
Scanning Tunneling Microscopy (STM)
Spectroscopy with the STM
154 MultiMode SPM Instruction Manual Rev. B
9.3.2 Operation of STS
In the following sections, the operation of the spectroscopic functions of the NanoScope III STM
will be discussed. Additional information can be obtained from the Command Reference Manual.
STS Plot
There are several items that you should be aware of when using the NanoScope to acquire
spectroscopic plots with the STS Plot commands. The spectroscopic capabilities can provide
information that can help to distinguish different species, although exact species identification is
difficult, especially in air. The spectroscopic plots should aid in comparative studies between
samples or between different regions on a sample, but they will not reveal the precise make-up of
that sample.
A comparison to STM imaging reveals two somewhat conflicting requirements. The sample and tip
should produce consistent STM images. The images should repeat well from frame-to-frame and
be fairly free of noise or areas on the surface that appear unstable. For current-versus-voltage type
plots, the spectroscopic plots may be smooth and repeat well, but switching back to the STM
imaging mode reveals noisy images because tip quality and uniformity are probably more critical
for imaging than for making the simpler spectroscopic plots. This is generally not true for the I vs.
S plots. Some general recommendations for acquiring spectroscopic plots are:
1. Low settings for the Integral gain are preferred. Since the tip is not tracking any topography,
the lower gains are acceptable and tend to make the plots more stable.
2. The maximum input range of ±100nA on the NanoScope with the standard preamps will
restrict the current-versus-voltage plots.
3. The spectroscopic functions do not adjust for any loss of bias voltage due to IR losses caused
by the input impedance of the preamplifier. This has different effects for the STS i(v) and
STS i(s) functions which are discussed individually below:
STS i(v)
The spectroscopic plots do not correct for reductions in bias voltage caused by the preamplifier,
which for current-versus-voltage is typically small, anyway. For example, a 1V scan on the bias
voltage, producing a 50nA response in the tunneling current would have a 5 percent error at the
extremes of the scan (50 nA X 1 MΩ = 50mV or 5 percent of 1V).
Input impedance of the preamplifier leads to reduced bias voltages at increased tunneling currents.
This effect can cause the I vs. S plot to be inaccurate. For example, a bias voltage of 20mV will
restrict the upper limit of the tunneling current to 20nA since that level of current would effectively
reduce the bias voltage to zero. Even before the tunneling current gets to 20nA, the reduced bias
voltage will make the measured current appear lower than it should be for a given tip height.
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