Main Page: Difference between revisions

From formulasearchengine
Jump to navigation Jump to search
No edit summary
No edit summary
 
(720 intermediate revisions by more than 100 users not shown)
Line 1: Line 1:
In [[combinatorics]], an '''expander graph''' is a [[sparse graph]] that has strong [[connectivity (graph theory)|connectivity]] properties, quantified using [[vertex (graph theory)|vertex]], [[edge (graph theory)|edge]] or spectral expansion as described below. Expander constructions have spawned research in pure and applied mathematics, with several applications to [[Computational complexity theory|complexity theory]], design of robust [[computer network]]s, and the theory of [[error-correcting code]]s.<ref>{{harvtxt|Hoory|Linial|Widgerson|2006}}</ref>
This is a preview for the new '''MathML rendering mode''' (with SVG fallback), which is availble in production for registered users.


==Definitions==
If you would like use the '''MathML''' rendering mode, you need a wikipedia user account that can be registered here [[https://en.wikipedia.org/wiki/Special:UserLogin/signup]]
* Only registered users will be able to execute this rendering mode.
* Note: you need not enter a email address (nor any other private information). Please do not use a password that you use elsewhere.


Intuitively, an expander is a finite, undirected [[multigraph]] in which every subset of the vertices "which 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.
Registered users will be able to choose between the following three rendering modes:  


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.
'''MathML'''
:<math forcemathmode="mathml">E=mc^2</math>


===Edge expansion===
<!--'''PNG''' (currently default in production)
The ''edge expansion'' (also ''isoperimetric number'' or [[Cheeger constant (graph theory)|Cheeger constant]]) <math>h(G)</math> of a graph <math>G</math> is defined as
:<math forcemathmode="png">E=mc^2</math>
: <math>h(G) = \min_{0 < |S| \le \frac{n}{2} } \frac{|\partial(S)|}{|S|}\,,</math>
where the minimum is over all nonempty sets <math>S</math> of at most <math>n/2</math> vertices and <math>\partial(S)</math> is the ''edge boundary'' of <math>S</math>, i.e., the set of edges with exactly one endpoint in <math>S</math>.<ref>Definition 2.1 in {{harvtxt|Hoory|Linial|Widgerson|2006}}</ref>


===Vertex expansion===
'''source'''
The ''vertex isoperimetric number'' <math>h_{\text{out}}(G)</math> (also ''vertex expansion'' or ''magnification'') of a graph <math>G</math> is defined as
:<math forcemathmode="source">E=mc^2</math> -->
: <math>h_{\text{out}}(G) = \min_{0 < |S|\le \frac{n}{2}} \frac{|\partial_{\text{out}}(S)|}{|S|}\,,</math>
where <math>\partial_{\text{out}}(S)</math> is the ''outer boundary'' of <math>S</math>, i.e., the set of vertices in <math>V(G)\setminus S</math> with at least one neighbor in <math>S</math>.<ref name="BobkovHoudre">{{harvtxt|Bobkov|Houdré|Tetali|2000}}</ref>
In a variant of this definition (called ''unique neighbor expansion'') <math>\partial_{\text{out}}(S)</math> is replaced by the set of vertices in <math>V</math> with ''exactly'' one neighbor in <math>S</math>.<ref name="AlonCapalbo">{{harvtxt|Alon|Capalbo|2002}}</ref>


The ''vertex isoperimetric number'' <math>h_{\text{in}}(G)</math> of a graph <math>G</math> is defined as
<span style="color: red">Follow this [https://en.wikipedia.org/wiki/Special:Preferences#mw-prefsection-rendering link] to change your Math rendering settings.</span> You can also add a [https://en.wikipedia.org/wiki/Special:Preferences#mw-prefsection-rendering-skin Custom CSS] to force the MathML/SVG rendering or select different font families. See [https://www.mediawiki.org/wiki/Extension:Math#CSS_for_the_MathML_with_SVG_fallback_mode these examples].
: <math>h_{\text{in}}(G) = \min_{0 < |S|\le \frac{n}{2}} \frac{|\partial_{\text{in}}(S)|}{|S|}\,,</math>
where <math>\partial_{\text{in}}(S)</math> is the ''inner boundary'' of <math>S</math>, i.e., the set of vertices in <math>S</math> with at least one neighbor in <math>V(G)\setminus S</math>.<ref name="BobkovHoudre" />


===Spectral expansion===
==Demos==
When <math>G</math> is [[regular graph|regular]], a [[linear algebra]]ic definition of expansion is possible based on the [[Eigenvalue#Eigenvalues of matrices|eigenvalues]] of the [[adjacency matrix]] <math>A=A(G)</math> of <math>G</math>, where <math>A_{ij}</math> is the number of edges between vertices <math>i</math> and <math>j</math>.<ref>cf. Section 2.3 in {{harvtxt|Hoory|Linial|Widgerson|2006}}</ref>
Because <math>A</math> is [[symmetric matrix|symmetric]], the [[spectral theorem]] implies that <math>A</math> has <math>n</math> real-valued eigenvalues <math>\lambda_1 \ge \lambda_2 \ge \cdots \ge \lambda_{n}</math>.
It is known that all these eigenvalues are in <math>[-d,d]</math>.


Because <math>G</math> is regular, the uniform distribution <math>u\in\R^n</math> with <math>u_i=1/n</math> for all <math>i=1,\dots,n</math> is the [[stationary distribution]] of <math>G</math>.
Here are some [https://commons.wikimedia.org/w/index.php?title=Special:ListFiles/Frederic.wang demos]:
That is, we have <math>Au=du</math>, and <math>u</math> is an eigenvector of <math>A</math> with eigenvalue <math>\lambda_1=d</math>, where <math>d</math> is the [[degree (graph theory)|degree]] of the vertices of <math>G</math>.
The ''[[spectral gap]]'' of <math>G</math> is defined to be <math>d-\lambda_2</math>, and it measures the spectral expansion of the graph <math>G</math>.<ref>This definition of the spectral gap is from Section 2.3 in {{harvtxt|Hoory|Linial|Widgerson|2006}}</ref>


It is known that <math>\lambda_n=-d</math> if and only if <math>G</math> is bipartite.
In many context, for example in the [[expander mixing lemma]], it is necessary to bound from below not only the gap between <math>\lambda_1</math> and <math>\lambda_2</math>, but also the gap between <math>\lambda_1</math> and
the second-largest eigenvalue in absolute value:
<math>\lambda=\max\{|\lambda_2|, |\lambda_{n}|\}</math>.
Since this is the largest eigenvalue corresponding to an eigenvector orthogonal to <math>u</math>, it can be equivalently defined using the [[Rayleigh quotient]]:
:<math>\lambda=\max_{0\neq v\perp u} \frac{\|Av\|_2}{\|v\|_2}\,,</math>
where <math>\|v\|_2=\left(\sum_{i=1}^n v_i^2\right)^{1/2}</math> is the [[2-norm]] of the vector <math>v\in\R^n</math>.


The normalized versions of these definitions are also widely used and more convenient in stating some results.
* accessibility:
Here one considers the matrix <math>\frac{1}{d} A</math>, which is the [[Markov transition matrix]] of the graph <math>G</math>.
** Safari + VoiceOver: [https://commons.wikimedia.org/wiki/File:VoiceOver-Mac-Safari.ogv video only], [[File:Voiceover-mathml-example-1.wav|thumb|Voiceover-mathml-example-1]], [[File:Voiceover-mathml-example-2.wav|thumb|Voiceover-mathml-example-2]], [[File:Voiceover-mathml-example-3.wav|thumb|Voiceover-mathml-example-3]], [[File:Voiceover-mathml-example-4.wav|thumb|Voiceover-mathml-example-4]], [[File:Voiceover-mathml-example-5.wav|thumb|Voiceover-mathml-example-5]], [[File:Voiceover-mathml-example-6.wav|thumb|Voiceover-mathml-example-6]], [[File:Voiceover-mathml-example-7.wav|thumb|Voiceover-mathml-example-7]]
Its eigenvalues are between <math>-1</math> and <math>1</math>.
** [https://commons.wikimedia.org/wiki/File:MathPlayer-Audio-Windows7-InternetExplorer.ogg Internet Explorer + MathPlayer (audio)]
For not necessarily regular graphs, the spectrum of a graph can be defined similarly using the eigenvalues of the [[Laplacian matrix]].
** [https://commons.wikimedia.org/wiki/File:MathPlayer-SynchronizedHighlighting-WIndows7-InternetExplorer.png Internet Explorer + MathPlayer (synchronized highlighting)]
For directed graphs, one considers the [[singular values]] of the adjacency matrix <math>A</math>, which are equal to the roots of the eigenvalues of the symmetric matrix <math>A^T A</math>.
** [https://commons.wikimedia.org/wiki/File:MathPlayer-Braille-Windows7-InternetExplorer.png Internet Explorer + MathPlayer (braille)]
** NVDA+MathPlayer: [[File:Nvda-mathml-example-1.wav|thumb|Nvda-mathml-example-1]], [[File:Nvda-mathml-example-2.wav|thumb|Nvda-mathml-example-2]], [[File:Nvda-mathml-example-3.wav|thumb|Nvda-mathml-example-3]], [[File:Nvda-mathml-example-4.wav|thumb|Nvda-mathml-example-4]], [[File:Nvda-mathml-example-5.wav|thumb|Nvda-mathml-example-5]], [[File:Nvda-mathml-example-6.wav|thumb|Nvda-mathml-example-6]], [[File:Nvda-mathml-example-7.wav|thumb|Nvda-mathml-example-7]].
** Orca: There is ongoing work, but no support at all at the moment [[File:Orca-mathml-example-1.wav|thumb|Orca-mathml-example-1]], [[File:Orca-mathml-example-2.wav|thumb|Orca-mathml-example-2]], [[File:Orca-mathml-example-3.wav|thumb|Orca-mathml-example-3]], [[File:Orca-mathml-example-4.wav|thumb|Orca-mathml-example-4]], [[File:Orca-mathml-example-5.wav|thumb|Orca-mathml-example-5]], [[File:Orca-mathml-example-6.wav|thumb|Orca-mathml-example-6]], [[File:Orca-mathml-example-7.wav|thumb|Orca-mathml-example-7]].
** From our testing, ChromeVox and JAWS are not able to read the formulas generated by the MathML mode.


==Relationships between different expansion properties==
==Test pages ==
The expansion parameters defined above are related to each other.
In particular, for any <math>d</math>-regular graph <math>G</math>,
:<math>h_{\text{out}}(G) \le h(G) \le d \cdot h_{\text{out}}(G)\,.</math>


Consequently, for constant degree graphs, vertex and edge expansion are qualitatively the same.
To test the '''MathML''', '''PNG''', and '''source''' rendering modes, please go to one of the following test pages:
*[[Displaystyle]]
*[[MathAxisAlignment]]
*[[Styling]]
*[[Linebreaking]]
*[[Unique Ids]]
*[[Help:Formula]]


===Cheeger inequalities===
*[[Inputtypes|Inputtypes (private Wikis only)]]
When <math>G</math> is <math>d</math>-regular, there is a relationship between <math>h(G)</math> and the spectral gap <math>d - \lambda_2</math> of <math>G</math>.  An inequality due to Tanner and independently [[Noga Alon|Alon]] and [[Vitali Milman|Milman]]{{Sfn|Alon|Spencer|2011}} states that
*[[Url2Image|Url2Image (private Wikis only)]]
 
==Bug reporting==
: <math>\frac{1}{2}(d - \lambda_2) \le h(G) \le \sqrt{2d(d - \lambda_2)}\,.</math><ref>Theorem 2.4 in {{harvtxt|Hoory|Linial|Widgerson|2006}}</ref>
If you find any bugs, please report them at [https://bugzilla.wikimedia.org/enter_bug.cgi?product=MediaWiki%20extensions&component=Math&version=master&short_desc=Math-preview%20rendering%20problem Bugzilla], or write an email to math_bugs (at) ckurs (dot) de .
 
This inequality is 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 ''&lambda;''<sub>2</sub> there corresponds to 2(''d''&nbsp;&minus;&nbsp;''&lambda;''<sub>2</sub>) 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{in}}(G) \le \sqrt{8(d-\lambda_2)}.</math>
Asymptotically speaking, the quantities
<math>\frac{h^2}{d}</math>, <math>h_{\text{out}}</math>, and <math>h_{\text{in}}^2</math> are all bounded above by the spectral gap <math>O(d-\lambda_2)</math>.
 
==Examples of expanders==
===Petersen graph===
[[image:Petersen graph blue.svg|thumb|The [[Petersen graph]]]]
Consider the 3-regular graph ''G'' on 10 vertices (''n'' = 10, ''d'' = 3) shown.
 
If we number the vertices by going around twice, starting with the outside pentagon and then the inside pentagon, ''G'' has the following adjacency matrix:
 
<math>
\begin{pmatrix}
0 & 1 & 0 & 0 & 1 & 1 & 0 & 0 & 0 & 0\\
1 & 0 & 1 & 0 & 0 & 0 & 1 & 0 & 0 & 0\\
0 & 1 & 0 & 1 & 0 & 0 & 0 & 1 & 0 & 0\\
0 & 0 & 1 & 0 & 1 & 0 & 0 & 0 & 1 & 0\\
1 & 0 & 0 & 1 & 0 & 0 & 0 & 0 & 0 & 1\\
1 & 0 & 0 & 0 & 0 & 0 & 0 & 1 & 1 & 0\\
0 & 1 & 0 & 0 & 0 & 0 & 0 & 0 & 1 & 1\\
0 & 0 & 1 & 0 & 0 & 1 & 0 & 0 & 0 & 1\\
0 & 0 & 0 & 1 & 0 & 1 & 1 & 0 & 0 & 0\\
0 & 0 & 0 & 0 & 1 & 0 & 1 & 1 & 0 & 0\\
\end{pmatrix}
</math>
 
One can calculate that the two largest eigenvalues of this matrix are 3 and 1.  From this, one may deduce that
 
<math>\frac{d - \lambda_2}{2} = \frac{3 - 1}{2} = 1</math>
 
<math>\sqrt{2 d (d - \lambda_2)} = \sqrt{2 \cdot 3 (3 - 1)} = 2 \sqrt{3}</math>
and consequently that <math>1 \leq h(G) \leq 2 \sqrt{3} \approx 3.46 </math>.
 
In fact, <math>h(G) = 1</math>. To persuade oneself of this, it suffices to consider the five vertices in the central star: there are five edges that touch exactly one of these vertices, giving an edge expansion for this set of 5/5 = 1.
 
===Ramanujan graphs===
By a theorem of Alon and Boppana, all large enough <math>d</math>-regular graphs satisfy <math>\lambda \ge 2\sqrt{d-1} - o(1)</math>.<ref>Theorem 2.7 of {{harvtxt|Hoory|Linial|Widgerson|2006}}</ref>
[[Ramanujan graph]]s are <math>d</math>-regular graphs that meet this bound, that is, they satisfy <math>\lambda \le 2\sqrt{d-1}</math>.<ref>Definition 5.11 of {{harvtxt|Hoory|Linial|Widgerson|2006}}</ref>
Hence Ramanujan graphs have an asymptotically smallest possible second-largest eigenvalue <math>\lambda</math> (in absolute value).
 
[[Alexander Lubotzky|Lubotzky]], Phillips, and Sarnak (1988), Margulis (1988), and Morgenstern (1994) show how Ramanujan graphs can be constructed explicitly.<ref>Theorem 5.12 of {{harvtxt|Hoory|Linial|Widgerson|2006}}</ref>
By a theorem of Friedman (2003), [[Random regular graph|random d-regular graphs]] on <math>n</math> vertices are almost Ramanujan, that is, they satisfy <math>\lambda \le 2\sqrt{d-1}+\epsilon</math> with probability <math>1-o(1)</math> as <math>n</math> tends to infinity.<ref>Theorem 7.10 of {{harvtxt|Hoory|Linial|Widgerson|2006}}</ref>
 
==Other examples==
[[Abstract algebra|Algebraic]] constructions based on [[Cayley graph]]s are known for various variants of expander graphs.
Most recently, combinatorial constructions of expanders have also been discovered.
 
==Applications and useful properties==
The original motivation for expanders is to build economical robust networks (phone or computer): an expander with bounded valence is precisely an asymptotic robust graph with number of edges growing linearly with size (number of vertices), for all subsets.
 
Expander graphs have found extensive applications in [[computer science]], in designing [[algorithm]]s, [[Expander code|error correcting codes]], [[Extractor (mathematics)|extractors]], [[pseudorandom generator]]s, [[sorting network]]s ({{harvtxt|Ajtai|Komlós|Szemerédi|1983}}) and robust [[computer network]]s. They have also been used in proofs of many important results in [[computational complexity theory]], such as [[SL (complexity)|SL]]=[[L (complexity)|L]] ({{harvtxt|Reingold|2008}}) and the [[PCP theorem]] ({{harvtxt|Dinur|2007}}). In [[cryptography]], expander graphs are used to construct [[hash function]]s.
 
The following are some properties of expander graphs that have proven useful in many areas.
 
===Expander mixing lemma===
{{Main|Expander mixing lemma}}
The expander mixing lemma states that, for any two subsets of the vertices <math>S, T \subseteq V</math>, the number of edges between <math>S</math> and <math>T</math> is approximately what you would expect in a random <math>d</math>-regular graph. The approximation is better, the smaller <math>\lambda=\max\{|\lambda_2|,|\lambda_n|\}</math> is.
In a random <math>d</math>-regular graph, as well as in an [[Erdős–Rényi model|Erdős–Rényi random graph]] with edge probability <math>d/n</math>, we expect <math>\frac{d}{n} \cdot |S| \cdot |T|</math> edges between <math>S</math> and <math>T</math>.
 
More formally, let <math>E(S, T)</math> denote the number of edges between <math>S</math> and <math>T</math>.
If the two sets are not disjoint, edges in their intersection are counted twice, that is,
<math>E(S,T)=2|E(G[S\cap T])| + E(S\setminus T,T) + E(S,T\setminus S)</math>.
 
Then the expander mixing lemma says that the following inequality holds:
:<math>\left|E(S, T) - \frac{d \cdot |S| \cdot |T|}{n}\right| \leq d\lambda  \sqrt{|S| \cdot |T|}\,.</math>
where <math>\lambda</math> is the absolute value of the '''normalized''' second largest eigenvalue.
 
===Expander walk sampling===
{{Main|Expander walk sampling}}
The [[Chernoff bound]] states that, when sampling many independent samples from a random variables in the range <math>[-1, 1]</math>, with high probability the average of our samples is close to the expectation of the random variable.  The expander walk sampling lemma, due to {{harvtxt|Ajtai|Komlós|Szemerédi|1987}} and {{harvtxt|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.
 
==See also==
*[[Algebraic connectivity]]
*[[Zig-zag product]]
 
==Notes==
{{Reflist|colwidth=25em}}
 
==References==
{{Refbegin|colwidth=25em}}
'''Textbooks and surveys'''
* {{cite book|title=The Probabilistic Method|first1=N.|last1=Alon|author1-link=Noga Alon|first2=Joel H.|last2=Spencer|author2-link=Joel Spencer|publisher=John Wiley & Sons|year=2011|edition=3rd|chapter=9.2. Eigenvalues and Expanders|ref=harv}}
* {{Citation | last=Chung |first=Fan R. K. | title=Spectral Graph Theory | series=CBMS Regional Conference Series in Mathematics | volume=92 | publisher=[[American Mathematical Society]] | year=1997 | isbn=0-8218-0315-8}}
* {{Citation | first1=Guiliana |last1=Davidoff | first2=Peter | last2=Sarnak | first3=Alain | last3=Valette | title=Elementary number theory, group theory and Ramanjuan graphs | publisher=[[Cambridge University Press]] | series=LMS student texts | volume=55 | year=2003 | isbn=0-521-53143-8}}
* {{Citation | first1=Shlomo | last1=Hoory | first2=Nathan | last2=Linial | author2-link = Nati Linial | first3=Avi | last3=Widgerson | author3-link = Avi Wigderson | title=Expander graphs and their applications | journal= Bulletin (New series) of the American Mathematical Society | volume=43 | issue=4 | pages=439–561 | url=http://www.cs.huji.ac.il/~nati/PAPERS/expander_survey.pdf | year=2006 | doi = 10.1090/S0273-0979-06-01126-8}}
* {{Citation | first1=Mike |last1=Krebs | first2=Anthony | last2=Shaheen | title=Expander families and Cayley graphs: A beginner's guide | publisher=Oxford University Press | year=2011 | isbn=0-19-976711-4}}
'''Research articles'''
* {{Citation|last1=Ajtai|first1=M.|author1-link=Miklós Ajtai|last2=Komlós|first2=J.|author2-link=János Komlós (mathematician)|last3=Szemerédi|first3=E.|author3-link=Endre Szemerédi|chapter=An O(n log n) sorting network|title=Proceedings of the 15th Annual ACM Symposium on Theory of Computing|pages=1–9|year=1983|doi=10.1145/800061.808726|isbn=0-89791-099-0}}
* {{Citation
| first1=M. | last1=Ajtai
| first2=J. | last2=Komlós
| first3=E. | last3=Szemerédi
| chapter=Deterministic simulation in LOGSPACE
| title=Proceedings of the 19th Annual ACM Symposium on Theory of Computing
| pages=132–140
| year=1987
| work=ACM
| doi=10.1145/28395.28410
| isbn=0-89791-221-7
}}
* {{cite doi|10.1109/SFCS.2002.1181884}}
* {{Citation
    |last1=Bobkov|first1=S.
    |last2=Houdré|first2=C.
    |last3=Tetali|first3=P.
    |title=λ<sub>∞</sub>, vertex isoperimetry and concentration|journal=Combinatorica|volume=20|issue=2|year=2000|doi=10.1007/s004930070018|pages = {153–172}}}.
* {{Citation|last=Dinur|first=Irit|title=The PCP theorem by gap amplification|journal=Journal of the ACM|volume=54|issue=3|year=2007|doi=10.1145/1236457.1236459|pages=12}}.
* {{Citation
| first=D. | last=Gillman
| title=A Chernoff Bound for Random Walks on Expander Graphs
| journal=SIAM Journal on Computing
| volume=27
| issue=4,
| pages=1203–1220
| year=1998
| publisher=Society for Industrial and Applied Mathematics
| doi=10.1137/S0097539794268765
}}
* {{Citation|first=Omer|last=Reingold|authorlink=Omer Reingold|title=Undirected connectivity in log-space|journal=[[Journal of the ACM]]|year=2008|
volume=55|issue=4|pages=Article 17, 24 pages|doi=10.1145/1391289.1391291
}}
{{Refend}}
 
== External links ==
* [http://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://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://www.yann-ollivier.org/specgraph/specgraph.html Definition and application of spectral gap]
 
{{DEFAULTSORT:Expander Graph}}
[[Category:Graph families]]
 
[[cs:Expander (graf)]]
[[fr:Graphe expanseur]]
[[he:גרף מרחיב]]
[[pl:Ekspander]]

Latest revision as of 23:52, 15 September 2019

This is a preview for the new MathML rendering mode (with SVG fallback), which is availble in production for registered users.

If you would like use the MathML rendering mode, you need a wikipedia user account that can be registered here [[1]]

  • Only registered users will be able to execute this rendering mode.
  • Note: you need not enter a email address (nor any other private information). Please do not use a password that you use elsewhere.

Registered users will be able to choose between the following three rendering modes:

MathML


Follow this link to change your Math rendering settings. You can also add a Custom CSS to force the MathML/SVG rendering or select different font families. See these examples.

Demos

Here are some demos:


Test pages

To test the MathML, PNG, and source rendering modes, please go to one of the following test pages:

Bug reporting

If you find any bugs, please report them at Bugzilla, or write an email to math_bugs (at) ckurs (dot) de .