charged particle passing through the chamber knocks negatively charged electrons out of atoms in the gas, leaving behind positive ions. The electrons are pulled towards the positively charged wires. They collide with other atoms on the way, producing an avalanche of electrons and ions. The movement of these electrons and ions induces an electric pulse in the wires which is collected by fast electronics. The size of the pulse is proportional to the energy loss of the original particle. Proportional wire chambers allow a much quicker reading than the optical or magnetoscriptive readout wire chambers.

Magnetoscriptive readout wire chamber. Multi-wire detectors contain layers of positively and negatively charged wires enclosed in a chamber full of gas. A charged particle passing through the chamber knocks negatively charged electrons out of atoms in the gas, leaving behind positive ions. The electrons are pulled towards the positively charged wires. They collide with other atoms on the way, producing an avalanche of electrons and ions. The movement of these electrons and ions induces an electric pulse in the wires which is collected by fast electronics. The size of the pulse is proportional to the energy loss of the original particle.