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Band Gap Regulator Analysis J. R. Biard, Ph.D. Honeywell 9/10/02 1 Silicon Band Gap The band gap of silicon changes with temperature 4 .7 3 10 4 T 2 E G 117 . T 636 Between -40oC and 200oC this can be fit with a linear equation to within ± 1.5meV EG 1.20585 2.745 10 4 T 2 Silicon Band Gap 1.22 1.6 1.2 EG = -2.74471E-4T + 1.205852 1.18 0.8 1.16 0.4 1.14 0.0 2 EG = 1.17-(4.73E-4*T )/(T + 636) 1.12 -0.4 1.10 -0.8 o -40 C 1.08 o o 200 C 25 C 1.06 0 100 200 300 EG (meV) Band Gap (eV) 1.20 400 -1.2 -1.6 500 o Temperature ( K) 3 Transistor Equation For an NPN bipolar transistor the collector current is given by dn dn nx 0 IC A e qDn , dx dx W b 2 ni qVbe nx 0 no exp , no kT NA 4 Transistor Equation Combining these expressions gives 2 ni qVbe IC A e qDn exp kT W NA 2 ni kT qEG AT exp n , Dn kT q 3 5 Transistor Equation The intrinsic carrier density expressed in terms of the linear fit to the band gap is given by n i2 2 ni q EGo mT AT exp kT 3 qEGo qm 3 A exp k T exp kT 6 Transistor Equation -40oC and 200oC the intrinsic carrier concentration is given by Between 2 ni qE Go A' T exp kT 3 Thus, silicon behaves as though it had a constant band gap of EGo. Constant band gap is used in PSPICE but the default value is wrong (1.11eV). 7 Transistor Equation Silicon mobility follows a power law with absolute temperature; the exponent is a function of the doping level. To n o T The same general form also works for P-type material 8 Transistor Equation /sq P-type resistor is PTAT Proportional To Absolute Temperature. This resistor gives a constant collector current in a band gap regulator. All other resistors require a temperature dependent collector current. A 2000 To I C I Co T 9 Transistor Equation Combining all these equations gives the form of the transistor equation needed for the band gap regulator 3 qE V T ICo A e A 'kT o To T exp W b NA Go be kT A e A 'k o 4 q EGo Vbe ICo T exp kT W N T b A o 10 Differential Equation Taking the derivative of the transistor equation with respect to temperature gives a differential equation dVbe E Go Vbe k 4 q dT T This nonlinear differential equation can be solved using an integration factor. 11 Differential Equation Solve the differential equation for Vbe T kT T Vbe E Go E Go Vbeo 4 ln q To To Where Vbeo is the value of Vbe @ To Vbe is a linear function of T only when (4 + - ) = 0. 12 Transistor Model PSPICE the term (4 - ) is called XTI, EGo is called EG and must be set to EG = 1.2058; PSPICE uses 1.11. Modeling Honeywell NPN transistors for PSPICE with EG = 1.2058 and = 0 gives XTI = 2.0599. = 4 - 2.0599 = 1.9401 In 13 Transistor Model = 100A and To = 298oK (25oC) linear regression of Vbe data between -40oC and 200oC gives: For IC dVbe Vbeo 0.67005 and 19978 . mV / o C dT The error between measured Vbe and the best straight line fit over temperature is ±2.0mV 14 Transistor Model 1.20 6 1.00 4 0.80 2 0.60 0 0.40 -2 0.20 -4 0.00 -6 200 -50 -25 0 25 50 75 100 125 150 175 Vbe Deviation (mV) Vbe (V) Vbe = -1.9978E-3(T-25) + 0.67005 o Temperature ( C) 15 Band Gap Regulator For a PTAT resistor in series with a diode connected transistor biased to Vref the drop across the resistor is PTAT regardless of the value of the resistor. For a zero TC resistor the resistor current and voltage are both PTAT, = 1, Vref is different, and the variation with temperature is greater. 16 Band Gap Regulator Vref = 1.2654V PTAT Resistor Resistor voltage is PTAT independent of resistor value. @ 0.1mA, Vbe = 0.6701V @ 1.0mA, Vbe = 0.7292V (dVbe/dT) drops by 0.1984mV/oC 17 Band Gap Regulator PTAT Resistors 5.953K & 3.0K 1.0 2.5 2.0 Vb = 1.266V 0.8 1.5 0.7 1.0 VR1 (V) 5.953K 3.0K 0.6 0.5 0.5 0.0 0.4 -0.5 0.3 -1.0 0.2 -1.5 TC1 = 3.3557E-3 TC2 = 0 0.1 Error Voltage (mV) 0.9 -2.0 0.0 -2.5 -40 10 60 110 160 o Absolute Temperature ( K) 18 Band Gap Regulator Implant Resistors 5.953K & 3.0K 1.0 5 Vb = 1.266V 0.9 4 0.8 3 5.953K 0.7 2 VR1 (V) 3.0K 0.6 1 0.5 0 0.4 -1 0.3 -2 TC1 = 3.660E-3 TC2 = 7.030e-7 0.2 -3 0.1 -4 0.0 -5 -40 10 60 110 160 o Absolute Temperature ( K) 19 Band Gap Regulator The voltage difference between the Vbe values of two transistors operated at different current density has a positive linear temperature coefficient and Vbe has a nearly linear negative temperature coefficient. These two characteristics can be combined to give a near zero temperature coefficient voltage source. 20 Differential Equation Taking the derivative of the transistor equation with respect to temperature gives a differential equation dVbe E Go Vbe k 4 q dT T This nonlinear differential equation can be solved using an integration factor. 11 Band Gap Regulator When the collector (emitter) current is changed by a factor of 10 at 298oK (25oC) the Vbe changes by 59.13mV and dVbe/dT changes by 0.1984mV/oC. Thus, the difference in Vbe of two transistors operated at a 10/1 current density ratio is proportional to absolute temperature. 21 Band Gap Regulator The band gap regulator is a compact analog computer that solves for a constant reference voltage (~EGo). The +0.1984mV/oC temperature coefficient difference between two junctions operated at 10/1 current density must be multiplied by 10.070 to equal the dVbe/dT of -1.9978mV/oC. 22 Band Gap Regulator Vbe difference of 59.13mV @ 25oC must also be multiplied by 10.070 which gives a voltage of 0.5953V. Adding this voltage to Vbeo = 0.6701V gives a reference voltage of 1.2654V. This reference voltage is equivalent to Vref = EGo + 2.32(kTo/q) @ 25oC. The 23 Band Gap Regulator The positive TC voltage that must be added to the Vbe to get the reference voltage is proportional to absolute temperature. With a 2000/sq implanted resistor which is proportional to absolute temperature the collector current is constant and = 0. 24 Band Gap Regulator The deviation of Vref from its nominal value over the temperature range is of the order of the ±2.0mV deviation in the Vbe from the best straight line fit. For smaller temperature ranges the best value of Vref is slightly different and the deviation from nominal is less. 25 Band Gap Regulator 26 Band Gap Regulator 27 Band Gap Regulator 28 Band Gap Regulator PTAT Resistors 29 Band Gap Regulator PTAT Resistors 1.2775 1.35 1.2770 TC1 = 3.3557E-3 TC2 = 0 EG = 1.2058V XTI = 2.0599 1.2765 1.33 1.2755 1.31 1.2750 1.2749V 1.2745 VBG (V) VBG (V) 1.2760 1.29 1.2845V 1.2740 EG = 1.110V XTI = 3.0 1.2735 1.27 1.2730 1.2725 1.25 -40 10 60 110 160 o Temperature ( C) 30 Band Gap Regulator 31 Band Gap Regulator Implant Resistors 32 Band Gap Regulator Implant Resistors 1.2735 1.33 TC1 = 3.660E-3 TC2 = 7.030e-7 1.2730 1.2725 EG = 1.2058V XTI = 2.0599 1.31 1.2720 1.30 1.2715 1.29 1.2715V 1.2843V 1.2710 VBG (V) VBG (V) 1.32 1.28 EG = 1.110V XTI = 3.0 1.2705 1.27 1.2700 1.26 1.2695 1.25 -40 10 60 110 160 Temperature ( oC) 33 Band Gap Regulator 34 Band Gap Regulator 35 Band Gap Regulator 36 Summary Know your circuit – What does it have to do? Know your simulator – When do you take exception to defaults? Characterize your devices in terms of the parameters used in your simulator – How were the measurements done? 37 PSPICE Models PTAT Resistor .MODEL Rptat RES (r=1.0 tc1=3.3557e-3 tc2=0) IMP Resistor .MODEL Rimp RES (r=1.0 tc1=3.6600e-3 tc2=7.0300e-6) NPN Transistor with N+ sinker, 10m x 10m emitter .MODEL QNPN NPN (is=8.41E-17 bf=1.928e+2 nf=1.00e+0 + vaf=1.046e+2 ikf=7.85e-3 ise=1.056e-18 ne=1.091e+00 br=3.257e+1 + nr=1.00e+0 var=1.052e+1 ikr=2.2775e-3 isc=4.1715e-15 + nc=1.752e+0 nk=5.00e-1 iss=0.00e+0 ns=1.00e+0 re=1.1025e+0 + rb=5.1475e+2 rbm=1.072e+2 rco=0.00e+0 vo=1.8519e+0 + gamma=1.1586e-10 qco=2.3742e-14 cje=1.80e-13 vje=7.40e-1 + mje=3.40e-1 cjc=5.9584e-14 vjc=6.00e-1 mjc=4.00e-1 xcjc=1.00e+0 + cjs=2.9648e-14 vjs=5.00e-1 mjs=3.10e-1 fc=5.00e-1 tf=2.1e-10 + xtf=0.00e+0 vtf=1.00e+2 itf=0.00e+0 ptf=0.00e+0 tr=1.00e-8 + eg=1.20585e+0 xtb=1.905e+0 xti=2.0599e+0 kf=0.00e+0 af=1.00e+0 + tre1=6.64e-4 tre2=-4.72e-7 trb1=4.00e-3 trb2=8.00e-6 trm1=8.24e-4 + trm2=5.13e-6 trc1=7.02e-3 trc2=1.91e-5) 38