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H3 Game Theory Session 11

SMU H3 Game Theory Session 11 Notes

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Wrapping Up

Independent Private Values Auctions

Second Price Auction

First Price Auction

E[max(v2,v3,...,vn)  v1>max(v2,v3,...,vn)]E[\max(v_2, v_3, ..., v_n) \space | \space v_1 > \max(v_2, v_3, ..., v_n)]

Random Variables

E[Xxv]=1F(v)avxf(x)dx=1F(v)avxdF(x)E[X | x \le v] = \frac{1}{F(v)} \int_a^v x f(x) dx = \frac{1}{F(v)} \int_a^v x dF(x)

Common and Known Values Auctions

First Price Auction

All Pay Auction

F(x)=x1n1,s.t. x[0,1]F(x) = x^{\frac{1}{n}-1}, \quad \text{s.t. } x \in [0, 1]

War of Attrition (Second-Price All-Pay Auction)

Definition

Solution

F1(x)=1eα2x,F2(x)=1eα1xF_1(x) = 1-e^{-\alpha_2x}, \quad F_2(x) = 1-e^{-\alpha_1x}

Setup

P1 indifference condition

Case 1

Case 2

E(π1)=0x(v1y)f2(y)dyWin Case+0x(x)(1F2(x))Loss CaseE(\pi_1) = \underbrace{\int_0^x (v_1 - y) f_2(y)dy}_{\text{Win Case}} + \underbrace{\vphantom{\int_0^x}(-x)(1-F_2(x))}_{\text{Loss Case}}

Applying the indifference condition

E(π1)=0x(v1y)f2(y)dyx(1F2(x))E(\pi_1) = \int_0^x (v_1 - y) f_2(y)dy - x(1-F_2(x)) E(π1)=v10xf2(y)dy0xyf2(y)dyx(1F2(x))E(\pi_1) = v_1 \int_0^x f_2(y)dy - \int_0^x y f_2(y)dy - x(1-F_2(x)) E(π1)=v1F2(x)0xyf2(y)dyx(1F2(x))E(\pi_1) = v_1 F_2(x) - \int_0^x yf_2(y)dy - x(1-F_2(x)) xE(π1)=v1f2(x)xf2(x)[(1F2(x))+x(f2(x))]=0\frac{\partial}{\partial x} E(\pi_1) = v_1 f_2(x) - x f_2(x) - \left[(1-F_2(x)) + x(-f_2(x))\right] = 0 v1f2(x)xf2(x)1+F2(x)+xf2(x)=0v_1 f_2(x) - x f_2(x) - 1 + F_2(x) + x f_2(x) = 0 v1f2(x)=1F2(x)v_1 f_2(x) = 1-F_2(x) F2(x)1F2(x)=1v1\frac{F_2'(x)}{1-F_2(x)} = \frac{1}{v_1} xln(1F2(x))=F2(x)1F2(x)\frac{\partial}{\partial x}\ln(1-F_2(x)) = -\frac{F_2'(x)}{1-F_2(x)} xln(1F2(x))=1v1=α1\frac{\partial}{\partial x}\ln(1-F_2(x)) = -\frac{1}{v_1} = -\alpha_1

Integration and boundary conditions

axtln(1F2(t))dt=axα1dt\int_a^x \frac{\partial}{\partial t}\ln(1-F_2(t))dt = \int_a^x -\alpha_1 dt ln(1F2(x))ln(1F2(a))=α1(xa)\ln(1-F_2(x)) - \ln(1-F_2(a)) = -\alpha_1(x-a) ln(1F2(x))=α1(xa)\ln(1-F_2(x)) = -\alpha_1(x-a) 1F2(x)=eα1(xa)1-F_2(x) = e^{-\alpha_1(x-a)} F2(x)=1eα1(xa)F_2(x) = 1-e^{-\alpha_1(x-a)}

Finding aa and bb

E(π1)=v1F2(a)0ayf2(y)dya(1F2(a))=0E(\pi_1) = v_1F_2(a)-\int_0^a yf_2(y)dy-a(1-F_2(a)) = 0 00ayf2(y)dya=00-\int_0^a yf_2(y)dy-a = 0 F2(x)=1eα1xF_2(x) = 1-e^{-\alpha_1 x} F1(x)=1eα2xF_1(x) = 1-e^{-\alpha_2 x}

P2 indifference condition

Remarks

0xf1(x)dx<0xf2(x)dx\int_0^\infty xf_1(x)dx < \int_0^\infty xf_2(x)dx v2<v1v_2 < v_1 P(P1 wins)=v2v1+v2=0f1(x)F2(x)dxP(\text{P1 wins}) = \frac{v_2}{v_1+v_2} = \int_0^\infty f_1(x)F_2(x)dx

First Price Common Value Auction with Independent Values

Setup

Solution

b(v)=vb(v) = v

Verify

0<v2<b0 < v_2 < bb<v2<100b < v_2 < 100
π>0\pi > 0π<0\pi < 0
E(π)=0b(v1+v2b)f(v2)dv2E(\pi) = \int_0^b(v_1+v_2-b)f(v_2)dv_2 E(π)=11000b(v1+v2b)dv2E(\pi) = \frac{1}{100} \int_0^b(v_1+v_2-b)dv_2 E(π)=1100[v2(v1b)]0b+1100(v222)0bE(\pi) = \frac{1}{100}\bigg[ v_2(v_1-b) \bigg]^b_0 + \frac{1}{100}\bigg( \frac{v_2^2}{2} \bigg)^b_0 E(π)=1200[2b(v1b)+b2]=1200 b(2v1b)E(\pi) = \frac{1}{200}\bigg[ 2b(v_1 - b) + b^2 \bigg] = \frac{1}{200}\space b( 2v_1 - b ) E(π)=1200 b(b2v1)E(\pi) = -\frac{1}{200}\space b( b - 2v_1 )

Second Price Common Value Auction

Solution

b(v1)=2v1b(v_1) = 2v_1

Verify

π=v1+v22v2\pi = v_1 + v_2 - 2v_2
0<v2<b20 < v_2 < \frac{b}{2}b2<v2<100\frac{b}{2} < v_2 < 100
π>0\pi > 0π<0\pi < 0
f(v2)=1100f(v_2) = \frac{1}{100} E(π)=0b2(v1v2)f(v2)dv2E(\pi) = \int_0^\frac{b}{2} (v_1-v_2)f(v_2)dv_2 E(π)=11000b2(v1v2)dv2E(\pi) = \frac{1}{100}\int_0^\frac{b}{2}(v_1-v_2)dv_2 E(π)=1100[v1v2v222]0b2E(\pi) = \frac{1}{100} \bigg[ v_1v_2 - \frac{v_2^2}{2} \bigg]_0^\frac{b}{2} E(π)=1100(v1b2b28)E(\pi) = \frac{1}{100} \bigg( \frac{v_1b}{2} - \frac{b^2}{8} \bigg) E(π)=b100(v12b8)E(\pi) = \frac{b}{100} \bigg( \frac{v_1}{2} - \frac{b}{8} \bigg) E(π)=1800 b(4v1b)E(\pi) = \frac{1}{800} \space b( 4v_1 - b )
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