Weinberg QFT p.65-66: Orthonormality of States with Momentum k

Thank you. In summary, the person is seeking clarification on the concept of orthonormal states with standard momentum k and the use of k' in the calculation of the scalar product for states with arbitrary momenta. In response, it is explained that states with the same momentum k should be orthogonal to each other, and the use of k' in the calculation is to represent the momentum of the second state, which is also k in this case.
  • #1
Rick89
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Homework Statement


He says "choose the states with standard momentum k to be orthonormal", does he mean for example state with momentum (0,0,0,M1) and with momentum (0,0,0,M2) to be orthogonal or states with the same k^2 to be orthogonal if they have different k?
Also where he calculates in the next page, the "scalar product for [states of] arbitrary momenta" why is k' defined there the "same" as that in formula (2.5.12)? I don't get it...


Homework Equations


in the book...


The Attempt at a Solution


if the states of one given k^2 are orthogonal among each other then I don't get why k' as defined in page 66 could have the same square as k (that comes from p)... otherwise I don't get why we expect k' to be of the form of a "standard momentum" according to the way it is defined
 
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  • #2


Based on the information provided, it seems like the person is asking for clarification on the concept of orthonormal states with standard momentum k. They are also confused about the use of k' in the calculation of the scalar product for states with arbitrary momenta.

my response would be:

Thank you for your question. When someone mentions "orthonormal states with standard momentum k," they are referring to states with the same momentum k being orthogonal to each other. In other words, states with different k values should not be orthogonal to each other. This is because the momentum k is a defining characteristic of a state, and states with different k values represent different physical states.

As for the use of k' in the calculation of the scalar product, it is defined as the same momentum as k because in the context of the calculation, we are looking at the scalar product between two states with the same momentum k. Therefore, it makes sense to use k' to represent the momentum of the second state.

I hope this helps clarify your confusion. If you have any further questions, please don't hesitate to ask.
 

FAQ: Weinberg QFT p.65-66: Orthonormality of States with Momentum k

What is Weinberg QFT p.65-66?

Weinberg QFT refers to the textbook "The Quantum Theory of Fields" written by renowned physicist Steven Weinberg. Pages 65-66 specifically discuss the concept of orthonormality of states with momentum k in quantum field theory.

What is orthonormality of states with momentum k?

In quantum field theory, orthonormality refers to the property of states with different quantum numbers being perpendicular to each other. In the context of momentum k, it means that states with different values of k are orthogonal to each other, or in other words, their inner product is zero.

Why is orthonormality important in quantum field theory?

Orthonormality is important because it ensures that different states with different quantum numbers are distinguishable from each other. This allows for the superposition of states and the calculation of transition amplitudes, which are essential in understanding the behavior of particles in quantum field theory.

How is orthonormality of states with momentum k mathematically expressed?

The orthonormality of states with momentum k is mathematically expressed as the inner product of two states, |k> and |k'>, being equal to 0 when k is not equal to k'. In other words, = 0 for k ≠ k'.

What are the implications of violating orthonormality in quantum field theory?

If orthonormality is violated, it would mean that states with different quantum numbers are no longer distinguishable from each other. This would lead to incorrect calculations and predictions about the behavior of particles in quantum field theory.

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