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Content-Location: file:///C:/9E4B22B3/Physics222StimEmissionAndLasers_files/master07.htm Content-Transfer-Encoding: quoted-printable Content-Type: text/html; charset="us-ascii"
Click to edit Master title style<= /div>
Click to edit Master subtitle sty= le
‹foote= r›
‹#R= 50;
‹date/time›
------=_NextPart_01C6B259.480AAB10 Content-Location: file:///C:/9E4B22B3/Physics222StimEmissionAndLasers_files/master07.xml Content-Transfer-Encoding: quoted-printable Content-Type: text/xml; charset="utf-8" ------=_NextPart_01C6B259.480AAB10 Content-Location: file:///C:/9E4B22B3/Physics222StimEmissionAndLasers_files/pres.xml Content-Transfer-Encoding: quoted-printable Content-Type: text/xml; charset="utf-8" ------=_NextPart_01C6B259.480AAB10 Content-Location: file:///C:/9E4B22B3/Physics222StimEmissionAndLasers_files/slide0164.htm Content-Transfer-Encoding: quoted-printable Content-Type: text/html; charset="us-ascii" Slide 1
No SE: = Rabi Oscillations
ωR
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Medium = SE ( u(f)B12 ~ A21 )
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High SE ( u(f)B12 << A21 )
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Atoms interacting with light…<= /div>
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Atoms interacting with light…<= /div>
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Atoms interacting with light…<= /div>
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Thought Question
•If I have N1 atom= s in the lower state, how many need to be in the upper state in order for lasing to occur?
•
= 211;A: An equal number (N2 = =3D N<= /span>1<= /span>)
= 211;B: One more than in the lower state (N2 =3D = N1 + 1)=
= 211;C: A bit more than the lower state (N2 =3D = N1 + ε)
= 211;D: Many (N= 2 = >> N= 1<= /span>)
= 211;E: I have no idea
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Hydrogen Maser
From Norman Ramsey’s 1989 Nobel Lecture
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What does LASER stand for?
Low Aptitude? Select Engineering or Refuse-collection.
Lasers Are So= Easy to Ruin
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Lasers
•Light Amplification by Stimulated Emission of Radiation =
•Component= s
–Gain Med= ium
–Optical Cavity
<= span class=3DB2B style=3D'position:absolute;left:-3.46%;top:-.15em'>•High reflectors and Output Couplers
–Pump = ;
<= span class=3DB2B style=3D'position:absolute;left:-3.46%;top:-.15em'>•Creates “Population Inversion”
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Typical Laser Design
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Laser Gain Mediums
<= span style=3D'font-size:44%'>•Gas
–Helium Neon
•Helium atoms excited by discharge
•Neon atoms excited by collisions with Helium
–Argon Ion
•Can be relatively high powered
•Can make a lot of green light – excellent for pumping other lasers <= /span>
•Also used to make semiconductors, medical
–Gas Masers
•Ammonia Maser – first maser (1954 by C. H. Townes, J. P. Gordon, and H. J. Zeiger)
•Hydrogen Masers still used for frequency standards
•Solid
–Light Pumped
•Ruby
–First optical laser (T. H. Maiman 1960)
•Nd:YAG (Nd atoms in a clear crystal)
•Ti:Sapphire
–Semiconductor
•Laser pointers, CD players, DVD players
•Simple, small, inexpensive, and very efficient
•Hard to get more than ~50 mW
•Arrays of them are used to pump other lasers
•Liquid
–Dye lasers
•Large tuning range
•A large range of dyes are available covering a wide spectral range
•Can be nasty to work with
•
•
•
------=_NextPart_01C6B259.480AAB10 Content-Location: file:///C:/9E4B22B3/Physics222StimEmissionAndLasers_files/slide0103.htm Content-Transfer-Encoding: quoted-printable Content-Type: text/html; charset="us-ascii" Slide 1
Ways to Pump a Laser
<= span style=3D'font-size:88%'>•With Light
–Flashlamps (Ruby Laser, Nd:YAG) =
–Other Lasers (Ti:Sapphire, Dye, Nd:YAG)
•With Electricity
–Electric Discharge – Collisions with Electrons
•Most Gas Lasers (Argon, Krypton, etc.)
–Discharge + Collision – HeNe
–Semiconductor Lasers
•Chemical Reactions
–Excimer Lasers
•
------=_NextPart_01C6B259.480AAB10 Content-Location: file:///C:/9E4B22B3/Physics222StimEmissionAndLasers_files/slide0104.htm Content-Transfer-Encoding: quoted-printable Content-Type: text/html; charset="us-ascii" Slide 1
Pulsed Lasers
<= span style=3D'font-size:75%'>•High Power for a Short Time
–PW pulses (1015 Watt= s) possible
–fs pulses possible (10-15 seconds)
–High intensity
•10^4 watts/sq cm at surface of sun
•10^9 w/cm2 highest for focused cw laser
•10^21 w/cm2 world record for focused pulsed laser
•What is needed to generate a short, high power pulse?
–Way to stop lasing until energy is built up in medium
•Q switching
–Active q switching
–Mode locked lasers
•Gain medium with wide gain spectrum
–Ti:sapph à 700-950 nm
–Dye lasers
–
------=_NextPart_01C6B259.480AAB10 Content-Location: file:///C:/9E4B22B3/Physics222StimEmissionAndLasers_files/slide0105.htm Content-Transfer-Encoding: quoted-printable Content-Type: text/html; charset="us-ascii" Slide 1
Three and Four State Lasers
pump=
fast decay
slow decay
pump<= /div>
fast decay
slow decay
fast decay
Metastable
State
The first laser
(the ruby laser)
was a 3 state laser
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ASE
“Slope Efficiency”
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