Transport and Piezoresistive Characteristics of Ruthenium‐Doped Bismuth–Borosilicate Glass Thin Films Grown by Pulsed Laser Deposition

Ruthenium-doped bismuth–borosilicate glass thin films were grown by pulsed laser deposition as a material with a chemical structure equivalent to that of the functional region in a thick-film resistor (TFR) with piezoresistivity. X-ray diffraction and electron energy-loss spectroscopy analyses indicated that the thin films were in amorphous and contained both trivalent and tetravalent states of ruthenium after annealing in air. Analyses of transport properties verified that the electrical conduction in the film was via variable range hopping with a hole carrier. Furthermore, one of the films exhibits piezoresistive sensitivity six times as that of the TFR; the sensitivity has a strong correlation with the spatial extension of the wave function in the localized electronic states.

[1]  T. Nonaka,et al.  Chemical and Piezoresistive Microanalyses at the Interface of RuO2-Glass Diffusion Pairs , 2010 .

[2]  X. Q. Wei,et al.  Comparative study on structural and optical properties of ZnO thin films prepared by PLD using ZnO powder target and ceramic target , 2009 .

[3]  S. Nahm,et al.  Effect of oxygen vacancy and Mn-doping on electrical properties of Bi4Ti3O12 thin film grown by pulsed laser deposition , 2009 .

[4]  T. Tani,et al.  Microanalyses on the RuO2 Particle–Glass Matrix Interface in Thick‐Film Resistors with Piezoresistive Effects , 2009 .

[5]  D. Bäuerle,et al.  Pulsed-laser deposition of smooth thin films of Er, Pr and Nd doped glasses , 2009 .

[6]  Virginie Nazabal,et al.  Dysprosium doped amorphous chalcogenide films prepared by pulsed laser deposition , 2006 .

[7]  O. Korostynska,et al.  Development of high sensitivity oxide based strain gauges and pressure sensors , 2006 .

[8]  Pulsed laser deposition and characterization of europium borate glass films , 2005 .

[9]  Darko Belavic,et al.  The influence of firing temperature on the electrical and microstructural characteristics of thick-film resistors for strain gauge applications , 2003 .

[10]  T. Maeder,et al.  Piezoresistivity and conductance anisotropy of tunneling-percolating systems , 2002, cond-mat/0211133.

[11]  Uichiro Mizutani,et al.  Introduction to the Electron Theory of Metals: Superconductivity , 2001 .

[12]  M. Hrovat,et al.  Characterisation of thick film resistor series for strain sensors , 2001 .

[13]  M. Somora,et al.  Conduction Mechanism in RuO2-Based Thick Films , 1998 .

[14]  M. Hiratani,et al.  SrRuO3 Thin Films Grown under Reduced Oxygen Pressure , 1996 .

[15]  Burke,et al.  Generalized Gradient Approximation Made Simple. , 1996, Physical review letters.

[16]  R. J. Brook,et al.  Conduction mechanisms in RuO2-glass composites , 1995 .

[17]  Kenji Adachi,et al.  Ruthenium clusters in lead-borosilicate glass in thick film resistors , 1994 .

[18]  Roger H. French,et al.  Thin Glass Film between Ultrafine Conductor Particles in Thick-Film Resistors , 1994 .

[19]  B. Chiou,et al.  Temperature dependence of the electrical conduction in RuO2-based thick film resistors , 1992 .

[20]  Peter Francis Carcia,et al.  Electrical conduction and strain sensitivity in RuO2 thick film resistors , 1983 .

[21]  Carleton H. Seager,et al.  Electrical properties and conduction mechanisms of Ru‐based thick‐film (cermet) resistors , 1977 .