Semiconductor Devices 2013 Semiconductor Devices - 2013

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Semiconductor Devices 2013 Semiconductor Devices - 2013 Lecture Course Part of Part of SS Module PY4P03 Dr. P. Stamenov School of Physics and CRANN, Trinity College, Dublin 2, Ireland Hilary Term, TCD 8 th of Feb ‘13

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Microsoft PowerPoint - SS_Semiconductor_Devices_2012_Lecture6 [Compatibility Mode]SS Module PY4P03
Dr. P. Stamenov
School of Physics and CRANN, Trinity College, Dublin 2, Ireland,
Hilary Term, TCD 8th of Feb ‘13
Process Flow Example – p-n Diode Wafer
Diffused  Region
V Groo e JFET
Si MESFET Diffused Grown H j i
FET MESFET GaAs MESFET
InP MESFET Multiple Gate Interdigitals
Si MOSFET NMOS, PMOS CMOS
MOSFET GaAs MOSFET
HMOS DMOS, DIMOSGaAs MOSFET VMOS SOS, SOI
Remarks on FETs • Essentially unipolar devices – the current flow (either holes or
electrons) bet een t o electrodes (so rce and drain) is controlled belectrons) between two electrodes (source and drain) is controlled by the potential difference to a third electrode (gate). Cl ( l ) t h i b h i Li l L t t l• Close (closer) to ohmic behaviour. Linear or square law. Lower total harmonic distortion and intermodulation distortion.
• Much higher input impedance. Lower input currents. Simpler matching to microwave circuits.
• Negative temperature coefficient. Self-limiting, with a much lower probability for a thermal runaway or breakdown.
• No minority carrier storage effects – higher switching speeds and higher cutoff frequencies.
• Conceptually simpler, with close to equilibrium carrier concentrations, virtually no carrier injection or extraction., y j
• Could have been the first ones to be realized...
...The First One • Part of Lilienfeld’s first
patent This resemblespatent. This resembles a modern MESFET, but was unrealisablewas unrealisable without semiconductors.
• Shockley et al ~ 1948Shockley et al ~ 1948 worked on similar concepts but had toconcepts, but had to abandon patenting them because of Lilienfeld’s because o e e d s work. Reproposed by Mead et al ~1966
• Most semiconductor transistors are nowtransistors are now unipolar.
MEtal Semiconductor - MESFET Contact Metal ImplantedMetal
Gate Recipe •DrainGate
O idi• Oxidize • Open windows • Implant • Metalize
Semiconductor base • ... FeaturesOxide InsulationEpitaxial Layer Features • Building block
id iR l ti l i l k ith • Provides gain • Voltage-control device
• Relatively simple – can work with compound semiconductors (Schottky gate) F hi h bili h l • Unipolar device• Fast – can use high mobility channels
• Can be done in SOI version, as well
Junction Field Effect Transistor - JFET Contact Metal ImplantedMetal
Gate Recipe •DrainGate
Semiconductor base • ... FeaturesOxide InsulationEpitaxial Layer Features • Building block
id iL i fi it t t • Provides gain • Voltage-control device
• Low noise – finite gate current • Very flexible intermediate frequencies
lifi ( d id l i ) • Unipolar deviceamplifier (used widely in preamps) • Enhancement and depletion modes
Metal Oxide Semiconductor - MOSFET Gate Metal ImplantedGate
Oxide Recipe •DrainOxide
Semiconductor base • ... FeaturesOxide InsulationEpitaxial Layer Features • Building block
id iV l t t b t h t i • Provides gain • Voltage-control device
• Very low gate current, but somewhat noisy • Can use both bias signs at the gate contact
• Unipolar device• Enhancement and depletion modes • Buried channel devices possible
Idealised JFET
After: G. C. Dacey
d I M Rand I. M. Ross, Proc. I. R. E. 41 970 (1953)41, 970 (1953)
Potential Distribution - JFET Poisson’s Equation for the channel
For n-type channelThreat as in diodes
Depletion depthDepletion depth at source
Depletion depth b i i
Preparing for a purely linear at arb. positionpurely linear approximation
Build-in potential
Pinch-off VoltageAt the opposite end of the gate
Current D i
of the gate
Drain Current
Potential variationRemember that λd is Potential variation in the channel
d variable in the channel
Saturation Current - JFET
Pinch-off currenr
The MOSFET
After: S. M. Sze, Physics of Semiconductor Devices, 2nd edition
Conductivity – MOSFET case
DistributedIntrinsic Charge
Intrinsic Capacitance
Drain CurrentCurrent
Threshold Voltage