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Lectures on Numerical Methods Lectures on Numerical Methods How to Solve/Use Life Cycle Models Tomoaki Yamada Meiji University September 5, 2011@IEAS

Lectures on Numerical Methods

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Page 1: Lectures on Numerical Methods

Lectures on Numerical Methods

Lectures on Numerical Methods� How to Solve/Use Life Cycle Models �

Tomoaki Yamada

Meiji University

September 5, 2011@IEAS

Page 2: Lectures on Numerical Methods

Lectures on Numerical Methods

Introduction

Introduction

I Basic framework (want to solve):I Life cycle versions of Bewley-Aiyagari-Huggett model

I Features of the model

1. Idiosyncratic risks)heterogeneity2. Aggregation,distribution dynamics

I Steady state, transition, and dynamics

Page 3: Lectures on Numerical Methods

Lectures on Numerical Methods

Introduction

Numerical Methods

Numerical Methods

I Global solution methodsI ,local approximation methods (e.g., linear quadraticapproximations)

I around the deterministic steady-stateI RBC, New Keynesian DSGE models etc.I called "Perturbation method"

I want to know policy functions

I Why global solution methods?

1. You may not know steady states before solving the problem2. Heterogeneous agents model: super rich and poor3. Income risks that individuals face is usually very large

I )Policy functions are potentially nonlinear

Page 4: Lectures on Numerical Methods

Lectures on Numerical Methods

Introduction

Numerical Methods

Numerical Methods (cont.)

I Need some numerical methods (o¤-the-shelf techniques)I Optimization: Judd (1998), Chap.4I Nonlinear equations: Judd (1998), Chap.5I Functional approximation: Judd (1998), Chap.6I Numerical integration/di¤erentiation: Judd (1998), Chap.7

I Useful booksI Judd (1998), Marimon and Scott (1999), Miranda and Fackler(2002), Heer and Maussner (2009)

Page 5: Lectures on Numerical Methods

Lectures on Numerical Methods

Introduction

Numerical Methods

Numerical Methods (cont.)

1. Value function iteration (VFI)I Finite iteration in life cycle models

2. Endogenous gridpoint methodI use the Euler equation

I Both methods are almost identical when solving life cyclemodels

I All codes used here are available fromI http://homepage2.nifty.com/~tyamada/teaching/numerical.htmlI written in Fortran 90/95

Page 6: Lectures on Numerical Methods

Lectures on Numerical Methods

Introduction

Software Choice

Software Choice

I Matlab/Gauss/Scilab/OctaveI Languages for scienti�c computing; matrix-orientedI Some useful tools: DYNARE, CompEcon (Miranda andFackler,2002)

I C/C++/Fortran:I Packages (Not free): IMSL/NAGI Numerical recipes (Book): Press et al. (2007)I Subroutine libraries (Free): LAPACK/BLAS/MINPACK etc.

I Mathmatica/Maple:I Symbolic math

Page 7: Lectures on Numerical Methods

Lectures on Numerical Methods

Introduction

Design of this Slide

Guide Map

1. Two-period model

2. Three-period model

3. (Full) Life cycle models:

3.1 Steady State3.2 Transition: Yamada (2011,JEDC)3.3 Aggregate shock

Page 8: Lectures on Numerical Methods

Lectures on Numerical Methods

Two-period Model

Basic Framework

Two-period Model

Consider a two-period model (no uncertainty)

I Basic setup:

maxcY ,cO ,a0

c1�γY

1� γ+ β

c1�γO

1� γ,

s.t.

cY + a0 = y + a,

cO = ss + Ra0

I (cY , cO ): consumption, β: discount factorI a0: savings, a: initial asset (given), R: gross interest rateI y : labor income (deterministic), ss: social security bene�t

Page 9: Lectures on Numerical Methods

Lectures on Numerical Methods

Two-period Model

Basic Framework

Calibration

I How to solve the two-period model?I Backward induction

I Before solving the model quantitatively, we need parametersI Usually this process is called "calibration"I One period is 30 years: Song et al. (2009)I β = 0.98530, γ = 2, R = 1.02530, y = 1, ss = 0.4

I What we want to know are policy functionsI cY = f Y (a): consumption function of young agentsI cO = f O (a0): consumption function of old agentsI a0 = g(a): saving function

Page 10: Lectures on Numerical Methods

Lectures on Numerical Methods

Two-period Model

Numerical Methods

Numerical Methods

1. In the last period (old), agents consume all wealthI cO = f O (a0) = ss + Ra0I Note that R and ss are given

2. Given the consumption function of old household f O (a0), wecompute young�s policy function from the Euler equation:

u0(cY ) = βRu0(cO ),

u0(y + a� a0) = βRu0(f O (a0))

= βRu0(ss + Ra0)

Page 11: Lectures on Numerical Methods

Lectures on Numerical Methods

Two-period Model

Numerical Methods

Consumption Function (Old):

0 1 2 3 4 50

2

4

6

8

10

12

Current Asset

Con

sum

ptio

n

Page 12: Lectures on Numerical Methods

Lectures on Numerical Methods

Two-period Model

Numerical Methods

Numerical Methods (cont.)

I How to �nd the policy functions f Y (a) and g(a) for younghouseholds from the Euler equation?

I There are some approaches

1. Discrete state space method

I Solve the Euler equation over discretized asset grids

2. Projection method: Judd (1992)

I Approximate policy functions by polynomialI Finite element method: McGrattan (1996,JEDC)

3. Endogenous gridpoint method (EGM): Carroll (2006)4. Parametric expectations algorithm (PEA): Christiano andFisher (2000)

Page 13: Lectures on Numerical Methods

Lectures on Numerical Methods

Two-period Model

Numerical Methods

Discrete State Space Method

I Discretize the initial asset (grid): ai 2 famin, . . . , amaxgI Tips: more grids near zero (if a borrowing constraint exists)

I Solve the Euler equation for each ai

u0(y + ai � a0) = βRu0(f O (a0)),

I How to solve the Euler equation?

u0(y + ai| {z }given

� a0|{z}choice

) = βR|{z}params.

u0(f O (a0)| {z }known

)

Page 14: Lectures on Numerical Methods

Lectures on Numerical Methods

Two-period Model

Numerical Methods

Discrete State Space Method (cont.)

I Use nonlinear equation solverI Find a zero of the residual:

Φ(ai ) = βRu0(f O (a0))

u0(y + ai � a0)� 1

I Useful techniques to �nd a zero:I Bisection method: bisect a zero between amin and amaxI Newton methodsI Broyden�s method: a variant of Newton methods

I You can �nd several root-�nding subroutines!I fzero: Matlab

Page 15: Lectures on Numerical Methods

Lectures on Numerical Methods

Two-period Model

Numerical Methods

Discrete State Space Method (cont.)

I You have a combination of current asset and savingsI fai , a0ig ) fcigI Use interpolation if you want to know consumption betweenthe discretized grids, ai < a < ai+1

Page 16: Lectures on Numerical Methods

Lectures on Numerical Methods

Two-period Model

Numerical Methods

Projection Method

I In the discrete state space method, we compute a set ofdiscretized asset and consumption

I Approximating the saving function over state spaceI E.g., monomial approximation

a0 = g(a; φ) =N

∑n=1

φnan�1

I Generally Chebyshev polynomial has some useful properties

a0 = g(a; φ) =N

∑n=1

φnTn(a)

I Tn(a): Basis function, e.g., cos((n� 1) arccos a)

Page 17: Lectures on Numerical Methods

Lectures on Numerical Methods

Two-period Model

Numerical Methods

Projection Method (cont.)

I Find coe¢ cients fφngNn=1 that minimizes the residual overstate Z

Φ(a; φ)da = 0

I How to compute the residual over state space?I E.g., Collocation method

I Given evaluation points famg,

Φ(am ; φ) = 0, m = 1, . . . ,M

I m < n: impossible to determine coe¢ cients fφngNn=0!I Other way to evaluate the residual, see text books

Page 18: Lectures on Numerical Methods

Lectures on Numerical Methods

Two-period Model

Numerical Methods

Endogenous Gridpoint Method

I Usually root-�ndings (using nonlinear equation solver) needcomputation time

I many iteration to �nd a zero

I Carroll (2006,EL): Endogenous Gridpoint MethodI Change the timing of discretization and state space

1. Discretize next period�s asset: a0j 2 fa01, . . . , a0Jg2. Solve consumption function over cash-on-hand

Page 19: Lectures on Numerical Methods

Lectures on Numerical Methods

Two-period Model

Numerical Methods

Endogenous Gridpoint Method (cont.)

I De�ne RHS of the Euler equation as

Γ(a0j ) � βRu0(ss + Ra0j )

I Because the marginal utility of CRRA utility function isinvertible,

u0(cY ,j ) = Γ(a0j ),

c�γY ,j = Γ(a0j ),

cY ,j = Γ(a0j )� 1

γ

Page 20: Lectures on Numerical Methods

Lectures on Numerical Methods

Two-period Model

Numerical Methods

Endogenous Gridpoint Method (cont.)

I We have a pair of fcY ,j , a0jgI cY ,j + a0j � xj (= y + a) is cash-on-handI We know consumption function over cash-on-hand

cY = fY (x)

Page 21: Lectures on Numerical Methods

Lectures on Numerical Methods

Two-period Model

Numerical Methods

Endogenous Gridpoint Method (cont.)

But, what we really want to know is consumption overcurrent asset

I Retrieve current asset from the cash-on-hand

xj = y + aj ,

aj = xj � y

I Policy function is a pair of fcj , ajg: cj = f Y (aj ), forj = 1, . . . , J

Page 22: Lectures on Numerical Methods

Lectures on Numerical Methods

Two-period Model

Numerical Methods

Numerical Examples

1. Consumption function when oldI mentioned above

2. Consumption function when young

3. Saving function

4. Numerical errorsI Closed-form solution

a0 =y + a� [βR ]�

1γ ss

1+ [βR ]�1γR

Page 23: Lectures on Numerical Methods

Lectures on Numerical Methods

Two-period Model

Numerical Methods

Consumption Function (Young)

0 1 2 3 4 50.5

1

1.5

2

2.5

3

3.5

4

Current Asset

Con

sum

ptio

n

Page 24: Lectures on Numerical Methods

Lectures on Numerical Methods

Two-period Model

Numerical Methods

Saving Function

0 1 2 3 4 50

0.5

1

1.5

2

2.5

Current Asset

Nex

t Ass

et

EGMAnalytical

Page 25: Lectures on Numerical Methods

Lectures on Numerical Methods

Two-period Model

Numerical Methods

Retrieve Current Asset

0 5 10 150

1

2

3

4

5

Current Asset

Nex

t Ass

et

Page 26: Lectures on Numerical Methods

Lectures on Numerical Methods

Two-period Model

Numerical Methods

Endogenous Gridpoint Method (cont.)

I This idea is applicable to any �nite (and in fact in�nite)horizon problems

I Need FOCs

I Let�s apply the EGM to three period model!

Page 27: Lectures on Numerical Methods

Lectures on Numerical Methods

Three-period Model

Basic Framework

Three-period modelExtend the model to three-period with uncertainty

I Consider a three-period model:

maxE

"c1�γY

1� γ+ β

c1�γM

1� γ+ β2

c1�γO

1� γ

#,

s.t.

cY + aM = yY + aY ,

cM + aO = yM + RaM ,

cO = ss + RaO

I (cY , cM , cO ): consumption, (aY , aM , aO ): asset holdingsI (yY , yM ): labor incomeI R: gross interest rate, ss: social security bene�t

Page 28: Lectures on Numerical Methods

Lectures on Numerical Methods

Three-period Model

Basic Framework

Three-period model (cont.)

Labor income is uncertain at middle

I E.g., labor income distribution

yM = yM + ε,

ε � N(0, σ2ε )

I Need numerical integration techniquesI Discretize εI Gauss-Legendre, Gauss-Chebyshev quadrature etc.

I Consider a very simple case: fyhighM , y lowM g with prob. 12

Page 29: Lectures on Numerical Methods

Lectures on Numerical Methods

Three-period Model

Numerical Methods

Three-period model (cont.)

I How to solve the model?I Backward induction again

I Why the three-period model is NOT a trivial extension oftwo-period model?

I Need an additional state variable: yMI Need functional approximation

Page 30: Lectures on Numerical Methods

Lectures on Numerical Methods

Three-period Model

Numerical Methods

Three-period model (cont.)

1. Old: cO = f O (aO ) = ss + RaO2. Middle: solve the Euler equation for each (aM ,i , yM )

u0(yM + RaM ,i � aO ) = βRu0(f O (aO ))

I Get a policy function f M (aM , yM ) using the EGM (or othermethods): fchighM ,i , a

highM ,i g and fc lowM ,i , alowM ,ig

I This step is completely the same as in the two-period model

3. Young: solve the Euler equation again

u0(yY + RaY ,i � aM ) = βREu0(f M (aM , yM ))

Page 31: Lectures on Numerical Methods

Lectures on Numerical Methods

Three-period Model

Numerical Methods

Three-period model (cont.)

I Policy function at middle f M (aM , yM ) is a set of discretizedpoints

I fchighM ,i , ahighY ,i g, fc lowM ,i , alowY ,ig

I What if the choice variable aM is between asset grids?

aM ,i < aM < aM ,i+1

I InterpolationI Linear approximation: non-di¤erentiable, interp1I Cubic spline interpolation: di¤erentiable, splineI Shape-preserving spline interpolation: di¤erentiable withconcavity

Page 32: Lectures on Numerical Methods

Lectures on Numerical Methods

Three-period Model

Numerical Methods

Three-period model (cont.)

I CalibrationI One period is 20 yearsI β = 0.98520, γ = 2, R = 1.02520I yY = 1I yhighM = 1+ ε, y lowM = 1� ε, ε = 0.2I ss = 0.4

Page 33: Lectures on Numerical Methods

Lectures on Numerical Methods

Three-period Model

Numerical Methods

Consumption Function (Old)

0 1 2 3 4 50

1

2

3

4

5

6

7

8

9

Current Asset

Con

sum

ptio

n

Page 34: Lectures on Numerical Methods

Lectures on Numerical Methods

Three-period Model

Numerical Methods

Consumption Function (Middle)

0 1 2 3 4 50.5

1

1.5

2

2.5

3

3.5

4

Current Asset

Con

sum

ptio

n

HighLow

Page 35: Lectures on Numerical Methods

Lectures on Numerical Methods

Three-period Model

Numerical Methods

Consumption Function (Young)

0 1 2 3 4 50.5

1

1.5

2

2.5

3

3.5

Current Asset

Con

sum

ptio

n

Page 36: Lectures on Numerical Methods

Lectures on Numerical Methods

Three-period Model

Numerical Methods

Saving Function (Middle)

0 1 2 3 4 50

0.5

1

1.5

2

2.5

Current Asset

Nex

t Ass

et

HighLow

Page 37: Lectures on Numerical Methods

Lectures on Numerical Methods

Three-period Model

Numerical Methods

Saving Function (Young)

0 1 2 3 4 50

0.5

1

1.5

2

2.5

3

Current Asset

Nex

t Ass

et

Page 38: Lectures on Numerical Methods

Lectures on Numerical Methods

Life Cycle Models

Life Cycle Models

I Generalize the simple two (three)-period modelsI Bewley/Huggett/Aiyagari frameworkI Agents live long periods

I Features of the model:I Life cycle �worker and retireeI Idiosyncratic labor income risksI Mortality risks (for demographic change)I Dynamic general equilibrium

1. Steady state2. Transition3. Aggregate shocks

Page 39: Lectures on Numerical Methods

Lectures on Numerical Methods

Life Cycle Models

Household Problem

Household Problem

I A continuum of households existsI There is no aggregate uncertaintyI Preferences are represented by

maxE1

J

∑j=1

ξ jβj�1 c

1�γj

1� γ

I j 2 f1, . . . , j ret, . . . , Jg: age

I ξj �j�1∏i=1

φi : unconditional probability of surviving to age j

Page 40: Lectures on Numerical Methods

Lectures on Numerical Methods

Life Cycle Models

Household Problem

Budget Constraint

I Budget constraints for worker and retiree:

cj + aj+1 � (1+ r) (aj + b) + (1� τss )wηjz ,

cj + aj+1 � (1+ r) (aj + b) + ss,

aj+1 � 0.

I r : interest rate, w : wage, b: accidental bequest (de�ned later)I ηj : age-speci�c productivity, z : idiosyncratic labor income riskI τss : payroll tax for social security

Page 41: Lectures on Numerical Methods

Lectures on Numerical Methods

Life Cycle Models

Household Problem

Household Problem (cont.)

I Idiosyncratic labor income risksI Storesletten et al. (2004,JME) etc.

I Logarithms of hours worked follows

ln zj+1 = ρ ln zj + κj , κ � N(0, σ2κ)

I ρ: persistence, κj : disturbance

Page 42: Lectures on Numerical Methods

Lectures on Numerical Methods

Life Cycle Models

Household Problem

Household Problem (cont.)

Bellman equation for workers: j = 1, . . . , j ret

Vj (a, z) = maxnu(cj ) + φjβEVj+1(a0, z 0)

o,

s.t.

cj + aj+1 � (1+ r) (aj + b) + wηjz ,

aj+1 � 0.

Page 43: Lectures on Numerical Methods

Lectures on Numerical Methods

Life Cycle Models

Household Problem

Household Problem (cont.)

Bellman equation for retirees: j = j ret + 1, . . . , J

Vj (a) = maxnu(cj ) + φjβVj+1(a

0)o,

s.t.

cj + aj+1 � (1+ r) (aj + b) + ss,

aj+1 � 0.

Page 44: Lectures on Numerical Methods

Lectures on Numerical Methods

Life Cycle Models

Household Problem

First Order Conditions

I Euler equation:

u0 (cj ) � φjβ (1+ r)Eu0 (cj+1)

I Why inequality?I A liquidity constraint exists: at+1 � 0

I What we want to know: policy function gj (a, z)

Page 45: Lectures on Numerical Methods

Lectures on Numerical Methods

Life Cycle Models

Aggregating the Economy

Transition Law of Motion

I Probability space: ((A�Z),B(A�Z),Φj )

I B(A�Z): Borel σ-�eldI Φj (a, z): probability measure

I Transition function from current state (a, z) to next stateX 2 B(A�Z)

Qj ((A�Z),X ) = ∑z 02Z

�Pr (z , z 0) if gj (a, z) 2 X0 else

I The distribution function by age:

Φj+1 (X ) =ZQj ((A�Z),X ) dΦj , (8X 2 B(A�Z))

Page 46: Lectures on Numerical Methods

Lectures on Numerical Methods

Life Cycle Models

Aggregating the Economy

Demography

I Some households die with probability φjI Transition of the fraction of cohort

µt+1 =1

1+ gφjµj

I µj : a fraction of age j , g : population growth rateI ∑Jj=0 µj = 1: total population is normalized to one

Page 47: Lectures on Numerical Methods

Lectures on Numerical Methods

Life Cycle Models

Aggregating the Economy

Production

I Aggregate capital:

K =J

∑j=1

µj

ZadΦj (a, z)

I Aggregate labor (exogenously �xed):

L =j ret

∑j=1

µj

ZηjzdΦj (a, z)

I A representative �rm: Cobb-Douglas production function

Y = AK θL1�θ

Page 48: Lectures on Numerical Methods

Lectures on Numerical Methods

Life Cycle Models

Aggregating the Economy

GovernmentI Social security system

j ret

∑j=1

µj

ZτsswηjzjdΦj (a, z) =

J

∑j=j ret+1

µj ss

=J

∑j=j ret+1

µj ϕwL

I ssdef= ϕwL

I Accidental bequest

b =J

∑j=1

µj

Z(1� φj )gj (a, z)dΦj (a, z)

Page 49: Lectures on Numerical Methods

Lectures on Numerical Methods

Life Cycle Models

Aggregating the Economy

De�nition of RCE

Recursive competitive equilibrium is a set of value function V ,policy function g , interest rate r , wage w , tax rate τss , and adistribution function Φ that satis�es the following conditions:

1. Household�s optimality

2. Firm�s optimality

r = θAK θ�1L1�θ, w = (1� θ)AK θL�θ

3. Market clearing conditionsI goods, capital and labor markets

4. Government budget constraint

5. Stationarity of distribution

Page 50: Lectures on Numerical Methods

Lectures on Numerical Methods

Life Cycle Models

Aggregating the Economy

Steady State

Computing a Steady State: Algorithm

1. Preamble: compute aggregate labor supply L, the tax rate forsocial security τss , and approximate idiosyncratic shocks

2. Initial guess: r03. Solve a household�s problem and get policy functions: gj (a, z)

4. Compute a cumulative density function: Φj (a, z)

5. Using the cumulative density function, compute aggregatecapital K1 and new interest rate r1

6. Check whether new interest rate r1 is su¢ ciently close to r06.1 Yes: It�s a steady state!6.2 No: repeat steps 3�6 with a new interest rate

Page 51: Lectures on Numerical Methods

Lectures on Numerical Methods

Life Cycle Models

Numerical Methods

How to Solve Life Cycle Models

1. Solving household�s problem

1.1 Value function iteration (VFI)1.2 Projection method1.3 Endogenous gridpoint method (EGM)

I This step is also applicable for structural estimation: SeeGourinchas and Parker (2002), Kaplan (2010)

2. Computing density function

2.1 Simulation2.2 Approximate density function

3. Find an equilibrium price (interest rate)I Bisection method etc.

Page 52: Lectures on Numerical Methods

Lectures on Numerical Methods

Life Cycle Models

Solving Household�s Problem

Dynamic Programming Approach

I Good points of VFII Safe (contraction mapping property): not important in lifecycle models

I Useful for nonlinear problemsI Many application

I Bad points of VFII Generally slow (but the number of iteration is �xed in life cyclemodels)

Page 53: Lectures on Numerical Methods

Lectures on Numerical Methods

Life Cycle Models

Solving Household�s Problem

Endogenous Gridpoint Method

I Good points of EGMI ReliableI Fast (need no optimization)

I Bad points of EGMI Without FOCs, it may not be applicable (e.g., nonlinearproblems)

Page 54: Lectures on Numerical Methods

Lectures on Numerical Methods

Life Cycle Models

Solving Household�s Problem

VFI

I Basic idea is the same as in in�nite horizon modelsI Points

I Find a maximum: OptimizationI Approximation: Value function is concave

I Discretized gridai 2 famin, . . . , amaxg

Page 55: Lectures on Numerical Methods

Lectures on Numerical Methods

Life Cycle Models

Solving Household�s Problem

VFI (cont.)

General idea: use backward induction again!

I Age J:VJ (ai ) = u ((1+ r)(ai + b) + ss)

I Age J � 1:

VJ�1 (ai ) = maxa0fu�(1+ r)(ai + b) + ss � a0

�+ φjβVJ

�a0�g

I Iterate to age 1:

VJ (a)) VJ�1 (a)) � � � � � � ) Vj ret (a, z)) � � � � � � ) V1 (a, z)

Page 56: Lectures on Numerical Methods

Lectures on Numerical Methods

Life Cycle Models

Solving Household�s Problem

VFI (cont.)

I Household�s problem

Vj (ai , z) = maxa0fu((1+ r)(ai + b) + wηjz � a0)

+φjβEVj+1�a0, z 0

�g

I Optimization tools: fminsearch in MatlabI Golden search(�Bisection method)I Quasi-Newton method

I Functional approximation:I Vj+1 (a0, z 0) is generally strictly concave function

Page 57: Lectures on Numerical Methods

Lectures on Numerical Methods

Life Cycle Models

Solving Household�s Problem

Endogenous Gridpoint Method (cont.)

I First order condition is de�ned as follows:

u0(cj ) � φjβ(1+ r)Eu0(cj+1)

I Discretized grid: a0 2 famin, . . . , amaxg, amin = 0I For example, #grid= 100

Page 58: Lectures on Numerical Methods

Lectures on Numerical Methods

Life Cycle Models

Solving Household�s Problem

Endogenous Gridpoint Method (cont.)

I Cash-on-hand of age j + 1:

x 0 ��(1+ r)(a0j+1 + b) + wηj+1z(1+ r)(a0j+1 + b) + ss

I Right hand side of the Euler equation

Γ0(a0, z , j) � (1+ r)φjβEc�γj+1

= (1+ r)φjβEfj+1(x 0, z 0)�γ

I cj = fj (x , z): consumption function over cash-on-hand

Page 59: Lectures on Numerical Methods

Lectures on Numerical Methods

Life Cycle Models

Solving Household�s Problem

Endogenous Gridpoint Method (cont.)

I FOC is rede�ned as

u0(cj ) � Γ0(a0, z , j)

I Thus, we have consumption as

cj = u0�1Γ0(a0, z , j)

I If the Euler equation holds with strict inequality, a0 = 0, i.e.,hand-to-mouth consumer

Page 60: Lectures on Numerical Methods

Lectures on Numerical Methods

Life Cycle Models

How to Approximate AR(1) Process

Tauchen�s Methods

I How to calibrate idiosyncratic income risks?I Empirical studies: Blundell et al. (2008,AER), Storesletten etal. (2004,JPE) etc.

I How to approximate it?I Tauchen (1986)/Tauchen and Hussey (1992)I Floden (2007): approximation error of Tauchen�s methods

Page 61: Lectures on Numerical Methods

Lectures on Numerical Methods

Life Cycle Models

How to Approximate AR(1) Process

Tauchen�s Methods (cont.)

I Consider AR(1) ProcessI yt � log zt

yt+1 = ρyt + κt , κ � N (0, σ2κ)

yt+1 = ρyt + σy (1� λ2)12 κ, κ � N (0, 1)

Page 62: Lectures on Numerical Methods

Lectures on Numerical Methods

Life Cycle Models

How to Approximate AR(1) Process

Tauchen�s Methods (cont.)

I Approximate AR(1) process by �nite Markov chainI For example, 7-states

I Suppose yN = 3σy , y1 = �3σy : State spaceY log = f�3σy ,�2σy ,�σy , 0, σy , 2σy , 3σy g

I De�ne intervals of the seven-states as follows:

I1 = [3σy ,52

σy ), I2 = [�52

σy ,�32

σy ),

I3 = [�32

σy ,�12

σy ), I4 = [�12

σy ,12

σy ),

I5 = [12

σy ,32

σy ), I6 = [32

σy ,52

σy ),

I7 = [52

σy , 3σy )

Page 63: Lectures on Numerical Methods

Lectures on Numerical Methods

Life Cycle Models

How to Approximate AR(1) Process

Tauchen�s Methods (cont.)I Current state: y i = log z 2 Y log)Next state: y j = log z 0 2 Y log

πij = Pr�log z 0 = y j j log z = y i

�=ZIj

1p2πσε

e�12(x�log z )2

σε dx

I Range between states is de�ned as w = y k � y k�1I For each i , if j 2 [2,N � 1], then

πij = Prhy j � w

2� y j � y j + w

2

i= Pr

hy j � w

2� λy i + εt � y j +

w2

i= F

y j � λy i + w

2

σε

!� F

y j � λy i � w

2

σε

!

Page 64: Lectures on Numerical Methods

Lectures on Numerical Methods

Life Cycle Models

How to Approximate AR(1) Process

Tauchen�s Methods (cont.)

I As a last step, take exponent to the log AR(1) process:flog ztg ) fztg

I Normalize Ez = ∑z2Z zπ∞ (z) = 1 (not necessary)

Z = fz1, . . . , z7g

=

�e�3σy

Ez,e�2σy

Ez,e�σy

Ez,1Ez,eσy

Ez,e2σy

Ez,e3σε

Ez

Page 65: Lectures on Numerical Methods

Lectures on Numerical Methods

Life Cycle Models

Computing Density Function

Density Functions

I How to compute the density function?

1. Simulation

I Easy to implement, but errors may be large (if #sample isinsu¢ cient)

I Easy to compute some statistics: variances, Gini etc.

2. Approximate density function

I Heer and Maussner (2009)/Young (2010,JEDC)

Page 66: Lectures on Numerical Methods

Lectures on Numerical Methods

Life Cycle Models

Computing Density Function

Density Functions (cont.)Simulation-based method

1. Generate a series of idiosyncratic income shocks for Shouseholds, e.g. S = 10, 000

I fz ij g10,000i=1 : index i represents household

2. Guess initial asset distribution ai1: a1 = 0 by assumption3. Using policy functions (we already get), compute a series ofasset holdings

ai2 = g1(ai1, z

i1)! ai3 = g1(a

i2, z

i2)! � � �

I Notice that some households may die before J

4. Aggregation

K =J

∑j=1

µj

10,000

∑i=1

aij/S

Page 67: Lectures on Numerical Methods

Lectures on Numerical Methods

Life Cycle Models

Computing Density Function

Density Functions (cont.)I Approximate the density function dΦj (a, z) by linearinterpolation

I Solve the density function forwardlyI Take discretized grid: ak 2 famin, . . . , amaxg

I should be �ner than policy function iteration: e.g., 10,000grids

I A household with (a, z) saves a0 = gj (ak , z)I However, a0 may not be on the discretized gridI De�ne a weight ω as follows

ω =a0 � a`ah � a`

, a0 2 [a`, ah ]

I Households with (ak , z) are divided a` and ah by the rule�Pr(z , z 0)(1�ω)dΦj (a, z)Pr(z , z 0)ωdΦj (a, z)

Page 68: Lectures on Numerical Methods

Lectures on Numerical Methods

Life Cycle Models

Computing Density Function

Approximated Density Function

0 5 10 15 20 250

0.5

1

1.5

2

2.5

3

3.5

4 x 10 ­3

Current Asset

Φj(a

,z)

30405060

Page 69: Lectures on Numerical Methods

Lectures on Numerical Methods

Life Cycle Models

Finding a Steady State

Find a Steady State

I Need to �nd a �xed point of interest rateI same as in the Bewley model with in�nitely-lived agentsI Use a bisection method: Aiyagari (1994)

I Set an initial interest rate r0I update to r1I if iteration error is su¢ ciently small, e.g. ε = 0.00001, stop

krk+1 � rkk < ε, or, K supply �Kdemand < ε

I Aggregate demand and supply curve in the model

Page 70: Lectures on Numerical Methods

Lectures on Numerical Methods

Life Cycle Models

Finding a Steady State

Capital Demand and Supply

3.5 4 4.5 5 5.53.6

3.8

4

4.2

4.4

4.6

4.8

5

5.2

Interest Rate (%)

Cap

ital

DemandSupply

Page 71: Lectures on Numerical Methods

Lectures on Numerical Methods

Life Cycle Models

Calibration and Results

CalibrationHow to Calibrate Life Cycle Models

I Many empirical research: choose a targetI j ret = 46, J = 81I β = 0.97: Target is K/Y � 3I γ = 2: microeconomic evidencesI Idiosyncratic income risks

I Blundell et al. (2008,AER) etc.I ρ = 0.98, σκ = 0.01

I Macroeconomic variables: Japanese economy

I θ = 0.377, δ = 0.08

I Age-e¢ ciency pro�le: fηjgI Hansen�s (1993) method

I Population distribution: fµjg

Page 72: Lectures on Numerical Methods

Lectures on Numerical Methods

Life Cycle Models

Calibration and Results

Numerical Results

I Numerical ResultsI Consumption and asset pro�les: fcj , ajgJj=0

I Economic inequality: Storesletten et al. (2004,JME)I How much consumption insurance?

I Computation time (Fortran): 180 secI #grid for policy function= 100I #grid for density function= 10, 000I #grid for AR1 process= 15

Page 73: Lectures on Numerical Methods

Lectures on Numerical Methods

Life Cycle Models

Calibration and Results

Consumption Pro�le

20 30 40 50 60 70 80

0.7

0.8

0.9

1

1.1

1.2

1.3

1.4

Age

Con

sum

ptio

n

Page 74: Lectures on Numerical Methods

Lectures on Numerical Methods

Life Cycle Models

Calibration and Results

Earnings Pro�le

20 30 40 50 60

0.8

1

1.2

1.4

1.6

1.8

2

Age

Ear

ning

s

Page 75: Lectures on Numerical Methods

Lectures on Numerical Methods

Life Cycle Models

Calibration and Results

Asset Pro�le

20 40 60 80 1000

2

4

6

8

10

12

Age

Ass

et

Page 76: Lectures on Numerical Methods

Lectures on Numerical Methods

Life Cycle Models

Calibration and Results

Inequality over Life Cycle

20 30 40 50 600

0.05

0.1

0.15

0.2

0.25

0.3

0.35

Age

Var

. of L

ogCons.EarningsCons. (Data)Earnings (Data)

Page 77: Lectures on Numerical Methods

Lectures on Numerical Methods

Life Cycle Models

Calibration and Results

Applications

I Endogenous labor supply:I Add intra-temporal FOC to the original problem

wηj zj =u0h(c , 1� h)u0c (c , 1� h)

I Can we use the endogenous gridpoint method again?I Yes: Barillas and Fernandez-Villaverde (2007), Krueger andLudwig (2006)

Page 78: Lectures on Numerical Methods

Lectures on Numerical Methods

Life Cycle Models

Calibration and Results

Applications (cont.)

I Economic inequality:I Huggett (1996,JME), Storesletten et al. (2004,JME),Heathcote et al. (2010,JPE)

I Include transitory shocks, education background, marriage etc.

I Social security reforms:I Imrohoroglu et al. (1995,1997)I Need additional state variable for social security accounts

I Optimal taxation:I Conesa, Kitao and Krueger (2008)

τ(y) = τ2

hy � (y�τ1 + τ0)

� 1τ1

i

Page 79: Lectures on Numerical Methods

Lectures on Numerical Methods

Life Cycle Models

Calibration and Results

And More...

I Two natural extension of life cycle models

1. Transition pathI Social security reforms, tax reforms, aging etc.

2. Aggregate shockI Business cycle, asset pricing etc.

Page 80: Lectures on Numerical Methods

Lectures on Numerical Methods

Life Cycle Models

Computing Transition Paths

Transition

I Literature:I Conesa and Krueger (1999)I Nishiyama and Smetters (2007,2009)

I Why transition?I Welfare implications may di¤er between steady statecomparison and considering transition path explicitly

I Why di¢ cult?I Need to solve many generations problems

Page 81: Lectures on Numerical Methods

Lectures on Numerical Methods

Life Cycle Models

Computing Transition Paths

Transition (cont.)

I Basic ideas:I application of computing a steady state with very longbackward induction

I T (terminal period)! T � 1, � � � ,! 1 (initial period)I Need computation time: several hours

I Transition path between two steady stateI Without �nal steady state, it is impossible to compute thetransition path (where to go?)

I Initial steady state is not MUST (e.g., Auerbach and Kotliko¤,1992)

I But, you need to have an initial wealth distribution for eachage, Φj (a, z): di¢ cult to calculate

Page 82: Lectures on Numerical Methods

Lectures on Numerical Methods

Life Cycle Models

Computing Transition Paths

An Example

Yamada (2011,JEDC)

I Research question: How well does the life cycle model work?I Results: Macroeconomic variables and inequalities in Japan is,at least partially, explained by the standard life cycle modelwith macroeconomic and demographic changes

I Include deterministic TFP growth rate and demographicchange in the model:

Yt = AtK θt L1�θt

µj+1,t+1 = φj ,tµj ,t

Page 83: Lectures on Numerical Methods

Lectures on Numerical Methods

Life Cycle Models

Computing Transition Paths

Model (cont.)

Original Problem

I Bellman equation:

Vj ,t (a, s) = maxc ,a0,h

nu(cj ,t+j , hj ,t+j ) + φj ,tβEVj+1,t+1(a0, s 0)

o

u(cj ,t+j , hj ,t+j ) =[cσj ,t+j (ht � hj ,t+j )1�σ]1�γ

1� γ

I t: calender year, j : ageI hj ,t+j : labor supply (endogenous), ht : time endowment

Page 84: Lectures on Numerical Methods

Lectures on Numerical Methods

Life Cycle Models

Computing Transition Paths

Model (cont.)

I Budget constraint:

cj ,t + aj+1,t+1 = (1+ (1� τcapt )rt )(aj ,t + bt ) + yj ,t

yj ,t =�(1� τsst � τlabt )wtηjejhj ,tϕtwtLt

I fτlabt , τcapt , τsst g: taxes for labor, capital and social securitysystem

I Idiosyncratic labor productivity shock s � (α, z , ε):

ln et = α+ zj + εj ,

ln zj+1 = ρ ln zj + κj

Page 85: Lectures on Numerical Methods

Lectures on Numerical Methods

Life Cycle Models

Computing Transition Paths

Model (cont.)

I Aggregate economy:

Kt = ∑100j=20 µj ,t

Zaj ,tdΦj ,t (a, s)

Lt = ∑65j=20 µj ,t

Zηjejhj ,t+jdΦj ,t (a, s)

Page 86: Lectures on Numerical Methods

Lectures on Numerical Methods

Life Cycle Models

Computing Transition Paths

Model (cont.)

I Social security system:

∑65j=20 µj ,t

Zτsst wtηjejhj ,t+jdΦj ,t (a, s)

= ∑100j=66 µj ,tϕtwtLt .

I Government budget constraint:

Gt = ∑100j=20 µj ,t

Zτcapt rtaj ,tdΦj ,t (a, s)

+∑65j=20 µj ,t

Zτlabt wtηjejhj ,t+jdΦj ,t (a, s)

Page 87: Lectures on Numerical Methods

Lectures on Numerical Methods

Life Cycle Models

Computing Transition Paths

Model (cont.)

Detrended Problem

I Detrend the problem:

vj ,t (a, s) = maxc ,a0,h

nu(cj ,t+j , hj ,t+j ) + φj ,t βtEvj+1,t+1(a

0, s 0)o

u(cj ,t+j , hj ,t+j ) =[cσj ,t+j (ht � hj ,t+j )1�σ]1�γ

1� γ

I cj ,t = cj ,t/A1/(1�θ)t , aj ,t = aj ,t/A

1/(1�θ)t , hj ,t = hj ,t

I βt = β(1+ gt )σ(1�γ), 1+ gt = A1/(1�θ)t+1 /A1/(1�θ)

t

Page 88: Lectures on Numerical Methods

Lectures on Numerical Methods

Life Cycle Models

Computing Transition Paths

Model (cont.)

I Budget constraints of the detrended problem

cj ,t + (1+ gt )aj+1,t+1 = (1+ (1� τcapt )rt )(aj ,t + bt ) + yj ,t

yj ,t =�(1� τsst � τlabt )wtηjej hj ,tϕwt Lt

Page 89: Lectures on Numerical Methods

Lectures on Numerical Methods

Life Cycle Models

Computing Transition Paths

Algorithm

1. Compute initial and �nal steady states: 1980 and 2200

2. Set an exogenous path of fgt , φt , htg2200t=1980, and guess anequilibrium sequence of fr0t , w0t g2200t=1980.

3. Given the policy function of the �nal steady state, compute asequence of policy functions using the EGM by backwardinduction

4. Given the policy functions, compute the distribution functionfrom 1980 forwardly and compute aggregate variables,fr1t , w1t g2200t=1980

5. Check whether new factor prices fr1t , w1t g. are su¢ cientlyclose to the old ones fr0t , w0t g for every year. If these are notclose, update the price sequences and repeat steps 3� 4

6. If the factor prices are close in all periods, then stop!

Page 90: Lectures on Numerical Methods

Lectures on Numerical Methods

Life Cycle Models

Computing Transition Paths

Algorithm (cont.)

I In step 3, use the EGM againI FOCs:

u0c (cj ,t , h� hj ,t )

� φj ,t βt(1+ (1� τcapt+1)rt+1)

(1+ gt )Eu0c (cj+1,t+1, h� hj+1,t+1)

hj ,t = max

"ht �

�1� σ

σ

�cj ,t

(1� τsst )wtηjej, 0

#

Page 91: Lectures on Numerical Methods

Lectures on Numerical Methods

Life Cycle Models

Computing Transition Paths

Algorithm (cont.)

I De�ne RHS of the Euler equation:

Γ0j ,t (aj , sj ) =(1+ (1� τcapt+1)rt+1)

(1+ gt )

φj ,t βtEj

([cσj+1,t+1(ht+1 � hj+1,t+1)1�σ]1�γ

cj+1,t+1

)I First order condition:

u0c (cj ,t , ht � hj ,t ) = Γ0j ,t (a0, s)

I Cobb-Douglas utility function is invertible

Page 92: Lectures on Numerical Methods

Lectures on Numerical Methods

Life Cycle Models

Computing Transition Paths

Example: Transition Path

1980 1985 1990 1995 20002

3

4

5

6

7

Year

Inte

rest

 Rat

e (%

)(a) After­Tax Interest Rate

ModelHayashi & Prescott

Page 93: Lectures on Numerical Methods

Lectures on Numerical Methods

Life Cycle Models

Computing Transition Paths

Example: Transition Path

1980 1985 1990 1995 20001.4

1.6

1.8

2

2.2

2.4

Year

K/Y

(b) Capital­Output Ratio

ModelHayashi & Prescott

Page 94: Lectures on Numerical Methods

Lectures on Numerical Methods

Life Cycle Models

Computing Transition Paths

Example: Transition Path

1980 1985 1990 1995 20000

5

10

15

Year

Sav

ing 

Rat

e (%

)(d) Saving Rate

ModelHayashi & Prescott

Page 95: Lectures on Numerical Methods

Lectures on Numerical Methods

Life Cycle Models

Computing Transition Paths

Example: Transition Path

1980 1985 1990 1995 2000­0.2

­0.1

0

0.1

0.2

Year

Dev

iatio

n fro

m M

ean

(a) Earning Inequal ity (Variance of Log)

20­6020­65Kohara & Ohtake

Page 96: Lectures on Numerical Methods

Lectures on Numerical Methods

Life Cycle Models

Computing Transition Paths

Example: Transition Path

1980 1985 1990 1995 2000

­0.1

­0.05

0

0.05

0.1

0.15

Year

Dev

iatio

n fro

m M

ean

(b) Income Inequality (Variance of Log)

20­6020­65Kohara & Ohtake

Page 97: Lectures on Numerical Methods

Lectures on Numerical Methods

Life Cycle Models

Computing Transition Paths

Example: Transition Path

1980 1985 1990 1995 2000

­0.1

­0.05

0

0.05

0.1

0.15

Year

Dev

iatio

n fro

m M

ean

(c) Consumption Inequality (Variance of Log)

20­6020­65Kohara & Ohtake

Page 98: Lectures on Numerical Methods

Lectures on Numerical Methods

Life Cycle Models

Computing Transition Paths

Example: Transition Path

1980 1985 1990 1995 20000.4

0.45

0.5

0.55

0.6

0.65

Year

Var

. of L

og(a) Earning Inequal ity (Variance of Log)

BenchmarkMis­predict

Page 99: Lectures on Numerical Methods

Lectures on Numerical Methods

Life Cycle Models

Computing Transition Paths

Example: Transition Path

1980 1985 1990 1995 20000.13

0.14

0.15

0.16

0.17

Year

Var

. of L

og(b) Consumption Inequality (Variance of Log)

BenchmarkMis­predict

Page 100: Lectures on Numerical Methods

Lectures on Numerical Methods

Life Cycle Models

Aggregate Shock

Aggregate Shock

I Add aggregate shock (e.g., TFP shock) in the modelI Storesletten et al. (2007,RED), Krusell et al. (2011)

I Why di¢ cult?I Distribution a¤ects factor prices:

u0�cj ,t�� φj β (1+ r(Kt+1))Eu0

�cj+1,t+1

�I Distribution function in the state space

Vj (a, z ;Φ) = maxnu(cj ) + ξj βEVj+1(a

0, z 0;Φ)o

I Distribution function is in�nite-dimensional objects)impossible to solve

Page 101: Lectures on Numerical Methods

Lectures on Numerical Methods

Life Cycle Models

Aggregate Shock

Aggregate Shock

I Approximate aggregationI Krusell and Smith (1998), den Haan (1997)I Use not exact distribution function, but moments

I E.g., approximate prediction function:

logKt+1 = β0(A) + β1(A) logKt

I Approximated Bellman equation:

Vj (a, z ;K ,A) = max�u(cj ) + ξ jβEVj+1(a0, z 0;K ,A)

Page 102: Lectures on Numerical Methods

Lectures on Numerical Methods

Advanced Topics

Solving Multi-dimensional Problems

Another Approach to Solve OLG Models

I Add another state variables)Curse of dimensionalityI E.g., physical asset and �nancial asset: 50� 50 = 2, 500

I Smolyak algorithm: sparse grid approximationsI Stochastic overlapping generations models

I Krueger and Kubler (2003,2005)I Malin, Krueger and Kubler (2010)I Glover, Heathcote, Krueger and Ríos-Rull (2011)

I Points:I No idiosyncratic risksI Explicit portfolio choices

Page 103: Lectures on Numerical Methods

Lectures on Numerical Methods

Advanced Topics

Computers

Advanced Topics

I Recent CPU have double/quad coresI Core2Duo, Core i7, Xeon etc.

I Use many cores simultaneouslyI MPI: need many PCsI Open MP: easy to implement

I Use Graphic ProcessorsI Very fast, but need additional programming skills and tools

Page 104: Lectures on Numerical Methods

Lectures on Numerical Methods

Very Incomplete List of References

Reference List: General

I Judd, K. (1998): Numerical Methods in Economics, The MITPress.

I Marimon, R. and A. Scott (1999): Computational Methodsfor the Study of Dynamic Economies, Oxford University Press.

I Miranda, M.J. and P.L. Fackler (2002): AppliedComputational Economics and Finance, The MIT Press.

I Heer, B. and A. Maussner (2009): Dynamic GeneralEquilibrium Modeling, 2nd Edition, Springer-Verlag.

I Press, W.H., S.A. Teukolsky, W.T. Vetterling, and B.P.Flannery (2007): Numerical Recipes: The Art of Scienti�cComputing, Third Edition, Cambridge University Press.

Page 105: Lectures on Numerical Methods

Lectures on Numerical Methods

Very Incomplete List of References

Reference List: Projection Methods & VFI

I Judd, K. (1992): �Projection Methods for Solving AggregateGrowth Models," Journal of Economic Theory, 58, 410�452.

I McGrattan, E.R. (1996): �Solving the Stochastic GrowthModel with a Finite Element Method," Journal of EconomicDynamics and Control, 20, 19�42.

I Christiano, L.J., and J.D.M. Fisher (2000): �Algorithms forSolving Dynamic Models with Occasionally BindingConstraints," Journal of Economic Dynamics and Control,1179�1232.

I S.B. Aruoba, J. Fernández-Villaverde, and J.F. Rubio-Ramírez(2006): �Comparing Solution Methods for DynamicEquilibrium Economies," Journal of Economic Dynamics andControl, 30, 2477�2508.

Page 106: Lectures on Numerical Methods

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Very Incomplete List of References

Reference List: EGM

I Carroll, C.D. (2006): �The Method of Endogenous Gridpointsfor Solving Dynamic Stochastic Optimization Problems,"Economics Letters, 91, 312�320.

I Barillas, F., and J. Fernandez-Villaverde (2007): �AGeneralization of the Endogenous Grid Method," Journal ofEconomic Dynamics and Control, 31, 2698�2712.

I Krueger, D. and A. Ludwig (2006): �On the Consequences ofDemographic Change for Rates of Returns to Capital, and theDistribution of Wealth and Welfare," Journal of MonetaryEconomics, 54, 49�87.

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Very Incomplete List of References

Reference List: Life Cycle Models

I Huggett, M. (1996): �Wealth Distribution in Life-CycleEconomies," Journal of Monetary Economics, 38, 469�494.

I Storesletten, K., C. Telmer, and A. Yaron (2004):�Consumption and Risk Sharing over the Life Cycle," Journalof Monetary Economics, 51, 609�633.

I Conesa, J.C., S. Kitao, and D. Krueger (2008): �TaxingCapital? Not a Bad Idea After All!," American EconomicReview, 99, 25�48.

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Very Incomplete List of References

Reference List: Transition

I Conesa, J.C. and D. Krueger (1998): �Social Security withHeterogeneous Agents," Review of Economic Dynamics, 2,757-795.

I Nishiyama, S. and K. Smetters (2005): �Consumption Taxesand Economic E¢ ciency with Idiosyncratic Wage Shocks,"Journal of Political Economy, 113, 1088�1115.

I Nishiyama, S. and K. Smetters (2007): �Does Social SecurityPrivatization Produce E¢ ciency Gains?" Quarterly Journal ofEconomics, 122, 1677�1719.

Page 109: Lectures on Numerical Methods

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Very Incomplete List of References

Reference List: Aggregate Shock

I Krusel, P. and A.A. Smith Jr. (1998): �Incoe and WealthHeterogeneity in the Macroeconomy," Journal of PoliticalEconomy, 106(5), 867�896.

I Storesletten, K., C. Telmer, and A. Yaron (2007): �AssetPricing with Idiosyncratic Risk and Overlapping Generations,"Review of Economic Dynamics, 10(4), 519-548.

I den Haan (2010): �Assessing the Accuracy of the AggregateLaw of Motion in Models with Heterogeneous Agents,"Journal of Economic Dynamics and Control, 34, 79�99.

I Krusell, P., T. Mukoyama, and A. Sahin (2011): �Asset Pricesin a Huggett Economy," Journal of Economic Theory, 146,812�844.

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Very Incomplete List of References

Reference List: AR(1)

I Tauchen, G. (1986): �Finite State Markov-ChainApproximations to Univariate and Vector Autoregresions,"Economics Letters, 20, 177�181.

I Tauchen, G. and R. Hussey (1991): �Quadrature-BasedMethods for Obtaining Approximate Solutions to NonlinearAsset Pricing Models," Econometrica, 59, 371�396.

I Floden, M. (2008): �A Note on the Accuracy ofMarkov-Chain Approximations to Highly PersistentAR(1)-Processes," Economics Letters, 99, 516�520.

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Very Incomplete List of References

Reference List: Stochastic OLG

I Krueger, D. and F. Kubler (2003): �Computing Equilibrium inOLG Models with Stochastic Production," Journal ofEconomic Dynamics and Control, 28(7), 1411�1436.

I Malin, B., D. Krueger, and F. Kubler (2010): �ComputingStochastic Dynamic Economic Models with a Large Numberof State Variables: A Description and Application of aSmolyak-Collocation Method," forthcoming, Journal ofEconomic Dynamics and Control.

I Glover, A., J. Heathcote, D. Krueger, and J.V. Ríos-Rull(2011): �Intergenerational Redistribution in the GreatRecesion," mimeo, University of Pennsylvania.

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Very Incomplete List of References

Reference List: Accuracy

I den Haan, W. and A. Marcet (1994): �Accuracy inSimulations," Review of Economic Studies, 61, 3�17.

I Santos, M. (2000): �Accuracy of Numerical Solutions usingthe Euler Equation Residuals," Econometrica, 68(6),1377�1402.

I Santos, M. and A. Peralta-Alva (2005): �Accuracy ofSimulations for Stochastic Dynamic Models," Econometrica,73(6), 1939�1976.

I Peralta-Alva, A. and M.S. Santos (2010): �Problems in theNumerical Simulation of Models with Heterogeneous Agentsand Economic Distortions," Journal of the EuropeanEconomic Association, 8(2-3), 617�625.

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Very Incomplete List of References

Reference List: Computers

I Aldrich, E.M., J. Fernández-Villaverde, A.R. Gallant, and J.F.Rubio-Ramírez (2010): �Tapping the Supercomputer UnderYour Desk: Solving Dynamic Equilibrium Models withGraphics Processors," mimeo, University of Pennsylvania.

I Morosov, S. and S. Mathur (2010): �Massive ParallelComputation using Graphics Processors with Application toOptimal Experimentation in Dynamic Control," mimeo,Morgan Stanley.