chp 27 gassian laser beam.pdf
TRANSCRIPT
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ME 587 Engineering Optics, Prof. X. Xu, School of Mechanical Engineering, Purdue University
Propagation of a Gaussian Laser Beam
2 22
2 2
n EEc t
Gaussian beam propagation is a complicated 3-D problem
1-D wave equation:2 2 2
2 2 2
E n Ez c t
3-D wave equation:
A plane wave: ( )0( , )i k r tE E r t E e
A spherical wave: 0 ( ),( , , , ) i k r tEE r t er
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ME 587 Engineering Optics, Prof. X. Xu, School of Mechanical Engineering, Purdue University
Paraxial approximations of laser beam propagation: EM wave propagation is close to the optical axis
Examine wave propagation close to the z-direction
x
y
z
rR
2 2 2 2( )r R x y 2 2
2 1/ 22
( )[ (1 )]x yr RR
If the laser beam is close to the z axis,
2 2 2x y R 2 2 2 2
2 1/ 22 2
( ) ( )[ (1 )] ~ (1 )2
x y x yr R RR R
2 2
2x yikikr ikR Re e e
Will be discussed later.
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ME 587 Engineering Optics, Prof. X. Xu, School of Mechanical Engineering, Purdue University
( ), , , ( , , ) i kz tE x y z t U x y z e
Let 2
2 22tEE E
z
2t : Laplacian operator in the transverse plane (x,y), or (r,).
Gaussian Laser Beam Solution
2 22
2 2( , , , )n EE x y z tc t
Need to solve:
Look for a solution in the form of:
Spherical wave like Plane wave like
2 2 ( ) 2 ( )[ ]i kz t i kz tt t tE Ue U e
2( ) ( )
2i kz t i kz tE U e ikUe
z zz
22 ( )
2( )i kz tU U Uik k U ik e
z z z
22 ( )
22i kz tU Uk U i k e
z z
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ME 587 Engineering Optics, Prof. X. Xu, School of Mechanical Engineering, Purdue University
22
2
E Et
2 2 2 2 22 ( )
2 2 2 22 0i kz tU U U U ni k k U U e
zx y z c
Combining all the terms:
=0
2
2 2U Ui k
zz
Assume:
2 2
2 2 2 0U U Ui k
zx y
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ME 587 Engineering Optics, Prof. X. Xu, School of Mechanical Engineering, Purdue University
Now write the equation in the cylindrical coordinate system:
2
2 2
1 1 2 0U U Ur ikr r r r z
Due to cylindrical symmetry, 0
1 2 0U Ur ikr r r z
Assume a trial solution: (Look for simplest solution, the so-called TEMoo mode)
2
0 exp exp 2ikrU E iP zq z
Longitudinal radialphase amplitude distribution
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ME 587 Engineering Optics, Prof. X. Xu, School of Mechanical Engineering, Purdue University
20 exp exp 2U ikr ikrE iPr q q
20 2exp exp 2U ikr ikrr E iP
r r q q
2 2
0 exp exp 2ikr ikr ikrE iP
q q q
2 22 20 01 22. . . exp exp exp exp2 2ikE k r Eikr ikrL H S iP iPq q q q
2. . . 2UL H S ikz
2 2 222 'exp exp exp exp2 2 2
ikr ikr ikrik iP iP iP qq q q
Insert into
is derivative with respect to z
2
0 exp exp 2ikrU E iP zq z
1 2 0U Ur ikr r r z
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ME 587 Engineering Optics, Prof. X. Xu, School of Mechanical Engineering, Purdue University
Cancel all exp (iP) and exp(ikr2/2q) we obtain:
2 2 2 2
2 2
2 2 0ik k r k rkP qq q q
1 oq q = q z
iPq
Guess a simplest solution:
2 22
2 2
2( 2 ) ( ) 0ik k kkP q rq q q
and
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ME 587 Engineering Optics, Prof. X. Xu, School of Mechanical Engineering, Purdue University
Choose z = 0 at the focal point, or waist of a beam
z=0
2
0 exp( )exp 2ikrU E iP
q
The second term needs to be real at z = 0, meaning all rays are in plane at z = 0, therefore qo is imaginary.
R z a numbero Rq iz is real
Since
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ME 587 Engineering Optics, Prof. X. Xu, School of Mechanical Engineering, Purdue University
Define: R, as: 22 2 1R Rz z zR z z
z z
which is Real
22 2 2 22 1RRR R
z zz z zkz k z
which is also Real
2 2
0 2exp exp exp 2r ikrE iP
R zz
The second term on the RHS indicates a Gaussian function,
2 2 2 2 2
1 1 1RR R R
zz i iq z iz Rz z z z
From
2
0 exp( )exp 2ikrU E iP
q
q = z -i zR
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ME 587 Engineering Optics, Prof. X. Xu, School of Mechanical Engineering, Purdue University
at z = 0, is minimum (at the focal point), called o . 2
2 2 1Rk
z zk z
2 2 2
2R
22 z2 2o o oR
okz or
k
Physical meaning of ZR, more to be discussed later
From
(z) - the width of a laser beam , which changes with z
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ME 587 Engineering Optics, Prof. X. Xu, School of Mechanical Engineering, Purdue University
Now solve for P:
1 , - R R
i iP iPq z iz z iz
ln RiP z z iz C
1tan
exp Rzi
zoiP ez
2 2
0 2exp exp exp 2r ikrU E iP
z R z
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ME 587 Engineering Optics, Prof. X. Xu, School of Mechanical Engineering, Purdue University
Complete solution for TEMoo mode Gaussian laser beam:
( )i kz tE Ue
2 21
2exp exp tan exp 2i to
oR
r z krE i kz i ez z z R z
amplitude longitudinal radial phase
phase
21 RzR z zz
2 2
2o o
Rkz
22 222( ) 1 1
2
o
R
R R
z z zzk z z
1/ 2222
21 1o oR R
z zz z
(z) varies with z as:
Important relations:
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ME 587 Engineering Optics, Prof. X. Xu, School of Mechanical Engineering, Purdue University
For a wave propagating close to the z - axis
x
y
zrz
2 2r z2 2
2 1/ 22 2[ (1 )] ~ (1 )2
r rq z zz z
2
2rikikq ikz ze e e
Therefore for a wave near the z-direction, 2
2krkz
z
q
2 2 2q z r
is a constant
for
which can be considered as radius of curvature
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ME 587 Engineering Optics, Prof. X. Xu, School of Mechanical Engineering, Purdue University
2 2
12exp exp tan exp 2
i too
R
r z krE E i kz i ez z z R z
The phase term is 2
1tan2R
z krkzz R z
For z >> zR
The phase term ~ 2
2krkzR z
Compared to the previous discussion on radius of curvature
R(z) is the radius of curvature
z=0
R
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ME 587 Engineering Optics, Prof. X. Xu, School of Mechanical Engineering, Purdue University
If z >> zR,
oR o
z zz
full angle = 2/z = 2 0.636o o
far field divergence angle. z=0
Divergence is proportional to and 1/o.
2
( )oRz
Divergence of a Gaussian beam
1/ 22
1oR
zz
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ME 587 Engineering Optics, Prof. X. Xu, School of Mechanical Engineering, Purdue University
Focusing of a Gaussian beam using a lens
Far field divergence angle:
2 0.636o o
Far field divergence angle can also be approximated as 2/f2 2
o f 0
f
043
f
Practically, some corrections are needed:
Equation to find the radius at the focal point, 0 ~ f, ~ , ~ 1/
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ME 587 Engineering Optics, Prof. X. Xu, School of Mechanical Engineering, Purdue University
1/#2 . .
ffd N A
1/#2 2 . .ff
N A
Relation with f number (f/#) and numerical aperture (N.A.):
04
3 . .N A
Note: in order to obtain the smallest spot, one must expand the beam to fill the diameter of the lens (d) to achieve a smallest spot
043
f
When 2 = d,
Again, the beam should fill the lens (2 = d).
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ME 587 Engineering Optics, Prof. X. Xu, School of Mechanical Engineering, Purdue University
Depth of focus
z=0
1/ 22
0/ 1 1.05R
zzz
0.32
R
zz
200.32z
2 2
2o o
Rkz
Total depth of focus: 200.64 0.64 Rz Z
Let
1/ 22
1oR
zz
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ME 587 Engineering Optics, Prof. X. Xu, School of Mechanical Engineering, Purdue University
Often, ZR is used for characterizing the depth of focus, also called the Rayleigh range:
Z2o
R
At z = zR, = 1.4o
1/ 22
1oR
zz
Since
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ME 587 Engineering Optics, Prof. X. Xu, School of Mechanical Engineering, Purdue University
Power carried by a Gaussian beam:
212 oavg avg
S ExH c E
Total power P:2 *1
2 oavg o oP S c EE rdrd
2 2 22
2 2
1 2exp2
o oo o o
E rc rdrdz z
221
2 2o
o ocE f z Energy is conserved.
[W/m2]
2 2
12exp exp tan exp 2
i too
R
r z krE E i kz i ez z z R z
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ME 587 Engineering Optics, Prof. X. Xu, School of Mechanical Engineering, Purdue University
Beam intensity (per unit area [W/m2]) distribution (variation of power intensity with r):
2 2 2*
2 2
o
1 1 2( , ) exp2 2
z
o o oo
cE rI r z c EEz z
z
2 4 2 2
* o2 2 2
E1 1 2( , ) exp2 2
o oo
c rI r z c EEz z
Elliptically shaped beam:
Circular beam:2 2 2
2 2
2exp exp 2r x yE
Elliptical beam:2 2
2 2exp 2x y
x yE
- Gaussian distribution
(when z is large)
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ME 587 Engineering Optics, Prof. X. Xu, School of Mechanical Engineering, Purdue University
Knife-edge method for measuring the Gaussian beam radius or diameter
2 4 2 2
* o2 2 2
E1 1 2( , ) exp2 2
o oo
c rI r z c EEz z
2
0 2
2( ) exp rI r I
2 2
0 2
2( )( , ) exp x yI x y I x
2 2
0 2
2( )( ) expx
x yI x dx dyI
Scan direction
At a given z location:
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ME 587 Engineering Optics, Prof. X. Xu, School of Mechanical Engineering, Purdue University
Propagation of a Gaussian beam in optical systems (lens, free space, etc.)2 2
12exp exp tan exp 2
oo
R
r z krE E j kz jz R
2 2 2 2 2 22 o RR RR
z zz R z zz kz
q(z) = z - izR 21 1 i
q z R
With the knowledge of q, the Gaussian beam properties are completely determined, such as z, zR, o, and .
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ME 587 Engineering Optics, Prof. X. Xu, School of Mechanical Engineering, Purdue University
12
1
,Aq BqCq D
A, B, C, D are the same as in the transfer matrix in geometry optics
This is called the ABCD Law.
Let q1 and q2 are the values of q before and after an optical element, then
Use q to describe propagation of a Gaussian beam
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ME 587 Engineering Optics, Prof. X. Xu, School of Mechanical Engineering, Purdue University
Example:
For free space: B 1 dC D 0 1A
2 11
1q dq q d
o
compare with q(z) = z -izR.
Thin Lens: 1 01- 1f
12
2 11
0 1 1 1 1 q1
qqf qq
f