Information Further information is available at the Royal Swedish Academy of Sciences, Information Department, Box 50005, SE104 05 Stockholm, Sweden Phone: +46 8 673 95 25, Fax: +46 8 15 56 70 Email: info@kva.se, Website: www.kva.se This press release is also available in Swedish 
The Royal Swedish Academy of Sciences has awarded Professor Robert B. Laughlin, Stanford University, California,
USA, The three researchers are being awarded the Nobel Prize for discovering that electrons acting together in strong magnetic fields can form new types of "particles", with charges that are fractions of electron charges. Citation:
Horst L. Störmer and Daniel C. Tsui made the discovery
in 1982 in an experiment using extremely powerful magnetic fields and
low temperatures. Within a year of the discovery Robert B. Laughlin
had succeeded in explaining their result. Through theoretical analysis
he showed that the electrons in a powerful magnetic field can condense
to form a kind of quantum fluid related to the quantum fluids that
occur in superconductivity and in liquid helium. What makes these fluids
particularly important for researchers is that events in a drop of quantum
fluid can afford more profound insights into the general inner structure
and dynamics of matter. The contributions of the three laureates have
thus led to yet another breakthrough in our understanding of quantum
physics and to the development of new theoretical concepts of significance
in many branches of modern physics.
Quantum effects become visible As a young student in 1879 Edwin H. Hall discovered an unexpected phenomenon.
He found that if a thin gold plate is placed in a magnetic field at right
angles to its surface an electric current flowing along the plate can
cause a potential drop at right angles both to the current and the magnetic
field (see figure 1). Termed the Hall effect, this takes place
because electrically charged particles (in this case electrons) moving
in a magnetic field are influenced by a force and deflect laterally. The
Hall effect can be used to determine the density of charge carriers (negative
electrons or positive holes) in conductors and semiconductors, and has
become a standard tool in physics laboratories the world over.
Fig. 1. A voltage V drives a current I in the positive x direction. Normal Ohmic resistance is V / I. A magnetic field in the positive z direction shifts positive charge carriers in the negative y direction. This generates a Hall potential ( V_{H }) and a Hall resistance (V_{H }/ I ) in the y direction. (Kosmos 1986) Hall performed his experiments at room temperature and with moderate magnetic fields of less than one tesla (T). At the end of the 1970's researchers used extremely low temperatures (only a few degrees from absolute zero, i.e. around 272°C) and very powerful magnetic fields (max approx. 30 T). They studied the Hall effect in the type of semiconductor design used in the electronics industry for manufacturing lownoise transistors. The material contains electrons which, though trapped close to an internal surface, separating two distinct parts of the material, are highly mobile along the surface. In such a layer at low temperatures electrons can be caused to move as if on a plane surface, i.e. in two dimensions only. This geometrical limitation leads to many unexpected effects. One is that the Hall effect changes character. This is seen most simply when one measures how the Hall resistance varies with the strength of the applied magnetic field. In 1980 the German physicist Klaus von Klitzing discovered in a similar
experiment that the Hall resistance does not vary in linear fashion, but
"stepwise" with the strength of the magnetic field (see figure
2). The steps occur at resistance values that do not depend on the properties
of the material but are given by a combination of fundamental physical
constants divided by an integer. We say that the resistance is quantized.
At quantized Hall resistance values, normal Ohmic resistance disappears
and the material becomes in a sense superconducting.
Fig. 2. The Hall resistance varies stepwise with changes in magnetic field B. Step height is given by the physical constant h/e^{2} ( value approximately 25 kiloohm ) divided by an integer i. The figure shows steps for i =2,3,4,5,6,8 and 10. The effect has given rise to a new international standard for resistance. Since 1990 this has been represented by the unit 1 klitzing, defined as the Hall resistance at the fourth step ( h/4e^{2} ). The lower peaked curve represents the Ohmic resistance, which disappears at each step. (Kosmos 1986) For his discovery of what is termed the integer quantum Hall effect von Klitzing received the Nobel Prize in Physics in 1985. The effect may be understood if one accepts the laws of quantum physics for how individual electrons behave in powerful magnetic fields. In simple terms, the electrons move only in certain circular paths, the basic sizes of which are determined by the magnetic field. The various steps turn out to show how many of the smallest paths are entirely full of electrons. In their refined experimental studies of the quantum Hall effect, using
among other things lower temperatures and more powerful magnetic fields,
Störmer, Tsui and their coworkers found to their great surprise
a new step in the Hall resistance which was three times higher than von
Klitzing's highest. They subsequently found more and more new steps, both
above and between the integers. All the new step heights can be expressed
with the same constant as earlier but now divided by different fractions.
For this reason the new discovery was named the fractional quantum
Hall effect. It posed a great mystery for the researchers who could
not explain how the new steps came about.
A new type of quantum fluid A year after the discovery of the fractional quantum Hall effect, Laughlin offered a theoretical explanation. According to his theory the low temperature and the powerful magnetic field compel the electron gas to condense to form a new type of quantum fluid. Since electrons are most reluctant to condense (they are what is termed fermions) they first, in a sense, combine with the "flux quanta" of the magnetic field. Particularly for the first steps discovered by Störmer and Tsui, the electrons each capture three flux quanta, thus forming a kind of composite particle with no objection to condensing (they become what is termed bosons). Quantum fluids have earlier occurred at very low temperatures in liquid helium (1962 Nobel Prize to Landau; 1978 to Kapitsa; 1996 to Lee, Osheroff and Richardson) and in superconductors (1913 Nobel prize to Kamerlingh Onnes; 1972 to Bardeen, Cooper and Schrieffer; 1987 to Bednorz and Müller). Quantum fluids have certain properties in common, e.g. superfluidity, but they also show important differences in behaviour. Some, like Laughlin's fluid, consist of composite particles. Apart from its superfluidity, which explains the disappearance of Ohmic
resistance at the Hall resistance steps, the new quantum fluid proposed
by Laughlin has many unusual properties. One of the most remarkable is
that if one electron is added the fluid will be affected (excited)
and a number of fractionally charged "quasiparticles"
created. These quasiparticles are not particles in the normal sense but
a result of the common dance of electrons in the quantum fluid. Laughlin
was the first to demonstrate that the quasiparticles have precisely the
correct fractional charge to explain Störmer's and Tsui's results.
Subsequent measurements have demonstrated more and more fractionally charged
steps in the Hall effect (see figure 3), and Laughlin's quantum fluid
has proved capable of explaining all the steps found experimentally.
Fig. 3. The dashed diagonal line represents the classical Hall resistance and the full drawn diagonal stepped curve the experimental results. The magnetic fields causing the steps are marked with arrows. Note particularly the step first discovered by Störmer and Tsui (1/3) at the highest value of the magnetic field and the steps earlier discovered by von Klitzing (integers) with a weaker magnetic field. (Science 1990)
Direct demonstration of quasiparticles The discovery and the explanation of the fractional quantum Hall effect in 198283 may be said to represent an indirect demonstration of the new quantum fluid and its fractionally charged quasiparticles. Several research groups have recently succeeded in observing these new particles directly (see reference list). This has for instance taken place in experiments where very small variations in a current have been ascribable to individual quasiparticles flowing through the circuit. These measurements, comparable to distinguishing the sound of individual hailstones during a hailstorm and determining that they are only a fraction of their normal size, were made possible by the astonishing development of microelectronics since this year's three laureates made their pioneering contributions. The measurements may be viewed as the conclusive verification of their discoveries. ***** Further reading Additional background material on the Nobel Prize in Physics 1998,
below Splitting the electron, by B. Daviss, New Scientist, 31 January
1998, p.36. *****
Professor Robert B. Laughlin
Horst L. Störmer Professor Horst L. Störmer
Professor Daniel C. Tsui


Additional background information on the Nobel Prize in Physics 1998. NOTE! If the above link doesn't work, the reason could be that you don't have the program Acrobat Reader. This program is free and can be downloaded from Adobe's website by clicking on the button below. 
