VCSEL Pulse Driver Designs for Tof Applications
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UCC27531 35-V Gate Driver for Sic MOSFET Applications (Rev. A)
(1) Application Report SLUA770A–March 2016–Revised May 2018 UCC27531 35-V Gate Driver for SiC MOSFET Applications Richard Herring........................................................................................... High Power Driver Solutions ABSTRACT SiC MOSFETs are gaining popularity in many high-power applications due to their significant switching performance advantages. SiC MOSFETs are also available with attractive voltage ratings and current capabilities. However, the characteristics of SiC MOSFETs require consideration of the gate-driver circuit to optimize the switching performance of the SiC device. Although SiC MOSFETs are not difficult to drive properly, many typical MOSFET drivers may result in compromised switching speed performance. The UCC27531 gate driver includes features and has operating parameters that allow for driving SiC power MOSFETs within the recommended optimum drive configuration. This application note reviews the characteristics of SiC MOSFETs and how to drive them to achieve the performance improvement that SiC can bring at the system level. The features of UCC27531 to achieve optimal performance of SiC are explained and results from a demonstration circuit are provided. 1 Introduction In the past, the majority of applications such as uninterruptible power supplies (UPS), photovoltaic (PV) inverters, and motor drive have utilized IGBTs for the power devices due to the combination of high- voltage ratings exceeding 1 kV and high current capability. Usable switching frequency of IGBTs has typically been limited to 20–30 kHz, due to the high turnoff losses caused by the long turnoff current tail. Design comparisons have shown that SiC MOSFET designs can operate at considerably higher switching frequency and achieve the same or better efficiency. Although the device cost of the SiC MOSFETs are higher than the equivalent IGBTs, the significant savings in transformer, capacitor, and enclosure size results in a lower system cost. -
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. -
Egan® Ics for Low Voltage DC-DC Applications Egan® Ics for Low Voltage DC-DC Applications EFFICIENT POWER CONVERSION
APPLICATION NOTE: AN025 eGaN® ICs for Low Voltage DC-DC Applications eGaN® ICs for Low Voltage DC-DC Applications EFFICIENT POWER CONVERSION Michael de Rooij, Ph.D., Vice President of Applications Engineering , Yuanzhe Zhang, Ph.D., Director of Applications Engineering eGaN® FETs from EPC have repeatedly demonstrated higher performance over Monolithic integration of the gate driver to the MOSFET counterparts in many applications [1]. The lateral structure and material FET offers the lowest possible common source properties of eGaN FETs make it possible to monolithically integrate a number of FETs inductance (CSI) as it is moved to within the as demonstrated by products such as the EPC2107 [2]. The next phase in the eGaN IC structure. Furthermore the gate driver has been optimized for the FET being driven to offer FET and IC evolution includes gate driver integration. Integrating the gate driver with maximum performance under any operating the FET offers a number of additional advantages over discrete gate driver and FET condition. These benefits are on top of the well- solutions such as extremely low common source inductance, matched gate driver established low capacitance and inductance, and to FET, and ease of design. All the traditional eGaN FET benefits such as significantly zero reverse recovery charge (QRR) that enable lower capacitance and inductance with zero reverse recovery charge (QRR) in a smaller efficient operation at high switching frequencies even under hard switching conditions. The key footprint for a given on-resistance (RDS(on)) than comparable MOSFETs are retained. However, the combined effect of the new characteristics and benefits ensures an ever characteristics of the EPC2112 are given in table 1. -
Resonant Gate-Drive Circuits for High-Frequency Power Converters
Resonant Gate-Drive Circuits for High-Frequency Power Converters A dissertation submitted in partial fulfillment of the requirements for the degree of Doctor of Philosophy By Hur Jedi B. S., University of Baghdad, Baghdad, Iraq, 2003 M. S., University Putra Malaysia, Selangor, Malaysia, 2010 2018 Wright State University WRIGHT STATE UNIVERSITY GRADUATE SCHOOL November 16, 2018 I HEREBY RECOMMEND THAT THE DISSERTATION PREPARED UNDER MY SUPERVISION BY Hur Jedi ENTITLED Resonant Gate-Drive Circuits for High-Frequency Power Converters BE ACCEPTED IN PARTIAL FULFILLMENT OF THE REQUIREMENTS FOR THE DEGREE OF Doctor of Philosophy. Marian K. Kazimierczuk, Ph.D. Dissertation Director Arnab Shaw, Ph.D. Director, Electrical Engineering Ph.D. Program Barry Milligan, Ph.D. Interim Dean of the Graduate School Committee on Final Examination Marian K. Kazimierczuk, Ph.D. Ray Siferd, Ph.D. Henry Chen, Ph.D. Saiyu Ren, Ph.D. Yan Zhuang, Ph.D. Abstract Jedi, Hur. Ph.D., Electrical Engineering Ph.D. Program, Department of Electrical Engineering, Wright State University, 2018. Resonant Gate-Drive Circuits for High- Frequency Power Converters. The development trend of power converters motivates the pursuit with high den- sity, high efficiency, and low cost. Increasing the frequency can improve the power density and lead to small passive elements and a fast dynamic response. Each one of these power converters must be driven by a gate-drive circuit to operate efficiently. Conventional gate-drivers are used up to frequencies of about 5 MHz and suffer from switching losses. Therefore, the development of switch-mode power supplies (SMPS) operating at high frequencies requires high-speed gate drivers. -
Igbts (Insulated Gate Bipolar Transistor) Application Note
IGBTs (Insulated Gate Bipolar Transistor) Application Note IGBTs (Insulated Gate Bipolar Transistor) Description This document describes the basic structures, ratings, and electrical characteristics of IGBTs. It also provides usage considerations for IGBTs. © 2018 1 2018-09-01 Toshiba Electronic Devices & Storage Corporation IGBTs (Insulated Gate Bipolar Transistor) Application Note Table of Contents Description ............................................................................................................................................ 1 Table of Contents ................................................................................................................................. 2 1. Device structure and characteristics of IGBTs ............................................................................. 6 1.1. Basic structure of the IGBT ................................................................................................................ 6 1.2. Comparison of different types of transistors (bipolar transistors, MOSFETs, and IGBTs) ....... 8 2. Different types of IGBTs and their structures ............................................................................ 11 2.1. Gating structures ................................................................................................................................11 2.2. IGBT classification based on the vertical structure ...................................................................... 12 2.2.1. Punch-through (PT) IGBTs ................................................................................................................12 -
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). -
Operating the Pulsed Laser Diode SPL LL90 3 Application Note
Operating the Pulsed Laser Diode SPL LL90_3 Application Note Introduction Optical peak power The SPL LL90_3 is a hybrid laser module. As shown in figure 2 the peak current and Additional to the laser chip the module therefore optical peak power is adjusted by contains two capacitors and a MOSFET the applied charge voltage. The SPL LL90_3 which act as a driver stage. The two typically delivers 70 W at 18.5 V (30 ns, 1 capacitors are connected in parallel to sum kHz). their individual capacitance of 47 nF. The The maximum rating of peak power is 80 W. emission wavelength is 905 nm. The By increasing of pulse repetition frequency specified optical peak power is 70 W. the peak optical power will be slightly decreased (as shown in fig 2). Principal of operation The capacitors are charged using a constant DC voltage. Each time the gate of the MOSFET is triggered, the capacitors are discharged via the laser chip leading to a short and high-amp current pulse. These high-amp current pulses are required to obtain the high peak power laser emission (at charge voltage of 18.5V a current pulse of up to 30A is possible) The pin configuration of the SPL LL90_3 laser diode is as follows: Pin 1: Trigger signal for the MOSFET gate Pin 2: Charge voltage Pin 3: Ground Figure 1: Hybrid pulsed laser diode SPL Variation of optical peak power LL90_3 with integrated driver stage. Figure 2: with charge voltage (pulse width 30 ns, PRF 1 kHz and 25kHz, gate voltage 15 V) for SPL LL90_3 using the MOSFET driver 3 Elantec EL7104C. -
Speed of Light with Nanosecond Pulsed 650 Nm Diode Laser M
Speed of Light with Nanosecond Pulsed 650 nm Diode Laser M. Gallant May 23, 2008 The speed of light has been measured many different ways using many ingenious methods. The following note describes a method which is conceptually very easy to understand and fairly easy to implement. The technique is the simple time-of-flight optical pulse delay method using a fairly short (nanosecond) optical pulse and an oscilloscope with bandwidth between 50 - 100 MHz. THE LASER Common low power laser pointers, typically emit at a wavelength of 650 nm and operate from two to four 1.5 V button cells. Many of these lasers can be easily extracted from the pointer assembly and pulse-modulated to several hundred megahertz. The laser used here was removed from a low power (< 5mW) laser pointer assembly from a popular retail outlet. GENERATION OF SHORT OPTICAL PULSES The laser is prebiased below threshold, at 5 - 10 mA current (threshold current for the laser used here is 24 mA) using an inductor as a bias insertion element. A short (< 5 ns) electrical pulse modulates the laser. Since a very low duty cycle is used for pulsing the laser, fairly high current pulses are possible without degrading the laser. The actual forward current and voltage achieved during the drive pulse are dependent on the details of the I-V characteristic of the specific laser used, but are typically in the range of 50 - 100 mA and 6 - 10 V respectively. The short electrical pulse is generated using a simple avalanche transistor circuit. Due to the high frequency content of the short pulse, the actual shape of the current pulse driving the laser will depend on the circuit components (series resistors etc.) and parasitic electrical effects (series inductance of connection wires etc.) The circuit has been described by Jim Williams in a Linear Technology Measurement and Control Circuit Collection and has many other uses. -
PLD-92 Laser Diode Datasheet
PLD-92 Series: 915-970 nm, 80 W Multi-mode Fiber-coupled Diode Lasers Features Amplifier Pumping Direct Diode Lasers 915, 940, 970 nm Center Wavelength Stabilization Laser Pumping Material Processing Wavelengths and Dichroic Options Graphic Arts / Printing Medical & Dental 80 W Output Power 0.15 NA into 110 μm Fiber Core Diameter Illumination Photovoltaics High Reliability Robust Compact Package IPG Photonics’ PLD-92 fiber-coupled diode lasers provide up to 80 W of output power within 0.15 NA. PLD-92 diode are provided with a 110 μm fiber core and center wavelengths at 915 nm, 940 nm or 970 nm. Wavelength stabilization and dichroic options are also available. IPG’s best-in-class diode technology offers an ideal combination of power, reliability and form factor. We manufacture to rigorous telecom-grade standards in the world’s largest high power diode fab. Each wafer is individually qualified, which sets IPG apart from alternative industrial pump products using short-lived diode bars and bar-stack technologies. PLD-92 diode lasers are preferred for fiber amplifier and laser pumping, material processing, and direct diode applications. PLD-92 Series: 915-970 nm, 80 W Multi-mode Fiber-coupled Diode Lasers Optical and Electrical Characteristics* PLD-92 Center Wavelength**, nm 971 Center Wavelength Tolerance, nm ± 5 Output Power, W 80 Spectral Width (FWHM), nm 4 Slope Efficiency, W/A 5 Minimum Efficiency, % 52 Threshold Current (ITH), A 0.8 Operating Current (IOP), A 16 Forward Voltage, V 9.3 Recommended Case Temperature, ⁰C 25 Wavelength Shift with Temperature, nm/⁰C 0.35 Wavelength Shift with Operating Current, nm/A 0.6 *Typical performance data measured at 16 A, 25⁰C. -
LM3445 Triac Dimmable Offline LED Driver
LM3445 Triac Dimmable Offline LED Driver February 19, 2010 LM3445 Triac Dimmable Offline LED Driver General Description Features The LM3445 is an adaptive constant off-time AC/DC buck ■ Triac dim decoder circuit for LED dimming (step-down) constant current controller designed to be com- ■ Application voltage range 80VAC – 277VAC patible with triac dimmers. The LM3445 provides a constant Capable of controlling LED currents greater than 1A current for illuminating high power LEDs and includes a triac ■ dim decoder. The dim decoder allows wide range LED dim- ■ Adjustable switching frequency ming using standard triac dimmers. The high frequency ca- ■ Low quiescent current pable architecture allows the use of small external passive ■ Adaptive programmable off-time allows for constant ripple components. The LM3445 includes a bleeder circuit to ensure current proper triac operation by allowing current flow while the line ■ Thermal shutdown voltage is low to enable proper firing of the triac. A passive No 120Hz flicker PFC circuit ensures good power factor by drawing current di- ■ rectly from the line for most of the cycle, and provides a ■ Low profile 10 pin MSOP Package or 14 pin SOIC constant positive voltage to the buck regulator. Additional ■ Patent pending drive architecture features include thermal shutdown, current limit and VCC un- der-voltage lockout. Applications ■ Retro Fit Triac Dimming ■ Solid State Lighting ■ Industrial and Commercial Lighting ■ Residential Lighting Typical LM3445 LED Driver Application Circuit 30060305 30060301 © 2010 National Semiconductor Corporation 300603 www.national.com Connection Diagrams LM3445 Top View Top View 30060303 10-Pin MSOP NS Package Number MUB10A 30060373 14-Pin SOIC NS Package Number M14A Ordering Information Order Number Spec. -
Fundamentals of MOSFET and IGBT Gate Driver Circuits
Application Report SLUA618A–March 2017–Revised October 2018 Fundamentals of MOSFET and IGBT Gate Driver Circuits Laszlo Balogh ABSTRACT The main purpose of this application report is to demonstrate a systematic approach to design high performance gate drive circuits for high speed switching applications. It is an informative collection of topics offering a “one-stop-shopping” to solve the most common design challenges. Therefore, it should be of interest to power electronics engineers at all levels of experience. The most popular circuit solutions and their performance are analyzed, including the effect of parasitic components, transient and extreme operating conditions. The discussion builds from simple to more complex problems starting with an overview of MOSFET technology and switching operation. Design procedure for ground referenced and high side gate drive circuits, AC coupled and transformer isolated solutions are described in great details. A special section deals with the gate drive requirements of the MOSFETs in synchronous rectifier applications. For more information, see the Overview for MOSFET and IGBT Gate Drivers product page. Several, step-by-step numerical design examples complement the application report. This document is also available in Chinese: MOSFET 和 IGBT 栅极驱动器电路的基本原理 Contents 1 Introduction ................................................................................................................... 2 2 MOSFET Technology ...................................................................................................... -
Driving Egantm Transistors for Maximum Performance
Driving eGaNTM Transistors for Maximum Performance Johan Strydom: Director of Applications, Efficient Power Conversion Corporation Alex Lidow: CEO, Efficient Power Conversion Corporation The recent introduction of enhancement mode MOSFET development, silicon has approached GaN transistors (eGaN™) as power MOSFET/ its theoretical limits. In contrast, GaN is young in IGBT replacements in power management its life cycle, and will see significant improvement applications enables many new products that in the years to come. promise to add great system value. In general, an eGaN transistor behaves much like a power MOSFET with a quantum leap in performance, but to extract all of the newly-available eGaN transistor performance requires designers to understand the differences in drive requirements. eGaN Power Transistor Characteristics As with silicon power MOSFETs, applying a positive bias to the gate relative to the source of an eGaN power transistor causes a field effect, which attracts electrons that complete a Figure 1. Theoretical resistance times die area limits of GaN, silicon, and silicon carbide versus voltage. bidirectional channel between the drain and the source. When the bias is removed from the gate, the electrons under it are dispersed into the GaN, Figure of Merit (FOM) recreating the depletion region and, once again, giving it the capability to block voltage. The FOM is a useful method for comparing power devices and has been used by MOSFET To obtain a higher-voltage device, the distance manufactures to show both generational between the drain and gate is increased. Doing improvements and to compare their parts to so increases the on-resistance of the transistor.