What does the following notation mean: $(L-lambda I)$












1












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In my tekstbook powervectors are discussed where
$(L-lambda I)^p textbf{v}=0$ was mentioned. Here is $L$ a linear operator on the vectorspace $V$, $lambda$ a scalar and $textbf{v} in V $.



My question: How is $L-lambda I$ definied? I'm confused because $L$ is here a function and not a matrix.










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  • 1




    $begingroup$
    You can think " I " as an identity function not a matrix
    $endgroup$
    – Euduardo
    Dec 10 '18 at 14:31
















1












$begingroup$


In my tekstbook powervectors are discussed where
$(L-lambda I)^p textbf{v}=0$ was mentioned. Here is $L$ a linear operator on the vectorspace $V$, $lambda$ a scalar and $textbf{v} in V $.



My question: How is $L-lambda I$ definied? I'm confused because $L$ is here a function and not a matrix.










share|cite|improve this question











$endgroup$








  • 1




    $begingroup$
    You can think " I " as an identity function not a matrix
    $endgroup$
    – Euduardo
    Dec 10 '18 at 14:31














1












1








1





$begingroup$


In my tekstbook powervectors are discussed where
$(L-lambda I)^p textbf{v}=0$ was mentioned. Here is $L$ a linear operator on the vectorspace $V$, $lambda$ a scalar and $textbf{v} in V $.



My question: How is $L-lambda I$ definied? I'm confused because $L$ is here a function and not a matrix.










share|cite|improve this question











$endgroup$




In my tekstbook powervectors are discussed where
$(L-lambda I)^p textbf{v}=0$ was mentioned. Here is $L$ a linear operator on the vectorspace $V$, $lambda$ a scalar and $textbf{v} in V $.



My question: How is $L-lambda I$ definied? I'm confused because $L$ is here a function and not a matrix.







linear-algebra notation definition






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edited Dec 10 '18 at 16:10







Keep_On_Cruising

















asked Dec 10 '18 at 14:29









Keep_On_CruisingKeep_On_Cruising

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  • 1




    $begingroup$
    You can think " I " as an identity function not a matrix
    $endgroup$
    – Euduardo
    Dec 10 '18 at 14:31














  • 1




    $begingroup$
    You can think " I " as an identity function not a matrix
    $endgroup$
    – Euduardo
    Dec 10 '18 at 14:31








1




1




$begingroup$
You can think " I " as an identity function not a matrix
$endgroup$
– Euduardo
Dec 10 '18 at 14:31




$begingroup$
You can think " I " as an identity function not a matrix
$endgroup$
– Euduardo
Dec 10 '18 at 14:31










2 Answers
2






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7












$begingroup$

$I$ is the identity operator on the vector space: $Ix = x$ for all $x in V$.
So $$(L - lambda I) x = L x - lambda I x = L x - lambda x$$






share|cite|improve this answer









$endgroup$





















    3












    $begingroup$

    Robert did fully answer the question, but I'd like to add a different example: The differential equation of the harmonic oscillator is
    $$frac{mathrm{d}^2 u(t)}{mathrm{d}t^2}+2beta frac{mathrm{d}u(t)}{mathrm{d}t}+omega^2 u(t)=0$$
    And it can be rewritten as
    $$(D^2+2beta D+omega^2 I)u(t)=0$$
    Where $D$ is the differential operator: $Du(t)=frac{mathrm{d}u(t)}{mathrm{d}t}$.

    Or the Klein-Gordon equation in $1+1$ dimensions:
    $$left(frac{1}{c^2} partial_t^2-partial_x^2+mu Iright)u(t)=0$$
    This kind of notation is very useful, because the differential operator will take it's eigenvalue on it's eigenfunction, so you can easily get the dispersion relation, with just substitutions of the eigenvalues: $partial_t to (-i omega)$ and $partial_x to (ik)$ in the case of a plane wave.






    share|cite|improve this answer











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      2 Answers
      2






      active

      oldest

      votes








      2 Answers
      2






      active

      oldest

      votes









      active

      oldest

      votes






      active

      oldest

      votes









      7












      $begingroup$

      $I$ is the identity operator on the vector space: $Ix = x$ for all $x in V$.
      So $$(L - lambda I) x = L x - lambda I x = L x - lambda x$$






      share|cite|improve this answer









      $endgroup$


















        7












        $begingroup$

        $I$ is the identity operator on the vector space: $Ix = x$ for all $x in V$.
        So $$(L - lambda I) x = L x - lambda I x = L x - lambda x$$






        share|cite|improve this answer









        $endgroup$
















          7












          7








          7





          $begingroup$

          $I$ is the identity operator on the vector space: $Ix = x$ for all $x in V$.
          So $$(L - lambda I) x = L x - lambda I x = L x - lambda x$$






          share|cite|improve this answer









          $endgroup$



          $I$ is the identity operator on the vector space: $Ix = x$ for all $x in V$.
          So $$(L - lambda I) x = L x - lambda I x = L x - lambda x$$







          share|cite|improve this answer












          share|cite|improve this answer



          share|cite|improve this answer










          answered Dec 10 '18 at 14:31









          Robert IsraelRobert Israel

          322k23212465




          322k23212465























              3












              $begingroup$

              Robert did fully answer the question, but I'd like to add a different example: The differential equation of the harmonic oscillator is
              $$frac{mathrm{d}^2 u(t)}{mathrm{d}t^2}+2beta frac{mathrm{d}u(t)}{mathrm{d}t}+omega^2 u(t)=0$$
              And it can be rewritten as
              $$(D^2+2beta D+omega^2 I)u(t)=0$$
              Where $D$ is the differential operator: $Du(t)=frac{mathrm{d}u(t)}{mathrm{d}t}$.

              Or the Klein-Gordon equation in $1+1$ dimensions:
              $$left(frac{1}{c^2} partial_t^2-partial_x^2+mu Iright)u(t)=0$$
              This kind of notation is very useful, because the differential operator will take it's eigenvalue on it's eigenfunction, so you can easily get the dispersion relation, with just substitutions of the eigenvalues: $partial_t to (-i omega)$ and $partial_x to (ik)$ in the case of a plane wave.






              share|cite|improve this answer











              $endgroup$


















                3












                $begingroup$

                Robert did fully answer the question, but I'd like to add a different example: The differential equation of the harmonic oscillator is
                $$frac{mathrm{d}^2 u(t)}{mathrm{d}t^2}+2beta frac{mathrm{d}u(t)}{mathrm{d}t}+omega^2 u(t)=0$$
                And it can be rewritten as
                $$(D^2+2beta D+omega^2 I)u(t)=0$$
                Where $D$ is the differential operator: $Du(t)=frac{mathrm{d}u(t)}{mathrm{d}t}$.

                Or the Klein-Gordon equation in $1+1$ dimensions:
                $$left(frac{1}{c^2} partial_t^2-partial_x^2+mu Iright)u(t)=0$$
                This kind of notation is very useful, because the differential operator will take it's eigenvalue on it's eigenfunction, so you can easily get the dispersion relation, with just substitutions of the eigenvalues: $partial_t to (-i omega)$ and $partial_x to (ik)$ in the case of a plane wave.






                share|cite|improve this answer











                $endgroup$
















                  3












                  3








                  3





                  $begingroup$

                  Robert did fully answer the question, but I'd like to add a different example: The differential equation of the harmonic oscillator is
                  $$frac{mathrm{d}^2 u(t)}{mathrm{d}t^2}+2beta frac{mathrm{d}u(t)}{mathrm{d}t}+omega^2 u(t)=0$$
                  And it can be rewritten as
                  $$(D^2+2beta D+omega^2 I)u(t)=0$$
                  Where $D$ is the differential operator: $Du(t)=frac{mathrm{d}u(t)}{mathrm{d}t}$.

                  Or the Klein-Gordon equation in $1+1$ dimensions:
                  $$left(frac{1}{c^2} partial_t^2-partial_x^2+mu Iright)u(t)=0$$
                  This kind of notation is very useful, because the differential operator will take it's eigenvalue on it's eigenfunction, so you can easily get the dispersion relation, with just substitutions of the eigenvalues: $partial_t to (-i omega)$ and $partial_x to (ik)$ in the case of a plane wave.






                  share|cite|improve this answer











                  $endgroup$



                  Robert did fully answer the question, but I'd like to add a different example: The differential equation of the harmonic oscillator is
                  $$frac{mathrm{d}^2 u(t)}{mathrm{d}t^2}+2beta frac{mathrm{d}u(t)}{mathrm{d}t}+omega^2 u(t)=0$$
                  And it can be rewritten as
                  $$(D^2+2beta D+omega^2 I)u(t)=0$$
                  Where $D$ is the differential operator: $Du(t)=frac{mathrm{d}u(t)}{mathrm{d}t}$.

                  Or the Klein-Gordon equation in $1+1$ dimensions:
                  $$left(frac{1}{c^2} partial_t^2-partial_x^2+mu Iright)u(t)=0$$
                  This kind of notation is very useful, because the differential operator will take it's eigenvalue on it's eigenfunction, so you can easily get the dispersion relation, with just substitutions of the eigenvalues: $partial_t to (-i omega)$ and $partial_x to (ik)$ in the case of a plane wave.







                  share|cite|improve this answer














                  share|cite|improve this answer



                  share|cite|improve this answer








                  edited Dec 10 '18 at 15:35

























                  answered Dec 10 '18 at 15:09









                  BotondBotond

                  5,7782732




                  5,7782732






























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