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期权Delta(Δ)

Delta

专题
Finance / 金融
难度
L4

题目详情

A. 无分红欧式看涨的 delta 是什么?如何推导?

B. ATM(平值)看涨在 r=0r=0 时 delta 约是多少?临近到期会怎样?

C. 你多头一份看涨,并用空头标的做动态 delta 对冲。如果股价跳涨,如何调仓?

D. 估计小 τ\tau、小 rr 下平值看涨的近似价格。

Δ=fS\Delta = \frac{\partial f}{\partial S}

For a European call on a stock with dividend yield yy:
Δ=eyτN(d1).\Delta = e^{-y\tau} \,N(d_1).

For a European put on a stock with dividend yield yy:
Δ=eyτ[1N(d1)].\Delta = -\,e^{-y\tau}\,\bigl[\,1 - N(d_1)\bigr].

A. What is the delta of a European call on a non-dividend paying stock? How do you derive it?

B. Estimate the delta of an at-the-money call on a stock with zero dividend. What happens to that delta as it approaches maturity?

C. You long a GM call and decide to dynamically hedge by shorting GM shares. If GM’s stock jumps up, how do you rebalance your hedge?

D. Estimate an at-the-money call’s value for a small τ\tau and low r.r.

解析

A. 无分红欧式看涨:

Δ=cS=N(d1).\Delta=\frac{\partial c}{\partial S}=N(d_1).

对 BS 公式对 SS 求导即可。

B. 平值 SKS\approx Kr0r\approx 0 时,通常 Δ0.5\Delta\approx 0.5。当 τ0\tau\to 0,平值极限仍趋近 0.5;深度实值趋近 1,深度虚值趋近 0。

C. 若 SS\uparrowd1d_1\uparrow,则 Δ\Delta\uparrow,要保持 delta 中性需空更多标的(增加空头股数)。

D. 常见短期限近似:

c0.4σSτ.c\approx 0.4\,\sigma S\sqrt{\tau}.

Original Explanation

AnswerA:
Δ=N(d1).\Delta = N(d_1).

The standard call formula is
c=SN(d1)    KerτN(d2),d1=ln ⁣(SK)+(r+σ22)τστ,d2=d1στ.c = S\,N(d_1) \;-\; K\,e^{-r\tau}\,N(d_2), \quad d_1 = \frac{\ln\!\bigl(\tfrac{S}{K}\bigr) +(r + \tfrac{\sigma^2}{2})\,\tau} {\sigma\sqrt{\tau}}, \quad d_2 = d_1 - \sigma\sqrt{\tau}. Differentiate cc w.r.t. SS and you find cS=N(d1).\frac{\partial c}{\partial S}=N(d_1).

AnswerB:
At-the-money (ATM): S=K.S=K. Typically Δ0.5\Delta\approx 0.5 if r=0.r=0. As τ0,\tau\to0, indeed Δ0.5.\Delta\to0.5. For deep in-the-money, Δ1;\Delta\to1; for deep out-of-the-money, Δ0.\Delta\to0.


AnswerC:
Δ=N(d1).\Delta= N(d_1). If S,S\uparrow, d1,d_1\uparrow, so Δ.\Delta\uparrow. You must short more GM shares to remain delta neutral.


AnswerD:
A short, near-ATM approximation: c0.4σSτ.c \approx 0.4\,\sigma\,S\,\sqrt{\tau}.