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Monotonicity of implied volatility for perpetual put options

Published online by Cambridge University Press:  19 June 2023

Erik Ekström*
Affiliation:
Uppsala University
Ebba Mellquist*
Affiliation:
Uppsala University
*
*Postal address: Department of Mathematics, Box 256, 75105 Uppsala, Sweden.
*Postal address: Department of Mathematics, Box 256, 75105 Uppsala, Sweden.
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Abstract

We define and study properties of implied volatility for American perpetual put options. In particular, we show that if the market prices are derived from a local volatility model with a monotone volatility function, then the corresponding implied volatility is also monotone as a function of the strike price.

Type
Original Article
Copyright
© The Author(s), 2023. Published by Cambridge University Press on behalf of Applied Probability Trust

1. Introduction

In Black–Scholes theory, the standard textbook approach is to specify a model for an underlying asset, and then derive an arbitrage-free value of derivative securities. One reason for the great success of Black–Scholes theory is that the above procedure can be inverted. In fact, if a model based on geometric Brownian motion is assumed, and if a market price of a European call option is given, then we can determine the unique volatility of the underlying asset which would give that particular price. This particular value is referred to as the implied volatility, and it provides an efficient way of quoting option prices.

The standard notion of implied volatility refers to the inversion of the Black–Scholes formula for the pricing of call options. If the implied volatility is inferred for several different options on the same underlying asset and maturity but with different strike prices, the notion ‘volatility smile’ refers to the implied volatility decreasing for small strikes and increasing for larger strikes; similarly, an implied volatility that is monotone as a function of the strike is referred to as a ‘volatility skew’. The occurrence of volatility smiles and skews shows that the use of a constant volatility is too simplistic for modeling purposes, and that more advanced models are needed. In [Reference Cont and Tankov6], a discussion of which models give rise to volatility skews is provided. In particular, it is argued that decreasing volatility skews may be obtained in (i) spectrally negative jump models, (ii) stochastic volatility models with negative correlation, and (iii) local volatility models with decreasing volatility functions. However, these are not necessarily precise mathematical results, but should rather be viewed as rules of thumb based on numerical evidence. In fact, it is shown in [Reference Ekström and Lu9] that spectrally negative jump models exhibit the opposite monotonicity (i.e. increasing implied volatility) for short-time implied volatility. Similarly, numerical plots of implied volatility in stochastic volatility models often exhibit a non-monotone dependence of the implied volatility in the strike price, cf., e.g., [Reference Berestycki, Busca and Florent4]. For an interesting study of the dependence between local volatility and implied volatility see [Reference Berestycki, Busca and Florent3], where a nonlinear partial differential equation for the implied volatility is derived; a closer inspection of this equation strongly indicates that models of type (iii) above always give rise to decreasing implied volatilities, but a full study of this case is still missing. For other qualitative results on implied volatility see [Reference Alòs and García-Lorite1], where Malliavin calculus is used to derive asymptotic properties of at-the-money implied volatility for short maturities in various models.

While the notion of implied volatility, as discussed above, is usually defined for European options, it makes sense to also quote prices of other types of financial products in terms of volatility. In this paper, we discuss implied volatility inferred from prices of perpetual American put options, and we study its properties. In comparison with the definition of implied volatility for European options, the inversion of the pricing formula for perpetual options is easier, and therefore allows for more explicit calculations. In particular, we show that if the market uses a local volatility model with a decreasing volatility function, then the implied volatility is also decreasing, thus verifying claim (iii) above within our setup. Similarly, if the market uses a local volatility model with an increasing volatility function, then the corresponding implied volatility is increasing in the strike price.

2. Setup and main result

On a complete filtered probability space $(\Omega, \mathcal F, \mathbb P, (\mathcal F_t)_{0\leq t\lt\infty})$ , let X be the solution of a stochastic differential equation

(1) \begin{equation} {\mathrm{d}} X_t = r X_t\,{\mathrm{d}} t + \sigma(X_t)X_t\,{\mathrm{d}} W_t\end{equation}

with initial condition $x_0\in(0,\infty)$ . Here, $r\gt0$ is the constant interest rate and $\sigma(\!\cdot\!)\;:\;(0,\infty)\to(0,\infty)$ is a given function. We will assume that the local volatility function $\sigma(\!\cdot\!)$ is continuous and bounded at infinity so that (Reference Alòs and García-Lorite1) has a unique strong solution up to the first hitting time of 0; we also assume that X is regular so that any point $y\in(0,\infty)$ can be reached in finite time, and we let 0 be an absorbing state so that if X reaches 0 in finite time, then it remains at 0 at all times.

For any given strike price $K\geq 0$ , consider the price $P(K) \;:\!=\; \sup_{\tau}\mathbb E[{\mathrm{e}}^{-r\tau}(K-X_\tau)^+]$ of a perpetual American put option with strike K, where the supremum is taken over all stopping times. Note here that the discounting rate r is the same as in the drift of X in (Reference Alòs and García-Lorite1), so by standard arbitrage theory, P(K) is the unique arbitrage-free price of the put option. The following result is immediate (and well known, cf. [Reference Ekström and Hobson8]).

Lemma 1. The function $P\;:\;[0,\infty)\to[0,\infty)$

  • is non-decreasing and convex;

  • satisfies $P(K)\gt0$ for $K\gt0$ ;

  • satisfies $(K-x_0)^+\leq P(K)\leq K$ .

2.1. Constant volatility and implied volatility

In the special case of constant volatility, $\sigma(\!\cdot\!)\equiv \gamma\gt0$ , it is well known that $P_{\gamma}(K)\;:\!=\;P(K)$ is given by

(2) \begin{equation} P_\gamma(K)=\left\{ \begin{array}{l@{\quad}l} (K-z(K))({z_\gamma(K)}/{x_0})^{2r/\gamma^2}, & K\lt\hat K_\gamma , \\ K-x_0, & K\geq \hat K_\gamma, \end{array}\right.\end{equation}

where $z_\gamma(K) \;:\!=\; {2rK}/({2r+\gamma^2})$ and $\hat K_\gamma \;:\!=\; {(2r+\gamma^2)K}/{2r}$ . Moreover,

\[\tau_{z_\gamma(K)}\;:\!=\;\inf\{t\geq 0 \;:\; X_t\leq z_\gamma(K)\}\]

is an optimal stopping time, so that $P_\gamma(K) = \mathbb E[{\mathrm{e}}^{-r\tau_{z_\gamma(K)}}(K-X_{\tau_{z_\gamma(K)}})^+]$ . Using the explicit formula (Reference Alvarez2), it is straightforward to check that the price is monotonically increasing in volatility: if $P_{\gamma_1}(K)$ is the price corresponding to a volatility $\gamma_1\gt0$ and $P_{\gamma_2}(K)$ is the price corresponding to a volatility $\gamma_2\gt0$ , then $\gamma_1\leq \gamma_2\implies P_{\gamma_1}(\!\cdot\!)\leq P_{\gamma_2}(\!\cdot\!)$ . Furthermore, if $P_{\gamma_1}(K)\gt (K-x_0)^+$ , then $P_{\gamma_2}(K)\gt P_{\gamma_1}(K)$ for $\gamma_2\gt\gamma_1$ , i.e. the price is strictly increasing in volatility in the continuation region.

Remark 1. Monotonicity of perpetual options with respect to volatility holds true for a much larger class of local volatility models; see [Reference Alvarez2] and [Reference Ekström7].

2.2. Main result

Now assume that a volatility function $\sigma(\!\cdot\!)$ is given, and let $P(\!\cdot\!)$ be the corresponding option price; recall that $P(\!\cdot\!)$ has the properties specified in Lemma 1. We write

\[\hat K\;:\!=\;\inf\{K\geq 0 \;:\; P(K)=(K-x_0)^+\}.\]

Then $\hat K\in(x_0,\infty]$ , $P(K)\gt (K-x_0)^+$ for $K\lt\hat K$ , and $P(K)=(K-x_0)^+$ for $K\geq \hat K$ . By the strict monotonicity of the function $P_\gamma (K)$ with respect to $\gamma$ (recall that $P_\gamma(K)$ is the price of a put option if the volatility is a constant $\gamma$ ), for each $K\in(0,\hat K)$ there exists a unique $\gamma=\gamma(K)\gt0$ such that $P(K)=P_\gamma(K)$ . This value is referred to as the implied volatility.

Remark 2. In contrast to the standard notion of implied volatility (defined by inverting the Black–Scholes formula for options with a finite horizon), which is well defined for all strikes, the implied volatility $\gamma(\!\cdot\!)$ is uniquely determined only for $K\lt\hat K$ .

We now present our main result.

Theorem 1. Let a volatility function $\sigma(\!\cdot\!)$ be given, let $P(\!\cdot\!)$ be the corresponding option value, and let $\hat K=\inf\{K\geq 0 \;:\; P(K)=(K-x_0)^+\}$ .

  1. (i) If $\sigma(\!\cdot\!)\;:\; (0,\infty)\to(0,\infty)$ is non-increasing, then the implied volatility $\gamma(\!\cdot\!)$ is non-increasing on $(0,\hat K)$ .

  2. (ii) If $\sigma(\!\cdot\!)\;:\; (0,\infty)\to(0,\infty)$ is non-decreasing, then the implied volatility $\gamma(\!\cdot\!)$ is non-decreasing on $(0,\hat K)$ .

A geometric approach to implied volatility is provided in Section 3, and the proof of Theorem 1 is then given in Section 4.

3. A geometric approach to option pricing and implied volatility

While the classical method to determine the price P (along with an optimal stopping time) would be to make a Markovian embedding by varying the initial point $x_0$ and then study an associated free-boundary problem, it is more convenient for our purposes to follow a geometric approach as presented in [Reference Ekström and Hobson8]. As we will see, this geometric approach is well aligned with the inversion of the pricing function in (Reference Alvarez2) that is needed to calculate the implied volatility.

Let $\varphi\;:\;(0,\infty)\to(0,\infty)$ be a non-increasing solution of

(3) \begin{equation} \frac{\sigma^2(x)x^2}{2}\varphi''(x)+rx\varphi'(x)-r\varphi(x)=0.\end{equation}

This function is unique up to multiplication with a positive constant, cf. [Reference Borodin and Salminen5, pp. 18, 19]; we will for simplicity (and without loss of generality) assume that $\varphi(x_0)=1$ . It is straightforward to check that

\begin{equation*} \varphi(x) = Dx\int_x^\infty\frac{1}{y^2} \exp\!\bigg\{{-}\int_{x_0}^y\frac{2r}{z\sigma^2(z)}\,{\mathrm{d}} z\bigg\}\,{\mathrm{d}} y,\end{equation*}

where

\[D=\frac{1}{x_0\int_{x_0}^\infty y^{-2} \exp\!\big\{{-}\int_{x_0}^y{2r}/({z\sigma^2(z)})\,{\mathrm{d}} z\big\}\,{\mathrm{d}} y}.\]

Moreover, straightforward differentiation yields

\[\varphi''(x)=\frac{2rD}{\sigma^2(x)x^2}\exp\!\bigg\{{-}\int_{x_0}^x\frac{2r}{z\sigma^2(z)}\,{\mathrm{d}} z\bigg\}\gt0,\]

so $\varphi$ is strictly convex. Furthermore, denoting by $\tau_z\;:\!=\;\inf\{t\geq 0\;:\; X_t\leq z\}$ the first passage time below a level $z\in(0,\infty)$ , we have, for any $x\geq z$ , $\mathbb E_x[{\mathrm{e}}^{-r\tau_z}] = {\varphi(x)}/{\varphi(z)}$ . In particular, using $\varphi(x_0)=1$ ,

(4) \begin{equation} \mathbb E_{x_0}[{\mathrm{e}}^{-r\tau_z}] = \frac{1}{\varphi(z)}\end{equation}

for $z\in(0,x_0]$ . Moreover, the above formulae also extend to $z=0$ as $\varphi(0)=\infty$ in the case when 0 is unattainable.

The following result was provided in [Reference Ekström and Hobson8]; for completeness of the presentation, we include its proof.

Proposition 1. The value function $P\;:\;[0,\infty)\to[0,\infty)$ satisfies

\begin{equation*} P(K)=\sup_{z\leq K\wedge x_0}\frac{K-z}{\varphi(z)}. \end{equation*}

Proof. Denote the required right-hand side by

\[\hat P(K)\;:\!=\;\sup_{z\leq K\wedge x_0}\frac{K-z}{\varphi(z)}.\]

We clearly have

\begin{equation*} P(K) = \sup_{\tau}\mathbb E[{\mathrm{e}}^{-r\tau}(K-X_\tau)^+] \geq \sup_{z\leq K\wedge x_0}\mathbb E[{\mathrm{e}}^{-r\tau_z}(K-X_{\tau_z})^+] = \sup_{z\leq K\wedge x_0} \frac{K-z}{\varphi(z)} = \hat P(K), \end{equation*}

where the second equality uses that $X_{\tau_z}=z$ on $\{\tau_z \lt\infty\}$ , $\mathbb P$ -almost surely, and (Reference Berestycki, Busca and Florent4).

For the reverse inequality, first assume that $K\leq K'\;:\!=\;-x_0/\varphi'(x_0)$ . For such K, we have

\[\hat P(K)=\sup_{z}\frac{K-z}{\varphi(z)},\]

so that $\hat P(K)\varphi(z)\geq (K-z)^+$ . Consequently,

\begin{equation*} P(K) = \sup_{\tau}\mathbb E[{\mathrm{e}}^{-r\tau}(K-X_\tau)^+] \leq \hat P(K)\sup_\tau\mathbb E[{\mathrm{e}}^{-r\tau}\varphi(X_\tau)] \leq \hat P(K)\varphi(x_0) = \hat P(K), \end{equation*}

where the second inequality uses that $\{{\mathrm{e}}^{-rt}\varphi(X_t),\,0 \leq t \leq \infty\}$ is a supermartingale.

Finally, the above argument gives that $P(K')=(K'-x_0)$ ; hence $P(K)=(K-x_0) \leq \hat P(K)$ for all $K\geq K'$ by Lemma 1, which completes the proof.

Remark 3. For a given K, the convexity of $\varphi$ yields the existence of a unique straight line through the point (K, 0) that is tangent to the graph $\{(z,\varphi(z)), z\leq K\wedge x_0\}$ . Denoting by $(z(K),\varphi(z(K)))$ the tangent point (which is unique by the strict convexity of $\varphi$ ), the price P(K) is given by $P(K)=(K-z(K))/\varphi(z(K))$ . Thus, P(K) equals the negative reciprocal of the slope of this tangent line, cf. Figure 1.

Figure 1. For a given $K \leq \hat K$ , the put price P(K) equals the negative reciprocal of the slope of the tangent line to $\varphi$ which passes through (K, 0).

Moreover, z(K) is non-decreasing in K, and it follows from the proof of Proposition 1 that $\tau_{z(K)}$ is an optimal stopping time.

Remark 4. In contrast to the standard embedding approach, where an option price is produced for a fixed strike K but for any initial stock price x, the geometric approach presented in Proposition 1 produces prices for all K, but for a fixed initial stock price $x_0$ . This feature will turn out useful for us when comparing implied volatility for different strike prices.

We now return to the problem of determining the implied volatility, assuming that market prices are calculated using a local volatility function $\sigma(\!\cdot\!)$ with corresponding function $\varphi(\!\cdot\!)$ as above. For a given $K\gt0$ , let $l_K$ be the unique straight line through (K, 0) that is tangent to $\{(z,\,\varphi(z)),z\leq K\wedge x_0\}$ . Denoting the tangent point by $(z(K),\varphi(z(K)))$ , we have

\[l_K(z)=-\frac{\varphi(z(K))}{K-z(K)}(z-K).\]

To describe how to determine the implied volatility in the local volatility model $\sigma(\!\cdot\!)$ , note that, for a given constant volatility $\gamma\gt0$ , the decreasing positive solution of $\frac12\gamma^2x^2f^{\prime\prime}(x)+rxf^{\prime}(x)-rf(x)=0$ on $(0,\infty)$ , also imposing the normalizing condition $f(x_0)=1$ , is given by

(5) \begin{equation} f(x)\;:\!=\;f_\gamma(x)\;:\!=\;\bigg(\frac{x}{x_0}\bigg)^{-2r/\gamma^2}.\end{equation}

Clearly, on $(0,x_0)$ , $f_\gamma$ is strictly decreasing in $\gamma$ . Consequently, given a strike price $K\gt0$ and the corresponding tangent line $l_K(\!\cdot\!)$ (constructed from $\sigma(\!\cdot\!)$ and $\varphi(\!\cdot\!)$ as above) with $l_K(x_0)\lt 1$ (equivalently, $z(K)\lt x_0$ ), there exists a unique $\gamma=\gamma(K)$ such that $l(\!\cdot\!)$ is also a tangent line to $f_\gamma(\!\cdot\!)$ . By Proposition 1, $\gamma(K)$ is the implied volatility of the option.

4. Monotone local volatility functions

In this section we provide a result regarding the function $\varphi$ corresponding to non-increasing local volatility functions (Proposition 2). For its proof we will use a monotonicity result (Lemma 2) with respect to the local volatility functions; its proof is adapted from a similar situation in [Reference Ekström7]. Using Proposition 2, the proof of Theorem 1 then follows.

Lemma 2. Assume that $\sigma_i\;:\;(0,\infty)\to(0,\infty)$ , $i=1,2$ , satisfy $\sigma_1(\!\cdot\!)\leq \sigma_2(\!\cdot\!)$ . Let $h_i$ , $i=1,2$ , be the solutions of

\begin{align*}\left\{ \begin{array}{l@{\quad}l} \displaystyle \frac12\sigma_i^2(x)x^2h''_{\!\!\!i}(x) + rxh'_{\!\!i}(x) - rh_i(x) = 0, & x\in(a,b), \\[10pt] h_i(a) = A,\ h_i(b) = B, \end{array}\right.\end{align*}

for $0\lt a\lt b\lt\infty$ and $A,B\geq 0$ . If ${A}/{a} \geq {B}/{b}$ , then $h_1(\!\cdot\!)\leq h_2(\!\cdot\!)$ on [a, b].

Proof. Denoting by $\varphi_1$ the decreasing fundamental solution corresponding to $\sigma_1$ , the general solution of the ordinary differential equation for $h_1$ is $h_1(x)= Cx + D \varphi_1(x)$ , where C and D are constants. Imposing the boundary conditions $h_1(a)=A$ and $h_2(b)=B$ yields

\[D=\frac{bA-aB}{b\varphi_1(a)-a\varphi_1(b)},\]

which is positive by assumption. Consequently, the function $h_1$ is convex.

Next, for $x\in(a,b)$ , let $X^2$ be the solution of ${\mathrm{d}} X^2_t = rX^2_t\,{\mathrm{d}} t + \sigma_2(X^2_t)X^2_t\,{\mathrm{d}} W_t$ with $X^2_0=x$ . By Itô’s formula, the process $Y_t \;:\!=\; {\mathrm{e}}^{-rt}h_1(X_t^2)$ satisfies

\begin{align*} dY_t & = {\mathrm{e}}^{-rt}\Big(\frac12\sigma^2_2(X^2_t)(X^2_t)^2 h''_{\!\!\!l}(X_t^2) + rX^2_th'_{\!\!l}(X^2_t) - rh_1(X_t^2)\Big)\,{\mathrm{d}} t + {\mathrm{e}}^{-rt}\sigma^2(X^2_t)X^2_th'_{\!\!l}(X^2_t)\,{\mathrm{d}} W_t \\[5pt] & = {\mathrm{e}}^{-rt}\frac12(\sigma^2_2(X^2_t)-\sigma^2_1(X^2_t)) (X^2_t)^2h''_{\!\!\!l}(X_t^2)\,{\mathrm{d}} t + {\mathrm{e}}^{-rt}\sigma^2(X^2_t)X^2_th'_{\!\!l}(X^2_t)\,{\mathrm{d}} W_t \end{align*}

for $t\leq \tau_{ab}\;:\!=\;\inf\{s\geq 0\;:\; X^2_s\notin(a,b)\}$ . Since $0\lt\sigma_1\leq\sigma_2$ and $h_1$ is convex, $Y_t$ is a submartingale. Similarly, the process ${\mathrm{e}}^{-rt}h_2(X_t^2)$ is a martingale. Consequently, optional sampling gives

\[h_1(x)\leq \mathbb E_x\big[{\mathrm{e}}^{-r\tau_{ab}}h_1(X^2_{\tau_{ab}})\big] = \mathbb E_x\big[{\mathrm{e}}^{-r\tau_{ab}}h_2(X^2_{\tau_{ab}})\big] = h_2(x),\]

which completes the proof.

Remark 5. The monotonicity result in Proposition 2 also extends to the case of $b=\infty$ and $B=0$ . In that case, the function $h_i$ coincides with the decreasing fundamental solution $\varphi_i$ (possibly scaled with a positive constant).

Proposition 2. Assume that $\sigma(\!\cdot\!)\;:\;(0,\infty)\to(0,\infty)$ is a given volatility function, and let $\varphi(\!\cdot\!)$ be the corresponding decreasing solution of (Reference Berestycki, Busca and Florent3). For a constant volatility $\gamma\gt0$ , let $f_\gamma$ be as in (Reference Borodin and Salminen5). Moreover, assume that $f_\gamma(a)=\varphi(a)$ for some $a\in(0,x_0)$ .

  1. (i) If $\sigma(\!\cdot\!)$ is non-increasing, then $f_\gamma(\!\cdot\!)\leq \varphi(\!\cdot\!)$ on $[a,x_0]$ .

  2. (ii) If $\sigma(\!\cdot\!)$ is non-decreasing, then $f_\gamma(\!\cdot\!)\geq \varphi(\!\cdot\!)$ on $[a,x_0]$ .

Proof. Assume that $\sigma(\!\cdot\!)$ is non-increasing. Then we have $\sigma(x_0)\leq \sigma(a)$ ; we consider the three cases $\gamma\leq\sigma(x_0)$ , $\sigma(a)\leq \gamma$ , and $\sigma(x_0)\lt \gamma\lt\sigma(a)$ separately.

First, assume that $\gamma\leq\sigma(x_0)$ . Then $\gamma\leq \sigma(x)$ for all $x\in[a,x_0]$ , and Lemma 2 immediately yields $f_\gamma(\!\cdot\!)\leq \varphi(\!\cdot\!)$ on $[a,x_0]$ .

Second, assume that $\sigma(a)\leq \gamma$ . If $\gamma=\sigma(x_0)$ , then $\sigma(\!\cdot\!)\equiv \gamma$ on $[a,x_0]$ , and $\varphi(\!\cdot\!)\equiv f_\gamma(\!\cdot\!)$ on $[a,x_0]$ . Therefore, we may assume that $\gamma\gt\sigma(x_0)$ . Note that $\sigma(\!\cdot\!)\leq \gamma$ on $[a,\infty)$ , so Lemma 2 and Remark 5 give $\varphi(\!\cdot\!)\leq f_\gamma(\!\cdot\!)$ on $[a,\infty)$ . Since $f_\gamma(x_0)=1=\varphi(x_0)$ and $f_\gamma(\!\cdot\!)\geq \varphi(\!\cdot\!)$ on $[a,\infty)$ , we then must have $f^\prime_\gamma(x_0)=\varphi'(x_0)$ and $f^{\prime\prime}_\gamma(x_0)\geq \varphi''(x_0)$ . Therefore,

\begin{align*} 0 = \frac12\sigma^2(x_0)x_0^2\varphi''(x_0)+rx_0\varphi'(x_0)-r\varphi(x_0) & \leq \frac12\sigma^2(x_0)x_0^2f^{\prime\prime}_\gamma(x_0)+rx_0f^{\prime}_\gamma(x_0)-rf_\gamma(x_0) \\[5pt] & \lt \frac12\gamma^2x_0^2f^{\prime\prime}_\gamma(x_0)+rx_0f^{\prime}_\gamma(x_0)-rf_\gamma(x_0) = 0, \end{align*}

which shows that the point $a\in(0,x_0)$ with $f_\gamma(a)=\varphi(a)$ cannot exist.

Third, assume that $\sigma(x_0) \lt \gamma \lt \sigma(a)$ . We first show that $f_\gamma(\!\cdot\!)\lt\varphi(\!\cdot\!)$ in a left-neighborhood $(x_0-\varepsilon,x_0)$ of $x_0$ (for some $\varepsilon\gt0$ ). To see this, note that $\sigma(\!\cdot\!)\leq \gamma$ on $(x_0,\infty)$ , so Lemma 2 yields $\varphi(\!\cdot\!)\leq f_\gamma(\!\cdot\!)$ on $(x_0,\infty)$ . Since $\varphi(x_0)=1=f_\gamma(x_0)$ , we have $\varphi'(x_0)\leq f^{\prime}_\gamma(x_0)$ ; consequently,

\begin{align*} 0 = \frac12\sigma^2(x_0)x_0^2\varphi''(x_0)+rx_0\varphi'(x_0)-r\varphi(x_0) & \lt \frac12\gamma^2x_0^2\varphi''(x_0)+rx_0f^{\prime}_\gamma(x_0)-rf_\gamma(x_0) \\[5pt] & = \frac12\gamma^2x_0^2(\varphi''(x_0)-f^{\prime\prime}_\gamma(x_0)), \end{align*}

so $\varphi''(x_0)\gt f^{\prime\prime}_\gamma(x_0)$ . This inequality, together with $\varphi(x_0)=f_\gamma(x_0)$ and $\varphi'(x_0)\leq f^{\prime}_\gamma(x_0)$ , imply that $f_\gamma(\!\cdot\!)\lt\varphi(\!\cdot\!)$ in a left-neighborhood of $x_0$ .

If the set $\{x\in(a,x_0)\;:\; f_\gamma(x)\gt\varphi(x)\}$ is empty, then $f_\gamma(\!\cdot\!)\leq \varphi(\!\cdot\!)$ on $[a,x_0]$ and there is nothing to prove. Instead, assume that $f_\gamma(x)\gt\varphi(x)$ for some $x\in(a,x_0)$ , and let $c\;:\!=\;\sup\{x\in(a,x_0)\;:\; f_\gamma(x)\gt\varphi(x)\}$ . Since $f_\gamma(\!\cdot\!)\lt\varphi(\!\cdot\!)$ in a left-neighborhood of $x_0$ , we then have $c\in(a,x_0)$ . Also note that, by continuity, $f_\gamma(c)=\varphi(c)$ .

Now, if $\gamma\geq\sigma(c)$ , then $\gamma\geq \sigma(\!\cdot\!)$ on $(c,x_0)$ . Thus, Lemma 2 gives $\varphi(\!\cdot\!)\leq f_\gamma(\!\cdot\!)$ on $(c,x_0)$ , which contradicts that $f_\gamma(\!\cdot\!)\lt\varphi(\!\cdot\!)$ in a left-neighborhood of $x_0$ . On the other hand, if $\gamma\lt\sigma(c)$ , then $\gamma\leq\sigma(\!\cdot\!)$ on (a,c), and Lemma 2 yields $f_\gamma(\!\cdot\!)\leq \varphi(\!\cdot\!)$ on (a, c). Since we also have $f_\gamma(\!\cdot\!)\leq \varphi(\!\cdot\!)$ on $(c,x_0)$ by the definition of c, this shows that $f_\gamma(\!\cdot\!)\leq \varphi(\!\cdot\!)$ on $(a,x_0)$ .

Next, assume that $\sigma(\!\cdot\!)$ is non-decreasing. Again, three cases are considered, namely $\sigma(x_0)\leq \gamma$ , $\gamma\leq \sigma(a)$ , and $\sigma(a)\lt\gamma\lt\sigma(x_0)$ .

First, if $\sigma(x_0)\leq \gamma$ , then $\gamma\geq \sigma(\!\cdot\!)$ on $[a,x_0]$ , and Lemma 2 yields $f_\gamma(\!\cdot\!)\geq\varphi$ on $[a,x_0]$ .

Second, if $\gamma\leq \sigma(a)$ , then $\gamma\leq \sigma(\!\cdot\!)$ on $[a,\infty)$ , so Lemma 2 implies that $f_\gamma(\!\cdot\!)\leq \varphi(\!\cdot\!)$ on $[a,\infty)$ . If $\gamma=\sigma(a)=\sigma(x_0)$ , then $f_\gamma(\!\cdot\!)= \varphi(\!\cdot\!)$ on $[a,x_0]$ , and there is nothing to prove. Thus, we may assume that $\gamma\leq \sigma(a)\lt\sigma(x_0)$ ; in this case, however, $f_\gamma(x_0)=1=\varphi(x_0)$ and $f_\gamma(\!\cdot\!)\leq\varphi(\!\cdot\!)$ imply that

\begin{align*} 0 = \frac12\sigma^2(x_0)x_0^2\varphi''(x_0)+rx_0\varphi'(x_0)-r\varphi(x_0) & \geq \frac12\sigma^2(x_0)x_0^2f^{\prime\prime}_\gamma(x_0)+rx_0f^{\prime}_\gamma(x_0)-rf_\gamma(x_0) \\[5pt] & \gt \frac12\gamma^2x_0^2f^{\prime\prime}_\gamma(x_0)+rx_0f^{\prime}_\gamma(x_0)-rf_\gamma(x_0)=0, \end{align*}

which is impossible.

Third, assume that $\sigma(a)\lt\gamma\lt\sigma(x_0)$ . We then have $\gamma\leq \sigma(\!\cdot\!)$ on $[x_0,\infty)$ , so $f_\gamma(\!\cdot\!)\leq\varphi(\!\cdot\!)$ on $[x_0,\infty)$ . Since $f_\gamma(x_0)=1=\varphi(x_0)$ , this implies that $f^{\prime}_\gamma(x_0)\leq \varphi'(x_0)$ , so

\begin{align*} 0 = \frac12\sigma^2(x_0)x_0^2\varphi''(x_0)+rx_0\varphi'(x_0)-r\varphi(x_0) & \gt \frac12\gamma^2x_0^2\varphi''(x_0)+rx_0f^{\prime}_\gamma(x_0)-rf_\gamma(x_0) \\[5pt] & = \frac12\gamma^2x_0^2(\varphi''(x_0)-f^{\prime\prime}_\gamma(x_0)). \end{align*}

Therefore, $f^{\prime\prime}_\gamma(x_0)\gt\varphi''(x_0)$ , and $f_\gamma(\!\cdot\!)\gt\varphi(\!\cdot\!)$ in a left-neighborhood $(x_0-\varepsilon,x_0)$ of $x_0$ .

Now, assume that there exists at least one point $x\in(a,x_0)$ with $f_\gamma(x)\lt\varphi(x)$ , and define $c\;:\!=\;\sup\{x\in(a,x_0)\;:\; f_\gamma(x)\lt\varphi(x)\}$ . Since $f_\gamma(\!\cdot\!)\gt\varphi(\!\cdot\!)$ in a left-neighborhood of $x_0$ , we then have $c\in(a,x_0)$ . If $\gamma\leq \sigma(c)$ , then $\gamma\leq \sigma(\!\cdot\!)$ on $[c,x_0]$ . Lemma 2 then yields $f_\gamma(\!\cdot\!)\leq \varphi(\!\cdot\!)$ on $[c,x_0]$ , which contradicts $f_\gamma(\!\cdot\!)\gt\varphi(\!\cdot\!)$ in a left-neighborhood of $x_0$ . On the other hand, if $\gamma \gt \sigma(c)$ , then Lemma 2 yields $f_\gamma(\!\cdot\!)\geq \varphi(\!\cdot\!)$ on [a, c] and, by the definition of c, we also find that $f_\gamma(\!\cdot\!)\geq \varphi(\!\cdot\!)$ on $[a,x_0]$ .

Proposition 3. Assume that $K\lt\hat K$ , and denote by z(K) the optimal stopping boundary for the volatility $\sigma(\!\cdot\!)$ . Let $\gamma=\gamma(K)$ be the corresponding implied volatility, and let $z_\gamma(K)$ be the corresponding optimal stopping boundary. Then $z(K)\leq z_\gamma(K)$ ( $z(K)\geq z_\gamma(K)$ ) provided $\sigma(\!\cdot\!)$ is non-increasing (non-decreasing).

Proof. First assume that $\sigma(\!\cdot\!)$ is non-increasing, and (for a contradiction) that $z(K)\gt z_\gamma(K)$ . Then, by the convexity of $\varphi(\!\cdot\!)$ and $f_\gamma(\!\cdot\!)$ , there exists a point $a\in( z_\gamma(K),z(K))$ such that $\varphi(a)=f_\gamma(a)$ . By Proposition 2, $f_\gamma\leq \varphi$ on $[a,x_0]$ , which contradicts $f_\gamma(z(K))\gt l_K(z(K))=\varphi(z(K))$ . Consequently, $z(K)\leq z_\gamma(K)$ .

Next, assume that $\sigma(\!\cdot\!)$ is non-decreasing, and that $z(K)\lt z_\gamma(K)$ . Then, by convexity, there exists a unique $a\in(z(K), z_\gamma(K))$ with $\varphi(a)=f_\gamma(a)$ (where $\gamma\;:\!=\;\gamma(K)$ is again the implied volatility). Proposition 2 then gives $f_\gamma\geq \varphi$ on $[a,x_0]$ , which is a contradiction of $f_\gamma(z_\gamma(K))=l_K(z(K)) \lt\varphi(z_\gamma(K))$ .

Proof of Theorem 1. For $i=1,2$ , let $K_i$ be given strike prices with $K_1\lt K_2$ , denote by $(z(K_i),\varphi(z(K_i)))$ the tangent point of the tangent line $l_{K_i}$ of $\varphi$ through the point $(K_i,0)$ , and let $\gamma_i\;:\!=\;\gamma(K_i)$ be the corresponding implied volatilities. Then the lines

\[l_{K_i}(z)=-\frac{\varphi(z(K_i))}{K_i-z(K_i)}(z-K_i), \qquad i=1,2,\]

are tangent lines to the functions

\[f_{\gamma_i}(z)=\bigg(\frac{z}{x_0}\bigg)^{-2r/\gamma_i^2},\]

respectively, with unique tangent points with z-coordinates $z'_{\!\!i}\;:\!=\;z_{\gamma_i}(K_i)$ , for which $f_{\gamma_i}(z'_{\!\!i})=l_{K_i}(z'_{\!\!i})$ . We denote by $\hat z$ the z-coordinate of the intersection point between $l_{K_1}$ and $l_{K_2}$ . For a graphical illustration, see Figure 2.

Figure 2. The function $\varphi$ , together with two strike prices $K_1\lt K_2$ , the corresponding tangent lines $l_{K_1}$ and $l_{K_2}$ , and their intersection point $\hat z$ .

Now assume that $\sigma(\!\cdot\!)$ is non-increasing. By Proposition 3, we then have $z(K_i)\leq z'_{\!\!i}$ , $i=1,2$ . If $z'_{\!\!1}\gt\hat z$ , then automatically $\gamma_1\geq\gamma_2$ since $f_\gamma$ is decreasing in $\gamma$ on $(0,x_0)$ . On the other hand, if $z'_{\!\!1}\in[z(K_1),\hat z]$ then, by convexity, there is a unique point $a\in[z(K_1),z'_{\!\!1}]$ such that $f_{\gamma_1}(a)=\varphi(a)$ . By Proposition 2, we then have $f_{\gamma_1}(\!\cdot\!)\leq\varphi(\!\cdot\!)$ on $[a,x_0]$ . Consequently, at $z(K_2)$ we have $f_{\gamma_1}(z(K_2))\leq \varphi(z(K_2))=l_{K_2}(z(K_2))$ . Since $f_\gamma$ is decreasing in $\gamma$ on $(0,x_0)$ , it follows that $\gamma_1\geq \gamma_2$ .

Next, assume that $\sigma(\!\cdot\!)$ is non-decreasing. Then $z'_{\!\!1}\leq z(K_1)$ by Proposition 3, so by convexity there exists a point $a\in [z'_{\!\!1},z(K_1)]$ with $f_1(a)=\varphi(a)$ . By Proposition 2, we must have $f_{\gamma_1}(\!\cdot\!)\geq\varphi(\!\cdot\!)\geq l_{K_2}(\!\cdot\!)$ on $[a,x_0]$ , and it follows that $\gamma_1\leq \gamma_2$ .

Funding Information

Support from the Swedish Research Council and from the Knut and Alice Wallenberg Foundation is gratefully acknowledged.

Competing Interests

There were no competing interests to declare which arose during the preparation or publication process of this article.

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Figure 0

Figure 1. For a given $K \leq \hat K$, the put price P(K) equals the negative reciprocal of the slope of the tangent line to $\varphi$ which passes through (K, 0).

Figure 1

Figure 2. The function $\varphi$, together with two strike prices $K_1\lt K_2$, the corresponding tangent lines $l_{K_1}$ and $l_{K_2}$, and their intersection point $\hat z$.