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Lagrangian optics and Hamiltonian optics are two formulations of geometrical optics which share much of the mathematical formalism with Lagrangian mechanics and Hamiltonian mechanics.
Contents
- Hamiltons principle
- Lagrangian and Hamiltonian optics
- Fermats principle
- The Euler Lagrange equations
- Optical momentum
- Hamiltons equations
- Applications
- Refraction and reflection
- Rays and wavefronts
- Phase space
- Conservation of etendue
- Imaging and nonimaging optics
- Generalizations
- General ray parametrization
- Generalized coordinates
- References
Hamilton's principle
In physics, Hamilton's principle states that the evolution of a system
where
with
The momentum is defined as
and the Euler-Lagrange equations can then be rewritten as
where
A different approach to solving this problem consists in defining a Hamiltonian (taking a Legendre transform of the Lagrangian) as
for which a new set of differential equations can be derived by looking at how the total differential of the Lagrangian depends on parameter σ, positions
with
Lagrangian and Hamiltonian optics
The general results presented above for Hamilton's principle can be applied to optics. In 3D euclidean space the generalized coordinates are now the coordinates of euclidean space.
Fermat's principle
Fermat's principle states that the optical length of the path followed by light between two fixed points, A and B, is a stationary point. It may be a maximum, a minimum, constant or an inflection point. In general, as light travels, it moves in a medium of variable refractive index which is a scalar field of position in space, that is,
In the context of calculus of variations this can be written as
where ds is an infinitesimal displacement along the ray given by
is the optical Lagrangian and
The optical path length (OPL) is defined as
where n is the local refractive index as a function of position along the path between points A and B.
The Euler-Lagrange equations
The general results presented above for Hamilton's principle can be applied to optics using the Lagrangian defined in Fermat's principle. The Euler-Lagrange equations with parameter σ =x3 and N=2 applied to Fermat's principle result in
with k=1,2 and where L is the optical Lagrangian and
Optical momentum
The optical momentum is defined as
and from the definition of the optical Lagrangian
or in vector form
where
where n is the refractive index at which p is calculated. Vector p points in the direction of propagation of light. If light is propagating in a gradient index optic the path of the light ray is curved and vector p is tangent to the light ray.
The expression for the optical path length can also be written as a function of the optical momentum. Having in consideration that
and the expression for the optical path length is
Hamilton's equations
Similarly to what happens in Hamiltonian mechanics, also in optics the Hamiltonian is defined by the expression given above for N=2 corresponding to functions
Comparing this expression with
And the corresponding Hamilton's equations with parameter σ =x3 and k=1,2 applied to optics are
with
Applications
It is assumed that light travels along the x3 axis, in Hamilton's principle above, coordinates
Refraction and reflection
If plane x1x2 separates two media of refractive index nA below and nB above it, the refractive index is given by a step function
and from Hamilton's equations
and therefore
An incoming light ray has momentum pA before refraction (below plane x1x2) and momentum pB after refraction (above plane x1x2). The light ray makes an angle θA with axis x3 (the normal to the refractive surface) before refraction and an angle θB with axis x3 after refraction. Since the p1 and p2 components of the momentum are constant, only p3 changes from p3A to p3B.
Figure "refraction" shows the geometry of this refraction from which
which is Snell's law of refraction.
In figure "refraction", the normal to the refractive surface points in the direction of axis x3, and also of vector
where i and r are a unit vectors in the directions of the incident and refracted rays. Also, the outgoing ray (in the direction of
A similar argument can be used for reflection in deriving the law of specular reflection, only now with nA=nB, resulting in θA=θB. Also, if i and r are unit vectors in the directions of the incident and refracted ray respectively, the corresponding normal to the surface is given by the same expression as for refraction, only with nA=nB
In vector form, if i is a unit vector pointing in the direction of the incident ray and n is the unit normal to the surface, the direction r of the refracted ray is given by:
with
If i·n<0 then -n should be used in the calculations. When
Rays and wavefronts
From the definition of optical path length
with k=1,2 where the Euler-Lagrange equations
combining the equations for the components of momentum p results in
Since p is a vector tangent to the light rays, surfaces S=Constant must be perpendicular to those light rays. These surfaces are called wavefronts. Figure "rays and wavefronts" illustrates this relationship. Also shown is optical momentum p, tangent to a light ray and perpendicular to the wavefront.
Vector field
and the optical path length S calculated along a curve C between points A and B is a function of only its end points A and B and not the shape of the curve between them. In particular, if the curve is closed, it starts and ends at the same point, or A=B so that
This result may be applied to a closed path ABCDA as in figure "optical path length"
for curve segment AB the optical momentum p is perpendicular to a displacement ds along curve AB, or
or
and the optical path length SBC between points B and C along the ray connecting them is the same as the optical path length SAD between points A and D along the ray connecting them. The optical path length is constant between wavefronts.
Phase space
Figure "2D phase space" shows at the top some light rays in a two-dimensional space. Here x2=0 and p2=0 so light travels on the plane x1x3 in directions of increasing x3 values. In this case
For example, ray rC crosses axis x1 at coordinate xB with an optical momentum pC, which has its tip on a circle of radius n centered at position xB. Coordinate xB and the horizontal coordinate p1C of momentum pC completely define ray rC as it crosses axis x1. This ray may then be defined by a point rC=(xB,p1C) in space x1p1 as shown at the bottom of the figure. Space x1p1 is called phase space and different light rays may be represented by different points in this space.
As such, ray rD shown at the top is represented by a point rD in phase space at the bottom. All rays crossing axis x1 at coordinate xB contained between rays rC and rD are represented by a vertical line connecting points rC and rD in phase space. Accordingly, all rays crossing axis x1 at coordinate xA contained between rays rA and rB are represented by a vertical line connecting points rA and rB in phase space. In general, all rays crossing axis x1 between xL and xR are represented by a volume R in phase space. The rays at the boundary ∂R of volume R are called edge rays. For example, at position xA of axis x1, rays rA and rB are the edge rays since all other rays are contained between these two.
In three-dimensional geometry the optical momentum is given by
Conservation of etendue
Figure "volume variation" shows a volume V bound by an area A. Over time, if the boundary A moves, the volume of V may vary. In particular, an infinitesimal area dA with outward pointing unit normal n moves with a velocity v.
This leads to a volume variation
The rightmost term is a volume integral over the volume V and the middle term is the surface integral over the boundary A of the volume V. Also, v is the velocity with which the points in V are moving.
In optics coordinate
and using Hamilton's equations
or
The volume occupied by a set of rays in phase space is called etendue, which is conserved as light rays progress in the optical system along direction x3. This corresponds to Liouville's theorem, which also applies to Hamiltonian mechanics.
However, the meaning of Liouville’s theorem in mechanics is rather different from the theorem of conservation of étendue. Liouville’s theorem is essentially statistical in nature, and it refers to the evolution in time of an ensemble of mechanical systems of identical properties but with different initial conditions. Each system is represented by a single point in phase space, and the theorem states that the average density of points in phase space is constant in time. An example would be the molecules of a perfect classical gas in equilibrium in a container. Each point in phase space, which in this example has 2N dimensions, where N is the number of molecules, represents one of an ensemble of identical containers, an ensemble large enough to permit taking a statistical average of the density of representative points. Liouville’s theorem states that if all the containers remain in equilibrium, the average density of points remains constant.
Imaging and nonimaging optics
Figure "conservation of etendue" shows on the left a diagrammatic two-dimensional optical system in which x2=0 and p2=0 so light travels on the plane x1x3 in directions of increasing x3 values.
Light rays crossing the input aperture of the optic at point x1=xI are contained between edge rays rA and rB represented by a vertical line between points rA and rB at the phase space of the input aperture (right, bottom corner of the figure). All rays crossing the input aperture are represented in phase space by a region RI.
Also, light rays crossing the output aperture of the optic at point x1=xO are contained between edge rays rA and rB represented by a vertical line between points rA and rB at the phase space of the output aperture (right, top corner of the figure). All rays crossing the output aperture are represented in phase space by a region RO.
Conservation of etendue in the optical system means that the volume (or area in this two-dimensional case) in phase space occupied by RI at the input aperture must be the same as the volume in phase space occupied by RO at the output aperture.
In imaging optics, all light rays crossing the input aperture at x1=xI are redirected by it towards the output aperture at x1=xO where xI=m xO. This ensures that an image of the input of formed at the output with a magnification m. In phase space, this means that vertical lines in the phase space at the input are transformed into vertical lines at the output. That would be the case of vertical line rA rB in RI transformed to vertical line rA rB in RO.
In nonimaging optics, the goal is not to form an image but simply to transfer all light from the input aperture to the output aperture. This is accomplished by transforming the edge rays ∂RI of RI to edge rays ∂RO of RO. This is known as the edge ray principle.
Generalizations
Above it was assumed that light travels along the x3 axis, in Hamilton's principle above, coordinates
General ray parametrization
A more general situation can be considered in which the path of a light ray is parametrized as
where now
with k=1,2,3 and where L is the optical Lagrangian. Also in this case the optical momentum is defined as
and the Hamiltonian P is defined by the expression given above for N=3 corresponding to functions
And the corresponding Hamilton's equations with k=1,2,3 applied optics are
with
The optical Lagrangian is given by
and does not explicitly depend on parameter σ. For that reason not all solutions of the Euler-Lagrange equations will be possible light rays, since their derivation assumed an explicit dependence of L on σ which does not happen in optics.
The optical momentum components can be obtained from
where
Comparing this expression for L with that for the Hamiltonian P it can be concluded that
From the expressions for the components
The optical Hamiltonian is chosen as
although other choices could be made. The Hamilton's equations with k=1,2,3 defined above together with
Generalized coordinates
As in Hamiltonian mechanics, it is also possible to write the equations of Hamiltonian optics in terms of generalized coordinates
where the optical momentum is given by
and