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  • 1
    Online Resource
    Online Resource
    Springer Science and Business Media LLC ; 2011
    In:  MRS Proceedings Vol. 1322 ( 2011)
    In: MRS Proceedings, Springer Science and Business Media LLC, Vol. 1322 ( 2011)
    Abstract: Silicon nanowire solar cells were simulated using the Silvaco TCAD software kit. For optimization of speed the simulations were performed in cylinder coordinates with cylindrical symmetry. Symmetric doping was assumed with a dopant density of 10 18 cm -3 in the p-type core and inside the n-type shell. In the implementation a cathode contact was wrapped around the semiconductor nanorod and an anode was assumed at the bottom of the rod. Optimization of cell efficiency was performed with regard to the rod radius and the rod length. In both optimization processes clear maxima in efficiency were visible, resulting in an optimal radius of 66 nm with the pn junction at 43.5 nm and an optimal rod length of about 48 μm. The maximum of efficiency with respect to the rod radius is due to a decrease of short-circuit current density (J sc ) and an increase of open-circuit voltage (U oc ) with radius, while the maximum with respect to the rod length is explained by the combination of an increase of J sc and a decrease of U oc . Fill factors stay rather constant at values between 0.6 and 0.8. Further, the influence of a back surface field (BSF) layer was surveyed in simulations. Positioning the BSF next to the cathode contact considerably improved cell efficiency. In addition, simulations with a cathode contact on top of the nanowire structure were undertaken. No severe deterioration of cell performance with increasing radius was observed so far in this configuration. Hence, nanorods with much larger radii can be used for solar cells using this contact scheme. In comparison to simulations with wrapped cathode contacts, J sc and U oc and therefore efficiency is considerably improved.
    Type of Medium: Online Resource
    ISSN: 0272-9172 , 1946-4274
    Language: English
    Publisher: Springer Science and Business Media LLC
    Publication Date: 2011
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  • 2
    Online Resource
    Online Resource
    American Physical Society (APS) ; 2010
    In:  Physical Review B Vol. 82, No. 12 ( 2010-9-27)
    In: Physical Review B, American Physical Society (APS), Vol. 82, No. 12 ( 2010-9-27)
    Type of Medium: Online Resource
    ISSN: 1098-0121 , 1550-235X
    RVK:
    Language: English
    Publisher: American Physical Society (APS)
    Publication Date: 2010
    detail.hit.zdb_id: 1473011-X
    detail.hit.zdb_id: 2844160-6
    detail.hit.zdb_id: 209770-9
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  • 3
    Online Resource
    Online Resource
    Elsevier BV ; 2012
    In:  Materials Science and Engineering: B Vol. 177, No. 17 ( 2012-10), p. 1558-1562
    In: Materials Science and Engineering: B, Elsevier BV, Vol. 177, No. 17 ( 2012-10), p. 1558-1562
    Type of Medium: Online Resource
    ISSN: 0921-5107
    RVK:
    Language: English
    Publisher: Elsevier BV
    Publication Date: 2012
    detail.hit.zdb_id: 1492109-1
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  • 4
    In: physica status solidi (a), Wiley, Vol. 208, No. 4 ( 2011-04), p. 893-899
    Abstract: Samples containing silicon nanowires (Si‐NWs) and highly porous structures (P‐Si) were prepared by electroless wet chemical etching (EWCE) of crystalline silicon wafers using various etching parameters. Photoluminescence (PL) measurements were performed with excitation at 488 nm and a photon energy flux of 337 mW cm −2 . According to the diameters of the Si‐NWs ( 〉 10 nm), from quantum confinement (QC) theory no shift in PL peak energy compared to the bandgap of crystalline silicon is expected. However, PL measurements show peak emission energies ranging between 1.4 and 1.6 eV. After further treatment of the samples with HF, substantial PL emission was still detectable with the measured PL peak pinned at 1.4 eV irrespective of etching time. We explain the observations by the hypothesis that the persistent part of PL emission is generated by nanocrystals located at the rough sidewalls of the Si‐NWs or residing within the porous sample structure. The part of the PL, which was present before HF treatment, but vanished after the treatment, is attributed to the presence of silicon suboxide surrounding the Si‐NWs or covering other Si surfaces. This hypothesis is explored by means of three sample series, prepared with different preparation parameters. In the first series the time used during the initial metallization step in order to prepare an Ag nanoparticle layer on the top surface was varied, in the second series the etching time was the changed parameter and in the third series the HF to H 2 O 2 concentration ratio was varied. magnified image Strong visible orange colored PL of a sample produced by EWCE starting from a heavily doped wafer (n‐type c‐Si (111), As as dopant) and excited at 337 nm (the sample was mounted on a glass substrate. Blue luminescence is due to the substrate).
    Type of Medium: Online Resource
    ISSN: 1862-6300 , 1862-6319
    URL: Issue
    Language: English
    Publisher: Wiley
    Publication Date: 2011
    detail.hit.zdb_id: 1481091-8
    detail.hit.zdb_id: 208850-2
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