Almost-sure hedging under permanent price impact
Y.Zou
Universit´ e Paris Dauphine
April 20, 2016
Y.Zou (Universit´ e Paris Dauphine) JPS les Houches April 20, 2016 1 / 16
Almost-sure hedging under permanent price impact Y.Zou Universit e - - PowerPoint PPT Presentation
Almost-sure hedging under permanent price impact Y.Zou Universit e Paris Dauphine April 20, 2016 Y.Zou (Universit e Paris Dauphine) JPS les Houches April 20, 2016 1 / 16 Outline 1 Introduction 2 Process dynamics and hedging problems
Y.Zou
Universit´ e Paris Dauphine
April 20, 2016
Y.Zou (Universit´ e Paris Dauphine) JPS les Houches April 20, 2016 1 / 16
1 Introduction 2 Process dynamics and hedging problems
Impact rule and continuous trading dynamics Hedging problem: covered options
3 Super-replication under gamma constraint
Statement of pricing PDE Viscosity solution of the pricing PDE
Y.Zou (Universit´ e Paris Dauphine) JPS les Houches April 20, 2016 2 / 16
Objective:
Y.Zou (Universit´ e Paris Dauphine) JPS les Houches April 20, 2016 3 / 16
Objective:
1 Consider a pricing model with impact and liquidity cost. Y.Zou (Universit´ e Paris Dauphine) JPS les Houches April 20, 2016 3 / 16
Objective:
1 Consider a pricing model with impact and liquidity cost. 2 Not high frequency (no bid-ask spread), but still impact on prices. Y.Zou (Universit´ e Paris Dauphine) JPS les Houches April 20, 2016 3 / 16
Objective:
1 Consider a pricing model with impact and liquidity cost. 2 Not high frequency (no bid-ask spread), but still impact on prices. 3 Permanent impact. Y.Zou (Universit´ e Paris Dauphine) JPS les Houches April 20, 2016 3 / 16
Objective:
1 Consider a pricing model with impact and liquidity cost. 2 Not high frequency (no bid-ask spread), but still impact on prices. 3 Permanent impact.
Approach:
Y.Zou (Universit´ e Paris Dauphine) JPS les Houches April 20, 2016 3 / 16
Objective:
1 Consider a pricing model with impact and liquidity cost. 2 Not high frequency (no bid-ask spread), but still impact on prices. 3 Permanent impact.
Approach:
1 Define a continuous time trading dynamics from a discrete time rule. Y.Zou (Universit´ e Paris Dauphine) JPS les Houches April 20, 2016 3 / 16
Objective:
1 Consider a pricing model with impact and liquidity cost. 2 Not high frequency (no bid-ask spread), but still impact on prices. 3 Permanent impact.
Approach:
1 Define a continuous time trading dynamics from a discrete time rule. 2 Provide the PDE characterization: stochastic target tool. Y.Zou (Universit´ e Paris Dauphine) JPS les Houches April 20, 2016 3 / 16
Basic rule: an order δ moves the price by Xt− − → Xt = Xt− + δf(Xt−), and costs δXt− + 1 2δ2f(Xt−) = δ(Xt− + Xt 2 ).
Y.Zou (Universit´ e Paris Dauphine) JPS les Houches April 20, 2016 4 / 16
Basic rule: an order δ moves the price by Xt− − → Xt = Xt− + δf(Xt−), and costs δXt− + 1 2δ2f(Xt−) = δ(Xt− + Xt 2 ). A trading signal is an Itˆ
Y = Y0 + · bsds + · asdWs.
Y.Zou (Universit´ e Paris Dauphine) JPS les Houches April 20, 2016 4 / 16
Trade at times tn
i = iT/n the quantity δn tn
i = Ytn i − Ytn i−1. Y.Zou (Universit´ e Paris Dauphine) JPS les Houches April 20, 2016 5 / 16
Trade at times tn
i = iT/n the quantity δn tn
i = Ytn i − Ytn i−1.
The stock price evolves according to X = Xtn
i +
·
tn
i
σ(Xs)dWs between two trades.(can add a drift or be multivariate.)
Y.Zou (Universit´ e Paris Dauphine) JPS les Houches April 20, 2016 5 / 16
Trade at times tn
i = iT/n the quantity δn tn
i = Ytn i − Ytn i−1.
The stock price evolves according to X = Xtn
i +
·
tn
i
σ(Xs)dWs between two trades.(can add a drift or be multivariate.) Dynamics of the wealth and of the asset: discrete trading and pass to the limit.
Y.Zou (Universit´ e Paris Dauphine) JPS les Houches April 20, 2016 5 / 16
Passing to the limit n → ∞, we have the following convergence in S2 Y = Y0 + · bsds + · asdWs X = X0 + · σ(Xs)dWs + · f(Xs)dYs + · (µ + asσf′)(Xs)ds V = V0 + · YsdXs + 1 2 · a2
sf(Xs)ds,
at a speed √n, where V = cash part + Y X = “portfolio value”.
Y.Zou (Universit´ e Paris Dauphine) JPS les Houches April 20, 2016 6 / 16
Covered options: No initial/final market impact.
Y.Zou (Universit´ e Paris Dauphine) JPS les Houches April 20, 2016 7 / 16
Covered options: No initial/final market impact. Super-replication: The minimum initial total wealth to cover the final payoff in almost sure sense.
Y.Zou (Universit´ e Paris Dauphine) JPS les Houches April 20, 2016 7 / 16
Covered options: No initial/final market impact. Super-replication: The minimum initial total wealth to cover the final payoff in almost sure sense. Gamma constraint: Re-write the dynamics of Y as below: dY = a dW + b dt = γa(X) dX + µa,b
Y (X) dt
with γa = a/(σ + af). Then γa(X) is bounded by some function.
Y.Zou (Universit´ e Paris Dauphine) JPS les Houches April 20, 2016 7 / 16
Super-hedging price under gamma constraint: v(t, x) := inf{v = c + yx : (c, y) ∈ R2 s.t. Gγ(t, x, v, y) = ∅} where Gγ(t, x, v, y) is the set of (a, b) s.t. φ := (y, a, b) satisfies: V t,x,v,φ
T
≥ g(Xt,x,φ
T
), and γa(X) ≤ ¯ γ(X) with f¯ γ < 1 − ǫ, ǫ > 0.
Y.Zou (Universit´ e Paris Dauphine) JPS les Houches April 20, 2016 8 / 16
If we follow the delta-hedging rule: V = v(·, X) , and Y = ∂xv(·, X)
Y.Zou (Universit´ e Paris Dauphine) JPS les Houches April 20, 2016 9 / 16
If we follow the delta-hedging rule: V = v(·, X) , and Y = ∂xv(·, X) Equating the dt terms on V = v(·, X) & dX terms on Y = ∂xv(·, X): 1 2a2f(X) = ∂tv(·, X) + 1 2(σ + af)2(X)∂2
xxv(·, X)
γa = ∂2
xxv(·, X)
Y.Zou (Universit´ e Paris Dauphine) JPS les Houches April 20, 2016 9 / 16
If we follow the delta-hedging rule: V = v(·, X) , and Y = ∂xv(·, X) Equating the dt terms on V = v(·, X) & dX terms on Y = ∂xv(·, X): 1 2a2f(X) = ∂tv(·, X) + 1 2(σ + af)2(X)∂2
xxv(·, X)
γa = ∂2
xxv(·, X)
By definition of γa and some calculate:
2 σ2 (1 − f∂2
xxv)∂2 xxv
Gamma constraint insures the non-singularity of the PDE.
Y.Zou (Universit´ e Paris Dauphine) JPS les Houches April 20, 2016 9 / 16
Pricing PDE: on [0, T) × R F[v¯
γ](t, x)
:= min
γ − 1
2 σ2 (1 − f∂2
xxv¯ γ)∂2 xxv¯ γ, ¯
γ − ∂2
xxv¯ γ
Propagation of the gamma constraint to the boundary: v¯
γ(T−, ·) = ˆ
g on R where ˆ g is the smallest (viscosity) super-solution of min{ϕ − g, ¯ γ − ∂2
xxϕ} = 0
Y.Zou (Universit´ e Paris Dauphine) JPS les Houches April 20, 2016 10 / 16
Theorem (Geometric Dynamic Programming Principle)
If V0 > v(0, X0), then there exists (a, b, Y0) such that Vθ ≥ v(θ, Xθ) for any stopping time θ ∈ [0, T]. Result: A super-solution v¯
γ ≤ v¯ γ. cf. N.Touzi, M.Soner.
Y.Zou (Universit´ e Paris Dauphine) JPS les Houches April 20, 2016 11 / 16
Objective: Construct a solution ¯ v¯
γ ≥ v¯ γ.
Theorem
Define the shaken operator F ǫ[ϕ](t, x) := min
x′∈Bǫ(x) min
σ2(x′) 2(1 − f(x′)∂2
xxϕ), ¯
γ(x′)−∂2
xxϕ
then ∀ǫ > 0, ∃¯ vǫ
¯ γ the unique continuous viscosity solution of
F ǫ[ϕ](t, x)✶[0,T) + [ϕ − (ˆ g + ǫ)]✶{T} = 0 Moreover, ¯ vǫ
¯ γ ≥ ˆ
g + ǫ/2 on [T − cǫ, T] × R.
Y.Zou (Universit´ e Paris Dauphine) JPS les Houches April 20, 2016 12 / 16
Objective: Construct a solution ¯ v¯
γ ≥ v¯ γ.
✶ ✶
Y.Zou (Universit´ e Paris Dauphine) JPS les Houches April 20, 2016 13 / 16
Objective: Construct a solution ¯ v¯
γ ≥ v¯ γ.
By the stability of viscosity solution: ¯ vǫ
¯ γ → ¯
v¯
γ,
as ǫ → 0 where ¯ v¯
γ is the unique viscosity solution of
F[ϕ](t, x)✶[0,T) + (ϕ − ˆ g)✶{T} = 0
Y.Zou (Universit´ e Paris Dauphine) JPS les Houches April 20, 2016 13 / 16
Objective: Construct a solution ¯ v¯
γ ≥ v¯ γ.
By the stability of viscosity solution: ¯ vǫ
¯ γ → ¯
v¯
γ,
as ǫ → 0 where ¯ v¯
γ is the unique viscosity solution of
F[ϕ](t, x)✶[0,T) + (ϕ − ˆ g)✶{T} = 0 Remain to prove: ¯ v¯
γ ≥ v¯ γ.
Y.Zou (Universit´ e Paris Dauphine) JPS les Houches April 20, 2016 13 / 16
Theorem
For ψ ∈ C∞, define ψδ = δ−2ψ(·/δ). Then ¯ vǫ,δ
¯ γ
:= ¯ vǫ
¯ γ ⋆ ψδ is a
super-solution of F[¯ vǫ,δ
¯ γ ](t, x)✶[δ,T) + (¯
vǫ,δ
¯ γ − ˆ
g)✶{T} = 0 Then Y := ∂x¯ vǫ,δ
¯ γ (·, X) provides a super-hedging strategy, i.e. ¯
vǫ,δ
¯ γ
≥ v¯
γ.
Moreover, lim
ǫ,δ→0¯
vǫ,δ
¯ γ
= ¯ v¯
γ.
Conclusion: ¯ v¯
γ = lim ǫ,δ→0 ¯
vǫ,δ
¯ γ
≥ v¯
γ ≥ v¯ γ ≥ ¯
v¯
γ
Y.Zou (Universit´ e Paris Dauphine) JPS les Houches April 20, 2016 14 / 16
Model: dXt = 0.2 dWt; Butterfly: g(x) = (x + 1)+ − 2x+ + (x − 1)+
1 2 0.0 0.2 0.4 0.6 0.8 x Value Function
1 2 0.00 0.05 0.10 0.15 x Price Difference
Figure 1: Left: Super-hedging price. Dashed line: λ = 0.5, ¯ γ = 1.75; solid line: λ = 0, ¯ γ = 1.75; dotted line: λ = 0, ¯ γ = +∞. Right: Difference with the price associated to λ = 0, ¯ γ = +∞. Dashed line: λ = 0.5, ¯ γ = 1.75; solid line: λ = 0, ¯ γ = 1.75 .
Y.Zou (Universit´ e Paris Dauphine) JPS les Houches April 20, 2016 15 / 16
Y.Zou (Universit´ e Paris Dauphine) JPS les Houches April 20, 2016 16 / 16