statistical physics and the “problem of firm growth” dongfeng fu advisor: h. e. stanley k....

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Statistical Physics and the “Problem of Firm Growth” Dongfeng Fu Advisor: H. E. Stanley K. Yamasaki, K. Matia, S. V. Buldyrev, DF Fu, F. Pammolli, K. Matia, M. Riccaboni, H. E. Stanley, 74, PRE 035103 (2006). . Pammolli, S. V. Buldyrev, K. Matia, M. Riccaboni, K. Yamasaki, H. E. Stanl 01 (2005) . S. V. Buldyrev, M. A. Salinger, and H. E. Stanley, PRE 74, 036118 (2006). Collaborato rs:

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Page 1: Statistical Physics and the “Problem of Firm Growth” Dongfeng Fu Advisor: H. E. Stanley K. Yamasaki, K. Matia, S. V. Buldyrev, DF Fu, F. Pammolli, K. Matia,

Statistical Physics and the “Problem of Firm Growth”

Dongfeng FuAdvisor: H. E. Stanley

K. Yamasaki, K. Matia, S. V. Buldyrev, DF Fu, F. Pammolli, K. Matia, M. Riccaboni, H. E. Stanley, 74, PRE 035103 (2006).

DF Fu, F. Pammolli, S. V. Buldyrev, K. Matia, M. Riccaboni, K. Yamasaki, H. E. Stanley 102, PNAS 18801 (2005) .

DF. Fu, S. V. Buldyrev, M. A. Salinger, and H. E. Stanley, PRE 74, 036118 (2006).

Collaborators:

Page 2: Statistical Physics and the “Problem of Firm Growth” Dongfeng Fu Advisor: H. E. Stanley K. Yamasaki, K. Matia, S. V. Buldyrev, DF Fu, F. Pammolli, K. Matia,

Motivation

Firm growth problem quantifying size changes of firms.

1) Firm growth problem is an unsolved problem in economics.

2) Statistical physics may help us to develop better strategies to improve economy.

3) Help people to invest by quantifying risk.

Page 3: Statistical Physics and the “Problem of Firm Growth” Dongfeng Fu Advisor: H. E. Stanley K. Yamasaki, K. Matia, S. V. Buldyrev, DF Fu, F. Pammolli, K. Matia,

Outline

1) Introduction of “classical firm growth problem”.

2) The empirical results of the probability density function of growth rate.

3) A generalized preferential-attachment model.

Page 4: Statistical Physics and the “Problem of Firm Growth” Dongfeng Fu Advisor: H. E. Stanley K. Yamasaki, K. Matia, S. V. Buldyrev, DF Fu, F. Pammolli, K. Matia,

Classical Problem of Firm Growth

t/year1 2 10

5

12log

)(

)1(log

tS

tSg

Firm growth rate:

Firm at time = 1

S = 5

Firm at time = 2

S = 12

Firm at time = 10

S = 33

Question: What is probability density function of growth rate P(g)?

Page 5: Statistical Physics and the “Problem of Firm Growth” Dongfeng Fu Advisor: H. E. Stanley K. Yamasaki, K. Matia, S. V. Buldyrev, DF Fu, F. Pammolli, K. Matia,

Classic Gibrat Law & Its Implication

Traditional View: Gibrat law of “Proportionate Effect” (1930)

S(t+1) = S(t) * t ( t is noise).

Growth rate g in t years

=

logS(t)

= logS(0) + log(t’ )t’=1

M

S(0)

S(t)log

M

t’=1= log(t’)

Gibrat: pdf of g is Gaussian.

Growth rate, g

Pro

babi

lity

den

sity

pdf(g) 2

2g

e

Gaussian

P(g) really Gaussian ?

Page 6: Statistical Physics and the “Problem of Firm Growth” Dongfeng Fu Advisor: H. E. Stanley K. Yamasaki, K. Matia, S. V. Buldyrev, DF Fu, F. Pammolli, K. Matia,

Databases Analyzed for P(g)

1. Country GDP: yearly GDP of 195 countries, 1960-2004.

2. American Manufacturing Companies: yearly sales of 23,896 U.S. publicly traded firms, based on Security Exchange Commission filings 1973-2004.

3. Pharmaceutical Industry: quarterly sales figures of 7184 firms in 21 countries (mainly in north America and European Union) covering 189,303 products in 1994-2004.

Page 7: Statistical Physics and the “Problem of Firm Growth” Dongfeng Fu Advisor: H. E. Stanley K. Yamasaki, K. Matia, S. V. Buldyrev, DF Fu, F. Pammolli, K. Matia,

Empirical Results for P(g) (all 3 databases)

Growth rate, g

PD

F,

P(g

)

Not Gaussian !

i.e. Not parabola

Traditional Gibrat view is NOT able to accurately predict P(g)!

Page 8: Statistical Physics and the “Problem of Firm Growth” Dongfeng Fu Advisor: H. E. Stanley K. Yamasaki, K. Matia, S. V. Buldyrev, DF Fu, F. Pammolli, K. Matia,

The New Model: Entry & Exit of Products and firms

Preferential attachment to add new product or delete old product

Rules:

b: birth prob. of a firm.

birth prob. of a prod.

death prob. of a prod.

( > )

New:

New: 1. Number n of products in a firm 2. size of product

Page 9: Statistical Physics and the “Problem of Firm Growth” Dongfeng Fu Advisor: H. E. Stanley K. Yamasaki, K. Matia, S. V. Buldyrev, DF Fu, F. Pammolli, K. Matia,

1. At time t, each firm has n(t) products of size i(t), i=1,2,…n(t),

where n and >0 are independent random variables that follow

the distributions P(n) and P(), respectively.

2. At time t+1, the size of each product increases or decreases by a

random factor i(t+1) = (t)i * i.

n

ii

n

ii

t

t

tS

tSg

1

1

)(

)1(log

)(

)1(log

Assume P() = LN(m,V), and P() = LN(m,V). LN Log-Normal.

“Multiplicative” Growth of Products

Hence:

Page 10: Statistical Physics and the “Problem of Firm Growth” Dongfeng Fu Advisor: H. E. Stanley K. Yamasaki, K. Matia, S. V. Buldyrev, DF Fu, F. Pammolli, K. Matia,

for large n. Vg = f(V, V)

= Variance

P(g|n) ~ Gaussian(m+V/2, Vg/n)

The shape of P(g) comes from the fact that P(g|n) is Gaussian but the convolution with P(n).

Growth rate, g

P(g

| n)

1

)|()()(n

ngPnPgPIdea:

How to understand the shape of P(g)

Page 11: Statistical Physics and the “Problem of Firm Growth” Dongfeng Fu Advisor: H. E. Stanley K. Yamasaki, K. Matia, S. V. Buldyrev, DF Fu, F. Pammolli, K. Matia,

Distribution of the Number of ProductsP

roba

bili

ty d

istr

ibut

ion,

P(n

)

Number of products in a firm, n

Pharmaceutical Industry Database

1.14

Page 12: Statistical Physics and the “Problem of Firm Growth” Dongfeng Fu Advisor: H. E. Stanley K. Yamasaki, K. Matia, S. V. Buldyrev, DF Fu, F. Pammolli, K. Matia,

1. for small g, P(g) exp[- |g| (2 / Vg)1/2].

2. for large g, P(g) ~ g-3 .

Characteristics of P(g)

Growth rate, g

P(g

)

222 )2|(|2

2)(

gg

g

VggVg

VgP

Our Fitting Function

P(g) has a crossover from exponential to power-law

Page 13: Statistical Physics and the “Problem of Firm Growth” Dongfeng Fu Advisor: H. E. Stanley K. Yamasaki, K. Matia, S. V. Buldyrev, DF Fu, F. Pammolli, K. Matia,

Our Prediction vs Empirical Data I

Scaled growth rate, (g – g) / Vg1/2

Sca

led

PD

F,

P(g

) V

g1/2

GDPPhar. Firm / 102

Manuf. Firm / 104

One Parameter: Vg

Page 14: Statistical Physics and the “Problem of Firm Growth” Dongfeng Fu Advisor: H. E. Stanley K. Yamasaki, K. Matia, S. V. Buldyrev, DF Fu, F. Pammolli, K. Matia,

Our Prediction vs Empirical Data IICentral & Tail Parts of P(g)

Central part is Laplace.

Scaled growth rate, (g – g) / Vg1/2

Sca

led

PD

F, P

(g)

Vg1/2

Tail part is power-law with exponent -3.

Page 15: Statistical Physics and the “Problem of Firm Growth” Dongfeng Fu Advisor: H. E. Stanley K. Yamasaki, K. Matia, S. V. Buldyrev, DF Fu, F. Pammolli, K. Matia,

Universality w.r.t Different Countries

Scaled growth rate, (g – g) / Vg1/2

Sca

led

PD

F, P

g(g)

Vg1/

2

Growth rate, g

PD

F, P

g(g)

Original pharmaceutical data Scaled data

Take-home-message: China/India same as developed countries.

Page 16: Statistical Physics and the “Problem of Firm Growth” Dongfeng Fu Advisor: H. E. Stanley K. Yamasaki, K. Matia, S. V. Buldyrev, DF Fu, F. Pammolli, K. Matia,

Conclusions

1. P(g) is tent-shaped (exponential) in the central part and power-law with exponent -3 in tails.

2. Our new preferential attachment model accurately reproduced the empirical behavior of P(g).

Page 17: Statistical Physics and the “Problem of Firm Growth” Dongfeng Fu Advisor: H. E. Stanley K. Yamasaki, K. Matia, S. V. Buldyrev, DF Fu, F. Pammolli, K. Matia,

Scaled growth rate, (g – g) / Vg1/2

Sca

led

PD

F, P

(g)

Vg1/2

Our Prediction vs Empirical Data III

Page 18: Statistical Physics and the “Problem of Firm Growth” Dongfeng Fu Advisor: H. E. Stanley K. Yamasaki, K. Matia, S. V. Buldyrev, DF Fu, F. Pammolli, K. Matia,

),()(

)(),1()(

1),1(

)(

1),(tnP

tn

ntnP

tn

ntnP

tn

n

t

tnP

Master equation:

Math for Entry & Exit

Case 1: entry/exit, but no growth of products.

n(t) = n(0) + (- + b) t

Initial conditions: n(0) 0, b 0.

Page 19: Statistical Physics and the “Problem of Firm Growth” Dongfeng Fu Advisor: H. E. Stanley K. Yamasaki, K. Matia, S. V. Buldyrev, DF Fu, F. Pammolli, K. Matia,

),()(

)(),1()(

1),1(

)(

1),(tnP

tn

ntnP

tn

ntnP

tn

n

t

tnP

Master equation:

Math for Entry & Exit

Solution:

Pold(n) exp(- A n)

Pnew(n)

)()0(

)()0(

)0()( nP

btn

btnP

btn

nnP newold

)()]/(2[ nfn b

Case 1: entry/exit, but no growth of units.

n(t) = n(0) + (- + b) t

Initial conditions: n(0) 0, b 0.

Page 20: Statistical Physics and the “Problem of Firm Growth” Dongfeng Fu Advisor: H. E. Stanley K. Yamasaki, K. Matia, S. V. Buldyrev, DF Fu, F. Pammolli, K. Matia,
Page 21: Statistical Physics and the “Problem of Firm Growth” Dongfeng Fu Advisor: H. E. Stanley K. Yamasaki, K. Matia, S. V. Buldyrev, DF Fu, F. Pammolli, K. Matia,

Different Levels

Class

A Country

A industry

A firm

Units

Industries

Firms

Products

is composed of

is composed of

is composed of

Page 22: Statistical Physics and the “Problem of Firm Growth” Dongfeng Fu Advisor: H. E. Stanley K. Yamasaki, K. Matia, S. V. Buldyrev, DF Fu, F. Pammolli, K. Matia,

The Shape of P(n)

Number of products in a firm, n

PD

F, P

(n)

b=0 P(n) is exponential.

b0, n(0)=0 P(n) is power law.

P(n) = Pold(n) + Pnew(n).

P(n) observed is due to initial condition: b0, n(0)0.

(b=0.1, n(0)=10000, t=0.4M)

Number of products in a firm, n

Page 23: Statistical Physics and the “Problem of Firm Growth” Dongfeng Fu Advisor: H. E. Stanley K. Yamasaki, K. Matia, S. V. Buldyrev, DF Fu, F. Pammolli, K. Matia,

P(g) from Pold(n) or Pnew(n) is same

222 )2|(|2

2)(

gg

g

VggVg

VgP

2/3

2

2

)(1

2

)(

2

1)(

g

V

tn

V

tngP

gg(1)

(2)

Based on Pold(n):

Based on Pnew(n):

Growth rate, g

P(g

)

Page 24: Statistical Physics and the “Problem of Firm Growth” Dongfeng Fu Advisor: H. E. Stanley K. Yamasaki, K. Matia, S. V. Buldyrev, DF Fu, F. Pammolli, K. Matia,

Statistical Growth of a Sample Firm

Firm size S = 5

Firm size S = 33

t/year1 2 10

Firm size S = 12

3=1

1=2

3 products:

2=2

n = 3

2=11=4

3=5

4=2

7=5

3=5

6=4

1=6

4=1

2=2

5=10

n = 4

n = 7

L.A.N. Amaral, et al, PRL, 80 (1998)

Page 25: Statistical Physics and the “Problem of Firm Growth” Dongfeng Fu Advisor: H. E. Stanley K. Yamasaki, K. Matia, S. V. Buldyrev, DF Fu, F. Pammolli, K. Matia,

Number and size of products in each firm change with time.

What we do

Pharmaceutical Industry Database

Pro

babi

lity

dis

trib

utio

n

The number of product in a firm, n

Traditional view is

To build a new model to reproduce empirical results of P(g).

Page 26: Statistical Physics and the “Problem of Firm Growth” Dongfeng Fu Advisor: H. E. Stanley K. Yamasaki, K. Matia, S. V. Buldyrev, DF Fu, F. Pammolli, K. Matia,
Page 27: Statistical Physics and the “Problem of Firm Growth” Dongfeng Fu Advisor: H. E. Stanley K. Yamasaki, K. Matia, S. V. Buldyrev, DF Fu, F. Pammolli, K. Matia,

Average Value of Growth Rate

S, Firm Size

Mea

n G

row

th R

ate

Page 28: Statistical Physics and the “Problem of Firm Growth” Dongfeng Fu Advisor: H. E. Stanley K. Yamasaki, K. Matia, S. V. Buldyrev, DF Fu, F. Pammolli, K. Matia,

Size-Variance Relationship

S, Firm Size

g|

S)

Page 29: Statistical Physics and the “Problem of Firm Growth” Dongfeng Fu Advisor: H. E. Stanley K. Yamasaki, K. Matia, S. V. Buldyrev, DF Fu, F. Pammolli, K. Matia,

Simulation on

S, Firm Size

(g|

S)

Page 30: Statistical Physics and the “Problem of Firm Growth” Dongfeng Fu Advisor: H. E. Stanley K. Yamasaki, K. Matia, S. V. Buldyrev, DF Fu, F. Pammolli, K. Matia,

Other Findings

S, firm sale

E(

|S),

exp

ecte

d

S, firm saleE

(N|S

), e

xpec

ted

N

Page 31: Statistical Physics and the “Problem of Firm Growth” Dongfeng Fu Advisor: H. E. Stanley K. Yamasaki, K. Matia, S. V. Buldyrev, DF Fu, F. Pammolli, K. Matia,
Page 32: Statistical Physics and the “Problem of Firm Growth” Dongfeng Fu Advisor: H. E. Stanley K. Yamasaki, K. Matia, S. V. Buldyrev, DF Fu, F. Pammolli, K. Matia,

Mean-field Solution

noldt0

t

nold nnew

nnew(t0, t)

Page 33: Statistical Physics and the “Problem of Firm Growth” Dongfeng Fu Advisor: H. E. Stanley K. Yamasaki, K. Matia, S. V. Buldyrev, DF Fu, F. Pammolli, K. Matia,

The Complete ModelRules:1. At t=0, there exist N classes with n units.2. At each step: a. with birth probability b, a new class is born b. with , a randomly selected class grows one unit in size based on “preferential attachment”. c. with a randomly selected class shrinks one unit in size based on “preferential dettachment”.

),,()(

)(),,1()(

1),,1(

)(

1),,(tnnP

tn

nttnP

tn

nttnP

tn

n

t

ttnPiii

i

Master equation:

Solution:

21),( IItnP )exp(1 nI

)]/(2[2

bnI

Page 34: Statistical Physics and the “Problem of Firm Growth” Dongfeng Fu Advisor: H. E. Stanley K. Yamasaki, K. Matia, S. V. Buldyrev, DF Fu, F. Pammolli, K. Matia,

Effect of b on P(n)

Simulation

The number of units, n

The

dis

trib

utio

n,

P(n

)

Page 35: Statistical Physics and the “Problem of Firm Growth” Dongfeng Fu Advisor: H. E. Stanley K. Yamasaki, K. Matia, S. V. Buldyrev, DF Fu, F. Pammolli, K. Matia,

The Size-Variance Relation

Page 36: Statistical Physics and the “Problem of Firm Growth” Dongfeng Fu Advisor: H. E. Stanley K. Yamasaki, K. Matia, S. V. Buldyrev, DF Fu, F. Pammolli, K. Matia,

),,()(

)(),,1()(

1),,1(

)(

1),,(tnnP

tn

nttnP

tn

nttnP

tn

n

t

ttnPiii

i

Master equation:

Solution:

)]/(2[2

bnI

Math for 1st Set of Assumption

)()0(

)()0(

)0()( nP

btN

btnP

btN

NnP newold

Pold(n) exp[- n / nold(t)]

Pnew(n) n -[2 + b/(1-b)] f(n)

Page 37: Statistical Physics and the “Problem of Firm Growth” Dongfeng Fu Advisor: H. E. Stanley K. Yamasaki, K. Matia, S. V. Buldyrev, DF Fu, F. Pammolli, K. Matia,

Math for 1st Set of Assumption

tn

tnbb

dt

tdn newnew

)0(

)()1(

)(

tn

tnb

dt

tdn oldold

)0(

)()1(

)(

nold(t) = [n(0)+t]1-b n(0)b

(1)

(2)

Initial condition:

nold(0)=n(0)

Solution:

nnew(t0, t) = [n(0)+t]1-b[n(0)+t0]b

)0(/)()( Ntntn oldold bb

new tntnttn 10

10 ])0(/[])0([),(

Page 38: Statistical Physics and the “Problem of Firm Growth” Dongfeng Fu Advisor: H. E. Stanley K. Yamasaki, K. Matia, S. V. Buldyrev, DF Fu, F. Pammolli, K. Matia,

Math Continued

)()0(

)()0(

)0()( nP

btN

btnP

btN

NnP newold

))(

exp()(

1)(

tn

n

tnnP

Pold(n) exp[- n / nold(t)]

Pnew(n) n -[2 + b/(1-b)] f(n)

Solution:

When t is large, Pold(n) converges to exponential distribution

Page 39: Statistical Physics and the “Problem of Firm Growth” Dongfeng Fu Advisor: H. E. Stanley K. Yamasaki, K. Matia, S. V. Buldyrev, DF Fu, F. Pammolli, K. Matia,

1

)|()()(n

gg ngPnPgP

]2/)(exp[2

)|( 2g

g

g VnggV

nngP

y

bg

bg dnnVngdyyygP .)2/exp()exp()(

)1

1

2

1(

2

0

1

1

Math for 2nd Set of Assumption

Idea:

222 )2|(|2

2)(

gg

gg

VggVg

VgP

2/3

2

2

)(1

2

)(

2

1)(

g

V

tn

V

tngP

ggg (3)

(4)

(5)(b 0)

for large n.

From Pold(n):

From Pnew(n):

Page 40: Statistical Physics and the “Problem of Firm Growth” Dongfeng Fu Advisor: H. E. Stanley K. Yamasaki, K. Matia, S. V. Buldyrev, DF Fu, F. Pammolli, K. Matia,
Page 41: Statistical Physics and the “Problem of Firm Growth” Dongfeng Fu Advisor: H. E. Stanley K. Yamasaki, K. Matia, S. V. Buldyrev, DF Fu, F. Pammolli, K. Matia,

Empirical Observations (before 1999)

g(S) ~ S- , 0.2

S, Firm size

Sta

ndar

d de

viat

ion

of g

Small Medium Large

g, growth rate

Small firms Medium firms Large firms

Reality: it is “tent-shaped”! P

roba

bili

ty d

ensi

ty Empirical

pdf(g|S) ~)(

||

S

g

e

Michael H. Stanley, et.al. Nature 379, 804-806 (1996). V. Plerou, et.al. Nature 400, 433-437 (1999).

Page 42: Statistical Physics and the “Problem of Firm Growth” Dongfeng Fu Advisor: H. E. Stanley K. Yamasaki, K. Matia, S. V. Buldyrev, DF Fu, F. Pammolli, K. Matia,

PHID

Page 43: Statistical Physics and the “Problem of Firm Growth” Dongfeng Fu Advisor: H. E. Stanley K. Yamasaki, K. Matia, S. V. Buldyrev, DF Fu, F. Pammolli, K. Matia,

Current Status on the Models of Firm Growth

Models

IssuesGibrat Simon Sutton Bouchaud Amaral

p(N) is power law

p(S) is log-normal

p() is log-normal

(S) ~ S- = 0.5 = 0.22 depends 0.17

p(g|S) is “tent”

p(|S) & scaling

p(N|S) & scaling

Page 44: Statistical Physics and the “Problem of Firm Growth” Dongfeng Fu Advisor: H. E. Stanley K. Yamasaki, K. Matia, S. V. Buldyrev, DF Fu, F. Pammolli, K. Matia,

The Models to Explain Some Empirical Findings

Sutton’s Model

Simon's Model explains the distribution of the division number is power law.

Based on partition theory

2(S) =1/3(12 +12+ 12) + 1/3(12 + 22) + 1/3(32) = 17/3

1 1 1

1 2

3

S = 32(g) = 2(S/S) = 2(S)/S2 = 0.63 ~ S-2

= -ln(0.63)/2ln(3) = 0.21

The probability of growing by a new division is proportional to the division number in the firm. Preferential attachment.

The distribution of division number is power law.

3 firms industry

Page 45: Statistical Physics and the “Problem of Firm Growth” Dongfeng Fu Advisor: H. E. Stanley K. Yamasaki, K. Matia, S. V. Buldyrev, DF Fu, F. Pammolli, K. Matia,

Bouchaud's Model:

)()())()(1

(1

K

j

iiiji

ttttKdt

d

assuming follows power-law distribution:

1)(

op

Firm S evolves like this:

Conclusion:

2

1

21 1.

2.

3.

25.0

0 1

Page 46: Statistical Physics and the “Problem of Firm Growth” Dongfeng Fu Advisor: H. E. Stanley K. Yamasaki, K. Matia, S. V. Buldyrev, DF Fu, F. Pammolli, K. Matia,

The Distribution of Division Number N

N, Division Number

p(N

) , P

roba

bili

ty D

ensi

ty

PHID

Page 47: Statistical Physics and the “Problem of Firm Growth” Dongfeng Fu Advisor: H. E. Stanley K. Yamasaki, K. Matia, S. V. Buldyrev, DF Fu, F. Pammolli, K. Matia,

Example Data (3 years time series)

A1 0 3 4

A2 2 1 2

B1 0 10 1

B2 11 4 7

B3 5 6 7

Firm S N

A 2 1 2

B 16 2 11, 5

In the 1st year:

S g log(S(t+1)/S(t))

2 log(4/2)

4 log(6/4)

16 log(20/16)

20 log(15/20)

S N

2 1

16 2

S

2 2

16 11

16 5

A, B are firms. A1, A2 are divisions of firm A; B1, B2, B3 are divisions of firm B.

Page 48: Statistical Physics and the “Problem of Firm Growth” Dongfeng Fu Advisor: H. E. Stanley K. Yamasaki, K. Matia, S. V. Buldyrev, DF Fu, F. Pammolli, K. Matia,

Predictions of Amaral at al model

Scaled division size , /S

Sca

led

pdf()

, p(

)*S

1(|S) ~ S- f1(/S) 2(N|S) ~ S

- f2(N/S)

Scaled division number , N/S

Sca

led

pdf(

N),

p(N

)*S

Page 49: Statistical Physics and the “Problem of Firm Growth” Dongfeng Fu Advisor: H. E. Stanley K. Yamasaki, K. Matia, S. V. Buldyrev, DF Fu, F. Pammolli, K. Matia,