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Reduction and Elimination in Philosophy and the Sciences

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386<br />

On <strong>the</strong> Characterization of Objects by <strong>the</strong> Language of Science — Paul We<strong>in</strong>gartner<br />

description can be obta<strong>in</strong>ed <strong>and</strong> used for <strong>the</strong> <strong>in</strong>dividuation<br />

of quantum mechanical objects. S<strong>in</strong>ce trans-world-identity<br />

of objects implies reidentifiablity of one unique object <strong>in</strong><br />

different worlds, it follows that trans-world-identity of quantum<br />

mechanical objects is not possible. There may be<br />

however a k<strong>in</strong>d of weak analogy of trans-world-identity if<br />

<strong>the</strong> follow<strong>in</strong>g restrictions <strong>and</strong> deviations with respect to a<br />

Kripke style semantics are made:<br />

(1) Possible worlds are replaced by measur<strong>in</strong>g<br />

processes.<br />

(2) "There is a world W' (different from <strong>the</strong> actual<br />

world W) <strong>in</strong> which <strong>the</strong> proposition A' about system<br />

S' is true" is replaced by: "There is a measur<strong>in</strong>g<br />

process M' (different from <strong>the</strong> actual (or<br />

earlier) measur<strong>in</strong>g process M) with <strong>the</strong> result<br />

that proposition A' about system S' is true."<br />

(3) The accessibility relation R(S, S') is satisfied,<br />

when A(S, M) = A'(S', M').<br />

(4) There is a non-zero probability for reach<strong>in</strong>g result<br />

A' about S' by measur<strong>in</strong>g process M' from<br />

<strong>the</strong> earlier result A about S by measur<strong>in</strong>g process<br />

M.<br />

(5) If (4) is satisfied, <strong>the</strong>re is a non-zero probability<br />

for a weak temporal identity of <strong>the</strong> system (object)<br />

S.<br />

4. Are <strong>the</strong> Pr<strong>in</strong>ciples about <strong>the</strong> Objects of<br />

Reference of Ch. 2 valid when applied to<br />

SR <strong>and</strong> GR?<br />

4.1 Value-Completeness<br />

Special Relativity (SR): Value-completeness or valuedef<strong>in</strong>iteness<br />

of properties of an object (reference system,<br />

cf. 2.4) is not satisfied for an observer at every po<strong>in</strong>t of<br />

time. But <strong>in</strong> this case (we have just <strong>in</strong>ertial movement <strong>and</strong><br />

no acceleration or gravitation <strong>and</strong> M<strong>in</strong>kowski space-time)<br />

<strong>the</strong> observer may always wait until <strong>the</strong> object appears <strong>in</strong><br />

his past light cone.<br />

General Relativity (GR): As soon as acceleration or gravitation<br />

is taken <strong>in</strong>to account, <strong>the</strong>re are always some doma<strong>in</strong>s<br />

<strong>in</strong> space-time with objects that will never appear <strong>in</strong><br />

<strong>the</strong> past light cone of <strong>the</strong> observer. This is so even if <strong>the</strong><br />

observer moves on a geodesic, i.e. free from forces. It is<br />

pla<strong>in</strong> <strong>the</strong>n that <strong>the</strong> description of such objects cannot be<br />

value-complete.<br />

4.2 Permanence<br />

SR <strong>and</strong> GR: The essential properties of <strong>the</strong> object of reference<br />

(as <strong>the</strong> bearer) are no more permanent, although<br />

with one exception: charge. The o<strong>the</strong>r properties like<br />

mass, length <strong>and</strong> geometrical shape change <strong>in</strong> case of fast<br />

<strong>in</strong>ertial motion <strong>in</strong> accordance with <strong>the</strong> Lorentz-<br />

Transformation; this holds also <strong>in</strong> local <strong>in</strong>ertial reference<br />

systems of Rimanean space-time (GR).<br />

which could not serve anymore as <strong>in</strong>dividuat<strong>in</strong>g) was proposed by Thomas<br />

Aqu<strong>in</strong>as (Ver), 19, as one, though not <strong>the</strong> only possibility, s<strong>in</strong>ce it is not sufficient<br />

<strong>in</strong> all cases (like children who die immediately after birth).<br />

4.3 Uniqueness<br />

Accord<strong>in</strong>g to 2.6, uniqueness of objects of Classical Mechanics<br />

can be satisfied by special values of <strong>the</strong> accidental<br />

properties position (p), momentum (q) <strong>and</strong> po<strong>in</strong>t of time (t).<br />

But <strong>in</strong> 3.3 it was shown that uniqueness is no more satisfied<br />

on <strong>the</strong> microlevel (<strong>in</strong> QM). Concern<strong>in</strong>g SR, uniqueness<br />

w.r.t. p, q, t holds only partially; namely it holds only for<br />

objects appear<strong>in</strong>g <strong>in</strong> <strong>the</strong> past <strong>and</strong> future light cone of <strong>the</strong><br />

observer (dynamical laws presupposed). With respect to<br />

GR, uniqueness is dependent on <strong>the</strong> space-time curvature.<br />

4.4 Reidentifiability<br />

With respect to both, SR <strong>and</strong> GR, <strong>the</strong> object of reference is<br />

not <strong>in</strong> general reidentifiable through time; this is so because<br />

essential properties of <strong>the</strong> object like geometrical<br />

shape <strong>and</strong> mass may change depend<strong>in</strong>g on movement.<br />

Therefore reidentifiability holds only approximately <strong>in</strong> local<br />

reference frames of space-time.<br />

4.5 Time <strong>and</strong> Simultaneity<br />

With respect to both, SR <strong>and</strong> GR, <strong>the</strong>re is nei<strong>the</strong>r a universal<br />

time, nor universal simultaneity. Each different observer<br />

(each different laboratory or reference system) has<br />

its own time <strong>and</strong> simultaneity. Therefore <strong>the</strong> object of reference<br />

is not <strong>the</strong> same for all observers.<br />

Literature<br />

Arnold, V.I. (1990, HBN) Huygens <strong>and</strong> Barrow, Newton <strong>and</strong> Hooke.<br />

Basel, Birkhäuser.<br />

Kant, I. (1787, KRV) Kritik der re<strong>in</strong>en Vernunft. Riga.<br />

Mittelstaedt, P. (1986, SRM) Sprache und Realität <strong>in</strong> der modernen<br />

Physik. Mannheim, Bibliographisches Institut.<br />

Mittelstaedt, P./We<strong>in</strong>gartner, P. (2005, LNt) Laws of Nature.<br />

Spr<strong>in</strong>ger, Heidelberg-Berl<strong>in</strong>.<br />

Russell, B. (1919, IMP) Introduction to Ma<strong>the</strong>matical <strong>Philosophy</strong>.<br />

London, Allen <strong>and</strong> Unw<strong>in</strong>.<br />

Russell, B. (1925, ABC) The ABC of Relativity. London, Kegan<br />

Paul.<br />

Russell, B. (1927, AMt) The Analysis of Matter. London, Kegan<br />

Paul.<br />

Thomas Aqu<strong>in</strong>as (Ver) De Veritate. Engl. Transl.: The Disputed<br />

Questions on Truth. Henry Regnery Company, Chicago 1952<br />

We<strong>in</strong>gartner, P. (1996, UWT) "Under What Transformations are<br />

Laws Invariant?" <strong>in</strong>: We<strong>in</strong>gartner, P./Schurz, G. (eds.) Law <strong>and</strong><br />

Prediction <strong>in</strong> <strong>the</strong> Light of Chaos Research. Spr<strong>in</strong>ger, Heidelberg-<br />

Berl<strong>in</strong>, p. 47-88.

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