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Introduction
Chapter
1: Introduction to Machining with Lasers
Chapter
2: Time Scales
Chapter
3: Machining with Long Pulses
Chapter
4: Nanosecond Machined Samples
Chapter
5: Machining with Ultrafast Laser Pulses
Chapter
6: Femtosecond Machined Samples
Chapter
7: Contamination, Debris, Etc.
Chapter
8: Heat Affected Zone (HAZ)
Chapter
9: Machining Accuracy
Chapter
10: Sub-micron Features
Chapter
11: Machining Inside Bulk Materials
Chapter
12: Introduction to Waveguides
Chapter
13: Active Waveguides
Chapter
14: Shortcomings of Femtosecond Lasers
Chapter
15: Materials We've Machined
Chapter
16: Conclusion
Appendices:
References
and Glossary |
Machining
with Ultrafast Laser Pulses
Short
Pulse Machining Examples
This
chapter is concerned with the ablation of matter with ultrafast
laser pulses. The most fundamental feature of laser-matter
interaction in the very fast pulse regime is that the heat
deposited by the laser into the material does not have time
to move away from the work spot during the time the laser
pulse is illuminating the material. The duration of the laser
pulse is shorter than the heat diffusion time. This is a very
unusual and very desirable regime, which can be reached only
with ultrafast lasers.
This
regime has numerous advantages as illustrated in Figure 5.1.
- Because
the energy does not have the time to diffuse away, the efficiency
of the machining process is high. If you remember the analogy
we made in Chapter 3, this is similar to filling a bucket
with no holes! The laser energy has nowhere to go (or more
precisely does not have the time to move away). It just
piles up at the level of the working spot, whose temperature
rises instantly past the melting point of the material and
goes, very quickly, well beyond even the evaporation point.
In fact, the temperature keeps on climbing into what is
called the plasma regime. This may seem strange. It is certainly
not a common experience. How can this happen?
- Femtosecond
lasers, like our model CPA-2101, deliver an incredible amount
of peak power. These systems routinely deliver 5 to 10 Gigawatts
of peak power (this is more than the average power delivered
by a large nuclear plant).The laser intensity easily reaches
the hundreds of Terawatts per square centimeter range at
the work spot. Absolutely, positively nothing else that
is man-made gets anywhere close to this power density.
- No
materials can withstand the forces at work at these power
densities. This means that with ultrafast laser pulses we
can machine very hard materials, as well as materials with
extremely high melting points such as Molybdenum, Rhenium,
etc.
Figure
5.1: Ultrafast Pulse Laser-Matter Interaction |
| You
will notice that this figure is much simpler than Figure
3.1, and there is a good reason for this. Physical processes
like heat conduction, etc. don't have time to leach energy
away from the process of plasma formation and subsequent
material ejection. |
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with short-pulse lasers.
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What
else does this lack of thermal diffusion do to the machining
process?
- After
the ultrafast laser pulse creates the plasma in the surface
of the material, the pressures created by the forces within
it cause the material to expand outward from the surface
in a highly energetic plume or gas. The internal forces
that previously held the material together are vastly
insufficient to contain this expansion of highly ionized
atoms (physicists call these charged atoms "ions")
and electrons from the surface. Because the electrons
are lighter and more energetic than the ions, they come
off the material first, followed later by the ions. And
because the ions all have some positive charge, they repel
each other as they expand away from the material. Consequently,
there are no droplets that condense onto the surrounding
material. Additionally, since there is no melt phase,
there is no splattering of material onto the surrounding
surface.
Micromachining
with femtosecond pulses offer some additional advantages
as shown in subsequent chapters.
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