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<record version="6" id="180">
 <title>Dirac equation and notations</title>
 <name>DiracNotation</name>
 <created>2006-05-30 11:18:21</created>
 <modified>2009-01-30 15:50:05</modified>
 <type>Topic</type>
 <creator id="441" name="bci1"/>
 <modifier id="441" name="bci1"/>
 <comment>This is a contributed topic entry in progress.</comment>
 <author id="441" name="bci1"/>
 <author id="132" name="metalac"/>
 <classification>
	<category scheme="msc" code="03.65.Ta"/>
 </classification>
 <synonyms>
	<synonym concept="Dirac equation and notations" alias="bra-ket notation"/>
 </synonyms>
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 <content>\subsection{Introduction}

\subsection{Non-Abelian Observable (Clifford) Algebra}


\subsection{Dirac relativistic quantum field equations}



\subsection{Dirac delta and $&lt;bra&gt;c&lt;ket&gt;$ notations}

Dirac notations (or ``bra-ket'' notation as commonly known in physics) is used to represent quantum states in quantum mechanics.  It was invented by Paul Dirac and since then has been a prefered way of notation in quantum mechanics.

The notation denotes the ``ket'' vector defined as $|{\psi}&gt;$ and its transpose vector is defined as $&lt;{\phi}|$ or ``bra'' vector. Then ``bra-ket'' is defined as the inner product of the two which is noted as $&lt;{\phi}|{\psi}&gt;$. Dirac notation also satisifies following identities:

$&lt;{\phi}|{\omega}|{\psi}&gt;{\equiv}&lt;{\phi}|{\omega}{\psi}&gt;$\\
$&lt;{\phi}|{\psi}&gt;{\equiv}\int_{-{\infty}}^{\infty} \widetilde{\phi} {\psi} dx \quad$\\
Where $\widetilde{\phi}$ is complex conjugate of ${\phi}$.

\begin{thebibliography}{9}
\bibitem(PAMD68)
Paul A.M. Dirac. 1968. {\em Principles of Quantum Mechanics}, 
Cambridge University Press, Cambridge, UK
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