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Deriving Ho-Lee Bond Prices from the Affine A and B Equations

Article Quant Q&A · Author: Michal

Summary

The document works through the affine bond-price form for the Ho-Lee short-rate model, where the short rate has a time-dependent drift and constant volatility. Substituting the model’s coefficients into the ordinary differential equations for A and B gives a differential equation for B with terminal boundary condition B(T,T)=0. Integrating backward from maturity yields B(t,T)=T−t; the endpoint condition is essential to determine the integration constant.

The answer also identifies errors in the question’s proposed A expression: it omits the square on volatility and a factor of one third. It gives the corrected integral for A as the sum of a variance contribution and a drift contribution, using b(s)=μs. These ordinary integrals determine the bond-price exponent. The explanation focuses on the boundary condition and correction to the algebra; it does not develop the broader derivation of the affine pricing equations or discuss calibration.

Key ideas

  • The Ho-Lee short-rate specification implies that B satisfies a differential equation with derivative −1.
  • The terminal condition B(T,T)=0 fixes the integration constant and gives B(t,T)=T−t.
  • The A term includes both a volatility contribution and an integral of the time-dependent drift.
  • The proposed A expression needs a squared volatility term and a factor of one third correction.

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Full text
# Ho-Lee model - A and B derivation for $P(t,T)=e^{-A(t,T)-B(t,T)r_t}$


# Ho-Lee model - A and B derivation for $P(t,T)=e^{-A(t,T)-B(t,T)r_t}$












I am analyzing the transition of the bond prices in the affine models in the form of $P(t,T)=e^{-A(t,T)-B(t,T)r_t}$

using the property that the diffusion and the drift of an affine model can be presented as $$b(t,r)=b(t)+\beta(t)r_t \quad \quad (1) $$ $$\sigma^2(t,r)=a(t)+\alpha(t)r_t \quad \quad (2) $$

where the A and B satisfy the system of the below ordinary differential equations $$\partial_t A(t,T) = \frac{1}{2} \ a(t) \ B^2(t,T) - b(t) \ B(t,T), \quad A(T,T)=0 \quad \quad (3)$$ $$\partial_t B(t,T) = \frac{1}{2} \ \alpha(t) \ B^2(t,T) - \beta(t) \ B(t,T) -1 , \quad B(T,T)=0 \quad \quad (4)$$

I am trying to derive bond price P(t,T) for the Ho-Lee model. $dr_t=\mu t dt + \sigma dW_t^*$ My understanding is that $b=\mu t, \ \beta=0, \ a=\sigma^2, \alpha=0$ will be the parameters for the eq (3) and (4), which gives

$$\partial A(t,T) = \frac{\sigma^2}{2} B^2(t,T) - \mu t \ B(t,T) \quad \quad (5)$$ $$\partial B(t,T) = -1 \quad \quad (6)$$ and further it should yield $$B(t,T)=T-t \quad \quad (7)$$

The last step is unclear to me. My questions 1) why T-t is is substituted for, not t or T 2) why the integration $\partial B=-1$ results in (T-t) and not -(T-t)? integrating a function f'(x)=-1 should give f(x)=-x, shouldn't it?

$$A(t,T)=\frac{-\sigma^2}{6}(T-t)^3 + \int_t^T b(s)(T-s)ds \quad \quad (8)$$ giving the final equation $$P(t,T)=exp \ \big{(}\frac{-\sigma}{6}(T-t)^3 -\frac{\mu}{6} T^3 + \frac{1}{2} \mu T t^2 -\frac{1}{3} \mu t^3 - (T-t)r_t \big{)} \quad \quad (9)$$

Question 3) How the integral $\int_t^T b(s)(T-s)ds$ gives $\frac{\mu}{6} T^3 - \frac{1}{2} \mu T t^2 + \frac{1}{3} \mu t^3$. I can't get the algebra here. Is this an ordinary integral?

## Answer by Hans (score 2, accepted)

https://quant.stackexchange.com/a/25836

From Equation (6), $B(t,T)=-t+c(T)$ for some function $c(T)$. $1=P(t,t)=e^{-A(t,t)-(c(t)-t)r_t}$ or $A(t,t)+(c(t)-t)r_t=0,\,\forall (r_t,t)$. So $c(t)=t, A(t,t)=0,\forall t$.

For Equation (8) you have missed the square on $\sigma$ and a factor of $\frac13$. Then you just need to substitute in the function for $b(s)$ and integrate the following to get the correct result. $$A(t,T) = -\frac{\sigma^2}{2}\int_t^T(T-s)^2ds +\mu\int_t^T s(T-s)ds.$$

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