12369_L7 Laser

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    L7LASER

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    LASER

    LLight

    AAmplification by

    SStimulated

    EEmission of

    RRadiation

    http://../01-01-10%20to%2001-06-10/PHY112/Course%20Content/LASER/laser/L%20is%20for%20Light.htmhttp://../01-01-10%20to%2001-06-10/PHY112/Course%20Content/LASER/laser/A%20is%20for%20Amplification.htmhttp://../01-01-10%20to%2001-06-10/PHY112/Course%20Content/LASER/laser/S%20is%20for%20Stimulated.htmhttp://../01-01-10%20to%2001-06-10/PHY112/Course%20Content/LASER/laser/S%20is%20for%20Stimulated.htmhttp://../01-01-10%20to%2001-06-10/PHY112/Course%20Content/LASER/laser/E%20is%20for%20Emission.htmhttp://../01-01-10%20to%2001-06-10/PHY112/Course%20Content/LASER/laser/R%20is%20for%20Radiation.htmhttp://../01-01-10%20to%2001-06-10/PHY112/Course%20Content/LASER/laser/R%20is%20for%20Radiation.htmhttp://../01-01-10%20to%2001-06-10/PHY112/Course%20Content/LASER/laser/R%20is%20for%20Radiation.htmhttp://../01-01-10%20to%2001-06-10/PHY112/Course%20Content/LASER/laser/E%20is%20for%20Emission.htmhttp://../01-01-10%20to%2001-06-10/PHY112/Course%20Content/LASER/laser/S%20is%20for%20Stimulated.htmhttp://../01-01-10%20to%2001-06-10/PHY112/Course%20Content/LASER/laser/A%20is%20for%20Amplification.htmhttp://../01-01-10%20to%2001-06-10/PHY112/Course%20Content/LASER/laser/L%20is%20for%20Light.htm
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    Properties of laser

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    Monochromatic

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    Directionality

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    Coherence

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    Incandescent vs. Laser Light

    1. Many wavelengths

    2. Multidirectional

    3. Incoherent

    1. Monochromatic

    2. Directional

    3. Coherent

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    BASIC PRINCIPLE NEEDEDFOR LASER

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    Stimulated Absorption

    Energy is absorbed by an atom, the electrons are

    excited into vacant energy shells.

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    Spontaneous Emission

    The atom decays from level 2 to level 1 through theemission of a photon with the energy hv. It is acompletely random process.

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    Stimulated Emission

    atoms in an upper energy level can be triggered or

    stimulated in phase by an incoming photon of a specific

    energy.

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    Stimulated Emission

    The stimulated photons have unique properties:

    In phase with the incident photon

    Same wavelength as the incident photon

    Travel in same direction as incident photon

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    WHY WE NEED META STABLE

    STATE?

    ANSWER IS

    With having the metastable state above the

    ground level. Atom reaches the meta stable

    state (after first stimulated emission) can

    remain there for longer time period. So the

    number of atom increases in the meta stable

    state. And when these atoms come back to theoriginal ground level it emits laser beam.

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    A state of a medium where a higher-lying electronic level has

    a higher population than a lower-lying level

    POPULATION INVERSION

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    The method particle of raising a particle from lower energy stateto higher energy state is called pumping.

    TYPES OF PUMPING :

    1. Optical pumping

    2. Electrical pumping

    3. X-ray pumping

    4. Chemical pumping

    PUMPING

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    All lasers have 3 essential components:

    A lasing or "gain" medium

    A source of energy to excite electrons in the gain medium to high energy

    states, referred to as "pump" energy

    An optical path which allows emitted photons to oscillate and interfere

    constructively as energy is added or "pumped" into the system, ie, a

    resonator

    LASER COMPONENTS

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    LASER ACTION

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    Types of Laser

    a.According to their sources:

    1.Gas Lasers2.Crystal Lasers

    3.Semiconductors Lasers

    4.Liquid Lasers

    a.According to the nature of emission:

    1.Continuous Wave

    2.Pulsed Laser

    a.According to their wavelength:1.Visible Region

    2.Infrared Region

    3.Ultraviolet Region

    4.Microwave RegionX-Ray Region

    d. According to different levels 1. 2-level laser

    2. 3-level laser

    3. 4-level laser

    e. According to mode of pumping

    1. optical

    2. chemical

    3. electric discharge4. electrical

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    2- Level Laser

    h

    E1

    E2

    AbsorptionE1

    E2h

    Spontaneous

    Emission

    E1

    E2hh h

    Stimulated

    Emission

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    THREE STEP LASER

    Stimulated absorption

    Spontaneous emission to the metastable state

    Stimulated emission from metastable state to ground state.

    E2

    E1

    E0

    E2 E1

    E1 E0

    META STABLESTATE

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    4-Level LASER

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    PRACTICAL LASERS

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    RUBY LASER

    Construction

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    ENERGY LEVEL IN RUBY

    LASER

    Energy

    4A2

    4T2

    4T1

    2T2

    2E

    LASING

    rapid decay

    Cr+

    Al2O3

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    LASER ACTION IN RUBY

    LASER

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    HE-NE LASER

    Construction

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    .

    Energy Level Diagram of He-Ne

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    Energy Level Diagram of He-Ne cont

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    Combined Laser Action

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    Emission wavelengths of common

    lasers

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    APPLICATION S OF LASER

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    04/13/11

    Not to be Taken LightlyThe Weighty Implications of Laser Technology

    Applications of

    Laser

    Technology

    Medical

    Entertainment

    Telecommunications

    Military

    Optical SurgeryGeneral Surgery Tattoo removal

    CD Players DVD Players Video Game Systems

    Information tech. Holograms

    Weapons

    Satellites

    Radar

    Industry

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    04/13/11

    Can You See the Light?

    Dentists use

    laser drills

    Bad eyesight can be

    corrected by optical

    surgery using lasers

    CD-Audio is

    read by a laser

    Tattoo removal is

    done using lasers

    Cd-Rom discs

    are read by lasers

    Laser pointers can

    enhance

    presentations Bar codes in

    grocery stores are

    scanned by lasers

    Video game systems such as

    PlayStation 2 utilize lasers

    DVD players read

    DVDs using lasers

    Airplanes areequipped with

    laser radar

    Military and Spaceaircraft are equipped

    with laser guns

    Laser tech. is used in printers,

    copiers, and scanners

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    Einsteins Coefficients

    Einstein gives a probability that stimulated

    emission is same as absorption.

    Means that if a stimulated absorption can

    occur then there is same probability that

    stimulated emission can occur.

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    Equilibrium condition

    In case of energy states the number of electron

    absorbed and emitted should be equal or the

    rate of change of numbers of atoms in two

    states should be equal.

    0=dt

    dN

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    Plancks Radiation Law

    ( )

    1

    18

    3

    3

    = kTh

    ec

    hE

    Planks gives the formula that howa gas radiate energy.

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    Spontaneous emission

    A21

    :- correspond to spontaneous emission

    probability per unit time

    This particular emission can occur

    without the presence of external field

    E(v)

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    Stimulated Absorption

    B12

    :- correspond to stimulated absorption

    probability per unit time

    This type of absorption can occur in

    presence of external field E(v) only

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    Stimulated Emission

    B21

    :- correspond to stimulated emission

    probability per unit time

    This type of emission can occur in presence of

    external field E(v) only

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    Total Emission Probability

    Spontaneous Emission + Stimulated Emission

    A21 + B21 E(v)

    Number of atoms that can jump from level E2 to E1 is

    ( )[ ] 22121 NEBA +

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    Total Absorption Probability

    ( )[ ] 112 NEB

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    At Equilibrium

    Then

    02 =dt

    dN

    ( ) ( )[ ] 22121112 NEBANEB +=

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    Emission and absorption are same

    ( )

    =

    B

    B

    N

    NB

    A

    E

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    Maxwell Bolzman Distribution

    KT

    E

    eNN

    1

    01

    =

    KT

    E

    eNN

    2

    02

    =

    In thermal equilibrium

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    So the equations become

    kT

    h

    eN

    N

    =2

    1

    So equation becomes

    ( )1

    1

    21

    1221

    21

    =B

    Be

    B

    A

    EkT

    h

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    Conclusions

    Stimulated emission have same probability as

    stimulated absorption

    Ratio between spontaneous and stimulated

    emission varies with v3

    All we need is to calculate one of the

    probability to find others.

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    THANKS SEE YOU IN NEXTLECTURE