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Delay Ait-Sahalia-type interest rate model with jumps and its strong approximation

  • Emmanuel Coffie EMAIL logo
Published/Copyright: August 25, 2023
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Abstract

In this paper, we study the analytical properties of the true solution to the generalised delay Ait-Sahalia-type interest rate model with Poisson-driven jumps. Since this model does not have a closed-form solution, we employ several new truncated Euler-Maruyama (EM) techniques to investigate the finite-time strong convergence theory of the numerical solution under the local Lipschitz condition plus the Khasminskii-type condition. We justify the strong convergence result for Monte Carlo calibration and valuation of some debt and derivative instruments.

Appendix

The proof for Lemma 3.2 is provided below.

Proof of Lemma 3.2.

If we assume that x < x ¯ , then the mean-value theorem gives us

| x ρ - x ¯ ρ | ρ ( | x | ρ - 1 + | x ¯ | ρ - 1 ) | x - x ¯ |

and

| x θ - x ¯ θ | θ ( | x | θ - 1 + | x ¯ | θ - 1 ) | x - x ¯ | .

It then follows that

| f ( x ) - f ( x ¯ ) | + | g ( x ) - g ( x ¯ ) | + | h ( x ) - h ( x ¯ ) |
= | α - 1 ( 1 x - 1 x ¯ ) + α 1 ( x - x ¯ ) - α 2 ( x ρ + x ¯ ρ ) | + | x θ - x ¯ θ | + α 3 | x - x ¯ |
α - 1 | 1 x x ¯ | | x - x ¯ | + α 1 | x - x ¯ | - α 2 ρ ( | x | ρ - 1 + | x ¯ | ρ - 1 ) | x - x ¯ | + θ ( | x | θ - 1 + | x ¯ | θ - 1 ) | x - x ¯ | + α 3 | x - x ¯ |
( α - 1 | 1 x x ¯ | + α 1 - α 2 ρ ( | x | ρ - 1 + | x ¯ | ρ - 1 ) + θ ( | x | θ - 1 + | x ¯ | θ - 1 ) + α 3 ) | x - x ¯ | .

Noting from Assumption 2.3 that

ρ + 1 > 2 θ ρ - 1 > 2 ( θ - 1 ) ρ - 1 > θ - 1 ,

then for any R > 0 , there exists a constant K R > 0 such that for x , x ¯ [ 1 R , R ] , we get

| f ( x ) - f ( x ¯ ) | + | g ( x ) - g ( x ¯ ) | + | h ( x ) - h ( x ¯ ) | K R | x - x ¯ | ,

as required, where

K R α 1 + α 3 + α - 1 | 1 x x ¯ | - α 2 ρ ( | x | ρ - 1 + | x ¯ | ρ - 1 ) + θ ( | x | θ - 1 + | x ¯ | θ - 1 ) .

Here is the proof for Lemma 3.3.

Proof of Lemma 3.3.

By Assumptions 2.1 and 2.3, we get

x f ( x ) + p - 1 2 | φ ( y ) g ( x ) | 2 = x ( α - 1 x - 1 - α 0 + α 1 x - α 2 x ρ ) + p - 1 2 | φ ( y ) g ( x ) | 2
( α - 1 - α 0 x + α 1 x 2 - α 2 x ρ + 1 ) + p - 1 2 σ 2 x 2 θ
Q ( p ) + α - 1 - α 0 x + α 1 x 2
Q ( p ) + α - 1 + α 1 x 2
𝒥 4 ( 1 + | x | 2 ) ,

where 𝒥 4 = ( α - 1 + Q ( p ) ) α 1 and Q ( p ) - α 2 x ρ + 1 + p - 1 2 σ 2 x 2 θ . ∎

Acknowledgements

The author would like to thank the University of Strathclyde for the scholarship and his first PhD supervisor, Professor Xuerong Mao.

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Received: 2022-06-19
Revised: 2023-03-26
Accepted: 2023-08-08
Published Online: 2023-08-25
Published in Print: 2023-09-01

© 2023 Walter de Gruyter GmbH, Berlin/Boston

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