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Maria Adler

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The Black-Scholes Model. Fit of the BS Model to Empirical Data. Hyperbolic Distribution ... tails than for the normal distribution, where the log-density is a parabola ... – PowerPoint PPT presentation

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Title: Maria Adler


1
Hyperbolic Processes in Finance
Alternative Models for Asset Prices
2
Outline
  • The Black-Scholes Model
  • Fit of the BS Model to Empirical Data
  • Hyperbolic Distribution
  • Hyperbolic Lévy Motion
  • Hyperbolic Model of the Financial Market
  • Equivalent Martingale Measure
  • Option Pricing in the Hyperbolic Model
  • Fit of the Hyperbolic Model to Empirical Data
  • Conclusion

3
The Black-Scholes Model
price process of a security described by the SDE
volatility
drift
Brownian motion
price process of a risk-free bond
interest rate
4
The Black-Scholes Model
  • Brownian motion has continuous paths
  • stationary and independent increments
  • market in this model is complete
  • ? allows duplication of the cash flow of
  • derivative securities and pricing by
  • arbitrage principle

5
Fit of the BS Model to Empirical Data
  • statistical analysis of daily stock-price data
    from 10 of the DAX30 companies
  • time period 2 Oct 1989 30 Sep 1992 (3 years)
  • ? 745 data points each for the returns
  • Result assumption of Normal distribution
    underlying the
  • Black- Scholes model does not
    provide a good fit to
  • the market data

6
Fit of the BS Model to Empirical Data
Quantile-Quantile plots density-plots for the
returns of BASF and Deutsche Bank to test
goodness of fit Fig. 4, E./K., p.7
7
Fit of the BS Model to Empirical Data
BASF
Deutsche Bank
8
Fit of the BS Model to Empirical Data
  • Brownian motion represents the net random effect
    of the various factors of influence in the
    economic environment
  • (shocks price-sensitive information)
  • actually, one would expect this effect to be
    discontinuous, as the individual shocks arrive
  • indeed, price processes are discontinuous looked
    at closely enough (discrete shocks)

9
Fit of the BS Model to Empirical Data
  • Fig. 1, E./K., p.4
  • typical path of a Brownian motion
  • continuous
  • the qualitative picture does not change if we
    change the time-scale,
  • due to self-similarity property

10
Fit of the BS Model to Empirical Data
  • real stock-price paths change significantly if we
    look at them on different time-scales
  • Fig. 2, E./K., p.5 daily stock-prices of
    five major companies over a period of three years

11
Fit of the BS Model to Empirical Data
  • Fig. 3, E./K., p.6
  • path, showing price changes of the Siemens stock
    during a single day

12
Fit of the BS Model to Empirical Data
  • Aim to model financial data more precisely than
    with the BS model
  • ? find a more flexible distribution than the
    normal distr.
  • ? find a process with stationary and
    independent increments (similar
  • to the Brownian motion), but with a more
    general distr.
  • this leads to models based on Lévy processes
  • ? in particular Hyperbolic processes
  • B./K. and E./K. showed that the Hyperbolic model
    is a more realistic market model than the
    Black-Scholes model, providing a better fit to
    stock prices than the normal distribution,
    especially when looking at time periods of a
    single day

13
Hyperbolic Distribution
  • introduced by Barndorff-Nielsen in 1977
  • used in various scientific fields
  • - modeling the distribution of the grain size
    of sand
  • - modeling of turbulence
  • - use in statistical physics
  • Eberlein and Keller introduced hyperbolic
    distribution functions into finance

14
Hyperbolic Distribution
  • Density of the Hyperbolic distribution

modified Bessel function with index 1
characterized by four parameters
tail decay behavior of density for
shape
skewness / asymmetry
location
scale
15
Hyperbolic Distribution
  • Density-plots for different parameters
  • 9 0
  • 0 0 0
  • 1 1
  • 0 0 0

16
Hyperbolic Distribution
  • 4
  • 0
  • 1
  • 3 2

17
Hyperbolic Distribution
  • 1
  • 0 0
  • 3
  • 0 0

18
Hyperbolic Distribution
  • the log-density is a hyperbola (? reason for the
    name)
  • this leads to thicker tails than for the normal
    distribution, where the log-density is a parabola

slopes of the asymptotics
location
curvature near the mode
19
Hyperbolic Distribution
  • Plots of the log-density for different parameters
  • 6
  • 1
  • 6
  • 0 0

20
Hyperbolic Distribution
  • 2
  • 1
  • 10
  • 0 0

21
Hyperbolic Distribution
  • 4 4
  • 2 2
  • 1 8
  • 1 1

22
Hyperbolic Distribution
  • setting
  • another parameterization of the density can
    be obtained
  • and invariant under changes of
    location and scale

? shape triangle
23
Hyperbolic Distribution
generalized inverse Gaussian
generalized inverse Gaussian
Fig. 6, E./K., p.13
24
Hyperbolic Distribution
  • Relation to other distributions

Normal distribution
generalized inverse Gaussian distribution
Exponential distribution
25
Hyperbolic Distribution
  • Representation as a mean-variance mixture of
    normals
  • Barndorff-Nielsen and Halgreen (1977)
  • the mixing distribution is the generalized
    inverse Gaussian with density
  • consider a normal distribution with mean
    and variance
  • such that is a random variable with
    distribution
  • the resulting mixture is a hyperbolic
    distribution

26
Hyperbolic Distribution
  • Infinite divisibility
  • Definition
  • Suppose is the characteristic
    function of a distribution.
  • If for every positive integer ,
    is also the power of a char.
  • fct., we say that the distribution is infinitely
    divisible.

The property of inf. div. is important to be able
to define a stochastic process with
independent and stationary (identically
distr.) increments.
27
Hyperbolic Distribution
  • Barndorff-Nielsen and Halgreen showed that the
    generalized inverse Gaussian distribution is
    infinitely divisible.
  • Since we obtain the hyperbolic distribution as a
    mean-variance mixture from the gen. inv. Gaussian
    distr. as a mixing distribution, this transfers
    infinite divisibility to the hyperbolic
    distribution.
  • ? The hyperbolic distribution is infinitely
    divisible and we can define the hyperbolic Lévy
    process with the required properties.

28
Hyperbolic Distribution
  • To fit empirical data it suffices to concentrate
    on the centered
  • symmetric case.
  • Hence, consider the hyperbolic density

29
Hyperbolic Distribution
  • Characteristic function
  • The corresponding char. fct. to
    is given by
  • All moments of the hyperbolic distribution exist.

30
Hyperbolic Lévy Motion
  • Definition
  • Define the hyperbolic Lévy process corresponding
    to the inf. div.
  • hyperbolic distr. with density

stoch. process on a prob. space
starts at 0
has distribution and char.
fct.
31
Hyperbolic Lévy Motion
  • For the char. fct. of
    we get

The density of is given by the
Fourier Inversion formula
only has hyperbolic distribution
32
Hyperbolic Lévy Motion
Fig. 10, E./K., p.19 densities for
33
Hyperbolic Lévy Motion
  • Recall for a general Lévy process
  • char. fct. is given by the Lévy-Khintchine
    formula
  • characterized by
  • a drift term
  • a Gaussian (e.g. Brownian) component
  • a jump measure

34
Hyperbolic Lévy Motion
  • in the symmetric centered case the hyperbolic
    Lévy motion
  • is a pure jump process
  • ? the Lévy-Khintchine representation of the char.
    function is

with being the density of the Lévy
measure
35
Hyperbolic Lévy Motion
  • Density of the Lévy measure
  • and are Bessel functions
  • using the asymptotic relations about Bessel
    functions, one can deduce that
  • behaves like 1 / at the origin
    (x ? 0)

- Lévy measure is infinite, - hyp. Lévy motion
has infinite variation, - every path has
infinitely many small jumps in every finite
time-interval
36
Hyperbolic Lévy Motion
  • The infinite Lévy measure is appropriate to model
    the everyday movement of ordinary quoted stocks
    under the market pressure of many agents.
  • The hyperbolic process is a purely discontinuous
    process but there exists a càdlag modification
    (again a Lévy process) which is always used.
  • The sample paths of the process are almost surely
  • continuous from the right and have limits
    from the left.

37
Hyperbolic Model of the Financial Market
price process of a risk-free bond
interest rate process
price process of a stock
hyperbolic Lévy motion
38
Hyperbolic Model of the Financial Market
  • to pass from prices to returns take logarithm of
    the price process

results in two terms
hyperbolic term
sum-of-jumps term
  • after approximation to first order the remaining
    term is
  • since Lévy measure is infinite and there are
    infinitely many small jumps,
  • the small jumps predominate in this term
    squared, they become even
  • smaller and are negligible

the sum-of-jumps term can be neglected and to a
first approximation we get hyperbolic returns
39
Hyperbolic Model of the Financial Market
  • Model with exactly hyperbolic returns along
    time-intervals of length 1

stock-price process
hyperbolic Lévy motion
40
Equivalent Martingale Measure
  • Definition
  • An equivalent martingale measure is a
    probability measure Q, equivalent to P such that
    the discounted price process
  • is a martingale w.r.t. to Q.
  • Complication in the Hyperbolic model
  • financial market is incomplete
  • no unique equivalent martingale measure (infinite
    number of e.m.m.)
  • we have to choose an appropriate e.m.m. for
    pricing purposes

41
Equivalent Martingale Measure
  • Two approaches to find a suitable e.m.m.
  • 1) minimal-martingale measure
  • 2) risk-neutral Esscher measure
  • In the Hyperbolic model the focus is on the
    risk-neutral Esscher measure. It is found with
    the help of Esscher transforms.

42
Equivalent Martingale Measure
  • Esscher transforms
  • The general idea is to define equivalent measures
    via
  • choose to satisfy the required
    martingale conditions
  • The measure P encapsulates information about
    market behavior
  • pricing by Esscher transforms amounts to choosing
    the e.m.m.
  • which is closest to P in terms of information
    content.

43
Equivalent Martingale Measure
  • In the hyperbolic model

moment generating function of the hyperbolic Lévy
motion
  • The Esscher transforms are defined by
  • The equiv. mart. measures are defined via

is called the Esscher measure of parameter
44
Equivalent Martingale Measure
  • The risk-neutral Esscher measure is the Esscher
    measure of parameter such that
    the discounted price process
  • is a martingale w.r.t. (r is the
    daily interest rate).
  • Find the optimal parameter !

45
Equivalent Martingale Measure
  • If is the density corresponding to
    the hyp. process,
  • define a new density via

? Density corresponding to the distribution of
under the Esscher measure

46
Equivalent Martingale Measure
  • To find consider the martingale condition
  • (expectation w.r.t. the Esscher measure
    )
  • This leads to
  • The moment generating function can be computed as

47
Equivalent Martingale Measure
  • Plug in, rearrange and take logarithms to get
  • Given the daily interest rate r and the
    parameters this
  • equation can be solved by numerical methods
    for the martingale
  • parameter .
  • ? determines the risk-neutral Esscher
    measure

48
Option Pricing in the Hyperbolic Model
  • Pricing a European call with maturity T and
    strike K ,
  • using the risk-neutral Esscher measure
  • A usefull tool will be the Factorization formula
  • Let g be a measurable function and h, k and t be
    real numbers, then

49
Option Pricing in the Hyperbolic Model
  • By the risk-neutral valuation principle (using
    the risk-neutral Esscher
  • measure) we have to calculate the following
    expectation

Pricing-Formula for a European call with strike K
and maturity T
50
Option Pricing in the Hyperbolic Model
Determine c
51
Option Pricing in the Hyperbolic Model
  • Computation of standard hedge parameters
    (greeks)
  • E.g. compute the delta of a European call C

by using subsequently the definition of
and
  • integral has to be computed numerically
  • useful for aspects of risk-management

52
Fit of the Hyperbolic Model to Empirical Data
  • E./K. performed the same statistical analysis for
    the hyperbolic model as for the Black-Scholes
    model (to fit empirical data)
  • E.g. consider again the QQ-plots and density
    plots
  • Fig. 8, E./K., p.16 BASF
  • Fig. 9, E./K., p.17 Deutsche Bank

53
Fit of the Hyperbolic Model to Empirical Data
54
Fit of the Hyperbolic Model to Empirical Data
55
Fit of the Hyperbolic Model to Empirical Data
56
Fit of the Hyperbolic Model to Empirical Data
57
Fit of the Hyperbolic Model to Empirical Data
  • ? QQ-plots almost no deviation from
    straight line
  • assumption of
    hyperbolic distribution is supported
  • ? density plots hyperbolic distribution provides
    an almost excellent fit
  • to the empirical data,
    esp. at the center and tails

The hyperbolic distribution fits empirical data
better than the normal distribution.
58
Fit of the Hyperbolic Model to Empirical Data
  • B./K. performed a similar study
  • - daily BMW returns during Sep 1992 Jul
    1996 (100 data points)
  • - standard estimates for mean and variance
    of normal distribution
  • - computer program to estimate parameters of
    the hyp. distr.
  • ? maximum likelihood estimates
  • Fig. 2, B./K., p.14 Density plots

Comparison of option prices obtained from the
Black-Scholes model and the hyperbolic model
with real market prices shows, that the
hyperbolic model provides a better fit.
59
Fit of the Hyperbolic Model to Empirical Data
60
Conclusion
  • The hyperbolic distribution provides a good fit
    for a range of financial data, not only in the
    tails but throughout the distribution
  • ? more accurate model for stock prices /
    returns
  • The hyperbolic model should esp. be preferred
    over the classical Black-Scholes model, when
    modeling daily stock returns, i.e. when looking
    at time periods of a single day.

61
Conclusion
  • For longer time periods the Black-Scholes model
    is still appropriate
  • E./K. estimated the parameters of
    the hyperbolic distr.
  • (2nd param.) for the stock returns of
    Commerzbank, considering
  • different time periods, i.e. 1, 4, 7, .,
    22 trading days

62
Conclusion
Fig. 7, E./K., p.15
the pairs ( , ) are given in the shape
triangle and one can see, that the parameters
tend to the normal distribution limit as the
number of trading days increases
Normal Distribution Limit
63
References
  •  Bingham, Kiesel (2001) Modelling asset returns
    with hyperbolic
  • distributions. In "Return Distributions in
    Finance", Butterworth-
  • Heinemann, p. 1-20 
  • Eberlein, Keller (1995) Hyperbolic
    distributions in finance.
  • Bernoulli 1, p. 281-299
  •  Barndorff-Nielsen, Halgreen (1977) Infinite
    divisibility of the
  • hyperbolic and generalized inverse Gaussian
    distributions. 
  • Wahrscheinlichkeitstheorie und verwandte
    Gebiete 38, p. 309-311
  • Hélyette Geman Pure jump Lévy processes for
    asset price modelling. Journal of Banking
    Finance 26, p. 1297-1316

64
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