Method and apparatus for shaping electromagnetic beams

• US 4,410,237 A
• Filed: 09/26/1980
• Issued: 10/18/1983
• Est. Priority Date: 09/26/1980
• Status: Expired due to Term

• Current Assignee: Massachusetts Institute of Technology
• Original Assignee: Massachusetts Institute of Technology
• Inventors: Veldkamp, Wilfrid B.
• Primary Examiner(s): Arnold, Bruce Y.
• Application Number:
  US06/191,006
• Time in Patent Office: 1,117 Days
• Field of Search: 350/162.17, 350/162.18, 350/162.2, 350/162.23, 350/162.24, 350/320
• US Class Current: 359/572
• CPC Class Codes: G02B 27/09 Beam shaping, e.g. changing the cross-sectional area, not otherwise provided for adapting the beam shape of a laser diode G02B19/0052; adapting the beam shape of an LED G02B19/0061; coupling into light guides using intermediate optical elements G02B6/4204; beam shaping specially adapted for lasers H01S3/005
• CPC Class Codes: G02B 27/0927 Systems for changing the beam intensity distribution, e.g. Gaussian to top-hat
• CPC Class Codes: G02B 27/0944 Diffractive optical elements, e.g. gratings, holograms gratings per se G02B5/18; holograms used as optical elements per se G02B5/32
• CPC Class Codes: G02B 27/0972 Prisms prisms per se G02B5/04
• CPC Class Codes: G02B 5/1871 Transmissive phase gratings
• CPC Class Codes: Y10S 359/90 Methods

Abstract

The intensity profile of a beam of electromagnetic waves such as a laser beam is shaped by means of a diffraction grating and/or prism in the beam path. In one embodiment, beams exhibiting Gaussian energy intensity profiles undergo an energy redistribution to approximately uniform profiles. A reflective or transmissive surface relief grating is employed with phase steps generally periodic except at the pattern center where a pattern phase reversal occurs. Prisms are cut and oriented relative to the incoming beam to operate at the Brewster'"'"'s angle for compressing or expanding the beam with minimum losses.

Claims

1. A method of shaping the intensity profile of a beam of electromagnetic waves comprising:

positioning a diffraction grating having a centrally symmetric grating pattern in the optical path of the beam, the grating pattern itself having a generally central phase reversal transverse to the axis of the beam.

2. A method as claimed in claim 1 wherein the grating is a surface relief phase grating.

3. A method as claimed in claim 2 wherein the grating is a binary grating.

5. A method as claimed in claim 1 or 4 further comprising positioning at least one beam compression prism in the optical path of the beam, each prism being cut and oriented relative to the incoming beam to operate at about the Brewster'"'"'s angle.

6. A method as claimed in claim 1 or 4 wherein the grating is a reflective grating.

7. A method as claimed in claim 1 or 4 wherein the grating is a transmissive grating.

8. A method as claimed in claim 1 or 4 wherein the electromagnetic beam is a light beam.

9. A method as claimed in claim 8 wherein the light beam is generated by a laser and initially has a Gaussian intensity profile.

10. A method as claimed in claim 1 or 4 wherein the grating is a linear grating.

11. A method as claimed in claim 1 or 4 wherein a beam having a Gaussian intensity profile is reshaped to provide a beam having a more uniform intensity thereacross.

12. A method as claimed in claim 1 or 4 in which the beam having the reshaped intensity profile is used in a radar system.

13. A method as claimed in claim 1 or 4 in which the beam having the reshaped intensity profile is used in heat treatment of a material.

14. A method as claimed in claim 12 wherein the beam is used in annealing semiconductor material.

15. A method as claimed in claim 12 wherein the beam is used in the surface treatment of metals.

4. A method of shaping the intensity profile of an electromagnetic beam by reflecting said beam off, or transmitting said beam through, a surface relief grating, said grating having a coded surface relief pattern composed of many spaced binary phase steps of height h, where h is chosen to provide an incremental wavelength path difference related to the wavelength of the light in the laser beam whose intensity profile is shaped, the spacing between said spaced binary phase steps being periodic except at the surface relief pattern center where a surface relief pattern phase reversal occurs such that the center phase step has a width twice the width of other phase steps in the pattern, the periodicity of the binary phase steps being determined on the basis of the width, divergence and wavelength of the original beam and the required profile of the beam after processing by the grating.