Lecture 2.0 Thermodynamics in Chip Processing Terry Ring.
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Transcript of Lecture 2.0 Thermodynamics in Chip Processing Terry Ring.
Lecture 2.0Lecture 2.0
Thermodynamics in Chip Processing
Terry Ring
Field Effect Transistor (FET)Field Effect Transistor (FET)
Gate OxideGate Oxide
Capacitor connecting Gate to center of npn or pnp heterojunction
Capacitance– Area– Thickness– Dielectric constant of oxide
Dictates the Speed of the Switch
Gate Oxide CapacitanceGate Oxide Capacitance
C=oA/d
=C/Co
=1+e
e =electric susceptibility
Field Effect Transistor (FET)Field Effect Transistor (FET)
Silicon OxidationSilicon Oxidation Thermodynamics
• (yes/no? How Far? Heat/cool)
– Furnace at T=850C– Pure Oxygen
• Si + O2 SiO2
Kinetics (how fast)– BL-Mass Transfer
• J=Kg(CA-0)
– SS-Diffusion• J=DO-SiO2 (dC/dx)
– Heat Transfer• BL, q=h(T1-T)• Solid, q=kSiO2(dT/dx)
– J=q/Hrxn
Thermodynamics of ReactionsThermodynamics of Reactions
Thermodynamics Can Tell you Three Things– Is reaction spontaneous
• Gibbs Free Energy, ΔGrxn(T) Grxn<0, Spontaneous Grxn>0, Non-Spontaneous
– What are Equilibrium Ratios?• ΔGrxn(T)= - RT ln(Keq)
– Does Reaction create heat?• Heat of Reaction, ΔHrxn(T)
– Exothermic, ΔHrxn(T)<0, get hot!– Endothermic, ΔHrxn(T)>0
Reaction to Make SiOReaction to Make SiO22
Si (s) + O2 (g) SiO2(s)
– Done in Vacuum Furnace.Does the Reaction Go?
– Po2 =0.001 atm
– T= 600 C
Gibbs Free EnergyGibbs Free Energy
Si (s) + O2 (g) SiO2(s)
ΔGrxn(T)=GSiO2 (T)- GSi(T) - GO2 (T) = - RT ln(Keq) -ΔGo
rxn(T)=GSiO2 (T)- GSi(T) - GO2 (T) Keq=Xo2=Po2/PTot
If ΔGrxn(T)=0, then • ΔGo
rxn(T) = - RT ln(Po2)
GSiO2 (T) = ΔHSiO2(T) -TΔSoSiO2
• ΔHSiO2(T) =Hof-SiO2+To∫TCp-SiO2(T) dT
GSi (T) = ΔHSi(T) -TΔSoSi
• ΔHSi(T) =Hof-Si+To∫TCp-Si(T) dT
Grxn<0, Spontaneous
webbook.nist.gov/chemistry/
Po2 = 0.001 atm
T = 600 C
ΔGrxn(T)= ΔGo
rxn(T) - RTln(Po2)-180 kcal/mole-(-10kcal/mole)= -170 kcal/moleSpontaneous!
Want to Create OWant to Create O22 with wet H with wet H22
H2O(g) H2(g) + ½ O2(g)
Equilibium ΔGrxn(T)= - RT ln(Keq)Keq = (XH2 √Xo2)/XH2O
ΔGrxn(T)= ΔGH2 (T)+1/2 ΔG o2 (T)- ΔGH2O(T)
At T = 600 C What H2/H2O
Ratio?
Want to Create OWant to Create O22 with CO/CO with CO/CO22 ratio ratio
2CO2(g) 2CO(g) + O2(g)
Equilibium ΔGrxn(T)= - RT ln(Keq)
Keq = (XCO2 Xo2)/XCO22
ΔGrxn(T)= 2ΔGCO (T)+ΔG o2 (T) - 2ΔGCO2(T)
At T = 600 C What CO/CO2
Ratio?
What Memory Chip Really Looks LikeWhat Memory Chip Really Looks Like
MetalizationMetalization
Transistor Contacts– Base– Emitter– Gate
Metal Deposition– Chemical Vapor Deposition
CVD of Poly Si – Gate conductorCVD of Poly Si – Gate conductor
SiH4 Si (s) + 2 H2
– 620C, vacuum
– N2 Carrier gas with SiH4 and dopant precursor
Stack of wafer into furnace– Higher temperature at exit to compensate for
gas conversion losses
Add gases Stop after layer is thick enough
CVD ReactorCVD Reactor
Wafers in Carriage (Quartz)
Gasses enterPumped out via
vacuum systemPlug Flow
Reactor
Vacuum
CVD of W – Metal plugsCVD of W – Metal plugs
3H2+WF6 W (s) + 6HF– T>800C, vacuum– He carrier gas with WF6
– Side Reactions at lower temperatures• Oxide etching reactions• 2H2+2WF6+3SiO2 3SiF4 + 2WO2 + 2H2O• SiO2 + 4HF 2H2O +SiF4
Stack of wafer into furnace Add gases Stop after layer is thick enough
Chemical EquilibriumChemical Equilibrium
DRAM Memory DRAM Memory CellCell
1 Bit1 Bit
Capacitor
Gate or Row Line
Column Line
N P N
SiO2
Si
Wafer
CVD of SiOCVD of SiO22 – Dielectric – Dielectric
Si(0C2H5)4 +7O2SiO2(s)+ 10 H2+ 8CO2
– 400C, vacuum– He carrier gas with vaporized(or atomized)
Si(0C2H5)4 and O2 and B(CH3)3 and/or P(CH3)3 dopants for BSG and BPSG
Stack of wafer into furnace– Higher temperature at exit to compensate for
gas conversion losses Add gases Stop after layer is thick enough
CVD of SiCVD of Si33NN44 - Implantation mask - Implantation mask
3 SiH2Cl2 + 4 NH3Si3N4(s)+ 6 HCl + 6 H2
– 780C, vacuum
– Carrier gas with NH3 / SiH2Cl2 >>1
Stack of wafer into furnace– Higher temperature at exit to compensate for
gas conversion losses
Add gases Stop after layer is thick enough