7.2. dopant diffusion 3,2013 microtech

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Microelectronics Technology Dopant Diffusion III

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Page 1: 7.2. dopant diffusion 3,2013 microtech

Microelectronics Technology

Dopant Diffusion III

Page 2: 7.2. dopant diffusion 3,2013 microtech

Advanced Models

• Advanced diffusion process models include the modifications to Fick’s laws to account for electric field effects, concentration-dependent diffusion, dopant segregation etc.

• Some advanced models based on point-defect driven diffusion processes at atomic scale have also been developed which predict doping profile very accurately.

Page 3: 7.2. dopant diffusion 3,2013 microtech

Modifications Of Fick's Laws A. Electric field effects

• When the doping is higher than ni, £-field effects become important.

• ε -field induced by higher mobility of electrons and holes compared with dopant ions.

• ε -field enhances the diffusion of dopants causing the field

24 i2 nC

C1h

WhereX

ChDf

++=

∂∂−= If all dopants is ionized

C: Net Doping concentrationh: Electric field enhancement factor

Page 4: 7.2. dopant diffusion 3,2013 microtech
Page 5: 7.2. dopant diffusion 3,2013 microtech

Process Simulation

• SUPREM simulation at 1000˚C. Note the boron profile after As N+ S/D regions e -field effects added. Significant change in the B profile in a NMOS Transistor.

• Field effects can dominate the doping distribution near the source/drain of a MOS device (SUPREM simulation).

Page 6: 7.2. dopant diffusion 3,2013 microtech

Dr. G. Eranna Integrated Circuit Fabrication Technology © CEERI Pilani

Modifications Of Fick's Laws

• Error function profile• Isoconcentration exp. B 10 & B 11

Page 7: 7.2. dopant diffusion 3,2013 microtech

Si B In As Sb P

D0.0 cm2sec-1 560 0.05 0.6 0.011 0.214 3.85

D0.E eV 4.76 3.5 3.5 3.44 3.65 3.66

D+.0 cm2sec-1 0.95 0.6

D+.E eV 3.5 3.5

D.0 cm2sec-1 31.0 15.0 4.44

D.E eV 4.15 4.08 4.0

D=.0 cm2sec-1 44.2

D=.E eV 4.37

Concentration dependent diffusivities

Page 8: 7.2. dopant diffusion 3,2013 microtech

Segregation

TSUPREM IV Plot of B contours after oxidation of uniformly B-doped substrate

• Dopants have different solubilities in different material: Redistribute until chemical potential is same on both sides of the interface.

• Segregation Coefficient: Ratio of equilibrium doping conc.on each side of interface

K0=Csi/CSiO2

K0= 0.3 (B)K0=10 (As,Sb,P)

Page 9: 7.2. dopant diffusion 3,2013 microtech

Dr. G. Eranna Integrated Circuit Fabrication Technology © CEERI Pilani

Segregation

Page 10: 7.2. dopant diffusion 3,2013 microtech

Interfacial Dopant Pile-up• Dopants may also pile up at the interface layer, perhaps only a

monolayer thick. Interfacial dopant dose loss or pile-up may consume up to 50% of the dose in a shallow layer.

• In the experiment (right) 40% of the dose was lost in a 30 sec anneal.

Page 11: 7.2. dopant diffusion 3,2013 microtech

Summary of Macroscopic Approach to Diffusion

• Fick's first law correctly describes dopant diffusion in the limit of low concentrations.

• "Fixes" to this law to account for experimental observations (concentration dependent diffusion and e -field effects), are useful, but at this point the complexity of the "fixes" begins to outweigh their usefulness.

We turn to an atomistic view of diffusion for a deeper understanding.

Page 12: 7.2. dopant diffusion 3,2013 microtech
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Kick-out and Interstitial(cy) Assisted Mechanisms.

Mathematically it is identical to the kick out process and both are referred to as interstitial assisted diffusion

Page 14: 7.2. dopant diffusion 3,2013 microtech
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Inferences About Mechanisms

• Oxidation provides an I injection source.• Nitridation provides a V injection source.• Stacking faults serve as "detectors" as do dopant which

diffuse.• Roles of both I &V in assisting dopant diffusion in Si

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Atomic Scale Interactions • Consider the simple Dopant-Defect Interactions A + I <----> AI • For example OED is explained because oxidation injects I driving the

equation to the right, creating more AI pairs and enhancing the dopant D.• Even under inert conditions, atomic-level description says that dopant

diffusion from the surface contains lot of AI,driving above Eq. to left thus pumping interstitials (Chemical Pumping)

• In the more complex example below, phosphorus diffuses with I, and releases them in the bulk. This enhances the tail region D.

Page 18: 7.2. dopant diffusion 3,2013 microtech

Dr. G. Eranna Integrated Circuit Fabrication Technology © CEERI Pilani

Emitter Push Effect

Pumping of interstitials by diffusion of P which builds up a high supersaturation of these point defects in the interior of sample

Page 19: 7.2. dopant diffusion 3,2013 microtech

Summary of Key Ideas

• Selective doping is a key process in fabricating semiconductor devices.

• Doping atoms generally must sit on substitutional sites to be electrically active.

• Both doping concentration and profile shape are critical in device electrical characteristics.

• Ion implantation is the dominant process used to introduce dopant atoms. This creates damage and thermal annealing is required to repair this damage.

• Powerful simulation tools exist today which model diffusion processes and can predict complex doping profiles.

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