Optical Constants used in Radiative Transfer Models A look at calculated Qabs and Qscat Jeremy Yates UCL.

Slides:



Advertisements
Similar presentations
Weather radar equations To convert equations for distributed targets into weather radar equations, we must determine the radar reflectivity of arrays of.
Advertisements

Modelling of Defects DFT and complementary methods
Shaping the color Optical property of photonic crystals Shine.
BIOP – Center for Biomedical Optics and New Laser Systems Light scattering from a single particle Peter E. Andersen Optics and Fluid Dynamics Dept. Risø.
METO 621 Lesson 6. Absorption by gaseous species Particles in the atmosphere are absorbers of radiation. Absorption is inherently a quantum process. A.
Efficient Monte Carlo continuum radiative transfer with SKIRT Maarten Baes 2 nd East-Asia Numerical Astrophysics Meeting, Daejeon, Korea 3 November 2006.
Gothic Cathedrals and Solar Cells (and maybe a Grail?) A short introduction to the phenomenon of Surface Plasmons and their role in the scattering of light.
1 Au-shell cavity mode - Mie calculations R core = 228 nm R total = 266 nm t Au = 38 nm medium = silica cavity mode 700 nm cavity mode 880 nm 880 nm =
To date: Observational manifestations of dust: 1.Extinction – absorption/scattering diminishes flux at wavelengths comparable to light – implies particles.
Chapter 11: Electromagnetic Waves
Spectroscopy for Hot Super- Earth Exoplanets P. F. Bernath and M. Dulick Department of Chemistry & Biochemistry Old Dominion University, Norfolk, VA.
Resonances and optical constants of dielectrics: basic light-matter interaction.
Radiation forces on a dielectric sphere in the Rayleigh and Mie scattering regime Yong-Gu Lee Reference: Yasuhiro Harada et al. Radiation forces on a dielectric.
Atmospheric effect in the solar spectrum
8/5/08Lecture 2 Part 21 Maxwell’s Equations of the Electromagnetic Field Theory Gauss’s Law – charge makes an electric field The magnetic field is solenoidal.
Photons of Light The smallest unit of light is a photon A photon is often called a particle of light The Energy of an individual photon depends on its.
Acceleration of a mass limited target by ultra-high intensity laser pulse A.A.Andreev 1, J.Limpouch 2, K.Yu.Platonov 1 J.Psikal 2, Yu.Stolyarov 1 1. ILPh.
METO 621 Lesson 12. Prototype problems in Radiative Transfer Theory We will now study a number of standard radiative transfer problems. Each problem assumes.
Guillermina Ramirez San Juan
Light Scattering Rayleigh Scattering & Mie Scattering.
Connecting Accretion Disk Simulations with Observations Part II: Ray Tracing Jason Dexter 10/9/2008.
LESSON 4 METO 621. The extinction law Consider a small element of an absorbing medium, ds, within the total medium s.
Nonlinear Optics: Phenomena, Materials and Devices -Honors senior undergraduate and graduate level course. -Approximately lecture hours + 3 seminars.
Nonlinear Optics Lab. Hanyang Univ. Chapter 3. Classical Theory of Absorption 3.1 Introduction Visible color of an object : Selective absorption, Scattering,
Wave Nature of Light and Quantum Theory
Ch. 5 - Basic Definitions Specific intensity/mean intensity Flux
02/19/2014PHY 712 Spring Lecture 151 PHY 712 Electrodynamics 10-10:50 AM MWF Olin 107 Plan for Lecture 15: Finish reading Chapter 6 1.Some details.
02/18/2015PHY 712 Spring Lecture 151 PHY 712 Electrodynamics 9-9:50 AM MWF Olin 103 Plan for Lecture 15: Finish reading Chapter 6 1.Some details.
Pat Arnott, ATMS 749 Atmospheric Radiation Transfer CH4: Reflection and Refraction in a Homogenous Medium.
1 Common Far-Infrared Properties of the Galactic Disk and Nearby Galaxies MNRAS 379, 974 (2007) Hiroyuki Hirashita Hiroyuki Hirashita (Univ. Tsukuba, Japan)
Radiative transfers in complex geometry for CFD modelling the urban canopy Maya Milliez.
Attenuation by absorption and scattering
Multiple Scattering in Vision and Graphics Lecture #21 Thanks to Henrik Wann Jensen.
Scattering by particles
Real part of refractive index ( m r ): How matter slows down the light: where c is speed of light Question 3: Into which direction does the Scattered radiation.
Ch ; Lecture 26 – Quantum description of absorption.
Chemistry 330 Chapter 11 Quantum Mechanics – The Concepts.
Hanjo Lim School of Electrical & Computer Engineering Lecture 2. Basic Theory of PhCs : EM waves in mixed dielectric.
Mie-theory for a golden sphere A story of waves PART I.
Lecture/Lab: Interaction of light with particles. Mie’s solution.
Comp. Mat. Science School 2001 Lecture 21 Density Functional Theory for Electrons in Materials Richard M. Martin Bands in GaAs Prediction of Phase Diagram.
1 PHY Lecture 5 Interaction of solar radiation and the atmosphere.
What does radar measure? Hydrometeors: rain drops, ice particles Other objects: e.g. birds, insects.
Introduction to materials physics #3
Near-Field Radiation by Quantum Mechanics Thomas Prevenslik QED Radiations Discovery Bay, Hong Kong ASME 4th Micro/Nanoscale Heat Transfer Conf. (MNHMT-13),
Lecture 21 Optical properties. Incoming lightReflected light Transmitted light Absorbed light Heat Light impinging onto an object (material) can be absorbed,
Developing a Force Field Molecular Mechanics. Experimental One Dimensional PES Quantum mechanics tells us that vibrational energy levels are quantized,
Electromagnetism Around 1800 classical physics knew: - 1/r 2 Force law of attraction between positive & negative charges. - v ×B Force law for a moving.
1 Atmospheric Radiation – Lecture 9 PHY Lecture 9 Infrared radiation in a cloudy atmosphere.
Physics 213 General Physics Lecture Exam 3 Results Average = 141 points.
Saturable absorption and optical limiting
Volume and Surface Scattering of Fibers
Remote sensing: the collection of information about an object without being in direct physical contact with the object. the collection of information about.
Comp. Mat. Science School Electrons in Materials Density Functional Theory Richard M. Martin Electron density in La 2 CuO 4 - difference from sum.
Hale COLLAGE (CU ASTR-7500) “Topics in Solar Observation Techniques” Lecture 3: Basic concepts in radiative transfer & polarization Spring 2016, Part 1.
1 8 Chapter Survey Hagen- Rubens Model Continuum theory: limited to frequencies for which the atomistic structure of solids does not play a.
1 8 Chapter 11. “Continuum Theory”“Atomic Structure of Solids”“Quantum Mechanics”
Thin Film Optics Physics of thin film optics
ELEC 401 MICROWAVE ELECTRONICS Lecture 2
Maxwell's equations Poynting's theorem time-harmonic fields.
How is B related to E? We derived the wave equation for Ex:
Diatomic molecules
Electronic Structure and First Principles Theory
ELEC 401 MICROWAVE ELECTRONICS Lecture 2
Do all the reading assignments.
Thin Film Optics Physics of thin film optics
Quantum Mechanical Treatment of The Optical Properties
Finish reading Chapter 6
Classical Principles of Electromagnetism
Finish reading Chapter 6
Presentation transcript:

Optical Constants used in Radiative Transfer Models A look at calculated Qabs and Qscat Jeremy Yates UCL

What do we use now Use MIE Theory n(a) = a -p n+ik for the specific material Geometry (spherical) of grains Produce Qabs and Qscat Solve RT equation and Energy Balance Gives T rad (x,y,z), SED, images

MIE Theory Solves Maxwells equation for a plane wave interacting with a small particle Can produce n+ik if wanted Produces Scattering and Extinction Coeffs –Absorption Coeff deduced from these Produces an exact solution using spherical harmonic equations

The Problems for Grains Current use of MIE theory assumes materials are homogeneous –No band gaps – creates features –No collective displacement of atoms – creates an electric field that can shift absorption bands Basically the n+ik data are too simple and dont have sufficient frequency resolution Poor or NO modellinf of features On Earth see lots of features, but no decent model Like Atomic Spectrocopy in the 1920s

What do Real Mineralogists do Balan et al 2001, Am Min 86, 1321 Did ab initio QM calculations of n+ik and the absorption coeff of Kaolinite (Al 2 Si 2 O 5 (OH) 4 ) –Took into account the size and shape of particles and structure of the crystals –Band gaps and displacement –Calculated accurate absorption coeffs from 227 microns to 2.7 microns See a wealth of features.

To Do UCL project – Yates and Bowey will –Compute absorption and scattering coeffs for sizes and shapes and materials of Astronomical interest –Quantify the feature temperature shift –Compare with IR Lab data –Compute RT using these to get accurate intensities for IR features and make predictions for new IR features to be observed with Spitzer and HSO