考试时间: 2011.1.4 上课时间和教室. chapter 7. lasers light amplification by stimulated...
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考试时间: 2011.1.4上课时间和教室
Chapter 7. Lasers
Light Amplification by Stimulated Emission of Radiation
(acronym)
The History 1916, Einstein predicted the stimulated emission. 1954, Townes and co-workers developed a Microwave A
mplifier by Stimulated Emission of Radiation(maser) using ammonia, NH3.
1958, Schawlow and Townes showed that the maser principle could be extended into the visible region .
1960, Maiman built the first laser using ruby as the active medium.
From then on, laser development was nothing short of miraculous, giving optics new impetus and wide publicity.
7.1 Stimulated Emission of Radiation 1. Boltzmann Distribution the transitions that occur between different energy states
absorption: the upward transition from a lower energy state to a higher state, E1 E2
Emission: the downward transition, E2 E1,
population N : the number of atoms, per unit volume, that exist in a given state.
given by Boltzmann's equation
TEeN /E : energy lever of the system : Boltzmann's constantT : absolute temperature.
7.1 Stimulated Emission of Radiation Boltzmann's ratio or relative population : the ratio of the populations in the two states, N2 / N1.
Or
plot the energy in the higher state relative to that in the lower state, versus the population in these states(E versus N), the result is an exponential curve known as a Boltzmann distribution.
When the Boltzmann distribution is normal, it means that the system is in thermal equilibrium, having more atoms in the lower state than in the higher state.
TE
TE
e
e
N
N
/
/
1
2
1
2
TEEeNN /)(12
12
7.1 Stimulated Emission of Radiation 2. Einstein's Prediction
Assume first: an ensemble of atoms is in thermal equilibrium and not subject to an external radiation field.
• At higher temperatures, a certain number of atoms is in the excited state; on return to the lower state, these atoms will emit radiation, in the form of quanta h . -- spontaneous emission
rate of the transition: the number of atoms in the higher state that make the transition to the lower state, per second.
lifetime of the transition: the reciprocal of the rate of transition.
rate of the spontaneous transition:
A21: constant of proportionality
N2 : number of atoms (per unit volume) in the higher state
21221 ANP
7.1 Stimulated Emission of Radiation
Assume next: the system is subject to some external radiation field.
one of two processes may occur, depending on:
the direction (the phase) of the field with respect to the phase of the oscillator.
7.1 Stimulated Emission of Radiation the two phases coincide:a quantum of the field may cause the emission of another quantum. -- stimulated emission.
Its rate is
B21 : constant of proportionality
u(): energy density (J m-3), function of frequency .
the two phase is opposite : the impulse transferred counteracts the oscillation, energy is consumed, and the system is raised to a higher state -- absorption.
Its rate is
B12 : constant of proportionality.
uBNP 21221
uBNP 12112
7.1 Stimulated Emission of Radiation
Transitions between energy states
7.1 Stimulated Emission of Radiation Einstein's coefficients: A21, B21, B12
Einstein's relations
B21 = B123
3
21
21 8
c
h
B
A
(1) the coefficients for both stimulated emission and absorption are numerically equal
(2) the ratio of the coefficients of spontaneous versus stimulated emission is proportional to the third power of the frequency of the transition radiation
explains why it is so difficult to achieve laser emission in the X-ray range, where is rather high
7.1 Stimulated Emission of Radiation 3. Population Inversion
thermal equilibrium system absorption and spontaneous emission take place side by side
N2 < N1, absorption dominates: an incident quantum is mo
re likely to be absorbed than to cause emission.
population inversion condition a majority of atoms in the higher state, N2 > N1
on return to the ground state, the system will probably lase.
Incandescent vs. Laser Light Light from bulbs are due to spontaneous emission
1. Many wavelengths
2. Multidirectional
3. Incoherent
1. Monochromatic
2. Directional
3. Coherent
CoherenceCoherent: If the phase of a light wave is well defined at all
times (oscillates in a simple pattern with time and varies in a smooth wave in space at any instant).
Example: a laser produces highly coherent light. In a laser, all of the atoms radiate in phase.
Incoherent: the phase of a light wave varies randomly from point to point, or from moment to moment.
Example: An incandescent or fluorescent light bulb produces incoherent light. All of the atoms in the phosphor of the bulb radiate with random phase.
Stimulated vs Spontaneous Emission
Stimulated emission requires the presence of a photon. An “incoming” photon stimulates a molecule in an excited state to decay to the ground state by emitting a photon. The stimulated photons travel in the same direction as the incoming photon.
Spontaneous emission does not require the presence of a photon. Instead a molecule in the excited state can relax to the ground state by spontaneously emitting a photon. Spontaneously emitted photons are emitted in all directions.
two-level system(ex. ammonia maser)
En, Nn
Em, Nm
En, Nn
Em, Nm
Even with very a intense pump source, the best one can achieve with a two-level system is
excited state population = ground state population
three-level system
in equilibrium normal Boltzmann distribution absorptive rather than emissive
excited
population inversion
7.2 Practical Realization 1. General Construction
Pumping: an energy source to supply the energy needed for raising the system to the excited state.
active medium: in which, reaches population inversion and lases when excited. may be a solid, liquid, or gas thousands of materials that have been found to lase
cavity:optionallaser amplifiers: no cavitylaser oscillators: medium enclosed in a cavity provides feedback and additional amplification cavity formed by two mirrors: one full reflectance, the other partially transparent
7.2 Practical Realization
Energy source Medium Full reflectance mirrors Partially transparent mirrors Radiation
Basic components of a laser oscillator
Common Components of all Lasers1. Active Medium
The active medium may be solid crystals such as ruby or Nd:YAG, liquid dyes, gases like CO2 or Helium/Neon, or semiconductors such as GaAs. Active mediums contain atoms whose electrons may be excited to a metastable energy level by an energy source.
2. Excitation Mechanism
Excitation mechanisms pump energy into the active medium by one or more of three basic methods; optical, electrical or chemical.
3. High Reflectance Mirror
A mirror which reflects essentially 100% of the laser light.
4. Partially Transmissive Mirror
A mirror which reflects less than 100% of the laser light and transmits the remainder.
2. Excitation
optical pumping: ruby laser a light source another laser.
electron excitation: argon laser , helium-neon laser
direct conversion of electric energy into radiation: light-emitting diodes(LEDs), semiconductor lasers
thermal excitation : CO2 laser.
chemical pumping: chemical laser
H2 + F2 2HF
7.2 Practical Realization
7.2 Practical Realization
3. Cavity Configurations
Plane-parallel cavity: very efficient ( good filling), difficult alignment(low stability)
confocal cavity: poor filling, easier to align
concentric cavity (spherical cavity) : poor filling, easier to align
hemispherical cavity: poor filling, much easy to align
long-radius cavity: good compromise between the plane-parallel and the confocal variety, type of cavity used most often in today's commercial lasers.
7.2 Practical Realization Cavity configurations
L:distance between mirrors
R:radius of curvature
7.2 Practical Realization 4. Mode Structure
Assume: the cavity is limited by two plane-parallel mirrors.
the wavelength possible of the standing-wave pattern inside the cavity is:
L : length of the cavityq : number of half-wavelengths, or axial modes
the resonance condition for axial modes:
n: index of medium contained in a laser cavity
Lq
2λ
nL2
cqν
7.2 Practical Realization
different frequencies are closely, and evenly, spaced, lie within the width of a single emission line.
the output of the laser consists of a number of lines separated by c/2S
two consecutive modes (which differ by q = 1), are separated by a frequency difference ,
S2
cν
Mode-locking
Active mode-locking
7.2 Practical Realization
TEM: transverse electromagnetic, modes
few in number, easy to see.
Aim the laser at a distant screen, spread the beam out by a negative lens.:
bright patches, separated from one another by intervals called "nodal lines".
Within each patch, the phase of the light is the same, but between patches the phase is reversed.
7.2 Practical Realization
lowest possible axial mode:
laser oscillates in one frequency
highest possible temporal coherence
TEM modesTEM00 :
lowest possible transverse mode
no phase reversal across the beam, the beam is "uniphase"
highest possible spatial coherence, can be focused to the smallest spot size and reach the highest power density.
5. Gain
Gain of a laser depends on several factors. Foremost among them is the separation of the energy levels that provide laser transition.
The two levels are father apart, the gain is higher because then the laser transition contains a larger fraction of the energy compared to the energy in the pump transition
7.2 Practical Realization
Gain is the opposite of absorption
--definition
: initial power in the cavity
: power of exit light
absorptivity positive: for thermal equilibrium where N2 < N1.
absorptivity negative: in population inversion, where N2 > N1,
laser emission could be considered negative absorption
gain coefficient : the negative of the "absorption coefficient“
xe 0
xe 0
0
7.2 Practical Realization
As the wave is reflected back and forth between the mirrors, it will lose some of its energy, mainly because of the limited reflectivity of one of mirrors.
If the two mirrors have reflectivities r1 and r2,
--each round trip210 rr err 21
: loss per round trip
--For the system xe )(
0
> : system will lase, threshold condition necessary to sustain laser emission.
7.2 Practical Realization
7.3 Types of Lasers
1. Solid-state Lasers
ruby laser
Ruby is synthetic aluminum oxide, Al2O3, with 0.03 to
0.05% of chromium oxide, Cr2O3, added to it. The
Cr3+ ions are the active ingredient; the aluminum and oxygen atoms are inert.
The ruby crystal is made into a cylindrical rod, several centimeters long and several millimeters in diameter, with the ends polished flat to act as cavity mirrors.
Pumping is by light from a xenon flash tube.
7.3 Types of Lasers E3: fairly wide and has a short lif
etime; the excited Cr3+ ions rapidly relax and drop to the next lower state, E2. This transition is non
radiative.
E2: metastable and has a lifetime
longer than that of E3, and the Cr3+ ions remain that much longer in E2 before they drop to the grou
nd state, E1.The E2 E1 transition is radiative; it produces the spontaneous, incoh
erent red fluorescence typical of ruby, with a peak near 694 nm.
As the pumping energy is increased above a critical threshold, population inversion occurs in E2 with respect to E1 and the system lases, wit
h a sharp peak at 694.3 nm.
Three-level energy diagram typical of ruby
Lasing Action DiagramEn
erg
y
Intr
od
ucti
on
Ground State
Excited State
Metastable State
Spontaneous Energy Emission
Stimulated Emission of Radiation
effi
cien
t p
um
pin
g
slo
w r
elax
atio
n
Metastable state
fast
slow Population inversion
Fast relaxation
Requirements for Laser Action
neodymium: YAG laser
The active ingredient is trivalent neodymium, Nd3+, added to an yttrium aluminum garnet, YAG, Y3Al5O12.
It has four energy levels. The laser transition begins at the metastable state and ends at an additional level somewhat above the ground state.
7.3 Types of Lasers
7.3 Types of Lasers 2. Gas Lasers Gas lasers consist of a gas filled tube placed in the laser cavity. A voltage (the external pump source) is applied to the tube to excite the atoms in the gas to a population inversion. The light emitted from this type of laser is normally continuous wave (CW).
helium-neon laser Typically, it consists of a tube about 30 cm long and 2 mm in diameter, with two electrodes on the side and fused silica windows at both ends. The tube contains a mixture of 5 parts helium and 1 part neon, kept at a pressure of 133 Pa.
7.3 Types of Lasers
argon laser
It generates a strong turquoise-blue line at 488 nm and a green line at 514.5 nm, in either pulsed or c. w. operation.
helium-cadmium
It emits a brilliant blue at 441.6 nm.
7.3 Types of Lasers carbon dioxide laser
high power: the first CO2 lasers had a continuous output of a
few milliwatts. Today we have powers of some 200 kW, more than enough to cut through steel plates several centimeters thick in a matter of seconds.
High efficient: the efficiency in converting electrical energy into radiation is better (more than 10%) than that of any other laser.(TEA CO2 laser)
Relatively simple in construction and operation are.
Tunable in a small range
Emission is at 10.6 m.
7.3 Types of Lasers
Excimer lasers
contain rare-gas halides such as XeCl, KrF, or others. These molecules are unstable in the ground state but bound in the excited state.
exceedingly powerful, with outputs as high as several GW.
emit in the ultraviolet.
7.3 Types of Lasers
3. Semiconductor Lasers
LED: light-emitting diode
emit almost anywhere in the spectrum, from the UV to the IR
an efficiency much higher than with optical pumping (around 40% versus 3%).
small ,less than 1 mm in diameter
main application :
• waveguides
• integrated optics
7.3 Types of Lasers 4. Tunable Lasers
dye lasers: first tunable lasers
parametric oscillator: more compact less expensive easier to operate tuning range much wider
Color center lasers: tuned over wide bands in the UV, the visible, and the IR.
free-electron laser: high powers of the order of megawatts very efficient tuned through a wide range of wavelengths.
Tunable lasers are most welcome to spectroscopists
Argon fluoride (Excimer-UV)Krypton chloride (Excimer-UV)Krypton fluoride (Excimer-UV)Xenon chloride (Excimer-UV)Xenon fluoride (Excimer-UV)Helium cadmium (UV)Nitrogen (UV)Helium cadmium (violet)Krypton (blue)Argon (blue)Copper vapor (green)Argon (green)Krypton (green)Frequency doubled Nd YAG (green)Helium neon (green)Krypton (yellow)Copper vapor (yellow)
0.1930.2220.2480.3080.3510.3250.3370.4410.4760.4880.5100.5140.5280.532
0.5430.5680.570
Helium neon (yellow)Helium neon (orange)Gold vapor (red)Helium neon (red)Krypton (red)Rohodamine 6G dye (tunable)Ruby (CrAlO3) (red)
Gallium arsenide (diode-NIR)Nd:YAG (NIR)Helium neon (NIR)Erbium (NIR)Helium neon (NIR)Hydrogen fluoride (NIR)Carbon dioxide (FIR)Carbon dioxide (FIR)
0.5940.6100.6270.6330.647
0.570-0.6500.6940.8401.0641.15 1.5043.392.709.6
10.6
Key: UV = ultraviolet (0.200-0.400 µm) VIS = visible (0.400-0.700 µm) NIR = near infrared (0.700-1.400 µm)
WAVELENGTHS OF MOST COMMON LASERS
Wavelength (m)Laser Type
Laser OutputContinuous Output (CW) Pulsed Output (P)
watt (W) - Unit of power or radiant flux (1 watt = 1 joule per second).
Joule (J) - A unit of energy
Energy (Q) The capacity for doing work. Energy content is commonly used to characterize the output from pulsed lasers and is generally expressed in Joules (J).
Irradiance (E) - Power per unit area, expressed in watts per square centimeter.
En
erg
y (W
atts
)
TimeE
ner
gy
(Jo
ule
s)Time
7.4 Applications
Compared to radiation from other sources, laser radiation stands out in several ways:
highly coherent, both spatially and temporally generated in the form of very short pulses, at high powers
7.4 Applications
1. Beam Shape
laser operating in the TEM00 mode
the energy has a Gaussian distribution at a given distance r from the axis, the irradiance I falls off exponentially
parameter w: the distance from the axis at which I has dropped to 1/e2 of I0, the irradiance in the center
2)/2(0)( wreIrI
w(z) :beam's radius
: wavelength w0:radius at the waist.
For a confocal cavity, this simplifies to
L : distance between the mirrors.
2
20
0 1)(
w
zwzw
20
Lw
7.4 Applications
far field: farther away from the laser
beam's parameters can be considered linear functions of the distance
far-field half-angle divergence
0w
7.4 Applications
place a converging lens in the path of the light:
• beam to contract to a "focus“• another waist where the beam's wavefronts are plane• diameter radius of beam at the focus 2r:
f: the lens a focal length•radius of beam at the focus r
7.4 Applications
0
42
d
fr
D
fr
22.1
Rayleigh's criterion : D
22.1
7.4 Applications
2. Power and Power Density
A typical laser pulse contains about 10 J of energy. If this energy is delivered within a pulse only 0.5 ms long, the output power is 20 kW.
Q awitching: compressing the energy into a very short period of time.
7.4 Applications
3. Nonlinear Effects
Linear:the refractive index and the absorptivity of a material are independent of the intensity of the light that passes through.
Nonlinear: with very intense light, either the index or the absorptivity or both may become nonlinear functions of the intensity.
•change the refractive index, even of completely transparent material.
•Heat and thermal expansion, as they occur with absorbing materials, are not involved.
7.4 Applications
plasma: a mixture of ions and free electrons rarely found in nature except in the atmosphere of the sun
self-focusing: a beam of light contracts into thin, short lived, powerful threads of light that quickly shatter the material through which they pass.
Optical bistability arises in saturable systems
Phase conjugation(wavefront reversal): a molecular reflection of light. The reflected wavefronts are now distorted opposite to those in the incident beam,
Frequency doubling: generation of second harmonics.
7.4 Applications
4. Industrial Applications
Cutting
Drilling
Welding
Communications
Optical radar
precision measurements
Laser Technique in GIS Data Acquisition
GIS:Globe Information System
Tasks
Acquire Laser mapping equipment for GIS spatial data acquisition:– Utility mapping (power poles, water valve, gas
pipe, water pipe, etc)– Construction (ask for higher accuracy)– Digital geology mapping (geologic features)
Laser Mapping – Why It is Needed
Laser + GPS = fast 3D spatial data acquisition
Mapping the inaccessible area
More efficient and cost effective
Technical Basics
Distance measure + Angle (H & V) measure
Using NIR / Red Laser pulse for distance measure
Using magnetic compass or encoder for angle measurement
Emitter
Receiver
Laser Instrument
Distance
Distance = C x T / 2
C – speed of light
T – time
Technical Assessment Standards
Accuracy Distance Angle (horizontal & verti
cal) Function
Support Reflectorless Motorized Autotrack (high-caliber) Continuous mode Remote control (high-ca
liber)
Ease of use
GPS integration
External interface
Display
Laser Plummet (high-caliber)
Cost
Performance
Measurement Time
Measurement Range
Company Briefs
Laser Atlanta Optics, Inc., Norcross, GA USA, has been designing and manufacturing eye-safe laser-based distance and speed measuring systems since 1989.
Currently manufacture a product line based on a core technology called the Advantage. All of its rangefinder products are based on this proven design.
Measurement Devices Ltd. (MDL) is a leading designer, manufacturer and supplier of laser measurement systems.MDL is committed to preserving a quality system throughout all levels of our business, as well as providing consistent, high standards of customer service.
Advantage V.S. LaserAce/ALS
Laser Atlanta
Advantage
MDL
LaserAce / ALS
Accuracy Distance ±15.3 cm Typically 10 cm Typically 5 cm
Angle ±0.01°(en) both H & V;
H:±1°;V:±0.4° w/o en
H(encoder):0.2°; V: 0.3°;
Better ±1° w/o encoder;
H & V(en):0.02°
Performance Range 2-610m w/o reflector;
2-91800m w/ reflector
300m w/o reflector;
5,000m w/ refelctor
300 (DM)/600(RF) w/o
5km (DM)/10km(RF) w/
Time 0.34 sec 0.3 sec 0.5s(DM)/self-adp(RF)
Function Reflectorless? yes Yes yes
Motorized? no No yes
Cont. Mode yes yes yes
Ease of Use
Ext. Interface RS232 to PC RS232 to PC RS232 to PC
GPS integration Yes(plug & play) No No
Display HUD+ LCD LCD LCD
Cost $4000 -$6000 $4,300 – $5,525 $21,000 - $27,720
Advantage From Laser Atlanta
Physicals
•905 nm class I eye safe laser
•11.5Hx21.5Wx19Lcm
•4.5 lbs(2.1kg)
•Handle batteries
LaserAce From MDL
Physical •GaAs Laser Diode 905nm•Class I eye Safe•175x106x55 mm (LxWxH)•600g•Alignment Telescope: red dot•Compass(option)•Pocket PC (option)
Physical•Semi-conductor 905 nm•Class I eye safe•209 x 243 x 420mm (LxWxH)
•9.7kg /10.3 kg (w/ tribrach)
•Optical encoder
•Laptop/palm/desk top PC
Topcon: Pulse Total Station GPT-2000 series
Using pulse laser technology Support both prism/non-prism mode High accuracy:
Millimeter accuracy in distance measurement (5mm+2ppm xD in non prism mode; 3mm+2ppmxD in prism mode)
1”/ 5” (H & V) angle measurement accuracy Fast data acquisition:
0.3 sec tacking mode 1.2 second fine mode
Long range: Prism: 7,000m Non prism: 150m
All weather operation: water /dust proof Large data storage: 8000 points Laser plummet
Total Station GTS-800/800A seriesfrom Topcon
Motorized & automatic tracking – high speed rotation (up to 50º /sec) and high speed auto-tracking (up to 5º /sec)
Remote control through radio link or optical remote controller – enables one man operation
Flexible data management: Huge data storage – 2Mb memory plus PCMCIA card, space for data and software
User friendly Large graphic display Built-in MS-DOS OS Compact and light weight Water / dust resistant Handheld data collector TDS Survey Pro software allows more
functions: job classification, stake out, etc.
Motorized, automatic target recognition, reflectorless and remote control
Accuracy: Angle measurement: from 1.5” to 5” Distance measurement: 3mm+2ppm w/o reflector; 2m
m+2ppm w/ reflector Range: 200m (w/o reflector) to 7.5 km (w/reflector) Time
1sec w/ reflector 3 sec w/o reflector
Data storage: PCMCIA card or export via RS232 Software supports:
computations of area, height, tie distance etc. stake outs Exchange data between instrument and PC Create code list
Leica TCRA1100 series Total Station
Laser Plummet
GPT2000 series Display
External Interface
The external interface provides a way for the instrument to communicate with a PC, a laptop, a palm or a data logger. All the models here have this ability
7.4 Applications
5. Medical Applications
Coagulation & photocoagulation.
Photodisruption
Treatment of retinal
Laser refractive surgery
Correcting a refractive error by changing the shape of the cornea with surgery.
Diagram of the Eye
diagram of an eye
Normal Focus
Short sightedness(Myopia)
•Distance vision blurry, near usually OK.
Short-sightedfocus
Short-sightedcorrection
Long-sightedness(Hyperopia)
•Difficulty seeing clearly and comfortably up close.Long-sighted focus Long-sighted correction
AstigmatismIrregular curvature of the eye (shaped more like a football than a basketball)Light in different planes focuses at different points
A
B90
180
Shaping the cornea
Flattening the cornea, decreases myopia Steepening the cornea decreases hyperopia Making the cornea more spherical decreases
astigmatism All are possible in most refractive surgeries
Suitability for refractive surgery
Stable refractive error
– must not have changed for at least two years
Healthy eyes
– no underlying corneal abnormalities
Contact lens wear
– needs to be ceased at least three weeks prior to surgery
Refractive surgery does not mean you will never wear glasses
again
Most people over 40-50 years will need glasses for reading– this may not be fixed by laser surgery
Sometimes the corneal shape can gradually change– (although this is minimised)
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