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2 votes
1 answer
787 views

LSZ reduction derivation Srednicki [duplicate]

In the derivation of the LSZ reduction formula equation (5.21) Srednicki claims that in case of an interaction term in the Lagrangian density $a^{\dagger}(\textbf{k})$ will no longer be time dependent....
Soumil's user avatar
  • 353
14 votes
2 answers
2k views

On the interpretation of Feynman diagrams

I am currently trying to find out about what exactly Feynman diagrams are, and up until now I have mainly used the lecture notes 'Mathematical ideas and notions of quantum field theory' by Etingof. In ...
S.Farr's user avatar
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5 votes
2 answers
1k views

The use of $a^\dagger(\mathbf{k}) = -i \int d^3x e^{ikx}\stackrel{\leftrightarrow}{\partial}_0 \phi(x)$ in the derivation of the LSZ-formula

I noticed that in Srednicki's derivation of the LSZ-formula the expression (chapter 5) for the creation (and also later for the annihilation) operator by the field operator: $$a^\dagger(\mathbf{k}) = -...
Frederic Thomas's user avatar
4 votes
3 answers
1k views

The contradiction between Gell-mann Low theorem and the identity of Møller operator $H\Omega_{+}=\Omega_{+}H_0$

This question originates from reading the proof of Gell-mann Low thoerem. $H=H_0+H_I$, let $|\psi_0\rangle$ be an eigenstate of $H_0$ with eigenvalue $E_0$, and consider the state vector defined as $$|...
346699's user avatar
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7 votes
2 answers
879 views

QFT - Why do in and out states have a non-trivial overlap?

I'm trying to follow chapter 4 about interacting fields in Peskin and Schröder. They define the S-matrix by $$_{\mathrm{out}}\langle p_1 p_2 | k_a k_b\rangle_{\mathrm {in}} = \langle p_1 p_2 | S | k_a ...
user2224350's user avatar
11 votes
2 answers
826 views

How to replace $T$-product with retarded commutator in LSZ formula?

I am reading Itzykson and Zuber's Quantum Field Theory book, and am unable to understand a step that is made on page 246: Here, they consider the elastic scattering of particle $A$ off particle $B$: ...
QuantumDot's user avatar
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3 votes
1 answer
730 views

Confusion about modes and quantum field theory

I'm learning quantum field theory from P&S and Srednicki. I'm having a lot of difficulties understanding the concept of a momentum state. In particular, I'm confused about how to interpret the ...
user avatar
3 votes
3 answers
353 views

Are the photons that we detect with our eyes virtual? [duplicate]

From asking several questions about virtual particles on this website, the most popular consensus (on PSE at least) seems to be that they are nothing more than a convenient way of expressing a ...
Alex Gower's user avatar
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3 votes
2 answers
414 views

Proof that asymptotic particle states are free

In quantum field theory, It’s often said that the interacting annihilation operator (defined by the Klein Gordon inner product between the interacting field and a plane wave) behaves like the free ...
user avatar
5 votes
1 answer
773 views

Vacuum, creation and annihilation operators in interacting QFT

I am reading the QFT book by M. Schwartz. More specifically, I have issues with the section about LSZ. I am puzzled with the way the creation and annihilation operators from the free theory act there. ...
Dr.Yoma's user avatar
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6 votes
1 answer
568 views

What is the role of wave packets in LSZ formulae?

When deriving LSZ formulae, we assume asymptotic particles’ creation/annihilation operators as: $$a_\text{g,in/out}\ \ (\mathbf{p})\equiv \int d^3k \ g(\mathbf{k}) a_\text{in/out}(\mathbf{k}), \ \text{...
Siam's user avatar
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1 vote
1 answer
470 views

I really wonder about the time derivative of creation and annihilation operators in the derivation of LSZ

On p. 71 below eq. (6.12) in Schwartz book, they assume that $$\lim_{t \to \pm\infty}\partial_0 a_p(t)=0.\tag{1}$$ But I thought that this is just an assumption. So we have to construct the ...
정재훈's user avatar
3 votes
1 answer
472 views

Asymptotic states in the Heisenberg and Schrödinger pictures

One can show that, in the interacting theory, the operators that create single-particle energy-momentum eigenstates from the vacuum are \begin{align} (a_p^{\pm\infty})^\dagger=\lim_{t\to\pm\infty}(...
Kris Walker's user avatar
  • 1,060
4 votes
0 answers
265 views

Why does $U(+\infty,-\infty)|0\rangle= e^{i \theta}|0\rangle$ hold ? i.e. time evolution of vacuum is still a vacuum

In quantum field theory, we always use $U(+\infty,-\infty)|0\rangle= e^{i \theta}|0\rangle$, where $$U(+\infty,-\infty)=\lim_{\epsilon\rightarrow +0} \mathcal{T}\exp\{i \int_{-\infty}^{+\infty} e^{-\...
user avatar
3 votes
0 answers
177 views

How can LSZ formalism deal with "glancing blows"?

My recent answer to the question Scattering, Perturbation and asymptotic states in LSZ reduction formula got me thinking again about wave packets and the LSZ reduction formula. In my answer, I claim ...
user1379857's user avatar
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