# Minggu 07 - Lasers by fanzhongqing

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```									 Lasers*

Stimulated Emission
Fast decay
Gain

Inversion
Pump           Laser
The Laser                      Transition        Transition

Four-level System

Threshold

Some lasers                                     Fast decay

* Light Amplification by Stimulated Emission of Radiation
Stimulated emission leads to a chain
reaction and laser emission.
If a medium has many excited molecules, one photon can become
many.
Excited medium

This is the essence of the laser. The factor by which an input beam is
amplified by a medium is called the gain and is represented by G.
The Laser
A laser is a medium that stores energy, surrounded by two mirrors.
A partially reflecting output mirror lets some light out.

I0                                          I1

I3             Laser medium                I2
R = 100%                    with gain, G                    R < 100%

A laser will lase if the beam increases in intensity during a round trip:
that is, if I 3  I 0

Usually, additional losses in intensity occur, such as absorption, scat-
tering, and reflections. In general, the laser will lase if, in a round trip:

Gain > Loss                This called achieving Threshold.
2
Calculating the gain:
Einstein A and B coefficients                               1

In 1916, Einstein considered the various transition rates between
molecular states (say, 1 and 2) involving light of irradiance, I:

Absorption rate = B N1 I

Spontaneous emission rate = A N2

Stimulated emission rate = B N2 I

where Ni is the number density of molecules in the ith state,
Laser medium
Laser gain                                           I(0)                        I(L)
Neglecting spontaneous emission:                                                  z
0            L
dI     dI
 c     BN 2 I - BN1I            [Stimulated emission minus absorption]
dt     dz
 B  N 2 - N1  I
Proportionality constant is the
The solution is:
absorption/gain cross-section, 

I ( z )  I (0) exp   N2  N1  z

There can be exponential gain or loss in irradiance.
Normally, N2 < N1, and there is loss (absorption).
But if N2 > N1, there’s gain, and we define the gain, G:

If N2 > N1:        g   N2  N1 
G  exp   N2  N1  L
If N2 < N1 :          N1  N2 
Inversion
In order to achieve G > 1, stimulated emission must exceed
absorption:

B N2 I > B N1 I                     Inversion

Or, equivalently,

“Negative

Energy
N2 > N1                                  temperature”

This condition is called inversion.
It does not occur naturally. It is                    Molecules
inherently a non-equilibrium state.

In order to achieve inversion, we must hit the laser medium very
hard in some way and choose our medium correctly.
Achieving inversion:
Pumping the laser medium
Now let I be the intensity of (flash lamp) light used to pump energy
into the laser medium:

I
I0                                        I1

I3             Laser medium               I2
R = 100%                                                  R < 100%

Will this intensity be sufficient to achieve inversion, N2 > N1?
It’ll depend on the laser medium’s energy level system.
Rate equations for a                                           2            N2
two-level system                                             Pump        Laser

1            N1
Rate equations for the densities of the two states:

Stimulated emission   Spontaneous
Absorption
emission
dN 2
 BI ( N1  N 2 )  AN 2                       If the total number
dt                                                 of molecules is N:
Pump intensity
dN1                                                  N  N1  N 2
 BI ( N 2  N1 )  AN 2
dt                                                N  N1  N 2
d N                                     2 N 2  ( N1  N 2 )  ( N1  N 2 )
       2 BI N  2 AN 2
dt                                            N  N
d N
       2 BI N  AN  AN
dt
Why inversion is impossible                                   2          N2
in a two-level system                                                   Laser

d N                                         1          N1
 2 BI N  AN  AN
dt
In steady-state:    0  2BI N  AN  AN
 ( A  2BI )N  AN
 N  AN /( A  2BI )
 N  N /(1  2BI / A)

N               where:        I sat  A / B
 N 
1  2 I / I sat      Isat is the saturation intensity.

N is always positive, no matter how high I is!
It’s impossible to achieve an inversion in a two-level system!
Rate equations for a                               3
Fast decay
three-level system                                 2

Pump          Laser
Assume we pump to a state 3 that
Transition       Transition
rapidly decays to level 2. No pump
stimulated emission!                               1
Spontaneous
emission
dN 2
 BIN1  AN 2
dt                                 The total number       Level 3
Absorption           of molecules is N:     decays
fast and
dN1                                  N  N1  N 2
  BIN1  AN 2                                        so is zero.
dt                                 N  N1  N 2
d N
 2 BIN1  2 AN 2              2N 2  N  N
dt
2N1  N  N
d N
        BIN  BI N  AN  AN
dt
3
Why inversion is possible                       2
Fast decay

in a three-level system
Pump      Laser
Transition   Transition
d N
  BIN  BI N  AN  AN        1
dt
In steady-state: 0  BIN  BI N  AN  AN

 ( A  BI )N  ( A  BI ) N

 N  N ( A  BI ) /( A  BI )

1  I / I sat
 N  N
1  I / I sat

Now if I > Isat, N is negative!
Rate equations for a                            3
Fast decay
four-level system                               2

Now assume the lower laser level 1            Pump         Laser
also rapidly decays to a ground level 0.   Transition      Transition
So N1  0 ! And N   N 2
1
Fast decay
dN 2                             0
As before:           BIN 0  AN 2
dt
dN 2                                    The total number
 BI ( N  N 2 )  AN 2            of molecules is N :
dt
N  N0  N2
Because      N   N 2
N0  N  N2
d N
       BIN  BI N  AN
dt
At steady state:    0  BIN  BI N  AN
3
Why inversion is easy                                Fast decay
2
in a four-level system
(cont’d)                                   Pump
Transition
Laser
Transition

0  BIN  BI N  AN                    1
Fast decay
0
 ( A  BI )N   BIN

 N   BIN /( A  BI )

 N  ( BIN / A) /(1  BI / A)

I / I sat
    N   N
1  I / I sat

Now, N is negative—always!
3
2
saturation intensity?
Pump              Laser
Transition           Transition
I sat  A / B
1
Fast decay
A is the excited-state relaxation rate: 1/t           0
B is the absorption cross-section, , divided by
the energy per photon, ħw:  / ħw
ħw ~10-19 J for visible/near IR light
Both  and t
depend on the                      w      t ~10-12 to 10-8 s for most molecules
molecule, the           I sat                10-9 to 10-3 s for laser molecules
frequency, and                    t       ~10-20 to 10-16 cm2 for molecules (on
the various                               resonance)
states involved.    1 to 1013 W/cm2

The saturation intensity plays a key role in laser theory.
Two-, three-, and four-level systems
It took laser physicists a while to realize that four-level systems are
best.

Two-level                   Three-level                   Four-level
system                       system                       system

Fast decay
Fast decay
Pump
Pump         Laser                                      Transition     Laser
Transition      Transition                                                Transition
Laser
Pump
Transition
Transition
Fast decay

At best, you get
If you hit it hard,
equal populations.                                           Lasing is easy!
you get lasing.
No lasing.
Achieving Laser Threshold
An inversion isn’t enough. The laser output and additional losses in
intensity due to absorption, scattering, and reflections, occur.

I0                                    I1
Laser medium
I3         Gain, G = exp(gL), and    I2
R = 100%              Absorption, A = exp(-L)        R < 100%

The laser will lase if the beam increases
Gain > Loss
in intensity during a round trip, that is, if:

This called achieving Threshold. It means: I3 > I0. Here, it means:

I 3  I 0 exp( gL) exp( L) R exp( gL) exp(  L)  I 0
 2( g   ) L  ln(1/ R)
Types of Lasers
Solid-state lasers have lasing material distributed in a solid matrix
(such as ruby or neodymium:yttrium-aluminum garnet "YAG"). Flash
lamps are the most common power source. The Nd:YAG laser
emits infrared light at 1.064 nm.
Semiconductor lasers, sometimes called diode lasers, are pn
junctions. Current is the pump source. Applications: laser printers or
CD players.
Dye lasers use complex organic dyes, such as rhodamine 6G, in liquid
solution or suspension as lasing media. They are tunable over a
Gas lasers are pumped by current. Helium-Neon lases in the visible
and IR. Argon lases in the visible and UV. CO2 lasers emit light in
the far-infrared (10.6 mm), and are used for cutting hard materials.
Excimer lasers (from the terms excited and dimers) use reactive
gases, such as chlorine and fluorine, mixed with inert gases such as
argon, krypton, or xenon. When electrically stimulated, a pseudo
molecule (dimer) is produced. Excimers lase in the UV.
The Ruby Laser

Invented in 1960 by Ted Maiman
at Hughes Research Labs, it was
the first laser.

Ruby is a three-level system, so
you have to hit it hard.
The Helium-
Neon Laser
Energetic electrons in a
glow discharge collide with
and excite He atoms,
which then collide with and
transfer the excitation to
Ne atoms, an ideal 4-level
system.
Carbon Dioxide Laser
The CO2 laser operates analogously. N2 is pumped, transferring
the energy to CO2.
CO2 laser in the
Martian atmosphere

The atmosphere is thin
and the sun is dim, but
the gain per molecule is
high, and the
pathlength is long.
Detuning from line center (MHz)

The population inversion scheme in HeCd is similar to
that in HeNe’s except that the active medium is
Cd+ ions.

The laser transitions occur in the blue and the
ultraviolet at 442 nm, 354 nm and 325 nm.

The UV lines are useful for applications that require
short wavelength lasers, such as high precision
printing on photosensitive materials. Examples include
lithography of electronic circuitry and making
master copies of compact disks.
The Argon
Ion Laser

Argon ion laser lines:

Wavelength   Relative Power   Absolute Power
454.6 nm           .03             .8 W
457.9 nm           .06            1.5 W        The Argon
465.8 nm           .03             .8 W        ion laser
472.7 nm           .05            1.3 W        also has
476.5 nm           .12            3.0 W        some laser
488.0 nm           .32            8.0 W        lines in the
496.5 nm           .12            3.0 W        UV.
501.7 nm           .07            1.8 W        But it’s very
514.5 nm           .40           10.0 W        inefficient.
528.7 nm           .07            1.8 W
The Krypton Ion Laser

Krypton ion laser lines:

Wavelength     Power
406.7 nm        .9 W
413.1 nm       1.8 W
415.4 nm       .28 W
468.0 nm        .5 W
476.2 nm        .4 W
482.5 nm        .4 W
520.8 nm        .7 W
530.9 nm       1.5 W
568.2 nm       1.1 W
647.1 nm       3.5 W
676.4 nm       1.2 W
Dye lasers

Dye lasers are an ideal four-level system, and a given dye will lase
over a range of ~100 nm.
A dye’s energy levels

The lower laser level can be almost any level in the S0 manifold.

S1: 1st excited
electronic state
manifold

Pump Transition             Laser Transitions

S0: Ground
electronic state
manifold

Dyes are so ideal that it’s often difficult to stop them from lasing in all
directions!
Dyes cover the visible, near-IR, and
near-UV ranges.
Titanium: Sapphire (Ti:Sapphire)

Absorption and emission
spectra of Ti:Sapphire

3.2 msec

Al2O3 lattice   oxygen
Ti:Sapphire lases from
aluminum
~700 nm to ~1000 nm.
Diode Lasers
Some everyday applications of diode
lasers

A CD burner           Laser Printer

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