Scanning Tunnelling Microscope (STM)

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SUMMARY

The Scanning Tunnelling Microscope (STM) is a powerful tool that probes the density of states (DOS) of materials by measuring the tunnelling current between its probe tip and the surface being scanned. This current is proportional to the tunnelling probability, which is influenced by the density of states at a specific bias voltage. The STM performs spectroscopy rather than imaging, generating an I vs. V curve where the density of states is represented by the derivative of this curve (dI/dV vs. V). Understanding the density of states is crucial, as it reflects how closely packed the energy levels are within a solid, distinguishing it from isolated atomic behavior.

PREREQUISITES
  • Understanding of quantum mechanics and solid-state physics
  • Familiarity with the concept of tunnelling current
  • Knowledge of spectroscopy techniques
  • Basic grasp of energy bands, including valence and conduction bands
NEXT STEPS
  • Research the principles of Scanning Tunnelling Microscopy (STM) and its applications
  • Study the mathematical formulation of density of states (DOS) in solid-state physics
  • Explore the differences between solid-state physics and atomic/molecular physics
  • Learn about the I-V characteristics and their significance in STM measurements
USEFUL FOR

Researchers in condensed matter physics, materials scientists, and anyone interested in advanced microscopy techniques and their applications in studying electronic properties of materials.

EIRE2003
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''The Scanning Tunnelling Microscope probes the density of states of a material''...

What does this actually mean?
 
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The signal from an STM is proportional to the tunnelling current between the tip of the probe and the surface that is being scanned.
Now, tunnelling current is of course proportional to the tunnelling propability which in turn is determined by -among other things- the number of states that are allowed to tunnell for a specfic bias, i.e. it is proportional to the density of states.
 
EIRE2003 said:
''The Scanning Tunnelling Microscope probes the density of states of a material''...

What does this actually mean?

It means that the STM is doing "spectroscopy" rather than imaging. It scans something resembling an "I vs. V", at a particular location of a material, where I is the current, and V is the bias potential between the STM tip and the material. The density of states (assuming you know what this is), is proportional to the the derivative of this curve, i.e. dI/dV vs. V.

Zz.
 
Ok, am I right in suggesting that the 'density of states' is, how closely packed the energy levels in an atom are, or is it how closely packed the energy levels in the material as a whole? That is, the energy gap between the valence band and the conduction band?
 
Your first definition of density of states is the more correct one. The density of states determines how closely packed (in energy space) the energy levels in a quantum mechanical system are.
 
EIRE2003 said:
Ok, am I right in suggesting that the 'density of states' is, how closely packed the energy levels in an atom are, or is it how closely packed the energy levels in the material as a whole? That is, the energy gap between the valence band and the conduction band?

Er... DOS is dN/dE, where N is the number of states per unit volume.

You can't really consider the "energy levels in an atom" when you're doing a STM on a solid. I'm sure I've mentioned this many times. A solid doesn't behave the same way as isolated atoms. That's why "solid state physics" isn't the same field of study as "atomic/molecular physics". An atom's "DOS" is meaningless because an atom has discrete energy levels, and thus a dN/dE operation would be strange. The DOS you get from an STM of a solid, such as a superconductor, gives a continuous result!

Zz.
 
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