Large piezoelectric d 33 coefficients around 600 pC/N are found in corona-charged non-uniform electrets consisting of elastically "soft" (microporous polytetrafluoroethylene PTFE) and "stiff" (perfluorinated cyclobutene PFCB) polymer layers. The piezoelectric activity of the twolayer fluoropolymer stack exceeds the d 33 coefficient of the ferroelectric ceramic lead zirconate titanate (PZT) by more than a factor of two and that of the ferroelectric polymer polyvinylidene fluoride (PVDF) by a factor of 20. Soft piezoelectric materials may become interesting for a large number of sensor and transducer applications, in areas such as security systems, medical diagnostics, and nondestructive testing. 77.84.Jd; 85.50.+k Piezoelectricity is the basis for a large number of sensor and transducer applications. Mass products emerge in security systems, medical diagnostics and nondestructive testing [1]. Basic science benefits from resonant ultrasound spectroscopy for the determination of acoustical properties of materials with sample masses of only a few µg [2]. Sensitive and low-cost piezoelectric materials are in high demand for these applications. In this rapid communication, very large piezoelectric coefficients are reported in charged heterogeneous electret films, surpassing all materials known so far. A heterogeneous two-layer electret stack, based on exceptionally stable fluoropolymer charge electrets is proposed and experimentally demonstrated. Preliminary results indicate not only very large, but also long-term stable piezoelectric effects, most promising for applications in sensor and transducer devices.
PACS:Piezoelectric material constants relate second-order symmetric tensors (stress T or strain S) to vectors (displacement D or electric field E). Since electric field and stress are independent variables easily to control experimentally, the most often used piezoelectric tensor is the third-rank d-tensor relating displacement D and stress T (direct piezoelectric effect) or strain S and electric field E (inverse piezoelectricIn piezoelectric sensors and thickness mode resonators, the d 33 coefficient is employed, 3 denotes the polar axis and the contracted notation is used. A necessary condition for the occurrence of piezoelectricity is the absence of a center of symmetry, piezoelectric materials are therefore intrinsically anisotropic. Large piezoelectric coefficients are usually found in ferroelectric crystals and polymers. The most widely employed piezoelectric material, lead zirconate titanate (PZT), with a composition near the morphotropic phase boundary between the rhombohedral and tetragonal phase shows a d 33 coefficient of 220 pC/N [4]. Since the use of lead-containing materials is environmentally hazardous, the development of new piezoelectric materials is a matter of urgency. For a large number of applications, e.g. in medical ultrasound, low-density piezoelectric materials (such as polymers) are interesting, with an acoustic impedance matched to that of the human body. Unfortunately, the d 33 coeff...