Design specific variation in pattern transfer by via/contact etch ...

Design specific variation in pattern transfer by via/contact etch ... Design specific variation in pattern transfer by via/contact etch ...

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“Thick Polymer” Approximation Ion-energy transfer through polymer layer is a limiting step in SiO 2 etch rate MC H = ρS k ER = K etch C etch k Γ D CF2 ⎛ kDΓ ⎜ ⎜1− ⎝ ηΓi E CF2 ⎛ H ⎞ ηΓi E0⎜1− ⎟ = K ⎝ H * ⎠ 0 ⎛ ⎜ ⎜ k Γ k′ Γ R O D ⎜1− C ⎞ ⎜ ketch ηΓi E ⎟ ⎠ ⎜ ⎝ etch CF2 ⎛ kDΓ ⎜ ⎜1− ⎝ ηΓi E ⎛ ⎜ ⎜ µ MC ηΓi E0⎜1− 1 ⎜ 3 ⎜ E0 ρS k ⎝ 0 1 CF2 C etch 0 2 ⎞ ⎟ ⎠ ⎞ ⎟ ⎟ ⎟ ⎟ ⎟ ⎠ k′ DΓCF 2 ⎛ k′ DΓ ⎜ ⎜1− ⎝ ηΓi E CF2 0 ⎛ ⎜ ⎜ k Γ k′ Γ R O D ⎜1− C ⎞ ⎜ ketch ηΓi E ⎟ ⎠ ⎜ ⎝ CF2 0 1 ⎛ k′ DΓ ⎜ ⎜1− ⎝ ηΓi E Matsui, M., Tatsumi, T. and Sekine, M., “Relationship of etch reaction and reactive species flux in C4F8/Ar/O2 plasma for SiO2 selective etching over Si and Si3N4,” J. Vac. Sci. Technol. A 19, 2089-2096 (2001). CF2 0 2 ⎞ ⎟ ⎠ ⎞⎞ ⎟⎟ ⎟⎟ ⎟⎟ ⎟⎟ ⎟⎟ ⎠⎠ Copyright ©2008, Mentor Graphics. 18

Etch Stop Condition � Etch stops when ions lose all their energy while penetrating the C-F layer. A condition for the etch stop is follows: k′ D LE ( Γ ) k i R Γ O Γ CF 2 = ρS M C � Knowledge of distributions of ion-neutrals fluxes along the etched surface: allows to determine a regions where etch is completely stopped 1 3 E0 µ Γ ( , y), Γ ( x, y), Γ ( x, y) 2 i x CF O Copyright ©2008, Mentor Graphics. 19

“Thick Polymer” Approximation<br />

Ion-energy <strong>transfer</strong> through polymer layer is a limit<strong>in</strong>g step <strong>in</strong> SiO 2 <strong>etch</strong> rate<br />

MC<br />

H =<br />

ρS<br />

k<br />

ER = K<br />

<strong>etch</strong><br />

C<br />

<strong>etch</strong><br />

k<br />

Γ<br />

D CF2<br />

⎛ kDΓ<br />

⎜<br />

⎜1−<br />

⎝ ηΓi<br />

E<br />

CF2<br />

⎛ H ⎞<br />

ηΓi<br />

E0⎜1−<br />

⎟ = K<br />

⎝ H * ⎠<br />

0<br />

⎛<br />

⎜<br />

⎜ k Γ k′<br />

Γ<br />

R O D<br />

⎜1−<br />

C<br />

⎞ ⎜ k<strong>etch</strong><br />

ηΓi<br />

E<br />

⎟<br />

⎠<br />

⎜<br />

⎝<br />

<strong>etch</strong><br />

CF2<br />

⎛ kDΓ<br />

⎜<br />

⎜1−<br />

⎝ ηΓi<br />

E<br />

⎛<br />

⎜<br />

⎜ µ MC<br />

ηΓi<br />

E0⎜1−<br />

1<br />

⎜ 3<br />

⎜<br />

E0<br />

ρS<br />

k<br />

⎝<br />

0<br />

1<br />

CF2<br />

C<br />

<strong>etch</strong><br />

0<br />

2<br />

⎞<br />

⎟<br />

⎠<br />

⎞<br />

⎟<br />

⎟<br />

⎟<br />

⎟<br />

⎟<br />

⎠<br />

k′<br />

DΓCF<br />

2<br />

⎛ k′<br />

DΓ<br />

⎜<br />

⎜1−<br />

⎝ ηΓi<br />

E<br />

CF2<br />

0<br />

⎛<br />

⎜<br />

⎜ k Γ k′<br />

Γ<br />

R O D<br />

⎜1−<br />

C<br />

⎞ ⎜ k<strong>etch</strong><br />

ηΓi<br />

E<br />

⎟<br />

⎠<br />

⎜<br />

⎝<br />

CF2<br />

0<br />

1<br />

⎛ k′<br />

DΓ<br />

⎜<br />

⎜1−<br />

⎝ ηΓi<br />

E<br />

Matsui, M., Tatsumi, T. and Sek<strong>in</strong>e, M., “Relationship of <strong>etch</strong> reaction and reactive species flux <strong>in</strong> C4F8/Ar/O2 plasma for SiO2 selective <strong>etch</strong><strong>in</strong>g<br />

over Si and Si3N4,” J. Vac. Sci. Technol. A 19, 2089-2096 (2001).<br />

CF2<br />

0<br />

2<br />

⎞<br />

⎟<br />

⎠<br />

⎞⎞<br />

⎟⎟<br />

⎟⎟<br />

⎟⎟<br />

⎟⎟<br />

⎟⎟<br />

⎠⎠<br />

Copyright ©2008, Mentor Graphics.<br />

18

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