dc.contributor.author | Nazir, N.S. | |
dc.contributor.author | Wahid, M.H.A. | |
dc.contributor.author | Hambali, N.A.M.A. | |
dc.contributor.author | Shahimin, M.M. | |
dc.contributor.author | Khairuddin, N.Z. | |
dc.contributor.author | Hasanuddin, N.H. | |
dc.contributor.author | Ramli, M. M. | |
dc.date.accessioned | 2020-11-05T01:31:56Z | |
dc.date.available | 2020-11-05T01:31:56Z | |
dc.date.issued | 2016 | |
dc.identifier.citation | MATEC Web of Conferences, vol.78, 2016, 10 pages | en_US |
dc.identifier.issn | 2261-236X (online) | |
dc.identifier.uri | http://dspace.unimap.edu.my:80/xmlui/handle/123456789/68617 | |
dc.description | Link to publisher's homepage at https://www.matec-conferences.org/ | en_US |
dc.description.abstract | Two-photon absorption with high intensity pump beam occurs in a SOA depends on fast phase change of a weak probe signal. This work analysed optical XOR logic function using two-photon absorption induced fast phase change. A rate equation for SOA and both input data signals A and B with high intensity, configured in the form of MZI has also been proved. The model shows that XOR operation at 10 Gb/s with good signal to noise ratio is obtained with high input intensities. The result on the generation of XOR indicates that operations on 10 Gb/s with a high signal to noise ratio can easily be implemented. The average input power into the SOA is 20 dbm corresponding to the peak power of 5.5 dBm at 10 Gb/s when the width of the input pulse 3.6 ps. The short narrow pulse width is utilised in the study for stronger effect of two-photon absorption. | en_US |
dc.language.iso | en | en_US |
dc.publisher | EDP Sciences | en_US |
dc.subject | XOR Logic Gate | en_US |
dc.subject | XOR logic | en_US |
dc.subject | Two-photon absorption | en_US |
dc.title | Design and Analysis of XOR Logic Gate Based on Two-Photon Absorption | en_US |
dc.type | Article | en_US |
dc.identifier.doi | https://doi.org/10.1051/matecconf/20167801108 | |
dc.contributor.url | najwasarihah@gmail.com | en_US |