Conformal Field Theory: Evaluating the Vertex Operator on the Vacuum

If k is non-zero, then the limit will be the vacuum state |0\rangle. If k is zero, then the limit will be undefined. In summary, the limit of the vertex operator :e^{ik \cdot X(z)}: as z goes to zero will be the vacuum state |0\rangle if k is non-zero, and undefined if k is zero.
  • #1
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Homework Statement



Evaluate
[tex]\lim_{z \to 0}:e^{ik \cdot X(z)}:|0\rangle [/tex]
where [itex]X(z)[/itex] is a free chiral scalar field in the complex plane.

Homework Equations



In Conformal Field Theory, the free chiral scalar field in the complex plane is given by:
[tex]\begin{array}{rcl} X(z) &=& \frac{1}{2}q - ip\log{z}+i\sum_{n \neq 0}\frac{1}{n}\alpha_n z^{-n}\\
&=& \frac{1}{2}q-ip\log{z}+X_{<}(z)+X_{>}(z)\end{array}[/tex]

Where [itex]q,p[/itex] are position and momentum respectively, and [itex]\alpha_n[/itex] are oscillator modes with the following properties:
[tex][\alpha_m^\mu,\alpha_n^\nu]=m\eta^{\mu\nu}\delta_{m+n,0}[/tex]
[tex]\alpha_{-n} = \alpha_n^\dagger\ ,\ \alpha_n|0\rangle = 0\ ,\ n>0[/tex]

The (normal-ordered) Vertex operator is defined to be:
[tex]: e^{i k \cdot X(z)}: = e^{ik X_<(z)} e^{ik\cdot q} z^{k \cdot p} e^{ik \cdot X_>(z)}[/tex]

The Attempt at a Solution



So effectively we want to evaluate:

[tex]\lim_{z \to 0}e^{ik X_<(z)} e^{ik\cdot q} z^{k \cdot p} e^{ik \cdot X_>(z)}|0\rangle[/tex]

We know that since [itex] e^{ik \cdot X_>(z)}[/itex] consists of annihilation operators, [itex] e^{ik \cdot X_>(z)}|0\rangle = |0\rangle[/itex]

But what about the other terms? I have no idea how they act on the vacuum. Moreover, when we take the limit to zero, doesn't the whole thing go to zero because we have [itex]z[/itex] in the base of an exponent here?
 
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  • #2


First, let's simplify the expression a bit by using the definition of the vertex operator and the properties of the oscillator modes:

\begin{align*}
:e^{ik \cdot X(z)}:|0\rangle &= e^{ik X_<(z)} e^{ik\cdot q} z^{k \cdot p} e^{ik \cdot X_>(z)}|0\rangle \\
&= e^{ik X_<(z)} e^{ik\cdot q} z^{k \cdot p} |0\rangle \\
&= e^{ik X_<(z)} e^{ik\cdot q} |0\rangle \\
&= e^{ik X_<(z)} |0\rangle \\
&= \exp \left( \sum_{n>0} \frac{i}{n}\alpha_n z^{-n} \right) |0\rangle
\end{align*}

Now, we can see that the limit as z goes to zero will depend on the value of k. If k is non-zero, then the exponential term will go to 1, since all the terms in the sum will go to zero. However, if k is zero then the exponential term will be undefined.

So, in general, the limit will depend on the value of k.
 

Related to Conformal Field Theory: Evaluating the Vertex Operator on the Vacuum

What is conformal field theory?

Conformal field theory (CFT) is a branch of theoretical physics that studies the behavior of two-dimensional systems that exhibit conformal symmetry. This symmetry means that the system looks the same at all length scales, allowing for a better understanding of the underlying physical phenomena.

What is the role of the vertex operator in CFT?

The vertex operator is a mathematical tool used in CFT to describe the interactions between different fields in a conformally invariant system. It is used to calculate correlation functions, which provide information about the behavior of the system at different points.

What does it mean to evaluate the vertex operator on the vacuum in CFT?

Evaluating the vertex operator on the vacuum refers to the process of calculating the correlation functions for a conformally invariant system in its ground state. This allows for the determination of important physical quantities, such as the scaling dimensions of operators and the central charge of the system.

Why is evaluating the vertex operator on the vacuum important in CFT?

Evaluating the vertex operator on the vacuum is important because it allows for the characterization and classification of conformally invariant systems. It also provides a way to study the behavior of these systems at different length scales, leading to a better understanding of their underlying physical principles.

What are some applications of CFT and the evaluation of the vertex operator on the vacuum?

CFT and the evaluation of the vertex operator on the vacuum have applications in various areas of physics, including string theory, condensed matter physics, and statistical mechanics. They are also used in cosmology, where they help in understanding the behavior of the early universe and the nature of dark energy.

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