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Bias Generator Design for High Temperature: Understanding Transistor Biasing and Equations, Study notes of Electrical and Electronics Engineering

An in-depth analysis of bias generator design for high temperature applications. It covers various aspects such as transistor biasing, the bias generator equation, stacking low vt and high vt devices, and cascode or signal transistors bias. The document also discusses the impact of temperature on biasing and the importance of decoupling v biases.

Typology: Study notes

Pre 2010

Uploaded on 11/08/2009

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koofers-user-g7s 🇺🇸

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Download Bias Generator Design for High Temperature: Understanding Transistor Biasing and Equations and more Study notes Electrical and Electronics Engineering in PDF only on Docsity! 1 HIGH TEMPERATURE BIAS GENERATOR DESIGN Presented by : Chris Hutchens Oklahoma State University 2 Outline • Transistor • The Bias Generator Equation • VB1 and VB4 • VB3 and VB4 • Stacking Low VT and High VT devices • Stacking “zero” VT and Low VT devices • Start-up Circuit 5 SOI Square Law Point 1 a--- Square Law CAN TRANSITION TO MODERATE INVERSION Square Law ---M's ΔV > 250 to 300mV I1 = I2 = I 1 2 1 1 1 Veff1KPL @Wf I Δ⎟ ⎠ ⎞ ⎜ ⎝ ⎛= in Square Law 2 2 2 2 Veff2KPL @Wf I Δ⎟ ⎠ ⎞ ⎜ ⎝ ⎛= in Square Law 21 2 21 2 3 211 R 2 VVand ff I Δ=Δ ⎥ ⎥ ⎦ ⎤ ⎢ ⎢ ⎣ ⎡ −= β 4 9 f f 2 1 = is a nice ratio. I is proportional to μ Cox.! [ ] [ ] 122222 22 VVR VgmRVVIR Δ−Δ=⋅Δ=⋅ΔΔ= β ⎟ ⎠ ⎞ ⎜ ⎝ ⎛ −= 1 2 2 12 S S gm R where gm = βΔV2 gm is set by selecting R and device geometry. 6 Squqre Law Bias Equation Point 1b --- Current Setting or Long Channel Bias DESIRED to Stabilize gm. Constant “Self Gain” 12 2 12 2 VVRVgmVVIR Δ−Δ=Δ⋅=Δ−Δ= ⎟ ⎠ ⎞ ⎜ ⎝ ⎛ −=⎟ ⎠ ⎞⎜ ⎝ ⎛ Δ Δ−= 1 2 2 1 2 1 212 S S RV V R gm ---- Low TempCo R i.e. pos. tempCo combined with a neg. tempCo VB1 = VDD - |VTPL|- Veff VB4 = VSS + VTNL+ Veff • Improved Matching • Reduced 1/f noise • Improved PSRR • Higher gain M1 M2 VB1 VB4 7 Square Law Bias Equation Point 1c --- Constant “Veff or V swing” Long Channel Bias DESIRED to Stabilize Veff. 12 2 12 2 VVRVgmVVIR Δ−Δ=Δ⋅=Δ−Δ= ( )DDR VKPSS Sgm Δ⎟ ⎠ ⎞ ⎜ ⎝ ⎛ −= 1 2 2 12 ---- MOS Resistor Veff = √m (SR/S)VDD - VT) DDR R VKPS gmS Δ ⋅ = 4 2 3 ( )effVKPSgm Δ= 22 VB1 = VDD - |VTPL|- Veff VB4 = VSS + VTNL+ Veff 10 Peregrine 0.5um SOS VB3 and VB2 Point 2a --- Cascode or Signal Transistors Bias VB3 = VB4 + VGS3 - VGS4 VB3 = VB4 + VTNs + 2Veff –[ VTNs +Veff/2 ] = VSS + VTNL+ Veff + VTNs + 2Veff –[ VTNs|+Veff/2 ] = VSS + VTNL+ 3/2 Veff And VB4 = VDD- |VTNL| + Veff VDSSAT + SM where SM is 25 to 200 mV MUST REQUIREMENT!! Optional M3 M4 11 Peregrine 0.5um SOS VB3 and VB2 Point 3 --- Cascode or Signal Transistors VDSSAT VB3 ≈ VSS + VTNL+ 2 Veff And VB4 = VSS- VTNL + 2 Veff VDSSAT + 100mV to 250mV MUST REQUIREMENT!! Selecting W = 2 verse 1 fingers provides a 83% decrease in Veff Selecting W = 48 verse 32 fingers provides a 20% decrease in Veff. Now for a Veff of 250mV of the safety margin on the current source becomes 103% or approximately 250mV. M3 M4 12 m=9 m=4 m=1 Peregrine 0.5um SOS Constant Gain Bias Point 4a --- Gain CONTANT with Temp /ggm A Odiff= Do I g effλ= ( )effdiffdiff VKPSgm Δ= ( )DDR VKPSS SVI Δ⎟⎟ ⎠ ⎞ ⎜⎜ ⎝ ⎛ −Δ= 9 4 4 1 Proportional to mobility 40% decrease Temp 30 TO 200 0C ( ) 1 S A 9 4 4 diff λ α DDR eff VKPSS SV VKP Δ⎟⎟ ⎠ ⎞ ⎜⎜ ⎝ ⎛ −Δ Δ⋅⋅ 15 Peregrine 0.5um SOS Constant gm bias Point 5b --- Gm and BW CONSTANT with Temp effeff diff V S S R V V Igm Δ ⎟⎟ ⎠ ⎞ ⎜⎜ ⎝ ⎛ −Δ ⋅= Δ ⋅= 9 44 1 22 ⎟⎟ ⎠ ⎞ ⎜⎜ ⎝ ⎛ −⋅ 9 412 S S R gmdiff α Bandwidth α gm 16 Peregrine 0.5um SOS Startup Circuit Point 6a --- Startup Ckt Required Bias Loop gain < 1 Required Very Small Possibility but still possib Many Versions 2 Possible Solutions 8 2@Wp/ 17 Peregrine 0.5um SOS Startup Circuit Point 6b --- Startup Loop Gain > 1 16/ >⋅≈⋅⋅= RgmRgmAA fol R > 6/gm = 3 ΔV/I Select R > 10 ΔV/I for VDS feedback > VTL+ VTsp+ VTL This ensures that the follower will shut off! R I + VTL > VDD. R >4 [ VDD - VTL ]/I Check for Strong Pull down! R m=9 m=4 m=1 20 SOI Moderate Inversion Point 7--- Subthreshold and Moderate Inv. Moderate Inversion ---M1 in subthreshold and M2 ΔV = 0V I1 = I2 = I IRe−⎟ ⎠ ⎞ ⎜ ⎝ ⎛= s 1 1 IL W I in Subthreshold ⎥⎦ ⎤ ⎢⎣ ⎡ +⎟ ⎠ ⎞ ⎜ ⎝ ⎛=⎥⎦ ⎤ ⎢⎣ ⎡ +⎟ ⎠ ⎞ ⎜ ⎝ ⎛= Δ TT nUnU V ee 0 2 s 2 2 s 2 2 1LNIL W 1LNI L W I at VGS = VT ( ) ( ) [ ]2LNIf If 2s2s1 =− IRe [ ] [ ] 42LN2 LNf f 422 2 1 >== IReeIR I 4 R > Vs is proportional to the UT2. Caution ( )2 LNIsIV 2 S ⋅== RR Is = 2•β(nUT)2 21 SOI Weak Inversion & BJTs RB M1 M2 RB Q1 Q2 S S/m AE 8 AE Point 7--- Subthreshold and BJTs. Moderate Inversion ---M1 in subthreshold and M2 ΔV = 0V I1 = I2 = I; VBE1 = VBE2 + IRB TBE nUVe /s1 1 I I = in BJTs; or ⎥⎦ ⎤ ⎢⎣ ⎡⋅⋅= Is ILNUnV TBE ⎥ ⎦ ⎤ ⎢ ⎣ ⎡ ⋅⋅−⎥ ⎦ ⎤ ⎢ ⎣ ⎡ ⋅⋅= 21 Is ILNUn Is ILNUnIR TTB [ ] 28 1 2 ⋅ ⋅ =⋅ ⋅ =⎥ ⎦ ⎤ ⎢ ⎣ ⎡ ⋅ ⋅ = B T B T B T R Un LN R Un AE AE LN R Un I IPTAT – Current (I) Proportional To Absolute Temperature 22 Weak Inversion & BJTs IPTAT – Current (I) Proportional To Absolute Temperature Improved 25 SOI PSRR - plus Point 10--- Use of Long channel All regions • Decreased 1/f and thermal noise • Improved matching • Increased VA – o PSRR improved o ro and gain • Choice of cascode type depends on application circuit and best VA. I is proportional to μ Cox.! [ ] [ ] 22222 22 VR VgmRVVIR Δ⋅=⋅Δ=⋅ΔΔ= αβ 2 2 gm R ⋅= α gm is set by R Long Channel Long Channel Cascode Distribution I 4xWL/LL {mx4xWL}/LL I R = Veff2 /2 R =Veff/ m) R ={1/gm} m) =10K ohms w VB4 8xWL/LL 200 fF WL/LL I = gm Veff /2 = 10uA gm = 10ms, kpn = 150uA/ V^2 Ws/Ls >???? Lerr < 5.5% Werr < 0.24% 4xWL/LL 4xWS/LS Interdigitate 2 Inter digitate 4 VB4 {4xWL}/LL 10 uA/leg 10uA/leg \ I = 4/2 xWL/LL kp Veff^2 = 10uA WL/LL= VB1 4xWS/LS 4xWS/LS 4xWS/LS 4xWS/LS 4xWS/LS 4xWL/LL 10uA/leg 4xWS/LS {4xWL}/LL 4xWS/LS {Wmin}/LLmax VSS I R =Veff/ m) m=2 VDD > |VT| + 4Veff VB2 VB3 VB4 26 SOI Temperature Considerations Point 11--- What do you want at temperature? All regions • PTAT bias? • Constant gm • Constant Av or Constant Vpp Constant gain is not feasible in Subthreshold - VA/UT PTAT - provides constant gm or constant BW in Subthreshold. TnU Igm κ= but PTAT bias current in subthreshold is ⎟ ⎠ ⎞ ⎜ ⎝ ⎛⋅⎟ ⎠ ⎞ ⎜ ⎝ ⎛= Rf f I 2 1 TnULN R biased Square is constant gm or constant BW. What about Moderate inversion?? 4xWL/LL {mx4xWL}/LL I R = Veff2 /2 R =Veff/ m) R ={1/gm} m) =10K ohms w VB4 8xWL/LL 200 fF WL/LL I = gm Veff /2 = 10uA gm = 10ms, kpn = 150uA/ V^2 Ws/Ls >???? Lerr < 5.5% Werr < 0.24% 4xWL/LL 4xWS/LS Interdigitate 2 Inter digitate 4 VB4 {4xWL}/LL 10 uA/leg 10uA/leg \ I = 4/2 xWL/LL kp Veff^2 = 10uA WL/LL= VB1 4xWS/LS 4xWS/LS 4xWS/LS 4xWS/LS 4xWS/LS 4xWL/LL 10uA/leg 4xWS/LS {4xWL}/LL 4xWS/LS {Wmin}/LLmax VSS I R =Veff/ m) m=2 VDD > |VT| + 4Veff VB2 VB3 VB4 27 SOI Decouping of V Biases Point 12--- Be aware of slow bias nodes. All regions • "Slow is relative" • Add extra C - low Z long recovery • Active is best but not low power! o Nice use of low VT devices. Trim Pot Engineering
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