{"id":167,"date":"2023-09-26T15:18:19","date_gmt":"2023-09-26T15:18:19","guid":{"rendered":"https:\/\/creol.ucf.edu\/sdl\/?page_id=167"},"modified":"2025-03-28T23:21:44","modified_gmt":"2025-03-28T23:21:44","slug":"scalable-phase-locking-and-synchronization-in-arrays","status":"publish","type":"page","link":"https:\/\/creol.ucf.edu\/sdl\/research\/scalable-phase-locking-and-synchronization-in-arrays\/","title":{"rendered":"Scalable Phase-locking and Synchronization in Laser Diode Arrays"},"content":{"rendered":"\t\t<div data-elementor-type=\"wp-page\" data-elementor-id=\"167\" class=\"elementor elementor-167\" data-elementor-post-type=\"page\">\n\t\t\t\t\t\t<section class=\"elementor-section elementor-top-section elementor-element elementor-element-2366e00 elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-id=\"2366e00\" data-element_type=\"section\" data-e-type=\"section\">\n\t\t\t\t\t\t<div class=\"elementor-container elementor-column-gap-default\">\n\t\t\t\t\t<div class=\"elementor-column elementor-col-100 elementor-top-column elementor-element elementor-element-41546a3\" data-id=\"41546a3\" data-element_type=\"column\" data-e-type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t<div class=\"elementor-element elementor-element-20cb2c8 elementor-widget elementor-widget-image\" data-id=\"20cb2c8\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"image.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<img fetchpriority=\"high\" decoding=\"async\" width=\"768\" height=\"432\" src=\"https:\/\/creol.ucf.edu\/sdl\/wp-content\/uploads\/sites\/48\/2024\/12\/Slide2-768x432.png\" class=\"attachment-medium_large size-medium_large wp-image-484\" alt=\"\" srcset=\"https:\/\/creol.ucf.edu\/sdl\/wp-content\/uploads\/sites\/48\/2024\/12\/Slide2-768x432.png 768w, https:\/\/creol.ucf.edu\/sdl\/wp-content\/uploads\/sites\/48\/2024\/12\/Slide2-300x169.png 300w, https:\/\/creol.ucf.edu\/sdl\/wp-content\/uploads\/sites\/48\/2024\/12\/Slide2-1024x576.png 1024w, https:\/\/creol.ucf.edu\/sdl\/wp-content\/uploads\/sites\/48\/2024\/12\/Slide2.png 1280w\" sizes=\"(max-width: 768px) 100vw, 768px\" \/>\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t<section class=\"elementor-section elementor-top-section elementor-element elementor-element-b33f298 elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-id=\"b33f298\" data-element_type=\"section\" data-e-type=\"section\">\n\t\t\t\t\t\t<div class=\"elementor-container elementor-column-gap-default\">\n\t\t\t\t\t<div class=\"elementor-column elementor-col-100 elementor-top-column elementor-element elementor-element-78c32c2\" data-id=\"78c32c2\" data-element_type=\"column\" data-e-type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t<div class=\"elementor-element elementor-element-7f54e16 elementor-widget elementor-widget-text-editor\" data-id=\"7f54e16\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"text-editor.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t<p>Semiconductor laser diodes are employed for a wide variety of applications. Such lasers can emit light in a wide range of wavelengths, exhibit high (in the range of 60-70%) electro-optical efficiency, are compact, and are low cost. However, a single diode\u2019s emission power is in the range of Watts or lower. Our goal is to increase the capacity of such lasers by phase locking and synchronizing them in scalable arrays. By beam combining many diodes, we aim to provide high-emission radiance [1,2].<\/p><p><u>Near IR\u00a0<\/u><\/p><p>One of the approaches to increase the functionality of semiconductor lasers has been the use of master oscillator power amplifier (MOPA). Such designs have been shown to allow for almost perfect semiconductor diode phase locking with arrays as large as 900 lasers [3\u20135]. The main challenges though are scalability to large power and engineering complexity. External cavity designs are very attractive since phase-locking is spontaneous and consequently engineering complexity to achieve phase-locking is much lower than for MOPA designs. While excellent beam quality from single mode and broad-area diode arrays has been demonstrated [6\u201311], the scalability to very large arrays and stacked-arrays remains an open matter. Accordingly, we are developing experimental designs to enable robust phase locking of large numbers of diodes in an array and have successfully demonstrated phase-locking of 1-D arrays very close to the diffraction limit in the near-infrared (NIR) optical regime [7]. Our experimental efforts are being supported and guided by computational simulations: we have developed codes to numerically simulate very large (O (100,000)) 1-D and 2-D diode arrays. Our external cavity design approach is supplemented by measurements aimed at optimizing the phase-locking system. \u00a0These measurements include simultaneous measurements of the time series, optical spectrum, far-field beam profile and beam quality factor, and others. Beam-combined high-power lasers emitting with excellent beam qualities are ideal sources for several applications including directed energy.<\/p><p><u>Blue Diodes<\/u><\/p><p>High-power, narrow-linewidth, tunable blue lasers are in high demand for many applications, such as high-resolution spectroscopy, holographic data storage, laser cooling, ultraviolet light generation, and underwater applications. For many applications, a single laser does not provide sufficient power, consequently, beam combining of multiple lasers is necessary. In our lab, we are designing and building high-power, high-quality blue laser systems via coherent beam combing and phase locking of broad-area blue laser diode arrays. Since blue diode arrays have only recently become commercially available and accumulated knowledge and experience with blue diodes are limited, beam combining of blue diode arrays is challenging. Consequently, high-power light sources in the blue spectral region are still deficient in beam quality. We are developing several optical setups involving blue laser arrays. One example is a V-shaped external Talbot cavity to couple the laser diodes and induce phase synchrony. We have recently demonstrated very narrow (O (10-15 pm)) linewidth emitted from broad-area blue diode array [12].\u00a0 The motivation of our work is to design and demonstrate the emission of a high-power blue laser with excellent beam quality. These high-power blue lasers will be a great source for several industrial applications and for underwater sensing and communication.<\/p>\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<div class=\"elementor-element elementor-element-df25f3b elementor-widget elementor-widget-image\" data-id=\"df25f3b\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"image.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<img decoding=\"async\" width=\"768\" height=\"378\" src=\"https:\/\/creol.ucf.edu\/sdl\/wp-content\/uploads\/sites\/48\/2025\/03\/Far-field-figures2-768x378.png\" class=\"attachment-medium_large size-medium_large wp-image-741\" alt=\"\" srcset=\"https:\/\/creol.ucf.edu\/sdl\/wp-content\/uploads\/sites\/48\/2025\/03\/Far-field-figures2-768x378.png 768w, https:\/\/creol.ucf.edu\/sdl\/wp-content\/uploads\/sites\/48\/2025\/03\/Far-field-figures2-300x148.png 300w, https:\/\/creol.ucf.edu\/sdl\/wp-content\/uploads\/sites\/48\/2025\/03\/Far-field-figures2-1024x504.png 1024w, https:\/\/creol.ucf.edu\/sdl\/wp-content\/uploads\/sites\/48\/2025\/03\/Far-field-figures2.png 1204w\" sizes=\"(max-width: 768px) 100vw, 768px\" \/>\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t<section class=\"elementor-section elementor-top-section elementor-element elementor-element-19d9969 elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-id=\"19d9969\" data-element_type=\"section\" data-e-type=\"section\">\n\t\t\t\t\t\t<div class=\"elementor-container elementor-column-gap-default\">\n\t\t\t\t\t<div class=\"elementor-column elementor-col-100 elementor-top-column elementor-element elementor-element-ea668bf\" data-id=\"ea668bf\" data-element_type=\"column\" data-e-type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t<div class=\"elementor-element elementor-element-231a8fa elementor-widget elementor-widget-text-editor\" data-id=\"231a8fa\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"text-editor.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t<p><u>Pulsed Lasers<\/u><\/p><p>Controllable pulsing in diode lasers has been in the spotlight in recent years. A variety of pulsing mechanisms have been explored, including mode-locking, gain-switching, Q-switching, and others. In our lab, we are studying phase-locking of pulsed lasers in arrays as well as mode-locking in multimode diode lasers. Several years ago, we computationally demonstrated the feasibility of phase-locking a 49-diode array [13]. We are now expanding these studies to 2-D homogeneous and heterogeneous arrays, along with the effects of modulating current amplitude and frequency on phase-locking.<\/p>\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t<section class=\"elementor-section elementor-top-section elementor-element elementor-element-fb926e8 elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-id=\"fb926e8\" data-element_type=\"section\" data-e-type=\"section\">\n\t\t\t\t\t\t<div class=\"elementor-container elementor-column-gap-default\">\n\t\t\t\t\t<div class=\"elementor-column elementor-col-100 elementor-top-column elementor-element elementor-element-08e00d3\" data-id=\"08e00d3\" data-element_type=\"column\" data-e-type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t<div class=\"elementor-element elementor-element-a7f1baa elementor-widget elementor-widget-image\" data-id=\"a7f1baa\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"image.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<img decoding=\"async\" width=\"561\" height=\"447\" src=\"https:\/\/creol.ucf.edu\/sdl\/wp-content\/uploads\/sites\/48\/2023\/10\/ThumbnailResearchArea_Scalable-phase-locking-and-synchronization-in-arrays-of-semiconductor-laser-diodes.png\" class=\"attachment-large size-large wp-image-214\" alt=\"\" srcset=\"https:\/\/creol.ucf.edu\/sdl\/wp-content\/uploads\/sites\/48\/2023\/10\/ThumbnailResearchArea_Scalable-phase-locking-and-synchronization-in-arrays-of-semiconductor-laser-diodes.png 561w, https:\/\/creol.ucf.edu\/sdl\/wp-content\/uploads\/sites\/48\/2023\/10\/ThumbnailResearchArea_Scalable-phase-locking-and-synchronization-in-arrays-of-semiconductor-laser-diodes-300x239.png 300w\" sizes=\"(max-width: 561px) 100vw, 561px\" \/>\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<div class=\"elementor-element elementor-element-48b009c elementor-widget elementor-widget-text-editor\" data-id=\"48b009c\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"text-editor.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t<p>Fig. 1: Evolution of the beam size of a single emitter in the array with the propagation distance around the near field focus. This measurement is of interest to derive the beam quality factor M\u00b2 that impacts the total width of the combined coherent beams from multiple emitters.<\/p>\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<div class=\"elementor-element elementor-element-267db99 elementor-widget elementor-widget-image\" data-id=\"267db99\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"image.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<img loading=\"lazy\" decoding=\"async\" width=\"768\" height=\"366\" src=\"https:\/\/creol.ucf.edu\/sdl\/wp-content\/uploads\/sites\/48\/2023\/10\/Picture1-768x366.png\" class=\"attachment-medium_large size-medium_large wp-image-271\" alt=\"\" srcset=\"https:\/\/creol.ucf.edu\/sdl\/wp-content\/uploads\/sites\/48\/2023\/10\/Picture1-768x366.png 768w, https:\/\/creol.ucf.edu\/sdl\/wp-content\/uploads\/sites\/48\/2023\/10\/Picture1-300x143.png 300w, https:\/\/creol.ucf.edu\/sdl\/wp-content\/uploads\/sites\/48\/2023\/10\/Picture1-1024x488.png 1024w, https:\/\/creol.ucf.edu\/sdl\/wp-content\/uploads\/sites\/48\/2023\/10\/Picture1.png 1430w\" sizes=\"(max-width: 768px) 100vw, 768px\" \/>\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<div class=\"elementor-element elementor-element-7b22682 elementor-widget elementor-widget-text-editor\" data-id=\"7b22682\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"text-editor.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t<p>Fig. 2: Synchronized pulsing behavior in a 1D-array of 49 lasers subject to optical feedback, global coupling, and periodic modulation of the bias current.<\/p>\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t<section class=\"elementor-section elementor-top-section elementor-element elementor-element-41e76fa elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-id=\"41e76fa\" data-element_type=\"section\" data-e-type=\"section\">\n\t\t\t\t\t\t<div class=\"elementor-container elementor-column-gap-default\">\n\t\t\t\t\t<div class=\"elementor-column elementor-col-100 elementor-top-column elementor-element elementor-element-9e4b1c2\" data-id=\"9e4b1c2\" data-element_type=\"column\" data-e-type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t<div class=\"elementor-element elementor-element-bfa13ec elementor-widget elementor-widget-text-editor\" data-id=\"bfa13ec\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"text-editor.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t<p><strong>Works Cited<\/strong><\/p><ol><li>T. Y. Fan, \u201cLaser beam combining for high-power, high-radiance sources,\u201d IEEE J. Sel. Top. Quantum Electron.\u00a0<strong>11<\/strong>(3), 567\u2013577 (2005).<\/li><li>A. M. Jones and J. T. Gopinath, \u201cFast-to-slow axis mode imaging for brightness enhancement of a broad-area laser diode array,\u201d Opt. Express\u00a0<strong>21<\/strong>(15), 17912\u201317919 (2013).<\/li><li>R. K. Huang, L. J. Missaggia, J. P. Donnelly, C. T. Harris, and G. W. Turner, \u201cHigh-brightness slab-coupled optical waveguide laser arrays,\u201d IEEE Photonics Technol. Lett.\u00a0<strong>17<\/strong>(5), 959\u2013961 (2005).<\/li><li>K. J. Creedon, S. M. Redmond, G. M. Smith, L. J. Missaggia, M. K. Connors, J. E. Kansky, T. Y. Fan, G. W. Turner, and A. Sanchez-Rubio, \u201cHigh efficiency coherent beam combining of semiconductor optical amplifiers,\u201d Opt. Lett.\u00a0<strong>37<\/strong>(23), 5006\u20135008 (2012).<\/li><li>J. L. Levy and K. Roh, \u201cCoherent array of 900 semiconductor laser amplifiers,\u201d in Photonics West \u201995,\u00a0<strong>2382<\/strong>, pp. 58\u201369. (1995)<\/li><li>B. Liu, Y. Liu, and Y. Braiman, \u201cCoherent beam combining of high-power broad-area laser diode array with a closed-V-shape external Talbot cavity,\u201d Opt. Express\u00a0<strong>18<\/strong>(7), 7361\u20137368 (2010).<\/li><li>B. Liu and Y. Braiman, \u201cCoherent beam combining of high-power broad-area laser diode array with near diffraction limited beam quality and high power conversion efficiency,\u201d Opt. Express\u00a0<strong>21<\/strong>(25), 31218\u201331228 (2013).<\/li><li>C. J. Corcoran and F. Durville, \u201cPassive coherent combination of a diode laser array with 35 elements,\u201d Opt. Express\u00a0<strong>22<\/strong>(7), 8420\u20138425 (2014).<\/li><li>K. Hirosawa, F. Shohda, T. Yanagisawa, and F. Kannari, \u201cIn-phase synchronization of array laser using intra- Talbot-cavity second harmonic generation,\u201d Proc. SPIE\u00a0<strong>9342<\/strong>, 934216 (2015).<\/li><li>D. Mehuys, K. Mitsunaga, L. Eng, W. K. Marshall, and A. Yariv, \u201cSupermode control in diffraction-coupled semiconductor laser arrays,\u201d Appl. Phys. Lett.\u00a0<strong>53<\/strong>(13), 1165\u20131167 (1988).<\/li><li>J. R. Leger and G. Mowry, \u201cExternal diode-laser-array cavity with mode-selecting mirror,\u201d Appl. Phys. Lett.\u00a0<strong>63<\/strong>(21), 2884\u20132886 (1993).<\/li><li>P. R. Nyaupane, P. L. Likamwa, and Y. Braiman,\u00a0<em>Spectral Linewidth Narrowing of Broad-Area Blue Diode Bar in V-Shape External Talbot Cavity<\/em>, Optics Letters\u00a0<strong>47<\/strong>, 2802 (2022).<\/li><li>Liu, Y. Braiman, N. Nair, Y. Lu, Y. Guo, P. Colet, and M. Wardlaw, \u201c<em>Nonlinear Dynamics and Synchronization of an Array of Single Mode Laser Diodes in External Cavity Subject to Current Modulation<\/em>\u201d, Optics Communications\u00a0<strong>324<\/strong>, 301 (2014).<\/li><\/ol><p><strong>Related Works\u00a0<\/strong><\/p><p><a href=\"https:\/\/pubs.acs.org\/doi\/10.1021\/acsphotonics.4c01062?articleRef=test\">Nyaupane, O. Spitz, G. Scranton, S. Koyu, M. A. Berrill, P. L. LiKamWa, Y. Braiman, \u201cCoherence and Phase-Locking in High-Power, Broad-Area, Highly Heterogeneous Blue Diode Laser Arrays\u201d, ACS Photonics 12, (2025)<\/a><\/p><p><a href=\"https:\/\/impact.ornl.gov\/en\/publications\/optimization-of-combined-coherent-gain-switch-pulsing-in-a-large-\">Spitz, L. E. Maldonado-Castillo, M. A. Berrill, Y. Braiman, \u201cOptimization of Combined Coherent Gain-Switch Pulsing in a Large Array of Semiconductor Lasers\u201d, IEEE Journal of Selected Topics in Quantum Electronics 31, 1501614 (2025)<\/a><\/p>\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t<\/div>\n\t\t","protected":false},"excerpt":{"rendered":"Semiconductor laser diodes are employed for a wide variety of applications. Such lasers can emit light in a wide range of wavelengths, exhibit high (in the range of 60-70%) electro-optical efficiency, are compact, and are low cost. However, a single diode\u2019s emission power is in the range of Watts or lower. Our goal is to&hellip;","protected":false},"author":83,"featured_media":0,"parent":15,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"_acf_changed":false,"footnotes":""},"class_list":["post-167","page","type-page","status-publish","hentry"],"acf":[],"_links":{"self":[{"href":"https:\/\/creol.ucf.edu\/sdl\/wp-json\/wp\/v2\/pages\/167","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/creol.ucf.edu\/sdl\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/creol.ucf.edu\/sdl\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/creol.ucf.edu\/sdl\/wp-json\/wp\/v2\/users\/83"}],"replies":[{"embeddable":true,"href":"https:\/\/creol.ucf.edu\/sdl\/wp-json\/wp\/v2\/comments?post=167"}],"version-history":[{"count":28,"href":"https:\/\/creol.ucf.edu\/sdl\/wp-json\/wp\/v2\/pages\/167\/revisions"}],"predecessor-version":[{"id":852,"href":"https:\/\/creol.ucf.edu\/sdl\/wp-json\/wp\/v2\/pages\/167\/revisions\/852"}],"up":[{"embeddable":true,"href":"https:\/\/creol.ucf.edu\/sdl\/wp-json\/wp\/v2\/pages\/15"}],"wp:attachment":[{"href":"https:\/\/creol.ucf.edu\/sdl\/wp-json\/wp\/v2\/media?parent=167"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}