LEADER 05468nam 22006134a 450 001 9910830878003321 005 20230829000843.0 010 $a1-280-64993-3 010 $a9786610649938 010 $a0-470-85546-0 010 $a0-470-85545-2 035 $a(CKB)1000000000356097 035 $a(EBL)274326 035 $a(OCoLC)476018669 035 $a(SSID)ssj0000120117 035 $a(PQKBManifestationID)11146443 035 $a(PQKBTitleCode)TC0000120117 035 $a(PQKBWorkID)10080909 035 $a(PQKB)11446384 035 $a(MiAaPQ)EBC274326 035 $a(EXLCZ)991000000000356097 100 $a20060215d2006 uy 0 101 0 $aeng 135 $aur|n|---||||| 181 $ctxt 182 $cc 183 $acr 200 10$aCharge-based MOS transistor modeling$b[electronic resource] $ethe EKV model for low-power and RF IC design /$fChristian C. Enz, Eric A. Vittoz 210 $aChichester, England ;$aHoboken, NJ $cJohn Wiley$dc2006 215 $a1 online resource (329 p.) 300 $aDescription based upon print version of record. 311 $a0-470-85541-X 320 $aIncludes bibliographical references (p. [291]-298) and index. 327 $aCharge-based MOS Transistor Modeling; Contents; Foreword; Preface; List of Symbols; 1 Introduction; 1.1 The Importance of Device Modeling for IC Design; 1.2 A Short History of the EKV MOS Transistor Model; 1.3 The Book Structure; Part I The Basic Long-Channel Intrinsic Charge-Based Model; 2 Definitions; 2.1 The N-channel Transistor Structure; 2.2 Definition of Charges, Current, Potential, and Electric Fields; 2.3 Transistor Symbol and P-Channel Transistor; 3 The Basic Charge Model; 3.1 Poisson's Equation and Gradual Channel Approximation; 3.2 Surface Potential as a Function of Gate Voltage 327 $a3.3 Gate Capacitance3.4 Charge Sheet Approximation; 3.5 Density of Mobile Inverted Charge; 3.5.1 Mobile Charge as a Function of Gate Voltage and Surface Potential; 3.5.2 Mobile Charge as a Function of Channel Voltage and Surface Potential; 3.6 Charge-Potential Linearization; 3.6.1 Linearization of Qi (s); 3.6.2 Linearized Bulk Depletion Charge Qb; 3.6.3 Strong Inversion Approximation; 3.6.4 Evaluation of the Slope Factor; 3.6.5 Compact Model Parameters; 4 Static Drain Current; 4.1 Drain Current Expression; 4.2 Forward and Reverse Current Components; 4.3 Modes of Operation 327 $a4.4 Model of Drain Current Based on Charge Linearization4.4.1 Expression Valid for All Levels of Inversion; 4.4.2 Compact Model Parameters; 4.4.3 Inversion Coefficient; 4.4.4 Approximation of the Drain Current in Strong Inversion; 4.4.5 Approximation of the Drain Current in Weak Inversion; 4.4.6 Alternative Continuous Models; 4.5 Fundamental Property: Validity and Application; 4.5.1 Generalization of Drain Current Expression; 4.5.2 Domain of Validity; 4.5.3 Causes of Degradation; 4.5.4 Concept of Pseudo-Resistor; 4.6 Channel Length Modulation; 4.6.1 Effective Channel Length 327 $a4.6.2 Weak Inversion4.6.3 Strong Inversion; 4.6.4 Geometrical Effects; 5 The Small-Signal Model; 5.1 The Static Small-Signal Model; 5.1.1 Transconductances; 5.1.2 Residual Output Conductance in Saturation; 5.1.3 Equivalent Circuit; 5.1.4 The Normalized Transconductance to Drain Current Ratio; 5.2 A General NQS Small-Signal Model; 5.3 The QS Dynamic Small-Signal Model; 5.3.1 Intrinsic Capacitances; 5.3.2 Transcapacitances; 5.3.3 Complete QS Circuit; 5.3.4 Domains of Validity of the Different Models; 6 The Noise Model; 6.1 Noise Calculation Methods; 6.1.1 General Expression 327 $a6.1.2 Long-Channel Simplification6.2 Low-Frequency Channel Thermal Noise; 6.2.1 Drain Current Thermal Noise PSD; 6.2.2 Thermal Noise Excess Factor Definitions; 6.2.3 Circuit Examples; 6.3 Flicker Noise; 6.3.1 Carrier Number Fluctuations (Mc Worther Model); 6.3.2 Mobility Fluctuations (Hooge Model); 6.3.3 Additional Contributions Due to the Source and Drain Access Resistances; 6.3.4 Total 1/f Noise at the Drain; 6.3.5 Scaling Properties; 6.4 Appendices; Appendix: The Nyquist and Bode Theorems; Appendix: General Noise Expression; 7 Temperature Effects and Matching; 7.1 Introduction 327 $a7.2 Temperature Effects 330 $aModern, large-scale analog integrated circuits (ICs) are essentially composed of metal-oxide semiconductor (MOS) transistors and their interconnections. As technology scales down to deep sub-micron dimensions and supply voltage decreases to reduce power consumption, these complex analog circuits are even more dependent on the exact behavior of each transistor. High-performance analog circuit design requires a very detailed model of the transistor, describing accurately its static and dynamic behaviors, its noise and matching limitations and its temperature variations. The charge-based EKV (Enz 606 $aMetal oxide semiconductors$xMathematical models 606 $aMetal oxide semiconductor field-effect transistors$xMathematical models 615 0$aMetal oxide semiconductors$xMathematical models. 615 0$aMetal oxide semiconductor field-effect transistors$xMathematical models. 676 $a621.3815284 700 $aEnz$b Christian$01339617 701 $aVittoz$b Eric A.$f1938-$0725311 801 0$bMiAaPQ 801 1$bMiAaPQ 801 2$bMiAaPQ 906 $aBOOK 912 $a9910830878003321 996 $aCharge-based MOS transistor modeling$94063873 997 $aUNINA