About the action S in quantum field theory

In summary, the question is whether the action constructed by H+dS/dt can be used to solve the quantization problem of non-renormalizable theories. However, non-renormalizability is no longer seen as a problem as theories with infinite terms can be allowed as long as their contribution is suppressed at higher energies.
  • #1
eljose79
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Let,s suppose we have a Hamiltonian H so we can construct the action by H+dS/dt then why no use the action to solve the problem of quantization of non renormalizable theories?..
 
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  • #2
I think you probably meant ∂S/∂t + H = 0. In any event, nonrenormalizability is no longer viewed as a problem. A theory is renormalizable if it's lagrangian need only contain a finite number of terms to absorb the different types of divergences that occur in it's perturbation theory. But now we know that it's perfectly alright to allow theories which require an infinite number of terms as long as their contribution to the theory are suppressed at higher energies.
 
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  • #3


The action S in quantum field theory is a mathematical quantity that describes the dynamics of a system. It is defined as the integral of the Lagrangian over all space and time. In this context, it is often used to derive the equations of motion for a system and to study its symmetries.

In the case of non-renormalizable theories, the problem of quantization arises because these theories have divergences in their calculations, making it difficult to obtain meaningful results. The use of the action to solve this problem is not straightforward, as it involves taking derivatives of the action with respect to time, which can lead to further divergences.

Furthermore, the action itself is not a physical observable, and therefore cannot be directly used to solve the problem of quantization. It is a mathematical tool that helps us understand the dynamics of a system, but it is not a substitute for physical measurements.

Instead, other techniques such as renormalization have been developed to deal with the problem of non-renormalizable theories. These techniques involve making adjustments to the theory in order to remove the divergences and obtain meaningful results.

In summary, while the action is a useful concept in quantum field theory, it is not a direct solution to the problem of quantization in non-renormalizable theories. Other approaches and techniques are needed to address this issue.
 

1. What is the action S in quantum field theory?

The action S in quantum field theory is a mathematical expression that describes the dynamics of a quantum field. It is a functional of the field variables and their derivatives, and is used to calculate the probabilities of different particle interactions.

2. How is the action S related to the Lagrangian in quantum field theory?

The action S is related to the Lagrangian through the principle of least action. The Lagrangian is the difference between the kinetic and potential energies of a system, and it is used to calculate the equations of motion. The action is then defined as the integral of the Lagrangian over time, and the system will follow the path of least action in order to minimize the action.

3. What is the significance of the action S in quantum field theory?

The action S is a fundamental concept in quantum field theory, as it allows us to calculate the amplitudes and probabilities of particle interactions. It is also used to derive the equations of motion for the fields, and plays a crucial role in understanding the dynamics of quantum fields.

4. How is the action S calculated in quantum field theory?

The action S is calculated by first determining the Lagrangian for the system, which involves identifying the relevant fields and their interactions. The Lagrangian is then integrated over time to obtain the action. This calculation involves complex mathematical techniques and can be challenging, but it is essential for understanding the behavior of quantum fields.

5. Can the action S be modified or changed in quantum field theory?

Yes, the action S can be modified or changed in certain situations. For example, in the presence of external fields or in different spacetime geometries, the action may need to be modified in order to accurately describe the dynamics of the system. Additionally, in certain theories beyond the standard model, such as supersymmetry, the action may be more complex and require additional terms to account for new particles and interactions.

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