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Muddiest Points
Electronic Properties II:
Intrinsic & Extrinsic Semiconductors
Muddiest Points:
โ€ข โ€œWhat are the differences between intrinsic and
extrinsic semiconductors?โ€
โ€ข โ€œWhat are the differences between n type and p type
extrinsic semiconductors?โ€
โ€ข โ€œHow does temperature affect each type of
semiconductor?โ€
โ€ข โ€œWhat are the differences in the conductivity equation
for intrinsic and extrinsic semiconductors?โ€
โ€ข โ€œWhat is the relation of electron and electron-hole
mobility to conductivity?โ€
Intrinsic Semiconductors

ENERGY

No Dopants

๏ฑ Less than 1021/m3 impurity
atoms (10-6 wt% impurities)
๏ฑ electron-hole pairs (n=p=ni)
๏ฑ Conductivity increases with
an increase in temperature
(creates more e-h pairs)
๏ฑ Energy Gap (Eg) is constant
and between 0.1eV-2eV
๏ฑ Group IV elemental
semiconductors
๏ฑ Group III + Group V are
compound semiconductors
Extrinsic Semiconductors: p-type

ENERGY

p-type Dopants

๏ฑ Impurity atoms have one less
valence electron than the host
๏ฑ Majority Charge Carriers:
electron holes (p>>n)
๏ฑ Minority Charge Carriers:
electrons (n<<p)
๏ฑ Acceptor States (contribute
electron holes)
๏ฑ Saturation = all acceptor states
filled
๏ฑ Example: Boron (B3+), Group III,
impurity atoms within a Silicon
host (Si4+), Group IV
Extrinsic Semiconductors: n-type

ENERGY

n-type Dopants

๏ฑ Impurity atoms have one more
valence electron than the host
๏ฑ Majority Charge Carriers:
electrons (n>>p)
๏ฑ Minority Charge Carriers:
electron holes (p<<n)
๏ฑ Donor States (contribute
electrons)
๏ฑ Exhaustion = every donated
electron in Cond. Band
๏ฑ Example: Phosphorus (P5+),
Group V, impurity atoms within
a Silicon host (Si4+), Group IV
Intrinsic - Electron and Hole Migration
ENERGY

Si4+

Si4+

-

Si4+

+-

+
Extrinsic p-type: Majority Carriers - Holes

ENERGY

Si4+
B3+

*No electric field applied
Extrinsic n-type: Majority Carriers - Electrons

ENERGY

Si4+
P5+

*No electric field applied
Effect of Temperature: Intrinsic
๐›” = ๐’ ๐’Š ๐’’(๐› ๐’† + ๐› ๐’‰ )

๐’๐’Š โˆ

๐‘ฌ๐’ˆ
โˆ’
๐’† ๐Ÿ๐’Œ๐‘ป

ni = intrinsic carrier density
(# of carriers/m3)
Eg = energy gap (eV)
k = Boltzmann Constant
(8.6173 x 10-16 eV-K-1)
T = Temperature (K)
Effect of Temperature: Intrinsic
๐›” = ๐’ ๐’Š ๐’’(๐› ๐’† + ๐› ๐’‰ )

๐’๐’Š โˆ

๐‘ฌ๐’ˆ
โˆ’
๐’† ๐Ÿ๐’Œ๐‘ป

ni = intrinsic carrier density
(# of carriers/m3)
Eg = energy gap (eV)
k = Boltzmann Constant
(8.6173 x 10-16 eV-K-1)
T = Temperature (K)
Effect of Temperature: Extrinsic
๏ฑ Freeze-out region: not
enough thermal energy for
dopant activation
๏ฑ Extrinsic region: limited
temperature effect on
extrinsic conductivity
๏ฑ Intrinsic region: an
increase in temperature,
increases thermal energy
creating a large number of
electron-hole pairs
Conductivity Equation
Intrinsic Semiconductors (n=p=ni)

๐›” = ๐ง๐ช๐› ๐’† + ๐ฉ๐ช๐› ๐’‰

๐›” = ๐’ ๐’Š ๐’’(๐› ๐’† + ๐› ๐’‰ )

ฯƒ = conductivity

(ohm-m)-1

ni = intrinsic carrier density

(# of carriers/m3)

q = electric charge

1.6x10-19 (C)

ฮผe = electron mobility

(m2/(V-s))

ฮผh = electron hole mobility

(m2/(V-s))
Conductivity Equation: p-type
Extrinsic Semiconductors: p-type (p>>n)

๐›” = ๐ง๐ช๐› ๐’† + ๐ฉ๐ช๐› ๐’‰

๐›” โ‰ˆ ๐’‘๐’’๐› ๐’‰

ฯƒ = conductivity

(ohm-m)-1

p = positive carrier density

(# of carriers/m3)

q = electric charge

1.6x10-19 (C)

ฮผh = electron hole mobility

(m2/(V-s))
Example 1: p-type Conductivity
What is the conductivity of silicon containing
3.13 x 1021 boron dopant atoms per m3? Silicon
has an electron mobility of 0.14 (m2/(V-s)) and
a hole mobility of 0.05 (m2/(V-s)).

๐›” = ๐ง๐ช๐› ๐’† + ๐ฉ๐ช๐› ๐’‰
๐› ๐’‰ = 0.05 (m2/(V-s))

๐›” = (3.13 x 1021

๐›” โ‰ˆ ๐’‘๐’’๐› ๐’‰
๐’‘= 3.13 x 1021 m-3

m-3)(1.6x10-19 C)(0.05 m2/(V-s))

๐›” = ๐Ÿ๐Ÿ“. ๐ŸŽ๐Ÿ’ (ฮฉ-m)-1
Conductivity Equation: n-type
Extrinsic Semiconductors: n-type (n>>p)

๐›” = ๐ง๐ช๐› ๐’† + ๐ฉ๐ช๐› ๐’‰

๐›” โ‰ˆ ๐’๐’’๐› ๐’†

ฯƒ = conductivity

(ohm-m)-1

n = negative carrier density

(# of carriers/m3)

q = electric charge

1.6x10-19 (C)

ฮผe = electron mobility

(m2/(V-s))
Example 2: n-type Conductivity
What is the conductivity of silicon containing
3.13 x 1021 phosphorus dopant atoms per m3?
Silicon has an electron mobility of 0.14 (m2/(Vs)) and a hole mobility of 0.05 (m2/(V-s)).

๐›” = ๐ง๐ช๐› ๐’† + ๐ฉ๐ช๐› ๐’‰
๐› ๐’† = 0.14 (m2/(V-s))

๐›” = (3.13 x 1021

๐›” โ‰ˆ ๐’๐’’๐› ๐’†
๐ง= 3.13 x 1021 m-3

m-3)(1.6x10-19 C)(0.14 m2/(V-s))

๐›” = ๐Ÿ•๐ŸŽ. ๐Ÿ๐Ÿ (ฮฉ-m)-1
Wrap-Up
Electronic Properties II:
Intrinsic & Extrinsic Semiconductors
โ€ข โ€œWhat are the differences between intrinsic and
extrinsic semiconductors?โ€
โ€ข โ€œWhat are the differences between n type and p
type extrinsic semiconductors?โ€
โ€ข โ€œHow does temperature affect each type of
semiconductor?โ€
โ€ข โ€œWhat are the differences in the conductivity
equation for intrinsic and extrinsic
semiconductors?โ€
โ€ข โ€œWhat is the relation of electron and electronhole mobility to conductivity?โ€

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MSEASUSlides: Muddiest points: Electronic Properties II

  • 1. Muddiest Points Electronic Properties II: Intrinsic & Extrinsic Semiconductors Muddiest Points: โ€ข โ€œWhat are the differences between intrinsic and extrinsic semiconductors?โ€ โ€ข โ€œWhat are the differences between n type and p type extrinsic semiconductors?โ€ โ€ข โ€œHow does temperature affect each type of semiconductor?โ€ โ€ข โ€œWhat are the differences in the conductivity equation for intrinsic and extrinsic semiconductors?โ€ โ€ข โ€œWhat is the relation of electron and electron-hole mobility to conductivity?โ€
  • 2. Intrinsic Semiconductors ENERGY No Dopants ๏ฑ Less than 1021/m3 impurity atoms (10-6 wt% impurities) ๏ฑ electron-hole pairs (n=p=ni) ๏ฑ Conductivity increases with an increase in temperature (creates more e-h pairs) ๏ฑ Energy Gap (Eg) is constant and between 0.1eV-2eV ๏ฑ Group IV elemental semiconductors ๏ฑ Group III + Group V are compound semiconductors
  • 3. Extrinsic Semiconductors: p-type ENERGY p-type Dopants ๏ฑ Impurity atoms have one less valence electron than the host ๏ฑ Majority Charge Carriers: electron holes (p>>n) ๏ฑ Minority Charge Carriers: electrons (n<<p) ๏ฑ Acceptor States (contribute electron holes) ๏ฑ Saturation = all acceptor states filled ๏ฑ Example: Boron (B3+), Group III, impurity atoms within a Silicon host (Si4+), Group IV
  • 4. Extrinsic Semiconductors: n-type ENERGY n-type Dopants ๏ฑ Impurity atoms have one more valence electron than the host ๏ฑ Majority Charge Carriers: electrons (n>>p) ๏ฑ Minority Charge Carriers: electron holes (p<<n) ๏ฑ Donor States (contribute electrons) ๏ฑ Exhaustion = every donated electron in Cond. Band ๏ฑ Example: Phosphorus (P5+), Group V, impurity atoms within a Silicon host (Si4+), Group IV
  • 5. Intrinsic - Electron and Hole Migration ENERGY Si4+ Si4+ - Si4+ +- +
  • 6. Extrinsic p-type: Majority Carriers - Holes ENERGY Si4+ B3+ *No electric field applied
  • 7. Extrinsic n-type: Majority Carriers - Electrons ENERGY Si4+ P5+ *No electric field applied
  • 8. Effect of Temperature: Intrinsic ๐›” = ๐’ ๐’Š ๐’’(๐› ๐’† + ๐› ๐’‰ ) ๐’๐’Š โˆ ๐‘ฌ๐’ˆ โˆ’ ๐’† ๐Ÿ๐’Œ๐‘ป ni = intrinsic carrier density (# of carriers/m3) Eg = energy gap (eV) k = Boltzmann Constant (8.6173 x 10-16 eV-K-1) T = Temperature (K)
  • 9. Effect of Temperature: Intrinsic ๐›” = ๐’ ๐’Š ๐’’(๐› ๐’† + ๐› ๐’‰ ) ๐’๐’Š โˆ ๐‘ฌ๐’ˆ โˆ’ ๐’† ๐Ÿ๐’Œ๐‘ป ni = intrinsic carrier density (# of carriers/m3) Eg = energy gap (eV) k = Boltzmann Constant (8.6173 x 10-16 eV-K-1) T = Temperature (K)
  • 10. Effect of Temperature: Extrinsic ๏ฑ Freeze-out region: not enough thermal energy for dopant activation ๏ฑ Extrinsic region: limited temperature effect on extrinsic conductivity ๏ฑ Intrinsic region: an increase in temperature, increases thermal energy creating a large number of electron-hole pairs
  • 11. Conductivity Equation Intrinsic Semiconductors (n=p=ni) ๐›” = ๐ง๐ช๐› ๐’† + ๐ฉ๐ช๐› ๐’‰ ๐›” = ๐’ ๐’Š ๐’’(๐› ๐’† + ๐› ๐’‰ ) ฯƒ = conductivity (ohm-m)-1 ni = intrinsic carrier density (# of carriers/m3) q = electric charge 1.6x10-19 (C) ฮผe = electron mobility (m2/(V-s)) ฮผh = electron hole mobility (m2/(V-s))
  • 12. Conductivity Equation: p-type Extrinsic Semiconductors: p-type (p>>n) ๐›” = ๐ง๐ช๐› ๐’† + ๐ฉ๐ช๐› ๐’‰ ๐›” โ‰ˆ ๐’‘๐’’๐› ๐’‰ ฯƒ = conductivity (ohm-m)-1 p = positive carrier density (# of carriers/m3) q = electric charge 1.6x10-19 (C) ฮผh = electron hole mobility (m2/(V-s))
  • 13. Example 1: p-type Conductivity What is the conductivity of silicon containing 3.13 x 1021 boron dopant atoms per m3? Silicon has an electron mobility of 0.14 (m2/(V-s)) and a hole mobility of 0.05 (m2/(V-s)). ๐›” = ๐ง๐ช๐› ๐’† + ๐ฉ๐ช๐› ๐’‰ ๐› ๐’‰ = 0.05 (m2/(V-s)) ๐›” = (3.13 x 1021 ๐›” โ‰ˆ ๐’‘๐’’๐› ๐’‰ ๐’‘= 3.13 x 1021 m-3 m-3)(1.6x10-19 C)(0.05 m2/(V-s)) ๐›” = ๐Ÿ๐Ÿ“. ๐ŸŽ๐Ÿ’ (ฮฉ-m)-1
  • 14. Conductivity Equation: n-type Extrinsic Semiconductors: n-type (n>>p) ๐›” = ๐ง๐ช๐› ๐’† + ๐ฉ๐ช๐› ๐’‰ ๐›” โ‰ˆ ๐’๐’’๐› ๐’† ฯƒ = conductivity (ohm-m)-1 n = negative carrier density (# of carriers/m3) q = electric charge 1.6x10-19 (C) ฮผe = electron mobility (m2/(V-s))
  • 15. Example 2: n-type Conductivity What is the conductivity of silicon containing 3.13 x 1021 phosphorus dopant atoms per m3? Silicon has an electron mobility of 0.14 (m2/(Vs)) and a hole mobility of 0.05 (m2/(V-s)). ๐›” = ๐ง๐ช๐› ๐’† + ๐ฉ๐ช๐› ๐’‰ ๐› ๐’† = 0.14 (m2/(V-s)) ๐›” = (3.13 x 1021 ๐›” โ‰ˆ ๐’๐’’๐› ๐’† ๐ง= 3.13 x 1021 m-3 m-3)(1.6x10-19 C)(0.14 m2/(V-s)) ๐›” = ๐Ÿ•๐ŸŽ. ๐Ÿ๐Ÿ (ฮฉ-m)-1
  • 16. Wrap-Up Electronic Properties II: Intrinsic & Extrinsic Semiconductors โ€ข โ€œWhat are the differences between intrinsic and extrinsic semiconductors?โ€ โ€ข โ€œWhat are the differences between n type and p type extrinsic semiconductors?โ€ โ€ข โ€œHow does temperature affect each type of semiconductor?โ€ โ€ข โ€œWhat are the differences in the conductivity equation for intrinsic and extrinsic semiconductors?โ€ โ€ข โ€œWhat is the relation of electron and electronhole mobility to conductivity?โ€