Bubble Nucleation and Eternal Inflation - cosmo 06

=0
C
r
III’’
III I
C
III’’
IV
II’’
IV’’
r C
III''
II’’
r C
Two
III
Tunnels
I
III'
II
IV''
IV
IV'
r C
BH
r BH
rBH
BH
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FIG. 10: Conformal diagrams for the thermalon spacetime
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II
II’
[6]
IV’’
D. J. Gross, M. J. Perry, andIV
L. G. Yaffe, Phys. Rev. D25,
IV’
330 (19
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I
III’
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FIG. IV 11: Tunneling through IV’ the worm hole.
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FIG. 11: Tunneling through the worm hole.
R Tunneling Geometry: goes through dS horizon.
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[15] I
III A. Aurilia, M. Palmer, III’ and E. Spallucci, Phys. Rev. D40, 2511 (198
III
r
BH
r C
L Tunneling Geometry: goes through wormhole.
II
IV
r
r C
BH
[18] T. FIG. R. 12: Choudhury Second option for tunneling. and T. Padmanabhan (2004), gr-qc/0404091.
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I
II’
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IV
IV’
IV’’
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IV’
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r BH
r C
III’
FIG. 12: Second option for tunneling.
II’’
IV’’
II’