Adjoint Operation in Shankar's "Principles of Quantum Mechanics

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Discussion Overview

The discussion revolves around the adjoint operation as presented in R. Shankar's "Principles of Quantum Mechanics," specifically examining the notation and implications of equations 1.3.8 and 1.3.9. Participants explore the meanings of various symbols and the relationships between kets and bras in quantum mechanics.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • Some participants question whether the notation in Shankar's text is a typo, particularly regarding the transition from to
  • Clarifications are sought about the meanings of symbols, with some participants explaining that a is a complex number, is a column vector.
  • There is a discussion about the notation used for the mapping of kets to bras, with some preferring a two-way association symbol (↔) instead of the one-way (→) used by Shankar.
  • Participants express uncertainty about whether a is a complex number or an operator, with differing opinions on the implications of this distinction.
  • One participant explains that the bra , and discusses the implications of complex conjugation in this context.
  • Another participant clarifies that complex conjugate applies only to complex numbers and not to kets, emphasizing the linearity of the inner product in quantum mechanics.

Areas of Agreement / Disagreement

Participants exhibit a mix of agreement and disagreement regarding the interpretation of the notation and the properties of the adjoint operation. Some points are clarified, but no consensus is reached on whether the original notation is a typo.

Contextual Notes

Participants note the importance of understanding the definitions and relationships between the symbols used in quantum mechanics, which may depend on the specific context and notation employed by Shankar.

Getterdog
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Confused
In R Shankar text on “principles of quantum mechanics’ discussing the adjoint operation, 1.3.8 shows that a|V> => <V|a*. Then 1.3.9 then states

that <aV| = <V|a*. Is this a typo error?
 
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Getterdog said:
Summary:: Confused

In R Shankar text on “principles of quantum mechanics’ discussing the adjoint operation, 1.3.8 shows that a|V> => <V|a*. Then 1.3.9 then states

that <aV| = <V|a*. Is this a typo error?
It might help if you were more explicit about what all these symbols mean. For example, what does this mean?
$$a|V \rangle \ \Rightarrow \ \langle V|a^*$$
 
PeroK said:
It might help if you were more explicit about what all these symbols mean. For example, what does this mean?
$$a|V \rangle \ \Rightarrow \ \langle V|a^*$$
Well.a is a complex number, <v| is a row vector, |V> is a column vector.
 
Getterdog said:
Well.a is a complex number, <v| is a row vector, |V> is a column vector.
Ah! When you said "adjoint operation" I thought ##V## was an operator. That makes sense.

I would say that ##\langle V|## is a bra and ##|V \rangle## is a ket.

It's not a typo. What are ##\langle aV|## and ##\langle V| a^*##? Before you can see they are equal you first have to understand fully what they are. Can you describe each precisely?
 
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Getterdog said:
Well.a is a complex number, <v| is a row vector, |V> is a column vector.
And, I guess ##\Rightarrow## means "is associated with" via the mapping of kets to bra?

I would tend to write ##\leftrightarrow##, as it's a two-way association. But, if that's Shankar's notation, then stick with it.
 
Getterdog said:
a is a complex number

A complex number or an operator? I think it's the latter (since otherwise ##a^*## would not need to multiply the bra ##\langle V \vert## from the right).
 
PeterDonis said:
A complex number or an operator? I think it's the latter (since otherwise ##a^*## would not need to multiply the bra ##\langle V \vert## from the right).

I think I've seen that convention where complex scalars are shown on the right of bras.
 
He states that a is a scalar. And I presume complex.
 
PeroK said:
Ah! When you said "adjoint operation" I thought ##V## was an operator. That makes sense.

I would say that ##\langle V|## is a bra and ##|V \rangle## is a ket.

It's not a typo. What are ##\langle aV|## and ##\langle V| a^*##? Before you can see they are equal you first have to understand fully what they are. Can you describe each precisely?
Inside the bra ,<aV |would be a complex scalar times V which is presumed to be the complex conjugate in row form of some other vector v in column form. Since complex multiplication is communitive, I assume <Va| is the same. I’m not clear why taking the a outside of the bra,creates the scalars complex conjugate
 
  • #10
Getterdog said:
Inside the bra ,<aV |would be a complex scalar times V which is presumed to be the complex conjugate in row form of some other vector v in column form. Since complex multiplication is communitive, I assume <Va| is the same. I’m not clear why taking the a outside of the bra,creates the scalars complex conjugate
##\langle aV |## is the bra associated with the ket ##|aV \rangle##

If you don't immediately see that, just let ##U = aV##.

And, what can you now say about ##|aV \rangle##?
 
  • #11
PeroK said:
##\langle aV |## is the bra associated with the ket ##|aV \rangle##

If you don't immediately see that, just let ##U = aV##.

And, what can you now say about ##|aV \rangle##?
Ok, doesn’t that mean that in <aV|, both a and V are complex conjugates of |aV> ?
 
  • #12
Getterdog said:
Ok, doesn’t that mean that in <aV|, both a and V are complex conjugates of |aV> ?
Complex conjugate applies only to complex numbers. You don't have the complex conjugate of a ket.

Let me explain this then.

First, as I already said: ##\langle aV |## is the bra associated with the ket ##|aV \rangle##

And, we know that ##|aV \rangle = a |V \rangle##.

Then, we know from your original post that the bra associated with ##a |V \rangle## is ##\langle V|a^*##.

Putting this all together we have: ##\langle aV | = \langle V|a^*##

Note that bras and kets are intended to form the inner product, which in QM is linear in the second argument. In other words we have:
$$\langle V|aU \rangle = a \langle V|U \rangle \ \text{and} \ \langle aV|U \rangle = a^* \langle V|U \rangle$$
And that's another reason that when you take a complex scalar outside of a bra you get its complex conjugate.
 
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  • #13
Getterdog said:
Ok, doesn’t that mean that in <aV|, both a and V are complex conjugates of |aV> ?
Yep got the obvious,, now. I guess my confusion what why it’s not marked inside the bra as it is outside. Presumably to avoid confusion when doing further inner product calculation. I seems obvious now. I feel stupid! Thanks
 
  • #14
PeroK said:
Complex conjugate applies only to complex numbers. You don't have the complex conjugate of a ket.

Let me explain this then.

First, as I already said: ##\langle aV |## is the bra associated with the ket ##|aV \rangle##

And, we know that ##|aV \rangle = a |V \rangle##.

Then, we know from your original post that the bra associated with ##a |V \rangle## is ##\langle V|a^*##.

Putting this all together we have: ##\langle aV | = \langle V|a^*##

Note that bras and kets are intended to form the inner product, which in QM is linear in the second argument. In other words we have:
$$\langle V|aU \rangle = a \langle V|U \rangle \ \text{and} \ \langle aV|U \rangle = a^* \langle V|U \rangle$$
And that's another reason that when you take a complex scalar outside of a bra you get its complex conjugate.
Yep,got it now. Thanks.your last equation clears it up.
 

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