Angular Correlation Experiments
|
|
- Philip McGee
- 6 years ago
- Views:
Transcription
1 Angular Correlation Experiments John M. LoSecco April 2, 2007 Angular Correlation Experiments J. LoSecco Notre Dame du Lac
2 Nuclear Spin In atoms one can use the Zeeman Effect to determine the spin state. Under the influence of a strong external magnetic field the multiple degenerate levels of a spin system with spin s are split into 2s + 1 levels. This method can not be used for nuclei. The magnetic moments are 2000 times smaller and the natural energy level spacing between states is 6 orders of magnitude greater than in atoms (MeV vs ev). The Mossbauer effect is a special case. Angular Correlation Experiments J. LoSecco Notre Dame du Lac 1
3 Radiation The energy of a gamma ray depends on the energy difference between nuclear levels. Gamma ray transitions depend on the spin and parities of the parent and daughter states Angular Correlation Experiments J. LoSecco Notre Dame du Lac 2
4 Multipole Moments The potential of a charge distribution can be expanded in a series of multipole moments. Monopole, dipole, quadrupole etc. These have different angular and radial distributions. 4π Q m l (r, θ,φ) = q 2l + 1 rl Yl m (θ, φ) Angular Correlation Experiments J. LoSecco Notre Dame du Lac 3
5 In classical physics oscillations of particular multipole moments give rise to different radiated angular distributions. For example dipole radiation vanishes along the pole and is maximum in the plane normal to the dipole. Angular Correlation Experiments J. LoSecco Notre Dame du Lac 4
6 Selection Rules Based on the addition rules for angular momentum Electric dipole Magnetic dipole Electric quadrupole Magnetic quadrupole Electric octupole (E1) (M1) (E2) (M2) (E3) Rigorous rules J = 0, ±1 J = 0, ±1, ±2 J no J = 0 0 no J = 0 0, 1 or J = no J = 0 0, 1, 2 M J = 0, ±1 M J = 0, ±1, ±2 M J Parity π f = π i π f = π i π f = π i Higher transitions suppressed over lower ones. So the transition is dominated by the first allowed one. Angular Correlation Experiments J. LoSecco Notre Dame du Lac 5
7 Correlated Photons Simple Example For states a, b, c Both transitions (a b and b c) are electric dipole (E1) In transition a b M J = 0,+1, 1 are equally probable. For M J = 0 angular distribution is proportional to 1 cos 2 θ For M J = ±1 angular distribution is proportional to 1 2 (1 + cos2 θ) So since each M J is equally likely the photons are isotropic. Angular Correlation Experiments J. LoSecco Notre Dame du Lac 6
8 But M J = 0 from a b must be followed by M J = 0 from b c. M J = ±1 must be followed by a transition M J = 1 The z direction is arbitrary. Angular Correlation Experiments J. LoSecco Notre Dame du Lac 7
9 Can pick z along the first photon direction. Can not get to state b with M J = 0 since the M J = 0 angular distribution is proportional to 1 cos 2 θ which vanishes in the z direction. So the b c transition must be via M J = ±1 to get to the J = 0 ground state. The M J = ±1 transitions have the angular distribution 1 2 (1+cos2 θ) which is what is measured. Angular Correlation Experiments J. LoSecco Notre Dame du Lac 8
10 Correlated Photons in 60 Ni 60 Ni is formed by beta decay of 60 Co to an excited state Photons of energy MeV and MeV are emitted In 60 Ni the levels have spins 4, 2 and 0. Angular Correlation Experiments J. LoSecco Notre Dame du Lac 9
11 Both transitions are quadrupole. Angular correlation is: cos θ cos θ4 Angular Correlation Experiments J. LoSecco Notre Dame du Lac 10
12 γγ Correlation Experiment Angular Correlation Experiments J. LoSecco Notre Dame du Lac 11
13 Particle Physics In particle physics the spin of unstable particles can be determined from the angular distribution of decay products. One frequently uses the production process to define the coordinate system. Angular Correlation Experiments J. LoSecco Notre Dame du Lac 12
14 Coincidence Methods W. Bothe Nobel 1954 Consider two counters, 1 and 2. Let ω 1,2 be the solid angle subtended and ǫ 1,2 be the counter efficiency and t 1,2 be the pulse width. The singles counting rate is: R i = Nω i ǫ i where N is the decay rate of the source. The correlated coincidence rate is: R c = Nω 1 ǫ 1 ω 2 ǫ 2 The accidental count rate is R a = R 1 R 2 t So the ratio of accidental to true coincidences is: Angular Correlation Experiments J. LoSecco Notre Dame du Lac 13
15 R a R c = N t So one wants a small t One can not lower N arbitrarily because other sources of background like cosmic rays, will enter. Want a high efficiency ǫ to get a high rate. One should not increase ω since the angular resolution will become poorer. t is the sum of the pulse widths from channel 1 and 2: t = t 1 + t 2 Angular Correlation Experiments J. LoSecco Notre Dame du Lac 14
16 Since a coincidence is recorded for any overlap of the pulses. The coincident circuit will be open for a fraction of time given by f = R 1 t. So accidental coincidences with counter 2 are R 2 f Angular Correlation Experiments J. LoSecco Notre Dame du Lac 15
17 Vacuum Methods A significant step forward for modern science. Permitted the study of cathode rays, electron beams which led to the discovery of x-rays, which led to the discovery of radioactivity. Similar to the use of spaced based observations in modern times to eliminate absorption and resolution effects of the Earth s atmosphere. Angular Correlation Experiments J. LoSecco Notre Dame du Lac 16
18 How to measure vacuum. Vacuum Gauges SI unit of pressure is the Pascal = 1 Newton per square meter. 1 atmosphere is Pascals or about 101 kpa. Units: Torr or mmhg. 1 Torr = Pascals Angular Correlation Experiments J. LoSecco Notre Dame du Lac 17
19 Thermocouple gauges measure the thermal conductivity of the gas. Useful range 10 3 to 10 torr. In this type of gauge, a wire filament is heated by running current through it. A thermocouple or Resistance Temperature Detector (RTD) can be used to measure the temperature of the filament. This temperature is dependent on the rate at which the filament loses heat to the surrounding gas, and therefore on the thermal conductivity. Angular Correlation Experiments J. LoSecco Notre Dame du Lac 18
20 Ion gauges measure the current due to ionization of residual gas. Useful range to 10 3 torr. Thermionic emission emissions generate electrons, which collide with gas atoms and generate positive ions. The ions are attracted to a suitably biased electrode known as the collector. The current in the collector is proportional to the rate of ionization, which is a function of the pressure in the system. Hence, measuring the collector current gives the gas pressure. There are several sub-types of ionization Angular Correlation Experiments J. LoSecco Notre Dame du Lac 19
21 gauge. Angular Correlation Experiments J. LoSecco Notre Dame du Lac 20
22 Mechanical gauges are based on a metallic pressure sensing element which flexes elastically under the effect of a pressure difference across the element. Bourdon gauge uses a coiled tube which as it expands due to pressure increase. commonly used on pressure regulators. Angular Correlation Experiments J. LoSecco Notre Dame du Lac 21
23 Diaphragm gauge uses the deflection of a flexible membrane that separates regions of different pressure. Used in barometers. Bellows gauge altimeters. Useful range above 10 2 torr. Angular Correlation Experiments J. LoSecco Notre Dame du Lac 22
24 Hydrostatic gauge measurements are independent of the type of gas being measured, and can be designed to have a very linear calibration. They have poor dynamic response. Height of mercury or other liquid in a column. McLeod gauge is a type of hydrostatic gauge in which the gas is compressed to increase sensitivity Useful range: above 10 4 torr Angular Correlation Experiments J. LoSecco Notre Dame du Lac 23
25 Vacuum Pumps Mechanical pumps Atmosphere down to 10 3 Torr Cryopumps Sorption pumps 10 3 Torr Oil diffusion pumps 10 6 to 100 Torr Turbomolecular pump 10 6 to 1 Torr Sputtering pumps or sputter-ion pump 10 4 to Torr Ion pumps 10 3 to Torr Angular Correlation Experiments J. LoSecco Notre Dame du Lac 24
26 Angular Correlation Experiments J. LoSecco Notre Dame du Lac 25
27 Regeneration Some pumps, such as Sorption pumps and Sputtering pumps needed to be regenerated after use. Regeneration of a cryopump is the process of evaporating the trapped gases. This can be done at room temperature and pressure, or the process can be made more complete by exposure to vacuum and faster by elevated temperatures. Best practice is to heat the whole chamber under vacuum to the Angular Correlation Experiments J. LoSecco Notre Dame du Lac 26
28 highest temperature allowed by the materials, allow time for outgassing products to be exhausted by the mechanical pumps, and then cool and use the cryopump without breaking the vacuum. Angular Correlation Experiments J. LoSecco Notre Dame du Lac 27
Gamma-ray decay. Introduction to Nuclear Science. Simon Fraser University Spring NUCS 342 March 7, 2011
Gamma-ray decay Introduction to Nuclear Science Simon Fraser University Spring 2011 NUCS 342 March 7, 2011 NUCS 342 (Lecture 18) March 7, 2011 1 / 31 Outline 1 Mössbauer spectroscopy NUCS 342 (Lecture
More informationRFSS: Lecture 6 Gamma Decay
RFSS: Lecture 6 Gamma Decay Readings: Modern Nuclear Chemistry, Chap. 9; Nuclear and Radiochemistry, Chapter 3 Energetics Decay Types Transition Probabilities Internal Conversion Angular Correlations Moessbauer
More informationConclusion. 109m Ag isomer showed that there is no such broadening. Because one can hardly
Conclusion This small book presents a description of the results of studies performed over many years by our research group, which, in the best period, included 15 physicists and laboratory assistants
More informationVacuum Pumps. Two general classes exist: Gas transfer physical removal of matter. Mechanical, diffusion, turbomolecular
Vacuum Technology Vacuum Pumps Two general classes exist: Gas transfer physical removal of matter Mechanical, diffusion, turbomolecular Adsorption entrapment of matter Cryo, sublimation, ion Mechanical
More informationEarlier Lecture. In the earlier lecture, we have seen non metallic sensors like Silicon diode, Cernox and Ruthenium Oxide.
41 1 Earlier Lecture In the earlier lecture, we have seen non metallic sensors like Silicon diode, Cernox and Ruthenium Oxide. Silicon diodes have negligible i 2 R losses. Cernox RTDs offer high response
More informationLecture 3 Vacuum Science and Technology
Lecture 3 Vacuum Science and Technology Chapter 3 - Wolf and Tauber 1/56 Announcements Homework will be online from noon today. This is homework 1 of 4. 25 available marks (distributed as shown). This
More information6. Atomic and Nuclear Physics
6. Atomic and Nuclear Physics Chapter 6.2 Radioactivity From IB OCC, prepared by J. Domingues based on Tsokos Physics book Warm Up Define: nucleon atomic number mass number isotope. Radioactivity In 1896,
More information( KS A ) (1) , vapour, vapor (USA) , saturation vapour pressure. , standard reference conditions for gases. , degree of saturation
( KS A 3014-91 ) (1), standard reference conditions for gases 0, 101325 Pa (1 =760mmHg ), vacuum, low ( rough ) vacuum 100Pa, medium vacuum 100 01 Pa, high vacuum 01 10 5 Pa, ultra high vacuum ( UHV )
More informationBETA-RAY SPECTROMETER
14 Sep 07 β-ray.1 BETA-RAY SPECTROMETER In this experiment, a 180, constant-radius magnetic spectrometer consisting of an electromagnet with a Geiger-Muller detector, will be used to detect and analyze
More information1.4 The Tools of the Trade!
1.4 The Tools of the Trade! Two things are required for material analysis: excitation mechanism for originating characteristic signature (radiation) radiation detection and identification system (spectroscopy)
More informationVacuum. Kai Schwarzwälder, Institut für Physik Universität Basel October 6 th 2006
Physics,, Technology and Techniques of the Vacuum Kai Schwarzwälder, Institut für Physik Universität Basel October 6 th 2006 Outline Introduction and basics Defintion of Vacuum Vacuum A vacuum is a volume
More informationChapter 3 Radioactivity
Chapter 3 Radioactivity Marie Curie 1867 1934 Discovered new radioactive elements Shared Nobel Prize in physics in 1903 Nobel Prize in Chemistry in 1911 Radioactivity Radioactivity is the spontaneous emission
More informationGeneral Physics (PHY 2140)
General Physics (PHY 2140) Lecture 37 Modern Physics Nuclear Physics Radioactivity Nuclear reactions http://www.physics.wayne.edu/~apetrov/phy2140/ Chapter 29 1 Lightning Review Last lecture: 1. Nuclear
More information1.5. The Tools of the Trade!
1.5. The Tools of the Trade! Two things are required for material analysis: excitation mechanism for originating characteristic signature (radiation) radiation detection and identification system (spectroscopy)
More informationRADIOACTIVITY. Nature of Radioactive Emissions
1 RADIOACTIVITY Radioactivity is the spontaneous emissions from the nucleus of certain atoms, of either alpha, beta or gamma radiation. These radiations are emitted when the nuclei of the radioactive substance
More informationMossbauer Effect and Spectroscopy. Kishan Sinha Xu Group Department of Physics and Astronomy University of Nebraska-Lincoln
Mossbauer Effect and Spectroscopy Kishan Sinha Xu Group Department of Physics and Astronomy University of Nebraska-Lincoln Emission E R γ-photon E transition hν = E transition - E R Photon does not carry
More informationL 37 Modern Physics [3] The atom and the nucleus. Structure of the nucleus. Terminology of nuclear physics SYMBOL FOR A NUCLEUS FOR A CHEMICAL X
L 37 Modern Physics [3] [L37] Nuclear physics what s inside the nucleus and what holds it together what is radioactivity carbon dating [L38] Nuclear energy nuclear fission nuclear fusion nuclear reactors
More informationAlpha-particle Stopping Powers in Air and Argon
Alpha-particle Stopping Powers in Air and Argon Mohammad QH 1* and Maghdid HA 2 1 Department of Physics, College of Science, Raparin University, Sulaimanyah, Iraqi Kurdistan, Iraq 2 Department of Physics,
More information3. Perturbed Angular Correlation Spectroscopy
3. Perturbed Angular Correlation Spectroscopy Dileep Mampallil Augustine K.U.Leuven, Belgium Perturbed Angular Correlation Spectroscopy (PAC) is a gamma ray spectroscopy and can be used to investigate
More informationβ and γ decays, Radiation Therapies and Diagnostic, Fusion and Fission Final Exam Surveys New material Example of β-decay Beta decay Y + e # Y'+e +
β and γ decays, Radiation Therapies and Diagnostic, Fusion and Fission Last Lecture: Radioactivity, Nuclear decay Radiation damage This lecture: nuclear physics in medicine and fusion and fission Final
More informationVACUUM PUMPING METHODS
VACUUM PUMPING METHODS VACUUM PUMPS (METHODS) Positive Displacement Vacuum Gas Transfer Vacuum Kinetic Vacuum Entrapment Vacuum Adsorption Reciprocating Displacement Rotary Drag Fluid Entrainment Ion Transfer
More informationThursday, April 23, 15. Nuclear Physics
Nuclear Physics Some Properties of Nuclei! All nuclei are composed of protons and neutrons! Exception is ordinary hydrogen with just a proton! The atomic number, Z, equals the number of protons in the
More informationGeneral Overview of Gas Filled Detectors
GAS-FILLED DETECTOR General Overview of Gas Filled Detectors Gas-Filled Detectors Ion chamber Proportional counter G-M (Geiger-Miller) counter Diagram of a Generic Gas-Filled Detector A Anode High-voltage
More informationSUPPLEMENTARY INFORMATION
SUPPLEMENTARY INFORMATION doi:10.1038/nature143 1. Supplementary Methods A. Details on the experimental setup Five 3 3 LaBr 3 :Ce-detectors were positioned 22 cm away from a 13 Cs gamma-ray source, which
More informationPhysics Important Terms and their Definitions
Physics Important Terms and their S.No Word Meaning 1 Acceleration The rate of change of velocity of an object with respect to time 2 Angular Momentum A measure of the momentum of a body in rotational
More informationControl Engineering BDA30703
Control Engineering BDA30703 Lecture 4: Transducers Prepared by: Ramhuzaini bin Abd. Rahman Expected Outcomes At the end of this lecture, students should be able to; 1) Explain a basic measurement system.
More informationChapter 29. Nuclear Physics
Chapter 29 Nuclear Physics Ernest Rutherford 1871 1937 Discovery that atoms could be broken apart Studied radioactivity Nobel prize in 1908 Some Properties of Nuclei All nuclei are composed of protons
More informationL 36 Modern Physics [3] The atom and the nucleus. Structure of the nucleus. The structure of the nucleus SYMBOL FOR A NUCLEUS FOR A CHEMICAL X
L 36 Modern Physics [3] [L36] Nuclear physics what s inside the nucleus and what holds it together what is radioactivity carbon dating [L37] Nuclear energy nuclear fission nuclear fusion nuclear reactors
More informationMossbauer Spectroscopy
Mossbauer Spectroscopy Emily P. Wang MIT Department of Physics The ultra-high resolution ( E = E 10 12 ) method of Mossbauer spectroscopy was used to probe various nuclear effects. The Zeeman splittings
More informationDesign, Construction, Operation, and Simulation of a Radioactivity Assay Chamber
Design, Construction, Operation, and Simulation of a Radioactivity Assay Chamber Wesley Ketchum and Abe Reddy EWI Group, UW REU 2006 Outline Neutrino Physics Background Double Beta Decay and the Majorana
More informationFoundation Year Programme
Foundation Year Programme Entrance Tests PHYSICS SPECIFICATION Standard ATS sample material 2 3 Physics 1. Electricity 1.1 Electrostatics: a. charging of insulators by friction b. object gaining electrons
More informationLecture 32 April
Lecture 32 April 08. 2016. Hydrogen Discharge Tube and Emission of Discrete Wavelengths Description of the discrete Hydrogen Emission Spectrum by the Balmer (1884) Rydberg Ritz formula (1908) Cathode Ray
More informationChapter 44. Nuclear Structure
Chapter 44 Nuclear Structure Milestones in the Development of Nuclear Physics 1896: the birth of nuclear physics Becquerel discovered radioactivity in uranium compounds Rutherford showed the radiation
More informationL-35 Modern Physics-3 Nuclear Physics 29:006 FINAL EXAM. Structure of the nucleus. The atom and the nucleus. Nuclear Terminology
9:006 FINAL EXAM L-5 Modern Physics- Nuclear Physics The final exam is on Monday MAY 7:0 AM - 9:0 AM in W90 CB The FE is not cumulative, and will cover lectures through 6. (50 questions) The last regular
More informationPhysics for Poets Lecture 2
Physics for Poets Lecture 2 Gaurang Yodh Development of quantum theory (and relativity) was in response to Experimental Observations that defied explanation in terms of Classical Physics (Newton's Laws
More informationChapter 30 Nuclear Physics and Radioactivity
Chapter 30 Nuclear Physics and Radioactivity 30.1 Structure and Properties of the Nucleus Nucleus is made of protons and neutrons Proton has positive charge: Neutron is electrically neutral: 30.1 Structure
More informationIndustrial Instrumentation Prof. A. Barua Department of Electrical Engineering Indian Institute of Technology - Kharagpur
Industrial Instrumentation Prof. A. Barua Department of Electrical Engineering Indian Institute of Technology - Kharagpur Lecture - 19 Low Pressure Measurement Welcome to the lesson 19 of Industrial Instrumentation.
More informationAt the conclusion of this lesson the trainee will be able to: a) Write a typical equation for the production of each type of radiation.
RADIOACTIVITY - SPONTANEOUS NUCLEAR PROCESSES OBJECTIVES At the conclusion of this lesson the trainee will be able to: 1. For~, p and 7 decays a) Write a typical equation for the production of each type
More informationNuclear Spin and Stability. PHY 3101 D. Acosta
Nuclear Spin and Stability PHY 3101 D. Acosta Nuclear Spin neutrons and protons have s = ½ (m s = ± ½) so they are fermions and obey the Pauli- Exclusion Principle The nuclear magneton is eh m µ e eh 1
More information2. With the help of diagram explain the Edison s discovery of thermionic emission. Mention the observations and the conclusion.
Work Sheet - 1 1. Explain the following terms i) Bound Electrons ii) Conduction/free electrons iii) Work function iv) Thermionic emission 2. With the help of diagram explain the Edison s discovery of thermionic
More informationAbsorber Alpha emission Alpha particle Atom. Atomic line spectra Atomic mass unit Atomic number Atomic structure. Background radiation
Material that prevent radioactive emission from passing through it Release of alpha particle from unstable nucleus(a 2+ helium ion or a helium nucleus) The nucleus of a helium atom (two protons and two
More informationPHYSICS 359E: EXPERIMENT 2.2 THE MOSSBAUER EFFECT: RESONANT ABSORPTION OF (-RAYS
PHYSICS 359E: EXPERIMENT 2.2 THE MOSSBAUER EFFECT: RESONANT ABSORPTION OF (-RAYS INTRODUCTION: In classical physics resonant phenomena are expected whenever a system can undergo free oscillations. These
More informationNuclear Reactions A Z. Radioactivity, Spontaneous Decay: Nuclear Reaction, Induced Process: x + X Y + y + Q Q > 0. Exothermic Endothermic
Radioactivity, Spontaneous Decay: Nuclear Reactions A Z 4 P D+ He + Q A 4 Z 2 Q > 0 Nuclear Reaction, Induced Process: x + X Y + y + Q Q = ( m + m m m ) c 2 x X Y y Q > 0 Q < 0 Exothermic Endothermic 2
More informationWhat is Radiation? Física da Radiação MEBiom 2016/2017 Patrícia Gonçalves. Supporting Slides and images
What is Radiation? Física da Radiação MEBiom 2016/2017 Patrícia Gonçalves Supporting Slides and images Radiation? Radiation is energy that comes from a source and travels through some material or through
More informationRecap I Lecture 41 Matthias Liepe, 2012
Recap I Lecture 41 Matthias Liepe, 01 Recap II Nuclear Physics The nucleus Radioactive decay Fission Fusion Particle Physics: What is the Higgs? Today: Nuclear Physics: The Nucleus Positive charge and
More informationOptics Definitions. The apparent movement of one object relative to another due to the motion of the observer is called parallax.
Optics Definitions Reflection is the bouncing of light off an object Laws of Reflection of Light: 1. The incident ray, the normal at the point of incidence and the reflected ray all lie in the same plane.
More informationRadioactive Decay. Becquerel. Atomic Physics. In 1896 Henri Becquerel. - uranium compounds would fog photographic plates as if exposed to light.
Radioactive Decay Atomic Physics Becquerel In 1896 Henri Becquerel - uranium compounds would fog photographic plates as if exposed to light. - a magnetic field could deflect the radiation that caused the
More information3.5. Accelerator Mass Spectroscopy -AMS -
3.5. Accelerator Mass Spectroscopy -AMS - AMS is a method which counts radioactive particles ( 14 C) rather than measuring the characteristic decay activity. Comparison Traditional 14 C dating and AMS
More informationNuclear Physics and Astrophysics
Nuclear Physics and Astrophysics PHY-30 Dr. E. Rizvi Lecture 4 - Detectors Binding Energy Nuclear mass MN less than sum of nucleon masses Shows nucleus is a bound (lower energy) state for this configuration
More informationGeneral Physics (PHY 2140)
General Physics (PHY 2140) Lecture 19 Modern Physics Nuclear Physics Nuclear Reactions Medical Applications Radiation Detectors Chapter 29 http://www.physics.wayne.edu/~alan/2140website/main.htm 1 Lightning
More informationGeneral Physics (PHY 2140)
General Physics (PHY 2140) Lightning Review Lecture 19 Modern Physics Nuclear Physics Nuclear Reactions Medical Applications Radiation Detectors Chapter 29 http://www.physics.wayne.edu/~alan/2140website/main.htm
More informationNicholas J. Giordano. Chapter 30. Nuclear Physics. Marilyn Akins, PhD Broome Community College
Nicholas J. Giordano www.cengage.com/physics/giordano Chapter 30 Nuclear Physics Marilyn Akins, PhD Broome Community College Atomic Nuclei Rutherford s discovery of the atomic nucleus caused scientists
More informationGAMMA RAY SPECTROSCOPY
GAMMA RAY SPECTROSCOPY Gamma Ray Spectroscopy 1 In this experiment you will use a sodium iodide (NaI) detector along with a multichannel analyzer (MCA) to measure gamma ray energies from energy level transitions
More informationFigure 1. Decay Scheme for 60Co
Department of Physics The University of Hong Kong PHYS3851 Atomic and Nuclear Physics PHYS3851- Laboratory Manual A. AIMS 1. To learn the coincidence technique to study the gamma decay of 60 Co by using
More informationEXAMINATION QUESTIONS (6)
1. What is a beta-particle? A a helium nucleus B a high-energy electron C four protons D two neutrons EXAMINATION QUESTIONS (6) 2. The diagram shows part of a circuit used to switch street lamps on and
More informationα particles, β particles, and γ rays. Measurements of the energy of the nuclear
.101 Applied Nuclear Physics (Fall 004) Lecture (1/1/04) Nuclear ecays References: W. E. Meyerhof, Elements of Nuclear Physics (McGraw-Hill, New York, 1967), Chap 4. A nucleus in an excited state is unstable
More informationUnit 3: Chemistry in Society Nuclear Chemistry Summary Notes
St Ninian s High School Chemistry Department National 5 Chemistry Unit 3: Chemistry in Society Nuclear Chemistry Summary Notes Name Learning Outcomes After completing this topic you should be able to :
More informationNuclear Spectroscopy: Radioactivity and Half Life
Particle and Spectroscopy: and Half Life 02/08/2018 My Office Hours: Thursday 1:00-3:00 PM 212 Keen Building Outline 1 2 3 4 5 Some nuclei are unstable and decay spontaneously into two or more particles.
More informationLECTURE 26 RADIATION AND RADIOACTIVITY. Instructor: Kazumi Tolich
LECTURE 26 RADIATION AND RADIOACTIVITY Instructor: Kazumi Tolich Lecture 26 2 30.4 Radiation and radioactivity Alpha decay Beta decay Gamma decay Decay series Nuclear radiation is a form of ionizing radiation
More informationPhysics 107: Ideas of Modern Physics
Physics 107: Ideas of Modern Physics Exam 3 Apr. 19, 2006 Name ID # Section # On the Scantron sheet, 1) Fill in your name 2) Fill in your student ID # (not your social security #) 3) Fill in your section
More informationPhysics 107: Ideas of Modern Physics
Physics 107: Ideas of Modern Physics Exam 3 Apr. 19, 2006 Name ID # Section # On the Scantron sheet, 1) Fill in your name 2) Fill in your student ID # (not your social security #) 3) Fill in your section
More informationModern Physics Laboratory (Physics 6180/7180)
Alpha Particle Spectroscopy Week of Jan. 18, 2010 Modern Physics Laboratory (Physics 6180/7180) The University of Toledo Instructor: Randy Ellingson Alpha Particle Spectroscopy Alpha particle source alpha
More informationDrickamer type. Disk containing the specimen. Pressure cell. Press
ε-fe Drickamer type Press Pressure cell Disk containing the specimen Low Temperature Cryostat Diamond Anvil Cell (DAC) Ruby manometry Re gasket for collimation Small size of specimen space High-density
More informationPart 12- Physics Paper 1 Atomic Structure Application Questions Combined Science
Part 12- Physics Paper 1 Atomic Structure Application Questions Combined Science Internal energy and energy transfers Internal energy and energy transfers Changes of state and the particle model Particle
More informationRotational states and rotational transitions of molecules. Microwave spectroscopic methods
Rotational states and rotational transitions of molecules Microwave spectroscopic methods Consequences of the BO approximation Within the BO approximation, the Schrödinger equation can be solved using
More informationPart 12- Physics Paper 1 Atomic Structure Knowledge Questions
Part 12- Physics Paper 1 Atomic Structure Knowledge Questions Internal energy and energy transfers Internal energy and energy transfers Changes of state and the particle model Particle Model of Matter
More information08 - Miscellaneous and historical detectors
08 - Miscellaneous and historical detectors Jaroslav Adam Czech Technical University in Prague Version 2 Jaroslav Adam (CTU, Prague) DPD_08, Miscellaneous and historical detectors Version 2 1 / 25 Streamer
More informationRadioactivity and energy levels
Radioactivity and energy levels Book page 497-503 Review of radioactivity β ; Free neutron proton β- decay is continuous β : Proton in nucleus neutron antineutrino neutrino Summary of useful equations
More informationPhotons in the universe. Indian Institute of Technology Ropar
Photons in the universe Photons in the universe Element production on the sun Spectral lines of hydrogen absorption spectrum absorption hydrogen gas Hydrogen emission spectrum Element production on the
More informationRb, which had been compressed to a density of 1013
Modern Physics Study Questions for the Spring 2018 Departmental Exam December 3, 2017 1. An electron is initially at rest in a uniform electric field E in the negative y direction and a uniform magnetic
More informationIntroduction to Modern Physics
SECOND EDITION Introduction to Modern Physics John D. McGervey Case Western Reserve University Academic Press A Subsidiary of Harcourt Brace Jovanovich Orlando San Diego San Francisco New York London Toronto
More informationChemistry Joke. Once you ve seen 6.02 x You ve seen a mole!
States of Matter Chemistry Joke Once you ve seen 6.02 x 10 23 atoms You ve seen a mole! Kinetic Theory Kinetic Theory explains the states of matter based on the concept that the particles in all forms
More informationSOLID 1. Make sure your state of matter is set on solid. Write your observations below:
Chemistry Ms. Ye Name Date Block Properties of Matter: Particle Movement Part 1: Follow the instructions below to complete the activity. Click on the link to open the simulation for this activity: http://phet.colorado.edu/sims/states-of-matter/states-of-matterbasics_en.jnlp***note:
More informationEQUIPMENT Beta spectrometer, vacuum pump, Cs-137 source, Geiger-Muller (G-M) tube, scalar
Modern Physics Laboratory Beta Spectroscopy Experiment In this experiment, electrons emitted as a result of the radioactive beta decay of Cs-137 are measured as a function of their momentum by deflecting
More informationPHYSICS B (ADVANCED PHYSICS) 2864/01 Field and Particle Pictures
THIS IS A LEGACY SPECIFICATION ADVANCED GCE PHYSICS B (ADVANCED PHYSICS) 2864/01 Field and Particle Pictures *CUP/T64120* Candidates answer on the question paper OCR Supplied Materials: Data, Formulae
More informationPhysical Vapor Deposition
Physical Vapor Deposition EVAPORATION SPUTTERING Typically used for metallization of semiconductors. Both Evaporation & Sputtering are done in vacuum environments. Typically: y Evaporation Pressures are
More informationEEE4106Z Radiation Interactions & Detection
EEE4106Z Radiation Interactions & Detection 2. Radiation Detection Dr. Steve Peterson 5.14 RW James Department of Physics University of Cape Town steve.peterson@uct.ac.za May 06, 2015 EEE4106Z :: Radiation
More informationGLOSSARY OF BASIC RADIATION PROTECTION TERMINOLOGY
GLOSSARY OF BASIC RADIATION PROTECTION TERMINOLOGY ABSORBED DOSE: The amount of energy absorbed, as a result of radiation passing through a material, per unit mass of material. Measured in rads (1 rad
More informationProperties of the nucleus. 9.1 Nuclear Physics. Isotopes. Stable Nuclei. Size of the nucleus. Size of the nucleus
Properties of the nucleus 9. Nuclear Physics Properties of nuclei Binding Energy Radioactive decay Natural radioactivity Consists of protons and neutrons Z = no. of protons (tomic number) N = no. of neutrons
More informationChapter 28. Atomic Physics
Chapter 28 Atomic Physics Quantum Numbers and Atomic Structure The characteristic wavelengths emitted by a hot gas can be understood using quantum numbers. No two electrons can have the same set of quantum
More informationRadioactive Decay 1 of 20 Boardworks Ltd 2016
Radioactive Decay 1 of 20 Boardworks Ltd 2016 Radioactive Decay 2 of 20 Boardworks Ltd 2016 What is radiation? 3 of 20 Boardworks Ltd 2016 The term radiation (also known as nuclear radiation) refers to
More informationVacuum. Residual pressure can thwart the best cryogenic design. Each gas molecule collision carries ~kt from the hot exterior to the cold interior.
Vacuum Residual pressure can thwart the best cryogenic design Each gas molecule collision carries ~kt from the hot exterior to the cold interior. 1 millitorr = 3.5x10¹³/cm³ Gas atoms leaving the hot surfaces
More informationUnits and Definition
RADIATION SOURCES Units and Definition Activity (Radioactivity) Definition Activity: Rate of decay (transformation or disintegration) is described by its activity Activity = number of atoms that decay
More informationParticle Energy Loss in Matter
Particle Energy Loss in Matter Charged particles loose energy when passing through material via atomic excitation and ionization These are protons, pions, muons, The energy loss can be described for moderately
More information11 Gamma Ray Energy and Absorption
11 Gamma Ray Energy and Absorption Before starting this laboratory, we must review the physiological effects and the proper use of the radioactive samples you will be using during the experiment. Physiological
More informationBeta Spectroscopy. Wolfgang Pauli Nobel Prize Enrico Fermi Nobel Prize 1938
Beta Spectroscopy Wolfgang Pauli Nobel Prize 1945 Enrico Fermi Nobel Prize 1938 Beta Spectroscopy The double focusing magnetic ß-spectrometer is a classical instrument for the measurement of continuous
More informationGCSE PHYSICS REVISION LIST
GCSE PHYSICS REVISION LIST OCR Gateway Physics (J249) from 2016 Topic P1: Matter P1.1 Describe how and why the atomic model has changed over time Describe the structure of the atom and discuss the charges
More informationContents. Preface to the First Edition Preface to the Second Edition
Contents Preface to the First Edition Preface to the Second Edition Notes xiii xv xvii 1 Basic Concepts 1 1.1 History 1 1.1.1 The Origins of Nuclear Physics 1 1.1.2 The Emergence of Particle Physics: the
More informationTotal probability for reaction Yield
Total probability for reaction Yield If target has thickness d, and target material has # nuclei/volume: n 0 [part./cm 3 ] Y=σ n 0 d The yield gives the intensity of the characteristic signal from the
More informationRadioactivity. The Nobel Prize in Physics 1903 for their work on radioactivity. Henri Becquerel Pierre Curie Marie Curie
Radioactivity Toward the end of the 19 th century, minerals were found that would darken a photographic plate even in the absence of light. This phenomenon is now called radioactivity. Marie and Pierre
More informationSample Examination Questions
Sample Examination Questions Contents NB. Material covered by the AS papers may also appear in A2 papers. Question Question type Question focus number (section A or B) 1 A Ideal transformer 2 A Induced
More informationMass Spectrometry in MCAL
Mass Spectrometry in MCAL Two systems: GC-MS, LC-MS GC seperates small, volatile, non-polar material MS is detection devise (Agilent 320-MS TQ Mass Spectrometer) Full scan monitoring SIM single ion monitoring
More informationModern Physics Laboratory Beta Spectroscopy Experiment
Modern Physics Laboratory Beta Spectroscopy Experiment Josh Diamond and John Cummings Fall 2009 Abstract In this experiment, electrons emitted as a result of the radioactive beta decay of 137 55 Cs are
More informationQuantum Mechanics. Exam 3. Photon(or electron) interference? Photoelectric effect summary. Using Quantum Mechanics. Wavelengths of massive objects
Exam 3 Hour Exam 3: Wednesday, November 29th In-class, Quantum Physics and Nuclear Physics Twenty multiple-choice questions Will cover:chapters 13, 14, 15 and 16 Lecture material You should bring 1 page
More informationIntroduction. Principle of Operation
Introduction Ionizing radiation that is associated with radioactivity cannot be directly detected by our senses. Ionization is the process whereby the radiation has sufficient energy to strip electrons
More information25.1. Nuclear Radiation
Nuclear Radiation Marie Curie was a Polish scientist whose research led to many discoveries about radiation and radioactive elements. In 1934 she died from leukemia caused by her long-term exposure to
More informationNUCLEI, RADIOACTIVITY AND NUCLEAR REACTIONS
NUCLEI, RADIOACTIVITY AND NUCLEAR REACTIONS VERY SHORT ANSWER QUESTIONS Q-1. Which of the two is bigger 1 kwh or 1 MeV? Q-2. What should be the approximate minimum energy of a gamma ray photon for pair
More informationGeneration of vacuum (pumps) and measurements
Generation of vacuum (pumps) and measurements Generation of vacuum (pumps): ᴥ pumping systems general considerations on their use and match with physical quantities introduced for the dimensioning of vacuum
More informationIntroduction. Introduction. Forces An. Forces An. Forces in Action. Forces in Action. Pressure and Pressure. Pressure and Pressure.
Forces An Introduction A force is a vector quantity. What does this mean? Forces An Introduction A vector quantity, such as force, has a direction as well as a magnitude. 1 1 Forces in Action The moment
More informationAngular Distribution of Neutrons from. by Frank Genevese Physical Review Vol.76, # 9 (Nov 1, 1949) A paper on experiment Paper Club, 22, Feb, 2011
Angular Distribution of Neutrons from the Photo-Disintegration of Deuteron by Frank Genevese Physical Review Vol.76, # 9 (Nov 1, 1949) A paper on experiment Paper Club, 22, Feb, 2011 The Outline of the
More information