University of Illinois Optical and Discharge Physics ETCH PROFILES IN SOLID AND POROUS SiO 2  Solid  Porosity = 45 % Pore radius = 10 nm  Porous SiO.

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University of Illinois Optical and Discharge Physics ETCH PROFILES IN SOLID AND POROUS SiO 2  Solid  Porosity = 45 % Pore radius = 10 nm  Porous SiO 2 is being investigated for low- permittivity dielectrics for interconnect wiring.  In polymerizing environments with heavy sidewall passivation, etch profiles differ little between solid and porous silica.  The “open” sidewall pores quickly fill with polymer.  Position (  m) ANIMATION SLIDE UTA_1102_36

University of Illinois Optical and Discharge Physics EFFECT OF PORE RADIUS ON CLEANING  Larger pores have poor view angles to ions and thicker polymer layers.  Lower rate of cleaning results. 4 nm16 nm ANIMATION SLIDE  Ar/O 2 =99/1, 40 sccm, 600 W, 4 mTorr GEM_0204_28

University of Illinois Optical and Discharge Physics CLEANING INTERCONNECTED PORES  Cleaning is inefficient with interconnected pores.  Higher interconnectivity leads to larger shadowing of ions. 60% 100% 0% ANIMATION SLIDE  Interconnectivity  Ar/O 2 =99/1, 40 sccm, 600 W, 4 mTorr GEM_0204_29

University of Illinois Optical and Discharge Physics POLYMER SURFACE STRUCTURES  The avalanche exposes the tubules to a burst of hot electrons, unevenly charging surfaces. Ion fluxes are also uneven.  Electron density  N 2 /O 2 /H 2 O =79.5 / 19.5 / 1, 1 atm, 15 kV, 2.5 ns MINMAX  Electron Temperature Animation Slide GEM_0204_41

University of Illinois Optical and Discharge Physics RESOLVING POLYMER SURFACE STRUCTURES  N 2 /O 2 /H 2 O =79.5 / 19.5 / 1, 1 atm, 15 kV, 2.5 ns MINMAX  Charge density  M+ density  The avalanche exposes the tubules to a burst of hot electrons, unevenly charging surfaces. Ion fluxes are also uneven. GEM_0204_42 Animation Slide