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)
{"title":"Special thanks to Professor Jagadish and an introduction to the new editorial team","authors":"M.D. Dawson (Editor-in-Chief), D.P. Tsai (Editor), H. Jelinkova (Editor), M. Kim (Editor), Z. Mi (Editor)","doi":"10.1016/j.pquantelec.2019.100246","DOIUrl":"https://doi.org/10.1016/j.pquantelec.2019.100246","url":null,"abstract":"","PeriodicalId":414,"journal":{"name":"Progress in Quantum Electronics","volume":"69 ","pages":"Article 100246"},"PeriodicalIF":11.7,"publicationDate":"2020-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/j.pquantelec.2019.100246","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"2620892","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 : 2019-11-01DOI: 10.1016/j.pquantelec.2019.100228
A. Rogalski, P. Martyniuk, M. Kopytko
The development of the HgCdTe alloy as the most important intrinsic semiconductor for infrared (IR) technology is well established and recognized. In spite of the achievements in material and device quality, the drawbacks still exist due to bulk and surface instability, lower yields and higher costs particularly in fabrication of long wavelength infrared arrays. The difficulties with this material encouraged to research on other compounds to improve device performance.
Since the first paper published by Sakaki and Esaki in 1978 it is well known that InAs and GaSb constitute a nearly lattice-matched material system offering great flexibility in the design of IR optoelectronic devices. After four decades, the III-V type-II superlattice (T2SL) detector technology is under strong development as a possible alternative to HgCdTe. The novel ideas coming in design of detectors have enhanced the position of T2SLs in IR materials detector technology. It appears that T2SLs are especially helpful in the design of unipolar barriers.
In this paper fundamental physical properties of two material systems, HgCdTe and T2SLs, are compared together with their influence on detector performance: dark current density, RA product, quantum efficiency, and noise equivalent different temperature. In comparison with HgCdTe, fundamental properties of T2SLs are inferior. On the other hand, T2SL and barrier detectors have several advantages to include lower tunnelling and surface leakage currents, and suppressed Auger recombination mechanism. Up to date, the promise of superior performance of these detectors has not been realized yet. In the paper we present that the performance of T2SL detectors (dark current, current responsivity, and noise equivalent difference temperature) is lower than bulk HgCdTe photodiodes.
Due to stronger, less ionic chemical bonding of III-V semiconductors, these materials are attractive due to manufacturability and stability. It is also predicted that the interband T2SL quantum cascade devices will outperform the performance of the high operating temperature HgCdTe detectors.
{"title":"Type-II superlattice photodetectors versus HgCdTe photodiodes","authors":"A. Rogalski, P. Martyniuk, M. Kopytko","doi":"10.1016/j.pquantelec.2019.100228","DOIUrl":"https://doi.org/10.1016/j.pquantelec.2019.100228","url":null,"abstract":"<div><p>The development of the HgCdTe alloy as the most important intrinsic semiconductor for infrared (IR) technology is well established and recognized. In spite of the achievements in material and device quality, the drawbacks still exist due to bulk and surface instability, lower yields and higher costs particularly in fabrication of long wavelength infrared arrays. The difficulties with this material encouraged to research on other compounds to improve device performance.</p><p><span>Since the first paper published by Sakaki and Esaki in 1978 it is well known that InAs and GaSb constitute a nearly lattice-matched material system offering great flexibility in the design of IR optoelectronic devices. After four decades, the III-V type-II </span>superlattice (T2SL) detector technology is under strong development as a possible alternative to HgCdTe. The novel ideas coming in design of detectors have enhanced the position of T2SLs in IR materials detector technology. It appears that T2SLs are especially helpful in the design of unipolar barriers.</p><p><span>In this paper fundamental physical properties of two material systems, HgCdTe and T2SLs, are compared together with their influence on detector performance: dark current density, </span><em>RA</em><span> product, quantum efficiency, and noise equivalent different temperature. In comparison with HgCdTe, fundamental properties of T2SLs are inferior. On the other hand, T2SL and barrier detectors have several advantages to include lower tunnelling and surface leakage currents, and suppressed Auger recombination mechanism. Up to date, the promise of superior performance of these detectors has not been realized yet. In the paper we present that the performance of T2SL detectors (dark current, current responsivity, and noise equivalent difference temperature) is lower than bulk HgCdTe photodiodes.</span></p><p>Due to stronger, less ionic chemical bonding of III-V semiconductors, these materials are attractive due to manufacturability and stability. It is also predicted that the interband T2SL quantum cascade devices will outperform the performance of the high operating temperature HgCdTe detectors.</p></div>","PeriodicalId":414,"journal":{"name":"Progress in Quantum Electronics","volume":"68 ","pages":"Article 100228"},"PeriodicalIF":11.7,"publicationDate":"2019-11-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/j.pquantelec.2019.100228","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"3386806","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}
Recent advances in the development of quantum dots (QDs) have offered new possibilities for the exploration of sensors, bio imaging, batteries, electrochemical water splitting and optoelectronic applications because of their intriguing optical, electrical, catalytic and electrochemical properties. Among QDs, atomically thin two-dimensional quantum dots (2D QDs) derived from graphene sheets, transition metal dichalcogenide (TMD) layers and phosphorene have been of considerable interest for the past few years. There have been several intensive studies of carbon QDs, but TMD QDs and heterostructures based on 2D QDs are rapidly advancing. Herein, the synthesis and properties of 2D QDs, particularly carbon and TMD QDs, are reviewed for the recent progress in their application toward electrochemical water splitting, photocatalytic wastewater treatment, supercapacitors, batteries and photodetectors. Moreover, the assembly of such 2D QDs to achieve industrial-scale production and boost their performance in widespread applications is emphasized.
{"title":"A critical review on two-dimensional quantum dots (2D QDs): From synthesis toward applications in energy and optoelectronics","authors":"Arumugam Manikandan , Yu-Ze Chen , Chih-Chiang Shen , Chin-Wei Sher , Hao-Chung Kuo , Yu-Lun Chueh","doi":"10.1016/j.pquantelec.2019.100226","DOIUrl":"https://doi.org/10.1016/j.pquantelec.2019.100226","url":null,"abstract":"<div><p><span><span>Recent advances in the development of quantum dots (QDs) have offered new possibilities for the exploration of sensors, bio imaging, batteries, electrochemical water splitting and </span>optoelectronic applications because of their intriguing optical, electrical, catalytic and electrochemical properties. Among QDs, atomically thin two-dimensional quantum dots (2D QDs) derived from graphene sheets, </span>transition metal dichalcogenide<span><span> (TMD) layers and phosphorene have been of considerable interest for the past few years. There have been several intensive studies of carbon QDs, but TMD QDs and </span>heterostructures<span> based on 2D QDs are rapidly advancing. Herein, the synthesis and properties of 2D QDs, particularly carbon and TMD QDs, are reviewed for the recent progress in their application toward electrochemical water splitting, photocatalytic wastewater treatment, supercapacitors<span>, batteries and photodetectors. Moreover, the assembly of such 2D QDs to achieve industrial-scale production and boost their performance in widespread applications is emphasized.</span></span></span></p></div>","PeriodicalId":414,"journal":{"name":"Progress in Quantum Electronics","volume":"68 ","pages":"Article 100226"},"PeriodicalIF":11.7,"publicationDate":"2019-11-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/j.pquantelec.2019.100226","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"3386804","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}