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Glk (обсуждение | вклад) (Создана новая страница размером '''Adjacency operator''' --- оператор смежности. A directed infinite graph <math>G</math> is a pair of the set <math>V<...) |
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'''Adjacency operator''' | '''Adjacency operator''' — ''[[оператор смежности]].'' | ||
A directed infinite graph <math>G</math> is a pair of the set <math>V</math> of the | A directed [[infinite graph]] <math>\,G</math> is a pair of the set <math>\,V</math> of the | ||
countable vertices and the set <math>E</math> of the arrows (arcs) <math>u \leftarrow | countable [[vertex|vertices]] and the set <math>\,E</math> of the arrows (arcs) <math>u \leftarrow v</math>. Let <math>{\mathcal H}</math> be a Hilbert space <math>\ell^{2}(G)</math> on <math>\,V</math> with a canonical basis <math>\{e_{v}| \; v \in V\}</math>. Since every arrow <math>u \leftarrow v \in E</math> induces a dyad <math>e_{u} \otimes e_{v}</math>, where <math>(x \otimes y)z = \langle z,y\rangle x</math> for <math>x, y, z \in {\mathcal H}</math>, the ''' adjacency operator''' <math>\,A(G)</math> is expressed by | ||
v</math>. Let <math>{\mathcal H}</math> be a Hilbert space <math>\ell^{2}(G)</math> on <math>V</math> with a canonical basis <math>\{e_{v}| \; v \in V\}</math>. Since every arrow <math>u | |||
\leftarrow v \in E</math> induces a dyad <math>e_{u} \otimes e_{v}</math>, where <math>(x | |||
\otimes y)z = \langle z,y\rangle x</math> for <math>x, y, z \in {\mathcal H}</math>, the | |||
''' adjacency operator''' <math>A(G)</math> is expressed by | |||
<math>A(G) = \sum_{u \leftarrow v} e_{u} \otimes e_{v}</math> | <math>A(G) = \sum_{u \leftarrow v} e_{u} \otimes e_{v}</math> | ||
if <math>G</math> has a bounded degree. | if <math>\,G</math> has a bounded degree. | ||
Adjacency operators are classified as follows: | Adjacency operators are classified as follows: | ||
* <math>A</math> is '''self-adjoint''' if <math>A = A^{\ast}</math>. | * <math>\,A</math> is '''self-adjoint''' if <math>A = A^{\ast}</math>. | ||
* <math>A</math> is '''unitary''' if <math>A^{\ast}A = AA^{\ast} = I</math>. | * <math>\,A</math> is '''unitary''' if <math>A^{\ast}A = AA^{\ast} = I</math>. | ||
* <math>A</math> is '''normal''' if <math>A^{\ast}A = AA^{\ast}</math>. | * <math>\,A</math> is '''normal''' if <math>A^{\ast}A = AA^{\ast}</math>. | ||
* <math>A</math> is '''hyponormal''' (resp. '''co-hyponormal''') if <math>A^{\ast}A \geq AA^{\ast}</math> (resp. <math>AA^{\ast} \geq A^{\ast}A</math>). | * <math>\,A</math> is '''hyponormal''' (resp. '''co-hyponormal''') if <math>A^{\ast}A \geq AA^{\ast}</math> (resp. <math>AA^{\ast} \geq A^{\ast}A</math>). | ||
* <math>A</math> is '''projection''' if <math>A = A^{\ast} = A^{2}</math>. | * <math>\,A</math> is '''projection''' if <math>A = A^{\ast} = A^{2}</math>. | ||
* <math>A</math> is '''partial isometry''' if <math>A^{\ast}A</math> and <math>AA^{\ast}</math>. | * <math>\,A</math> is '''partial isometry''' if <math>A^{\ast}A</math> and <math>AA^{\ast}</math>. | ||
* <math>A</math> is '''isometry''' (resp. '''co-isometry''') if <math>A^{\ast}A = I</math> (resp.<math>AA^{\ast} = I</math>). | * <math>\,A</math> is '''isometry''' (resp. '''co-isometry''') if <math>A^{\ast}A = I</math> (resp.<math>AA^{\ast} = I</math>). | ||
* <math>A</math> is '''nilpotent''' if there exists a number <math>n</math> such that <math>A^{n} = | * <math>\,A</math> is '''nilpotent''' if there exists a number <math>\,n</math> such that <math>\,A^{n} = 0</math>. | ||
0</math>. | * <math>\,A</math> is '''idempotent''' if <math>\,A = A^{2}</math>. | ||
* <math>A</math> is '''idempotent''' if <math>A = A^{2}</math>. | * <math>\,A</math> is '''positive''' if <math>(Ax|x) \geq 0</math> for <math>x \in H</math>. | ||
* <math>A</math> is '''positive''' if <math>(Ax|x) \geq 0</math> for <math>x \in H</math>. | |||
Here <math>G^{\ast}</math> is the '' adjoint'' graph for a graph <math>G</math>. | Here <math>G^{\ast}</math> is the '' adjoint'' graph for a graph <math>\,G</math>. |