"Transport n\u00E1boje a \u0161um v tlust\u00FDch vrstv\u00E1ch na b\u00E1zi polymeru"@cs . . "MIDEM" . "Charge carrier transport and noise in polymer based thick films" . . "2"^^ . "26220" . . "6"^^ . . "961-91023-4-7" . "468473" . "15-20" . . "P(GA102/05/2095), Z(MSM0021630503)" . "[291C75D787B2]" . "2"^^ . "Charge carrier transport and noise in polymer based thick films"@en . "Noise, Non-linearity, Polymers based TFRs, Charge carrier transport"@en . . . "We have studied thick film layers made from different polymer vehicles and three types of conducting particles \u2013 silver, carbon, graphite, and their mixture. We proposed the point contact model for the charge carrier transport in the polymer based thick film structures. The model is based on the assumption, that the charge transport is due to the electrons thermally emitted from a metallic grain and that their transfer to another grain has a main component given by ballistic transport [1] and tunneling [2] through the barrier between these two particles. Main noise and non-linearity sources in polymer based thick film layer are considered to be the contacts between conducting grains. On the basis of our model the sheet resistance and effective number of electrons acting as mobility fluctuators in one point contact can be calculated. From the low frequency noise measurements we can estimate the number of point contacts in the thick film resistive layer. The influence of the polymer vehicle and therma" . "\u0160ikula, Josef" . "Charge carrier transport and noise in polymer based thick films"@en . . . "We have studied thick film layers made from different polymer vehicles and three types of conducting particles \u2013 silver, carbon, graphite, and their mixture. We proposed the point contact model for the charge carrier transport in the polymer based thick film structures. The model is based on the assumption, that the charge transport is due to the electrons thermally emitted from a metallic grain and that their transfer to another grain has a main component given by ballistic transport [1] and tunneling [2] through the barrier between these two particles. Main noise and non-linearity sources in polymer based thick film layer are considered to be the contacts between conducting grains. On the basis of our model the sheet resistance and effective number of electrons acting as mobility fluctuators in one point contact can be calculated. From the low frequency noise measurements we can estimate the number of point contacts in the thick film resistive layer. The influence of the polymer vehicle and therma"@en . "RIV/00216305:26220/06:PU58473!RIV07-GA0-26220___" . . . "Slovinsko" . "Transport n\u00E1boje a \u0161um v tlust\u00FDch vrstv\u00E1ch na b\u00E1zi polymeru"@cs . "We have studied thick film layers made from different polymer vehicles and three types of conducting particles \u2013 silver, carbon, graphite, and their mixture. We proposed the point contact model for the charge carrier transport in the polymer based thick film structures. The model is based on the assumption, that the charge transport is due to the electrons thermally emitted from a metallic grain and that their transfer to another grain has a main component given by ballistic transport [1] and tunneling [2] through the barrier between these two particles. Main noise and non-linearity sources in polymer based thick film layer are considered to be the contacts between conducting grains. On the basis of our model the sheet resistance and effective number of electrons acting as mobility fluctuators in one point contact can be calculated. From the low frequency noise measurements we can estimate the number of point contacts in the thick film resistive layer. The influence of the polymer vehicle and therma"@cs . "RIV/00216305:26220/06:PU58473" . . . . "4th European Microelectronics and Packaging Symposium with Table-Top Exhibition - Proceedings" . "2006-05-21+02:00"^^ . . "Sedl\u00E1kov\u00E1, Vlasta" . . . . . . "Charge carrier transport and noise in polymer based thick films" . "Terme Catez" .