BSIM Models: From MultiMulti-gate to symmetric BSIM6 Yogesh S. Chauhan, Sriram Venugopalan, Muhammed A. Karim, Pankaj Thakur, Navid Paydavosi, y , Ali Niknejad j and Chenming g Hu BSIM Group University of California, Berkeley March 16, 2012 MOS-AK Workshop, Delhi SPICE and Device Compact Models Prof. at UCB – SPICE designer (1925-2004) Prof. at UCB/Emeritus Prof Prof Prof. at CMU – CANCER designer which later led to SPICE development Ron R R Rohrer h Special Issue on 40th Anniversary of SPICE 2 SPICE Transistor Modeling for Circuit Simulation Medium of information exchange Simulation Time ~ 10μs per DC data point No complex p numerical method allowed Accuracy requirements ~ 1% RMS Error after fitting Excellent Convergence Example: BSIM4 25,000 lines of C code 200+ parameters Open-source software i implemented l d in i all ll EDA tools l 3 BSIM Family of Compact Device Models 1990 BSIM1 2 BSIM1,2 1995 2000 2005 2010 BSIM3 Bulk MOSFET BSIM4 New BSIM5 BSIM6 Silicon on Insulator BSIMSOI MOSFET BSIM-MG Multi-Gate Multi Gate MOSFET BSIM: Berkeley Short-channel IGFET Model 4 Bulk MOSFET Models New BSIM3 Threshold Voltage based MOSFET Model First Fi t CMC standard t d d Model M d l BSIM4 Threshold Voltage based MOSFET Model with enhanced physics features (mobility, BTBT, gate leakage…..) BSIM6 Charge based Symmetric MOSFET Model Charge Ch ge b based ed core o e BSIM4 physics models and parameters Under standardization review in CMC 5 BSIM6: Bulk MOSFET Model 6 Why new Bulk MOS Model: BSIM6 Harmonic Distortion Output spectrum of RF signal at frequency should only l contain i ffundamental d l frequency f Nonlinear MOS behavior adds other frequency components p ((at 2, 3 3 …)) visible above noise floor harmonic distortion Harmonics amplitude higher order derivatives of signal Negative g capacitance p from BSIM4 model may y cause convergence problem 7 Why new Bulk MOS Model: BSIM6 Taylor Series Expansion iout ( t ) f (V v(t )) f (V ) iout ( t ) f x x V 1 2 f v 2 x 2 1 3 f v 6 x 3 v 3 ... 2 x V x V RF design needs correct derivatives to predict harmonic distortion Incorrect derivatives=Wrong harmonic results Model must satisfy both DC & AC symmetry Method of testing derivatives Gummel Symmetry (DC) AC Symmetry BSIM4 simulationWrong derivatives around VDS=0 8 BSIM6: Charge based MOSFET model BSIM6 is the next BSIM Bulk MOSFET model Charge based core derived from Poisson’s solution Physical effects (SCE, CLM etc.) taken from BSIM4 Parameter names matched to BSIM4 parameters Gummel Symmetry (symmetric @ VDS=0) AC Symmetry Continuous in all regions of operations Physical y Capacitance p model Capacitances/derivatives are symmetric @VDS=0 Short channel CV– CV–Velocity saturation & other effects No glitches – smooth current and capacitance b h i behavior 9 Physics of BSIM6 Model Other models ignored circled terms 2nq 2qi ln(qi ) ln 2nq qi 2 2qi p p 2 f vch No approximation to solve the charge equation We solved the charge equation using first & second order NewtonNewton-Raphson p technique q to obtain analytical expression of qi 10 Drain current expression dQi dS VT I D I drift I diff W Qi dx dx Drain current Mobility model Using charge linearization & normalization ID v dQi dS VT W Qi 2 dx dx v dS 1 v dx sat Qi ID Qi 2 V , id , c v t nq P S , q W Cox 2nq CoxVT vsat L 2nq v CoxVt 2 L id q 2 s qs qd2 qd 1 2 1 1 c qs qd 2 11 Normalized IDS-VGS & derivatives Error (%) IDS vs VG Red – Numerical Surf. Pot. model Blue – BSIM6 model 2ndd derivative d i i 3rdd derivative d i i 1st derivative 12 BSIM6 Development Status BSIM6 development started in Q4 2010 First beta code was released in Jan. 2011 BSIM6.0.0 Beta7 was released on 28th Feb. 2012 to CMC members BSIM6 to cover all technology nodes and applications Continuously working with industry partners Digital – Accuracy in entire bias range Analog – Symmetry and accuracy in derivatives RF – Symmetry and harmonics Detailed BSIM6 technical presentation tomorrow 13 BSIM MultiMulti-Gate Models: BSIM--CMG BSIM BSIM--IMG BSIM 14 MOSFET in sub sub--22nm era FinFET UTBSOI Multi-Gate era has arrived Why new MOSFET structures? NY Times SOI Consortium: ST, SOITEC, … 15 Good Old MOSFET nearing Limits Sub-threshold swing (SS) & SubThreshold Voltage are bad Random dopant fluctuation Sensitive to gate length V i bilit iis an iissue Variability Requirements Low Vth and low Ioff Low Power Less variation Courtesy – Chenming Hu 16 Making Oxide thin is NOT enough! Gate can’t can t control the leakage paths far from the gate Drain has now much more influence compared to long channel! 17 Why not remove PATHS far from Gate? UTBSOI Y.-K. Choi et al., IEEE EDL, 2000 FinFET X. Huang et al., IEDM, 1999 18 Versatile Multi-Gate Compact Models P+ back-gate p-sub BG ETSOI BG-ETSOI Fin Gate e1 BOX UTBSOI Gate 2 BSIM-IMG Vertical Fin IMG BOX BSIM-CMG Lg G S D Tsi FinFETs on Bulk and SOI Substrates 19 BSIM--CMG BSIM 20 Common--Multi Common Multi--Gate Modeling Common MultiMulti-gate (BSIM (BSIM--CMG): All gates tied together Surface-potential Surfacepotential--based core II-V and CC-V model Supports doubledouble-gate, triple triple--gate, quadruple--gate, cylindrical quadruple cylindrical--gate; Bulk and SOI substrates 21 Surface Potential Calculation Vg Surface potential obtained by solving the 1D Poisson’’s equation Poisson Vs 2ψ qni 2 x εSi qV qφ qφB qψ B ch kT kT kT kT e e e e Body Doping Inversion Carriers n+ x y NA n+ Vd Vg A Perturbation approach is used to handle M. V. Dunga et al.,TED 2006 finite body doping ψ Net Surface Potential ψinv Inversion Carriers only ψ pert P t b ti due Perturbation d to t finite fi it doping d i 22 Surface Po otential (V V) Surface Potential Calculation 0.8 Symbols y : TCAD Lines : Model 0.4 1 15 Na = 1x10 18 Na = 1x10 18 Na = 3x10 18 Na = 5x10 0.0 -0 0.4 4 0.0 0.4 0.8 1.2 Gate Voltage (V) Model d l matches h 2 2D TCAD C very well ll without fitting parameters for different body doping. doping 23 I-V Model & Verification Drain current derived from driftdrift-diffusion -3 Dra ain Current (A) Drain n Currentt (A) Na = 3e18cm 1m Vg = 1.5V 500µ Vg = 1.2V Vg = 0.9V 0 0.0 0.5 1.0 Drain Voltage (V) 1.5 1m Na = 3e18 cm-3 Vd = 0.1 Vd = 0.2 Vd = 0.4 Vd = 0.6 500µ 0 0.0 0.5 1.0 1.5 Gate Voltage (V) M. V. Dunga, UCB Ph.D. Thesis 24 Drain Current in Volume Inversion Draiin Curre ent (A) 10µ µ Vds = 0.2V 10n -3 Na = 1e15 cm Tsi = 5nm Tsi = 10nm Tsi = 20nm 10p 10f 0.00 0.25 0.50 Li Lines: M Model d l Symbols: TCAD 0.75 Gate Voltage (V) In volume inversion Id TSi in sub sub-threshold. threshold. M. V. Dunga, VLSI 2007 25 1.0 -3 Na = 3e18cm Symbols : TCAD Lines : Model Vds = 1.5V Cgg 0.5 Csg Cdg 0.0 0.5 1.0 Gate Voltage (V) 1.5 Normalize ed Capacittance Normaliz zed Capaciitance C-V Model Verification 1.0 Cgg Model Symmetry Symbols : TCAD Lines : Model Cgs 0.5 Csg Na = 3e18 Vg = 1.5V 0.0 0.0 0.5 Cdg Cgd 1.0 1.5 Drain Voltage (V) C-V model ode agrees ag ees well e with t TCAD C without t out any fitting parameters. The transcapacitances p exhibit the correct symmetry behaviors. 26 BSIM--IMG BSIM 27 Independent--gate Device Structure: BSIM Independent BSIM--IMG Vfg Asymmetric structure Different Gate Workfunctions Allows dissimilar Gate Potentials Different Oxide thickness and Material ! F Front t Gate G t Tox1 Source y x Tsi Drain NA Tox2 Captures important C i features Threshold Voltage tuning through BackBack Gate Multi-Vth technology Vd Vs Back Gate Vbg 28 Surface Potential Calculation Analytical Solution for s is i k known VFG TOX1 Y. Taur, TED 2001 H. Lu et al., TED 2006 ΦM1 D S TOX2 Newton iteration needed for s calculation VBG ΦM2 Approximation for frontfront-, backback-surface potential and charge developed Better computational efficiency D. Lu D L att el., l "A computationally t ti ll efficient ffi i t compactt model d l for f fullyf ll depleted SOI MOSFETs with independently-controlled front- and back-gates," Solid State Electronics, 2011 29 Surface Potential: Verification with TCAD 0.7 Symbols: TCAD Front Surface Pote ential (V) Front S Surface Poten ntial (V) 0.8 Lines : Model 0.6 0.5 Tox2 Tox2 Tox2 Tox2 T 2 Tox2 0.4 0.3 0.2 0.1 0.0 -0.4 -0.2 0.0 0.2 0.4 = = = = = 40 nm 20 nm 10 nm 5 nm 2.5 2 5 nm 0.6 0.8 1.0 Front Gate Voltage (V) 0.9 0.6 Vch = 0.0 V Vch = 0.3 V Vch = 0.6 V Vch = 0.9 V 0.3 0.0 Tox1=1.2nm Tox1=1 2nm Tox2 = 20nm Tsi = 15nm Vbg = 0 -0.3 0.0 0.5 1.0 Front Gate Voltage (V) Front S Surface Pote ential (V) 0.9 0.8 0.7 0.6 05 0.5 Symbols: TCAD Lines : Model Scalable w.r.t. physical parameters like Tsi, Tox (front and back) and node voltages etc. T ox2=1.2nm 0.4 0.3 Tsi Tsi Tsi Tsi 0.2 0.1 00 0.0 -0.1 -0.2 -0.4 -0.2 0.0 0.2 0.4 = = = = 5 10 15 20 0.6 nm nm nm nm 0.8 Front Gate Voltage (V) 1.0 30 Drain Current Model Drain Current W I ds L Qinv , s Qinv ,d s1,d s1,s kT Qinv,s Qinv,d 2 q Drift Diffusion 2 2 si Es 2 Qinv 2 si Es 2 Qinv: inversion carrier density Es2: back-side electric field ψs1: front-side surface potential Very high accuracy No Charge-sheet Approximation 250 200 Errror Relative to o TCAD (%) 15 Drrain Current (A) Vfg = 0.2v, 0.4v, 0.6v, 0.8v, 1.0v Charge sheet This Work TCAD 150 100 50 0 0.0 0.2 0.4 0.6 Drain Voltage (V) 0.8 1.0 Charge-sheet Model This Work 10 5 0 -5 -10 -15 -0.5 0.0 0.5 1.0 Front Gate Voltage (V) 31 Capacitance Model Model inherently exhibits symmetry Cij = Cji @ Vds= 0 V Model overlies TCAD results No tuning parameters used Toxf = 1.2nm, Toxb = 20nm, Tsi = 15nm, Vbg = 0 V 1.0 Vfg = 0.8V, 0 8V Vbg = 0 V 0.4 0.3 Cds Csd Css Cdd 0.2 0.1 0.0 0 0 0.0 0.2 0.4 0.6 Drain Voltage (V) 0.8 1.0 Normalized C N Capacitance Normalized Capacitance e 0.5 0.8 0.6 Tox1 = 1 1.2nm 2nm Tsi = 15nm Tox2 = 20nm Vbg = 0 V Cfg,fg 0.4 02 0.2 Cbg,fg 0.0 Cd,fg -0.2 -0.4 -0.5 Cs,fg 0.0 0.5 1.0 1.5 Front Gate Voltage (V) Symbols: TCAD Results; Lines: Model 32 Gummel Symmetry Test Drain Current Symmetry V fg=0.2 0.00 V fg=0.4 -0.02 V fg=0.6 V fg=0.8 08 -0.04 0 04 Vbg=0 3 3 3 d Ix / dVx (A / V ) 0.02 -0.06 -0.10 -0.05 0.00 0.10 Vx (V) Analog /RF Ready AC (charge) Symmetry 20 10 -1 dccsd / dVx (V ) V bg=0 16 V fg =0.2 12 8 V fg =0.6 V fg =0.8 V fg =0.4 4 0 -0.10 -0.05 8 V bg=0 V fg =0.2 =0 2 -1 dcgg / dVx (V ) 0.05 0.00 Vx (V) 0.05 0.10 V fg =0.6 6 V fg =0.8 4 V fg =0.4 2 0 -0.10 -0.05 C. C. McAndrew, TED 2006 0.00 Vx 0.05 0.10 33 Real Device Effects Channel Length Modulation and DIBL Mobility Degradation g Velocity Saturation GIDL Current Short Channel Effects Core SPE I-V Q Quantum Effects Temperature T t Effects C-V Fringe Capacitances Impact Ionization current Direct tunneling gate current S/D Resistance/ Parasitic Resistance Noise models Overlap capacitances 34 Short Channel Effects BOX P+ back-gate back gate p-sub BOX Lg↓ p-sub Vt Rolll-off (V) 0.00 -0.05 -0.10 Vds = 50mV Vds = 1.0V -0.15 -0.20 -0.25 -0.30 0 01 0.01 Symbols: TCAD Lines: Model 01 0.1 1 Lg (um) T = 8nm si Tbox = 4nm Scale L Length th 35 Self Heating Model Thermal Node: Rth/Cth methodology T Relies on Accurate physical modeling of Temperature Effects in the model Draiin Curren nt (A) 1000 800 Without Self Heating With Self Heating Vgs=1.0 600 Vgs=0.8 400 Vgs=0.6 g 200 Vgs=0.4 0 0.0 0.2 0.4 0.6 0.8 1.0 Vds (V) 36 BSIM--CMG: Global Extraction BSIM Validation on SOI FinFETs Hfin=60nm, Tfin=22nm, EOT=2nm, L=75nm, 85nm, 90nm, 235nm, 1um 37 BSIM--CMG: Global Extraction BSIM Validation on SOI FinFETs Hfin=60nm, =60nm Tfin=22nm, =22nm EOT=2nm 38 BSIM--IMG validation BSIM Measurement from CEA-LETI Tbox=145nm EOT=1.6nm L = 50nm Na=1e15 Vbg = 10V, 15V, 20V, 25V Id,lin -2 Id,lin 10 -3 10 -4 10 W=50 x 0 0.5 5m L = 50 nm -5 10 Vbg = 10v, 15v, -6 10 20v, 25v -7 10 Cross: Measurements Lines: BSIM-IMG -8 10 -9 10 Tsi= 8nm g22 = 5.0 50 Drain Current (mA) Drain n Current (A) -0.2 0.0 0.2 0.4 0.6 0.8 Gate Voltage (V) 1.0 W=0.5um x 50 g11 = 4.55 4 55 (fitted) 2.5 2.0 Cross: Measurements Lines: BSIM-IMG 1.5 Vbg = 10v, 10 15 15v, 20v, 25v Increasing Vbg 1.0 0.5 W=50 x 0.5m L = 50 nm 0.0 -0.4 -0.2 0.0 0.2 0.4 0.6 0.8 1.0 1.2 G t V Gate Voltage lt (V) 39 Summary BSIM6 – New bulk MOSFET model in BSIM family Ready for immediate use and under standardization at CMC BSIM-CMG and BSIM-IMG are Production Ready model BSIM-CMG BSIM CMG – First CMC standard FinFET Model BSIM-IMG submitted to CMC for standardization Physical, Scalable Core Models with plethora of Real Device Effects Available in Verilog-A code and validated on measurements from different technologies Available in major EDA tools Ready for Technology/Design Evaluation Verilog-A code and Well-documented Technical Manual 40