Term Structure Driven by general Lvy processes

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Term Structure Driven by general Lvy processes

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Title: Term Structure Driven by general Lvy processes


1
Term Structure Driven by general Lévy processes
  • Bonaventure Ho
  • HKUST, Math Dept.
  • Oct 6, 2005

2
Outline
  • Why do we need to model term structure?
  • Going from Brownian motion to Lévy process
  • Model assumption and bond price dynamics
  • Markovian short rate and stationary volatility
    structure
  • Comparison between Gaussian and Lévy setting
  • Conclusion and Discussion

3
Why do we need to model term structure?
  • Term structure is the information contained in
    the forward rate curve, short rate curve, and
    yield curve observed from market data.
  • There are deterministic relationships among
    forward rates (f), short rates (instantaneous
    interest rate)(r) and zero-coupon bond prices
    (P).
  • Usually, a model on fixed income assumes certain
    dynamics on the zero-coupon bond (eg. HJM) or on
    forward rates (eg. LIBOR). One can calculate the
    model price for f, r, and P under this model.
  • Arbitrage opportunities arise when the predicted
    values for f, r, or P are different from the
    currently observed market data.
  • Therefore, an arbitrage-free model should
    incorporate the term structure into itself.

4
History of the Gaussian model
  • No-arbitrage ? Existence of risk neutral
    measure
  • What is risk neutral measure?
  • An equivalent probability measure under which all
    tradable securities, when discounted, are
    martingales.
  • Discount factor (numeraire)
  • Log-normal model
  • Initiated by Bachelier (1900), modeling the
    French government bonds using Brownian motion.
  • Samuelson (1965) gave the price process in
    exponential form
  • Black and Scholes (1973) framework of
    log-normality of stock prices
  • Eg.) Heath-Jarrow-Morton model under the risk
    neutral measure
  • where W is a standard Brownian motion
  • Major shortcomings
  • Cannot generate volatility smile/skew as shown in
    the market data
  • Distribution itself does not fit the market data
    very well fatter tail and high peak, jump!

5
Lévy Process
  • Lévy process Lt a generalization to the
    Brownian motion.
  • stochastic process with stationary and
    independent increments
  • continuous in probability (P(Lu -Lve) ? 0, as
    u ? v for all v)
  • L00 a.s.
  • viewed as Brownian motion with jump
  • associated Lévy measure F
  • characterized by (?,?,F) for drift, variance, and
    the Lévy measure for jump
  • Examples of Lévy processes
  • Brownian motion W
  • BM with jump
  • (Merton) Merton Jump Part (Compound Poisson jump)
  • (Carr) Variance Gamma
  • (Eberlein) Hyperbolic (used as an example in the
    paper)

6
Examples of Lévy Processes
Remarks K1 is the modified Bessel function of
the third kind with index 1
7
Motivation to use Lévy processes
  • To incorporate jump into the price dynamics.
  • Merton (1976) added an independent Poisson jump
    process with normal jump size.
  • Eberlein (author of the presenting paper) and
    Keller
  • It is in certain way opposite to the Brownian
    world, since its (Lévy process) paths are purely
    discontinuous. If one looks at real stock price
    movements on the intraday scale it is exactly
    this discontinuous behavior what one
    observes. Eberlein and Keller (1997),
    promoting the hyperbolic Lévy model.
  • In 1995, they performed empirical studies and
    revealed a much better fit of return
    distributions on stock prices if the Brownian
    motion is replaced by a Lévy process. However,
    evidence for non-Gaussian behavior on bond prices
    is not as complete.
  • In 2005, Eberlein Özkan explore the LIBOR model
    using Lévy processes.
  • Volatility smile/skew cannot be generated by the
    log-normal model
  • Jump and/or stochastic volatility can generate
    such smile/skew.
  • I will discuss the jump part as a component of
    Lévy processes in this presentation, based mostly
    on the paper by Eberlein and Raible.
  • Stochastic volatility can be generated by the
    time-change method, which will be my research
    topic. Idea change the calendar time to a
    random business-activity clock.

8
Model assumptions
  • (initial bond prices)P(0,T) is deterministic,
    positive, and twice continuously differentiable
    function in T for all T?0,T for a fixed time
    horizon T
  • (boundary condition)P(T,T)1 for all T?0,T
  • (volatility bounds)Define ??(s,T) 0?s?T
    ?T?(s,T)gt0 for all (s,T)???, s??T, and
    ?(T,T)0 for all T??0,T
  • (integrability)There exists constants M, ?gt0
    such that
  • (volatility smoothness)?(s,T), defined on ?, is
    twice continuously differentiable in both
    variables and is bounded by M from 4

9
Bond price dynamics
  • In HJM model, the solution to the SDE is
    simply
  • Note that the above solution of the SDE is
    evaluated under the risk neutral measure.
  • Our generalization
  • Replace W by L, thus source of randomness
  • Replace the discount factor by a more general
    numéraire ??(t)
  • Under this numéraire, P(t,T) is a martingale
    under this measure when expressed in terms of
    units of ?(t).

10
Basic Lemmas(1)
  • Lemma 1.1
  • If f is left-continuous with limits from the
    right and bounded by M, then
  • where denotes the log MGF of L1
  • In particular, take f to be ?, we have
  • Here we relate the expected value of the source
    of randomness to the log MGF of the Lévy process,
    which is known when the process is specified.

Proof
11
Basic Lemmas(2)
  • Lemma 1.2
  • Forward rate process f(?,T) has the form
  • where ?2 denotes the partial derivative of ? in
    its second variable (T)
  • Lemma 1.3
  • The numéraire ?(t) is given by , where
    ?(t) is the usual money market account process
  • Remark Substituting the result back to our
    initial assumption, we obtainFor Gaussian
    model, ??(u)u2/2, we obtain the usual case

Proof
Proof
12
Term structure of the volatility
  • We want to explore the class of volatility
    structure so that the short rate process is
    Markovian.
  • Furthermore, we want to restrict our volatility
    structure to be stationary. That is, ? .
  • It will be proven that the volatility has either
    Vasicek volatility structure or Ho-Lee volatility
    structure!
  • or
  • for real constants

13
Proof steps(1)
  • Lemma 2.1
  • Suppose the CF of L1 is bounded, with real
    constants C, ?, ?gt0, such that
  • If f, g are continuous functions such that
    f(s)??kg(s) for all s, then the joint
    distribution of X and Y is continuous w.r.t.
    Lebesgue measure ?2 on ?2, where
  • Lemma 2.2
  • The short rate process r is Markovian if and only
    if
  • where 0ltTltUltT, and note that ? may depend on T
    and U, but not on t.
  • Corollary

Proof
Proof
14
Proof steps(2) Hull-White revisit
  • Theorem 2.3
  • Further assume that the volatility structure is
    stationary, then it must be either of Vasicek or
    Ho-Lee structure.
  • Corollary
  • Under the above stationarity and Markovian
    assumptions, we can take the volatility to have
    the Vasicek volatility structure. Then the short
    rate process follows
  • If we take L to be W, we revert back to the
    Hull-White model (or the extended Vasicek model)

Proof
15
Comparing forward rates
  • Using similar steps, we can derive the forward
    rate process.?
  • Comparing it to the Gaussian case, we obtain

16
Examples using Lévy processes (hyperbolic)
  • Eberlein and Keller (1995) used hyperbolic Lévy
    motion to model stock price dynamics. They
    claimed that the hyperbolic model allows an
    almost perfect statistical fit of stock return
    data.
  • In order to compare with the Gaussian case, we
    restrict L1 to be centered, symmetric, and with
    unit variance. That is, we pick
  • K1 and K2 denotes the modified Bessel function
    of the third kind with index 1 and 2
    respectively.
  • We investigate the case ?10 (density close to
    normal) and ?0.01 (considerably heavier weight
    in the tails and in the center than normal).
  • Vasicek volatility structure,
  • Initial term structure flat at f(0,t)0.05 for
    all t

17
Hyperbolic vs normal
18
Comparing forward rates
Figure 1 Forward rate predicted by hyperbolic
Lévy (?0.01)
Figure 2 fhyper(t,T)-fGauss(t,T)
Forward rates predicted by hyperbolic Lévy motion
are marginally higher than that predicted by
Brownian motion.
19
Comparing bond options
Bond call option current time 0, option
maturity t, bond maturity T, strike K In
the Gaussian case, there is an analytic
solution However, in the Lévy setting, the
expectation becomes Fortunately, a numerical
solution is available because the joint density
function for the last two stochastic terms can be
found. (Very complicated) Comparison method We
compare the pricing difference against the
various forward price/strike price ratio. Option
maturity 1yr, bond maturity 2yr Note that
at-the-money strike ? 0.951
20
Comparing bond options result
Figure 3 Differences in option pricing vs
forward/strike price ratio
As one can see, for ??10, the difference is
minimal, but for ?0.01, At-the-money option is
lower for the hyperbolic model (10) while the
in-the-money and out-of-the-money prices are
slightly higher, forming the W-shaped pattern as
show in Figure 3.
21
Conclusion
  • Lévy process a generalization to Brownian
    motion that allows jumps, which is more realistic
    to model bond/stock price movements.
  • Under the assumption of Markovian short rate and
    stationary volatility structure, the only
    possible volatility structures are Ho-Lee and
    Vasicek.
  • We can re-derive the mean-reverting short rate
    process (Hull-White) when we utilize Vasicek
    volatility even under Lévy process.
  • When we use hyperbolic model, forward rates
    predicted by Lévy model is always slightly higher
    than the Gaussian model.
  • For bond option, the price differences form a
    W-shaped against the forward/strike price ratio,
    due to heavier weight in the center and in the
    tail for the hyperbolic distribution.

22
Discussion
  • Future research on time-changed Lévy process,
    which can capture both jump and stochastic
    volatility.
  • Apply time-changed Lévy process to the LIBOR
    model and explore the term structure under the
    model.
  • Apply time-changed Lévy process to model
    stock/bond price movement for option pricing with
    correlation, or to model firm value movement for
    credit derivative pricing (for structural model
    evaluation)

23
References
  • Carr, P. Geman, H., Madan, D., Wu, L., Yor, M.
    (2003) Option Pricing using Integral
    Transforms. Stanford Financial Mathematics
    Seminar (Winter 2003).
  • Carr, P., Wu, L. (2003) Time-Changed Lévy
    Processes and Option Pricing. Journal of
    Financial Economics, Elsevier, Vol 71(1),
    113-141.
  • Eberlein, E., Baible, S. (1999). Term structure
    models driven by general Lévy processes.
    Mathematical Finance, Vol 9(1), 31-53.
  • Eberlein, E., Keller, U. (1995). Hyperbolic
    distributions in finance. Bernoulli, 1, 281-299.
  • Eberlein, E., Keller, U., Prause, K. (1998) New
    insights into smile, mispricing and value at
    risk the hyperbolic model. Journal of Business
    71.
  • Eberlein, E., Özkan, F. (2005) The Lévy Libor
    Model. Finance and Stochastics 9, 327-348.

24
THE END
  • Thank you for participating.

25
Appendix
  • Appendix 1.1

BACK
26
Appendix
  • Appendix 1.2
  • From (1), and lemma 1.1,
  • Take log, we get,
  • Differentiate w.r.t. T, we have,

BACK
27
Appendix
  • Appendix 1.3
  • From (1), and lemma 1.1,
  • From (2), setting t?T
  • Integrate r(T),

BACK
28
Appendix
  • Appendix 2.2
  • From (2),
  • we can see that r is Markov iff Z(T) is Markov,
    where
  • (?) Assume r is Markov. Then
  • is independent of because of
    the independent increments
  • of L. Thus the last two terms are equal,
    implying the equality of the first two terms.

BACK
29
Appendix
  • Appendix 2.2 (cont)
  • However is measurable w.r.t. . Therefore,
  • is some function of Z(T), say
  • . Then the joint distribution of X and Y,
    where
  • is only defined on (x,G(x)), thus cant be
    continuous w.r.t. ?2 on ?2. By lemma 2.1,

BACK
30
Appendix
  • Appendix 2.2 (cont)
  • (?) Assume , then

BACK
31
Appendix
  • Appendix 2.2 (cont)
  • For the corollary, simply take UT, ?then we
    have ?2(t,T) ? ?2(t,T), where ? is independent
    of t (yet it may depend on T and T). If ?0,
    then ?2(t,T)0 for all t. However, this implies
    that ?(t,T)constant for all T, which violates
    the assumption that ?(t,T)gt0 for t?T and
    ?(t,t)0. Therefore, ? ? 0.
  • Then we can define
  • and obtain our desired result, where

BACK
32
Appendix
  • Appendix 2.3
  • Write . Then . Writing
  • we have Rearranging terms, we
    have
  • Since both sides cannot depend on t or T, it
    must equal to some constant a.
  • If a0, then
  • (Ho-Lee)
  • If a??0, then
  • (Vasicek)

BACK
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