In the last post, we
learnt that the uncertainty principle means that for microscopic systems, we
cannot say for certain what exactly will happen when one thing affects another:
all we can say is that there is a certain probability that an outcome will occur.
Although this may seem like a backward step from classical physics, where we
can say with absolute certainty what will happen, quantum physics is the only
accurate model we have for predicting the outcomes of quantum systems. However,
the probabilities we do calculate do translate into real life, and thus the
technologies built on them can perform in ways that would be impossible under
the laws of classical physics, giving these new technologies huge advantages
over older technologies.
Consider throwing a ball
straight up into the air: it rises, reaches a definite apex where it's vertical
velocity is zero, and then falls back down. Now, imagine that instead of a
macroscopic ball, we're dealing with a microscopic particle. As we've already
discussed, it's impossible to tell the exact position of our particle at any
time: so what does this mean for the "flight" of our particle? It
means that it's impossible to tell when the particle reaches any sort of
"apex", be it the natural limit to its movement through space, some
sort of barrier, or a gap between materials. More importantly, the uncertainty
principle means that there's is even some probability that the particle will
pass on even further! This probability decreases the further the
particle moves past the point it should, and quickly drops toward zero, meaning
that it is unlikely to see particles passing through metres of concrete, for
example. This phenomena is is known as "quantum tunnelling" and is
one of the most useful practical applications of the Uncertainty
Principle.
The scanning tunnelling
microscope (STM) is the most direct application of quantum tunnelling in
technology. It uses the ability of an electron current to tunnel to image
surfaces of materials right down to the individual atoms that make it up. It
was first invented in 1981 by IBM Zurich, and has since become absolutely
essential to anyone studying the atomic structure of solid materials,
physicists, biologists and nanotechnologists included.
The STM works by passing
a very small current round a metal needle which is then moved over the surface
of a sample. The metal needle at its tip is only one atom thick. The
metal tip is held at around 5 nanometres, 0.000000005m, from the surface,
meaning that mathematically, the wavefunctions of the electrons in the current
flowing around the metal needle and the electrons in the surface overlap and
because the metal tip is held at a different voltage to the surface of the
material, the electrons in the current begin to tunnel across at a rate
proportional to the distance between the metal tip and the surface of the
material. This flow of electrons across the gap creates a tiny current which
can be amplified and then measured. The smaller the distance between the metal
tip and the surface, the more electrons will tunnel across the gap and the
larger the current will be. The tunnelling current is incredibly sensitive to
even tiny changes in distance, so even the difference between one atom and the
next can be detected. Creating an image with an STM is analogous to taking a
rubbing of a tree bark: the places where there are ridges in the bark give you
darker lines, like how places where the atoms are closer to the metal tip will
give you higher currents. Using a computer and a current amplifier, it’s
possible to interpret the values of current measured and build up an image of
the surface of the material.
STMs have helped to
revolutionise the way scientists in a variety of fields work when studying
microscopic structures. For example, before the invention of the STM, if a
chemist wanted to learn about what chemicals work with what catalysts, they
would have to go through a trial and error type experiment, simply trying to
fit “keys in locks”, as it were. However, by using an STM, chemists can now
image and study the actual active sites of the catalysts and other chemicals,
and fit them together without having to go through the trial and error
process. Furthermore, by taking advantage of the fact that an STM is
not limited to just vacuums and can function in any atmosphere at a large range
of temperatures, it is possible to watch these chemical reactions occur in real
time at a molecular level. This allows us to build a much greater understanding of the processes
involved. The STM has also been used to study strands of DNA to help us
understand the behaviour of genetic material in more detail, which could lead
to the development of new medicines to treat genetic diseases.
However, the STM isn’t
perfect. It can only provide a view of the first layer or so of a material, as
“the experimental ‘‘image’’ is relatively insensitive to the positions of atoms
beyond the first atomic layer”. It also requires the material to be an electrical
conductor, which limits the numbers of materials it can be used to scan.
It also requires the material to be extremely stable and clean, the tip
of metal point to be very sharp, the sample to be isolated from any external
vibrations, and sophisticated electronics. These requirements can make using an
STM a challenging and expensive process.
Another month, another blog post. I should really do these more regularly. This one was going to be part of my EP, but I had to scrap it as my question wasn't really suitable for the qualification, as there's not enough debate in the discussion of -how- an effect is used. I didn't want to waste all the research I've done, so I'm going to slowly adapt my dissertation into a number of posts.
Thanks for reading as always,
GM ^^