Interest rate models in fixed income all belong to the same family: mean-reverting diffusions. The short rate is modelled as a process that is pulled back toward a long-run mean at rate , with randomness added by a Brownian shock. The two workhorses are:
- Vasicek/OU: — rates are Gaussian, can go negative.
- CIR: — rates stay non-negative when (Feller condition).
The explicit solution for OU/Vasicek via the integrating factor is the cleanest example of an exactly solvable SDE. The CIR process is the square of a Bessel process (from Local Martingales and the Bessel Process); its transition density is non-central chi-squared, giving an explicit bond-pricing formula via the Feynman-Kac PDE.
In the Black-Scholes world, the short rate is constant. Switching to Vasicek or CIR introduces rate risk into bond prices, allowing the term structure (yield curve) to be modelled dynamically. Zero-coupon bond prices become functions of alone (Markov property), and the Feynman-Kac PDE gives closed-form affine expressions .
Learning objectives. By the end of this note you should be able to:
- Derive the explicit solution for the OU/Vasicek SDE via the integrating factor.
- State the mean, variance, and stationary distribution of the OU process.
- State the Feller condition for CIR and explain its connection to the Bessel process.
- Write the Feynman-Kac PDE for Vasicek bond prices and state the affine solution form.
- Interpret the CIR non-central chi-squared transition density.
In this lesson
- The OU/Vasicek Process
- The CIR Process
- Bond Pricing via Feynman-Kac
- Simulation
Before you start
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