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Separating internal and external dynamics of complex systems Marcio Argollo de Menezes Albert-László Barabási
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Scale-free: P(k) ≈ k - Hierarchical: C(k) ≈ k - Small World:
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Networks support dynamical processes
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Understand the dynamical processes that take place on networks. Inspiration: real data WWW Internet Metabolic networks Social network maps Network dynamics: diversity of the observed behavior, rather than any degree of universality. Beyond topology M. Argollo de Menezes and A.-L. Barabási, Phys. Rev. Lett. 92, 028701 (2004). Our approach: identify and study simultaneously dynamical variables f i (t) on different regions/nodes of the system
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Internet f i (t)=number of bytes passing through router i at time t. 347 routers t max =2 days (5 minutes resolution)
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World Wide Web f i (t) = number of visits to web site i on day t 3000 web sites. Daily visitation for a 30 day period
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Highways f i (t)=traffic at a given point of a road i on day t. Daily traffic on 127 roads of the Colorado highway network from 1998 to 2001.
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Computer chip f i (t)=state of a given logic component i at clock cycle t. 462 signal carriers 8,862 clock cycles.
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1)For each node i: 2) Create a scatter plot:
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Scaling of fluctuations i ~ = 1/2 = 1
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1) Start with an arbitrary network (SF/SW or ER). A simple diffusion model 3) Let each walker perform N steps. 2) Place W walkers on randomly selected nodes. 4) Record for each node i the number of visitations f i i 5) Repeat (2-4) T times, generating for each node i a series f i (1), f i (2), … f i (T). i ≈ 1/2 = 1/2
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The origin of =1/2 Random connections: decoupling of nodes What about =1? After walkers perform N steps:
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Internal fluctuations Randomness of the particle arrival or diffusion process External fluctuations Fluctuations of the number of agents/particles Two sources of fluctuations
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1) Start with an arbitrary network (SF/SW or ER). Introducing external fluctuations 3) Each walker performs N steps. 2) Place W walkers on randomly selected nodes. 4) Record for each node i the total visitation f i 5) Repeat (2-4) T times, generating for each node f i (1), f i (2), … f i (T). Let the number of walkers fluctuate: W(t)= + (t) = 0, = ( W) 1/2 tt’ W: magnitude of external fluctuations i ≈ = 1 For large W
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The origin of =1 Random connections: decoupling of nodes After walkers perform N steps:
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W large External fluctuations dominate (large W large): =1 www, highways W=0 Small external fluctuations (small W): =1/2 Internet, chip Summary B. Huberman et al., Science 280, 95 (1998).
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Separating external and internal fluctuations External perturbations affect nodes differently. A i : node i’s share of the total traffic: f i ext (t)=A i F(t), where F(t)= i f i (t): total flux on the network at time t f i int (t) = f i (t) - f i ext (t) Model with sinusoidal external signal W(t)=W 0 + W sin( t) large W small W
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Fluctuation ratios and the exponent From f i ext (t) and f i int (t) calculate i ext and i int for each node i. i = i ext / i int : ratio between external and internal fluctuations. P( i ): quantifies the impact of external fluctuations. =1/2 =1 =1/2
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Scaling of fluctuations and the exponent From f i ext (t) and f i int (t) measure, i ext and, i int =1/2 Internal dynamics dominate i int > i ext =1 External dynamics dominate i int ~ i ext
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Measuring electric activity on the brain EEG: local voltage differences in the brain neural activity. Time resolved activity measured simultaneously in 64 regions in the head. (i=1..64; t=1..256) Two different systems: Alcoholic vs. non-alcoholic person Alcoholics: deficit ininhibition (hyperexcitability) in the central nervous system. (Alcohool Clin. Exp. Res. vol. 25, 330-337, 2001). Higher excitability stronger internal dynamics Smaller i ext / i int ratios
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-empirical data: two universality classes -modeling data: =1/2: internal dyamics = 1: externally driven dyamics -separating internal/external components: =1/2: Internet, chip: internal fluctuations dominate = 1 : www, highways: external fluctuations dominate Are the exponents universal? =1 is, the =1/2 perhaps not. Conclusions Monitor the simultaneous dynamics of numerous nodes = Obtain more information about the system.
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