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ImperiumImperium Quant

Methodology — 13 methods · 40 sources

The statistics behind the scripts

Each indicator is assembled from a small number of well-documented estimators. This page states each one in its bar-by-bar form, names the known failure modes and links the references the research was built from. Notation: x[1] is the previous bar, N a lookback window, rt = ln(Ct / Ct−1). The first two methods are open to everyone; the rest are for members.

01Method

Ornstein–Uhlenbeck via AR(1)

IMP·OU

A discrete-time Ornstein–Uhlenbeck process sampled at fixed intervals is exactly an AR(1). Estimating the lag-one coefficient b over a rolling window therefore yields the mean-reversion speed θ = −ln b, the half-life ln 2 / θ, the long-run mean μ and the stationary variance σ²e / (1 − b²). The z-score of the current observation should use that stationary standard deviation, not a rolling standard deviation of price.

The engine uses the known-mean estimator (μ = window mean, b = lag-1 autocovariance / lag-1 variance), which avoids the intercept-driven blow-up of a/(1−b) when b approaches one.

AR(1)
xt = a + b·xt−1 + et
OU map
θ = −ln b, μ = a/(1−b), HL = ln 2/θ, σeq2 = σe2/(1−b2)
Expected path
E[xt+h] = μ + (xt − μ)·bh

Pitfalls

  • θ is biased upward in finite samples; below ~250 observations μ and σ are unreliable and θ needs far more.
  • Raw price is nearly a random walk (b ≈ 1); fit spreads or detrended series.
  • Jumps and microstructure noise inflate θ and σ.

02Method

Dickey–Fuller unit-root test

IMP·OU

Regress Δx on xt−1 with a constant. The coefficient γ equals b − 1 from the AR(1) fit, so the t-statistic of γ is a unit-root test that shares the OU regression. Without lag augmentation this is the plain DF test; the pack uses no lags to keep it a single OLS.

Regression
Δxt = α + γ·xt−1 + ut, tDF = γ̂ / se(γ̂)
Std error
se(γ̂) = √( su2 / Σ(xt−1 − x̄t−1)2 )
Critical values
1%: −3.43, 5%: −2.86, 10%: −2.57 (constant, no trend, large n)

Pitfalls

  • Critical values are asymptotic; rolling windows of 100–300 bars have slightly more negative true thresholds.

Members only

The remaining 11 methods, with formulas, pitfalls and sources, are part of every pack.

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