Implied Volatility with Time to Maturity
Series 1 Strike (%spot) Series 2 Strike (%spot) P-Value
6. The Profitability of Covered Call Writing with Anchoring
6.1 The Zero-Beta Straddle Performance with Anchoring
Another empirical puzzle in the Black-Scholes/CAPM framework is that zero beta straddles lose money. Goltz and Lai (2009), Coval and Shumway (2001) and others find that zero beta straddles earn negative returns on average. This is in sharp contrast with the Black-Scholes/CAPM prediction which says that the zero-beta straddles should earn the risk free rate. A zero-beta straddle is
constructed by taking a long position in corresponding call and put options with weights chosen so as to make the portfolio beta equal to zero:
π β π½πΆπππ+ (1 β π) β π½ππ’π‘ = 0 => π = βπ½ππ’π‘ π½πΆπππβ π½ππ’π‘ Where π½πΆπππ= π(π1) βππ‘πππ πΆπππ β π½ππ‘πππ and π½ππ’π‘ = (π(π1) β 1) β ππ‘πππ ππ’π‘ β π½π π‘πππ
It is straightforward to show that with anchoring, where call and put prices are determined in accordance with proposition 1, the zero-beta straddle earns a significantly smaller return than the risk free rate (with returns being negative for a wide range of realistic parameter values). See Appendix E for proof. Intuitively, with anchoring, both call and put options are more expensive when compared with Black-Scholes prices. Hence, the returns are smaller, and are typically negative.
32 Anchoring provides a unified explanation for key option pricing puzzles even in the simplest setting of geometric Brownian motion. Furthermore, two novel predictions of the anchoring model are strongly supported in the data.
7. Conclusions
Intriguing option pricing puzzles include: 1) the implied volatility skew, 2) superior historical performance of covered call writing, 3) worse-than-expected performance of zero beta straddles, and 4) the puzzling findings regarding leverage adjusted index option returns. Furthermore, it is well known that average put returns are far more negative than what the theory predicts, and average call returns are smaller than what one would expect given their systematic risk.
If the volatility of the underlying stock returns is used as a starting point which gets adjusted upwards to arrive at call option volatility, then the anchoring bias implies that such adjustments are insufficient. There is considerable field and experimental evidence of the role of anchoring in option pricing. In this article, an anchoring-adjusted option pricing model is put forward. The model provides a unified explanation for the puzzles mentioned above. Furthermore, the anchoring price lies within the bounds implied by risk-averse expected utility maximization. Two novel predictions of the model are empirically tested and found to be strongly supported in the data.
The challenge for financial economics is to enrich the elegant option pricing framework sufficiently so that it captures key empirical regularities. This article shows that incorporating the anchoring bias in the option pricing framework provides the needed enrichment, while preserving the elegance of the framework. Furthermore, anchoring works regardless of the distributional assumptions that are made about the underlying stock behavior. Hence, it is easy to combine anchoring with jump diffusion and stochastic volatility approaches. This is the subject of future research.
33
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Appendix A
The anchoring adjusted PDE can be solved by converting to heat equation and exploiting its solution.
Start by making the following transformations in (2.6): π =π 2 2 (π β π‘) π₯ = πππ πΎ=> π = πΎπ π₯ πΆ(π, π‘) = πΎ β π(π₯, π) = πΎ β π (ππ (π πΎ) , π2 2 (π β π‘)) It follows, ππΆ ππ‘ = πΎ β ππ ππβ ππ ππ‘ = πΎ β ππ ππβ (β π2 2) ππΆ ππ= πΎ β ππ ππ₯β ππ₯ ππ= πΎ β ππ ππ₯β 1 π
39 π2πΆ ππ2 = πΎ β 1 π2β π2πΆ ππ₯2 β πΎ β 1 π2 ππΆ ππ₯
Plugging the above transformations into (2.6) and writing πΜ =2(π+πΏ)π2 , and πΜ =
2π΄πΏ π2 we get: ππ ππ = π2π ππ₯2+ (πΜ β 1) ππ ππ₯β (πΜ + πΜ)π (π·1) With the boundary condition/initial condition:
πΆ(π, π) = πππ₯{π β πΎ, 0} πππππππ π(π₯, 0) = πππ₯{ππ₯β 1,0}
To eliminate the last two terms in (D1), an additional transformation is made: π(π₯, π) = ππΌπ₯+π½ππ’(π₯, π) It follows, ππ ππ₯= πΌπ πΌπ₯+π½ππ’ + ππΌπ₯+π½πππ’ ππ₯ π2π ππ₯2 = πΌ 2ππΌπ₯+π½ππ’ + 2πΌππΌπ₯+π½πππ’ ππ₯+ π πΌπ₯+π½ππ2π’ ππ₯2 ππ ππ = π½π πΌπ₯+π½ππ’ + ππΌπ₯+π½πππ’ ππ
Substituting the above transformations in (D1), we get: ππ’ ππ = π2π’ ππ₯2+ (πΌ 2+ πΌ(πΜ β 1) β (πΜ + πΜ) β π½)π’ + (2πΌ + (πΜ β 1))ππ’ ππ₯ (D2) Choose πΌ = β(πΜβ1) 2 and π½ = β (πΜ+1)2
4 β (πΜ). (D2) simplifies to the Heat equation: ππ’
ππ = π2π’
ππ₯2 (π·3) With the initial condition:
π’(π₯0, 0) = πππ₯{(π(1βπΌ)π₯0 β πβπΌπ₯0), 0} = πππ₯ {(π(
πΜ+1
40 The solution to the Heat equation in our case is:
π’(π₯, π) = 1 2βππ β« π β(π₯βπ₯4π0)2 β ββ π’(π₯0, 0)ππ₯0 Change variables: =π₯0βπ₯ β2π , which means: ππ§ = ππ₯0
β2π. Also, from the boundary condition, we know that π’ > 0 πππ π₯0 > 0. Hence, we can restrict the integration range to π§ > βπ₯
β2π π’(π₯, π) = 1 β2π β« π βπ§22 β π(πΜ+12 )(π₯+π§β2π)ππ§ β β β π₯ β2π 1 β2π β« π βπ§22 β β π₯ β2π β π(πΜβ12 )(π₯+π§β2π)ππ§ =: π»1β π»2
Complete the squares for the exponent in π»1: πΜ + 1 2 (π₯ + π§β2π) β π§2 2 = β 1 2(π§ β β2π(πΜ + 1) 2 ) 2 +πΜ + 1 2 π₯ + π (πΜ + 1)2 4 =: β1 2π¦ 2+ π
We can see that ππ¦ = ππ§ and π does not depend on π§. Hence, we can write:
π»1 = π π β2π β« π βπ¦22 ππ¦ β βπ₯ β2π β ββπ 2β (πΜ+1)
A normally distributed random variable has the following cumulative distribution function:
π(π) = 1 β2π β« π βπ¦22 ππ¦ π ββ Hence, π»1 = πππ(π1) where π1 = π₯ β2π β + βπ 2β (πΜ + 1)
41 Similarly, π»2 = πππ(π2) where π2 = π₯
β2π
β + βπ 2β (πΜ β 1) and π = πΜβ12 π₯ + π(πΜβ1)2 4
The anchoring adjusted European call pricing formula is obtained by recovering original variables: πΆ = πβπ΄βπΏ(πβπ‘){ππ(π 1π΄) β πΎπβ(π+πΏ)(πβπ‘)π(π2π΄)} Where π ππ¨ = ππ(πΊ/π²)+(π+πΉ+ ππ π)(π»βπ) πβπ»βπ πππ π π π¨ = ππ( πΊ π²)+(π+πΉβ ππ π)(π»βπ) πβπ»βπ Appendix B
By definition, at the threshold: πβπ΄πΎπΏ(πβπ‘){ππ(π
1π΄) β πΎπβ(π+πΏ)(πβπ‘)π(π2π΄)} = ππ(π1) β πΎπβπ(πβπ‘)π(π2) (E1) Solving (E1) for π΄πΎ gives the threshold value:
ππ (ππ(π1π΄)βπΎπβ(π+πΏ)(πβπ‘)π(π2π΄)
ππ(π1)βπΎπβπ(πβπ‘)π(π2) ) β
1
(πβπ‘)= |π΄Μ Μ Μ Μ | β πΏ πΎ (E2)
Appendix E
Following Coval and Shumway (2001) and some algebraic manipulations, the return from a zero- beta-straddle can be written as:
ππ π‘ππππππ = ββ¦ππΆ + π
β¦ππ β β¦ππΆ + πβ πππππ +
β¦ππ + π
β¦ππ β β¦ππΆ + πβ πππ’π‘
Where πΆ and π denote call and put prices respectively, πππππ is expected call return, πππ’π‘ is expected put return, and β¦π is call price elasticity w.r.t the underlying stock price.
Under anchoring: πππππ = π + π΄
πππ’π‘ =
(π + π΄)πΆ β ππ + πππ(πΎ) π
42 Substituting πππππ and πππ’π‘ in the expression for ππ π‘ππππππ, and simplifying implies that as long as the risk premium on the underlying is positive, it follows that:
ππ π‘ππππππ < π
Appendix F
Note that for a put option, if the underlying stock has a positive risk premium, then the expected put payoff must be less than its price. That is, expected put return is negative. The proof follows directly from realizing that if the risk premium on the underlying stock is positive, the price of a put option under anchoring is larger than the price of a put option in the Black Scholes model.