Quantum Mechanics And Classical Field Theory

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\large Relativity is the theory of particles moving with speeds comparable to the speed of light $v \sim c$ ($c$ is speed of light). Quantum mechanics is the theory describing the motion of microscopic particles. If we want to explain the behavior of microscopic particles moving with very high velocities (or high energies comparable to their rest mass energy) we need a theory which encapsulates both; the principles of relativity and quantum mechanics. So we need a quantum mechanical theory consistent with relativity. \par

\section{Why Quantum field Theory}
$\bullet$ Quantization of single relativistic particles leads to unphysical situations like negative energy states and negative probability density.
\\ $ \bullet $ Causality is not preserved in non-relativistic quantum mechanics, but as we know from the special relativity that for any theory …show more content…

This can be explained by saying that there is a proton field pervading throughout the whole universe and protons are quanta of this field.
\section{Elements of Classical Field Theory}
Classical Field theory deals with systems having infinitely large degrees of freedom. In case of infinite degrees of freedom the dynamical variables are no longer position and momentum of individual particles,the dynamical quantity is field, position and momentum become labels. For example we can think about a system having infinite number of springs coupled to each other then to describe the system, we use the vibration amplitude of those springs as a dynamical variable $\phi (x)$.\par
\subsection{Lagrangian Formalism}
In classical mechanics, we define action as time integral of Lagrangian. In field theory Lagrangian $L$ can be written as volume integral of Lagrangian density $\mathcal{L}$. Where $\mathcal{L}$ is a function of field ($\phi(x)$) and it's derivative ($\partial_{\mu}

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