Dear all,

The CamPoS (Cambridge Philosophy of Science) seminar continues this 
Wednesday, 20th February, 1-2:30pm in HPS Seminar Room 2. Brian Pitts 
(Philosophy, Cambridge) will give a talk entitled “Real Change Happens in 
General Relativity, Even in Hamiltonian Form”. The abstract is below.

All are very welcome, and we hope to see many of you there.

Best wishes,
Vashka

--

From time to time natural philosophers have argued that there is no real 
change, despite manifest appearances. A recent powerful claim to this end 
has been made from Einstein’s General Relativity (GR), the standard theory 
of gravity, as expressed in Hamiltonian form. Hamiltonian mechanics employs 
not coordinates q and their velocities, but coordinates q and their 
conjugate momenta p: more fields but fewer derivatives. Various physicists 
and philosopher Earman have questioned objective change due to Hamiltonian 
GR, while common sense has been defended by Kuchař and Maudlin, yielding a 
stand-off.
         Fortunately confusion dissipates when one insists on the golden 
principle, employed by Salisbury, Pons, and Shepley, that Hamiltonian 
General Relativity be equivalent to General Relativity in more familiar 
Lagrangian or 4-dimensional differential geometric form. In GR in more 
familiar form, there is change for solutions that are not stationary, that 
is, that lack a time-like Killing vector field: no matter how one labels 
space-time, the metric depends on time. Hamiltonian change thus must be the 
Hamiltonian form of lacking a time-like Killing vector field. Castellani’s 
distinction between the 4-dimensional gauge (coordinate) transformation 
generator (t)G(t) and the Hamiltonian H clarifies matters.
         Pace Dirac and Bergmann, a first-class constraint in 
Dirac-Bergmann constrained Hamiltonian dynamics typically does not generate 
a physically equivalent configuration. In Maxwell’s electromagnetism, a 
first-class constraint generates an (anti)-physical change in the electric 
field, spoiling equivalence to Gauss’s law. First-class constraints in GR, 
working together, not separately, appear both in the Hamiltonian to 
generate time evolution and in the gauge transformation generator to 
generate coordinate transformations. Gauge (coordinate) equivalence in GR 
must be understood in terms of histories, not instantaneous states as Dirac 
envisaged. More confusion is avoided by not introducing primitive point 
identities into mathematical physics. There is no reason that “observables” 
should be spatially changeless constants of the motion, especially if 
observables have something to do with observations (as Bergmann held). He 
developed the notion of observables in GR by analogy to Hamiltonian 
electromagnetism while neglecting equivalence with Lagrangian GR.


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