Qualitative insight into the properties of a quantum-mechanical system
can be gained from the study of the relationship between the system's
classical newtonian dynamics, and its quantum dynamics as described b
y the Schrodinger equation. The Bohr-Sommerfeld quantization scheme--w
hich underlies the historically important Bohr model for hydrogen-like
atoms--describes the relationship between the classical and quantum-m
echanical regimes, but only for systems with stable, periodic or quasi
periodic orbits'. Only recently has progress been made in understandin
g the quantization of systems that exhibit non-periodic, chaotic motio
n. The spectra of quantized energy levels for such systems are irregul
ar, and show fluctuations associated with unstable periodic orbits of
the corresponding classical system(1-3). These orbits appear as 'scars
'-concentrations of probability amplitude--in the wavefunction of the
system(4). Although wavefunction scarring has been the subject of exte
nsive theoretical investigation(5-10), it has not hitherto been observ
ed experimentally in a quantum system. Here we use tunnel-current spec
troscopy to map the quantum-mechanical energy levels of an electron co
nfined in a semiconductor quantum well in a high magnetic held(10-13).
We find clear experimental evidence for wavefunction scarring, in ful
l agreement with theoretical predictions(10).