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When Real-World and Risk-Neutral Density Ratios Exist

Article Quant Q&A · Author: Otto Winata

Summary

The document explains when the ratio of a real-world probability density to a risk-neutral density can represent a change of measure. That ratio is the Radon–Nikodym derivative when the real-world measure is absolutely continuous with respect to the risk-neutral measure: events assigned zero probability under the latter must also have zero probability under the former. This is the condition that makes the density ratio meaningful as a scaling factor.

A pair of lognormal distributions with the same positive support illustrates a valid ratio, even when they assign different probabilities to outcomes. By contrast, a normal distribution has positive density for negative values while a lognormal distribution does not; the ratio in the direction from the lognormal measure to the normal measure is undefined there. The examples clarify that matching supports is sufficient in the illustrated case, while the formal condition is one-way absolute continuity. The discussion establishes when a density ratio exists, but does not derive a specific stochastic discount factor for a market model.

Key ideas

  • A ratio of probability densities represents a Radon–Nikodym derivative when the required absolute continuity condition holds.
  • For the derivative from one measure to another to exist, every event assigned zero probability by the reference measure must also have zero probability under the target measure.
  • Two lognormal distributions with common positive support can have a well-defined density ratio despite differing probabilities.
  • A normal distribution cannot be absolutely continuous with respect to a lognormal distribution when it assigns probability to negative outcomes.

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Full text
# Ratio of real world to risk-neutral density


# Ratio of real world to risk-neutral density












Suppose I have a risk-neutral pdf and a real-world pdf of an asset. Both functions are related by a scaling factor or the sdf which would transform the risk-neutral into the real-world density, is this correct? Would I be able to obtain this scaling factor by simply computing the ratio of the RW/RN density across X? If not, why?

## Answer by Jan Stuller (score 5)

https://quant.stackexchange.com/a/80216

The ratio of any two PDFs (if it can be defined: see below) is just the Radon-Nikodym derivative. The conditions for the Radon-Nikodym derivative to exist are given by the Radon-Nikodym theorem.

Whilst on a first read basis, the rigorous phrasing of the theorem might sound a bit abstract / difficult, the intuition is easy. The theorem says that given two probability measures $\mathbb{P}_1$ and $\mathbb{P}_2$, the Radon-Nikodym derivative $\frac{\partial\mathbb{P}_2}{\partial\mathbb{P}_1}$ exists if the two measures agree on "what is possible", which means they agree on where probabilities are zero and where they are non-zero (see footnote*).

Example 1:

Consider two log-normal random variables $X$ and $Y$, where:

$$\ln{(X)}\sim N\left(\mu -0.5 \sigma^2, \sigma\right), \quad \ln{(Y)}\sim N\left(r -0.5 \sigma^2, \sigma\right)$$

Let the PDF of $X$ be $f_X$ and the PDF of $Y$ be $f_Y$ (and the associated probability measures induced by $X$ and $Y$ are $\mathbb{P}_X$ and $\mathbb{P}_Y$). Note that the support of $X$ and $Y$ are the same: specifically the two random variables have positive densities on the real-line for $x>0$, whilst their densities are zero for $x\leq0$: therefore, these two random variables "agree on what is possible" (any $x>0$): they just assign slightly different probabilities to these outcomes. So the conditions for the Radon-Nikodym derivative to exist are satisfied and we can write:

$$\frac{\partial\mathbb{P}_Y}{\partial\mathbb{P}_X}=\frac{f_Y}{f_X}$$

Example 2:

Consider now a log-normal random variable $X$ and a normal random variable $Z$, where:

$$\ln{(X)}\sim N\left(\mu -0.5 \sigma^2, \sigma\right), \quad Z\sim N\left(\mu -0.5 \sigma^2, \sigma\right)$$

The problem here is that $Z$ has positive densities across the entire real line $\mathbb{R}$ whilst $X$ only has positive densities for $x>0$. So for the case where we want to go from $\mathbb{P}_X$ to $\mathbb{P}_Z$, the conditions for the Radon-Nikodym theorem are not satisfied and the Radon-Nikodym derivative does not exist. Indeed, if we tried to compute the ratio of the two PDFs, we would run into the following issues:

$$\frac{\partial\mathbb{P}_Z}{\partial\mathbb{P}_X}=\frac{f_Z}{f_X}=??$$

The derivative is clearly undefined $\forall x \leq 0$ due to division by zero.

*Footnote: strictly speaking, for $\frac{d\mathbb{P}_2}{d\mathbb{P}_1}$ to exsist, the theorem states that $\mathbb{P}_2$ must be absolutely continuous w.r.t. $\mathbb{P}_1$, which means that whenever $\mathbb{P}_2(A)=0$ for any $A \in \mathcal{F}$, it implies that $\mathbb{P}_1(A)=0$ (but the converse needs not to be true).

Shown in full with attribution under the source's licence. Licence: CC BY-SA 4.0 (Stack Exchange)

This summary was written by Stratmill's research agent from the original; it is not a copy of the source.