sum of infinite series: $sum_{m=1}^{infty}frac{sin^2(mpi)}{(m^2-a^2)^2}$, and...











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0
down vote

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Not having a great series background, I turn to the wider world... :)



I need to find two sums:



$$sum_{m=1}^{infty}frac{sin^2(mpi)}{(m^2-a^2)^2}$$



and



$$sum_{m=1}^{infty}frac{m^2}{(m^2-a^2)^2}$$



I've seen some related series on here, but not close enough that I can figure out how to get these sums from the ones posted. Any help would be much appreciated.










share|cite|improve this question






















  • What is $a$? If it is an integer then both series are undefined...
    – Servaes
    Nov 16 at 23:55










  • a is not an integer. For my case $a=n[1+frac{1}{4}cos(n)]$ where n is an integer
    – Michael Cloud
    Nov 17 at 0:43












  • In more detail the first sum should be $sum_{m=1}^{infty}frac{sin^2(frac{mpi}{gamma_n}){(m^2-gamma_n^2n^2)^2}$ where $gamma_n=[1+frac{1}{4}cos(n)]$ and $n$ is a positive natural number
    – Michael Cloud
    Nov 17 at 0:49












  • trying one more time to get the formatting right on my previous comment: sum_{m=1}^{infty}frac{sin^2(frac{mpi}{gamma_n}){(m^2-gamma_n^2n^2)^2} where gamma_n=[1+frac{1}{4}cos(n)] and n is a positive natural number
    – Michael Cloud
    Nov 17 at 0:56










  • You can add $ sign to format Mathjax.
    – Tianlalu
    Nov 17 at 0:57















up vote
0
down vote

favorite
2












Not having a great series background, I turn to the wider world... :)



I need to find two sums:



$$sum_{m=1}^{infty}frac{sin^2(mpi)}{(m^2-a^2)^2}$$



and



$$sum_{m=1}^{infty}frac{m^2}{(m^2-a^2)^2}$$



I've seen some related series on here, but not close enough that I can figure out how to get these sums from the ones posted. Any help would be much appreciated.










share|cite|improve this question






















  • What is $a$? If it is an integer then both series are undefined...
    – Servaes
    Nov 16 at 23:55










  • a is not an integer. For my case $a=n[1+frac{1}{4}cos(n)]$ where n is an integer
    – Michael Cloud
    Nov 17 at 0:43












  • In more detail the first sum should be $sum_{m=1}^{infty}frac{sin^2(frac{mpi}{gamma_n}){(m^2-gamma_n^2n^2)^2}$ where $gamma_n=[1+frac{1}{4}cos(n)]$ and $n$ is a positive natural number
    – Michael Cloud
    Nov 17 at 0:49












  • trying one more time to get the formatting right on my previous comment: sum_{m=1}^{infty}frac{sin^2(frac{mpi}{gamma_n}){(m^2-gamma_n^2n^2)^2} where gamma_n=[1+frac{1}{4}cos(n)] and n is a positive natural number
    – Michael Cloud
    Nov 17 at 0:56










  • You can add $ sign to format Mathjax.
    – Tianlalu
    Nov 17 at 0:57













up vote
0
down vote

favorite
2









up vote
0
down vote

favorite
2






2





Not having a great series background, I turn to the wider world... :)



I need to find two sums:



$$sum_{m=1}^{infty}frac{sin^2(mpi)}{(m^2-a^2)^2}$$



and



$$sum_{m=1}^{infty}frac{m^2}{(m^2-a^2)^2}$$



I've seen some related series on here, but not close enough that I can figure out how to get these sums from the ones posted. Any help would be much appreciated.










share|cite|improve this question













Not having a great series background, I turn to the wider world... :)



I need to find two sums:



$$sum_{m=1}^{infty}frac{sin^2(mpi)}{(m^2-a^2)^2}$$



and



$$sum_{m=1}^{infty}frac{m^2}{(m^2-a^2)^2}$$



I've seen some related series on here, but not close enough that I can figure out how to get these sums from the ones posted. Any help would be much appreciated.







sequences-and-series






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share|cite|improve this question











share|cite|improve this question




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asked Nov 16 at 23:49









Michael Cloud

816




816












  • What is $a$? If it is an integer then both series are undefined...
    – Servaes
    Nov 16 at 23:55










  • a is not an integer. For my case $a=n[1+frac{1}{4}cos(n)]$ where n is an integer
    – Michael Cloud
    Nov 17 at 0:43












  • In more detail the first sum should be $sum_{m=1}^{infty}frac{sin^2(frac{mpi}{gamma_n}){(m^2-gamma_n^2n^2)^2}$ where $gamma_n=[1+frac{1}{4}cos(n)]$ and $n$ is a positive natural number
    – Michael Cloud
    Nov 17 at 0:49












  • trying one more time to get the formatting right on my previous comment: sum_{m=1}^{infty}frac{sin^2(frac{mpi}{gamma_n}){(m^2-gamma_n^2n^2)^2} where gamma_n=[1+frac{1}{4}cos(n)] and n is a positive natural number
    – Michael Cloud
    Nov 17 at 0:56










  • You can add $ sign to format Mathjax.
    – Tianlalu
    Nov 17 at 0:57


















  • What is $a$? If it is an integer then both series are undefined...
    – Servaes
    Nov 16 at 23:55










  • a is not an integer. For my case $a=n[1+frac{1}{4}cos(n)]$ where n is an integer
    – Michael Cloud
    Nov 17 at 0:43












  • In more detail the first sum should be $sum_{m=1}^{infty}frac{sin^2(frac{mpi}{gamma_n}){(m^2-gamma_n^2n^2)^2}$ where $gamma_n=[1+frac{1}{4}cos(n)]$ and $n$ is a positive natural number
    – Michael Cloud
    Nov 17 at 0:49












  • trying one more time to get the formatting right on my previous comment: sum_{m=1}^{infty}frac{sin^2(frac{mpi}{gamma_n}){(m^2-gamma_n^2n^2)^2} where gamma_n=[1+frac{1}{4}cos(n)] and n is a positive natural number
    – Michael Cloud
    Nov 17 at 0:56










  • You can add $ sign to format Mathjax.
    – Tianlalu
    Nov 17 at 0:57
















What is $a$? If it is an integer then both series are undefined...
– Servaes
Nov 16 at 23:55




What is $a$? If it is an integer then both series are undefined...
– Servaes
Nov 16 at 23:55












a is not an integer. For my case $a=n[1+frac{1}{4}cos(n)]$ where n is an integer
– Michael Cloud
Nov 17 at 0:43






a is not an integer. For my case $a=n[1+frac{1}{4}cos(n)]$ where n is an integer
– Michael Cloud
Nov 17 at 0:43














In more detail the first sum should be $sum_{m=1}^{infty}frac{sin^2(frac{mpi}{gamma_n}){(m^2-gamma_n^2n^2)^2}$ where $gamma_n=[1+frac{1}{4}cos(n)]$ and $n$ is a positive natural number
– Michael Cloud
Nov 17 at 0:49






In more detail the first sum should be $sum_{m=1}^{infty}frac{sin^2(frac{mpi}{gamma_n}){(m^2-gamma_n^2n^2)^2}$ where $gamma_n=[1+frac{1}{4}cos(n)]$ and $n$ is a positive natural number
– Michael Cloud
Nov 17 at 0:49














trying one more time to get the formatting right on my previous comment: sum_{m=1}^{infty}frac{sin^2(frac{mpi}{gamma_n}){(m^2-gamma_n^2n^2)^2} where gamma_n=[1+frac{1}{4}cos(n)] and n is a positive natural number
– Michael Cloud
Nov 17 at 0:56




trying one more time to get the formatting right on my previous comment: sum_{m=1}^{infty}frac{sin^2(frac{mpi}{gamma_n}){(m^2-gamma_n^2n^2)^2} where gamma_n=[1+frac{1}{4}cos(n)] and n is a positive natural number
– Michael Cloud
Nov 17 at 0:56












You can add $ sign to format Mathjax.
– Tianlalu
Nov 17 at 0:57




You can add $ sign to format Mathjax.
– Tianlalu
Nov 17 at 0:57










2 Answers
2






active

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up vote
2
down vote













The first one is $0$ because $sin mpi = 0$ for any $min Bbb Z$.



For the second one, we split it into two sums,
begin{align*}
S=sum_{m=1}^inftyfrac{m^2}{(m^2-a^2)^2}&=sum_{m=1}^inftyfrac{m^2-a^2+a^2}{(m^2-a^2)^2}\
&=underbrace{sum_{m=1}^inftyfrac{1}{m^2-a^2}}_{S_1}+a^2underbrace{sum_{m=1}^inftyfrac{1}{(m^2-a^2)^2}}_{S_2}.
end{align*}

From this answer, we know
$$S_1=frac1{2a^2}-frac{picot,pi a}{2a}.tag{*}$$
Differentiate $(*)$ with respect to $a$ (we can do that because $S_1$ uniformly converges),
begin{align*}S_1'=frac d{da}sum_{m=1}^inftyfrac{1}{m^2-a^2}&=2asum_{m=1}^inftyfrac{1}{(m^2-a^2)^2}=2aS_2\
implies S_2&=frac{1}{2a}S_1'.
end{align*}

$$therefore S=S_1+frac{a}{2}S_1'=frac{pi^2}{4}csc^2pi a-frac{picot pi a}{4a}.$$






share|cite|improve this answer





















  • Thanks @Tianlalu ! For the first one, I had overly pared down the real problem, should read: $sum_{m=1}{infty} frac{sin^2(frac{mpi}{gamma_n)}{(m^2-gamma_n^2n^2)}$ where $gamma_n=1+frac{1}{4}cos(n)$ with $n$ a positive natural
    – Michael Cloud
    Nov 17 at 1:39










  • @MichaelCloud: I don't think there is a nice closed form for that. Even if we take some simple constants such as $gamma_n=1/2$ and $n=1$, we will get a complicated answer $$sum_{m=1}^inftyfrac{sin(frac{mpi}{2})}{(m^2-1/4)^2}=G+frac 18zeta(2,frac{5}{4})-2-pi+frac{5}{8}pi^2,$$where $G$ is Catalan's constant and $zeta(s,a)$ is the generalized zeta function.
    – Tianlalu
    Nov 17 at 1:50




















up vote
1
down vote













I did find an answer to the second one:



$$sum_{m=1}^{infty} frac{m^2}{(m^2-a^2)^2}= frac{pi[2pi a-sin(2pi a)]}{8asin^2(pi a)}$$



According to a Dodonov, Klimov, and Nikonov "Quantum Particle in a Box with Moving Walls" J. Math. Phys. 34 (8) August 1993






share|cite|improve this answer





















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    2 Answers
    2






    active

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    2 Answers
    2






    active

    oldest

    votes









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    oldest

    votes






    active

    oldest

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    up vote
    2
    down vote













    The first one is $0$ because $sin mpi = 0$ for any $min Bbb Z$.



    For the second one, we split it into two sums,
    begin{align*}
    S=sum_{m=1}^inftyfrac{m^2}{(m^2-a^2)^2}&=sum_{m=1}^inftyfrac{m^2-a^2+a^2}{(m^2-a^2)^2}\
    &=underbrace{sum_{m=1}^inftyfrac{1}{m^2-a^2}}_{S_1}+a^2underbrace{sum_{m=1}^inftyfrac{1}{(m^2-a^2)^2}}_{S_2}.
    end{align*}

    From this answer, we know
    $$S_1=frac1{2a^2}-frac{picot,pi a}{2a}.tag{*}$$
    Differentiate $(*)$ with respect to $a$ (we can do that because $S_1$ uniformly converges),
    begin{align*}S_1'=frac d{da}sum_{m=1}^inftyfrac{1}{m^2-a^2}&=2asum_{m=1}^inftyfrac{1}{(m^2-a^2)^2}=2aS_2\
    implies S_2&=frac{1}{2a}S_1'.
    end{align*}

    $$therefore S=S_1+frac{a}{2}S_1'=frac{pi^2}{4}csc^2pi a-frac{picot pi a}{4a}.$$






    share|cite|improve this answer





















    • Thanks @Tianlalu ! For the first one, I had overly pared down the real problem, should read: $sum_{m=1}{infty} frac{sin^2(frac{mpi}{gamma_n)}{(m^2-gamma_n^2n^2)}$ where $gamma_n=1+frac{1}{4}cos(n)$ with $n$ a positive natural
      – Michael Cloud
      Nov 17 at 1:39










    • @MichaelCloud: I don't think there is a nice closed form for that. Even if we take some simple constants such as $gamma_n=1/2$ and $n=1$, we will get a complicated answer $$sum_{m=1}^inftyfrac{sin(frac{mpi}{2})}{(m^2-1/4)^2}=G+frac 18zeta(2,frac{5}{4})-2-pi+frac{5}{8}pi^2,$$where $G$ is Catalan's constant and $zeta(s,a)$ is the generalized zeta function.
      – Tianlalu
      Nov 17 at 1:50

















    up vote
    2
    down vote













    The first one is $0$ because $sin mpi = 0$ for any $min Bbb Z$.



    For the second one, we split it into two sums,
    begin{align*}
    S=sum_{m=1}^inftyfrac{m^2}{(m^2-a^2)^2}&=sum_{m=1}^inftyfrac{m^2-a^2+a^2}{(m^2-a^2)^2}\
    &=underbrace{sum_{m=1}^inftyfrac{1}{m^2-a^2}}_{S_1}+a^2underbrace{sum_{m=1}^inftyfrac{1}{(m^2-a^2)^2}}_{S_2}.
    end{align*}

    From this answer, we know
    $$S_1=frac1{2a^2}-frac{picot,pi a}{2a}.tag{*}$$
    Differentiate $(*)$ with respect to $a$ (we can do that because $S_1$ uniformly converges),
    begin{align*}S_1'=frac d{da}sum_{m=1}^inftyfrac{1}{m^2-a^2}&=2asum_{m=1}^inftyfrac{1}{(m^2-a^2)^2}=2aS_2\
    implies S_2&=frac{1}{2a}S_1'.
    end{align*}

    $$therefore S=S_1+frac{a}{2}S_1'=frac{pi^2}{4}csc^2pi a-frac{picot pi a}{4a}.$$






    share|cite|improve this answer





















    • Thanks @Tianlalu ! For the first one, I had overly pared down the real problem, should read: $sum_{m=1}{infty} frac{sin^2(frac{mpi}{gamma_n)}{(m^2-gamma_n^2n^2)}$ where $gamma_n=1+frac{1}{4}cos(n)$ with $n$ a positive natural
      – Michael Cloud
      Nov 17 at 1:39










    • @MichaelCloud: I don't think there is a nice closed form for that. Even if we take some simple constants such as $gamma_n=1/2$ and $n=1$, we will get a complicated answer $$sum_{m=1}^inftyfrac{sin(frac{mpi}{2})}{(m^2-1/4)^2}=G+frac 18zeta(2,frac{5}{4})-2-pi+frac{5}{8}pi^2,$$where $G$ is Catalan's constant and $zeta(s,a)$ is the generalized zeta function.
      – Tianlalu
      Nov 17 at 1:50















    up vote
    2
    down vote










    up vote
    2
    down vote









    The first one is $0$ because $sin mpi = 0$ for any $min Bbb Z$.



    For the second one, we split it into two sums,
    begin{align*}
    S=sum_{m=1}^inftyfrac{m^2}{(m^2-a^2)^2}&=sum_{m=1}^inftyfrac{m^2-a^2+a^2}{(m^2-a^2)^2}\
    &=underbrace{sum_{m=1}^inftyfrac{1}{m^2-a^2}}_{S_1}+a^2underbrace{sum_{m=1}^inftyfrac{1}{(m^2-a^2)^2}}_{S_2}.
    end{align*}

    From this answer, we know
    $$S_1=frac1{2a^2}-frac{picot,pi a}{2a}.tag{*}$$
    Differentiate $(*)$ with respect to $a$ (we can do that because $S_1$ uniformly converges),
    begin{align*}S_1'=frac d{da}sum_{m=1}^inftyfrac{1}{m^2-a^2}&=2asum_{m=1}^inftyfrac{1}{(m^2-a^2)^2}=2aS_2\
    implies S_2&=frac{1}{2a}S_1'.
    end{align*}

    $$therefore S=S_1+frac{a}{2}S_1'=frac{pi^2}{4}csc^2pi a-frac{picot pi a}{4a}.$$






    share|cite|improve this answer












    The first one is $0$ because $sin mpi = 0$ for any $min Bbb Z$.



    For the second one, we split it into two sums,
    begin{align*}
    S=sum_{m=1}^inftyfrac{m^2}{(m^2-a^2)^2}&=sum_{m=1}^inftyfrac{m^2-a^2+a^2}{(m^2-a^2)^2}\
    &=underbrace{sum_{m=1}^inftyfrac{1}{m^2-a^2}}_{S_1}+a^2underbrace{sum_{m=1}^inftyfrac{1}{(m^2-a^2)^2}}_{S_2}.
    end{align*}

    From this answer, we know
    $$S_1=frac1{2a^2}-frac{picot,pi a}{2a}.tag{*}$$
    Differentiate $(*)$ with respect to $a$ (we can do that because $S_1$ uniformly converges),
    begin{align*}S_1'=frac d{da}sum_{m=1}^inftyfrac{1}{m^2-a^2}&=2asum_{m=1}^inftyfrac{1}{(m^2-a^2)^2}=2aS_2\
    implies S_2&=frac{1}{2a}S_1'.
    end{align*}

    $$therefore S=S_1+frac{a}{2}S_1'=frac{pi^2}{4}csc^2pi a-frac{picot pi a}{4a}.$$







    share|cite|improve this answer












    share|cite|improve this answer



    share|cite|improve this answer










    answered Nov 17 at 1:08









    Tianlalu

    2,629632




    2,629632












    • Thanks @Tianlalu ! For the first one, I had overly pared down the real problem, should read: $sum_{m=1}{infty} frac{sin^2(frac{mpi}{gamma_n)}{(m^2-gamma_n^2n^2)}$ where $gamma_n=1+frac{1}{4}cos(n)$ with $n$ a positive natural
      – Michael Cloud
      Nov 17 at 1:39










    • @MichaelCloud: I don't think there is a nice closed form for that. Even if we take some simple constants such as $gamma_n=1/2$ and $n=1$, we will get a complicated answer $$sum_{m=1}^inftyfrac{sin(frac{mpi}{2})}{(m^2-1/4)^2}=G+frac 18zeta(2,frac{5}{4})-2-pi+frac{5}{8}pi^2,$$where $G$ is Catalan's constant and $zeta(s,a)$ is the generalized zeta function.
      – Tianlalu
      Nov 17 at 1:50




















    • Thanks @Tianlalu ! For the first one, I had overly pared down the real problem, should read: $sum_{m=1}{infty} frac{sin^2(frac{mpi}{gamma_n)}{(m^2-gamma_n^2n^2)}$ where $gamma_n=1+frac{1}{4}cos(n)$ with $n$ a positive natural
      – Michael Cloud
      Nov 17 at 1:39










    • @MichaelCloud: I don't think there is a nice closed form for that. Even if we take some simple constants such as $gamma_n=1/2$ and $n=1$, we will get a complicated answer $$sum_{m=1}^inftyfrac{sin(frac{mpi}{2})}{(m^2-1/4)^2}=G+frac 18zeta(2,frac{5}{4})-2-pi+frac{5}{8}pi^2,$$where $G$ is Catalan's constant and $zeta(s,a)$ is the generalized zeta function.
      – Tianlalu
      Nov 17 at 1:50


















    Thanks @Tianlalu ! For the first one, I had overly pared down the real problem, should read: $sum_{m=1}{infty} frac{sin^2(frac{mpi}{gamma_n)}{(m^2-gamma_n^2n^2)}$ where $gamma_n=1+frac{1}{4}cos(n)$ with $n$ a positive natural
    – Michael Cloud
    Nov 17 at 1:39




    Thanks @Tianlalu ! For the first one, I had overly pared down the real problem, should read: $sum_{m=1}{infty} frac{sin^2(frac{mpi}{gamma_n)}{(m^2-gamma_n^2n^2)}$ where $gamma_n=1+frac{1}{4}cos(n)$ with $n$ a positive natural
    – Michael Cloud
    Nov 17 at 1:39












    @MichaelCloud: I don't think there is a nice closed form for that. Even if we take some simple constants such as $gamma_n=1/2$ and $n=1$, we will get a complicated answer $$sum_{m=1}^inftyfrac{sin(frac{mpi}{2})}{(m^2-1/4)^2}=G+frac 18zeta(2,frac{5}{4})-2-pi+frac{5}{8}pi^2,$$where $G$ is Catalan's constant and $zeta(s,a)$ is the generalized zeta function.
    – Tianlalu
    Nov 17 at 1:50






    @MichaelCloud: I don't think there is a nice closed form for that. Even if we take some simple constants such as $gamma_n=1/2$ and $n=1$, we will get a complicated answer $$sum_{m=1}^inftyfrac{sin(frac{mpi}{2})}{(m^2-1/4)^2}=G+frac 18zeta(2,frac{5}{4})-2-pi+frac{5}{8}pi^2,$$where $G$ is Catalan's constant and $zeta(s,a)$ is the generalized zeta function.
    – Tianlalu
    Nov 17 at 1:50












    up vote
    1
    down vote













    I did find an answer to the second one:



    $$sum_{m=1}^{infty} frac{m^2}{(m^2-a^2)^2}= frac{pi[2pi a-sin(2pi a)]}{8asin^2(pi a)}$$



    According to a Dodonov, Klimov, and Nikonov "Quantum Particle in a Box with Moving Walls" J. Math. Phys. 34 (8) August 1993






    share|cite|improve this answer

























      up vote
      1
      down vote













      I did find an answer to the second one:



      $$sum_{m=1}^{infty} frac{m^2}{(m^2-a^2)^2}= frac{pi[2pi a-sin(2pi a)]}{8asin^2(pi a)}$$



      According to a Dodonov, Klimov, and Nikonov "Quantum Particle in a Box with Moving Walls" J. Math. Phys. 34 (8) August 1993






      share|cite|improve this answer























        up vote
        1
        down vote










        up vote
        1
        down vote









        I did find an answer to the second one:



        $$sum_{m=1}^{infty} frac{m^2}{(m^2-a^2)^2}= frac{pi[2pi a-sin(2pi a)]}{8asin^2(pi a)}$$



        According to a Dodonov, Klimov, and Nikonov "Quantum Particle in a Box with Moving Walls" J. Math. Phys. 34 (8) August 1993






        share|cite|improve this answer












        I did find an answer to the second one:



        $$sum_{m=1}^{infty} frac{m^2}{(m^2-a^2)^2}= frac{pi[2pi a-sin(2pi a)]}{8asin^2(pi a)}$$



        According to a Dodonov, Klimov, and Nikonov "Quantum Particle in a Box with Moving Walls" J. Math. Phys. 34 (8) August 1993







        share|cite|improve this answer












        share|cite|improve this answer



        share|cite|improve this answer










        answered Nov 17 at 1:03









        Michael Cloud

        816




        816






























             

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