TY - JOUR
T1 - 1/f or flicker noise in cellular percolation systems
AU - Chiteme, C.
AU - McLachlan, D. S.
AU - Balberg, I.
PY - 2003/1/1
Y1 - 2003/1/1
N2 - Flicker or 1/f noise is studied in a series of four composite discs, which consists of carbon black (ground and unground), graphite, and graphite/boron nitride, as the conducting components coating, and a common insulating matrix of talc wax. The measurements were done on the conducting side (π > πc) of the critical volume fraction (πc), within a frequency range of 1.2-1001.2 Hz. The results are analyzed in terms of Hooge's empirical formula with frequency and voltage exponents y and m, respectively. Values of γ obtained are in the range 0.97-1.2. Samples with larger (π - πc) have m ≈ 2, while those with smaller (π - πc) have m significantly lower than 2. The normalized noise at 10 Hz (Sv10Hz/Vm) obey the well-established relationships Sv(f)/Vm∞(π - πc)-k and Sv(f)/Vm∞Rw, where Vis the voltage across the sample with resistance R, while m, k, and w are exponents. However, a change in the value of the exponent k and w was observed in the measured systems, with k taking the values k1 ∼ 0.75-5.23 close to πc and k2 ∼ 2.23-5.54 further into the conducting region. Values of w1 range from 0.36-1.37, while w2 ∼ 0.99-1.59. The k1(w1) are observed when m < 2. The nonuniversality of the k1 and k2 regimes are interpreted as due to the superposition of the behavior that results from the geometry (a random voidlike structure) and the behavior resulting from the presence of non-Ohmic, intergranular contacts between the conducting grains. These exponents are tested for consistency using w =k/t, and compared with predictions from recent theoretical models.
AB - Flicker or 1/f noise is studied in a series of four composite discs, which consists of carbon black (ground and unground), graphite, and graphite/boron nitride, as the conducting components coating, and a common insulating matrix of talc wax. The measurements were done on the conducting side (π > πc) of the critical volume fraction (πc), within a frequency range of 1.2-1001.2 Hz. The results are analyzed in terms of Hooge's empirical formula with frequency and voltage exponents y and m, respectively. Values of γ obtained are in the range 0.97-1.2. Samples with larger (π - πc) have m ≈ 2, while those with smaller (π - πc) have m significantly lower than 2. The normalized noise at 10 Hz (Sv10Hz/Vm) obey the well-established relationships Sv(f)/Vm∞(π - πc)-k and Sv(f)/Vm∞Rw, where Vis the voltage across the sample with resistance R, while m, k, and w are exponents. However, a change in the value of the exponent k and w was observed in the measured systems, with k taking the values k1 ∼ 0.75-5.23 close to πc and k2 ∼ 2.23-5.54 further into the conducting region. Values of w1 range from 0.36-1.37, while w2 ∼ 0.99-1.59. The k1(w1) are observed when m < 2. The nonuniversality of the k1 and k2 regimes are interpreted as due to the superposition of the behavior that results from the geometry (a random voidlike structure) and the behavior resulting from the presence of non-Ohmic, intergranular contacts between the conducting grains. These exponents are tested for consistency using w =k/t, and compared with predictions from recent theoretical models.
UR - http://www.scopus.com/inward/record.url?scp=0037222067&partnerID=8YFLogxK
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AN - SCOPUS:0037222067
SN - 0163-1829
VL - 67
SP - 242071
EP - 2420712
JO - Physical Review B - Condensed Matter and Materials Physics
JF - Physical Review B - Condensed Matter and Materials Physics
IS - 2
M1 - 024207
ER -