13. Bipolar transistors Optoelectronicshadley/psd/lectures19/jan22.pdf · Institute of Solid State...

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Institute of Solid State Physics Technische Universität Graz 13. Bipolar transistors Optoelectronics Jan. 22, 2020

Transcript of 13. Bipolar transistors Optoelectronicshadley/psd/lectures19/jan22.pdf · Institute of Solid State...

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Institute of Solid State PhysicsTechnische Universität Graz

13. Bipolar transistorsOptoelectronics

Jan. 22, 2020

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Heterojunction bipolar transistors

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Heterojunction bipolar transistor

small emitter-base capacitance to increase speed

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HBT current gain

0

0

(npn)1

B

E

np

C BI I

Higher doping in the emitter makes the minority carrier concentration lower in the emitter.

2

0

exp( / )C V gB BiB

A A

N N E k TnnN N

2

0

exp( / )C V gE BiE

D D

N N E k TnpN N

If the emitter and the base have different band gaps

exp 100000gc vE

B c v B

EN NNN N N k T

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HBT current gain

A HBT has an emitter bandgap of 1.62 and a base bandgap of 1.42.A BJT has an emitter bandgap of 1.42 and a base bandgap of 1.42.Both have an emitter doping of 1018 cm-3 and a base doping of 1015cm-3. How much larger is the gain in the HBT?

HBT 1.62 1.42exp exp 2257BJT 0.0259

g

B

Ek T

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HBT

Trade off gain for higher speed

Higher base dopinglower base resistancereduced Early effectless trouble with punch throughbase can be made thinner -> faster transistors

Because of higher base doping, a higher collector doping is possible without punch through

lower collector resistance

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HBT current gain

band discontinuity reduces emitter efficiencyGraded layer emitter and base improve performance

Si/SiGeAlInAs/InGaAs

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Heterojunction bipolar transistors

Fastest InP/InGaAs HBT's have an fT of 710 GHz.

Higher doping in the base allows for a thinner base without punch through and lower base resistance and thus higher frequency operation

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Microwave engineering

Electronics: L<< f <~ 10 GHz

Microwave: L 10 GHz < f < 1 THz

TeraHertz: L 1 THz < f < 100 THz

Optics: L 100 THz

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Thyristors

Reverse blocking

Forward blocking

Forward conducting

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Thyristors

Used for switching high currents or voltages

1*2 > 1

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Latch-up

http://www.ece.drexel.edu/courses/ECE-E431/latch-up/latch-up.html

Both BJT's conduct, creating a low resistance path between Vdd and GND. The product of the gains of the two transistors in the feedback loop, is greater than one. The result of latchup is at the minimum a circuit malfunction, and in the worst case, the destruction of the device.

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Subthreshold current

If the p-concentration in the channel is low, electrons emitted into the channel by the forward biased junction diffuse across the channel without recombining.

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Interdigitated contacts in power transistors

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http://lampx.tugraz.at/~hadley/psd/L13/igbt.html

Used to switch large currents (in electric cars or trains).

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Insulated gate bipolar transistor (IGBT)

Used to switch large currents (in electric cars or trains).

Equivalent circuit in the on-state. From Streetman.

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BiCMOS

Bipolar junction transistors: high speedhigh gainlow output impedance good for analog amplifiers

CMOS high impedancelow power logic

See: http://www.iue.tuwien.ac.at/phd/puchner/node48_app.html

Fransila

Only one additional step to CMOS is needed for BiCMOS

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Institute of Solid State PhysicsTechnische Universität Graz

Optoelectronics

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Institute of Solid State Physics

OptoelectronicsTechnische Universität Graz

light emitting diodelaser diode solar cellphoto detectors

communications, memory (DVD), displays, printing, bar-code readers, solar energy, lighting, laser surgery, measurement, guidance, spectroscopy, LiFi

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Photo detectors

Intrinsic semiconductor = e(nn + pp) (used in copiers)

Unbiased pn junction - like a solar cell

Reverse biased pn junction - smaller capacitance, higher speed, less noise

Phototransistor - light injects carriers into the base. This forward biases the emitter base junction. High responsivity.

Ambient light detectors.

Active Pixel sensors for automated parking and gesture control (uses time-of-flight to image in 3-D).

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Laser printer

semiconducting photoconductor

https://en.wikipedia.org/wiki/Laser_printing

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Absorption

0( ) xx e Photon flux:

Sharp absorption edge for direct bandgap materials

32*

6 -1

0

3.5 10 cmgrEm

m

direct bandgap indirect bandgap

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Confinement of light by total internal reflection

less pulse spreading for parabolically graded fiber

0.6 dB/km at 1.3 m and 0.2 dB/km at 1.55 m

n1sin n2sin2

n n

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Light emitting diodes

Solid state lighting is efficient.

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direct bandgap:k = 0

photons can be emitted

indirect bandgap:k = 0

phonons are emitted

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Light emitting diodes

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IR LED

Measurement by Jan Enenkel

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Light emitting diodes

absorptionreflectiontotal internal reflection

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Galaxy Tab

Encapsulation technology

OLEDs

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Prof. Günther Leising

Electroluminescence in poly(p-phenylene)

poly(3-hexylthiophene)

In 1992, Leising et al. for the first time reported on blue electroluminescence from OLEDs containing poly(p-phenylene) (PPP).

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OLEDs

GlassITO anode

Aluminum cathode

Cathode is typically a low work function material Al, Ca - injects electrons

Anode is typically a high work function material ITO - injects holes

Cathode

Anode

Eg

Hole transport layer

Electron transport layerEmission layer

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Q-dot LEDs

Coe-Sullivan, et al. Advanced Functional Materials, 10.1002/adfm.200400468