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Ross Recovery theorem and its extension Ho Man Tsui Kellogg College University of Oxford A thesis submitted in partial fulfillment of the MSc in Mathematical Finance April 22, 2013

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Page 1: Ross Recovery theorem and its extension - University … Recovery theorem and its extension Ho Man Tsui Kellogg College University of Oxford A thesis submitted in partial ful llment

Ross Recovery theorem and itsextension

Ho Man Tsui

Kellogg College

University of Oxford

A thesis submitted in partial fulfillment of the MSc in

Mathematical Finance

April 22, 2013

Page 2: Ross Recovery theorem and its extension - University … Recovery theorem and its extension Ho Man Tsui Kellogg College University of Oxford A thesis submitted in partial ful llment

Acknowledgements

I am sincerely grateful to my supervisor, Dr. Johannes Ruf, for the support and

guidance he showed me throughout my dissertation writing, also for giving me the

chance to work on this interesting topic.

I would also like to express my gratitude to Dr. Kostas Kardaras and Dr. Umut

Cetin from LSE, Dr. Aleksandar Mijatovic from Imperial College, Dr. Samuel

Cohen and Pedro Vitoria from Oxford University for their helpful advices and com-

ments on my thesis.

Finally I wish to thank my parents in Hong Kong and my brother in mainland

China, who always love and support me.

Page 3: Ross Recovery theorem and its extension - University … Recovery theorem and its extension Ho Man Tsui Kellogg College University of Oxford A thesis submitted in partial ful llment

Abstract

Stephen Ross recently suggested the “Recovery Theorem”, which pro-

vides a way to reconstruct the real-world probability measure given the

risk-neutral measure, under a discrete time and state space context. Pe-

ter Carr and Jiming Yu modified Ross’s model and deduced a similar

result, under a univariate continuous diffusion context. This disserta-

tion is dedicated to access the theoretical basis and possible extensions

to the frameworks of both Ross’s recovery model and its extension Carr

and Yu’s recovery model.

To put the model in a more robust theoretical ground, we clarify each

of the assumptions, seeking the sufficient assumption set to derive each

model. Properties of the two models are established, highlighting the

limitations, similarities and other properties of the two models. Based

on the evidences presented in this thesis, we postulate that the existence

of the stationary distribution is a necessary condition for the recovery

theorem to succeed. A table of comparison between the two recovery

models is included to summrize the result in this thesis.

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Contents

1 Introduction 1

1.1 Notations and market set-up . . . . . . . . . . . . . . . . . . . . . . . 3

1.2 Indexing of the assumptions . . . . . . . . . . . . . . . . . . . . . . . 3

2 Ross’s model - basic framework 4

2.1 Assumptions and definitions . . . . . . . . . . . . . . . . . . . . . . . 5

2.2 Derivation . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 9

3 Ross’s model - analysis and discussion 12

3.1 The utility function in Ross’s model . . . . . . . . . . . . . . . . . . . 12

3.2 Existence of stationary distribution . . . . . . . . . . . . . . . . . . . 17

3.3 Interest rate process in Ross’s model . . . . . . . . . . . . . . . . . . 18

4 Carr and Yu’s model - basic framework 22

4.1 Assumptions and definitions . . . . . . . . . . . . . . . . . . . . . . . 23

4.2 Derivation . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 29

5 Carr and Yu’s model - analysis and discussion 35

5.1 Boundary conditions of the numeraire portfolio . . . . . . . . . . . . 36

5.2 Market completeness in Carr and Yu’s model . . . . . . . . . . . . . . 37

5.3 Existence of stationary distribution . . . . . . . . . . . . . . . . . . . 38

5.4 Recovery theorem on unbounded domain . . . . . . . . . . . . . . . . 41

5.4.1 Black-Scholes model . . . . . . . . . . . . . . . . . . . . . . . 42

5.4.2 CIR process . . . . . . . . . . . . . . . . . . . . . . . . . . . . 44

6 Conclusion and further research 47

Bibliography 51

Appendices 53

A Perron Frobenius theorem 54

i

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B Numeraire portfolio 56

C Regular Sturm Liouville theorem 61

D Markov chain 63

ii

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Chapter 1

Introduction

The basic objective of derivative pricing theory is to determine the fair price of a

given security in terms of more liquid securities whose price is determined by the

law of supply and demand [23]. In a market with no arbitrage opportunities, one

can determine the price of the security by using the “risk-neutral” measure (also

known as equivalent local martingale measure) due to fundamental theorem of asset

pricing [6]. The idea of the risk-neutral probability measure has been extensively

used in deriving pricing and mathematical finance in general. A gentle introduction

of the concept can be found in [9]. The risk-neutral measure is typically denoted by

the blackboard font letter “Q”.

On the other hand, risk and portfolio management aims at modelling the prob-

ability distribution of the market prices of all the securities at the given future in-

vestment horizon [23]. Based on the “real-world” probability distribution, one could

take investment decisions in order to improve the prospective profit-and-loss profile

of their positions considered as a portfolio. The real-world probability measure can

be thought of the subjective probability measure perceived by the agents in the

market. The real-world probability measure is typically denoted by the blackboard

font letter “P”.

The difference between the real-world measure and the risk-neutral measure can

be understood as the “risk-premium” of the market. Risk premium is the expected

rate of return demanded by investors over the risk-free interest rate [24]. Intu-

itively, under the risk-neutral measure, the expected return of all asset prices are

the risk-free rate, so the risky assets are priced as if the investors have a risk neutral

preference. On the contrary, investors are typically risk averse in the real world,

and hence demand a higher return over risk-free rate for investing in risky assets.

The difference between the real world expected return and the risk-free rate is the

risk-premium.

1

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The risk premium is neither tradable nor directly observable in the market. There

are a number of approaches to estimate this quantity, such as historical risk premium,

dividend yield models, market survey for market participants and institutional peers

[18]. However, the risk premium obtained from these approaches are often unstable,

conflicting and hence unreliable.

Despite the practical difficulties, there is a number of useful applications in es-

tablishing a connection between the real-world probability measure and the risk-

neutral measure. For example, based on the derivative prices of an equity asset one

can access the market subjective forecast of the return distribution of the underly-

ing equity, to derive the optimal investment strategy or to compute the risk control

measures.

Stephen Ross recently suggested the “Recovery Theorem” [19], which provides

a new way to connect the two sets of probability measures. When the risk-neutral

measure is provided, the theorem provides a way to reconstruct the real-world prob-

ability measure and deduce the risk-premium. His model is based on a discrete time

and state space with a restriction on preference of the representation agent. The

result of this paper has shed light on alternative approaches to risk management,

market forecast as well as many other applications.

Following this, Peter Carr and Jiming Yu [4] modified the model and deduced a

similar result by using a different set of assumptions. In particular, they assumed

a continuous diffusion driver of the market without assuming the existence of a

representative agent. They utilized a concept called the “numeraire portfolio”, which

is a strictly positive self-financing portfolio such that all assets, when measured in

the unit of the numeraire portfolio, are local martingales under real-world measure.

By restricting the form and the dynamics of the numeraire portfolio, they successful

proved the recovery theorem in an univariate bounded diffusion context. However,

to what extent the result is valid on the unbounded domain is still an open question.

Motivated by the two models of recovery theory, this thesis aims to review and

analyse the models in detail to access the theoretical basis and possible extensions

to the models. Our strategy to achieve this goal is twofold. First, to put the

frameworks to more robust theoretical grounds, we review and clarify each of the

assumptions in mathematical statements, seeking the sufficient assumption sets to

derive the conclusions for Ross’s model in Chapter 2 and for Carr and Yu’s model

in Chapter 4. Second, we discuss their properties, highlighting the limitations,

similarities, and other properties for Ross’s model in Chapter 3 and for Carr and

Yu’s model in Chapter 5. Notably, we prove the the existence of the stationary

2

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distribution for Ross’s model in Section 3.2 and provide heuristic argument for the

existence for Carr and Yu’s model in Section 5.3.

Based on evidences presented in the thesis, in Chapter 6 we postulate that the

existence of the stationary distribution is a necessary condition for the recovery

theorem to succeed. We propose area for further research, and conclude the thesis

by a table of comparison between the two models in Figure 6.1, summarizing the

results in the thesis.

1.1 Notations and market set-up

For the convenience of both authors and readers, the notations and the market set-

up common to both models are provided in this section.

R and R≥0 denote the set of real numbers and positive real numbers with zero

respectively. N and N+ denote the set of natural numbers and positive natural

numbers respectively.

The analysis is placed over a filtered probability space (Ω,F , (Ft),P), where

F = σ(⋃tFt).

In addition, for some fixed n ∈ N, there exists a vector of n + 1 securities

St = (S0t , S

2t , S

3t , . . . , S

nt ) ∈ Rn+1

≥0 , where

1. S0t is the risk-free security,

2. Sit for i = 1, 2, . . . , n are risky securities.

All other assumptions of models will be stated in the corresponding chapter.

1.2 Indexing of the assumptions

To clearly express the model, all the assumptions are indexed with a letter and a

number. The number of the index is in line with Carr and Yu’s paper [4], and that

in Ross’s model is constructed in parallel with that in Carr and Yu’s model. All

the assumptions in Carr and Yu’s model are started with letter “C” followed by a

number (for example, C3), and assumptions in Ross’s model are started with “R”

followed by a number (for example, R3).

3

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Chapter 2

Ross’s model - basic framework

This chapter aims at presenting the basic framework of Ross’s model, based on his

paper [19]. While Ross did not clearly specify the assumption set of the model in

mathematical terms, but rather descriptively explained the framework and derived

the result, this chapter could be treated as a formalization of the model. The pre-

sentation in this chapter is also different from Ross’s, in particular in the treatment

of the existence of representation agent in the market and his utility function, as

we found that there are inconsistencies in the derivation, which will be discussed in

Section 3.1.

We attempt to keep the material self-contained within the scope of this thesis,

therefore the definitions and theorems that are necessary to understand the model

and its conclusion are all included. Our discussion begins by laying out the assump-

tions and definitions of the models in the first section, followed by the deviation

of the result in the second section. The main result is Ross’s recovery theorem

(Theorem 2.2.1).

The objective of Ross’s recovery model is to determine the real-world transition

probabilities from the state-price securities, which is obtained from the market prices

of derivatives written on the underlying state variables.

The derivation of Ross’s model is summarized as follow:

1. The assumptions of the model are:

(a) Finite state space,

(b) Discrete time-step,

(c) No-arbitrage market (R3),

(d) Time-homogeneity of the state-price function and the real-world transi-

tion probability function (R4),

(e) The state prices are known (R5),

4

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(f) Transition independent pricing kernel (R6), and

(g) Non-negativeness and irreducibility of the state-price matrix (R7).

2. The pricing kernel can be written as matrix form (2.8), which can be refor-

mulated as a eigenvector / eigenvalue problem (2.11). The Perron Frobenius

theorem (Appendix A) is applied (Theorem 2.2.1) to solve for the real-world

transition probability.

All assumptions in this chapter start with letter ’R’ (for example, R3).

2.1 Assumptions and definitions

With reference to the market set-up in Section 1.1, the economy in Ross’s model is

discrete in time with finite state space, i.e.

1. t = t1, t2, . . . is a discrete time with a fixed time-step.

2. The state space as Π is finite, with the state variable Xt ∈ Π and |Π| = M ∈ N.

Additionally, there exists a stochastic interest rate rt ∈ R≥0, such that S0t satis-

fies:

S0t+1 = S0

t (1 + rt) for all t ∈ N (2.1)

with

S00 = 1. (2.2)

The first assumption of the model is stated as follow:

R3: “No arbitrage” condition applies in the economy.

Definition 2.1.1 (State-prices)

A state-price (also called Arrow-Debreu price) is the price of a contract that agrees

to pay one unit of a numeraire of the economy if a particular state occurs in the

next time step and pays zero in all other states.1

By the First Fundamental Theorem of Asset pricing [6], no arbitrage implies

the existence of state prices. Notice that this does not imply the contracts of the

state-price securities are tradable in the market, but simply the set of state-prices

exists and can be theoretically used for pricing purpose. Also, the set of state-prices

1This definition is referenced to [21].

5

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may not be unique.2

The following assumption considers the state-price function, which is the price

of a state-price security at a given time, given an initial state and a next transition

state.

R4 (part i): The state-price function, p, satisfies the Markov property, is time-

homogeneous and only depends on the initial state and the next transition state, i.e.

p : Π× Π→ [0, 1].

Each state price is denoted as pi,j, where i represents the initial state and j

represents the next state, as well as the state-price matrix of the model as P , where

P =

p1,1 p1,2 · · · p1,M

p2,1 p2,2 · · · p2,M...

.... . .

...pM,1 pM,2 · · · pM,M

. (2.3)

From this one can also define the risk-neutral probability matrix Q, where

Q =

p1,1/

∑Mj=1 p1,j p1,2/

∑Mj=1 p1,j · · · p1,M/

∑Mj=1 p1,j

p2,1/∑M

j=1 p2,j p2,2/∑M

j=1 p2,j · · · p2,M/∑M

j=1 p2,j

......

. . ....

pM,1/∑M

j=1 pM,j pM,2/∑M

j=1 pM,j · · · pM,M/∑M

j=1 pM,j

. (2.4)

Notice that Q is a probability transition matrix, as the sum of each of its row is

1.

We now consider the transition density function of the model, which is the prob-

ability of transition under P from an initial state to the next transition state.

R4 (part ii): The transition density function, f , satisfies the Markov property,

is time-homogeneous and only depends on the initial state and the next transition

state, i.e. f : Π× Π→ [0, 1].

The transition density function is denoted as fi,j, where i represents the initial

state and j represents the next state, as well as the transition probability matrix of

2If the set of state-prices is unique or the contracts are all tradable, then the market is complete.

6

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the model as F , where

F =

f1,1 f1,2 · · · f1,M

f2,1 f2,2 · · · f2,M...

.... . .

...fM,1 fM,2 · · · fM,M

. (2.5)

With the definitions above it is clear that the goal of the model is to recover the

matrix F from the matrix P . he following assumption:

R5: The state-price matrix P is known ex ante.

Now the pricing kernel of the model is defined:

Definition 2.1.2 (Pricing kernel in Ross’s model)

The pricing kernel from state i to state j is defined as the following quotient:

ϕi,j =pi,jfi,j

.

The pricing kernel matrix is defined as

Φ =

ϕ1,1 ϕ1,2 · · · ϕ1,M

ϕ2,1 ϕ2,2 · · · ϕ2,M...

.... . .

...ϕM,1 ϕM,2 · · · ϕM,M

. (2.6)

Definition 2.1.3 (Transition independent pricing kernel)

A pricing kernel is transition independent if it can be written in the following form:

ϕi,j =pi,jfi,j

= δh(i)

h(j), (2.7)

where

h : Π→ R>0 is a positive function, and

δ is a positive constant, called a discount factor.

The following assumption is pivotal in deriving the recovery theorem.

R6: The pricing kernel is transition independent.

7

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Remark 2.1.1

In his paper [19], Ross introduced the model in a different way. Instead of assuming

R6, he introduced the model by the existence of a representative agent with inter-

temporal additive separable utility. The transition independent pricing kernel was

then derived from the optimization of the utility. However, as we will explain in

Section 3.1, the derivation is not consistent and the transition independent pricing

kernel does not follow from the utility function.

Before stating the last assumption in Ross’s model, we need the following two

definitions:

Definition 2.1.4 (Non-negative matrix)

A square n× n matrix A is said to be non-negative if all the elements are equal to

or greater than zero, i.e.

ai,j ≥ 0

for all i = 1, 2, . . .m and j = 1, 2, . . . n.

A square matrix that is not reducible is said to be irreducible.

Definition 2.1.5 (Irreducible matrix)

A square n × n matrix (A)i,j = ai,j is said to be reducible if the indices 1, 2, . . . , n

can be divided into two disjoint non-empty sets i1, i2, . . . , iu and j1, j2, . . . , jv, with

u+ v = n, such that

aiα,jβ = 0

for α = 1, 2, . . . , u and β = 1, 2, . . . , v.

R7: The state-price matrix, P , is non-negative and irreducible.

This assumption will be used to apply the Perron Frobenius Theorem in the next

section (Theorem 2.2.1).

Remark 2.1.2

As mentioned by Ross [19], since the risk-neutral measure is equivalent to the real-

world measure, the irreducibility of the matrix P is equivalent to the irreducibility

of the matrix F . We can justify this statement by the following: an entry pi,j of

P is zero if and only if fi,j of F is zero (by the definition of equivalent probability

measures), so the indices of P can be separated into two disjoint sets if and only if

the indices of F can be separated. Therefore the irreducibility of P is equivalent to

8

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the irreducibility of F . The fact that the non-negativeness of P is equivalent to the

non-negativeness of F can be easily deduced.

Using a similar argument the irreducibility and non-negativeness of P is equiv-

alent to the irreducibility and non-negativeness of Q, because Q is just a rescaled

P .

The assumptions of Ross’s model will be further discussed in Chapter 3. In the

next section, we will see how the recovery theorem of Ross’s model is arrived based

on the set of assumptions presented in this section.

2.2 Derivation

The diagonal matrix D is defined as:

D =

h(1) 0 · · · 0

0 h(2) · · · 0...

.... . .

...0 0 · · · h(M)

.

D−1, the inverse of the matrix D, is:

D−1 =

1

h(1)0 · · · 0

0 1h(2)

· · · 0...

.... . .

...0 0 · · · 1

h(M)

.

The transition independent pricing kernel equation (2.7) can now be written in

matrix form,

P = δD−1FD.

Reorganize the equation,

F =1

δDPD−1. (2.8)

Lemma 2.2.1 (Identity for transition probability)

Let e be a M×1 column vector of 1, i.e. e =(1 1 · · · 1

)T. The following identity

holds:

Fe = e. (2.9)

Proof. The intuition for this lemma is simple: the rows on F are essentially proba-

bility to different states given the current state, the sums if each row must be equal

to one.

9

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As defined in (2.5), (F )i,j = fi,j is the probability of transiting from the initial

state i to j. Summing up all the transition probabilities one will get:

M∑j=1

fi,j = 1 for all i = 1, 2, . . . ,M .

To write this equality in matrix form, we have

Fe = e.

Multiply both sides of (2.8) by e and reorganize, we have

PD−1e = δD−1e.

Let

x = D−1e. (2.10)

Then

Px = δx. (2.11)

Hence the equation has been transformed to an eigenvalue and eigenvector prob-

lem.

Before we proceed, notice that:

1. The entries of x are actually the diagonal elements of the matrix D−1, which

is 1h(i)

. Therefore they must be positive.

2. δ is the subjective discount factor so it must be a non-negative number less

than or equal to one.

The following theorem guarantees a unique solution of this problem, which sat-

isfies these two conditions.

Theorem 2.2.1 (Ross recovery theorem)

There exists a unique positive solution of x (up to a positive scaling) and δ to the

problem (2.11). Moreover, we can recover the matrix D (up to a positive scaling)

and the matrix F .

Proof. This proof uses the Perron Frobenius theorem (Appendix A).

From R7, P is an irreducible matrix. Applying the Perron Frobenius theorem,

the only eigenvector of P whose entries are all positive is its Perron vector, which

is unique up to a positive scaling. Therefore it is the only possible solution to x.

10

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In addition, δ must be equal to the corresponding eigenvalue Perron root ρ(P ) >

0. Notice that δ is unique while x is unique up to a positive scaling.

δ is bounded above by the maximum sum of row and the minimum sum of row

of P . Since P is a state-price matrix, each of its sum of row must be non-negative

(by R7, each entry of P is non-negative). Moreover, the maximum pay-off of each

state-price security is one, if all state-price securities are purchased a pay-off of one

will be guaranteed. This implies that the sum of each of its row is always less than

or equal to one,3 i.e.

0 ≤ δ ≤ 1.

Once x is found, one can imply D by (2.10) (up to a positive scaling), and then

recover the matrix F by (2.8). The recover matrix F is unique since the scaling

factor is cancelled on the R.H.S. of (2.8).

Remark 2.2.1

Ross [19] pointed out that the transition independent pricing kernel (R6) is crucial in

deriving the recovery theorem - it allows the pricing kernel to be separated from the

real-world probability. To illustrate this point, notice that (2.7) can be rearranged

as:

pi,j = ϕi,jfi,j = δh(i)

h(j)fi,j.

Given only the knowledge of pi,j, the recovery theorem uses the transition inde-

pendence to separately determine ϕi,j and fi,j. Without the transition independent

pricing kernel, the recovery of real-world measure P is not feasible.

The foregoing deviation provides a theoretical basis to uniquely determine the

matrix F from the matrix P . By recovering the matrix F , the main objective of the

model is achieved - to obtain the real-world probability measure from the risk-neutral

probability.

The analysis and discussion for this model is contained in the next chapter.

3This argument will be elaborated in detail in Section 3.3.

11

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Chapter 3

Ross’s model - analysis anddiscussion

While the last chapter gave the mathematical foundation for Ross’s framework, the

present chapter focuses the analysis and discussions of Ross’s model. We attempt to

highlight the features and limitations of the model, and these results will be contrast

with those of Carr and Yu’s model in the later chapters.

This chapter is divided into the following sections:

Section 3.1: The utility function in Ross’s model

We begin the discussion by pointing out a major gap in Ross’s paper [19]: the

transition independent pricing kernel (Definition 2.1.3) does not logically follow

from inter-temporal additive separable utility as Ross suggested. We will review

how Ross introduced a representative agent and his utility function, and explain the

inconsistencies in the derivation.

Section 3.2: Existence of stationary distribution

The discussion progresses to discuss a common feature of the two recovery model.

We analyse Ross’s model from a perspective of the Markov chain theory. The Perron

Frobenius theorem is then used to show the existence of the stationary distribution

in Ross’s model.

Section 3.3: Interest rate process in Ross’s model

Lastly a few properties relating to the interest rate process in Ross’s model are

explored.

3.1 The utility function in Ross’s model

In Chapter 2, we have reviewed how the real-world probability P is recovered from

the risk-neutral probability Q in Ross’s framework. The derivation starts from the

12

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transition independent pricing kernel (2.1.3) as in A6, the equation is rewritten in

a matrix form and the Perron Frobenius theorem is applied to solve for the unique

solution of the matrix F .

However, in Ross’s paper [19], he introduced the model in a different way: he

first assumed the existence of a representative agent with an inter-temporal addi-

tive separable utility function, the transition independent pricing kernel was then

deduced from optimizing the agent’s utility, and the matrix F was uniquely solved

afterwards. In other words, instead of directly making the transition independent

pricing kernel as one of the assumptions, Ross deduced it by assuming the existence

of a representative agent with a specific form of utility function.

In fact, we deviate from Ross’s approach for a reason - it is because the transi-

tion independent pricing kernel does not logically follow from inter-temporal additive

separable utility function as Ross has suggested. In this section, we illustrate why

this is the case. This section is based on Carr and Yu’s paper [4, P. 11-13].

To begin with, the definition of the inter-temporally additive separable utility

function is introduced.

Definition 3.1.1 (Inter-temporally additive separable utility function)

An inter-temporally additive separable utility function U : C → R in discrete two-

period economy is

U(c) = u(c0) + δE[u(c1)], (3.1)

where

C is the space of all feasible consumption processes,

c = (c0, c1) ∈ C, is the consumption at t = 0 and t = 1,

u : R+ → R is a strictly concave function, and

δ is a constant impatient factor, with 0 < δ < 1.

Specializing this definition to the setting of Ross’s model, an agent faces the

following optimization problem:

supc∈C

u(c0,i) + δ

M∑j=1

u(c1,j)fi,j s.t. c0,i +M∑j=1

c1,jpi,j = w, (3.2)

where the first index of c is the time index and the second index is the state

index; w is the initial wealth of the representative agent.

13

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Assuming in this section, R6 in Chapter 2 is replaced with the following two

assumptions, R6’ (part i) and R6’ (part ii).

R6’ (part i): There exists a representative agent in the economy with inter-

temporally additive separable utility.

The existence of the representative agent assumption is valid when, for example,

the market is complete and the economy is in equilibrium state. A reference for this

could be found in [7].

R6’ (part ii): The optimal consumption process is time-homogeneous.

In other words, the consumption only depends on the state in which the con-

sumption takes place. The consumption at state j ∈ Π is denoted as cj.

We will first see how the transition independent kernel is derived and then ex-

plain why we found the derivation inconsistent.1

Suppose the current state is i. Since the state space Π is finite, and from (3.2)

the representative agent faces the following problem:

supc∈C

u(c0,i) + δM∑j=1

u(c1,j)fi,j s.t. c0,i +M∑j=1

c1,jpi,j = w.

Define the Lagrangian L as:

L ≡ u(c0,i) + δ

M∑j=1

u(c1,j)fi,j + λ

(w − c0,i −

M∑j=1

c1,jpi,j

).

The first order condition for the optimal solution are:

u′(c∗0,i)− λ = 0 for all i ∈ Π

and

δu′(c∗1,j)fi,j − λpi,j = 0 for all i, j ∈ Π.

Solving these equations give formula for the pricing kernel in terms of the optimal

consumption process:

pi,jfi,j

= δu′(c∗1,j)

u′(c∗0,i)for all i, j ∈ Π. (3.3)

1In Ross’s paper [19], Ross didn’t derive the transition independent kernel in detail, but ratherexplained it descriptively. The derivation here largely follows Carr and Yu’s paper [4], in whichthey tried to provide the missing derivation steps in Ross’s model.

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Using assumption R6’ (part ii), the optimal consumption process is time-

homogeneous. Hence we can drop the time index of c∗ in the expression:

pi,jfi,j

= δu′(c∗j)

u′(c∗i )for all i, j ∈ Π. (3.4)

Therefore the kernel is the transition independent as defined in (2.7).

However, the derivation above is inconsistent for two reasons:

First, while (3.2) is an one-period optimization problem, the time-homogeneous

optimal consumption assumption (R6’ (part ii)) is satisfied only when the con-

sumption horizon is infinite. Given a one-period consumption horizon, a rational

agent will consume differently at time zero and time one to maximize his utility, be-

cause two consumptions contribute differently to his total utility, i.e. consumption

is discounted by factor δ only at time one but not at time zero. The same argument

could be applied to argue that optimal consumption is not time-homogeneous for

any finite-period consumption horizon.

On the other hand, if the consumption horizon is infinite, the agent will be indif-

ferent to the current time, since he will be faced with the same set of infinite period

optimization problems regardless of time. This implies that the optimal consump-

tion process will not depend on time but only depend on the current state of the

system. In other words, the optimal consumption process will be time-homogeneous.

Second, the optimal solution to (3.2) should depend on the initial state, and with

different initial states the optimal solutions should be different. However, in (3.3),

the optimal solutions are considered the same regardless of the initial state of the

optimization problem2.

This idea can be illustrated by the following simple example. Suppose, for sim-

plicity, there are only two states, α and β, with the following transition probabilities

and state prices:

fα,α = 0.6, pα,α = 0.5,

fα,β = 0.4, pα,β = 0.4,

fβ,α = 0.7, pβ,α = 0.6,

fβ,β = 0.3, pβ,β = 0.2.

2This inconsistency was suggested by Carr and Yu on [4, p. 13].

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with w = 10, δ = 0.9, and function u(x) = log x.

If the current state is α, then the optimization problem is:

sup log(cα) + 0.9[0.6 log(cα) + 0.4 log(cβ)] s.t. cα + 0.5cα + 0.4cβ = 10. (3.5)

β

α α

β

f = 0.6, p = 0.5

f = 0.4, p = 0.4

Figure 3.1: Optimization problem when the current state is α

The optimal solution to problem (3.5) is:

(c∗α)1 = 5.40351 and (c∗β)1 = 4.73684.

On the other hand, if the current state is β, the optimization problem is:

supu(cβ) + 0.9[0.7 log(cα) + 0.3u(cβ)] s.t. cβ + 0.6cα + 0.2cβ = 10. (3.6)

β

α α

β

f = 0.7, p = 0.6

f = 0.3, p = 0.2

Figure 3.2: Optimization problem when the current state is β

The optimal solution to (3.6) is:

(c∗α)2 = 5.36184 and (c∗β)2 = 7.10526.

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Obviously (c∗α)1 6= (c∗α)2 and (c∗β)1 6= (c∗β)2.

This example shows the optimal solutions to (3.2) are different with different

initial states. However, in the transition independent kernel expression (3.4), all

optimal consumptions are considered the same regardless of the initial states of the

optimization problems.

Based on the two reasons above we conclude that the transition independent

kernel (3.3) is not consistent with inter-temporally additive separable utility.

3.2 Existence of stationary distribution

In this section, we will analyse Ross’s model from the perspective of the Markov chain

theory to prove existence of the stationary distribution in Ross’s model. Similar to

the derivation of Ross’s recovery theorem, the proof utilizes the Perron Frobenius

theorem (Appendix A).

Intuitively, a finite state Markov chain is a system that undergoes transitions

from one state to another, between a finite number of possible states. It also satisfies

the Markov property (also known as “memoryless” property): the next state only

depends on the current state but not the sequence of events that precedes it [22]. A

formal definition of Markov chain and some of its useful properties could be found

in Appendix D.

It is easy to see that Ross’s model is a time-homogeneous finite state irreducible

Markov chain. The state variable is Xn ∈ Π, and with either

1. the transition density matrix F , as defined in (2.5), or

2. the risk-neutral probability matrix Q, as defined in (2.4)

as the transition probability matrix.

Stationary distributions play a important role in analysing Markov chains. In-

formally, a stationary distribution represents a steady state in the Markov chains

behaviour. The formal definition of the stationary distribution of a Markov chain is

given below:

Definition 3.2.1 (Stationary distribution of a Markov chain)

Let Xn be a time-homogeneous Markov chain having state-space Π and the tran-

sition probability matrix P . If π is a probability distribution such that:

Pπ = π,

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then π is called the stationary distribution of Xn.

This definition basically means that if a chain reaches a stationary distribution,

then it maintains that distribution for all future time. The proof for the existence

of the stationary distribution in Ross’s model is given in the following theorem:

Theorem 3.2.1 (Existence of stationary distribution in Ross’s model)

Given the Markov chain formulation of Ross’s model, with

1. the transition density matrix F , or

2. the risk-neutral probability matrix Q,

as transition probability, there exists a unique stationary distribution in Ross’s

model.

Proof. This theorem is proved by the Perron Frobenius theorem (Appendix A).

We only prove for the transition density matrix F , but the same argument could

hold for Q.

For the transition probability matrix F , the sum of its row must be 1. By the

Perron Frobenius theorem, its spectral radius r must be

1 = mini

∑j

fi,j ≤r ≤ maxi

∑j

fi,j = 1,

So 1 is a eigenvalue of F , and the corresponding Perron vector, v, satisfies:

Fv = v.

Hence v is the stationary distribution of the Markov chain in Ross’s model.

3.3 Interest rate process in Ross’s model

In this section the important features of Ross’s model related to the interest rate

process are derived. This section is largely based on remarks and theorems in Ross’s

paper [19].

The following will be discussed:

1. The interest rate process is time-homogeneous.

2. The subjective discount rate δ is bounded above by the largest interest rate

factor and below by the lowest interest rate factor.

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3. If the interest rate process is a constant, then the real-world probability mea-

sure will be the same as the risk-neutral probability measure.

First we show that the interest rate process is time-homogeneous. Note that

this feature is not an assumption but rather than an implication of the model, in

contrast with Carr and Yu’s model, where the interest rate process is assumed to

be time-homogeneous (C6 (part ii)).

Theorem 3.3.1 (Time-homogeneity of interest rate process)

In Ross’s model, the interest rate for each period, rt, only depends on the current

state, but is independent of time, i.e. it is a time-homogeneous process. Moreover,

rt =1∑M

j=1 pi,j− 1.

Proof. The conclusion is mainly followed by the R4 (part i).

Consider the sum of row i of the state-price matrix P . Given a state i as the

current state, if one purchases all state-price securities pi,j, j ∈ Π, one will be guar-

anteed a pay-off of one no matter what state is realized. Hence in a market without

arbitrage (R3), the sum∑M

j=1 pi,j should be equal to the one-period discounted

value of one, i.e.M∑j=1

pi,j =1

1 + rt(3.7)

Rearrange:

rt =1∑M

j=1 pi,j− 1.

Since the R.H.S. only depends on the current state, i, so the interest rate for

each period is a time-homogeneous process.

Second, based on the similar argument, one can prove that the subjective dis-

count factor, δ, is bounded above by the largest interest rate factor and bounded

below by the smallest interest rate factor.

Theorem 3.3.2 (Bounds for subjective discount rate)

In Ross’s model, the subjective discount rate δ is bounded above by the largest

interest discount factor and bounded below by the smallest interest discount factor,

i.e.1

1 + maxi∈Π ri≤ δ ≤ 1

1 + mini∈Π ri

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Proof. First an argument from the Perron Frobenius theorem is used. The Perron

root δ is between minimum sum of row and maximum sum of row of P (inclusive),

i.e.

mini

M∑j=1

pi,j ≤ δ ≤ maxi

M∑j=1

pi,j.

From (3.7) we know thatM∑j=1

pi,j =1

1 + ri.

Substitute this into the equation above we have

1

1 + maxi∈Π ri≤ δ ≤ 1

1 + mini∈Π ri.

Lastly, the following is proved:

Theorem 3.3.3 (Implication for constant interest rate)

In Ross’s model, if the interest rate is also independent of the current state, i.e. the

interest rate is constant, then the real-world probability measure will be the same

as the risk-neutral measure, i.e.

P = Q.

Proof. If the interest rate is constant, from (3.7) each sum of rows of P is the same.

M∑j=1

pi,j =1

1 + r= k for all i ∈ Π,

where k is the constant interest discount factor.

This can be rewritten in matrix form,

Pe = ke,

where e be a M × 1 column vector of one.

From the Perron Frobenius theorem, the Perron vector of P is e and the Perron

root is one.

By (2.8),

F =1

kP .

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From (2.4), the definition of the risk-neutral probability matrix Q is

Q =1∑M

j=1 pi,jP

= (1 + r)P

=1

kP

= F .

Therefore the real-world probability measure P is the same as the risk-neutral

measure Q.

In the next chapter, we will review how Carr and Yu arrive at a similar re-

sult as Ross did on a bounded continuous state space, based on a different set of

assumptions.

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Chapter 4

Carr and Yu’s model - basicframework

As an extension to Ross’s model, Carr and Yu’s model aimed at establishing the

recovery theorem under a bounded diffusion context. They utilized the concept of

the numeraire portfolio, which is a strictly positive self-financing portfolio such that

all assets, when measured in the unit of the numeraire portfolio, are local martingales

under real-world measure P.

As Carr and Yu [4] pointed out, their model differs from the Ross’s model in two

ways. First, their model is based on a bounded diffusion context, compared with the

finite state Markov chain in Ross’s model. Second, they restrict a structure on the

dynamics of the numeraire portfolio to replace the restriction on the representative

agent’s preference as in Ross’s model.

Similar to Ross’s model in Chapter 2, in this chapter we present the framework of

Carr and Yu’s model, starting with its market setting and assumptions and followed

by the deviation of the recovery theorem. The main result is the recovery theorem

in Carr and Yu’s model (Theorem 4.2.3).

The steps in the derivation of Carr and Yu’s model are listed as follow:

1. The main objective is to recover the real-world measure P from the risk-neutral

measure Q, together with the Radon-Nikodym derivative dPdQ .

2. The main feature of Carr and Yu’s model is the role played by the numeraire

portfolio.

3. The assumptions of the model are:

(a) A continuous time and space model,

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(b) “No free lunch with vanishing risk” applies in the market, and the nu-

meraire portfolio Lt is equal toS0t

Mt, where Mt = dQ

dP

∣∣Ft

(C3),

(c) A continuous, time-homogeneous, bounded, and univariate driver, from

which all asset prices can be determined (C4),

(d) The dynamics of the interest rate and the driver under the risk-neutral

measure Q are known (C5),

(e) The numeraire portfolio depends only on the current value of the driver

and time (C6 (part i)),

(f) Time-homogeneity of the interest rate process (C6 (part ii)) and diffu-

sion coefficient of the numeraire portfolio (C6 (part iii)),

(g) Continuity and differentiability assumptions (C7), and

(h) The boundary conditions for the numeraire portfolio are known (C8).

4. Based on this set of assumptions, if the diffusion coefficient of the numeraire

portfolio is determined, the market price of risk can be determined (Theo-

rem 4.1.1).

5. The problem of solving the diffusion coefficient can be transformed to a prob-

lem of eigenvalue and eigenfunction (4.21).

6. The regular Sturm Liouville theorem (Appendix C) is then applied (Theo-

rem 4.2.3) to uniquely determine the diffusion coefficient.

7. The Girsanov’s theorem and the change of numeraire theorem are applied to

determine the dynamics of the driver under the real-world measure P and the

Radon-Nikodym density dPdQ (Theorem 4.2.4).

In this chapter we utilize the sufficient set of assumptions to derive the result of

Carr and Yu’s model. On top of the existing assumptions, we state the additional

assumptions to the model (C7, C8) which are necessary but have been omitted in

Carr and Yu’s paper [4].

All the assumptions in this chapter model start with letter ’C’ (for example,

C3).

4.1 Assumptions and definitions

With reference to the market set-up in Chapter 1.1, the economy in Carr and Yu’

model is continuous for time and state space, i.e.

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1. t is a continuous time index on a finite interval t ∈ [0, T ].

2. The state space is continuous.

Moreover, there exists a stochastic interest rate rt ∈ R≥0, such that S0t satisfies:

S0t = e

∫ t0 rsds t ∈ [0, T ], (4.1)

or equivalently,

dS0t = rtS

0t dt t ∈ [0, T ], (4.2)

with

S00 = 1. (4.3)

C3 (part i): “No free lunch with vanishing risk” (NFLVR) condition applies in

the economy.

By the Fundamental Theorem of Asset Pricing [6], there exists an equivalent

local martingale measure (ELMM) Q such that (Si/S0)t is a local martingale for all

i = 0, 1, . . . , n under Q.

Furthermore we can define the Radon-Nikodym derivative, Mt, as

Mt =dQdP

∣∣∣∣Ft

. (4.4)

The concept of the numeraire portfolio is introduced, which plays an important

role in deriving the result of the model. More about the numeraire portfolio could

be found in Appendix B.

Definition 4.1.1 (The numeraire portfolio)

A numeraire portfolio Lt is a strictly positive self-financing portfolio, such that

(Si/L)t is a local martingale under P-measure for all i = 0, 1, . . . , n.

NFLVR condition implies the existence of numeraire portfolio, which is discussed

Appendix B.

C3 (part ii): The numeraire portfolio, Lt, is equal toS0t

Mt.1

This assumption can be satisfied, for example, if the market is complete. The

proof of this statement could also be found in Appendix B.

The numeraire portfolio has the following property:

1This assumption will be discussed in detail in Section 5.2.

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Theorem 4.1.1 (Dynamic of the numeraire portfolio under P)

Lt has a dynamics of the following form under P:

dLtLt

= (rt + σ2t )dt+ σtdW

Pt , (4.5)

where W Pt is a Brownian motion under P, and σt is an adapted process.

Proof. (Si/L)t is a local martingale for all i = 0, 1, . . . , n.

In particular, by Martingale Representation Theorem,

d(S0/L)t(S0/L)t

= −σtdW Pt (4.6)

for some adapted process σt.

Let A be an Ito process. From Ito’s formula we have

d

(1

A

)= − 1

A2dA+

1

A3(dA)2.

Set A = (S0/L)t,

d

(L

S0

)t

= − L2t

(S0t )

2d

(S0

L

)t

+L3t

(S0t )

3

(d

(S0

L

)t

)2

.

Divide both sides by Lt/S0t and substitute (4.6) implies:

d

(L

S0

)t

/

(L

S0

)t

= σ2t dt+ σtdW

Pt .

Again by Ito’s formula,

d

(L

S0

)t

=1

S0t

dLt −Lt

(S0t )

2dS0

t .

Substitute the dynamics for S0t as in (4.2)

d

(L

S0

)t

=1

S0t

dLt −LtrtS0t

dt

d

(L

S0

)t

/

(L

S0

)t

=dLtLt− rtdt

σ2t dt+ σtdW

Pt =

dLtLt− rtdt

dLtLt

= (rt + σ2t )dt+ σtdW

Pt .

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An important consequence of Theorem 4.1.1 is the following relationship:

Corollary 4.1.1 (The market price of risk)

The “market price of risk”, Θt, (also known as the “risk premium”) of the model is

equal to the diffusion coefficient of the numeraire portfolio, i.e.

Θt = σt.

Proof. The market price of risk is defined as

Θt =αt − rtσt

,

where αt is the drift coefficient of a tradable asset, σt is the drift coefficient of a

tradable asset, and rt is the interest rate process.

From Theorem 4.1.1 the market price of risk can be deduced as:

Θt =rt + σ2

t − rtσt

.

Hence

Θt = σt.

Definition 4.1.2 (Time-homogeneous Ito diffusion2)

An one-dimensional bounded time-homogeneous Ito diffusion Xt is an adapted

stochastic process satisfying a stochastic differential equation of the form:

dXt = b(Xt)dt+ a(Xt)dWt,

where Wt is an one-dimensional Brownian motion, and also b : R → R, a : R → Rsatisfy the Lipschitz continuity condition, that is,

|b(x)− b(y)|+ |a(x)− a(y)| ≤ D|x− y| x, y ∈ R for some constant D.

Definition 4.1.3 (Infinitesimal generator of an Ito diffusion)

The infinitesimal generator G of an one-dimensional Ito diffusion Xt is defined by

Gf(x) = limt→0

E [f(Xt)|X0 = x]− f(x)

tfor x ∈ R.

2This definition is referenced to [17, p. 116]

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The infinitesimal generator can be shown to be equivalent to3:

G =∂

∂t+a2(x)

2

∂2

∂x2+ b(x)

∂x.

The “driver” of the model is now introduced, from which all security prices are

derived.

C4: There exists an univariate bounded time-homogeneous Ito diffusion Xt ∈[u, l] such that Sit = Si(Xt, t) for i = 0, 1, . . . , n. Xt is called the driver in the model.

By definition the driver Xt satisfies the following stochastic differential equation:

dXt = b(Xt)dt+ a(Xt)dWQt , (4.7)

where WQ is a Brownian motion under Q.

(4.1) can be written as;

rt =∂

∂tlogS0

t .

From C4, S0t = S0(Xt, t), so rt = rt(Xt, t). In other words, the interest rate

process rt is also driven by the driver Xt.

The dynamics of the driver under Q is calibrated using the market data. This

is stated in the following assumption:

C5: a(x), b(x), and r(x, t) are known ex ante. In addition, a(x) 6= 0 for all

x ∈ [u, l].4

The next assumption is pivotal in deriving the conclusion of the model. It is

divided into three parts, but they are all related to the structure of the numeraire

portfolio.

C6 (part i): The numeraire portfolio, Lt, depends only on the current value of

the driver Xt and time t, i.e.

Lt ≡ L(Xt, t) (4.8)

3A reference for this can be found on [17, p. 123].4The condition a(x) 6= 0 is different from the assumption a(x) ≥ 0 as in Carr and Yu’s paper

[4]. As we will see in the next section this weaker condition is sufficient to derive the result.

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C6 (part ii): The interest rate process, rt, is time-homogeneous, i.e.

r(x, t) ≡ r(x) (4.9)

C6 (part iii): The diffusion coefficient of Lt, σt, is time-homogeneous, i.e.

σ(x, t) ≡ σ(x) (4.10)

Under the risk-neutral measure Q, all self-financing portfolios have the drift

coefficient of rt. As Lt is a self-financing portfolio, it also has the drift coefficient of

rt. Therefore Lt can be written as:

dLtLt

= r(Xt)dt+ σ(Xt)dWQt . (4.11)

In other words, the numeraire portfolio Lt is a time-homogeneous process under

measure Q.

The next assumption C7 is also divided into three parts. They were not included

in Carr and Yu’s paper, but they are important in deriving the recovery theorem.

C7 (part i): a(x), b(x), and r(x) are continuous functions. r(x) is also bounded

below.

Together with a(x) 6= 0 as in C5, one can deduce that either a(x) > 0 or a(x) < 0

for all x ∈ [u, l], i.e. a(x) never changes sign.

C7 (part ii): Si(x, t) for i = 0, 1, . . . , n are twice continuously differentiable

C7 (part iii): Lt = L(Xt, t) is a twice differentiable function.

They will be applied in different parts of the derivation.

Theorem 4.1.2 (PDE for asset prices)

Assets in the market satisfy the following equation:

GSi(x, t) = r(x)Si(x, t) for i = 0, 1, . . . , n. (4.12)

Proof. Under the risk-neutral probability Q, the following identity holds:

SitS0t

= EQ[SiTS0T

|Ft]

.

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Rearrange this identity and substitute (4.1), we have:

Si(x, t) = EQ[exp

(−∫ T

t

r(Xs)ds

)Si(XT , T )|Ft

].

Since the price functions Si are twice continuously differentiable (C7 (part ii))

and r is continuous and bounded below (C7 (part i)), we can apply Feynman-Kac

formula5,

∂Si(x, t)

∂t+a2(x)

2

∂2Si(x, t)

∂x2+ b(x)

∂Si(x, t)

∂x− r(x)Si(x, t) = 0.

Rewrite it using the infinitesimal generator,

GSi(x, t) = r(x)Si(x, t).

Like C7, the following assumption was not included in Carr and Yu’s paper.

C8: The boundary conditions of L(x, t) and ∂∂xL(x, t) at x = l and x = u are

known ex-ante.6

The assumptions of Carr and Yu’s model will be further discussed in Chapter 5.

In the next section we will see how the recovery theorem of Carr and Yu’ model is

arrived.

4.2 Derivation

In this section the recovery theorem of Carr and Yu’s model is derived.

We first derive the diffusion coefficient of the numeraire portfolio σt, which is

equivalent to the market price of risk Θt by Corollary 4.1.1. The Girsanov theorem

is then applied to recover the dynamics of the process Xt under P-measure, together

with the dynamics of all the security prices Sit . As mentioned, an important fea-

ture of Carr and Yu’s model is the assumption on the form and dynamics of the

numeraire portfolio (C6).

5A reference for this formula is on [20, p. 145].6Although not included in the paper, this condition was suggested by Peter Carr in an email

to Johannes Ruf. This assumption is needed in applying the regular Sturm Liouville theorem, aswe will see in the next section. This assumption will also be discussed in detail in Section 5.1.

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Substitute (4.9) and (4.10) into (4.5), one can derive an expression for dynamics

of Lt under P:dLtLt

= [r(Xt) + σ2(Xt)]dt+ σ(Xt)dWPt . (4.13)

An expression for the dynamics of Xt under P is also needed:

Theorem 4.2.1 (Dynamics of the driver under P)

The dynamics of the driver, Xt, under P is given by

dXt = [b(Xt) + σ(Xt)a(Xt)]dt+ a(Xt)dWPt , (4.14)

which is a time-homogeneous diffusion process.

Proof. With reference to (4.7), the change of measure only changes the drift coeffi-

cient by the Girsanov’s Theorem. Therefore the diffusion term of Xt under P is still

a(Xt).

From Corollary 4.1.1, the market price of risk is σ(Xt). By the Girsanov’s theo-

rem, the drift coefficient of Xt under P is b(Xt) + σ(Xt)a(Xt), i.e.

dXt = [b(Xt) + σ(Xt)a(Xt)]dt+ a(Xt)dWPt .

Theorem 4.2.2 (Diffusion coefficient of the numeraire portfolio)

The diffusion coefficient function, σ(x), satisfies the following equation:

σ(x) = a(x)∂

∂xlogL(x, t). (4.15)

Proof. As Lt is twice differentiable (C7 (part iii)), Ito’s formula can be applied to

(4.8),

dLt =∂Lt∂t

dt+∂Lt∂x

dXt +1

2

∂2Lt∂x2

(dXt)2

dLtLt

=1

Lt

∂Lt∂t

dt+1

Lt

∂Lt∂x

dXt +1

2

1

Lt

∂2Lt∂x2

(dXt)2.

Substitute (4.14) and compare only the diffusion terms of dLL

with equation (4.13):

σ(x) =1

Lt

∂Lt∂x

a(x).

Rearrange the equation,

σ(x) = a(x)∂

∂xlogL(x, t).

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The equality in (4.15) will be reorganized such that it can fit into the regular

Sturm Liouville theorem (Appendix C).

Since a(x) 6= 0 (by C5), for some function f(t),

logL(x, t) =

∫ x

l

σ(y)

a(y)dy + f(t). (4.16)

Note that σ(x) and a(x) are continuous functions (C7 (part i)), so σ(x)a(x)

is

integrable.

Take exp(·) on the both sides and let:

π(x) = e∫ xlσ(y)a(y)

dy

p(t) = ef(t).

Thus, a separable expression of L(x, t) is obtained:

L(x, t) = π(x)p(t). (4.17)

Substitute this into the generator equation (4.12):

π(x)p′(t) +a2(x)

2π′′(x)p(t) + b(x)π′(x)p(t) = r(x)p(t)π(x).

Dividing by π(x)p(t) implies:

p′(t)

p(t)+a2(x)

2

π′′(x)

π(x)+ b(x)

π′(x)

π(x)= r(x)

a2(x)

2

π′′(x)

π(x)+ b(x)

π′(x)

π(x)− r(x) = −p

′(t)

p(t).

The two sides can only be equal if they are each equal to a constant λ ∈ R:

p′(t)

p(t)= λ, (4.18)

a2(x)

2

π′′(x)

π(x)+ b(x)

π′(x)

π(x)− r(x) = −λ. (4.19)

The solution to (4.18) is the following:

p(t) = p(0)eλt (4.20)

and λ is still an unknown.

Reorganize the problem for (4.19):

a2(x)

2π′′(x) + b(x)π′(x)− r(x)π(x) = −λπ(x), (4.21)

which is an eigenvalue and eigenfunction problem.

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Theorem 4.2.3 (Recovery theorem in Carr and Yu’s model)

The only valid solution to (4.21), in which the corresponding the numeraire portfolio

is positive, is:

π(x) = φ(x)

λ = ρ,

where

1. ρ is the smallest eigenvalue of the problem, and

2. φ(x) is eigenfunction correspond to ρ.

Proof. The problem can be re-written in self-adjoint form:

a2(x)

2c(x)

∂x

(c(x)

∂π(x)

∂x

)− r(x)π(x) = −λπ(x),

where

c(x) = exp

(∫ x

l

2b(y)

a2(y)dy

).

Dividing the function a2(x)2c(x)

the problem becomes

∂x

(c(x)

∂x

)− q(x)π(x) = −λπ(x)w(x), (4.22)

where

q(x) =2c(x)r(x)

a2(x), and

w(x) =2c(x)

a2(x).

We know that:

1. c(x), w(x) are positive,

2. c(x), c′(x), q(x) and w(x) are continuous (because from C7 (part i), a(x),

b(x) and r(x) are all continuous functions), and

3. The boundary conditions of π(x) and π′(x) at x = l and x = u are known

(because from C8, the boundary conditions of L(x, t) and ∂∂xL(x, t) at x = l

and x = u are known, which can be used to deduced the bounary conditions

for π(x) and π′(x)).

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The problem (4.22) is a regular Sturm Liouville problem (Appendix C).

One can numerically solve for all of the eigenfunctions and eigenvalues. Moreover,

the eigenvalues of the problem can be denoted as:

λ1 < λ2 < · · · < λn < · · · → ∞,

and its corresponding eigenfunctions to be:

π1(x), π2(x), π3(x), . . .

Let

φ(x) = π1(x), and

ρ = λ1.

From (4.17),

L(x, t) = π(x)p(t).

Since L(x, t) is positive, of all the eigenfunctions only φ(x) is positive and never

changes sign. So φ(x) is the only valid eigenfunction to the problem (4.22), and

hence the only valid eigenvalue is the corresponding eigenvalue ρ.

Remark 4.2.1

Notice that the form and dynamics of the numeraire portfolio (C6) allow Lt to be

separated as a function of the driver x and a function of time t in (4.17), deriving

the recovery theorem. Without C6, the recovery theorem of Carr and Yu’s model is

not possible. This feature will be contrasted with the transition independent pricing

kernel in Ross’s model in Chapter 6.

Substitute the result of Theorem 4.2.3 and (4.20) into (4.17),

L(x, t) = φ(x)ef(0)eρt. (4.23)

Substitute (4.23) into expression (4.15),

σ(x) = a(x)∂

∂xlog φ(x).

Once the function σ(x) is found, we can derive the dynamics of Xt under P by

Theorem 4.2.1:

dXt = [b(Xt) + σ(Xt)a(Xt)]dt+ a(Xt)dWPt ,

and dPdQ in the following theorem.

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Theorem 4.2.4 (Expression for the Radon-Nikodym derivative)

The Radon-Nikodym derivative dPdQ is given by:

dPdQ

= e−∫ T0 rsds

φ(XT )

φ(X0)eρT .

Proof. dPdQ can be determined by the change of numeraire theorem [20], using the

numeraire portfolio as the numeraire, we have

dPdQ

=S0

0

S0T

L(XT , T )

L(X0, 0).

Substitute (4.23) and (4.1) into this expression,

dPdQ

= e−∫ T0 rsds

φ(XT )

φ(X0)eρT .

In other words, the dynamics of Xt under the real-world measure P and the

Radon-Nikodym density dPdQ have been recovered.

In the next chapter we will analyse and discuss the features and implications of

Carr and Yu’s model.

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Chapter 5

Carr and Yu’s model - analysisand discussion

In the preceding chapters we have reviewed the basic frameworks of Ross’s model

and Carr and Yu’s model, and also discussed the limitations and features of Ross’s

model. In this chapter Carr and Yu’s model is analysed to highlight its limitations,

similarities with Ross’s model and also other features.

This chapter is divided into the following sections:

Section 5.1: Diffusion coefficient of the numeraire portfolio

The discussion begins by analysing C8: the boundary conditions for the nu-

meraire portfolio is known ex-ante. We attempt to argue that if there is no general

method of obtaining the boundary conditions of the numeraire portfolio, the imple-

mentation of the recovery theorem could be difficult in practice.

Section 5.2: Market completeness in Carr and Yu’s model

An implicit restriction in Carr and Yu’s model is the market completeness con-

dition. We argue that, although not explicit assumed in the model, the market

completeness condition is necessary for Carr and Yu’s model.

Section 5.3: Existence of stationary distribution

The discussion will progress to illustrate the similarities between Ross’s model

and Carr and Yu’s model. In particular, we focus on the existence of the stationary

distribution. In this section we provide heuristic argument for the existence of the

stationary distribution in Carr and Yu’s model.

Section 5.4: Recovery theorem on unbounded domain

In addition to bounded diffusion considered in Chapter 4, we expand the scope

to consider examples of the model under unbounded domain. Two examples of the

recovery theorem of Carr and Yu’s model on unbounded domain are investigated:

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the Black-Scholes model and the CIR model. The stationary distribution existence

condition is also checked for each model.

5.1 Boundary conditions of the numeraire port-

folio

In this section we discuss an important but often overlooked assumption, C8. We

argue that this assumption could be difficult to be satisfied in practice.

An important element in the derivation of Carr and Yu’s recovery model is the

use of the regular Sturm Liouville theorem to numerically solve eigenfunction and

eigenvalue problem (4.22) for the unique solution. The solution is then used to

deduce the solution of the numeraire portfolio and recover the real-world measure

P. However, in order to apply the regular Sturm Liouville theorem, one must have

the knowledge of the boundary conditions for the problem.

The knowledge of the boundary conditions is assumed in C8, which states that

the values of the numeraire portfolio L(x, t) and its partial derivative ∂∂xL(x, t) at

boundary values x = l and x = u are known ex-ante. Without this assumption, one

could only imply that the unique solution for the problem (4.22) exists, but would

not be able to solve for its solution, and therefore the knowledge of P cannot be

recovered.

While assuming the knowledge of the information required to apply the regular

Sturm Liouville theorem, Carr and Yu provided no practical method to obtain the

boundary conditions for the numeraire portfolio. In a typical calibration process, one

uses the prices of the derivative instruments to determine the information about the

risk-neutral measure Q, in Carr and Yu’s framework this is equivalent to knowing the

functions a(x), b(x) and r(x). But this does not imply that the boundary conditions

for the numeraire portfolio can be determined. After all, the numeraire portfolio is

a theoretical tool to derive the result of the recovery theorem, and the composition

of the numeraire portfolio is not explicitly known ex ante. In general, its value at

the boundaries could not be easily determined except for trivial cases.

This leads us to conclude that, without a general method of obtaining the bound-

ary conditions for the numeraire portfolio, the implementation of the recovery the-

orem of Carr and Yu’s model would be difficult in practice.

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5.2 Market completeness in Carr and Yu’s model

The discussion in this section focuses on the market completeness condition in Carr

and Yu’s model. While the condition is not explicitly assumed, we attempt to argue

that in general the market completeness condition is necessary for the model.

Recall that following assumptions were made in the model:

1. “No free lunch with vanishing risk” (NFLVR) (C3 (part i)),

2. The numeraire portfolio Lt is equal toS0t

Mt(C3 (part ii)),

3. The dynamics of Xt, including its coefficient a(x) and b(x), is known by cali-

bration (C5).

First consider the trivial case when n ≥ 1, i.e. There exists at least one risky

asset. According to the meta-theorem1, if there is only 1 randomness in the market

(originated from the driver Xt), the market is complete.

Now consider the case when n = 0, i.e. There is only a risk-free asset S0 in the

market. Since the randomness in the driver Xt cannot be hedged, the market is

incomplete. We will illustrate that under this scenario the recovery theorem may

fail.

Market incompleteness implies both Q and Mt = dQdP

∣∣Ft

not unique. Let the set

of possible Mt asM. Since there is only one asset S0 in the market, the only possible

self-financing portfolio is S0 itself. By Definition 4.1.1, the numeraire portfolio Lt is

a self-financing portfolio. Thus the only possible solution is Lt = S0t , corresponds to

S0t

S0t

= 1 = M1t ∈ M, i.e. P = Q1 ∈ Q. For Mt ∈ M : Mt 6= M1

t , the numeraire

portfolio Lt =S0t

Mtis not a self-financing portfolio.

However, a(x) and b(x) calibrated as in (C5) could correspond to any risk-neutral

probability measure Q2, which corresponds to M2t = dQ2

dP

∣∣∣Ft

. There is no guarantee

that Q2 = Q1, or equivalently M2t = M1

t = 1. If Q2 6= Q1, Lt is no longer a self-

financing portfolio, and the rest of the analysis will fail.

One possible remedy for this issue is to enforce the following assumption in the

model:

1A reference to this theorem is [3, p. 118].

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C3’ (part iii): The calibrated risk-neutral measure Q corresponds to the Mt

which makes Lt =S0t

Mta self-financing portfolio.

While it can resolve the issue highlighted above, this assumption is a rather

unusual and awkward. There is no obvious economics reason to guarantee that such

a condition would be satisfied. Unless further analysis provides the basis for such

an assumption, it should generally be avoided.

Therefore, we argue that the market completeness condition is necessary for the

model. Otherwise without this condition one have resort to unusual assumption

such as C3’ (part iii) to derive the recovery theorem.

To further expand this argument, one can consider a more general case when

Carr and Yu’s model is extended to a multivariate diffusion driver, i.e.

dX = b(Xt) +d∑j=1

aj(Xi)dWjt ,

where W jt are correlated Brownian motions for j = 1, . . . , d, and there are n

traded risky assets in the market.

If n < d, the market is incomplete by the meta-theorem. Again the risk-neutral

measure Q is not unique and one must consider the issue highlighted above.

5.3 Existence of stationary distribution

After reviewing the limitation of Carr and Yu’s model, we turn our attention to its

similarities with Ross’s model. In this section we attempt to argue for the existence

of the stationary distribution in Carr and Yu’s model. The argument in this section

is heuristic in nature, and technicalities of the proof have not been dealt with. We

refer interested readers to [13, Chapter 3] for the conditions that the existence of

the stationary distribution of Markov processes required. Attentive readers will also

notice the similarities between this argument and the recovery theorem of Carr and

Yu’s model in Section 2.22.

The intuition behind the existence condition is simple. Recalled that Carr and

Yu’s model is established under a bounded domain with a time-homogeneous driver

Xt. As Xt diffuses within the bounded domain [u, l], the process will either return to

2The argument in this section is based on a discussion with Pedro Vitoria.

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its original position or converge to a point in the domain. In either case the system

will exhibit an limiting behaviour and the distribution of Xt becomes ”stationary”.

We begin by introducing the transition density function:

Definition 5.3.1 (Transition density for the driver Xt)

The transition density for a diffusion process, f(t, x;T, y), is the density of the

probability distribution function for the stochastic process in that for any set A ⊂ R,

P(XT ∈ A|Xt = x) =

∫A

f(t, x;T, y)dy.

We focus on the transition density of the driver Xt under P, which is time-

homogeneous as shown in (4.14).

The driver Xt in Carr and Yu’s model as defined in (4.1.2):

dXt = b(Xt)dt+ a(Xt)dWt,

the transition density, f(x, t; y, T ), of Xt satisfies the Kolmogorov forward equa-

tion (KFE)3.

∂Tf(x, t; y, T ) +

∂y(b(y)f(x, t; y, T ))− 1

2

∂2

∂y2(a2(y)f(x, t; y, T )) = 0, (5.1)

together with the boundary conditions:∫ ∞−∞

f(x, t; y, T )dy = 1 and f(x, t; y, T ) ≥ 0.

As we only focus on the future time T and the future value y of Xt in the

argument, f(x, t; y, T ) is written as fx,t(y, T ).

A stationary distribution is a transition distribution which is independent of fu-

ture time T , which will be found below.

We try to find a solution f to (5.1) of a separable form:

fx,t(y, T ) = βx,t(T )αx,t(y).

Substitute into (5.1),

αx,t(y)∂βx,t(T )

∂T= −βx,t(t)

∂(b(y)αx,t(y))

∂y+ βx,t(T )

1

2

∂2(a2(y)αx,t(y))

∂y2.

Rearrange we get:

β′x,t(T )

βx,t(T )=

1

αx,t(y)

(− ∂

∂y(b(y)αx,t(y)) +

1

2

∂2

∂y2(a2(y)αx,t(y))

).

3A reference for Kolmogorov forward equation could be found in [8, p. 26].

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The two sides can only be equal if both are equal to a constant λ ∈ R,

For L.H.S.,β′x,t(T )

βx,t(T )= λ.

Solving this we have

βx,t(T ) = βx,t(0)eλT .

For R.H.S.,(− ∂

∂y(b(y)αx,t(y)) +

1

2

∂2

∂y2(a2(y)αx,t(y))

)= λαx,t(y).

Expand the expression:

a2(y)

2α′′x,t(y)+[2a(y)a′(y)−b(y)]α′x,t(y)+[a(y)a′′(y)+(a′(y))2−b′(y)]α(y) = λαx,t(y),

which can be written as self-adjoint form:

a2(y)

2c(y)

∂y

(c(y)

∂αx,t(y)

∂y

)− d(y)αx,t(x) = −λαx,t(y),

where

c(y) = − exp

(∫ y

l

2[2a(u)a′(u)− b(u)]

a2(u)du

), and

d(y) = a(y)a′′(y)− (a′(y))2 − b′(y).

Dividing the function a2(y)2c(y)

the problem becomes:

∂y

(c(y)

∂αx,t(y)

∂y

)− q(y)αx,t(y) = −λαx,t(y)w(y),

where

q(y) =2c(y)d(y)

a2(y), and

w(y) =2c(y)

a2(y).

Similar to the recovery theorem in Carr and Yu’s, the equation becomes a regular

Sturm Liouville problem (Appendix C).

The eigenvalues of the problem are denoted as:

λ1 < λ2 < · · · < λn < · · · → ∞,

and its corresponding eigenfunctions to be

π1(y), π2(y), π3(y), . . .

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Let

φ(y) = π1(y), and

ρ = λ1.

Since probability density is positive, of all the eigenfunctions only φ(y) is positive

and never changes sign. Hence φ(y) is the only valid eigenfunction to the problem,

and ρ is also the only valid eigenvalue.

Therefore the transition probability f must equal to:

fx,t(y, T ) = CeρTφ(y)

for some constant C which is independent of y and T .

Together with the boundary condition,∫ ∞−∞

fx,t(y, T )dy =

∫ ∞−∞

CeρTφ(y)dy = 1 for all T .

This implies:

C =1

eρT∫∞−∞ φ(y)dy

.

Therefore,

fx,t(y, T ) =φ(y)∫∞

−∞ φ(y)dy.

Therefore a transition density function f which is independent of future time T

has been deduced, i.e. It is the stationary probability distribution of the driver Xt.

However exploratory, the argument in this section has shed light on an impor-

tant property of Carr and Yu’s model: the existence of the stationary distribution.

Notice that the stationary distribution also exists in Ross’s model, which has been

proved in Section 3.2. In the next section we will explore the Carr and Yu’s model

unbounded domains, which will provide further evidence that the existence is a

necessary condition for the succeeding of the recovery theorem.

5.4 Recovery theorem on unbounded domain

So far, all the discussions of Carr and Yu’s model are established under a bounded

domain. As mentioned in Chapter 1, the extend that the recovery theorem is suc-

ceed in unbounded domain remains an open question. To provide insight on this

question, in this section we investigate two examples of the Carr and Yu’s model

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under unbounded domain: the Black-Scholes model and the CIR model. Part of

this section is based on [5].

We examine if the recovery theorem succeeds in these two examples and also if

the stationary distribution exists.

5.4.1 Black-Scholes model

The driver of the Black-Scholes model is the stock prices St, which follows a geomet-

ric Brownian motion SDE under the risk-neutral measure. For simplicity we assume

no dividend and zero interest rate.

dSt = σStdWQt with St ≥ 0, (5.2)

where σ is a constant and WQt is the Brownian motion under the risk-neutral

measure.

As geometric Brownian motion is not a bounded process, the standard analysis

in Carr and Yu’s model does not apply.

Substitute a2(x) = σ2x2, b(x) = r(x) = 0 into (4.21), we have the following:

σ2x2

2π′′(x) = −λπ(x) for all x ≥ 0, (5.3)

which is a eigenvalue and eigenfunction problem.

Theorem 5.4.1 (Solution set to eigenvalue and eigenfunction problem in

Black-Scholes model)

There are uncountably many eigenvalues λ and eigenfunctions π satisfy the problem

(5.3) with π(x) ≥ 0 for all x ≥ 0.

Proof. If π is assumed to be of the form π(x) = xm, then π′′(x) = m(m− 1)xm−2.

Substitute into (5.3),

σ2x2

2m(m− 1)xm−2 = −λxm

σ2m2 − σ2m+ 2λ = 0

m =σ2 ±

√σ4 − 8σ2λ

2σ2.

This problem has real solution m when

σ4 − 8σ2λ ≥ 0

λ ≤ 8

σ2,

which has infinite many solutions for λ.

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For each λ, the corresponding π is:

π(x) = xm with m =σ2 ±

√σ4 − 8σ2λ

2σ2,

which is positive for all x ≥ 0.

We can see that the real-world measure P can not be uniquely recovered here -

there are infinite many positive π, together with (4.17) implies the solution for the

numeraire portfolio is not unique. From Corollary 4.1.1, the market price of risk is

not unique, therefore the real-world measure cannot be uniquely recovered.

Theorem 5.4.2 (No stationary distribution exists in Black-Scholes model)

The stationary distribution does not exist in the Black-Scholes model.

Proof. The stationary distribution satisfies the stationary Kolmogorov forward equa-

tion:

− 1

2

∂2

∂S2(σ2S2f(S)) = 0, (5.4)

together with the boundary conditions:

f(S) ≥ 0 for all S ≥ 0 and

∫ ∞0

f(S)dS = 1.

Expand and reorganize (5.4),

S2f ′′(S) + 4Sf ′(S) + 2f(S) = 0.

Solving this equation one will get

f(S) =C1

S2+C2

S

for some constants C1 and C2.

Consider the second boundary condition:∫ ∞0

f(S)dS =

∫ ∞0

(C1

S2+C2

S

)dS.

However, this integral does not converge. Therefore the stationary distribution

does not exist.

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5.4.2 CIR process

The CIR process is defined as

drt = (µ− κrt)dt+ σ√rtdW

Qt with rt ≥ 0,

where µ, κ, and σ are positive constant and WQt is a Brownian motion under Q.

Substitute into (4.21) with a2(x) = σ2x, b(x) = µ − κx, r(x) = x, l = 0, and

u =∞:

σ2x

2π′′(x) + (µ− κx)π′(x)− xπ(x) = −λπ(x), x ∈ (0,∞), (5.5)

which again is an eigenvalue and eigenfunction problem. Notice that the eigen-

function solution to this problem must be positive for x ≥ 0.

Theorem 5.4.3 (Solution to eigenvalue and eigenfunction problem in CIR

model)

There exists a unique solution to the problem (5.5), in which the eigenfunction is

positive for x ≥ 0. All other eigenfunction to (5.5) switch sign at least once.4

Proof. According to [10], the spectrum of eigenvalues is discrete and known in closed

form, and can be organized as

λ1 < λ2 < · · · < λn < · · · → ∞.

The smallest eigenvalue is

λ1 =µ

σ2(γ − κ),

where

γ =√κ2 + 2σ2.

The corresponding eigenfunction:

π1(x) = exp

(−γ − κ

σ2x

),

is positive for x ≥ 0. All other eigenfunctions to (5.5) switch signs at least

once.

4This theorem and its proof are referenced to [5].

44

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Once the unique solution for π(x) is found, the rest is simple - the numeraire

portfolio Lt is equal to

L(x, t) = π1(x)ef(0)eλ1t,

and the rest of the analysis proceeds the same as we did in Section 4.2.

The following theorem shows that the stationary distribution exists in the CIR

process.

Theorem 5.4.4 (Stationary distribution exists in CIR model)

The distribution:

f(r) = Cr2µ−σ2

σ2 e−2κσ2r for all r ∈ R≥0.

is the stationary distribution in the CIR model, where

C =

(2κ

σ2

) 2µ

σ2 1

Γ(

2µσ2

) ,

and Γ is the gamma function

Γ(z) =

∫ ∞0

tz−1e−tdt.

Proof. The stationary distribution satisfies the stationary Kolmogorov forward equa-

tion:∂

∂r((µ− κr)f(r))− 1

2

∂2

∂r2(σ2rf(r)) = 0, (5.6)

together with the boundary conditions:

f(r) ≥ 0 for all r ≥ 0 and

∫ ∞0

f(r)dr = 1.

We will check the conditions one by one. First,

f ′(r) =2

σ2r

(µ− 1

2σ2 − κr

)f(r)

f ′′(r) =2

σ2r

(−1

r

(µ− 1

2σ2 − κr

)− κ+

2

σ2r

(σ − 1

2σ2 − κr

)2)f(r).

Now substitute these into L.H.S. of (5.6), it becomes

− κf(r)+(µ− κr)f ′(r)− σ2f ′(r)− 1

2σ2rf ′′(r)

= 0.

Second, it is obvious that:

f(r) ≥ 0 for all r ≥ 0.

45

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Lastly, ∫ ∞0

f(r)dr = C

∫ ∞0

r2µ−σ2

σ2 e−2κσ2rdr

= C

(σ2

) 2µ

σ2

Γ

(2µ

σ2

)= 1.

Following the discussion and analysis of the two models, in the next chapter we

will summarize the result and draw a comparison between the two recovery models

to conclude this thesis.

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Chapter 6

Conclusion and further research

In this thesis we have reviewed and clarified the assumptions of the recovery theorem

in Ross’s model and that in Carr and Yu’s model. We have also discussed a number

of properties of the two models, highlighting the limitations, similarities and other

features of the two recovery models. We have also considered the examples of Carr

and Yu’s model under unbounded domain.

For limitations of the models, we have discussed that the transition indepen-

dent pricing kernel does not follow from inter-temporal additive separable utility for

Ross’s model in Section 3.1, obtaining the boundary conditions for the numeraire

portfolio could be difficult in practice for Carr and Yu’s model in Section 5.1, and

market completeness condition is necessary Carr and Yu’s model in Section 5.2.

We have proved the existence of the stationary distribution for Ross’s model in

Section 3.2 and provided an heuristic argument for Carr and Yu’s model Section 5.3.

It is easy to notice the similarities between the argument for the existence of the

stationary distribution and deriving the recovery theorem in Ross’s model (using

the Perron Frobenius theorem) as well as in Carr and Yu’s model (using the regular

Sturm Liouville theorem).

Additionally, in Section 5.4, we reviewed that the recovery theorem of Carr

and Yu’s model succeeds in the CIR model but fails in the Black-Scholes model.

Interestingly, we also found that the stationary distribution exists only in the CIR

model but not in the Black-Scholes model, which has been also shown in the same

section.

These evidences lead us to postulate that the existence of the stationary distri-

bution is a necessary condition for the recovery theorem to succeed1. In other words,

in order to recover the real-world probability measure P from the risk-neutral prob-

ability measure Q, one must ensure that the stationary distribution exists in the

model being considered. This postulation, if valid, will be helpful in looking for the

1This idea was originally suggested by Dr. Samuel Cohen in a meeting.

47

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minimal assumption sets to the models. This postulation could also provide insight

into the extension of the models, such as market with multivariate drivers, drivers

under unbounded domain or incomplete market.

In their paper [4], Carr and Yu took a different track: based on the fact that reg-

ular Strum Liouville theorem ensures the discreteness and countability of the point

spectrum in bounded domain, they conjectured the countability of point spectrum

is a condition for the recovery theorem under an unbounded domain. They also

provided further evidence by showing that the point spectrum of the CIR model

was discrete and countable while that of the Black-Scholes model was continuous.

Based on these two conjectures, exploring the connections between the existence

of the stationary distribution and the countability of point spectrum could be a

direction of future research. For example, one can check the set of assumptions

required for each of the two conditions and the relationship between them. One

can also examine other unbounded or multivariate models to access to what extent

these two conditions are valid, and their relationships with succeeding of the recovery

theorem.

The results of our analysis also highlight the fact that the assumption sets in

the two recovery models are relatively restrictive, such as transition independence of

pricing kernel in Ross’s model and the time-homogeneous dynamics of the numeraire

portfolio in Carr and Yu’s model. In a real financial market, these assumptions may

not be justified or even be verified. Therefore, in addition to the extensions to

the recovery theorem, the research community can benefit from searching for a less

restrictive and more realistic assumption sets for the current recovery models.

On the other hand, our discussion has been confined to the theoretical aspect

of the recovery theory, but the practicability of the theory should be verified by

empirical evidences. In principle the recovery theory can be applied to a wide range

of financial markets, and to find out which product types and markets most suitable

for applying the theorem is a worthy research topic. In his paper [19], Ross used

the S & P 500 index to verify his model. This result could be treated as a starting

point for this line of research. One could also explore how to practically apply the

theory into areas like risk management and market prediction.

We conclude this thesis with the following table, which draws a comparison

between the two models to summarize the results in this thesis.

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49

Table 6.1: Comparison between the two recovery models

Item Ross’s model Carr and Yu’s model Remark

Setting Discrete time and state space. Continuous time and state space.Formulation Finite state irreducible Markov chain

(Section 3.2).Univariate diffusion process Xt on abounded domain.

Aim To recover the real-world transitionprobability matrix F from thestate-price matrix P .

To recover the dynamics of the driverXt under P from Q, deducing dP

dQ .

Marketcondition

No Arbitrage (R3). NFLVR and the numeraire portfolio

Lt is equal toS0t

Mt,

where S0t is the risk-free asset and

Mt = dQdP

∣∣Ft

(C3).

We argue for the necessity of marketcompleteness in Carr and Yu’smodel (Section 5.2).

Time homo-geneity

State-price function p and real-worldtransition density function f of thestate variable are time-homogeneous(R4).

The driver Xt is time-homogeneousunder Q (C4) and P(Theorem 4.2.1).

Calibration The state-price matrix P is known(R5), and the interest rate processrt can be deduced (Theorem 3.3.1).

Dynamics of the driver Xt under Qand the interest rate process rt areknown (C5).

Mainassumption

Pricing kernel ϕ is transitionindependent:ϕi,j =

pi,jfi,j

= δ h(i)h(j)

(R6).

1. Lt ≡ L(Xt, t),2. rt is time-homogeneous,3. Diffusion coefficient of thenumeraire portfolio, σt, istime-homogeneous (C6).

Despite suggested by Ross, weexplain that the transitionindependent pricing kernel does notfollow from inter-temporal additiveseparable utility function(Section 3.1).

Otherassumptions

P is non-negative and irreducible(R7).

1. Differentiability and continuityassumptions (C7),2. The boundary conditions for thenumeraire portfolio are known (C8).

We argue that C8 could be difficultto be satisfied in practice(Section 5.1).

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50

(Continued from previous page)

Item Ross’s model Carr and Yu’s model Remark

Derivation Given its separable form, thetransition independent pricing kernelequation is formulated as aneigenvalue and eigenvector problem,for which a unique solution exists(Theorem 2.2.1).

The market price of risk, Θt, is equalto σt (Corollary 4.1.1). Byseparation of variables, an identityfor σt is formulated as an eigenvalueand eigenfunction problem, forwhich a unique solution exists(Theorem 4.2.3).

Carr and Yu’s for unboundeddomain:1. the Black-Scholes model (recoverytheorem does not succeed),2. the CIR model (recovery theoremsucceeds)(Section 5.4).

Separationof variables

Pricing kernel can be separated fromreal-world probability:pi,j = ϕi,jfi,j = δ h(i)

h(j)fi,j

(Remark 2.2.1).

The numeraire portfolio can beseparated by a function of the driverand a function of time:L(x, t) = π(x)p(t) (Remark 4.2.1).

R6 and C6 guarantee the separationof variables in the respective models.

Maintheoremused

The Perron Frobenius theorem(Appendix A).

The regular Sturm Liouville theorem(Appendix C).

Stationarydistribution

Existence proved (Section 3.2). Heuristic argument for existence(Section 5.3).

Carr and Yu’s for unboundeddomain:1. the Black-Scholes model (notexists),2. the CIR model (exists)(Section 5.4).We postulate that the existence ofstationary distribution is a necessarycondition for the recovery theoremto succeed (Chapter 6).

Interest rateprocess

Time-homogeneous (Theorem 3.3.1). Time-homogeneous (C6 (part ii)).

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Bibliography

[1] D. Becherer. The numeraire portfolio for unbounded semimartingales. Finance

and Stochastics, 5:327–341, 2001.

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20:38–59, 2012.

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cial models. Finance and Stochastics, 11:447–493, 2007.

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[12] I. Karatzas and S. Shreve. Brownian Motion and Stochastic Calculus. Springer,

2nd edition, 1991.

[13] R. Khasminskii. Stochastic Stability of Differential Equations. Stochastic Mod-

elling and Applied Probability, Vol. 66. Springer, 1980.

[14] R. Korn and M. Schal. The numeraire portfolio in discrete time: existence,

related concepts and applications. In Advanced Financial Modelling, volume 8

of Radon Series on Computational and Applied Mathematics, page 303326. De

Gruyter, 2009.

[15] J. Long. The numeraire portfolio. Journal of Financial Economics, 26:29–69,

1990.

[16] C. Meyer. Matrix Analysis and Applied Linear Algebra. Society for Industrial

and Applied Mathematics, 2000.

[17] B. Øksendal. Stochastic Differential Equations: An Introduction with Applica-

tions. Universitext. Springer, 6th edition, 2003.

[18] S. Ross. Predicting the market. Annual Conference on General Equilibrium

and its Applications, April 2012.

[19] S. Ross. The recovery theorem. Journal of Finance, Forthcoming, 2013.

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Springer Finance Textbooks. Springer, 1st edition, 2004.

[21] Wikipedia. State prices — Wikipedia, the free encyclopedia, 2012. [Online;

accessed 3-April-2013].

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Appendices

53

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Appendix A

Perron Frobenius theorem

The Perron Frobenius theorem encompasses a number of related results about pos-

itive and irreducible matrices. In this appendix we focus on the theorem on irre-

ducible matrices, with the results that are useful in this thesis.

Definition A.0.1 (Spectral radius of a square matrix)

Let A be an n× n square matrix with real elements and with the set of eigenvalues

Λ = λ : Av = λv for some non-zero vector v . The spectral radius ρ(A) of A is

defined as:

ρ(A) = maxλ∈Λ|λ|.

Theorem A.0.5 (Perron Frobenius theorem for irreducible matrices)

Let A be an n× n irreducible matrix with real elements with ρ(A) = r, then

1. r is positive and it is an eigenvalue of the matrix A,

2. The entries of eigenvector v associated with eigenvalue r are all positive,

3. Eigenvalue r is simple, i.e. v is unique up to a positive scaling,

4. All of the other eigenvectors are not strictly positive, i.e. There are zero and

negative elements in the vectors, and

5. r is between minimum sum of row and maximum sum of row of A (inclusive),

i.e.

mini

∑j

ai,j ≤ r ≤ maxi

∑j

ai,j. (A.1)

r is called the Perron root and v is called the Perron vector.

Proof. A reference and the detailed proof of statement 1 to 4 of this theorem can be

found on [16, p. 673: Perron Frobenius Theorem]. As for statement 5, the inequality

A.1 can be proved by:

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1. applying Collatz-Wielandt formula [16, p. 666] by setting x as a vector of

(1, 1, . . . , 1) to get the L.H.S. mini∑

j ai,j ≤ r, and

2. applying Gerschgorin Circles [16, p. 498] to get the R.H.S. r ≤ maxi∑

j ai,j.

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Appendix B

Numeraire portfolio

In this appendix we first introduce the numeraire portfolio and provide background

and references on the topic. After that a statement mentioned in the Section 4.1 is

proved: if the market is complete then numeraire portfolio, Lt, is equal toS0t

Mt, where

S0t is the risk-free asset and Mt is the Radon-Nikodym derivative dQ

dP

∣∣Ft

.

The notion of the numeraire portfolio was first introduced by Long [15] in 1990.

The discrete time version of the numeraire portfolio, as in Long’s paper, is defined

as the following:

Definition B.0.2 (Numeraire portfolio (discrete time))

A numeraire portfolio Nt in discrete time economy is defined as a self-financing

portfolio with always positive value such that, for each asset j,

P jt

Nt

= E

[P jt+1

Nt+1

|Ft

]for all 0 ≤ t ≤ T with probability one,

where P jt is the price process of the asset j, and E denotes the expectation under

the real-world measure. (The definition here is simplified with the assumption that

there is no dividend.)

Long showed that the numeraire portfolio exists in a discrete time economy if

and only if there are no profit opportunities ([15, Theorem 1]). In addition, he

showed that the expected excess return of the numeraire portfolio is its the variance

of its rate of return. ([15, Theorem 3])

In fact the numeraire portfolio can be also obtained from the growth optimal

portfolio (GOP) which maximizes the expected utility of a log utility function. A

reference of this is [14].

The continuous time version of the numeraire portfolio, as described in [1], is the

following:

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Definition B.0.3 (The numeraire portfolio (continuous time))

A numeraire portfolio Nt is a strictly positive self-financing portfolio, such that PtNt

is a supermartingale for all strictly positive self-financing portfolio, Pt under the

real-world measure.1

Karatzas and Kardaras [11] proved that “No unbounded profit with bounded

risk” (NUPBR) is sufficient to ensure the existence of the numeraire portfolio. This

condition is weaker than the usual ”No free lunch with vanishing risk” (NFLVR) [6]

as usually seen in financial literatures.

However, the existence of the numeraire portfolio does not automatically imply

that it is equal toS0t

Mt, as shown in the example in Section 5.2. However, in a com-

plete market with ”No Free Lunch with Vanishing Risk” (NFLVR), this is always

the case, as it will be shown below.

Definition B.0.4 (Self-financing portfolio)

A portfolio (φ0t , φ

1t , . . . , φ

nt ) is self-financing if

dVt =n∑i=0

φitdSit .

where

Vt =n∑i=0

φitSit ,

Lemma B.0.1 (Self-financing portfolio identity)

A portfolio (φ0t , φ

1t . . . , φ

nt ) with value Vt =

∑ni=0 φ

itS

it is self-financing if and only if

dVt =n∑i=1

φitdSit ,

where Yt = Yt/S0t denotes the discounted value of trading strategy or asset price

process.

Proof. By the definition of self-financing portfolio,

dVt =n∑i=0

φitdSit .

1Although the supermartingale condition is used in the referenced paper, in this thesis we usethe stricter definition used in Carr and Yu’s paper: Pt

Ntis a (local) martingale.

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By Ito’s formula, for all i = 1, 2, . . . , n

dSit =1

S0t

dSi,t −Sit

(S0t )

2dS0

t

dSitS0t

= dSit +Sit

(S0t )

2dS0

t .

Consider dVt,

dVt =1

S0t

dVt −Vt

(S0t )

2dS0

t

=1

S0t

n∑i=0

φitdSit −

Vt(S0

t )2dS0

t

= φ0t

dS0t

S0t

+n∑i=1

φit

(dSit +

Sit(S0

t )2dS0

t

)− Vt

(S0t )

2dS0

t

=n∑i=1

φitdSit +

n∑i=0

φitSit

(S0t )

2dS0

t −Vt

(S0t )

2dS0

t

=n∑i=1

φitdSit .

Theorem B.0.6 (Numeraire portfolio in complete market)

If the market is complete with NFLVR, then the numeraire portfolio exists and

Lt ≡S0t

Mt

. (B.1)

Proof. First, we show that Sit/Lt is a local martingale under P-measure for all i =

0, 1, . . . , n, Pt.

By the Fundamental Theorem of Asset Pricing [6], there exists a unique equiv-

alent local martingale measure (ELMM) Q such that (Si/S0)t is a local martingale

for all i = 0, 1, . . . , n under Q, i.e. for each i = 0, 1, . . . , n, there exists a sequence of

stopping times τm →∞ almost surely such that:

EQ[

(SiT )τm

(SiT )τm|Ft]

=(Sit)

τm

(Sit)τm, t ∈ [0, T ], i = 0, 1, . . . , n (B.2)

for all m. (The notation P τmt denotes the stopped process Pmin(t,τm).)

Consider the following expression:

EP[M τm

T

M τmt

(SiT )τm

(S0T )τm|Ft]

=1

M τmt

EP[M τm

T

(SiT )τm

(S0T )τm|Ft]

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(Split the expression into τm > t and τm ≤ t)

= 1τm>t1

M τmt

EP[M τm

T

(SiT )τm

(S0T )τm|Ft]

+ 1τm≤t1

M τmt

EP[M τm

T

(SiT )τm

(S0T )τm|Ft]

(On the first term, since MT is a martingale, we can write it as an expection of MT condi-tioned on time t)

= 1τm>t1

M τmt

EP[EP [MT |Fmin(τm,T )

] (SiT )τm

(S0T )τm|Ft]

+ 1τm≤t1

M τmt

EP[M τm

T

(SiT )τm

(S0T )τm|Ft]

= 1τm>t1

M τmt

EP[EP[MT

(SiT )τm

(S0T )τm|Fmin(τm,T )

]|Ft]

+ 1τm≤t1

M τmt

EP[M τm

T

(SiT )τm

(S0T )τm|Ft]

(From Tower property of conditional expectation, the first term is expressed as a singleexpectation.)

= 1τm>t1

M τmt

EP[MT

(SiT )τm

(S0T )τm|Ft]

+ 1τm≤t1

M τmt

EP[M τm

T

(SiT )τm

(S0T )τm|Ft]

(Expectation changed to Q using Generalized Bayes’ Theorem [12])

= 1τm>tEQ[

(SiT )τm

(S0T )τm|Ft]

+ 1τm≤tEQ[

(SiT )τm

(S0T )τm|Ft]

(Combined the two terms into one)

= EQ[

(SiT )τm

(S0T )τm|Ft]

(Using (B.2))

=(SiT )τm

(S0T )τm

. (B.3)

Hence

EP[

(SiT )τm

LτmT|Ft]

= EP[M τm

t

M τmt

(SiT )τm

(S0T )τm/M τm

T

|Ft]

= M τmt EP

[M τm

T

M τmt

(SiT )τm

(S0T )τm|Ft]

(Using (B.3))

= M τmt

(SiT )τm

(S0T )τm

=(SiT )τm

Lτmt.

Second, we show that Lt is a self-financing portfolio.

Since the Radon-Nikodym derivative Mt = dQdP

∣∣Ft

is a F-martingale, 1Mt

= dPdQ

∣∣∣Ft

is a Q-martingale.

Now consider

d

(L

S0

)t

= d

(S0/M

S0

)t

= d

(1

M

)t

.

This implies (L/S0)t is a martingale.

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Under Q, S0t is a martingale for all i. By Martingale representation Theorem,

d

(L

S0

)t

= dLt =n∑i=1

φi,tdS0t .

From this one can apply Lemma B.0.1 to show Lt is a self-financing portfolio.

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Appendix C

Regular Sturm Liouville theorem

In Section 4.2, the result of the regular Sturm Liouville theorem has been used to

prove the existence and the uniqueness of solution for the eigenfunction and eigen-

value problem (4.22). This step is crucial to deduce the solution of the numeraire

portfolio and recover the real-world measure P. In this appendix we state the main

result of the regular Sturm Liouville theorem and provides reference for it.

Theorem C.0.7 (Regular Sturm Liouville theorem)

A Sturm-Liouville equation is a second-order homogenous linear differential equation

of the following form:

d

dx

(p(x)

dy(x)

dx

)− q(x)y(x) = −λρ(x)y(x),

where p(x) and ρ(x) are positive functions, and p(x), p′(x), q(x), ρ(x) are con-

tinuous functions over a finite interval [a, b]. Also, the boundary conditions are of

the form:

α1y(a) + α2y′(a) = 0 α2

1 + α22 > 0, and

β1y(b) + β2y′(b) = 0 β2

1 + β22 > 0.

Then

1. The set of eigenvalues λ = λ1, λ2, . . . are real and discrete, with

λ1 < λ2 < · · · < λn <→∞.

2. Corresponding to each eigenvalue λn, there is an eigenfunction yn(x) which

has exactly n− 1 zeros in (l, u), and is uniquely determined up to a constant factor.

In particular, y1(x) has no zeros in (a, b) and can be taken to be positive.

3. All of the eigenfunctions and eigenvalues can be numeraically solved.

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Proof. A reference for this is [2, p. 320 Theorem 5], which contains the proof and

detailed explanation of the theorem.

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Appendix D

Markov chain

In Section 3.2, Ross’ model is reformulated as a finite state time-homogeneous

Markov chain. In this section we provide the relevant definitions and theorems

for completeness.

Definition D.0.5 (Markov chain and its transition probability)

A finite state Markov chain is a sequence of random variables X1, X2, X3, . . . with

values from finite state space S, and satisfies the Markov property, i.e.

P(Xn+1 = x|X1 = x1, X2 = x2, . . . , Xn = xn) = P(Xn+1 = x|Xn = xn),

where P denotes a probability measure.

The transition probability function of a Markov chain, p : Π× Π× N+ → [0, 1],

is defined as the probability

pi,j(n) = P(Xn = j|Xn−1 = i),

where N+ denotes the set of positive integers.

Definition D.0.6 (Time-homogeneity of a Markov chain)

A finite state Markov chain is time-homogeneous if it satisfies the following condition:

P(Xn+1 = i|Xn = j) = P(Xn = i|Xn−1 = j) for all i, j ∈ Π and n ∈ N+.

In other words, a Markov chain is time-homogeneous if its transition probability

function does not depend on time.

If a finite state Markov chain is time-homogeneous, one can define its transition

probability matrix as:

P =

p1,1 p1,2 · · · p1,M

p2,1 p2,2 · · · p2,M...

.... . .

...pM,1 pM,2 · · · pM,M

,

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where M is the number of states in S.

Definition D.0.7 (Irreducibility of a Markov chain)

The irreducibility of a Markov chain can be defined through the following:

1. A state j is said to be accessible from a state i (written as i→ j) if a system

started in state i has a non-zero probability of transitioning into state j at

some point.

2. A state i is said to communicate with state j if both i→ j and j → i.

3. A set of states C is a communicating class if every pair of states in C commu-

nicates with each other.

4. A Markov chain is said to be irreducible if its state space is a single commu-

nicating class.

As the name suggested, the irreducibility of a Markov chain and the irreducibility

of its transition probability matrix are equivalent, which is proved in the following

theorem.

Theorem D.0.8 (Irreducibility of Markov chain and transition probability

matrix)

If a finite state Markov chain is time-homogeneous, then the irreducibility of the

Markov chain is equivalent to the irreducibility of its transition probability matrix

(as defined in Definition 2.1.5).

Proof. It is easier to prove the opposite: the reducibility of the Markov chain is

equivalent to the reducibility of its transition probability matrix.

⇒ )

If the Markov chain is reducible, then there exists two sets of communicating

classes C1 and C2 such that states i1, i2, . . . , iu in C1 does not communicate with

states j1, j2, . . . , jv in C2.

Consider the transition probability matrix (A)i,j = ai,j of the Markov chain, we

have:

aiα,jβ = 0

for α = 1, 2, . . . , u and β = 1, 2, . . . , v.

Therefore the transition probability matrix is reducible.

⇐ )

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If the transition probability matrix (A)i,j = ai,j is reducible, then the indices

1, 2, . . . , n can be divided into two disjoint non-empty sets i1, i2, . . . , iu and j1, j2, . . . , jv,

with u+ v = n, such that

aiα,jβ = 0

for α = 1, 2, . . . , u and β = 1, 2, . . . , v.

Obviously the states in C1 = i1, i2, . . . , iu and C2 = j1, j2, . . . , jv are not commu-

nicating, since the probability of transition between the two sets is zero. Therefore

the Markov chain is reducible.

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