Studies of Trapping and Luminescence Phenomena in Yttrium
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ZEPLIN I—The UKDM Single Phase Xenon Experiment at Boulby Neil Spooner∗ Department of Physics and Astronomy University of Sheffield, Hounsfield Road, Sheffield, S3 7RH, UK
ZEPLIN I—The UKDM Single Phase Xenon Experiment at Boulby Neil Spooner∗ Department of Physics and Astronomy University of Sheffield, Hounsfield Road, Sheffield, S3 7RH, UK I briefly review the ZEPLIN I liquid xenon detector of the UKDM collaboration. 1. ZEPLIN I Detector The ZEPLIN I detector is a single phase, 3.6 kg fiducial mass, liquid xenon scintillation detector built by the UKDM Collaboration (RAL-Sheffield-ICSTM) and running at the Boulby underground site (see Figure 1). The target mass is housed in a Cu-101 copper vessel, shaped to maximise light collection, which provides a uniform temperature environment through the use of a cryo- liquid jacket. The fiducial volume of xenon is surrounded bya5mmPTFE reflector, giving diffuse scattering of the 175 nm scintillation photons to maximise light collection. This volume is viewed through 3 mm silica windows by three quartz windowed photomultipliers through optically isolated Œturrets¹ of liquid xenon. These act both as light guides and passive shielding for the X-ray emission from the photomultipliers. The novel use of the xenon turrets arose from experience with NaI detectors where solid high-grade silica is used for light guides and shields. However, the extensive use of such material for liquid xenon is precluded due to the absorption of the 175 nm photons. Scintillation light produced in the turret regions is seen predominantly by the nearest photomultiplier which allows the rejection of the photomultiplier X-ray events and the definition of a fiducial volume through a comparison of the light seen by each tube. Purification of the xenon is performed using Oxysorb ion exchange columns with additional purification by vacuum pumping on frozen xenon and subsequent fractionation of the xenon gas. -
Muon Decay 1
Muon Decay 1 LIFETIME OF THE MUON Introduction Muons are unstable particles; otherwise, they are rather like electrons but with much higher masses, approximately 105 MeV. Radioactive nuclear decays do not release enough energy to produce them; however, they are readily available in the laboratory as the dominant component of the cosmic ray flux at the earth’s surface. There are two types of muons, with opposite charge, and they decay into electrons or positrons and two neutrinos according to the rules + + µ → e νe ν¯µ − − µ → e ν¯e νµ . The muon decay is a radioactiveprocess which follows the usual exponential law for the probability of survival for a given time t. Be sure that you understand the basis for this law. The goal of the experiment is to measure the muon lifetime which is roughly 2 µs. With care you can make the measurement with an accuracy of a few percent or better. In order to achieve this goal in a conceptually simple way, we look only at those muons that happen to come to rest inside our detector. That is, we first capture a muon and then measure the elapsed time until it decays. Muons are rather penetrating particles, they can easily go through meters of concrete. Nevertheless, a small fraction of the muons will be slowed down and stopped in the detector. As shown in Figure 1, the apparatus consists of two types of detectors. There is a tank filled with liquid scintillator (a big metal box) viewed by two photomultiplier tubes (Left and Right) and two plastic scintillation counters (flat panels wrapped in black tape), each viewed by a photomul- tiplier tube (Top and Bottom). -
Preparation of Barium Strontium Titanate Powder from Citrate
APPLIED ORGANOMETALLIC CHEMISTRY Appl. Organometal. Chem. 13, 383–397 (1999) Preparation of Barium Strontium Titanate Powder from Citrate Precursor Chen-Feng Kao* and Wein-Duo Yang Department of Chemical Engineering, National Cheng Kung University, Tainan, 70101, Taiwan TiCl4 or titanium isopropoxide reacted with INTRODUCTION citric acid to form a titanyl citrate precipitate. Barium strontium citrate solutions were then BaTiO3 is ferroelectric and piezoelectric and has added to the titanyl citrate reaction to form gels. extensive applications as an electronic material. It These gels were dried and calcined to (Ba,Sr)- can be used as a capacitor, thermistor, transducer, TiO3 powders. The gels and powders were accelerometer or degausser of colour television. characterized by DSC/TGA, IR, SEM and BaTiO3 doped with strontium retains its original XRD analyses. These results showed that, at characteristics but has a lower Curie temperature 500 °C, the gels decomposed to Ba,Sr carbonate for positive temperature coefficient devices under and TiO2, followed by the formation of (Ba,Sr)- various conditions. TiO3. The onset of perovskite formation oc- Besides solid-state reactions, chemical reactions curred at 600 °C, and was nearly complete at have also been used to prepare BaTiO3 powder. 1 1000 °C. Traces of SrCO3 were still present. Among them the hydrolysis of metal alkoxide , The cation ratios of the titanate powder oxalate precipitation in ethanol2, and alcoholic prepared in the pH range 5–6 were closest to dehydration of citrate solution3 are among the more the original stoichiometry. Only 0.1 mol% of the attractive methods. In 1956 Clabaugh et al.4 free cations remained in solution. -
CHAPTER 8: Diffusion
1 Chapter 8 CHAPTER 8: Diffusion Diffusion and ion implantation are the two key processes to introduce a controlled amount of dopants into semiconductors and to alter the conductivity type. Figure 8.1 compares these two techniques and the resulting dopant profiles. In the diffusion process, the dopant atoms are introduced from the gas phase of by using doped-oxide sources. The doping concentration decreases monotonically from the surface, and the in-depth distribution of the dopant is determined mainly by the temperature and diffusion time. Figure 8.1b reveals the ion implantation process, which will be discussed in Chapter 9. Generally speaking, diffusion and ion implantation complement each other. For instance, diffusion is used to form a deep junction, such as an n-tub in a CMOS device, while ion implantation is utilized to form a shallow junction, like a source / drain junction of a MOSFET. Boron is the most common p-type impurity in silicon, whereas arsenic and phosphorus are used extensively as n-type dopants. These three elements are highly soluble in silicon with solubilities exceeding 5 x 1020 atoms / cm3 in the diffusion temperature range (between 800oC and 1200oC). These dopants can be introduced via several means, including solid sources (BN for B, As2O3 for As, and P2O5 for P), liquid sources (BBr3, AsCl3, and POCl3), and gaseous sources (B2H6, AsH3, and PH3). Usually, the gaseous source is transported to the semiconductor surface by an inert gas (e.g. N2) and is then reduced at the surface. 2 Chapter 8 Figure 8.1: Comparison of (a) diffusion and (b) ion implantation for the selective introduction of dopants into a semiconductor substrate. -
1. Gamma-Ray Detectors for Nondestructive Analysis P
1. GAMMA-RAY DETECTORS FOR NONDESTRUCTIVE ANALYSIS P. A. Russo and D. T. Vo I. INTRODUCTION AND OVERVIEW Gamma rays are used for nondestructive quantitative analysis of nuclear material. Knowledge of both the energy of the gamma ray and its rate of emission from the unknown mass of nuclear material is required to interpret most measurements of nuclear material quantities. Therefore, detection of gamma rays for nondestructive analysis of nuclear materials requires both spectroscopy capability and knowledge of absolute specific detector response. Some techniques nondestructively quantify attributes other than nuclear material mass, but all rely on the ability to distinguish elements or isotopes and measure the relative or absolute yields of their corresponding radiation signatures. All require spectroscopy and most require high resolution. Therefore, detection of gamma rays for quantitative nondestructive analysis (NDA) of the mass or of other attributes of nuclear materials requires spectroscopy. A previous book on gamma-ray detectors for NDA1 provided generic descriptions of three detector categories: inorganic scintillation detectors, semiconductor detectors, and gas-filled detectors. This report described relevant detector properties, corresponding spectral characteristics, and guidelines for choosing detectors for NDA. The current report focuses on significant new advances in detector technology in these categories. Emphasis here is given to those detectors that have been developed at least to the stage of commercial prototypes. The type of NDA application – fixed installation in a count room, portable measurements, or fixed installation in a processing line or other active facility (storage, shipping/receiving, etc.) – influences the choice of an appropriate detector. Some prototype gamma-ray detection techniques applied to new NDA approaches may revolutionize how nuclear materials are quantified in the future. -
Contactless, Nondestructive Determination of Dopant Profiles Of
www.nature.com/scientificreports OPEN Contactless, nondestructive determination of dopant profles of localized boron-difused regions in Received: 11 November 2018 Accepted: 9 July 2019 silicon wafers at room temperature Published: xx xx xxxx Hieu T. Nguyen , Zhuofeng Li, Young-Joon Han , Rabin Basnet, Mike Tebyetekerwa , Thien N. Truong , Huiting Wu, Di Yan & Daniel Macdonald We develop a photoluminescence-based technique to determine dopant profles of localized boron- difused regions in silicon wafers and solar cell precursors employing two excitation wavelengths. The technique utilizes a strong dependence of room-temperature photoluminescence spectra on dopant profles of difused layers, courtesy of bandgap narrowing efects in heavily-doped silicon, and diferent penetration depths of the two excitation wavelengths in silicon. It is fast, contactless, and nondestructive. The measurements are performed at room temperature with micron-scale spatial resolution. We apply the technique to reconstruct dopant profles of a large-area (1 cm × 1 cm) boron-difused sample and heavily-doped regions (30 μm in diameter) of passivated-emitter rear localized-difused solar cell precursors. The reconstructed profles are confrmed with the well- established electrochemical capacitance voltage technique. The developed technique could be useful for determining boron dopant profles in small doped features employed in both photovoltaic and microelectronic applications. An attractive approach for improving light-to-electricity power conversion efciencies of crystalline silicon (c-Si) solar cells is to minimize surface areas of heavily-doped layers. Tis is due to the high recombination-active nature of the heavily-doped layers, causing a signifcant loss of photo-induced electrons and holes. Several solar cell designs employing this concept have been proved to achieve efciencies over 24% such as interdigitated back-contact (IBC)1–3 and passivated-emitter rear localized-difused (PERL)4–6 cell structures. -
Scintillation Detectors for X-Rays
INSTITUTE OF PHYSICS PUBLISHING MEASUREMENT SCIENCE AND TECHNOLOGY Meas. Sci. Technol. 17 (2006) R37–R54 doi:10.1088/0957-0233/17/4/R01 REVIEW ARTICLE Scintillation detectors for x-rays Martin Nikl Institute of Physics, Academy of Sciences of the Czech Republic, Cukrovarnicka 10, 162 53 Prague, Czech Republic Received 23 March 2005 Published 10 February 2006 Online at stacks.iop.org/MST/17/R37 Abstract Recent research in the field of phosphor and scintillator materials and related detectors is reviewed. After a historical introduction the fundamental issues are explained regarding the interaction of x-ray radiation with a solid state. Crucial parameters and characteristics important for the performance of these materials in applications, including the employed measurement methods, are described. Extended description of the materials currently in use or under intense study is given. Scintillation detector configurations are further briefly overviewed and selected applications are mentioned in more detail to provide an illustration. Keywords: luminescence intensity, luminescence kinetics, light detection, x-ray detection, scintillators, phosphors, traps and material imperfections (Some figures in this article are in colour only in the electronic version) 1. Introduction development of phosphor and scintillator materials to be used in their exploitation. It was 110 years ago in November 1895 that Wilhelm Conrad It is to be noticed that for registration of x-ray the so- Roentgen noticed the glow of a barium platino-cyanide screen, called direct registration principle is widely used, in which the placed next to his operating discharge tube, and discovered new incoming radiation is directly converted into electrical current invisible and penetrating radiation [1], which was named x-ray in a semiconducting material. -
Sensitization of Titanium Dioxide and Strontium Titanate Electrodes By
Subscriber access provided by University of Texas Libraries Sensitization of titanium dioxide and strontium titanate electrodes by ruthenium(II) tris(2,2'-bipyridine-4,4'-dicarboxylic acid) and zinc tetrakis(4-carboxyphenyl)porphyrin: an evaluation of sensitization efficiency for component photoelectrodes in a multipanel device Reza Dabestani, Allen J. Bard, Alan Campion, Marye Anne Fox, Thomas E. Mallouk, Stephen E. Webber, and J. M. White J. Phys. Chem., 1988, 92 (7), 1872-1878 • DOI: 10.1021/j100318a035 Downloaded from http://pubs.acs.org on February 2, 2009 More About This Article The permalink http://dx.doi.org/10.1021/j100318a035 provides access to: • Links to articles and content related to this article • Copyright permission to reproduce figures and/or text from this article The Journal of Physical Chemistry is published by the American Chemical Society. 1155 Sixteenth Street N.W., Washington, DC 20036 1872 J. Phys Chem. 1988, 92, 1872-1878 Sensitization of Titanium Dioxide and Strontium Titanate Electrodes by Ruthenium( I I) Trls (2,2’- bipyridine-4,4’-dicar box y lic acid) and Zinc Tetrakis (4-carboxy phen yl) porphyrin: An Evaluation of Sensitization Efficiency for Component Photoelectrodes in a Muitipanei Device Reza Dabestani, Allen J. Bard, Alan Campion, Marye Anne Fox,* Thomas E. Mallouk, Stephen E. Webber, and J. M. White Department of Chemistry, University of Texas, Austin, Texas 78712 (Received: December 1. 1986; In Final Form: October 6, 1987) The utility of polycrystalline anatase Ti02 and SrTi03 semiconductor electrodes sensitized by ruthenium(I1) tris(2,2’-bi- pyridine-4,4’-dicarboxylicacid) (1) and by zinc tetrakis(4-carboxypheny1)porphyrin (2) as component photoelectrodes in a multipanel array has been evaluated. -
Production Scientifique 2004-2007
Production scientifique 2004-2007 Articles parus dans des revues internationales ou nationales avec comité de lecture 2004 • H. Bandulet, C. Labaune, K. Lewis and S. Depierreux, Thomson scattering study of the subharmonic decay of ion-acoustic waves driven by the Brillouin instability, Phys. Rev. Lett. 93, 035002 (2004) • S. Bastiani-Ceccotti, P. Audebert, V. Nagels-Silvert, J.P. Geindre, J.C. Gauthier, J.C. Adam, A. Héron and C. Chenais- Popovics, Time-resolved analysis of the x-ray emission of femtosecond-laser-produced plasmas in the 1.5-keV range, Appl. Phys. B 78, 905 (2004) • D. Batani, F. Strati, H. Stabile, M. Tomasini, G. Lucchini, A. Ravasio, M. Koenig, A. Benuzzi-Mounaix, H. Nishimura, Y. Ochi, J. Ullschmied, J. Skala, B. Kralikova, M. Pfeifer, C. Kadlec, T. Mocek, A. Prag, T. Hall, P. Milani, E. Barborini and P. Piseri, Hugoniot data for carbon at megabar pressures, Phys. Rev. Lett. 92, 065503 (2004) • A. Benuzzi-Mounaix, M. Koenig, G. Huse, B. Faral, N. Grandjouan, D. Batani, E. Henry, M. Tomasini, T. Hall and F. Guyot, Generation of a double shock driven by laser, Phys. Rev. E 70, 045401 (2004) • S. Bouquet, C. Stehlé, M. Koenig, J.P. Chièze, A. Benuzzi-Mounaix, D. Batani, S. Leygnac, X. Fleury, H. Merdji, C. Michaut, F. Thais, N. Grandjouan, T. Hall, E. Henry, V. Malka and J.P. Lafon, Observations of laser driven supercritical radiative shock precursors, Phys. Rev. Lett. 92, 225001 (2004) • P. Celliers, G. Collins, D. Hicks, M. Koenig, E. Henry, A. Benuzzi-Mounaix, D. Batani, D. Bradley, L. Da Silva, R. -
(YAG) Laser Capsulotomy Reference Number: CP.VP.65 Coding Implications Last Review Date: 12/2020 Revision Log
Clinical Policy: Yttrium Aluminium Garnet (YAG) Laser Capsulotomy Reference Number: CP.VP.65 Coding Implications Last Review Date: 12/2020 Revision Log See Important Reminder at the end of this policy for important regulatory and legal information. Description This policy describes the medical necessity requirements for yttrium aluminium garnet (YAG) laser capsulotomy. Policy/Criteria I. It is the policy of health plans affiliated with Centene Corporation® (Centene) that YAG laser capsulotomy is medically necessary for the following indications: A. Posterior capsular opacification following cataract surgery resulting in best corrected visual acuity of 20/30 or worse associated with symptoms of blurred vision, visual distortion or glare affecting activities of daily living; B. Contraction of the posterior capsule with resulting displacement of the intraocular lens; C. Posterior capsular opacification resulting in best corrected visual acuity of 20/25 or worse, reducing the ability to evaluate and treat retinal detachment. Background YAG capsulotomy is the incision of an opaque posterior lens capsule in an aphakic or pseudophakic eye. This incision allows the capsule to retract and no longer serve as an obstruction to the passage of light through the media to the retina. The incision is performed with YAG laser. The eye examination must confirm the diagnosis of posterior capsular opacification and excludes other ocular causes of functional impairment by one of the following methods: The eye examination should demonstrate decreased light transmission (visual acuity worse than 20/30 or 20/25 if the procedure is performed to assist in the diagnosis and treatment of retinal detachment). Manifest refraction must be recorded with decrease in best-corrected visual acuity. -
Structuraland Magnetic Properties of Er3fe5-Xalxo12 Garnets
CHAPTER 3 Structural and Magnetic Properties of Er3Fe5-xAlxO12 Garnets Ibrahim Bsoul1,a, Khaled Hawamdeh1,b, Sami H. Mahmood2,c 1Physics Department, Al al-Bayt University, Mafraq 13040, Jordan 2Physics Department, The University of Jordan, Amman 11942, Jordan [email protected], [email protected], [email protected] Abstract Er3Fe5-xAlxO12 (0.0 ≤ x ≤ 0.8) garnets were prepared by ball milling and sintering at 1300ºC. Rietveld refinement of the samples revealed a garnet structure with Ia3d symmetry. The lattice parameter, cell volume, X-ray density and magnetization of the prepared garnets decreased with the increase of Al content (x). The coercivity of the garnets increased with x, but remained generally low, being below 20 Oe. Low temperature magnetic measurements versus temperature indicated that the magnetization of x = 0.0 exhibited a compensation temperature at ˗186º C, however, x = 0.8 exhibited a minimum at a higher temperature of ˗134º C. Keywords Rare Earth Iron Garnet; Structural Characteristics; Magnetic Properties; Compensation Temperature; Thermomagnetic curves. Contents 1. Introduction 2. Experimental procedures 3. Results and discussion 3.1 XRD measurements 3.2 Magnetic measurements 3.3 Temperature dependence of the magnetic properties 3.4 Low temperature measurements 4. Conclusions References 1. INTRODUCTION Ferrimagnetic garnets exemplified by yttrium iron garnet (YIG) was discovery in 1956, and received considerable interest due to their low dielectric losses and remarkable performance in microwave devices and magnetic bubbles for digital memories [1, 2], in addition to their importance in the field of fundamental magnetism. The garnets have a cubic crystal structure 3+ 3+ 3+ 2− 3+ with space group Ia3d and chemical formula {R3 }c[Fe2 ]a(Fe3 )d O12 , where R is a trivalent rare-earth ion occupying dodecahedral (c) sites, and Fe3+ ions occupy octahedral [a- sublattice] and tetrahedral (d-sublattice) sites in the garnet lattice. -
Colourless Gemstones
GEMS THE gem DeteCTIVE: COLOURLess gemstONes superseded in the 1970s by a man-made gemstone called cubic zirconia that is still the most popular and common diamond imitation in modern jewellery due to its low cost, high dispersion and good hardness (8.5 on Mohs scale). Another man-made gemstone called synthetic Moissanite was introduced as a diamond simulant in the late 1990s. Although TED A synthetic Moissanite tests positive on a FFILI A diamond tester, it is easily distinguished from diamond by a property called double refraction, detected using a 10x loupe. This property is also displayed by zircon, a natural CCREESH, O’NEILS O’NEILS CCREESH, gemstone with a sub-adamantine lustre. M N N A Complicating the process of identification are treatments that may affect the value of gemstones. For example, a laser may be used to drill down to a dark diamond inclusion and remove it using acid in a process called GE COURTESY OF BREND OF COURTESY GE laser drilling. Also common is fracture filling, ma I where a high refractive-index lead glass is used to fill surface-reaching fractures to make Sparkling, colourless gemstones may People love to assume that their great ALTHOUGH them less visible. Fortunately, both of these appear similar to the naked eye but they grandma’s solitaire engagement ring SYNTHETIC treatments are easily identified using a loupe can vary significantly in identity, rarity contained a natural diamond by virtue MOISSANITE or microscope. TESTS POSITIVE and value. Making such distinctions of its age but they should think again. Some off-coloured diamonds may be ON A DIamOND requires the detective skills of a qualified Synthetically-produced sapphire, spinel and TESTER, IT CAN BE whitened using High Pressure High gemmologist.