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RELEVANCE OF DEVICE MODELING AND NUMERICAL SIMULATION FOR :

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ELECTROMAGNETIC WAVE EFFECTS ON MICROWAVE TRANSISTORS. FROM THE ANALYSIS OF ... ADVANCED DEVICE MODELING (HIGHER ORDER MOMENT EQUATIONS) AND NUMERICAL METHODS ... – PowerPoint PPT presentation

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Title: RELEVANCE OF DEVICE MODELING AND NUMERICAL SIMULATION FOR :


1
RELEVANCE OF DEVICE MODELING AND NUMERICAL
SIMULATION FOR
  • INTERCONNECT SIMULATION
  • ELECTROMAGNETIC WAVE EFFECTS ON MICROWAVE
    TRANSISTORS
  • FROM THE ANALYSIS OF SOME RELEVANT LITERATURE
  • ADVANCED DEVICE MODELING (HIGHER ORDER MOMENT
    EQUATIONS) AND NUMERICAL METHODS (HIGH
    RESOLUTION CONSERVATIVE SCHEMES) REQUIRED !

2
MODELS INCORPORTATED IN COMMERCIAL SIMULATORS
  • ISE
  • DRIFT-DIFFUSION
  • ENERGY TRANSPORT
  • SIMPLIFIED HYDRODYNAMICAL
  • THERMAL
  • PARAMETERS PHENOMENOLOGICALLY ADJUSTED
  • LACKING
  • PHYSICS BASED MODELS
  • ELECTROMAGNETIC INTERACTIONS
  • INTERCONNECTS

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MODELLING AND SIMULATING INTERCONNECTS
  • ON CHIP INTERCONNECTS ARE A LIMITING FACTOR TO
    THE OVERALL PERFORMANCE OF CIRCUITS. ON CHIP
    WIRING DELAYS ARE A SIGNIFICANT PORTION OF THE
    TOTAL CHIP DELAY TIME.
  • METAL-INSULATOR-SEMICONDUCTOR INTERCONNECTS ARE
    OF PARAMOUNT INTEREST
  • ELECTROMAGNETIC FIELD COUPLING WITH DEVICE CHARGE
    CARRIERES TRANSPORT IS REQUIRED FOR ACCURATE
    DESCRIPTION
  • G.WANG, R.W.DUTTON, C.S..RAFFERTY, DEVICE LEVEL
    SIMULATION OF WAVE PROPAGATION ALONG
    METAL-INSULATOR SEMICONDUCTOR INTERCONNECTS, IEEE
    TRANS ON MICROWAVE THEORY AND TECHNIQUES, VOL.50,
    (2002), pp.1127-1137.

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MAIN RESULTS
  • DETERMINATION OF THE SLOW SPEED FOR THE
    FUNDAMENTAL TM MODE
  • AT VARIANCE WITH THE USUAL TREATMENT WHERE THE
    SEMICONDUCTOR IS TREATED AS A MEDIUM WITH UNIFORM
    CONDUCTIVITY, THE DEVICE DESCRIPTION ENABLES TO
    I
  • ANALYZE THE HIGHER MODES GENERATION THROUGH THE
    NON LINEAR BEHAVIOUR OF THE SEMICONDUCTOR
  • TREAT BOTH SMALL SIGNAL AND LARGE SIGNAL CASES

9
FUNDAMENTAL MODE PROPAGATION Ex AND Ez
10
FUNDAMENTAL MODE PROPAGATION ELECTRON AND HOLE
CONCENTRATIONS
11
SECOND HARMONIC Ex AND n
12
HIERARCHY OF MOMENT EQUATIONS
  • THE NON STATIONARY DRIFT DIFFUSION EQUATIONS ARE
    THE FIRST TERM IN THE HIERARCHY OF MOMENT
    EQUATIONS (1) AND (3)

13
RELATIVE MAGNITUDES OF THE RELAXATION TIMES
  • IN THE HIERARCHY OF THE MOMENT EQUATIONS THE
    RELAXATION TIMES FOR MOMENTUM, ENERGY, ENERGY
    FLUX, FLUX OF ENERGY FLUX, ETC. APPEAR
  • IT IS POSSIBLE TO LIMIT TO THE DRIFT-DIFFUSION
    EQUATIONS ONLY IF THE OTHER RELAXATION TIMES
    COULD BE CONSIDERED NEGLIGIBLE
  • HOWEVER
  • MONTE CARLO SIMULATIONS (MUSCATO) SHOW THAT THE
    RELAXATION TIME FOR ENERGY IS LARGER THAN THE
    OTHERS AND THE MOMENTUM AND ENERGY FLUX
    RELAXATION TIMES ARE COMPARABLE !

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EXTENDED MODELS
  • INCORPORATE BALANCE EQUATIONS FOR MOMENTUM,
    ENERGY AND ENERGY FLUX
  • THE RELAXATION TIMES FOR MOMENTUM AND ENERGY FLUX
    ARE OF THE SAME ORDER OF MAGNITUDE
  • THE ONSAGER RECIPROCITY THEOREM OF IRREVERSIBLE
    STATISTICAL PHYSICS MANDATES THAT AT LEAST THE
    ENERGY FLUX BALANCE EQUATIONS MUST BE INCLUDED
    (MUSCATO, 1998)
  • THE PARAMETERS APPEARING IN THE PDE MUST BE
    OBTAINED FROM THE PHYSICAL MODEL, EITHER THROUGH
    MONTE CARLO DATA FITTING OR BY ASYMPTOTIC
    SOLUTIONS OF THE BOLTZMANN EQUATION.

17
ELECTROMAGNETIC WAVE EFFETCS ON MICROWAVE
TRANSISTORS
  • WHEN SEMICONDUCTOR DEVICES ARE OPERATED AT
    SUFFICIENTLY HIGH FREQUENCY THE QUASI STATIC
    (POISSON BASED) SEMICONDUCTOR DEVICE MODELS FAIL
    TO REPRESENT ACCURATELY THE COUPLING OF THE
    ELECTROMAGNETIC WAVE PROPAGATING IN THE DEVICE
    WITH THE CARRIERS.
  • THE FULL MAXWELL EQUATIONS MUST BE COUPLED TO THE
    DEVICE EQUATIONS (MOMENTS EQUATIONS)
  • ALSUNAIDI, IMTIAZ, EL-GHALAZY, ELECTROMAGNETIC
    WAVE EFFECTS ON MICROWAVE TRANSISTORS USING A
    FULL WAVE TIME DOMAIN MODEL, IEEE TRANS ON
    MICROWAVE THEORY AND TECHNIQUES, 44, (1996),
    799-899

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DEVICE MODEL USED BY ALSUNAIDI ET AL.
20
SOME RESULTS
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LIMITATIONS
  • ELECTROMAGNETIC PROPAGATION THROUGH THE DEVICE
  • THE RELAXATION TIMES OF THE ENERGY FLUX ARE OF
    THE SAME ORDER AS THOSE FOR MOMENTUM.
  • THEREFORE THE ENERGY FLUX MOMENT EQUATION SHOULD
    BE CONSIDERED
  • THE DEVICE MODEL, AS IN THE PREVIOUS CASE, DOES
    NOT OBEY THE ONSAGER RECIPROCITY THEOREM.TO
    RESTORE THE ONSAGER RECIPROCITY THEOREM AT LEAST
    THE ENERGY FLUX BALANCE EQUATION MUST BE INCLUDED
  • NECESSITY OF EXTENDED MODELS (HIGHER ORDER
    MOMENTS).

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EXTENDED HYDRODYNAMICAL MODELS
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APPLICATION OF THE METHOD
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TEST 1D DIODE N N N
35
TEST FOR THE EXTENDED MODEL WITH 1D
STRUCTURESMUSCATO ROMANO, 2001
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TEST OF THE EXTENDED (MEP-CLOSURE) MODELS ON A 2D
BIPOLAR TRANSISTOR
43
ENERGY BAND AND HOT ELECTRONS
44
MOMENTUM PRODUCTION (y-COMPONENT)
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