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Ion Implantation and Synthesis of Materials - Studium

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11.4 The Mechanisms Behind the <strong>Ion</strong>-Cut Process 151a number <strong>of</strong> techniques. Figure 11.7 shows a high resolution scanning electronmicroscopy (SEM) cross-section image <strong>of</strong> the exfoliated layer. The image showsthe roughness <strong>of</strong> the surface, where the <strong>Ion</strong>-Cut occurred, to be quite small. Alsovisible is the 75 nm thick silicon oxide layer beneath the bond interface. The largearea analysis possible with SEM reveals a uniform thickness <strong>of</strong> the exfoliatedlayer <strong>and</strong> consequently a smooth cut <strong>of</strong> the H-implanted silicon crystal. The SEMdeterminedthickness <strong>of</strong> the exfoliated layer is measured to be 1.42 µm. A surfaceheight analysis using atomic force microscopy (AFM) shows the transferred layerto be 1.40 µm thick. Examination <strong>of</strong> the exfoliated layer by means <strong>of</strong> cross-sectiontransmission electron microscopy (XTEM) measures the thickness <strong>of</strong> thetransferred layer as 1.42 µm.Figure 11.8 combines all the data mentioned above. The H concentration <strong>and</strong> Silattice damage distributions are superimposed. The dashed vertical lines in thefigure represent the range in the <strong>Ion</strong>-Cut location determined by XSEM, AFM <strong>and</strong>XTEM. This data clearly shows that the <strong>Ion</strong>-Cut occurs at the region <strong>of</strong> highestimplantation damage rather than at the H concentration peak. To underst<strong>and</strong> whythe <strong>Ion</strong>-Cut depth is correlated with the ion implantation damage requires a closerexamination <strong>of</strong> the nature <strong>of</strong> the damage.4Hydrogen concentration (at %)32101.0 1.2 1.4 1.6 1.8 2.0Depth (µm)Fig. 11.6. The H concentration depth distribution obtained from an ERD analysis on thesilicon sample implanted with 175 keV protons to a dose <strong>of</strong> 5 × 10 16 H cm 2

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