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Reduction and Elimination in Philosophy and the Sciences

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determ<strong>in</strong>ation <strong>the</strong>sis; it fails as a refutation of that <strong>the</strong>sis.<br />

Physical determ<strong>in</strong>ation is a very strong negative <strong>the</strong>sis: it<br />

claims that <strong>the</strong>re do not exist any two possible worlds that<br />

match with respect to <strong>the</strong> non-nomic details but have different<br />

laws of nature. So one way to argue aga<strong>in</strong>st it is<br />

simply to try to describe a pair of possible worlds that constitute<br />

a counter example. This strategy is employed by<br />

Michael Tooley (1977, pp.669-672) <strong>and</strong> also is used <strong>in</strong><br />

Carroll (1990). I will consider <strong>the</strong> so called mirror argument<br />

aga<strong>in</strong>st Physical Determ<strong>in</strong>ation here.<br />

The argument beg<strong>in</strong>s with a possible world, U1, that<br />

consists of five X-particles <strong>and</strong> five Y-fields. When each<br />

particle enters its Y-field it acquires sp<strong>in</strong> up. All of <strong>the</strong><br />

particles move <strong>in</strong> a straight l<strong>in</strong>e for all of eternity. But close<br />

to <strong>the</strong> route of one particle <strong>the</strong>re is a mirror on a swivel.<br />

(Call this particle “particle b”). The mirror is <strong>in</strong> such a<br />

position (call it “position c”) that it does not get <strong>in</strong> <strong>the</strong> way<br />

of <strong>the</strong> trajectory of particle b. It seems plausible that <strong>the</strong><br />

follow<strong>in</strong>g is a law <strong>in</strong> U1:<br />

(L) All X-particles subject to Y-fields have sp<strong>in</strong> up.<br />

Now consider U2, a world that is just like U1 except that<br />

particle b does not acquire sp<strong>in</strong> up upon enter<strong>in</strong>g <strong>the</strong><br />

Y-field. Hence, L is not true at U2. Now, U1 <strong>and</strong> U2 do not<br />

pose a problem for <strong>the</strong> MRL view because <strong>the</strong> worlds differ<br />

<strong>in</strong> <strong>the</strong>ir particular matters of fact. The problem stems from<br />

consider<strong>in</strong>g what would have occurred <strong>in</strong> each of <strong>the</strong><br />

worlds had <strong>the</strong> mirror been <strong>in</strong> position d, stopp<strong>in</strong>g particle<br />

b from enter<strong>in</strong>g <strong>the</strong> field. Consider <strong>the</strong> nearest possible<br />

world to U1, U1*; here, it seems reasonable to say that L is<br />

a law because <strong>the</strong> worlds only differ <strong>in</strong> that <strong>the</strong> mirror<br />

blocks <strong>the</strong> particle from enter<strong>in</strong>g <strong>the</strong> field. Now consider<br />

<strong>the</strong> closest world to U2, U2*, where <strong>the</strong> mirror blocks <strong>the</strong><br />

particle. It seems that although L is true <strong>in</strong> U2* it is an accident<br />

because had <strong>the</strong> mirror not been <strong>in</strong> <strong>the</strong> way L would<br />

be false. U1* <strong>and</strong> U2* are identical <strong>in</strong> <strong>the</strong>ir particular matters<br />

of fact; yet it seems that L is a law at U1* but not at<br />

U2*. Hence, laws do not supervene on particular matters<br />

of fact. Therefore, Physical determ<strong>in</strong>ation is false.<br />

I guess <strong>the</strong>re is one reasonable response to <strong>the</strong><br />

Mirror Argument given by Humeans. The Humean just<br />

retorts that any counter<strong>in</strong>tuitiveness is not a strike aga<strong>in</strong>st<br />

Physical determ<strong>in</strong>ation, for such <strong>in</strong>tuitions presuppose an<br />

anti-determ<strong>in</strong>ationist vantage po<strong>in</strong>t. Helen Beebee offers<br />

this sort of response to <strong>the</strong> Mirror Argument. She writes:<br />

As a friend of supervenience, I have no desire to<br />

f<strong>in</strong>d a way of ground<strong>in</strong>g <strong>the</strong> ‘fact’ that L is a law <strong>in</strong><br />

U1*, but not <strong>in</strong> U2*, s<strong>in</strong>ce I th<strong>in</strong>k L is a law <strong>in</strong> U2*<br />

<strong>and</strong> not an accident. This commits me to <strong>the</strong> apparently<br />

unacceptable claim that <strong>the</strong> position of <strong>the</strong> mir<br />

Assess<strong>in</strong>g Humean Supervenience — Amir Karbasizadeh<br />

ror <strong>in</strong> U2 affects what <strong>the</strong> laws of nature are, s<strong>in</strong>ce I<br />

am committed to <strong>the</strong> truth of <strong>the</strong> counterfactual ‘if<br />

<strong>the</strong> mirror had been <strong>in</strong> position d, L would have<br />

been a law.’ But I truly see no harm <strong>in</strong> that … As I<br />

said earlier, part of <strong>the</strong> Humean creed is that laws of<br />

nature depend on particular matters of fact <strong>and</strong> not<br />

<strong>the</strong> o<strong>the</strong>r way around; it is no surprise to <strong>the</strong><br />

Humean, <strong>the</strong>n, that by counterfactually suppos<strong>in</strong>g<br />

<strong>the</strong> particular matters of fact to be different one<br />

might easily change what <strong>the</strong> laws of nature are too.<br />

The <strong>in</strong>tuition that’s really do<strong>in</strong>g <strong>the</strong> work <strong>in</strong> this<br />

counterexample, <strong>the</strong>n, is <strong>the</strong> <strong>in</strong>tuition that laws are<br />

not purely descriptive … But to describe <strong>the</strong> example<br />

<strong>in</strong> those terms is not to describe it <strong>in</strong> neutral<br />

terms but to describe it <strong>in</strong> terms which explicitly presuppose<br />

an anti-Humean start<strong>in</strong>g po<strong>in</strong>t …<br />

At first blush at least, it is clear why <strong>the</strong> Humean would feel<br />

compelled to assert this. After all, <strong>the</strong>re is a sense <strong>in</strong> which<br />

<strong>the</strong>y are be<strong>in</strong>g told that <strong>the</strong>ir view is false simply because it<br />

doesn’t say <strong>the</strong> laws govern. The Humean th<strong>in</strong>ks <strong>the</strong> anti-<br />

Humean position is <strong>in</strong> <strong>the</strong> grip of an <strong>in</strong>tuition which is ultimately<br />

<strong>in</strong>correct.<br />

7. Conclusion<br />

I have considered Humean Supervenience <strong>and</strong> its two<br />

components <strong>and</strong> <strong>the</strong>ir plausibility. I conclude that <strong>the</strong> first<br />

component of Humean Supervenience namely Separability<br />

is untenable. However, I see no reason not to believe <strong>in</strong><br />

<strong>the</strong> second component of it.<br />

Literature<br />

Albert, D. Z., 1992, Quantum Mechanics <strong>and</strong> Experience. Harvard<br />

University Press.<br />

Beebee, Helen., 2000, “The Non-Govern<strong>in</strong>g Conception of Laws of<br />

Nature”, <strong>Philosophy</strong> <strong>and</strong> Phenomenological Research, LXI, No.3.<br />

Carroll, John., 1994,.Laws of Nature Cambridge: Cambridge University<br />

Press.<br />

Lewis, D., 1973, Counterfactuals, Cambridge: Harvard University<br />

Press.<br />

-----------, 1983, “New Work for a Theory of Universals, Australasian<br />

Journal of <strong>Philosophy</strong>, 61: 343-377.<br />

-----------, 1986, Philosophical Papers, Volume II, New York: Oxford<br />

University Press.<br />

Roberts, John., 1998. “Lewis, Carroll <strong>and</strong> See<strong>in</strong>g Through <strong>the</strong><br />

Look<strong>in</strong>g Glass” Australasian Journal of <strong>Philosophy</strong> 76(3).<br />

Tooley, M.,1977, “The Nature of Law”, Canadian Journal of <strong>Philosophy</strong>,<br />

7: 667-98<br />

165

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