Quantum mechanics Hermitian operator

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SUMMARY

The discussion focuses on the properties of Hermitian operators in quantum mechanics, specifically the operator ##L_n## and its relationship with physical states ##|p>## and ##|p'>##. Participants clarify that if ## = 0## for all states, it implies ##L_n|p> = 0## for ##n > 0##. The equivalence of the inner products and the implications of conjugation between operators are emphasized, leading to the conclusion that demonstrating the operator's action on arbitrary states is sufficient for proving its properties.

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Homework Statement



I have the criteria:

## <p'| L_{n} |p>=0 ##,for all ##n \in Z ##

##L## some operator and ## |p> ##, ## |p'> ##some different physical states

I want to show that given ## L^{+}=L_{-n} ## this criteria reduces to only needing to show that:

##L_n |p>=0 ## for ##n>0 ##

Homework Equations


look up , look down,

The Attempt at a Solution


[/B]
##<p'|L_n|p>^{+}=<p|L_n^{+}|p'>=<p|L_{-n}|p'>##

So from this I can deduce that showing :

##<p'|L_n|p>^{+}## is satisfied is equivalent to showing that ##<p|L_{-n}|p'>## is satisfied.

I.e I can reduce the criteria from showing for all ##n \in Z## to showing for ##n>0## only, BUT I am still sandwiched between two different physical states, I don't understand how this means you can reduce further to showing only that ##L_n |p>=0##, ##n >0 ## acting on solely a ket/bra...

Many thanks in advance.
 
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So I don't understand some of your notation. Do you mean L_n^\dagger = L_{-n}? Also are |p&gt; and |p&#039;&gt; arbitrary? It seems like having an operator act on a ket and then taking the inner product always giving zero would mean the operator gives zero on the ket. All the extra parts about n aren't really relevant. You can consider one n. If L_n=0 the you can show L_{-n} =0 if they are related by conjugation.
 
Dazed&Confused said:
So I don't understand some of your notation. Do you mean L_n^\dagger = L_{-n}? Also are |p&gt; and |p&#039;&gt; arbitrary?

yes
Dazed&Confused said:
It seems like having an operator act on a ket and then taking the inner product always giving zero would mean the operator gives zero on the ket.

mm I thought the idea for using two different states ## |p'> ## and ## |p> ## is to show that this result holds for general arbitrary states, rather than showing that ##<p|L_n|p> = 0 ## . I agree that if we wanted to show that this was zero then ##L_n|p> = 0## is enough for the inner product to be zero.
Dazed&Confused said:
All the extra parts about n aren't really relevant. You can consider one n. If L_n=0 the you can show L_{-n} =0 if they are related by conjugation.

yup
 
I just can't imagine a situation where if &lt;p|L_n|p&#039;&gt;=0 for all |p&gt; and |p&#039;&gt; and they aren't equal that L_n \neq 0. For example say |p&#039;&gt; = L_n|p&gt;. I mean it must be some state right? Then the condition implies &lt;p&#039;|p&#039;&gt; =0 which by the properties of vector implies |p&#039;&gt; = L_n |p&gt; =0.
 

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