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Treinamento : Testes Paramétricos em Semicondutores Setembro 2012

Treinamento : Testes Paramétricos em Semicondutores Setembro 2012. Cyro Hemsi Engenheiro de Aplicação. Section 4 – Capacitance Measurement Basics. Agenda. Technology Area Where Capacitance Measurement is Used Fundamental of Capacitance Measurement

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Treinamento : Testes Paramétricos em Semicondutores Setembro 2012

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  1. Treinamento:Testes ParamétricosemSemicondutoresSetembro 2012 Cyro Hemsi Engenheiro de Aplicação Section 4 – Capacitance Measurement Basics

  2. Agenda • Technology Area Where Capacitance Measurement is Used • Fundamental of Capacitance Measurement • Basic Techniques to Achieve Accurate Capacitance Measurement

  3. Technology Area Where Capacitance Measurement is Used

  4. What is Capacitance ? Basic Equations Electrode W: Width L: Length e0: Permittivity of vacuum A d: Distance e: Relative permittivity A: Area of electrode Relation of Charge and Applied Voltage V Dielectrics Q: Total charge Positive charge V: Applied voltage Negative charge Most important equation to remember!! Capacitance is amount of charge stored between the electrodes when applying a unit voltage.

  5. Physical Dimensions of Semiconductor Devices Thickness of dielectrics can be determined from the gate capacitance. MOS FET Inter Connection L Gate-Source Overwrap W Gate Gate Dielectrics d Cgb Inter layer dielectrics d Source Drain Cgs Semiconductor Substrate Thickness of interlayer dielectrics can be determined from the capacitance between interconnecting wires. Cgd Cgb: Gate to body capacitance Cgd: Gate to drain capacitance Cgs: Gate to source capacitance Overwrap width between the gate electrode and drain or source area can be determined from the gate to drain or gate to source capacitances. Gate-Source Overwrap • Each capacitance represents actual physical dimensions and it is really important information to adjust conditions of manufacturing processes like lithography, etching, deposition time etc. • Also, those parasitic capacitances are important to determine the gate delay of electric circuit in the logic devices.

  6. SEQ. Why Are MOSFET Capacitance Measurements Important? Note that the value of the capacitance varies with applied DC voltage • Gate oxide capacitance • Gate oxide thickness • Substrate impurity concentration • Fermi potential • Flat band capacitance • Flat band voltage • Surface charge density • Fixed depletion layer charge • Threshold voltage Capacitance versus voltage measurement + Physical device parameters (area, work function, etc.) Key Device Parameters Mathematical Calculations

  7. Doping Profile of Semiconductor Devices N-MOS Cap Distribution of boundary defect density by comparing CV curve measured by high frequency(>1 kHz) and low frequency (<10 Hz) CV measurement. Thickness of gate dielectrics can be extracted from Cmax. Ld Low Frequency Gate Dielectrics Cg V Space Charge (depletion) Layer High Frequency Cd Vth V Doping profile can be extracted from the Cmax and Cmin. Ld: Depth of depletion layer q: Charge of electron Na: Density of acceptor p-Si Threshold voltage can be extracted from the intersection point of Cmin and extrapolation of CV curve. • CV characteristics of MOS-CAP (MOS-FET) is one of most important measurement item because it reveals various parameters related to the manufacturing process and device operation.

  8. Capacitance Measurements for Solar Cell Equivalent circuit model is determined by frequency sweep of impedance to optimize extra circuit to convert DC power generated by solar cell to AC Power. - N-type Junction Leakage Space Charge Layer Rs Rp P-type Junction Capacitor + Residual Resistance Photo current • Schematic of Solar Cell Impedance Spectroscopy Rp Carrier density distribution over the depletion width is obtained from the slope of 1/Cp2 to Voltage plot (Mott-Schottky plot ) Defect density distribution is obtained from the Cp to AC voltage amplitude of capacitance measurement plot. Rs Frequency C AC Level (mVpp) • Mott-Schottky Plot Drive-level Capacitance Profiling (DLCP)

  9. Mobility Measurement of Organic Semiconductor Materials T. Okachi et al. / Thin Solid Films 517 (2008) 1331–1334 d Vdc Organic Material Mobility of carrier is obtained from the maximum frequency of negative differential susceptance −ΔB=−w{C1(w)−Cgeo}. w: angular velocity of measurement signal. Cgeo: Geographical capacitance tt: Carrier transit time m: Mobility of carrier Improvement of mobility of organic material is most critical to put it to practical use.

  10. Capacitance C0 0 Bias Voltage or Displacement Characterization of Electrostatic Capacitive MEMS (Micro Electro Mechanical System) Sensor Also, displacement of diaphragm is caused by the applied external bias voltage. Electrostatic capacitive MEMS sensor detects displacement of diaphragm by mechanical stimulations like acceleration, pressure or sonic wave as a modulation of electrostatic capacitance. Mechanical Stimulus Diaphragm Spring Fixed Electrode Electrical Field by Applied Bias • Mechanical characteristics of MEMS sensor can be obtained from its capacitance to voltage characteristics. • Electrical capacitance measurement is easier and faster than the measurement by a mechanical stimulus. • Also frequency dependency of capacitance reveals mechanical response of the diaphragm spring.

  11. Importance of On-Wafer Capacitance Measurement On-wafer measurement becomes standard to develop various devices. Probe Wafer Chuck Wafer Semi-auto prober To carry out accurate capacitance measurement, specific attention is necessary. • Advantage of On-wafer Measurement • Quick evaluation and lower cost are possible because packaging is not necessary. • Challenges • There are many possible course of error from the cablings, wafer chuck, probing etc.

  12. Fundamental of Capacitance Measurement

  13. Basic Equations Related to Capacitance Measurement Basic Equation Equation to Measure Capacitance Derivation Stimulus Capacitance is calculated from the measured charge and amplitude of applied step voltage. Step Voltage Capacitance is calculated from the measured current and ramp rate of applied ramp voltage. Ramp Voltage Capacitance is calculated from the measured impedance and frequency of applied AC signal. AC Voltage Most widely-used method by capacitance meter

  14. Function of Each Terminal of Capacitance Meter Agilent 4284A Keep “0V” in AC manner by active feedback. So called “Virtual Ground”, not actual ground. Auto Balancing Bridge I voltage of the test signal applied to DUT HCUR LPOT HPOT LCUR DUT current that flows through DUT V 0 V A I V LCUR LPOT HPOT HCUR Connect terminals based on its functionalities is important to measure capacitance correctly. • Advantages of Auto Balancing Bridge Method • High accuracy (0.05 % basic accuracy) • Wide frequency range (20 Hz to 100 MHz) • Various choices are available based on frequency range and functions. • Agilent 4284A, 4285A, E4980A, E4981A, 4294A, B1500A

  15. Equivalent Circuit Model and Equations to Extract Capacitance Appropriate Parameter Complex Vector Parallel Model Equations Admittance Plane Im Im Cp-Rp Cp-G Cp-D Cp-Q Cp Rp Re Y G: Conductance D: Dissipation factor Q: Quality factor Appropriate Parameter Series Model Complex Vector Equations Impedance Plane Cs Cs-Rs Cs-D Cs-Q Rs Z Choosing appropriate measurement parameter is essential to extract capacitance correctly. Re

  16. V2 = I2 x R2 V1 V1R2 = Z = I2 V2 How Do Capacitance Meters Work? Auto-Balancing Bridge Method Virtual ground V2 Rs I1 = I2 R2 Lc Hc DUT Hp I2 I1 Lp virtual ground of the Op Amp V1 Impedance is calculated by Z = V1*R2/V2.

  17. 4TP: Minimize residual impedance ~ Shields: Minimize stray capacitance Current flow: Minimize inductive coupling Four Terminal Pair (4TP) Measurement Method Measurement Circuit V ~ Lc Lp Hp Hc A Measurement Path Connection with DUT DUT Virtual ground

  18. 1 kHz 5 MHz 110 MHz B1500A Capacitance Measurement Coverage EasyEXPERT 4.x HFCV Ultra-HFCV QSCV B1500A (SMU) B1500A (MFCMU) 4294A Standard (>25 A) dielectrics Thin-gate (<25 A) dielectrics

  19. Basic Techniques to Achieve Accurate Capacitance Measurement

  20. Possible Sources of Measurement Error • Inappropriate selection of measurement parameter • Capacitance is extracted based on the equation of the equivalent circuit model for selected measurement parameter. • Mismatch of equation and equivalent circuit model causes measurement error. • Selection of appropriate measurement parameter (equivalent circuit ) is important. • Parasitic capacitance, residual resistance and inductance • Cablings between the instruments and device affects measurement results. • Minimizing influence of cablings are critical to achieve accurate measurement. • Inappropriate execution of compensation • Compensation is commonly used to remove the influence from the cablings. • But inappropriate compensation has a devastating impact on measurement results. • Compensation have to be done in correct manner!! • Parasitic capacitance of wafer probing system. • On-wafer measurement has a specific error caused by a parasitic of the wafer chuck not considered when measuring discrete components. • Special care is required for on-wafer capacitance measurement.

  21. Error Caused by Using Inappropriate Selection of Equivalent Circuit Model Measurement Parameter • Measured Value Actual Device Cp-Rp Cp Rp Error caused by measurement parameter mismatch Cs-Rs Cp-Rp Cs Quick Tips: If measured capacitance value is stable when measurement frequency is changed, the selection of measurement parameter is appropriate, because error component has frequency dependency. Rs Cs-Rs Inappropriate selection of measurement parameter increases measurement error.

  22. Measurement Parameter Selection for Actual Device Parameter to select Conditions MOS-FET Source Gate Drain Cp-Rp Cp-G Cp-D Cp-Q Gate Resistance Cp Rp AND Gate Contact resistance of via Sub Gate Leakage Junction Resistance Cs-Rs Cs-D Cs-Q AND Cs Cp Rp Rs Relatively thick dielectrics of technology node over 90 nm will satisfy either of above. Rs For more shrunk process, parameter extraction using multi-frequency is necessary. Actual Equivalent Circuit

  23. Error Caused by Cablings Residual Inductance LCR Meter Residual Resistance Device to Measure Output terminals of LCR Meter Calibration Plane Parasitic Capacitance Rres is Included in the Rs when using Cs-Rs mode. But in Cs-Rp mode, Rres is included in the error of measured capacitance. Influence of residual inductance Increases along with a square of frequency Total impedance measured by LCR Meter Rres Lres Cdev Cpar Higher frequency results in larger measurement error Additional Error Not related to the measurement frequency

  24. Minimizing Error from Cablings Eliminate parasitic capacitance of cable extension by usingcoaxial cable and connect shield to the shield of the test leads. Connect shield of cable extensions at end of cable each other to minimize residual inductance. Connect shield of test leads each other to terminate four terminal pair. LCR Meter LCR Meter Test Leads Cable Extension Probe HCUR HPOT V LPOT LCUR LPOT HCUR HPOT LCUR Output Terminals A Make unshielded part as short as possible to minimize residual inductance and Extends output to the device to measure near as possible by using the test leads of LCR meter Test Leads for LCR Meter Measurement Current Current return to HCUR

  25. END Of section 4

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