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Mathematics aild Computers in Simulation 33 (1992) 575-580 North-Holland
575
of Some Continuous
ome iblonte Ca
Y. K. Tse
National UniveGty of Singapore
iMany financial models are based on assumptions concerning the stochastic movements
of some security prices. % evaluate the price of a derivative security, the parameters
dking the stochastic process of the underlying asset have to be estimated. Lo (1988)
studied the theory of maximum likelihood estimation of Ito processes, He established
a characterization theorem of the exact likelihood function of data that are sampled
at discrete time points which may or may not be equally apart. Under standard
asymptot,: theoYes, the maximum likelihood estimators (MLE) of these processes
ca be straightforward!y established.
While it is possible LO charP.cterize the exact likelihood function of an Ito process,
the existence and the derivation of it are by no means guaranteed. Hence in many
models of application, researchers have to rely 0~1 a discretized approximation of
the likelib~od function. As pointed out by Lo, the discretized MLE is in general
inconsistcn:. The magnitude of the inconsistency depends on the sampling interval
and typically decreases as the sampling interval is shortened. It is thus important
to know the consequences of the approximation, especially its effect on the size of
the inconGstency. In a recent paper Tse (191) derived closed form solutions for the
.LILE oi uome diffu$on processes commonly used to describe interest rate mcvements,
providing asvmptotic results of the discretized MILE as w4 as the exact MLE. In
lhis pa!Jrr we present so~ne XIonte Carlo results for comparing the perfor .nauw o!’ the
discretized nud csact 4lLE of the Ornstein-Uhlenbeck process. The comparison is
extended to include the geometric Brownian motion for :Ttocl. price mc,vements. jve
find that the discretized MLE gives results comparable to the exact MLE, provided
the dala are based on a judicious choice of sampling interval supported by appropriate
salllp]e sizcb. it is alsO fount’ thaw the rates of converi;:l;<e of the estimalcd parameters.
witllin the sitme model, to tlwir asymptotic distribution can be drastically diKerent
IT c!stiInaLiug volatility is me main concern, our findings favour choosing data wit11 a
short sampling intcrva!.
0378-1754/92/$05.00 0 1992 - Elscvicr Scicncc Publishers B.V. All righls rcscrvcd
516 X.K. Tse I MLE of continuous time financial models
nterest
Two types of diffusion processes are considered in this paper: stock price model and
interest rate model. We denote S, and & as stock pri ce and interest rate, respectively.
For stock price movement, we consider the geometric Brownian (GB) motion given
by the following equation
dSt = pSt dt + US, dll, (11
where dIVt is a Wiener process. For convenience, we assume that the observations are
equally spaced and let h be the sampling interval. It is we!l-known that (see, e.g.,
Hull (1989, p.83)) ln(&/S,_,) are IID N((p - (u”/2))h,a2h). Thus, the following
,MLE can be obtained by solving the the exact log-likelihood function
where
it = ln($) - l4SJSo)
t-1 n *
The discretized version of t:le GB process can be written as
S, - St-1 - ph -!- Et,
St-1 -
where Et w IID N(0, &‘h). Thus, the MLE of the discretized process are
(2)
(3)
(4)
For interest rate movement, we consider the Ornstein-Uhlenbeck (OU) process
given by the following equation
dR, = ct(p - R,) dt -!- is dl;V,. (6)
This process has the property of reverting to the mean, where p represents the steady-
state mean level and r~ is the speed af adjustment coefficient. From results given by
Vasicclk (1977), conditional on R6_1, & is normally distributed with mean c-Ohfi!t_i +
p( 1 - esrzh) and variance o?( 1 - cmJoh )/(2o). The exact MLE, denoted by c%,F and
Y.K. Tsc I MLE qf continuous time financial models 577
ir’, are given in TV (1991). The discrctized QU process can be represented by the
equation
Rt - RI-1 = a(p - Rt_l)h + ct. (7)
The formula for the MLE of the discretized process, denoted by &,$ and 2, can be
found in Tse (1991), where it has been established that /; = i. Besides, the following
points have also been noted: (1) while b is consistent, both (j: and 6’ are incc nsistent,
(2) the asymptotic biases of & and 6* are negative and increase with cr to the first
order in h. For 8*, the asymptotic bias also increases with cr’, (3) the asymptotic
variances of the exact MLE do not depend on ~1: and (4) the asymptotic variance of
& does not depend on u*.
3 onte esults
Optimality properties of the MLE, such as consistency and asymptotic efficiency, are
applicable only when the sample size is sufficiently large. As the rate of convergenw
to the asymptotic distributicn varies according to the underlying model, it is difficult
to provide rule of thumb that is suitable for all models. It is thus important to
consider small sample distributions of the MLE in order to obtain come information
regarding the sample size needed to justify the application of asymptotic results. This
information may also affect the choice of sampling interval. In this section we examine
these issues using a Monte Carlo experiment.
For !,he GB process: we consider p = 0.12,0.18; cr2 = 0.0625: h = 1,4,13 (in
weeks) znd n = 100,200,~OO. Random sampies of observations were generated based
on the exact diffusion process. The discretized and the exact MLE were calculated for
each sample, and this was repeated 1000 times. To conserve space, not all results of
the experiment are reported. Selected findings are summarized in Table 1, which gives
the means and the standard deviations of the MLE frc~nl the Monte Carlo sample. It
can be observed that b and fi are quite similar, except that, as expected, fi is larger
on average and shows signs of upward bias for h equals 1 and 13. The precision of
estimates of p is rather low, and it decreases with h. We note that 100 observations
of four-weekly data achieve the same accuracy as 400 observations of weekly data.
as far as the estimation of p is concerned. In contrast, the standard deviations of
estimates of 2’ are quite small and they do not vary with h. It can be seen that
6’ is upward biased when h is large . When h = 13, the relative bias is about 10
percent. To examine the convergence to normality, we calculated the nominal 95
percent conlidence interval for each ;Ilontc Carlo sample. based on the asynlptotic
norlnal distribution al1c.i cstimatcs of variance. The results (not reported hcrc) shol\
that the asymptotic distribution is in good approximation for 71 = 100.
578 Y.K. Tse I MLE of contintcous time financial models
Table 1
Monte Carlo Estimates of GB Process
/L = 0.18, u2 = 0.0625
Estimates
h(weeks) n *
1 100 0.1718 0.0618
O.lSOO O.OOY9 400 0.1758 0.0623
0.0917 0.0045
4 100 0.1816 0.0624 0.1832 0.0643
0.0897 0.0085 0.0910 0.0089
400 0.1807 0.06;20 0.1320 0.0639 0.0454 0.00.!3 0.0460 0.0046
13 100 O.lXd
0.0501 -100 0.1803
0.0216
0.061s
0.00% 0.0624
0.0045
0.1724 0.0622
0 !8?5 0.0090
6.1762 0.0627 0.0920 0.0045
O.lS32 0.0651
0.0524 0.0103 0.1845 O.OGS9
0.0257 0.0053
Note: The llmtc Carlo sample size is 1000. For each case, the first number refers
to the sample mean and the second number refers to the sample standard deviation.
Y.K. Tse / MLE iIf continuous time financial models 579
Table 2
Monte Carlo Estimates of OU Process
h(weeks) n Estimates
Exact Discretized 6 p=j 2-y x100) B fY( x 100)
Panel A: CI = 0.8,~ = 0.07,~~’ = 0.1225 x 10s2
1 100 3.5791 0.0527 0.12:7 3.4029 0.1165 2.5193 0.4228 0.0175 2.2830 0.0162
400 1.3990 0.0696 0.1237 1.3755 0.1205 0.7213 0.0154 0.0086 0.6962 0.0064
-l 100 1.111s o.oioo 0.1255 1.31s9 0.7504 O.OlSl O.Old4 0.6506
100 0.5261 0.0698 0.1227 0.8931 0.2694 0.0075 CL0087 0.2436
13 100 0.9903 0.0701 0.1256 0.3504 O.OOS6 0.0204
400 O.t34S6 0.0699 0.1233 0.1502 0.0012 0.0098
0.8656 0.2621 0 7f.F 0: 12;;
0.1128 0.0166 0.1113 o.ooi9
O.OYS9 0.0145 (3.1004 0.0072
Panel B: cy = 0.4. p = 0.03. u2 = 0.1225 x 10s2
1 100 3.2402 0.0240 0.1245 3.0650 0.1171 IL.5350 0 . 1’31 _- 0.0177 2.2314 0.0165
600 1.0320 0.0255 0.1232 1.0!80 0.120s 0.6463 0.0506 O.OOK 0.62S3 0.0084
4 100 1.0653 0.0259 0.1345 I.0017 0.1241 0.7257 0.04s: 0.0166 0.6415 0.0167
400 0.5539 0 . O”96 _ 0.1231 0.5405 3.1180 O.Zl’-’ 0.015s O.OOSY 0.2103 0.008::
13 100 0.5S63 0.0290 0 l”33 . ” 0.5378 0.1064
O.“o;S7 0.016s 0.0184 i).Z’l 0.0151 2400 0.4‘I11 G.0300 P. 12% 0.:1:66 0.1102
0.106s O.OOG iI.OOY.5 0.0949 O.OOSl
Note: Tlic Mlontc! Carlo samplr size is . ‘000. I;br each case, the lirst number refers
to the sample mc’an and the second number refers to the sample standard deviakw.
580 Y.K. Tse / W.E of continuous time jkancicl models
To investigate the use of daily data, we condccted further experiments. The
results show that with 100 observations of daily data, the standard deviations of the
estimates of o2 are approximately the same as those obtained from 100 observations
of weekly data. Thus, for the purpose of obtaining estimates of d as input to the
Bla&-Scholes formula, daily data are recommended. Since only a few months of past
data are required, nonstationarity of the variance parameter is unlikely to pose asy
serious difficulty.
For the OU process, we set up the parameters as follows: Q* = Q.001225, and
(a,~) = (O.S.O.O7), (0.4,0.03) and (1.2,O.ll). b ‘imilar to the GB process, we consider
h = 1,4,13 (in weeks) and n = 100,200,400. Selected findings are summarized in
Table 2. We observe that 6’ and fi(fi) converge to their asymptotic meai 5 from
helow, while &‘, 2u aud & converge to their asyrl.ptotic means from above, The
rates of convergence are very different foi estimates of &.&rent parameters. For
example. the rate of convergence of & and iu appear to be very slow and standard
deviations of these estimates are quite large. To investigate further the behaviour
of & and ti we performed an extra experiment with (a,~) = (OS, 0.07) for n =
600. d00.1000. V;hen n = 1fklO and h = 1, the mean of 6 is 1.0395 and its standard
deviation is 0.3573. Thus, & is still far from its asymptotic value of 0.8. The resuhs,
hewever, do show tnat there is a tendency of convergence to :he true parameter value.
The results also verify that & is asymptotically downward biased, as is predicted
from the anaiysis. In contrast, estimares of p and q2 converge very quickly to their
asymptotic means. The experiment also shows that Es2 is asymptotically downward
biased. As the asymptotic variance of estimates of the parameters depend on a, which
cannot be estimated precisely, statistical inference concerning the parameters using
the asymptotic approximation should be interpreted with care.
eferences
[l] Hull. J.. 1959. Options, Murea. und Other Deriuatiae Swurities, Eng!cwood
Cliffs: Prentice-Hall.
[‘) Lo. A.\$!., 19%. *‘Maximum lil~elihood estimation of generalized Ito processes
wilh discreteI!. sampled data.” Eoo7~or:ze~ric Z%tor~ 4. 231 - 247.
[:J] Tse. Y.K.. 1991, “On estimating some co;Kicuous time models for inturcst late
movements.” mimeo.
111 Va~ic& 0.X.. 1977, “:1n equilibrium charzclerization of the term structurr,‘,”
Jvtimul of’ F’inunciul Economics 5. 177 - 188.