Materials Map

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The Materials Map is an open tool for improving networking and interdisciplinary exchange within materials research. It enables cross-database search for cooperation and network partners and discovering of the research landscape.

The dashboard provides detailed information about the selected scientist, e.g. publications. The dashboard can be filtered and shows the relationship to co-authors in different diagrams. In addition, a link is provided to find contact information.

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The Materials Map is still under development. In its current state, it is only based on one single data source and, thus, incomplete and contains duplicates. We are working on incorporating new open data sources like ORCID to improve the quality and the timeliness of our data. We will update Materials Map as soon as possible and kindly ask for your patience.

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in Cooperation with on an Cooperation-Score of 37%

Topics

Publications (7/7 displayed)

  • 2011Double-pass erbium-doped zirconia fiber amplifier for wide-band and flat-gain operations14citations
  • 2010Performance comparison of Zr-based and Bi-based erbium-doped fiber amplifiers40citations
  • 2010Wideband EDFA based in erbium doped crystalline zirconia yttria alumino silicate fiber46citations
  • 2010Yb2O3-doped YAG nano-crystallites in silica-based core glass matrix of optical fiber preform22citations
  • 2010Ytterbium-doped Y2O3 nanoparticle silica optical fibers for high power fiber lasers with suppressed photodarkening39citations
  • 2009All Fibre based Hydrogen Sensing using Palladium coated Long Period Gratingscitations
  • 2009Ytterbium doped nanostructured optical fibers for high power fiber laserscitations

Places of action

Chart of shared publication
Hamzah, A.
3 / 3 shared
Huri, N. A. D.
3 / 3 shared
Ahmad, H.
3 / 14 shared
Boyland, A. J.
6 / 12 shared
Yoo, S.
6 / 25 shared
Paul, M. C.
6 / 8 shared
Das, S.
6 / 43 shared
Harun, S. W.
3 / 3 shared
Kalita, M. P.
6 / 10 shared
Pal, M.
6 / 10 shared
Sahu, Jayanta Kumar
6 / 64 shared
Bysakh, S.
1 / 2 shared
Webb, A. S.
2 / 8 shared
Standish, R. J.
2 / 6 shared
Miller, James
1 / 2 shared
Maier, Rrj
1 / 24 shared
Carter, Richard
1 / 16 shared
Allsop, Tom
1 / 1 shared
Jones, Benjamin
1 / 5 shared
Barton, James
1 / 7 shared
Mcculloch, Scott
1 / 4 shared
Codemard, C.
1 / 5 shared
Sen, R.
1 / 7 shared
Dhar, A.
1 / 8 shared
Nilsson, Johan
1 / 26 shared
Chart of publication period
2011
2010
2009

Co-Authors (by relevance)

  • Hamzah, A.
  • Huri, N. A. D.
  • Ahmad, H.
  • Boyland, A. J.
  • Yoo, S.
  • Paul, M. C.
  • Das, S.
  • Harun, S. W.
  • Kalita, M. P.
  • Pal, M.
  • Sahu, Jayanta Kumar
  • Bysakh, S.
  • Webb, A. S.
  • Standish, R. J.
  • Miller, James
  • Maier, Rrj
  • Carter, Richard
  • Allsop, Tom
  • Jones, Benjamin
  • Barton, James
  • Mcculloch, Scott
  • Codemard, C.
  • Sen, R.
  • Dhar, A.
  • Nilsson, Johan
OrganizationsLocationPeople

article

Double-pass erbium-doped zirconia fiber amplifier for wide-band and flat-gain operations

  • Hamzah, A.
  • Huri, N. A. D.
  • Ahmad, H.
  • Boyland, A. J.
  • Yoo, S.
  • Paul, M. C.
  • Das, S.
  • Harun, S. W.
  • Kalita, M. P.
  • Pal, M.
  • Sahu, Jayanta Kumar
  • Bhadra, S. K.
Abstract

The double-pass erbium-doped zirconia fiber amplifier (EDZFA) is proposed and demonstrated to provide a wide-band amplification as well as flat-gain operation in both the C- and L-band regions using only a single-gain medium.The proposed amplifier utilizes an erbium-doped zirconia fiber (EDZF) with erbium ion concentration of 2800 ppm as a gain medium. The medium is fabricated in a ternary glass host, zirconia-yttria-aluminium codoped silica fiber through solution doping technique along with modified chemical vapor deposition (MCVD). Compared to a single-pass operation, the double-pass EDZFA shows a better gain performance. At input signal power of 0 dBm and the optimum EDZF length of 2m, a flat gain of around 16dB is achieved by the proposed double-pass amplifier with gain variation of approximately 2.5dB throughout the wavelength range from 1530 to 1590nm. However, the noise figure of the double-pass amplifier is slightly higher than that of the single-pass due to inefficient population inversion at the input part of the amplifier.

Topics
  • impedance spectroscopy
  • aluminium
  • glass
  • glass
  • positron annihilation lifetime spectroscopy
  • Photoacoustic spectroscopy
  • chemical vapor deposition
  • Erbium