"Resonance Raman Spectroscopy" In: Encyclopedia of Inorganic and Bioinorganic Chemistry
Total Page:16
File Type:pdf, Size:1020Kb
Load more
Recommended publications
-
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. -
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 -
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. -
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. -
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. -
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. -
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. -
UNIT -1 Microwave Spectrum and Bands-Characteristics Of
UNIT -1 Microwave spectrum and bands-characteristics of microwaves-a typical microwave system. Traditional, industrial and biomedical applications of microwaves. Microwave hazards.S-matrix – significance, formulation and properties.S-matrix representation of a multi port network, S-matrix of a two port network with mismatched load. 1.1 INTRODUCTION Microwaves are electromagnetic waves (EM) with wavelengths ranging from 10cm to 1mm. The corresponding frequency range is 30Ghz (=109 Hz) to 300Ghz (=1011 Hz) . This means microwave frequencies are upto infrared and visible-light regions. The microwaves frequencies span the following three major bands at the highest end of RF spectrum. i) Ultra high frequency (UHF) 0.3 to 3 Ghz ii) Super high frequency (SHF) 3 to 30 Ghz iii) Extra high frequency (EHF) 30 to 300 Ghz Most application of microwave technology make use of frequencies in the 1 to 40 Ghz range. During world war II , microwave engineering became a very essential consideration for the development of high resolution radars capable of detecting and locating enemy planes and ships through a Narrow beam of EM energy. The common characteristics of microwave device are the negative resistance that can be used for microwave oscillation and amplification. Fig 1.1 Electromagnetic spectrum 1.2 MICROWAVE SYSTEM A microwave system normally consists of a transmitter subsystems, including a microwave oscillator, wave guides and a transmitting antenna, and a receiver subsystem that includes a receiving antenna, transmission line or wave guide, a microwave amplifier, and a receiver. Reflex Klystron, gunn diode, Traveling wave tube, and magnetron are used as a microwave sources. -
High Performance Raman Spectroscopy with Simple Optical Components ͒ ͒ W
High performance Raman spectroscopy with simple optical components ͒ ͒ W. R. C. Somerville, E. C. Le Ru,a P. T. Northcote, and P. G. Etchegoinb The MacDiarmid Institute for Advanced Materials and Nanotechnology, School of Chemical and Physical Sciences, Victoria University of Wellington, P.O. Box 600, Wellington, New Zealand ͑Received 6 December 2009; accepted 19 April 2010͒ Several simple experimental setups for the observation of Raman scattering in liquids and gases are described. Typically these setups do not involve more than a small ͑portable͒ CCD-based spectrometer ͑without scanning͒, two lenses, and a portable laser. A few extensions include an inexpensive beam-splitter and a color filter. We avoid the use of notch filters in all of the setups. These systems represent some of the simplest but state-of-the-art Raman spectrometers for teaching/ demonstration purposes and produce high quality data in a variety of situations; some of them traditionally considered challenging ͑for example, the simultaneous detection of Stokes/anti-Stokes spectra or Raman scattering from gases͒. We show examples of data obtained with these setups and highlight their value for understanding Raman spectroscopy. We also provide an intuitive and nonmathematical introduction to Raman spectroscopy to motivate the experimental findings. © 2010 American Association of Physics Teachers. ͓DOI: 10.1119/1.3427413͔ I. INTRODUCTION and finish with a higher energy than the original one. This case corresponds to anti-Stokes Raman scattering. The Raman effect was discovered in 1928 by Raman1 and In reality, the photon is usually provided by a laser, which is now a major research tool with applications in physics, has a well defined frequency. -
Neutron Vibrational Spectroscopy
Neutron Vibrational Spectroscopy A.J. (Timmy) Ramirez-Cuesta Luke L. Daemen Yongqiang Cheng Spallation Neutron Source Oak Ridge National Laboratory ORNL is managed by UT-Battelle for the US Department of Energy The S(Q,w) Map w=0 Elastic Scattering Diffraction Structural Information 2 "Let there be light" 3 4 How to measure INS (1) Direct Geometry Instrumentation 4000 3500 Direct geometry instruments 3000 ) 1 - m measure Q trajectory is c ( 2500 r e f determined by the angle s n 2000 a r t and energy transfer. y g r 1500 e n Examples: ARCS, CNCS, E HYSPEC, SEQUIOA 1000 500 0 0 10 20 30 Momentum transfer (A-1) ) . U . A ( y t i s n e L t 2 n I Incident neutron beam is 0 10 20 30 40 50 60 70 Energy (meV) s monochromatic t n u o c determining the incident n o r t u Distance energy E1. e N That determines T1. We L1 12000 13000 14000 15000 16000 measure the ToF and we ToF (ms) can work out T2. Resolution is almost constant in units of Ei time 5 VISION: a high throughput spectrometer for neutron vibrational spectroscopy Yongqiang Cheng, Luke Daemen, A.J. (Timmy) Ramirez-Cuesta Spallation Neutron Source, Oak Ridge National Laboratory, Oak Ridge, TN 37931 USA VISION offers users a variety of sample environments How to measure INS (2) Polybenzene nanothreads synthesized at high pressure: single nanothreads VISION is best thought of as and experimental/computational capabilities: the neutron analogue of a Structural inference through modeling of vibrational spectra Indirect Geometry Instrumentation Raman spectrometer. -
Femtosecond Time-Resolved Observation of Butterfly Vibration In
www.nature.com/scientificreports OPEN Femtosecond time-resolved observation of butterfy vibration in electronically excited Received: 7 June 2017 Accepted: 11 October 2017 o-fuorophenol Published: xx xx xxxx Fengzi Ling1,2, Shuai Li1,2, Xinli Song1,2, Yanmei Wang1,2, Jinyou Long1,2 & Bing Zhang 1,2 The butterfy vibration during the hydrogen tunneling process in electronically excited o-fuorophenol has been visualized in real time by femtosecond time-resolved ion yield spectroscopy coupled with time-resolved photoelectron imaging technique. A coherent superposition of out-of-plane C–F butterfy motions is prepared in the frst excited electronic state (S1). As the C–F bond vibrates with respect to the aromatic ring, the nuclear geometry varies periodically, leading to the corresponding variation in the photoionization channel. By virtue of the more favorable ionization probability from the nonplanar minimum via resonance with the Rydberg states, the evolution of the vibrational wave packet is manifested as a superimposed beat in the parent-ion transient. Moreover, time-resolved photoelectron spectra ofer a direct mapping of the oscillating butterfy vibration between the planar geometry and nonplanar minimum. The beats for the photoelectron peaks originating from the planar geometry are out of phase with those from the nonplanar minimum. Our results provide a physically intuitive and complete picture of the oscillatory fow of energy responsible for the coherent vibrational motion on the excited state surface. Ultrafast molecular vibration is one of the fundamental motions that characterize chemical bonding and decide reaction dynamics at the molecular level1–3. Over the past few decades, frequency-resolved spectroscopies such as infrared and Raman spectra4 and resonant two-photon ionization (R2PI) spectroscopy5 have devoted to pro- viding detailed spectroscopic data about molecular vibration. -
Surface-Enhanced Raman Scattering (SERS)
Focal Point Review Applied Spectroscopy 2018, Vol. 72(7) 987–1000 ! The Author(s) 2018 Surface-Enhanced Raman Scattering Reprints and permissions: sagepub.co.uk/journalsPermissions.nav (SERS) in Microbiology: Illumination and DOI: 10.1177/0003702818764672 journals.sagepub.com/home/asp Enhancement of the Microbial World Malama Chisanga, Howbeer Muhamadali, David I. Ellis, and Royston Goodacre Abstract The microbial world forms a huge family of organisms that exhibit the greatest phylogenetic diversity on Earth and thus colonize virtually our entire planet. Due to this diversity and subsequent complex interactions, the vast majority of microorganisms are involved in innumerable natural bioprocesses and contribute an absolutely vital role toward the maintenance of life on Earth, whilst a small minority cause various infectious diseases. The ever-increasing demand for environmental monitoring, sustainable ecosystems, food security, and improved healthcare systems drives the continuous search for inexpensive but reproducible, automated and portable techniques for detection of microbial isolates and understanding their interactions for clinical, environmental, and industrial applications and benefits. Surface-enhanced Raman scattering (SERS) is attracting significant attention for the accurate identification, discrimination and characteriza- tion and functional assessment of microbial cells at the single cell level. In this review, we briefly discuss the technological advances in Raman and Fourier transform infrared (FT-IR) instrumentation and their application for the analysis of clinically and industrially relevant microorganisms, biofilms, and biological warfare agents. In addition, we summarize the current trends and future prospects of integrating Raman/SERS-isotopic labeling and cell sorting technologies in parallel, to link genotype-to-phenotype in order to define community function of unculturable microbial cells in mixed microbial communities which possess admirable traits such as detoxification of pollutants and recycling of essential metals.