Understanding Peskin's QFT: Deriving Equations (2.35) and (2.54)

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In summary, the conversation is about two questions regarding Peskin's QFT book, specifically the derivation of equations (2.35) and (2.54). The first question involves a discrepancy between the prefactors in Peskin's equation (2.36) and the combined ket equation, while the second question is about the inclusion of semi-cycles in a principal value integral.
  • #1
Beginner_2010
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Homework Statement


Hi,

I have two stupid questions about Peskin's QFT book.

(1) P23, How to derive from (2.35) to (2.36)
(2) P30, How to derive (2.54)

Homework Equations



(1)
peskin_23.gif

(2)
Perskin_30.gif


The Attempt at a Solution



(1) If I consider the dual-space vector, [tex] \langle \mathbf{q} | = \sqrt{2 E_{\mathbf{q} }} \langle 0 | a_{\mathbf{q}} [/tex]

Combine with the ket (2.35), obtain
[tex]

\langle\mathbf{q} | \mathbf{p} \rangle = 2 \sqrt{ E_{\mathbf{q}} E_{\mathbf{p} } } \langle 0 | a_{\mathbf{q}} a_{\mathbf{p}}^{\dag} | 0 \rangle
= 2 \sqrt{ E_{\mathbf{q}} E_{\mathbf{p} } } (2 \pi)^{3} \delta^{(3)} (\mathbf{p} - \mathbf{q})
[/tex]

Therefore
[tex]
\langle \mathbf{p} | \mathbf{q} \rangle = \langle \mathbf{q} | \mathbf{p} \rangle^* = 2 \sqrt{ E_{\mathbf{q}} E_{\mathbf{p} } } (2 \pi)^{3} \delta^{(3)} (\mathbf{p} - \mathbf{q})
[/tex]

But Peskin's (2.36) has a prefactor [tex] 2 E_{\mathbf{p}} [/tex] instead of [tex] 2 \sqrt{ E_{\mathbf{q}} E_{\mathbf{p} } } [/tex], is that made to be the convention?

(2) Is that the principal value of integral [tex] \int_{- \infty}^{+\infty} d p^0 [/tex] or including the little semi-cycles around [tex] -E_{\mathbf{p}} [/tex] and[tex] +E_{\mathbf{p}} [/tex] ? If includes the semi-cycles, i can get the result

Thank you ^_^
 
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  • #2
Beginner_2010 said:

The Attempt at a Solution



(1) If I consider the dual-space vector, [tex] \langle \mathbf{q} | = \sqrt{2 E_{\mathbf{q} }} \langle 0 | a_{\mathbf{q}} [/tex]

Combine with the ket (2.35), obtain
[tex]

\langle\mathbf{q} | \mathbf{p} \rangle = 2 \sqrt{ E_{\mathbf{q}} E_{\mathbf{p} } } \langle 0 | a_{\mathbf{q}} a_{\mathbf{p}}^{\dag} | 0 \rangle
= 2 \sqrt{ E_{\mathbf{q}} E_{\mathbf{p} } } (2 \pi)^{3} \delta^{(3)} (\mathbf{p} - \mathbf{q})
[/tex]

Therefore
[tex]
\langle \mathbf{p} | \mathbf{q} \rangle = \langle \mathbf{q} | \mathbf{p} \rangle^* = 2 \sqrt{ E_{\mathbf{q}} E_{\mathbf{p} } } (2 \pi)^{3} \delta^{(3)} (\mathbf{p} - \mathbf{q})
[/tex]

But Peskin's (2.36) has a prefactor [tex] 2 E_{\mathbf{p}} [/tex] instead of [tex] 2 \sqrt{ E_{\mathbf{q}} E_{\mathbf{p} } } [/tex], is that made to be the convention?
The delta function is non-zero only when p=q, so Ep=Eq.
(2) Is that the principal value of integral [tex] \int_{- \infty}^{+\infty} d p^0 [/tex] or including the little semi-cycles around [tex] -E_{\mathbf{p}} [/tex] and[tex] +E_{\mathbf{p}} [/tex]? If it includes the semi-cycles, I can get the result.
 
  • #3
Thank you!
 

Related to Understanding Peskin's QFT: Deriving Equations (2.35) and (2.54)

1. What is Peskin's QFT?

Peskin's QFT (Quantum Field Theory) is a theoretical framework used in particle physics to describe the interactions between particles and their associated fields.

2. Why is it called "Two stupid questions about Peskin's QFT"?

The term "Two stupid questions" is often used as a humorous way to refer to questions that may seem simple or basic, but are actually important to understanding a complex topic such as QFT.

3. What are the main concepts of Peskin's QFT?

The main concepts of Peskin's QFT include the quantization of fields, renormalization, and the use of Feynman diagrams to calculate particle interactions.

4. Is Peskin's QFT widely accepted in the scientific community?

Yes, Peskin's QFT is a well-established and widely accepted framework in the scientific community for understanding and studying the behavior of particles and their interactions.

5. What are some practical applications of Peskin's QFT?

Peskin's QFT has many practical applications in particle physics, including predicting and explaining the behavior of particles in high-energy collisions, and providing a framework for developing new theories and models in particle physics.

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