How to prove that two subspaces are equal if and only if their annihilators are equal












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By definition, $W_1=W_2 rightarrow W_1^0=W_2^0$, $W_1, W_2 subseteq V$ are subspaces of $V$. But how does one show the reverse implication? $V$ is not assumed to be finite dimensional.



The annihilator is defined as $S^0= {fin V^*| f(s)=0 forall sin S}$, where $Ssubseteq V, S$ is a subset of vector space V.










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  • $begingroup$
    What is your definition of the annihilator?
    $endgroup$
    – Bernard
    Nov 16 '15 at 20:27










  • $begingroup$
    @Bernard, added the definition.
    $endgroup$
    – grayQuant
    Nov 16 '15 at 20:32










  • $begingroup$
    That's what I thought, but I wondered if you were hiding an underlying structure.
    $endgroup$
    – Bernard
    Nov 16 '15 at 20:33
















1












$begingroup$


By definition, $W_1=W_2 rightarrow W_1^0=W_2^0$, $W_1, W_2 subseteq V$ are subspaces of $V$. But how does one show the reverse implication? $V$ is not assumed to be finite dimensional.



The annihilator is defined as $S^0= {fin V^*| f(s)=0 forall sin S}$, where $Ssubseteq V, S$ is a subset of vector space V.










share|cite|improve this question











$endgroup$












  • $begingroup$
    What is your definition of the annihilator?
    $endgroup$
    – Bernard
    Nov 16 '15 at 20:27










  • $begingroup$
    @Bernard, added the definition.
    $endgroup$
    – grayQuant
    Nov 16 '15 at 20:32










  • $begingroup$
    That's what I thought, but I wondered if you were hiding an underlying structure.
    $endgroup$
    – Bernard
    Nov 16 '15 at 20:33














1












1








1





$begingroup$


By definition, $W_1=W_2 rightarrow W_1^0=W_2^0$, $W_1, W_2 subseteq V$ are subspaces of $V$. But how does one show the reverse implication? $V$ is not assumed to be finite dimensional.



The annihilator is defined as $S^0= {fin V^*| f(s)=0 forall sin S}$, where $Ssubseteq V, S$ is a subset of vector space V.










share|cite|improve this question











$endgroup$




By definition, $W_1=W_2 rightarrow W_1^0=W_2^0$, $W_1, W_2 subseteq V$ are subspaces of $V$. But how does one show the reverse implication? $V$ is not assumed to be finite dimensional.



The annihilator is defined as $S^0= {fin V^*| f(s)=0 forall sin S}$, where $Ssubseteq V, S$ is a subset of vector space V.







linear-algebra vector-spaces






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share|cite|improve this question








edited Nov 16 '15 at 20:30







grayQuant

















asked Nov 16 '15 at 20:22









grayQuantgrayQuant

1,11621749




1,11621749












  • $begingroup$
    What is your definition of the annihilator?
    $endgroup$
    – Bernard
    Nov 16 '15 at 20:27










  • $begingroup$
    @Bernard, added the definition.
    $endgroup$
    – grayQuant
    Nov 16 '15 at 20:32










  • $begingroup$
    That's what I thought, but I wondered if you were hiding an underlying structure.
    $endgroup$
    – Bernard
    Nov 16 '15 at 20:33


















  • $begingroup$
    What is your definition of the annihilator?
    $endgroup$
    – Bernard
    Nov 16 '15 at 20:27










  • $begingroup$
    @Bernard, added the definition.
    $endgroup$
    – grayQuant
    Nov 16 '15 at 20:32










  • $begingroup$
    That's what I thought, but I wondered if you were hiding an underlying structure.
    $endgroup$
    – Bernard
    Nov 16 '15 at 20:33
















$begingroup$
What is your definition of the annihilator?
$endgroup$
– Bernard
Nov 16 '15 at 20:27




$begingroup$
What is your definition of the annihilator?
$endgroup$
– Bernard
Nov 16 '15 at 20:27












$begingroup$
@Bernard, added the definition.
$endgroup$
– grayQuant
Nov 16 '15 at 20:32




$begingroup$
@Bernard, added the definition.
$endgroup$
– grayQuant
Nov 16 '15 at 20:32












$begingroup$
That's what I thought, but I wondered if you were hiding an underlying structure.
$endgroup$
– Bernard
Nov 16 '15 at 20:33




$begingroup$
That's what I thought, but I wondered if you were hiding an underlying structure.
$endgroup$
– Bernard
Nov 16 '15 at 20:33










2 Answers
2






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To prove $ W_1^0=W_2^0 Rightarrow W_1=W_2 $ we proceed by contraposition; suppose $ W_1 neq W_2$ then there is some vector $alpha in W_1 setminus W_2$. Now suppose $B_{W_2} = {w_1,...,w_k}$ be a basis of $W_2$. Then $ B_{W_2}cup { alpha }$ is linearly independent since $alphanotin W_2$. Extend $ B_{W_2}cup { alpha }$ to a basis of $V$ by $B_V={w_1,...,w_k,alpha,w_{k+2},...,w_n}.$
Now define a (unique) linear functional $f:Vrightarrow Bbb F $ such that $f(w_i)=0$ for $ i=1,...,k quad; f(alpha)=1_{Bbb F} ; $and $f(w_j)=1_{Bbb F}$ for $j=k+2,...,n$. Then clearly $f(w)=0 ; forall win W_2 $ (since $forall w in W_2 ;, w=a_1w_1+...+a_kw_k ; $for some $a_1,...,a_k in Bbb F$) i.e $f in W_2^0$ but $fnotin W_1^0$ since $alpha in W_1 $ and $f(alpha) neq 0$. Hence $ W_1^0 neq W_2^0$.



(We assume that $V$ is finite dimensional with $dim;V=n$)






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    I assume that here we are dealing with a finite dimensional vector space $V$. In this case, there exists some basis $B=v_1,...,v_n$ for $V$. We define the dual basis to be $B'=phi_1,...,phi_n$, where the bases satisfy the Kroenecker Delta condition. That is
    $$ phi_i(v_j)=delta_{ij}.$$
    This means that $phi_i(v_j)=1$ if and only if $i=j$. So consider then that we can express $W_1,W_2$ in terms of the basis vectors for $V$. So let
    $$ W_1=span(v_k,...,v_{ell})=W_2$$
    Then, by definition
    $$ W_1^0=span(phi_1,...phi_{k-1},phi_{ell+1},...,phi_n)=W_2^0.$$
    So, if we are given that $W_1^0=W_2^0$, we know that they are spanned by the same elements of the dual basis. And so:
    $$ W_1^0=span(phi_1,...phi_{k-1},phi_{ell+1},...,phi_n)=W_2^0 implies W_1=span(v_k,...,v_{ell})=W_2.$$
    This completes the proof.






    share|cite|improve this answer









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      2 Answers
      2






      active

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      2 Answers
      2






      active

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      active

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      active

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      1












      $begingroup$

      To prove $ W_1^0=W_2^0 Rightarrow W_1=W_2 $ we proceed by contraposition; suppose $ W_1 neq W_2$ then there is some vector $alpha in W_1 setminus W_2$. Now suppose $B_{W_2} = {w_1,...,w_k}$ be a basis of $W_2$. Then $ B_{W_2}cup { alpha }$ is linearly independent since $alphanotin W_2$. Extend $ B_{W_2}cup { alpha }$ to a basis of $V$ by $B_V={w_1,...,w_k,alpha,w_{k+2},...,w_n}.$
      Now define a (unique) linear functional $f:Vrightarrow Bbb F $ such that $f(w_i)=0$ for $ i=1,...,k quad; f(alpha)=1_{Bbb F} ; $and $f(w_j)=1_{Bbb F}$ for $j=k+2,...,n$. Then clearly $f(w)=0 ; forall win W_2 $ (since $forall w in W_2 ;, w=a_1w_1+...+a_kw_k ; $for some $a_1,...,a_k in Bbb F$) i.e $f in W_2^0$ but $fnotin W_1^0$ since $alpha in W_1 $ and $f(alpha) neq 0$. Hence $ W_1^0 neq W_2^0$.



      (We assume that $V$ is finite dimensional with $dim;V=n$)






      share|cite|improve this answer











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        1












        $begingroup$

        To prove $ W_1^0=W_2^0 Rightarrow W_1=W_2 $ we proceed by contraposition; suppose $ W_1 neq W_2$ then there is some vector $alpha in W_1 setminus W_2$. Now suppose $B_{W_2} = {w_1,...,w_k}$ be a basis of $W_2$. Then $ B_{W_2}cup { alpha }$ is linearly independent since $alphanotin W_2$. Extend $ B_{W_2}cup { alpha }$ to a basis of $V$ by $B_V={w_1,...,w_k,alpha,w_{k+2},...,w_n}.$
        Now define a (unique) linear functional $f:Vrightarrow Bbb F $ such that $f(w_i)=0$ for $ i=1,...,k quad; f(alpha)=1_{Bbb F} ; $and $f(w_j)=1_{Bbb F}$ for $j=k+2,...,n$. Then clearly $f(w)=0 ; forall win W_2 $ (since $forall w in W_2 ;, w=a_1w_1+...+a_kw_k ; $for some $a_1,...,a_k in Bbb F$) i.e $f in W_2^0$ but $fnotin W_1^0$ since $alpha in W_1 $ and $f(alpha) neq 0$. Hence $ W_1^0 neq W_2^0$.



        (We assume that $V$ is finite dimensional with $dim;V=n$)






        share|cite|improve this answer











        $endgroup$
















          1












          1








          1





          $begingroup$

          To prove $ W_1^0=W_2^0 Rightarrow W_1=W_2 $ we proceed by contraposition; suppose $ W_1 neq W_2$ then there is some vector $alpha in W_1 setminus W_2$. Now suppose $B_{W_2} = {w_1,...,w_k}$ be a basis of $W_2$. Then $ B_{W_2}cup { alpha }$ is linearly independent since $alphanotin W_2$. Extend $ B_{W_2}cup { alpha }$ to a basis of $V$ by $B_V={w_1,...,w_k,alpha,w_{k+2},...,w_n}.$
          Now define a (unique) linear functional $f:Vrightarrow Bbb F $ such that $f(w_i)=0$ for $ i=1,...,k quad; f(alpha)=1_{Bbb F} ; $and $f(w_j)=1_{Bbb F}$ for $j=k+2,...,n$. Then clearly $f(w)=0 ; forall win W_2 $ (since $forall w in W_2 ;, w=a_1w_1+...+a_kw_k ; $for some $a_1,...,a_k in Bbb F$) i.e $f in W_2^0$ but $fnotin W_1^0$ since $alpha in W_1 $ and $f(alpha) neq 0$. Hence $ W_1^0 neq W_2^0$.



          (We assume that $V$ is finite dimensional with $dim;V=n$)






          share|cite|improve this answer











          $endgroup$



          To prove $ W_1^0=W_2^0 Rightarrow W_1=W_2 $ we proceed by contraposition; suppose $ W_1 neq W_2$ then there is some vector $alpha in W_1 setminus W_2$. Now suppose $B_{W_2} = {w_1,...,w_k}$ be a basis of $W_2$. Then $ B_{W_2}cup { alpha }$ is linearly independent since $alphanotin W_2$. Extend $ B_{W_2}cup { alpha }$ to a basis of $V$ by $B_V={w_1,...,w_k,alpha,w_{k+2},...,w_n}.$
          Now define a (unique) linear functional $f:Vrightarrow Bbb F $ such that $f(w_i)=0$ for $ i=1,...,k quad; f(alpha)=1_{Bbb F} ; $and $f(w_j)=1_{Bbb F}$ for $j=k+2,...,n$. Then clearly $f(w)=0 ; forall win W_2 $ (since $forall w in W_2 ;, w=a_1w_1+...+a_kw_k ; $for some $a_1,...,a_k in Bbb F$) i.e $f in W_2^0$ but $fnotin W_1^0$ since $alpha in W_1 $ and $f(alpha) neq 0$. Hence $ W_1^0 neq W_2^0$.



          (We assume that $V$ is finite dimensional with $dim;V=n$)







          share|cite|improve this answer














          share|cite|improve this answer



          share|cite|improve this answer








          edited Oct 16 '17 at 12:40

























          answered Oct 16 '17 at 10:45









          Arpan DasArpan Das

          1078




          1078























              0












              $begingroup$

              I assume that here we are dealing with a finite dimensional vector space $V$. In this case, there exists some basis $B=v_1,...,v_n$ for $V$. We define the dual basis to be $B'=phi_1,...,phi_n$, where the bases satisfy the Kroenecker Delta condition. That is
              $$ phi_i(v_j)=delta_{ij}.$$
              This means that $phi_i(v_j)=1$ if and only if $i=j$. So consider then that we can express $W_1,W_2$ in terms of the basis vectors for $V$. So let
              $$ W_1=span(v_k,...,v_{ell})=W_2$$
              Then, by definition
              $$ W_1^0=span(phi_1,...phi_{k-1},phi_{ell+1},...,phi_n)=W_2^0.$$
              So, if we are given that $W_1^0=W_2^0$, we know that they are spanned by the same elements of the dual basis. And so:
              $$ W_1^0=span(phi_1,...phi_{k-1},phi_{ell+1},...,phi_n)=W_2^0 implies W_1=span(v_k,...,v_{ell})=W_2.$$
              This completes the proof.






              share|cite|improve this answer









              $endgroup$


















                0












                $begingroup$

                I assume that here we are dealing with a finite dimensional vector space $V$. In this case, there exists some basis $B=v_1,...,v_n$ for $V$. We define the dual basis to be $B'=phi_1,...,phi_n$, where the bases satisfy the Kroenecker Delta condition. That is
                $$ phi_i(v_j)=delta_{ij}.$$
                This means that $phi_i(v_j)=1$ if and only if $i=j$. So consider then that we can express $W_1,W_2$ in terms of the basis vectors for $V$. So let
                $$ W_1=span(v_k,...,v_{ell})=W_2$$
                Then, by definition
                $$ W_1^0=span(phi_1,...phi_{k-1},phi_{ell+1},...,phi_n)=W_2^0.$$
                So, if we are given that $W_1^0=W_2^0$, we know that they are spanned by the same elements of the dual basis. And so:
                $$ W_1^0=span(phi_1,...phi_{k-1},phi_{ell+1},...,phi_n)=W_2^0 implies W_1=span(v_k,...,v_{ell})=W_2.$$
                This completes the proof.






                share|cite|improve this answer









                $endgroup$
















                  0












                  0








                  0





                  $begingroup$

                  I assume that here we are dealing with a finite dimensional vector space $V$. In this case, there exists some basis $B=v_1,...,v_n$ for $V$. We define the dual basis to be $B'=phi_1,...,phi_n$, where the bases satisfy the Kroenecker Delta condition. That is
                  $$ phi_i(v_j)=delta_{ij}.$$
                  This means that $phi_i(v_j)=1$ if and only if $i=j$. So consider then that we can express $W_1,W_2$ in terms of the basis vectors for $V$. So let
                  $$ W_1=span(v_k,...,v_{ell})=W_2$$
                  Then, by definition
                  $$ W_1^0=span(phi_1,...phi_{k-1},phi_{ell+1},...,phi_n)=W_2^0.$$
                  So, if we are given that $W_1^0=W_2^0$, we know that they are spanned by the same elements of the dual basis. And so:
                  $$ W_1^0=span(phi_1,...phi_{k-1},phi_{ell+1},...,phi_n)=W_2^0 implies W_1=span(v_k,...,v_{ell})=W_2.$$
                  This completes the proof.






                  share|cite|improve this answer









                  $endgroup$



                  I assume that here we are dealing with a finite dimensional vector space $V$. In this case, there exists some basis $B=v_1,...,v_n$ for $V$. We define the dual basis to be $B'=phi_1,...,phi_n$, where the bases satisfy the Kroenecker Delta condition. That is
                  $$ phi_i(v_j)=delta_{ij}.$$
                  This means that $phi_i(v_j)=1$ if and only if $i=j$. So consider then that we can express $W_1,W_2$ in terms of the basis vectors for $V$. So let
                  $$ W_1=span(v_k,...,v_{ell})=W_2$$
                  Then, by definition
                  $$ W_1^0=span(phi_1,...phi_{k-1},phi_{ell+1},...,phi_n)=W_2^0.$$
                  So, if we are given that $W_1^0=W_2^0$, we know that they are spanned by the same elements of the dual basis. And so:
                  $$ W_1^0=span(phi_1,...phi_{k-1},phi_{ell+1},...,phi_n)=W_2^0 implies W_1=span(v_k,...,v_{ell})=W_2.$$
                  This completes the proof.







                  share|cite|improve this answer












                  share|cite|improve this answer



                  share|cite|improve this answer










                  answered Nov 16 '15 at 20:29









                  Antonios-Alexandros RobotisAntonios-Alexandros Robotis

                  10.6k41741




                  10.6k41741






























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