R. T. Prabu, Dhilipkumar Santhakumar, Ata Kishore Kumar, Sangeetham Dharuman Lalitha, Jeneetha Jebanazer, Salem Balamurugan Mohan, Aisha abd Rahman Ahmed
This paper has clarified verified of leakage loss, birefringence, nonlinear parameters and total number of modes in silica/silica doped and plastic fibers for fiber system efficiency improvement. The signal power loss is demonstrated with silica/silica doped/plastic fibers at various ambient temperatures. The estimated number of fiber modes is clarified in the core against silica/silica doped/plastic fiber core radius. The fiber birefringence is studied against silica/silica doped/plastic fiber core radius. The silica/silica doped/plastic fibers effective refractive index is clarified versus ambient temperature variations. The nonlinear parameter is demonstrated based silica doped fiber against the dopant concentration ratio with different temperature variations. The effective area cross section is studied based silica doped fiber against the dopant concentration ratio with different temperature variations. The predicted fiber loss is demonstrated against the fiber operating wavelength for silica glass fibers/silica doped fibers/plastic fibers. As well as the predicted fiber loss is clarified and studied versus fiber core radius for silica glass/silica doped/plastic fibers.
{"title":"Verified of leakage loss, birefringence, nonlinear parameters and total number of modes in silica/silica doped and plastic fibers for fiber system efficiency improvement","authors":"R. T. Prabu, Dhilipkumar Santhakumar, Ata Kishore Kumar, Sangeetham Dharuman Lalitha, Jeneetha Jebanazer, Salem Balamurugan Mohan, Aisha abd Rahman Ahmed","doi":"10.1515/joc-2024-0058","DOIUrl":"https://doi.org/10.1515/joc-2024-0058","url":null,"abstract":"\u0000 This paper has clarified verified of leakage loss, birefringence, nonlinear parameters and total number of modes in silica/silica doped and plastic fibers for fiber system efficiency improvement. The signal power loss is demonstrated with silica/silica doped/plastic fibers at various ambient temperatures. The estimated number of fiber modes is clarified in the core against silica/silica doped/plastic fiber core radius. The fiber birefringence is studied against silica/silica doped/plastic fiber core radius. The silica/silica doped/plastic fibers effective refractive index is clarified versus ambient temperature variations. The nonlinear parameter is demonstrated based silica doped fiber against the dopant concentration ratio with different temperature variations. The effective area cross section is studied based silica doped fiber against the dopant concentration ratio with different temperature variations. The predicted fiber loss is demonstrated against the fiber operating wavelength for silica glass fibers/silica doped fibers/plastic fibers. As well as the predicted fiber loss is clarified and studied versus fiber core radius for silica glass/silica doped/plastic fibers.","PeriodicalId":509395,"journal":{"name":"Journal of Optical Communications","volume":null,"pages":null},"PeriodicalIF":0.0,"publicationDate":"2024-05-09","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140997745","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
R. T. Prabu, Shibu Soman, Vasumathi Gunasekaran, Ramkumar Velayudam, Jeneetha Jebanazer, Benisha Maria Xavier, Ayman Zain Hemadan
This paper has demonstrated the hybrid pumped laser sources based hybrid traveling wave SOA and optical EDFA amplifies for the signal quality improvement. The previous effective noise figure and fiber loss variations are clarified against wavelength band with/without amplification. The related previous signal output power versus Raman/EDFA pumped amplification and signal power conversion efficiency are indicated versus the launched pump power with the Raman/EDFA pumped amplification. The signal quality factor/BER against the transmission distance with/without amplification after receiver side. The modified amplified light signal power is demonstrated after 300 km distance SMF channel with wavelength band variations. The modified amplified light signal power is clarified after 300 km distance SMF channel by using optical power meter. The modified amplified light signal power is clarified after 300 km distance SMF channel with time band variations. The modified amplified electrical signal power is demonstrated after 350 km distance SMF channel with frequency band variations. The modified amplified electrical signal power is clarified after 350 km distance SMF channel with time band variations. The modified amplified electrical signal power is demonstrated after 350 km distance SMF channel by using electrical power meter.
{"title":"Hybrid pumped laser sources based hybrid traveling wave SOA and optical EDFA amplifies for signal quality improvement","authors":"R. T. Prabu, Shibu Soman, Vasumathi Gunasekaran, Ramkumar Velayudam, Jeneetha Jebanazer, Benisha Maria Xavier, Ayman Zain Hemadan","doi":"10.1515/joc-2024-0055","DOIUrl":"https://doi.org/10.1515/joc-2024-0055","url":null,"abstract":"\u0000 This paper has demonstrated the hybrid pumped laser sources based hybrid traveling wave SOA and optical EDFA amplifies for the signal quality improvement. The previous effective noise figure and fiber loss variations are clarified against wavelength band with/without amplification. The related previous signal output power versus Raman/EDFA pumped amplification and signal power conversion efficiency are indicated versus the launched pump power with the Raman/EDFA pumped amplification. The signal quality factor/BER against the transmission distance with/without amplification after receiver side. The modified amplified light signal power is demonstrated after 300 km distance SMF channel with wavelength band variations. The modified amplified light signal power is clarified after 300 km distance SMF channel by using optical power meter. The modified amplified light signal power is clarified after 300 km distance SMF channel with time band variations. The modified amplified electrical signal power is demonstrated after 350 km distance SMF channel with frequency band variations. The modified amplified electrical signal power is clarified after 350 km distance SMF channel with time band variations. The modified amplified electrical signal power is demonstrated after 350 km distance SMF channel by using electrical power meter.","PeriodicalId":509395,"journal":{"name":"Journal of Optical Communications","volume":null,"pages":null},"PeriodicalIF":0.0,"publicationDate":"2024-05-09","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140995817","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
To enhance the transmission capacity for energy consumption and low cost system, mode division multiplexing (MDM) using mode 0 and mode 1 is proposed and investigated. A pair of eight downlink and uplink wavelengths is transmitted by using each MDM mode in an integrated bidirectional next generation passive optical network and free space optics (NGPON–FSO) system at 10 Gbps per channel transmission rate under the impact of FSO–fiber links impairments. Simulation results indicate that received power of −21.2 dBm with 0.2 dB power penalty can be obtained over 1 km FSO and 100 m multimode fiber under unfavourable turbulent effects. The system provides extended FSO link range, and fiber range of 150 km and 600 m respectively at threshold limit of 10−3. Besides, the mathematical analysis depicts the receiver sensitivity and splitter power budget of 42 dBm and 18 dB, respectively, for the proposed system. The system offers finest performance than other pre-existing systems.
{"title":"Investigation of 16 × 10 Gbps mode division multiplexed enabled integrated NGPON–FSO architecture under wired-wireless link losses","authors":"Meet Kumari","doi":"10.1515/joc-2024-0036","DOIUrl":"https://doi.org/10.1515/joc-2024-0036","url":null,"abstract":"\u0000 To enhance the transmission capacity for energy consumption and low cost system, mode division multiplexing (MDM) using mode 0 and mode 1 is proposed and investigated. A pair of eight downlink and uplink wavelengths is transmitted by using each MDM mode in an integrated bidirectional next generation passive optical network and free space optics (NGPON–FSO) system at 10 Gbps per channel transmission rate under the impact of FSO–fiber links impairments. Simulation results indicate that received power of −21.2 dBm with 0.2 dB power penalty can be obtained over 1 km FSO and 100 m multimode fiber under unfavourable turbulent effects. The system provides extended FSO link range, and fiber range of 150 km and 600 m respectively at threshold limit of 10−3. Besides, the mathematical analysis depicts the receiver sensitivity and splitter power budget of 42 dBm and 18 dB, respectively, for the proposed system. The system offers finest performance than other pre-existing systems.","PeriodicalId":509395,"journal":{"name":"Journal of Optical Communications","volume":null,"pages":null},"PeriodicalIF":0.0,"publicationDate":"2024-03-29","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140365106","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
R. T. Prabu, Vanitha Lingaraj, Jegadish Kumar KailairaJan Jeyaprakash, Jeneetha Jebanazer, Nishanthi Govindaswamy, Sathish Kumar Natarajan, Orabi Salem Orabi
This paper has clarified the light emitting diode and laser diode system behaviour description and their external quantum efficiency measurements. Light output of LED spontaneous emission and laser diode stimulated emission are clarified. Stimulated and amplified spontaneous emission of laser diode and LED system configuration are demonstrated. The management of hybrid light sources spectrum illumination interaction for efficient solar cells light intensity and short circuit current density enhancement. The laser diode has presented better performance in the light output power especially under the same temperature effects. It is ensured that the dramatic effects of the temperature on both laser diode performance efficiency.
{"title":"Light emitting diode and laser diode system behaviour description and their performance signature measurements","authors":"R. T. Prabu, Vanitha Lingaraj, Jegadish Kumar KailairaJan Jeyaprakash, Jeneetha Jebanazer, Nishanthi Govindaswamy, Sathish Kumar Natarajan, Orabi Salem Orabi","doi":"10.1515/joc-2024-0043","DOIUrl":"https://doi.org/10.1515/joc-2024-0043","url":null,"abstract":"\u0000 This paper has clarified the light emitting diode and laser diode system behaviour description and their external quantum efficiency measurements. Light output of LED spontaneous emission and laser diode stimulated emission are clarified. Stimulated and amplified spontaneous emission of laser diode and LED system configuration are demonstrated. The management of hybrid light sources spectrum illumination interaction for efficient solar cells light intensity and short circuit current density enhancement. The laser diode has presented better performance in the light output power especially under the same temperature effects. It is ensured that the dramatic effects of the temperature on both laser diode performance efficiency.","PeriodicalId":509395,"journal":{"name":"Journal of Optical Communications","volume":null,"pages":null},"PeriodicalIF":0.0,"publicationDate":"2024-03-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140376520","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
R. T. Prabu, Arunsundar Balasubramanian, Nithyasundari Balakrishnan, Jeneetha Jebanazer, Mohana Sundaram Kandasamy, Nishanthi Govindaswamy, Rashida Maher Mahmoud
This paper has demonstrated the high efficient net gain and low noise figure based vertical cavity semiconductor light amplifiers for wavelength division multiplexing applications. Previous study on the chip reflective gain variations versus SOA current under temperature effects is clarified. We have transferred light semiconductor amplifiers for wavelength multiplexing schemes applications. Amplifier output power is demonstrated with bias current and amplifier active layer region length variations based input signal power of 3, 6.5, 10 dBm, 1550 nm wavelength and optimum amplifier confinement factor of 0.45. The amplifier output noise variations are clarified against the bias current and amplifier active layer region width variations based input signal power of 3, 6.5, 10 dBm, 1550 nm wavelength and optimum amplifier confinement factor of 0.45. The output OSNR variations are studied clearly and deeply against the bias current and amplifier active layer region length variations based input signal power of 3, 6.5, 10 dBm, 1550 nm wavelength and optimum amplifier confinement factor of 0.45. The signal loss is demonstrated versus both active layer width/length and temperature based optimum 30 % gallium core dopant ratio and 28 % arsenide cladding dopant ratio at optimum input signal power of 10 dBm, 1550 nm wavelength and optimum amplifier confinement factor of 0.45. SOA amplifier output power can be enhance with the management of both bias current and input signal power and the reduction of active amplifier length. The amplifier output noise can be enhance with the management of both bias current and input signal power and the reduction of active amplifier width. Output OSNR system can be improved with the management of both bias current and input signal power and the reduction of active amplifier length. The SOA amplifier gain can be improved with the management of both bias current and input signal power and the reduction of active amplifier length. The SOA amplifier noise figure can be improved with the management of both bias current and input signal power and the reduction of active amplifier width. The signal loss can be controlled and managed by adjusting optimum 30 % gallium core dopant ratio and 28 % arsenide cladding dopant ratio, optimum active layer/with and the presence of room temperature.
{"title":"High efficient net gain and low noise figure based vertical cavity semiconductor optical amplifiers for wavelength division multiplexing applications","authors":"R. T. Prabu, Arunsundar Balasubramanian, Nithyasundari Balakrishnan, Jeneetha Jebanazer, Mohana Sundaram Kandasamy, Nishanthi Govindaswamy, Rashida Maher Mahmoud","doi":"10.1515/joc-2024-0048","DOIUrl":"https://doi.org/10.1515/joc-2024-0048","url":null,"abstract":"\u0000 This paper has demonstrated the high efficient net gain and low noise figure based vertical cavity semiconductor light amplifiers for wavelength division multiplexing applications. Previous study on the chip reflective gain variations versus SOA current under temperature effects is clarified. We have transferred light semiconductor amplifiers for wavelength multiplexing schemes applications. Amplifier output power is demonstrated with bias current and amplifier active layer region length variations based input signal power of 3, 6.5, 10 dBm, 1550 nm wavelength and optimum amplifier confinement factor of 0.45. The amplifier output noise variations are clarified against the bias current and amplifier active layer region width variations based input signal power of 3, 6.5, 10 dBm, 1550 nm wavelength and optimum amplifier confinement factor of 0.45. The output OSNR variations are studied clearly and deeply against the bias current and amplifier active layer region length variations based input signal power of 3, 6.5, 10 dBm, 1550 nm wavelength and optimum amplifier confinement factor of 0.45. The signal loss is demonstrated versus both active layer width/length and temperature based optimum 30 % gallium core dopant ratio and 28 % arsenide cladding dopant ratio at optimum input signal power of 10 dBm, 1550 nm wavelength and optimum amplifier confinement factor of 0.45. SOA amplifier output power can be enhance with the management of both bias current and input signal power and the reduction of active amplifier length. The amplifier output noise can be enhance with the management of both bias current and input signal power and the reduction of active amplifier width. Output OSNR system can be improved with the management of both bias current and input signal power and the reduction of active amplifier length. The SOA amplifier gain can be improved with the management of both bias current and input signal power and the reduction of active amplifier length. The SOA amplifier noise figure can be improved with the management of both bias current and input signal power and the reduction of active amplifier width. The signal loss can be controlled and managed by adjusting optimum 30 % gallium core dopant ratio and 28 % arsenide cladding dopant ratio, optimum active layer/with and the presence of room temperature.","PeriodicalId":509395,"journal":{"name":"Journal of Optical Communications","volume":null,"pages":null},"PeriodicalIF":0.0,"publicationDate":"2024-03-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140377604","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
R. T. Prabu, Suvitha Sundar, Merlin Livingston Louis Mary, Arunya Revathi Arumugam, P. Devi, Thankamony Devakhi Subha, Karem Tarek Anwer
This work clarified various multimode fiber configurations with spatial continuous wave lasers based different coding configurations for high speed fiber systems. The optimum lighted power form after linear index multimode fibers versus spectral wavelength is clarified. The optimum lighted form power after parabolic index multimode fibers versus spectral wavelength is demonstrated. The max lighted form power after measured index multimode fibers versus spectral wavelength is illustrated. Optimum lighted form signal power variations after linear index multimode fibers versus time are demonstrated. The max optimum form signal band form power after parabolic index multimode fibers versus time is indicated. The max optimum lighted signal power after measured index multimode fibers versus time is clarified. Total lighted signal power form after linear index multimode fibers is demonstrated. The total lighted signal power form after parabolic index multimode fibers is clarified. Total lighted power signal form after measured index multimode fibers is clarified. Max optimum signal electrical power form amplitude after PIN photodetector based various index multimode fibers is simulated and studied. Total lighted base form power against MMF length for different proposed optical multimode fibers is studied. Signal base band per noise form ratio against MMF length for different base proposed band optical multimode fibers is demonstrated. Total signal form electrical band power against MMF length for different proposed optical multimode fibers is observed. Max Q base band factor form against MMF length for different base band proposed lighted multimode fibers is clarified.
{"title":"High speed broadband light spatial laser system with hybrid linear/parabolic/measured indexed multimode optical fibers performance signature","authors":"R. T. Prabu, Suvitha Sundar, Merlin Livingston Louis Mary, Arunya Revathi Arumugam, P. Devi, Thankamony Devakhi Subha, Karem Tarek Anwer","doi":"10.1515/joc-2023-0396","DOIUrl":"https://doi.org/10.1515/joc-2023-0396","url":null,"abstract":"\u0000 This work clarified various multimode fiber configurations with spatial continuous wave lasers based different coding configurations for high speed fiber systems. The optimum lighted power form after linear index multimode fibers versus spectral wavelength is clarified. The optimum lighted form power after parabolic index multimode fibers versus spectral wavelength is demonstrated. The max lighted form power after measured index multimode fibers versus spectral wavelength is illustrated. Optimum lighted form signal power variations after linear index multimode fibers versus time are demonstrated. The max optimum form signal band form power after parabolic index multimode fibers versus time is indicated. The max optimum lighted signal power after measured index multimode fibers versus time is clarified. Total lighted signal power form after linear index multimode fibers is demonstrated. The total lighted signal power form after parabolic index multimode fibers is clarified. Total lighted power signal form after measured index multimode fibers is clarified. Max optimum signal electrical power form amplitude after PIN photodetector based various index multimode fibers is simulated and studied. Total lighted base form power against MMF length for different proposed optical multimode fibers is studied. Signal base band per noise form ratio against MMF length for different base proposed band optical multimode fibers is demonstrated. Total signal form electrical band power against MMF length for different proposed optical multimode fibers is observed. Max Q base band factor form against MMF length for different base band proposed lighted multimode fibers is clarified.","PeriodicalId":509395,"journal":{"name":"Journal of Optical Communications","volume":null,"pages":null},"PeriodicalIF":0.0,"publicationDate":"2024-02-29","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140412114","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
R. T. Prabu, Balamuralitharan Balakrishnan, H. Praveena, Thulasi Bai Vijayan, Benisha Maria Xavier, Elayaraja Perumal, Wafaa Fahim Hossam Zain
This study clarified the simulation of the high modulation effects on hybrid optical fiber links and OWC channel based on optical DP-QSK transceiver systems. The optimum lighted signal power band with the spectral wavelength after optical wireless communication channel is clarified. Total lighted form band power after optical fiber cable channel is studied. Total lighted form band power form after optical wireless communication channel is shown in numerical values. The total electrical band power form after optical DPSK receiver based optical fiber cable channel is demonstrated. Total base electrical band power form after optical DPSK receiver based optical wireless communication channel is clarified. Base band signal base form per noise base band form ratio is studied and numerical clarified after optical DPSK receiver against propagation length for both OFC and OWC channels. Total lighted base form power versus propagation length based both OFC and OWC channels is demonstrated. Optimum lighted form base power band form with time after optical fiber cable channel is studied. The max lighted form base power band form with time after optical wireless communication channel is simulated. Optimum lighted signal power band with the spectral wavelength after optical fiber cable channel is demonstrated. The total base electrical band form power after optical DPSK receiver is clarified numerically against propagation length for both OFC and OWC channels.
{"title":"High modulation effects on hybrid optical fiber links and OWC Channel based on optical DP-QSK transceiver systems","authors":"R. T. Prabu, Balamuralitharan Balakrishnan, H. Praveena, Thulasi Bai Vijayan, Benisha Maria Xavier, Elayaraja Perumal, Wafaa Fahim Hossam Zain","doi":"10.1515/joc-2024-0015","DOIUrl":"https://doi.org/10.1515/joc-2024-0015","url":null,"abstract":"\u0000 This study clarified the simulation of the high modulation effects on hybrid optical fiber links and OWC channel based on optical DP-QSK transceiver systems. The optimum lighted signal power band with the spectral wavelength after optical wireless communication channel is clarified. Total lighted form band power after optical fiber cable channel is studied. Total lighted form band power form after optical wireless communication channel is shown in numerical values. The total electrical band power form after optical DPSK receiver based optical fiber cable channel is demonstrated. Total base electrical band power form after optical DPSK receiver based optical wireless communication channel is clarified. Base band signal base form per noise base band form ratio is studied and numerical clarified after optical DPSK receiver against propagation length for both OFC and OWC channels. Total lighted base form power versus propagation length based both OFC and OWC channels is demonstrated. Optimum lighted form base power band form with time after optical fiber cable channel is studied. The max lighted form base power band form with time after optical wireless communication channel is simulated. Optimum lighted signal power band with the spectral wavelength after optical fiber cable channel is demonstrated. The total base electrical band form power after optical DPSK receiver is clarified numerically against propagation length for both OFC and OWC channels.","PeriodicalId":509395,"journal":{"name":"Journal of Optical Communications","volume":null,"pages":null},"PeriodicalIF":0.0,"publicationDate":"2024-02-29","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140414792","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Riyaz Saiyyed, Manoj Sindhwani, B. Ambudkar, Shippu Sachdeva, Abhishek Kumar, M. K. Shukla
FSO (free space optical) communication holds emanated position in the role of propitious innovation with exorbitant-speed using the data transmission mechanism without the wire, propounding an accomplishable explication to the surging need for bandwidth in communication networks. This research paper probes into the improvements and obstacles in FSO communication systems, pursuing to anticipate a compendious encapsulation of the state-of-the-art establishment in this discipline. The evaluation incorporates a meticulous inspection of vital constituents such as laser sources, modulators, and receivers, elucidating their contribution to accomplishing coherent data transfer. The scrutinizing also investigates innumerable atmospheric circumstances affecting FSO links, including weather conditions and turbulence, and puts forward ingenious approaches to alleviate their repercussion on communication performance. Furthermore, the paper explores the homogenization of ultra-modern signal processing techniques to amplify the credibility and robustness of FSO systems, corroborating seamless communication even in challenging environments. Moreover, the research inquiries into the neoteric experimental framework and real-world execution of FSO communication, shedding light on heuristic contemplation, and substantiating theoretical unearthing. The conclusion of this research shells out treasures perception of the ongoing attempt to optimize FSO communication for variegated applications, including, inter-satellite communication, high-speed internet access, and last-mile connectivity. As FSO perpetuates progress, this paper suffices as a recent and inclusive resource for researchers, engineers, and policymakers maneuvering the edges of optical communication technologies.
{"title":"Free space optical communication system: a review of practical constraints, applications, and challenges","authors":"Riyaz Saiyyed, Manoj Sindhwani, B. Ambudkar, Shippu Sachdeva, Abhishek Kumar, M. K. Shukla","doi":"10.1515/joc-2024-0011","DOIUrl":"https://doi.org/10.1515/joc-2024-0011","url":null,"abstract":"\u0000 FSO (free space optical) communication holds emanated position in the role of propitious innovation with exorbitant-speed using the data transmission mechanism without the wire, propounding an accomplishable explication to the surging need for bandwidth in communication networks. This research paper probes into the improvements and obstacles in FSO communication systems, pursuing to anticipate a compendious encapsulation of the state-of-the-art establishment in this discipline. The evaluation incorporates a meticulous inspection of vital constituents such as laser sources, modulators, and receivers, elucidating their contribution to accomplishing coherent data transfer. The scrutinizing also investigates innumerable atmospheric circumstances affecting FSO links, including weather conditions and turbulence, and puts forward ingenious approaches to alleviate their repercussion on communication performance. Furthermore, the paper explores the homogenization of ultra-modern signal processing techniques to amplify the credibility and robustness of FSO systems, corroborating seamless communication even in challenging environments. Moreover, the research inquiries into the neoteric experimental framework and real-world execution of FSO communication, shedding light on heuristic contemplation, and substantiating theoretical unearthing. The conclusion of this research shells out treasures perception of the ongoing attempt to optimize FSO communication for variegated applications, including, inter-satellite communication, high-speed internet access, and last-mile connectivity. As FSO perpetuates progress, this paper suffices as a recent and inclusive resource for researchers, engineers, and policymakers maneuvering the edges of optical communication technologies.","PeriodicalId":509395,"journal":{"name":"Journal of Optical Communications","volume":null,"pages":null},"PeriodicalIF":0.0,"publicationDate":"2024-02-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140424248","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Vashista Bharadwaj K, Sai Chaitanya D, Pujith K, Maneesha Y, Manoj Sindhwani, Shippu Sachdeva, Manoj Singh Adhikari
These days usage of wireless communication has become vast compared to wired communication. The landline is replaced with a mobile, wi-fi with DAS. From the era of 1970 to the 1980s, wireless communication has evolved and wireless communication uses RF waves to communicate which is called RF communication. As the demand for the speed of data rate, the new technology is evolving in the unguided medium due to its range, cost, and availability. In this evolution, it first came with optical fiber and after RF wireless or electromagnetic wireless technologies. Later, researchers have been found optical communication. In present days it is facing a lot of challenges and trials. Optical communication means communication using the light ray or light spectrum which can achieve great speed and long distance with secure data transfer. The major challenge to achieve this communication is atmospheric turbulence. Although lots of experiments have been done still the problem is the detection of atmospheric conditions and making communication possible according to atmospheric turbulence. In this paper, we are going to discuss a few techniques to detect atmospheric turbulence.
如今，与有线通信相比，无线通信的使用已变得非常广泛。固定电话被移动电话取代，无线网络被 DAS 取代。从 1970 年到 1980 年代，无线通信不断发展，无线通信使用射频波进行通信，这就是射频通信。随着对数据传输速率的要求越来越高，新技术因其范围、成本和可用性而在无引导媒介中不断发展。在这一演变过程中，首先出现的是光纤，然后是射频无线或电磁无线技术。后来，研究人员又发现了光通信。如今，光通信正面临着许多挑战和考验。光通信是指利用光线或光谱进行的通信，可以实现高速、远距离和安全的数据传输。实现这种通信的主要挑战是大气湍流。尽管已经进行了大量实验，但问题仍然在于如何检测大气条件，并根据大气湍流情况实现通信。本文将讨论几种检测大气湍流的技术。
{"title":"Detection of atmospheric turbulence parameters in free space optical communication","authors":"Vashista Bharadwaj K, Sai Chaitanya D, Pujith K, Maneesha Y, Manoj Sindhwani, Shippu Sachdeva, Manoj Singh Adhikari","doi":"10.1515/joc-2023-0377","DOIUrl":"https://doi.org/10.1515/joc-2023-0377","url":null,"abstract":"\u0000 These days usage of wireless communication has become vast compared to wired communication. The landline is replaced with a mobile, wi-fi with DAS. From the era of 1970 to the 1980s, wireless communication has evolved and wireless communication uses RF waves to communicate which is called RF communication. As the demand for the speed of data rate, the new technology is evolving in the unguided medium due to its range, cost, and availability. In this evolution, it first came with optical fiber and after RF wireless or electromagnetic wireless technologies. Later, researchers have been found optical communication. In present days it is facing a lot of challenges and trials. Optical communication means communication using the light ray or light spectrum which can achieve great speed and long distance with secure data transfer. The major challenge to achieve this communication is atmospheric turbulence. Although lots of experiments have been done still the problem is the detection of atmospheric conditions and making communication possible according to atmospheric turbulence. In this paper, we are going to discuss a few techniques to detect atmospheric turbulence.","PeriodicalId":509395,"journal":{"name":"Journal of Optical Communications","volume":null,"pages":null},"PeriodicalIF":0.0,"publicationDate":"2024-02-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140424030","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Lasers are paradigmatic examples of nonlinear systems and have played a crucial role in developing nonlinear dynamics into an interdisciplinary topic. Indeed, a freely operating laser represents a nontrivial system, but the phenomena that occur are much more interesting when the laser is exposed to external factors such as optical feedback (OFB) and optical injection (OI). This paper deals with the analysis of the dynamic behavior of a quantum dot semiconductor laser (QDSL) model under the influence of optical injection from another laser. The proposed model was studied numerically with the help of MATLAB. A QDSL system with optical injection was proposed and studied numerically. The quantum dot (QD) laser was used, which is a quantum semiconductor laser and has strong stability without external perturbation. When it is subjected to feedback, it has a critical effect on the follower laser and changes its stable behavior before injection to a set of nonlinear dynamics. The effect of both optical feedback strength and the delay time on the performance and behavior of the bifurcation patterns in the follower laser output was studied, taking into account changing the bifurcation parameters, the injection force k, the slave laser frequency, and the slave laser delay time. The behavior of the slave was studied each time and compared with the behavior of the master. We observed the chaotic paths (essentially stable and continuous pulsating oscillations evolving into periodic and semi-periodic oscillations and then chaotic ones). The time series corresponding to the bifurcation diagrams and the probability of the time interval between spikes and attractors were studied.
{"title":"Optically injected quantum dot lasers and its complex dynamics","authors":"Tahani Adil Kareem, H. A. Al Husseini","doi":"10.1515/joc-2024-0010","DOIUrl":"https://doi.org/10.1515/joc-2024-0010","url":null,"abstract":"\u0000 Lasers are paradigmatic examples of nonlinear systems and have played a crucial role in developing nonlinear dynamics into an interdisciplinary topic. Indeed, a freely operating laser represents a nontrivial system, but the phenomena that occur are much more interesting when the laser is exposed to external factors such as optical feedback (OFB) and optical injection (OI). This paper deals with the analysis of the dynamic behavior of a quantum dot semiconductor laser (QDSL) model under the influence of optical injection from another laser. The proposed model was studied numerically with the help of MATLAB. A QDSL system with optical injection was proposed and studied numerically. The quantum dot (QD) laser was used, which is a quantum semiconductor laser and has strong stability without external perturbation. When it is subjected to feedback, it has a critical effect on the follower laser and changes its stable behavior before injection to a set of nonlinear dynamics. The effect of both optical feedback strength and the delay time on the performance and behavior of the bifurcation patterns in the follower laser output was studied, taking into account changing the bifurcation parameters, the injection force k, the slave laser frequency, and the slave laser delay time. The behavior of the slave was studied each time and compared with the behavior of the master. We observed the chaotic paths (essentially stable and continuous pulsating oscillations evolving into periodic and semi-periodic oscillations and then chaotic ones). The time series corresponding to the bifurcation diagrams and the probability of the time interval between spikes and attractors were studied.","PeriodicalId":509395,"journal":{"name":"Journal of Optical Communications","volume":null,"pages":null},"PeriodicalIF":0.0,"publicationDate":"2024-02-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140431359","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
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