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2 October (Wednesday)
5:00
PM
Room
226 |
Balázs Gyenis
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Institute of Philosophy, Research Center for the Humanities,
Hungarian Academy of Sciences
Department of History and Philosophy of Science, University of Pittsburgh
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The birth of statistical mechanics: a colored vision
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Previously
we investigated Maxwell's attempt to justify the assumptions behind his
1860 derivation of the normal distribution. Here we add a further, not
yet investigated, piece to the historical and intellectual puzzle
surrounding his derivation. We are going to argue that Maxwell's prior
and contemporaneous work on color vision provided him familiarity with
and sensitivity to application of statistical reasoning in physics. This
includes an encounter with distributions outside the context of error
theory. We also call attention to a notion of independence of variables
employed in his works on color vision that might have impacted the
mistake he made in his famous Proposition IV. Finally, by analyzing the
parallels Maxwell draws between color mixing in his three dimensional
color space and addition of vectors in three dimensions in mechanics we
speculate that the birth of statistical mechanics might have been
impacted by the contingent fact that the normal human eye has three
color receptors.
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9 October (Wednesday)
5:00
PM
Room
226 |
Michael Epperson
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Center for Philosophy and the Natural Sciences
California State University, Sacramento
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Potentiality and Contextuality in Quantum Mechanics: The Relational Realist Approach
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A
central thesis of the relational realist speculative philosophical
program introduced in the recent volume by M. Epperson and E. Zafiris, Foundations of Relational Realism: A Topological Approach to Quantum Mechanics and the Philosophy of Nature
(Lexington Books / Rowman & Littlefield, New York, 2013) is that
the relationship between the observer and the observed in quantum
mechanics is considered to be ontologically significant, such that the
eigenstates of a measured system always correlate with the particular
Boolean measurement context (e.g., the preferred orthonormal measurement
basis and representative Boolean subalgebra) of the chosen measuring
apparatus. Thus the global objectivity of facts generated by measurement
is at least in some sense conditioned by the ‘subjective’ local context
of the measurement—i.e., the facts constitutive of the measuring
apparatus by which the preferred basis is defined. At the same time,
however, the relationship between the observer and the unobserved
in quantum mechanics can likewise be considered ontologically
significant, as evinced by the phenomenon of quantum decoherence, such
that the probability valuations of the eigenstates of the locally
contextualized measured system are objectively conditioned by global
facts ‘environmental’ to the measured system. In this way, the
bidirectional mutual implication of local contextuality and global
objectivity in quantum mechanics is exemplified by the concurrence of
[1] extension of locally contextualized actual measurement outcomes to
the global quantum state, and [2] restriction of locally contextualized
potential measurement outcomes by the global quantum state.
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16 October (Wednesday)
5:00
PM
Room
226 |
Márta Ujvári
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Institute of Sociology and Social Policy
Corvinus University, Budapest
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Mereological principles doing metaphysical job
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The
colocation of qua-objects under different sortals is a metaphysical
claim recently often mixed with the mereological approach of applying
the parthood relation to such colocated objects. Simons and Thomson
hold that two colocated objects like the statue as a sortal-token and
the lump of clay as its material constitutor are each part of the
other. Koslicki (2008) denies symmetry and claims asymmetry to the
effect that only the lump is part of the statue, moreover, its proper
part, but not vice versa since the statue has an immaterial part not
shared by the lump. This position is heavily loaded with metaphysical
assumptions while her argument pretends to rely only on mereological
principles. Donnely (2011) is critical with the asymmetry argument
saying that ‘the best methodology is to develop a
mereological theory in conjunction with a particular metaphysical
theory, and not to assume principles prior to any more substantial
metaphysical commitment.’
While
agreeing with his overall conclusion I suggest a different strategy.
I say that Koslicki’s argument trades on the equivocity of
the very notion of ‘part’. In the scholastic-metaphysical
tradition ‘part’ shows up with various meanings and connotations.
Not all of these meanings admit the mereological reading of ‘part’
the argument hinges on; while that meaning of ‘part’ supporting
the metaphysical conclusion about the statue/clay asymmetry and the
material objects’ having also immaterial parts is the one not
matching with the mereological meaning explored to make the argument
go. Further, if asymmetry cannot be claimed purely
on mereological grounds, as I believe it cannot, the absurd
consequence ensues that the materia designata, the lump, also has an
immaterial part not shared by the statue, the sortal-token. For the
argument for the postulation of an immaterial part of the statue can
be repeated for the case of the lump: by parity, the lump can also be
shown to have an immaterial part not shared by the statue.
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