Pub Date : 2024-12-09DOI: 10.1109/JSTQE.2024.3513458
Babak Olyaeefar;Enes Şeker;Ramy El-Ganainy;Abdullah Demir
In recent years, engineering the spatial distribution of optical gain and loss has emerged as a new paradigm for tailoring light transport, trapping, and its interaction with matter. In this regard, it was shown that the notion of PT-symmetry can be employed to build new on-chip laser devices that operate in single longitudinal/transverse mode. Until recently, however, obtaining realistic power output and beam qualities from these systems was impossible. A recent study on quasi-PT-symmetric (q-PTS) lasers has changed this landscape by demonstrating up to 0.5 W output power with a high-quality Gaussian beam profile. In that work, PTS was implemented only for the higher-order mode in what can be considered a two-mode supersymmetric laser. Encouraged by these results and to present a clear roadmap for building practical chip-scale lasers with high performance, here we present a detailed comparison between the performance of PTS and q-PTS lasers in terms of power, mode filtering, and beam quality. Our experimental results, which are also supported by theoretical analysis, indicate that both q-PTS and PTS lasers scale similarly in terms of output power levels as a function of the pump current. However, when it comes to mode filtering and beam quality, our results clearly indicate that quasi-PTS lasers outperform PTS counterpart devices by a large margin. This can be explained by noting that while PTS geometry provides modal filtering for the higher order modes in the lasing cavity, it introduces side lobe contribution from the passive cavity which degrades the far-field emission pattern.
{"title":"Quasi PT-Symmetric Edge-Emitting Lasers Outperform PT-Symmetric Ones","authors":"Babak Olyaeefar;Enes Şeker;Ramy El-Ganainy;Abdullah Demir","doi":"10.1109/JSTQE.2024.3513458","DOIUrl":"https://doi.org/10.1109/JSTQE.2024.3513458","url":null,"abstract":"In recent years, engineering the spatial distribution of optical gain and loss has emerged as a new paradigm for tailoring light transport, trapping, and its interaction with matter. In this regard, it was shown that the notion of PT-symmetry can be employed to build new on-chip laser devices that operate in single longitudinal/transverse mode. Until recently, however, obtaining realistic power output and beam qualities from these systems was impossible. A recent study on quasi-PT-symmetric (q-PTS) lasers has changed this landscape by demonstrating up to 0.5 W output power with a high-quality Gaussian beam profile. In that work, PTS was implemented only for the higher-order mode in what can be considered a two-mode supersymmetric laser. Encouraged by these results and to present a clear roadmap for building practical chip-scale lasers with high performance, here we present a detailed comparison between the performance of PTS and q-PTS lasers in terms of power, mode filtering, and beam quality. Our experimental results, which are also supported by theoretical analysis, indicate that both q-PTS and PTS lasers scale similarly in terms of output power levels as a function of the pump current. However, when it comes to mode filtering and beam quality, our results clearly indicate that quasi-PTS lasers outperform PTS counterpart devices by a large margin. This can be explained by noting that while PTS geometry provides modal filtering for the higher order modes in the lasing cavity, it introduces side lobe contribution from the passive cavity which degrades the far-field emission pattern.","PeriodicalId":13094,"journal":{"name":"IEEE Journal of Selected Topics in Quantum Electronics","volume":"31 2: Pwr. and Effic. Scaling in Semiconductor Lasers","pages":"1-8"},"PeriodicalIF":4.3,"publicationDate":"2024-12-09","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142890317","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-12-05DOI: 10.1109/JSTQE.2024.3499575
{"title":"IEEE Journal of Selected Topics in Quantum Electronics Publication Information","authors":"","doi":"10.1109/JSTQE.2024.3499575","DOIUrl":"https://doi.org/10.1109/JSTQE.2024.3499575","url":null,"abstract":"","PeriodicalId":13094,"journal":{"name":"IEEE Journal of Selected Topics in Quantum Electronics","volume":"30 6: Advances and Applications of Hollow-Core Fibers","pages":"C2-C2"},"PeriodicalIF":4.3,"publicationDate":"2024-12-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://ieeexplore.ieee.org/stamp/stamp.jsp?tp=&arnumber=10779591","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142789148","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-12-05DOI: 10.1109/JSTQE.2024.3499579
{"title":"IEEE Journal of Selected Topics in Quantum Electronics Information for Authors","authors":"","doi":"10.1109/JSTQE.2024.3499579","DOIUrl":"https://doi.org/10.1109/JSTQE.2024.3499579","url":null,"abstract":"","PeriodicalId":13094,"journal":{"name":"IEEE Journal of Selected Topics in Quantum Electronics","volume":"30 6: Advances and Applications of Hollow-Core Fibers","pages":"C3-C3"},"PeriodicalIF":4.3,"publicationDate":"2024-12-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://ieeexplore.ieee.org/stamp/stamp.jsp?tp=&arnumber=10779584","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142789149","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-12-05DOI: 10.1109/JSTQE.2024.3499581
{"title":"IEEE Journal of Selected Topics in Quantum Electronics Topic Codes and Topics","authors":"","doi":"10.1109/JSTQE.2024.3499581","DOIUrl":"https://doi.org/10.1109/JSTQE.2024.3499581","url":null,"abstract":"","PeriodicalId":13094,"journal":{"name":"IEEE Journal of Selected Topics in Quantum Electronics","volume":"30 6: Advances and Applications of Hollow-Core Fibers","pages":"C4-C4"},"PeriodicalIF":4.3,"publicationDate":"2024-12-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://ieeexplore.ieee.org/stamp/stamp.jsp?tp=&arnumber=10779972","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142789099","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-12-04DOI: 10.1109/JSTQE.2024.3511716
Md. Shamim Reza;Tuhin Dey;Augustus W. Arbogast;Qian Meng;Seth R. Bank;Mark A. Wistey
Models of GeSn and GeCSn quantum well (QW) lasers were compared to predict net gain and threshold for computing applications. GeSn showed weak confinement of electrons in both k-space (directness) and real space, as well as a weak optical confinement factor. Using material parameters from ab-initio calculations, adding 1-2% carbon to Ge or GeSn could provide all three confinements simultaneously, with up to 350 meV of electron confinement by Ge QW barriers and a direct bandgap that is 50-220 meV below the indirect gap. A 2-4x increase in electron effective mass preserves strong confinement even in narrow, 5 nm GeCSn/Ge quantum wells. Simply keeping electrons out of non-lasing, higher energy states doubles the differential gain compared with GeSn lasers and reduces free carrier absorption, while deeper QWs further enhance gain. GeCSn laser thresholds as low as 160 A/cm 2