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Semi-reflecting mirror: classical optics approach

In this blog post, I explore the classical optics model of a light beam interacting with a semi-reflecting mirror. This analysis focuses on the mathematical relationships that govern the behavior of light as it splits into transmitted and reflected components at the interface of a semi-reflecting mirror.

Introduction

When a light beam encounters a semi-reflecting mirror, it divides into two paths: one that transmits through the mirror and another that reflects off it. This phenomenon is central to many optical devices and experiments, including those in quantum optics and laser systems.

Theoretical framework

The setup involves two orthogonal input beams directed towards the mirror at the origin. Beam (1) travels horizontally from left to right, and beam (2) travels vertically downward. At the interface, beam (1) is partially transmitted as beam (4) and partially reflected as beam (3). Similarly, beam (2) is partially transmitted as beam (3) and partially reflected as beam (4). This can be expressed by the equations:

\begin{aligned} E_3^{(+)} & = r E_1^{(+)} + t E_2^{(+)} \\ E_4^{(+)} & = t E_1^{(+)} - r E_2^{(+)} \end{aligned}

Here, r represents the reflection coefficient, and t represents the transmission coefficient, both of which are complex amplitudes. The minus sign associated with the reflection of beam (2) is crucial for ensuring the conservation of energy.

Energy Conservation

For the beam splitter to be considered lossless, the sum of the intensities of the output beams must equal the intensities of the input beams. This is expressed as:

r^2 + t^2 = 1

This condition ensures that the total power in the beams is conserved after interaction with the mirror.

Matrix Representation

The transformation of the input beams into the output beams can be neatly represented using a matrix form:

\begin{bmatrix} E_3^{(+)} \\ E_4^{(+)} \end{bmatrix} = \begin{bmatrix} r & t \\ t & -r \end{bmatrix} \begin{bmatrix} E_1^{(+)} \\ E_2^{(+)} \end{bmatrix}

This matrix, \mathbf{S}, is unitary, which implies that it preserves the norm of the vector it acts upon, a necessary condition for energy conservation.

Practical implications

The analysis of the semi-reflecting mirror using classical optics principles is more than a theoretical exercise. It has practical implications in designing optical circuits where light paths need to be controlled and manipulated precisely. Understanding the mathematical underpinnings helps in predicting the behavior of light in complex setups, essential for advancements in optical computing and quantum communication.

Conclusion

Through a detailed exploration of classical optics, I’ve highlighted the principles that govern light interactions with semi-reflecting mirrors. The use of matrix representation provides a clear and concise method to visualize and calculate the behavior of light in such scenarios.

For more insights into this topic, you can find the details here.