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Ballistic Transport in Schottky-Barrier and
       MOSFET-like Carbon Nanotube Field Effect
       Transistors: Modeling, Simulation and Analysis


                       Presented by:
                       Protik Das
                       Exam Roll: 2240



Department of Applied Physics, Electronics & Communication Engineering, University of Dhaka   1
Outline

   Carbon Nanotube Field Effect Transistor
    (CNTFET)
   NEGF Formalism
   Results
        Quantum Effects
        I-V Characteristics
        Scaling Effects




Department of Applied Physics, Electronics & Communication Engg., University of Dhaka   2
Objective

   Analysis of ballistic transport in CNTFETs.
   Comparison of performance between
    Schottky-Barrier & MOSFET-like
    CNTFETs.




Department of Applied Physics, Electronics & Communication Engg., University of Dhaka   3
Carbon Nanotube (CNT)

   Rolled up Graphene sheet




                                                                                        A spinning Carbon
                                                                                             Nanotube


Department of Applied Physics, Electronics & Communication Engg., University of Dhaka                       4
CNT Types



(a) zigzag type
(b) armchair type




Department of Applied Physics, Electronics & Communication Engg., University of Dhaka   5
Field Effect Transistor (FET)

   The Field-Effect Transistor (FET) is a transistor that
    uses an electric field to control the conductivity of a
    channel in a semiconductor material.




A generic FET structure
Showed in figure.




Department of Applied Physics, Electronics & Communication Engg., University of Dhaka   6
Keyword: Ballistic Transport

   Ballistic Transport is the transport of electrons in a medium
    with negligible electrical resistivity due to scattering. Without
    scattering, electrons simply obey Newton's second law of
    motion at non-relativistic speeds.
   Simply, Ballistic Transport is the transport of electrons in a
    channel considering no impurity or scatterer in the region.
   Ballistic Transport can be considered when mean free path of
    an electron is greater than channel length. i. e.,
                                 λ >> L




Department of Applied Physics, Electronics & Communication Engg., University of Dhaka   7
Carbon Nanotube FET (CNTFET)

   A Carbon Nanotube Field Effect Transistor (CNTFET)
    refers to a field effect transistor that utilizes a single
    carbon nanotube or an array of carbon nanotubes as the
    channel material.




Department of Applied Physics, Electronics & Communication Engg., University of Dhaka   8
Why Carbon Nanotube?

   Near ballistic transport
   Symmetric conduction/valence bands
   Direct bandgap
   Small size
   Confinement of charge inside the nanotube allows ideal
    control of the electrostatics




Department of Applied Physics, Electronics & Communication Engg., University of Dhaka   9
CNTFET Structures

   Back Gated CNTFETs
   Top Gated CNTFETs
   Vertical CNTFETs
                                                                               Back Gated CNTFET




               Top Gated CNTFET                                                    Vertical CNTFET

Department of Applied Physics, Electronics & Communication Engg., University of Dhaka                10
CNTFET Operation

   Schottky-Barrier CNTFET
        Schottky-Barrier is formed between Source/Drain and channel
        Direct tunneling through the Schottky barrier at the source-
         channel junction
        Barrier width is controlled by Gate voltage

   MOSFET-like/Doped Contact CNTFET
        Heavily doped Source and Drain instead of metal
        Barrier height is controlled by gate voltage




Department of Applied Physics, Electronics & Communication Engg., University of Dhaka   11
Schottky-Barrier CNTFET




Department of Applied Physics, Electronics & Communication Engg., University of Dhaka   12
Doped Contact CNTFET




Department of Applied Physics, Electronics & Communication Engg., University of Dhaka   13
NEGF Formalism Review




 Retarded Green’s
function in matrix form,

 Hamiltonian matrix
for the subbands,
Department of Applied Physics, Electronics & Communication Engg., University of Dhaka   14
NEGF Formalism Review (contd.)

   Current,



 Where T(E) is
the transmision
coefficient,



Department of Applied Physics, Electronics & Communication Engg., University of Dhaka   15
NEGF Formalism Review (contd.)




                    Self-consistantly solving NEGF & Poisson’s Equation


Department of Applied Physics, Electronics & Communication Engg., University of Dhaka   16
Device Structure & Parameters

   Channel length, Lch = 20nm
   Source/Drain length, LSD = 30nm
   Oxide Thickness, tOX = 2nm
   Dielectric Constant, k = 16
   Source/Drain Doping, NSD = 1.5/nm
   CNT (13, 0) diameter, 1.01nm
   Bandgap 0.68eV




Department of Applied Physics, Electronics & Communication Engg., University of Dhaka   17
Results

   Quantum Effects
        Quantum-Mechanical Interference
        Quantum Confinement
        Tunneling
   I-V characteristics
   Effect of Gate Dielectric Constant
   Scaling Effects
        Diameter
        Length
        Oxide Thickness



Department of Applied Physics, Electronics & Communication Engg., University of Dhaka   18
Quantum Effects




Quantum-Mechanical Interference                                              Quantum Confinement
                    At VGS = 0.5V and VD=0.5V for doped contact CNTFET

Department of Applied Physics, Electronics & Communication Engg., University of Dhaka              19
Quantum Effects (contd.)
Tunneling in Channel Region of                                  Current in Channel Region of
Schottky-Barrier CNTFET [1]                                     Doped Contact CNTFET




[1] J. Guo, “Carbon Nanotube Electronics: Modeling, Physics and Applications”


Department of Applied Physics, Electronics & Communication Engg., University of Dhaka          20
I-V Characteristics
   ID-VD Comparison
    Doped Contact CNTFET provides more current for same VGS.

                                                                         15 uA
      5 uA




     Schottky-Barrier CNTFET                                               Doped Contact CNTFET

Department of Applied Physics, Electronics & Communication Engg., University of Dhaka             21
I-V Characteristics (contd.)

   ID-VGS Comparison




     Schottky-Barrier CNTFET                                               Doped Contact CNTFET

Department of Applied Physics, Electronics & Communication Engg., University of Dhaka             22
Effect of Gate Dielectric Constant
  Higher Dielectric Constant provides more Drain Current

                                                                                    7.5 uA
     2.5 uA




      Schottky-Barrier CNTFET                                               Doped Contact CNTFET    [Table]

Constant table
 Department of Applied Physics, Electronics & Communication Engg., University of Dhaka             23
Effect of Gate Dielectric Constant
 (contd.)                                                                                K = 3.9




                                                                                         K = 14



The conduction band profile of SB CNTFET
at VG= 0.5V . The solid line is for k = 25 the
dashed line for k = 8 and the dash-dot line for k
= 1 [2]
 [2] J. Guo, “Carbon Nanotube Electronics: Modeling, Physics and Applications”

Constant table
 Department of Applied Physics, Electronics & Communication Engg., University of Dhaka             24
Scaling Effects: Diameter
  Lower diameter provides better ON/OFF ratio.




ID− VGS characteristics at VD= 0.5V for SB                             ID− VGS characteristics at VD= 0.5V
CNTFET. The solid line with circles is for                             for doped contact CNTFET.
d ∼1nm, the sold line is for d ∼1.3nm,
and the dashed line is for d ∼2nm [3]
  [3] J. Guo, “Carbon Nanotube Electronics: Modeling, Physics and Applications”                          [Table]

   [Cause]
  Department of Applied Physics, Electronics & Communication Engg., University of Dhaka                 25
Scaling Effect: Channel Length
Channel Length have very negligible effect on Drain Current.




     Schottky-Barrier CNTFET                                               Doped Contact CNTFET

                                                                                                   [Table]


Department of Applied Physics, Electronics & Communication Engg., University of Dhaka             26
Scaling Effect: Length (contd.)




     Lch = 30nm                                   Lch = 15nm                            Lch = 5nm




        Conduction band profile for doped contact CNTFET at (a) Lch= 30mn,
       (b) Lch = 15nm & (c) Lch = 5nm for VGS= 0.5V and VDS= 0.3V




Department of Applied Physics, Electronics & Communication Engg., University of Dhaka               27
Scaling Effect: Oxide Thickness

Thinner oxide provides much more ON/OFF ratio for both types of CNTFETs.




       Schottky-Barrier CNTFET                                               Doped Contact CNTFET    [Table]


  Department of Applied Physics, Electronics & Communication Engg., University of Dhaka             28
Overview of Our Findings
          Parameter                                     Effect                                Comment

  Dielectric Constant, k                  Higher k provides better                    Doped Contact CNTFET
                                            electrostatic control                     gives better performance
    Channel Diameter                     Lower diameter provides                          Doped Contact have
                                             higher current                               higher ON/OFF ratio
      Channel Length                        Channel length have                             No mentionable
                                           negligible effect on I-V                       advantage for length
     Oxide Thickness                     Thinner oxide provides                       Doped Contact CNTFET
                                        much higher ON/OFF ratio                      have higher ratio than SB


One of our key findings: Thinner oxide provides much higher ON/OFF ratio but
it also increases leakage current. So using thinner oxide of higher k ensures less
leakage current & gives more electrostatic control over channel.

  Department of Applied Physics, Electronics & Communication Engg., University of Dhaka                          29
Conclusions

   The ON/OFF current ratio improves with high-κ gate
    dielectric.
   This improvement is relatively higher in doped contact
    devices.
   Thinner oxide provides better electrostatic control and
    improves device performance for both type of contacts.




Department of Applied Physics, Electronics & Communication Engg., University of Dhaka   30
Future Perspectives

   Completion of the partial code we have
    developed.
   Convert the devices characteristic into SPICE
    model for circuit design.
   Including the effect of phonon scattering.




Department of Applied Physics, Electronics & Communication Engg., University of Dhaka   31
Questions




Department of Applied Physics, Electronics & Communication Engg., University of Dhaka   32
Thank You

Department of Applied Physics, Electronics & Communication Engg., University of Dhaka   33
Dielectric Constant Table [3]
                 Oxide Material                                             Dielectric Constant, k
                          SiO2                                                          3.9
                         Si3N4                                                          8
                          HfO2                                                          14
                          ZrO2                                                          25




[3] Robertson, J. "High dielectric constant oxides." The European Physical Journal Applied Physics 28.03 (2004): 265-291.

                                                                                                             return


Department of Applied Physics, Electronics & Communication Engg., University of Dhaka                                 34
Simulator Software Screenshot




              CNTFET Lab                                       Cylindrical CNT MOSFET Simulator

Department of Applied Physics, Electronics & Communication Engg., University of Dhaka        35
Effect of Diameter

   Bandgap,




                                                                                        return

Department of Applied Physics, Electronics & Communication Engg., University of Dhaka        36

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Project presentation

  • 1. Ballistic Transport in Schottky-Barrier and MOSFET-like Carbon Nanotube Field Effect Transistors: Modeling, Simulation and Analysis Presented by: Protik Das Exam Roll: 2240 Department of Applied Physics, Electronics & Communication Engineering, University of Dhaka 1
  • 2. Outline  Carbon Nanotube Field Effect Transistor (CNTFET)  NEGF Formalism  Results  Quantum Effects  I-V Characteristics  Scaling Effects Department of Applied Physics, Electronics & Communication Engg., University of Dhaka 2
  • 3. Objective  Analysis of ballistic transport in CNTFETs.  Comparison of performance between Schottky-Barrier & MOSFET-like CNTFETs. Department of Applied Physics, Electronics & Communication Engg., University of Dhaka 3
  • 4. Carbon Nanotube (CNT)  Rolled up Graphene sheet A spinning Carbon Nanotube Department of Applied Physics, Electronics & Communication Engg., University of Dhaka 4
  • 5. CNT Types (a) zigzag type (b) armchair type Department of Applied Physics, Electronics & Communication Engg., University of Dhaka 5
  • 6. Field Effect Transistor (FET)  The Field-Effect Transistor (FET) is a transistor that uses an electric field to control the conductivity of a channel in a semiconductor material. A generic FET structure Showed in figure. Department of Applied Physics, Electronics & Communication Engg., University of Dhaka 6
  • 7. Keyword: Ballistic Transport  Ballistic Transport is the transport of electrons in a medium with negligible electrical resistivity due to scattering. Without scattering, electrons simply obey Newton's second law of motion at non-relativistic speeds.  Simply, Ballistic Transport is the transport of electrons in a channel considering no impurity or scatterer in the region.  Ballistic Transport can be considered when mean free path of an electron is greater than channel length. i. e., λ >> L Department of Applied Physics, Electronics & Communication Engg., University of Dhaka 7
  • 8. Carbon Nanotube FET (CNTFET)  A Carbon Nanotube Field Effect Transistor (CNTFET) refers to a field effect transistor that utilizes a single carbon nanotube or an array of carbon nanotubes as the channel material. Department of Applied Physics, Electronics & Communication Engg., University of Dhaka 8
  • 9. Why Carbon Nanotube?  Near ballistic transport  Symmetric conduction/valence bands  Direct bandgap  Small size  Confinement of charge inside the nanotube allows ideal control of the electrostatics Department of Applied Physics, Electronics & Communication Engg., University of Dhaka 9
  • 10. CNTFET Structures  Back Gated CNTFETs  Top Gated CNTFETs  Vertical CNTFETs Back Gated CNTFET Top Gated CNTFET Vertical CNTFET Department of Applied Physics, Electronics & Communication Engg., University of Dhaka 10
  • 11. CNTFET Operation  Schottky-Barrier CNTFET  Schottky-Barrier is formed between Source/Drain and channel  Direct tunneling through the Schottky barrier at the source- channel junction  Barrier width is controlled by Gate voltage  MOSFET-like/Doped Contact CNTFET  Heavily doped Source and Drain instead of metal  Barrier height is controlled by gate voltage Department of Applied Physics, Electronics & Communication Engg., University of Dhaka 11
  • 12. Schottky-Barrier CNTFET Department of Applied Physics, Electronics & Communication Engg., University of Dhaka 12
  • 13. Doped Contact CNTFET Department of Applied Physics, Electronics & Communication Engg., University of Dhaka 13
  • 14. NEGF Formalism Review  Retarded Green’s function in matrix form,  Hamiltonian matrix for the subbands, Department of Applied Physics, Electronics & Communication Engg., University of Dhaka 14
  • 15. NEGF Formalism Review (contd.)  Current,  Where T(E) is the transmision coefficient, Department of Applied Physics, Electronics & Communication Engg., University of Dhaka 15
  • 16. NEGF Formalism Review (contd.) Self-consistantly solving NEGF & Poisson’s Equation Department of Applied Physics, Electronics & Communication Engg., University of Dhaka 16
  • 17. Device Structure & Parameters  Channel length, Lch = 20nm  Source/Drain length, LSD = 30nm  Oxide Thickness, tOX = 2nm  Dielectric Constant, k = 16  Source/Drain Doping, NSD = 1.5/nm  CNT (13, 0) diameter, 1.01nm  Bandgap 0.68eV Department of Applied Physics, Electronics & Communication Engg., University of Dhaka 17
  • 18. Results  Quantum Effects  Quantum-Mechanical Interference  Quantum Confinement  Tunneling  I-V characteristics  Effect of Gate Dielectric Constant  Scaling Effects  Diameter  Length  Oxide Thickness Department of Applied Physics, Electronics & Communication Engg., University of Dhaka 18
  • 19. Quantum Effects Quantum-Mechanical Interference Quantum Confinement At VGS = 0.5V and VD=0.5V for doped contact CNTFET Department of Applied Physics, Electronics & Communication Engg., University of Dhaka 19
  • 20. Quantum Effects (contd.) Tunneling in Channel Region of Current in Channel Region of Schottky-Barrier CNTFET [1] Doped Contact CNTFET [1] J. Guo, “Carbon Nanotube Electronics: Modeling, Physics and Applications” Department of Applied Physics, Electronics & Communication Engg., University of Dhaka 20
  • 21. I-V Characteristics  ID-VD Comparison Doped Contact CNTFET provides more current for same VGS. 15 uA 5 uA Schottky-Barrier CNTFET Doped Contact CNTFET Department of Applied Physics, Electronics & Communication Engg., University of Dhaka 21
  • 22. I-V Characteristics (contd.)  ID-VGS Comparison Schottky-Barrier CNTFET Doped Contact CNTFET Department of Applied Physics, Electronics & Communication Engg., University of Dhaka 22
  • 23. Effect of Gate Dielectric Constant Higher Dielectric Constant provides more Drain Current 7.5 uA 2.5 uA Schottky-Barrier CNTFET Doped Contact CNTFET [Table] Constant table Department of Applied Physics, Electronics & Communication Engg., University of Dhaka 23
  • 24. Effect of Gate Dielectric Constant (contd.) K = 3.9 K = 14 The conduction band profile of SB CNTFET at VG= 0.5V . The solid line is for k = 25 the dashed line for k = 8 and the dash-dot line for k = 1 [2] [2] J. Guo, “Carbon Nanotube Electronics: Modeling, Physics and Applications” Constant table Department of Applied Physics, Electronics & Communication Engg., University of Dhaka 24
  • 25. Scaling Effects: Diameter Lower diameter provides better ON/OFF ratio. ID− VGS characteristics at VD= 0.5V for SB ID− VGS characteristics at VD= 0.5V CNTFET. The solid line with circles is for for doped contact CNTFET. d ∼1nm, the sold line is for d ∼1.3nm, and the dashed line is for d ∼2nm [3] [3] J. Guo, “Carbon Nanotube Electronics: Modeling, Physics and Applications” [Table] [Cause] Department of Applied Physics, Electronics & Communication Engg., University of Dhaka 25
  • 26. Scaling Effect: Channel Length Channel Length have very negligible effect on Drain Current. Schottky-Barrier CNTFET Doped Contact CNTFET [Table] Department of Applied Physics, Electronics & Communication Engg., University of Dhaka 26
  • 27. Scaling Effect: Length (contd.) Lch = 30nm Lch = 15nm Lch = 5nm Conduction band profile for doped contact CNTFET at (a) Lch= 30mn, (b) Lch = 15nm & (c) Lch = 5nm for VGS= 0.5V and VDS= 0.3V Department of Applied Physics, Electronics & Communication Engg., University of Dhaka 27
  • 28. Scaling Effect: Oxide Thickness Thinner oxide provides much more ON/OFF ratio for both types of CNTFETs. Schottky-Barrier CNTFET Doped Contact CNTFET [Table] Department of Applied Physics, Electronics & Communication Engg., University of Dhaka 28
  • 29. Overview of Our Findings Parameter Effect Comment Dielectric Constant, k Higher k provides better Doped Contact CNTFET electrostatic control gives better performance Channel Diameter Lower diameter provides Doped Contact have higher current higher ON/OFF ratio Channel Length Channel length have No mentionable negligible effect on I-V advantage for length Oxide Thickness Thinner oxide provides Doped Contact CNTFET much higher ON/OFF ratio have higher ratio than SB One of our key findings: Thinner oxide provides much higher ON/OFF ratio but it also increases leakage current. So using thinner oxide of higher k ensures less leakage current & gives more electrostatic control over channel. Department of Applied Physics, Electronics & Communication Engg., University of Dhaka 29
  • 30. Conclusions  The ON/OFF current ratio improves with high-κ gate dielectric.  This improvement is relatively higher in doped contact devices.  Thinner oxide provides better electrostatic control and improves device performance for both type of contacts. Department of Applied Physics, Electronics & Communication Engg., University of Dhaka 30
  • 31. Future Perspectives  Completion of the partial code we have developed.  Convert the devices characteristic into SPICE model for circuit design.  Including the effect of phonon scattering. Department of Applied Physics, Electronics & Communication Engg., University of Dhaka 31
  • 32. Questions Department of Applied Physics, Electronics & Communication Engg., University of Dhaka 32
  • 33. Thank You Department of Applied Physics, Electronics & Communication Engg., University of Dhaka 33
  • 34. Dielectric Constant Table [3] Oxide Material Dielectric Constant, k SiO2 3.9 Si3N4 8 HfO2 14 ZrO2 25 [3] Robertson, J. "High dielectric constant oxides." The European Physical Journal Applied Physics 28.03 (2004): 265-291. return Department of Applied Physics, Electronics & Communication Engg., University of Dhaka 34
  • 35. Simulator Software Screenshot CNTFET Lab Cylindrical CNT MOSFET Simulator Department of Applied Physics, Electronics & Communication Engg., University of Dhaka 35
  • 36. Effect of Diameter  Bandgap, return Department of Applied Physics, Electronics & Communication Engg., University of Dhaka 36