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Understanding Delta-Hedged Option Returns in Stochastic Volatility Environments

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Abstract

In this paper, we provide a novel representation of delta-hedged option returns in a stochastic volatility environment. The representation of delta-hedged option returns provided in this paper consists of two terms: volatility risk premium and parameter estimation risk. In an empirical analysis, we examine delta-hedged option returns based on the result of a historical simulation with the USD-JPY currency option market data from October 2003 to June 2010. We find that the delta-hedged option returns for OTM put options are strongly affected by parameter estimation risk as well as the volatility risk premium, especially in the post-Lehman shock period.

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Notes

  1. See 9.3 in Shreves (2004) for details.

  2. Details will be described in Sect. 4.1.

  3. In this section, we focus on an European call option, but the discussion and results provided in this section can apply more generally to other options such as put options and straddle options.

  4. We assume that the SDE (2) has a strong solution for \(\tilde{S}_t\) under the parameters of \(\tilde{\mu _t}\), \(\tilde{\theta _t}\), \(\tilde{\eta _t}\), and \(\tilde{\rho }\).

  5. Carr and Wu (2009) assume that the futures price \(F_t\) solves the following stochastic differential equation,

    $$\begin{aligned} dF_t = F_{t-} \sigma _{t-} dW_t + \int _{(-\infty , \infty ) \backslash {0}} F_{t-} \big ( e^x -1 \big ) \big [ \mu (dx,dt)-\nu _t(x)dxdt \big ] \end{aligned}$$

    (see Carr and Wu 2009 for details on a notation). The equation represented above models the futures price change as the summation of the increments of two orthogonal martingales: a purely continuous martingale and a purely discontinuous (jump) martingale. This decomposition is generic for any continuous time martingales. So, in general, Proposition 2 should be stated including the effect of jump component. But, in this paper, we only assume a continuous martingale in order to represent an underlying exchange rate process, so we leave the term induced by the jump component out of (15) in Proposition 2.

  6. Brunner and Hafner (2003) approximate the implied volatility \(\sigma _t^T(K)\), whose the strike price is \(K\) and the maturity date is \(T\), as a polynomial as follows; \(\sigma _t^T(K)=\beta _0 + \beta _1 M + \beta _2 M^2 + D \beta _3 M^3\), where \( D \equiv 0 (if M \le 0), \equiv 1 (if M > 0) \) and \( M \equiv \log \big ( \frac{K}{F_t^T} \big ) / \sqrt{T-t} \), under the definition that \(F_t^T\) is a forward rate whose the maturity date is \(T\) at each time \(t\).

  7. The ATM-forward straddle contract is a combination of a call and a put option with the same strike price of ATM forward rate and the same maturity to the underlying forward contract.

  8. As we mentioned before, we take account of transactions costs only in selling the option contracts in our empirical study.

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Correspondence to Hiroshi Sasaki.

Additional information

I have benefitted from many helpful comments by an anonymous referee, and for their helpful comments on this article, I also wish to thank Hidetoshi Nakagawa, Kazuhiko Ohashi, Toshiki Honda, Nobuhiro Nakamura, Fumio Hayashi, Tatsuyoshi Okimoto, Ryozo Miura, and the participants at the 2010 JAFEE Conference and the RIMS Workshop on Financial Modeling and Analysis.

Appendices

Appendix 1: Proof of Proposition 2

The following equation can be derived by applying Ito’s lemma to the market price \(C_t^{M} = G(t, S_t, \sigma _t)\),

$$\begin{aligned} \begin{aligned} C_{t+\tau }^{M}&= C_t^{M} + \int _t^{t+\tau } \frac{\partial G}{\partial S}(u,S_u,\sigma _u)d S_u \\&\quad \,\, + \int _t^{t+\tau } \frac{\partial G}{\partial \sigma }(u,S_u,\sigma _u)d \sigma _u + \int _t^{t+\tau } \mathcal {D} G(u,S_u,\sigma _u)du, \end{aligned} \end{aligned}$$
(21)

where

$$\begin{aligned} \begin{aligned} \mathcal {D}G(t,S_t,\sigma _t)&= \frac{\partial G}{\partial t}(t,S_t,\sigma _t) + \frac{1}{2} \sigma _t^2 S_t^2 \frac{\partial ^2 G}{\partial S^2} (t,S_t,\sigma _t) \\&\quad \,\, + \frac{1}{2} \eta _t^2 \frac{\partial ^2 G}{\partial \sigma ^2}(t,S_t,\sigma _t) + \rho \eta _t \sigma _t S_t \frac{\partial ^2 G}{\partial S \partial \sigma }(t,S_t,\sigma _t), \end{aligned} \end{aligned}$$

and \(C_t^{M} = G(t, S_t, \sigma _t)\) is also solves the Eq. (7). Under the two equations of (7) and (21), we can derive the following equation with the market price \(C_t^{M}\),

$$\begin{aligned} C_{t+\tau }^{M}&= C_t^{M} + \int _t^{t+\tau } \frac{\partial C_u^{M}}{\partial S_u} d S_u + \int _t^{t+\tau } \frac{\partial C_u^{M}}{\partial \sigma _u} d \sigma _u \nonumber \\&\quad + \int _t^{t+\tau } \Big [ \Big ( r_d C_u^{M} - ( r_d - r_f ) S_u \frac{\partial C_u^{M}}{\partial S_u} \Big ) - (\tilde{\theta }_u - \lambda _u) \frac{\partial C_u^{M}}{\partial \sigma _u} - \frac{1}{2} {\tilde{\eta }_u}^2 \frac{\partial ^2 C_u^{M}}{\partial {\sigma _u}^2} \nonumber \\&\quad - \,\tilde{\rho } \tilde{\eta }_u \sigma _u S_u \frac{\partial ^2 C_u^{M}}{\partial S \partial \sigma } + \frac{1}{2} {\eta _u}^2 \frac{\partial ^2 C_u^{M}}{\partial {\sigma _u}^2} + \rho \eta _u \sigma _u S_u \frac{\partial ^2 C_u^{M}}{\partial S \partial \sigma } \Big ] du \nonumber \\&= C_t^M + \int _t^{t+\tau } r_d C_u^{M} du+ \int _t^{t+\tau } \lambda _u \frac{\partial C_u^{M}}{\partial \sigma _u} du \nonumber \\&\quad + \,\int _t^{t+\tau } \Big [ (\theta _u - \tilde{\theta }_u) \frac{\partial C_u^{M}}{\partial \sigma _u} + \frac{1}{2} ({\eta _u}^2 - {\tilde{\eta }_u}^2) \frac{\partial ^2 C_u^{M}}{\partial {\sigma _u}^2}\nonumber \\&\quad + \,(\rho \eta _u - \tilde{\rho } \tilde{\eta }_u) \sigma _u S_u \frac{\partial ^2 C_u^{M}}{\partial S \partial \sigma } \Big ] du \nonumber \\&\quad +\, \int _t^{t+\tau } \sigma _u S_u \frac{\partial C_u^{M}}{\partial S_u} (\sqrt{1-\rho ^2} d W_u^1 + \rho d W_u^2) + \int _t^{t+\tau } \eta _u \frac{\partial C_u^{M}}{\partial \sigma _u} d W_u^2.\nonumber \\ \end{aligned}$$
(22)

The last equation is valid because of the assumption of \(\mu _u = r_d - r_f\) in this proposition.

\(C_t^{M}[\lambda _u]\) denotes the time-\(t\) call option price which is consistent with the underlying exchange rate process (2) and the equivalent martingale measure \(\mathbb {Q}[\lambda _u]\). By replacing \(\tau \) with \(T-t\) in (22), the following equation can be derived because of the fact that \(C_T^{M}[\lambda _u]=C_T^{M}[0]\) at the maturity date.

$$\begin{aligned} \begin{aligned}&C_t^M[\lambda _u] + \int _t^{T} r_d C_u^{M}[\lambda _u] du + \int _t^{T} \lambda _u \frac{\partial C_u^{M}[\lambda _u]}{\partial \sigma _u} du \\&\quad + \int _t^{T} \Big [ (\theta _u - \tilde{\theta }_u) \frac{\partial C_u^{M}[\lambda _u]}{\partial \sigma _u} + \frac{1}{2} ({\eta _u}^2 - {\tilde{\eta }_u}^2) \frac{\partial ^2 C_u^{M}[\lambda _u]}{\partial {\sigma _u}^2}\\&\quad + (\rho \eta _u - \tilde{\rho } \tilde{\eta }_u) \sigma _u S_u \frac{\partial ^2 C_u^{M}[\lambda _u]}{\partial S \partial \sigma } \Big ] du \\&\quad + \int _t^{T} \sigma _u S_u \frac{\partial C_u^{M}[\lambda _u]}{\partial S_u} (\sqrt{1-\rho ^2} d W_u^1 + \rho d W_u^2) + \int _t^{T} \eta _u \frac{\partial C_u^{M}[\lambda _u]}{\partial \sigma _u} d W_u^2 \\&=\,C_t^M[0] + \int _t^{T} r_d C_u^{M}[0] du \\&\quad + \int _t^{T} \Big [ (\theta _u - \tilde{\theta }_u) \frac{\partial C_u^{M}[0]}{\partial \sigma _u} + \frac{1}{2} ({\eta _u}^2 - {\tilde{\eta }_u}^2) \frac{\partial ^2 C_u^{M}[0]}{\partial {\sigma _u}^2}\\&\quad + (\rho \eta _u - \tilde{\rho } \tilde{\eta }_u) \sigma _u S_u \frac{\partial ^2 C_u^{M}[0]}{\partial S \partial \sigma } \Big ] du \\&\quad + \int _t^{T} \sigma _u S_u \frac{\partial C_u^{M}[0]}{\partial S_u} (\sqrt{1-\rho ^2} d W_u^1 + \rho d W_u^2) + \int _t^{T} \eta _u \frac{\partial C_u^{M}[0]}{\partial \sigma _u} d W_u^2. \end{aligned} \end{aligned}$$

Rearranging the above equation and taking expectation to the rearranged equation under \(\mathbb {P}\), we can obtain the following expression.

$$\begin{aligned} C_t^{M} [0] - C_t^{M}[\lambda _u]&= \int _t^{T} \mathbb {E}^\mathbb {P} \Big [ \lambda _u \frac{\partial C_u^{M}[\lambda _u]}{\partial \sigma _u} \Big ] du + r_d \int _t^{T} \mathbb {E}^\mathbb {P} \Big [ C_u^{M}[\lambda _u]-C_u^{M}[0] \Big ] du \nonumber \\&\quad +\, \int _t^{T} \mathbb {E}^\mathbb {P} \Big [ (\theta _u - \tilde{\theta }_u) \frac{\partial C_u^{M}[\lambda _u]}{\partial \sigma _u} + \frac{1}{2} ({\eta _u}^2 - {\tilde{\eta }_u}^2) \frac{\partial ^2 C_u^{M}[\lambda _u]}{\partial {\sigma _u}^2}\nonumber \\&\quad +\,(\rho \eta _u - \tilde{\rho } \tilde{\eta }_u) \sigma _u S_u \frac{\partial ^2 C_u^{M}[\lambda _u]}{\partial S \partial \sigma }\Big ] du\nonumber \\&\quad -\,\int _t^{T} \mathbb {E}^\mathbb {P} \Big [ (\theta _u - \tilde{\theta }_u) \frac{\partial C_u^{M}[0]}{\partial \sigma _u} + \frac{1}{2} ({\eta _u}^2 - {\tilde{\eta }_u}^2) \frac{\partial ^2 C_u^{M}[0]}{\partial {\sigma _u}^2}\nonumber \\&\quad +\,(\rho \eta _u - \tilde{\rho } \tilde{\eta }_u) \sigma _u S_u \frac{\partial ^2 C_u^{M}[0]}{\partial S \partial \sigma } \Big ] du \nonumber \\&\!= \int _t^{T} \mathbb {E}^\mathbb {P} \Big [ \lambda _u \frac{\partial C_u^{M}[\lambda _u]}{\partial \sigma _u} \Big ] du + r_d \int _t^{T} \mathbb {E}^\mathbb {P} \Big [ C_u^{M}[\lambda _u]-C_u^{M}[0] \Big ] du\nonumber \\&\quad +\,I_{t,T}(\lambda _u) - I_{t,T}(0). \end{aligned}$$
(23)

First, let us assume \(\lambda _u \ge 0\). We have the following inequations on the option premium,

$$\begin{aligned} \begin{aligned} C_u^{M}[\lambda _u]-C_u^{M}[0]&\le 0 \quad (\forall u \in [t,T]) \\&\mathrm{and} \\ \frac{\partial }{\partial u} \mathbb {E}^\mathbb {P} \Big [ C_u^{M}[\lambda _u]-C_u^{M}[0] \Big ]&= \mathbb {E}^\mathbb {P} \Big [ \frac{\partial }{\partial u} \Big ( C_u^{M}[\lambda _u]-C_u^{M}[0] \Big ) \Big ] \ge 0. \end{aligned} \end{aligned}$$

Thus, from (23),

$$\begin{aligned} \begin{aligned}&C_t^{M}[0] - C_t^{M}[\lambda _u] \\&\quad = \int _t^{T} \mathbb {E}^\mathbb {P} \Big [ \lambda _u \frac{\partial C_u^{M}[\lambda _u]}{\partial \sigma _u} \Big ] du\\&\quad \quad + r_d \int _t^{T} \mathbb {E}^\mathbb {P} \Big [ C_u^{M}[\lambda _u]-C_u^{M}[0] \Big ] du + I_{t,T}(\lambda _u) - I_{t,T}(0) \\&\quad \ge \int _t^{T} \mathbb {E}^\mathbb {P} \Big [ \lambda _u \frac{\partial C_u^{M}[\lambda _u]}{\partial \sigma _u} \Big ] du + r_d(T-t) \Big ( C_t^{M}[\lambda _u]-C_t^{M}[0] \Big )\\&\quad \quad + I_{t,T}(\lambda _u) - I_{t,T}(0). \\ \therefore&\quad \quad \Big (1+r_d(T-t) \Big ) \Big ( C_t^{M}[0]-C_t^{M}[\lambda _u] \Big ) + I_{t,T}(0) - I_{t,T}(\lambda _u) \\&\quad \ge \int _t^{T} \mathbb {E}^\mathbb {P} \Big [ \lambda _u \frac{\partial C_u^{M}[\lambda _u]}{\partial \sigma _u} \Big ] du. \end{aligned} \end{aligned}$$

We also have an inequation of \( \mathbb {E}^\mathbb {P} \Big [ C_u^{M}[\lambda _u]-C_u^{M}[0] \Big ] \le 0 \), so the following inequation can be derived with the equation of (23).

$$\begin{aligned} C_t^{M}[0] - C_t^{M}[\lambda _u] \le \int _t^{T} \mathbb {E}^\mathbb {P} \Big [ \lambda _u \frac{\partial C_u^{M}[\lambda _u]}{\partial \sigma _u} \Big ] du + I_{t,T}(\lambda _u) - I_{t,T}(0). \end{aligned}$$

Thus we can derive the following inequation with two inequations derived above,

$$\begin{aligned} \begin{aligned} C_t^{M}[0] - C_t^{M}[\lambda _u] + I_{t,T}(0) - I_{t,T}(\lambda _u)&\le \int _t^{T} \mathbb {E}^\mathbb {P} \Big [ \lambda _u \frac{\partial C_u^{M}[\lambda _u]}{\partial \sigma _u} \Big ] du \\&\le \Big (1+r_d(T-t) \Big ) \Big ( C_t^{M}[0]-C_t^{M}[\lambda _u] \Big ) \\&\quad + I_{t,T}(0) - I_{t,T}(\lambda _u). \end{aligned} \end{aligned}$$

Second, in the case of \( \lambda _u < 0 \), we have the following inequations,

$$\begin{aligned} \begin{aligned} C_u^{M}[\lambda _u]-C_u^{M}[0]&\ge 0 (\forall u \in [t,T]) \\&\mathrm{and} \\ \frac{\partial }{\partial u} \mathbb {E}^\mathbb {P} \Big [ C_u^{M}[\lambda _u]-C_u^{M}[0] \Big ]&= \mathbb {E}^\mathbb {P} \Big [ \frac{\partial }{\partial u} \Big ( C_u^{M}[\lambda _u]-C_u^{M}[0] \Big ) \Big ] \le 0. \end{aligned} \end{aligned}$$

Thus we can derive the inequation asserted in this Proposition with the similar approach to the discussion explored above. \(\square \)

Appendix 2: Time Series Data

See Table 7 and Figs. 3, 4, 5.

Table 7 Summary statistics for implied volatilities
Fig. 3
figure 3

USD-JPY WM/Reuter closing spot rate. This figure shows the time-series data in the period from October 31, 2003 to June 30, 2010

Fig. 4
figure 4

USD-JPY 1M ATM implied Volatility (Mid Price). This figure shows the time-series data in the period from October 31, 2003 to June 30, 2010

Fig. 5
figure 5

USD-JPY 1M ATM mid-bid spread. This figure shows the time-series data in the period from October 31, 2003 to June 30, 2010

Appendix 3: Parameter Estimation Results for the Heston (1993) model

See Figs. 6, 7 and 8.

Fig. 6
figure 6

The time-series of the estimated parameter: \(\tilde{\kappa }\). This figure shows estimation results of \(\tilde{\kappa }\) at each time point in the period from October 31, 2003 to June 30, 2010. These parameters are estimated with the maximum liklihood method proposed by Aït-Sahalia and Kimmel (2007) and we update the parameters daily based on historical 1,750 days daily data with a rolling estimation procedure

Fig. 7
figure 7

The time-series of the estimated parameter: \(\tilde{v}\). This figure shows estimation results of \(\tilde{v}\) at each time point in the period from October 31, 2003 to June 30, 2010. These parameters are estimated with the maximum liklihood method proposed by Aït-Sahalia and Kimmel (2007) and we update the parameters daily based on historical 1,750 days daily data with a rolling estimation procedure

Fig. 8
figure 8

The time-series of the estimated parameter: \(\tilde{\rho }\). This figure shows estimation results of \(\tilde{\rho }\) at each time point in the period from October 31, 2003 to June 30, 2010. These parameters are estimated with the maximum liklihood method proposed by Aït-Sahalia and Kimmel (2007) and we update the parameters daily based on historical 1,750 days daily data with a rolling estimation procedure

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Sasaki, H. Understanding Delta-Hedged Option Returns in Stochastic Volatility Environments. Asia-Pac Financ Markets 22, 151–184 (2015). https://doi.org/10.1007/s10690-014-9198-3

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