Physics 681: Solar Physics and Instrumentation – Lecture 9 Carsten Denker NJIT Physics Department Center for Solar–Terrestrial Research.

Slides:



Advertisements
Similar presentations
Optics, Eugene Hecht, Chpt. 8
Advertisements

Modern Approaches to Protein structure Determination (6 lectures)
Start EM Ch.5: Magnetostatics finish Modern Physics Ch.7: J=L+S Methods of Math. Physics, Thus. 24 Feb. 2011, E.J. Zita Magnetostatics: Lorentz Force and.
Physics 681: Solar Physics and Instrumentation – Lecture 13 Carsten Denker NJIT Physics Department Center for Solar–Terrestrial Research.
Physics 121: Electricity & Magnetism – Lecture 1 Carsten Denker NJIT Physics Department Center for Solar–Terrestrial Research.
Physics 681: Solar Physics and Instrumentation – Lecture 20 Carsten Denker NJIT Physics Department Center for Solar–Terrestrial Research.
Physics 121: Electricity & Magnetism – Lecture 6 Carsten Denker NJIT Physics Department Center for Solar–Terrestrial Research.
Physics 121: Electricity & Magnetism – Lecture 9 Carsten Denker NJIT Physics Department Center for Solar–Terrestrial Research.
Physics 681: Solar Physics and Instrumentation – Lecture 7 Carsten Denker NJIT Physics Department Center for Solar–Terrestrial Research.
P460 - real H atom1 The Real Hydrogen Atom Solve SE and in first order get (independent of L): can use perturbation theory to determine: magnetic effects.
Physics 110G Waves TOC 1 Transverse Waves in Space Transverse Waves in Time Longitudinal Waves in Space Longitudinal Waves in Time.
Physics 681: Solar Physics and Instrumentation – Lecture 10 Carsten Denker NJIT Physics Department Center for Solar–Terrestrial Research.
Physics 320: Astronomy and Astrophysics – Lecture IX
Physics 681: Solar Physics and Instrumentation – Lecture 8 Carsten Denker NJIT Physics Department Center for Solar–Terrestrial Research.
QM in 3D Quantum Ch.4, Physical Systems, 24.Feb.2003 EJZ Schrödinger eqn in spherical coordinates Separation of variables (Prob.4.2 p.124) Angular equation.
Lecture 12: The Zeeman Effect
Physics 681: Solar Physics and Instrumentation – Lecture 4
Physics 121: Electricity & Magnetism – Lecture 11 Carsten Denker NJIT Physics Department Center for Solar–Terrestrial Research.
Physics 121: Electricity & Magnetism – Lecture 10 Carsten Denker NJIT Physics Department Center for Solar–Terrestrial Research.
Spin and the Exclusion Principle Modern Ch. 7, Physical Systems, 20
Physics 121: Electricity & Magnetism – Lecture 4 Carsten Denker NJIT Physics Department Center for Solar–Terrestrial Research.
Quantum Ch.4 - continued Physical Systems, 27.Feb.2003 EJZ Recall solution to Schrödinger eqn in spherical coordinates with Coulomb potential (H atom)
Physics 121: Electricity & Magnetism – Lecture 2 Carsten Denker NJIT Physics Department Center for Solar–Terrestrial Research.
Physics 111: Elementary Mechanics – Lecture 12 Carsten Denker NJIT Physics Department Center for Solar–Terrestrial Research.
Physics 121: Electricity & Magnetism – Lecture 12 Carsten Denker NJIT Physics Department Center for Solar–Terrestrial Research.
European Joint PhD Programme, Lisboa, Diagnostics of Fusion Plasmas Spectroscopy Ralph Dux.
Physics 111: Elementary Mechanics – Lecture 9 Carsten Denker NJIT Physics Department Center for Solar–Terrestrial Research.
Measuring Magnetic Field with Light Presentation of Thesis for the Masters of Science Degree by Andreas Danielsson.
Physics 111: Elementary Mechanics – Lecture 3 Carsten Denker NJIT Physics Department Center for Solar–Terrestrial Research.
Physics 681: Solar Physics and Instrumentation – Lecture 17 Carsten Denker NJIT Physics Department Center for Solar–Terrestrial Research.
LESSON 4 METO 621. The extinction law Consider a small element of an absorbing medium, ds, within the total medium s.
March 2, 2011 Fill in derivation from last lecture Polarization of Thomson Scattering No class Friday, March 11.
Physics 681: Solar Physics and Instrumentation – Lecture 5 Carsten Denker NJIT Physics Department Center for Solar–Terrestrial Research.
Physics 681: Solar Physics and Instrumentation – Lecture 25 Carsten Denker NJIT Physics Department Center for Solar–Terrestrial Research.
Department of Electronics Nanoelectronics 11 Atsufumi Hirohata 12:00 Wednesday, 18/February/2015 (P/L 006)
By Bhaskar Department of Physics K L University. Lecture 2 (28 July) Interference.
Spectral Line Physics Atomic Structure and Energy Levels Atomic Transition Rates Molecular Structure and Transitions 1.
Arnold Sommerfeld extended the Bohr model to include elliptical orbits Bohr’s concept of quantization of angular momentum led to the principal quantum.
Chapter 41 Atomic Structure
A. Lagg - Abisko Winter School 1  The radiative transfer equation The radiative transfer equation  Solving the RTE Solving the RTE Exercise 1:Exercise.
Physics 681: Solar Physics and Instrumentation – Lecture 19 Carsten Denker NJIT Physics Department Center for Solar–Terrestrial Research.
Spicule observed in He Å Solar seminar in 2009 April 20 Short : Tetsu Anan HAZEL Bueno et al Nuño et al , 2, 3,
ATOMIC PHYSICS Dr. Anilkumar R. Kopplkar Associate Professor
Phys 102 – Lecture 26 The quantum numbers and spin.
An Electron Trapped in A Potential Well Probability densities for an infinite well Solve Schrödinger equation outside the well.
Magnetism Physics T Soft Gamma Repeater , is the most powerful known magnetic object in the universe. Only 10 of these unusual objects.
Ch4 Fine structure of atoms Magnetic moments Spin of the electron Stern-Gerlach experiment Spectrum of the alkali atoms Spin-orbit coupling (interaction)
Assistant Professor in Physics
Physics 681: Solar Physics and Instrumentation – Lecture 22 Carsten Denker NJIT Physics Department Center for Solar–Terrestrial Research.
Physics 541 A quantum approach to condensed matter physics.
Optical Pumping Simulation of Copper for Beta-NMR Experiment Julie Hammond Boston University ISOLDE, CERN
Final Exam Lectures EM Waves and Optics. Electromagnetic Spectrum.
SHINE 2008 Vector Magnetic Fields from the Helioseismic and Magnetic Imager Steven Tomczyk (HAO/NCAR) Juan Borrero (HAO/NCAR and MPS)
Total Angular Momentum L, L z, S, S z J and J z are quantized Orbital angular momentumSpin angular momentum Total angular momentum.
Atomic Physics Quantum Physics 2002 Recommended Reading: Harris Chapter 7.
The Zeeman Effect in Mercury Casey Wall with Advisor Alan Thorndike Summer 2011 Purpose The purpose of this experiment was to observe the effect of a magnetic.
Solar Spectral Lines with Special Polarization Properties for the Calibration of Instrument Polarization Wenxian Li, Roberto Casini, T. del Pino Alemán.
Quantum Mechanics in three dimensions.
Polarization in spectral lines
Chapter 41 Atomic Structure
Hydrogen Revisited.
Zeeman effect HFS and isotope shift
The Real Hydrogen Atom Solve SE and in first order get (independent of L): can use perturbation theory to determine: magnetic effects (spin-orbit and hyperfine.
Pauli Paramagnetism.
Consider the He atom. The Hamiltonian is
Chapter 41 Atomic Structure
Molecules in Magnetic Fields
Multielectron Atoms The quantum mechanics approach for treating multielectrom atoms is one of successive approximations The first approximation is to treat.
Energy hn Photon Electron Frequency n “Size”? l = c/n momentum?
Physics 319 Classical Mechanics
Presentation transcript:

Physics 681: Solar Physics and Instrumentation – Lecture 9 Carsten Denker NJIT Physics Department Center for Solar–Terrestrial Research

September 27, 2005Center for Solar-Terrestrial Research Polarimetry  Zeeman splitting  Assume weak magnetic field (LS or Russel-Saunders coupling)  Quantum numbers: L orbital angular momentum of the electrons, S spin angular momentum, J total angular momentum, and M J magnetic quantum number  Landé factor  Displacement of the line in the presence of a magnetic field  Normal Zeeman effect or Lorentz triplet: S = S’ = 0 and ΔM J = –1, 0, +1  g* = –1, 0, +1

September 27, 2005Center for Solar-Terrestrial Research Normal and Anomalous Zeeman Effect

September 27, 2005Center for Solar-Terrestrial Research  Solar spectral lines are broadened by micro- and macro-turbulence and by pressure  the components of a Zeeman multiplet are normally not resolved  The triplet consists of two shifted σ-components and an unshifted π- component  Longitudinal Zeeman effect: line-of-sight (LOS) || B  σ-components with circular polarization of opposite sense  Transverse Zeeman effect: LOS ̲|̲̲ B  π-component (linearly polarized ̲|̲̲ B ) and σ-components (linearly polarized || B )  Δλ B ≈ λ 2  Δλ D ≈ λ  Polarized light (propagating in the z-direction)  Stokes vector

September 27, 2005Center for Solar-Terrestrial Research Schlichenmaier and Collados (2002)

September 27, 2005Center for Solar-Terrestrial Research Bellot Rubio et al. (2004)

September 27, 2005Center for Solar-Terrestrial Research  Superposition of a large number of independent waves  Degree of polarization  Stokes profiles I(λ), Q(λ), U(λ), and V(λ)  Longitudinal Zeeman triplet

September 27, 2005Center for Solar-Terrestrial Research Unno’s Equations

September 27, 2005Center for Solar-Terrestrial Research Transfer of Polarized Light  Longitudinal magnetic field  Radiative transfer equations

September 27, 2005Center for Solar-Terrestrial Research  Transverse magnetic field  Radiative transfer equations

September 27, 2005Center for Solar-Terrestrial Research SOLIS