Quantum mechanics Hermitian operator

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Homework Help Overview

The discussion revolves around the properties of Hermitian operators in quantum mechanics, specifically focusing on the criteria involving the inner product of states and an operator. The original poster attempts to show that certain conditions can be simplified when considering the operator's action on different physical states.

Discussion Character

  • Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants explore the implications of the operator's action on arbitrary states and question the relevance of the parameter n in the context of the problem. There is a discussion about the relationship between the operator and its adjoint, as well as the significance of the inner product being zero.

Discussion Status

Participants are actively questioning the notation and assumptions presented, with some suggesting that the original poster's reasoning may be overly complex. There is a recognition that demonstrating the condition for one state may suffice, but the exploration of generality remains a point of discussion.

Contextual Notes

Some participants express confusion regarding the notation and the role of the states involved, indicating a need for clarification on the definitions and relationships between the operator and the states.

binbagsss
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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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