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VERSION:2.0
METHOD:PUBLISH
CALSCALE:GREGORIAN
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LOCATION:234 Moses Hall
SEQUENCE:0
DTEND:20090513T200000
DTSTART:20090513T180000
UID:philosophy.berkeley.edu:events:513
DTSTAMP:20091124T031300
DESCRIPTION:The goal of the talk is to clarify certain points about "space"
  and "spatial geometry" within the framework of general relativity. (Within
  that framework\, talk about four-dimensional spacetime geometry is perfect
 ly unambiguous\, but not so talk about three-dimensional spatial geometry.)
   So\, for example\, consider this question:  "How big was space just after
  the big bang."  It is a trick question because it depends on what one mean
 s by "space". Indeed\, if the universe is described by a standard Friedmann
 -Robertson-Walker cosmological model in which k = 0 or k = -1\, then the an
 swer is "infinitely large" in one sense of "space"\, but "incredibly small"
  in another sense of "space".
SUMMARY:Working Group in HPLMS\nDavid Malament\nHow Space Can Be (and Is) F
 inite
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