Michael Burns - Associate Director for Science
Over the years I've participated in a number of, to me, fascinating projects,
most of them at the Rowland Institute. I have found no particular common thread other than simple
curiosity coupled with an opportunity to indulge that curiosity. Some of the more interesting
ones are described below.
Electromigration in single crystal copper
In a metal conducting a current the electrons, in the process of colliding with
the atoms in the lattice, can actually knock the atoms out of their lattice positions. Since the
electrons are all flowing in one direction, there can be a net movement of atoms in the wire. At high
enough current densities this can lead to a measurable macroscopic movement of the metal along
the wire (one mode of failure in modern integrated circuits). We are studying some of the effects of
surface electromigration in thin single crystal copper wires in an effort to better understand the
electromigration process itself. Copper is a particularly interesting metal in this regards technologically
since the most recent semiconductor processes have moved from using aluminum interconnects to
using copper. Understanding (and controlling) electromigration is necessary for successful use of
copper in this new role.
Single crystal metal whiskers
To observe the binding of cold atoms around a wire (described below), we needed
a long, thin wire. One potential method for producing such a wire is to use an old technique of growing
metallic single crystal metal whiskers. Although it is surprisingly easy to grow forests of these whiskers
in a rather uncontrolled fashion, it is a much more difficult problem to grow them on demand, at a
certain location, with a particular crystal orientation. Although the wires needed for the atom-orbits are
now being produced by other methods, the technique of metal whisker growth is still being pursued.
One reason is that single crystal iron whiskers produced by this technique look like they can be used
as the tip in an STM (scanning-tunneling microscope), perhaps as a source and/or detector of spin
polarized electrons. This would be of great interest in the emerging field of spintronics. Additionally
they are the source of the wires in the electromigration experiments described above.
Atoms orbiting a wire
This project is an exploration of the binding of neutral atoms in stable orbits around
a wire charged by a time-varying sinusoidal voltage. Both classical and quantum-mechanical theories for
this system have been studied and a unified approach to the Kapitza picture of effective potentials
associated with high-frequency fields produced. It appears that cavities and waveguides for neutral atomic
matter waves may be constructed using these principles. [Phys. Rev. A, 45, 6468, (1992)]
One may also bind a magnetic atom to a current in a wire through the interaction
between the atomic dipole moment and the wire's magnetic field. The theoretical description is based on
an extension of the concept of supersymmetry to multi-component wave functions. An analytic solution
for spin 1/2 particles can be obtained directly in coordinate space. Experimentally, the system should be
realizable for 25 micro-Kelvin sodium atoms around a wire with a diameter of 0.5 microns and a current
of 400 micro-amps. [Phys. Rev. Lett. 74,3138 (1995)]
Spin 1 particles present more of a problem theoretically. We have found bound states
via numerical and approximate analytic results, and have calculated the decay due to various effects,
which bodes well for experimental realizations. Theoretically the supersymmetry method that was so
successful in the spin 1/2 state is only approximate for the spin 1 state. The eigenvalues are not degenerate
in the angular quantum number, but they almost are. This presents an interesting, unanswered, question:
what is the small physical parameter responsible for the small breaking of the symmetry, which we observe
in the numerically computed energy eigenvalues? [Phys. Rev. A, 53, 1653, (1996)]
Optical Matter
Properly fashioned electromagnetic fields coupled to microscopic dielectric objects can
be used to create arrays of extended crystalline and noncrystalline structures. Organization can be achieved
in two ways: In the first, dielectric matter moves in direct response to the externally applied standing wave
optical fields. In the second, the external optical fields induce interactions between dielectric objects that
can also result in the creation of complex structures. In either case, these new ordered structures, whose
existence depends on the presence of both light and polarizable matter, are referred to as optical matter.
[Science, 249, 749 (1990)]
The interactions in the second group are formed by the significant forces between
dielectric objects induced by intense optical fields. These forces are very long range (the forces decay only
as 1/r) and oscillate in sign at the optical wavelength. We performed an experiment that demonstrates the
simplest case by observing a series of bound states between two 1.43 micron diameter plastic spheres in
water. The application to more complex cases (with more spheres) is not currently understood: naive
integration of the 1/r forces leads to infinities, which in practice must somehow saturate. It is not known,
for example, what the ground-state equilibrium configuration is and hence we do not yet even know what
optical matter formed in this fashion would look like. [Phys. Rev. Lett., 63, 1233 (1989)]
Human Vision
Human vision has the remarkable property that, over a wide range, changes in the
wavelength composition of the source light illuminating a scene result in very little change in the color of
any of the objects. Computations for the color perception of an object depend on knowing more than the
amount of light from a point on that object (as in Dr. Land's retinex theory, for example); hence long-range
interactions of neural signals is necessary. It was not clear whether these long-range interactions take place
right in the retina or further along the pathway in the cortex. We tested the role of the cortex in a human
subject in whom the nerve fibers connecting cortical areas subserving two separate parts of the visual field
had been severed, and found that the cortex is necessary for long-range color computations.
[Nature, 303, 616 (1983)]
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