geometric brownian
TRANSCRIPT
-
Steven R. DunbarDepartment of Mathematics203 Avery HallUniversity of Nebraska-LincolnLincoln, NE 68588-0130http://www.math.unl.edu
Voice: 402-472-3731Fax: 402-472-8466
Math 489/Math 889
Stochastic Processes and
Advanced Mathematical FinanceDunbar, Fall 2009
Properties of Geometric Brownian Motion
Rating
Mathematically Mature: may contain mathematics beyond calculus withproofs.
1
-
Section Starter Question
For the ordinary differential equation
dx
dt= rx x(0) = x0
what is the rate of growth of the solution?
Key Concepts
1. Geometric Brownian Motion is the continuous time stochastic processz0 exp(t+ W (t)) where W (t) is standard Brownian Motion.
2. The mean of Geometric Brownian Motion is
z0 exp(t+ (1/2)2t).
3. The variance of Geometric Brownian Motion is
z20 exp(2t+ 2t)(exp(2t) 1).
Vocabulary
1. Geometric Brownian Motion is the continuous time stochastic pro-cess z0 exp(t+ W (t)) where W (t) is standard Brownian Motion.
2
-
2. A random variable X is said to have the lognormal distribution (withparameters and ) if log(X) is normally distributed (log(X) N(, 2)).The p.d.f. for X is
fX(x) =1
2pixexp((1/2)[(ln(x) )/]2).
Mathematical Ideas
Geometric Brownian Motion
Geometric Brownian Motion is the continuous time stochastic processX(t) = z0 exp(t+ W (t)) where W (t) is standard Brownian Motion. Mosteconomists prefer Geometric Brownian Motion as a model for market pricesbecause it is everywhere positive (with probability 1), in contrast to BrownianMotion, even Brownian Motion with drift. Furthermore, as we have seenfrom the stochastic differential equation for Geometric Brownian Motion,the relative change is a combination of a deterministic proportional growthterm similar to inflation or interest rate growth plus a normally distributedrandom change
dX
X= r dt+ dW .
See Itos Formula and Stochastic Calculus. On a short time scale this is asensible economic model.
Theorem 1. At fixed time t, Geometric Brownian Motion z0 exp(t+W (t))has a lognormal distribution with parameters (ln(z0) + t) and
t.
3
-
Figure 1: The p.d.f. for a lognormal random variable
Proof.
FX(x) = P [X x]= P [z0 exp(t+ W (t)) x]= P [t+ W (t) ln(x/z0)]= P [W (t) (ln(x/z0) t)/]= P
[W (t)/
t (ln(x/z0) t)/(
t)]
=
(ln(x/z0)t)/(t)
12pi
exp(y2/2) dy
Now differentiating with respect to x, we obtain that
fX(x) =1
2pixt
exp((1/2)[(ln(x) ln(z0) t)/(t)]2).
Calculation of the Mean
We can calculate the mean of Geometric Brownian Motion by using the m.g.f.for the normal distribution.
4
-
Theorem 2. E [z0 exp(t+ W (t))] = z0 exp(t+ (1/2)2t)
Proof.
E [X(t)] = E [z0 exp(t+ W (t))]= z0 exp(t)E [exp(W (t))]= z0 exp(t)E [exp(W (t)u)] |u=1= z0 exp(t) exp(
2tu2/2)|u=1= z0 exp(t+ (1/2)
2t)
since W (t) N(0, 2t) and E [exp(Y u)] = exp(2tu2/2) when Y N(0, 2t).See Moment Generating Functions, Theorem 4.
Calculation of the Variance
We can calculate the variance of Geometric Brownian Motion by using them.g.f. for the normal distribution, together with the common formula
Var [X] = E[(X E [X])2] = E [X2] (E [X])2
and the previously obtained formula for E [X].Theorem 3. Var [z0 exp(t+ W (t))] = z
20 exp(2t+
2t)[exp(2t) 1]Proof. First compute:
E[X(t)2
]= E
[z20 exp(t+ W (t))
2]
= z20E [exp(2t+ 2W (t))]= z20 exp(2t)E [exp(2W (t))]= z20 exp(2t)E [exp(2W (t)u)] |u=1= z20 exp(2t) exp(4
2tu2/2)|u=1= z20 exp(2t+ 2
2t)
Therefore,
Var [z0 exp(t+ W (t))] = z20 exp(2t+ 2
2t) z20 exp(2t+ 2t)= z20 exp(2t+
2t)[exp(2t) 1].
5
-
Note that this has the consequence that the variance starts at 0 and thenincreases. The variation of Geometric Brownian Motion starts small, andthen increases, so that the motion generally makes larger and larger swingsas time increases.
Parameter Summary
If a Geometric Brownian Motion is defined by the stochastic differential equa-tion
dX = rX dt+X dW X(0) = z0
then the Geometric Brownian Motion is
X(t) = z0 exp((r (1/2)2)t+ W (t)).
At each time the Geometric Brownian Motion has lognormal distributionwith parameters (ln(z0)+rt(1/2)2t) and
t. The mean of the Geometric
Brownian Motion is E [X(t)] = z0 exp(rt). The variance of the GeometricBrownian Motion is
Var [X(t)] = z20 exp(2rt)[exp(2t) 1]
If the primary object is the Geometric Brownian Motion
X(t) = z0 exp(t+ W (t)).
then by Itos formula the SDE satisfied by this stochastic process is
dX = (+ (1/2)2)X(t) dt+X(t) dW X(0) = z0.
At each time the Geometric Brownian Motion has lognormal distributionwith parameters (ln(z0)+t) and
t. The mean of the Geometric Brownian
Motion is E [X(t)] = z0 exp(t + (1/2)2t). The variance of the GeometricBrownian Motion is
z20 exp(2t+ 2t)[exp(2t) 1].
6
-
Ruin and Victory Probabilities for Geometric BrownianMotion
Because of the exponential-logarithmic connection between Geometric Brow-nian Motion and Brownian Motion, many results for Brownian Motion canbe immediately translated into results for Geometric Brownian Motion. Hereis a result on the probability of victory, now interpreted as the condition ofreaching a certain multiple of the initial value. For A < 1 < B define theduration to ruin or victory, or the hitting time as
TA,B = min{t 0 : z0 exp(t+ W (t))z0
= A,z0 exp(t+ W (t))
z0= B}
Theorem 4. For a Geometric Brownian Motion with parameters and ,and A < 1 < B,
P[z0 exp(tA,B + W (TA,B))
z0= B
]=
1 A1(22)/2B1(22)/2 A1(22)/2
Quadratic Variation of Geometric Brownian Motion
The quadratic variation of Geometric Brownian Motion may be deduced fromItos formula:
dX = ( 2/2)X dt+X dWso that
(dX)2 = ( 2/2)2X2dt2 + ( 2/2)X2 dt dW +2X2(dW )2.Operating on the principle that terms of order (dt)2 and dt dW are small
and may be ignored, and that (dW )2 = dt, we obtain:
(dX)2 = 2X2 dt .
Sources
This section is adapted from: A First Course in Stochastic Processes, SecondEdition, by S. Karlin and H. Taylor, Academic Press, 1975, page 357; AnIntroduction to Stochastic Modeling 3rd Edition, by H. Taylor, and S. Karlin,
7
-
Academic Press, 1998, pages 514-516; and Introduction to Probability Models9th Edition, S. Ross, Academic Press, 2006.
Problems to Work for Understanding
1. Differentiate (ln(x/z0)t)/(t)
12pi
exp(y2/2) dy
to obtain the p.d.f. of Geometric Brownian Motion.
2. What is the probability that Geometric Brownian Motion with param-eters = 2/2 and (so that the mean is constant) ever rises tomore than twice its original value? In economic terms, if you buy astock or index fund whose fluctuations are described by this GeometricBrownian Motion, what are your chances to double your money?
3. What is the probability that Geometric Brownian Motion with param-eters = 0 and ever rises to more than twice its original value? Ineconomic terms, if you buy a stock or index fund whose fluctuations aredescribed by this Geometric Brownian Motion, what are your chancesto double your money?
4. Derive the probability of ruin (the probability of Geometric BrownianMotion hitting A < 1 before hitting B > 1).
8
-
Reading Suggestion:
References
[1] S. Karlin and H. Taylor. A Second Course in Stochastic Processes. Aca-demic Press, 1981.
[2] Sheldon M. Ross. Introduction to Probability Models. Academic Press,9th edition, 2006.
[3] H. M. Taylor and Samuel Karlin. An Introduction to Stochastic Modeling.Academic Press, third edition, 1998.
Outside Readings and Links:
1.
2.
3.
4.
I check all the information on each page for correctness and typographicalerrors. Nevertheless, some errors may occur and I would be grateful if you wouldalert me to such errors. I make every reasonable effort to present current andaccurate information for public use, however I do not guarantee the accuracy ortimeliness of information on this website. Your use of the information from thiswebsite is strictly voluntary and at your risk.
I have checked the links to external sites for usefulness. Links to externalwebsites are provided as a convenience. I do not endorse, control, monitor, orguarantee the information contained in any external website. I dont guaranteethat the links are active at all times. Use the links here with the same caution as
9
-
you would all information on the Internet. This website reflects the thoughts, in-terests and opinions of its author. They do not explicitly represent official positionsor policies of my employer.
Information on this website is subject to change without notice.Steve Dunbars Home Page, http://www.math.unl.edu/~sdunbar1Email to Steve Dunbar, sdunbar1 at unl dot eduLast modified: Processed from LATEX source on June 29, 2011
10