Why Black–Scholes Call Prices Decrease with Strike
Summary
The document examines why a European call’s Black–Scholes value falls as its strike rises. The central calculation differentiates the pricing formula with respect to strike. A mistaken derivative step in the original attempt obscures the result; using the identity linking the normal densities at the two Black–Scholes terms cancels the density contributions and leaves the strike sensitivity as the negative discounted probability term.
The answers also offer two broader arguments. Homogeneity of option value yields the same sensitivity, and a model-free portfolio argument compares calls at adjacent strikes: the higher-strike call has no greater payoff, with a strictly lower payoff in some states. The strict inequality requires positive probability of finishing above the lower strike. These arguments explain monotonicity, but the explicit formula applies to the stated Black–Scholes setup, and the portfolio proof relies on the option prices respecting no-arbitrage valuation.
Key ideas
- The Black–Scholes call’s strike derivative simplifies to a negative discounted normal cumulative probability.
- The identity between the two normal-density terms removes the extra terms in direct differentiation.
- Call-value homogeneity provides an alternative route to the strike sensitivity.
- A higher-strike call has a payoff no greater than a lower-strike call in any state.
- Strict decrease in the portfolio argument requires positive probability of finishing above the lower strike.
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# Attempt of an analytical proof that a call price decreases as its strike increases
# Attempt of an analytical proof that a call price decreases as its strike increases
I'm stuck trying to analytically prove that a partial derivative of a specific, lower defined function $C$ is negative. The context of this problem is actually a Black-Scholes market situation, where a price of a call option decreases as its strike increases.
For given positive constants $S, K, r, \sigma$ and $T$, we have: $$C(S,K,r, \sigma,T)=S \Phi(d_1)-Ke^{-rT}\Phi(d_2),$$ where $$d_1=\frac{\ln \frac{S}{K}+(r+\frac{1}{2}\sigma^2)T}{\sigma \sqrt{T}},$$ $$d_2=d_1-\sigma \sqrt{T}.$$
I have to prove that the function $C$ is decreasing if $K$ is increasing. First, I calculate the partial derivation: \begin{align} \frac{\partial C}{\partial K}&=S\frac{d \Phi(d_1)}{d (d_1)} \frac{\partial d_1}{\partial K}-e^{-rT}\Phi(d_2)-Ke^{-rT}\frac{d \Phi(d_2)}{d (d_2)}\frac{\partial d_2}{\partial K}\\ & = S \varphi(d_1)\frac{K}{\sigma \sqrt{T}}-e^{-rT}\Phi(d_2)-Ke^{-rT}\varphi(d_2)\frac{K}{\sigma \sqrt{T}}\\ & = K^2 \left( -e^{-rT} \frac{\varphi(d_2)}{\sigma \sqrt{T}} \right) + K \left( S \frac{\varphi(d_1)}{\sigma \sqrt{T}}\right) -e^{-rT}\Phi(d_2). \end{align} where $\Phi(x)$ is the standard normal cumulative, and $\varphi(x)$ standard normal density function.
This is more or less what I've got. I understand that I should somehow prove that the last expression is always non-negative, so I've tried calculating the determinant of the quadratic function of $K$, and I got $$D= \frac{S^2 (\varphi(d_1)^2)}{\sigma^2 T}-4 \frac{e^{-2rT }\varphi(d_2)\Phi(d_2)}{\sigma \sqrt{T}}.$$
And now I should prove that it is positive. No idea how? There is also a chance I misunderstood something and am leaving out some necessary conditions, I'm not sure.
Thanks for an insights on this, I really appreciate it.
## Answer by LocalVolatility (score 6, accepted)
https://quant.stackexchange.com/a/34682
Something went wrong in the third equality of the equation where you compute $\partial C_0 / \partial K$. Starting from the second equality, you can use that
\begin{equation} S_0 \mathcal{N}' \left( d_1 \right) = K e^{-r T} \mathcal{N}' \left( d_2 \right), \end{equation}
see e.g. Equation (1.29) in Wystup (2006). Alternatively, you could use the homogeneity result
\begin{equation} C_0 = S_0 \frac{\partial C_0}{\partial S_0} + K \frac{\partial C_0}{\partial K} \end{equation}.
see Equation (1.36) in Wystup (2006). This immediately yields the result as
\begin{equation} \frac{\partial C_0}{\partial K} = \frac{C_0 - S_0 \partial C_0 / \partial S_0}{K} = -e^{-r T} \mathcal{N} \left( d_2 \right). \end{equation}
The homogeneity result actually holds for all models with constant returns to scale, not just geometric Brownian motion, see Theorem 9 in Merton (1973).
Yet another approach to show that $\partial C_0 / \partial K < 0$ in a model-free setting is to note that the portfolio which is long a call with strike $K + \Delta$ and short a call with strike $K$ has a payoff equal to
\begin{equation} C_T = \begin{cases} -\Delta < 0 & \text{if } S_T > K + \Delta\\ K - S_T < 0 & \text{if } K + \Delta \geq S_T > K\\ 0 & \text{otherwise} \end{cases}. \end{equation}
Since the portfolio payoff is non-positive everywhere but strictly negative for some $S_T$, its initial value $C_0$ must be strictly negative if $\mathbb{P} \left\{ S_T > K \right\} > 0$. Now divide by $\Delta$, take the limit as $\Delta \downarrow 0$ and you have
\begin{equation} \frac{\partial C_0}{\partial K} = \lim_{\Delta \downarrow 0} \frac{C_0(K + \Delta) - C_0(K)}{\Delta} < 0. \end{equation}
References
Merton, Robert C. (1973) "Theory of Rational Option Pricing," Bell Journal of Economics and Management Science, Vol. 4, No. 1, pp. 141-183
Wystup, Uwe (2006) FX Options and Structured Products, Wiley Finance
## Answer by Najee (score 4)
https://quant.stackexchange.com/a/71146
One interesting property among the variables in the Black-Scholes formula is $$ S_0 \varphi(d_1) = K e^{-rT} \varphi(d_2), $$ where $\varphi(x) = \Phi'(x)$ is the normal distribution PDF.
This is because $$ d_1^2 - d_2^2 = (A+B)^2 - (A-B)^2 = 4AB = 2\log(S_0\,e^{rT}/K) $$ where $$A = \frac{\log(S_0\,e^{rT}/K)}{\sigma\sqrt{T}} \quad\text{and}\quad B = \frac{\sigma\sqrt{T}}{2}.$$
So the last line of @Milan's derivation is simplified to $$ \frac{\partial C}{\partial K} = K^2 \left( -e^{-rT} \frac{\varphi(d_2)}{\sigma \sqrt{T}} \right) + K \left( S \frac{\varphi(d_1)}{\sigma \sqrt{T}}\right) -e^{-rT}\Phi(d_2) = -e^{-rT}\Phi(d_2), $$ which is negative.
BTW, this property is also useful in the derivation of the Black-Scholes delta. See my answer.
## Answer by Milan (score -1)
https://quant.stackexchange.com/a/34683
Ok, I think I've figured it out.
\begin{align} \frac{\partial C}{\partial K}& = S \varphi(d_1)\frac{K}{\sigma \sqrt{T}}-e^{-rT}\Phi(d_2)-Ke^{-rT}\varphi(d_2)\frac{K}{\sigma \sqrt{T}}\\ & = -e^{-rT}\Phi(d_2)+\frac{K}{\sigma \sqrt{T}} \left[ S \varphi(d_1)-K e^{-rT} \varphi(d_2) \right] \\ & = -e^{-rT}\Phi(d_2)+\frac{K}{\sigma \sqrt{T}} \left[ e^{\ln S} \frac{1}{\sqrt{2 \pi}}e^{-\frac{d_1^2}{2}}-e^{\ln K} e^{-rT} \frac{1}{\sqrt{2 \pi}}e^{-\frac{d_2^2}{2}}\right] \\ & = -e^{-rT}\Phi(d_2)+\frac{K}{\sigma \sqrt{2\pi T}} \left[ e^{\ln S-\frac{d_1^2}{2}}- e^{\ln K-rT-\frac{d_2^2}{2}}\right] . \end{align} Now, we can try proving that \begin{align} \ln S-\frac{d_1^2}{2} & \stackrel{?}{=} \ln K-rT-\frac{d_2^2}{2} \\ \ln S-\frac{d_1^2}{2} & \stackrel{?}{=} \ln K-rT-\frac{(d_1-\sigma \sqrt{T})^2}{2} \\ \ln S-\frac{d_1^2}{2} & \stackrel{?}{=} \ln K-rT-\frac{(d_1^2-2d_1\sigma \sqrt{T}+\sigma^2 T)}{2} \\ \ln \frac{S}{K} & \stackrel{?}{=} -rT + d_1 \sigma \sqrt{T}-\frac{\sigma^2 T}{2} \\ \ln \frac{S}{K} +(r+\frac{\sigma^2 }{2})T & \stackrel{?}{=} d_1 \sigma \sqrt{T} \\ d_1 & = \frac{\ln \frac{S}{K} +(r+\frac{\sigma^2 }{2})T}{\sigma \sqrt{T}}. \end{align} Thus we are left with $$ \frac{\partial C}{\partial K} = -e^{-rT}\Phi(d_2), $$ implying that the partial derivative is always negative.Shown in full with attribution under the source's licence. Licence: CC BY-SA 4.0 (Stack Exchange)
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