Piezoresponse force microscopy (PFM) is a variant of atomic force microscopy (AFM) that allows imaging and manipulation of piezoelectric/ferroelectric materials domains. This is achieved by bringing a sharp conductive probe into contact with a ferroelectric surface (or piezoelectric material) and applying an alternating current (AC) bias to the probe tip in order to excite deformation of the sample through the converse piezoelectric effect (CPE). The resulting deflection of the probe cantilever is detected through standard split photodiode detector methods and then demodulated by use of a lock-in amplifier (LiA). In this way topography and ferroelectric domains can be imaged simultaneously with high resolution.

Basic principles

General overview

Piezoresponse force microscopy is a technique which since its inception and first implementation by Güthner and Dransfeld ^[1] has steadily attracted more and more interest. This is due in large part to the many benefits and few drawbacks that PFM offers researchers in varying fields from ferroelectrics, semiconductors and even biology.^[2] In its most common format PFM allows for identification of domains from relatively large scale e.g. 100×100 μm² scans right down to the nanoscale with the added advantage of simultaneous imaging of sample surface topography. Also possible is the ability to switch regions of ferroelectric domains with the application of a sufficiently high bias to the probe which opens up the opportunity of investigating domain formation on nanometre length scales with nanosecond time resolution.^[3] Many recent advances have expanded the list of applications for PFM and further increased this powerful technique. Indeed what started as a user modified AFM has now attracted the attention of the major SPM manufacturers so much so that in fact many now supply ‘ready-made’ systems specifically for PFM each with novel features for research. This is testament to the growth of the field and reflects the numbers of users throughout the scientific world who are at the forefront of scientific research.

Consider that a static or DC voltage applied to a piezoelectric surface will produce a displacement but as applied fields are quite low and the piezoelectric tensor coefficients are relatively small then the physical displacement will also be small such that it is below the level of possible detection of the system. Take as an example, the d₃₃ piezoelectric tensor coefficient of BaTiO₃, it has a value of 85.6 pmV⁻¹ meaning that applying 1 V across the material results in a displacement of 85.6 pm or 0.0856 nm, a minute cantilever displacement even for the high precision of AFM deflection detection. In order to separate this low level signal from random noise a lock-in technique is used wherein a modulated voltage reference signal,

${\displaystyle V({\boldsymbol {\omega }})=V_{\mathrm {ac} }\cos({\boldsymbol {\omega }}t)\;}$

of frequency ω and amplitude V_ac is applied to the tip giving rise to an oscillatory deformation of the sample surface,

${\displaystyle d=d_{\mathrm {0} }+D\cos({\boldsymbol {\omega }}t+{\boldsymbol {\varphi }})\;}$

from the equilibrium position d₀ with amplitude D, and an associated phase difference φ. The resulting movement of the cantilever is detected by the photodiode and so an oscillating surface displacement is converted into an oscillating voltage. A lock-in-amplifier (LiA) is then able to retrieve the amplitude and phase of the CPE induced surface deformation by the process outlined below.

Converse piezoelectric effect

The converse piezoelectric effect (CPE) describes how an applied electric field will create a resultant strain which in turn leads to a physical deformation of the material. This effect can be described through the constitutive equations.^[4] The CPE can be written as

${\displaystyle X_{\mathrm {i} }=d_{\mathrm {ki} }E_{\mathrm {k} }\;}$

where X_i is the strain tensor, d_ki is the piezoelectric tensor, and E_k is the electric field. If the piezoelectric tensor is considered to be that of the tetragonal crystal system (that of BaTiO₃) then it is

${\displaystyle {\begin{bmatrix}X_{1}\\X_{2}\\X_{3}\\X_{4}\\X_{5}\\X_{6}\end{bmatrix}}={\begin{bmatrix}0&0&d_{31}\\0&0&d_{32}\\0&0&d_{33}\\0&d_{15}&0\\d_{15}&0&0\\0&0&0\end{bmatrix}}{\begin{bmatrix}E_{1}\\E_{2}\\E_{3}\end{bmatrix}}}$

such that the equation will lead to the strain components for an applied field. If the field is applied exclusively in one direction i.e. E₃ for example, then the resulting strain components are: d₃₁E₃, d₃₂E₃, d₃₃E₃

Thus for an electric field applied along the c-axis of BaTiO₃ i.e. E₃, then the resulting deformation of the crystal will be an elongation along the c-axis and an axially symmetric contraction along the other orthogonal directions. PFM uses the effect of this deformation to detect domains and also to determine their orientation.

Conductive probe

The most important property of the probe for use in PFM is that it should be conducting. This is generally required in order to provide a means of applying a bias to the sample, and can be achieved through manufacturing standard silicon probes and coating them in a conductive material. Common coatings are platinum, gold, tungsten and even conductive diamond.

Lock-in amplifier

In the general case a lock-in amplifier (LiA) ‘compares’ an input signal against that of a reference signal (either generated internally or supplied by an external function generator) in order to separate the information contained in the input signal at the frequency of the reference signal. This is called demodulation and is done in a number of easy steps. The reference signal ${\displaystyle \scriptstyle V_{\mathrm {ref} }=B\cos({\boldsymbol {\omega }}t)}$, and input signal, ${\displaystyle \scriptstyle V_{\mathrm {in} }=A\cos({\boldsymbol {\omega }}t+{\boldsymbol {\varphi }})}$, are multiplied together to give the demodulator output,

${\displaystyle V_{\mathrm {out} }={\frac {1}{2}}AB\cos({\boldsymbol {\varphi }})+{\frac {1}{2}}AB\cos(2{\boldsymbol {\omega }}t+{\boldsymbol {\varphi }})}$

where A is the input signal Amplitude and B is the reference signal Amplitude, ω is the frequency of both the reference and input signals, and φ is any phase shift between the two signals.

The above equation has an AC component at twice the frequency of the original signals (second term) and a DC component (first term) whose value is related to both the amplitude and phase of the input signal. The demodulator output is sent through a low-pass filter to remove the 2ω component and leave the DC component then the signal is integrated over a period of time defined as the Time Constant, τ_LiA which is a user-definable parameter. Several different outputs are commonly available from a LiA: X output is the demodulator output and Y is the second demodulator output which is shifted by 90° in reference to the first output, together they hold both the phase, θ, and magnitude, R, information and are given by

${\displaystyle X={\frac {1}{2}}AB\cos({\boldsymbol {\theta }})}$ and

${\displaystyle Y={\frac {1}{2}}AB\cos({\boldsymbol {\theta }}+{\frac {\pi }{2}})={\frac {1}{2}}AB\sin({\boldsymbol {\theta }})}$

However, phase and amplitude of the input signal can also be calculated and made output from the LiA if desired, so that the full amount of information is available. The phase output can be determined from the following equation:

${\displaystyle {\boldsymbol {\theta }}=\tan ^{-1}{\frac {Y}{X}}}$

The magnitude is then given by:

${\displaystyle R={\sqrt {X^{2}+Y^{2}}}}$

This allows R to be calculated even if the input signal differs in phase from the reference signal.

Differentiating vertical and lateral PFM signals

A basic interpretation of PFM (which is generally accepted) identifies that two modes of imaging are possible, one that is sensitive to out-of-plane and one to in-plane piezoresponse, termed, vertical and lateral PFM (VPFM and LPFM) respectively.^[5] The separation of these components is possible through the use of a split photodiode detector, standard to all optical detection AFM systems. In this setup the detector is split into quadrants, nominally A, B, C and D. The centre of the entire detector outputs 0 V but as the laser spot moves a radial distance from this centre point, the magnitude of the voltage in output will increase linearly. A vertical deflection can be defined as {(A+B)-(C+D)}/(ABCD) so that now positive and negative voltages are ascribed to positive and negative cantilever vertical displacements. Similarly a lateral deflection is defined as {(B+D)-(A+C)}/(ABCD) to describe positive and negative torsional movements of the cantilever. So VPFM will utilise the vertical deflection signal from the photodiode detector so will only be sensitive to out-of-plane polar components and LPFM will utilise the lateral deflection signal from the photodiode and will only be sensitive to in-plane polar components.

For polar components orientated such that they are parallel to the electric field the resulting oscillating movement will be entirely in-phase with the modulated electric field but for an anti-parallel alignment the motion will be 180° out-of-phase. In this way it is possible to determine the orientation of the vertical components of polarisation from analysis of the phase information, φ, contained in the input signal, readily available after demodulation in the LiA, when using the VPFM mode. In a similar sense the orientations of in-plane polar components can also be determined from the phase difference when using the LPFM mode. The amplitude of the piezoresponse of either VPFM or LPFM is also given by the LiA, in the form of the magnitude, R.

Examples of PFM imaging

The image shows periodically poled 180° domains in potassium titanyl phosphate (KTP) as imaged by VPFM. In the image piezoresponse amplitude can be seen where dark areas represent the zero amplitude that is expected at domain boundaries where the unit cell is cubic i.e. centrosymmetric and so therefore not ferroelectric. On the left hand side piezoresponse phase can be seen where the measured phase changes to show the out-of-plane components that are pointing out of the screen, white areas, and into the screen, dark areas. The scan area is 20×10 μm². Below each scan is the relevant cross-section that shows in arbitrary units the PR amplitude and phase.

PFM applied to biological materials

PFM has been successfully applied to a range of biological materials such as teeth,^[6] bone, lung,^[7] and single collagen fibrils.^[8] It has been hypothesized that the endogenous piezoelectricity in these materials may be relevant in their mechanobiology. For example, using PFM it has been shown that a single collagen fibril as small as 100 nm behaves predominantly as a shear piezoelectric material with an effective piezoelectric constant of ~1 pm/V.

Advanced PFM modes

Zdroj:https://en.wikipedia.org?pojem=Piezoresponse_force_microscopy
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