1 / 32

Electric Force Microscopy (EFM)

Review Last Week about EFM. Electric Force Microscopy (EFM)

ccrouch
Download Presentation

Electric Force Microscopy (EFM)

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript

  1. Review Last Week about EFM Electric Force Microscopy (EFM) EFM is used to map the vertical (z) and near-vertical gradient of the electric field between the tip and the sample versus the in-plane coordinates x and y. This is done using LiftModeTM. The field due to trapped charges—on or beneath the sample surface—is often sufficiently large to generate contrast in an EFM image. Otherwise, a field can be induced by applying a voltage between the tip and the sample. The voltage may be applied directly from the microscope’s electronics under AFM software control, or from an external power supply with appropriate current-limiting elements in place. EFM is performed in one of three modes: amplitude detection, phase detection, or frequency modulation (FM).

  2. The application of EFM EFM is used for electrical failure analysis, detecting trapped charges, mapping electric polarization, and performing electrical read/write, among other applications.

  3. Electrostatic Interactions is long range interaction

  4. EFM/MFM Piezoelectric materials Conductive Domains Magnetic tip, instead of only a conductive tip

  5. In this method, the cantilever is vibrated by a small piezoelectric element near its resonant frequency. The cantilever’s resonant frequency changes in response to any additional force gradient. Attractive forces make the cantilever effectively “softer,” reducing the cantilever resonant frequency. Conversely, repulsive forces make the cantilever effectively “stiffer,” increasing the resonant frequency.

  6. Driving frequency Phase line  Resonance frequency  Normal TM AFM: ver der Waal Force gradient EFM: lift mode: Electrostatic Force gradient

  7. Mechanical Driven Mode V piezo = Vac sin(t+ 1) Constant drive frequency Free cantilever: A1 (d) sin(dt)+ 1) Interacted cantilever: A2(d) sin( d t) + 2) Normal TM AFM: ver der Waal Force gradient EFM: lift mode: Electrostatic Force gradient

  8. Electric Force Microscopy (EFM) • Mechanical vibration given to tip • Electric field will produce a change in phase of tip • Measure phase lag relative to piezo drive signal. • In most cases, it is necessary to apply a voltage across the tip or sample to achieve a high-quality image. • Even if a layer of insulating material covered the conductive domains, they still can be detected.

  9. EFM/MFM Piezoelectric materials Magnetic domains Conductive Domains Magnetic tip, instead of only a conductive tip

  10. Comparison: Phase imaging and the phase image in EFM During phase imaging, tapping mode imaging the tip is tapping the surface, the phase change due to the ver der Waal force gradient of the sample • Phase image in EFM Noncontact techniques, phase images are obtained in lift mode And the phase changes results from Electrostatic Force gradient

  11. Surface Potential Detectionor Kelvin Probe Microscopy

  12. Surface Potential (SP) Imaging SP imaging maps the electrostatic potential on the sample surface with or without a voltage applied to the sample. SP imaging is a nulling technique. As the tip travels above the sample surface in LiftMode, the tip and the cantilever experience a force wherever the potential on the surface is different from the potential of the tip. The force is nullified by varying the voltage of the tip so that the tip is at the same potential as the region of the sample surface underneath it. The voltage applied to the tip in nullifying the force is plotted versus the in-plane coordinates, creating the surface potential image.

  13. Surface Potential Detectionor Kelvin Probe Microscopy The piezo disengaged to stop mechanically driving the cantilever to vibrate, a AC voltage directly applied to the tip

  14. Detects the potential of the surface • AC voltage to the tip • (no induced mechanical vibration) Vac= 0 - 12 Vpp Sample surface V1 V2 but the conducting regions should not be passivated.

  15. Surface Potential Detection • Let  = fo • Potential on surface will shift phase of the cantilever • Detect phase change, use potential feedback loop to keep phase constant Vac= 0 - 12 Vpp Sample surface V1 V2

  16. Electrostatic Force in a Capacitor Energy Treatment Classical Treatment

  17. Surface Potential Detection First Harmonic Force Second Harmonic Force

  18. ( Deflection Amplitude caused by electrical force) Not force gradient • Let  = Vdriving • The lock-in technique allows extraction of the first harmonic of tip deflection proportional to F. A feedback loop is employed to keep it equal to zero by adjusting the Vdc on the tip. • Vdc=Vsurf • Therefore the surface potential is directly measurement by adjusting the potential offest on the tip and keep the fisrt harmonic response to zero.

  19. Comparison: EFM and Surface PotentialMicroscopy • Phase image in EFM Noncontact techniques, phase images are obtained in lift mode And the phase changes results from Electrostatic Force gradient • Potential image in Surface potential Microscope • (Amplitude modulation ( AM-KPFM) • The lock-in technique allows extraction of the first harmonic of tip deflection proportional to F. A feedback loop is employed to keep it equal to zero by adjusting the Vdc on the tip. • Vdc=Vsurf • Therefore the surface potential is directly measurement by adjusting the potential offest on the tip and keep the first harmonic response to zero.

  20. EFM and Frequency modulation KPFM

  21. Kelvin Probe Force Microscopy Study on Conjugated Polymer/Fullerene Bulk Heterojunction Organic Solar Cells Nano Letters 2005, 5, 269 A breakthrough in power conversion efficiency in polymer solar cells was achieved for bulk heterojunctions with the MDMO-PPV/PCBM (poly-[2-(3,7-dimethyloctyloxy)-5-methyloxy]-para-phenylene-vinylene/1-(3-methoxycarbonyl) propyl-1-phenyl [6,6]C61) system. The drastic increase in the power conversion efficiency was a result of changing the spin casting solvent from toluene to chlorobenzene, which accounted for a change in the film nanomorphology.

  22. Charge separation in bulk heterojunctions is based on the Photoinduced charge transfer, and photoexcited excitons in Organic materials have a very limited diffusion length on the Order of 10 nm. Not all photoexcitations will dissociate into separated charges carries. Photoluminescence of PCBM was found for toluene cast blends. This means that part of the adsorbed photons is not used for Photocurrent generation. Another study reported that hole mobility of prinstine MDMO-PPV Films to decrease when cast from toluene as compared to chlorobezene.

  23. In this study, Kelvin probe force microscope was used to reveal that the electronic work functions of films prepared from Different solvent. sample - tip = q CP tip=4.28 eV, PtIr coated Si cantilevers CP: contact potential, q is the elementary charge

More Related