Chemistry Reference
In-Depth Information
where we can assume that all j values are nonzero. This last equation is equivalent
to a polynomial equation of degree s,sothereares real or complex roots. Clearly,
g./ D 1;
g./ D˙1
lim
lim
!˙1
!
1
a j .1
C
r j /
˙
0
and
X
s
j
.1 a j .1 C r j / / 2 <0:
g 0 ./ D
j D1
Using these properties we can graph g./ as shown in Fig. 2.1. This figure indicates
that the structure of the roots is such that there is one root before 1 a 1 .1 C r 1 /,
and one root between each pair of poles 1 a j .1 C r j / and 1 a j C1 .1 C r j C1 / for
j D 1;2;:::;s 1. So all roots have been found and they are real. Furthermore all
are inside the unit circle if and only if
1 a 1 .1 C r 1 /> 1; and g. 1/ > 0:
At least one eigenvalue is outside the unit circle if either 1 a 1 .1 C r 1 / 1 or
g. 1/ < 0.
In the case of constant speeds of adjustment we usually assume that 0<a k
1
for all k, and from relation (2.7) we know that 1<r k
0. So condition (2.21) is
usually satisfied in this case.
1- a 1 (1+ r 1 )
1- a 2 (1+ r 2 )
1- a 3 (1+ r 3 )
a s -1 (1+ r s -1 )
1- a s (1+ r s )
-1
1
λ
Fig. 2.1 Graph of g./, the roots of which are eigenvalues of the Jacobian of the system describing
the dynamics of the discrete time oligopoly under best reply dynamics
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