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Scanning tunnelling spectroscopy

Scanning tunnelling spectroscopy. STM, STS, and the densities of states includes effect of tunnel barrier shape

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Page 1: Scanning tunnelling spectroscopy. STM, STS, and the densities of states includes effect of tunnel barrier shape

Scanning tunnelling spectroscopy

Page 2: Scanning tunnelling spectroscopy. STM, STS, and the densities of states includes effect of tunnel barrier shape

STM, STS, and the densities of states

EFermi

EFermi

Energy

xSample Tip

sample tip

includes effect of tunnel barrier shape

Page 3: Scanning tunnelling spectroscopy. STM, STS, and the densities of states includes effect of tunnel barrier shape

Spectroscopy – what can we learn?

dI/dV reflects major features of local density of states of the sample (+ tip) near the fermi level.

We can learn about the electronic properties (valence states) of the surface very locally!

Page 4: Scanning tunnelling spectroscopy. STM, STS, and the densities of states includes effect of tunnel barrier shape

Scanning Tunnelling Spectroscopy:how to do it

Switch off feedback loop and measure one of the following curves:

I(V) , I(z) , dI/dV , dI/dz , d2I/d2V

Measure curves in each point of an image,display di/dV maps at specific voltages

dI/dV of Ag(111) at different biasesK. Morgenstern et al., Phys. Rev. B 71 (2005) 155413

Display dI/dV vs. V in points of interest

Overgaag et al., ACS Nano, in press (2008)

Page 5: Scanning tunnelling spectroscopy. STM, STS, and the densities of states includes effect of tunnel barrier shape

Overgaag et al., ACS Nano, in press (2008)

Spectroscopy on isolated PbSe quantum dots

Spectroscopy on PbSe and CdSe quantum dots

Spectroscopy on PbSe quantum dots dimers, trimers,and larger aggregates

Page 6: Scanning tunnelling spectroscopy. STM, STS, and the densities of states includes effect of tunnel barrier shape

Stable STM is needed - STS is extremely sensitive to noise!

Cool sample, make sure you have good vibrational damping and a good tip.

Experimental considerations in STS

Instead of measuring I(V) and taking the derivative:

measure dI/dV right away!

Use Lock-in amplifier.

Page 7: Scanning tunnelling spectroscopy. STM, STS, and the densities of states includes effect of tunnel barrier shape

Lock-in amplifier

0'sinsin

dttt

2sinsin

ABdttBtA

0cossin

dttt

Orthogonality relationships for sinusoidal functions:

Out of phase

Page 8: Scanning tunnelling spectroscopy. STM, STS, and the densities of states includes effect of tunnel barrier shape

Lock-in amplifier

e.g. I(V) curve measured over 10 seconds

(e.g.1kHz):

Page 9: Scanning tunnelling spectroscopy. STM, STS, and the densities of states includes effect of tunnel barrier shape

Lock-in amplifier

From material by R. Scholten – University of Melbourne

Page 10: Scanning tunnelling spectroscopy. STM, STS, and the densities of states includes effect of tunnel barrier shape

Lock-in amplifier – noise reduction

Page 11: Scanning tunnelling spectroscopy. STM, STS, and the densities of states includes effect of tunnel barrier shape

Derivative with lock-in

Page 12: Scanning tunnelling spectroscopy. STM, STS, and the densities of states includes effect of tunnel barrier shape

Derivative with lock-in

Page 13: Scanning tunnelling spectroscopy. STM, STS, and the densities of states includes effect of tunnel barrier shape

Phase control

• Reference has phase control• Can vary from 0 to 360°• Arbitrary input signal phase• Tune reference phase to give maximum DC output

Reference

Phaseshift

Input Output Mixer

Page 14: Scanning tunnelling spectroscopy. STM, STS, and the densities of states includes effect of tunnel barrier shape

dI/dV spectroscopy in nanowires

•Modulate tunneling voltage with a 50mV ~1kHz sinus signal

•Clean up current & measure dI/dV with lock-in amplifier

•Now keep STM tip fixed and vary voltage to obtain dI/dV vs V

•Density of states at specific positions on the surface with atom resolution!

GaAs(110)

The bright feature at (II) is a Ga vacancy (we are imaging As atoms)

Page 15: Scanning tunnelling spectroscopy. STM, STS, and the densities of states includes effect of tunnel barrier shape

Spectroscopy to determine doping

GaAs(110) n-type GaAs overgrowth p-type

EF=EC-kTln(rC/rD)

C: Conduction bandV: Valence bandA: Additional tip induced charge

EF=kTln(rV/rA)-EV

Page 16: Scanning tunnelling spectroscopy. STM, STS, and the densities of states includes effect of tunnel barrier shape

STS on a nanowire

a

Page 17: Scanning tunnelling spectroscopy. STM, STS, and the densities of states includes effect of tunnel barrier shape

K. W. Hipps,Handbook ofApplied Solid State Spectroscopy

The role of thesecond derivativein STS

Page 18: Scanning tunnelling spectroscopy. STM, STS, and the densities of states includes effect of tunnel barrier shape

The role of the second derivative in STS

Feature enhancementby taking the derivative

B.C. Stipe. et. al., Science 280, 1732 (1998)

Page 19: Scanning tunnelling spectroscopy. STM, STS, and the densities of states includes effect of tunnel barrier shape

Vibration excitation of the molecule occurs when tunneling electrons have enough energy to excite a quantized vibrational level Inelastic tunneling channel

Single Molecule Vibrational Spectroscopy

B.C. Stipe. et. al., Science 280, 1732 (1998)

Page 20: Scanning tunnelling spectroscopy. STM, STS, and the densities of states includes effect of tunnel barrier shape

Further improvements and problems

Bandbending.

Changes in tip will induce changesin tunneling spectra!!!

Safe way: compare with ab-initio theory

Suppres exp. rise in current

Page 21: Scanning tunnelling spectroscopy. STM, STS, and the densities of states includes effect of tunnel barrier shape

Full calculation with sample + tip!!

Page 22: Scanning tunnelling spectroscopy. STM, STS, and the densities of states includes effect of tunnel barrier shape

Tip influences sample...