Method of laser marking a body of material having a thermal conductivity approximately equal to that of glass

• US 5,767,483 A
• Filed: 07/01/1996
• Issued: 06/16/1998
• Est. Priority Date: 08/19/1993
• Status: Expired due to Fees

• Current Assignee: United Distillers PLC
• Original Assignee: United Distillers PLC
• Inventors: Cameron, Allan, Stockdale, Mary Violet, Jeffree, Christopher Edward, Clement, Robert Marc, Ledger, Neville Richard
• Primary Examiner(s): Walberg, Teresa J.
• Assistant Examiner(s): Mills, Gregory L.
• Application Number:
  US08/602,734
• Time in Patent Office: 715 Days
• Field of Search: 219/121.6, 219/121.68, 219/121.69, 219/121.78, 219/121.8, 219/121.85, 347/224, 347/225, 347/260, 250/492.1, 204/157.41, 204/157.44, 264/482
• US Class Current: 219/121.85
• CPC Class Codes: B41M 3/14 Security printing securities B42D25/29
• CPC Class Codes: B41M 5/262 recording or marking of inorganic surfaces or materials, e.g. glass, metal, or ceramics marking of plastic artifacts with inorganic additives B41M5/267
• CPC Class Codes: B41M 5/267 Marking of plastic artifacts, e.g. with laser

Abstract

A method of providing a body of material (14), having a thermal conductivity approximately equal to that of glass, with a sub-surface mark. A beam of laser radiation (12) to which the material (14) is substantially opaque is directed to surface of the body, so as to cause beam energy to be aborbed at the surface of the material in an amount sufficient to produce localised stresses within the body (14) at a location spaced from the surface without any detectable change at the surface, the localised stresses thus produced being normally invisible to the naked eye but capable of being rendered visible under polarised light.

Claims

1. A method of providing a body of material having thermal conductivity approximately equal to that of glass with a sub-surface mark, said method comprising directing at a surface of the body a beam of laser radiation to which the material is substantially opaque, so as to cause beam energy to be absorbed at the surface of the material in an amount sufficient to produce localised stresses within the body at a location spaced from said surface without any detectable change at said surface, the localised stresses thus produced being normally invisible to the naked eye but capable of being rendered visible under polarized light.

2. A method in accordance with claim 1, wherein the mark created by the localised stresses is representative of one or more numerals, letters or symbols or a combination thereof.

3. A method in accordance with claim 1, wherein the beam of laser radiation is concentrated so as to form an illuminated spot at a location on the surface of the body, the spot being moveable relative to the body to be marked thereby enabling the mark created by the localised stresses to be of a predetermined shape.

4. A method in accordance with claim 3, wherein the spot is moved relative to the body to be marked in such a way as to produce an elongate region of localised stresses that when rendered visible under polarized light has the appearance of a line.

5. A method in accordance with claim 3, wherein the spot is moved relative to the body to be marked in such a way as to produce a series of spaced apart regions of localised stresses that when rendered visible under polarized light has the appearance of a series of dots.

6. A method in accordance with claim 5, wherein the series of spaced apart regions of localised stresses are formed by moving the spot at a constant speed relative to the body to be marked and periodically varying the power density of the beam.

7. A method in accordance with claim 5, wherein the series of spaced apart regions of localised stresses are formed by maintaining the power density of the beam substantially constant and varying the time the spot is used to illuminate successive locations on the surface.

8. A method in accordance with claim 7, wherein the spot is moved relative to the body to be marked at a speed that varies periodically between zero and 3 m/s.

9. A method in accordance with claim 8, wherein the spot is moved relative to the body to be marked at an average speed in the range from 2 to 3 m/s.

10. A method in accordance with any of claim 5, wherein the beam energy absorbed at successive locations on the surface varies smoothly from one location to the next.

11. A method in accordance with any of claim 3, wherein the laser radiation has a power density at the spot of up to 10 kw/cm².

12. A method in accordance with claim 1, wherein the beam of laser radiation is caused to illuminate a mask placed in front of the body to be marked, the mask having one or more apertures thereby enabling the mark created by the localised stresses to be of a predetermined shape.

13. A method in accordance with claim 1, wherein the beam of laser radiation is generated by a CO₂ laser.

14. A method of providing a body of glass with a subsurface mark, comprising directing at a surface of the glass body a beam of laser radiation to which the glass is substantially opaque, so as to cause beam energy to be absorbed at the surface of the glass body in an amount sufficient to produce localised stresses within the glass body at a location spaced from said surface without any detectable change at said surface, the localised stresses thus produced being normally invisible to the naked eye but capable of being rendered visible under polarised light.

15. A method of providing a body of plastics material with a sub-surface mark, the plastics material having a thermal conductivity approximately equal to that of glass, said method comprising directing at a surface of the body a beam of laser radiation to which the plastics material is substantially opaque, so as to cause beam energy to be absorbed at the surface of the body in an amount sufficient to produce localised stresses within the body at a location spaced from said surface without any detectable change at said surface, the localised stresses thus produced being normally invisible to the naked eye but capable of being rendered visible under polarised light.