Ket Notation - Effects of the Projection Operator

In summary, the conversation discusses the effects of the projection operator in relation to Sakurai's Modern Quantum Mechanics (Revised Edition) and equation 1.3.12. It is mentioned that the summation can be moved to the left and a fundamental property of the inner product is referenced. The conversation also considers the case of considering the eigenkets of a hermitian operator and whether all operators on it are real. The conclusion is that there is no assumption that the operator is real, but that the absolute value appears in the formula due to the property of the inner product.
  • #1
Questioneer
7
0
Ket Notation -- Effects of the Projection Operator

Homework Statement


From Sakurai's Modern Quantum Mechanics (Revised Edition), it is just deriving equation 1.3.12.


Homework Equations


[tex] \begin{eqnarray*}\langle \alpha |\cdot (\sum_{a'}^N |a'\rangle \langle a'|) \cdot|\alpha \rangle \end{eqnarray*} [/tex]

The Attempt at a Solution


The summation can be moved to the left, so everything is being summed from a' to N, but does an alpha bra inner product with a' (or <α|a'>) does the sum of this from all a' to N equal Ʃ<a'|α>? maybe this is simple and I just can't see it?
 
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  • #2


Check (1.2.12), which is a fundamental property of the inner product. That property holds even when the bras and kets correspond to different bases.
 
  • #3


fzero said:
Check (1.2.12), which is a fundamental property of the inner product. That property holds even when the bras and kets correspond to different bases.

So, is it in this particular case that they are equal because we are considering the eigenkets of A, a hermitian operator? Because these are the eigenkets of A, does that mean that all operators on it are real? Even though it is the operator <α| acting on it and not A?
 
  • #4


Questioneer said:
So, is it in this particular case that they are equal because we are considering the eigenkets of A, a hermitian operator? Because these are the eigenkets of A, does that mean that all operators on it are real? Even though it is the operator <α| acting on it and not A?

There's no assumption here that [itex]\langle \alpha | a'\rangle[/itex] is real, just that [itex]\langle \alpha | a'\rangle = \langle a'| \alpha\rangle^*.[/itex] That is why the absolute value appears in the formula.
 
  • #5



Ket notation, also known as bra-ket notation, is a powerful tool used in quantum mechanics to represent and manipulate quantum states. The projection operator, denoted by |a'><a|, is a fundamental concept in quantum mechanics and is used to project a quantum state onto a specific subspace. This operator has important effects on the resulting state and can be represented in ket notation as |a><a|.

In the given equation, the summation is being performed over all possible states a' to N. This means that the resulting state will be a combination of all these states, weighted by their respective inner product with the state |α>. In other words, the projection operator is projecting the state |α> onto the subspace spanned by the states |a'>, and the resulting state is a linear combination of these projected states. This is a powerful tool in quantum mechanics, as it allows us to manipulate and study quantum states in a more intuitive way.

Moving the summation to the left does not change the overall result, as it is simply a rearrangement of terms. However, it is important to note that the projection operator is a Hermitian operator, meaning that its transpose is equal to its complex conjugate. This property ensures that the resulting state will also be normalized, preserving the probabilistic interpretation of quantum mechanics.

In conclusion, the projection operator in ket notation has important effects on the resulting state, allowing us to project and manipulate quantum states in a more intuitive way. It is a fundamental concept in quantum mechanics and is crucial for understanding and solving problems in this field.
 

Related to Ket Notation - Effects of the Projection Operator

1. What is Ket notation?

Ket notation, also known as Dirac notation, is a mathematical notation used in quantum mechanics to represent vectors in a Hilbert space. It is written as a vertical bar enclosing the vector, such as |psi>. The ket represents the state of a quantum system.

2. What is the Projection Operator in Ket notation?

The Projection Operator is a mathematical operator represented by the symbol P. In Ket notation, it is used to project a vector onto a subspace. It is commonly used to determine the probability of a quantum state collapsing into a specific state upon measurement.

3. How is the Projection Operator applied in Ket notation?

The Projection Operator is applied by multiplying it with a ket vector. This results in a new vector, representing the projection of the original vector onto the subspace. Mathematically, it is written as P|v> = |w>, where |v> is the original vector, P is the Projection Operator, and |w> is the projected vector.

4. What are the effects of the Projection Operator in Ket notation?

The effects of the Projection Operator depend on the properties of the subspace onto which the vector is projected. If the subspace is orthogonal, the projected vector will be the same as the original vector. However, if the subspace is not orthogonal, the Projection Operator will "collapse" the vector onto the closest vector in the subspace.

5. How is the Projection Operator used in quantum mechanics?

The Projection Operator is commonly used in quantum mechanics to calculate the probability of a quantum system being in a certain state. By projecting the state vector onto a specific subspace, the squared magnitude of the resulting vector represents the probability of the system being in that state upon measurement.

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