VICTORY PROCESS Full Physical 3D Semiconductor Simulator VICTORY - - PowerPoint PPT Presentation

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VICTORY PROCESS Full Physical 3D Semiconductor Simulator VICTORY - - PowerPoint PPT Presentation

VICTORY PROCESS Full Physical 3D Semiconductor Simulator VICTORY Process 3D Process Simulator VICTORY Process provides the capability to simulate comprehensive full process flows Etching, Deposition, Lithography Oxidation, Stress


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SLIDE 1

VICTORY PROCESS

Full Physical 3D Semiconductor Simulator

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SLIDE 2

Full Physical 3D Semiconductor Simulator

VICTORY Process – 3D Process Simulator

  • VICTORY Process provides the capability to simulate

comprehensive full process flows

  • Etching, Deposition, Lithography
  • Oxidation, Stress
  • Implantation
  • Diffusion
  • Self explanatory process flow description
  • Based on ATHENA syntax
  • Open interface for modeling
  • Model parameters and functions can be accessed and modified
  • Open C-code is used to implement the model functions
  • Pre-compiled library is provided
  • Makefile to create an extend model library is provided
  • 2 -
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SLIDE 3

Full Physical 3D Semiconductor Simulator

VICTORY Process – Numerics

  • Level set based framework
  • for structure representation and
  • for interface propagation
  • Very stable surface propagation algorithms
  • Important for Etching, Deposition, Oxidation
  • Based on the multi-layer structure concept
  • Automatic void detection
  • Avoids the problem of loop creation and correction
  • 3 -
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SLIDE 4

Full Physical 3D Semiconductor Simulator

VICTORY Process – Meshes

  • VICTORY Process uses two types of meshes
  • Hierarchical Cartesian mesh for implicit geometry representation
  • Irregular Cartesian mesh for volume data representation
  • Doping, Stress, .....
  • Manual and automatic mesh refinement
  • Manual refinement of the geometry mesh
  • Automatic refinement of the geometry mesh
  • Automatic set-up of volume data mesh
  • Manual refinement of the volume data mesh
  • 4 -
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SLIDE 5

Full Physical 3D Semiconductor Simulator

VICTORY Process – Etching/Deposition/Lithography

  • Comprehensive mask support
  • GDSII – format masks
  • lay – format masks (MaskViews)
  • Definition of mask polygons inside the processing deck
  • Mask variations via the deck (shrink and expand)
  • Selection of a simulation window
  • Lithography
  • Calculation of aerial images
  • Pattern transfer of aerial images
  • 5 -
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SLIDE 6

Full Physical 3D Semiconductor Simulator

VICTORY Process – Etching/Deposition/Lithography (con’t)

  • Geometrical Etching
  • Idealized directional mask pattern or image transfer
  • Pattern transfer with tilted sidewalls and rounded corners
  • Idealized isotropic, dry and directional etching
  • Selective and non-selective mode
  • Fast structure prototyping
  • 6 -
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SLIDE 7

Full Physical 3D Semiconductor Simulator

VICTORY Process – Etching/Deposition/Lithography (con’t)

  • Geometrical Deposition
  • Idealized vertical resists or material regions defined by a mask
  • Idealized conformal deposition
  • Deposition of features with tilted sidewalls and rounded corners
  • Planarisation mode to partially fill holes
  • 7 -
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SLIDE 8

Full Physical 3D Semiconductor Simulator

VICTORY Process – Etching/Deposition/Lithography (con’t)

  • Geometrical CMP
  • Idealized planarization
  • Selective and non-selective mode
  • 8 -

Selective Non-Selective

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SLIDE 9

Full Physical 3D Semiconductor Simulator

VICTORY Process – Etching/Deposition/Lithography (con’t)

  • Physical Etching
  • Selective etching of several materials
  • Comprehensive set of default models
  • Selective Etching
  • Isotropic, Anisotropic, Directional
  • Crystal orientation dependent
  • Plasma Etching
  • Ion-Milling
  • Material dependent yield functions
  • Re-deposition (material dependent efficiencies)
  • Rotating beams, static beams, divergent beams
  • Reactive Ion Etching
  • Deep Reactive Ion Etching
  • Ballistic transport of reactants
  • High performance due to multi-threading
  • Near linear speedup on multi-core machines
  • 9 -
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SLIDE 10

Full Physical 3D Semiconductor Simulator

VICTORY Process – Etching/Deposition/Lithography (con’t)

  • 10 -

Ion milling with re-deposition

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SLIDE 11

Full Physical 3D Semiconductor Simulator

VICTORY Process – Etching/Deposition/Lithography (con’t)

  • Physical Deposition
  • Comprehensive set of default models
  • Conformal Deposition
  • Non-conformal Deposition
  • Directional Deposition
  • Selective Deposition
  • Empirical epitaxial growth
  • Ion beam deposition
  • User accessible yield functions
  • Rotating beams, static beams and divergent beams
  • Sputter deposition
  • Ion assisted sputter deposition
  • Ballistic transport of reactants
  • High performance due to multi-threading
  • Near linear speedup on multi-core machines
  • 11 -
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SLIDE 12

Full Physical 3D Semiconductor Simulator

VICTORY Process – Etching/Deposition/Lithography (con’t)

  • 12 -

Ion beam deposition with tilted beam

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SLIDE 13

Full Physical 3D Semiconductor Simulator

VICTORY Process – Etching/Deposition/Lithography (con’t)

  • Physical Etching and Deposition - Open modeling system

 Open C-function model library  User definable transport characteristics ( flux model )

 Define particles involved in the process  Determines how the reactants approach the wafer surface  Determines how the reactants are re-emitted from the surface

 User definable surface reaction ( surface reaction model )

 Determines how the local etch rate is calculated

 User definable etching / deposition models ( topography model )

 Defines the link between particle transport and surface reaction

 C-function models for material characteristics

 Etch rates, conformity, anisotropy, sticking efficiency  Technological models (e.g etch rate versus gas flow)

  • 13 -
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SLIDE 14

Full Physical 3D Semiconductor Simulator

Modes for Flux Calculation

Primary-Ballistic Mode:

  • Only particles approaching the surface

directly from the reactor chamber (primary particles) are taken into account

  • The velocity distribution function of the

primary particles in the vicinity of the wafer is a modeling function definable by the user

  • 14 -
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SLIDE 15

Full Physical 3D Semiconductor Simulator

Modes for Flux Calculation (con’t)

Reflective-Ballistic Mode:

  • Along with primary sources (reactor

chamber) also secondary sources (particles reflected or emitted from surface) are taken into account.

  • The velocity distribution function of the

primary and secondary particles are modeling functions definable by the user

  • 15 -
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SLIDE 16

Full Physical 3D Semiconductor Simulator

Modes for Flux Calculation (con’t)

Rate-Coupled-Reflective-Ballistic Mode:

  • Along with primary sources (reactor

chamber) also secondary sources (particles reflected

  • r

emitted from surface) are taken into account.

  • The velocity distribution function of the

primary and secondary particles are modeling functions definable by the user

  • The amount of secondary particles is a

function of the rate (e.g redeposition)

  • 16 -
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SLIDE 17

Full Physical 3D Semiconductor Simulator

VICTORY Process – Ion Implantation – Analytical

  • Analytical and Monte-Carlo methods for ion implantation
  • Analytical method uses a well established database for a wide

range of implantation conditions

  • Gaussian profiles, Pearson profiles and Dual Pearson profiles
  • User definable profiles
  • By means of moments of the profile
  • By means of data files
  • Range scaling techniques are applied to take into account multi-

material layers

  • High performance due to
  • Very efficient numerical algorithms
  • Efficient multi-threading
  • 17 -
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SLIDE 18

Full Physical 3D Semiconductor Simulator

VICTORY Process – Ion Implantation – Monte-Carlo

  • Monte Carlo method is more appropriate
  • For complex geometries
  • For large tilted implants

because many effects cannot be accounted for by even the most elaborated analytical procedure

  • Monte Carlo method takes into account all important implantation

effects:

  • Ion channelling
  • Ion dose dependency due to damage accumulation
  • Effect of multiple layers of different materials
  • Partial shadowing of ion flux for tilted implants
  • Multiple ion reflections within structures with complex 3D geometry
  • Lateral ion scattering from mask walls or so-called implantation proximity

effect

  • 18 -
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SLIDE 19

Full Physical 3D Semiconductor Simulator

VICTORY Process – Ion Implantation – Monte-Carlo (con‘t)

  • Is completely physically based
  • Uses best available electronic and nuclear stopping models
  • Acceleration techniques
  • Trajectory splitting
  • High performance due to efficient multi-threading
  • 19 -
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SLIDE 20

Full Physical 3D Semiconductor Simulator

VICTORY Process – Ion Implantation – Monte-Carlo (con‘t)

Implant at tilt 50 degrees and twist along structure’s diagonal.

  • 5 million trajectories can be simulated in a few minutes on an 8 core machine
  • 20 -
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SLIDE 21

Full Physical 3D Semiconductor Simulator

Primary, i.e. direct impact implantation Shadowed, i.e. secondary impact implantation

VICTORY Process – Ion Implantation – Monte-Carlo (con‘t)

Implant at tilt 50 degrees and twist along structure’s diagonal.

  • All geometrical effects are taken into account
  • 21 -

Ion distribution in silicon

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SLIDE 22

Full Physical 3D Semiconductor Simulator

VICTORY Process – Annealing/Diffusion

  • Based on an Open Modeling System
  • PDE system is extendable by the user
  • Modelling species can be added
  • Reactions between species can be extended and modified
  • Comprehensive set of default models
  • Direct, Fermi, FullCPL, Single-Pair, Five-stream
  • Dopant activation and solid solubility
  • Impurity segregation at material interfaces
  • Point defect trapping
  • Point defect clustering
  • Concurrent simulation of several impurities
  • 22 -
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SLIDE 23

Full Physical 3D Semiconductor Simulator

VICTORY Process – Annealing/Diffusion (con‘t)

 Finite difference scheme is applied to discretize the PDE‘s  Solved on a Cartesian mesh

 Guarantees high performance and high stability  Irregular Cartesian mesh is used to facilitate local refinement  Interface points are inserted to properly grasp material interfaces  Free line points are inserted to resolve high gradients near interfaces

 Special numerical discretization for

 interface points and  free line points

 Very efficient multi-threading

 High multi-core performance gain

  • 23 -
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SLIDE 24

Full Physical 3D Semiconductor Simulator

VICTORY Process – Annealing/Diffusion (con‘t)

  • 24 -

Mesh for annealing simulation

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SLIDE 25

Full Physical 3D Semiconductor Simulator

VICTORY Process – Annealing/Diffusion (con‘t)

  • Default models :
  • Direct model
  • Fermi model
  • FullCPL model
  • 25 -

( )

D

J t C   ⋅ ∇ − = ∂ ∂ C D J

C D

∇ ⋅ − =         ⋅ ⋅ ⋅ ⋅ − ∇ ⋅ − = T k E q C Z C D J

C F

   ( )

F

J t C   ⋅ ∇ − = ∂ ∂ ( )

CPL

J t C   ⋅ ∇ − = ∂ ∂

=

      ⋅ ⋅ ⋅         ⋅ −         ∇ ⋅ − =

V I X X X A X X A AX X CPL

T k E q C C C Z C C C D f J

, * *

  

slide-26
SLIDE 26

Full Physical 3D Semiconductor Simulator

VICTORY Process – Annealing/Diffusion (con‘t)

  • Default models :
  • Five-Stream model
  • 26 -

( ) ( ) ( )

AV AI A V I I I I AV I A V I I I

C C C C C R J R R R J t C

s

,

, , , + ⋅ ∇ − = + + + ⋅ ∇ − = ∂ ∂

↔ ↔ ↔

    ( ) ( ) ( )

AV AI A V I V V V AI V A V I V V

C C C C C R J R R R J t C

s

,

, , , + ⋅ ∇ − = + + + ⋅ ∇ − = ∂ ∂

↔ ↔ ↔

    ( )

AV AI A V I A I AV V AI AV AI A

C C C C C R R R R R t C

s s s

,

, , , = − − + = ∂ ∂

↔ ↔

( ) ( ) ( )

AV AI A V I AV AV I AV AV AV AV

C C C C C R J R R J t C

s

,

, , , + ⋅ ∇ − = + − ⋅ ∇ − = ∂ ∂

    ( ) ( ) ( )

AV AI A V I AI AI V AI AI AI AI

C C C C C R J R R J t C

s

,

, , , + ⋅ ∇ − = + − ⋅ ∇ − = ∂ ∂

   

All model species are defined in a C-function model file

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SLIDE 27

Full Physical 3D Semiconductor Simulator

VICTORY Process – Annealing/Diffusion (con‘t)

  • Default models :
  • Five-Stream model
  • 27 -

( ) ( ) ( )

AV AI A V I I I I AV I A V I I I

C C C C C R J R R R J t C

s

,

, , , + ⋅ ∇ − = + + + ⋅ ∇ − = ∂ ∂

↔ ↔ ↔

    ( ) ( ) ( )

AV AI A V I V V V AI V A V I V V

C C C C C R J R R R J t C

s

,

, , , + ⋅ ∇ − = + + + ⋅ ∇ − = ∂ ∂

↔ ↔ ↔

    ( )

AV AI A V I A I AV V AI AV AI A

C C C C C R R R R R t C

s s s

,

, , , = − − + = ∂ ∂

↔ ↔

( ) ( ) ( )

AV AI A V I AV AV I AV AV AV AV

C C C C C R J R R J t C

s

,

, , , + ⋅ ∇ − = + − ⋅ ∇ − = ∂ ∂

    ( ) ( ) ( )

AV AI A V I AI AI V AI AI AI AI

C C C C C R J R R J t C

s

,

, , , + ⋅ ∇ − = + − ⋅ ∇ − = ∂ ∂

   

Reactions are defined in a C-function model file

slide-28
SLIDE 28

Full Physical 3D Semiconductor Simulator

VICTORY Process – Annealing/Diffusion (con‘t)

  • Default models :
  • Five-Stream model
  • 28 -

( ) ( ) ( )

AV AI A V I I I I AV I A V I I I

C C C C C R J R R R J t C

s

,

, , , + ⋅ ∇ − = + + + ⋅ ∇ − = ∂ ∂

↔ ↔ ↔

    ( ) ( ) ( )

AV AI A V I V V V AI V A V I V V

C C C C C R J R R R J t C

s

,

, , , + ⋅ ∇ − = + + + ⋅ ∇ − = ∂ ∂

↔ ↔ ↔

    ( )

AV AI A V I A I AV V AI AV AI A

C C C C C R R R R R t C

s s s

,

, , , = − − + = ∂ ∂

↔ ↔

( ) ( ) ( )

AV AI A V I AV AV I AV AV AV AV

C C C C C R J R R J t C

s

,

, , , + ⋅ ∇ − = + − ⋅ ∇ − = ∂ ∂

    ( ) ( ) ( )

AV AI A V I AI AI V AI AI AI AI

C C C C C R J R R J t C

s

,

, , , + ⋅ ∇ − = + − ⋅ ∇ − = ∂ ∂

   

Stream functions are selected in a C-function model file

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SLIDE 29

Full Physical 3D Semiconductor Simulator

  • Default models :
  • Single-Pair model
  • Simplification of the Five-Stream model where one dopant defect-pair is

neglected

  • Special model variant for interstitial supersaturation where only dopant-

interstitial pairs are taken into account

  • Is about 30% faster than the full Five-Stream model

VICTORY Process – Annealing/Diffusion (con‘t)

  • 29 -

( ) ( ) ( )

AV AI A V I V V V AI V A V I V V

C C C C C R J R R R J t C

s

,

, , , + ⋅ ∇ − = + + + ⋅ ∇ − = ∂ ∂

↔ ↔ ↔

    ( ) ( ) ( )

AV AI A V I I I I AV I A V I I I

C C C C C R J R R R J t C

s

,

, , , + ⋅ ∇ − = + + + ⋅ ∇ − = ∂ ∂

↔ ↔ ↔

    ( )

AV AI A V I A I AV V AI AV AI A

C C C C C R R R R R t C

s s s

,

, , , = − − + = ∂ ∂

↔ ↔

( ) ( ) ( )

AV AI A V I I AV I AV V I I AV I AV I AV I AV

C C C C C R J R R J t C

s

, / / / / / / /

, , , + ⋅ ∇ − = + − ⋅ ∇ − = ∂ ∂

   

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SLIDE 30

Full Physical 3D Semiconductor Simulator

Implant/Diffusion – Annealing/Diffusion (con‘t)

  • 30 -

 Simulation time scales with the complexity of the model and with the number of nodes  Diffusion simulation may last only few minutes with simple models (Fermi)

Implant arsenic energy=30.0 dose=3e15 \ tilt = 0 plus.one \ cluster311 clust.fact=0.1 \ min.clust=1e16 max.clust=1e19 Method material=silicon model=fullcpl Diffuse temp = 1000.0 time = 10 sec Implant arsenic energy=30.0 dose=3e15 \ tilt = 0 plus.one \ cluster311 clust.fact=0.1 \ min.clust=1e16 max.clust=1e19 Method material=silicon model=fullcpl Diffuse temp = 1000.0 time = 10 sec

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SLIDE 31

Full Physical 3D Semiconductor Simulator

VICTORY Process – Oxidation/Stress

  • Numerically very demanding process:
  • Involves different processes
  • Oxygen diffusion
  • Chemical reaction: Si + O2 = SiO2
  • Material deformation
  • Processes are interlinked
  • Diffusion and reaction depend on oxide flow (via stresses)
  • Oxide flow depends on diffusion
  • Mechanical properties of oxide change significantly with temperature
  • Complex behavior near corners
  • 31 -
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SLIDE 32

Full Physical 3D Semiconductor Simulator

VICTORY Process – Oxidation/Stress (con‘t)

  • Oxidation step is represented as a succession of 4 sub-steps :
  • 1. sub-step - Diffusion of oxygen through the oxide
  • Solving diffusion equation
  • 2. sub-step - Reaction at SiO2/Si interface
  • Calculating volume expansion velocity
  • Calculating reactive interface velocity
  • 3. sub-step - Deformation velocity field according to the mechanical

behavior of each material

  • Viscous
  • Solving creep flow problem
  • 4. sub-step - Deformation of the entire structure according to the

velocity fields

  • Interface propagation
  • Solving moving boundary problem
  • 32 -
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SLIDE 33

Full Physical 3D Semiconductor Simulator

VICTORY Process – Oxidation/Stress (con‘t)

  • 1. sub-step - Oxygen transport models :
  • Obtains the oxygen concentration in oxide

Volume equation : Boundary conditions (oxygen flux across interfaces) : (supply) (reaction)

  • 33 -

( )

  • xide

ambient

  • xide

ambient

C C h n n n C D J

/ /

− ⋅ ⋅ = ⋅ ∂ ∂ − =   

  • xide

silicon

  • xide

silicon

C k n n n C D J

/ /

⋅ ⋅ = ⋅ ∂ ∂ ⋅ − =   

= ⋅ ∇

Volume

J 

C D Jvolume ∇ ⋅ − =  

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SLIDE 34

Full Physical 3D Semiconductor Simulator

VICTORY Process – Oxidation/Stress (con‘t)

  • 1- sub-step - Oxygen transport models :
  • Linear transport model :
  • 34 -

dependent rature

  • nly tempe

are .... , , h k D         ⋅ − ⋅ = T k E D T D

B D

exp ) (         ⋅ − ⋅ = T k E k T k

B k

exp ) (         ⋅ − ⋅ = T k E h T h

B h

exp ) (

.... Oxygen diffusivity .... Reaction coefficient .... Transport coefficient

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SLIDE 35

Full Physical 3D Semiconductor Simulator

VICTORY Process – Oxidation/Stress (con‘t)

  • 1. sub-step - Oxygen transport models :
  • Stress-dependent transport model :
  • 35 -

ture

  • n tempera

and pressure c hydrostati local

  • n the

depends .... D         ⋅ − ⋅ = T k E D T D

B D

exp ) (      ≤ >         ⋅ ⋅ − ⋅ = ) ( .... ) ( ) ( .... ) ( exp ) ( ) , ( x p T D x p T k V x P T D T x D

B d

  

slide-36
SLIDE 36

Full Physical 3D Semiconductor Simulator

VICTORY Process – Oxidation/Stress (con‘t)

  • 1- sub-step - Oxygen transport models :
  • Stress-dependent reaction model :
  • 36 -

ture

  • n tempera

and stress interface

  • n the

depends .... k         ⋅ − ⋅ = T k E k T k

B k

exp ) (      ≤ >         ⋅ ⋅ − ⋅ = ) ( .... ) ( ) ( .... ) ( exp ) ( ) , ( x T k x T k V x T k T x k

n n B k n

σ σ σ   

j ij i n

n n ⋅ ⋅ = σ σ

.... Force in the direction of the normal

slide-37
SLIDE 37

Full Physical 3D Semiconductor Simulator

VICTORY Process – Oxidation/Stress (con‘t)

  • 3. sub-step - Deformation models :
  • Obtains the deformation velocity of all materials above the reactive

surface

  • Solution variables :
  • 37 -

equation ive Constituit .....         ∂ ∂ + ∂ ∂ ⋅ = ∂ ∂ +

i j j i ij ij

x V x V t G µ σ µ σ tensor Stress .....

ij

σ field n velocity Deformatio .....

i

V equation flow Creap .....

j ij i

x x P ∂ ∂ = ∂ ∂ σ pressure c Hydrostati ..... P

slide-38
SLIDE 38

Full Physical 3D Semiconductor Simulator

VICTORY Process – Oxidation/Stress (con‘t)

  • 3.sub-step - Deformation models :
  • Linear incompressible viscous flow model :
  • Viscoelastic term is neglected (assumes infinite shear modulus G)
  • 38 -

        ∂ ∂ + ∂ ∂ ⋅ = ∂ ∂ +

i j j i ij ij

x V x V t G µ σ µ σ condition ibiliy incompress ..... = ⋅ ∇ V   dependent rature

  • nly tempe

is ..... µ Viscosity ..... exp ) (         ⋅ − ⋅ = T k E T

B µ

µ µ

slide-39
SLIDE 39

Full Physical 3D Semiconductor Simulator

VICTORY Process – Oxidation/Stress (con‘t)

  • Oxygen transport, material flow and moving boundary problem are

solved on the same Cartesian mesh

  • High stability
  • Special boundary nodes are added to implement proper boundary

conditions (special method developed in-house)

  • 39 -

Formulate standard equations for regular nodes Introduce cross-points with the interface Formulate standard equations for irregular nodes (considering cross-points) Formulate cross-point equation (tangential equation)

n u t t t t u t t u        ∂ ∂ × × = ⋅ ∂ ∂ − ⋅ ∂ ∂ ) (

β α α β β α

slide-40
SLIDE 40

Full Physical 3D Semiconductor Simulator

VICTORY Process – Oxidation/Stress (con‘t)

 Multiple operational modes  Analytical mode

 Grows a layer of oxide of the requested thickness

 Empirical mode

 Calculates the oxide thickness on the basis of the Massoud model  Can be applied to oxide layers thinner than the mesh size

 Full physical mode

 Full solution of the transport and the flow equations in oxide  Requires appropriate high mesh resolution in oxide

 Hybrid mode

 Low mesh resolution can be applied in planar regions

 Empirical solution is calculated in these planar regions

 Coupled with full physical solution in curved regions  Significantly reduces the number of required mesh nodes  Automatic switching between modes

  • 40 -
slide-41
SLIDE 41

Full Physical 3D Semiconductor Simulator

VICTORY Process – Oxidation/Stress (con‘t)

  • 41 -

LOCOS: Long simulations are stable without meshing issues

slide-42
SLIDE 42

Full Physical 3D Semiconductor Simulator

VICTORY Process – Oxidation/Stress (con‘t)

  • 42 -

Simulation is stable for complex structures (multi-layer concept) STI liner oxidation Buffered field oxidation

slide-43
SLIDE 43

Full Physical 3D Semiconductor Simulator

VICTORY Process – Oxidation/Stress (con‘t)

  • 43 -

Stress-dependent oxygen transport is taken into account

stress independent stress dependent

slide-44
SLIDE 44

Full Physical 3D Semiconductor Simulator

VICTORY Process – Interface to VICTORY Device

  • A special device meshing engine is

used to export structures to VICTORY Device

  • Supports different base meshes

 Process - geometry mesh  Process - volume data mesh

  • Provides comprehensive automatic and

manual mesh adaptation features

 Refinement boxes  Refinement lines  Refinement near interfaces  Refinement according to doping

  • 44 -
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SLIDE 45

Full Physical 3D Semiconductor Simulator

VICTORY Process – Interface to VICTORY Device (con't)

  • A special device meshing engine is

used to export structures to VICTORY Device

  • Supports different base meshes

 Process - geometry mesh  Process - volume data mesh

  • Provides comprehensive automatic and

manual mesh adaptation features

 Refinement boxes  Refinement lines  Refinement near interfaces  Refinement according to doping

  • 45 -
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SLIDE 46

Full Physical 3D Semiconductor Simulator

VICTORY Process – Interface to VICTORY Device (con't)

  • A special device meshing engine is

used to export structures to VICTORY Device

  • Supports different base meshes

 Process - geometry mesh  Process - volume data mesh

  • Provides comprehensive automatic and

manual mesh adaptation features

 Refinement boxes  Refinement lines  Refinement near interfaces  Refinement according to doping

  • 46 -
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SLIDE 47

Full Physical 3D Semiconductor Simulator

VICTORY Process – Interface to VICTORY Device (con't)

  • Structure mirroring capability
  • Process simulation can make use of any geometrical symmetry
  • Allows for faster process simulation of symmetrical devices
  • 47 -
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SLIDE 48

Full Physical 3D Semiconductor Simulator

Applications: Re-Oxidation - STRESS

  • 48 -
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SLIDE 49

Full Physical 3D Semiconductor Simulator

Applications: Re-oxidation – Regions

  • 49 -
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SLIDE 50

Full Physical 3D Semiconductor Simulator

Applications: Re-oxidation – Stresses in Oxide

  • 50 -
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SLIDE 51

Full Physical 3D Semiconductor Simulator

Applications: Planar MOS Technology

  • 51 -

Boron profile Phosphorus profile Arsenic profile

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SLIDE 52

Full Physical 3D Semiconductor Simulator

Applications: FinFET

  • 52 -
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SLIDE 53

Full Physical 3D Semiconductor Simulator

Applications: Tri-gate FET with Contact Area

  • 53 -

Donor profile Acceptor profile

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SLIDE 54

Full Physical 3D Semiconductor Simulator

Applications: MEMS Cantilever Structure

  • 54 -
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SLIDE 55

Full Physical 3D Semiconductor Simulator

Current Development

  • Stress-dependent viscous oxidation
  • Performance improvement of the oxidation module
  • Extended default set of diffusion models
  • Extended default set of etching and deposition models
  • Improvement of the device meshing export
  • 55 -
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SLIDE 56

Full Physical 3D Semiconductor Simulator

Conclusion

  • VICTORY Process is the next generation tool for the investigation
  • f 3D process and device effects
  • Suitable for many semiconductor technologies such as
  • Planar MOS, FinFET, Power devices
  • Sensor and LED’s,
  • MEMS and
  • Complex quantum structures
  • Also suitable for non-semiconductor applications such as
  • Hard coating and
  • Mass storage applications
  • Very high stability due to
  • Multi-layer concept and
  • Robust and accurate methods for moving interfaces
  • Flexible due to open interface for modeling
  • 56 -