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SEMICONDUCTORS AND NANOSTRUCTURES 2009Mobility spectrum analysis in InN:MgThe mechanism of electrical conductivity and the possibleoccurr<strong>en</strong>ce of superconductivity in InN remains the subjectof considerable controversy. All rec<strong>en</strong>t Hall measurem<strong>en</strong>tsof InN samples doped with Mg or Be acceptors give a signfor the Hall voltage appropriate for electrons. This anomalousresult is presumably due to the pres<strong>en</strong>ce of an n-typesurface inversion layer. One of the method used to detectthe expected pres<strong>en</strong>ce of multi-carrier conduction in theInN system is the measurem<strong>en</strong>t of the resistivity t<strong>en</strong>sor as afunction of magnetic field to perform a quantitative mobilityspectrum analysis. In the case of InN:Mg such an analysisshould in particular give the signs of the contributionsoriginating from electrons and holes if both are pres<strong>en</strong>t.However, in the case of InN:Mg this is a chall<strong>en</strong>ging measurem<strong>en</strong>tsince the mobility of holes is probably very lowand comparable with that of the surface electrons. In addition,the samples are inhomog<strong>en</strong>ous and unfortunately, theycan be measured only in the van der Pauw configurationbecause etching of InN samples to produce Hall bars stillposes a problem. All this makes it difficult to obtain preciseabsolute values of the ρ xx and ρ xy resistivity compon<strong>en</strong>ts,which is indisp<strong>en</strong>sable for a reliable mobility spectrumanalysis. Moreover, ev<strong>en</strong> for strictly n-type samplesthere oft<strong>en</strong> appears in the mobility spectrum the so called“ghost holes” which can lead to errors in the interpretationof the results. Thus, an appearance of a hole peak in themobility spectrum is not necessarily a reliable signature ofthe real pres<strong>en</strong>ce of holes in a sample.peak is higher than electron peak revealed a positive signfor the thermopower). It also agrees very well with the conclusionthat only for moderate Mg cont<strong>en</strong>t can free holesreally be detected in InN:Mg, while for higher doping theformation of donor-like defects (in agreem<strong>en</strong>t with amphotericdefects model) makes the sample progressively moreand more n-type.Figure 56: Magnetic field dep<strong>en</strong>d<strong>en</strong>ce of a resistivity t<strong>en</strong>sor compon<strong>en</strong>tsρ xx and ρ xy of the E1053 sampleWe have performed a systematic investigation of 11InN:Mg samples with Mg-doping from 6 × 10 18 cm −3 to7.3 × 10 20 cm −3 together with 3 undoped (n-type) InN refer<strong>en</strong>cesamples. Our previous preliminary measurem<strong>en</strong>tswith two van der Pauw configurations and magnetic fieldup to 19 T showed hole peaks in mobility spectrum analysisbut it was problematic to find a reasonable correlationbetwe<strong>en</strong> the mobility spectra and the nominal Mg-doping.Our rec<strong>en</strong>t measurem<strong>en</strong>ts show that only all possible permutationsof configurations of curr<strong>en</strong>t and voltage probesand both polarities of the magnetic field up to 28 T givesreliable results. Figure.56 pres<strong>en</strong>ts typical ρ xx and ρ xytraces as a function of the magnetic field. In figure 57 wepres<strong>en</strong>t the results of mobility spectrum analysis for a seriesof samples with increasing Mg cont<strong>en</strong>t (from 6 × 10 18to 4.2×10 20 cm −3 ) for the samples E1003 to E1041 respectively).The obtained series of spectra correlates well withthe measurem<strong>en</strong>ts of thermoelectric power performed onthe same set of samples (only sample E1053 for which holeFigure 57: Mobility spectrum analysis of a series of InN:Mg sampleswith increasing Mg cont<strong>en</strong>t (from E1053 to E1041, respectively).D.K. MaudeL. Dmowski (Institute of High Pressure Physics, Warsaw), L.Konczewicz (GES-UM2, Montpellier), M.Baj (Institute ofExperim<strong>en</strong>tal Physics, University of Warsaw)44

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