Part VIII · The whole market · Chapter 8D

Two regimes

When hedging calms the market and when it pushes it

Where we are

Chapters 8A to 8C added every dealer's gamma into one number, gamma exposure, showed that its sign rests on an assumption about who holds what, and drew it strike by strike. This chapter shows what each sign does to prices: calm, mean-reverting markets on one side, trending and volatile ones on the other. It gives a simple model of the feedback and traces the model to the theory it comes from, from the portfolio insurance of 1987 to modern models of market impact. It also says what the model's feedback coefficient means in dollars and index points.

What you need first
  • Gamma exposure (GEX), and the dealers' hedge trade for a given move (Chapter 8A).
  • Why the sign of GEX is an assumption, and the two conventions that fill it in (Chapter 8B).
  • Why a long-gamma hedge trades against a move and a short-gamma hedge trades with it (Chapter 6D).
  • The AR(1) model, in which each return carries a fixed fraction, the weight ww, of the one before (Chapter 3B).
  • Realized volatility against implied volatility (Chapter 5E), and the square-root law of market impact (Chapter 2D).

Everything in Parts I to VII compresses to a single regime question: is the dealer book net long gamma or net short gamma? The answer sets the sign of the feedback loop between hedging and prices, and with it the whole character of intraday price action.

In plain terms

A dealer who is long gamma behaves like a thermostat, cooling the room when it warms and heating it when it cools. A dealer who is short gamma behaves like a microphone held too close to its speaker, so that every sound comes back louder. The news that moves prices is the same in both cases. What differs is whether the dealers' hedging pushes back against each move or joins it.

1 · Two regimes, one mechanism

The two regimes are mirror images of each other, row by row:

Dealers long gamma: positive GEXDealers short gamma: negative GEX
HedgingSells strength, buys weaknessBuys strength, sells weakness
Intraday behaviorMean reversionMomentum
VolatilityCompressed relative to its unhedged levelExpanded relative to its unhedged level
Favored styleRange tradingTrend following
PremiumSelling it is favored, because dealer hedging suppresses the realized volatility you are betting againstBuying it is favored, because realized volatility is amplified
What failsBreakouts often fail, because the dealer flow fades themMean reversion is dangerous: fades against the move get crushed

A toy example shows the mechanism. Suppose GEX is +$5 billion per 1% move. By Chapter 8A's hedge-flow formula, a 1% rally then has dealers selling about $5 billion of index exposure and a 1% fall has them buying about $5 billion, so each move meets a flow against it. If GEX is −$5 billion instead, the same rally has dealers buying about $5 billion and the same fall has them selling about $5 billion. The news, and the first 1% move it caused, are identical in both cases. Only the sign of the response differs.

The table is the Dealer Mechanics Lab's, and the theory later in this chapter adds two rows to it. The sign of dealer gamma changes liquidity as well as volatility, and neither sign makes prices better informed.

2 · Same shocks, opposite character

The figure below draws six price paths from 100 over 60 steps. Each step's return is a random shock, with a standard deviation of 0.08%, plus a feedback term equal to 0.45 times the previous step's return. The feedback is subtracted when dealers are long gamma (positive GEX) and added when they are short it (negative GEX). Both regimes use the same six runs of random shocks, so the sign of the feedback is the only difference. Switch between the two regimes and compare how far the paths wander.

The same shocks, opposite character. Six simulated price paths from 100 over 60 steps, each driven by its own seeded run of random returns (0.08% standard deviation a step), the same six runs in both regimes. Each step also carries a feedback term, 0.45 times the previous step's return: subtracted when dealers are long gamma (positive GEX), added when they are short it (negative GEX). Switch the regime: under positive GEX the paths cluster around 100, under negative GEX the same shocks fan out.

Under positive GEX the six paths stay between about 99.5 and 101. Under negative GEX the same shocks spread them from about 98.9 to 102.5, more than twice as wide. In the language of Chapter 3B, each regime makes returns an AR(1) process, with weight w=−0.45w = -0.45 (mean reversion) when dealers are long gamma and w=+0.45w = +0.45 (momentum) when they are short gamma. One mechanism produces both behaviors.

The same fundamentals can therefore produce qualitatively different price behavior, depending on the dealer-positioning regime. That is why regime-conditional strategy selection, the subject of Part XI, matters. The weight of 0.45 is chosen so the difference shows in six paths. It is an illustration, not a measurement, and the measured effects are far smaller, as a later section shows.

3 · The mathematics of feedback

Published GEX is positive when hedging is stabilizing, but the feedback maths reads more naturally with the opposite sign. So define the destabilizing gamma GG as the negation of published GEX, in whatever units the model uses. It is positive when dealers are net short gamma, so that their pro-trend hedging amplifies moves. It is negative when they are net long gamma, so that their contra-trend hedging damps moves. With that sign convention, the Dealer Mechanics Lab writes

σeff2=σ2(1−κG)2 \sigma_\text{eff}^2 = \frac{\sigma^2}{(1 - \kappa G)^2} (8D.1)

in which each symbol has a plain meaning, and the feedback coefficient κ\kappa carries the state of the market:

symbolmeaning
σ\sigmathe information volatility: how volatile prices would be from news alone, with no hedging feedback
σeff\sigma_\text{eff}the effective volatility: the volatility prices show once dealer hedging feeds back into them
GGthe destabilizing gamma, the negation of published GEX
κ\kappathe feedback coefficient: how far prices move per unit of hedging flow, larger when market depth is thin and when dealers hedge aggressively

Only the product κG\kappa G matters, so the units of GG and κ\kappa can be anything that makes it a pure number. Taking square roots, and keeping κG\kappa G below 1, gives σeff=σ/(1−κG)\sigma_\text{eff} = \sigma / (1 - \kappa G), and the denominator sorts the regimes:

GGPublished GEXDealers1−κG1 - \kappa GEffective volatilityRegime
below 0positivelong gammaabove 1below σ\sigmaStabilized
0zeroflat1equal to σ\sigmaNeutral
above 0negativeshort gammabelow 1above σ\sigmaAmplified
toward +1/κ+1/\kappastrongly negativedeeply short gamma, in extreme stresstoward 0toward infinityEdge of feedback explosion

In the Dealer Mechanics Lab's reading, that divergence is, mathematically, what February 5, 2018 (Volmageddon), March 16, 2020 (the Great Liquidity Crisis) and August 5, 2024 (the yen carry unwind) looked like. Chapter 8H takes the cases in detail and weighs that reading against what regulators and researchers later found.

Where the formula comes from: a feedback multiplier

One simple model produces (8D.1) exactly. It is a toy rather than the Dealer Mechanics Lab's derivation, but it shows what κ\kappa and GG do.

Step 1: the first round. News moves the price by a return ε\varepsilon, with standard deviation σ\sigma. Dealers hedge that move, and their trade moves the price by a further κG ε\kappa G\,\varepsilon, with the first move if G>0G > 0 and against it if G<0G < 0.

Step 2: the rounds that follow. The extra move needs hedging too, which adds κG\kappa G times it, (κG)2ε(\kappa G)^2 \varepsilon, and that needs hedging in turn. When κG\kappa G lies between −1 and 1, the rounds shrink and the total is a geometric series:

move=ε (1+κG+(κG)2+⋯)=ε1−κG \begin{aligned} \text{move} &= \varepsilon\,\big(1 + \kappa G + (\kappa G)^2 + \cdots\big) \\ &= \frac{\varepsilon}{1 - \kappa G} \end{aligned} (8D.2)

Step 3: the volatility. Dividing a random quantity by a constant divides its standard deviation by the same constant. The total move therefore has standard deviation σ/(1−κG)\sigma/(1 - \kappa G), and squaring it gives (8D.1).

Step 4: over time. The regime figure spreads the same feedback over successive steps, rt=w rt−1+εtr_t = w\,r_{t-1} + \varepsilon_t. A shock then reaches the price as εt\varepsilon_t in its own step, w εtw\,\varepsilon_t in the next and w2εtw^2\varepsilon_t in the one after, for a total of εt/(1−w)\varepsilon_t/(1 - w) once the echoes die out. The paths' volatility over many steps follows the same formula, with w=κGw = \kappa G.

The next figure draws the grind box's rounds one at a time, in units of the news shock ε\varepsilon. The first bar is the news, and each bar after it is one round of hedging, κG\kappa G times the round before, drawn from where the running total stood. The two sliders set κG\kappa G, from −0.9 to +0.95 and starting at +0.45, and the number of rounds shown, from 0 to 12. Watch the running total approach ε/(1−κG)\varepsilon/(1 - \kappa G), then push κG\kappa G toward 0.95 and count how many rounds are still large.

+0.45
12
total ε/(1 − κG) = 1.82ε
after 12 rounds: 1.82ε (100%)
round 12 adds under 0.01ε

Amplifying. Each round joins the move before it, so the total grows to 1.82 times the news.

One shock, and the hedging it sets off. The first bar is a news shock, ε. Each bar after it is one round of dealer hedging, κG times the round before, drawn from where the last one ended, so the bars add up to the running total. The rounds slider adds them one at a time. κG is positive when dealers are net short gamma, which is negative published GEX. Every round then joins the move before it (rose), and the total climbs toward ε/(1 − κG), the dashed line and the last bar. With κG negative every round opposes the move before it (green), and the total zigzags down to a level below the shock. Drag κG toward 0.95 and the rounds stop dying out: 12 of them leave the total far short of its limit.

At the starting κG\kappa G of +0.45, every round joins the move before it, and the total reaches 1.82ε, which 12 rounds match to within 0.01ε. At −0.45 the rounds alternate and the total settles at 0.69ε, below the shock itself. At +0.95 the limit is 20ε, but 12 rounds reach only 9.73ε, 49% of it, and the twelfth still adds 0.54ε. At −0.9 the total zigzags, 0.66ε after 12 rounds against a limit of 0.53ε. Near κG=1\kappa G = 1 the rounds stop dying out: that is the singular point of (8D.1), seen as a process.

Worked example: The regime figure, in the formula

Step 1: the weights. The regime figure's feedback of 0.45 is κG=−0.45\kappa G = -0.45 under positive GEX and κG=+0.45\kappa G = +0.45 under negative GEX.

Step 2: the multipliers. Under positive GEX the multiplier is 1/(1+0.45)=0.691/(1 + 0.45) = 0.69, so hedging removes about 31% of the volatility. Under negative GEX it is 1/(1−0.45)=1.821/(1 - 0.45) = 1.82, so hedging adds about 82%. These are the cascade figure's two totals.

Step 3: the comparison. The ratio of the two multipliers is 1.82/0.69=2.641.82/0.69 = 2.64. The regime figure's six paths span about 3.6 points under negative GEX against 1.5 under positive, a ratio of about 2.4. Six paths over 60 steps are too small a sample for a closer match.

Familiar ground

The feedback multiplier works like the design effect of a cluster-randomized trial. When outcomes within a cluster are positively correlated, the variance of an estimate is inflated by a factor that grows with the correlation, while a negative correlation would deflate it. Returns work the same way: positive feedback correlates each step with the one before and inflates the variance of the cumulative move, while negative feedback deflates it. The variance ratio test of Chapter 3B measures exactly this inflation.

Instant or lagged: what the regimes do to autocorrelation

The grind box summed its rounds within one instant, and the regime figure spread them over successive steps. Both give the same multiplier for the volatility of the cumulative move, σ/(1−w)\sigma/(1 - w). They differ on autocorrelation. If dealers hedge within the instant, each return is larger or smaller than the news, but it carries nothing of the return before: volatility changes and autocorrelation does not. If they hedge one step late, as in the figure, each return carries ww times the one before, and the lag-1 autocorrelation is ww itself.

The table's rows on mean reversion and momentum are therefore the lagged reading, and two lines of research bear on it. Baltussen, Da, Lammers and Martens (2021) study intraday returns on over 60 futures markets from 1974 to 2020. They find that "the return during the last 30 minutes before the market close is positively predicted by the return during the rest of the day". They link that intraday momentum to the gamma hedging demand of option market makers and leveraged ETFs. The predictive power "reverts over the next days".

Grossman and Zhou (1996) model portfolio insurers in general equilibrium. Like a dealer short gamma, an insurer sells as prices fall and buys as they rise, and a later section returns to the insurers of 1987. Insurers sell to other investors in bad states, and to induce those investors to buy, the risk premium must rise. The authors show that portfolio insurance "increases price volatility, causes mean reversion in asset returns". So the price overshoots within the move and partly comes back afterward. Short gamma means momentum within the move, not necessarily over the days that follow.

The measured sizes are small beside the figure's 0.45. In single stocks, Yang (2015), a job-market paper that was not published, finds that moving from the lowest to the highest quintile of option writers' hedging demand raises daily return autocorrelation from −5.0% to −1.6%. That is a change of 3.4 percentage points of autocorrelation, where the figure's weight of 0.45 is an autocorrelation of 45%. Chapter 8G gives the rest of the measured effects.

The divergence is nonlinear

A linear reading, that at G=0G = 0 effective volatility equals σ\sigma, understates what makes the formula matter in practice. Fix σ=0.15\sigma = 0.15, a baseline information volatility of 15%, and a small illustrative feedback coefficient κ=0.0010\kappa = 0.0010, then sweep GG across the regimes:

G (positioning regime)1−κG1 - \kappa Gσeff\sigma_\text{eff}
−800 (deeply stabilizing)1.808.3%
−400 (mildly stabilizing)1.4010.7%
0 (neutral)1.0015.0%
+400 (mildly destabilizing)0.6025.0%
+600 (moderate stress)0.4037.5%
+800 (acute stress)0.2075%
+900 (near-critical)0.10150%
+9500.05300%
+990 (edge of explosion)0.011,500%

From G=+800G = +800 to G=+900G = +900, a roughly 12% increase in destabilizing positioning, σeff\sigma_\text{eff} doubles from 75% to 150%. That is the operational signal: small changes in aggregate positioning produce outsized realized-volatility consequences in the stress regime. The slope of the curve makes this exact: differentiating σ/(1−κG)\sigma / (1 - \kappa G) with respect to GG gives

dσeffdG=κ σ(1−κG)2 \frac{d\sigma_\text{eff}}{dG} = \frac{\kappa\,\sigma}{(1 - \kappa G)^2} (8D.3)
Worked example: How steep the curve gets

Step 1: at neutral. At G=0G = 0, (8D.3) gives 0.0010×0.15=0.000150.0010 \times 0.15 = 0.00015 per unit of GG, so a hundred more units of GG add about 100×0.00015=0.015100 \times 0.00015 = 0.015, or 1.5 points of volatility.

Step 2: in acute stress. At G=+800G = +800 the denominator is 0.22=0.040.2^2 = 0.04, so the slope is 0.00015/0.04=0.003750.00015/0.04 = 0.00375, which is 25 times as steep. A straight line from there predicts 37.5 more points for the next 100 units of GG.

Step 3: the curve. The table's actual rise from G=+800G = +800 to +900+900 is 75 points, double even that, because the slope keeps growing along the way. The local sensitivity of σeff\sigma_\text{eff} to GG is unbounded as GG approaches 1/κ1/\kappa.

The Dealer Mechanics Lab draws a lesson for the gamma flip, the level at which estimated dealer gamma crosses zero. It reads the curve as the reason the flip matters as a level, even though no single trade is responsible for it. Read the formula closely and it adds a qualification. At G=0G = 0 damping turns into amplification smoothly, and nothing in (8D.1) jumps there. The point where the curve turns violent is κG=1\kappa G = 1, and it depends on κ\kappa, which is liquidity, as much as on positioning. No study found tests the flip as a price level (Chapter 8G).

The value κ=0.0010\kappa = 0.0010 is only illustrative, since in practice κ\kappa is fitted to the regime and varies with depth, with dealer aggressiveness and with how concentrated positioning is. The qualitative shape, slow at the wings and explosive near the critical point, is the universal feature. A later section says what κ=0.0010\kappa = 0.0010 and G=+800G = +800 mean in dollars.

A note on signs. GG is the negation of standard published GEX. Suppose a vendor reports "GEX = +$2.3B" under the JPM-era convention, where positive means stabilizing. The corresponding GG in (8D.1) is −$2.3B. Both ways of signing the number coexist in practice, so check which one your model or vendor uses before you read the sign.

Explore the curve

The figure below draws σeff=σ/(1−κG)\sigma_\text{eff} = \sigma/(1 - \kappa G) against GG from −1 to +1. Its variable is labeled "destabilizing gamma G": the negation of published GEX, positive when dealers are net short gamma. Sliders set the underlying σ\sigma from 10% to 50%, starting at 20%, and the feedback strength κ\kappa from 0 to 2, starting at 0.5. Dashed lines mark σ\sigma and the current GG, while readouts give κG\kappa G, the effective volatility and the amplification, with a verdict that runs from strongly damped to explosive.

The trigger stress button walks GG from −0.6 to +0.6 over five days, which is published GEX flipping from positive to negative. Press it at the defaults, then raise κ\kappa to 1.5 and press it again.

20%
0.50
+0.00
underlying σ = 20%
κ·G = +0.00
effective σ = 20%
amplification = 1.00×

Neutral. Effective vol equals the underlying.

The same information vol, damped or amplified by feedback. The curve is σeff = σ / (1 − κ·G) across the destabilizing gamma G, the negation of published GEX (positive when dealers are net short gamma), for the underlying σ and feedback strength κ set by the sliders; the dashed lines mark σ and the current G. Trigger stress to walk G from −0.6 to +0.6 over five days, published GEX flipping from positive to negative, and watch effective vol climb. Raise κ and the curve bends up toward the singularity at G = 1/κ, where the denominator vanishes; the curve is cut at 200%, and past that point the readouts hold at 100 times σ.

At the defaults, the stress run lifts effective volatility from 15%, strongly damped at κG=−0.30\kappa G = -0.30, to 29%, amplifying at κG=+0.30\kappa G = +0.30: less than double. With κ=1.5\kappa = 1.5, the same run reads 24% on day 3 and 43% on day 4, and ends on day 5 at κG=+0.90\kappa G = +0.90. Effective volatility there is 200%, ten times the underlying, and the verdict reads explosive. The positioning moved the same distance both times, and only the feedback strength differed.

Past G=1/κG = 1/\kappa the formula has no meaning, so the figure cuts its curve at 200% and holds its readouts at 100 times σ\sigma. To connect the figures, set κ\kappa to 0.45 and GG to +1 and then to −1. The amplification readout shows 1.82× and 0.69×, the regime figure's two multipliers and the cascade's two totals.

4 · The theory behind the formula

The formula is older than the Dealer Mechanics Lab. A line of papers from the 1990s derived it, or close relatives of it, from explicit models of hedgers whose trades move prices. Knowing that literature tells you what the formula assumes and where it stops being true.

Frey and Stremme, and Frey

Frey and Stremme (1997), in Mathematical Finance, split a market into two groups. "Reference traders" are price takers with an ordinary demand for the stock. "Program traders" follow a hedging rule for a book of options they have written, and so must trade whenever the price moves. Setting supply equal to demand gives the price process, and the abstract reports "an explicit expression for the transformation of market volatility" under the hedgers' impact:

It turns out that volatility increases and becomes time and price dependent. The strength of these effects however depends not only on the share of total demand that is due to hedging, but also significantly on the heterogeneity of the distribution of hedged payoffs. Frey and Stremme (1997)

In their logarithmic-demand case, as later papers restate it, the volatility becomes σ/(1−ρSϕS)\sigma/(1 - \rho S \phi_S). Here ρ\rho measures how much the hedgers' trading moves the price, and ϕS\phi_S is how fast their holding changes with the price. That is the book's σ/(1−κG)\sigma/(1 - \kappa G), with κ=ρ\kappa = \rho and G=SϕSG = S\phi_S. The last clause of the abstract matters for the rest of this part. A hedged book spread evenly over many strikes changes volatility everywhere a little, while a book concentrated at one strike changes it a lot near that strike and little elsewhere. That is the theoretical root of strike-local effects, pinning among them (Chapter 8E).

Frey (1998), in Finance and Stochastics, gives the cleanest version. One large trader's holding moves the price directly, and the trader replicates a claim by holding its delta. The attempt produces a nonlinear version of the Black-Scholes equation, whose solution Frey proves exists and is unique.

Frey's model in one step

Step 1: the price. Write αt\alpha_t for the large trader's holding of the stock. Frey's price follows

dSt=μSt dt+σSt dWt+ρSt dαt \begin{aligned} dS_t ={}& \mu S_t\,dt + \sigma S_t\,dW_t \\ &+ \rho S_t\,d\alpha_t \end{aligned} (8D.4)

where dWtdW_t is the random news of Chapter 7A and ρ\rho is the "market liquidity parameter": each share the trader buys lifts the price by the fraction ρ\rho.

Step 2: the hedge. A trader who replicates a claim worth V(t,S)V(t, S) holds αt=VS\alpha_t = V_S, the claim's delta. When the price moves by dSdS, the holding changes by VSS dSV_{SS}\,dS, plus terms in dtdt that do not affect volatility.

Step 3: substitute. The random part of the price move becomes dS=σS dW+ρSVSS dSdS = \sigma S\,dW + \rho S V_{SS}\,dS. Collecting the dSdS terms gives dS (1−ρSVSS)=σS dWdS\,(1 - \rho S V_{SS}) = \sigma S\,dW.

Step 4: the volatility. Dividing through, the price's volatility is σ/(1−ρSVSS)\sigma/(1 - \rho S V_{SS}). A claim with a convex payoff has VSS>0V_{SS} > 0, so its replicator buys after rises and sells after falls, and volatility goes up. That is a dealer who has sold the claim, or a portfolio insurer who promised it: short gamma, G=SVSS>0G = S V_{SS} > 0. The equation is singular where ρSVSS\rho S V_{SS} reaches 1.

State Frey's assumptions whenever you quote the formula: impact is linear and permanent, the hedger rebalances continuously to the delta of a known book, and the feedback stays below its critical value. A later section says how each assumption fails.

Other derivations, and a counter-result

Three more papers of the 1990s reach the same shape from different starting points.

  • Platen and Schweizer (1998) add hedgers' demand to noise and speculative demand in an equilibrium model. Hedging makes volatility "endogenously determined by agents' trading behavior", and their simulations "quantitatively substantiate the idea that option price distortions can be induced by feedback effects from hedging strategies". The feedback bends the implied volatility smile and skew of Chapters 5E and 5G, not only realized volatility.
  • Sircar and Papanicolaou (1998) use reference traders and "programme traders" who hedge by Black-Scholes, and derive a nonlinear pricing equation. Their models "do predict increased implied volatilities with minimal assumptions beyond those of the Black-Scholes theory", and reduce to Black-Scholes when the feedback is removed. When hedgers are a small share of the market, the correction to σ\sigma is small, which fits a modest effect on typical days.
  • Schönbucher and Wilmott (2000) derive the modified price process for an illiquid market and simulate the replication of a put, which is portfolio insurance. The family of models they belong to gives volatility of the form σ/(1−ρλ(S)SuSS)\sigma/(1 - \rho\lambda(S) S u_{SS}), rising as the replicating strategy's convexity grows.

Loeper (2018), in The Annals of Applied Probability, gives the rigorous modern version for a hedger whose every trade moves the price linearly. The resulting Black-Scholes equation "is fully non-linear and singular". Loeper shows that it is nonetheless "well posed", and proves the "existence of smooth solutions for a large class of final payoffs". The qualifier "a large class" matters: the equation is still singular, and the results cover payoffs that keep the hedge clear of the singular point.

The sign rule is not a theorem of every model. Basak (1995) models portfolio insurers as optimizing investors in a frictionless general equilibrium. He finds that "the market volatility and risk premium are decreased, and the asset and market price levels increased, by the presence of portfolio insurance". The rule of this chapter comes from models with price impact and limited liquidity. Take those away and the result can reverse.

A newer working paper by Sornette, Ulmann and Wehrli, posted on SSRN, adds the asymmetry the nonlinear table shows. It finds that option hedging creates short-lived directional instabilities. The effect is "strongly asymmetric, with a significantly more pronounced effect on the spot price when the option market maker is short compared to long the option". The damping side is bounded, and the amplifying side is not.

5 · Portfolio insurance and October 1987

Portfolio insurance was a strategy of the 1980s that gave a stock portfolio a floor without buying listed puts. The insurer replicated a put by trading, selling stock or index futures as prices fell and buying as they rose. That is a synthetic long put, and its hedging is a short-gamma program: it trades with every move, like a dealer short gamma. It is the historical case of the formula's amplifying side.

The Presidential Task Force on Market Mechanisms, known as the Brady Commission, reconstructed the market of October 14 to 20, 1987, from trade records. Its report of January 1988 put the assets under portfolio insurance at about $60 billion to $90 billion, "only 2-3% of equity assets outstanding". On October 19, as summaries of the report give it:

  • Sell programs by three portfolio insurers made up just under $2 billion of the New York Stock Exchange's sales of just under $21 billion.
  • In futures, three portfolio insurers sold the equivalent of $2.8 billion of stock, and portfolio-insurance sales totaled about $6 billion: $4 billion in futures and $2 billion in stock.
  • In the first half hour a few insurers sold futures equivalent to just under $400 million of stock, 28% of public volume. Between 11:40 AM and 2:00 PM they sold about 10,000 futures contracts.
  • Roughly 40% of futures sales by traders other than market makers came from portfolio insurers.

The Commission concluded that futures-based strategies were not the "sole cause" of the fall but "a significant factor in accelerating and exacerbating the declines". One account of the report puts insurance selling at "roughly 15% of total stock and futures sold that day". Rubinstein (1988), a co-founder of a portfolio-insurance firm and so an interested party, estimated "perhaps 12 per cent of the dollar change in net sold positions on October 19". He judged a large causal role unlikely. He also noted that the crash undermined two preconditions of every portfolio-insurance program: low transaction costs and price continuity. Replication fails exactly when prices gap, the same weakness a short-gamma dealer has.

Worked example: A small share of assets, a large share of a day

Step 1: the stock. At $60 billion to $90 billion, insured assets were 2% to 3% of equities.

Step 2: the flow. On October 19 insurers sold about $6 billion. In the first half hour, their futures sales were 28% of public volume.

Step 3: the lesson. A flow that is small against what exists can be large against what trades in a given hour. Hedge flow per 1% move, the unit of GEX, is a flow, and it has to be set against the market's depth at that moment, which is what κ\kappa does.

Why so large a fall from so small a share? Gennotte and Leland (1990) put the question in their abstract: "traditional models cannot explain how a relatively small amount of selling could cause so large a price drop". In their model some traders are informed, others infer information from prices, and hedging demand is not fully observed. Markets are then "much less liquid in their model than in traditional models". In the authors' words, "Discontinuities (or 'crashes') can occur even with relatively little hedging". The crash needs the hedging to be unobserved or underestimated. If hedging demand is known, its price impact is much smaller.

Two papers of the same period make the information point from other angles. Grossman (1988) argues that without a traded put there is "less information about the future price volatility associated with current dynamic hedging strategies". As a result, "the stocks' future price volatility can rise because of a current lack of information about the extent to which dynamic hedging strategies are in place". Jacklin, Kleidon and Pfleiderer (1992) show that if the market underestimates dynamic hedging, prices first run above fundamentals, and "the price falls when the amount of portfolio insurance is revealed". Black (1988), in an essay on the crash, noted that futures prices went far below their theoretical values just when portfolio insurers wanted to sell.

The lesson for a GEX reader is double-edged. Listed open interest is visible, so the hedging it implies can be anticipated, which is Grossman's case for traded options. The hedging a public map cannot see, in FLEX, over-the-counter and structured-product books, is the kind that did the damage in these models (Chapter 8B).

Kyle and Obizhaeva, in a paper on large bets and stock market crashes in the Review of Finance, measured how badly a linear intuition failed in 1987. Portfolio insurers sold $10.48 billion of index futures and $3.27 billion of NYSE stocks from October 15 to 20, $13.75 billion gross. "Conventional wisdom" predicted declines of 0.51% net and 0.63% gross. Their invariance model, calibrated on over 400,000 portfolio transition orders, predicted 16.77%. The actual decline was 32%.

6 · Two tests of the sign rule

A measured market: currency options

Anderegg, Ulmann and Sornette (2022), in the Journal of International Money and Finance, fit a model of this family to real positions. An earlier version was a Swiss National Bank working paper of 2019. Their model has two aggregate traders, an option market maker and an option market taker, "whose exposures reflect the total outstanding positions of all option traders in the market". The net hedge flow moves the spot rate through "a simple linear permanent impact model". Foreign exchange options trade over the counter, with no public open interest, so the authors rebuilt the market maker's gamma from trade-repository records. Their sample runs from October 21, 2017 to June 30, 2018, in EURUSD and USDJPY.

Spot volatility "is increased (decreased) by a negative (positive) gamma exposure" of the market maker. The rebuilt gamma was negative, because option takers were net long options. In size, "a negative gamma exposure of the OMM of approximately -1000 billion USD" leads "to an absolute increase in volatility of 0.7% in EURUSD and 0.9% in USDJPY". Here OMM is the option market maker, and about −1,000 billion dollars is roughly what the authors' reconstruction shows. The gamma is in the authors' own measure, whose unit the abstract does not state. The increases are absolute: 0.7 and 0.9 points of annualized volatility, under one point in the two largest currency pairs. The 2019 version explains the larger USDJPY effect by "the higher market impact of a transaction in the USDJPY spot market", EURUSD being the more liquid. Impact is the book's κ\kappa: the same dealer gamma does more in the thinner market.

A simulated market: liquidity and price discovery

Buis, Pieterse-Bloem, Verschoor and Zwinkels (2024), in the Journal of Economic Dynamics and Control, simulate an order book with an agent-based model. That is a simulation in which many traders follow simple rules and prices emerge from their orders. The authors add delta hedgers with a positive or negative net gamma, and compare normal and stressed conditions. Their findings, in the abstract's words:

  • "the presence of dynamic hedgers enhances market liquidity under normal conditions";
  • "positive gamma helps sustain liquidity in stressed scenarios, while negative gamma depletes it";
  • "an increase in the net gamma positioning of dynamic hedgers reduces volatility and increases market stability, whereas a negative gamma positioning increases volatility and makes the market more prone to failure";
  • "Price discovery typically worsens when dynamic hedgers become more prevalent, regardless of the sign of their positioning."

These are the two rows the regime table lacked. Negative gamma drains liquidity in stress, which is how κ\kappa rises in the same step as GG. Because the two move together, the explosive corner of (8D.1) is reached faster than either alone suggests. And hedging of either sign worsens price discovery, the process by which trading moves prices to what the available information justifies. A damped, pinned market is not a better-informed one. The authors suggest steering hedgers' net gamma as a policy tool, most useful for illiquid instruments. The simulation's background traders place orders by simple random rules, a "zero-intelligence" order book, so the result is a model's, not an estimate.

A market where the dealer's gamma is measured rather than assumed points the same way. Atanasova and co-authors (2025) study the bitcoin options venue Deribit from January 2021 to December 2024. When market makers' aggregate gamma inventory is negative, they "trade in the same direction as BTC price momentum", and option spreads widen. A one-standard-deviation fall in the measure goes with effective spreads 0.12% wider for out-of-the-money calls and 0.19% for puts.

7 · What sets κ: impact, in dollars and points

The units

Only κG\kappa G matters, but a reader holding a GEX number in dollars needs κ\kappa in matching units. Take GG in billions of dollars per 1% move, the negation of published GEX. Write λ\lambda for the impact of hedge flow: the index points that $1 billion of buying or selling moves the index.

A 1% move is 0.01S0.01S points. By Chapter 8A's hedge-flow formula it makes the dealers trade GG billion dollars with the move, and that flow moves the index a further λG\lambda G points. The feedback per unit of move is the second move over the first:

κG=λ G0.01 S \kappa G = \frac{\lambda\,G}{0.01\,S} (8D.5)

so κ=λ/(0.01S)\kappa = \lambda/(0.01S) per billion dollars. At S=6,000S = 6{,}000, a 1% move is 60 points.

Worked example: The table in dollars and points

Step 1: the table's κ. With GG in billions of dollars per 1% move, κ=0.0010\kappa = 0.0010 at SPX 6,000 means λ=0.0010×60=0.06\lambda = 0.0010 \times 60 = 0.06 points per $1 billion.

Step 2: the table's G. The acute-stress row, G=+800G = +800, is then $800 billion of dealer short gamma per 1% move, and the last row $990 billion. The Dealer Mechanics Lab puts aggregate dealer GEX in the range of $20 billion to $100 billion per 1% move (Chapter 8A), so the table's stress rows sit far above any total it quotes.

Step 3: a larger impact. Take instead λ=1\lambda = 1 point per $1 billion, the starting impact of the pinning figure in Chapter 8E. Then κ=1/60\kappa = 1/60 per billion, and the acute-stress κG=0.8\kappa G = 0.8 needs only 0.8×60=$480.8 \times 60 = \$48 billion of dealer short gamma per 1% move.

The same rows, restated at the two impacts. GG is in billions of dollars per 1% move, so a negative GG is a positive published GEX.

κG\kappa Gσeff\sigma_\text{eff} at σ=15%\sigma = 15\%GG at 0.06 points per $1BGG at 1 point per $1B
−0.410.7%−$400B−$24B
+0.425.0%+$400B+$24B
+0.875%+$800B+$48B
+0.9150%+$900B+$54B

Now run the check the other way. Take a constant λ\lambda of 1 point per $1 billion, and dealers short $20 billion to $100 billion of gamma per 1% move. That gives κG\kappa G from 0.33 to 1.67: amplifying at the bottom of the range and past the explosion point at the top. Nothing in the evidence shows the index behaving that way on ordinary days (Chapter 8G). Either impact per dollar of hedge flow is smaller and more curved than a constant λ\lambda, or the flow actually hedged is much smaller than gross GEX, or both. What impact research says about λ\lambda decides which.

What impact research says

The idea of one number for impact per unit of flow goes back to Kyle (1985). In his model of an informed trader, the market makers' price rises in proportion to net order flow. The slope, known as Kyle's lambda, is the price move per unit of flow, and market depth is its inverse. In that model the slope is set by how much information the flow might carry. Hedge flow is mechanical, and a market that can recognize it has less reason to move far on it, so its impact tends to be smaller and to fade.

Measured impact is not linear in size. The price impact of a metaorder, a large order worked in pieces, grows roughly as the square root of its size, the law of Chapter 2D, (2D.5). In the form the research uses,

I≈Y σDQVD I \approx Y\,\sigma_D\sqrt{\frac{Q}{V_D}} (8D.6)

where II is the move, QQ the size of the order, VDV_D the daily volume and σD\sigma_D the daily volatility, with YY a constant of order one. Sato and a co-author survey all liquid Tokyo Stock Exchange stocks over eight years. They find the exponent "equal to 1/2 within statistical errors at both the individual stock level and the individual trader level". Bucci and co-authors (2019) find "a clear crossover between a linear market impact regime and a square-root regime" in 8 million US institutional trades. Zarinelli and co-authors (2015) find that the square root fits "only across about two orders of magnitude in order size", a logarithm fitting better across five. They also find that impact relaxes on average to "approximately 2/3 of the peak impact". Tóth and co-authors (2011) trace the law to a latent order book that "vanishes around the current price".

Worked example: A day's hedge flow under the square root

Step 1: the assumptions. These inputs are assumptions for illustration, not measurements: a daily volatility of 1%, about 16% a year; $500 billion of S&P 500 exposure traded a day; and YY between 0.5 and 1.

Step 2: $1 billion. By (8D.6), 1/500=0.045\sqrt{1/500} = 0.045, so a $1 billion flow over a day moves the index by Y×1%×0.045Y \times 1\% \times 0.045. For YY from 0.5 to 1 that is 2.2 to 4.5 bps, or 1.3 to 2.7 points at 6,000.

Step 3: $10 billion. Now 10/500=0.14\sqrt{10/500} = 0.14, a move of 7 to 14 bps, or 4 to 8.5 points. Ten times the flow moves the index about three times as far.

Step 4: the loop gain. Dealers short $20 billion to $100 billion per 1% move would, on these assumptions, add 0.10 to 0.45 of each 1% move. That is a gain of 0.10 to 0.45, against 0.33 to 1.67 with a constant 1 point per $1 billion.

Four more findings bracket λ\lambda for the index:

  • The permanent anchor. Gabaix and Koijen (2021), in an NBER working paper, estimate that "investing $1 in the stock market increases the market's aggregate value by about $5", a price elasticity of demand of 0.2. It is an estimate for persistent flows over a quarter, and it is contested. At an assumed US market value of $55 trillion, $1 billion of persistent flow would add about $5 billion, roughly 1 bp or half an index point at 6,000. Hedge flow that later reverses leaves less than that behind, while its transient impact is larger.
  • Predictable flows. Brøgger (2021) finds that the daily rebalancing of leveraged volatility products is predictable in size, sign and timing. Yet "larger and more predictable flows have smaller price impact coefficients, and ... there are no excess profits from trading ahead of rebalancing flows". A flow everyone can see coming is partly absorbed in advance, which is Gennotte and Leland's point from the other side.
  • Stress. Kyle and Obizhaeva's crash comparisons show how far impact can rise. On May 6, 2010, a seller's program of 75,000 E-mini contracts, about $4.1 billion, coincided with a 5.12% drop in five minutes, from 1,113 to 1,056, against an invariance prediction of 0.61%. In 1987 the actual fall was about twice the prediction, and in 2010 about eight times. The authors read the larger-than-predicted drops as a sign that "rapid selling exacerbates transitory price impact".
  • Depth over time. A working paper by Boyarchenko, Larsen, Venter and Whelan is described in Larsen's 2024 doctoral thesis. It finds that "the depth and dealer number of the S&P 500 futures contract have decreased by 80% over a ten-year period from 2012 to 2022". It is unpublished, and the figure depends on how it defines depth. If it holds, the same GEX moves the index more than it did a decade before, so GEX numbers from different years are not comparable without a depth adjustment.

No published estimate gives the impact of dealer hedge flow in SPX in points per $1 billion. The pinning figure's range of 0 to 3 points per $1 billion spans the calm-day bracket for flows worked over a day. Stress would need values several times higher.

Worked example: Measured effects, read as loop gains

Step 1: 0DTE options. Amaya, Garcia-Ares, Pearson and Vasquez (2025), a working paper distributed by Cboe, bound the effect of market makers' 0DTE gamma on S&P 500 volatility (Chapter 8G gives the study). It adds at most 3.3 points of annualized daily volatility, and 6.4 points over 30-minute periods. Assume an information volatility of 15%. Then σeff/σ\sigma_\text{eff}/\sigma is at most 18.3/15=1.2218.3/15 = 1.22, which is 1/(1−κG)1/(1 - \kappa G) for κG=1−15/18.3=0.18\kappa G = 1 - 15/18.3 = 0.18. Over 30 minutes, 1−15/21.4=0.301 - 15/21.4 = 0.30.

Step 2: a leveraged-ETF episode. Zhao (2026), an arXiv preprint, estimates that in Korea in 2026, self-reinforcing leveraged-ETF rebalancing "raised SK Hynix's annualized volatility from 100.0% to 136.7% over nine weeks". That is a multiplier of 1.367, a gain of 1−1/1.367=0.271 - 1/1.367 = 0.27.

Step 3: the comparison. Both gains are far below 1, and far below the table's stress rows. No study found estimates an SPX feedback gain near the singular point.

The figure below puts the three views of λ\lambda on one chart. The horizontal axis is GG, dealers' short gamma in billions of dollars per 1% move, the negative of published GEX, from −$100 billion to +$100 billion and starting at +$20 billion. The vertical axis is the loop gain κG\kappa G for a 1% move. The straight line is constant impact at the λ\lambda you set, from 0 to 3 points per $1 billion and starting at 1, by (8D.5), with spot starting at 6,000. The band is square-root impact on the worked example's assumptions, with YY from 0.5 to 1. A green strip marks the gains of 0.18 to 0.30 read from the studies, and a dashed line the explosive gain of 1.

short $20B
1.0 pt per $1B
6,000
constant: κG = +0.33, ×1.50
square root: +0.10 to +0.20
constant λ explodes at G = $60B

Amplifying. Dealers short $20 billion per 1% move multiply each move by 1.50 with constant impact, and by 1.11 to 1.25 with square-root impact.

The same dealers, two laws of impact. The horizontal axis is G, the dealers' short gamma in billions of dollars per 1% move, the negative of published GEX. The vertical axis is the loop gain κG, the share of each 1% move that the dealers' own hedging adds, and the amplification 1/(1 − κG) is in the readouts. The straight line is a constant impact of λ index points per $1 billion, κG = λG/(0.01S). The band is square-root impact for a 1% move, Y × σD × √(G/VD) ÷ 1%, on the chapter's illustrative assumptions: daily volatility σD of 1%, $500 billion traded a day and Y from 0.5 to 1. The shaded strip is the gains the chapter reads from two studies, 0.18 to 0.30. At a gain of 1 the loop is explosive, and the formula has no finite answer.

At the start, constant impact gives κG=0.33\kappa G = 0.33 and multiplies every move by 1.50, while square-root impact gives 0.10 to 0.20, a multiplier of 1.11 to 1.25. Drag GG to +$100 billion: the straight line crosses the explosive gain at $60 billion and reads 1.67, while the band stays between 0.22 and 0.45. Across the Lab's range of $20 billion to $100 billion the band stays within reach of the studies' strip, and the straight line has left it before $20 billion. Drag GG below zero and long gamma damps, with the two laws apart in the same way: at −$50 billion, constant impact shrinks each move to ×0.55 and square-root impact to ×0.76 to ×0.86.

8 · What the formula leaves out

Each of the formula's assumptions fails in a known way, and each failure has a literature:

  1. Linear, permanent impact. Impact is concave and partly transient, as above.
  2. Continuous hedging of a known book. Almgren and Li (2016) find that an optimal hedger "trades smoothly towards the classical Black-Scholes delta, with trading intensity proportional to instantaneous mishedge and inversely proportional to illiquidity". Aubert, Chevalier and Ly Vath (2025) model a market maker whose hedging has transient as well as permanent impact, and who hedges in discrete bursts rather than continuously. Either way the flow is spread out and lumpy, not delivered at each tick.
  3. Everyone else's demand is unchanged. Other traders anticipate predictable flow and trade against it, as Brøgger's result shows, so gross mechanical flow is not net price pressure.
  4. Feedback below its critical value. Near κG=1\kappa G = 1 the smooth model gives way to gaps and crashes, as in Gennotte and Leland's model and Kyle and Obizhaeva's comparisons.

Two further omissions matter for anyone reading a map of open-interest gamma. The first is new trades. Egebjerg and Kokholm (2024), in an SSRN working paper, split the impact of market makers' hedging in two. The "gamma effect" is rebalancing an unchanged book as spot moves, and the "inventory effect" is hedging new option trades. Studying the gamma effect alone "can underestimate the total effect when the OMM's inventory adjustments reinforce the gamma impact and overestimate it when the adjustments move in the opposite direction". In SPX data, both components "are significant and with impact in line with the model predictions". A burst of customer call buying is hedged at once and moves the index even when the stock of gamma has not changed. A map of yesterday's open interest shows only the first effect.

The second omission is other hedgers. GG in the formula is everyone who trades with the move, not only option dealers. A leveraged or inverse ETF with assets AA and multiple LL trades L(L−1)xAL(L-1)xA after a day's return xx, always with the move (Chapter 8H). Tuzun (2013), in a Federal Reserve working paper, estimated for the fund assets of that time that "A 1% increase in broad stock-market indexes induces LETFs to originate rebalancing flows equivalent to $1.04 billion worth of stock". Volatility-targeting funds and trend followers also trade with moves, on longer lags. Target-date funds trade against them: Parker, Schoar and Sun (2023) find that they move retirement investors into "macrocontrarian strategies that sell stocks after relatively good stock market performance". Dealer GEX is one term in the market's net GG, and a map of option gamma shows none of the others.

9 · How large the feedback is in practice

The dealer-feedback story is real and quantifiable, but its practical effect is modest on a typical day. Chapter 8G reviews the studies that measure it and sets them side by side in their own units. They run from Barbon and Buraschi's intraday momentum and reversal in stocks to the 0DTE studies of Dim, Eraker and Vilkov and of Adams and co-authors.

In the Dealer Mechanics Lab's reading, the episodes that everyone remembers are February 2018, March 2020, the GME squeeze and the August 5, 2024 unwind. They are the right tail of this distribution, where feedback briefly approached the unstable threshold (Chapters 8H and 8I). On most days, GEX is a probabilistic prior you can use to bias your strategy selection, not a deterministic forecast.

What to do with a regime reading is Chapter 8J's subject, and the book's two sources weigh it differently. The Dealer Mechanics Lab pairs the sign of GEX with the shape of the VIX term structure as a decision boundary for choosing strategies. The Edge Book keeps the sign as a low-confidence filter, worth 10% to 15% of one filter's weight, and ignores it when it disagrees with the term structure (Chapter 10H). Chapter 8J sets out both, and turns the regime into a multiplier on size rather than a trigger for trades.

In practice

In an account, the regime changes size and stops before it changes which trades you take. A stop set at two standard deviations of a day's move sits at about 1.9% when effective volatility is 15%, because a day's standard deviation is then 15%/252=0.94%15\%/\sqrt{252} = 0.94\% (Chapter 5E). At 29%, the top of the explorer's default stress run, the same rule puts the stop at about 3.7%, and a stop left at 1.9% is hit by ordinary noise. Size falls for the same reason: with the stop nearly twice as far away, the same dollar risk buys about half the position.

When it fails

The regime read fails in three ways. The sign itself can be wrong, since it rests on a convention about who holds what (Chapter 8B). κ\kappa is not a constant: when depth vanishes, the same destabilizing gamma that meant mild amplification can approach the singular point, where a linear intuition badly understates the move (Chapter 8H). And the formula's own assumptions, linear permanent impact and continuous hedging of a known book, fail most in the episodes where it predicts the most.

Decision rule

Read the regime as a statement about volatility, and convert before you compute:

  • Convert the sign first. GG is minus published GEX, and published GEX carries a vendor's convention (Chapter 8B). Check both before you read either.
  • Use the formula for direction and shape, not for a number. No published estimate gives κ\kappa for SPX hedge flow, so do not turn a GEX number into a volatility forecast.
  • Watch depth as closely as positioning. The same GG matters more on a thin day, when κ\kappa is high, and thin depth and short gamma tend to arrive together.
  • Size stops from effective volatility, as in the practice callout, and cut size when dealers are short gamma and the market is thin at the same time.
  • Leave the choice of strategy to Chapter 8J, where the sign is a size multiplier, not a trigger.
Common mistake: reading the regime as a forecast

Positive GEX does not mean the market cannot move: on most days the regime is only a probabilistic prior. The episodes that did damage were the right tail, when the feedback briefly approached its unstable threshold. A sizing rule has to survive those episodes, not only the typical day.

Common mistake: mixing up G and GEX

The feedback formula uses GG, the negation of published GEX. Put a vendor's "+$2.3B" into it unconverted, and a stabilizing regime reads as an amplifying one. Convert the sign first, and then check the vendor's convention from Chapter 8B as well. A dollar GEX also needs an impact in points per dollar before it means anything in (8D.1), by (8D.5).

What to carry forward
  • Long dealer gamma (positive GEX) makes hedging trade against moves: mean reversion and compressed volatility. Short dealer gamma (negative GEX) makes it trade with them: momentum and expanded volatility.
  • With destabilizing gamma G=−GEXG = -\text{GEX}, effective volatility is σ/(1−κG)\sigma/(1 - \kappa G): damped for G<0G < 0, amplified for G>0G > 0, and unbounded as GG nears 1/κ1/\kappa. Its slope grows as 1/(1−κG)21/(1 - \kappa G)^2, so small changes in positioning matter most in stress.
  • The formula is Frey and Stremme's (1997) and Frey's (1998), from models with linear, permanent impact and continuous hedging of a known book. The sign rule holds in models with impact and limited liquidity, not in every equilibrium model.
  • In dollars, κG=λG/(0.01S)\kappa G = \lambda G/(0.01S). The illustrative κ=0.001\kappa = 0.001 is 0.06 points per $1 billion, and its stress rows are hundreds of billions per 1%. Measured impact is concave, lower for predictable flow and several times higher in fast one-sided selling.
  • Measured effects are modest on typical days and large only in the right tail. What to do with the regime is Chapter 8J's subject.

10 · Check yourself

Question 1

With σ=20%\sigma = 20\% and κ=0.5\kappa = 0.5, what is effective volatility at G=+0.8G = +0.8, and what does that GG say about dealers?

Answer

Since 1−0.5×0.8=0.61 - 0.5 \times 0.8 = 0.6, effective volatility is 0.20/0.6=33%0.20/0.6 = 33\%. A positive GG is negative published GEX: dealers are net short gamma, and their hedging amplifies moves.

Question 2

With σ=0.15\sigma = 0.15 and κ=0.0010\kappa = 0.0010, how much does effective volatility rise when GG moves from +400 to +600, and when it moves from −600 to −400?

Answer

From +400 to +600 it rises from 25% to 37.5%, which is 12.5 points. From −600 to −400 it rises from 0.15/1.6=9.4%0.15/1.6 = 9.4\% to 0.15/1.4=10.7%0.15/1.4 = 10.7\%, about 1.3 points. The same 200 units of positioning do about ten times as much on the destabilizing side.

Question 3

Why do the regime figure's negative-GEX paths trend, although the random shocks have no drift?

Answer

Each return carries +0.45 times the one before, so a move tends to be followed by another in the same direction, which is positive autocorrelation, or momentum. Over many steps each shock's effect on the price is multiplied by 1/(1−0.45)=1.821/(1 - 0.45) = 1.82.

Question 4

A vendor shows GEX of −$15 billion per 1% move with SPX at 6,000. If each $1 billion of hedge flow moves the index 2 points, what is κG\kappa G, and what does (8D.1) give for an information volatility of 16%? Why should you not trust the answer?

Answer

G=+15G = +15, so by (8D.5) κG=2×15/60=0.5\kappa G = 2 \times 15/60 = 0.5, and effective volatility is 16%/0.5=32%16\%/0.5 = 32\%. The answer rests on a constant impact of 2 points per $1 billion, which no study measures for SPX. Real impact is concave and partly transient, the flow actually hedged can be smaller than gross GEX, and the sign itself rests on the vendor's convention.

Question 5

Portfolio insurance covered only 2% to 3% of equity assets in 1987. How could it matter so much?

Answer

What matters is the flow against what trades at the moment, not the stock against what exists. On October 19 insurers sold about $6 billion, and in the first half hour their futures sales were 28% of public volume. Gennotte and Leland add that when the market cannot see the hedging, it is far less liquid than traditional models assume, so relatively little hedging can cause a crash.

Question 6

In Frey's model, where does the formula break, and what does the break mean?

Answer

Where ρSVSS\rho S V_{SS}, the book's κG\kappa G, reaches 1. There the nonlinear Black-Scholes equation is singular: the hedger's own trades would move the price as much as the move they respond to, and the smooth price process no longer exists. Models that go past that point, such as Gennotte and Leland's, produce gaps and crashes rather than a very high but finite volatility.