Time in Process Philosophy

KronoScope ◽  
2001 ◽  
Vol 1 (1) ◽  
pp. 75-99 ◽  
Author(s):  
David Ray Griffin

AbstractAfter contrasting process philosophy's pantemporalism with the two other possibilities — nontemporalism and dualism — I argue the following points:The great negative virtue of J.T.Fraser's version of emergent dualism is that it explicitly brings out the paradoxes that must be faced if pantemporalism is denied. Its great positive virtue,especially when read in conjunction with Grünbaum's position, is that it brings out the fact that time (in the full-fledged sense) requires experience.These two virtues combined suggest the truth of both pantemporalism and panexperientialism, which are mutually implicatory.Pantemporalism, or even the weaker conviction, shared by almost everyone, that time has existed at least since the origin of our universe, conflicts with another belief that initially seems equally well grounded — the belief in an ontological dualism between experiencing and nonexperiencing things. But this latter conviction belongs at best only to soft-core, not hard-core, common sense, so it can be given up without selfcontradiction. Because panexperientialism, like pantemporalism, solves a host of philosophical problems, a pantemporalisticpanexperientialist worldview can be defended in terms of selfconsistency and adequacy to the facts, including the facts of hard-core common sense.

1985 ◽  
Vol 4 (2) ◽  
pp. 101-109 ◽  
Author(s):  
Guillermo Latorre ◽  
M. Angélica Kaulen
Keyword(s):  

2006 ◽  
Vol 125 (16) ◽  
pp. 164503 ◽  
Author(s):  
Elisabeth Schöll-Paschinger ◽  
Albert Reiner
Keyword(s):  

1981 ◽  
Vol 17 (4) ◽  
pp. 319-343 ◽  
Author(s):  
Barry S. Sapolsky ◽  
Dolf Zillmann
Keyword(s):  

2006 ◽  
Vol 104 (20-21) ◽  
pp. 3137-3146 ◽  
Author(s):  
David M. Heyes ◽  
Michael Cass ◽  
Arkadiusz C. Brańka

2011 ◽  
Vol 20 (11) ◽  
pp. 2317-2327 ◽  
Author(s):  
DIPTI PACHOURI ◽  
MANJARI SHARMA ◽  
SYED RAFI ◽  
W. HAIDER

In the present work we describe our results concerning the calculation of equation of state of symmetric zero temperature nuclear matter and the microscopic optical potential using the soft-core Argonne inter-nucleon potentials in first order Brueckner–Hartree–Fock (BHF) theory. The nuclear matter saturates at a density 0.228 nucleon/fm 3 with 17.52 MeV binding energy per nucleon for Argonne av-14 and at 0.228 nucleon/fm 3 with 17.01 MeV binding energy per nucleon for Argonne av-18. As a test case we present an analysis of 65 and 200 MeV protons scattering from 208 Pb . The Argonne av-14 has been used for the first time to calculate nucleon optical potential in BHF and analyze the nucleon scattering data. We also compare our reaction matrix results with those using the old hard-core Hamada–Johnston and the soft-core Urbana uv-14 and Argonne av-18 inter-nucleon potentials. Our results indicate that the microscopic potential obtained using av-14 gives marginally better agreement with the experimental data than the other three Hamiltonians used in the present work.


2010 ◽  
Vol 19 (12) ◽  
pp. 2448-2453
Author(s):  
◽  
C. J. Yoon ◽  
H. Akikawa ◽  
K. Aoki ◽  
Y. Fukao ◽  
...  

We determine ΛΛ scattering parameters from a ΛΛ invariant mass spectrum that was obtained by 12 C (K-, K+ΛΛ) reaction at the KEK Proton Synchrotron. In the framework of Watson's procedure, the obtained scattering length [Formula: see text] and effective range [Formula: see text] are most consistent with the values predicted by using the Nijmegen soft core models (NSC97's). However, the predicted values by using the Nijmegen hard-core ND ( G -matrix) and the extended soft-core (ESC00) models are out of two standard deviations from the determined scattering parameters.


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