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# Chapter 2 pertubation

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### Chapter 2 pertubation

1. 1. Perturbation Methods Jesús Fernández-Villaverde University of Pennsylvania July 10, 2011Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 1 / 91
2. 2. IntroductionIntroduction Remember that we want to solve a functional equation of the form: H (d ) = 0 for an unknown decision rule d. Perturbation solves the problem by specifying: n d n (x, θ ) = ∑ θ i (x x0 )i i =0 We use implicit-function theorems to …nd coe¢ cients θ i ’s. Inherently local approximation. However, often good global properties.Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 2 / 91
3. 3. IntroductionMotivation Many complicated mathematical problems have: 1 either a particular case 2 or a related problem. that is easy to solve. Often, we can use the solution of the simpler problem as a building block of the general solution. Very successful in physics. Sometimes perturbation is known as asymptotic methods.Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 3 / 91
4. 4. IntroductionThe World Simplest Perturbation p What is 26? Without your Iphone calculator, it is a boring arithmetic calculation. But note that: p q p 26 = 25 (1 + 0.04) = 5 1.04 5 1.02 = 5.1 Exact solution is 5.099. p We have solved a much simpler problem ( 25) and added a small coe¢ cient to it. More in general q p p y= x 2 (1 + ε ) = x 1 + ε where x is an integer and ε the perturbation parameter.Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 4 / 91
5. 5. IntroductionApplications to Economics Judd and Guu (1993) showed how to apply it to economic problems. Recently, perturbation methods have been gaining much popularity. In particular, second- and third-order approximations are easy to compute and notably improve accuracy. A …rst-order perturbation theory and linearization deliver the same output. Hence, we can use much of what we already know about linearization.Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 5 / 91
6. 6. IntroductionRegular versus Singular Perturbations Regular perturbation: a small change in the problem induces a small change in the solution. Singular perturbation: a small change in the problem induces a large change in the solution. Example: excess demand function. Most problems in economics involve regular perturbations. Sometimes, however, we can have singularities. Example: introducing a new asset in an incomplete markets model.Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 6 / 91
7. 7. IntroductionReferences General: 1 A First Look at Perturbation Theory by James G. Simmonds and James E. Mann Jr. 2 Advanced Mathematical Methods for Scientists and Engineers: Asymptotic Methods and Perturbation Theory by Carl M. Bender, Steven A. Orszag. Economics: 1 Perturbation Methods for General Dynamic Stochastic Models” by Hehui Jin and Kenneth Judd. 2 Perturbation Methods with Nonlinear Changes of Variables” by Kenneth Judd. 3 A gentle introduction: “Solving Dynamic General Equilibrium Models Using a Second-Order Approximation to the Policy Function” by Martín Uribe and Stephanie Schmitt-Grohe.Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 7 / 91
8. 8. A Baby ExampleA Baby Example: A Basic RBCModel: ∞ max E0 ∑ βt log ct t =0 s.t. ct + kt +1 = e zt ktα + (1 δ) kt , 8 t > 0 zt = ρzt 1 + σεt , εt N (0, 1)Equilibrium conditions: 1 1 = βEt 1 + αe zt +1 ktα+1 δ 1 ct ct + 1 ct + kt +1 = e zt ktα + (1 δ) kt zt = ρzt 1 + σεtJesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 8 / 91
9. 9. A Baby ExampleComputing a Solution The previous problem does not have a known “paper and pencil” solution except when (unrealistically) δ = 1. Then, income and substitution e¤ect from a technology shock cancel each other (labor constant and consumption is a …xed fraction of income). Equilibrium conditions with δ = 1: 1 1 αe zt +1 ktα+1 = βEt ct ct + 1 ct + kt +1 = e zt ktα zt = ρzt 1 + σεt By “guess and verify”: ct = ( 1 αβ) e zt ktα kt +1 = αβe zt ktαJesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 9 / 91
10. 10. A Baby ExampleAnother Way to Solve the Problem Now let us suppose that you missed the lecture when “guess and verify” was explained. You need to compute the RBC. What you are searching for? A decision rule for consumption: ct = c (kt , zt ) and another one for capital: kt +1 = k (kt , zt ) Note that our d is just the stack of c (kt , zt ) and k (kt , zt ).Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 10 / 91
11. 11. A Baby ExampleEquilibrium Conditions We substitute in the equilibrium conditions the budget constraint and the law of motion for technology. And we write the decision rules explicitly as function of the states. Then: 1 αe ρzt +σεt +1 k (kt , zt )α 1 = βEt c (kt , zt ) c (k (kt , zt ) , ρzt + σεt +1 ) c (kt , zt ) + k (kt , zt ) = e zt ktα System of functional equations.Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 11 / 91
12. 12. A Baby ExampleMain Idea Transform the problem rewriting it in terms of a small perturbation parameter. Solve the new problem for a particular choice of the perturbation parameter. This step is usually ambiguous since there are di¤erent ways to do so. Use the previous solution to approximate the solution of original the problem.Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 12 / 91
13. 13. A Baby ExampleA Perturbation Approach Hence, we want to transform the problem. Which perturbation parameter? Standard deviation σ. Why σ? Discrete versus continuous time. Set σ = 0 )deterministic model, zt = 0 and e zt = 1. We know how to solve the deterministic steady state.Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 13 / 91
14. 14. A Baby ExampleA Parametrized Decision Rule We search for decision rule: ct = c (kt , zt ; σ) and kt +1 = k (kt , zt ; σ) Note new parameter σ. We are building a local approximation around σ = 0.Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 14 / 91
15. 15. A Baby ExampleTaylor’ Theorem s Equilibrium conditions: ! 1 αe ρzt +σεt +1 k (kt , zt ; σ)α 1 Et β =0 c (kt , zt ; σ) c (k (kt , zt ; σ) , ρzt + σεt +1 ; σ) c (kt , zt ; σ) + k (kt , zt ; σ) e zt ktα = 0 We will take derivatives with respect to kt , zt , and σ. Apply Taylor’ theorem to build solution around deterministic steady s state. How?Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 15 / 91
16. 16. A Baby ExampleAsymptotic Expansion I ct = c (kt , zt ; σ)jk ,0,0 = c (k, 0; 0) +ck (k, 0; 0) (kt k ) + cz (k, 0; 0) zt + cσ (k, 0; 0) σ 1 1 + ckk (k, 0; 0) (kt k )2 + ckz (k, 0; 0) (kt k ) zt 2 2 1 1 + ck σ (k, 0; 0) (kt k ) σ + czk (k, 0; 0) zt (kt k ) 2 2 1 2 1 + czz (k, 0; 0) zt + cz σ (k, 0; 0) zt σ 2 2 1 1 + cσk (k, 0; 0) σ (kt k ) + cσz (k, 0; 0) σzt 2 2 1 2 + cσ2 (k, 0; 0) σ + ... 2Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 16 / 91
17. 17. A Baby ExampleAsymptotic Expansion II kt +1 = k (kt , zt ; σ)jk ,0,0 = k (k, 0; 0) +kk (k, 0; 0) (kt k ) + kz (k, 0; 0) zt + kσ (k, 0; 0) σ 1 1 + kkk (k, 0; 0) (kt k )2 + kkz (k, 0; 0) (kt k ) zt 2 2 1 1 + kk σ (k, 0; 0) (kt k ) σ + kzk (k, 0; 0) zt (kt k ) 2 2 1 2 1 + kzz (k, 0; 0) zt + kz σ (k, 0; 0) zt σ 2 2 1 1 + kσk (k, 0; 0) σ (kt k ) + kσz (k, 0; 0) σzt 2 2 1 2 + kσ2 (k, 0; 0) σ + ... 2Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 17 / 91
18. 18. A Baby ExampleComment on Notation From now on, to save on notation, I will write " # 1 αe ρzt +σεt +1 k (k ,zt ;σ)α 1 β c (k (kt ,zt ;σ),ρztt+σεt +1 ;σ) 0 F (kt , zt ; σ) = Et c (kt ,zt ;σ ) = c (kt , zt ; σ) + k (kt , zt ; σ) e zt ktα 0 Note that: F (kt , zt ; σ) = H (ct , ct +1 , kt , kt +1 , zt ; σ) = H (c (kt , zt ; σ) , c (k (kt , zt ; σ) , zt +1 ; σ) , kt , k (kt , zt ; σ) , zt ; σ) I will use Hi to represent the partial derivative of H with respect to the i component and drop the evaluation at the steady state of the functions when we do not need it.Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 18 / 91
19. 19. A Baby ExampleZeroth-Order Approximation First, we evaluate σ = 0: F (kt , 0; 0) = 0 Steady state: 1 αk α 1 =β c c or 1 1 = αβk α Then: α 1 c = c (k, 0; 0) = (αβ) 1 α (αβ) 1 α 1 k = k (k, 0; 0) = (αβ) 1 αJesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 19 / 91
20. 20. A Baby ExampleFirst-Order Approximation We take derivatives of F (kt , zt ; σ) around k, 0, and 0. With respect to kt : Fk (k, 0; 0) = 0 With respect to zt : Fz (k, 0; 0) = 0 With respect to σ: Fσ (k, 0; 0) = 0Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 20 / 91
21. 21. A Baby ExampleSolving the System I Remember that: F (kt , zt ; σ) = H (c (kt , zt ; σ) , c (k (kt , zt ; σ) , zt +1 ; σ) , kt , k (kt , zt ; σ) , zt ; σ) = 0 Because F (kt , zt ; σ) must be equal to zero for any possible values of kt , zt , and σ, the derivatives of any order of F must also be zero. Then: Fk (k, 0; 0) = H1 ck + H2 ck kk + H3 + H4 kk = 0 Fz (k, 0; 0) = H1 cz + H2 (ck kz + ck ρ) + H4 kz + H5 = 0 Fσ (k, 0; 0) = H1 cσ + H2 (ck kσ + cσ ) + H4 kσ + H6 = 0Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 21 / 91
22. 22. A Baby ExampleSolving the System II A quadratic system: Fk (k, 0; 0) = H1 ck + H2 ck kk + H3 + H4 kk = 0 Fz (k, 0; 0) = H1 cz + H2 (ck kz + ck ρ) + H4 kz + H5 = 0 of 4 equations on 4 unknowns: ck , cz , kk , and kz . Procedures to solve quadratic systems: 1 Blanchard and Kahn (1980). 2 Uhlig (1999). 3 Sims (2000). 4 Klein (2000). All of them equivalent. Why quadratic? Stable and unstable manifold.Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 22 / 91
23. 23. A Baby ExampleSolving the System III Also, note that: Fσ (k, 0; 0) = H1 cσ + H2 (ck kσ + cσ ) + H4 kσ + H6 = 0 is a linear, and homogeneous system in cσ and kσ . Hence: cσ = kσ = 0 This means the system is certainty equivalent. Interpretation)no precautionary behavior. Di¤erence between risk-aversion and precautionary behavior. Leland (1968), Kimball (1990). Risk-aversion depends on the second derivative (concave utility). Precautionary behavior depends on the third derivative (convex marginal utility).Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 23 / 91
24. 24. A Baby ExampleComparison with LQ and Linearization After Kydland and Prescott (1982) a popular method to solve economic models has been to …nd a LQ approximation of the objective function of the agents. Close relative: linearization of equilibrium conditions. When properly implemented linearization, LQ, and …rst-order perturbation are equivalent. Advantages of perturbation: 1 Theorems. 2 Higher-order terms.Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 24 / 91
25. 25. A Baby ExampleSome Further Comments Note how we have used a version of the implicit-function theorem. Important tool in economics. Also, we are using the Taylor theorem to approximate the policy function. Alternatives?Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 25 / 91
26. 26. A Baby ExampleSecond-Order Approximation We take second-order derivatives of F (kt , zt ; σ) around k, 0, and 0: Fkk (k, 0; 0) = 0 Fkz (k, 0; 0) = 0 Fk σ (k, 0; 0) = 0 Fzz (k, 0; 0) = 0 Fz σ (k, 0; 0) = 0 Fσσ (k, 0; 0) = 0 Remember Young’ theorem! s We substitute the coe¢ cients that we already know. A linear system of 12 equations on 12 unknowns. Why linear? Cross-terms kσ and zσ are zero. Conjecture on all the terms with odd powers of σ.Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 26 / 91
27. 27. A Baby ExampleCorrection for Risk We have a term in σ2 . Captures precautionary behavior. We do not have certainty equivalence any more! Important advantage of second-order approximation. Changes ergodic distribution of states.Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 27 / 91
28. 28. A Baby ExampleHigher-Order Terms We can continue the iteration for as long as we want. Great advantage of procedure: it is recursive! Often, a few iterations will be enough. The level of accuracy depends on the goal of the exercise: 1 Welfare analysis: Kim and Kim (2001). 2 Empirical strategies: Fernández-Villaverde, Rubio-Ramírez, and Santos (2006).Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 28 / 91
29. 29. A Numerical ExampleA Numerical Example Parameter β α ρ σ Value 0.99 0.33 0.95 0.01 Steady State: c = 0.388069 k = 0.1883 First-order terms: ck (k, 0; 0) = 0.680101 kk (k, 0; 0) = 0.33 cz (k, 0; 0) = 0.388069 kz (k, 0; 0) = 0.1883 Second-order terms: ckk (k, 0; 0) = 2.41990 kkk (k, 0; 0) = 1.1742 ckz (k, 0; 0) = 0.680099 kkz (k, 0; 0) = 0.33 czz (k, 0; 0) = 0.388064 kzz (k, 0; 0) = 0.1883 cσ2 (k, 0; 0) 0 kσ2 (k, 0; 0) 0 cσ (k, 0; 0) = kσ (k, 0; 0) = ck σ (k, 0; 0) = kk σ (k, 0; 0) = cz σ (k, 0; 0) = kz σ (k, 0; 0) = 0.Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 29 / 91
30. 30. A Numerical ExampleComparison ct = 0.6733e zt kt0.33 ct 0.388069 + 0.680101 (kt k ) + 0.388069zt 2.41990 0.388064 2 (kt k )2 + 0.680099 (kt k ) zt + zt 2 2and: kt +1 = 0.3267e zt kt0.33 kt +1 0.1883 + 0.33 (kt k ) + 0.1883zt 1.1742 0.1883 2 (kt k )2 + 0.33 (kt k ) zt + zt 2 2Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 30 / 91
31. 31. A Numerical ExampleJesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 31 / 91
32. 32. A Numerical ExampleA Computer In practice you do all this approximations with a computer: 1 First-, second-, and third-order: Matlab and Dynare. 2 Higher-order: Mathematica, Dynare++, Fortran code by Jinn and Judd. Burden: analytical derivatives. Why are numerical derivatives a bad idea? Alternatives: automatic di¤erentiation?Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 32 / 91
33. 33. A Numerical ExampleLocal Properties of the Solution Perturbation is a local method. It approximates the solution around the deterministic steady state of the problem. It is valid within a radius of convergence. What is the radius of convergence of a power series around x? An r 2 R∞ such that 8x 0 , jx 0 z j < r , the power series of x 0 will + converge.A Remarkable Result from Complex AnalysisThe radius of convergence is always equal to the distance from the centerto the nearest point where the policy function has a (non-removable)singularity. If no such point exists then the radius of convergence is in…nite. Singularity here refers to poles, fractional powers, and other branch powers or discontinuities of the functional or its derivatives.Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 33 / 91
34. 34. A Numerical ExampleRemarks Intuition of the theorem: holomorphic functions are analytic. Distance is in the complex plane. Often, we can check numerically that perturbations have good non local behavior. However: problem with boundaries.Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 34 / 91
35. 35. A Numerical ExampleNon Local Accuracy Test Proposed by Judd (1992) and Judd and Guu (1997). Given the Euler equation: 1 αe zt +1 k i (kt , zt )α 1 i (k , z ) = Et c t t c i (k i (kt , zt ), zt +1 ) we can de…ne: αe zt +1 k i (kt , zt )α 1 EE i (kt , zt ) 1 c i (kt , zt ) Et c i (k i (kt , zt ), zt +1 ) Units of reporting. Interpretation.Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 35 / 91
36. 36. A Numerical ExampleJesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 36 / 91
37. 37. The General CaseThe General Case Most of previous argument can be easily generalized. The set of equilibrium conditions of many DSGE models can be written as (note recursive notation) Et H(y , y 0 , x, x 0 ) = 0, where yt is a ny 1 vector of controls and xt is a nx 1 vector of states. De…ne n = nx + ny . Then H maps R ny R ny R nx R nx into R n .Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 37 / 91
38. 38. The General CasePartitioning the State Vector The state vector xt can be partitioned as x = [x1 ; x2 ]t . x1 is a (nx n ) 1 vector of endogenous state variables. x2 is a n 1 vector of exogenous state variables. Why do we want to partition the state vector?Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 38 / 91
39. 39. The General CaseExogenous Stochastic Process 0 x2 = Λx2 + ση 0 Process with 3 parts: 1 The deterministic component Λx2 : 1 Λ is a n n matrix, with all eigenvalues with modulus less than one. 2 More general: x2 = Γ(x2 ) + ση 0 , where Γ is a non-linear function 0 satisfying that all eigenvalues of its …rst derivative evaluated at the non-stochastic steady state lie within the unit circle. 2 The scaled innovation η 0 where: 1 η is a known n n matrix. 2 is a n 1 i.i.d innovation with bounded support, zero mean, and variance/covariance matrix I . 3 The perturbation parameter σ. We can accommodate very general structures of x2 through changes in the de…nition of the state space: i.e. stochastic volatility. Note we do not impose Gaussianity.Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 39 / 91
40. 40. The General CaseThe Perturbation Parameter The scalar σ 0 is the perturbation parameter. If we set σ = 0 we have a deterministic model. Important: there is only ONE perturbation parameter. The matrix η takes account of relative sizes of di¤erent shocks. Why bounded support? Samuelson (1970) and Jin and Judd (2002).Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 40 / 91
41. 41. The General CaseSolution of the Model The solution to the model is of the form: y = g (x; σ) 0 0 x = h(x; σ) + ση where g maps R nx R + into R ny and h maps R nx R + into R nx . The matrix η is of order nx n and is given by: ∅ η= ηJesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 41 / 91
42. 42. The General CasePerturbation We wish to …nd a perturbation approximation of the functions g and h around the non-stochastic steady state, xt = x and σ = 0. ¯ We de…ne the non-stochastic steady state as vectors (x, y ) such that: ¯ ¯ H(y , y , x, x ) = 0. ¯ ¯ ¯ ¯ Note that y = g (x; 0) and x = h(x; 0). This is because, if σ = 0, ¯ ¯ ¯ ¯ then Et H = H.Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 42 / 91
43. 43. The General CasePlugging-in the Proposed Solution Substituting the proposed solution, we de…ne: F (x; σ) Et H(g (x; σ), g (h(x; σ) + ησ 0 , σ), x, h(x; σ) + ησ 0 ) = 0 Since F (x; σ) = 0 for any values of x and σ, the derivatives of any order of F must also be equal to zero. Formally: Fx k σj (x; σ) = 0 8x, σ, j, k, where Fx k σj (x, σ) denotes the derivative of F with respect to x taken k times and with respect to σ taken j times.Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 43 / 91
44. 44. The General CaseFirst-Order Approximation We look for approximations to g and h around (x, σ) = (x, 0): ¯ g (x; σ) = g (x; 0) + gx (x; 0)(x ¯ ¯ x ) + gσ (x; 0)σ ¯ ¯ h(x; σ) = h(x; 0) + hx (x; 0)(x ¯ ¯ x ) + hσ (x; 0)σ ¯ ¯ As explained earlier, g (x; 0) = y ¯ ¯ and h(x; 0) = x. ¯ ¯ The four unknown coe¢ cients of the …rst-order approximation to g and h are found by using: Fx (x; 0) = 0 ¯ and Fσ (x; 0) = 0 ¯ Before doing so, I need to introduce the tensor notation.Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 44 / 91
45. 45. The General CaseTensors General trick from physics. An nth -rank tensor in a m-dimensional space is an operator that has n indices and mn components and obeys certain transformation rules. [Hy ]iα is the (i, α) element of the derivative of H with respect to y : 1 The derivative of H with respect to y is an n ny matrix. 2 Thus, [Hy ]iα is the element of this matrix located at the intersection of the i-th row and α-th column. n ∂ H i ∂g α ∂h β Thus, [Hy ]iα [gx ]α [hx ]j = ∑α=1 ∑nx 1 β y ∂y α ∂x β ∂x j . 3 β β= [Hy 0 y 0 ]iαγ : 1 Hy 0 y 0 is a three dimensional array with n rows, ny columns, and ny pages. 2 Then [Hy 0 y 0 ]iαγ denotes the element of Hy 0 y 0 located at the intersection of row i, column α and page γ.Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 45 / 91
46. 46. The General CaseSolving the System I gx and hx can be found as the solution to the system: [Fx (x; 0)]ij = [Hy 0 ]iα [gx ]α [hx ]j + [Hy ]iα [gx ]jα + [Hx 0 ]iβ [hx ]j + [Hx ]ij = β β ¯ β i = 1, . . . , n; j, β = 1, . . . , nx ; α = 1, . . . , ny Note that the derivatives of H evaluated at (y , y 0 , x, x 0 ) = (y , y , x, x ) ¯ ¯ ¯ ¯ are known. Then, we have a system of n nx quadratic equations in the n nx unknowns given by the elements of gx and hx . We can solve with a standard quadratic matrix equation solver.Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 46 / 91
47. 47. The General Case Solving the System II gσ and hσ are identi…ed as the solution to the following n equations: [Fσ (x; 0)]i = ¯ Et f[Hy 0 ]iα [gx ]α [hσ ] β + [Hy 0 ]iα [gx ]α [η ]φ [ 0 ]φ + [Hy 0 ]iα [gσ ]α β β β +[Hy ]iα [gσ ]α + [Hx 0 ]iβ [hσ ] β + [Hx 0 ]iβ [η ]φ [ 0 ]φ g β i = 1, . . . , n; α = 1, . . . , ny ; β = 1, . . . , nx ; φ = 1, . . . , n . Then:[Fσ (x; 0)]i = [Hy 0 ]iα [gx ]α [hσ ] β + [Hy 0 ]iα [gσ ]α + [Hy ]iα [gσ ]α + [fx 0 ]iβ [hσ ] β = 0; ¯ β i = 1, . . . , n; α = 1, . . . , ny ; β = 1, . . . , nx ; φ = 1, . . . , n . Certainty equivalence: this equation is linear and homogeneous in gσ and hσ . Thus, if a unique solution exists, it must satisfy: hσ 6 = 0 gσ = 0 Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 47 / 91
48. 48. The General CaseSecond-Order Approximation IThe second-order approximations to g around (x; σ) = (x; 0) is ¯ [g (x; σ)]i = [g (x; 0)]i + [gx (x; 0)]ia [(x x )]a + [gσ (x; 0)]i [σ] ¯ ¯ ¯ ¯ 1 + [gxx (x; 0)]iab [(x x )]a [(x x )]b ¯ ¯ ¯ 2 1 + [gx σ (x; 0)]ia [(x x )]a [σ] ¯ ¯ 2 1 + [gσx (x; 0)]ia [(x x )]a [σ] ¯ ¯ 2 1 + [gσσ (x; 0)]i [σ][σ] ¯ 2where i = 1, . . . , ny , a, b = 1, . . . , nx , and j = 1, . . . , nx .Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 48 / 91
49. 49. The General CaseSecond-Order Approximation IIThe second-order approximations to h around (x; σ) = (x; 0) is ¯ [h(x; σ)]j = [h(x; 0)]j + [hx (x; 0)]ja [(x x )]a + [hσ (x; 0)]j [σ] ¯ ¯ ¯ ¯ 1 + [hxx (x; 0)]jab [(x x )]a [(x x )]b ¯ ¯ ¯ 2 1 + [hx σ (x; 0)]ja [(x x )]a [σ] ¯ ¯ 2 1 + [hσx (x; 0)]ja [(x x )]a [σ] ¯ ¯ 2 1 + [hσσ (x; 0)]j [σ][σ], ¯ 2where i = 1, . . . , ny , a, b = 1, . . . , nx , and j = 1, . . . , nx .Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 49 / 91
50. 50. The General CaseSecond-Order Approximation III The unknowns of these expansions are [gxx ]iab , [gx σ ]ia , [gσx ]ia , [gσσ ]i , [hxx ]jab , [hx σ ]ja , [hσx ]ja , [hσσ ]j . These coe¢ cients can be identi…ed by taking the derivative of F (x; σ) with respect to x and σ twice and evaluating them at (x; σ) = (x; 0). ¯ By the arguments provided earlier, these derivatives must be zero.Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 50 / 91
51. 51. The General CaseSolving the System IWe use Fxx (x; 0) to identify gxx (x; 0) and hxx (x; 0): ¯ ¯ ¯ [Fxx (x; 0)]ijk = ¯ [Hy 0 y 0 ]iαγ [gx ]γ [hx ]k + [Hy 0 y ]iαγ [gx ]k + [Hy 0 x 0 ]iαδ [hx ]k + [Hy 0 x ]iαk [gx ]α [hx ]j δ γ δ β δ β +[Hy 0 ]iα [gxx ]α [hx ]k [hx ]j + [Hy 0 ]iα [gx ]α [hxx ]jk δ β β βδ β + [Hyy 0 ]iαγ [gx ]γ [hx ]k + [Hyy ]iαγ [gx ]k + [Hyx 0 ]iαδ [hx ]k + [Hyx ]iαk [gx ]jα δ δ γ δ +[Hy ]iα [gxx ]jk α+ [Hx 0 y 0 ]iβγ [gx ]γ [hx ]k + [Hx 0 y ]iβγ [gx ]k + [Hx 0 x 0 ]iβδ [hx ]k + [Hx 0 x ]iβk [hx ]j δ γ δ β δ +[Hx 0 ]iβ [hxx ]jk β +[Hxy 0 ]ij γ [gx ]γ [hx ]k + [Hxy ]ij γ [gx ]k + [Hxx 0 ]ij δ [hx ]k + [Hxx ]ijk = 0; δ δ γ δ i = 1, . . . n, j, k, β, δ = 1, . . . nx ; α, γ = 1, . . . ny .Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 51 / 91
52. 52. The General CaseSolving the System II We know the derivatives of H. We also know the …rst derivatives of g and h evaluated at (y , y 0 , x, x 0 ) = (y , y , x, x ). ¯ ¯ ¯ ¯ Hence, the above expression represents a system of n nx nx linear equations in then n nx nx unknowns elements of gxx and hxx .Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 52 / 91
53. 53. The General CaseSolving the System IIISimilarly, gσσ and hσσ can be obtained by solving:[Fσσ (x; 0)]i ¯ = [Hy 0 ]iα [gx ]α [hσσ ] β β +[Hy 0 y 0 ]iαγ [gx ]γ [η ]δ [gx ]α [η ]φ [I ]ξ β φ δ ξ β +[Hy 0 x 0 ]iαδ [η ]δ [gx ]α [η ]φ [I ]ξ β φ ξ β +[Hy 0 ]iα [gxx ]α [η ]δ [η ]φ [I ]ξ + [Hy 0 ]iα [gσσ ]α β φ βδ ξ +[Hy ]iα [gσσ ]α + [Hx 0 ]iβ [hσσ ] β +[Hx 0 y 0 ]iβγ [gx ]γ [η ]δ [η ]φ [I ]ξ β φ δ ξ +[Hx 0 x 0 ]iβδ [η ]δ [η ]φ [I ]ξ = 0; β φ ξ i = 1, . . . , n; α, γ = 1, . . . , ny ; β, δ = 1, . . . , nx ; φ, ξ = 1, . . . , na system of n linear equations in the n unknowns given by the elements ofgσσ and hσσ .Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 53 / 91
54. 54. The General CaseCross Derivatives The cross derivatives gx σ and hx σ are zero when evaluated at (x, 0). ¯ Why? Write the system Fσx (x; 0) = 0 taking into account that all ¯ terms containing either gσ or hσ are zero at (x, 0). ¯ Then: [Fσx (x; 0)]ij = [Hy 0 ]iα [gx ]α [hσx ]j + [Hy 0 ]iα [gσx ]α [hx ]jγ + β ¯ β γ [Hy ]iα [gσx ]jα + [Hx 0 ]iβ [hσx ]j = 0; β i = 1, . . . n; α = 1, . . . , ny ; β, γ, j = 1, . . . , nx . a system of n nx equations in the n nx unknowns given by the elements of gσx and hσx . The system is homogeneous in the unknowns. Thus, if a unique solution exists, it is given by: gσx = 0 hσx = 0Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 54 / 91
55. 55. The General CaseStructure of the Solution The perturbation solution of the model satis…es: gσ (x; 0) = 0 ¯ hσ (x; 0) = 0 ¯ gx σ (x; 0) = 0 ¯ hx σ (x; 0) = 0 ¯ Standard deviation only appears in: 1 A constant term given by 1 gσσ σ2 for the control vector yt . 2 2 The …rst nx 1 n elements of 2 hσσ σ2 . Correction for risk. Quadratic terms in endogenous state vector x1 . Those terms capture non-linear behavior.Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 55 / 91
56. 56. The General CaseHigher-Order Approximations We can iterate this procedure as many times as we want. We can obtain n-th order approximations. Problems: 1 Existence of higher order derivatives (Santos, 1992). 2 Numerical instabilities. 3 Computational costs.Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 56 / 91
57. 57. Change of VariablesErik EadyIt is not the process of linearization that limits insight.It is the nature of the state that we choose to linearize about.Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 57 / 91
58. 58. Change of VariablesChange of Variables We approximated our solution in levels. We could have done it in logs. Why stop there? Why not in powers of the state variables? Judd (2002) has provided methods for changes of variables. We apply and extend ideas to the stochastic neoclassical growth model.Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 58 / 91
59. 59. Change of VariablesA General Transformation We look at solutions of the form: µ ζ cµ c0 = a kζ k0 + bz k 0γ γ ζ k0 = c kζ k0 + dz Note that: 1 If γ, ζ, and µ are 1, we get the linear representation. 2 As γ, ζ and µ tend to zero, we get the loglinear approximation.Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 59 / 91
60. 60. Change of VariablesTheory The …rst-order solution can be written as f (x ) f (a ) + (x a ) f 0 (a ) Expand g (y ) = h (f (X (y ))) around b = Y (a), where X (y ) is the inverse of Y (x ). Then: g (y ) = h (f (X (y ))) = g (b ) + gα (b ) (Y α (x ) bα ) where gα = hA fi A Xα comes from the application of the chain rule. i From this expression it is easy to see that if we have computed the values of fi A , then it is straightforward to …nd gα .Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 60 / 91
61. 61. Change of VariablesCoe¢ cients Relation Remember that the linear solution is: k0 k0 = a1 ( k k0 ) + b1 z (l l0 ) = c1 (k k0 ) + d1 z Then we show that: γ ζ γ 1 a3 = γ k0 ζ a1 b3 = γk0 b1 µ µ 1 1 ζ µ 1 c3 = ζ l0 k0 c1 d3 = µl0 d1Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 61 / 91
62. 62. Change of VariablesFinding the Parameters Minimize over a grid the Euler Error. Some optimal results Euler Equation Errors γ ζ µ SEE 1 1 1 0.0856279 0.986534 0.991673 2.47856 0.0279944Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 62 / 91
63. 63. Change of VariablesSensitivity Analysis Di¤erent parameter values. Most interesting …nding is when we change σ: Optimal Parameters for di¤erent σ’s σ γ ζ µ 0.014 0.98140 0.98766 2.47753 0.028 1.04804 1.05265 1.73209 0.056 1.23753 1.22394 0.77869 A …rst-order approximation corrects for changes in variance!Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 63 / 91
64. 64. Change of VariablesJesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 64 / 91
65. 65. Change of VariablesA Quasi-Optimal Approximation Sensitivity analysis reveals that for di¤erent parametrizations γζ This suggests the quasi-optimal approximation: k 0γ γ γ k0 = a3 k γ k0 + b3 z µ γ lµ l0 = c3 k γ k0 + d3 z b If we de…ne k = k γ k0 and b = l µ γ l µ l0 we get: b b k 0 = a3 k + b3 z b = c3 k + d3 z l b Linear system: 1 Use for analytical study. 2 Use for estimation with a Kalman Filter.Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 65 / 91
66. 66. Perturbing the Value FunctionPerturbing the Value Function We worked with the equilibrium conditions of the model. Sometimes we may want to perform a perturbation on the value function formulation of the problem. Possible reasons: 1 Gain insight. 2 Di¢ culty in using equilibrium conditions. 3 Evaluate welfare. 4 Initial guess for VFI.Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 66 / 91
67. 67. Perturbing the Value FunctionBasic Problem Imagine that we have: " # 1 γ c V (kt , zt ) = max (1 β) t + βEt V (kt +1 , zt +1 ) ct 1 γ s.t. ct + kt +1 = e zt ktθ + (1 δ) kt zt = λzt 1 + σεt , εt N (0, 1) Write it as: " # 1 γ c V (kt , zt ; χ) = max (1 β) t + βEt V (kt +1 , zt +1 ; χ) ct 1 γ s.t. ct + kt +1 = e zt ktθ + (1 δ) kt zt = λzt 1 + χσεt , εt N (0, 1)Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 67 / 91
68. 68. Perturbing the Value FunctionAlternative Another way to write the value function is: V (kt , zt ; χ) = " 1 γ # max (1 β ) c t γ + 1 ct βEt V e zt ktθ + (1 δ) kt ct , λzt + χσεt +1 ; χ This form makes the dependences in the next period states explicit. The solution of this problem is value function V (kt , zt ; χ) and a policy function for consumption c (kt , zt ; χ).Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 68 / 91
69. 69. Perturbing the Value FunctionExpanding the Value FunctionThe second-order Taylor approximation of the value function around thedeterministic steady state (kss , 0; 0) is: V (kt , zt ; χ) Vss + V1,ss (kt kss ) + V2,ss zt + V3,ss χ 1 1 1 + V11,ss (kt kss )2 + V12,ss (kt kss ) zt + V13,ss (kt kss ) χ 2 2 2 1 1 1 + V21,ss zt (kt kss ) + V22,ss zt2 + V23,ss zt χ 2 2 2 1 1 1 + V31,ss χ (kt kss ) + V32,ss χzt + V33,ss χ2 2 2 2where Vss = V (kss , 0; 0) Vi ,ss = Vi (kss , 0; 0) for i = f1, 2, 3g Vij ,ss = Vij (kss , 0; 0) for i, j = f1, 2, 3gJesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 69 / 91
70. 70. Perturbing the Value FunctionExpanding the Value Function By certainty equivalence, we will show below that: V3,ss = V13,ss = V23,ss = 0 Taking advantage of the equality of cross-derivatives, and setting χ = 1, which is just a normalization: V (kt , zt ; 1) Vss + V1,ss (kt kss ) + V2,ss zt 1 1 + V11,ss (kt kss )2 + V22,ss ztt 2 2 2 1 +V12,ss (kt kss ) z + V33,ss 2 Note that V33,ss 6= 0, a di¤erence from the standard linear-quadratic approximation to the utility functions.Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 70 / 91
71. 71. Perturbing the Value FunctionExpanding the Consumption Function The policy function for consumption can be expanded as: ct = c (kt , zt ; χ) css + c1,ss (kt kss ) + c2,ss zt + c3,ss χ where: c1,ss = c1 (kss , 0; 0) c2,ss = c2 (kss , 0; 0) c3,ss = c3 (kss , 0; 0) Since the …rst derivatives of the consumption function only depend on the …rst and second derivatives of the value function, we must have c3,ss = 0 (precautionary consumption depends on the third derivative of the value function, Kimball, 1990).Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 71 / 91
72. 72. Perturbing the Value FunctionLinear Components of the Value Function To …nd the linear approximation to the value function, we take derivatives of the value function with respect to controls (ct ), states (kt , zt ), and the perturbation parameter χ. Notation: 1 Vi ,t : derivative of the value function with respect to its i-th argument, evaluated in (kt , zt ; χ) . 2 Vi ,ss : derivative evaluated in the steady state, (kss , 0; 0). 3 We follow the same notation for higher-order (cross-) derivatives.Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 72 / 91
73. 73. Perturbing the Value FunctionDerivatives Derivative with respect to ct : γ (1 β ) ct βEt V1,t +1 = 0 Derivative with respect to kt : V1,t = βEt V1,t +1 θe zt ktθ 1 +1 δ Derivative with respect to zt : h i V2,t = βEt V1,t +1 e zt ktθ + V2,t +1 λ Derivative with respect to χ: V3,t = βEt [V2,t +1 σεt +1 + V3,t +1 ] In the last three derivatives, we apply the envelope theorem to eliminate the derivatives of consumption with respect to kt , zt , and χ.Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 73 / 91
74. 74. Perturbing the Value FunctionSystem of Equations INow, we have the system: ct + kt +1 = e zt ktθ + (1 δ) kt 1 γ ct V (kt , zt ; χ) = (1 β) + βEt V (kt +1 , zt +1 ; χ) 1 γ γ (1 β ) ct βEt V1,t +1 = 0 V1,t = βEt V1,t +1 θe zt ktθ 1 + 1 δ h i V2,t = βEt V1,t +1 e zt ktθ + V2,t +1 λ V3,t = βEt [V2,t +1 σεt +1 + V3,t +1 ] zt = λzt 1 + χσεtJesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 74 / 91
75. 75. Perturbing the Value FunctionSystem of Equations IIIf we set χ = 0 and compute the steady state, we get a system of sixequations on six unknowns, css , kss , Vss , V1,ss , V2,ss , and V3,ss : θ css + δkss = kss 1 γ css Vss = (1 β) + βVss 1 γ (1 β) css γ βV1,ss = 0 V1,ss = βV1,ss θkss 1 + 1 δ θ h i θ V2,ss = β V1,ss kss + V2,ss λ V3,ss = βV3,ss From the last equation: V3,ss = 0. 1 γ From the second equation: Vss = css γ . 1 1 β γ From the third equation: V1,ss = β css .Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 75 / 91
76. 76. Perturbing the Value FunctionSystem of Equations III After cancelling redundant terms: θ css + δkss = kss 1 = β θkss 1 + 1 δ θ h i θ V2,ss = β V1,ss kss + V2,ss λ Then: 1 1 1 θ 1 kss = 1+δ θ β θ css = kss δkss 1 β θ γ V2,ss = k c 1 βλ ss ss V1,ss > 0 and V2,ss > 0, as predicted by theory.Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 76 / 91
77. 77. Perturbing the Value FunctionQuadratic Components of the Value FunctionFrom the previous derivations, we have: γ (1 β) c (kt , zt ; χ) βEt V1,t +1 = 0 V1,t = βEt V1,t +1 θe zt ktθ 1 + 1 δ h i V2,t = βEt V1,t +1 e zt ktθ + V2,t +1 λ V3,t = βEt [V2,t +1 σεt +1 + V3,t +1 ]where: kt +1 = e zt ktθ + (1 δ) kt c (kt , zt ; χ) zt = λzt 1 + χσεt , εt N (0, 1) We take derivatives of each of the four equations w.t.r. kt , zt , and χ. We take advantage of the equality of cross derivatives. The envelope theorem does not hold anymore (we are taking derivatives of the derivatives of the value function).Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 77 / 91
78. 78. Perturbing the Value FunctionFirst Equation IWe have: γ (1 β) c (kt , zt ; χ) βEt V1,t +1 = 0 Derivative with respect to kt : γ 1 (1 β) γc (kt , zt ; χ) c1,t h i βEt V11,t +1 e zt θktθ 1 +1 δ c1,t =0 In steady state: h i 1 1 βV11,ss (1 β) γcss γ θ c1,ss = β V11,ss θkss +1 δ or V11,ss c1,ss = γ 1 βV11,ss (1 β) γcss where we have used that 1 = β θkss θ 1 +1 δ .Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 78 / 91
79. 79. Perturbing the Value FunctionFirst Equation II Derivative with respect to zt : γ 1 (1 β) γc (kt , zt ; χ) c2,t βEt V11,t +1 e zt ktθ c2,t + V12,t +1 λ = 0 In steady state: 1 βV11,ss (1 β) γcss γ c2,ss = β V11,ss ktθ + V12,ss λ or β θ c2,ss = γ 1 V11,ss kss + V12,ss λ βV11,ss (1 β) γcssJesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 79 / 91
80. 80. Perturbing the Value FunctionFirst Equation III Derivative with respect to χ: γ 1 (1 β) γc (kt , zt ; χ) c3,t βEt ( V11,t +1 c3,t + V12,t +1 σεt +1 + V13,t +1 ) = 0 In steady state: 1 βV11,ss (1 β) γcss γ c3,ss = βV13,ss or β c3,ss = V13,ss γ 1 βV11,ss (1 β) γcssJesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 80 / 91
81. 81. Perturbing the Value FunctionSecond Equation IWe have: V1,t = βEt V1,t +1 θe zt ktθ 1 +1 δ Derivative with respect to kt : " # V11,t +1 θe zt ktθ 1 + 1 δ c1,t θe zt ktθ 1 +1 δ V11,t = βEt 2 +V1,t +1 θ (θ 1) e zt ktθ In steady state: 1 θ 2 V11,ss = V11,ss c1,ss + βV1,ss θ (θ 1) kss β or β θ 2 V11,ss = 1 V1,ss θ (θ 1) kss 1 β + c1,ssJesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 81 / 91
82. 82. Perturbing the Value FunctionSecond Equation II Derivative with respect to zt : 2 3 V11,t +1 e zt ktθ c2,t θe zt ktθ 1 + 1 δ V12,t = βEt 4 5 +V12,t +1 λ θe zt ktθ 1 + 1 δ + V1,t +1 θe zt ktθ 1 In steady state: θ 1 V12,ss = V11,ss kss c2,ss + V12,ss λ + βV1,ss θktθ or h i 1 θ θ 1 V12,ss = V11,ss kss c2,ss + βV1,ss θkss 1 λJesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 82 / 91
83. 83. Perturbing the Value FunctionSecond Equation III Derivative with respect to χ: V13,t = βEt [ V11,t +1 c3,t + V12,t +1 σεt +1 + V13,t +1 ] In steady state, V13,ss = β [ V11,ss c3,ss + V13,ss ] ) β V13,ss = V11,ss c3,ss β 1 but since we know that: β c3,ss = V13,ss γ 1 βV11,ss (1 β) γcss the two equations can only hold simultaneously if V13,ss = c3,ss = 0.Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 83 / 91
84. 84. Perturbing the Value FunctionThird Equation IWe have h i V2,t = βEt V1,t +1 e zt ktθ + V2,t +1 λ Derivative with respect to zt : V11,t +1 e zt ktθ c2,t e zt ktθ + V12,t +1 λe zt ktθ V22,t = βEt +V1,t +1 e zt ktθ + V21,t +1 λ e zt ktθ c2,t + V22,t +1 λ2 In steady state: V11,ss ktθ c2,ss kss + V12,ss λkss + V1,ss kss θ θ θ V22,t = β ) +V21,ss λ kss c2,ss + V22,ss λ2 θ β V11,ss ktθ c2,ss kss + 2V12,ss λkss θ θ V22,ss = 1 βλ2 +V1,ss kss V12,ss λc2,ss θ where we have used V12,ss = V21,ss .Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 84 / 91
85. 85. Perturbing the Value FunctionThird Equation II Derivative with respect to χ: V11,t +1 e zt ktθ c3,t + V12,t +1 e zt ktθ σεt +1 + V13,t +1 e zt ktθ V23,t = βEt V21,t +1 λc3,t + V22,t +1 λσεt +1 + V23,t +1 λ In steady state: V23,ss = 0Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 85 / 91
86. 86. Perturbing the Value FunctionFourth EquationWe have V3,t = βEt [V2,t +1 σεt +1 + V3,t +1 ] . Derivative with respect to χ: V21,t +1 c3,t σεt +1 + V22,t +1 σ2 ε2+1 + V23,t +1 σεt +1 t V33,t = βEt V31,t +1 c3,t + V32,t +1 σεt +1 + V33,t +1In steady state: β V33,ss = V22,ss 1 βJesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 86 / 91
87. 87. Perturbing the Value FunctionSystem I V11,ss c1,ss = γ 1 βV11,ss (1 β) γcss β θ c2,ss = γ 1 V11,ss kss + V12,ss λ βV11,ss (1 β) γcss β V11,ss = 1 1) kss 2 θ V1,ss θ (θ 1 β + c1,ss 1 h i V12,ss = V11,ss kss c2,ss + βV1,ss θkss 1 θ θ 1 λ β V11,ss ktθ c2,ss kss + 2V12,ss λkss θ θ V22,ss = 1 βλ2 +V1,ss kss V12,ss λc2,ss θ β V33,ss = σ2 V22,ss 1 βplus c3,ss = V13,ss = V23,ss = 0.Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 87 / 91
88. 88. Perturbing the Value FunctionSystem II This is a system of nonlinear equations. However, it has a recursive structure. By substituting variables that we already know, we can …nd V11,ss . Then, using this results and by plugging c2,ss , we have a system of two equations, on two unknowns, V12,ss and V22,ss . Once the system is solved, we can …nd c1,ss , c2,ss , and V33,ss directly.Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 88 / 91
89. 89. Perturbing the Value FunctionThe Welfare Cost of the Business Cycle An advantage of performing the perturbation on the value function is that we have evaluation of welfare readily available. Note that at the deterministic steady state, we have: 1 V (kss , 0; χ) Vss + V33,ss 2 Hence 1 V33,ss is a measure of the welfare cost of the business cycle. 2 This quantity is not necessarily negative: it may be positive. For example, in an RBC with leisure choice (Cho and Cooley, 2000).Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 89 / 91
90. 90. Perturbing the Value FunctionOur Example 1 γ css We know that Vss = 1 γ. We can compute the decrease in consumption τ that will make the household indi¤erent between consuming (1 τ ) css units per period with certainty or ct units with uncertainty. Thus: 1 γ css 1 (css (1 τ ))1 γ + V33,ss = ) 1 γ 2 1 γ 1 (1 τ )1 γ 1 1 css γ = (1 γ) V33,ss 2 or 1 1 γ1 1 γ τ=1 1+ 1 V γ 2 33,ss cssJesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 90 / 91
91. 91. Perturbing the Value FunctionA Numerical Example We pick standard parameter values by setting β = 0.99, γ = 2, δ = 0.0294, θ = 0.3, and λ = 0.95. We get: V (kt , zt ; 1) 0.54000 + 0.00295 (kt kss ) + 0.11684zt 2 0.00007 (kt kss ) 0.00985zt2 0.97508σ2 0.00225 (kt kss ) zt c (kt , zt ; χ) 1.85193 + 0.04220 (kt kss ) + 0.74318zt DYNARE produces the same policy function by linearizing the equilibrium conditions of the problem. The welfare cost of the business cycle (in consumption terms) is 8.8475e-005, lower than in Lucas (1987) because of the smoothing possibilities allowed by capital. Use as an initial guess for VFI.Jesús Fernández-Villaverde (PENN) Perturbation Methods July 10, 2011 91 / 91