Fabrication Process 3

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    Ion Implantation

    Doping

    The dominant doping method

    A particle accelerator is used to accelerate a doping atom so that it can

    penetrate a silicon crystal to a depth of several microns Excellent control of dose (cm-2)

    Good control of implant depth with energy (KeV to MeV)

    Repairing crystal damage and dopant activation requires annealing, whichcan cause dopant diffusion and loss of depth control.

    Dopant ions

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    Ion Implantation

    Ion implanter

    The ion implantation process is conducted in a vacuum chamber at very low pressure (10-4to 10-5torr).Large numbers of ions (typically 10

    16

    to 10

    17

    ions/cm

    2

    ) bombard and penetrate a surface, interacting withthe substrate atoms immediately beneath the surface.Typical depth of ion penetration is a fraction of a micron.

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    Annealing

    After ion implantation, lattice damage to the crystal is repaired by heatingthe wafer at a moderate temperature for a few minutes. This process is

    called annealing.

    Furnace annealing takes minutes and causes too much diffusion of dopantsfor some applications.

    Rapid thermal annealing (RTA), the wafer is heated to high temperature inseconds by a bank of heat lamps.

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    Diffusion

    Diffusionis atom movement along concentration gradients.

    There are different mechanisms in which an atom moves within the crystal:

    a) Interstitial diffusion, atoms jump from one interstitial site to another, whichis always available (small atoms, like sodium and lithium).

    b)Substitutional/vacancy diffusion, necessitates that empty lattice site isavailable next to the diffusing atom (antimony and arsenic).

    c) Interstitialcy mechanism, the self-interstitial atoms move to the lattice

    sites, and kick the dopants to the interstitial sites, and from there they moveto the lattice sites (boron and phosphorus).

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    A uniformly doped ingot is sliced intowafers.

    An oxide film is then grown on thewafers.

    The film is patterned and etched usingphotolithography exposing specificsections of the silicon.

    The wafers are then spun with anopposite polarity doping sourceadhering only to the exposed areas.

    The wafers are then heated in a furnace(800-1250oC) to drive the doping atomsinto the silicon.

    Diffusion

    Process

    The doping material used can either be solid,

    liquid or gaseous. In carrier gas diffusion doping, a carrier gas

    carries the doping atoms to the silicon waferswhich been brought by radiant heat totemperatures of 1000C to 1285C.

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    Comparison of Diffusion and Ion Implantation

    Diffusion

    cheaper and more simplisticmethod,

    can only be performed from thesurface of the wafers.

    dopants also diffuse unevenly,and interact with each otheraltering the diffusion rate.

    Ion implantation

    more expensive and complex. It does not require high

    temperatures and also allowsfor greater control of dopantconcentration and profile.

    anisotropic process andtherefore does not spread thedopant implant as much asdiffusion.

    aids in the manufacture of self-aligned structures which

    greatly improve theperformance of MOStransistors.

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    Question??

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    1. Sami Franssila, Introduction to Microfabrication John Wiley & Sons Ltd,2004.

    2. http://www.daviddarling.info/encyclopedia/S/AE_silicon.html

    3. Infrastructure -copyright, 1999

    4. http://en.wikipedia.org/wiki/Photoresist

    5. http://www.n2bio.com/surface-modification-technology/ion-implantation.php

    6. http://www.oxford-instruments.com/

    7. http://www.tpub.com/neets/book14/57d.htm

    References

    Thank you for attention