Underwater wireless optical communication (UWOC) is an emerging and feasible underwater communication technology and has developed rapidly in recent years. Building a high-performance and practical UWOC system requires comprehensive consideration and optimization design from the device to the system, as well as from the internal modulation to the external environment. This paper provides an overview of the recent developments in UWOC systems, covering aspects about the system transmitters and receivers, advanced modulation formats and underwater channels. Some key technologies to improve transmission capacity of UWOC are classified and summarized to provide guidance for system design. The main challenges and perspectives to achieve a reliable UWOC system are also mentioned. The summary and analysis of these advances and techniques will shed light on the future development of UWOC technology and assist in the construction of the internet of underwater things.
{"title":"Recent progress in and perspectives of underwater wireless optical communication","authors":"Shijie Zhu , Xinwei Chen , Xiaoyan Liu , Guoqi Zhang , Pengfei Tian","doi":"10.1016/j.pquantelec.2020.100274","DOIUrl":"https://doi.org/10.1016/j.pquantelec.2020.100274","url":null,"abstract":"<div><p><span><span>Underwater wireless optical communication (UWOC) is an emerging and feasible </span>underwater communication technology and has developed rapidly in recent years. Building a high-performance and practical UWOC system requires comprehensive consideration and optimization design from the device to the system, as well as from the internal modulation to the external environment. This paper provides an overview of the recent developments in UWOC systems, covering aspects about the system transmitters and receivers, advanced </span>modulation formats and underwater channels. Some key technologies to improve transmission capacity of UWOC are classified and summarized to provide guidance for system design. The main challenges and perspectives to achieve a reliable UWOC system are also mentioned. The summary and analysis of these advances and techniques will shed light on the future development of UWOC technology and assist in the construction of the internet of underwater things.</p></div>","PeriodicalId":414,"journal":{"name":"Progress in Quantum Electronics","volume":"73 ","pages":"Article 100274"},"PeriodicalIF":11.7,"publicationDate":"2020-09-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/j.pquantelec.2020.100274","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"2183580","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":1,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2020-08-01DOI: 10.1016/j.pquantelec.2020.100265
C.A. Reynaud , D. Duché , J.-J. Simon , E. Sanchez-Adaime , O. Margeat , J. Ackermann , V. Jangid , C. Lebouin , D. Brunel , F. Dumur , D. Gigmes , G. Berginc , C.A. Nijhuis , L. Escoubas
Rectifying antennas are often prensented as a potentiel technological breakthrough for energy harvesting. First theorized in the 1970’s, the downsizing of an antenna coupled with a rectifier has become technologically achievable with the progresses of fabrication techniques such as electron beam or photolithography. However, reaching infrared or visible region of the electromagnetic spectra still entails challenges on the integration of a rectifier operating in the terahertz range. New bottom up approaches are likely to bring a promising solution to this issue. To improve our understanding of the key points of rectifying antennas’ design for the infrared and visible light, and the challenges of device fabrication, this work reviews the progresses of this technology, going back from the first historical RF energy harvesting systems and covering the most innovative trends to this date.
{"title":"Rectifying antennas for energy harvesting from the microwaves to visible light: A review","authors":"C.A. Reynaud , D. Duché , J.-J. Simon , E. Sanchez-Adaime , O. Margeat , J. Ackermann , V. Jangid , C. Lebouin , D. Brunel , F. Dumur , D. Gigmes , G. Berginc , C.A. Nijhuis , L. Escoubas","doi":"10.1016/j.pquantelec.2020.100265","DOIUrl":"https://doi.org/10.1016/j.pquantelec.2020.100265","url":null,"abstract":"<div><p><span>Rectifying antennas are often prensented as a potentiel technological breakthrough for energy harvesting. First theorized in the 1970’s, the downsizing of an antenna coupled with a </span>rectifier<span><span><span> has become technologically achievable with the progresses of fabrication techniques such as electron beam or </span>photolithography<span>. However, reaching infrared or visible region of the electromagnetic spectra still entails challenges on the integration of a rectifier operating in the terahertz range. New bottom up approaches are likely to bring a promising solution to this issue. To improve our understanding of the key points of rectifying antennas’ design for the infrared and </span></span>visible light<span>, and the challenges of device fabrication, this work reviews the progresses of this technology, going back from the first historical RF energy harvesting systems and covering the most innovative trends to this date.</span></span></p></div>","PeriodicalId":414,"journal":{"name":"Progress in Quantum Electronics","volume":"72 ","pages":"Article 100265"},"PeriodicalIF":11.7,"publicationDate":"2020-08-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/j.pquantelec.2020.100265","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"2183581","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":1,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
We report on the first watt-level ultrafast laser inscribed Thulium waveguide (WG) lasers. Depressed-index buried channel WGs with a circular cladding (type III) are produced in monoclinic Tm3+:KLu(WO4)2 crystals. Laser operation is achieved under conventional (3H6 → 3H4) and in-band (3H6 → 3F4) pumping. In the former case, employing a Raman fiber laser emitting at 1679 nm as pump, the continuous-wave Tm channel WG laser generated 1.37 W at 1915–1923 nm with a record-high slope efficiency of 82.7% (with respect to the absorbed pump power), a threshold of only 17 mW and a spatially single-mode output with linear polarization. The WG propagation losses were 0.2 ± 0.3 dB/cm. Passive Q-switching of Tm channel WG lasers is achieved using Cr2+:ZnS and Cr2+:ZnSe saturable absorbers. With Cr2+:ZnS, record-short pulses of 2.6 ns/6.9 μJ at a repetition rate of 8.0 kHz were generated. The developed WGs are promising for compact GHz mode-locked lasers at ~2 μm.
{"title":"Watt-level ultrafast laser inscribed thulium waveguide lasers","authors":"Esrom Kifle , Pavel Loiko , Carolina Romero , Javier Rodríguez Vázquez de Aldana , Magdalena Aguiló , Francesc Díaz , Patrice Camy , Uwe Griebner , Valentin Petrov , Xavier Mateos","doi":"10.1016/j.pquantelec.2020.100266","DOIUrl":"https://doi.org/10.1016/j.pquantelec.2020.100266","url":null,"abstract":"<div><p><span><span><span>We report on the first watt-level ultrafast laser inscribed </span>Thulium </span>waveguide (WG) lasers. Depressed-index buried channel WGs with a circular cladding (type III) are produced in monoclinic Tm</span><sup>3+</sup>:KLu(WO<sub>4</sub>)<sub>2</sub> crystals. Laser operation is achieved under conventional (<sup>3</sup>H<sub>6</sub> → <sup>3</sup>H<sub>4</sub>) and in-band (<sup>3</sup>H<sub>6</sub> → <sup>3</sup>F<sub>4</sub><span><span>) pumping. In the former case, employing a Raman fiber laser emitting at 1679 nm as pump, the continuous-wave Tm channel WG laser generated 1.37 W at 1915–1923 nm with a record-high slope efficiency of 82.7% (with respect to the absorbed pump power), a threshold of only 17 mW and a spatially single-mode output with </span>linear polarization. The WG propagation losses were 0.2 ± 0.3 dB/cm. Passive Q-switching of Tm channel WG lasers is achieved using Cr</span><sup>2+</sup>:ZnS and Cr<sup>2+</sup>:ZnSe saturable absorbers. With Cr<sup>2+</sup>:ZnS, record-short pulses of 2.6 ns/6.9 μJ at a repetition rate of 8.0 kHz were generated. The developed WGs are promising for compact GHz mode-locked lasers at ~2 μm.</p></div>","PeriodicalId":414,"journal":{"name":"Progress in Quantum Electronics","volume":"72 ","pages":"Article 100266"},"PeriodicalIF":11.7,"publicationDate":"2020-08-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/j.pquantelec.2020.100266","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"2620886","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":1,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2020-08-01DOI: 10.1016/j.pquantelec.2020.100255
Markus Pollnau , Marc Eichhorn
<div><p>The degree of spectral coherence characterizes the spectral purity of light. It can be equivalently expressed in the time domain by the decay time <em>τ</em> or the quality factor <em>Q</em><span> of the light-emitting oscillator, the coherence time </span><em>τ</em> <sup><em>coh</em></sup> or length <span><math><mi>ℓ</mi></math></span><sup><em>coh</em></sup><span> of emitted light or, via Fourier transformation to the frequency domain, the linewidth Δ</span><em>ν</em><span><span><span> of emitted light. We quantify these parameters for the reference situation of a passive Fabry-Pérot resonator. We investigate its </span>spectral line shapes, mode profiles, and Airy distributions and verify that the sum of all mode profiles generates the corresponding Airy distribution. The Fabry-Pérot resonator is described, as an oscillator, by its Lorentzian linewidth and finesse and, as a scanning spectrometer, by its Airy linewidth and finesse. Furthermore, stimulated and spontaneous emission are analyzed semi-classically by employing Maxwell′s equations and the law of energy conservation. Investigation of emission by atoms inside a Fabry-Pérot resonator, the Lorentz oscillator model, the Kramers-Kronig relations, the amplitude-phase diagram, and the summation of quantized electric fields consistently suggests that stimulated and spontaneous emission of light occur with a phase 90° in lead of the incident field. These findings question the quantum-optical picture, which proposed, firstly, that </span>stimulated emission occurred in phase, whereas spontaneous emission occurred at an arbitrary phase angle with respect to the incident field and, secondly, that the laser linewidth were due to amplitude and phase fluctuations induced by spontaneous emission. We emphasize that the first derivation of the Schawlow-Townes laser linewidth was entirely semi-classical but included the four approximations that (i) it is a truly continuous-wave (cw) laser, (ii) it is an ideal four-level laser, (iii) its resonator exhibits no intrinsic losses, and (iv) one photon is coupled spontaneously into the lasing mode per photon-decay time </span><em>τ</em><sub><em>c</em></sub> of the resonator, independent of the pump rate. After discussing the inconsistencies of existing semi-classical and quantum-optical descriptions of the laser linewidth, we introduce the spectral-coherence factor, which quantifies spectral coherence in an active compared to its underlying passive mode, and derive semi-classically, based on the principle that the gain elongates the photon-decay time and narrows the linewidth, the fundamental linewidth of a single lasing mode. This linewidth is valid for lasers with an arbitrary energy-level system, operating below, at, or above threshold and in a cw or a transient lasing regime, with the gain being smaller, equal, or larger compared to the losses. By applying approximations (i)-(iv) we reproduce the original Schawlow-Townes equation. It provides the hi
{"title":"Spectral coherence, Part I: Passive-resonator linewidth, fundamental laser linewidth, and Schawlow-Townes approximation","authors":"Markus Pollnau , Marc Eichhorn","doi":"10.1016/j.pquantelec.2020.100255","DOIUrl":"https://doi.org/10.1016/j.pquantelec.2020.100255","url":null,"abstract":"<div><p>The degree of spectral coherence characterizes the spectral purity of light. It can be equivalently expressed in the time domain by the decay time <em>τ</em> or the quality factor <em>Q</em><span> of the light-emitting oscillator, the coherence time </span><em>τ</em> <sup><em>coh</em></sup> or length <span><math><mi>ℓ</mi></math></span><sup><em>coh</em></sup><span> of emitted light or, via Fourier transformation to the frequency domain, the linewidth Δ</span><em>ν</em><span><span><span> of emitted light. We quantify these parameters for the reference situation of a passive Fabry-Pérot resonator. We investigate its </span>spectral line shapes, mode profiles, and Airy distributions and verify that the sum of all mode profiles generates the corresponding Airy distribution. The Fabry-Pérot resonator is described, as an oscillator, by its Lorentzian linewidth and finesse and, as a scanning spectrometer, by its Airy linewidth and finesse. Furthermore, stimulated and spontaneous emission are analyzed semi-classically by employing Maxwell′s equations and the law of energy conservation. Investigation of emission by atoms inside a Fabry-Pérot resonator, the Lorentz oscillator model, the Kramers-Kronig relations, the amplitude-phase diagram, and the summation of quantized electric fields consistently suggests that stimulated and spontaneous emission of light occur with a phase 90° in lead of the incident field. These findings question the quantum-optical picture, which proposed, firstly, that </span>stimulated emission occurred in phase, whereas spontaneous emission occurred at an arbitrary phase angle with respect to the incident field and, secondly, that the laser linewidth were due to amplitude and phase fluctuations induced by spontaneous emission. We emphasize that the first derivation of the Schawlow-Townes laser linewidth was entirely semi-classical but included the four approximations that (i) it is a truly continuous-wave (cw) laser, (ii) it is an ideal four-level laser, (iii) its resonator exhibits no intrinsic losses, and (iv) one photon is coupled spontaneously into the lasing mode per photon-decay time </span><em>τ</em><sub><em>c</em></sub> of the resonator, independent of the pump rate. After discussing the inconsistencies of existing semi-classical and quantum-optical descriptions of the laser linewidth, we introduce the spectral-coherence factor, which quantifies spectral coherence in an active compared to its underlying passive mode, and derive semi-classically, based on the principle that the gain elongates the photon-decay time and narrows the linewidth, the fundamental linewidth of a single lasing mode. This linewidth is valid for lasers with an arbitrary energy-level system, operating below, at, or above threshold and in a cw or a transient lasing regime, with the gain being smaller, equal, or larger compared to the losses. By applying approximations (i)-(iv) we reproduce the original Schawlow-Townes equation. It provides the hi","PeriodicalId":414,"journal":{"name":"Progress in Quantum Electronics","volume":"72 ","pages":"Article 100255"},"PeriodicalIF":11.7,"publicationDate":"2020-08-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/j.pquantelec.2020.100255","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"2620887","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":1,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2020-05-01DOI: 10.1016/j.pquantelec.2020.100254
Andrew J. Lee, David J. Spence, Helen M. Pask
In this paper we review the field of terahertz (THz) sources which make use of the nonlinear, stimulated polariton scattering (SPS) process. A historical perspective of the technology is offered, in addition to an investigation of modern SPS-based THz sources. Breakthroughs in these source technologies have coincided with rapid developments in laser technology over the past 10 years. We are now in an age where pulsed SPS-THz sources are generating peak powers in excess of 50 kW, and continuous wave SPS-THz sources can be produced using diode pump powers as low as 2.3 W. The versatility of this approach to THz generation has enabled the generation of coherent THz radiation across continuous wave (CW), nanosecond-, and picosecond-pulsed modalities, with sources spanning the frequency range 0.5–13 THz. Being based on robust and well-developed, crystalline solid-state laser technology, these sources hold great promise as an enabling technology for a plethora of THz applications.
{"title":"Terahertz sources based on stimulated polariton scattering","authors":"Andrew J. Lee, David J. Spence, Helen M. Pask","doi":"10.1016/j.pquantelec.2020.100254","DOIUrl":"https://doi.org/10.1016/j.pquantelec.2020.100254","url":null,"abstract":"<div><p>In this paper we review the field of terahertz (THz) sources which make use of the nonlinear, stimulated polariton scattering (SPS) process. A historical perspective of the technology is offered, in addition to an investigation of modern SPS-based THz sources. Breakthroughs in these source technologies have coincided with rapid developments in laser technology over the past 10 years. We are now in an age where pulsed SPS-THz sources are generating peak powers in excess of 50 kW, and continuous wave SPS-THz sources can be produced using diode pump powers as low as 2.3 W. The versatility of this approach to THz generation has enabled the generation of coherent THz radiation across continuous wave (CW), nanosecond-, and picosecond-pulsed modalities, with sources spanning the frequency range 0.5–13 THz. Being based on robust and well-developed, crystalline solid-state laser technology, these sources hold great promise as an enabling technology for a plethora of THz applications.</p></div>","PeriodicalId":414,"journal":{"name":"Progress in Quantum Electronics","volume":"71 ","pages":"Article 100254"},"PeriodicalIF":11.7,"publicationDate":"2020-05-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/j.pquantelec.2020.100254","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"2620888","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":1,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2020-05-01DOI: 10.1016/j.pquantelec.2020.100263
Xiaojie Zhou , Pengfei Tian , Chin-Wei Sher , Jiang Wu , Hezhuang Liu , Ran Liu , Hao-Chung Kuo
Micro light-emitting diode (micro-LED) display, mainly based on inorganic GaN-based LED, is an emerging technique with high contrast, low power consumption, long lifetime and fast response time compared to liquid crystal display (LCD) and organic light-emitting diode (OLED) display. Therefore, many research institutes and companies have conducted in-depth research on micro-LED in the full-colour display, gradually realizing the commercialization of micro-LED. And the current research results of micro-LED indicate that it can be widely used in display, visible light communication (VLC), biomedicine and other fields. Although micro-LED has broad commercial prospects, it still faces great challenges, such as the effect of size reduction on performance, the realization of high-density integration on a single wafer for independent addressing of full-colour micro-LED display, the improvement of repair technique and yield et al. This paper reviews the key solutions to the technical difficulties of the full-colour micro-LED display. Specifically, this review analyzes and discusses a variety of advanced full-colour micro-LED display techniques with a focus on three aspects: growth technique, transfer printing technique and colour conversion technique. This review demonstrates the opportunities, progress and challenges of these techniques, aiming to guide the development of full-colour micro-LED display.
{"title":"Growth, transfer printing and colour conversion techniques towards full-colour micro-LED display","authors":"Xiaojie Zhou , Pengfei Tian , Chin-Wei Sher , Jiang Wu , Hezhuang Liu , Ran Liu , Hao-Chung Kuo","doi":"10.1016/j.pquantelec.2020.100263","DOIUrl":"https://doi.org/10.1016/j.pquantelec.2020.100263","url":null,"abstract":"<div><p>Micro light-emitting diode (micro-LED) display, mainly based on inorganic GaN-based LED, is an emerging technique with high contrast, low power consumption, long lifetime and fast response time compared to liquid crystal display<span> (LCD) and organic light-emitting diode (OLED) display. Therefore, many research institutes and companies have conducted in-depth research on micro-LED in the full-colour display, gradually realizing the commercialization of micro-LED. And the current research results of micro-LED indicate that it can be widely used in display, visible light communication (VLC), biomedicine and other fields. Although micro-LED has broad commercial prospects, it still faces great challenges, such as the effect of size reduction on performance, the realization of high-density integration on a single wafer for independent addressing of full-colour micro-LED display, the improvement of repair technique and yield et al. This paper reviews the key solutions to the technical difficulties of the full-colour micro-LED display. Specifically, this review analyzes and discusses a variety of advanced full-colour micro-LED display techniques with a focus on three aspects: growth technique, transfer printing technique and colour conversion technique. This review demonstrates the opportunities, progress and challenges of these techniques, aiming to guide the development of full-colour micro-LED display.</span></p></div>","PeriodicalId":414,"journal":{"name":"Progress in Quantum Electronics","volume":"71 ","pages":"Article 100263"},"PeriodicalIF":11.7,"publicationDate":"2020-05-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/j.pquantelec.2020.100263","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"2620889","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":1,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2020-05-01DOI: 10.1016/j.pquantelec.2020.100264
Ying Han , Yubin Guo , Bo Gao , Chunyang Ma , Ruohan Zhang , Han Zhang
Ultrafast femtosecond mode-locked fiber laser plays an indispensable role in medical imaging, space ranging, ophthalmology, terahertz spectroscopy, material micromachining, and so on. It’s not only an important tool for people to explore the world, but also a pillar field of laser technology. This review present the generation of femtosecond pulses in ultrafast mode-locked fiber lasers using active, passive, hybrid mode-locking techniques, the emphasis is given to passively mode-locked fiber lasers. In terms of the optimization of femtosecond pulses, we introduce the external compression technique to obtain shorter pulse width, chirped pulse amplification technique to increase pulse energy and obtain high energy femtosecond pulses at the practical band. Furthermore, the coherent beam combination and divided pulse amplification technique to further boost pulse energy are summarized. At the end of this review, we present a detailed overview of the applications of femtosecond pulses including the generation of supercontinuum and tunable femtosecond pulses, and some practical applications. Several perspectives and research directions of femtosecond pulses are also addressed.
{"title":"Generation, optimization, and application of ultrashort femtosecond pulse in mode-locked fiber lasers","authors":"Ying Han , Yubin Guo , Bo Gao , Chunyang Ma , Ruohan Zhang , Han Zhang","doi":"10.1016/j.pquantelec.2020.100264","DOIUrl":"https://doi.org/10.1016/j.pquantelec.2020.100264","url":null,"abstract":"<div><p>Ultrafast femtosecond mode-locked fiber laser plays an indispensable role in medical imaging, space ranging, ophthalmology, terahertz spectroscopy<span>, material micromachining, and so on. It’s not only an important tool for people to explore the world, but also a pillar field of laser technology. This review present the generation of femtosecond pulses in ultrafast mode-locked fiber lasers using active, passive, hybrid mode-locking techniques, the emphasis is given to passively mode-locked fiber lasers. In terms of the optimization of femtosecond pulses, we introduce the external compression technique to obtain shorter pulse width, chirped pulse amplification technique to increase pulse energy and obtain high energy femtosecond pulses at the practical band. Furthermore, the coherent beam combination and divided pulse amplification technique to further boost pulse energy are summarized. At the end of this review, we present a detailed overview of the applications of femtosecond pulses including the generation of supercontinuum and tunable femtosecond pulses, and some practical applications. Several perspectives and research directions of femtosecond pulses are also addressed.</span></p></div>","PeriodicalId":414,"journal":{"name":"Progress in Quantum Electronics","volume":"71 ","pages":"Article 100264"},"PeriodicalIF":11.7,"publicationDate":"2020-05-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/j.pquantelec.2020.100264","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"2620890","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":1,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2020-03-01DOI: 10.1016/j.pquantelec.2020.100247
K.H. Li, W.Y. Fu, H.W. Choi
Blue LEDs and HEMTs based on III-Nitride have been flourishing commercially across the globe, thanks largely to breakthroughs in the material quality of the wide-bandgap compound semiconductor back in the 1990s. The realizations of white-light LEDs, blu-ray systems, and lately efficient compact chargers have drastically changed the way we live and have contributed tremendously to global energy saving efforts. The maturity and diversity of modern discrete GaN-based devices open up opportunities for an integrated GaN platform with extended functionalities and applications. In this review paper, we present an overview of the monolithic and heterogeneous integration of GaN devices and components. Various methods for the integration of electronic, optoelectronic, and optical components based on GaN are discussed.
{"title":"Chip-scale GaN integration","authors":"K.H. Li, W.Y. Fu, H.W. Choi","doi":"10.1016/j.pquantelec.2020.100247","DOIUrl":"https://doi.org/10.1016/j.pquantelec.2020.100247","url":null,"abstract":"<div><p><span>Blue LEDs<span><span> and HEMTs based on III-Nitride have been flourishing commercially across the globe, thanks largely to breakthroughs in the material quality of the wide-bandgap compound semiconductor back in the 1990s. The realizations of white-light LEDs, blu-ray systems, and lately efficient compact chargers have drastically changed the way we live and have contributed tremendously to global energy saving efforts. The maturity and diversity of modern discrete GaN-based devices open up opportunities for an integrated GaN platform with extended functionalities and applications. In this review paper, we present an overview of the monolithic and heterogeneous integration of GaN devices and components. Various methods for the integration of electronic, </span>optoelectronic, and </span></span>optical components based on GaN are discussed.</p></div>","PeriodicalId":414,"journal":{"name":"Progress in Quantum Electronics","volume":"70 ","pages":"Article 100247"},"PeriodicalIF":11.7,"publicationDate":"2020-03-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/j.pquantelec.2020.100247","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"2164454","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":1,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2020-01-01DOI: 10.1016/j.pquantelec.2019.100237
Lam Anh Bui
This paper reviews the field of microwave photonics instantaneous frequency measurements (IFM). It aims to consolidate the literature, explains the key implementations and reviews the recent developments. Current photonic IFMs are capable of operating over a wide bandwidth with a good resolution. However, their implementations are often based on discrete components and exhibit limited dynamic range and moderate efficiency. Photonic integration and improvements of dynamic range and efficiency are thus necessary, and they are anticipated as the future research directions and developments.
{"title":"Recent advances in microwave photonics instantaneous frequency measurements","authors":"Lam Anh Bui","doi":"10.1016/j.pquantelec.2019.100237","DOIUrl":"https://doi.org/10.1016/j.pquantelec.2019.100237","url":null,"abstract":"<div><p>This paper reviews the field of microwave photonics<span> instantaneous frequency measurements (IFM). It aims to consolidate the literature, explains the key implementations and reviews the recent developments. Current photonic IFMs are capable of operating over a wide bandwidth with a good resolution. However, their implementations are often based on discrete components and exhibit limited dynamic range and moderate efficiency. Photonic integration and improvements of dynamic range and efficiency are thus necessary, and they are anticipated as the future research directions and developments.</span></p></div>","PeriodicalId":414,"journal":{"name":"Progress in Quantum Electronics","volume":"69 ","pages":"Article 100237"},"PeriodicalIF":11.7,"publicationDate":"2020-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/j.pquantelec.2019.100237","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"2620893","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":1,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2020-01-01DOI: 10.1016/j.pquantelec.2019.100246
M.D. Dawson (Editor-in-Chief), D.P. Tsai (Editor), H. Jelinkova (Editor), M. Kim (Editor), Z. Mi (Editor)
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