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===Spectral expansion===
===Spectral expansion===
When {{mvar|G}} is [[regular graph|{{mvar|d}}-regular]], a [[linear algebra]]ic definition of expansion is possible based on the [[Eigenvalue#Eigenvalues of matrices|eigenvalues]] of the [[adjacency matrix]] {{math|1=''A'' = ''A''(''G'')}} of {{mvar|G}}, where {{mvar|A{{sub|ij}}}} is the number of edges between vertices {{mvar|i}} and {{mvar|j}}.<ref>cf. Section 2.3 in {{harvtxt|Hoory|Linial|Wigderson|2006}}</ref> Because {{mvar|A}} is [[symmetric matrix|symmetric]], the [[spectral theorem]] implies that {{mvar|A}} has {{mvar|n}} real-valued eigenvalues {{math|λ{{sub|1}} ≥ λ{{sub|2}} ≥ … ≥ λ{{sub|''n''}}}}. It is known that all these eigenvalues are in {{math|[−''d'', ''d'']}} and more specifically, it is known that {{math|1=λ{{sub|''n''}} = −''d''}} if and only if {{mvar|G}} is bipartite.
When {{mvar|G}} is [[regular graph|{{mvar|d}}-regular]], a [[linear algebra]]ic definition of expansion is possible based on the [[Eigenvalue#Eigenvalues of matrices|eigenvalues]] of the [[adjacency matrix]] {{math|1=''A'' = ''A''(''G'')}} of {{mvar|G}}, where {{mvar|A{{sub|ij}}}} is the number of edges between vertices {{mvar|i}} and {{mvar|j}}.<ref>cf. Section 2.3 in {{harvtxt|Hoory|Linial|Wigderson|2006}}</ref> Because {{mvar|A}} is [[symmetric matrix|symmetric]], the [[spectral theorem]] implies that {{mvar|A}} has {{mvar|n}} real-valued eigenvalues {{math|''λ''{{sub|1}} ≥ ''λ''{{sub|2}} ≥ … ≥ ''λ''{{sub|''n''}}}}. It is known that all these eigenvalues are in {{math|[−''d'', ''d'']}} and more specifically, it is known that {{math|1=''λ''{{sub|''n''}} = −''d''}} if and only if {{mvar|G}} is bipartite.


More formally, we refer to an {{mvar|n}}-vertex, {{mvar|d}}-regular graph with
More formally, we refer to an {{mvar|n}}-vertex, {{mvar|d}}-regular graph with
:<math>\max_{i \neq 1}|\lambda_i| \leq \lambda</math>
:<math>\max_{i \neq 1}|\lambda_i| \leq \lambda</math>
as an {{math|(''n'', ''d'', λ)}}-''graph''. The bound given by an {{math|(''n'', ''d'', λ)}}-graph on {{math|λ{{sub|''i''}}}} for {{math|''i'' ≠ 1}} is useful many contexts, including the [[expander mixing lemma]].
as an {{math|(''n'', ''d'', ''λ'')}}-''graph''. The bound given by an {{math|(''n'', ''d'', ''λ'')}}-graph on {{math|''λ''{{sub|''i''}}}} for {{math|''i'' ≠ 1}} is useful many contexts, including the [[expander mixing lemma]].


Spectral expansion can be two-sided, as above, with <math>\max_{i \neq 1}|\lambda_i| \leq \lambda</math>, or it can be one-sided, with <math>\max_{i \neq 1}\lambda_i \leq \lambda</math>. The latter is a weaker notion that holds also for bipartite graphs and is still useful for many applications, such as the Alon-Chung lemma.<ref>N. Alon and F. R. K. Chung, Explicit construction of linear sized tolerant networks. Discrete Math., vol. 72, pp. 15-19, 1988.</ref>
Spectral expansion can be ''two-sided'', as above, with <math>\max_{i \neq 1}|\lambda_i| \leq \lambda</math>, or it can be ''one-sided'', with <math>\max_{i \neq 1}\lambda_i \leq \lambda</math>. The latter is a weaker notion that holds also for bipartite graphs and is still useful for many applications, such as the Alon–Chung lemma.<ref>N. Alon and F. R. K. Chung, Explicit construction of linear sized tolerant networks. Discrete Math., vol. 72, pp. 15–19, 1988.</ref>


Because {{mvar|G}} is regular, the uniform distribution <math>u\in\R^n</math> with {{math|1=''u{{sub|i}}'' = {{frac|1|''n''}}}} for all {{math|1=''i'' = 1, …, ''n''}} is the [[stationary distribution]] of {{mvar|G}}. That is, we have {{math|1=''Au'' = ''du''}}, and {{mvar|u}} is an [[eigenvector]] of {{mvar|A}} with eigenvalue {{math|1=λ{{sub|1}} = ''d''}}, where {{mvar|d}} is the [[degree (graph theory)|degree]] of the vertices of {{mvar|G}}. The ''[[spectral gap]]'' of {{mvar|G}} is defined to be {{math|''d'' − λ{{sub|2}}}}, and it measures the spectral expansion of the graph {{mvar|G}}.<ref>This definition of the spectral gap is from Section 2.3 in {{harvtxt|Hoory|Linial|Wigderson|2006}}</ref>
Because {{mvar|G}} is regular, the uniform distribution <math>u\in\R^n</math> with {{math|1=''u{{sub|i}}'' = {{frac|1|''n''}}}} for all {{math|1=''i'' = 1, …, ''n''}} is the [[stationary distribution]] of {{mvar|G}}. That is, we have {{math|1=''Au'' = ''du''}}, and {{mvar|u}} is an [[eigenvector]] of {{mvar|A}} with eigenvalue {{math|1=''λ''{{sub|1}} = ''d''}}, where {{mvar|d}} is the [[degree (graph theory)|degree]] of the vertices of {{mvar|G}}. The ''[[spectral gap]]'' of {{mvar|G}} is defined to be {{math|''d'' − ''λ''{{sub|2}}}}, and it measures the spectral expansion of the graph {{mvar|G}}.<ref>This definition of the spectral gap is from Section 2.3 in {{harvtxt|Hoory|Linial|Wigderson|2006}}</ref>


If we set
If we set
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===Cheeger inequalities===
===Cheeger inequalities===
When {{mvar|G}} is {{mvar|d}}-regular, meaning each vertex is of degree {{mvar|d}}, there is a relationship between the isoperimetric constant {{math|''h''(''G'')}} and the gap {{math|''d'' − λ{{sub|2}}}} in the spectrum of the adjacency operator of {{mvar|G}}. By standard spectral graph theory, the trivial eigenvalue of the adjacency operator of a {{mvar|d}}-regular graph is {{math|1=λ{{sub|1}} = ''d''}} and the first non-trivial eigenvalue is {{math|λ{{sub|2}}}}. If {{mvar|G}} is connected, then {{math|λ{{sub|2}} < ''d''}}. An inequality due to Dodziuk{{Sfn|Dodziuk|1984}} and independently [[Noga Alon|Alon]] and [[Vitali Milman|Milman]]{{Sfn|Alon|Spencer|2011}} states that<ref>Theorem 2.4 in {{harvtxt|Hoory|Linial|Wigderson|2006}}</ref>
When {{mvar|G}} is {{mvar|d}}-regular, meaning each vertex is of degree {{mvar|d}}, there is a relationship between the isoperimetric constant {{math|''h''(''G'')}} and the gap {{math|''d'' − ''λ''{{sub|2}}}} in the spectrum of the adjacency operator of {{mvar|G}}. By standard spectral graph theory, the trivial eigenvalue of the adjacency operator of a {{mvar|d}}-regular graph is {{math|1=''λ''{{sub|1}} = ''d''}} and the first non-trivial eigenvalue is {{math|''λ''{{sub|2}}}}. If {{mvar|G}} is connected, then {{math|''λ''{{sub|2}} < ''d''}}. An inequality due to Dodziuk{{Sfn|Dodziuk|1984}} and independently [[Noga Alon|Alon]] and [[Vitali Milman|Milman]]{{Sfn|Alon|Spencer|2011}} states that<ref>Theorem 2.4 in {{harvtxt|Hoory|Linial|Wigderson|2006}}</ref>
: <math>\tfrac{1}{2}(d - \lambda_2) \le h(G) \le \sqrt{2d(d - \lambda_2)}.</math>
: <math>\tfrac{1}{2}(d - \lambda_2) \le h(G) \le \sqrt{2d(d - \lambda_2)}.</math>
In fact, the lower bound is tight. The lower bound is achieved in limit for the [[Hypercube graph|hypercube]] {{mvar|Q{{sub|n}}}}, where {{math|1=''h''(''G'') = 1}} and {{math|1=''d'' – λ = 2}}. The upper bound is (asymptotically) achieved for a cycle, where {{math|1=''H''(''C{{sub|n}}'') = 4/''n''= Θ(1/''n'')}} and {{math|1=''d'' – λ = 2-2cos(2<math>\pi</math>/''n'') ≈ (2<math>\pi</math>/''n'')^2= Θ(1/''n''{{sup|2}})}}.<ref name="Hoory 2006"/> A better bound is given in <ref>B. Mohar. Isoperimetric numbers of graphs. J. Combin. Theory Ser. B, 47(3):274–291,
In fact, the lower bound is tight. The lower bound is achieved in limit for the [[Hypercube graph|hypercube]] {{mvar|Q{{sub|n}}}}, where {{math|1=''h''(''G'') = 1}} and {{math|1=''d'' – ''λ''{{sub|2}} = 2}}. The upper bound is (asymptotically) achieved for a cycle, where {{math|1=''h''(''C{{sub|n}}'') = 4/''n'' = Θ(1/''n'')}} and {{math|1=''d'' – ''λ''{{sub|2}} = 22cos(2<math>\pi</math>/''n'') ≈ (2<math>\pi</math>/''n''){{sup|2}} = Θ(1/''n''{{sup|2}})}}.<ref name="Hoory 2006"/> A better bound is given in <ref>B. Mohar. Isoperimetric numbers of graphs. J. Combin. Theory Ser. B, 47(3):274–291,
1989.</ref> as
1989.</ref> as
: <math> h(G) \le \sqrt{d^2 - \lambda_2^2}.</math>
: <math> h(G) \le \sqrt{d^2 - \lambda_2^2}.</math>
These inequalities are closely related to the [[Cheeger bound]] for [[Markov chains]] and can be seen as a discrete version of [[Cheeger constant#Cheeger.27s inequality|Cheeger's inequality]] in [[Riemannian geometry]].
These inequalities are closely related to the [[Cheeger bound]] for [[Markov chains]] and can be seen as a discrete version of [[Cheeger constant#Cheeger.27s inequality|Cheeger's inequality]] in [[Riemannian geometry]].


Similar connections between vertex isoperimetric numbers and the spectral gap have also been studied:<ref>See Theorem 1 and p.156, l.1 in {{harvtxt|Bobkov|Houdré|Tetali|2000}}. Note that {{math|λ{{sub|2}}}} there corresponds to {{math|2(''d'' − λ{{sub|2}})}} of the current article (see p.153, l.5)</ref>
Similar connections between vertex isoperimetric numbers and the spectral gap have also been studied:<ref>See Theorem 1 and p.156, l.1 in {{harvtxt|Bobkov|Houdré|Tetali|2000}}. Note that {{math|''λ''{{sub|2}}}} there corresponds to {{math|2(''d'' − ''λ''{{sub|2}})}} of the current article (see p.153, l.5)</ref>
: <math>h_{\text{out}}(G)\le \left(\sqrt{4 (d-\lambda_2)} + 1\right)^2 -1</math>
: <math>h_{\text{out}}(G)\le \left(\sqrt{4 (d-\lambda_2)} + 1\right)^2 -1</math>
: <math>h_{\text{in}}(G) \le \sqrt{8(d-\lambda_2)}.</math>
: <math>h_{\text{in}}(G) \le \sqrt{8(d-\lambda_2)}.</math>
Asymptotically speaking, the quantities {{math|{{frac|''h''{{sup|2}}|''d''}}}}, {{math|''h''{{sub|out}}}}, and {{math|''h''{{sub|in}}{{sup|2}}}} are all bounded above by the spectral gap {{math|''O''(''d'' – λ{{sub|2}})}}.
Asymptotically speaking, the quantities {{math|{{frac|''h''{{sup|2}}|''d''}}}}, {{math|''h''{{sub|out}}}}, and {{math|''h''{{sub|in}}{{sup|2}}}} are all bounded above by the spectral gap {{math|''O''(''d'' – ''λ''{{sub|2}})}}.


==Constructions==
==Constructions==
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===Ramanujan graphs===
===Ramanujan graphs===
{{main article|Ramanujan graph}}
{{main article|Ramanujan graph}}
By a [[Alon-Boppana bound|theorem of Alon and Boppana]], all sufficiently large {{mvar|d}}-regular graphs satisfy <math>\lambda_2 \ge 2\sqrt{d-1} - o(1)</math>, where {{math|λ{{sub|2}}}} is the second largest eigenvalue in absolute value.<ref>Theorem 2.7 of {{harvtxt|Hoory|Linial|Wigderson|2006}}</ref> As a direct consequence, we know that for every fixed {{mvar|d}} and <math>\lambda< 2 \sqrt{d-1}</math> , there are only finitely many {{math|(''n'', ''d'', λ)}}-graphs. [[Ramanujan graph]]s are {{mvar|d}}-regular graphs for which this bound is tight, satisfying <ref>Definition 5.11 of {{harvtxt|Hoory|Linial|Wigderson|2006}}</ref>
By a [[Alon–Boppana bound|theorem of Alon and Boppana]], all sufficiently large {{mvar|d}}-regular graphs satisfy <math>\lambda_2 \ge 2\sqrt{d-1} - o(1)</math>, where {{math|''λ''{{sub|2}}}} is the second largest eigenvalue in absolute value.<ref>Theorem 2.7 of {{harvtxt|Hoory|Linial|Wigderson|2006}}</ref> As a direct consequence, we know that for every fixed {{mvar|d}} and <math>\lambda< 2 \sqrt{d-1}</math> , there are only finitely many {{math|(''n'', ''d'', ''λ'')}}-graphs. [[Ramanujan graph]]s are {{mvar|d}}-regular graphs for which this bound is tight, satisfying <ref>Definition 5.11 of {{harvtxt|Hoory|Linial|Wigderson|2006}}</ref>
:<math>\lambda = \max_{|\lambda_i| < d} |\lambda_i| \le 2\sqrt{d-1}.</math>
:<math>\lambda = \max_{|\lambda_i| < d} |\lambda_i| \le 2\sqrt{d-1}.</math>
Hence Ramanujan graphs have an asymptotically smallest possible value of {{math|λ{{sub|2}}}}. This makes them excellent spectral expanders.
Hence Ramanujan graphs have an asymptotically smallest possible value of {{math|''λ''{{sub|2}}}}. This makes them excellent spectral expanders.


[[Alexander Lubotzky|Lubotzky]], Phillips, and [[Peter Sarnak|Sarnak]] (1988), Margulis (1988), and Morgenstern (1994) show how Ramanujan graphs can be constructed explicitly.<ref>Theorem 5.12 of {{harvtxt|Hoory|Linial|Wigderson|2006}}</ref>
[[Alexander Lubotzky|Lubotzky]], Phillips, and [[Peter Sarnak|Sarnak]] (1988), Margulis (1988), and Morgenstern (1994) show how Ramanujan graphs can be constructed explicitly.<ref>Theorem 5.12 of {{harvtxt|Hoory|Linial|Wigderson|2006}}</ref>
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[[Adam Marcus (mathematician)|Marcus]], [[Daniel Spielman|Spielman]] and [[Nikhil Srivastava|Srivastava]],<ref name="mss13">{{cite conference|author=Adam Marcus|author1-link=Adam Marcus (mathematician)|author2=Daniel Spielman|author2-link=Daniel Spielman|author3=Nikhil Srivastava|author3-link=Nikhil Srivastava|year=2013|title=Interlacing families I: Bipartite Ramanujan graphs of all degrees|url=https://annals.math.princeton.edu/wp-content/uploads/Marcus_Spielman_SrivastavaIFI.pdf|conference=Foundations of Computer Science (FOCS), 2013 IEEE 54th Annual Symposium}}</ref><ref name="mss15">{{cite conference|author=Adam Marcus|author1-link=Adam Marcus (mathematician)|author2=Daniel Spielman|author2-link=Daniel Spielman|author3=Nikhil Srivastava|author3-link=Nikhil Srivastava|year=2015|title=Interlacing families IV: Bipartite Ramanujan graphs of all sizes|url=https://www.cs.yale.edu/homes/spielman/PAPERS/IF4.pdf|conference=Foundations of Computer Science (FOCS), 2015 IEEE 56th Annual Symposium}}</ref> gave a construction of [[bipartite graph|bipartite]] Ramanujan graphs based on [[#Lifts|lifts]].
[[Adam Marcus (mathematician)|Marcus]], [[Daniel Spielman|Spielman]] and [[Nikhil Srivastava|Srivastava]],<ref name="mss13">{{cite conference|author=Adam Marcus|author1-link=Adam Marcus (mathematician)|author2=Daniel Spielman|author2-link=Daniel Spielman|author3=Nikhil Srivastava|author3-link=Nikhil Srivastava|year=2013|title=Interlacing families I: Bipartite Ramanujan graphs of all degrees|url=https://annals.math.princeton.edu/wp-content/uploads/Marcus_Spielman_SrivastavaIFI.pdf|conference=Foundations of Computer Science (FOCS), 2013 IEEE 54th Annual Symposium}}</ref><ref name="mss15">{{cite conference|author=Adam Marcus|author1-link=Adam Marcus (mathematician)|author2=Daniel Spielman|author2-link=Daniel Spielman|author3=Nikhil Srivastava|author3-link=Nikhil Srivastava|year=2015|title=Interlacing families IV: Bipartite Ramanujan graphs of all sizes|url=https://www.cs.yale.edu/homes/spielman/PAPERS/IF4.pdf|conference=Foundations of Computer Science (FOCS), 2015 IEEE 56th Annual Symposium}}</ref> gave a construction of [[bipartite graph|bipartite]] Ramanujan graphs based on [[#Lifts|lifts]].


=== Zig-Zag product ===
=== Zig-zag product ===
{{Main articles|Zig-zag product}}
{{Main articles|Zig-zag product}}
[[Omer Reingold|Reingold]], [[Salil Vadhan|Vadhan]], and [[Avi Wigderson|Wigderson]] introduced the zig-zag product in 2003.<ref name=":0">{{Cite book|last1=Reingold|first1=O.|last2=Vadhan|first2=S.|last3=Wigderson|first3=A.|title=Proceedings 41st Annual Symposium on Foundations of Computer Science |chapter=Entropy waves, the zig-zag graph product, and new constant-degree expanders and extractors |chapter-url=http://dx.doi.org/10.1109/sfcs.2000.892006|year=2000|pages=3–13|publisher=IEEE Comput. Soc|doi=10.1109/sfcs.2000.892006|isbn=0-7695-0850-2|s2cid=420651}}</ref> Roughly speaking, the zig-zag product of two expander graphs produces a graph with only slightly worse expansion. Therefore, a zig-zag product can also be used to construct families of expander graphs. If {{mvar|G}} is a {{math|(''n'', ''m'', λ{{sub|1}})}}-graph and {{mvar|H}} is an {{math|(''m'', ''d'', λ{{sub|1}})}}-graph, then the zig-zag product {{math|''G'' ◦ ''H''}} is a {{math|(''nm'', ''d''{{sup|2}}, ''φ''(λ{{sub|1}}, λ{{sub|2}}))}}-graph where {{mvar|φ}} has the following properties.
[[Omer Reingold|Reingold]], [[Salil Vadhan|Vadhan]], and [[Avi Wigderson|Wigderson]] introduced the zig-zag product in 2003.<ref name=":0">{{Cite book|last1=Reingold|first1=O.|last2=Vadhan|first2=S.|last3=Wigderson|first3=A.|title=Proceedings 41st Annual Symposium on Foundations of Computer Science |chapter=Entropy waves, the zig-zag graph product, and new constant-degree expanders and extractors |chapter-url=http://dx.doi.org/10.1109/sfcs.2000.892006|year=2000|pages=3–13|publisher=IEEE Comput. Soc|doi=10.1109/sfcs.2000.892006|isbn=0-7695-0850-2|s2cid=420651}}</ref> Roughly speaking, the zig-zag product of two expander graphs produces a graph with only slightly worse expansion. Therefore, a zig-zag product can also be used to construct families of expander graphs. If {{mvar|G}} is a {{math|(''n'', ''d'', ''λ''{{sub|1}})}}-graph and {{mvar|H}} is an {{math|(''m'', ''d'', ''λ''{{sub|2}})}}-graph, then the zig-zag product {{math|''G'' ◦ ''H''}} is a {{math|(''nm'', ''d''{{sup|2}}, ''φ''(''λ''{{sub|1}}, ''λ''{{sub|2}}))}}-graph where {{mvar|φ}} has the following properties.


# If {{math|λ{{sub|1}} < 1}} and {{math|λ{{sub|2}} < 1}}, then {{math|''φ''(λ{{sub|1}}, λ{{sub|2}}) < 1}};
# If {{math|''λ''{{sub|1}} < 1}} and {{math|''λ''{{sub|2}} < 1}}, then {{math|''φ''(''λ''{{sub|1}}, ''λ''{{sub|2}}) < 1}};
# {{math|''φ''(λ{{sub|1}}, λ{{sub|2}}) ≤ λ{{sub|1}} + λ{{sub|2}}}}.
# {{math|''φ''(''λ''{{sub|1}}, ''λ''{{sub|2}}) ≤ ''λ''{{sub|1}} + ''λ''{{sub|2}}}}.
Specifically,<ref name=":0" />
Specifically,<ref name=":0" />
:<math>\phi(\lambda_1, \lambda_2)=\frac{1}{2}(1-\lambda^2_2)\lambda_2 +\frac{1}{2}\sqrt{(1-\lambda^2_2)^2\lambda_1^2 +4\lambda^2_2}.</math>
:<math>\phi(\lambda_1, \lambda_2)=\frac{1}{2}(1-\lambda^2_2)\lambda_2 +\frac{1}{2}\sqrt{(1-\lambda^2_2)^2\lambda_1^2 +4\lambda^2_2}.</math>
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Note that property (1) implies that the zig-zag product of two expander graphs is also an expander graph, thus zig-zag products can be used inductively to create a family of expander graphs.
Note that property (1) implies that the zig-zag product of two expander graphs is also an expander graph, thus zig-zag products can be used inductively to create a family of expander graphs.


Intuitively, the construction of the zig-zag product can be thought of in the following way. Each vertex of {{mvar|G}} is blown up to a "cloud" of {{mvar|m}} vertices, each associated to a different edge connected to the vertex. Each vertex is now labeled as {{math|(''v'', ''k'')}} where {{mvar|v}} refers to an original vertex of {{mvar|G}} and {{mvar|k}} refers to the {{mvar|k}}th edge of {{mvar|v}}. Two vertices, {{math|(''v'', ''k'')}} and {{math|(''w'',''l'')}} are connected if it is possible to get from {{math|(''v'', ''k'')}} to {{math|(''w'', ''l'')}} through the following sequence of moves.
Intuitively, the construction of the zig-zag product can be thought of in the following way. Each vertex of {{mvar|G}} is blown up to a "cloud" of {{mvar|m}} vertices, each associated to a different edge connected to the vertex. Each vertex is now labeled as {{math|(''v'', ''k'')}} where {{mvar|v}} refers to an original vertex of {{mvar|G}} and {{mvar|k}} refers to the {{mvar|k}}th edge of {{mvar|v}}. Two vertices, {{math|(''v'', ''k'')}} and {{math|(''w'','''')}} are connected if it is possible to get from {{math|(''v'', ''k'')}} to {{math|(''w'', '''')}} through the following sequence of moves.


# ''Zig'' - Move from {{math|(''v'', ''k'')}} to {{math|(''v'', ''k' '')}}, using an edge of {{mvar|H}}.
# ''Zig'' Move from {{math|(''v'', ''k'')}} to {{math|(''v'', ''k' '')}}, using an edge of {{mvar|H}}.
# Jump across clouds using edge {{mvar|k'}} in {{mvar|G}} to get to {{math|(''w'', ''l' '')}}.
# Jump across clouds using edge {{mvar|k'}} in {{mvar|G}} to get to {{math|(''w'', ''ℓ&prime;'')}}.
# ''Zag'' - Move from {{math|(''w'', ''l' '')}} to {{math|(''w'', ''l'')}} using an edge of {{mvar|H}}.<ref name=":0" />
# ''Zag'' Move from {{math|(''w'', ''ℓ&prime;'')}} to {{math|(''w'', '''')}} using an edge of {{mvar|H}}.<ref name=":0" />


===Lifts===
===Lifts===
An [[Covering_graph|{{mvar|r}}-lift]] of a graph is formed by replacing each vertex by {{mvar|r}} vertices, and each edge by a matching between the corresponding sets of <math>r</math> vertices. The lifted graph inherits the eigenvalues of the original graph, and has some additional eigenvalues. Bilu and [[Nati Linial|Linial]]<ref>{{cite arXiv|last1=Bilu|first1=Yonatan|last2=Linial|first2=Nathan|date=2004-04-08|title=Constructing expander graphs by 2-lifts and discrepancy vs. spectral gap|eprint=math/0312022}}</ref><ref>{{cite journal|last1=Bilu|first1=Yonatan|last2=Linial|first2=Nathan|title=Lifts, discrepancy and nearly optimal spectral gap|journal=[[Combinatorica]]|volume=26|issue=5|year=2006|pages=495–519|doi=10.1007/s00493-006-0029-7|s2cid=14422668 |issn=0209-9683}}</ref> showed that every {{mvar|d}}-regular graph has a 2-lift in which the additional eigenvalues are at most <math>O(\sqrt{d\log^3 d})</math> in magnitude. They also showed that if the starting graph is a good enough expander, then a good 2-lift can be found in [[polynomial time]], thus giving an efficient construction of {{mvar|d}}-regular expanders for every {{mvar|d}}.
An [[Covering_graph|{{mvar|r}}-lift]] of a graph is formed by replacing each vertex by {{mvar|r}} vertices, and each edge by a matching between the corresponding sets of <math>r</math> vertices. The lifted graph inherits the eigenvalues of the original graph, and has some additional eigenvalues. Bilu and [[Nati Linial|Linial]]<ref>{{cite arXiv|last1=Bilu|first1=Yonatan|last2=Linial|first2=Nathan|date=2004-04-08|title=Constructing expander graphs by 2-lifts and discrepancy vs. spectral gap|eprint=math/0312022}}</ref><ref>{{cite journal|last1=Bilu|first1=Yonatan|last2=Linial|first2=Nathan|title=Lifts, discrepancy and nearly optimal spectral gap|journal=[[Combinatorica]]|volume=26|issue=5|year=2006|pages=495–519|doi=10.1007/s00493-006-0029-7|s2cid=14422668 |issn=0209-9683}}</ref> showed that every {{mvar|d}}-regular graph has a 2-lift in which the additional eigenvalues are at most <math>O(\sqrt{d\log^3 d})</math> in magnitude. They also showed that if the starting graph is a good enough expander, then a good 2-lift can be found in [[polynomial time]], thus giving an efficient construction of {{mvar|d}}-regular expanders for every {{mvar|d}}.


Bilu and Linial conjectured that the bound <math>O(\sqrt{d\log^3 d})</math> can be improved to <math>2\sqrt{d-1}</math>, which would be optimal due to the [[Alon-Boppana bound]]. This conjecture was proved in the bipartite setting by [[Adam Marcus (mathematician)|Marcus]], [[Daniel Spielman|Spielman]] and [[Nikhil Srivastava|Srivastava]],<ref name="mss13">{{cite conference|author=Adam Marcus|author1-link=Adam Marcus (mathematician)|author2=Daniel Spielman|author2-link=Daniel Spielman|author3=Nikhil Srivastava|author3-link=Nikhil Srivastava|year=2013|title=Interlacing families I: Bipartite Ramanujan graphs of all degrees|url=https://annals.math.princeton.edu/wp-content/uploads/Marcus_Spielman_SrivastavaIFI.pdf|conference=Foundations of Computer Science (FOCS), 2013 IEEE 54th Annual Symposium}}</ref><ref name="mss15">{{cite conference|author=Adam Marcus|author1-link=Adam Marcus (mathematician)|author2=Daniel Spielman|author2-link=Daniel Spielman|author3=Nikhil Srivastava|author3-link=Nikhil Srivastava|year=2015|title=Interlacing families IV: Bipartite Ramanujan graphs of all sizes|url=https://www.cs.yale.edu/homes/spielman/PAPERS/IF4.pdf|conference=Foundations of Computer Science (FOCS), 2015 IEEE 56th Annual Symposium}}</ref> who used the method of interlacing polynomials. As a result, they obtained an alternative construction of [[bipartite graph|bipartite]] [[Ramanujan graph|Ramanujan graphs]]. The original non-constructive proof was turned into an algorithm by Michael B. Cohen.<ref name="c16">{{cite conference|author=Michael B. Cohen|year=2016|title=Ramanujan Graphs in Polynomial Time|conference=Foundations of Computer Science (FOCS), 2016 IEEE 57th Annual Symposium|arxiv=1604.03544|doi=10.1109/FOCS.2016.37}}</ref> Later the method was generalized to {{mvar|r}}-lifts by Hall, Puder and Sawin.<ref>{{cite journal|last1=Hall|first1=Chris|last2=Puder|first2=Doron|last3=Sawin|first3=William F.|date=2018|title=Ramanujan coverings of graphs|journal=[[Advances in Mathematics]] |volume=323 |pages=367–410 |doi=10.1016/j.aim.2017.10.042 |arxiv=1506.02335}}</ref>
Bilu and Linial conjectured that the bound <math>O(\sqrt{d\log^3 d})</math> can be improved to <math>2\sqrt{d-1}</math>, which would be optimal due to the [[Alon–Boppana bound]]. This conjecture was proved in the bipartite setting by [[Adam Marcus (mathematician)|Marcus]], [[Daniel Spielman|Spielman]] and [[Nikhil Srivastava|Srivastava]],<ref name="mss13"/><ref name="mss15"/> who used the method of interlacing polynomials. As a result, they obtained an alternative construction of [[bipartite graph|bipartite]] [[Ramanujan graph|Ramanujan graphs]]. The original non-constructive proof was turned into an algorithm by Michael B. Cohen.<ref name="c16">{{cite conference|author=Michael B. Cohen|year=2016|title=Ramanujan Graphs in Polynomial Time|conference=Foundations of Computer Science (FOCS), 2016 IEEE 57th Annual Symposium|arxiv=1604.03544|doi=10.1109/FOCS.2016.37}}</ref> Later the method was generalized to {{mvar|r}}-lifts by Hall, Puder and Sawin.<ref>{{cite journal|last1=Hall|first1=Chris|last2=Puder|first2=Doron|last3=Sawin|first3=William F.|date=2018|title=Ramanujan coverings of graphs|journal=[[Advances in Mathematics]] |volume=323 |pages=367–410 |doi=10.1016/j.aim.2017.10.042 |arxiv=1506.02335}}</ref>


===Randomized constructions===
===Randomized constructions===
There are many results that show the existence of graphs with good expansion properties through probabilistic arguments. In fact, the existence of expanders was first proved by Pinsker<ref>{{Cite journal|last=Pinkser|first=M.|title=On the Complexity of a Concentrator|journal=[[SIAM Journal on Computing]]|year=1973|publisher=SIAM|citeseerx=10.1.1.393.1430}}</ref> who showed that for a randomly chosen {{mvar|n}} vertex left {{mvar|d}} regular [[bipartite graph]], {{math|{{abs|''N''(''S'')}} ≥ (''d'' – 2){{abs|''S''}}}} for all subsets of vertices {{math|{{abs|''S''}} ≤ ''c{{sub|d}}n''}} with high probability, where {{mvar|c{{sub|d}}}} is a constant depending on {{mvar|d}} that is {{math|''O''(''d''{{sup|-4}})}}. Alon and Roichman <ref>{{Cite journal|last1=Alon|first1=N.|last2=Roichman|first2=Y.|title=Random Cayley graphs and Expanders|url=https://onlinelibrary.wiley.com/doi/abs/10.1002/rsa.3240050203|journal=Random Structures and Algorithms|year=1994|volume=5|issue=2|pages=271–284|publisher=Wiley Online Library|doi=10.1002/rsa.3240050203}}</ref> showed that for every {{math|1 > ''ε'' > 0}}, there is some {{math|''c''(''ε'') > 0}} such that the following holds: For a group {{mvar|G}} of order {{mvar|n}}, consider the Cayley graph on {{mvar|G}} with {{math|''c''(''ε'') log{{sub|2}} ''n''}} randomly chosen elements from {{mvar|G}}. Then, in the limit of {{mvar|n}} getting to infinity, the resulting graph is almost surely an {{math|''ε''}}-expander.
There are many results that show the existence of graphs with good expansion properties through probabilistic arguments. In fact, the existence of expanders was first proved by Pinsker<ref>{{Cite journal|last=Pinkser|first=M.|title=On the Complexity of a Concentrator|journal=[[SIAM Journal on Computing]]|year=1973|publisher=SIAM|citeseerx=10.1.1.393.1430}}</ref> who showed that for a randomly chosen {{mvar|n}} vertex left {{mvar|d}} regular [[bipartite graph]], {{math|{{abs|''N''(''S'')}} ≥ (''d'' – 2){{abs|''S''}}}} for all subsets of vertices {{math|{{abs|''S''}} ≤ ''c{{sub|d}}n''}} with high probability, where {{mvar|c{{sub|d}}}} is a constant depending on {{mvar|d}} that is {{math|''O''(''d''{{sup|-4}})}}. Alon and Roichman <ref>{{Cite journal|last1=Alon|first1=N.|last2=Roichman|first2=Y.|title=Random Cayley graphs and Expanders|url=https://onlinelibrary.wiley.com/doi/abs/10.1002/rsa.3240050203|journal=Random Structures and Algorithms|year=1994|volume=5|issue=2|pages=271–284|publisher=Wiley Online Library|doi=10.1002/rsa.3240050203}}</ref> showed that for every {{math|1 > ''ε'' > 0}}, there is some {{math|''c''(''ε'') > 0}} such that the following holds: For a group {{mvar|G}} of order {{mvar|n}}, consider the Cayley graph on {{mvar|G}} with {{math|''c''(''ε'') log{{sub|2}} ''n''}} randomly chosen elements from {{mvar|G}}. Then, in the limit of {{mvar|n}} getting to infinity, the resulting graph is almost surely an {{math|''ε''}}-expander.

In 2021, Alexander modified an MCMC algorithm to look for randomized constructions to produce Ramanujan graphs with a fixed vertex size and degree of regularity. [DOI: 10.48550/arXiv.2110.01407] The results show the Ramanujan graphs exist for every vertex size and degree pair up to 2000 vertices.
In 2024 Alon produced an explicit construction for near Ramanujan graphs of every vertex size and degree pair.


==Applications and useful properties==
==Applications and useful properties==
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===Expander mixing lemma===
===Expander mixing lemma===
{{Main article|Expander mixing lemma}}
{{Main article|Expander mixing lemma}}
The expander mixing lemma states that for an {{math|(''n'', ''d'', λ)}}-graph, for any two subsets of the vertices {{math|''S'', ''T'' ⊆ ''V''}}, the number of edges between {{mvar|S}} and {{mvar|T}} is approximately what you would expect in a random {{mvar|d}}-regular graph. The approximation is better the smaller {{math|λ}} is. In a random {{mvar|d}}-regular graph, as well as in an [[Erdős–Rényi model|Erdős–Rényi random graph]] with edge probability {{math|{{frac|''d''|''n''}}}}, we expect {{math|{{frac|''d''|''n''}} • {{abs|''S''}} • {{abs|''T''}}}} edges between {{mvar|S}} and {{mvar|T}}.
The expander mixing lemma states that for an {{math|(''n'', ''d'', ''λ'')}}-graph, for any two subsets of the vertices {{math|''S'', ''T'' ⊆ ''V''}}, the number of edges between {{mvar|S}} and {{mvar|T}} is approximately what you would expect in a random {{mvar|d}}-regular graph. The approximation is better the smaller {{math|''λ''}} is. In a random {{mvar|d}}-regular graph, as well as in an [[Erdős–Rényi model|Erdős–Rényi random graph]] with edge probability {{math|{{frac|''d''|''n''}}}}, we expect {{math|{{frac|''d''|''n''}} • {{abs|''S''}} • {{abs|''T''}}}} edges between {{mvar|S}} and {{mvar|T}}.


More formally, let {{math|''E''(''S'', ''T'')}} denote the number of edges between {{mvar|S}} and {{mvar|T}}. If the two sets are not disjoint, edges in their intersection are counted twice, that is,
More formally, let {{math|''E''(''S'', ''T'')}} denote the number of edges between {{mvar|S}} and {{mvar|T}}. If the two sets are not disjoint, edges in their intersection are counted twice, that is,
Line 152: Line 155:


:<math>\left|E(S, T) - \frac{d \cdot |S| \cdot |T|}{n}\right| \leq \lambda \sqrt{|S| \cdot |T|}.</math>
:<math>\left|E(S, T) - \frac{d \cdot |S| \cdot |T|}{n}\right| \leq \lambda \sqrt{|S| \cdot |T|}.</math>
Many properties of {{math|(''n'', ''d'', λ)}}-graphs are corollaries of the expander mixing lemmas, including the following.<ref name="Hoory 2006"/>
Many properties of {{math|(''n'', ''d'', ''λ'')}}-graphs are corollaries of the expander mixing lemmas, including the following.<ref name="Hoory 2006"/>


* An [[Independent set (graph theory)|independent set]] of a graph is a subset of vertices with no two vertices adjacent. In an {{math|(''n'', ''d'', λ)}}-graph, an independent set has size at most {{math|{{frac|λ''n''|''d''}}}}.
* An [[Independent set (graph theory)|independent set]] of a graph is a subset of vertices with no two vertices adjacent. In an {{math|(''n'', ''d'', ''λ'')}}-graph, an independent set has size at most {{math|{{frac|''λn''|''d''}}}}.
* The [[Graph coloring|chromatic number]] of a graph {{mvar|G}}, {{math|χ(''G'')}}, is the minimum number of colors needed such that adjacent vertices have different colors. Hoffman showed that {{math|{{frac|''d''|λ}} ≤ χ(''G'')}},<ref>{{Cite journal|last1=Hoffman|first1=A. J.|last2=Howes|first2=Leonard|date=1970|title=On Eigenvalues and Colorings of Graphs, Ii|url=https://onlinelibrary.wiley.com/doi/abs/10.1111/j.1749-6632.1970.tb56474.x|journal=Annals of the New York Academy of Sciences|language=en|volume=175|issue=1|pages=238–242|doi=10.1111/j.1749-6632.1970.tb56474.x|bibcode=1970NYASA.175..238H|s2cid=85243045|issn=1749-6632}}</ref> while Alon, Krivelevich, and Sudakov showed that if {{math|''d'' < {{frac|2''n''|3}}}}, then<ref>{{Cite journal|last1=Alon|first1=Noga|author-link1=Noga Alon|last2=Krivelevich|first2=Michael|author-link2=Michael Krivelevich|last3=Sudakov|first3=Benny|author-link3=Benny Sudakov|date=1999-09-01|title=Coloring Graphs with Sparse Neighborhoods|journal=[[Journal of Combinatorial Theory]] | series=Series B |language=en|volume=77|issue=1|pages=73–82|doi=10.1006/jctb.1999.1910|doi-access=free|issn=0095-8956}}</ref><p><math>\chi(G) \leq O \left( \frac{d}{\log(1+d/\lambda)} \right).</math></p>
* The [[Graph coloring|chromatic number]] of a graph {{mvar|G}}, {{math|''χ''(''G'')}}, is the minimum number of colors needed such that adjacent vertices have different colors. Hoffman showed that {{math|{{frac|''d''|''λ''}} ≤ ''χ''(''G'')}},<ref>{{Cite journal|last1=Hoffman|first1=A. J.|last2=Howes|first2=Leonard|date=1970|title=On Eigenvalues and Colorings of Graphs, Ii|url=https://onlinelibrary.wiley.com/doi/abs/10.1111/j.1749-6632.1970.tb56474.x|journal=Annals of the New York Academy of Sciences|language=en|volume=175|issue=1|pages=238–242|doi=10.1111/j.1749-6632.1970.tb56474.x|bibcode=1970NYASA.175..238H|s2cid=85243045|issn=1749-6632}}</ref> while Alon, Krivelevich, and Sudakov showed that if {{math|''d'' < {{frac|2''n''|3}}}}, then<ref>{{Cite journal|last1=Alon|first1=Noga|author-link1=Noga Alon|last2=Krivelevich|first2=Michael|author-link2=Michael Krivelevich|last3=Sudakov|first3=Benny|author-link3=Benny Sudakov|date=1999-09-01|title=Coloring Graphs with Sparse Neighborhoods|journal=[[Journal of Combinatorial Theory]] | series=Series B |language=en|volume=77|issue=1|pages=73–82|doi=10.1006/jctb.1999.1910|doi-access=free|issn=0095-8956}}</ref><p><math>\chi(G) \leq O \left( \frac{d}{\log(1+d/\lambda)} \right).</math></p>
* The [[Distance (graph theory)|diameter]] of a graph is the maximum distance between two vertices, where the distance between two vertices is defined to be the shortest path between them. Chung showed that the diameter of an {{math|(''n'', ''d'', λ)}}-graph is at most<ref>{{Cite journal|last=Chung|first=F. R. K.|date=1989|title=Diameters and eigenvalues|url=https://www.ams.org/jams/1989-02-02/S0894-0347-1989-0965008-X/|journal=Journal of the American Mathematical Society|language=en|volume=2|issue=2|pages=187–196|doi=10.1090/S0894-0347-1989-0965008-X|issn=0894-0347|doi-access=free}}</ref><p><math>\left\lceil \log \frac{n}{ \log(d/\lambda)} \right\rceil.</math></p>
* The [[Distance (graph theory)|diameter]] of a graph is the maximum distance between two vertices, where the distance between two vertices is defined to be the shortest path between them. Chung showed that the diameter of an {{math|(''n'', ''d'', ''λ'')}}-graph is at most<ref>{{Cite journal|last=Chung|first=F. R. K.|date=1989|title=Diameters and eigenvalues|url=https://www.ams.org/jams/1989-02-02/S0894-0347-1989-0965008-X/|journal=Journal of the American Mathematical Society|language=en|volume=2|issue=2|pages=187–196|doi=10.1090/S0894-0347-1989-0965008-X|issn=0894-0347|doi-access=free}}</ref><p><math>\left\lceil \log \frac{n}{ \log(d/\lambda)} \right\rceil.</math></p>


===Expander walk sampling===
===Expander walk sampling===
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==Notes==
==Notes==
{{Reflist|25em}}
{{Reflist|25em}}
Alexander, C. "On Near Optimal Expander Graphs of Fixed Size", September 2021, DOI: 10.48550/arXiv.2110.01407


==References==
==References==
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== External links ==
== External links ==
* [https://www.ams.org/notices/200407/what-is.pdf Brief introduction in Notices of the American Mathematical Society]
* [https://www.ams.org/notices/200407/what-is.pdf Brief introduction in Notices of the American Mathematical Society]
* [http://michaelnielsen.org/blog/archive/notes/expander_graphs.pdf Introductory paper by Michael Nielsen]
* [http://michaelnielsen.org/blog/archive/notes/expander_graphs.pdf Introductory paper by Michael Nielsen] {{Webarchive|url=https://web.archive.org/web/20160817025506/http://michaelnielsen.org/blog/archive/notes/expander_graphs.pdf |date=2016-08-17 }}
* [https://web.archive.org/web/20160629170338/http://www.math.ias.edu/~boaz/ExpanderCourse/ Lecture notes from a course on expanders (by Nati Linial and Avi Wigderson)]
* [https://web.archive.org/web/20160629170338/http://www.math.ias.edu/~boaz/ExpanderCourse/ Lecture notes from a course on expanders (by Nati Linial and Avi Wigderson)]
* [http://ttic.uchicago.edu/~prahladh/teaching/spring05/index.html Lecture notes from a course on expanders (by Prahladh Harsha)]
* [http://ttic.uchicago.edu/~prahladh/teaching/spring05/index.html Lecture notes from a course on expanders (by Prahladh Harsha)]

Latest revision as of 01:47, 9 December 2024

In graph theory, an expander graph is a sparse graph that has strong connectivity properties, quantified using vertex, edge or spectral expansion. Expander constructions have spawned research in pure and applied mathematics, with several applications to complexity theory, design of robust computer networks, and the theory of error-correcting codes.[1]

Definitions

[edit]

Intuitively, an expander graph is a finite, undirected multigraph in which every subset of the vertices that is not "too large" has a "large" boundary. Different formalisations of these notions give rise to different notions of expanders: edge expanders, vertex expanders, and spectral expanders, as defined below.

A disconnected graph is not an expander, since the boundary of a connected component is empty. Every connected graph is an expander; however, different connected graphs have different expansion parameters. The complete graph has the best expansion property, but it has largest possible degree. Informally, a graph is a good expander if it has low degree and high expansion parameters.

Edge expansion

[edit]

The edge expansion (also isoperimetric number or Cheeger constant) h(G) of a graph G on n vertices is defined as

where

which can also be written as S = E(S, S) with S := V(G) \ S the complement of S and

the edges between the subsets of vertices A,BV(G).

In the equation, the minimum is over all nonempty sets S of at most n2 vertices and S is the edge boundary of S, i.e., the set of edges with exactly one endpoint in S.[2]

Intuitively,

is the minimum number of edges that need to be cut in order to split the graph in two. The edge expansion normalizes this concept by dividing with smallest number of vertices among the two parts. To see how the normalization can drastically change the value, consider the following example. Take two complete graphs with the same number of vertices n and add n edges between the two graphs by connecting their vertices one-to-one. The minimum cut will be n but the edge expansion will be 1.

Notice that in min |S|, the optimization can be equivalently done either over 0 ≤ |S| ≤ n2 or over any non-empty subset, since . The same is not true for h(G) because of the normalization by |S|. If we want to write h(G) with an optimization over all non-empty subsets, we can rewrite it as

Vertex expansion

[edit]

The vertex isoperimetric number hout(G) (also vertex expansion or magnification) of a graph G is defined as

where out(S) is the outer boundary of S, i.e., the set of vertices in V(G) \ S with at least one neighbor in S.[3] In a variant of this definition (called unique neighbor expansion) out(S) is replaced by the set of vertices in V with exactly one neighbor in S.[4]

The vertex isoperimetric number hin(G) of a graph G is defined as

where is the inner boundary of S, i.e., the set of vertices in S with at least one neighbor in V(G) \ S.[3]

Spectral expansion

[edit]

When G is d-regular, a linear algebraic definition of expansion is possible based on the eigenvalues of the adjacency matrix A = A(G) of G, where Aij is the number of edges between vertices i and j.[5] Because A is symmetric, the spectral theorem implies that A has n real-valued eigenvalues λ1λ2 ≥ … ≥ λn. It is known that all these eigenvalues are in [−d, d] and more specifically, it is known that λn = −d if and only if G is bipartite.

More formally, we refer to an n-vertex, d-regular graph with

as an (n, d, λ)-graph. The bound given by an (n, d, λ)-graph on λi for i ≠ 1 is useful many contexts, including the expander mixing lemma.

Spectral expansion can be two-sided, as above, with , or it can be one-sided, with . The latter is a weaker notion that holds also for bipartite graphs and is still useful for many applications, such as the Alon–Chung lemma.[6]

Because G is regular, the uniform distribution with ui = 1n for all i = 1, …, n is the stationary distribution of G. That is, we have Au = du, and u is an eigenvector of A with eigenvalue λ1 = d, where d is the degree of the vertices of G. The spectral gap of G is defined to be dλ2, and it measures the spectral expansion of the graph G.[7]

If we set

as this is the largest eigenvalue corresponding to an eigenvector orthogonal to u, it can be equivalently defined using the Rayleigh quotient:

where

is the 2-norm of the vector .

The normalized versions of these definitions are also widely used and more convenient in stating some results. Here one considers the matrix 1/dA, which is the Markov transition matrix of the graph G. Its eigenvalues are between −1 and 1. For not necessarily regular graphs, the spectrum of a graph can be defined similarly using the eigenvalues of the Laplacian matrix. For directed graphs, one considers the singular values of the adjacency matrix A, which are equal to the roots of the eigenvalues of the symmetric matrix ATA.

Relationships between different expansion properties

[edit]

The expansion parameters defined above are related to each other. In particular, for any d-regular graph G,

Consequently, for constant degree graphs, vertex and edge expansion are qualitatively the same.

Cheeger inequalities

[edit]

When G is d-regular, meaning each vertex is of degree d, there is a relationship between the isoperimetric constant h(G) and the gap dλ2 in the spectrum of the adjacency operator of G. By standard spectral graph theory, the trivial eigenvalue of the adjacency operator of a d-regular graph is λ1 = d and the first non-trivial eigenvalue is λ2. If G is connected, then λ2 < d. An inequality due to Dodziuk[8] and independently Alon and Milman[9] states that[10]

In fact, the lower bound is tight. The lower bound is achieved in limit for the hypercube Qn, where h(G) = 1 and dλ2 = 2. The upper bound is (asymptotically) achieved for a cycle, where h(Cn) = 4/n = Θ(1/n) and dλ2 = 2 – 2cos(2/n) ≈ (2/n)2 = Θ(1/n2).[1] A better bound is given in [11] as

These inequalities are closely related to the Cheeger bound for Markov chains and can be seen as a discrete version of Cheeger's inequality in Riemannian geometry.

Similar connections between vertex isoperimetric numbers and the spectral gap have also been studied:[12]

Asymptotically speaking, the quantities h2d, hout, and hin2 are all bounded above by the spectral gap O(dλ2).

Constructions

[edit]

There are four general strategies for explicitly constructing families of expander graphs.[13] The first strategy is algebraic and group-theoretic, the second strategy is analytic and uses additive combinatorics, the third strategy is combinatorial and uses the zig-zag and related graph products, and the fourth strategy is based on lifts. Noga Alon showed that certain graphs constructed from finite geometries are the sparsest examples of highly expanding graphs.[14]

Margulis–Gabber–Galil

[edit]

Algebraic constructions based on Cayley graphs are known for various variants of expander graphs. The following construction is due to Margulis and has been analysed by Gabber and Galil.[15] For every natural number n, one considers the graph Gn with the vertex set , where : For every vertex , its eight adjacent vertices are

Then the following holds:

Theorem. For all n, the graph Gn has second-largest eigenvalue .

Ramanujan graphs

[edit]

By a theorem of Alon and Boppana, all sufficiently large d-regular graphs satisfy , where λ2 is the second largest eigenvalue in absolute value.[16] As a direct consequence, we know that for every fixed d and , there are only finitely many (n, d, λ)-graphs. Ramanujan graphs are d-regular graphs for which this bound is tight, satisfying [17]

Hence Ramanujan graphs have an asymptotically smallest possible value of λ2. This makes them excellent spectral expanders.

Lubotzky, Phillips, and Sarnak (1988), Margulis (1988), and Morgenstern (1994) show how Ramanujan graphs can be constructed explicitly.[18]

In 1985, Alon, conjectured that most d-regular graphs on n vertices, for sufficiently large n, are almost Ramanujan.[19] That is, for ε > 0, they satisfy

.

In 2003, Joel Friedman both proved the conjecture and specified what is meant by "most d-regular graphs" by showing that random d-regular graphs have for every ε > 0 with probability 1 – O(n), where[20][21]

A simpler proof of a slightly weaker result was given by Puder.[22][23][24]

Marcus, Spielman and Srivastava,[25][26] gave a construction of bipartite Ramanujan graphs based on lifts.

Zig-zag product

[edit]

Reingold, Vadhan, and Wigderson introduced the zig-zag product in 2003.[27] Roughly speaking, the zig-zag product of two expander graphs produces a graph with only slightly worse expansion. Therefore, a zig-zag product can also be used to construct families of expander graphs. If G is a (n, d, λ1)-graph and H is an (m, d, λ2)-graph, then the zig-zag product GH is a (nm, d2, φ(λ1, λ2))-graph where φ has the following properties.

  1. If λ1 < 1 and λ2 < 1, then φ(λ1, λ2) < 1;
  2. φ(λ1, λ2) ≤ λ1 + λ2.

Specifically,[27]

Note that property (1) implies that the zig-zag product of two expander graphs is also an expander graph, thus zig-zag products can be used inductively to create a family of expander graphs.

Intuitively, the construction of the zig-zag product can be thought of in the following way. Each vertex of G is blown up to a "cloud" of m vertices, each associated to a different edge connected to the vertex. Each vertex is now labeled as (v, k) where v refers to an original vertex of G and k refers to the kth edge of v. Two vertices, (v, k) and (w,) are connected if it is possible to get from (v, k) to (w, ) through the following sequence of moves.

  1. Zig – Move from (v, k) to (v, k' ), using an edge of H.
  2. Jump across clouds using edge k' in G to get to (w, ℓ′).
  3. Zag – Move from (w, ℓ′) to (w, ) using an edge of H.[27]

Lifts

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An r-lift of a graph is formed by replacing each vertex by r vertices, and each edge by a matching between the corresponding sets of vertices. The lifted graph inherits the eigenvalues of the original graph, and has some additional eigenvalues. Bilu and Linial[28][29] showed that every d-regular graph has a 2-lift in which the additional eigenvalues are at most in magnitude. They also showed that if the starting graph is a good enough expander, then a good 2-lift can be found in polynomial time, thus giving an efficient construction of d-regular expanders for every d.

Bilu and Linial conjectured that the bound can be improved to , which would be optimal due to the Alon–Boppana bound. This conjecture was proved in the bipartite setting by Marcus, Spielman and Srivastava,[25][26] who used the method of interlacing polynomials. As a result, they obtained an alternative construction of bipartite Ramanujan graphs. The original non-constructive proof was turned into an algorithm by Michael B. Cohen.[30] Later the method was generalized to r-lifts by Hall, Puder and Sawin.[31]

Randomized constructions

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There are many results that show the existence of graphs with good expansion properties through probabilistic arguments. In fact, the existence of expanders was first proved by Pinsker[32] who showed that for a randomly chosen n vertex left d regular bipartite graph, |N(S)| ≥ (d – 2)|S| for all subsets of vertices |S| ≤ cdn with high probability, where cd is a constant depending on d that is O(d-4). Alon and Roichman [33] showed that for every 1 > ε > 0, there is some c(ε) > 0 such that the following holds: For a group G of order n, consider the Cayley graph on G with c(ε) log2 n randomly chosen elements from G. Then, in the limit of n getting to infinity, the resulting graph is almost surely an ε-expander.

In 2021, Alexander modified an MCMC algorithm to look for randomized constructions to produce Ramanujan graphs with a fixed vertex size and degree of regularity. [DOI: 10.48550/arXiv.2110.01407] The results show the Ramanujan graphs exist for every vertex size and degree pair up to 2000 vertices. In 2024 Alon produced an explicit construction for near Ramanujan graphs of every vertex size and degree pair.

Applications and useful properties

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The original motivation for expanders is to build economical robust networks (phone or computer): an expander with bounded degree is precisely an asymptotic robust graph with the number of edges growing linearly with size (number of vertices), for all subsets.

Expander graphs have found extensive applications in computer science, in designing algorithms, error correcting codes, extractors, pseudorandom generators, sorting networks (Ajtai, Komlós & Szemerédi (1983)) and robust computer networks. They have also been used in proofs of many important results in computational complexity theory, such as SL = L (Reingold (2008)) and the PCP theorem (Dinur (2007)). In cryptography, expander graphs are used to construct hash functions.

In a 2006 survey of expander graphs, Hoory, Linial, and Wigderson split the study of expander graphs into four categories: extremal problems, typical behavior, explicit constructions, and algorithms. Extremal problems focus on the bounding of expansion parameters, while typical behavior problems characterize how the expansion parameters are distributed over random graphs. Explicit constructions focus on constructing graphs that optimize certain parameters, and algorithmic questions study the evaluation and estimation of parameters.

Expander mixing lemma

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The expander mixing lemma states that for an (n, d, λ)-graph, for any two subsets of the vertices S, TV, the number of edges between S and T is approximately what you would expect in a random d-regular graph. The approximation is better the smaller λ is. In a random d-regular graph, as well as in an Erdős–Rényi random graph with edge probability dn, we expect dn • |S| • |T| edges between S and T.

More formally, let E(S, T) denote the number of edges between S and T. If the two sets are not disjoint, edges in their intersection are counted twice, that is,

Then the expander mixing lemma says that the following inequality holds:

Many properties of (n, d, λ)-graphs are corollaries of the expander mixing lemmas, including the following.[1]

  • An independent set of a graph is a subset of vertices with no two vertices adjacent. In an (n, d, λ)-graph, an independent set has size at most λnd.
  • The chromatic number of a graph G, χ(G), is the minimum number of colors needed such that adjacent vertices have different colors. Hoffman showed that dλχ(G),[34] while Alon, Krivelevich, and Sudakov showed that if d < 2n3, then[35]

  • The diameter of a graph is the maximum distance between two vertices, where the distance between two vertices is defined to be the shortest path between them. Chung showed that the diameter of an (n, d, λ)-graph is at most[36]

Expander walk sampling

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The Chernoff bound states that, when sampling many independent samples from a random variable in the range [−1, 1], with high probability the average of our samples is close to the expectation of the random variable. The expander walk sampling lemma, due to Ajtai, Komlós & Szemerédi (1987) and Gillman (1998), states that this also holds true when sampling from a walk on an expander graph. This is particularly useful in the theory of derandomization, since sampling according to an expander walk uses many fewer random bits than sampling independently.

AKS sorting network and approximate halvers

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Sorting networks take a set of inputs and perform a series of parallel steps to sort the inputs. A parallel step consists of performing any number of disjoint comparisons and potentially swapping pairs of compared inputs. The depth of a network is given by the number of parallel steps it takes. Expander graphs play an important role in the AKS sorting network, which achieves depth O(log n). While this is asymptotically the best known depth for a sorting network, the reliance on expanders makes the constant bound too large for practical use.

Within the AKS sorting network, expander graphs are used to construct bounded depth ε-halvers. An ε-halver takes as input a length n permutation of (1, …, n) and halves the inputs into two disjoint sets A and B such that for each integer kn2 at most εk of the k smallest inputs are in B and at most εk of the k largest inputs are in A. The sets A and B are an ε-halving.

Following Ajtai, Komlós & Szemerédi (1983), a depth d ε-halver can be constructed as follows. Take an n vertex, degree d bipartite expander with parts X and Y of equal size such that every subset of vertices of size at most εn has at least 1 – ε/ε neighbors.

The vertices of the graph can be thought of as registers that contain inputs and the edges can be thought of as wires that compare the inputs of two registers. At the start, arbitrarily place half of the inputs in X and half of the inputs in Y and decompose the edges into d perfect matchings. The goal is to end with X roughly containing the smaller half of the inputs and Y containing roughly the larger half of the inputs. To achieve this, sequentially process each matching by comparing the registers paired up by the edges of this matching and correct any inputs that are out of order. Specifically, for each edge of the matching, if the larger input is in the register in X and the smaller input is in the register in Y, then swap the two inputs so that the smaller one is in X and the larger one is in Y. It is clear that this process consists of d parallel steps.

After all d rounds, take A to be the set of inputs in registers in X and B to be the set of inputs in registers in Y to obtain an ε-halving. To see this, notice that if a register u in X and v in Y are connected by an edge uv then after the matching with this edge is processed, the input in u is less than that of v. Furthermore, this property remains true throughout the rest of the process. Now, suppose for some kn2 that more than εk of the inputs (1, …, k) are in B. Then by expansion properties of the graph, the registers of these inputs in Y are connected with at least 1 – ε/εk registers in X. Altogether, this constitutes more than k registers so there must be some register A in X connected to some register B in Y such that the final input of A is not in (1, …, k), while the final input of B is. This violates the previous property however, and thus the output sets A and B must be an ε-halving.

See also

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Notes

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  1. ^ a b c Hoory, Linial & Wigderson (2006)
  2. ^ Definition 2.1 in Hoory, Linial & Wigderson (2006)
  3. ^ a b Bobkov, Houdré & Tetali (2000)
  4. ^ Alon & Capalbo (2002)
  5. ^ cf. Section 2.3 in Hoory, Linial & Wigderson (2006)
  6. ^ N. Alon and F. R. K. Chung, Explicit construction of linear sized tolerant networks. Discrete Math., vol. 72, pp. 15–19, 1988.
  7. ^ This definition of the spectral gap is from Section 2.3 in Hoory, Linial & Wigderson (2006)
  8. ^ Dodziuk 1984.
  9. ^ Alon & Spencer 2011.
  10. ^ Theorem 2.4 in Hoory, Linial & Wigderson (2006)
  11. ^ B. Mohar. Isoperimetric numbers of graphs. J. Combin. Theory Ser. B, 47(3):274–291, 1989.
  12. ^ See Theorem 1 and p.156, l.1 in Bobkov, Houdré & Tetali (2000). Note that λ2 there corresponds to 2(dλ2) of the current article (see p.153, l.5)
  13. ^ see, e.g., Yehudayoff (2012)
  14. ^ Alon, Noga (1986). "Eigenvalues, geometric expanders, sorting in rounds, and ramsey theory". Combinatorica. 6 (3): 207–219. CiteSeerX 10.1.1.300.5945. doi:10.1007/BF02579382. S2CID 8666466.
  15. ^ see, e.g., p.9 of Goldreich (2011)
  16. ^ Theorem 2.7 of Hoory, Linial & Wigderson (2006)
  17. ^ Definition 5.11 of Hoory, Linial & Wigderson (2006)
  18. ^ Theorem 5.12 of Hoory, Linial & Wigderson (2006)
  19. ^ Alon, Noga (1986-06-01). "Eigenvalues and expanders". Combinatorica. 6 (2): 83–96. doi:10.1007/BF02579166. ISSN 1439-6912. S2CID 41083612.
  20. ^ Friedman, Joel (2004-05-05). "A proof of Alon's second eigenvalue conjecture and related problems". arXiv:cs/0405020.
  21. ^ Theorem 7.10 of Hoory, Linial & Wigderson (2006)
  22. ^ Puder, Doron (2015-08-21). "Expansion of random graphs: New proofs, new results". Inventiones Mathematicae. 201 (3): 845–908. arXiv:1212.5216. Bibcode:2015InMat.201..845P. doi:10.1007/s00222-014-0560-x. S2CID 253743928.
  23. ^ Puder, Doron (2015). "Expansion of random graphs: new proofs, new results". Inventiones Mathematicae. 201 (3): 845–908. arXiv:1212.5216. Bibcode:2015InMat.201..845P. doi:10.1007/s00222-014-0560-x. ISSN 0020-9910. S2CID 16411939.
  24. ^ Friedman, Joel; Puder, Doron (2023). "A note on the trace method for random regular graphs". Israel Journal of Mathematics. 256: 269–282. arXiv:2006.13605. doi:10.1007/s11856-023-2497-5. S2CID 220042379.
  25. ^ a b Adam Marcus; Daniel Spielman; Nikhil Srivastava (2013). Interlacing families I: Bipartite Ramanujan graphs of all degrees (PDF). Foundations of Computer Science (FOCS), 2013 IEEE 54th Annual Symposium.
  26. ^ a b Adam Marcus; Daniel Spielman; Nikhil Srivastava (2015). Interlacing families IV: Bipartite Ramanujan graphs of all sizes (PDF). Foundations of Computer Science (FOCS), 2015 IEEE 56th Annual Symposium.
  27. ^ a b c Reingold, O.; Vadhan, S.; Wigderson, A. (2000). "Entropy waves, the zig-zag graph product, and new constant-degree expanders and extractors". Proceedings 41st Annual Symposium on Foundations of Computer Science. IEEE Comput. Soc. pp. 3–13. doi:10.1109/sfcs.2000.892006. ISBN 0-7695-0850-2. S2CID 420651.
  28. ^ Bilu, Yonatan; Linial, Nathan (2004-04-08). "Constructing expander graphs by 2-lifts and discrepancy vs. spectral gap". arXiv:math/0312022.
  29. ^ Bilu, Yonatan; Linial, Nathan (2006). "Lifts, discrepancy and nearly optimal spectral gap". Combinatorica. 26 (5): 495–519. doi:10.1007/s00493-006-0029-7. ISSN 0209-9683. S2CID 14422668.
  30. ^ Michael B. Cohen (2016). Ramanujan Graphs in Polynomial Time. Foundations of Computer Science (FOCS), 2016 IEEE 57th Annual Symposium. arXiv:1604.03544. doi:10.1109/FOCS.2016.37.
  31. ^ Hall, Chris; Puder, Doron; Sawin, William F. (2018). "Ramanujan coverings of graphs". Advances in Mathematics. 323: 367–410. arXiv:1506.02335. doi:10.1016/j.aim.2017.10.042.
  32. ^ Pinkser, M. (1973). "On the Complexity of a Concentrator". SIAM Journal on Computing. SIAM. CiteSeerX 10.1.1.393.1430.
  33. ^ Alon, N.; Roichman, Y. (1994). "Random Cayley graphs and Expanders". Random Structures and Algorithms. 5 (2). Wiley Online Library: 271–284. doi:10.1002/rsa.3240050203.
  34. ^ Hoffman, A. J.; Howes, Leonard (1970). "On Eigenvalues and Colorings of Graphs, Ii". Annals of the New York Academy of Sciences. 175 (1): 238–242. Bibcode:1970NYASA.175..238H. doi:10.1111/j.1749-6632.1970.tb56474.x. ISSN 1749-6632. S2CID 85243045.
  35. ^ Alon, Noga; Krivelevich, Michael; Sudakov, Benny (1999-09-01). "Coloring Graphs with Sparse Neighborhoods". Journal of Combinatorial Theory. Series B. 77 (1): 73–82. doi:10.1006/jctb.1999.1910. ISSN 0095-8956.
  36. ^ Chung, F. R. K. (1989). "Diameters and eigenvalues". Journal of the American Mathematical Society. 2 (2): 187–196. doi:10.1090/S0894-0347-1989-0965008-X. ISSN 0894-0347.

Alexander, C. "On Near Optimal Expander Graphs of Fixed Size", September 2021, DOI: 10.48550/arXiv.2110.01407

References

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Textbooks and surveys

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Research articles

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Recent Applications

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