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only have to focus on the (broad) set of structures M p , and can ignore many of the
finer points of structuralist theorising.
The question is now whether a
approach to the theory of
absolute reaction rates is capable of characterising the inter-theory relationships
appearing in Fig. 2.1 . I will now briefly, and largely informally, discuss the sort of
relationships that are at play.
conceptual spaces
'
'
1. The simplest relationship exists between the
'
statistical mechanics
''
quantum
mechanics ' boxes and the theory of absolute reaction rates.
A ' simple ' quantum mechanics (of the type I argued that was used in quantum
chemistry) is characterised by a Hilbert space and a set of operators as a structure 2 s
Definition 2 (QM-S) x is a characterisation of a simple quantum mechanics,
( x
2
2 s )if
σ A
;
, A ,
1. x
¼
S,
H
2.
is a system of particles;
3. H is a separable Hilbert space;
4.
J
A is an operator on
H
;
σ A is the spectrum of A .
5.
As was argued by Muller ( 1998 , 2003 ), quantum mechanics is not easily
characterisable in terms of a structuralist model, and,
in fact,
'
all quantum-
mechanical set-structures float in a sea of stories
(Muller 2003 , p. 198). As Muller
argues, many of the practical applications of quantum mechanics rely on specifi-
cations of
'
and the like which are fluidly adapted to the
situation at hand. All of these adaptations make up the ' sea of stories ' .
One such story is quantum chemistry. In Hettema ( 2012a ) I characterised ab initio
quantum chemistry as a structure of structures, comprising of a molecular frame, an
electronic structure and an atomic basis set. The simple definition is as follows:
systems
,
measurement
'
'
'
'
Definition 3 x
is
a potential model
for
ab initio quantum chemistry
( x
2
M p (QCAI)) if there are (sub)structures F, E and B, such that
1. x
(F,E,B,);
2. F represents the molecular frame of the form R
¼
Z ;
3. E represents the electronic structure of the for m
;
;
; σ ; ʨ; A
P e ;
r
;
M
;
4. B represents an atomic basis set of the form R B ; ˇ; ʱ
For now, it is sufficient to recognise that the connections between a generic
(
) quantum mechanics and an ab initio quantum mechanics depend on the
moves discussed by G¨rdenfors and Zenker ( 2011 ) in the following sense.
simple
'
'
depends, in the terminology of
G¨rdenfors and Zenker, on a change of scale or metrics as well as the salience of
dimensions as well as on a change in the separability of dimensions. The
The specification of a molecular
frame
'
'
frame
'
'
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