Isoperimetric constant on random graph
$begingroup$
Show that there is a constant $c=c(p) > 0 $ such that almost all graphs in $mathcal{G}_{n,p}$ verify the following property : for each subset $X in V(G)$ with cardinality $|X|leq n/2$,
$$ e(X, Vbackslash X) geq c |X| $$
Where $ e(X, Vbackslash X)$ denotes the number of edges connecting $X$ and $Vbackslash X$.
I found a "standard" solution, using combinatorial arguments (the constant $c(p)=p$ satisfies the condition), but I have the feeling that a "more elegant" proof should exist.
My intuition is as follow : the problem is equivalent to proving, with $i(G)$ the isoperimetric constant :
$$ forall p, exists c(p)>0, s.t. mathbb{P}[ i(G) > c] rightarrow 1 text{ when }nrightarrow infty $$
And for any graph $G$, we know a lower bound for $i(G)$:
$$ mu_2 /2 leq i(G)$$
With $mu_2$ being the second smallest eigenvalue of the Laplacian matrix of $G$. Now if I can find some bound for $mu_2$ I should be able to do something.
I know that for fixed $p$ the probability that $G$ is connected tends to 1, hence $mu_2 > 0$. But can we find similar argument for $mu_2 > c$ for some constant $c$ ? in term of connectivity surely?
Thanks for the help!
graph-theory eigenvalues-eigenvectors random-graphs
$endgroup$
add a comment |
$begingroup$
Show that there is a constant $c=c(p) > 0 $ such that almost all graphs in $mathcal{G}_{n,p}$ verify the following property : for each subset $X in V(G)$ with cardinality $|X|leq n/2$,
$$ e(X, Vbackslash X) geq c |X| $$
Where $ e(X, Vbackslash X)$ denotes the number of edges connecting $X$ and $Vbackslash X$.
I found a "standard" solution, using combinatorial arguments (the constant $c(p)=p$ satisfies the condition), but I have the feeling that a "more elegant" proof should exist.
My intuition is as follow : the problem is equivalent to proving, with $i(G)$ the isoperimetric constant :
$$ forall p, exists c(p)>0, s.t. mathbb{P}[ i(G) > c] rightarrow 1 text{ when }nrightarrow infty $$
And for any graph $G$, we know a lower bound for $i(G)$:
$$ mu_2 /2 leq i(G)$$
With $mu_2$ being the second smallest eigenvalue of the Laplacian matrix of $G$. Now if I can find some bound for $mu_2$ I should be able to do something.
I know that for fixed $p$ the probability that $G$ is connected tends to 1, hence $mu_2 > 0$. But can we find similar argument for $mu_2 > c$ for some constant $c$ ? in term of connectivity surely?
Thanks for the help!
graph-theory eigenvalues-eigenvectors random-graphs
$endgroup$
add a comment |
$begingroup$
Show that there is a constant $c=c(p) > 0 $ such that almost all graphs in $mathcal{G}_{n,p}$ verify the following property : for each subset $X in V(G)$ with cardinality $|X|leq n/2$,
$$ e(X, Vbackslash X) geq c |X| $$
Where $ e(X, Vbackslash X)$ denotes the number of edges connecting $X$ and $Vbackslash X$.
I found a "standard" solution, using combinatorial arguments (the constant $c(p)=p$ satisfies the condition), but I have the feeling that a "more elegant" proof should exist.
My intuition is as follow : the problem is equivalent to proving, with $i(G)$ the isoperimetric constant :
$$ forall p, exists c(p)>0, s.t. mathbb{P}[ i(G) > c] rightarrow 1 text{ when }nrightarrow infty $$
And for any graph $G$, we know a lower bound for $i(G)$:
$$ mu_2 /2 leq i(G)$$
With $mu_2$ being the second smallest eigenvalue of the Laplacian matrix of $G$. Now if I can find some bound for $mu_2$ I should be able to do something.
I know that for fixed $p$ the probability that $G$ is connected tends to 1, hence $mu_2 > 0$. But can we find similar argument for $mu_2 > c$ for some constant $c$ ? in term of connectivity surely?
Thanks for the help!
graph-theory eigenvalues-eigenvectors random-graphs
$endgroup$
Show that there is a constant $c=c(p) > 0 $ such that almost all graphs in $mathcal{G}_{n,p}$ verify the following property : for each subset $X in V(G)$ with cardinality $|X|leq n/2$,
$$ e(X, Vbackslash X) geq c |X| $$
Where $ e(X, Vbackslash X)$ denotes the number of edges connecting $X$ and $Vbackslash X$.
I found a "standard" solution, using combinatorial arguments (the constant $c(p)=p$ satisfies the condition), but I have the feeling that a "more elegant" proof should exist.
My intuition is as follow : the problem is equivalent to proving, with $i(G)$ the isoperimetric constant :
$$ forall p, exists c(p)>0, s.t. mathbb{P}[ i(G) > c] rightarrow 1 text{ when }nrightarrow infty $$
And for any graph $G$, we know a lower bound for $i(G)$:
$$ mu_2 /2 leq i(G)$$
With $mu_2$ being the second smallest eigenvalue of the Laplacian matrix of $G$. Now if I can find some bound for $mu_2$ I should be able to do something.
I know that for fixed $p$ the probability that $G$ is connected tends to 1, hence $mu_2 > 0$. But can we find similar argument for $mu_2 > c$ for some constant $c$ ? in term of connectivity surely?
Thanks for the help!
graph-theory eigenvalues-eigenvectors random-graphs
graph-theory eigenvalues-eigenvectors random-graphs
edited Jan 5 at 18:35
David G. Stork
11k31432
11k31432
asked Jan 5 at 18:25
Thomas LesgourguesThomas Lesgourgues
71517
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From this paper we can estimate the normalized Laplacian spectrum of $mathcal G_{n,p}$ from the spectrum of an "average-case Laplacian" $$bar{L} = I - bar{D}^{-1/2} bar{A}bar{D}^{-1/2}$$
where $bar{D} = (n-1)pI$ is the expected value of $D$, and $bar{A} = p(J-I)$ is the expected value of $A$. (As usual, $J$ is the all-ones matrix.) Since $bar{D}$ commutes with everything, we can rewrite this as $I - bar{D}^{-1}bar{A}$ which simplifies to$$frac{n}{n-1}I - frac{1}{n-1}J.$$ The eigenvalues of $J$ are $n,0,0,dots,0,0$ and so the eigenvalues of $bar{L}$ are $0, frac{n}{n-1}, frac{n}{n-1}, dots, frac{n}{n-1}$.
This looks like a rather stupid estimate that doesn't depend on $p$, but the dependence on $p$ is hidden in the error bound. For all constant $epsilon>0$, we have $$|lambda_i(L) - lambda_i(bar{L})| le mathcal Oleft(sqrt{frac{log(n/epsilon)}{(n-1)p}}right)$$ provided $(n-1)p > k(epsilon)log n$. In other words, as long as $p$ is not a too-small function of $n$, we have $lambda_2(L) ge 1 - o(1)$ with high probability.
I guess Theorem 4 in the paper provides a slightly-tighter answer more easily, but then this answer would have been too short. (Also I didn't find Theorem 4 until I wrote all of the above.)
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$begingroup$
From this paper we can estimate the normalized Laplacian spectrum of $mathcal G_{n,p}$ from the spectrum of an "average-case Laplacian" $$bar{L} = I - bar{D}^{-1/2} bar{A}bar{D}^{-1/2}$$
where $bar{D} = (n-1)pI$ is the expected value of $D$, and $bar{A} = p(J-I)$ is the expected value of $A$. (As usual, $J$ is the all-ones matrix.) Since $bar{D}$ commutes with everything, we can rewrite this as $I - bar{D}^{-1}bar{A}$ which simplifies to$$frac{n}{n-1}I - frac{1}{n-1}J.$$ The eigenvalues of $J$ are $n,0,0,dots,0,0$ and so the eigenvalues of $bar{L}$ are $0, frac{n}{n-1}, frac{n}{n-1}, dots, frac{n}{n-1}$.
This looks like a rather stupid estimate that doesn't depend on $p$, but the dependence on $p$ is hidden in the error bound. For all constant $epsilon>0$, we have $$|lambda_i(L) - lambda_i(bar{L})| le mathcal Oleft(sqrt{frac{log(n/epsilon)}{(n-1)p}}right)$$ provided $(n-1)p > k(epsilon)log n$. In other words, as long as $p$ is not a too-small function of $n$, we have $lambda_2(L) ge 1 - o(1)$ with high probability.
I guess Theorem 4 in the paper provides a slightly-tighter answer more easily, but then this answer would have been too short. (Also I didn't find Theorem 4 until I wrote all of the above.)
$endgroup$
add a comment |
$begingroup$
From this paper we can estimate the normalized Laplacian spectrum of $mathcal G_{n,p}$ from the spectrum of an "average-case Laplacian" $$bar{L} = I - bar{D}^{-1/2} bar{A}bar{D}^{-1/2}$$
where $bar{D} = (n-1)pI$ is the expected value of $D$, and $bar{A} = p(J-I)$ is the expected value of $A$. (As usual, $J$ is the all-ones matrix.) Since $bar{D}$ commutes with everything, we can rewrite this as $I - bar{D}^{-1}bar{A}$ which simplifies to$$frac{n}{n-1}I - frac{1}{n-1}J.$$ The eigenvalues of $J$ are $n,0,0,dots,0,0$ and so the eigenvalues of $bar{L}$ are $0, frac{n}{n-1}, frac{n}{n-1}, dots, frac{n}{n-1}$.
This looks like a rather stupid estimate that doesn't depend on $p$, but the dependence on $p$ is hidden in the error bound. For all constant $epsilon>0$, we have $$|lambda_i(L) - lambda_i(bar{L})| le mathcal Oleft(sqrt{frac{log(n/epsilon)}{(n-1)p}}right)$$ provided $(n-1)p > k(epsilon)log n$. In other words, as long as $p$ is not a too-small function of $n$, we have $lambda_2(L) ge 1 - o(1)$ with high probability.
I guess Theorem 4 in the paper provides a slightly-tighter answer more easily, but then this answer would have been too short. (Also I didn't find Theorem 4 until I wrote all of the above.)
$endgroup$
add a comment |
$begingroup$
From this paper we can estimate the normalized Laplacian spectrum of $mathcal G_{n,p}$ from the spectrum of an "average-case Laplacian" $$bar{L} = I - bar{D}^{-1/2} bar{A}bar{D}^{-1/2}$$
where $bar{D} = (n-1)pI$ is the expected value of $D$, and $bar{A} = p(J-I)$ is the expected value of $A$. (As usual, $J$ is the all-ones matrix.) Since $bar{D}$ commutes with everything, we can rewrite this as $I - bar{D}^{-1}bar{A}$ which simplifies to$$frac{n}{n-1}I - frac{1}{n-1}J.$$ The eigenvalues of $J$ are $n,0,0,dots,0,0$ and so the eigenvalues of $bar{L}$ are $0, frac{n}{n-1}, frac{n}{n-1}, dots, frac{n}{n-1}$.
This looks like a rather stupid estimate that doesn't depend on $p$, but the dependence on $p$ is hidden in the error bound. For all constant $epsilon>0$, we have $$|lambda_i(L) - lambda_i(bar{L})| le mathcal Oleft(sqrt{frac{log(n/epsilon)}{(n-1)p}}right)$$ provided $(n-1)p > k(epsilon)log n$. In other words, as long as $p$ is not a too-small function of $n$, we have $lambda_2(L) ge 1 - o(1)$ with high probability.
I guess Theorem 4 in the paper provides a slightly-tighter answer more easily, but then this answer would have been too short. (Also I didn't find Theorem 4 until I wrote all of the above.)
$endgroup$
From this paper we can estimate the normalized Laplacian spectrum of $mathcal G_{n,p}$ from the spectrum of an "average-case Laplacian" $$bar{L} = I - bar{D}^{-1/2} bar{A}bar{D}^{-1/2}$$
where $bar{D} = (n-1)pI$ is the expected value of $D$, and $bar{A} = p(J-I)$ is the expected value of $A$. (As usual, $J$ is the all-ones matrix.) Since $bar{D}$ commutes with everything, we can rewrite this as $I - bar{D}^{-1}bar{A}$ which simplifies to$$frac{n}{n-1}I - frac{1}{n-1}J.$$ The eigenvalues of $J$ are $n,0,0,dots,0,0$ and so the eigenvalues of $bar{L}$ are $0, frac{n}{n-1}, frac{n}{n-1}, dots, frac{n}{n-1}$.
This looks like a rather stupid estimate that doesn't depend on $p$, but the dependence on $p$ is hidden in the error bound. For all constant $epsilon>0$, we have $$|lambda_i(L) - lambda_i(bar{L})| le mathcal Oleft(sqrt{frac{log(n/epsilon)}{(n-1)p}}right)$$ provided $(n-1)p > k(epsilon)log n$. In other words, as long as $p$ is not a too-small function of $n$, we have $lambda_2(L) ge 1 - o(1)$ with high probability.
I guess Theorem 4 in the paper provides a slightly-tighter answer more easily, but then this answer would have been too short. (Also I didn't find Theorem 4 until I wrote all of the above.)
answered Jan 6 at 16:07
Misha LavrovMisha Lavrov
46k656107
46k656107
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