Stylized facts of financial returns are robust qualitative statistical regularities found across many instruments or datasets, abstracting from their individual details. Examples include heavy return-distribution tails relative to a Gaussian model, weak linear autocorrelation of many liquid-market returns beyond short lags, and persistent clustering of large absolute or squared returns. Some markets also show asymmetric return-volatility responses and partial movement toward a Gaussian aggregate distribution at longer horizons.
These are empirical tendencies with sampling-scale and market qualifications, not exact universal equations. In particular, weak return autocorrelation does not imply independent increments: volatility clustering and higher-order dependence can remain. A useful model should state which regularities it explains and which its assumptions exclude, rather than treating one convenient random-walk model as an observed law.
Let ST be the terminal asset price and K a common strike or forward delivery price. A long European call and put have expiry payoffsThe call is zero below K and then rises with slope one; the put falls with slope minus one below K and is zero above it. A long forward instead has FTlong=ST−K and a short forward has FTshort=K−ST. Both are straight lines crossing zero at K, with negative as well as positive outcomes.
CT=(ST−K)+,PT=(K−ST)+.
The option's exercise right truncates the unfavourable side, whereas the forward is an obligation. These are payoffs, not total profits: an option premium and its financing cost have not been subtracted. A newly agreed fair forward may have zero initial value while still having a nonzero future delivery price.
Assume a non-dividend-paying tradable asset follows geometric Brownian motion dS=μSdt+σSdW, with constant volatility σ and risk-free rate r. Trading is continuous, frictionless and divisible; borrowing and lending occur at the same rate, short selling is allowed, the strategy is self-financing, and there are no jumps or arbitrage opportunities. These are modelling assumptions, not assertions that market returns are exactly Gaussian or that hedging is costless in practice.
For a smooth option price V(S,t), Itô's formula givesReplicate it by Δ shares and a cash account of value b=V−ΔS. Self-financing requires dV=ΔdS+rbdt. Matching the stochastic term fixes Δ=VS. Matching the remaining drift and cancelling the physical drift μ then givesThis is the Black-Scholes equation. The cancellation does not assert that the actual expected asset return equals r; risk-neutral valuation is a consequence of replication under these assumptions.
dV=(Vt+μSVS+21σ2S2VSS)dt+σSVSdW.
Vt+21σ2S2VSS+rSVS−rV=0.
For a European call, impose V(S,T)=(S−K)+, with V(0,t)=0 and V(S,t)∼S−Ke−r(T−t) for large S. Its writer hedges the short option by holding Δ=∂V/∂S shares and investing or borrowing the residual cash V−ΔS, rebalancing as S and time change. In the constant-parameter model Δ=N(d1), where d1=[log(S/K)+(r+σ2/2)(T−t)]/[σT−t] and N is the standard normal cumulative distribution. Continuous rebalancing is an ideal limit: transaction costs, discrete trading, jumps and changing volatility create residual hedge risk. Writing the self-financing gains equation explicitly avoids incorrectly adding an unfinanced SdΔ term to the strategy.
Implied volatility is the volatility parameter that makes a specified option-pricing model reproduce an observed option price. For a call, it solvesFor positive time to expiry and positive asset and strike prices, the Black-Scholes call price increases with σ, so an interior arbitrage-consistent price gives a unique finite positive value. It is an inverse model parameter, not the sample standard deviation of past returns or a guaranteed forecast of future realised volatility. Different implied volatilities across strikes or maturities form smiles or surfaces, signalling that one constant volatility does not fit all prices simultaneously.
CBS(S,K,T−t,r;σimp)=Cmarket.
Ancestors (10)
- S9
- 2012
- Past exam of the short options paper shared by Prelims and Parts A and B of the physics course of the University of Oxford
- Short options paper shared by Prelims and Parts A and B of the physics course of the University of Oxford
- Physics course of the University of Oxford
- Undergraduate course of the University of Oxford
- Course of the University of Oxford
- University of Oxford
- List of universities
- Home
Discussion (0)
New discussionThere are no discussions about this article yet.
Articles by others on the same topic (0)
There are currently no matching articles.
