Find Vector Representation of |ψi> in |ei> basis

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Homework Help Overview

The discussion revolves around finding the vector representation of a quantum state |ψi> in a specified basis |ei>. The original poster presents a ket expressed in terms of complex coefficients and seeks both column and row vector representations in the corresponding basis.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants explore the relationship between the coefficients c1 and c2 and their representations in vector form. There is an attempt to derive these coefficients through inner products with basis states. Questions arise regarding the correct representation of the bra corresponding to the ket, with some confusion about the distinction between transposition and Hermitian transposition.

Discussion Status

The conversation includes attempts to clarify the mathematical representations and the nature of the bra-ket relationship. Some guidance has been provided regarding the arrangement of coefficients in vector form, but there remains uncertainty about the proper notation and representation for the bra.

Contextual Notes

Participants are working under the constraints of homework guidelines, which may limit the extent of assistance provided. There is an emphasis on understanding the conventions used in quantum mechanics regarding vector representations.

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Homework Statement



Consider the following ket: |ψi> = c1|e1> + c2|e2>, where ci are some complex coefficients. Find the column-vector representation of |ψi> in the |ei> basis. Find the row-vector representation of <ψ| in the <ei| basis.

Homework Equations


i> = c1|e1> + c2|e2>

The Attempt at a Solution



Well I'm not sure what to do so I tried to start off by solving c1 and c2. To do this I multiplied |ψi> = c1|e1> + c2|e2> by <e1| to get that c1 = <e1|ψ> . Multiplying the same equation by <e2| gives c2 = <e2|ψ>

So I wrote |ψ> = <e1|ψ|e1> + <e2|ψ|e2>

Now I'm not sure what to do
 
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The question asks for you to write it as column and row vectors, i.e.,
$$
\begin{pmatrix} a \\ b \end{pmatrix}
$$
and ##(\alpha, \beta)##.

I'll give you the answer for the first part, since you are almost there and there is no fundamental principle here, just a convention. Basically, you simply need to arrange your ##c_i## in a vector, so for ##|\psi_i\rangle##, you get the representation
$$
|\psi_i\rangle \doteq \begin{pmatrix} \langle e_1 | \psi_i \rangle \\ \langle e_2 | \psi_i \rangle \end{pmatrix} = \begin{pmatrix} c_1 \\ c_2 \end{pmatrix}
$$
(with ##\doteq## meaning "is represented by," as the representation is not unique and will depend on the basis used and the order of the base states in that basis).

I'll let you figure out what the answer looks like for a bra.
 
Wouldn't the bra just be

(c1 c2) as you can just take the transpose of the matrix?
 
jasonchiang97 said:
Wouldn't the bra just be

(c1 c2) as you can just take the transpose of the matrix?
Not exactly. The bra is not equivalent to the transpose of the ket, but to its Hermitian transpose.
 
Ah I see. Thanks!
 
jasonchiang97 said:

Homework Statement



Consider the following ket: |ψi> = c1|e1> + c2|e2>, where ci are some complex coefficients. Find the column-vector representation of |ψi> in the |ei> basis. Find the row-vector representation of <ψ| in the <ei| basis.

Homework Equations


i> = c1|e1> + c2|e2>

The Attempt at a Solution



Well I'm not sure what to do so I tried to start off by solving c1 and c2. To do this I multiplied |ψi> = c1|e1> + c2|e2> by <e1| to get that c1 = <e1|ψ> . Multiplying the same equation by <e2| gives c2 = <e2|ψ>

So I wrote |ψ> = <e1|ψ|e1> + <e2|ψ|e2>

Now I'm not sure what to do
Watch out, the last expression you wrote is nonsensical because you have a ket on the left and a number on the right. You really meant
|ψ> = <e1|ψ> |e1> + <e2|ψ> |e2>
 
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