Related to a Solvay meeting.Literature
Casimir, Hendrik Brugt GerhardLee model, field theories and quantum electrodynamics.Manuscript
Källén, GunnarFormulae relating to vacuum polarization.Manuscript
Kawabe, Rokuo Umezawa, HiroomiArticle on Onsager's theory of reciprocal relations in irreversible processes, and more precisely on the application of this theory to electrical networks.Manuscript
Casimir, Hendrik Brugt GerhardS-Matrix, applications to Meson theoryNotes
Pauli, WolfgangS-Matrix, applications to Meson theory
Pauli, WolfgangCalculations on S-matrix.Calculations
Pauli, WolfgangSlides for the conference on Rydberg and the periodical system of elements.Slide on glass
[unknown]Slides for the conference on Rydberg and the periodical system of elements.
[unknown]Slice through an LHC superconducting quadrupole (focusing) magnet. The slice includes a cut through the magnet wiring (niobium titanium), the beampipe and the steel magnet yokes. Particle beams in the Large Hadron Collider (LHC) have the same energy as a high-speed train, squeezed ready for collision into a space narrower than a human hair. Huge forces are needed to control them. Dipole magnets (2 poles) are used to bend the paths of the protons around the 27 km ring. Quadrupole magnets (4 poles) focus the proton beams and squeeze them so that more particles collide when the beams’ paths cross. Bringing beams into collision requires a precision comparable to making two knitting needles collide, launched from either side of the Atlantic Ocean.