Light-Emitting Diodes Second Edition
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Fundamentals of Microelectronics Chapter 3 Diode Circuits
9/17/2010 Fundamentals of Microelectronics CH1 Why Microelectronics? CH2 Basic Physics of Semiconductors CH3 Diode Circuits CH4 Physics of Bipolar Transistors CH5 Bipolar Amplifiers CH6 Physics of MOS Transistors CH7 CMOS Amplifiers CH8 Operational Amplifier As A Black Box 1 Chapter 3 Diode Circuits 3.1 Ideal Diode 3.2 PN Junction as a Diode 3.3 Applications of Diodes 2 1 9/17/2010 Diode Circuits After we have studied in detail the physics of a diode, it is time to study its behavior as a circuit element and its many applications. CH3 Diode Circuits 3 Diode’s Application: Cell Phone Charger An important application of diode is chargers. Diode acts as the black box (after transformer) that passes only the positive half of the stepped-down sinusoid. CH3 Diode Circuits 4 2 9/17/2010 Diode’s Action in The Black Box (Ideal Diode) The diode behaves as a short circuit during the positive half cycle (voltage across it tends to exceed zero), and an open circuit during the negative half cycle (voltage across it is less than zero). CH3 Diode Circuits 5 Ideal Diode In an ideal diode, if the voltage across it tends to exceed zero, current flows. It is analogous to a water pipe that allows water to flow in only one direction. CH3 Diode Circuits 6 3 9/17/2010 Diodes in Series Diodes cannot be connected in series randomly. For the circuits above, only a) can conduct current from A to C. CH3 Diode Circuits 7 IV Characteristics of an Ideal Diode V V R = 0⇒ I = = ∞ R = ∞⇒ I = = 0 R R If the voltage across anode and cathode is greater than zero, the resistance of an ideal diode is zero and current becomes infinite. -
The Art of Electronics
VOLTAGE REGULATORS AND POWER CIRCUITS 312 Chapter 6 (unregulated) I 3A fuse 3 + heat Figure 6.5. Five volt regulator with outboard pass transistor and crowbar. and the 33 ohm resistor. Its func- fuse somewhere in the power supply, as tion is to short the output if some circuit shown. We will treat overvoltage crowbar fault causes the output voltage to exceed circuits in more detail in Section 6.06. about 6.2 volts (this could happen if one of the resistors in the divider were to open up, for instance, or if some component in the HEAT AND POWER DESIGN 723 were to fail). is an SCR controlled rectifier), a device that is nor- 6.04 Power transistors and heat sinking mally nonconducting but that goes into saturation when the gate-cathode junction As in the preceding circuit, it is often nec- is forward-biased. Once turned on, it will essary to use power transistors or other not turn off again until anode current is re- high-current devices like or power moved externally. In this case, gate current rectifiers that can dissipate many watts. flows when the output exceeds The an inexpensive power tran- voltage plus a diode drop. When that hap- sistor of great popularity, can dissipate as pens, the regulator will go into a much as 1 15 watts if properly mounted. limiting condition, with the output held All power devices are packaged in cases near ground by the SCR. If the failure that that permit contact between a metal sur- produces the abnormally high output also face and an external heat sink. -
Compact Fluorescent Light Bulbs
Compact Fluorescent Light Bulbs What is a compact fluorescent lamp (CFL) bulb? A CFL bulb is a type of fluorescent bulb that screws into a standard light socket, such as a lamp or ceiling light fixture. CFLs use much less energy and last up to 10 times longer than standard light bulbs. What is in a compact fluorescent lamp (CFL) bulb? A CFL bulb is made of glass, a ceramic and metal base, a luminous powder called phosphor, and a small amount of mercury. How much mercury is contained in a CFL bulb? Manufacturers report that the amount of mercury contained in a CFL bulb is five milligrams, which is less than two ten-thousandths of an ounce. The mercury could be in the form of an invisible vapor or in a bead the size of the period at the end of this sentence. A mercury fever thermometer contains about 100 times more mercury than a CFL bulb. Is it harmful is it to be in the room where a CFL bulb has broken? The amount of mercury vapor that is released from one broken bulb is not enough to make anyone sick. However, it is best to avoid any exposure to mercury. We recommend that you ventilate the room air to the outdoors by opening a window or a door and leave the room for a few hours before cleaning up the broken bulb. How should I clean up a broken CFL bulb? It is not necessary to hire a professional to clean up the bulb. By following the directions below, you can safely clean up a broken CFL bulb. -
M7 Electroluminescence of Polymers
Universität Potsdam Institute of Physics and Astronomy Advanced Physics Lab Course March 2020 M7 ELECTROLUMINESCENCE OF POLYMERS I. INTRODUCTION The recombination of holes and electrons in a luminescent material can produce light. This emitted light is referred to as electroluminescence (EL) and was discovered in organic single crystals by Pope, Magnante, and Kallmann in 1963.[1] EL from conjugated polymers was first reported by Burroughes et al.[2] The polymer used was poly(p-phenylenevinylene) (PPV). Since then, a variety of other polymers has been investigated. Organic EL devices have applications in a wide field ranging from multi-color displays and optical information processing to lighting. Polymers have the advantage over inorganic and monomolecular materials in the ease with which thin, structurally robust and large area films can be perpared from solutions. Using printing techniques, patterned structures can be produced easily. Even flexible displays can be produced because of the good mechanical properties of polymers. In this lab course, basic optical and electrical properties of conjugated polymers will be investigated. Advanced Lab Course: Electroluminescence of Polymers 2 EXPERIMENTAL TASKS Measure the absorption spectra of your polymers (thin films spin coated onto glass substrates). Characterize the setup used for luminescence measurements. Identify possible sources of error and collect data necessary for their correction. Measure the photoluminescence emission spectra for the polymer films, using suitable excitation wavelengths. Measure the photoluminescence excitation spectra for the polymer films, using suitable detection wavelengths. Measure the current through the OLEDs and the spectral radiant intensity of electroluminescence as a function of applied voltage (the current-radiance-voltage characteristics). -
Light Sources and Photodetectors for OBS® Sensors Application Note
APPLICATION NOTE APPLICATION App. Note Code: 2Q-R Written by John Downing Light Sources and Photo- detectors for OBS® Sensors ® CAMPBELL SCIENTIFIC, INC. WHENW H E N MEASUREMENTSM E A S U R E M E N T S MMATTERA T T E R Copyright (C) April 2008 Campbell Scientifi c, Inc. Light Sources and Photodetectors for OBS® Sensors Sensors that use the OBS® method have narrow- or intermediate-band illumination systems, depending on whether a laser diode (LD) or infrared-emitting diode (IRED) is used in their construction. This application note describes infrared-emitting diodes and laser diodes, as well as photodiodes, daylight fi lters, and operating spectra. Laser Diodes Laser diodes have narrow, multimode emission spectra resembling the one shown in Figure 1. The LD bandwidth is about 2 nm at half power (FWHM). They have built-in photodiodes to monitor the light output of the laser chip so that photocur- rent can be used to control the illumination of the sample. In this way, fluctuations in light power caused by sensor temperature and laser aging are virtually elimi- nated. The drift of our OBS-4 LD-based sensor, for example, is less than 2% per year of continuous operation. The two disadvantages of lasers are that they emit coherent light, which because of interferences can fluctuate in intensity in a sample volume by as much as 50%, and they are less efficient in converting electrical current to light than IREDs. Figure 1. Graph shows the relative power, transmission and responsivity of a laser diode. Laser diodes have narrow, multimode emission spectra. -
Induction in Alocasia Macrorrhiza' Received for Publication December 8, 1987 and in Revised Form March 18, 1988
Plant Physiol. (1988) 87, 818-821 0032-0889/88/87/081 8/04/$0 1.00/0 Gas Exchange Analysis of the Fast Phase of Photosynthetic Induction in Alocasia macrorrhiza' Received for publication December 8, 1987 and in revised form March 18, 1988 MIKO U. F. KIRSCHBAUM2 AND ROBERT W. PEARCY* Department ofBotany, University ofCalifornia, Davis, California 95616 ABSTRACT and Pearcy (10) used gas exchange techniques to investigate the slow phase of induction from about 1 to 45 min. These studies When leaves ofAlocasia macrorrhiza that had been preconditioned in indicated that there might also be a fast phase of induction that 10 micromoles photons per square meter per second for at least 2 hours is complete within the first minute after an increase in PFD. This were suddenly exposed to 500 micromoles photons per square meter per fast induction phase is difficult to analyze with gas exchange second, there was an almost instantaneous increase in assimilation rate. techniques because instrument response times are typically so After this initial increase, there was a secondary increase over the next slow as to obscure the underlying plant response. In the present minute. This secondary increase was more pronounced in high CO2 (1400 study, measurements of the induction response were made in a microbars), where assimilation rate was assumed to be limited by the gas-exchange system modified to resolve very fast responses. This rate of regeneration of ribulose 1,5-bisphosphate (RuBP). It was absent investigation of the fast induction phase extends our work done in low CO2 (75 microbars), where RuBP carboxylase/oxygenase (Rub- previously on the dynamics of photosynthesis of the Australian isco) was assumed to be limiting. -
Iii-Nitride Ultraviolet Light-Emitting Diodes: Approaches for the Enhanced Efficiency
Copyright Warning & Restrictions The copyright law of the United States (Title 17, United States Code) governs the making of photocopies or other reproductions of copyrighted material. Under certain conditions specified in the law, libraries and archives are authorized to furnish a photocopy or other reproduction. One of these specified conditions is that the photocopy or reproduction is not to be “used for any purpose other than private study, scholarship, or research.” If a, user makes a request for, or later uses, a photocopy or reproduction for purposes in excess of “fair use” that user may be liable for copyright infringement, This institution reserves the right to refuse to accept a copying order if, in its judgment, fulfillment of the order would involve violation of copyright law. Please Note: The author retains the copyright while the New Jersey Institute of Technology reserves the right to distribute this thesis or dissertation Printing note: If you do not wish to print this page, then select “Pages from: first page # to: last page #” on the print dialog screen The Van Houten library has removed some of the personal information and all signatures from the approval page and biographical sketches of theses and dissertations in order to protect the identity of NJIT graduates and faculty. ABSTRACT III-NITRIDE ULTRAVIOLET LIGHT-EMITTING DIODES: APPROACHES FOR THE ENHANCED EFFICIENCY by Moulik Patel III-nitride ultraviolet (UV) light-emitting diodes (LEDs) offer marvelous potential for a wide range of applications, including air/water purification, surface disinfection, biochemical sensing, cancer cell elimination, and many more. III-nitride semiconductor alloys, especially AlGaN and AlInN, have drawn significant attention due to their significant advantages that include environmental-friendly material composition, compact in size, longer lifetime, low power consumption, and tunable optical emission. -
Modelling Transitions in Consumer Lighting — Consequences of the E.U
Modelling Transitions in Consumer Lighting — Consequences of the E.U. ban on light bulbs Maarten Afman Energy & Industry section Infrastructure Systems & Services Faculty of Technology, Policy and Management Delft University of Technology Modelling Transitions in Consumer Lighting — Consequences of the E.U. ban on light bulbs M.Sc. Thesis ‘Final version d.d. 4th February 2010’ Maarten Afman Graduation committee: Prof.dr.ir. M.P.C. Weijnen (chair; TU Delft, Energy & Industry section ) Dr.ir. G.P.J. Dijkema (first supervisor; TU Delft, Energy & Industry section) Dr.ir. C. van Daalen (second supervisor; TU Delft, Policy Analysis section) ir. E.J.L. Chappin (daily supervisor; TU Delft, Energy & Industry section) dr. W. Jager (external supervisor; University of Groningen, Marketing department) Programme SEPAM – Systems Engineering, Policy Analysis and Management Graduation Delft, 18th February 2010 Address M.R. Afman, v.d. Heimstr. 55, 2613EA Delft, The Netherlands E-mail addr. [email protected] Student no. 9006424 Energy & Industry section Infrastructure Systems & Services Faculty of Technology, Policy and Management Delft University of Technology Summary The need for a ban on bulbs? Energy consumption of the residential lighting sector is high: 3.8 TWh per year for the Netherlands alone, approximately the production of a power plant of 800 MW. Consequently, if 40% of the energy consumption for consumer lighting could be saved, a 320 MW power plant could be taken off the grid. Such a saving would be realistic if consumers would not rely so much on outdated and inefficient lighting technology, i.e. the standard incandescent light bulb and halogen lighting. -
Article Soot Photometer Using Supervised Machine Learning
Atmos. Meas. Tech., 12, 3885–3906, 2019 https://doi.org/10.5194/amt-12-3885-2019 © Author(s) 2019. This work is distributed under the Creative Commons Attribution 4.0 License. Classification of iron oxide aerosols by a single particle soot photometer using supervised machine learning Kara D. Lamb1,2 1Cooperative Institute for Research in Environmental Sciences, University of Colorado Boulder, Boulder, CO, USA 2NOAA Earth System Research Laboratory Chemical Sciences Division, Boulder, CO, USA Correspondence: Kara D. Lamb ([email protected]) Received: 15 March 2019 – Discussion started: 22 March 2019 Revised: 20 June 2019 – Accepted: 21 June 2019 – Published: 15 July 2019 Abstract. Single particle soot photometers (SP2) use laser- each class are compared with the true class for those particles induced incandescence to detect aerosols on a single particle to estimate generalization performance. While the specific basis. SP2s that have been modified to provide greater spec- class approach performed well for rBC and Fe3O4 (≥ 99 % tral contrast between their narrow and broad-band incandes- of these aerosols are correctly identified), its classification of cent detectors have previously been used to characterize both other aerosol types is significantly worse (only 47 %–66 % refractory black carbon (rBC) and light-absorbing metallic of other particles are correctly identified). Using the broader aerosols, including iron oxides (FeOx). However, single par- class approach, we find a classification accuracy of 99 % for ticles cannot be unambiguously identified from their incan- FeOx samples measured in the laboratory. The method al- descent peak height (a function of particle mass) and color lows for classification of FeOx as anthropogenic or dust-like ratio (a measure of blackbody temperature) alone. -
Semiconductor Light Sources
Laser Systems and Applications Couse 2020-2021 Semiconductor light sources Prof. Cristina Masoller Universitat Politècnica de Catalunya [email protected] www.fisica.edu.uy/~cris SCHEDULE OF THE COURSE Small lasers, biomedical Semiconductor light sources lasers and applications . 1 (11/12/2020) Introduction. 7 (19/1/2021) Small lasers. Light-matter interactions. 8 (22/1/2021) Biomedical lasers. 2 (15/12/2020) LEDs and semiconductor optical amplifiers. Laser models . 3 (18/12/2020) Diode lasers. 9 (26/1/2021) Laser turn-on and modulation response. Laser Material Processing . 10 (29/1/2021) Optical injection, . 4 (22/12/2020) High power laser optical feedback, polarization. sources and performance improving novel trends . 11 (2/2/2021) Students’ . 5 (12/1/2021) Laser-based presentations. material macro processing. 12 (5/2/2021) Students’ . 6 (15/1/2020) Laser-based presentations. material micro processing. 9/2/2021: Exam Lecturers: C. Masoller, M. Botey 2 Learning objectives . Understand the physics of semiconductor materials and the electron-hole recombination mechanisms that lead to the emission of light. Learn about the operation principles of light emitting diodes (LEDs) and semiconductor optical amplifiers (SOAs). Become familiar with the operation principles and characteristics of laser diodes (LDs). 3 Outline: Semiconductor light sources . Introduction . Light-matter interactions in semiconductor materials . Light Emitting Diodes (LEDs) . Semiconductor optical amplifiers (SOAs) . Laser diodes (LDs) The start of the laser diode story: the invention of the transistor Nobel Prize in Physics 1956 “For their research on semiconductors and their discovery of the transistor effect”. The invention of the transistor in 1947 lead to the development of the semiconductor industry (microchips, computers and LEDs –initially only green, yellow and red). -
Introduction 1
1 1 Introduction . ex arte calcinati, et illuminato aeri [ . properly calcinated, and illuminated seu solis radiis, seu fl ammae either by sunlight or fl ames, they conceive fulgoribus expositi, lucem inde sine light from themselves without heat; . ] calore concipiunt in sese; . Licetus, 1640 (about the Bologna stone) 1.1 What Is Luminescence? The word luminescence, which comes from the Latin (lumen = light) was fi rst introduced as luminescenz by the physicist and science historian Eilhardt Wiede- mann in 1888, to describe “ all those phenomena of light which are not solely conditioned by the rise in temperature,” as opposed to incandescence. Lumines- cence is often considered as cold light whereas incandescence is hot light. Luminescence is more precisely defi ned as follows: spontaneous emission of radia- tion from an electronically excited species or from a vibrationally excited species not in thermal equilibrium with its environment. 1) The various types of lumines- cence are classifi ed according to the mode of excitation (see Table 1.1 ). Luminescent compounds can be of very different kinds: • Organic compounds : aromatic hydrocarbons (naphthalene, anthracene, phenan- threne, pyrene, perylene, porphyrins, phtalocyanins, etc.) and derivatives, dyes (fl uorescein, rhodamines, coumarins, oxazines), polyenes, diphenylpolyenes, some amino acids (tryptophan, tyrosine, phenylalanine), etc. + 3 + 3 + • Inorganic compounds : uranyl ion (UO 2 ), lanthanide ions (e.g., Eu , Tb ), doped glasses (e.g., with Nd, Mn, Ce, Sn, Cu, Ag), crystals (ZnS, CdS, ZnSe, CdSe, 3 + GaS, GaP, Al 2 O3 /Cr (ruby)), semiconductor nanocrystals (e.g., CdSe), metal clusters, carbon nanotubes and some fullerenes, etc. 1) Braslavsky , S. et al . ( 2007 ) Glossary of terms used in photochemistry , Pure Appl. -
Application Note AN-1057
Application Note AN-1057 Heatsink Characteristics Table of Contents Page Introduction.........................................................................................................1 Maximization of Thermal Management .............................................................1 Heat Transfer Basics ..........................................................................................1 Terms and Definitions ........................................................................................2 Modes of Heat Transfer ......................................................................................2 Conduction..........................................................................................................2 Convection ..........................................................................................................5 Radiation .............................................................................................................9 Removing Heat from a Semiconductor...........................................................11 Selecting the Correct Heatsink........................................................................11 In many electronic applications, temperature becomes an important factor when designing a system. Switching and conduction losses can heat up the silicon of the device above its maximum Junction Temperature (Tjmax) and cause performance failure, breakdown and worst case, fire. Therefore the temperature of the device must be calculated not to exceed the Tjmax. To design a good