Title: Wittenberg 2: Tunneling Spectroscopy
1Wittenberg 2 Tunneling Spectroscopy
Andreas Heinrich heinrich_at_almaden.ibm.com
2Wittenberg 2 Spectroscopy
- Spectroscopy with STM
- Example quantum corral
- Example BCS superconductor
- Inelastic Tunneling Spectroscopy
- CO on Cu(111) vibrational spectroscopy
- Measuring the g-value of single atoms
- H2 physisorbed on Cu (111)
3STM Imaging Spectroscopy
Tip
Keep I constant
V
VVac
- turn off servo
- add Vac
- measure dI/dV
I , R
I Iac, R
Sample
4STM Spectroscopy
Barrier
EF
EF
LDOS
Sample
Tip
5Standing Waves on the Cu (111) Surface
M.F. Crommie, C.P. Lutz and D.M. Eigler, Nature
363, 524 (1993)
6Shockley-Type Surface States on Cu (111)
- Gap in bulk band structure in the lt111gt direction
- Surface breaks symmetry resulting in localized
states
- Free 2-d electron gas at the surface
7Spectroscopy of Surface State
- Compare spectra of step edge vs. terrace
- Step in conductance at V -0.45V
- Bottom of band is close to EF
8Dispersion Relation
- Scattering from step edge
- Energy resolved wavelength
- Free electron gas
- Modified electron mass
- meff 0.38 me, ?F 30 Å
9Construction of Circle
- Fe on Cu(111)
- 48 atom circle
10Quantum Corral
20nm 20nm R 27 unit cells V 10mV I 1nA
- Same corral built with CO ? more stable
- topograph measures purely electronic structure
orbits - peaked in center for l0 state s-like
- 71Å radius circle
11Corral Spectroscopy
- Spectra in circle center
- From I/V to dI/dV
- Particle in a box
12QM 1d Particle in a Box
- Infinite walls at z0 and za
- Schroedinger equation between z0 and za
- Wavefunction is zero outside for zlt0 and zgta
- The energy spacing is non-linear in 1d
13QM 2d Particle in a Circle
- 2d solutions are Bessel functions
- l0 and l1 are energy separated
- l2 is same energy as l0
EF
14Eigenstates of Circle
- Fit using l0,2,7
- The surprising details of the spectrum can be
reproduced - High ns and ls contribute
15Identifying States
- s-states in circle
- l0 states are peaked in center
- n counts number of nodes
16Off-Center Spectroscopy
center of corral
10 Å off center
- higher l states contribute to the spectrum
- lx and ly do not have fixed phase, no nodes in
angular pattern
17Wittenberg 2 Spectroscopy
- Spectroscopy with STM
- Example quantum corral
- Excitation spectrum of superconductor
- Inelastic Tunneling Spectroscopy
- CO on Cu(111) vibrational spectroscopy
- Measuring the g-value of single atoms
- H2 physisorbed on Cu (111)
18Superconductor Excitation Spectrum
19How to get Tlt4K?
3He pump P0.01Torr
UHV
l-4He
4.2K
STM
0.5K
l-3He
l-3He
0.35K
Vacuum
20Schematic of Dewar
UHV Chamber
3He _at_ 2 atm
3He Exhaust to Pump
0.5 K, 7T UHV STM
Dewar
Vibration free Joule-Thompson 3He refrigerator
Counter flow heat exchanger
l-4He
Shutter
Vacuum
7T Split coil magnet
3He expansion
H
STM
21Niobium BCS Thermometer
- temperature of tip is really T0.5K
- radio frequency noise is less than 0.5K
22Wittenberg 2 Spectroscopy
- Spectroscopy with STM
- Example quantum corral
- Excitation spectrum of superconductor
- Inelastic Tunneling Spectroscopy
- CO on Cu(111) vibrational spectroscopy
- Measuring the g-value of single atoms
- H2 physisorbed on Cu (111)
23Inelastic Electron Tunneling Spectroscopy (IETS)
Barrier
elastic se
inelastic sie
Sample
Tip
dI/dV
se sie
se
se
V
Vmode
24IETS of CO on Cu (111)
B.C. Stipe et al. Science 280, 1732 (1998).
25IETS Mapping of C Isotopes
Topograph
dI/dV image
11nm11nm, 513 CO I3.55nA, V35.5mV, VAC1.5mVRMS
26Isotope Controlled Assembly
Topograph
dI/dV image
I3.55nA, V35.5mV, VAC1.5mVRMS
27Isotope Graffiti
Topograph
dI/dV image
4.6nm5.8nm, 160 CO I3.55nA, V35.5mV,
VAC1.5mVRMS
28Timing Linked Chevrons
- Only 1 molecule hops
- Mixed isotope cascade?
29Mixed-Isotope Cascade
13C16O
12C16O
13C16O
dI/dV image
12C16O 13C16O
30Tunneling from Excited State
A1012 /s 10-7
Shared activation energy E 9.5 meV A
12C 105.8/s A 13C 105.4/s
- Great fit at all T
- Prefactor is product of attempt rate and tunnel
probability
31New Vibrational Mode in Chevron?
Continuous ?3 overlayer Center of stabilized
chevron
Stabilized chevron
32Vibrational Modes in Circle
- flat top spectrum
- 4mV vibrational mode
33Wittenberg 2 Spectroscopy
- Spectroscopy with STM
- Example quantum corral
- Excitation spectrum of superconductor
- Inelastic Tunneling Spectroscopy
- CO on Cu(111) vibrational spectroscopy
- Measuring the g-value of single atomssubmitted
A.J. Heinrich et. al (2004) - H2 physisorbed on Cu (111)submitted J.A. Gupta
et. al (2004)
34IETS of Magnetic Atoms
A non-magnetic tip
Magnetic atom
eVgµBH
A non-magnetic surface