lecture 2.0 thermodynamics in chip processing terry ring

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Lecture 2.0 Lecture 2.0 Thermodynamics in Chip Processing Terry Ring

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Page 1: Lecture 2.0 Thermodynamics in Chip Processing Terry Ring

Lecture 2.0Lecture 2.0

Thermodynamics in Chip Processing

Terry Ring

Page 2: Lecture 2.0 Thermodynamics in Chip Processing Terry Ring

Field Effect Transistor (FET)Field Effect Transistor (FET)

Page 3: Lecture 2.0 Thermodynamics in Chip Processing Terry Ring

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

Page 4: Lecture 2.0 Thermodynamics in Chip Processing Terry Ring

Gate Oxide CapacitanceGate Oxide Capacitance

C=oA/d

=C/Co

=1+e

e =electric susceptibility

Page 5: Lecture 2.0 Thermodynamics in Chip Processing Terry Ring

Field Effect Transistor (FET)Field Effect Transistor (FET)

Page 6: Lecture 2.0 Thermodynamics in Chip Processing Terry Ring

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

Page 7: Lecture 2.0 Thermodynamics in Chip Processing Terry Ring

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

Page 8: Lecture 2.0 Thermodynamics in Chip Processing Terry Ring

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

Page 9: Lecture 2.0 Thermodynamics in Chip Processing Terry Ring

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/

Page 10: Lecture 2.0 Thermodynamics in Chip Processing Terry Ring

Po2 = 0.001 atm

T = 600 C

ΔGrxn(T)= ΔGo

rxn(T) - RTln(Po2)-180 kcal/mole-(-10kcal/mole)= -170 kcal/moleSpontaneous!

Page 11: Lecture 2.0 Thermodynamics in Chip Processing Terry Ring

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)

Page 12: Lecture 2.0 Thermodynamics in Chip Processing Terry Ring

At T = 600 C What H2/H2O

Ratio?

Page 13: Lecture 2.0 Thermodynamics in Chip Processing Terry Ring

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)

Page 14: Lecture 2.0 Thermodynamics in Chip Processing Terry Ring

At T = 600 C What CO/CO2

Ratio?

Page 15: Lecture 2.0 Thermodynamics in Chip Processing Terry Ring

What Memory Chip Really Looks LikeWhat Memory Chip Really Looks Like

Page 16: Lecture 2.0 Thermodynamics in Chip Processing Terry Ring

MetalizationMetalization

Transistor Contacts– Base– Emitter– Gate

Metal Deposition– Chemical Vapor Deposition

Page 17: Lecture 2.0 Thermodynamics in Chip Processing Terry Ring

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

Page 18: Lecture 2.0 Thermodynamics in Chip Processing Terry Ring

CVD ReactorCVD Reactor

Wafers in Carriage (Quartz)

Gasses enterPumped out via

vacuum systemPlug Flow

Reactor

Vacuum

Page 19: Lecture 2.0 Thermodynamics in Chip Processing Terry Ring

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

Page 20: Lecture 2.0 Thermodynamics in Chip Processing Terry Ring

Chemical EquilibriumChemical Equilibrium

Page 21: Lecture 2.0 Thermodynamics in Chip Processing Terry Ring

DRAM Memory DRAM Memory CellCell

1 Bit1 Bit

Capacitor

Gate or Row Line

Column Line

N P N

SiO2

Si

Wafer

Page 22: Lecture 2.0 Thermodynamics in Chip Processing Terry Ring

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

Page 23: Lecture 2.0 Thermodynamics in Chip Processing Terry Ring

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