In most laser micro-machining applications using copper vapour lasers, the system is configured for near-diffraction limited beam quality. This enables the beam to be tightly focussed to very small spot sizes and can be used for drilling very small holes or trepanning larger ones. The focused spot has a gaussian-like profile. In this paper a new laser system is presented that has a flat-top beam when focused. This has many advantages over gaussian beams when applied to percussion drilling and certain other applications. This system has demonstrated high speed percussion drilling of high quality 100 micron diameter holes in metals. We also report high speed (>200 holes/sec) percussion drilling in green sheet ceramic.

The new laser system is a compact copper vapour laser (CVL) master-oscillator power-amplifier (MOPA) incorporating telescopic beam expansion in a high-gain double-pass amplifier. By configuring an oscillator for low coherence output and using a multimode optical fibre between the oscillator and a double-pass amplifier, high power (up to 34W) low divergence output beams having well defined flat-top far field beam profiles have been produced. This scheme generates a flat-top far-field beam profile by control of the spatial coherence of a flat-top near-field beam rather than the usual techniques of producing flattened gaussian beams from coherent gaussian beams. The output of such a MOPA has also demonstrated high power (34W average power, 80kW peak power) damage-free transmission through 100 micron core diameter optical fibres. This is of significant interest to system integrators and for certain applications.

1.
D. W.
Coutts
, “Time resolved beam divergence form a copper vapour laser with unstable resonator,”
IEEE J. Quantum Electron.
, vol
31
, pp
330
342
,
1995
.
2.
B. E.
Warner
, “
Status of copper vapor laser technology at Lawrence Livermore National Laboratory
,”
Tech. Dig. Conf. Lasers Electro Optics
,
1991
, paper CFH4, pp.
516
518
.
3.
R. S.
Hargrove
,
R.
Grove
and
T.
Kan
, “
Copper vapor laser unstable resonator oscillator and oscillator-amplifier characteristics
,”
IEEE J. Quantum Electron.
, vol
QE-15
, pp
1228
1233
,
1979
.
4.
M.
Amit
,
S.
Lavi
,
G.
Erez
and
E.
Miron
, “
Temporal and spatial properties of an oscillator-amplifier copper vapor laser
,”
Optics Commun.
, vol
62
, pp.
110
1987
.
5.
V. V.
Zubov
,
N. A.
Lyabin
and
A. D.
Chursin
, “
Efficient master-oscillator-amplifier system ustilizing copper vapor laser active elements
,”
Sov. J. Quantum Electron.
, vol
16
, pp.
1606
1610
,
1986
.
6.
D. S.
Knowles
and
D. J. W.
Brown
, “
Compact 24-kHz copper-laser-pumped Ti-sapphire lasers
,”
Optics Letters
, vol.
20
pp.
569
571
,
1995
.
7.
M. J.
Withford
,
D. J. W.
Brown
,
R. J.
Carman
and
J. A.
Piper
, “
Enhanced performance of elemental copper-vapor lasers by use of H-2-HCl-Ne buffer-gas mixtures
,’
Optics Lett.
, vol.
23
, pp
706
708
,
1998
8.
M. J.
Withford
,
D. J. W.
Brown
,
R. J.
Carman
and
J. A.
Piper
, ‘Kinetically enhanced copper vapour lasers employing H-2-HCl-Ne buffer gas mixtures,’
Optics Commun.
, vol.
154
, pp.
160
166
,
1998
.
9.
J. A.
Hoffnagle
and
C. M.
Jefferson
, ‘Design and performance of a refractive optical system that converts a gaussian to a flattop beam,’
Appl. Optics
, vol.
30
, pp
5488
5499
,
2000
.
10.
F.
Gori
,
Flattened gaussian beams
,”
Opt. Commun.
vol.
107
pp.
335
341
,
1994
.
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