Quantum mechanics- eigenvectots of a linear transformation

Therefore, the number of eigenvectors will always be equal to the dimension of the vector space.In summary, the conversation discusses the use of eigenvectors as a basis for a linear operator on a vector space. The text states that if the eigenvectors span the space, they can be used as a basis. However, there is a mention of a possible scenario where the eigenvectors may not form a basis if they are not linearly independent. This is a basic result from linear algebra for vector spaces of finite dimension, where every basis must have the same number of vectors as the dimension of the vector space.
  • #1
Syrus
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Homework Statement



My quantum mechanics text (in an appendix on linear algebra) states, "f the eigenvectors span the space... we are free to use them as a basis..." and then states:

T|f1> = λ1f1
.
.
.
T|fn> = λnfn


My question is: is it not true that fewer than n vectors might constitute this "new" basis? In other words, if the eigenvectors span the space, they may not (all together, at least) form a basis.




Homework Equations





The Attempt at a Solution

 
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  • #2
No, this is a basic result from linear algebra for vector spaces of finite dimension. In an n-dimensional space, every basis has to have n vectors.
 
  • #3
Yes, I see. But when, then, all the talk about "An eigenbasis for a linear operator that operates on a vector space is a basis for that consists entirely of eigenvectors of (possibly with different eigenvalues). Such a basis may not exist."

See http://en.wikipedia.org/wiki/Eigenvalues_and_eigenvectors under the heading 'eigenbasis'
 
  • #4
It's possible that an operator will not have n linearly independent eigenvectors, so its eigenvectors can not span the vector space and therefore will not form a basis.

Your text, however, is saying if the eigenvectors span the space, they can be used as a basis. The assumption is that the linear operator has n linearly independent eigenvectors.
 
  • #5


Yes, it is possible for fewer than n eigenvectors to constitute a basis for the space. This is because eigenvectors can be linearly independent, meaning they can form a basis for the space without needing all n vectors. This is known as a "minimal eigenbasis" and is often used in quantum mechanics calculations for simplicity and ease of use. However, it is important to note that the number of eigenvectors needed for a minimal eigenbasis will vary depending on the specific transformation and the dimension of the space.
 

FAQ: Quantum mechanics- eigenvectots of a linear transformation

What are eigenvectors in quantum mechanics?

Eigenvectors in quantum mechanics are special vectors that represent the states in which a quantum system can exist. They are associated with specific eigenvalues, which represent the possible outcomes of a measurement on that system.

How are eigenvectors used in quantum mechanics?

Eigenvectors are used to describe the behavior of quantum systems and to make predictions about their behavior. They are also used to determine the possible states that a system can occupy and the probabilities of measuring those states.

What is the significance of eigenvectors in quantum mechanics?

Eigenvectors are significant in quantum mechanics because they represent the fundamental states of a quantum system. They also play a key role in determining the behavior and properties of quantum systems, and are essential for making accurate predictions.

How are eigenvectors of a linear transformation related to quantum mechanics?

Eigenvectors of a linear transformation are related to quantum mechanics because they represent the possible states of a quantum system and how they are transformed by the system's dynamics. They are also used to find the eigenvalues of the associated Hamiltonian, which determines the energy levels of the system.

Can you explain the concept of superposition in terms of eigenvectors?

Superposition in quantum mechanics refers to the ability of a quantum system to exist in multiple states simultaneously. This can be understood in terms of eigenvectors, as the system can be represented as a linear combination of its eigenvectors, with each eigenvector corresponding to a different state. The coefficients of the linear combination determine the probabilities of measuring each state.

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