10'4 Rare Earth Lasers - PowerPoint PPT Presentation

1 / 12
About This Presentation
Title:

10'4 Rare Earth Lasers

Description:

A Common Solid State Laser material is made by doping rare earth (Nd), in to a ... host materials such as glass (mostly SiO2),YAG (Y3Al5O12) and Sapphire (Al2O3) ... – PowerPoint PPT presentation

Number of Views:324
Avg rating:3.0/5.0
Slides: 13
Provided by: Priya56
Category:
Tags: earth | lasers | rare | sapphire

less

Transcript and Presenter's Notes

Title: 10'4 Rare Earth Lasers


1
10.4 Rare Earth Lasers Amplifiers
2
10.4.1 General Considerations
  • Rare Earth Elements
  • Elements with atomic numbers from 57-71.
  • Nd(60) and Er(68) are the most important
    ones.
  • A Common Solid State Laser Material
  • A Common Solid State Laser material is made by
    doping rare earth (Nd), in to a variety of
    optically transparent host materials such as
    glass (mostly SiO2),YAG (Y3Al5O12) and Sapphire
    (Al2O3).
  • Active atom is the Rare Earth.

3
Spectroscopic Notation
  • The characteristic of a quantum state is
    specified by the notation,
  • 2S1LetterJ
  • S Spin angular momentum
  • J Total angular momentum
  • Prescription for the Letter symbol

4
E.g. Ground State of Neodymium
  • Spectroscopic Notation 4 I 9/2
  • Degeneracy 2J1 10
  • There are 10 different wave functions describing
    this state.

5
Description
  • In rare earths (RE), the active e- participating
    in the optical transition is one of the 4f e-
    that is shielded by n5 and n6 orbits.
  • Energy levels of the rare earths are only weakly
    dependent on the host lattice.
  • Changes in the wavelength of the RE laser
    depending on the host lattice are very small and
    those changes appear in the 3rd or 4th
    significant figure.

6
Stark Effect Energy Splitting
  • These active atoms (RE) experience a local E
    field generated by the host lattice and hence
    degenerate energy levels are shifted (Stark
    effect).
  • Since stark effect is proportional to E (not to
    the direction), the positive negative fields
    yield the same shift.
  • For an example consider NdYAG, One can reduce
    the degeneracy in to (2J1)/2 doubly degenerate
    states.

7
10.4.2 NdYAG Lasers
  • Laser Material Y3Al5O12 (or YAG) Small
    amount of Nd
  • (host
    material) (RE)
  • Active atoms participate as if they were triply
    ionized, Nd 3 depend on the host lattice.
  • The Nd3 substitutes for Y3 in the cubic crystal
    of YAG, and thus each dopant atom sees more or
    less identical environment.
  • Since active atoms are in well defined
    environment, the energy levels are well defined
    and narrow.

8
Pumping
  • Flash Lamp
  • Semiconductor laser (808 nm)

9
Energy Level Diagram
Source www.star.le.ac.uk/rw/courses/lect4313_fig
14.jpg
10
Laser Output
  • NdYAG laser system can be operated either CW or
    pulsed mode, mode locked or Q-switched.
  • By using frequency doubling techniques O/P
    wavelength can be converted to green 1.064
    /2 532 nm with diffraction limited TEM00
    mode.

11
Source Joseph T. Verdeyen, Laser Electronics,
3rd edition (prentice-Hall, 1995)
12
Source Joseph T. Verdeyen, Laser Electronics,
3rd edition (prentice-Hall, 1995)
Write a Comment
User Comments (0)
About PowerShow.com