ABCD Matrixes

are used in **paraxial ** optical design.

The angles are measured

**in radians**!

A beam is described by a distance r from the optical axis and a offset angle from the optical axis

An ABCD Matrix that describes the optical element is formed

The ABCD Matrix is multiplied by the input vector

The result is an output vector that describes the output beam with a new distance from the optical axis and a new angle off the optical axis

is a short for for the equation system

with

with

**Examples of ABCD matrices for simple optical elements :**

**Propagation in free space or in a medium of constant refractive index :**

Where d = reduced distance= thickness / refraction index

**Propagation through a series i=1..k of planparallel media with constant refraction indices :**

Where d_i = reduced distance_i= thickness_i / refraction index_i

**Refraction at a flat surface:**

Where:

= initial refractive index

= final refractive index

**Refraction at a curved surface:**

Where:

R = radius of curvature, for a convex surface (centre of curvature after interface)

= initial refractive index

= final refractive index

**Reflection vrom a flat mirror:**

Identity matrix

**Reflection from a curved mirror:**

Where:

effective radius of curvature in tangential plane (horizontal direction)

effective radius of curvature in the sagittal plane (vertical direction)

With for convex mirrors (centre of curvature after interface)

**Refraction at a thin lens**

Where:

f = focal length of the lens, where for convex/positive/converging lenses. Valid if if and only if the focal length is much bigger than the thickness of the lens

**Refraction at a thick lens**

Where:

= refractive index outside of the lens.

= refractive index of the lens itself (inside the lens).

= Radius of curvature of First surface.

= Radius of curvature of Second surface.

t = center thickness of lens.