1 Chapter 5-1. PN-junction electrostatics You will also learn about: Poisson’s Equation Built-In...

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1 Chapter 5-1. PN-junction electrostatics You will also learn about: Poisson’s Equation Built-In Potential Depletion Approximation Step-Junction Solution In this chapter you will learn about pn junction electrostatics: Charge density, electric field and electrostatic potential existing inside the diode under equilibrium and steady state conditions.

Transcript of 1 Chapter 5-1. PN-junction electrostatics You will also learn about: Poisson’s Equation Built-In...

Page 1: 1 Chapter 5-1. PN-junction electrostatics You will also learn about: Poisson’s Equation Built-In Potential Depletion Approximation Step-Junction Solution.

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Chapter 5-1. PN-junction electrostatics

You will also learn about:

Poisson’s Equation

Built-In Potential

Depletion Approximation

Step-Junction Solution

In this chapter you will learn about pn junction electrostatics:

Charge density, electric field and electrostatic potential existing

inside the diode under equilibrium and steady state conditions.

Page 2: 1 Chapter 5-1. PN-junction electrostatics You will also learn about: Poisson’s Equation Built-In Potential Depletion Approximation Step-Junction Solution.

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PN-junction fabrication

PN-junctions are created by several processes including:

1. Diffusion

2. Ion-implantation

3. Epitaxial deposition

Each process results in different doping profiles

Page 3: 1 Chapter 5-1. PN-junction electrostatics You will also learn about: Poisson’s Equation Built-In Potential Depletion Approximation Step-Junction Solution.

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Ideal step-junction doping profile

Page 4: 1 Chapter 5-1. PN-junction electrostatics You will also learn about: Poisson’s Equation Built-In Potential Depletion Approximation Step-Junction Solution.

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Equilibrium energy band diagram for the pn junction

kT

EEnp Fi

i exp

EF = same everywhere under equilibrium

Join the two sides of the band by a smooth curve.

kT

EEnn iF

i exp

Page 5: 1 Chapter 5-1. PN-junction electrostatics You will also learn about: Poisson’s Equation Built-In Potential Depletion Approximation Step-Junction Solution.

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Electrostatic variables for the equilibrium pn junction

x

E

qx

E

q d

d1

d

d1 iC E

Potential, V = (1/q) (EC–Eref). So,potential difference between the two sides (also called built-in voltage, Vbi) is equal to (1/q)(EC).

xd

dE

refC1

EEq

V

= charge density = Ks o

Page 6: 1 Chapter 5-1. PN-junction electrostatics You will also learn about: Poisson’s Equation Built-In Potential Depletion Approximation Step-Junction Solution.

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Conceptual pn-junction formationConceptual pn-junction formation

Holes and electrons will diffuse towards opposite directions, uncovering ionized dopant atoms. This will build up an electric field which will prevent further movement of carriers.

p and n type regionsbefore junction formation

Page 7: 1 Chapter 5-1. PN-junction electrostatics You will also learn about: Poisson’s Equation Built-In Potential Depletion Approximation Step-Junction Solution.

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The built-in potential, Vbi

When the junction is formed, electrons from the n-side and holes from the p-side will diffuse leaving behind charged dopant atoms. Remember that the dopant atoms cannot move! Electrons will leave behind positively charged donor atoms and holes will leave behind negatively charged acceptor atoms.

The net result is the build up of an electric field from the positively charged atoms to the negatively charged atoms, i.e., from the n-side to p-side. When steady state condition is reached after the formation of junction (how long this takes?) the net electric field (or the built in potential) will prevent further diffusion of electrons and holes. In other words, there will be drift and diffusion currents such that net electron and hole currents will be zero.

Page 8: 1 Chapter 5-1. PN-junction electrostatics You will also learn about: Poisson’s Equation Built-In Potential Depletion Approximation Step-Junction Solution.

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Equilibrium conditions

Under equilibrium conditions, the net electron current and hole current will be zero.

electron drift currentopposite to electron flux

NA = 1017 cm3 ND = 1016 cm3

electron diffusion currentopposite to electron flux

hole diffusion current

hole drift current

net current = 0

net current = 0

E-field

Page 9: 1 Chapter 5-1. PN-junction electrostatics You will also learn about: Poisson’s Equation Built-In Potential Depletion Approximation Step-Junction Solution.

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The built-in potential, Vbi

p-side n-side

EC

Ei

EV

iFi ln

n

pkTEE

q Vbi = (Ei EF)p-side + (EF Ei)n-side

iiF ln

n

nkTEE

EC

Ei

EV

EF

Page 10: 1 Chapter 5-1. PN-junction electrostatics You will also learn about: Poisson’s Equation Built-In Potential Depletion Approximation Step-Junction Solution.

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The built-in potential, Vbi

The built-in potential, Vbi, measured in Volts, is numerically equal to the “shift” in the bands expressed in eV.

Vbi = (1/q) {(Ei EF)p-side + (EF Ei)n-side }

sidenonionconcentratelectronand

sideponionconcentratholewhere

ln

lnln

n

p

2i

np

ii

n

p

n

np

q

kT

n

n

q

kT

n

p

q

kT

kT

Vq

n

n

p

p biexpp

n

n

pAn interesting fact:

Page 11: 1 Chapter 5-1. PN-junction electrostatics You will also learn about: Poisson’s Equation Built-In Potential Depletion Approximation Step-Junction Solution.

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Majority and minority carrier concentrations

pp

np

nn

pn

xp xn

x

p-side NA ND n-side

Page 12: 1 Chapter 5-1. PN-junction electrostatics You will also learn about: Poisson’s Equation Built-In Potential Depletion Approximation Step-Junction Solution.

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Built-in potential as a function of doping concentration for an abrupt p+n or n+p junction

Page 13: 1 Chapter 5-1. PN-junction electrostatics You will also learn about: Poisson’s Equation Built-In Potential Depletion Approximation Step-Junction Solution.

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Depletion approximation

elseeverywhere0

for)(0

0d

d

npADs

s

xxxNNK

q

Kx

EPoisson equation

We assume that the free carrier concentration inside the depletion region is zero.

Page 14: 1 Chapter 5-1. PN-junction electrostatics You will also learn about: Poisson’s Equation Built-In Potential Depletion Approximation Step-Junction Solution.

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Example 1

A p-n junction is formed in Si with the following parameters. Calculate the built-in voltage, Vbi.

ND = 1016 cm–3 NA = 1017 cm–3

Calculate majority carrier concentration in n-side and p-side. Assume nn = ND = 1016 cm3 and pp = NA= 1017 cm3.

2i

DA2i

npbi lnln

n

NN

q

kT

n

np

q

kTV

Plug in the numerical values to calculate Vbi.

Page 15: 1 Chapter 5-1. PN-junction electrostatics You will also learn about: Poisson’s Equation Built-In Potential Depletion Approximation Step-Junction Solution.

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Example 2

A pn junction is formed in Si with the following parameters. Calculate the built-in voltage, Vbi.

ND = 2 1016 cm–3 NA = 3 1017 cm–3

NA = 1 1016 cm–3 ND = 2 1017 cm–3

Calculate majority carrier concentration in n-side and p-side. nn = “effective ND” = 1016 cm-3; pp = “effective NA” = 1017 cm–3

2i

DA2i

npbi lnln

n

NN

q

kT

n

np

q

kTV

Plug in the numerical values to calculate Vbi.

Here NA and ND

are “effective” ornet values.