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30.1 Radioactivity The atom is the smallest unit of achemical
30.1 Radioactivity The atom is the smallest unit of achemical

The Nuclear Many-Body Problem Lecture 2
The Nuclear Many-Body Problem Lecture 2

... unavoidable. Observables other than the energy also needs to be transformed. ...
Chapter 7 - Bakersfield College
Chapter 7 - Bakersfield College

... B. Plutonium is a transuranium element, meaning that it has an atomic number greater than the 92 of uranium. C. The fissionable plutonium produced in a uranium-fueled reactor can be used as a fuel or in nuclear weapons. 7-12. A Nuclear World? A. Nuclear energy generates about 21 percent of the elect ...
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4PS Talk

INTRO TO NUCLEAR CHEMISTRY
INTRO TO NUCLEAR CHEMISTRY

... The actual mass of the atom is measured to be 4.00260 amu! That is 0.03038 amu less then the sum of all of its particles. 3. The mass defect is caused by the conversion of mass (m) to energy (E) when the nucleus was originally formed. 4. nuclear binding energy- the energy that was released when a nu ...
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Electromagnetic radiation

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10-GHz Bandwidth RF Spectral Analyzer With MHz Resolution
10-GHz Bandwidth RF Spectral Analyzer With MHz Resolution

... leading to a number of frequency channels equal to 10 000. The inset in Fig. 3(a) is an illustration of this resolution. The upper trace corresponds to the probing of two engraved tones MHz/ms. separated by 1.2 MHz with a chirp value The two peaks are well resolved. The other quadrature of the demod ...
Mass Spectroscopy
Mass Spectroscopy

... field. • Amount of deflection depends on m/z. • The detector signal is proportional to the number of ions hitting it. • By varying the magnetic field, ions of all masses are collected and counted. => ...
PG510 Symmetry and Molecular Spectroscopy
PG510 Symmetry and Molecular Spectroscopy

... - If a molecule is in the state j it tends to loose energy to go to state i emitting a photon of frequency ! - The probability for this to occur is given by Einstein’s coefficient: A=(16$3!3|µ|2)/(3)0hc3) (s-1) - If we have Nj molecules in j then energy is emitted at a rate: I=NjAh! (J s-1) The proc ...
PHYS 1443 – Section 501 Lecture #1
PHYS 1443 – Section 501 Lecture #1

Experiment Descriptions - USU Physics Department
Experiment Descriptions - USU Physics Department

Plasmonic modes of gold nano-particle arrays on thin gold
Plasmonic modes of gold nano-particle arrays on thin gold

... Fig. 1(c) depicts the measured extinction spectra of arrays of square gold nanoparticles [Fig. 1(a,b)] with side length d ∼ 100 nm, height hp = 30 nm and array periods Λ = 200 − 500 nm on a hf = 25 nm thick gold film. The overall size of the arrays is 100 × 100 µm. For all array periods we observe o ...
Physics 102, Class 25 The Atomic Nucleus and Radioactivity
Physics 102, Class 25 The Atomic Nucleus and Radioactivity

What do I know about……
What do I know about……

Physics 535 lectures notes: 1 * Sep 4th 2007
Physics 535 lectures notes: 1 * Sep 4th 2007

Population Analysis
Population Analysis

Daedalon EO-85 Computerized Spectrophotometer
Daedalon EO-85 Computerized Spectrophotometer

... wavelength at which the spectrum is a maximum. Notice that you can read the wavelengths at each point by putting the mouse arrow on the point and reading the cursor position located along the bottom status bar. Don’t spend too much time on finding the maximum; it’s a rather broad peak. Enter the val ...
Stopped light with storage times greater than one second using EIT
Stopped light with storage times greater than one second using EIT

4) Spectroscopies Involving Energy Exchange
4) Spectroscopies Involving Energy Exchange

... (1) Fluorescence: Emission of a photon when the analyte returns to a lower-energy state with the same spin as the higher energy state, i.e., S1→S0, in which the electron life time in the excited state is ~10–5–10–8 s. (2) Phosphorescence: Emission of a photon when the analyte returns to a lower-ener ...
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ib atomic and nuclear physics definitions and concepts

... NUCLEON: The particles in the nucleus (proton or neutron). NUCLEON NUMBER, A: The number of nucleons in the nucleus. PROTON NUMBER, Z: The number of protons in the nucleus. NEUTRON NUMBER, N: duh! N=A-Z RADIOACTIVE DECAY: A random and spontaneous process in which unstable nuclei emit a particle (dis ...
Poster
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Detection of Organic Pollutants with a Pulsed Ion Mobility
Detection of Organic Pollutants with a Pulsed Ion Mobility

A brief history of particle physics
A brief history of particle physics

... challenge is to select the useful data and record them with minimum loss (deadtime) when the detector and accelerator is running properly; and of course to analyze them and acquire results that are statistically rather than systematically limited. When the statistical uncertainty becomes smaller tha ...
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Two-dimensional nuclear magnetic resonance spectroscopy

Two-dimensional nuclear magnetic resonance spectroscopy (2D NMR) is a set of nuclear magnetic resonance spectroscopy (NMR) methods which give data plotted in a space defined by two frequency axes rather than one. Types of 2D NMR include correlation spectroscopy (COSY), J-spectroscopy, exchange spectroscopy (EXSY), and nuclear Overhauser effect spectroscopy (NOESY). Two-dimensional NMR spectra provide more information about a molecule than one-dimensional NMR spectra and are especially useful in determining the structure of a molecule, particularly for molecules that are too complicated to work with using one-dimensional NMR.The first two-dimensional experiment, COSY, was proposed by Jean Jeener, a professor at the Université Libre de Bruxelles, in 1971. This experiment was later implemented by Walter P. Aue, Enrico Bartholdi and Richard R. Ernst, who published their work in 1976.
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