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Sökning: WFRF:(Janson M.S.)

  • Resultat 1-10 av 29
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1.
  • Achtziger, N, et al. (författare)
  • Hydrogen passivation of silicon carbide by low-energy ion implantation
  • 1998
  • Ingår i: Applied Physics Letters. - : AIP Publishing. - 0003-6951 .- 1077-3118. ; 73, s. 945-947
  • Tidskriftsartikel (refereegranskat)abstract
    • implantation of deuterium is performed to investigate the mobility and passivating effect of hydrogen in epitaxial alpha-SiC (polytypes 4H and 6H). To avoid excessive damage and the resulting trapping of hydrogen, the implantation is performed with low energy (600 eV H-2(2)+). The H-2 depth profile is analyzed by secondary ion mass spectrometry. Electrical properties are measured by capacitance-voltage profiling and admittance spectroscopy. In p-type SIG, hydrogen diffuses on a mu m scale even at room temperature and effectively passivates accepters. In n-type SiC, the incorporation of H is suppressed and no passivation is detected. (C) 1998 American Institute of Physics.
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2.
  • Badel, Xavier, et al. (författare)
  • Formation of pn junctions in deep silicon pores for X-ray imaging detector applications
  • 2003
  • Ingår i: Nuclear Instruments and Methods in Physics Research Section A. - 0168-9002 .- 1872-9576. ; 509:1-3, s. 96-101
  • Tidskriftsartikel (refereegranskat)abstract
    • The formation of pn junctions in deep silicon pores has been studied for a new concept of X-ray imaging detectors. The sensitive part of the device is an array of CsI(Tl) columns formed by filling a silicon matrix of pores having pn junctions in their walls. Under X-ray illumination, the CsI(TI) scintillator emits photons that are collected by the pn junctions. Relatively high signal collection efficiency is expected. However, the formation of pn junctions inside pore walls represents a challenging step in the detector fabrication. In this work pore matrices were fabricated in n-type silicon by deep reactive ion etching and by photo-electrochemical etching. The pn junctions were formed either by boron diffusion or deposition of boron doped poly-silicon. Various techniques were used to analyze the transverse depth profiles of boron atoms at different pore depths. The study shows successful results for pn-junctions formed both by diffusion and by poly-silicon deposition.
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3.
  • Hallen, A, et al. (författare)
  • Implanted p(+)n-junctions in silicon carbide
  • 2003
  • Ingår i: APPLICATION OF ACCELERATORS IN RESEARCH AND INDUSTRY. ; , s. 653-657
  • Konferensbidrag (refereegranskat)abstract
    • Ion implantation is considered a key technology for the realisation of silicon carbide electronic devices. Here we will give an overview of the field and present some recent results of ion implanted 4H SiC epitaxial layers. Mainly Al ions of keV energies have been used at different fluence, flux and target temperature. The samples have been investigated by secondary ion mass spectrometry (SIMS), channeling Rutherford backscattering (RBS-c) and transmission electron microscopy (TEM), both as-implanted and after annealing up to 1900 degreesC. Also the electrical activation of Al-implanted and annealed material has been investigated by scanning spreading resistance microscopy (SSRM). The damage accumulation, monitored by RBS-c, is linear with ion fluence but depends strongly on implantation temperature and ion flux. Annealing at temperatures above 1700 degreesC is needed to remove the damage and to electrically activate implanted Al ions. At these high annealing temperatures, however, dislocation loops are formed that have a negative influence on device performance.
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4.
  • Hallén, Anders., et al. (författare)
  • Ion implantation of silicon carbide
  • 2002
  • Ingår i: Nuclear Instruments and Methods in Physics Research Section B. - 0168-583X .- 1872-9584. ; 186, s. 186-194
  • Tidskriftsartikel (refereegranskat)abstract
    • Ion implantation is an important technique for a successful implementation of commercial SiC devices. Much effort has also been devoted to optimising implantation and annealing parameters to improve the electrical device characteristics. However, there is a severe lack of understanding of the fundamental implantation process and the generation and annealing kinetics of point defects and defect complexes. Only very few of the most elementary intrinsic point defects have been unambiguously identified so far. To reach a deeper understanding of the basic mechanisms SiC samples have been implanted with a broad range of ions, energies, doses, etc., and the resulting defects and damage produced in the lattice have been studied with a multitude of characterisation techniques. In this contribution we will review some of the results generated recently and also try to indicate where more research is needed. In particular, deep level transient spectroscopy (DLTS) has been used to investigate point defects at very low doses and transmission electron microscopy (TEM) and Rutherford backscattering spectrometry (RBS) are used for studying the damage build-up at high doses.
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5.
  • Henry, Anne, et al. (författare)
  • Boron-related luminescence in SiC
  • 2003
  • Ingår i: Physica B: Condensed Matter. - : Elsevier BV. - 0921-4526.
  • Konferensbidrag (refereegranskat)abstract
    • We report a photoluminescence (PL) study for both 4H and 6H-SiC epilayers on boron-related recombination. The PL is not observed from as-grown epilayers, but after secondary ion mass spectrometry. In 4H the no-phonon (NP) line spectrum is near 3838Å, whereas it is located close to 4182 Å in the 6H. The two spectra have almost the same phonon structure with localized modes. The luminescence is predominantly polarized perpendicular to the c-axis. The temperature dependence shows that the NP lines have at least three excited states higher in energy with energy separation depending on the polytype. The luminescence is quenched at T > 70K with a thermalization energy of about 40meV. The absence of splitting or shift of the lines originating from excited states under applied magnetic field shows that the excited states have singlet character, whereas splitting is observed for the low-temperature NP lines. The luminescence of the NP lines in these samples is shown to increase with excitation time. © 2003 Elsevier B.V. All rights reserved.
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6.
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7.
  • Henry, Anne, et al. (författare)
  • The 3838 Å photoluminescence line in 4H-SiC
  • 2003
  • Ingår i: Journal of Applied Physics. - : AIP Publishing. - 0021-8979 .- 1089-7550. ; 94:5, s. 2901-2906
  • Tidskriftsartikel (refereegranskat)abstract
    • The results of a study of the origins of the peak near 3838 Å observed in the photoluminescence (PL) spectrum of 4H-SiC was reported. A band was observed for 6H material, displaced in energy position by the band-gap difference between the two polytypes. The recombination leading to the PL line was associated with an isoelectronic complex defect.
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8.
  • Intarasiri, S., et al. (författare)
  • RBS and ERDA determinations of depth distributions of high-dose carbon ions implanted in silicon for silicon-carbide synthesis study
  • 2006
  • Ingår i: Nuclear Instruments and Methods in Physics Research Section B. - : Elsevier BV. - 0168-583X .- 1872-9584. ; 249, s. 859-864
  • Tidskriftsartikel (refereegranskat)abstract
    • For ion beam synthesis of silicon carbide (SiC), a knowledge of the depth distribution of implanted carbon ions in silicon is crucial for successful development. Based on its simplicity and availability, we selected Rutherford backscattering spectrometry (RBS) as an analysis technique for this purpose. A self-developed computer program dedicated to extract depth profiles of lighter impurities in heavier matrix is established. For control, calculated results are compared with an other ion beam analysis (IBA) technique superior for studying lighter impurity in heavier substrate i.e. elastic recoil detection analysis (ERDA). The RBS was performed with a 1.7-MV Tandetron accelerator using He2+ as the probe ions. The ERDA was performed with a 5-MV Pelletron accelerator using I8+ as the probe ions. This work shows that the RBS-extracted data had no significant deviations from those of ERDA and simulations by SRIM2003 and SIMPL computer codes. We also found that annealing at temperatures as high as 1000 degrees C had quite limited effect on the redistribution of carbon in silicon.
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9.
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10.
  • Janson, M S, et al. (författare)
  • Channeled implants in 6H silicon carbide
  • 2000
  • Ingår i: SILICON CARBIDE AND RELATED MATERIALS - 1999 PTS, 1 & 2. ; , s. 889-892
  • Konferensbidrag (refereegranskat)abstract
    • Implants of MeV B-11, Al-27 and Ga-69 into the <0001> channel of 6H-SiC have been performed and concentration versus depth profiles have been obtained utilizing secondary ion mass spectrometry (SIMS). The experiment shows that the deepest channeled Ga ions reach a depth of 6.6 mum, which is 4 times deeper than the projected range of a random angle implantation, while the deepest channeled B ions only exceed the random projected range by 40%. Measurements at several implantation fluences show that implantation induced damage quench the deep channeling at fluences around 2 and 10x10(13) cm(-2) for Al and Ga, respectively, while only a minor fluence dependence is found in the B implants at fluences up to 2.6x10(14) cm(-2). The ion mass dependence of these effects is explained by the electronic to nuclear stopping ratios. Monte Carlo simulations of the channeling implants have also been performed and good agreements are found between simulations and experimental data.
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  • Resultat 1-10 av 29

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