scaling of pfc abatement using plasma burn boxes*0 20 40 60 80 100 0 200 400 600 800 1000 cf 4...
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SCALING OF PFC ABATEMENT USING PLASMABURN BOXES*
Xudong “Peter” Xu and Mark J. KushnerUniversity of Illinois
Department of Electrical and Computer EngineeringUrbana, IL 61801
November 1998
*Work supported by National Science Foundation andSemiconductor Research Corp.
UNIVERSITY OF ILLINOISOPTICAL AND DISCHARGE PHYSICS
AGENDA
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• Introduction • Geometries of Etching Reactor and Burn Box • Plasma Chemistry for Ar/PFCs/O 2
• Consumption and Generation of PFCs in Etching Reactor
• Comparison of Predicted C 2F6 Abatement with Experiments
• Plasma Remediation of PFCs in Burn Box
• Concluding Remarks
GWP (100-year ITH)Lifetime (years)
CF4
C2F6
C3F8
CHF3
SF6
NF3
CO2
5000 10,000 15,000 25,000 50,000
6,50050,000
9,20010,000
2,6007,000
11,700250
23,9003,200
13,100740
2001
UNIVERSITY OF ILLINOISOPTICAL AND DISCHARGE PHYSICS
PERFLUOROCOMPOUNDs (PFCs)
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• Perfluorocompounds (PFCs) are widely used as process gases in microelectronics fabrication for etching and chamber cleaning.
• PFCs are absorbers of infrared radiation having long atmospheric lifetimes and thus have high global warming potential.
*
* J. V. Gompel and T. Walling, Semiconductor International, Semp., 1997, p95
UNIVERSITY OF ILLINOISOPTICAL AND DISCHARGE PHYSICS
INVESTIGATION OF PLASMA GENERATION ANDREMEDIATION OF PFCS
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• Since finding suitable substitutes for PFCs is unlikely, remediation of the effluent of plasma etching reactors must be done.
• Destruction of C 2F6 by plasmas has been experimentally demonstrated in
low pressure devices.
• Computer modeling is a useful tool for investigate the physical processes occurring in plasma remediation of PFCs.
• 2-d HPEM simulations have been performed to investigate- Consumption and generation of PFCs in ICP etching reactors - Abatement of PFCs in a plasma burn box
GEOMETRIES OF ETCHING REACTOR AND PLASMABURN BOX
UNIVERSITY OF ILLINOISOPTICAL AND DISCHARGE PHYSICS
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• The test system consists of a plasma etching chamber and a downstream plasma burn box.
• The plasma etching chamber is a 13.56 MHz ICP reactor using Ar/C 2F6 at 10 mTorr. A 20 cm diameter wafer sits on the substrate
• The burn box, which is down stream of the turbopump, is also an ICP reactor with O 2 injection at the higher pressure of 150 mTorr.
Burn Box
Plasma EtchingChamber
Wafer
Coils
O2
Coils
Showerhead Nozzle (Ar /C2F6)
Turbopump
UNIVERSITY OF ILLINOISOPTICAL AND DISCHARGE PHYSICS
OXIDATION CHEMISTRY IN BURN BOX
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O + CF3 → COF2 + F O + CF2 → COF + F
O + CF2 → CO + F + F O + CF → CO + F
O + COF → CO2 + F
O(1D) + CF 3 → COF2 + F O(1D) + CF 2 → COF + F
O(1D) + CF 2 → CO + F + F O(1D) + CF → CO + F
O(1D) + COF → CO2 + F
O+ + CF4 → CF3+ + FO O+ + C2F6 → CF3+ + CF3 + O
O+ + C2F6 → C2F5+ + FO
COF + CF2 → CF3 + CO COF + CF2 → COF2 + CF
COF + CF3 → CF4 + CO COF + CF3 → COF2 + CF2
COF + COF → COF2 + CO
UNIVERSITY OF ILLINOISOPTICAL AND DISCHARGE PHYSICS
EXPERIMENTAL ABATEMENT OF C2F6 IN BURN BOX
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• Sawin and Vitale * investigated the abatement of C 2F6 in an ICP burn box using an internal coil.
• C 2F6: 200 sccm
• O 2: 200 sccm
• Pressure: 500 mTorr
C2F6/O2 =50/50
* 51st Annual Gaseous Electronics Conference
D = 10 cm
0
20
40
60
80
100
0 200 400 600 800 1000
C F4(cal.)
C2F
6(cal.)
C F4(exp.)
C2F
6(exp.)
UNIVERSITY OF ILLINOISOPTICAL AND DISCHARGE PHYSICS
SIMULATION RESULTS FOR EXPERIMENTAL CONDITIONS
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• C 2F6: 200 sccm• O 2: 200 sccm• Pressure: 500 mTorr
Percent of C 2F6:remaining andpercent conversion of CF 4
Power (w)
• The decomposition of C 2F6 is mainly caused by electron impact.
C 2F6 + e → CF3+ + CF3 + e + e
C 2F6 + e → CF3 + CF3 + e
C 2F6 + e → CF3- + CF3 0.16
C2F6 + e → CF5 + F - 0.84
• The generation of CF 4 is via radical
recombination. CF 3 + F → CF4
• The formation of CF 4 depends on the
gas temperature [k=1.78•10 -8•(T/298) -7.73
•exp(-4271/T) cm 3•s -1] and the availability
of F atoms to recombine with CF 3.
• The branching ratio for C 2F6 + e → negative ions significantly changes the formation of CF 4.
UNIVERSITY OF ILLINOISOPTICAL AND DISCHARGE PHYSICS
SIMULATION RESULTS FOR ABATEMENT EXPERIMENT
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• Plasma is generated only near the coils for 500 mTorr pressure due to the finite skin depth.
• Lower level of C 2F6 decomposition is due, in part, to pass through of gases in center.
• C 2F6: 200 sccm• O 2: 200 sccm• Pressure: 500 mTorr• Power: 500 Watts
4.8
0.02
E (10 11cm-3)
0 50
Radius (cm)
26Source-C2F6 (10 17cm-3)
0.0
-5.2
0 515
26
Radius (cm)
Log scale
PLASMA PARAMETER IN ETCHING REACTOR
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• A “standard” ICP reactor having a 4-turn coil is used as a baseline.• Power: 650 W • Gas Mixture: Ar/C 2F6 =60/40• Gas flow: 200 sccm • Pressure: 10 mTorr
11.30.0
Radius (cm) 0 15
0
15
[Eθ] (V/cm)
150 Radius (cm)
1.460.00
E (10 11 cm-3)
1.50.0
15
[P] (W/cm 3)
0Radius (cm)
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FEEDSTOCK NEUTRAL DISSOCIATION
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C2F6(10 13 cm-3)
15
0150
Radius (cm)
CF3 (10 13 cm-3) CF2 (10 13 cm-3)
150 Radius (cm)
• C 2F6 can be dissociated mainly to CF 3, and CF3 can be continuously dissociated to generate CF 2. Due to subsequent reassociation, the densities of C 2F6 increase near pump port.
C2F6 + e → CF3 + CF3 C2F6 + Ar * → CF3 + CF3 + Ar
CF3 + e → CF2 + F + e CF3 + Ar * → CF2 + F + Ar
CF3 + CF3 +M → C2F6 + M
150 Radius (cm)
4.60
0.00
6.03
0.00
6.49
0.00
UNIVERSITY OF ILLINOISOPTICAL AND DISCHARGE PHYSICS
PFC GENERATION IN ETCHING CHAMBER
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• Some PFCs are generated due to radical recombination.
CF3 + F → CF4 CF3 + F 2 → CF4 + F
CF2 + CF3 → C2F5 CF2 + CF2 → C2F4
150 Radius (cm)
C2F4 (10 12 cm-3) C2F5 (10 12 cm-3)
150 Radius (cm)
CF4(10 13 cm-3)
15
0150
Radius (cm)
2.45
0.00
2.22
0.00
8.98
0.00
UNIVERSITY OF ILLINOISOPTICAL AND DISCHARGE PHYSICS
C2F6 CONSUMPTION IN ETCHING REACTOR
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Power (w)Gas Flow Rate
(SCCM)
600500
400
50
80
60
70
100150
200250 300
Input C2F6 = 40%
C2F6 (%)
2030
4050
60Gas Flow Rate
(SCCM)
100150
200250
300
60
70
POWER =500 W
Power (w)
600500
400C2F6 (%)20
3040
50 60
Gas Flow Rate = 200 SCCM
50
60
70
• A design of experiment has been performed to determine the functional relationships for C 2F6 consumption.
• The consumption increases nearly linearly with a decrease in C 2F6 percentage and gas flow rate, and with an increase of power deposition.
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PLASMA PARAMETERS IN BURN BOX
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• A “standard” ICP burn box having a 2-turn coil with radius 4.25 cm and height 26.5 cm is used as a baseline.
• Power: 650 W • Effluent: 227.7 sccm• O 2 injection: 90 sccm
• Pressure: 150 mTorr
21.1
0.12
Power ( W cm -3) Electric field ( V cm -1)
11.9
0.08
1.60
0.76
0.01
E density ( 10 12 cm-1) E Temperature ( ev )
3.59
1.93
0.02
9.98 5.64
UNIVERSITY OF ILLINOISOPTICAL AND DISCHARGE PHYSICS
EFFLUENT CmFn REMOVAL IN PLASMA BURN BOX
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1.94
0.01
2.66
0.02
1.53
0.72
0.01
7.65
3.62
0.05
0.92 1.26
• CF 2, CF3, C2F4 and C2F5 from the etching reactor effluent are almost completely removed in the burn box.
CF2 (10 14cm-3) CF3 (10 14cm-3) C2F4 (10 13cm-3) C2F5 (10 13cm-3)
99.95%Abatement
99.99%Abatement
99.97%Abatement
99.9996%Abatement
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C2F6 ABATEMENT AND CF4 GENERATION
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1.27
0.01
6.15
3.10
0.04
0.64
• In the burn box, C 2F6 in the etching reactor effluent is abated by 75%, but a significant amount of CF 4 can be generated (triple CF 4 in the effluent).
C2F6 (10 15cm-3) CF4 (10 14cm-3)
C2F6 ABATEMENT AND CF4 GENERATION vs POWER, O2• C 2F6 abatement increases with increasing power and O 2 fraction.
• More dissociation of C 2F6 → CF3, O2 → O • Subsequent reactions of O + CF 3• CF 4 generation increases with increasing power and decreasing O 2. CF4 is generated by the reaction of CF 3 + F. In O atom rich environments, CF 3 reacts to produce COF 2.
UNIVERSITY OF ILLINOISOPTICAL AND DISCHARGE PHYSICS
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Relative Percent(to input C 2F6 amount)
150
100
Power (w)600
1000
400
O2 (sccm)80050
40
60
80
Power (w)600
800
400
40
60
O2 (SCCM) 150
100
50
1000
20
80
OXIDATION PRODUCT GENERATION vs POWER, O2
UNIVERSITY OF ILLINOISOPTICAL AND DISCHARGE PHYSICS
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• CO is preferentially formed at high power and high O 2 since CF2 leads to CO. The sources of CF 2 and O are large at higher discharge power.
• CO 2 and COF2 are preferentially formed at high O 2, however subsequent dissociation of CO 2 and COF2 reduces this sensitivity.
Relative Percent (to input C 2F6 amount)
Power (w)600
800
400 O2 (%)
150
50100
0
50
100
1000
O2 (sccm)
150
50
100
Power (w)
1000800
600400
10
20
30
Power (w) O2 (SCCM)
150
100
50
80
40
60
1000800
600400
100
UNIVERSITY OF ILLINOISOPTICAL AND DISCHARGE PHYSICS
CONCLUSION
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• PFC consumption and generation in an ICP plasma etching reactor, and PFC abatement in an ICP burn box have been discussed.
• C 2F6 consumption for Ar/C 2F6 gas mixtures in the etching reactor is
proportional to ICP power deposition, and inversely proportional to C 2F6
mole fraction and total gas flow rate.
• PFCs from the plasma etching effluent can be abated in the ICP burn box at high power and high O 2. With low O 2, C2F6 can be decomposed,
however CF 4 is generated. The major oxidation products are CO 2, CO and
COF2.
• Low decomposition of C 2F6 in can result from the finite electromagnetic
skin depth resulting in “outside” power deposition and “pass through” of gases in the center.