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SUMMARY:Jeffrey C. Morton (SUNY Buffalo State)
DTSTART:20220126T170000Z
DTEND:20220126T180000Z
DTSTAMP:20260423T024530Z
UID:TQFT/49
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/TQFT/49/">Th
 e Fock Pseudomonad: Groupoidifying Second Quantization</a>\nby Jeffrey C. 
 Morton (SUNY Buffalo State) as part of Topological Quantum Field Theory Cl
 ub (IST\, Lisbon)\n\n\nAbstract\n<p>Edward Nelson said "First quantization
  is a mystery\, but second quantization is a functor". This functor takes 
 the Hilbert space H representing a quantum mechanical system\, and gives i
 ts Fock space F(H)\, representing a multi-particle system with any number 
 of indistinguishable copies of the original system as in quantum field the
 ory (I am considering the bosonic case). In a categorical analysis of the 
 harmonic oscillator\, Vicary revised Nelson's slogan to say "second quanti
 zation is a monad" - that is\, the functor in question is equipped with so
 me extra algebraic structure\, making it the "Fock Monad" (F\,$\\eta$\,$\\
 epsilon$).</p>\n\n<p>Groupoidification is one of a number of approaches to
  "categorifying" quantum-mechanical systems: finding higher-categorical an
 alogs of those systems. It uses a 2-category Span(Gpd) whose objects are g
 roupoids\, and whose morphisms are "spans". This has had some success in d
 escribing extensions of topological field theory to systems with boundary\
 , with the "categorified" theory describing the evolution of open systems\
 , which can be composed along their boundaries\, over time. In this talk\,
  I will use this framework to describe a categorification of F to the "Foc
 k Pseudomonad" which can be defined in any suitable 2-category\, and the c
 ompatibility of this pseudomonad in Span(Gpd) with that in 2-Hilbert space
 s\, and\, under the "degroupoidification" map\, with the usual Fock constr
 uction on Hilbert spaces.</p>\n
LOCATION:https://researchseminars.org/talk/TQFT/49/
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