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CUUS2079-04 CUUS2079-Zafarani 978 1 107 01885 3 January 13, 2014 16:54
90 Network ModelsWe also havenlim→∞(
n− 1
d)
=nlim→∞(n−1)!
(n− 1 −d)!d!=nlim→∞((n−1)×(n−2)×···(n−d))(n− 1 −d)!
(n− 1 −d)!d!=nlim→∞((n−1)×(n−2)×···(n−d))
d!≈(n−1)d
d!. (4.10)
We can compute the degree distribution of random graphs in the limit
by substituting Equations4.10,4.9, and4.4in Equation4.8,nlim→∞P(dv=d)=nlim→∞(
n− 1
d)
pd(1−p)n−^1 −d=
(n−1)d
d!(
c
n− 1)d
e−c=e−ccd
d!, (4.11)
which is basically thePoisson distributionwith meanc. Thus, in the limit,
random graphs generate Poisson degree distribution, which differs from the
power-law degree distribution observed in real-world networks.Clustering CoefficientProposition 4.6.In a random graph generated by G(n,p), the expected
local clustering coefficient for nodevis p.Proof.The local clustering coefficient for nodevisC(v)=number of connected pairs ofv’s neighbors
number of pairs ofv’s neighbors. (4.12)
However,vcan have different degrees depending on the edges that are
formed randomly. Thus, we can compute the expected value forC(v):E(C(v))=∑n−^1d= 0E(C(v)|dv=d)P(dv=d). (4.13)