Inelastic electron tunneling spectroscopy

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A schematic drawing of the system under investigation, with two metal contacts (left and right reservoir), a molecule in between (bridge electronic level) and a voltage applied between the two contacts. The wide band limit is assumed for both the contacts.
Left: Traveling electrons do not have sufficient energy to excite a vibration. Only elastic tunneling can take place.
Middle: When increasing the bias voltage beyond V=E/e (where e is the electronic charge), traveling electrons do have sufficient energy to excite a vibration with energy E. Inelastic tunneling can take place.
Right: Traveling electrons can also excite and subsequently reabsorb a vibration, which leads to second order elastic tunneling.

Inelastic electron tunneling spectroscopy (IETS) is an experimental tool for studying the vibrations of molecular adsorbates on metal oxides. It yields vibrational spectra of the adsorbates with high resolution (< 0.5 meV) and high sensitivity (< 1013 molecules are required to provide a spectrum).[1] An additional advantage is the fact that optically forbidden transitions may be observed as well.[2] Within IETS, an oxide layer with molecules adsorbed on it is put between two metal plates. A bias voltage is applied between the two contacts. An energy diagram of the metal-oxide-metal device under bias is shown in the top figure. The metal contacts are characterized by a constant density of states, filled up to the Fermi energy. The metals are assumed to be equal. The adsorbates are situated on the oxide material. They are represented by a single bridge electronic level, which is the upper dashed line. If the insulator is thin enough, there is a finite probability that the incident electron tunnels through the barrier. Since the energy of the electron is not changed by this process, it is an elastic process. This is shown in the left figure.

Some of the tunneling electrons can lose energy by exciting vibrations of the oxide or the adsorbate. These inelastic processes lead to a second tunneling path, which gives an additional current contribution to the tunneling current. Since the incident electron should have enough energy to excite this vibration, there is a minimum energy that is the onset of this (inelastic) process. This is shown in the middle figure, where the lower dashed line is a vibronic state. This minimum energy for the electron corresponds with a minimum bias voltage, which is the onset for the additional contribution. The inelastic contribution to the current is small compared to the elastic tunneling current (~0.1%) and is more clearly seen as a peak in the second derivative of the current to the bias voltage, as can be seen in the bottom figure.

There is however also an important correction to the elastic component of the tunneling current at the onset. This is a second order effect in electron-vibration coupling, where a vibration is emitted and reabsorbed or vice versa. This is shown in the upper figure on the right. Depending on the energetic parameters of the system, this correction may be negative and it may outweigh the positive contribution of the inelastic current, resulting in a dip in the IETS spectrum. This is experimentally verified in both regular IETS[3] and in STM-IETS[4] and is also predicted theoretically.[5] Not only peaks and dips may be observed, but depending on the energetic parameters also derivative-like features may be observed, both experimentally[6] and theoretically.[7]

STM-IETS[edit]

A change of slope in the current vs voltage leads to a step in the first derivative and to a peak in the second derivative of the current to the voltage.

Keeping the tip of a scanning tunneling microscope (STM) at fixed position over the surface and sweeping the bias voltage, one can record a I-V characteristic. This technique is called scanning tunneling spectroscopy (STS). The first derivative gives information about the local density of states (LDOS) of the substrate, assuming that the tip has a constant density of states. The second derivative gives information on vibrations of the adsorbate as in IETS, which is why this technique is commonly called STM-IETS. In this case the role of the insulating oxide layer is played by the gap between the tip and the adsorbate.

STM-IETS was first demonstrated by Stipe, Rezaei and Ho in 1998, seventeen years after the development of the STM.[8] The requirements of cryogenic temperatures and extreme mechanical stability (mechanical vibrations of the tip over the adsorbate must have amplitudes in the range of picometers or less) make this technique experimentally challenging to realize.

In recent years molecular transport junctions have been produced with one single molecule between two electrodes, sometimes with an additional gate electrode near the molecule.[9][10][11] The advantage of this method in comparison with STM-IETS is that there is contact between both electrodes and the adsorbate, whereas in STM-IETS there is always a tunneling gap between the tip and the adsorbate. The disadvantage of this method is that it is experimentally very challenging to create and identify a junction with exactly one molecule between the electrodes.

The STM-IETS technique was extended to the spin excitations of an individual atom by A. J . Heinrich, J. A. Gupta, C. Lutz and Don Eigler in 2004, at IBM Almaden.[12] Specifically, they probed transition between Zeeman split states of Mn atom on various surfaces conducting surfaces coated with insulating thin films. The technique was later applied to probe atomic spin transitions of Mn spin chains of up to 10 atoms, assembled one by one, also in IBM Almaden in 2006, in a team led by A. J. Heinrich.[13] The results showed that the Mn spin chain was a realization of the one dimensional Heisenberg model for S=5/2 spins. STM-IETS was also used to measure the atomic spin transitions split by single ion magnetic anisotropy of individual atoms[14][15][16] and molecules.[17] The underlying physical mechanism that permits tunnelling electrons to excite atomic spin transitions has been studied by several authors.[18][19][20] Whereas the most frequent mode of operation probes spin excitations from the ground state to excited states, the possibility to drive the system away from equilibrium and probe transition between excited states, as well as the possibility of controlling the spin orientation of single atoms with spin polarized currents were also reported.[21] In the case of coupled spin structures, the technique provides information not only about the energies spin excitations, but also about their spread across the structure, making it possible to image the spin wave modes in nanoengineered spin chains.[22]

References[edit]

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  2. ^ K.W. Hipps and U. Mazur (2001) Inelastic Electron Tunneling Spectroscopy, Handbook of Vibrational Spectroscopy, ISBN 978-0-471-98847-2
  3. ^ Bayman, A.; Hansma, P.; Kaska, W. (1981). "Shifts and dips in inelastic-electron-tunneling spectra due to the tunnel-junction environment". Physical Review B. 24 (5): 2449. Bibcode:1981PhRvB..24.2449B. doi:10.1103/PhysRevB.24.2449. 
  4. ^ Hahn, J.; Lee, H.; Ho, W. (2000). "Electronic Resonance and Symmetry in Single-Molecule Inelastic Electron Tunneling". Physical Review Letters. 85 (9): 1914–7. Bibcode:2000PhRvL..85.1914H. doi:10.1103/PhysRevLett.85.1914. PMID 10970646. 
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  6. ^ Wang, Wenyong; Lee, Takhee; Kretzschmar, Ilona; Reed, Mark A. (2004). "Inelastic Electron Tunneling Spectroscopy of an Alkanedithiol Self-Assembled Monolayer". Nano Letters. 4 (4): 643. Bibcode:2004NanoL...4..643W. doi:10.1021/nl049870v. 
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  10. ^ Park, Jiwoong; Pasupathy, Abhay N.; Goldsmith, Jonas I.; Chang, Connie; Yaish, Yuval; Petta, Jason R.; Rinkoski, Marie; Sethna, James P.; et al. (2002). "Coulomb blockade and the Kondo effect in single-atom transistors". Nature. 417 (6890): 722–5. Bibcode:2002Natur.417..722P. doi:10.1038/nature00791. PMID 12066179. 
  11. ^ Liang, Wenjie; Shores, Matthew P.; Bockrath, Marc; Long, Jeffrey R.; Park, Hongkun (2002). "Kondo resonance in a single-molecule transistor". Nature. 417 (6890): 725–9. Bibcode:2002Natur.417..725L. doi:10.1038/nature00790. PMID 12066180. 
  12. ^ Heinrich, A. J.; Gupta, J. A.; Lutz, C. P.; Eigler, D. M. (2004-10-15). "Single-Atom Spin-Flip Spectroscopy". Science. 306 (5695): 466–469. doi:10.1126/science.1101077. ISSN 0036-8075. PMID 15358866. 
  13. ^ Hirjibehedin, Cyrus F.; Lutz, Christopher P.; Heinrich, Andreas J. (2006-05-19). "Spin Coupling in Engineered Atomic Structures". Science. 312 (5776): 1021–1024. doi:10.1126/science.1125398. ISSN 0036-8075. PMID 16574821. 
  14. ^ Hirjibehedin, Cyrus F.; Lin, Chiung-Yuan; Otte, Alexander F.; Ternes, Markus; Lutz, Christopher P.; Jones, Barbara A.; Heinrich, Andreas J. (2007-08-31). "Large Magnetic Anisotropy of a Single Atomic Spin Embedded in a Surface Molecular Network". Science. 317 (5842): 1199–1203. doi:10.1126/science.1146110. ISSN 0036-8075. PMID 17761877. 
  15. ^ Khajetoorians, Alexander A.; Chilian, Bruno; Wiebe, Jens; Schuwalow, Sergej; Lechermann, Frank; Wiesendanger, Roland (2010-10-28). "Detecting excitation and magnetization of individual dopants in a semiconductor". Nature. 467 (7319): 1084–1087. doi:10.1038/nature09519. ISSN 0028-0836. 
  16. ^ Rau, Ileana G.; Baumann, Susanne; Rusponi, Stefano; Donati, Fabio; Stepanow, Sebastian; Gragnaniello, Luca; Dreiser, Jan; Piamonteze, Cinthia; Nolting, Frithjof (2014-05-08). "Reaching the Magnetic Anisotropy Limit of a 3d Metal Atom". Science: 1252841. doi:10.1126/science.1252841. ISSN 0036-8075. PMID 24812206. 
  17. ^ Tsukahara, Noriyuki (2009-01-01). "Adsorption-Induced Switching of Magnetic Anisotropy in a Single Iron(II) Phthalocyanine Molecule on an Oxidized Cu(110) Surface". Physical Review Letters. 102 (16). doi:10.1103/PhysRevLett.102.167203. 
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