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MOSFET SECOND ORDER
          EFFECTS
    GATE OXIDE THICKNESS REDUCTION




            Loren K. Schwappach
        EE660 Modern Electronic Design
              2 November 2011



1
Why Shrink MOSFETS
2

       70% Reduction of Line Width Results in 50% Reduction
        in Area (i.e. 0.7x0.7=0.49):
           Significantly Reduces Cost per Circuit
       Other Parameters Reduced as a Result:
           Power Supply Voltage
           Gate Oxide Thickness
       Changes Together Allow:
           Reduced Circuit Delays
           Historically Circuit Speed Has Increased 30% At Each Tech
            Node
Factors Affecting Scaling
3

       Requires Threshold Voltage Reduction
           Improves Propagation Delays
       Low Threshold Affects Noise Margins and Sub-
        Threshold Conduction
       Gate Oxide Thickness Reduction Increases Gate
        Leakage Due to Electron Tunneling and Hot Carrier
        Injection from Substrate to Gate
Scaling Parameters
4
Reducing the Gate Insulator
    Thickness
5

       SiO2:
           Preferred Gate Insulator from the Beginning
           TOX=300nm for 10um technology to 1.2nm for 65nm technology
           Thinner Oxides Result in Faster Circuits!
           Oxide Thickness has been Scaled Roughly in Proportion to Line
            Width
Problems Resulting From Reduced
    TOX
6

       Oxide Breakdown Caused By Electric Field
       Loss of Inversion Charge Due to Polysilicon Gate
        Depletion and Inversion Layer Quantization Effects
       Long Term Operation at High Field and High
        Temperatures Breaks Weaker Atomic Bonds:
           Creating Oxide Charge and VT Shifts
       SiO2 thinner than 1.5nm suffers from Extreme Tunneling
        Leakage
           Would Drain Battery of a Cell Phone in Minutes!
Transistor Leakage
7

       Increases in Leakage Power with Technology Scaling
How Are Defects Injected in
    Oxide
8

       Pinch-off Region Near Drain-Substrate Junction of n-
        channel MOSFET
PhotoInjection of Hot-Carriers
9
Gate Leakage
10

        Reduction in Oxide Thickness Results in Higher Electric
         Field
        Electrons can Tunnel Through Oxide, Causing Leakage
        Occurs when VOX < the Tunneling Barrier Height
Solutions to Shrinking TOX
11

        High-k dielectrics to replace SiO2
            Example: HfO2 has Dielectric Constant (k) of 24 (Six Times That
             of SiO2)
                Other Candidates Include ZrO2 and Al2O3
                Often Requires Inserting Thin SiO2 Interfacial layer Between Silicon
                 Substrate and High-k Dielectric to Reduce Unwanted Chemical
                 Reactions
Modifying the SPICE Model
12

        Note: PSPICE Levels 2-4 are only Accurate for Models
         >1um
        Recommended PSPICE Level 5 Model (Used for Short
         Channel Effects Correction) and Accounting for COX
        Scaling Factor from Ex 23 was .36 Going from 5V to
         1.8V Circuit (Adjusted VTO Accordingly)
        Original COX Set to 7E-4 (Default)
            COX = EOX/TOX
        Results to Analyze:
            How COX*2 Changes Effect Circuit Power Usage
            How COX*2 Changes Effect Circuit Speed
Schematic
13

                                GND_0                                  GND_0

                        GND_0

                                        VDD1                                   VDD2
                                        1.8Vdc                                 1.8Vdc
                           0


                        PMOS1                                  PMOS2




                        Mbreakp1                               Mbreakp2
                        W = 30u                                W = 30u
               VGate
                        L = .36u                               L = .36u
       GND_0
                                         Vout1                                  Vout2
               1.8Vdc

                        NMOS1                                  NMOS2

                                                         C1                                     C2
                                                         40p                                    40p

                        Mbreakn1                               Mbreakn2
                        W = 14.4u                              W = 14.4u
                        L = .36u                               L = .36u


                                GND_0            GND_0                 GND_0            GND_0
NMOS1 and PMOS1 Models
14
NMOS2 and PMOS2 Models
15
Results
16
Results
17
Results
18
Results
19
Conclusions
20

       PSPICE   Proved Useful For Analyzing Second
        Order Oxide Thickness Effects
       Lowering the Gate Oxide Thickness Reduced
        Power Usage (By 1mV During Switching)
       Lowering the Gate Oxide Thickness Also
        Decreased the Max Switching Frequency
        (6.3MHz to 6MHz)
       Scaling Parameters and Model Level Played a
        Huge Impact for Obtaining Usable PSPICE
        Results
       Gate Oxide Thickness Has a Tremendous Impact
        On the Power and Frequency of a Circuit
Questions?
21
References
22

        http://etd.library.vanderbilt.edu/available/etd-
         12032003-100902/unrestricted/Thesis.pdf
        http://www.smdp.iitkgp.ernet.in/PDF/TCAD/AK
         M.pdf

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Ee660 ex 25_second_order_effects_schwappach

  • 1. MOSFET SECOND ORDER EFFECTS GATE OXIDE THICKNESS REDUCTION Loren K. Schwappach EE660 Modern Electronic Design 2 November 2011 1
  • 2. Why Shrink MOSFETS 2  70% Reduction of Line Width Results in 50% Reduction in Area (i.e. 0.7x0.7=0.49):  Significantly Reduces Cost per Circuit  Other Parameters Reduced as a Result:  Power Supply Voltage  Gate Oxide Thickness  Changes Together Allow:  Reduced Circuit Delays  Historically Circuit Speed Has Increased 30% At Each Tech Node
  • 3. Factors Affecting Scaling 3  Requires Threshold Voltage Reduction  Improves Propagation Delays  Low Threshold Affects Noise Margins and Sub- Threshold Conduction  Gate Oxide Thickness Reduction Increases Gate Leakage Due to Electron Tunneling and Hot Carrier Injection from Substrate to Gate
  • 5. Reducing the Gate Insulator Thickness 5  SiO2:  Preferred Gate Insulator from the Beginning  TOX=300nm for 10um technology to 1.2nm for 65nm technology  Thinner Oxides Result in Faster Circuits!  Oxide Thickness has been Scaled Roughly in Proportion to Line Width
  • 6. Problems Resulting From Reduced TOX 6  Oxide Breakdown Caused By Electric Field  Loss of Inversion Charge Due to Polysilicon Gate Depletion and Inversion Layer Quantization Effects  Long Term Operation at High Field and High Temperatures Breaks Weaker Atomic Bonds:  Creating Oxide Charge and VT Shifts  SiO2 thinner than 1.5nm suffers from Extreme Tunneling Leakage  Would Drain Battery of a Cell Phone in Minutes!
  • 7. Transistor Leakage 7  Increases in Leakage Power with Technology Scaling
  • 8. How Are Defects Injected in Oxide 8  Pinch-off Region Near Drain-Substrate Junction of n- channel MOSFET
  • 10. Gate Leakage 10  Reduction in Oxide Thickness Results in Higher Electric Field  Electrons can Tunnel Through Oxide, Causing Leakage  Occurs when VOX < the Tunneling Barrier Height
  • 11. Solutions to Shrinking TOX 11  High-k dielectrics to replace SiO2  Example: HfO2 has Dielectric Constant (k) of 24 (Six Times That of SiO2)  Other Candidates Include ZrO2 and Al2O3  Often Requires Inserting Thin SiO2 Interfacial layer Between Silicon Substrate and High-k Dielectric to Reduce Unwanted Chemical Reactions
  • 12. Modifying the SPICE Model 12  Note: PSPICE Levels 2-4 are only Accurate for Models >1um  Recommended PSPICE Level 5 Model (Used for Short Channel Effects Correction) and Accounting for COX  Scaling Factor from Ex 23 was .36 Going from 5V to 1.8V Circuit (Adjusted VTO Accordingly)  Original COX Set to 7E-4 (Default)  COX = EOX/TOX  Results to Analyze:  How COX*2 Changes Effect Circuit Power Usage  How COX*2 Changes Effect Circuit Speed
  • 13. Schematic 13 GND_0 GND_0 GND_0 VDD1 VDD2 1.8Vdc 1.8Vdc 0 PMOS1 PMOS2 Mbreakp1 Mbreakp2 W = 30u W = 30u VGate L = .36u L = .36u GND_0 Vout1 Vout2 1.8Vdc NMOS1 NMOS2 C1 C2 40p 40p Mbreakn1 Mbreakn2 W = 14.4u W = 14.4u L = .36u L = .36u GND_0 GND_0 GND_0 GND_0
  • 14. NMOS1 and PMOS1 Models 14
  • 15. NMOS2 and PMOS2 Models 15
  • 20. Conclusions 20  PSPICE Proved Useful For Analyzing Second Order Oxide Thickness Effects  Lowering the Gate Oxide Thickness Reduced Power Usage (By 1mV During Switching)  Lowering the Gate Oxide Thickness Also Decreased the Max Switching Frequency (6.3MHz to 6MHz)  Scaling Parameters and Model Level Played a Huge Impact for Obtaining Usable PSPICE Results  Gate Oxide Thickness Has a Tremendous Impact On the Power and Frequency of a Circuit
  • 22. References 22  http://etd.library.vanderbilt.edu/available/etd- 12032003-100902/unrestricted/Thesis.pdf  http://www.smdp.iitkgp.ernet.in/PDF/TCAD/AK M.pdf