Can I make general formula for this problem
$begingroup$
I want to find how many pairs of numbers satisfy this condition on $[1,n]$.
For given $n$ , how many pairs $(a,b)$ are there such that $gcd(a,b) = 2^t , t > 0 $ for some whole number $t$.
All pairs $(a,b)$ should be bounded by $1leq a < b leq n $ .
Now I know that if $2|a land2|b implies 2|gcd(a,b)$ and this excludes all odd numbers .
But the space is too big to count for very large $n$.
Can I make general formula for $forall n $ ?
$a,b,n,t$ are whole numbers.
number-theory greatest-common-divisor
$endgroup$
add a comment |
$begingroup$
I want to find how many pairs of numbers satisfy this condition on $[1,n]$.
For given $n$ , how many pairs $(a,b)$ are there such that $gcd(a,b) = 2^t , t > 0 $ for some whole number $t$.
All pairs $(a,b)$ should be bounded by $1leq a < b leq n $ .
Now I know that if $2|a land2|b implies 2|gcd(a,b)$ and this excludes all odd numbers .
But the space is too big to count for very large $n$.
Can I make general formula for $forall n $ ?
$a,b,n,t$ are whole numbers.
number-theory greatest-common-divisor
$endgroup$
$begingroup$
Is an asymptotic answer sufficient? It's not too hard to figure out that, if $f(n)$ is the number of such pairs, then $lim_{nrightarrowinfty}frac{f(n)}{n^2}$ is positive and finite (and it's not even so hard to compute this constant). I don't see how one would get an exact answer for all $n$ though without considerable computation.
$endgroup$
– Milo Brandt
Jan 2 at 0:10
$begingroup$
that is the main problem here, for $n = 10^{6} $ , with brute force it takes about 3-4 hours to compute them , if its not possible for a general formula to be made maybe decreasing the search space will help but this of course requires more properties for such pairs
$endgroup$
– Noodle
Jan 2 at 0:15
add a comment |
$begingroup$
I want to find how many pairs of numbers satisfy this condition on $[1,n]$.
For given $n$ , how many pairs $(a,b)$ are there such that $gcd(a,b) = 2^t , t > 0 $ for some whole number $t$.
All pairs $(a,b)$ should be bounded by $1leq a < b leq n $ .
Now I know that if $2|a land2|b implies 2|gcd(a,b)$ and this excludes all odd numbers .
But the space is too big to count for very large $n$.
Can I make general formula for $forall n $ ?
$a,b,n,t$ are whole numbers.
number-theory greatest-common-divisor
$endgroup$
I want to find how many pairs of numbers satisfy this condition on $[1,n]$.
For given $n$ , how many pairs $(a,b)$ are there such that $gcd(a,b) = 2^t , t > 0 $ for some whole number $t$.
All pairs $(a,b)$ should be bounded by $1leq a < b leq n $ .
Now I know that if $2|a land2|b implies 2|gcd(a,b)$ and this excludes all odd numbers .
But the space is too big to count for very large $n$.
Can I make general formula for $forall n $ ?
$a,b,n,t$ are whole numbers.
number-theory greatest-common-divisor
number-theory greatest-common-divisor
asked Jan 2 at 0:04
NoodleNoodle
717
717
$begingroup$
Is an asymptotic answer sufficient? It's not too hard to figure out that, if $f(n)$ is the number of such pairs, then $lim_{nrightarrowinfty}frac{f(n)}{n^2}$ is positive and finite (and it's not even so hard to compute this constant). I don't see how one would get an exact answer for all $n$ though without considerable computation.
$endgroup$
– Milo Brandt
Jan 2 at 0:10
$begingroup$
that is the main problem here, for $n = 10^{6} $ , with brute force it takes about 3-4 hours to compute them , if its not possible for a general formula to be made maybe decreasing the search space will help but this of course requires more properties for such pairs
$endgroup$
– Noodle
Jan 2 at 0:15
add a comment |
$begingroup$
Is an asymptotic answer sufficient? It's not too hard to figure out that, if $f(n)$ is the number of such pairs, then $lim_{nrightarrowinfty}frac{f(n)}{n^2}$ is positive and finite (and it's not even so hard to compute this constant). I don't see how one would get an exact answer for all $n$ though without considerable computation.
$endgroup$
– Milo Brandt
Jan 2 at 0:10
$begingroup$
that is the main problem here, for $n = 10^{6} $ , with brute force it takes about 3-4 hours to compute them , if its not possible for a general formula to be made maybe decreasing the search space will help but this of course requires more properties for such pairs
$endgroup$
– Noodle
Jan 2 at 0:15
$begingroup$
Is an asymptotic answer sufficient? It's not too hard to figure out that, if $f(n)$ is the number of such pairs, then $lim_{nrightarrowinfty}frac{f(n)}{n^2}$ is positive and finite (and it's not even so hard to compute this constant). I don't see how one would get an exact answer for all $n$ though without considerable computation.
$endgroup$
– Milo Brandt
Jan 2 at 0:10
$begingroup$
Is an asymptotic answer sufficient? It's not too hard to figure out that, if $f(n)$ is the number of such pairs, then $lim_{nrightarrowinfty}frac{f(n)}{n^2}$ is positive and finite (and it's not even so hard to compute this constant). I don't see how one would get an exact answer for all $n$ though without considerable computation.
$endgroup$
– Milo Brandt
Jan 2 at 0:10
$begingroup$
that is the main problem here, for $n = 10^{6} $ , with brute force it takes about 3-4 hours to compute them , if its not possible for a general formula to be made maybe decreasing the search space will help but this of course requires more properties for such pairs
$endgroup$
– Noodle
Jan 2 at 0:15
$begingroup$
that is the main problem here, for $n = 10^{6} $ , with brute force it takes about 3-4 hours to compute them , if its not possible for a general formula to be made maybe decreasing the search space will help but this of course requires more properties for such pairs
$endgroup$
– Noodle
Jan 2 at 0:15
add a comment |
1 Answer
1
active
oldest
votes
$begingroup$
Let $psi(n)=#{(x,y) : 1 leqslant x,y leqslant n, gcd(x, y) = 1}$. Then, for $1 leqslant d leqslant n$,
$$#{(x,y) : 1 leqslant x,y leqslant n, gcd(x, y) = d} = psibig(lfloor n/d rfloorbig),$$
and the union of these sets is just ${(x,y) : 1 leqslant x,y leqslant n}$. This gives
$$color{blue}{sum_{d=1}^{n}psibig(lfloor n/d rfloorbig)=n^2} implies psi(n)=sum_{d=1}^{n}mu(d)lfloor n/d rfloor^2$$
(by the "second" Möbius inversion formula). This leads to a solution of your problem:
$$2^t leqslant n implies #{(a, b) : 1 leqslant a < b leqslant n, gcd(a, b) = 2^t } = frac{psi(lfloor 2^{-t} n rfloor) - 1}{2}.$$
There's an algorithm which computes $psi(n)$ in $mathcal{O}(n^{1+epsilon})$ time and $mathcal{O}(n^{1/2+epsilon})$ space (without computing any values of $mu$). The idea is to use the "blue" formula above recursively (or rather iteratively), noting that there are just $mathcal{O}(sqrt{n})$ different values of $lfloor n/d rfloor$ for $1 leqslant d leqslant n$, which allows to simplify the sum; namely, for any $1 leqslant k leqslant n$,
$$n^2=sum_{d=1}^{n}psileft(leftlfloorfrac{n}{d}rightrfloorright)=sum_{d=1}^{lfloor n/(k+1) rfloor}psileft(leftlfloorfrac{n}{d}rightrfloorright)+sum_{d=1}^{k}psi(d)left(leftlfloorfrac{n}{d}rightrfloor-leftlfloorfrac{n}{d+1}rightrfloorright),$$
and we may put $k=lfloorsqrt{n}rfloor$ here. This recurrence for $psi(n)$ gives the algorithm.
$endgroup$
$begingroup$
I was just going to ask how do you compute $ psi (n) $ , it will help lots if you can or provide some info
$endgroup$
– Noodle
Jan 2 at 0:38
$begingroup$
How does one compute $mu (d)$
$endgroup$
– Noodle
Jan 2 at 0:45
$begingroup$
The formula for $psi$ with $mu$ is still of use (to show that $displaystylelim_{ntoinfty}frac{psi(n)}{n^2} = frac{6}{pi^2}$ - see comments to the OP).
$endgroup$
– metamorphy
Jan 2 at 1:45
$begingroup$
Does $$psi (n) = n prod_{p|n}(1+frac{1}{p})$$ here ?
$endgroup$
– Noodle
Jan 2 at 2:15
$begingroup$
No, there's no such simple formula here.
$endgroup$
– metamorphy
Jan 2 at 2:21
|
show 2 more comments
Your Answer
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$begingroup$
Let $psi(n)=#{(x,y) : 1 leqslant x,y leqslant n, gcd(x, y) = 1}$. Then, for $1 leqslant d leqslant n$,
$$#{(x,y) : 1 leqslant x,y leqslant n, gcd(x, y) = d} = psibig(lfloor n/d rfloorbig),$$
and the union of these sets is just ${(x,y) : 1 leqslant x,y leqslant n}$. This gives
$$color{blue}{sum_{d=1}^{n}psibig(lfloor n/d rfloorbig)=n^2} implies psi(n)=sum_{d=1}^{n}mu(d)lfloor n/d rfloor^2$$
(by the "second" Möbius inversion formula). This leads to a solution of your problem:
$$2^t leqslant n implies #{(a, b) : 1 leqslant a < b leqslant n, gcd(a, b) = 2^t } = frac{psi(lfloor 2^{-t} n rfloor) - 1}{2}.$$
There's an algorithm which computes $psi(n)$ in $mathcal{O}(n^{1+epsilon})$ time and $mathcal{O}(n^{1/2+epsilon})$ space (without computing any values of $mu$). The idea is to use the "blue" formula above recursively (or rather iteratively), noting that there are just $mathcal{O}(sqrt{n})$ different values of $lfloor n/d rfloor$ for $1 leqslant d leqslant n$, which allows to simplify the sum; namely, for any $1 leqslant k leqslant n$,
$$n^2=sum_{d=1}^{n}psileft(leftlfloorfrac{n}{d}rightrfloorright)=sum_{d=1}^{lfloor n/(k+1) rfloor}psileft(leftlfloorfrac{n}{d}rightrfloorright)+sum_{d=1}^{k}psi(d)left(leftlfloorfrac{n}{d}rightrfloor-leftlfloorfrac{n}{d+1}rightrfloorright),$$
and we may put $k=lfloorsqrt{n}rfloor$ here. This recurrence for $psi(n)$ gives the algorithm.
$endgroup$
$begingroup$
I was just going to ask how do you compute $ psi (n) $ , it will help lots if you can or provide some info
$endgroup$
– Noodle
Jan 2 at 0:38
$begingroup$
How does one compute $mu (d)$
$endgroup$
– Noodle
Jan 2 at 0:45
$begingroup$
The formula for $psi$ with $mu$ is still of use (to show that $displaystylelim_{ntoinfty}frac{psi(n)}{n^2} = frac{6}{pi^2}$ - see comments to the OP).
$endgroup$
– metamorphy
Jan 2 at 1:45
$begingroup$
Does $$psi (n) = n prod_{p|n}(1+frac{1}{p})$$ here ?
$endgroup$
– Noodle
Jan 2 at 2:15
$begingroup$
No, there's no such simple formula here.
$endgroup$
– metamorphy
Jan 2 at 2:21
|
show 2 more comments
$begingroup$
Let $psi(n)=#{(x,y) : 1 leqslant x,y leqslant n, gcd(x, y) = 1}$. Then, for $1 leqslant d leqslant n$,
$$#{(x,y) : 1 leqslant x,y leqslant n, gcd(x, y) = d} = psibig(lfloor n/d rfloorbig),$$
and the union of these sets is just ${(x,y) : 1 leqslant x,y leqslant n}$. This gives
$$color{blue}{sum_{d=1}^{n}psibig(lfloor n/d rfloorbig)=n^2} implies psi(n)=sum_{d=1}^{n}mu(d)lfloor n/d rfloor^2$$
(by the "second" Möbius inversion formula). This leads to a solution of your problem:
$$2^t leqslant n implies #{(a, b) : 1 leqslant a < b leqslant n, gcd(a, b) = 2^t } = frac{psi(lfloor 2^{-t} n rfloor) - 1}{2}.$$
There's an algorithm which computes $psi(n)$ in $mathcal{O}(n^{1+epsilon})$ time and $mathcal{O}(n^{1/2+epsilon})$ space (without computing any values of $mu$). The idea is to use the "blue" formula above recursively (or rather iteratively), noting that there are just $mathcal{O}(sqrt{n})$ different values of $lfloor n/d rfloor$ for $1 leqslant d leqslant n$, which allows to simplify the sum; namely, for any $1 leqslant k leqslant n$,
$$n^2=sum_{d=1}^{n}psileft(leftlfloorfrac{n}{d}rightrfloorright)=sum_{d=1}^{lfloor n/(k+1) rfloor}psileft(leftlfloorfrac{n}{d}rightrfloorright)+sum_{d=1}^{k}psi(d)left(leftlfloorfrac{n}{d}rightrfloor-leftlfloorfrac{n}{d+1}rightrfloorright),$$
and we may put $k=lfloorsqrt{n}rfloor$ here. This recurrence for $psi(n)$ gives the algorithm.
$endgroup$
$begingroup$
I was just going to ask how do you compute $ psi (n) $ , it will help lots if you can or provide some info
$endgroup$
– Noodle
Jan 2 at 0:38
$begingroup$
How does one compute $mu (d)$
$endgroup$
– Noodle
Jan 2 at 0:45
$begingroup$
The formula for $psi$ with $mu$ is still of use (to show that $displaystylelim_{ntoinfty}frac{psi(n)}{n^2} = frac{6}{pi^2}$ - see comments to the OP).
$endgroup$
– metamorphy
Jan 2 at 1:45
$begingroup$
Does $$psi (n) = n prod_{p|n}(1+frac{1}{p})$$ here ?
$endgroup$
– Noodle
Jan 2 at 2:15
$begingroup$
No, there's no such simple formula here.
$endgroup$
– metamorphy
Jan 2 at 2:21
|
show 2 more comments
$begingroup$
Let $psi(n)=#{(x,y) : 1 leqslant x,y leqslant n, gcd(x, y) = 1}$. Then, for $1 leqslant d leqslant n$,
$$#{(x,y) : 1 leqslant x,y leqslant n, gcd(x, y) = d} = psibig(lfloor n/d rfloorbig),$$
and the union of these sets is just ${(x,y) : 1 leqslant x,y leqslant n}$. This gives
$$color{blue}{sum_{d=1}^{n}psibig(lfloor n/d rfloorbig)=n^2} implies psi(n)=sum_{d=1}^{n}mu(d)lfloor n/d rfloor^2$$
(by the "second" Möbius inversion formula). This leads to a solution of your problem:
$$2^t leqslant n implies #{(a, b) : 1 leqslant a < b leqslant n, gcd(a, b) = 2^t } = frac{psi(lfloor 2^{-t} n rfloor) - 1}{2}.$$
There's an algorithm which computes $psi(n)$ in $mathcal{O}(n^{1+epsilon})$ time and $mathcal{O}(n^{1/2+epsilon})$ space (without computing any values of $mu$). The idea is to use the "blue" formula above recursively (or rather iteratively), noting that there are just $mathcal{O}(sqrt{n})$ different values of $lfloor n/d rfloor$ for $1 leqslant d leqslant n$, which allows to simplify the sum; namely, for any $1 leqslant k leqslant n$,
$$n^2=sum_{d=1}^{n}psileft(leftlfloorfrac{n}{d}rightrfloorright)=sum_{d=1}^{lfloor n/(k+1) rfloor}psileft(leftlfloorfrac{n}{d}rightrfloorright)+sum_{d=1}^{k}psi(d)left(leftlfloorfrac{n}{d}rightrfloor-leftlfloorfrac{n}{d+1}rightrfloorright),$$
and we may put $k=lfloorsqrt{n}rfloor$ here. This recurrence for $psi(n)$ gives the algorithm.
$endgroup$
Let $psi(n)=#{(x,y) : 1 leqslant x,y leqslant n, gcd(x, y) = 1}$. Then, for $1 leqslant d leqslant n$,
$$#{(x,y) : 1 leqslant x,y leqslant n, gcd(x, y) = d} = psibig(lfloor n/d rfloorbig),$$
and the union of these sets is just ${(x,y) : 1 leqslant x,y leqslant n}$. This gives
$$color{blue}{sum_{d=1}^{n}psibig(lfloor n/d rfloorbig)=n^2} implies psi(n)=sum_{d=1}^{n}mu(d)lfloor n/d rfloor^2$$
(by the "second" Möbius inversion formula). This leads to a solution of your problem:
$$2^t leqslant n implies #{(a, b) : 1 leqslant a < b leqslant n, gcd(a, b) = 2^t } = frac{psi(lfloor 2^{-t} n rfloor) - 1}{2}.$$
There's an algorithm which computes $psi(n)$ in $mathcal{O}(n^{1+epsilon})$ time and $mathcal{O}(n^{1/2+epsilon})$ space (without computing any values of $mu$). The idea is to use the "blue" formula above recursively (or rather iteratively), noting that there are just $mathcal{O}(sqrt{n})$ different values of $lfloor n/d rfloor$ for $1 leqslant d leqslant n$, which allows to simplify the sum; namely, for any $1 leqslant k leqslant n$,
$$n^2=sum_{d=1}^{n}psileft(leftlfloorfrac{n}{d}rightrfloorright)=sum_{d=1}^{lfloor n/(k+1) rfloor}psileft(leftlfloorfrac{n}{d}rightrfloorright)+sum_{d=1}^{k}psi(d)left(leftlfloorfrac{n}{d}rightrfloor-leftlfloorfrac{n}{d+1}rightrfloorright),$$
and we may put $k=lfloorsqrt{n}rfloor$ here. This recurrence for $psi(n)$ gives the algorithm.
edited Jan 2 at 3:19
answered Jan 2 at 0:30
metamorphymetamorphy
3,6821621
3,6821621
$begingroup$
I was just going to ask how do you compute $ psi (n) $ , it will help lots if you can or provide some info
$endgroup$
– Noodle
Jan 2 at 0:38
$begingroup$
How does one compute $mu (d)$
$endgroup$
– Noodle
Jan 2 at 0:45
$begingroup$
The formula for $psi$ with $mu$ is still of use (to show that $displaystylelim_{ntoinfty}frac{psi(n)}{n^2} = frac{6}{pi^2}$ - see comments to the OP).
$endgroup$
– metamorphy
Jan 2 at 1:45
$begingroup$
Does $$psi (n) = n prod_{p|n}(1+frac{1}{p})$$ here ?
$endgroup$
– Noodle
Jan 2 at 2:15
$begingroup$
No, there's no such simple formula here.
$endgroup$
– metamorphy
Jan 2 at 2:21
|
show 2 more comments
$begingroup$
I was just going to ask how do you compute $ psi (n) $ , it will help lots if you can or provide some info
$endgroup$
– Noodle
Jan 2 at 0:38
$begingroup$
How does one compute $mu (d)$
$endgroup$
– Noodle
Jan 2 at 0:45
$begingroup$
The formula for $psi$ with $mu$ is still of use (to show that $displaystylelim_{ntoinfty}frac{psi(n)}{n^2} = frac{6}{pi^2}$ - see comments to the OP).
$endgroup$
– metamorphy
Jan 2 at 1:45
$begingroup$
Does $$psi (n) = n prod_{p|n}(1+frac{1}{p})$$ here ?
$endgroup$
– Noodle
Jan 2 at 2:15
$begingroup$
No, there's no such simple formula here.
$endgroup$
– metamorphy
Jan 2 at 2:21
$begingroup$
I was just going to ask how do you compute $ psi (n) $ , it will help lots if you can or provide some info
$endgroup$
– Noodle
Jan 2 at 0:38
$begingroup$
I was just going to ask how do you compute $ psi (n) $ , it will help lots if you can or provide some info
$endgroup$
– Noodle
Jan 2 at 0:38
$begingroup$
How does one compute $mu (d)$
$endgroup$
– Noodle
Jan 2 at 0:45
$begingroup$
How does one compute $mu (d)$
$endgroup$
– Noodle
Jan 2 at 0:45
$begingroup$
The formula for $psi$ with $mu$ is still of use (to show that $displaystylelim_{ntoinfty}frac{psi(n)}{n^2} = frac{6}{pi^2}$ - see comments to the OP).
$endgroup$
– metamorphy
Jan 2 at 1:45
$begingroup$
The formula for $psi$ with $mu$ is still of use (to show that $displaystylelim_{ntoinfty}frac{psi(n)}{n^2} = frac{6}{pi^2}$ - see comments to the OP).
$endgroup$
– metamorphy
Jan 2 at 1:45
$begingroup$
Does $$psi (n) = n prod_{p|n}(1+frac{1}{p})$$ here ?
$endgroup$
– Noodle
Jan 2 at 2:15
$begingroup$
Does $$psi (n) = n prod_{p|n}(1+frac{1}{p})$$ here ?
$endgroup$
– Noodle
Jan 2 at 2:15
$begingroup$
No, there's no such simple formula here.
$endgroup$
– metamorphy
Jan 2 at 2:21
$begingroup$
No, there's no such simple formula here.
$endgroup$
– metamorphy
Jan 2 at 2:21
|
show 2 more comments
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$begingroup$
Is an asymptotic answer sufficient? It's not too hard to figure out that, if $f(n)$ is the number of such pairs, then $lim_{nrightarrowinfty}frac{f(n)}{n^2}$ is positive and finite (and it's not even so hard to compute this constant). I don't see how one would get an exact answer for all $n$ though without considerable computation.
$endgroup$
– Milo Brandt
Jan 2 at 0:10
$begingroup$
that is the main problem here, for $n = 10^{6} $ , with brute force it takes about 3-4 hours to compute them , if its not possible for a general formula to be made maybe decreasing the search space will help but this of course requires more properties for such pairs
$endgroup$
– Noodle
Jan 2 at 0:15