# Ray transfer matrix analysis

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Ray transfer matrix analysis (also known as ABCD matrix analysis) is a type of ray tracing technique used in the design of some optical systems, particularly lasers. It involves the construction of a ray transfer matrix which describes the optical system; tracing of a light path through the system can then be performed by multiplying this matrix with a vector representing the light ray. The same analysis is also used in accelerator physics to track particles through the magnet installations of a particle accelerator, see Beam optics.

The technique that is described below uses the paraxial approximation of ray optics, which means that all rays are assumed to be at a small angle (θ in radians) and a small distance (x) relative to the optical axis of the system.[1]

## Definition of the ray transfer matrix

In ray transfer (ABCD) matrix analysis, an optical element (here, a thick lens) gives a transformation between ${\displaystyle (x_{1},\theta _{1})}$ at the input plane and ${\displaystyle (x_{2},\theta _{2})}$ when the ray arrives at the output plane.

The ray tracing technique is based on two reference planes, called the input and output planes, each perpendicular to the optical axis of the system. Without loss of generality, we will define the optical axis so that it coincides with the z-axis of a fixed coordinate system. A light ray enters the system when the ray crosses the input plane at a distance x1 from the optical axis while traveling in a direction that makes an angle θ1 with the optical axis. Some distance further along, the ray crosses the output plane, this time at a distance x2 from the optical axis and making an angle θ2. n1 and n2 are the indices of refraction of the medium in the input and output plane, respectively.

These quantities are related by the expression

${\displaystyle {x_{2} \choose \theta _{2}}={\begin{pmatrix}A&B\\C&D\end{pmatrix}}{x_{1} \choose \theta _{1}},}$

where

${\displaystyle A={x_{2} \over x_{1}}{\bigg |}_{\theta _{1}=0}\qquad B={x_{2} \over \theta _{1}}{\bigg |}_{x_{1}=0},}$

and

${\displaystyle C={\theta _{2} \over x_{1}}{\bigg |}_{\theta _{1}=0}\qquad D={\theta _{2} \over \theta _{1}}{\bigg |}_{x_{1}=0}.}$

This relates the ray vectors at the input and output planes by the ray transfer matrix (RTM) M, which represents the optical system between the two reference planes. A thermodynamics argument based on the blackbody radiation can be used to show that the determinant of a RTM is the ratio of the indices of refraction:

${\displaystyle \det(\mathbf {M} )=AD-BC={n_{1} \over n_{2}}.}$

As a result, if the input and output planes are located within the same medium, or within two different media which happen to have identical indices of refraction, then the determinant of M is simply equal to 1.

Note that at least one source[2] uses a different convention for the ray vectors. The optical direction cosine, n sin θ, is used instead of θ. This would alter some of the ABCD matrices, especially for refraction.

A similar technique can be used to analyze electrical circuits. See Two-port networks.

## Some examples

• For example, if there is free space between the two planes, the ray transfer matrix is given by:
${\displaystyle \mathbf {S} ={\begin{pmatrix}1&d\\0&1\end{pmatrix}}}$,

where d is the separation distance (measured along the optical axis) between the two reference planes. The ray transfer equation thus becomes:

${\displaystyle {x_{2} \choose \theta _{2}}=\mathbf {S} {x_{1} \choose \theta _{1}}}$,

and this relates the parameters of the two rays as:

${\displaystyle {\begin{matrix}x_{2}&=&x_{1}+d\theta _{1}\\\theta _{2}&=&\theta _{1}\end{matrix}}}$
• Another simple example is that of a thin lens. Its RTM is given by:
${\displaystyle \mathbf {L} ={\begin{pmatrix}1&0\\{\frac {-1}{f}}&1\end{pmatrix}}}$,

where f is the focal length of the lens. To describe combinations of optical components, ray transfer matrices may be multiplied together to obtain an overall RTM for the compound optical system. For the example of free space of length d followed by a lens of focal length f:

${\displaystyle \mathbf {L} \mathbf {S} ={\begin{pmatrix}1&0\\{\frac {-1}{f}}&1\end{pmatrix}}{\begin{pmatrix}1&d\\0&1\end{pmatrix}}={\begin{pmatrix}1&d\\{\frac {-1}{f}}&1-{\frac {d}{f}}\end{pmatrix}}}$.

Note that, since the multiplication of matrices is non-commutative, this is not the same RTM as that for a lens followed by free space:

${\displaystyle \mathbf {SL} ={\begin{pmatrix}1&d\\0&1\end{pmatrix}}{\begin{pmatrix}1&0\\{\frac {-1}{f}}&1\end{pmatrix}}={\begin{pmatrix}1-{\frac {d}{f}}&d\\{\frac {-1}{f}}&1\end{pmatrix}}}$.

Thus the matrices must be ordered appropriately, with the last matrix premultiplying the second last, and so on until the first matrix is premultiplied by the second. Other matrices can be constructed to represent interfaces with media of different refractive indices, reflection from mirrors, etc.

## Table of ray transfer matrices

for simple optical components

Element Matrix Remarks
Propagation in free space or in a medium of constant refractive index ${\displaystyle {\begin{pmatrix}1&d\\0&1\end{pmatrix}}}$ d = distance
Refraction at a flat interface ${\displaystyle {\begin{pmatrix}1&0\\0&{\frac {n_{1}}{n_{2}}}\end{pmatrix}}}$ n1 = initial refractive index

n2 = final refractive index.

Refraction at a curved interface ${\displaystyle {\begin{pmatrix}1&0\\{\frac {n_{1}-n_{2}}{R\cdot n_{2}}}&{\frac {n_{1}}{n_{2}}}\end{pmatrix}}}$ R = radius of curvature, R > 0 for convex (centre of curvature after interface)

n1 = initial refractive index
n2 = final refractive index.

Reflection from a flat mirror ${\displaystyle {\begin{pmatrix}1&0\\0&1\end{pmatrix}}}$ Only valid for mirrors perpendicular to the ray.
Reflection from a curved mirror ${\displaystyle {\begin{pmatrix}1&0\\-{\frac {2}{R_{e}}}&1\end{pmatrix}}}$ ${\displaystyle R_{e}=R\cos \theta }$ effective radius of curvature in tangential plane (horizontal direction)

${\displaystyle R_{e}=R/\cos \theta }$ effective radius of curvature in the sagittal plane (vertical direction)
R = radius of curvature, R > 0 for concave, valid in the paraxial approximation
${\displaystyle \theta }$ is the mirror angle of incidence in the horizontal plane.

Thin lens ${\displaystyle {\begin{pmatrix}1&0\\-{\frac {1}{f}}&1\end{pmatrix}}}$ f = focal length of lens where f > 0 for convex/positive (converging) lens.

Only valid if the focal length is much greater than the thickness of the lens.

Thick lens ${\displaystyle {\begin{pmatrix}1&0\\{\frac {n_{2}-n_{1}}{R_{2}n_{1}}}&{\frac {n_{2}}{n_{1}}}\end{pmatrix}}{\begin{pmatrix}1&t\\0&1\end{pmatrix}}{\begin{pmatrix}1&0\\{\frac {n_{1}-n_{2}}{R_{1}n_{2}}}&{\frac {n_{1}}{n_{2}}}\end{pmatrix}}}$ n1 = refractive index outside of the lens.

n2 = refractive index of the lens itself (inside the lens).
R1 = Radius of curvature of First surface.
R2 = Radius of curvature of Second surface.
t = center thickness of lens.

Single right angle prism ${\displaystyle {\begin{pmatrix}k&{\frac {d}{nk}}\\0&{\frac {1}{k}}\end{pmatrix}}}$ k = (cos${\displaystyle \psi }$/cos${\displaystyle \phi }$) is the beam expansion factor, where ${\displaystyle \phi }$ is the angle of incidence, ${\displaystyle \psi }$ is the angle of refraction, d = prism path length, n = refractive index of the prism material. This matrix applies for orthogonal beam exit.[3]
Multiple prism expander made of r right angle prisms ${\displaystyle {\begin{pmatrix}M&B\\0&{\frac {1}{M}}\end{pmatrix}}}$ M is the total beam magnification given by ${\displaystyle M=k_{1}k_{2}k_{3}...k_{r}}$, where k is defined in the previous entry and B is the total optical propagation distance of the multiple prism expander.[3]

## Resonator stability

RTM analysis is particularly useful when modeling the behaviour of light in optical resonators, such as those used in lasers. At its simplest, an optical resonator consists of two identical facing mirrors of 100% reflectivity and radius of curvature R, separated by some distance d. For the purposes of ray tracing, this is equivalent to a series of identical thin lenses of focal length f=R/2, each separated from the next by length d. This construction is known as a lens equivalent duct or lens equivalent waveguide. The RTM of each section of the waveguide is, as above,

${\displaystyle \mathbf {M} =\mathbf {L} \mathbf {S} ={\begin{pmatrix}1&d\\{\frac {-1}{f}}&1-{\frac {d}{f}}\end{pmatrix}}}$.

RTM analysis can now be used to determine the stability of the waveguide (and equivalently, the resonator). That is, it can be determined under what conditions light travelling down the waveguide will be periodically refocussed and stay within the waveguide. To do so, we can find all the "eigenrays" of the system: the input ray vector at each of the mentioned sections of the waveguide times a real or complex factor λ is equal to the output one. This gives:

${\displaystyle \mathbf {M} {x_{1} \choose \theta _{1}}={x_{2} \choose \theta _{2}}=\lambda {x_{1} \choose \theta _{1}}}$.

which is an eigenvalue equation:

${\displaystyle \left[\mathbf {M} -\lambda \mathbf {I} \right]{x_{1} \choose \theta _{1}}=0}$,

where I is the 2x2 identity matrix.

We proceed to calculate the eigenvalues of the transfer matrix:

${\displaystyle \operatorname {det} \left[\mathbf {M} -\lambda \mathbf {I} \right]=0}$,

${\displaystyle \lambda ^{2}-\operatorname {tr} (\mathbf {M} )\lambda +\operatorname {det} (\mathbf {M} )=0}$,

where

${\displaystyle \operatorname {tr} (\mathbf {M} )=A+D=2-{d \over f}}$

is the trace of the RTM, and

${\displaystyle \operatorname {det} (\mathbf {M} )=AD-BC=1}$

is the determinant of the RTM. After one common substitution we have:

${\displaystyle \lambda ^{2}-2g\lambda +1=0}$,

where

${\displaystyle g\ {\stackrel {\mathrm {def} }{=}}\ {\operatorname {tr} (\mathbf {M} ) \over 2}=1-{d \over 2f}}$

is the stability parameter. The eigenvalues are the solutions of the characteristic equation. From the quadratic formula we find

${\displaystyle \lambda _{\pm }=g\pm {\sqrt {g^{2}-1}}\,}$

Now, consider a ray after N passes through the system:

${\displaystyle {x_{N} \choose \theta _{N}}=\lambda ^{N}{x_{1} \choose \theta _{1}}}$.

If the waveguide is stable, no ray should stray arbitrarily far from the main axis, that is, λN must not grow without limit. Suppose ${\displaystyle g^{2}>1}$. Then both eigenvalues are real. Since ${\displaystyle \lambda _{+}\lambda _{-}=1}$, one of them has to be bigger than 1 (in absolute value), which implies that the ray which corresponds to this eigenvector would not converge. Therefore, in a stable waveguide, ${\displaystyle g^{2}}$ ≤ 1, and the eigenvalues can be represented by complex numbers:

${\displaystyle \lambda _{\pm }=g\pm i{\sqrt {1-g^{2}}}=\cos(\phi )\pm i\sin(\phi )=e^{\pm i\phi }}$,

with the substitution g = cos(ϕ).

For ${\displaystyle g^{2}<1}$ let ${\displaystyle r_{+}}$ and ${\displaystyle r_{-}}$ be the eigenvectors with respect to the eigenvalues ${\displaystyle \lambda _{+}}$ and ${\displaystyle \lambda _{-}}$ respectively, which span all the vector space because they are orthogonal, the latter due to ${\displaystyle \lambda _{+}}$${\displaystyle \lambda _{-}}$. The input vector can therefore be written as

${\displaystyle c_{+}r_{+}+c_{-}r_{-}}$,

for some constants ${\displaystyle c_{+}}$ and ${\displaystyle c_{-}}$.

After N waveguide sectors, the output reads

${\displaystyle \mathbf {M} ^{N}(c_{+}r_{+}+c_{-}r_{-})=\lambda _{+}^{N}c_{+}r_{+}+\lambda _{-}^{N}c_{-}r_{-}=e^{iN\phi }c_{+}r_{+}+e^{-iN\phi }c_{-}r_{-}}$,

which represents a periodic function.

## Ray transfer matrices for Gaussian beams

The matrix formalism is also useful to describe Gaussian beams.[4] If we have a Gaussian beam of wavelength ${\displaystyle \lambda _{0}}$, radius of curvature R (positive for diverging, negative for converging), beam spot size w and refractive index n, it is possible to define a complex beam parameter q by:[5]

${\displaystyle {\frac {1}{q}}={\frac {1}{R}}-{\frac {i\lambda _{0}}{\pi nw^{2}}}}$.

(R, w, and q are functions of position.) If the beam axis is in the z direction, with waist at ${\displaystyle z_{0}}$ and Rayleigh range ${\displaystyle z_{R}}$, this can be equivalently written as[5]

${\displaystyle q=(z-z_{0})+iz_{R}}$.

This beam can be propagated through an optical system with a given ray transfer matrix by using the equation:

${\displaystyle {q_{2} \choose 1}=k{\begin{pmatrix}A&B\\C&D\end{pmatrix}}{q_{1} \choose 1}}$,

where k is a normalisation constant chosen to keep the second component of the ray vector equal to 1. Using matrix multiplication, this equation expands as

${\displaystyle q_{2}=k(Aq_{1}+B)\,}$

and

${\displaystyle 1=k(Cq_{1}+D)\,}$

Dividing the first equation by the second eliminates the normalisation constant:

${\displaystyle q_{2}={\frac {Aq_{1}+B}{Cq_{1}+D}}}$,

It is often convenient to express this last equation in reciprocal form:

${\displaystyle {1 \over q_{2}}={C+D/q_{1} \over A+B/q_{1}}.}$

### Example: Free space

Consider a beam traveling a distance d through free space, the ray transfer matrix is

${\displaystyle {\begin{bmatrix}A&B\\C&D\end{bmatrix}}={\begin{bmatrix}1&d\\0&1\end{bmatrix}}}$.

and so

${\displaystyle q_{2}={\frac {Aq_{1}+B}{Cq_{1}+D}}={\frac {q_{1}+d}{1}}=q_{1}+d}$

consistent with the expression above for ordinary Gaussian beam propagation, i.e. ${\displaystyle q=(z-z_{0})+iz_{R}}$. As the beam propagates, both the radius and waist change.

### Example: Thin lens

Consider a beam traveling through a thin lens with focal length f. The ray transfer matrix is

${\displaystyle {\begin{bmatrix}A&B\\C&D\end{bmatrix}}={\begin{bmatrix}1&0\\-1/f&1\end{bmatrix}}}$.

and so

${\displaystyle q_{2}={\frac {Aq_{1}+B}{Cq_{1}+D}}={\frac {q_{1}}{-{\frac {q_{1}}{f}}+1}}}$
${\displaystyle {\frac {1}{q_{2}}}={\frac {-{\frac {q_{1}}{f}}+1}{q_{1}}}={\frac {1}{q_{1}}}-{\frac {1}{f}}}$.

Only the real part of 1/q is affected: the reciprocal of the radius of curvature is reduced by 1/f, while the waist is the same on either side of the thin lens.

## Higher order matrices

Higher order matrices, that is 3X3, 4X4, and 6X6, are also used in optical analysis[6][7][8] In particular, 4X4 propagation matrices are used in the design and analysis of prism sequences for pulse compression in femtosecond lasers.[3]

## References

1. ^ An exact method for tracing meridional rays is available here.
2. ^ Gerrard, Anthony; Burch, James M. (1994). Introduction to matrix methods in optics. Courier Dover. ISBN 9780486680446.
3. ^ a b c F. J. Duarte (2003). Tunable Laser Optics. New York: Elsevier-Academic. Chapter 6.
4. ^ Rashidian vaziri, M R. "New ducting model for analyzing the Gaussian beam propagation in nonlinear Kerr media and its application to spatial self-phase modulations". Journal of Optics. 15 (3). Bibcode:2013JOpt...15c5202R. doi:10.1088/2040-8978/15/3/035202.
5. ^ a b C. Tim Lei. "Physics 4510 Optics webpage". especially Chapter 5
6. ^ W. Brouwer, Matrix Methods in Optical Design (Benjamin, New York, 1964).
7. ^ A. E. Siegman, Lasers (University Science Books, Mill Valley, 1986).
8. ^ H. Wollnik, Optics of Charged Particles (Academic, New York, 1987).