Physics and Properties of Semiconductors – A Review
- Introduction
- Crystal Structure
- Primitive Cell and Crystal Plane
- Fig. 1- Some Important primitive cells
- Fig. 2- Miller indices of some important planein cubic crystal
- Table 1 – Miller Indices and Their Represented Plane
- Reciprocal Lattice
- eqn(1) to eqn(4)
- Primitive Cell and Crystal Plane
- Energy bands and Energy Gap
- Fig. 3- Brillouin zones
- eqn(5) to eqn(7)
- Table 2 – Brilloun Zoneof fee, Diamond
- Fig. 4- Energy-band structures
- eqn(8) to eqn(10)
- Carrier Concentration at Thermal Equilibrium
- Fig. 7- Three basic bond pictures of semiconductor
- Carrier Concentration and Fermi Level**
- eqn(11) to eqn(22)
- Fig. 8 – Fermi-Dirac integral F1/2 as a function of Fermi Energy
- Degenerate Semiconductors
- eqn(23a) and eqn(23b)
- Intrinsic Concentration
- eqn(24) to eqn(26)
- eqn(27a) and eqn(27b
- Donors and Acceptors
- Fig. 9 – Intrinsic carrier concentration of Si and GaAs
- eqn(28) to eqn(30)
- Fig. 9 – Intrinsic carrier concentration of Si and GaAs
- Calculation of Fermi Level
- eqn(31)
- Fig. 10 – Measured ionization energies for various impurities
- Fig. 11 – Schematic band diagram densityof states
- eqn(32) to eqn(41)
- Fig. 12 – A graphical method to determine the Fermi energy level
- Fig. 13 – Electron density as a function of temperature for a Si sample with donor impurity
- Fig. 14 – Fermi level for (a) Si and (b) GaAs as a function of temperature and impurity concentration
- eqn(39) to eqn(44)
- Carrier-transport Phenomena
- Drift and Mobility
- eqn(45) to eqn(50)
- Fig. 15 – Drift Mobilities of (a) Si
- Phonon, Optical and Thermal Properties
- Heterojunctions and Nanostructures
- Basic Equations and Examples
- Resistivity and Hall Effect
- eqn(51)
- Fig. 16 – Mobility of Electron and holes in Si as a function of temperature
- Fig. 17 – Electron (circles) and holes (square) mobility versus bandgap for direct
- eqn(52) and eqn(53)
- Fig. 18 – The correction factor for the measurement of the resistivity
- Fig. 19 – Resistivity versus impurity concentration for (a) Si and (b) GaAs
- eqn(52) and eqn(53)
- Hall Effect
- Fig. 20 – Basic setup to measure carrier concentration using the Hall effect
- eqn(54) to eqn(60)
- Fig. 20 – Basic setup to measure carrier concentration using the Hall effect
- High-electric-Field Properties
- eqn(61) to eqn(64)
- Fig. 21 – The measured carrier velocity Vs electric field for high-purity Si and GaAs
- eqn(65) to eqn(69)
- Recombination, Generation and Carrier Lifetimes
- eqn(70) and eqn(71)
- eqn(72a) and eqn(72b)
- Fig. 24 – Ionization rates at 300K
- Fig. 25 – Electron ionization rate versus the reciprocal electric field in Si
- Fig. 26 – Recombination processes
- eqn(73) to eqn(88)
- eqn(89a) and eqn(89b)
- eqn(90) to eqn(95)
- Diffusion
- eqn(96) to eqn(99)
- eqn(100a) and eqn(100b)
- eqn(101)
- Thermionic Emission
- eqn(102) to eqn(103)
- Tunneling
- eqn(104) to eqn(107)
- Space-Charge Effect
- eqn(108) to eqn(113)
- Phonon, Optical and Thermal Properties
- Phonon Spectra
- eqn(114)
- Optical Properties
- eqn(115) to eqn(124)
- Thermal Properties
- eqn(125) to eqn(129)
- Phonon Spectra
- Heterojunctions and Nanostructures
- Heterojunctions
- eqn(130) to eqn(140)
- Heterojunctions
- Basic Equations and Examples
- Basic Equations
- The Poisson Equation
- eqn(141) to eqn(148)
- Current-Density Equation
- eqn(149a) and eqn(149b)
- eqn(150)
- eqn(151a) and eqn(151b)
- Continuity Equations
- eqn(152a) and eqn(152b)
- eqn(153a) and eqn(153b)
- Lattice Temperature Equation
- eqn(154) and eqn(155)
- The Poisson Equation
- Examples
- Decay of Excess Carriers with Time
- eqn(156) to eqn(158)
- Fig. 44 – Decay of photo-excited carriers
- eqn(159)
- Decay of Excess Carriers with Distance
- eqn(160) to eqn(163)
- Fig. 45 – Steady State carrier injection from one side
- Decay of Excess Carriers with Time and Distance
- eqn(164) and eqn(165)
- Fig. 46 – Transient and steady-state carrier diffusion
- Surface Recombination
- eqn(166) to eqn(168)
- Fig. 47 – Surface recombination at x = 0
- Problems 1 to 36
- Decay of Excess Carriers with Time
- Basic Equations
- p-n junctions
- Introduction
- Deplection region
- Abrupt Junction
- Built-In Potential and Depletion-Layer Width
- eqn(1)
- Fig. 1 – An abrupt p-n junction in thermal equilibrium
- eqn(2) to eqn(8)
- eqn(9a) and eqn(9b)
- eqn(10)
- eqn(11a) and eqn(11b)
- eqn(12) to eqn(16)
- eqn(17a) and eqn(17b)
- eqn(18) and eqn(19)
- eqn(20a) and eqn(20b)
- eqn(21)
- eqn(22a) and eqn(22b)
- eqn(23) to eqn(25)
- Depletion-Layer Capacitance
- eqn(26) to eqn(28)
- eqn()**
- Fig. 2 – Depletion layer width and depletion-layer capacitance per unit area as a function of net potential
- eqn(27) and eqn(28)
- Fig. 3 – A 1/C2-V plot can yield the built-in potential and doping density N
- eqn(29) to eqn(31)
- Linearly Graded Junctions
- Fig. 4 – The Debye length in Si at room temperature
- eqn(32) to eqn(34)
- Fig. 5 – A linearily graded junction in thermal equilibrium
- eqn(35) to eqn(39)
- Fig. 6 – Gradient voltages for linearity graded junctions in Si and GaAs
- Fig. 7 – The depletion layer width and depletion layer capacitance per unit area
- Fig. 4 – The Debye length in Si at room temperature
- Arbitrary Doping Profile**
- eqn(40) and eqn(41)
- Fig. 8 – A p-n junction with different doping profiles in thermal equilibrium
- eqn(42) to eqn(46)
- Current-Voltage Characteristic
- Ideal Case– – Shockley Equation
- eqn(47a) and eqn(47b)
- eqn(48a) and eqn(48b)
- eqn(50) to eqn(52)
- Fig. 9 – An energy-band diagram, with Fermi-levels for electrons and holes
- eqn(53)
- eqn(54a) and eqn(54b)
- eqn(55a) and eqn(55b)
- eqn(56) to eqn(60)
- eqn(61a) and eqn(61b)
- eqn(62) and eqn(63)
- Fig. 10 – Carrier distribution and current densities
- Fig. 11 – Ideal current-voltage charateristics
- eqn(64)
- Generation-Recombination Process
- eqn(65) to eqn(68)
- Fig. 12 – Current-Voltage characteristic of a practical Si diode
- eqn(69) to eqn(74)
- High-Injection Condition
- eqn(75)
- Fig. 14 – Carrier concentrations and energy-band diagrams for a Si p+–n junction
- Diffusion Capacitance**
- eqn(76) to eqn(87)
- Junction breakdown
- Thermal Instability
- Fig. 15 – Normalized diffusion conductance and diffusion capacitance versus 𝜔𝜏
- Tunneling
- eqn(88)
- Fig. 16 – Reverse current-voltage characteristic of thermal berakdown
- Fig. 17 – Energy band diagrams showing breakdown mechanism
- Avalanche Multiplication
- eqn(89) to eqn(94)
- eqn(95a) and eqn(96b)
- eqn(96) to eqn(102)
- Edge Effects
- eqn(103) to eqn(107)
- Fig. 23 – Normalized avalanche breakdown voltage versus lattice temperature
- Fig. 24 – A planar diffusion or implantation process form a junction curvature
- Transient Behavior and Noise
- Transient Behavior
- Fig. 26 – Transient behavior of a p-n junction
- eqn(108) to eqn(117)
- Fig. 26 – Transient behavior of a p-n junction
- Noise
- Fig. 27 – Normalized time versus the ratio of reverse current to forward current
- eqn(118) to eqn(121)
- Fig. 27 – Normalized time versus the ratio of reverse current to forward current
- Terminal Functions
- Rectifier
- eqn(122) to eqn(126)
- Zener Diode
- Varistor
- Varactor
- eqn(127)
- Fig. 28 – Various impurity distribution(normalized at xo)
- eqn(128) to eqn(130)
- Fig. 28 – Various impurity distribution(normalized at xo)
- eqn(127)
- Fast-Recovery Diode
- Fig. 29 – A plot of the normalized measured capacitance versus gate voltage
- Charge-Storage Diode
- p-i-n Diode
- eqn(131)
- Fig. 30 – The simulated p-i-n diode with uniform doping profiles in thermal equilibrium
- eqn(132) and eqn(133)
- Rectifier
- Heterojunctions
- Anisotype Heterojunction
- Fig. 31 – Typical RF resistance as a function of dc forward current
- eqn(134a) and eqn(134b)
- Fig. 32 – Energy-band diagrams for (a) two isolated semiconductor of opposite type
- eqn(135) and eqn(136)
- eqn(137a) and eqn(137b)
- eqn(138) and eqn(139**)
- Fig. 31 – Typical RF resistance as a function of dc forward current
- Isotype Heterojunction**
- eqn(140) to eqn(145) **
- Fig. 33 – Energy-band diagrams for ideal (a) n-n and (b) p-p isotype heterojunctions
- Anisotype Heterojunction
- Transient Behavior
- Problems 1 to 23
- Metal-Semiconductor Contacts
- Formation of Barrier
- Introduction
- Ideal Condition
- Fig 1 – Energy-band diagram of metal-semiconductor contacts
- eqn(1) to eqn(3)
- Fig 2 – Metal workfunction for a clean surface in a vacuum atomic number
- Fig 1 – Energy-band diagram of metal-semiconductor contacts
- Depletion Layer
- eqn(4) and eqn(5)
- Fig 3 – Energy-band diagram of metal on n
- eqn(6) to eqn(11)
- Interface States
- eqn(12)
- Fig. 5 – Detailed energy-band diagram
- eqn(13) to eqn(26)
- Image-Force Lowering**
- eqn(27) to eqn(36)
- Fig. 13 – An energy-band diagram incorporating the Schottky effect
- Barrier-Height Adjustment
- Fig. 15 – Idealized controlled barrier conctact
- eqn(37) to eqn(42)
- Fig. 15 – Idealized controlled barrier conctact
- Ideal Condition
- Current Transport Processes
- Fig. 18 – Five basic transport processes under forward bias
- Thermionic-Emission Theory**
- eqn(43) to eqn(64)
- Diffusion Theory
- eqn(65) to eqn(72)
- Thermionic-Emission-Diffusion Theory**
- eqn(73) to eqn(78)
- Fig. 19 – An energy band diagram incorporating the Schottky effect
- eqn(79) to eqn(85)
- Tunneling Current**
- eqn(86) and eqn(87)
- Fig. 21 – Theoretical and experimental current-voltage charateristic
- Fig. 22 – Saturation current density versus doping concentration
- Fig. 23 – The ratio of tunneling current component
- Fig. 24 – Energypband diagrams showing qualitatively tunneling currents in a Schottky diode
- eqn(88) to eqn(96)
- Minority-Carrier Injection
- eqn(97) to eqn(100)
- Fig. 25 – An Energy-band diagram of an epitaxial Schottky barrier
- eqn(101) to eqn(106)
- MIS Tunnel Diode
- eqn(107) to eqn(109)
- Measurement of Barrier Height
- Current-Voltage Measurement
- eqn(110) to eqn(115)
- Activation-Energy Measurement
- eqn(116)
- Capasitance-Voltage Measurement
- eqn(117)
- Photoelectric Measurement
- Fig. 33 – 1/C2 versus applied voltage
- eqn(118) and eqn(119)
- Measured Barrier Heights
- Current-Voltage Measurement
- Device Structures
- Fig. 36 – Barrier heights on n-type Si and GaAs
- Fig. 37 – Various metal-semiconductor device structure
- eqn(120) to eqn(125)
- Fig. 42 – A plot of small-signal equivalent circuit of a Schottky diode
- Ohmic Contact
- eqn(126) to eqn(129)
- Fig. 43 – Dependence of specific contact resistance on doping concentration
- eqn(130) to eqn(132)
- Problems 1 to 13
- Thermionic-Emission Theory**
- Fig. 18 – Five basic transport processes under forward bias
- Metal-Insulator-Semiconductor Capacitors
- Introduction
- Ideal MIS Capacitor
- eqn(1a)
- Fig. 1 – An Illustration of a MIS capacitor
- Fig. 2 – Energy-band diagram of ideal MIS capacitor at equilibrium
- Fig. 3 – Energy-band diagram for ideal MIS capacitor under different bias
- eqn(1b)
- Surface Space-Charge Region
- eqn(2) to eqn(4)
- eqn(5a) and eqn(5b)
- eqn(6a) and eqn(6b)
- eqn(7) to eqn(22)**
- Fig. 5 – Variation of space-charge density in the semiconductor
- Ideal MIS Capacitance Curves
- eqn(23)
- Fig. 6 – (a) A band diagram of an ideal MIS Capacitor under strong inversion
- eqn(24) to eqn(27)
- Low-Frequency Capacitance
- eqn**(28)
- Fig. 7 – MIS C-F curves (a) Low frequency, (b) Intermediate frequency, (c) high frequency
- eqn**(29) to eqn(35
- High-Frequency Capacitance
- eqn(36) and eqn(37)
- Fig. 8 – In strong inversion, capacitance is a fuction of the small-signal frquency
- Fig. 9 – The frequency effect on C-V curve of MIS capacitor
- eqn(38) and eqn(39)
- Fig. 10 – A plot of the maximum depletion-layer width WDm versus the impurity concentration of semoconductors Si and GaAs
- eqn(40) and eqn(41)
- Fig. 11 – (a) Ideal C-V curves of MIS capasitor with respect to versus oxide thickness
- Silicon MOS Capacitor
- Fig. 12 Critical parameters of ideal Si-SiO2 MOS capacitors as a function of doping level and oxide thickness
- Interface Traps
- Fig. 13 Terminology for charges associated with thermally oxidized
- eqn(42a) and eqn(42b)
- eqn(43) to eqn(48)
- Fig. 15 Equivalent circuits including effects of the interface trap Cu and Ru
- Fig. 13 Terminology for charges associated with thermally oxidized
- Measurement of Interface Traps
- Fig. 16 (a) Influence of interface traps on high-frequency and low-frequency C-V curves
- eqn(52) and eqn(53)
- High-Low Frequency Capacitance Method
- eqn(54) and eqn(55)
- Conductance Method
- eqn(56) to eqn(58)
- Fig. 17 A comparison of capacitance and conductance measurement of the MOS capacitor
- eqn(59)
- eqn(60a) and eqn(60b)
- Fig. 20 Variation of trap time constant 𝜏it versus energy T=300K
- Fig. 23 Gp/𝜔 versus frequency for a Si-SiO2 MOS capacitor biased in depletion region
- Oxide charges and Workfunction Difference
- eqn(61) to eqn(65)
- Fig. 24 (a) High-ferquency C-V curve(on p-semiconductor)
- eqn(62)
- Fig. 25 (a) For Qf >0, the thickness of depletion layer W is smaller than that of Qf =0
- eqn(63)
- Fig. 27 Solution concentration versus depth in SiO2
- eqn(64) and eqn(65)
- Workfunction Difference
- eqn(66) and eqn(67)
- Fig. 28 (a) Band diagram at flat band 𝜙ms=0
- Fig. 29 Colleration of (a) flat-band voltage form capacitance measurement
- Fig. 30 Workfunction different 𝜙ms versus doping
- Fig. 31 C-V curves of a p-type MOS device
- Accumulation and Inversion-Layer Thickness
- Classical Model (CL)
- eqn(68) and eqn(69)
- Quantum-Mechanical (QM) Model
- Fig. 32 Classical calculation of potential and carrier profiles
- Fig. 33 (a) Constant energy surfaces for conduction band of Si
- eqn(70) and eqn**(71)
- Fig. 34 (a) The calculated conduction band
- Fig. 35 Electron concentration of an type MOS capacitor
- Fig. 36 Spatial distribution of electron concentration versus the different thickness of SiO2
- eqn(72)
- Fig. 37 Average displacement of electron from the semiconductor surface as a function of applied voltage
- Fig. 38 For an n-type MOS capacitor with n+ – polysilicon gate
- Fig. 39 QM calculation of capacitance reduction
- Fig. 40 A comparison of the simulated and measured C-F curves for CL and QM Model
- eqn(73) and eqn(74)
- Carrier Transport in MOS Capacitor
- Carrier Transport
- eqn(75)
- Table 3 Basic Conduction Processes in Insulator**
- Tunneling
- Thermionic emission
- Frenkel-Poole emmison
- Ohmic
- Ionic conduction
- Space-charge-limited
- Fig. 41 Energy-band diagram showing conduction mechanism
- eqn(76) and eqn(77)
- Fig. 42 Current density versus 1/T for Si3N4 and SiO2 films
- Fig. 43 Current voltage characteristics of Au-Si3N4-Si
- eqn(78) to eqn(85)
- Fig. 44 The Optimal coefficient (a)Co (b)C1
- Fig. 45 The calculated IG using the model with the CL
- Carrier Transport
- Nonequilibrium and Avalanche
- Fig. 46 Energy band diagram for s MOS Capacitor
- Fig. 47 Band diagram of an ideal MIS capacitor
- Fig. 48 Breakdown voltage of the MOS capacitor
- Fig 49 Electric field and the edge of the depletion region
- Fig 50 Capacitance and conductance versus the applied voltagefor a MOS capacitor
- Dielectric Breakdown
- eqn(86)
- Fig 51 Percolation theory breakdown occurs when randomly
- eqn(87)
- Fig 51 Time to breakdown tBD versus electric field of SiO2
- Fig 52 The breakdown electric field versus oxide thickness in SiO2
- Problems 1 to 23
- Interface Traps
- Fig. 12 Critical parameters of ideal Si-SiO2 MOS capacitors as a function of doping level and oxide thickness
- Thermal Instability
- Ideal Case– – Shockley Equation
- Built-In Potential and Depletion-Layer Width
- Bipolar Transistors
- Introduction
- Static Characteristic
- Basic Current-Voltage Relationship**
- Fig 1 Symbols and nomenclatures
- Fig 2 Three biasing configuration of n-p-n transistor in the normal mode
- Fig 3 An n-p-n transistor biased in the normal operating condition
- eqn(1) to eqn(17)**
- Fig 4 (a) A contour plot of a cross-sectional view of a process simulated n-p-n transistor
- Current Gain
- eqn(18) to eqn(34)
- Table 2 – Conventional Parameters for Bipolar Transistor
- eqn(35) to eqn(43)
- Output Characteristics
- Fig 9 A plot of the measured current gain versus as a function of different collector doping concentration
- Fig 10 Electron-density profiles in the neutral base of an n-p-n transistor for various applied voltages
- Fig 11 Output characteristic of an n-p-n transistor in (a) common base configuration and (b) common-emitter configuration
- eqn(44) to eqn(47)
- Nonideal Effect
- Emitter Bandgap Narrowing
- eqn(48)
- eqn(49a) and eqn(49b)
- eqn(50) and eqn(51)
- Kirk Effect
- Fig 14 Electric field distributions as a function of distance for various collector current densities
- eqn(52) to eqn(56)
- Fig 15 The space-charge region showing the effective base width widening at high current
- eqn(60) to eqn(62)
- Fig 14 Electric field distributions as a function of distance for various collector current densities
- Compact Models of Bipolar transistors
- The Ebers-Moll Model**
- eqn(63)
- Fig 17 An equivalent circuit model of an n-p-n bipolar transistor
- eqn(64) to eqn(71)**
- The Gummel-Poon Model**
- eqn(72) to eqn(77)
- Fig 18 An equivalent circuit diagram of Gummel-Poon model
- eqn(78) to eqn(88)
- The MEXTRAM and VIBC Models
- The MEXTRAM Model
- eqn(89)
- The VBIC Model
- The MEXTRAM Model
- The HICUM and others Models
- The HICUM Model
- Table 3**
- The MODELLA Model
- The UCSD HBT Model
- Fig 20 Two different equivalent circuits of a lateral p-n-p bipolar transistor
- The HICUM Model
- The Ebers-Moll Model**
- Microwave Characteristics
- Cutoff Frequency
- eqn(90)
- Fig 21 Schematic circuits to analysis cutoff frequency
- eqn(91) to eqn(97)
- Fig 22 A reduction of base charging time by Gaussian and exponential base profiles
- Fig 23 Deviation of the space-charge density and width in the collector due to injected electrons
- eqn(98) to eqn(102**)
- Fig 24 (a) Cutoff frequency as a function of collector density (b)A plot 1/fT versus 1/Jc to separate the current dependence
- eqn(103) and eqn(104)
- Fig 25 The open circles are measured cut off frequency versus the collector current
- Small-Signal Characterization
- eqn(105)
- Fig 26 Two-port network showing incident waves
- eqn(106)**
- Fig 27 (a) s11 and (b) s22 traces at VBE = 0.8V and 1.0V, and VCE = 2.0V
- Table 4 List of RMS Errors of s-Parameters of the Gummel-Poon and VBIC Models
- eqn(107) to eqn(120)
- Fig 28 Simplified small-signal equivalent circuits
- eqn(121) to eqn(124)
- Switching Characteristic
- Fig 29 (a) QB and JC response to a step base-current input
- eqn(125) to eqn(128)
- Fig 29 (a) QB and JC response to a step base-current input
- eqn(125) to eqn(128)
- Device Geometry and Performance
- Fig 30 A bipolar transistor with a Schottky clamp to reduce minority-carrier injection
- Fig 31 Cross-section of Si bipolar transistors (a) A conventional structure (b) A modern single-poly structure with deep trench isolation
- Cutoff Frequency
- Emitter Bandgap Narrowing
- Related Device Structures
- Power Transistor
- High-Voltage Limit
- High-Current Effects
- Fig 32 (a) Common-emitter I-V curves showing quasi-saturation at high current and low VCE
- eqn(129) to eqn(133)
- Thermal Runaway
- Second Breakdown
- eqn(134) and eqn(135)
- Fig 33 (a) Common-emitter I-V characteristics showing the second break-down at high voltage and high current
- Fig 34 The second-break-down triggering time versus applied pulse power for various ambient temperature To
- Safe Operating Area
- Fig 35 An Examaple of safety operating area (SOA) for power transistor operation
- eqn(136)
- Fig 35 An Examaple of safety operating area (SOA) for power transistor operation
- Basic Bipolar Transistor Logic Circuits
- Fig 36 Logics via different bipolar integrated circuits (a) An inverter or amplifier (b) an emitter-coupled logic (c) transistor-transistor logic (d) an integrated-injection logic
- ECL
- TTL
- IIL
- BiCMOS
- Power Transistor
- Heterojunction Bipolar Transistor
- eqn(137) to eqn(139)
- Fig 37 A comparison of doping profiles of homojunction and heterojunction bipolar transistors
- Fig 38 Energy-band diagram of heterojunctionbetween a larger bandgap n-type emitter and smaller p-type base
- Fig 39 An energy-band diagram for (a) the abrupt HBT (b) the graded HBT (c) the graded DHBT
- eqn(140)
- eqn(137) to eqn(139)
- Double-Heterojunction Bipolar Transistor
- Fig 40 (a) Typical structure of an HBT (b) A special structure using collector-up to minimze the collector capacitance
- Fig 41 (a) VCE offset existing in an HBT
- Graded-Base Bipolar Transistor**
- eqn(141) to eqn(145)
- Hot-Electron Transistor
- Fig 42 The measure Early voltage versus the reciprocal temperature
- Fig 43 (a) Electron group velocity as function of energy above the conduction band
- Self-Heating Effects
- Fig 44 Other form of hot-electron transistors
- eqn(146)
- Fig 45 Measured current gain versus the collect current with respect to the substrate temperature
- Fig 46 A cross section view of the fabricated InGaP HBT
- Fig 47 The measured and simulated IC – VCE
- Fig 48 The OIP3 versus the collector current density
- Fig 44 Other form of hot-electron transistors
- Abrupt Junction
- Problems 1 to 11
- MOSFETs
- Introduction
- Field-Effect Transistors: Family Tree
- Fig 3 The distintion between (a) FET and (b) PET
- Fig 4 Family tree of field-effect transistor
- Version of Field-Effect Transistors
- Fig 5 Versions of MOSFETs their transfer (ID_VG) and ouput (ID-VD) Characteristics
- Field-Effect Transistors: Family Tree
- Basic Device Characteristics
- Fig 7 (a) Schematic diagram of an n-channel enhancement-type MOSFET
- Inversion Charge in Channel**
- Fig 8 2-D energy-band diagrams of an n-channel MOSFET
- eqn(1) to eqn(5)
- Fig 9 Comparison of change distribution(in log scale) and energy band variation of an inverted p-region
- eqn(6) to eqn(14)
- Charge-Sheet Model
- eqn(15) to eqn(20)
- Current-Voltage Characteristics
- eqn(21) to eqn(24 )
- Constant Mobility**
- eqn(25)
- Fig 10 The position of integration from the source end to the drain end
- Fig 11 An ideal output characteristic of drain current versus drain voltage (ID versus FD)
- Fig 12 An n-channel MOSFET operated
- eqn(26) to eqn(39 ); eqn(28)**
- Velocity-Electric-Field Relationship
- Fig 13 𝜈 –E relationship for n=1 and 2
- eqn(40)
- Fig 13 𝜈 –E relationship for n=1 and 2
- Electric-Field Dependent Mobility: Two-Piece Linear Approximation
- eqn(45) to eqn(51)
- Velocity Saturation
- eqn(52) to eqn(54)
- Fig 14 A comparison of I-V characteristic for (a) constant mobility (b) the velocity saturation
- Ballistic Transport
- eqn(55) to eqn(60)
- Fig 16 Injection velocity vinj and inversion charge
- eqn(59) and eqn(60)
- Threshold Voltage
- eqn(61) to eqn(63)
- Subthreshold Region
- Fig 17 A plot of the dependent relation between deltaVT
- Fig 18 Transfer characteristics (ID versus VG)
- eqn(64) and eqn(65)
- Fig 19 A zoom in plot of Fig 9b
- eqn(66) to eqn(70)
- Fig 20 Experimental subtreshold characteristic
- Fig 21 The subtreshold swing versus a with respect to different substrate reverse bias.
- eqn(71) to eqn(74)
- Fig 22 Theoretical (dots) and experimental (solid lines) drain characteristic of a p-MOSFET with d=200
- Mobility Behavior
- eqn(75)
- Fig 23 Electron and hole inversion-layer mobilities
- Fig 24 Electron surface drift velocity versus longitudinal field
- Temperature Dependence
- eqn(76) to eqn(80*)
- Fig 25 The calculated lattice temperature shift of a 0.5𝜇m n-type MOSFET
- eqn(79) and eqn(80)
- Fig 26 The threshold-voltage shift(dVT/dT)
- Fig 27 Experimental measurement of deltaVT versus temperature
- Fig 28 Plot of the computed subthresfold of the 0.5𝜇m n-type MOSFET
- Nonuniform Doping and Buried-Channel Device
- Fig 29 Plot ID versus VG curves of the 1.5𝜇m n-MOSFET
- Fig 30 Nonuniform channel doping profiles N(x) deep from the surface of channel to the substrate
- eqn(81) and eqn(82)
- High-Low Doping Profile
- eqn(83) to eqn(104)
- Low-High Doping Profile
- eqn(105) and eqn(106)
- Buried-Channel Device
- eqn(107) and eqn(110)
- Table 1** – List of Drain Current Equations
- eqn(111 and eqn(112)
- Device Scalling and Short-Channel Effects
- Device Scalling
- eqn(113) and eqn(114)
- Charge Sharing from Source/Drain
- eqn(115) to eqn(123)
- eqn(124a and eqn(124b)
- Channel-Length Modulation
- Drain-Induced Barrier Lowering (DIBL)
- eqn(125) and eqn(126)
- Characteristic Fluctuation
- eqn(127) and eqn(128)
- Multiplication and Oxide Reliability
- eqn(129) to eqn(132)
- Device Scalling
- Mosfet Structures
- Channel Doping Profile
- Gate Stack
- eqn(133)
- Source/Drain Design
- Schottky-Barrier Source/Drain
- Raised Source/Drain
- SOI and TFT
- SOI
- TFT
- eqn(134) and eqn(135)
- Three-Dimensional Structures
- Power MOSFETs
- DMOS
- LDMOS
- Circuit Applications
- Compact Models of MOSFETs
- Equivalent Circuit and Microwave Performance
- eqn(136) and eqn(137)
- **eqn()
- eqn(138) to eqn(143)
- Basic Circuit Blocks
- eqn(144)
- NCFET and TFET
- Negative-Capasitance Field-Effect Transistor
- eqn(145)
- Tunneling Field-Effect Transistor
- eqn(146)
- Fig. 81
- eqn(146)
- Negative-Capasitance Field-Effect Transistor
- Single-Electron Transistor
- eqn(147) to eqn(159)
- Introduction
- Nonvolatile Memory Devices
- Introduction
- Mask-Programmed ROM
- PROM
- EPROM
- Flash EEPROM
- EEPROM
- Nonvolatile RAM
- The Concept of Floating Gate
- eqn(1) to eqn(6)
- Device structures
- The Floating-Gate Memory
- The Floating Trap of Charge-Trapping Memory
- eqn(7) to eqn(9)
- Compact Model of Floating-Gate Memory Cells
- The Classical Capacitive Model
- eqn(11) to eqn(17)
- The Charge-Balance Model
- eqn(18) and eqn(19)
- The Classical Capacitive Model
- Multi-Level Cells and 3-Dimensional Structures
- Multi-Level Cells
- Precise Control of the Amount of Charge Prorammed into the Memory Cell
- Precise Voltage or Current Sensing Circuit
- Stable Charges Sustenance of Long Retention
- 3-Dimensional (3-D) Structures
- Multi-Level Cells
- Introduction