You can get the complex impedance, f is the frequency in Hertz and C is the capacitor's value in Faradic current. You can get and calculate faradic capacitance value from EIS (Impedance spectra).
Calculate the complex capacitance from the admittance, i.e. divide Y-imag by j.omega and plot this in a double log plot versus frequency. This will show the (approximate) capacitance plateaus. You can also analyze the impedance with a Nonlinear least Squares program that gives you an equivalent circuit. True capacitance will be obvious, but when you encounter a constant phase element (CPE or symbol 'Q' with Y=Y0.(j.omega)^n) in parallel with a resistance you can calculate an apparent capacitance using the following formula: C-app = [(R.Y0)^(1/n)]/R.
As far as I understood, you have EIS data from which you can construct Z'-Z" plot (i.e., Nyquist Plot). From this plot, you have to determine Z" (imaginary component of impedance) at any frequency inside the semi-circle (arc). From this relation, capacitance = -1 / (angular frequency * Z"), you can easily calculate the value of capacitance, C. As you know, angular frequency = 2 * pi* frequency (in Hz used for measurement of EIS).
Ideally, the equation C=1/(2*pi*frequency*Z'') only applies for the simple R-C series (i.e. without considering mixed kinetic and diffusion control). For a real case, a higher frequency (no lower than 100 kHz) is chosen to omit diffusion control.
Be attention to the applied potential and frequency you use, the calculated capacitance varies accordingly. Based on my experience, a higher frequency leads to shorter testing time and lower capacitance (maybe not right, considering a faster-scan-rate CV). The applied potential should be in the region where only capacitance process occurring in order to omit any faradaic response.
In the introduction of the paper "On Mott-Schottky analysis interpretation of capacitance measurements in organometal Perovskite solar cells" your doubt is completely solved
Md Saiful Alam Refer to this paper by P. Taberna, Electrochemical Characteristics and Impedance Spectroscopy Studies of Carbon-Carbon Supercapacitors, Journal of The Electrochemical Society.
My answer is based on the the directly previous answer of Mithun Sarkar ,
The first point is that you you curve is a semi circle terminated at in finite frequency at the real impedance = Rs which is the series resistance of an equivalent circuit composed of a parallel resistance Rp and capacitance Cp and the parallel combination is in series with a resistance Rs.
The half circle diagonal is equal to Rp. Then it remains only to determine Cp.
If you choose the point on the circle such that R=X , the angle phi of z will be 45 degrees where R= Rp/2 and X= 1/wC. Then at this point Rp/2= 1/wC,
since w is known and Rp is known one can get C.
For the shape of the impedance curves of a forward biased p-n junction please follow the paper:Article A distributed SPICE-model of a solar cell