Amr M. Mahmoud

Dr. Amr M. Mahmoud

orcid

Research Focus & Metrics

Academic Career Length

18Years (2009-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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6 November 2018 in ACS Sensors
Verified
Journal Article
Closed access
MMMaral P. S. Mousavi
Maral P. S. Mousavi
MEMohamed K. Abd El-Rahman
Mohamed K. Abd El-Rahman
AMAmr M. Mahmoud
Amr M. Mahmoud
RARania M. Abdelsalam
Rania M. Abdelsalam
PBPhilippe Buhlmann
Philippe Buhlmann

1 March 2015 in Sensors and Actuators B: Chemical
Verified
Journal Article
Closed access
MEMohamed K. Abd El-Rahman
Mohamed K. Abd El-Rahman
MRMamdouh R. Rezk
Mamdouh R. Rezk
AMAmr M. Mahmoud
Amr M. Mahmoud
mohamed elghobashymohamed elghobashy
mohamed elghobashy

1 February 2009 in Applied Spectroscopy
Verified
Journal Article
Closed access
LSLian C. T. Shoute
Lian C. T. Shoute
ABAdam Johan Bergren
Adam Johan Bergren
AMAmr M. Mahmoud
Amr M. Mahmoud
KHKen D. Harris
Ken D. Harris
RMRichard L. McCreery
Richard L. McCreery
This paper presents results showing that the design of substrates used for surface-enhanced Raman spectroscopy (SERS) can impact the apparent enhancement factors (EFs) obtained due to optical interference effects that are distinct from SERS, providing additional enhancement of the Raman intensity. Thus, a combination of SERS and a substrate designed to maximize interference-based enhancement is demonstrated to give additional Raman intensity above that observed for SERS alone. The system explored is 4-nitroazobenzene (NAB) and biphenyl (BP) chemisorbed on a nanostructured silver film obtained by vacuum deposition of Ag on thermally oxidized silicon wafers. The enhancing silver layer is partially transparent, enabling a standing wave to form as a result of the combination of the incident light and light reflected from the underlying Si substrate (i.e., light that passes through the Ag and the intervening dielectric layer of SiOx). The Raman intensity is measured as a function of the thickness of the thermal oxide layer in the range from ∼150 to ∼400 nm, and despite a lack of morphological variation in the silver films, there is a strong dependence of the Raman intensity on the oxide thickness. The Raman signal for the optimal SiOx interlayer thickness is 38 times higher than the intensity obtained when the Ag particles are deposited directly onto Si (with native oxide). To account for the trends observed in the Raman intensity versus thickness data, calculations of the relative mean square electric field (MSEF) at the surface of the SiOx are carried out. These calculations are also used to further optimize the experimental setup.

8 June 2022 in Journal of Electroanalytical Chemistry
Verified
Journal Article
Closed access
NANoha F. El Azab
Noha F. El Azab
AMAmr M. Mahmoud
Amr M. Mahmoud
YTYossra A. Trabik
Yossra A. Trabik

29 November 2022 in Talanta
Verified
Journal Article
Closed access
SSShymaa S Soliman
Shymaa S Soliman
AMAmr M. Mahmoud
Amr M. Mahmoud
mohamed elghobashymohamed elghobashy
mohamed elghobashy
HZHala E. Zaazaa
Hala E. Zaazaa
GSGhada A. Sedik
Ghada A. Sedik

7 August 2020 in Microchimica Acta
Verified
Journal Article
Closed access
PDF file
SHSaid A. Hassan
Said A. Hassan
NINourhan Badr Ibrahim
Nourhan Badr Ibrahim
HZHala E. Zaazaa
Hala E. Zaazaa
AMAzza A. Moustafa
Azza A. Moustafa
AMAmr M. Mahmoud
Amr M. Mahmoud