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Coupled Diffusions and Systemic Risk Systemic Risk Illustrated Jean-Pierre Fouque University of California Santa Barbara Joint work with Li-Hsien Sun Meeting on Financial Risks RiskLab Madrid, May 24th, 2012 HANDBOOK ON SYSTEMIC RISK


  1. Coupled Diffusions and Systemic Risk “Systemic Risk Illustrated” Jean-Pierre Fouque University of California Santa Barbara Joint work with Li-Hsien Sun Meeting on Financial Risks RiskLab Madrid, May 24th, 2012

  2. HANDBOOK ON SYSTEMIC RISK Editors: J.-P. Fouque and J. Langsam Cambridge University Press (to appear in 2012) • 2008: Committee to establish a National Institute of Finance (data and research on systemic risk) • 2010: Dodd-Frank Bill includes the creation of the Office of Financial Research • 2012: Director nominated: Richard Berner will form a Financial Research Advisory Committee

  3. HANDBOOK ON SYSTEMIC RISK Editors: J.-P. Fouque and J. Langsam Cambridge University Press (to appear in 2012) • 2008: Committee to establish a National Institute of Finance (data and research on systemic risk) • 2010: Dodd-Frank Bill includes the creation of the Office of Financial Research • 2012: Director nominated: Richard Berner will form a Financial Research Advisory Committee

  4. HANDBOOK ON SYSTEMIC RISK Editors: J.-P. Fouque and J. Langsam Cambridge University Press (to appear in 2012) • 2008: Committee to establish a National Institute of Finance (data and research on systemic risk) • 2010: Dodd-Frank Bill includes the creation of the Office of Financial Research • 2012: Director nominated: Richard Berner will form a Financial Research Advisory Committee

  5. HANDBOOK ON SYSTEMIC RISK Editors: J.-P. Fouque and J. Langsam Cambridge University Press (to appear in 2012) • 2008: Committee to establish a National Institute of Finance (data and research on systemic risk) • 2010: Dodd-Frank Bill includes the creation of the Office of Financial Research • 2012: Director nominated: Richard Berner will form a Financial Research Advisory Committee

  6. Correlated Diffusions: Credit Risk Y ( i ) , i = 1 , . . . , N denote log-values t dY ( i ) = b ( i ) t dt + σ ( i ) t dW ( i ) i = 1 , . . . , N. t t Three ingredients: • Drifts b ( i ) t • Volatilities σ ( i ) t • Brownian motions W ( i ) t Credit Risk (structural approach): drifts imposed by risk neutrality Correlation is created between the BMs Joint distribution of hitting times is a problem! Correlation can also be created through stochastic volatilities σ ( i ) t (Fouque-Wignall-Zhou 2008)

  7. Correlated Diffusions: Credit Risk Y ( i ) , i = 1 , . . . , N denote log-values t dY ( i ) = b ( i ) t dt + σ ( i ) t dW ( i ) i = 1 , . . . , N. t t Three ingredients: • Drifts b ( i ) t • Volatilities σ ( i ) t • Brownian motions W ( i ) t Credit Risk (structural approach): drifts imposed by risk neutrality Correlation is created between the BMs Joint distribution of hitting times is a problem! Correlation can also be created through stochastic volatilities σ ( i ) t (Fouque-Wignall-Zhou 2008)

  8. Correlated Diffusions: Credit Risk Y ( i ) , i = 1 , . . . , N denote log-values t dY ( i ) = b ( i ) t dt + σ ( i ) t dW ( i ) i = 1 , . . . , N. t t Three ingredients: • Drifts b ( i ) t • Volatilities σ ( i ) t • Brownian motions W ( i ) t Credit Risk (structural approach): drifts imposed by risk neutrality Correlation is created between the BMs Joint distribution of hitting times is a problem! Correlation can also be created through stochastic volatilities σ ( i ) t (Fouque-Wignall-Zhou 2008)

  9. Correlated Diffusions: Credit Risk Y ( i ) , i = 1 , . . . , N denote log-values t dY ( i ) = b ( i ) t dt + σ ( i ) t dW ( i ) i = 1 , . . . , N. t t Three ingredients: • Drifts b ( i ) t • Volatilities σ ( i ) t • Brownian motions W ( i ) t Credit Risk (structural approach): drifts imposed by risk neutrality Correlation is created between the BMs Joint distribution of hitting times is a problem! Correlation can also be created through stochastic volatilities σ ( i ) t (Fouque-Wignall-Zhou 2008)

  10. Coupled Diffusions: Systemic Risk Y ( i ) , i = 1 , . . . , N denote log-monetary reserves of N banks t dY ( i ) = b ( i ) t dt + σ ( i ) t dW ( i ) i = 1 , . . . , N. t t Assume independent Brownian motions W ( i ) t , i = 1 , . . . , N and identical constant volatilities σ ( i ) = σ t Model borrowing and lending through the drifts: � N = α dY ( i ) ( Y ( j ) − Y ( i ) ) dt + σdW ( i ) , i = 1 , . . . , N. t t t t N j =1 The overall rate of borrowing and lending α/N has been normalized by the number of banks and we assume α > 0 Denote the default level by η < 0 and simulate the system for various values of α : 0 , 1 , 10 , 100 with fixed σ = 1

  11. Coupled Diffusions: Systemic Risk Y ( i ) , i = 1 , . . . , N denote log-monetary reserves of N banks t dY ( i ) = b ( i ) t dt + σ ( i ) t dW ( i ) i = 1 , . . . , N. t t Assume independent Brownian motions W ( i ) t , i = 1 , . . . , N and identical constant volatilities σ ( i ) = σ t Model borrowing and lending through the drifts: � N = α dY ( i ) ( Y ( j ) − Y ( i ) ) dt + σdW ( i ) , i = 1 , . . . , N. t t t t N j =1 The overall rate of borrowing and lending α/N has been normalized by the number of banks and we assume α > 0 Denote the default level by η < 0 and simulate the system for various values of α : 0 , 1 , 10 , 100 with fixed σ = 1

  12. Coupled Diffusions: Systemic Risk Y ( i ) , i = 1 , . . . , N denote log-monetary reserves of N banks t dY ( i ) = b ( i ) t dt + σ ( i ) t dW ( i ) i = 1 , . . . , N. t t Assume independent Brownian motions W ( i ) t , i = 1 , . . . , N and identical constant volatilities σ ( i ) = σ t Model borrowing and lending through the drifts: � N = α dY ( i ) ( Y ( j ) − Y ( i ) ) dt + σdW ( i ) , i = 1 , . . . , N. t t t t N j =1 The overall rate of borrowing and lending α/N has been normalized by the number of banks and we assume α > 0 Denote the default level by η < 0 and simulate the system for various values of α : 0 , 1 , 10 , 100 with fixed σ = 1

  13. Coupled Diffusions: Systemic Risk Y ( i ) , i = 1 , . . . , N denote log-monetary reserves of N banks t dY ( i ) = b ( i ) t dt + σ ( i ) t dW ( i ) i = 1 , . . . , N. t t Assume independent Brownian motions W ( i ) t , i = 1 , . . . , N and identical constant volatilities σ ( i ) = σ t Model borrowing and lending through the drifts: � N = α dY ( i ) ( Y ( j ) − Y ( i ) ) dt + σdW ( i ) , i = 1 , . . . , N. t t t t N j =1 The overall rate of borrowing and lending α/N has been normalized by the number of banks and we assume α > 0 Denote the default level by η < 0 and simulate the system for various values of α : 0 , 1 , 10 , 100 with fixed σ = 1

  14. One realization of the trajectories of the coupled diffusions Y ( i ) with t α = 1 (left plot) and trajectories of the independent Brownian motions ( α = 0) (right plot) using the same Gaussian increments. Solid horizontal line: default level η = − 0 . 7

  15. One realization of the trajectories of the coupled diffusions Y ( i ) with t α = 10 (left plot) and trajectories of the independent Brownian motions ( α = 0) (right plot) using the same Gaussian increments. Solid horizontal line: default level η = − 0 . 7

  16. One realization of the trajectories of the coupled diffusions Y ( i ) with t α = 100 (left plot) and trajectories of the independent Brownian motions ( α = 0) (right plot) using the same Gaussian increments. Solid horizontal line: default level η = − 0 . 7

  17. These simulations “show” that STABILITY is created by increasing the rate α of borrowing and lending. Next, we compare the loss distributions for the coupled and independent cases. We compute these loss distributions by Monte Carlo method using 10 4 simulations, and with the same parameters as previously. In the independent case, the loss distribution is Binomial( N, p ) with parameter p given by � � p = I P 0 ≤ t ≤ T ( σW t ) ≤ η min � � η √ = 2Φ , σ T where Φ denotes the N (0 , 1)-cdf, and we used the distribution of the minimum of a Brownian motion (see Karatzas-Shreve 2000 for instance). With our choice of parameters, we have p ≈ 0 . 5

  18. These simulations “show” that STABILITY is created by increasing the rate α of borrowing and lending. Next, we compare the loss distributions for the coupled and independent cases. We compute these loss distributions by Monte Carlo method using 10 4 simulations, and with the same parameters as previously. In the independent case, the loss distribution is Binomial( N, p ) with parameter p given by � � p = I P 0 ≤ t ≤ T ( σW t ) ≤ η min � � η √ = 2Φ , σ T where Φ denotes the N (0 , 1)-cdf, and we used the distribution of the minimum of a Brownian motion (see Karatzas-Shreve 2000 for instance). With our choice of parameters, we have p ≈ 0 . 5

  19. These simulations “show” that STABILITY is created by increasing the rate α of borrowing and lending. Next, we compare the loss distributions for the coupled and independent cases. We compute these loss distributions by Monte Carlo method using 10 4 simulations, and with the same parameters as previously. In the independent case, the loss distribution is Binomial( N, p ) with parameter p given by � � p = I P 0 ≤ t ≤ T ( σW t ) ≤ η min � � η √ = 2Φ , σ T where Φ denotes the N (0 , 1)-cdf, and we used the distribution of the minimum of a Brownian motion (see Karatzas-Shreve 2000 for instance). With our choice of parameters, we have p ≈ 0 . 5

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