Palladium and metal-free phthalocyanine bilayer structures for hydrogen detection in the SAW sensor system based on interaction speed

被引:8
|
作者
Jakubik, Wieslaw P. [1 ]
Urbanczyk, Marian W. [1 ]
Maciak, Erwin [1 ]
机构
[1] Silesian Tech Univ, Optoelect Dept, Inst Phys, PL-44100 Gliwice, Poland
关键词
bilayer structure; hydrogen detection; interaction speed; metal-free phthalocyanine (H2PC); palladium (Pd); surface acoustic wave (SAW); SELECTIVE LAYER; GAS SENSOR; FILM;
D O I
10.1109/JSEN.2006.881343
中图分类号
TM [电工技术]; TN [电子技术、通信技术];
学科分类号
0808 ; 0809 ;
摘要
Bilayer structures with various thicknesses of metal-free phthalocyanine (H2Pc) (similar to 80, similar to 120, and similar to 160 nm) but the same thickness of palladium (Pd) (similar to 20 mn), have been studied for hydrogen gas-sensing application at temperatures of similar to 30 degrees C and similar to 50 degrees C with a method based on interaction speed. The structures were fabricated in two different vacuum deposition processes (first the H2Pc film and than the Pd) onto an LiNbO3 Y- cut Z-propagating substrate for the surface acoustic wave (SAW) method and additionally (in these same technological processes) onto a glass substrate with a planar microelectrode array for the simultaneous monitoring of the structure planar resistance. A very good correlation has been observed between these two methods (frequency changes for the SAW method coincide with the decrease of the bilayer structure resistance), especially for higher hydrogen concentrations. Although simultaneous measurements were not always feasible (too great resistance in the samples for the structure with the thinnest H2Pc), they can provide information about the acoustoelectric interactions between SAW and charge carriers in the bilayer structure. The interaction speed method is based on the great variance in interaction speeds at various hydrogen concentrations (from 2.5% to 4% in synthetic dry air), even though the amplitude signal reaches almost the same frequency level. For a particular chosen initial interaction time interval, a distinct interaction speed can be distinguished with great resolution (from 7.5 Hz/s for 2.5% H-2 in air to 29.1 Hz/s for 4% for the structure with 160-nm H2Pc and 20-nm Pd). These initial interaction fragments are linear versus time for the investigated medium hydrogen concentrations in synthetic dry air. In the case of the investigated bilayer structures, the interaction speed is higher for the structure with the thinnest H2Pc film (similar to 80 nm).
引用
收藏
页码:1178 / 1185
页数:8
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