Show $fracf(z)sin(pi z) = sum_-infty^infty frac(-1)^nf(n)(z-n)$ The 2019 Stack Overflow Developer Survey Results Are InProve that $frac1sin^2 z = sumlimits_n= -infty ^ +infty frac1(z-pi n)^2 $Determine all entire functions $f$ with $f(z)notin (-infty,0]$.Show that $sum_k=1^Nfrac1(k+a)(k+b)=frac1b-asum_a<kleq bfrac1k-frac1b-asum_a<kleq bfrac1k+N$Evaluating $int_0 ^inftyfracdxx^1/3(1+x)$ using Complex AnalysisIf $1 leq |f(z)| leq |g(z)||z|^-1-epsilon$ for $|z| geq Delta$, prove that the sum of the residues of $fracfg$ at all its poles is $0$.Mistake with using residue theory for calculating $int_-infty^inftyfracsin(x)xdx$Trigonometric Improper Integral - $int_-infty^infty fracxsin axx^2+1dx$Entire Functions with no zeros are equalEvaluating the complex integral $int_0^infty frac sin (ln x) dx x^2 + 4 $Residue Calculus Integrable Model

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Show $fracf(z)sin(pi z) = sum_-infty^infty frac(-1)^nf(n)(z-n)$



The 2019 Stack Overflow Developer Survey Results Are InProve that $frac1sin^2 z = sumlimits_n= -infty ^ +infty frac1(z-pi n)^2 $Determine all entire functions $f$ with $f(z)notin (-infty,0]$.Show that $sum_k=1^Nfrac1(k+a)(k+b)=frac1b-asum_a<kleq bfrac1k-frac1b-asum_a<kleq bfrac1k+N$Evaluating $int_0 ^inftyfracdxx^1/3(1+x)$ using Complex AnalysisIf $1 leq |f(z)| leq |g(z)||z|^-1-epsilon$ for $|z| geq Delta$, prove that the sum of the residues of $fracfg$ at all its poles is $0$.Mistake with using residue theory for calculating $int_-infty^inftyfracsin(x)xdx$Trigonometric Improper Integral - $int_-infty^infty fracxsin axx^2+1dx$Entire Functions with no zeros are equalEvaluating the complex integral $int_0^infty frac sin (ln x) dx x^2 + 4 $Residue Calculus Integrable Model










2












$begingroup$


Let $f(z)$ be entire function satisfying $|f(x+iy)| leq Ce^y$ for $C > 0$ and $a in (-pi, pi).$



Show $fracf(z)sin(pi z) = sum_-infty^infty frac(-1)^nf(n)(z-n)$



All I have noticed in this problem is that the poles on the LHS matches the poles of the RHS. I thought about using residue theorem, but I don’t know how that will determine if two functions are equal. Most importantly, I don’t understand the bounded condition. Please help me, any hint will be nice.










share|cite|improve this question











$endgroup$
















    2












    $begingroup$


    Let $f(z)$ be entire function satisfying $|f(x+iy)| leq Ce^y$ for $C > 0$ and $a in (-pi, pi).$



    Show $fracf(z)sin(pi z) = sum_-infty^infty frac(-1)^nf(n)(z-n)$



    All I have noticed in this problem is that the poles on the LHS matches the poles of the RHS. I thought about using residue theorem, but I don’t know how that will determine if two functions are equal. Most importantly, I don’t understand the bounded condition. Please help me, any hint will be nice.










    share|cite|improve this question











    $endgroup$














      2












      2








      2





      $begingroup$


      Let $f(z)$ be entire function satisfying $|f(x+iy)| leq Ce^y$ for $C > 0$ and $a in (-pi, pi).$



      Show $fracf(z)sin(pi z) = sum_-infty^infty frac(-1)^nf(n)(z-n)$



      All I have noticed in this problem is that the poles on the LHS matches the poles of the RHS. I thought about using residue theorem, but I don’t know how that will determine if two functions are equal. Most importantly, I don’t understand the bounded condition. Please help me, any hint will be nice.










      share|cite|improve this question











      $endgroup$




      Let $f(z)$ be entire function satisfying $|f(x+iy)| leq Ce^y$ for $C > 0$ and $a in (-pi, pi).$



      Show $fracf(z)sin(pi z) = sum_-infty^infty frac(-1)^nf(n)(z-n)$



      All I have noticed in this problem is that the poles on the LHS matches the poles of the RHS. I thought about using residue theorem, but I don’t know how that will determine if two functions are equal. Most importantly, I don’t understand the bounded condition. Please help me, any hint will be nice.







      complex-analysis residue-calculus entire-functions






      share|cite|improve this question















      share|cite|improve this question













      share|cite|improve this question




      share|cite|improve this question








      edited Apr 7 at 9:33









      user

      6,48311031




      6,48311031










      asked Apr 7 at 4:38









      William AmbroseWilliam Ambrose

      213




      213




















          3 Answers
          3






          active

          oldest

          votes


















          2












          $begingroup$

          Put $g(z)=f(z)sin(pi z)^-1$. Since $f(z)$ is entire, $g(z)$ has simple poles at $a_n=n$ with residues $b_n=textRes(g(z); n) = f(n)textRes(csc(pi z); n) =frac(-1)^npi f(n)$. On the contours suggested by Yiorgios S. Smyrlis, $|sin(pi z)|$ is bounded below by either $cosh(pitextImz)$ or $|sinh(pi(npi + pi/2))|$ so $|g(z)|$ is bounded by $Ce^cosh(pi|textImz|)^-1$ on the vertical sides of $gamma_n$ or $Ce^sinh(pi|textImz|)^-1$ on the horizontal sides. Applying L'Hopital's rule shows $Ce^sinh(pi|textImz|)^-1$ tends to infinity like $Ce^cosh(pi|textImz|)^-1$. By the hypothesis on $a$, this shows that for $zin gamma_n$, $|g(z)|to 0$ as $|textImz|to infty$, while remaining bounded near the real line. In particular, $left|frac w2pi iint_gamma_nfracg(z)z-wright|to 0$ as $nto infty$. If $w$ is not a pole of $g$ and $gamma_n$ encircles $w$, the Residue Thm. gives
          $$frac 12pi iint_gamma_nfracg(z)z-wtextdz=g(w)+sum_a_k text in gamma_n fracb_ka_k-w=g(w)+frac 1pisum_frac(-1)^kf(k)k-w$$
          Letting $nto infty$ yields
          $$fracf(z)sin(pi z)=frac 1pi sum_k=-infty^inftyfrac(-1)^kf(k)w-k $$






          share|cite|improve this answer









          $endgroup$




















            0












            $begingroup$

            Hint: use the given inequality to show that LHS remains bounded as $|z| to infty$ through non-integer values. Then verify that LHS $-$ RHS is an entire function and apply Loiville's Theorem.






            share|cite|improve this answer









            $endgroup$












            • $begingroup$
              Upon first glance; how will the LHS - RHS be entire? It seems as though there will be poles at integers. Also, suppose it is entire and bounded. Lioville will tell us that the LHS - RHS is a constant. How to show the constant is 0?
              $endgroup$
              – Nicholas Roberts
              Apr 7 at 21:33










            • $begingroup$
              @NicholasRoberts You have already observed that the poles on the two sides match. The poles cancel out and you get an entire function.
              $endgroup$
              – Kavi Rama Murthy
              Apr 7 at 23:18


















            0












            $begingroup$

            Hint. Apply Mittag-Leffler's Theorem, to
            $$
            g(z)=fracf(z)sin pi z
            $$

            using the sequence of contours $gamma_n$, $ninmathbb N$, which are squares with vertices $(n+1/2)(pm 1pm i)$.






            share|cite|improve this answer









            $endgroup$













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              3 Answers
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              3 Answers
              3






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              2












              $begingroup$

              Put $g(z)=f(z)sin(pi z)^-1$. Since $f(z)$ is entire, $g(z)$ has simple poles at $a_n=n$ with residues $b_n=textRes(g(z); n) = f(n)textRes(csc(pi z); n) =frac(-1)^npi f(n)$. On the contours suggested by Yiorgios S. Smyrlis, $|sin(pi z)|$ is bounded below by either $cosh(pitextImz)$ or $|sinh(pi(npi + pi/2))|$ so $|g(z)|$ is bounded by $Ce^cosh(pi|textImz|)^-1$ on the vertical sides of $gamma_n$ or $Ce^sinh(pi|textImz|)^-1$ on the horizontal sides. Applying L'Hopital's rule shows $Ce^sinh(pi|textImz|)^-1$ tends to infinity like $Ce^cosh(pi|textImz|)^-1$. By the hypothesis on $a$, this shows that for $zin gamma_n$, $|g(z)|to 0$ as $|textImz|to infty$, while remaining bounded near the real line. In particular, $left|frac w2pi iint_gamma_nfracg(z)z-wright|to 0$ as $nto infty$. If $w$ is not a pole of $g$ and $gamma_n$ encircles $w$, the Residue Thm. gives
              $$frac 12pi iint_gamma_nfracg(z)z-wtextdz=g(w)+sum_a_k text in gamma_n fracb_ka_k-w=g(w)+frac 1pisum_frac(-1)^kf(k)k-w$$
              Letting $nto infty$ yields
              $$fracf(z)sin(pi z)=frac 1pi sum_k=-infty^inftyfrac(-1)^kf(k)w-k $$






              share|cite|improve this answer









              $endgroup$

















                2












                $begingroup$

                Put $g(z)=f(z)sin(pi z)^-1$. Since $f(z)$ is entire, $g(z)$ has simple poles at $a_n=n$ with residues $b_n=textRes(g(z); n) = f(n)textRes(csc(pi z); n) =frac(-1)^npi f(n)$. On the contours suggested by Yiorgios S. Smyrlis, $|sin(pi z)|$ is bounded below by either $cosh(pitextImz)$ or $|sinh(pi(npi + pi/2))|$ so $|g(z)|$ is bounded by $Ce^cosh(pi|textImz|)^-1$ on the vertical sides of $gamma_n$ or $Ce^sinh(pi|textImz|)^-1$ on the horizontal sides. Applying L'Hopital's rule shows $Ce^sinh(pi|textImz|)^-1$ tends to infinity like $Ce^cosh(pi|textImz|)^-1$. By the hypothesis on $a$, this shows that for $zin gamma_n$, $|g(z)|to 0$ as $|textImz|to infty$, while remaining bounded near the real line. In particular, $left|frac w2pi iint_gamma_nfracg(z)z-wright|to 0$ as $nto infty$. If $w$ is not a pole of $g$ and $gamma_n$ encircles $w$, the Residue Thm. gives
                $$frac 12pi iint_gamma_nfracg(z)z-wtextdz=g(w)+sum_a_k text in gamma_n fracb_ka_k-w=g(w)+frac 1pisum_frac(-1)^kf(k)k-w$$
                Letting $nto infty$ yields
                $$fracf(z)sin(pi z)=frac 1pi sum_k=-infty^inftyfrac(-1)^kf(k)w-k $$






                share|cite|improve this answer









                $endgroup$















                  2












                  2








                  2





                  $begingroup$

                  Put $g(z)=f(z)sin(pi z)^-1$. Since $f(z)$ is entire, $g(z)$ has simple poles at $a_n=n$ with residues $b_n=textRes(g(z); n) = f(n)textRes(csc(pi z); n) =frac(-1)^npi f(n)$. On the contours suggested by Yiorgios S. Smyrlis, $|sin(pi z)|$ is bounded below by either $cosh(pitextImz)$ or $|sinh(pi(npi + pi/2))|$ so $|g(z)|$ is bounded by $Ce^cosh(pi|textImz|)^-1$ on the vertical sides of $gamma_n$ or $Ce^sinh(pi|textImz|)^-1$ on the horizontal sides. Applying L'Hopital's rule shows $Ce^sinh(pi|textImz|)^-1$ tends to infinity like $Ce^cosh(pi|textImz|)^-1$. By the hypothesis on $a$, this shows that for $zin gamma_n$, $|g(z)|to 0$ as $|textImz|to infty$, while remaining bounded near the real line. In particular, $left|frac w2pi iint_gamma_nfracg(z)z-wright|to 0$ as $nto infty$. If $w$ is not a pole of $g$ and $gamma_n$ encircles $w$, the Residue Thm. gives
                  $$frac 12pi iint_gamma_nfracg(z)z-wtextdz=g(w)+sum_a_k text in gamma_n fracb_ka_k-w=g(w)+frac 1pisum_frac(-1)^kf(k)k-w$$
                  Letting $nto infty$ yields
                  $$fracf(z)sin(pi z)=frac 1pi sum_k=-infty^inftyfrac(-1)^kf(k)w-k $$






                  share|cite|improve this answer









                  $endgroup$



                  Put $g(z)=f(z)sin(pi z)^-1$. Since $f(z)$ is entire, $g(z)$ has simple poles at $a_n=n$ with residues $b_n=textRes(g(z); n) = f(n)textRes(csc(pi z); n) =frac(-1)^npi f(n)$. On the contours suggested by Yiorgios S. Smyrlis, $|sin(pi z)|$ is bounded below by either $cosh(pitextImz)$ or $|sinh(pi(npi + pi/2))|$ so $|g(z)|$ is bounded by $Ce^cosh(pi|textImz|)^-1$ on the vertical sides of $gamma_n$ or $Ce^sinh(pi|textImz|)^-1$ on the horizontal sides. Applying L'Hopital's rule shows $Ce^sinh(pi|textImz|)^-1$ tends to infinity like $Ce^cosh(pi|textImz|)^-1$. By the hypothesis on $a$, this shows that for $zin gamma_n$, $|g(z)|to 0$ as $|textImz|to infty$, while remaining bounded near the real line. In particular, $left|frac w2pi iint_gamma_nfracg(z)z-wright|to 0$ as $nto infty$. If $w$ is not a pole of $g$ and $gamma_n$ encircles $w$, the Residue Thm. gives
                  $$frac 12pi iint_gamma_nfracg(z)z-wtextdz=g(w)+sum_a_k text in gamma_n fracb_ka_k-w=g(w)+frac 1pisum_frac(-1)^kf(k)k-w$$
                  Letting $nto infty$ yields
                  $$fracf(z)sin(pi z)=frac 1pi sum_k=-infty^inftyfrac(-1)^kf(k)w-k $$







                  share|cite|improve this answer












                  share|cite|improve this answer



                  share|cite|improve this answer










                  answered Apr 8 at 1:11









                  Guacho PerezGuacho Perez

                  3,97911134




                  3,97911134





















                      0












                      $begingroup$

                      Hint: use the given inequality to show that LHS remains bounded as $|z| to infty$ through non-integer values. Then verify that LHS $-$ RHS is an entire function and apply Loiville's Theorem.






                      share|cite|improve this answer









                      $endgroup$












                      • $begingroup$
                        Upon first glance; how will the LHS - RHS be entire? It seems as though there will be poles at integers. Also, suppose it is entire and bounded. Lioville will tell us that the LHS - RHS is a constant. How to show the constant is 0?
                        $endgroup$
                        – Nicholas Roberts
                        Apr 7 at 21:33










                      • $begingroup$
                        @NicholasRoberts You have already observed that the poles on the two sides match. The poles cancel out and you get an entire function.
                        $endgroup$
                        – Kavi Rama Murthy
                        Apr 7 at 23:18















                      0












                      $begingroup$

                      Hint: use the given inequality to show that LHS remains bounded as $|z| to infty$ through non-integer values. Then verify that LHS $-$ RHS is an entire function and apply Loiville's Theorem.






                      share|cite|improve this answer









                      $endgroup$












                      • $begingroup$
                        Upon first glance; how will the LHS - RHS be entire? It seems as though there will be poles at integers. Also, suppose it is entire and bounded. Lioville will tell us that the LHS - RHS is a constant. How to show the constant is 0?
                        $endgroup$
                        – Nicholas Roberts
                        Apr 7 at 21:33










                      • $begingroup$
                        @NicholasRoberts You have already observed that the poles on the two sides match. The poles cancel out and you get an entire function.
                        $endgroup$
                        – Kavi Rama Murthy
                        Apr 7 at 23:18













                      0












                      0








                      0





                      $begingroup$

                      Hint: use the given inequality to show that LHS remains bounded as $|z| to infty$ through non-integer values. Then verify that LHS $-$ RHS is an entire function and apply Loiville's Theorem.






                      share|cite|improve this answer









                      $endgroup$



                      Hint: use the given inequality to show that LHS remains bounded as $|z| to infty$ through non-integer values. Then verify that LHS $-$ RHS is an entire function and apply Loiville's Theorem.







                      share|cite|improve this answer












                      share|cite|improve this answer



                      share|cite|improve this answer










                      answered Apr 7 at 4:59









                      Kavi Rama MurthyKavi Rama Murthy

                      74.1k53270




                      74.1k53270











                      • $begingroup$
                        Upon first glance; how will the LHS - RHS be entire? It seems as though there will be poles at integers. Also, suppose it is entire and bounded. Lioville will tell us that the LHS - RHS is a constant. How to show the constant is 0?
                        $endgroup$
                        – Nicholas Roberts
                        Apr 7 at 21:33










                      • $begingroup$
                        @NicholasRoberts You have already observed that the poles on the two sides match. The poles cancel out and you get an entire function.
                        $endgroup$
                        – Kavi Rama Murthy
                        Apr 7 at 23:18
















                      • $begingroup$
                        Upon first glance; how will the LHS - RHS be entire? It seems as though there will be poles at integers. Also, suppose it is entire and bounded. Lioville will tell us that the LHS - RHS is a constant. How to show the constant is 0?
                        $endgroup$
                        – Nicholas Roberts
                        Apr 7 at 21:33










                      • $begingroup$
                        @NicholasRoberts You have already observed that the poles on the two sides match. The poles cancel out and you get an entire function.
                        $endgroup$
                        – Kavi Rama Murthy
                        Apr 7 at 23:18















                      $begingroup$
                      Upon first glance; how will the LHS - RHS be entire? It seems as though there will be poles at integers. Also, suppose it is entire and bounded. Lioville will tell us that the LHS - RHS is a constant. How to show the constant is 0?
                      $endgroup$
                      – Nicholas Roberts
                      Apr 7 at 21:33




                      $begingroup$
                      Upon first glance; how will the LHS - RHS be entire? It seems as though there will be poles at integers. Also, suppose it is entire and bounded. Lioville will tell us that the LHS - RHS is a constant. How to show the constant is 0?
                      $endgroup$
                      – Nicholas Roberts
                      Apr 7 at 21:33












                      $begingroup$
                      @NicholasRoberts You have already observed that the poles on the two sides match. The poles cancel out and you get an entire function.
                      $endgroup$
                      – Kavi Rama Murthy
                      Apr 7 at 23:18




                      $begingroup$
                      @NicholasRoberts You have already observed that the poles on the two sides match. The poles cancel out and you get an entire function.
                      $endgroup$
                      – Kavi Rama Murthy
                      Apr 7 at 23:18











                      0












                      $begingroup$

                      Hint. Apply Mittag-Leffler's Theorem, to
                      $$
                      g(z)=fracf(z)sin pi z
                      $$

                      using the sequence of contours $gamma_n$, $ninmathbb N$, which are squares with vertices $(n+1/2)(pm 1pm i)$.






                      share|cite|improve this answer









                      $endgroup$

















                        0












                        $begingroup$

                        Hint. Apply Mittag-Leffler's Theorem, to
                        $$
                        g(z)=fracf(z)sin pi z
                        $$

                        using the sequence of contours $gamma_n$, $ninmathbb N$, which are squares with vertices $(n+1/2)(pm 1pm i)$.






                        share|cite|improve this answer









                        $endgroup$















                          0












                          0








                          0





                          $begingroup$

                          Hint. Apply Mittag-Leffler's Theorem, to
                          $$
                          g(z)=fracf(z)sin pi z
                          $$

                          using the sequence of contours $gamma_n$, $ninmathbb N$, which are squares with vertices $(n+1/2)(pm 1pm i)$.






                          share|cite|improve this answer









                          $endgroup$



                          Hint. Apply Mittag-Leffler's Theorem, to
                          $$
                          g(z)=fracf(z)sin pi z
                          $$

                          using the sequence of contours $gamma_n$, $ninmathbb N$, which are squares with vertices $(n+1/2)(pm 1pm i)$.







                          share|cite|improve this answer












                          share|cite|improve this answer



                          share|cite|improve this answer










                          answered Apr 7 at 8:50









                          Yiorgos S. SmyrlisYiorgos S. Smyrlis

                          63.7k1385165




                          63.7k1385165



























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