Study of the piezoresistivity of doped nanocrystalline silicon thin films

dc.contributor.authorGaspar, J.
dc.contributor.authorGieschke, P.
dc.contributor.authorEhling, C.
dc.contributor.authorKistner, J.
dc.contributor.authorGonçalves, N. J.
dc.contributor.authorVasilevskiy, Mikhail
dc.contributor.authorPaul, O.
dc.contributor.authorAlpuim, P.
dc.date.accessioned2011-07-08T11:45:24Z
dc.date.available2011-07-08T11:45:24Z
dc.date.issued2011-06
dc.description.abstractThe piezoresistive response of n- and p-type hydrogenated nanocrystalline silicon thin films, deposited by hot-wire (HW) and plasma-enhanced chemical vapor deposition (PECVD) on thermally oxidized silicon wafers, has been studied using four-point bending tests. The piezoresistive gauge factor (GF) was measured on patterned thin-film micro-resistors rotated by an angle θ with respect to the principal strain axis. Both longitudinal (GFL) and transverse (GFT) GFs, corresponding to θ = 0° and 90°, respectively, are negative for n-type and positive for p-type films. For other values of θ (30°, 45°, 120°, and 135°) GFs have the same signal as GFL and GFT and their value is proportional to the normal strain associated with planes rotated by θ relative to the principal strain axis. It is concluded that the films are isotropic in the growth plane since the GF values follow a Mohr’s circle with the principal axes coinciding with those of the strain tensor. The strongest p-type pirezoresistive response (GFL = 41.0, GFT = 2.84) was found in a film deposited by PECVD at a substrate temperature of 250 °C and working pressure of 0.250 Torr, with dark conductivity 1.6 Ω−1cm−1. The strongest n-type response (GFL =− 28.1, GFT =− 5.60) was found in a film deposited by PECVD at 150 °C and working pressure of 3 Torr, with dark conductivity 9.7 Ω−1cm−1. A model for the piezoresistivity of nc-Si is proposed, based on a mean-field approximation for the conductivity of an ensemble of randomly oriented crystallites and neglecting grain boundary effects. The model is able to reproduce the measured GFL values for both n- and p-type films. It fails, however, to explain the transversal GFT data. Both experimental and theoretical data show that nanocrystalline silicon can have an isotropic piezoresistive effect of the order of 40% of the maximum response of crystalline silicon.por
dc.description.sponsorshipFundação para a Ciência e a Tecnologia (FCT) - PTDC/CTM/66558/2006, bolsa de investigação SFRH/BSAB/883/2009por
dc.identifier.doi10.1063/1.3599881por
dc.identifier.issn0021-8979por
dc.identifier.urihttps://hdl.handle.net/1822/12753
dc.language.isoengpor
dc.peerreviewedyespor
dc.publisherAIP Publishingpor
dc.relation.publisherversionhttp://m.jap.aip.org/resource/1/japiau/v109/i12/p123717_s1por
dc.rightsopenAccesspor
dc.subjectBendingpor
dc.subjectDark conductivitypor
dc.subjectNanostructured materialspor
dc.subjectPiezoresistancepor
dc.subjectPlasma CVDpor
dc.subjectSemiconductor thin filmspor
dc.subjectSiliconpor
dc.subjectNanofabricationpor
dc.subject.wosScience & Technologypor
dc.titleStudy of the piezoresistivity of doped nanocrystalline silicon thin filmspor
dc.typearticlepor
dspace.entity.typePublicationen
oaire.citationEndPage123717-9por
oaire.citationIssue12por
oaire.citationStartPage123717-1por
oaire.citationTitleJournal of Applied Physicspor
oaire.citationVolume109por
sdum.journalJournal of Applied Physicspor

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