class 05 device physics ii

Upload: kumaranraj

Post on 08-Aug-2018

216 views

Category:

Documents


0 download

TRANSCRIPT

  • 8/22/2019 Class 05 Device Physics II

    1/13

    1

    Class 05: Device Physics II

    Topics:

    1. Introduction

    2. NFET Model and Cross Section with Parasitics

    3. NFET as a Capacitor

    4. Capacitance vs. Voltage Curves

    5. NFET as a Capacitor - Band Diagrams at V=0

    6. NFET as a Capacitor - Accumulation V0

    8. NFET as a Capacitor - Inversion V>>0

    9. Band Diagrams, Charges, E-Field, and Potential

    10. Band Diagrams at various biasing

    11. Depletion Layer Width vs. Substrate Doping12. NFET Cross Section, Parasitics, and Biasing

    13. Full CV Curve for reference

  • 8/22/2019 Class 05 Device Physics II

    2/13

    2

    Class 05: Device Physics II

    Goal is to understand the parasitic regions and terms shown in the model and cross section

    Last lecture covered the pn junctions of the source and drain

    This lecture will cover the channel

    Question - where is the biggest capacitor?

    NFET Model and Cross Section with Parasitics (Martin p.101)

  • 8/22/2019 Class 05 Device Physics II

    3/13

    3

    Class 05: Device Physics IINFET as a Capacitor (Martin p.87, Singh p.418)

    The channel region of an FET can be thought of as a series connection

    of capacitors, the capacitance due to the thin oxide, and the capacitance due to

    the semiconductor.

    The thin oxide capacitance is fixed.

    The semiconductor capacitance depends on the biasing

  • 8/22/2019 Class 05 Device Physics II

    4/13

    4

    Class 05: Device Physics IICapacitance vs. Voltage Curves (Singh p.419)

    Much like IV curves define a transistor, CV curves define capacitors

    Three regions of importance: (1) accumulation (2) depletion (3) inversion

    Further foils will describe each of these regions

    Once again, this is the channel region of a transistor and how it behaves when biased

    To obtain a CV curve, one biases the top plate with a DC bias, and uses an AC signal

    to determine the response of the carriers at the surface to the AC signal. So from

    I=C dv/dt, one can back out the capacitance based on the measured current

  • 8/22/2019 Class 05 Device Physics II

    5/13

    5

    Class 05: Device Physics IINFET as a Capacitor - Band Diagrams at V=0 (Sze p.427)

    This state is referred to as the flat-bandcondition

    that is, no applied potential, the bands are flat in the ideal

    case. So why is Vfb not at Vg=0 in the CV plot below?

    Important terms to take from these diagrams are:

    d insulator thickness

    qB Energy of offset between Fermi and intrinsic levels

    Important observations to make:

    How can you tell from the band diagram which is n-type andwhich is p-type semiconductor?

    Even the oxide has bands of allowed states, it is just that

    the band gap is very large

    This portion of CV curve referred to as the flat band capacitance

  • 8/22/2019 Class 05 Device Physics II

    6/13

    6

    Class 05: Device Physics IINFET as a Capacitor - Accumulation V

  • 8/22/2019 Class 05 Device Physics II

    7/13

    7

    Class 05: Device Physics IINFET as a Capacitor - Depletion V>0 (Sze p.428; Martin p.89)

    This state is referred to as the depletioncondition because the

    majority carrier are depleted from the surface

    Important observations to make:

    With a parallel plate analogy, this is where the thickness of the Cs plate

    is increasing, due to the increase in the depletion regions.

    Thus the capacitance is going down.

    CG

    = COX

    Cdep

    / (COX

    + Cdep

    ) < COX

  • 8/22/2019 Class 05 Device Physics II

    8/13

    8

    Class 05: Device Physics IINFET as a Capacitor - Inversion V>>0 (Sze p.428; Martin p.89)

    This state is referred to as the inversioncondition because the

    minority carriers are brought to the surface of the channel. However,

    minority carrier respond slower to the AC signal (minority

    carrier lifetimes). Thus inversion in a CV curve is only obtained

    with very slow varying signals.

    Important observations to make:

    With a parallel plate analogy, this is where the thickness of the Cs plate

    is at its maximum.

    During normal operation of a transistor, the carriers are suppliedby the source and drain, so there is no lack of carriers.

    The definition of inversion is where surface potential > bulk potential

    Vt is defined as the condition in which the surface is inverted, based on Cmi

  • 8/22/2019 Class 05 Device Physics II

    9/13

    9

    Class 05: Device Physics IIBand Diagrams, Charges, E-Field, and Potential (Sze p.434)

    Spice model parameter

    PHI is 2s

  • 8/22/2019 Class 05 Device Physics II

    10/13

    10

    Class 05: Device Physics IIBand Diagrams at various biasing (Sze p.430)

  • 8/22/2019 Class 05 Device Physics II

    11/13

    11

    Class 05: Device Physics IIDepletion Layer Width vs. Substrate Doping (Sze p.437)

  • 8/22/2019 Class 05 Device Physics II

    12/13

    12

    Class 05: Device Physics IINFET Cross Section, Parasitics, and Biasing (Martin p.101)

    We have covered the source/drain to substrate junctions, and now

    the gate/oxide/surface junction

    Next, how they come together for the operation of an NFET

  • 8/22/2019 Class 05 Device Physics II

    13/13

    13

    Class 05: Device Physics IIFull CV Curve for reference (Sze p.438)