Search:  Catalog   or  Website 
Enter Catalog # Suffix
 
or Enter Master
 
or Enter Grooves per mm
   
Enter your query of Richardson Gratings
 
Home Products Information Contact Us Partner Tools
中文 日本語
Home > Information > Technical Notes > Technical Note 2

Technical Notes

Technical Note 1
Technical Note 2
Technical Note 3
Technical Note 4
Technical Note 5
Technical Note 6
Technical Note 7
Technical Note 8
Technical Note 9
Technical Note 10
Technical Note 11
Technical Note 12
Technical Note 13


Print Technical Note 2

Technical Note 2
PULSE COMPRESSION AND STRETCHING WITH DIFFRACTION GRATINGS

Diffraction gratings, used in conjunction with chirped pulses, are the key to compressing or stretching a laser pulse (i.e., increasing or decreasing their peak power with little loss in energy).

PULSE COMPRESSION

When a spectrally broad laser pulse is incident on a diffraction grating, the various wavelengths that make up the pulse will diffract from the grating at angles that depend on wavelength. If this pulse has its wavelength "chirped" so that the frequency increases during the length of the pulse, then diffraction will spread out the light in proportion, with the first part of the pulse (longer wavelengths) diffracting at a larger angle. The trailing portion of the pulse (shorter wavelengths) will diffract at a smaller angle and is directed to the leading edge of the second grating (see Figure 1). When the light diffracts from the second grating, which is oriented parallel to the first grating, the different parts of the pulse (with their correspondingly different wavelengths) will diffract at angles which yield a pulse whose parts are nearly in time synchronism. Peak power greatly increases, while total energy remains nearly the same.

PULSE STRETCHING

A pulse is sometimes stretched instead, in order to extract the maximum stored energy as well as reduce possible damage to optical components from excessive powers. This can be accomplished by using a pair of gratings in an "antiparallel" arrangement (see Figure 2). This works exactly opposite to the compression scheme in that the chirped pulse is spread out more by the gratings so that the resulting laser beam is longer in duration.

DISPERSION

The grating equation,

ml = d (sina + sinb), (1)

can be differentiated to give the angular spread (dispersion) of the spectrum:

. (1)

Here a and b are the angles of incidence and diffraction, m is the diffraction order, l is the wavelength and d is the groove spacing.


Figure 1 – Pulse compression using two gratings with the same groove frequency and efficiencies peaked for the polarization and wavelength of the laser. The damage threshold is about 200 to 300 mJ/cm2 for pulses of duration under 1 nsec.


Figure 2 – Pulse stretching. This arrangement of two identical gratings allows for lower peak power to be transmitted through the laser system, thereby increasing the amount of stored energy which can be extracted.


EFFICIENCY BEHAVIOR

The efficiency behavior of several typical gratings used for pulse compression and stretching are shown in the figures below.


Figure 3 – Efficiency curve: 1800 g/mm. [5138]. Red dashed curve: P-plane; solid black curve: S-plane.


Figure 4 – Efficiency curve: 1200 g/mm. [2917]. Red dashed curve: P-plane; solid black curve: S-plane.


Figure 5 – Efficiency curve: 600 g/mm. [MR131]. Red dashed curve: P-plane; solid black curve: S-plane.


Figure 6 – Efficiency curve: 316 g/mm. [1503]. Solid: 45° polarization.


ORDERING INFORMATION

Popular transmission grating sizes and prices are listed in the Diffraction Grating Catalog and Price Guide. Different specifications can be accommodated: please contact us for price quotations. Prices are subject to change without notice.

FOR FURTHER INFORMATION

For additional information, please contact us.

SOME TECHNICAL REFERENCES

  • A. Sullivan et al., "Multiterawatt 100-fs laser", Optics Letters 16, 1406-1408 (1991).
  • F. G. Patterson, R. Gonzales & M. D. Perry, "Compact 10-TW, 800-fs Nd:glass laser", Optics Letters 16, 107-1109 (1991).
  • D. Strickland & G. Mourou, Opt. Commun. 56, 219 (1985).
  • K. Yamakawa, C. Barty et al., "Generation of a High-Energy Picosecond Laser Pulse with a High-Contrast Ratio by CPA", IEEE JQE 27, (1991).
back to top

Newport Corporation
705 St. Paul Street, Rochester, New York 14605 USA
Telephone: (585) 248-4100, Fax: (585) 248-4111
E-mail: gratings@newport.com,
Web Site: http://gratings.newport.com

Founded in 1969, Newport is a pioneering single-source solutions provider of laser and photonics components to the leaders in scientific research, life and health sciences, microelectronics, industrial manufacturing, and homeland security markets.


Site Map Terms of Use Privacy Policy © Newport Corporation. All rights reserved
Site design and development by WinBiz, Inc.
Newport Home
Richardson Gratings Home
Product Tables                   >>
Supplemental Information  >>
How to Request a Quote...
New Products
Overstock
1: Plane Ruled Reflectance Gratings
2: Plane Holographic Reflectance Gratings
3: Concave Ruled Reflectance Gratings
4: Echelle Gratings
5: Large Astronomical Gratings
6: Plane Transmission Gratings - Visible
7: Plane Transmission Gratings - Ultraviolet
8: Gratings for Dye Laser Tuning
9: Molecular Laser Tuning Gratings
10: Concave Holographic Reflectance Gratings
11: Pulse Compression Gratings
12: Fiber Optic Telecommunication Gratings
13: UV / Vis Gratings
The Catalog Number System
Types of Diffraction Gratings
Special Requests & Custom Gratings
Grating Specifications
Grating Efficiency
Standard Tolerances
Certification & Warranty
Cleaning Gratings & Surface Defects
Standard Terms & Conditions of Sale
Addendum to Terms & Conditions of Sale
     – Master Gratings
Credit Application
Diffraction Grating Handbook
Technical Data                 >>
Technical Notes                >>
Publications
Our Capabilities
About Richardson Gratings
Reflectance Curves of Standard Coatings, UV-VIS-NIR
Epoxy Transmission Curves, UV-VIS-NIR
Refractive Index of Epoxies in the Visible Spectrum
Refractive Index of Epoxies in the Infrared Spectrum
Blaze Angle vs Blaze Wavelength curves (Littrow Angle)
1: Laser Tuning with Diffraction Gratings
2: Pulse Compression and Stretching with Diffraction Gratings
3: Concave Gratings
4: Transmission Gratings
5: Grisms
6: Echelle Gratings
7: The Blaze Arrow
8: Handling Gratings
9: Scattered Light and Stray Light
10: Guidelines for Specifying Diffraction Gratings
11: Determination of the Blaze Wavelength
12: Sources of Error in Monochromator-Mode Efficiency
      Measurements of Plane Diffraction Gratings
13: Measurement of Polarization-Dependent Loss (PDL)
      for Plane Diffraction Gratings
Main Sales Office
Worldwide Distributors
Information Request
Literature Request
Quotation Request
Catalog Request
Handbook Request
English
Simplified Chinese