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| === Barabási–Albert (BA) 优先链接模型 === | | === Barabási–Albert (BA) 优先链接模型 === |
| + | The [[Barabási–Albert model]] is a random network model used to demonstrate a preferential attachment or a "rich-get-richer" effect. In this model, an edge is most likely to attach to nodes with higher degrees.The network begins with an initial network of ''m''<sub>0</sub> nodes. ''m''<sub>0</sub> ≥ 2 and the degree of each node in the initial network should be at least 1, otherwise it will always remain disconnected from the rest of the network. |
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| [[BA模型]]是一个随机网络模型,用于说明偏好依附效应(优先链接)preferential attachment或“富人越富”效应。 在这个模型中,边最有可能附着在度数较高的节点上。 这个网络从一个 ''m''<sub>0</sub>节点的初始网络开始。 ''m''<sub>0</sub> ≥ 2,初始网络中每个节点的度至少为 1,否则它将始终与网络的其余部分断开。 | | [[BA模型]]是一个随机网络模型,用于说明偏好依附效应(优先链接)preferential attachment或“富人越富”效应。 在这个模型中,边最有可能附着在度数较高的节点上。 这个网络从一个 ''m''<sub>0</sub>节点的初始网络开始。 ''m''<sub>0</sub> ≥ 2,初始网络中每个节点的度至少为 1,否则它将始终与网络的其余部分断开。 |
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| + | In the BA model, new nodes are added to the network one at a time. Each new node is connected to <math>m</math> existing nodes with a probability that is proportional to the number of links that the existing nodes already have. Formally, the probability ''p''<sub>''i''</sub> that the new node is connected to node ''i'' is<ref name=RMP>{{Cite journal |
| + | |url = http://www.nd.edu/~networks/Publication%20Categories/03%20Journal%20Articles/Physics/StatisticalMechanics_Rev%20of%20Modern%20Physics%2074,%2047%20(2002).pdf |
| + | |author1 = R. Albert |
| + | |author2 = A.-L. Barabási |
| + | |title = Statistical mechanics of complex networks |
| + | |journal = [[Reviews of Modern Physics]] |
| + | |volume = 74 |
| + | |issue = 1 |
| + | |pages = 47–97 |
| + | |year = 2002 |
| + | |doi = 10.1103/RevModPhys.74.47 |
| + | |bibcode = 2002RvMP...74...47A |
| + | |arxiv = cond-mat/0106096 |
| + | |url-status = dead |
| + | |archiveurl = https://web.archive.org/web/20150824235818/http://www3.nd.edu/~networks/Publication%20Categories/03%20Journal%20Articles/Physics/StatisticalMechanics_Rev%20of%20Modern%20Physics%2074,%2047%20(2002).pdf |
| + | |archivedate = 2015-08-24 |
| + | |citeseerx = 10.1.1.242.4753 |
| + | }}</ref> |
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| + | : <math>p_i = \frac{k_i}{\sum_j k_j},</math> |
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| + | where ''k''<sub>''i''</sub> is the degree of node ''i''. Heavily linked nodes ("hubs") tend to quickly accumulate even more links, while nodes with only a few links are unlikely to be chosen as the destination for a new link. The new nodes have a "preference" to attach themselves to the already heavily linked nodes. |
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| + | [[File:Barabasi-albert model degree distribution.svg|thumb|The degree distribution of the BA Model, which follows a power law. In loglog scale the power law function is a straight line.<ref name=Barabasi1999>{{Cite journal |
| + | |url = http://www.nd.edu/~networks/Publication%20Categories/03%20Journal%20Articles/Physics/EmergenceRandom_Science%20286,%20509-512%20(1999).pdf |
| + | |author = [[Albert-László Barabási]] & [[Réka Albert]] |
| + | |title = Emergence of scaling in random networks |
| + | |journal = [[Science (journal)|Science]] |
| + | |volume = 286 |
| + | |pages = 509–512 |
| + | |date = October 1999 |
| + | |doi = 10.1126/science.286.5439.509 |
| + | |issue = 5439 |
| + | |pmid = 10521342 |
| + | |arxiv = cond-mat/9910332 |
| + | |bibcode = 1999Sci...286..509B |
| + | |url-status = dead |
| + | |archiveurl = https://web.archive.org/web/20120417112354/http://www.nd.edu/~networks/Publication%20Categories/03%20Journal%20Articles/Physics/EmergenceRandom_Science%20286,%20509-512%20(1999).pdf |
| + | |archivedate = 2012-04-17 |
| + | }}</ref>]] |
| + | The degree distribution resulting from the BA model is scale free, in particular, it is a power law of the form: |
| + | : <math>P(k)\sim k^{-3} \, </math> |
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| 在BA模型中,每次向网络中添加一个新节点。每个新节点和已有的<math>m</math>个节点相连接,连接的概率正比于每个已存在节点当前的度。形式上,新节点与节点''i''相连的概率''p''<sub>''i''</sub>为<ref name=RMP>{{Cite journal | | 在BA模型中,每次向网络中添加一个新节点。每个新节点和已有的<math>m</math>个节点相连接,连接的概率正比于每个已存在节点当前的度。形式上,新节点与节点''i''相连的概率''p''<sub>''i''</sub>为<ref name=RMP>{{Cite journal |
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| BA模型得到的度分布是无标度的,特别是它的形式是幂律: | | BA模型得到的度分布是无标度的,特别是它的形式是幂律: |
| : <math>P(k)\sim k^{-3} \, </math> | | : <math>P(k)\sim k^{-3} \, </math> |
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| + | Hubs exhibit high betweenness centrality which allows short paths to exist between nodes. As a result, the BA model tends to have very short average path lengths. The clustering coefficient of this model also tends to 0. |
| + | While the diameter, D, of many models including the Erdős Rényi random graph model and several small world networks is proportional to log N, the BA model exhibits D~loglogN (ultrasmall world).<ref>{{cite journal|last=Cohen|first=R. |title=Scale-free networks are ultrasmall|journal=Phys. Rev. Lett.|year=2003|volume=90|pages=058701|url=http://havlin.biu.ac.il/Publications.php?keyword=Scale-free+networks+are+ultrasmall&year=*&match=all|doi=10.1103/PhysRevLett.90.058701|pmid=12633404|first2=S.|last2=Havlin|issue=5|bibcode=2003PhRvL..90e8701C |arxiv=cond-mat/0205476}}</ref> |
| + | Note that the average path length scales with N as the diameter. |
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| 中心节点表现出很高的介数中心性,这使得节点之间存在捷径。因此,BA模型的平均路径长度往往很短。该模型的聚类系数也趋于0。 | | 中心节点表现出很高的介数中心性,这使得节点之间存在捷径。因此,BA模型的平均路径长度往往很短。该模型的聚类系数也趋于0。 |