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NanoCMOS Effects and Analogue Circuits University of Edinburgh

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Presentation on theme: "NanoCMOS Effects and Analogue Circuits University of Edinburgh"— Presentation transcript:

1 NanoCMOS Effects and Analogue Circuits University of Edinburgh
Statistical Design and Verification of Analogue Systems NanoCMOS Effects and Analogue Circuits University of Edinburgh Wolfson Microelectronics

2 MOSFETs as analogue devices Static nano-effects Dynamic nano-effects
Agenda MOSFETs as analogue devices undergraduate level! Static nano-effects Dynamic nano-effects Drift … all as “cartoon-physics”

3 “Normal” MOSFET Met Met Met Poly Vgs>Vt P- N+ N+
Doping is (here, exceptionally!) uniform

4 “Normal” MOSFET Met Met Met Poly P- N+ - N+ - - - - - <v>
Terminal velocity … cf swimming through porridge <v>

5 “Normal” MOSFET Saturated On Off Linear Interactive MOSFET curves

6 Nanoscale MOSFET P- Poly Met N+

7 Nanoscale MOSFET P- Poly Met N+ c10-9M

8 Nanoscale MOSFET Crash sites Sources of statistical variability
Random discrete dopants Line Edge Roughness Grains in polysilicon Combined

9 Device number 1 Nanoscale MOSFET Met Met Met Poly P- N+ N+ -
crash sites - Device number 1

10 Device number 2, next door
Nanoscale MOSFET Met Met Met Poly P- N+ N+ - - Device number 2, next door

11 Nanoscale MOSFETs - mismatch
These devices are NOT THE SAME Nothing can make them the same, short of placing the dislocations, impurities and dopant atoms by hand and identically in every device The mismatch is intrinsic -

12 Nanoscale MOSFET Interactive MOSFET curves

13 Nanoscale MOSFET Current Mirror, Iin = Iout

14 Nanoscale MOSFET – solutions#1 - overdesign
Iin Iout

15 Nanoscale MOSFET – solution#2?
Iin Iout Iin Iout Vt Vt nanoscale variation of Vt, K’ Systematic variation of Vt, K’ X (distance)

16 Trapping in MOSFETs Met Met Met Poly P- N+ N+ - - - - trap release

17 Many traps, micro-scale device
Flicker noise Many traps, micro-scale device Constant succession of trapping and detrapping Flicker noise I t

18 Nanoscale MOSFET Interactive MOSFET curves

19 nanoscale … Random Telegraph Signal noise
Few traps, nano-scale device, discontinuous Sudden discontinuities in Ids hence “Telegraph Signal “ Ids t

20 Nanoscale MOSFET I2 I1

21 no trapped charge with trapped Random doping I-V curve extraction
2 compact models (BSIM4) per device no trapped charge with trapped Random doping I-V curve extraction

22 Method – single trap Initialise trap states and bias conditions
Two compact models: 1) trap filled 2) trap empty Select model (1) or (2) Initialise circuit SPICE simulation Store SPICE nodal voltages Recalculate trap occupancy based o probability of trapping

23 4-quadrant multiplier

24 4-quadrant multiplier

25 Single RTS-noisy MOSFET

26 30x RTS-noisy MOSFET

27 Negative Bias Temperature Instability (NBTI) Effects
Met Met Met Poly V<0 E N- P+ P+ + + E Vdd Vgs<Vdd E→E – E Trapped charge works against Vgs E-field causing inversion is reduced Threshold Vt is raised

28 Negative Bias Temperature Instability (NBTI) Effects
Most prevalent in pMOS devices when a negative voltage is applied to the PMOS gate this is the “stress voltage” Capture of positive charge carriers (holes) at the Si-SiO2 interface → positive (trapped) charge Threshold Voltage Vt is raised Removal of the stress removes some traps partial recovery

29 Negative Bias Temperature Instability (NBTI) Effects
Vt of pMOSFETs at different temperatures (500MHz, Vdd = 1.2).


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