The Basics of UV-Vis Spectroscopy
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Developing Back Reflectance Absorbance As a Useful Technique
Design of a Simple Cryogenic System for Ultraviolet-Visible Absorption Spectroscopy with a Back-reflectance Fiber Optic Probe Andrew Vinyard, Kaj Hansen, Ross Byrd, Douglas A Stuart * and John Hansen * Department of Chemistry, University of West Georgia *Corresponding Authors, email: [email protected] and [email protected] Abstract We report a convenient and inexpensive technique for the rapid acquisition of absorption spectra from small samples at cryogenic temperatures using a home built cryostat with novel collection optics. A cylindrical copper block was constructed with a coaxial bore to hold a 4.00 mm diameter EPR tube and mounted on a copper feed in thermal contact with liquid nitrogen. A 6.35 mm diameter hole was bored into the side of the cylinder so a fiber optic cable bundle could be positioned orthogonally to the EPR tube. The light passing through the sample is reflected off of the opposing surfaces of the EPR tube and surrounding copper, back through the sample. The emergent light is then collected by the fiber optic bundle, and analyzed by a dispersive spectrometer. Absorption spectra for KMnO4 were measured between 400 nm and 700 nm. Absorption intensity at 506 nm, 525 nm, 545 nm and 567 nm was found to be proportional to concentration, displaying Beer’s law like behavior. The EPR tube had an internal diameter of 3.2 mm; the double pass of the probe beam through the sample affords a central path length of about 6.4 mm. Comparing these measurements with those recorded on a conventional tabletop spectrometer using a cuvette with a 10.00 mm path length, we consistently found a ratio between intensities of 0.58 rather than the anticipated 0.64. -
2 in 1 Fluorescence and Absorbance Spectrometer
2 in 1 Fluorescence and Application Fluorescence Absorbance Spectrometer: Note How does it work? Life Sciences Figure 1: Duetta (left) and the inside of the Duetta sample compartment (right) with direction of the light path Introduction Duetta™ is a 2-in-1 fluorescence and absorbance excitation energy and the spectrum at longer wavelengths spectrometer from HORIBA Scientific. There are several is acquired to measure the distribution of intensity and benefits of having two different spectroscopies in one energy (wavelength) of the photons emitted. instrument. For high concentration solutions of interest, both primary and secondary inner-filter effects will affect Fluorescence Excitation Spectrum the fluorescence spectrum measured on a standard Acquiring the intensity of photons emitted at a single fluorometer. Having absorbance and fluorescence emission wavelength and scanning the excitation spectroscopy on the same instrument enables Duetta monochromator to excite the population of molecules in and EzSpec software to apply corrections for inner-filter the sample with different wavelengths. A fluorescence effect and provide more accurate data, for a wider range of excitation spectrum is analogous to an absorbance sample concentrations. Another benefit of the two in one spectrum, but is specific to a single emitting species/ instrument is that absorbance results and fluorescence wavelength as opposed to collecting all absorbing species results contain less error since the sample does not move in a sample or solution. from one instrument to another to get both measurements. Standard fluorescence methods such as Emission %Transmittance Spectrum Spectrum and Excitation Spectrum are available on Duetta, This is a ratio, in terms of percentage, of the intensity of but EzSpec software gives a user the ability to measure transmitted light through an absorbing sample (I) compared the Absorbance Spectrum as a stand-alone method or to the transmitted light through a blank solvent (I0). -
Quantum Coherence and Control in One-And Two-Photon Optical Systems
Quantum coherence and control in one- and two-photon optical systems Andrew J. Berglund∗ Department of Physics and Astronomy, Dartmouth College, Hanover, NH 03755, USA and Physics Division, P-23, Los Alamos National Laboratory, Los Alamos, NM 87545, USA We investigate coherence in one- and two-photon optical systems, both theoretically and ex- perimentally. In the first case, we develop the density operator representing a single photon state subjected to a non-dissipative coupling between observed (polarization) and unobserved (frequency) degrees of freedom. We show that an implementation of “bang-bang” quantum control protects pho- ton polarization information from certain types of decoherence. In the second case, we investigate the existence of a “decoherence-free” subspace of the Hilbert space of two-photon polarization states under the action of a similar coupling. The density operator representation is developed analytically and solutions are obtained numerically. [Note: This manuscript is taken from the author’s un- photon polarization-entangled state that, due to its sym- dergraduate thesis (A.B. Dartmouth College, June 2000, metry properties, is immune to collective decoherence advised by Dr. Walter E. Lawrence), an experimental of the type mentioned above. That is, this state is a and theoretical investigation under the supervision of Dr. decoherence-free subspace (DFS) of the Hilbert space of Paul G. Kwiat.1] photon polarization [6, 7]. Photon pairs entangled in both polarization and frequency degrees of freedom, such as hyper-entangled photons produced in down-conversion I. INTRODUCTION sources (see [8, 9]), further complicate this particular de- coherence mechanism . In particular, energy conserva- tion imposes frequency correlations which affect the co- Decoherence in two-state quantum systems is a sig- herence properties of these two-photon states. -
Vacuum Ultra Violet Monochromator I Grating & OEM
Feature Article JY Division nformation Vacuum Ultra Violet Monochromator I Grating & OEM Erick Jourdain Abstract Taking the advantage of Jobin Yvon(JY) leading position in the design and realisation of diffraction grating JY has developed over the last past 30 years some of the most innovative Vacuum Ultra Violet (VUV) monochromators for synchrotron centre. These monochromators, which combine the ultimate advanced diffraction grating technologies and some ultra precise under vacuum mechanics, have been installed in several synchrotron centres and have demonstrated superior performances. Today the development of new compact VUV sources and applications require compact VUV monochromators. Based on diffraction grating capabilities and our large experience acquired in the difficult and demanding market of under vacuum synchrotron monochromators JY is currently developing new compact monochromators for application such as Extreme UV lithography or X-ray Photoemission Spectroscopy. Introduction In the middle of the seventies thank to the development of the aberration corrected holographic toroidal gratings at Jobin Yvon (JY) we introduced on the market a new VUV monochromator concept that drastically enhanced the spectroscopic performances in this field [1]. During the eighties the Toroidal Grating Monochromator (TGM) and its associated toroidal gratings had a large and world wide success. At that time most of the synchrotron VUV beamline got equipped with this monochromator type and even today some recent beamline are still been developed Fig. -
FT-IR Spectroscopy
ORIEL ORIEL PRODUCT TRAINING FT-IR Spectroscopy SECTION FOUR FEATURES • Glossary of Terms • Introduction to FT-IR Spectroscopy Stratford, CT • Toll Free 800.714.5393 Fax 203.378.2457 • www.newport.com/oriel • [email protected] GLOSSARY OF TERMS Before we start the technical discussion on FT-IR Spectrometers, we devote a couple of pages to a Glossary, to facilitate the discussion that follows. 100% Line: Calculated by ratioing two background spectra Collimation: The ideal input beam is a cylinder of light. No taken under identical conditions. Ideally, the result is a flat beam of finite dimensions can be perfectly collimated; at best line at 100% transmittance. there is a diffraction limit. In practice the input beam is a Absorbance: Units used to measure the amount of IR cone that is determined by the source size or aperture used. radiation absorbed by a sample. Absorbance is commonly The degree of collimation can affect the S/N and the used as the Y axis units in IR spectra. Absorbance is defined resolution. by Beer’s Law, and is linearly proportional to concentration. Constructive Interference: A phenomenon that occurs when Aliasing: If frequencies above the Nyquist Frequency are not two waves occupy the same space and are in phase with filtered out, energy in these will appear as spectral artefacts each other. Since the amplitudes of waves are additive, the below the Nyquist Frequency. Optical and electronic anti two waves will add together to give a resultant wave which is aliasing can be used to prevent this. Sometimes the higher more intense than either of the individual waves. -
Optical and Electron Paramagnetic Resonance Characterization of Point Defects in Semiconductors
Air Force Institute of Technology AFIT Scholar Theses and Dissertations Student Graduate Works 3-1-2019 Optical and Electron Paramagnetic Resonance Characterization of Point Defects in Semiconductors Elizabeth M. Scherrer Follow this and additional works at: https://scholar.afit.edu/etd Part of the Electromagnetics and Photonics Commons Recommended Citation Scherrer, Elizabeth M., "Optical and Electron Paramagnetic Resonance Characterization of Point Defects in Semiconductors" (2019). Theses and Dissertations. 2463. https://scholar.afit.edu/etd/2463 This Dissertation is brought to you for free and open access by the Student Graduate Works at AFIT Scholar. It has been accepted for inclusion in Theses and Dissertations by an authorized administrator of AFIT Scholar. For more information, please contact [email protected]. OPTICAL AND ELECTRON PARAMAGNETIC RESONANCE CHARACTERIZATION OF POINT DEFECTS IN SEMICONDUCTORS DISSERTATION Elizabeth M. Scherrer, Captain, USAF AFIT-ENP-DS-19-M-091 DEPARTMENT OF THE AIR FORCE AIR UNIVERSITY AIR FORCE INSTITUTE OF TECHNOLOGY Wright-Patterson Air Force Base, Ohio DISTRIBUTION STATEMENT A APPROVED FOR PUBLIC RELEASE; DISTRIBUTION UNLIMITED. The views expressed in this thesis are those of the author and do not reflect the official policy or position of the United States Air Force, Department of Defense, or the United States Government. This material is declared a work of the U.S. Government and is not subject to copyright protection in the United States. AFIT-ENP-DS-19-M-091 OPTICAL AND ELECTRON PARAMAGNETIC RESONANCE CHARACTERIZATION OF POINT DEFECTS IN SEMICONDUCTORS DISSERTATION Presented to the Faculty Department of Engineering Physics Graduate School of Engineering and Management Air Force Institute of Technology Air University Air Education and Training Command In Partial Fulfillment of the Requirements for the Doctor of Philosophy Degree Elizabeth M. -
Lecture Notes
Solid State Physics PHYS 40352 by Mike Godfrey Spring 2012 Last changed on May 22, 2017 ii Contents Preface v 1 Crystal structure 1 1.1 Lattice and basis . .1 1.1.1 Unit cells . .2 1.1.2 Crystal symmetry . .3 1.1.3 Two-dimensional lattices . .4 1.1.4 Three-dimensional lattices . .7 1.1.5 Some cubic crystal structures ................................ 10 1.2 X-ray crystallography . 11 1.2.1 Diffraction by a crystal . 11 1.2.2 The reciprocal lattice . 12 1.2.3 Reciprocal lattice vectors and lattice planes . 13 1.2.4 The Bragg construction . 14 1.2.5 Structure factor . 15 1.2.6 Further geometry of diffraction . 17 2 Electrons in crystals 19 2.1 Summary of free-electron theory, etc. 19 2.2 Electrons in a periodic potential . 19 2.2.1 Bloch’s theorem . 19 2.2.2 Brillouin zones . 21 2.2.3 Schrodinger’s¨ equation in k-space . 22 2.2.4 Weak periodic potential: Nearly-free electrons . 23 2.2.5 Metals and insulators . 25 2.2.6 Band overlap in a nearly-free-electron divalent metal . 26 2.2.7 Tight-binding method . 29 2.3 Semiclassical dynamics of Bloch electrons . 32 2.3.1 Electron velocities . 33 2.3.2 Motion in an applied field . 33 2.3.3 Effective mass of an electron . 34 2.4 Free-electron bands and crystal structure . 35 2.4.1 Construction of the reciprocal lattice for FCC . 35 2.4.2 Group IV elements: Jones theory . 36 2.4.3 Binding energy of metals . -
A) Single-Beam
Lecture 2 Spectrophotometer Spectrophotometry is the basis for many of the instruments used in clinical chemistry. The primary reasons for this are ease of measurement, satisfactory accuracy and precision, and the suitability of spectrophotometric techniques to use in automated instruments. Spectrophotometer measures light absorption by a liquid substance at various wavelengths. The Components of unknown material can be determined, or the concentration of a number of known substances can be measured. Types of Spectrophotometer Ultraviolet (UV) Spectrophotometers. Uses ultraviolet light of wave lengths from 200 nm to 350 nm. light) of wave lengths from 350 nm to 700 nm. Spectrophotometer Block Diagram a) Single-beam b) Double-beam Most common Spectrophotometer 1. Photodiode 2. Connection wire 3. Lamp 4. Filter/Detector 5. On/Off switch and zero transmission adjustment knob 6. Wavelength selector/Readout 7. Sample chamber 8. Transmittance/absorbance control 9. Absorbance/Transmittance scale 1. Light Sources Tungsten lamp: Vis. near IR (320 nm~2500 nm) Deuterium arc lamp: UV (200~400 nm) Uses a tungsten filament and anode placed on opposite sides of a nickel box structure designed to produce the best output spectrum. Unlike tungsten lamps, the filament is not the source of light in deuterium lamps. Instead an arc is created from the filament to the anode. The arc created excites the molecular deuterium contained within the bulb to a higher energy state. The deuterium then emits light as it transitions back to its initial state Its continuous spectrum is only from 180 nm to 370 nm. Light Intensity of Tungsten and Deuterium lamps A problem with tungsten lamps is that, during operation, the tungsten progressively vaporizes from the filaments and condenses on the glass envelope. -
Spectrophotometry Light and Spectra
Page: 1 Spectrophotometry Spectrophotometry and colorimetry are conventional techniques for quantitatively determining substances encountered in biochemistry. All substances in solution absorb light of some wavelength and transmit light of other wavelengths. Absorbance is a characteristic of a substance just like melting point, boiling point, density and solubility. Absorbance can be related to the amount of the substance in solution, thus it can be used to quantitatively determine the amount of substance that is present. Light and Spectra Light or electromagnetic radiation is composed of photons moving in a wave that oscillates along the path of motion. The wavelength of light is defined as the distance between adjacent peaks in the wave and can be further defined by the equation: λ = c / ν where λ is the wavelength, c is the speed of light, and ϖ is the frequency or number of waves passing a certain point per unit time. Photons of different wavelengths have different energies that are given by: E = hc / λ = h ν where h is Planck's constant. Thus, the shorter the wavelength, the greater the energy. Electromagnetic radiation can be divided into various regions according to wavelength: the ultraviolet region has wavelengths 200-400 nm and the visible region has wavelengths of 400-700 nm. There are other regions such as infrared, radio wave, microwave and more, but you will not apply them in this course. In the visible region, lights of different wavelengths have different colors: violet and blue in the low wavelength region and orange and red in the high wavelength region. When a substance in solution appears blue, it means that the substance is absorbing red light and transmitting blue light. -
1. What Is the Difference Between Slit and Monochromator? a Slit Is A
1. What is the difference between slit and monochromator? A slit is a mechanical opening in a black painted metallic sheet, with a circular or triangular hole through which incident rays pass which lead to a monochromator. The slit permits passage of only a small fraction of incident radiation, which is selected for further processing such as wavelength selection and detection etc. Usually the output of the radiation is in the image of the slit. When the slit is wide relative to the wavelength, diffraction is difficult to observe. But when the wavelength and slit opening are of the same order of magnitude, diffraction is observed easily. Here the slit behaves as if it is a source of radiation. The output in this case occurs in a series of 1800 arcs. The plot of the frequency of the radiation as a function of peak transmittance is in the form of a Gaussian curve with maximum intensity being the midpoint of the frequency range. In contrast, monochromator may be defined as a device to select different wavelength of the original source radiation. Usually monochromators used in a UV-Visible/Fluorescence/AAS refer to the combination of slits, lenses, mirrors, windows, prisms and gratings. The output of monochromator is also a narrow band of continuous radiation. The band width is an inverse measure of the quality of the monochromator device. The band widths obtained from filters, prisms, gratings etc., become progressively narrower in each case. 2. Where is the monochromator being placed between source and sample or sample and detector in UV visible spectrophotometer? In a UV- Visible spectrophotometer, the monochromator is placed between the source of light and the sample. -
Electron Paramagnetic Resonance of Radicals and Metal Complexes. 2. International Conference of the Polish EPR Association. Wars
! U t S - PL — voZ, PL9700944 Warsaw, 9-13 September 1996 ELECTRON PARAMAGNETIC RESONANCE OF RADICALS AND METAL COMPLEXES 2nd International Conference of the Polish EPR Association INSTITUTE OF NUCLEAR CHEMISTRY AND TECHNOLOGY UNIVERSITY OF WARSAW VGL 2 8 Hi 1 2 ORGANIZING COMMITTEE Institute of Nuclear Chemistry and Technology Prof. Andrzej G. Chmielewski, Ph.D., D.Sc. Assoc. Prof. Hanna B. Ambroz, Ph.D., D.Sc. Assoc. Prof. Jacek Michalik, Ph.D., D.Sc. Dr Zbigniew Zimek University of Warsaw Prof. Zbigniew Kqcki, Ph.D., D.Sc. ADDRESS OF ORGANIZING COMMITTEE Institute of Nuclear Chemistry and Technology, Dorodna 16,03-195 Warsaw, Poland phone: (0-4822) 11 23 47; telex: 813027 ichtj pi; fax: (0-4822) 11 15 32; e-mail: [email protected] .waw.pl Abstracts are published in the form as received from the Authors SPONSORS The organizers would like to thank the following sponsors for their financial support: » State Committee of Scientific Research » Stiftung fur Deutsch-Polnische Zusammenarbeit » National Atomic Energy Agency, Warsaw, Poland » Committee of Chemistry, Polish Academy of Sciences, Warsaw, Poland » Committee of Physics, Polish Academy of Sciences, Poznan, Poland » The British Council, Warsaw, Poland » CIECH S.A. » ELEKTRIM S.A. » Broker Analytische Messtechnik, Div. ESR/MINISPEC, Germany 3 CONTENTS CONFERENCE PROGRAM 9 LECTURES 15 RADICALS IN DNA AS SEEN BY ESR SPECTROSCOPY M.C.R. Symons 17 ELECTRON AND HOLE TRANSFER WITHIN DNA AND ITS HYDRATION LAYER M.D. Sevilla, D. Becker, Y. Razskazovskii 18 MODELS FOR PHOTOSYNTHETIC REACTION CENTER: STEADY STATE AND TIME RESOLVED EPR SPECTROSCOPY H. Kurreck, G. Eiger, M. Fuhs, A Wiehe, J. -
UV-VIS Nomenclature and Units
IN804 Info Note 804: UV-VIS Nomenclature and Units Ultraviolet-visible spectroscopy or ultraviolet-visible spectrophotometry (UV/VIS) involves the spectroscopy of photons in the UV-visible region. It uses light in the visible and adjacent near ultraviolet (UV) and near infrared (NIR) ranges. In this region of the electromagnetic spectrum, molecules undergo electronic transitions. This technique is complementary to fluorescence spectroscopy, in that fluorescence deals with transitions from the excited state to the ground state, while absorption measures transitions from the ground state to the excited state. UV/VIS is based on absorbance. In spectroscopy, the absorbance A is defined as: (1) where I is the intensity of light at a specified wavelength λ that has passed through a sample (transmitted light intensity) and I is the intensity of the light before it enters the sample or 0 incident light intensity. Absorbance measurements are often carried out in analytical chemistry, since the absorbance of a sample is proportional to the thickness of the sample and the concentration of the absorbing species in the sample, in contrast to the transmittance I / I of a 0 s ample, which varies exponentially with thickness and concentration. The Beer-Lambert law is used for concentration determination. The term absorption refers to the physical process of absorbing light, while absorbance refers to the mathematical quantity. Also, absorbance does not always measure absorption: if a given sample is, for example, a dispersion, part of the incident light will in fact be scattered by the dispersed particles, and not really absorbed. Absorbance only contemplates the ratio of transmitted light over incident light, not the mechanism by which light intensity decreases.