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Central to Hess and Klein's method is something called the Green's function. Lasers
concentrate light by trapping it within a cylinder of reactive semiconducting
material and bouncing it back and forth between mirrors placed at both ends. The
beam is amplified with each pass as photons -- the individual packets of light
energy -- induce atoms in the reactive material to emit photons that are clones of
the original; that is, they radiate at exactly the same frequency, energy, phase,
and direction. The extraordinary intensity of lasers owes to the uniformity of this
emission.
The majority of researchers designing VCSELs rely on analytical studies that
approximate the lasers' geometry and physics. While suitable for conceptual designs,
theoretical modelers such as Hess argue that these methods lack the precision
required for optimizing microtechnology.
But simulating laser behavior requires solving two complicated sets of
equations -- one for light (the optics) and the other for the behavior of
the electrical current that initiates lasing (the electronics). They must
be solved almost simultaneously so that the results from each set
continually feeds into the other. Sophisticated methods exist for modeling
the electronics. What remains to be tackled are the optics. "What makes
Karl's work unique," says Shun-Lien Chuang, an electrical engineering
professor at Illinois, "is that he's found an efficient way of combining
both."
Here's where the Green's function comes in. For most VCSEL models,
researchers place a computational mesh, or grid, over the entire laser
diode and define the field at each point on this matrix with a linear
relationship: the field at point A equals the field at point B plus the
field at point C, and so on. They then solve the resulting set of equations
to obtain a solution for the system at all of the points. When the
engineers are refining a laser design, their code races through the
calculations that generate the equations defining the mesh points. It slows
to a grind, though, when it has to actually solve these equations. This
must be done simultaneously, with the computer's processors exchanging data
back and forth about the state of these millions of equations. This is the
step that takes 12 hours. And that is assuming the data are a constant for
the electronically conducting portion of the equation. If they calculate
this portion as well, they're up to 600 hours.
  
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