Cox–Ingersoll–Ross model explained

In mathematical finance, the Cox–Ingersoll–Ross (CIR) model describes the evolution of interest rates. It is a type of "one factor model" (short-rate model) as it describes interest rate movements as driven by only one source of market risk. The model can be used in the valuation of interest rate derivatives. It was introduced in 1985[1] by John C. Cox, Jonathan E. Ingersoll and Stephen A. Ross as an extension of the Vasicek model, itself an Ornstein–Uhlenbeck_process.

The model

The CIR model describes the instantaneous interest rate

rt

with a Feller square-root process, whose stochastic differential equation is

drt=a(b-rt)dt+\sigma\sqrt{rt}dWt,

where

Wt

is a Wiener process (modelling the random market risk factor) and

a

,

b

, and

\sigma

are the parameters. The parameter

a

corresponds to the speed of adjustment to the mean

b

, and

\sigma

to volatility. The drift factor,

a(b-rt)

, is exactly the same as in the Vasicek model. It ensures mean reversion of the interest rate towards the long run value

b

, with speed of adjustment governed by the strictly positive parameter

a

.

The standard deviation factor,

\sigma\sqrt{rt}

, avoids the possibility of negative interest rates for all positive values of

a

and

b

.An interest rate of zero is also precluded if the condition

2ab\geq\sigma2

is met. More generally, when the rate (

rt

) is close to zero, the standard deviation (

\sigma\sqrt{rt}

) also becomes very small, which dampens the effect of the random shock on the rate. Consequently, when the rate gets close to zero, its evolution becomes dominated by the drift factor, which pushes the rate upwards (towards equilibrium).

In the case

4ab=\sigma2

,[2] the Feller square-root process can be obtained from the square of an Ornstein–Uhlenbeck process. It is ergodic and possesses a stationary distribution. It is used in the Heston model to model stochastic volatility.

Distribution

The distribution of future values of a CIR process can be computed in closed form:

rt+T=

Y
2c

,

where

c=2a
(1-e-aT)\sigma2
, and Y is a non-central chi-squared distribution with
4ab
\sigma2
degrees of freedom and non-centrality parameter

2c

-aT
r
te
. Formally the probability density function is:

f(rt+T

-u-v
;r
t,a,b,\sigma)=ce

\left(

v
u

\right)q/2Iq(2\sqrt{uv}),

where

q=

2ab
\sigma2

-1

,

u=crte-aT

,

v=crt+T

, and

Iq(2\sqrt{uv})

is a modified Bessel function of the first kind of order

q

.

Due to mean reversion, as time becomes large, the distribution of

rinfty

will approach a gamma distribution with the probability density of:
f(r
infty;a,b,\sigma)=\beta\alpha
\Gamma(\alpha)
\alpha-1
r
infty
-\betarinfty
e

,

where

\beta=2a/\sigma2

and

\alpha=2ab/\sigma2

.To derive the asymptotic distribution

pinfty

for the CIR model, we must use the Fokker-Planck equation:

{\partialp\over{\partialt}}+{\partial\over{\partialr}}[a(b-r)p]={1\over{2}}\sigma2{\partial2\over{\partialr2

}}(rp)

Our interest is in the particular case when

\partialtp0

, which leads to the simplified equation:

a(b-r)pinfty={1\over{2}}\sigma2\left(pinfty+r{dpinfty\over{dr}}\right)

Defining

\alpha=2ab/\sigma2

and

\beta=2a/\sigma2

and rearranging terms leads to the equation:

{\alpha-1\over{r}}-\beta={d\over{dr}}logpinfty

Integrating shows us that:

pinfty\proptor\alpha-1e-\beta

Over the range

pinfty\in(0,infty]

, this density describes a gamma distribution. Therefore, the asymptotic distribution of the CIR model is a gamma distribution.

Properties

\sigma\sqrt{rt}

),

r0

the process will never touch zero, if

2ab\geq\sigma2

; otherwise it can occasionally touch the zero point,

\operatornameE[rt\midr0]=r0e-at+b(1-e-at)

, so long term mean is

b

,

\operatorname{Var}[rt\midr0]=r0

\sigma2
a

(e--e-2a)+

b\sigma2
2a

(1-e-)2.

Calibration

The continuous SDE can be discretized as follows

rt+\Delta-rt=a(b-rt)\Deltat+\sigma\sqrt{rt\Deltat}\varepsilont,

which is equivalent to

rt+\Delta-rt=
\sqrtrt
ab\Deltat
\sqrtrt

-a\sqrtrt\Deltat+\sigma\sqrt{\Deltat}\varepsilont,

provided

\varepsilont

is n.i.i.d. (0,1). This equation can be used for a linear regression.

Simulation

Stochastic simulation of the CIR process can be achieved using two variants:

Bond pricing

Under the no-arbitrage assumption, a bond may be priced using this interest rate process. The bond price is exponential affine in the interest rate:

P(t,T)=A(t,T)

-B(t,T)rt
e

where

A(t,T)=\left(

2he(a+h)(T-t)/2
2h+(a+h)(eh(T-t)-1)
2ab/\sigma2
\right)

B(t,T)=

2(eh(T-t)-1)
2h+(a+h)(eh(T-t)-1)

h=\sqrt{a2+2\sigma2}

Extensions

The CIR model uses a special case of a basic affine jump diffusion, which still permits a closed-form expression for bond prices. Time varying functions replacing coefficients can be introduced in the model in order to make it consistent with a pre-assigned term structure of interest rates and possibly volatilities. The most general approach is in Maghsoodi (1996).[3] A more tractable approach is in Brigo and Mercurio (2001b)[4] where an external time-dependent shift is added to the model for consistency with an input term structure of rates.

A significant extension of the CIR model to the case of stochastic mean and stochastic volatility is given by Lin Chen (1996) and is known as Chen model. A more recent extension for handling cluster volatility, negative interest rates and different distributions is the so-called "CIR #" by Orlando, Mininni and Bufalo (2018,[5] 2019,[6] [7] 2020,[8] 2021,[9] 2023[10]) and a simpler extension focussing on negative interest rates was proposed by Di Francesco and Kamm (2021,[11] 2022[12]), which are referred to as the CIR- and CIR-- models.

See also

Further References

Notes and References

  1. Web site: A Theory of the Term Structure of Interest Rates - The Econometric Society . 2023-10-14 . www.econometricsociety.org . en.
  2. Yuliya Mishura, Andrey Pilipenko & Anton Yurchenko-Tytarenko(10 Jan 2024): Low-dimensional Cox-Ingersoll-Ross process, Stochastics, DOI:10.1080/17442508.2023.2300291
  3. Maghsoodi . Yoosef . January 1996 . Solution of the Extended Cir Term Structure and Bond Option Valuation . Mathematical Finance . en . 6 . 1 . 89–109 . 10.1111/j.1467-9965.1996.tb00113.x . 0960-1627.
  4. Brigo . Damiano . Mercurio . Fabio . 2001-07-01 . A deterministic–shift extension of analytically–tractable and time–homogeneous short–rate models . Finance and Stochastics . en . 5 . 3 . 369–387 . 10.1007/PL00013541 . 35316609 . 0949-2984.
  5. Book: Orlando . Giuseppe . Mininni . Rosa Maria . Bufalo . Michele . A New Approach to CIR Short-Term Rates Modelling . New Methods in Fixed Income Modeling . Contributions to Management Science . 2018 . 35–43 . 10.1007/978-3-319-95285-7_2 . Springer International Publishing. 978-3-319-95284-0 .
  6. Orlando . Giuseppe . Mininni . Rosa Maria . Bufalo . Michele . A new approach to forecast market interest rates through the CIR model . Studies in Economics and Finance . 1 January 2019 . 37. 2. 267–292 . 10.1108/SEF-03-2019-0116 . 204424299 . 1086-7376.
  7. Orlando . Giuseppe . Mininni . Rosa Maria . Bufalo . Michele . Interest rates calibration with a CIR model . The Journal of Risk Finance . 19 August 2019 . 20 . 4 . 370–387 . 10.1108/JRF-05-2019-0080 . 204435499 . en . 1526-5943.
  8. Orlando. Giuseppe. Mininni. Rosa Maria. Bufalo. Michele. July 2020. Forecasting interest rates through Vasicek and CIR models: A partitioning approach. Journal of Forecasting. en. 39. 4. 569–579. 10.1002/for.2642. 0277-6693. 1901.02246. 126507446 .
  9. Orlando. Giuseppe. Bufalo. Michele. 2021-05-26. Interest rates forecasting: Between Hull and White and the CIR#—How to make a single-factor model work. Journal of Forecasting. 40 . 8 . en. 1566–1580. 10.1002/for.2783. 0277-6693. free.
  10. Orlando . Giuseppe . Bufalo . Michele . 2023-07-14 . Time series forecasting with the CIR# model: from hectic markets sentiments to regular seasonal tourism . Technological and Economic Development of Economy . en . 29 . 4 . 1216–1238 . 10.3846/tede.2023.19294 . 2029-4921. free .
  11. Di Francesco . Marco . Kamm . Kevin . How to handle negative interest rates in a CIR framework . 4 October 2021 . SeMa Journal. 79 . 4 . 593–618 . 10.1007/s40324-021-00267-w. 235358123 . free . 2106.03716 .
  12. Di Francesco . Marco . Kamm . Kevin . On the Deterministic-Shift Extended CIR Model in a Negative Interest Rate Framework . International Journal of Financial Studies. 2022 . 10 . 2 . 38 . 10.3390/ijfs10020038. free . 11585/916048 . free .