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            | "METAL-POLYMER NANOCOMPOSITES OBTAINED BY COMBINED PLASMA TEHNIQUES" |  
            | TE_229 |  |  
            
              
                
                  
   Stage II. Investigation of species present in polymerization plasma (PECVD) and in magnetron sputtering plasma (PVD); Synthesis, by means of sequential PECVD/PVD deposition, of metal-polymer nanocomposites materials with controlled surface plasmon resonance frequency, using various metals   Representative images associated to the results obtained in the second stage of TE_229 project: 
                
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                  | Schematic of the experimental set-up for the synthesis of metal-polymer composites and plasma diagnostics |  # Experimental set-up for the metal-polymer composite consists in a stainless steel vacuum chamber provided with a magnetron sputtering source and a PECVD plasma source; # 
              The sources are mounted perpendicular one to each other, and respectively at 45 degrees in respect to the substrate;
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              The setup allows the sequential or simultaneous substrate exposure to the PVD plasma source and to the PECVD plasma source;
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              The system includes mounting on perpendicular port of mass spectrometer head, Langmuir probes and optical fiber slots for Optical Emission Spectroscopy.
   # Topographical and morphological investigations of the copper-polythiophene reveal the formation of core-shell type structures consisting of nanometer sized Cu nanoparticles coated with a thin polythiohene layer. # 
              Spectroscopic ellipsometry measurements followed by model fiting of the Cu-PPTh composites show a strong absorption peak around 740 nm, associated with the surface plasmon resonance effect due to the presence of Cu nanoparticles in the plasma polymer matrix
   # Typical MS spectrum of the Ar/C4H4S mixture  presents the expected cracking pattern of the thiophene inside the mass  spectrometer with major peaks corresponding to C4H4S (84  amu), C2H2S (58 amu) and CHS (45 amu),the Ar – related  peaks at 40 and 20 amu Ar neutrals; once the plasma is ignited, the appearance  of completely new formed species, as CS2 at 76 amu is obvious;
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                The mass spectra signal of ions associated to the masses higher than  that of thiophene (C2H3S2+ (91  amu), C4H4S2+ (116 amu), etc).proves  oligomerization reactions in the plasma volume;
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                Monomer depletion was calculated for the  prominent mass signals; a sharp increase of the monomer depletion immediately  upon plasma ignition (1-3 W) and a much slighter
   
                
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                  | Dependence of the Ar and Cu abundances in the mass spectra as function of the applied RF power masses |  # Ar peak (40 amu) and Cu peaks (63 and 65 amu) dominated the mass spectra of the plasma generated by the magnetron plasma source;# 
              Ar neutrals present a maximum intensity around 100 W applied RF power;
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              Cu neutrals show a maximum intensity around 110 W applied RF.
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