
Local volatility 45
(2.37): for
t = 0
, the density
ρ
σ
0
vanishes unless
S = S
0
, while for
t = T
the dollar
gamma S
2
d
2
P
σ
0
dS
2
vanishes, unless S = K.
In (2.42), the largest weight is obtained for
y = 0
: this singles out a path for
ln(S)
which is a straight line starting at
ln(S
0
)
for
t = 0
and ending at
ln(K)
at
t = T
.
Replacing the integral over
y
by the value for
y = 0
would give an approximation
of bσ
KT
as a uniform average of the local volatility along this line:
bσ
KT
'
1
T
Z
T
0
σ
t, F
t
e
t
T
ln
K
F
T
dt (2.43)
Summing over values of
y 6= 0
, includes other paths in the average, with their
ends pinned down at S
0
at t = 0 and at K for t = T by the factor
p
σ
2
0
(T − t) t.
However appealing expression ...