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Ion Implantation-Overview
is a low-temperature technique for the introduction of
impurities (dopants) into semiconductors and offers
more flexibility than diffusion.
Wafer is Target in High Energy Accelerator
Impurities “Shot” into Wafer
Ion Implantation
x
Blocking mask
Si
+ C(x) as-implant
depth profile
Depth xEqual-Concentration
contours
Reminder: During implantation, temperature is ambient. However,
post-implant annealing step (>900oC) is required to anneal out defects.
y
Ion Stopping
Ions gradually lose their energy as they travel through
the solid
The loss of ion energy in the target is called stopping.
Ion Implantation Energy Loss
Mechanisms
Si+
+
Si
Si
e
e
+
+
Electronic
stopping
Nuclear
stopping
Crystalline Si substrate damaged by collision
Electronic excitation creates heat
Ion Energy Loss Characteristics
EE143 – Ali Javey
Light ions/at higher energy more electronic stopping
Heavier ions/at lower energy more nuclear stopping
EXAMPLES
Implanting into Si:
H+
B+
As+
Electronic stopping
dominates
Electronic stopping
dominates
Nuclear stopping
dominates
Nuclear collisions: ions collide with atoms. The
positively charged ions are coulombically repealed by
the positive cores of the wafers lattice atoms. This
coulombic repulsion is “screened” by the cloud of
electrons surrounding each atom.
Electronic stopping: If ions graze the lattice atoms,
they do not interact with the lattice atom’s electrons
and not the positive core. This interaction slows the
ions by “viscous friction” similar to a rock thrown into
water.
Advantages of Ion Implantation:
Precise control of dose and depth profile
Very fast (1 6" wafer can take as little as 6 seconds for a
moderate dose)
Wide selection of masking materials
e.g. photoresist, oxide, poly-Si, metal
Less sensitive to surface cleaning procedures
Excellent lateral uniformity (< 1%
variation across 12” wafer)
Disadvantages of Ion
Implantation:
Not all the damage can be corrected by annealing.
Typically has higher impurity content than does
diffusion.
Often uses extremely toxic gas sources such as arsine
(AsH3), and phosphine (PH3).
Expensive
Application
Doping
Nitrogen or other ions can be implanted into a tool
steel target (drill bits, for example).
prosthetic devices such as artificial joints, it is desired
to have surfaces very resistant to both chemical
corrosion and wear due to friction.
ion beam mixing, i.e. mixing up atoms of different
elements at an interface.
Range Distributions
The range of a distribution with a discrete random
variable is the difference between the maximum
value and the minimum value. For a distribution
with a continuous random variable, the range is the
difference between the two extreme points on the
distribution curve, where the value of the function
falls to zero. For any value outside the range of a
distribution, the value of the function is equal to 0.
Range-is the difference between the highest and the
lowest values in a frequency distribution.
-It also the average total of a path length .
Where:
n(x= Rp) = is the peak concentration
Rp = is the projected range
∆Rp(Ợp) = is the standard deviation
Gaussian distribution
Implant Uniformity
 Non uniformity of implanted dopants across a wafer
can be readily untraveled from sheet resistance
measurements.
 Sheet resistance maps of 3 samples implanted with
50keV phosphorous as a function of dose.
(a) 5x 1013 cm-2, (b) 2x 1014 cm-2, (c) 2 x1015 cm-2.
Annealing
 Annealing- It is a process that produces conditions by
heating to above the critical temperature, maintaining a
suitable temperature, and then cooling.
 Annealing is used to induce ductility, soften material,
relieve internal stresses, refine the structure by making
it homogeneous, and improve cold working properties.
Diffusion During Subsequent Anneals
 For implantations far away from the surface and for
reasonable short characteristic diffusion lengths , the
new profile can be approximated by:

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Ion implantation

  • 1.
  • 2. Ion Implantation-Overview is a low-temperature technique for the introduction of impurities (dopants) into semiconductors and offers more flexibility than diffusion. Wafer is Target in High Energy Accelerator Impurities “Shot” into Wafer
  • 3.
  • 4.
  • 5. Ion Implantation x Blocking mask Si + C(x) as-implant depth profile Depth xEqual-Concentration contours Reminder: During implantation, temperature is ambient. However, post-implant annealing step (>900oC) is required to anneal out defects. y
  • 6. Ion Stopping Ions gradually lose their energy as they travel through the solid The loss of ion energy in the target is called stopping.
  • 7. Ion Implantation Energy Loss Mechanisms Si+ + Si Si e e + + Electronic stopping Nuclear stopping Crystalline Si substrate damaged by collision Electronic excitation creates heat
  • 8. Ion Energy Loss Characteristics EE143 – Ali Javey Light ions/at higher energy more electronic stopping Heavier ions/at lower energy more nuclear stopping EXAMPLES Implanting into Si: H+ B+ As+ Electronic stopping dominates Electronic stopping dominates Nuclear stopping dominates
  • 9. Nuclear collisions: ions collide with atoms. The positively charged ions are coulombically repealed by the positive cores of the wafers lattice atoms. This coulombic repulsion is “screened” by the cloud of electrons surrounding each atom. Electronic stopping: If ions graze the lattice atoms, they do not interact with the lattice atom’s electrons and not the positive core. This interaction slows the ions by “viscous friction” similar to a rock thrown into water.
  • 10. Advantages of Ion Implantation: Precise control of dose and depth profile Very fast (1 6" wafer can take as little as 6 seconds for a moderate dose) Wide selection of masking materials e.g. photoresist, oxide, poly-Si, metal Less sensitive to surface cleaning procedures Excellent lateral uniformity (< 1% variation across 12” wafer)
  • 11. Disadvantages of Ion Implantation: Not all the damage can be corrected by annealing. Typically has higher impurity content than does diffusion. Often uses extremely toxic gas sources such as arsine (AsH3), and phosphine (PH3). Expensive
  • 12. Application Doping Nitrogen or other ions can be implanted into a tool steel target (drill bits, for example). prosthetic devices such as artificial joints, it is desired to have surfaces very resistant to both chemical corrosion and wear due to friction. ion beam mixing, i.e. mixing up atoms of different elements at an interface.
  • 13. Range Distributions The range of a distribution with a discrete random variable is the difference between the maximum value and the minimum value. For a distribution with a continuous random variable, the range is the difference between the two extreme points on the distribution curve, where the value of the function falls to zero. For any value outside the range of a distribution, the value of the function is equal to 0. Range-is the difference between the highest and the lowest values in a frequency distribution. -It also the average total of a path length .
  • 14. Where: n(x= Rp) = is the peak concentration Rp = is the projected range ∆Rp(Ợp) = is the standard deviation Gaussian distribution
  • 15.
  • 16.
  • 17. Implant Uniformity  Non uniformity of implanted dopants across a wafer can be readily untraveled from sheet resistance measurements.  Sheet resistance maps of 3 samples implanted with 50keV phosphorous as a function of dose. (a) 5x 1013 cm-2, (b) 2x 1014 cm-2, (c) 2 x1015 cm-2.
  • 18. Annealing  Annealing- It is a process that produces conditions by heating to above the critical temperature, maintaining a suitable temperature, and then cooling.  Annealing is used to induce ductility, soften material, relieve internal stresses, refine the structure by making it homogeneous, and improve cold working properties.
  • 19. Diffusion During Subsequent Anneals  For implantations far away from the surface and for reasonable short characteristic diffusion lengths , the new profile can be approximated by: