Gas discharge laser electrode with reduced sensitivity to...

Coherent light generators – Particular active media – Gas

Reexamination Certificate

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C372S058000

Reexamination Certificate

active

06363094

ABSTRACT:

BACKGROUND OF THE INVENTION
The principal components of a prior art KrF excimer laser chambers are shown in FIG.
1
. This chamber is a part of a laser system used as a light source for integrated circuit lithography. These components include a chamber housing
2
. The housing contains two electrodes cathode
84
and anode
83
each about 55 cm long and spaced apart by about 20 mm, a blower
4
for circulating a laser gas between the electrodes at velocities fast enough to clear (from a discharge region between the two electrodes) debris from one pulse prior to the next succeeding pulse at a pulse repetition rate in the range of 1000 Hz or greater. (Gas velocities of about 10 m/s for each 1000 Hz pulse rate is typical.) The chamber includes a water cooled finned heat exchanger
6
for removing heat added to the laser gas by the fan and by electric discharges between the electrodes. Blower
4
is typically a squirrel cage type tangential fan providing high gas flow but at relatively low differential pressure. The chamber may also include baffles
60
and
64
and vanes
66
and
68
for improving reducing discharge caused acoustic effects and the aerodynamic geometry of the chamber. The laser gas is comprised of a mixture of about 0.1 percent fluorine, about 1.0 percent krypton and the rest neon. Each pulse is produced by applying a very high voltage potential across the electrodes with a pulse power supply which causes a discharge between the electrodes lasting about 30 nanoseconds to produce a gain region about 20 mm high, 3 mm wide and 525 mm long. (Two capacitors of a peaking capacitor bank are shown at
62
.) The discharge deposits about 2.5 J of energy into the gain region. As shown in
FIG. 2
, lasing is produced in a resonant cavity, defined by an output coupler
20
and a grating based line narrowing unit (called a line narrowing package or LNP, shown disproportionately large)
22
comprising a three prism beam expander, a tuning mirror and a grating disposed in a Littrow configuration. The energy of the output pulse
3
in this prior art KrF lithography laser is typically about 10 mJ.
FIG. 3
shows an enlarged view of cathode
84
and anode
83
. Each is about 3 cm wide but the discharge region
85
is only about 3 to 4 mm wide. The direction of gas flow is shown at
86
and a gas flow of 20 m/s is indicated. The cathode and anode are typically brass. The cathode is typically slidingly mounted on an insulator
84
a
and the anode is typically mounted on a metal support
83
A.
These KrF lithography lasers typically operate in bursts of pulses at pulse rates of about 1000 to 4000 Hz. Each burst consists of a number of pulses, for example, about 80 pulses, one burst illuminating a single die section on a wafer with the bursts separated by down times of a fraction of a second while the lithography machine shifts the illumination between die sections. There is another down time of a few seconds when a new wafer is loaded. Therefore, in production, for example, a 2000 Hz, KrF excimer laser may operate at a duty factor of about 30 percent. The operation is 24 hours per day, seven days per week, 52 weeks per year. A laser operating at 2000 Hz “around the clock” at a 30 percent duty factor will accumulate more than 1.5 billion pulses per month. Any disruption of production can be extremely expensive. For these reasons, prior art excimer lasers designed for the lithography industry are modular so that maintenance down time is minimized.
Maintaining high quality of the laser beam produced by these lasers is very important because the lithography systems in which these laser light sources are used are currently required to produce integrated circuits with features smaller than 0.25 microns and feature sizes get smaller each year. Laser beam specifications limit the variation in individual pulse energy, the variation of the integrated energy of series of pulses, the variation of the laser wavelength and the magnitude of the bandwidth of the laser beam.
Typical operation of electric discharge laser chambers such as that depicted in
FIG. 1
causes electrode erosion. Erosion of these electrodes affects the shape of the discharge which in turn affects the quality of the output beam as well as the laser efficiency. Typically, anode erosion in these excimer lasers is two to three times as severe as cathode erosion.
Electrode designs have been proposed which are intended to minimize the effects of erosion by providing on the electrode a protruding part having the same width as the discharge. Some examples are described in Japanese Patent No. 2631607. These designs allow erosion to occur without substantially affecting electric fields.
What is needed is a gas discharge laser having electrodes with reduced erosion rates.
SUMMARY OF THE INVENTION
The present invention provides a long life laser chamber for a halogen containing gas discharge laser. In a preferred embodiment electrode erosion caused by excited fluorine (i.e., atomic fluorine and fluorine ions) is reduced by forcing the excited fluorine away from the discharge footprint of the electrodes. Preferred embodiments include electrodes with a large number of small holes in the discharge footprint through which laser gas flows to remove the excited fluorine from the footprint region in the time period between electric discharges.


REFERENCES:
patent: 4414488 (1983-11-01), Hoffmann et al.
patent: 4546482 (1985-10-01), Bagaglia et al.
patent: 4686682 (1987-08-01), Haruta et al.
patent: 4703490 (1987-10-01), Brumme et al.
patent: 4774714 (1988-09-01), Javan
patent: 4876693 (1989-10-01), Lucero et al.
patent: 4959840 (1990-09-01), Akins et al.
patent: 5070513 (1991-12-01), Letardi
patent: 5535233 (1996-07-01), Mizoguchi et al.
patent: 5557629 (1996-09-01), Mizoguchi et al.
patent: 5771258 (1998-06-01), Morton et al.
patent: 6018537 (2000-01-01), Hofmann et al.
patent: 6128323 (2000-10-01), Myers et al.
patent: 2631607 (1997-07-01), None

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