Lectures on Quantum Optics and Quantum Information
Lectures on Quantum Optics and Quantum Information
Lectures on Quantum Optics and Quantum Information
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Quantizati<strong>on</strong> of the Electromagnetic Field<br />
• For each wave vector:<br />
This equati<strong>on</strong> is similar to the <strong>on</strong>e describing the evoluti<strong>on</strong> of a<br />
harm<strong>on</strong>ic oscillator with frequency , which can be described<br />
by a vector a, functi<strong>on</strong> of p (positi<strong>on</strong>) <strong>and</strong> q (momentum).<br />
• By analogy, we introduce an operator a<br />
<strong>and</strong> define a field operator :<br />
We can also define the quadrature operators:<br />
Where <strong>and</strong> can be identified to<br />
the creati<strong>on</strong> <strong>and</strong> annihilati<strong>on</strong> operators for<br />
harm<strong>on</strong>ic oscillators<br />
• By c<strong>on</strong>sidering Fourier-limited wavepackets, it can be shown finally for <strong>on</strong>e mode<br />
(<strong>on</strong>e dimensi<strong>on</strong> quantized harm<strong>on</strong>ic oscillator) :<br />
Total number<br />
of phot<strong>on</strong>s