Applications of Resonance Raman Spectroscopy to the Study of Bioinorganic Macromolecules

Total Page:16

File Type:pdf, Size:1020Kb

Applications of Resonance Raman Spectroscopy to the Study of Bioinorganic Macromolecules Applications of resonance Raman spectroscopy to the study of bioinorganic macromolecules DISSERTATION Presented in Partial Fulfillment of the Requirements for the Degree Doctor of Philosophy in the Graduate School of The Ohio State University By Pearson T. Maugeri, B.S. Biophysics Graduate Program The Ohio State University 2017 Dissertation Committee: Professor Hannah S. Shafaat, Advisor Professor James A. Cowan Professor Terry L. Gustafson Professor Marcos Sotomayor © Copyright by Pearson T. Maugeri 2017 Abstract Transition metals are absolutely critical for the existence and maintenance of biologi- cal systems. Many cellular processes, such as metabolism, the detoxifying of harmful chemicals, gene regulation, and extracellular signaling rely on the unique properties that metal cofactors provide. One very important group of metalloproteins is the ferritin-like superfamily. The ferritin-like superfamily contains proteins that have a large array of functions, ranging from the storage and transport of essential nutri- ents such as iron and oxygen (ferritin and hemerythrin) to the 2-electron oxidation of the stable C-H bonds found in hydrocarbons (di-iron hydroxylases). Of particular interest are the ribonucleotide reductases, enzymes that catalyze the de novo syn- thesis of deoxyribonucleotides from ribonucleotides. Additionally, different classes of ribonucleotide reductases use dissimilar sets of metals to achieve similar end results. In 2009, a novel protein group called the R2-like ligand-binding oxidases, or R2lox, was discovered. The function of R2lox is not currently known, although it does do 2-electron chemistry, as seen by a novel Tyr-Val linkage that forms during the acti- vation of oxygen. This new class of proteins exhibits sequence similarity to the R2 subunit of the ribonucleotide reductases and is reminiscent of bacterial multicom- ponent monooxygenses (BMMs) in both the bound ligand and also its hypothesized chemistry. It has been shown that this protein is upregulated in the virulent strain of Mycobacterium tuberculosis, and therefore it is of great interest to uncover the role that this protein plays in its various hosts. ii There are many ways to study bioinorganic systems; however, one of the most ver- satile and sensitive techniques is spectroscopy. Many different wavelength regimes are able to be plied to furthering the understanding of bioinorganic systems. One of the most useful types of spectroscopy in a chemist’s toolbox is vibrational spectroscopy, due to the opportunity that it affords to extract structural information. One typeof vibrational spectroscopy is Raman scattering, which uses inelastically scattered pho- tons to report on the vibrational modes of a molecule. Furthermore, the resonance Raman phenomenon can and has been used to great effect in bioinorganic systems by tuning the Raman excitation beam to an electronic absorption, enhancing the signal and making resonance Raman spectroscopy a very useful tool for the study of bioinorganic structure and function. This thesis presents two main projects that are different in character. The first is the development of a custom variable wavelength resonance Raman experimental sys- tem. A brief background of resonance Raman scattering is presented before outlining the layout of the experimental setup. Collaborations with other research groups were also conducted, and the custom resonance Raman system was used to probe a wide range of bioinorganic systems. The other section of the thesis details experiments on R2lox. One chapter outlines the investigation of an unusual phenomenon where the optical properties of R2lox change drastically upon irradiation with light. The other chapter discusses setting up R2lox to be probed via transient absorption so that electron transfer constants may be extracted. iii For Charlene, my dearest love iv Acknowledgments No man is an island, Entire of itself, Every man is a piece of the continent, A part of the main. The above excerpt from John Donne’s 1623 work, Meditations XVII: Devotions upon Emergent Occasions, is an absolutely spot on summary of what my academic experience has been up to this point. I could not have done any of this without the firm and unyielding support that I have received from friends, family and fellow academics. I am truly not an island. First, I would like to acknowledge my advisor, Dr. Hannah Shafaat. She has provided an excellent model of scientific excellence to emulate. I would like to thank her for giving me the opportunity to work in her group and to assemble the custom resonance Raman system, which is detailed in chapter 3. I would also like to thank Dr. Dongping Zhong, in whose lab I gained a lot of my fundamental understanding of ultrafast laser systems as well as biological spectroscopy. In addition, thank you to my thesis committee, who sacrificed their time to give me good feedback on this document as well as on my research projects. Each of you have helped me grow as a scientist and I am very grateful for your mentorship. I would also like to thank my collaborators on the projects discussed in this work. Thank you to Dr. Cowan, Dr. Jingwei Li, and Stephen Pearson for collaborating with me on the project in chapter 6. To Dr. Thomas Rauchfuss and Michaela Carlson, v thank you for your collaboration on the project described in chapter 7. Thank you to Dr. Kyle Lancaster, Dr. John Caranto, and Avery Vilbert for the collaboration on the project described in chapter 8. Special thanks to Dr. Martin Högbom, Dr. Julia Griese, and Dr. Rui Branca for all of your help in running experiments in the study described in chapter 4, including providing mutants, as well as all of your helpful discussions regarding R2lox. Thank you to all for your contributions to this work. I would also like to thank my labmates in the Shafaat research group. Each and every one of you has affected my academic life for the better and I would not be here if it wasn’t for your influence. Thank you Tasha, for helping me to integrate intothis lab and for providing me with someone to bounce ideas off and for watching my dog on the rare occasions I got out of town. Thank you Jeff for all the discussions about Game of Thrones, and for all your help with the resonance Raman system. Thank you Cami for all your help with troubleshooting the labeling conditions in Chapter 5 and for our discussions on the pros and cons of OSU football. Thank you Shelby for helping me with my inorganic chemistry knowledge, especially with point groups, and for all our geeky conversations about video games. I would also like to thank Dr. Michael Stevenson, who provided me with an invaluable viewpoint of the academic process though the lens of a postdoctoral researcher. We will always have Akron. Thank you Sean for being a good TA partner when we taught CHEM 4310. You made teaching that class much more enjoyable. Thank you Effie for your help in all of the R2lox purification and experiments as well as for being a good officemate the past year despite my, shall we say, less than orderly desk. I will look back on all of our discussions about how finicky R2lox is with fondness. I have been blessed beyond measure to have been afforded the opportunity to work and grow scientifically with all of you during my time here. I would also like to thank my undergraduate professors at Harding University vi who nurtured my love for science. Thank you Dr. Stewart for teaching me how to think outside of the box and solve puzzles in organic synthesis. I have applied that skill to so many other things here at OSU. Thank you Dr. Matlock for taking time out of your day to speak with me about biochemistry and to help me transition to thinking in a more biophysical context. Finally, I would like to thank Dr. Murray, who was so patient with me when I was fumbling around in his upper-level physics courses and had no idea what I was doing. Thank you all for showing me that one can simultaneously be a scientist and a man of God. Finally, I would like to extend my boundless appreciation to family, who has listened to my joys and my frustrations for these last several years. They have always been a source of unwavering support and I cannot thank them enough for everything they have done. Finally, thank you to my amazing wife, Charlene. I would not have finished if it wasn’t for you. You have been by my side this whole time andIamso thankful that were always ready to listen when I had bad news and celebrate with me when I had good news. I would like to thank each and every person who has helped me in my academic journey, but there is not enough room in this document for that. Again, I am in no way an island and the work described herein, while it has my name on it, would simply not have been possible without a massive amount of assistance and support from an incalculable number of sources. vii Vita February 17, 1990 . Born, Gainesville, FL May 2008 . Dacula High School, Dacula, GA May 2012 . B.S. in Biochemistry and Molecular Bi- ology, Harding University, Searcy, AR September 2012 to August 2014 . Graduate Teaching Associate, Depart- ment of Chemistry and Biochemistry and Department of Physics, The Ohio State University September 2014 to August 2015 . CMBP Fellow, Cellular, Molecular, and Biochemical Sciences Training Pro- gram, The Ohio State University September 2015 to present . Graduate Teaching Associate, Depart- ment of Chemistry and Biochemistry Publications Slater, J. W., Marguet, S. C., Cirino, S. L., Maugeri, P. T. & Shafaat, H. S. Ex- perimental and DFT Investigations Reveal the Influence of the Outer Coordination Sphere on the Vibrational Spectra of Nickel-Substituted Rubredoxin, a Model Hydro- genase Enzyme.
Recommended publications
  • DEVELOPMENT of a RAMAN SPECTROMETER to STUDY SURFACE-ENHANCED RAMAN SCATTERING by Nandita Biswas, Ridhima Chadha, Sudhir Kapoor, Sisir K
    BARC/2011/E/003 BARC/2011/E/003 DEVELOPMENT OF A RAMAN SPECTROMETER TO STUDY SURFACE-ENHANCED RAMAN SCATTERING by Nandita Biswas, Ridhima Chadha, Sudhir Kapoor, Sisir K. Sarkar and Tulsi Mukherjee Radiation & Photochemistry Division 2011 BARC/2011/E/003 GOVERNMENT OF INDIA ATOMIC ENERGY COMMISSION BARC/2011/E/003 DEVELOPMENT OF A RAMAN SPECTROMETER TO STUDY SURFACE-ENHANCED RAMAN SCATTERING by Nandita Biswas, Ridhima Chadha, Sudhir Kapoor, Sisir K. Sarkar and Tulsi Mukherjee Radiation & Photochemistry Division BHABHA ATOMIC RESEARCH CENTRE MUMBAI, INDIA 2011 BARC/2011/E/003 BIBLIOGRAPHIC DESCRIPTION SHEET FOR TECHNICAL REPORT (as per IS : 9400 - 1980) 01 Security classification : Unclassified 02 Distribution : External 03 Report status : New 04 Series : BARC External 05 Report type : Technical Report 06 Report No. : BARC/2011/E/003 07 Part No. or Volume No. : 08 Contract No. : 10 Title and subtitle : Development of a Raman spectrometer to study surface-enhanced Raman scattering 11 Collation : 31 p., 15 figs. 13 Project No. : 20 Personal author(s) : Nandita Biswas; Ridhima Chadha; Sudhir Kapoor; Sisir K. Sarkar; Tulsi Mukherjee 21 Affiliation of author(s) : Radiation and Photochemistry Division , Bhabha Atomic Research Centre, Mumbai 22 Corporate author(s) : Bhabha Atomic Research Centre, Mumbai - 400 085 23 Originating unit : Radiation and Photochemistry Division, BARC, Mumbai 24 Sponsor(s) Name : Department of Atomic Energy Type : Government Contd... BARC/2011/E/003 30 Date of submission : January 2011 31 Publication/Issue date : February 2011 40 Publisher/Distributor : Head, Scientific Information Resource Division, Bhabha Atomic Research Centre, Mumbai 42 Form of distribution : Hard copy 50 Language of text : English 51 Language of summary : English, Hindi 52 No.
    [Show full text]
  • The Term Fluorescence Was Coined by Stokes Circa 1850 to Name A
    Fluorescence primer v4.doc Page 1/11 19/11/2008 Fluorescence The term fluorescence was coined by Stokes circa 1850 to name a phenomenon resulting in the emission of light at longer wavelength than the absorbed light, and his name is still used to describe the wavelength shift (Figure 1A). Figure 1 The following general rules of fluorescence (see Jameson et al., 20031) are of practical importance: 1) In a pure substance existing in solution in a unique form, the fluorescence spectrum is invariant, remaining the same independent of the excitation wavelength. 2) The fluorescence spectrum lies at longer wavelengths than the absorbtion. 3) The fluorescence spectrum is, to a good approximation, a mirror image of the absorption band of least frequency These rules follow from quantum optical considerations depicted in the Perrin-Jablonski diagram (Figure 1B). Note that although the fluorophore may be excited into different singlet state energy levels (S1, S2, etc.) rapid thermal relaxation invariably brings the fluorophore to the lowest vibrational level of the first excited electronic state (S1) and emission occurs from that level. This fact explains the independence of the emission spectrum from the excitation wavelength. The fact that ground state fluorophores (at room temperature) are predominantly in the lowest vibrational level of the ground electronic state accounts for the Stokes shift. Finally, the fact that the spacings of the vibrational energy levels of S0 and S1 are usually similar accounts for the fact that the emission and the absorption spectra are approximately mirror images. The presence of appreciable Stokes shift is principally important for practical applications of fluorescence because it allows to separate (strong) excitation light from (weak) emitted fluorescence using appropriate optics.
    [Show full text]
  • Resonant Raman Spectroscopy of Nanotubes
    10.1098/rsta.2004.1444 Resonant Raman spectroscopy of nanotubes By Christian Thomsen1, Stephanie Reich2 and Janina Maultzsch1 1Technische Universit¨at Berlin, Hardenbergstraße 36, 10623 Berlin, Germany 2Department of Engineering, University of Cambridge, Trumpington Street, Cambridge CB2 1PZ, UK ([email protected]) Published online 28 September 2004 Single and double resonances in Raman scattering are introduced and six criteria for the observation and identification of double resonances stated. The experimental situation in carbon nanotubes is reviewed in view of these criteria. The evidence for the D mode and the high-energy mode is found to be overwhelming for a double- resonance process to take place, whereas the nature of the radial breathing-mode Raman process remains undecided at this point. Consequences for the application of Raman scattering to the characterization of nanotubes are discussed. Keywords: carbon nanotubes; double resonance; Raman scattering; defects 1. Introduction Raman scattering in carbon nanotubes has developed into a method of choice in the investigation of their physical properties and their characterization. The study of electronic resonances in the Raman spectra, a method which has been used exten- sively, for example, in work on semiconductors (Cardona 1982), gives us a wealth of information about the electronic band structure of a material. This is also true for the Raman work on carbon nanotubes, where resonance studies have moved into the focus of research. Traditional Raman studies of carbon nanotubes focus on the radial breathing mode (RBM), a mode where all atoms vibrate in phase in the radial direction (Dresselhaus et al. 1995). Its frequency, as can easily be shown (Jishi et al.
    [Show full text]
  • Raman Scattering and Fluorescence
    Fluorescence 01 Raman Scattering and Fluorescence Introduction The existence of such virtual states also explains why the non-resonance Raman effect Raman scattering and Fluorescence emission does not depend on the wavelength of the are two competing phenomena, which have excitation, since no real states are involved in similar origins. Generally, a laser photon this interaction mechanism. In fact, the Raman bounces off a molecule and looses a certain spectrum generally does not depend on the amount of energy that allows the molecule to laser excitation. vibrate (Stokes process). The scattered photon is therefore less energetic and the associated However, when the energy of the excitation light exhibits a frequency shift. The various photon gets close to the transition energy frequency shifts associated with different between two electronic states, one then deals molecular vibrations give rise to a spectrum, with resonance Raman or resonance that is characteristic of a specific compound. fluorescence (fig.1, case (d)). The basic difference between these two processes is In contrast, fluorescence or luminescence related to the time scales involved, as well as emission follows an absorption process. For a with the nature of the so-called intermediate better understanding, one can refer to the states. In contrast with resonant fluorescent, diagram below. relaxed fluorescence results from the emission of a photon from the lowest vibrational level of an excited electronic state, following a direct absorption of the photon and relaxation of the molecule from its vibrationally excited level of the electronic state back to the lowest vibrational level of the electronic state. A fluorescence process typically requires more than 10-9 s.
    [Show full text]
  • The Electromagnetic Spectrum
    The Electromagnetic Spectrum Wavelength/frequency/energy MAP TAP 2003-2004 The Electromagnetic Spectrum 1 Teacher Page • Content: Physical Science—The Electromagnetic Spectrum • Grade Level: High School • Creator: Dorothy Walk • Curriculum Objectives: SC 1; Intro Phys/Chem IV.A (waves) MAP TAP 2003-2004 The Electromagnetic Spectrum 2 MAP TAP 2003-2004 The Electromagnetic Spectrum 3 What is it? • The electromagnetic spectrum is the complete spectrum or continuum of light including radio waves, infrared, visible light, ultraviolet light, X- rays and gamma rays • An electromagnetic wave consists of electric and magnetic fields which vibrates thus making waves. MAP TAP 2003-2004 The Electromagnetic Spectrum 4 Waves • Properties of waves include speed, frequency and wavelength • Speed (s), frequency (f) and wavelength (l) are related in the formula l x f = s • All light travels at a speed of 3 s 108 m/s in a vacuum MAP TAP 2003-2004 The Electromagnetic Spectrum 5 Wavelength, Frequency and Energy • Since all light travels at the same speed, wavelength and frequency have an indirect relationship. • Light with a short wavelength will have a high frequency and light with a long wavelength will have a low frequency. • Light with short wavelengths has high energy and long wavelength has low energy MAP TAP 2003-2004 The Electromagnetic Spectrum 6 MAP TAP 2003-2004 The Electromagnetic Spectrum 7 Radio waves • Low energy waves with long wavelengths • Includes FM, AM, radar and TV waves • Wavelengths of 10-1m and longer • Low frequency • Used in many
    [Show full text]
  • Technical Application Note
    Compact Rugged Spectrometers - A Universe of Spectroscopy Systems Technical Application Note Vibrational Spectroscopy: Infrared vs. Raman StellarNet, Inc. Tampa, Fl USA Tony Rizzuto, PhD April 12, 2017 Vibrational spectroscopies are integral in analyzing some of the most fundamentally important processes in physical chemistry: molecular vibrations. While there are many different experimental techniques used to analyze those vibrations, most are variations of the “Big Two,” FTIR and Raman scattering spectroscopies. This article aims to analyze the benefits and drawbacks of each of the “Big Two,” with the hope that it helps one choose the correct technique for one’s research interests. 1. What are the “Big Two?” Fourier Transform Infrared Spectroscopy Raman spectroscopy relies on inelastic (FTIR) is a simple absorption measurement scattering phenomenon that probes the where the detector measures the molecular vibration. Where FTIR will use a absorbance of infrared radiation by the broadband IR source, Raman spectroscopy sample. Each sample will absorb different typically uses a narrow-band, amounts of each frequency resulting in a monochromatic light source in order to “chemical fingerprint” that is the FTIR excite the vibrations of the molecule in your spectrum. sample. 2. Selection Rules: What molecular vibrations are being probed? Imagining a molecular bond vibration with the traditional ball and spring model (Figure 1a) and its resultant harmonic oscillator depiction (Figure 1b) allows us to calculate the selection rules for vibrational transitions to be = 1. However, that does not tell the whole story. In order to truly differentiate FTIR from Raman Spectroscopy, we must think about it on a molecular level. Compact Rugged Spectrometers - A Universe of Spectroscopy Systems Technical Application Note A B Figure 1: A.
    [Show full text]
  • Including Far Red in an LED Lighting Spectrum
    technically speaking BY ERIK RUNKLE Including Far Red in an LED Lighting Spectrum Far red (FR) is a one of the radiation (or light) wavebands larger leaves can be desired for other crops. that regulates plant growth and development. Many people We have learned that blue light (and to a smaller extent, consider FR as radiation with wavelengths between 700 and total light intensity) can influence the effects of FR. When the 800 nm, although 700 to 750 nm is, by far, the most active. intensity of blue light is high, adding FR only slightly increases By definition, FR is just outside the photosynthetically active extension growth. Therefore, the utility of including FR in an radiation (PAR) waveband, but it can directly and indirectly indoor lighting spectrum is greater under lower intensities increase growth. In addition, it can accelerate of blue light. One compelling reason to deliver at least some flowering of some crops, especially long-day plants, FR light indoors is to induce early flowering of young plants, which are those that flower when the nights are short. especially long-day plants. As we learn more about the effects of FR on plants, growers sometimes wonder, is it beneficial to include FR in a light-emitting diode (LED) spectrum? "As the DLI increases, Not surprisingly, the answer is, it depends on the application and crop. In the May 2016 issue of GPN, I wrote about the the utility of FR in effects of FR on plant growth and flowering (https:// bit.ly/2YkxHCO). Briefly, leaf size and stem length photoperiodic lighting increase as the intensity of FR increases, although the magnitude depends on the crop and other characteristics of the light environment.
    [Show full text]
  • Stokes Shift
    Stokes shift ticular molecular structure. If a material has a direct bandgap in the range of visible light, the light shining on it is absorbed, causing electrons to become excited to a higher energy state. The electrons remain in the ex- cited state for about 10−8 seconds. This number varies over several orders of magnitude depending on the sam- ple, and is known as the fluorescence lifetime of the sam- ple. After losing a small amount of energy in some way (hence the longer wavelength), the molecule returns to the ground state and energy is emitted. 2 References Absorption and emission spectra of Rhodamine 6G with ~25 nm [1] Gispert, J.R. (2008). Coordination Chemistry. Wiley- Stokes shift VCH. p. 483. ISBN 3-527-31802-X. [2] Albani, J.R. (2004). Structure and Dynamics of Macro- Not to be confused with Stark shift. molecules: Absorption and Fluorescence Studies. Elsevier. p. 58. ISBN 0-444-51449-X. Stokes shift is the difference (in wavelength or frequency [3] Lakowicz, J.R. 1983. Principles of Fluorescence Spec- units) between positions of the band maxima of the troscopy, Plenum Press, New York. ISBN 0-387-31278- absorption and emission spectra (fluorescence and Raman 1. being two examples) of the same electronic transition.[1] [4] Guilbault, G.G. 1990. Practical Fluorescence, Second It is named after Irish physicist George G. Stokes.[2][3][4] Edition, Marcel Dekker, Inc., New York. ISBN 0-8247- When a system (be it a molecule or atom) absorbs a 8350-6. photon, it gains energy and enters an excited state.
    [Show full text]
  • Electromagnetic Spectrum
    Electromagnetic Spectrum Why do some things have colors? What makes color? Why do fast food restaurants use red lights to keep food warm? Why don’t they use green or blue light? Why do X-rays pass through the body and let us see through the body? What has the radio to do with radiation? What are the night vision devices that the army uses in night time fighting? To find the answers to these questions we have to examine the electromagnetic spectrum. FASTER THAN A SPEEDING BULLET MORE POWERFUL THAN A LOCOMOTIVE These words were used to introduce a fictional superhero named Superman. These same words can be used to help describe Electromagnetic Radiation. Electromagnetic Radiation is like a two member team racing together at incredible speeds across the vast regions of space or flying from the clutches of a tiny atom. They travel together in packages called photons. Moving along as a wave with frequency and wavelength they travel at the velocity of 186,000 miles per second (300,000,000 meters per second) in a vacuum. The photons are so tiny they cannot be seen even with powerful microscopes. If the photon encounters any charged particles along its journey it pushes and pulls them at the same frequency that the wave had when it started. The waves can circle the earth more than seven times in one second! If the waves are arranged in order of their wavelength and frequency the waves form the Electromagnetic Spectrum. They are described as electromagnetic because they are both electric and magnetic in nature.
    [Show full text]
  • Resonance Enhancement of Raman Spectroscopy: Friend Or Foe?
    www.spectroscopyonline.com ® Electronically reprinted from June 2013 Volume 28 Number 6 Molecular Spectroscopy Workbench Resonance Enhancement of Raman Spectroscopy: Friend or Foe? The presence of electronic transitions in the visible part of the spectrum can provide enor- mous enhancement of the Raman signals, if these electronic states are not luminescent. In some cases, the signals can increase by as much as six orders of magnitude. How much of an enhancement is possible depends on several factors, such as the width of the excited state, the proximity of the laser to that state, and the enhancement mechanism. The good part of this phenomenon is the increased sensitivity, but the downside is the nonlinearity of the signal, making it difficult to exploit for analytical purposes. Several systems exhibiting enhancement, such as carotenoids and hemeproteins, are discussed here. Fran Adar he physical basis for the Raman effect is the vibra- bound will be more easily modulated. So, because tional modulation of the electronic polarizability. electrons are more loosely bound than electrons, the T In a given molecule, the electronic distribution is polarizability of any unsaturated chemical functional determined by the atoms of the molecule and the electrons group will be larger than that of a chemically saturated that bind them together. When the molecule is exposed to group. Figure 1 shows the spectra of stearic acid (18:0) and electromagnetic radiation in the visible part of the spec- oleic acid (18:1). These two free fatty acids are both con- trum (in our case, the laser photons), its electronic dis- structed from a chain of 18 carbon atoms, in one case fully tribution will respond to the electric field of the photons.
    [Show full text]
  • Fiber Amplifiers and Fiber Lasers Based on Stimulated Raman
    micromachines Review Fiber Amplifiers and Fiber Lasers Based on Stimulated Raman Scattering: A Review Luigi Sirleto * and Maria Antonietta Ferrara National Research Council (CNR), Institute of Applied Sciences and Intelligent Systems, Via Pietro Castellino 111, 80131 Naples, Italy; [email protected] * Correspondence: [email protected] Received: 10 January 2020; Accepted: 24 February 2020; Published: 26 February 2020 Abstract: Nowadays, in fiber optic communications the growing demand in terms of transmission capacity has been fulfilling the entire spectral band of the erbium-doped fiber amplifiers (EDFAs). This dramatic increase in bandwidth rules out the use of EDFAs, leaving fiber Raman amplifiers (FRAs) as the key devices for future amplification requirements. On the other hand, in the field of high-power fiber lasers, a very attractive option is provided by fiber Raman lasers (FRLs), due to their high output power, high efficiency and broad gain bandwidth, covering almost the entire near-infrared region. This paper reviews the challenges, achievements and perspectives of both fiber Raman amplifier and fiber Raman laser. They are enabling technologies for implementation of high-capacity optical communication systems and for the realization of high power fiber lasers, respectively. Keywords: stimulated raman scattering; fiber optics; amplifiers; lasers; optical communication systems 1. Introduction Optical communication systems require optoelectronic devices, such as sources, detectors and so on, and utilize fiber optics to transmit the light carrying the signals impressed by modulators. Optical fibers are affected by chromatic dispersion, losses, and nonlinearity. Dispersion control is, usually, achieved via fiber geometry and material composition. Losses limit the transmission distance in modern long haul fiber-optic communication systems, so in order to boost a weak signal, optical amplifiers have been developed.
    [Show full text]
  • Article Intends to Provide a for the Necessary Virtual Electronic Brief Overview of the Differences and Transition
    ADVANCES IN RAMAN TECHNIQUES Laser requirements and advances for Raman techniques Andreas Isemann Laser Quantum GmbH, 78467 Konstanz, Germany INTRODUCTION 473 nm and 1064 nm, a narrow Raman scattering as a probe of bandwidth output of few tens of GHz vibrational transitions has made or below 1 MHz if needed within the leaps and bounds since its discovery, linewidth of vibrational transitions and various schemes based on this for high resolution, low noise (less phenomenon have been developed than 0.02%) and excellent beam with great success. quality (fundamental transversal Applications range from basic electromagnetic mode TEM00) scientific research, to medical and provides optimised performance industrial instrumentation. Some for the resolution of the Raman schemes utilise linear Raman measurement needed. scattering, whilst others take advantage The wavelength is chosen based of high peak-power fields to probe on the sample under investigation, nonlinear Raman responses. with 532 nm being commonly used This article intends to provide a for the necessary virtual electronic brief overview of the differences and transition. In the following section, benefits, together with the laser source four examples from different areas of requirements and the advancements Raman applications show the diverse in techniques enabled by recent applications of linear Raman and what developments in lasers. advances have been achieved. An example of studying a real-world LINEAR RAMAN application, the successful control of Figure 1 An example of the RR microfluidic device counting of The advent of the laser in providing a food quality using Raman spectroscopy photosynthetic microorganisms. As the cells of the model strain high-intensity coherent light source and multivariate analysis, is described Synechocystis sp.
    [Show full text]