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- Newsgroups: sci.physics
- Path: sparky!uunet!sun-barr!cs.utexas.edu!tamsun.tamu.edu!zeus.tamu.edu!dwr2560
- From: dwr2560@zeus.tamu.edu (RING, DAVID WAYNE)
- Subject: Re: the nature of exclusion
- Message-ID: <18AUG199208291048@zeus.tamu.edu>
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- Organization: Texas A&M University, Academic Computing Services
- References: <1992Aug14.020848.11073@math.ucla.edu> <1992Aug14.210429.23650@galois.mit.edu> <1992Aug18.115432.2269@aoa.aoa.utc.com>
- Date: Tue, 18 Aug 1992 13:29:00 GMT
- Lines: 14
-
- carl@aoa.aoa.utc.com (Carl Witthoft) writes...
- >An interesting continuation of this: if you pull enough energy
- >out of the right fermionic system and squish it enough, fermions
- >occasionally pair off to form boson-like units. These units then
- >drop into a common energy state. Cold He3 is one example, if I
- >remember correctly :=).
-
- This one has always bugged the heck out of me. Say A1 and A2 pair up
- and B1 and B2 pair up. And each pair is in the same quantum state, then
- either A1 is in the same state as B1, or A1 is in the same state as B2.
- Both of which are forbidden. What's wrong?
-
- Dave Ring
- dwr2560@zeus.tamu.edu
-