SLIDE 1 On the Martingale Property
- f Exponential Local Martingales
Aleksandar Mijatovi´ c1 Mikhail Urusov2
1University of Warwick 2Ulm University
Analysis, Stochastics, and Applications. A Conference in Honour of Walter Schachermayer — Vienna University, July 12–16, 2010
SLIDE 2
Outline
Introduction Formulation of the main result Some examples Ways of proving the theorem and their restrictions
SLIDE 3
Outline
Introduction Formulation of the main result Some examples Ways of proving the theorem and their restrictions
SLIDE 4 Description of the main result
Diffusion Y: dYt = µ(Yt) dt + σ(Yt) dWt Zt = E . b(Ys) dWs
= exp t b(Ys) dWs − 1 2 t b2(Ys) ds
- Z nonnegative local martingale =
⇒ supermartingale Z martingale ⇐ ⇒ EZt = 1, t ∈ [0, ∞) Input: functions µ, σ, and b Output: deterministic necessary and sufficient conditions for Z to be a true martingale in terms of µ, σ, and b
SLIDE 5 Description of the main result
Diffusion Y: dYt = µ(Yt) dt + σ(Yt) dWt Zt = E . b(Ys) dWs
= exp t b(Ys) dWs − 1 2 t b2(Ys) ds
- Z nonnegative local martingale =
⇒ supermartingale Z martingale ⇐ ⇒ EZt = 1, t ∈ [0, ∞) Input: functions µ, σ, and b Output: deterministic necessary and sufficient conditions for Z to be a true martingale in terms of µ, σ, and b Questions Literature Where applies?
SLIDE 6
Literature
Sufficient conditions Novikov (1972), Kazamaki (1977) Many participants of AnStAp10 Cheridito, Filipovi´ c, and Yor (2005) Necessary and sufficient conditions Blei and Engelbert (2009) Mayerhofer, Muhle-Karbe, and Smirnov (2009)
SLIDE 7 Where applies?
SA: examples and counterexamples MF: characterizations of NFLVR, NGA, and NRA in
- ne-dimensional diffusion setting
MF: other problems also reduce to this setting with appropriately chosen µ, σ, b
SLIDE 8
Precise formulation of the problem
J = (l, r), −∞ ≤ l < r ≤ ∞ dYt = µ(Yt) dt + σ(Yt) dWt, Y0 = x0 ∈ J ζ the explosion time of Y
◮ σ(x) = 0 ∀x ∈ J ◮ 1/σ2, µ/σ2 ∈ L1 loc(J)
Zt = exp{ t∧ζ b(Ys) dWs − (1/2) t∧ζ b2(Ys) ds}
◮ b2/σ2 ∈ L1 loc(J) ◮ Zt := 0 for t ≥ ζ on {
ζ
0 b2(Ys) ds = ∞}
SLIDE 9
Precise formulation of the problem
J = (l, r), −∞ ≤ l < r ≤ ∞ dYt = µ(Yt) dt + σ(Yt) dWt, Y0 = x0 ∈ J ζ the explosion time of Y
◮ σ(x) = 0 ∀x ∈ J ◮ 1/σ2, µ/σ2 ∈ L1 loc(J)
Zt = exp{ t∧ζ b(Ys) dWs − (1/2) t∧ζ b2(Ys) ds}
◮ b2/σ2 ∈ L1 loc(J) ◮ Zt := 0 for t ≥ ζ on {
ζ
0 b2(Ys) ds = ∞}
Question Why considering possibility of explosion?
SLIDE 10
Why explosions?
◮ Examples and counterexamples ◮ In MF there are models, where explosion happens.
E.g. CEV: for α ∈ R, dYt = cY α
t dWt,
Y0 = x0 ∈ J := (0, ∞). Y explodes at 0 ⇐ ⇒ α < 1
SLIDE 11
Outline
Introduction Formulation of the main result Some examples Ways of proving the theorem and their restrictions
SLIDE 12 Terminology
s: (l, r) → R scale function of diffusion Y, ρ := s′ r is good if s(r) < ∞ and (s(r) − s)b2 ρσ2 ∈ L1
loc(r−)
l is good if . . . Auxiliary diffusion (with the same state space J = (l, r)): d Yt = (µ + bσ)( Yt) dt + σ( Yt) d Wt,
- Y0 = x0
- s: J → R scale function of diffusion
Y, ρ := s′
SLIDE 13 Useful facts
s(r) < ∞ and (s(r) − s)b2 ρσ2 ∈ L1
loc(r−)
- r, equivalently,
- s(r) < ∞ and (
s(r) − s)b2
∈ L1
loc(r−)
- 2. If one of the diffusions Y and
Y explodes at r and the other does not, then r is bad These facts are often helpful in the application of the theorem below to specific situations
SLIDE 14
Main result
Theorem Z martingale ⇐ ⇒ ((a) or (b)) and ((c) or (d)) (a) Y does not explode at r (b) r is good (c) Y does not explode at l (d) l is good Theorem above together with Fact 2 on the previous slide imply Corollary Suppose Y is non-explosive. Then Z is a martingale ⇐ ⇒ Y is non-explosive
SLIDE 15
Outline
Introduction Formulation of the main result Some examples Ways of proving the theorem and their restrictions
SLIDE 16 Example: funny
Fix α > −1 and define diffusion Y by dYt = |Yt|α dt + dWt, Y0 = x0 ∈ J := R. Let Z be the local martingale given by Zt = exp t∧ζ Ys dWs − 1 2 t∧ζ Y 2
s ds
Our results imply the following classification: α ∈ (−1, 1]: Z martingale, not u.i. α ∈ (1, 3]: Z strict local martingale α > 3: Z u.i. martingale
SLIDE 17 Example: bubbles and not only
dYt = σ(Yt) dWt, Y0 = x0 ∈ J := (0, ∞). We stop Y after it reaches 0 Corollary Y is a martingale ⇐ ⇒ x/σ2(x) / ∈ L1
loc(∞−)
Delbaen and Shirakawa (2002) Carr, Cherny, and Urusov (2007) Reduction to our setting Yt = x0E . σ(Ys) Ys dWs
SLIDE 18 Example: bubbles and not only
dYt = σ(Yt) dWt, Y0 = x0 ∈ J := (0, ∞). We stop Y after it reaches 0 Corollary Y is a martingale ⇐ ⇒ x/σ2(x) / ∈ L1
loc(∞−)
Delbaen and Shirakawa (2002) Carr, Cherny, and Urusov (2007) Reduction to our setting Yt = x0E . σ(Ys) Ys dWs
Why interesting? SA: nice problem, simple explicit answer MF: characterization of existence/absence of bubbles in
- ne-dimensional diffusion models
SLIDE 19
Why interesting — another MF argument
Stock price Y (complete market), interest rate := 0 (YT − K)+ − (K − YT)+ = YT − K Ct − Pt = E(YT|Ft) − K (1) Ct − Pt = Yt − K (2) (1) holds always, (2) holds iff Y is a martingale Arbitrageurs = ⇒ in practice (2) tends to hold, not (1) = ⇒ practitioners would not work with a model, where Y is not a martingale
SLIDE 20 Further applications in MF
Characterizations of NFLVR, NGA, and NRA in
- ne-dimensional diffusion setting, i.e.
dYt = µ(Yt) dt + σ(Yt) dWt, Y0 = x0 ∈ J := (0, ∞)
◮ For NFLVR, b(x) := −µ(x)/σ(x) does only a part of the job ◮ Recall Delbaen and Schachermayer (1998)
A simple counterexample to several problems in the theory
◮ For NRA, b(x) := σ(x)/x − µ(x)/σ(x)
SLIDE 21
Outline
Introduction Formulation of the main result Some examples Ways of proving the theorem and their restrictions
SLIDE 22
A possible way
Reduce the problem to the canonical setting 1 ? = EPZt = limn EP(ZtI(τn > t)) = . . . = P(ζ > t). Done! Recall the talk by Damir Filipovi´ c Sin (1998), Carr, Cherny, and Urusov (2007) This method works only if the coordinate process is nonexplosive under P. Otherwise lim
n EP(ZtI(τn > t)) = EP(ZtI(ζ > t)), which may be < EPZt
SLIDE 23
Our approach
= ⇒ we needed to refuse this argument and elaborate a different one in order to consider the possibility of explosion under P This is needed in MF, as they sometimes consider models with explosions (e.g. CEV) From the viewpoint of SA, the reward that we get is a possibility to construct pathological (counter)examples
SLIDE 24 On my website
c and M. Urusov (2010). On the martingale property
- f certain local martingales. To appear in Probability Theory
and Related Fields.
c and M. Urusov (2010). Deterministic criteria for the absence of arbitrage in diffusion models. To appear in Finance and Stochastics. The talk covered a part of the first paper.
SLIDE 25
Dear Walter, happy birthday and many happy returns!
SLIDE 26 Blei, S. and H.-J. Engelbert (2009). On exponential local martingales associated with strong Markov continuous local martingales. Stochastic Process. Appl. 119(9), 2859–2880. Carr, P ., A. Cherny, and M. Urusov (2007). On the martingale property of time-homogeneous diffusions. Preprint, available at: http://www.uni-ulm.de/mawi/finmath/people/urusov.html. Cheridito, P ., D. Filipovi´ c, and M. Yor (2005). Equivalent and absolutely continuous measure changes for jump-diffusion processes.
- Ann. Appl. Probab. 15(3), 1713–1732.
Delbaen, F . and W. Schachermayer (1998). A simple counter-example to several problems in the theory
Mathematical Finance 8(2), 1–11. Delbaen, F . and H. Shirakawa (2002).
SLIDE 27 No arbitrage condition for positive diffusion price processes. Asia-Pacific Financial Markets 9, 159–168. Kazamaki, N. (1977). On a problem of Girsanov. Tˆ
- hoku Math. J. 29(4), 597–600.
Mayerhofer, E., J. Muhle-Karbe, and A. Smirnov (2009). A characterization of the martingale property of exponentially affine processes. Preprint, available at: http://www.mat.univie.ac.at/˜muhlekarbe/. Novikov, A. A. (1972). A certain identity for stochastic integrals. Theory Probab. Appl. 17, 761–765. Sin, C. A. (1998). Complications with stochastic volatility models.
- Adv. in Appl. Probab. 30(1), 256–268.