The power of analytical spectroscopy

Size: px
Start display at page:

Download "The power of analytical spectroscopy"

Transcription

1 The power of aalytical spectroscopy Daiila et al. J. Rama Spectr. 33, 807 (00) Reflected light Red lake varish UV light Rama spectrum Lead white ciabar Caput mortuum Byzatie Ico (AD Our 534), Lady, Our i X-rays UV Lady, light the Life-givig Sprig

2 .. Basic Priciples of Atomic Physics xtremely simplified quatum mechaical model of the atom is the Bohr model based o Rutherford scatterig experimets. Negative electros are boud by electric (Coulomb) attractio to positive ucleus excitatio de-excitatio The atomic ucleus: positive charge: C atomic mass: ~ A g miiscule size: ~ cm L M N The electro orbits: egative charge: C egligible mass: ~ g fair size: ~ cm Oly certai orbits for electros are allowed: quatum states are characterized by certai radius ad eergy state, oly limited umber of electros allowed per quatum state

3 The Hydroge Atom l Z 0 ev is eergy ecessary to ioize atom Z 0 is charge of ucleus, Z mai quatum umber l - orbital mometum quatum umber l0 l0

4 Mathematics of Quatum Trasitios Hydroge atom: sigle proto i ucleus, sigle electro i orbit r [ m] 9 lectro orbit radius [ ev ] 34,,,... lectro orbit eergy lectro trasitio betwee orbits requires or releases eergy: ergy comes quatized as light particles: photos ev J

5 Trasitio betwee ergy Orbitals Possible emissio or absorptio of light with fixed wavelegths by trasitios of electros betwee orbits! Wavelegth depeds o eergy differece betwee orbits! Hydroge emissio spectrum Balmer Series -3.6/

6 ergy ad wavelegth of emitted or ν ν absorbed light photos 3.6 i f f i h c 3.6 h ν h c λ λ f i [ ev ] [ ev ] 34 h Plack Costat: [ Js] c Speed of Light: [ ev ] c h [ m/ s] m R H

7 xamples Calculate the wavelegth of a photo emitted by a electro trasitio i the hydroge atom from the L-shell ( ) to the -shell ( ) (Lyma-series L α )! λ R H f λ i R H m.5 m :.097 wavelegth 0 7 [ / m] 0.75 I iterstellar space you fid highly excited hydroge atoms which emit radio waves. The wavelegth correspods trasitio from 73 to 7. Calculate the wavelegth! RH R H λ f i 7 λ 0.93 m : radio wavelegth [ / m]

8 Wavelegth rage i the electromagetic spectrum The wavelegth rage exteds from 0-5 m (γ-radiatio) or 0-9 m (X-ray radiatio) through 0-6 m (visible light) to radio wave legths m.

9 ultraviolet visible ifrared Characteristic spectrum of elemets Solar Spectrum ach elemet has its ow characteristic trasitios depedig o the orbit quatum umbers ad the charge Z (umber of electros, protos). These trasitios ca be aalyzed by so-called spectroscopy of light to determie the elemetal abudace!

10 Multi-lectro Atoms Z is the charge ad determies the chemical characteristics of the elemet, e.g. Z(Hydroge) Z47 (Silver). lectro trasitios ad photo emissio is more complex ad depeds o Z ad the shieldig S by ier electro shells. -trasitios to λ ( Z S ) ( Z ) ( Z ) hc γ 3.6 ( Z ) + ( Z ) 3.6 hc 3.6 hc λ

11 X-ray trasitios i high Z atoms Ag aalysis L αβγ (.9 kev) α (.6 kev) β (4.9 kev)

12 xample: Calculate the ad L x-ray lies for Ag Ag : ( Z ) 3.6[ ev ] Z 47 i 3 α β [ ev ] 583[ ev ] 9 [ ev ] 5580[ ev ] β L α L L α ( Z ) 3.6[ ev ] 4 9 ( 46) 3.6[ ev ] 3997[ ev ] i α

13 trasitio scheme with orbital mometum quatum umber Level splittig occurs due to elliptic orbitals. This itroduces fie structure i the atomic light spectrum

14 higher accuracy x-ray eergies Z lemet α α β Lα Lα Lβ Lβ 47 Ag L αβγ (.9 kev) L αβγ (.9 kev) α (.6 kev) β (4.9 kev) α (.6 kev) β (4.9 kev) asy to obtai: Typical spectra:

15 Summary For usig atomic spectroscopy methods we eed to excite the atoms of the material that should be aalyzed. The decay back to the atomic groud state cofiguratio causes the emissio of photos with characteristic eergies which ca be observed by spectroscopy methods!

Physics Methods in Art and Archaeology

Physics Methods in Art and Archaeology Physics Methods i Art ad Archaeology Michael Wiescher PHYS 78 Archaeologist i the 90ties Somewhere i South America 80 years later --- i the Valley of the Kigs, gypt Physics Tools & Techology Dager & Adveture

More information

PHYS-3301 Lecture 7. CHAPTER 4 Structure of the Atom. Rutherford Scattering. Sep. 18, 2018

PHYS-3301 Lecture 7. CHAPTER 4 Structure of the Atom. Rutherford Scattering. Sep. 18, 2018 CHAPTER 4 Structure of the Atom PHYS-3301 Lecture 7 4.1 The Atomic Models of Thomso ad Rutherford 4.2 Rutherford Scatterig 4.3 The Classic Atomic Model 4.4 The Bohr Model of the Hydroge Atom 4.5 Successes

More information

Phys 102 Lecture 25 The quantum mechanical model of light

Phys 102 Lecture 25 The quantum mechanical model of light Phys 102 Lecture 25 The quatum mechaical model of light 1 Recall last time Problems with classical physics Stability of atoms Atomic spectra Photoelectric effect Quatum model of the atom Bohr model oly

More information

Absorption in Solar Atmosphere

Absorption in Solar Atmosphere Absorpto Solar Atmosphere A black body spectrum emtted from solar surface causes exctato processes o atoms the solar atmosphere. Ths tur causes absorpto of characterstc wavelegths correspodg to those atoms

More information

Shedding light on atomic energy levels (segment of Hydrogen spectrum)

Shedding light on atomic energy levels (segment of Hydrogen spectrum) 3.0 ev.85 ev.55 ev.69 ev Fri. 8.4-.7 More Eergy Quatizatio RE 8.b Mo. Tues. Wed. Lab Fri. 9.-., (.8) Mometum ad Eergy i Multiparticle Systems 9.3 Rotatioal Eergy Quiz 8 Review Exam (Ch 5-8) Exam (Ch 5-8)

More information

Experimental Fact: E = nhf

Experimental Fact: E = nhf CHAPTR 3 The xperimetal Basis of Quatum PHYS-3301 Lecture 4 Sep. 6, 2018 3.1 Discovery of the X Ray ad the lectro 3.2 Determiatio of lectro Charge 3.3 Lie Spectra 3.4 Quatizatio 3.5 Blackbody Radiatio

More information

Lecture 36 (Atomic Spectra) Physics Spring 2018 Douglas Fields

Lecture 36 (Atomic Spectra) Physics Spring 2018 Douglas Fields Lecture 36 (Atomic Spectra) Physics 6-1 Sprig 18 Douglas Fields Frauhofer Lies I the late 17s ad early 18s, oe of the premier skills was that of glassmaker. Joseph Frauhofer became oe of the most skilled

More information

Name Solutions to Test 2 October 14, 2015

Name Solutions to Test 2 October 14, 2015 Name Solutios to Test October 4, 05 This test cosists of three parts. Please ote that i parts II ad III, you ca skip oe questio of those offered. The equatios below may be helpful with some problems. Costats

More information

Development of QM. What do we know from classical physics? 1. Energy can take any continuous value.

Development of QM. What do we know from classical physics? 1. Energy can take any continuous value. Developmet of QM 1-1 What do we kow from classical physics? 1. Eergy ca take ay cotiuous value.. Electromagetic radiatio is a electric field oscillatig perpedicular to the directio of propagatio. 3. Ay

More information

Things you should know when you leave Discussion today for one-electron atoms:

Things you should know when you leave Discussion today for one-electron atoms: E = -R Thigs ou should kow whe ou leave Discussio toda for oe-electro atoms: = -.79 0-8 J = -.6eV ΔEmatter=E-Em ; Ioizatio Eerg=E E(iitial) ΔΕlight=hνlight= IE +KE. Cosider the followig eerg levels of

More information

PHYS-3301 Lecture 5. CHAPTER 3 The Experimental Basis of Quantum. 3.8: Compton Effect. 3.8: Compton Effect. Sep. 11, 2018

PHYS-3301 Lecture 5. CHAPTER 3 The Experimental Basis of Quantum. 3.8: Compton Effect. 3.8: Compton Effect. Sep. 11, 2018 CHAPTER 3 The Experimetal Basis of Quatum PHYS-3301 Lecture 5 Sep. 11, 2018 3.1 Discovery of the X Ray ad the Electro 3.2 Determiatio of Electro Charge 3.3 Lie Spectra 3.4 Quatizatio 3.5 Blackbody Radiatio

More information

sessions lectures 3-4

sessions lectures 3-4 Chemistry 1B Fall 016 quatizatio of eergy Chemistry 1B Fall 016 sessios lectures 3-4 E photo = h absorptio ad emissio spectra of hydroge atom 18 Z E. 17810 J Z=1 for H atom, =1,, 3,... 18 1. 17810 J 1

More information

Exercises and Problems

Exercises and Problems HW Chapter 4: Oe-Dimesioal Quatum Mechaics Coceptual Questios 4.. Five. 4.4.. is idepedet of. a b c mu ( E). a b m( ev 5 ev) c m(6 ev ev) Exercises ad Problems 4.. Model: Model the electro as a particle

More information

True Nature of Potential Energy of a Hydrogen Atom

True Nature of Potential Energy of a Hydrogen Atom True Nature of Potetial Eergy of a Hydroge Atom Koshu Suto Key words: Bohr Radius, Potetial Eergy, Rest Mass Eergy, Classical Electro Radius PACS codes: 365Sq, 365-w, 33+p Abstract I cosiderig the potetial

More information

5. Quantum Nature of the Nano-world ( Fundamental of. Quantum mechanics)

5. Quantum Nature of the Nano-world ( Fundamental of. Quantum mechanics) 5. Quatu Nature of the Nao-world Fudaetal of What is the defiitio of aoaterials?? Quatu echaics i Origial: quatu size effect where the electroic properties of solids are altered with great reductios i

More information

Physics 201 Final Exam December

Physics 201 Final Exam December Physics 01 Fial Exam December 14 017 Name (please prit): This test is admiistered uder the rules ad regulatios of the hoor system of the College of William & Mary. Sigature: Fial score: Problem 1 (5 poits)

More information

PLANCESS RANK ACCELERATOR

PLANCESS RANK ACCELERATOR PLANCESS RANK ACCELERATOR CHEMISTRY FOR JEE MAIN & ADVANCED 4+questios with topic wise exercises + problems of IIT-JEE & AIEEE exams of last 5 years 4 Levels of Exercises categorized ito JEE Mai & Advaced

More information

Recombiatio Lies Itroductio to Radio Spectral Lies Á Ü Spectral lies are arrow ( ) emissio or absorptio features i the spectra of gaseous sources. Examples of radio spectral lies iclude the Õ = cm hyperfie

More information

PHYS-3301 Lecture 3. EM- Waves behaving like Particles. CHAPTER 3 The Experimental Basis of Quantum. CHAPTER 3 The Experimental Basis of Quantum

PHYS-3301 Lecture 3. EM- Waves behaving like Particles. CHAPTER 3 The Experimental Basis of Quantum. CHAPTER 3 The Experimental Basis of Quantum CHAPTER 3 The Experimetal Basis of Quatum PHYS-3301 Lecture 3 Sep. 4, 2018 3.1 Discovery of the X Ray ad the Electro 3.2 Determiatio of Electro Charge 3.3 Lie Spectra 3.4 Quatizatio 3.5 Blackbody Radiatio

More information

Review Sheet for Final Exam

Review Sheet for Final Exam Sheet for ial To study for the exam, we suggest you look through the past review sheets, exams ad homework assigmets, ad idetify the topics that you most eed to work o. To help with this, the table give

More information

Mihai V. Putz: Undergraduate Structural Physical Chemistry Course, Lecture 6 1

Mihai V. Putz: Undergraduate Structural Physical Chemistry Course, Lecture 6 1 Mihai V. Putz: Udergraduate Structural Physical Chemistry Course, Lecture 6 Lecture 6: Quatum-Classical Correspodece I. Bohr s Correspodece Priciple Turig back to Bohr atomic descriptio it provides the

More information

Andrei Tokmakoff, MIT Department of Chemistry, 5/19/

Andrei Tokmakoff, MIT Department of Chemistry, 5/19/ drei Tokmakoff, MT Departmet of Chemistry, 5/9/5 4-9 Rate of bsorptio ad Stimulated Emissio The rate of absorptio iduced by the field is E k " (" (" $% ˆ µ # (" &" k k (4. The rate is clearly depedet o

More information

University of Washington Department of Chemistry Chemistry 453 Winter Quarter 2015

University of Washington Department of Chemistry Chemistry 453 Winter Quarter 2015 Uiversity of Wasigto Departmet of Cemistry Cemistry 453 Witer Quarter 15 Lecture 14. /11/15 Recommeded Text Readig: Atkis DePaula: 9.1, 9., 9.3 A. Te Equipartitio Priciple & Eergy Quatizatio Te Equipartio

More information

Chapter 7 : Atomic Structure and Periodicity

Chapter 7 : Atomic Structure and Periodicity Chapter 7 : Atomic Structure ad Periodicity Newto's famous apple tree (actually, a descedet of it) located outside his quarters at Triity. E. Rutherford J. Dalto Newto! Are you correct? Electromagetic

More information

PHYS-3301 Lecture 10. Wave Packet Envelope Wave Properties of Matter and Quantum Mechanics I CHAPTER 5. Announcement. Sep.

PHYS-3301 Lecture 10. Wave Packet Envelope Wave Properties of Matter and Quantum Mechanics I CHAPTER 5. Announcement. Sep. Aoucemet Course webpage http://www.phys.ttu.edu/~slee/3301/ PHYS-3301 Lecture 10 HW3 (due 10/4) Chapter 5 4, 8, 11, 15, 22, 27, 36, 40, 42 Sep. 27, 2018 Exam 1 (10/4) Chapters 3, 4, & 5 CHAPTER 5 Wave

More information

FI 3103 Quantum Physics

FI 3103 Quantum Physics 05/09/04 FI 303 Quatum Pysics Alexader A. Iskadar Pysics of Magetism ad Potoics Researc Group Istitut Tekologi Badug Te Emergece of Quatum Pysics Wave Properties of Particle Bor Atom Alexader A. Iskadar

More information

Why? The atomic nucleus. Radioactivity. Nuclear radiations. The electrons and the nucleus. Length scale of the nature

Why? The atomic nucleus. Radioactivity. Nuclear radiations. The electrons and the nucleus. Length scale of the nature The atomic ucleus. Radioactivity. Nuclear radiatios László Smeller Why? Medical alicatios of the uclear radiatio: - Nuclear imagig - Radiotheray Legth scale of the ature m meter me -3 millimeter size of

More information

ATOMIC STRUCTURE. electron

ATOMIC STRUCTURE. electron J-Physics VRIOUS MODL S FOR STRUCTUR OF TOM TOMIC STRUCTUR Dalto' s Theory very material is composed of miute particles kow as atom. tom is idivisible i.e. it caot be subdivided. It ca either be created

More information

Vibrational Spectroscopy 1

Vibrational Spectroscopy 1 Applied Spectroscopy Vibratioal Spectroscopy Recommeded Readig: Bawell ad McCash Chapter 3 Atkis Physical Chemistry Chapter 6 Itroductio What is it? Vibratioal spectroscopy detects trasitios betwee the

More information

Physics Oct Reading

Physics Oct Reading Physics 301 21-Oct-2002 17-1 Readig Fiish K&K chapter 7 ad start o chapter 8. Also, I m passig out several Physics Today articles. The first is by Graham P. Collis, August, 1995, vol. 48, o. 8, p. 17,

More information

Bohr s Atomic Model Quantum Mechanical Model

Bohr s Atomic Model Quantum Mechanical Model September 7, 0 - Summary - Itroductio to Atomic Theory Bohr s Atomic Model Quatum Mechaical Model 3- Some Defiitio 3- Projects Temperature Pressure Website Subject Areas Plasma is a Mixture of electros,

More information

Why? The atomic nucleus. Radioactivity. Nuclear radiations. Length scale of the nature. The electrons and the nucleus

Why? The atomic nucleus. Radioactivity. Nuclear radiations. Length scale of the nature. The electrons and the nucleus The atomic ucleus. Radioactivity. Nuclear radiatios László Smeller Why? Medical alicatio of uclear radiatio: Nuclear imagig Radiotheray Legth scale of the ature m meter me -3 millimeter size of letters

More information

Atomic Physics 4. Name: Date: 1. The de Broglie wavelength associated with a car moving with a speed of 20 m s 1 is of the order of. A m.

Atomic Physics 4. Name: Date: 1. The de Broglie wavelength associated with a car moving with a speed of 20 m s 1 is of the order of. A m. Name: Date: Atomic Pysics 4 1. Te de Broglie wavelegt associated wit a car movig wit a speed of 0 m s 1 is of te order of A. 10 38 m. B. 10 4 m. C. 10 4 m. D. 10 38 m.. Te diagram below sows tree eergy

More information

This exam is formed of four exercises in four pages numbered from 1 to 4 The use of non-programmable calculator is recommended

This exam is formed of four exercises in four pages numbered from 1 to 4 The use of non-programmable calculator is recommended وزارة التربية والتعلين العالي الوديرية العاهة للتربية دائرة االهتحانات اهتحانات الشهادة الثانىية العاهة الفرع : علىم عاهة مسابقة في مادة الفيزياء المدة ثالث ساعات االسن: الرقن: الدورة العادية للعام This

More information

Atomic and nuclear physics

Atomic and nuclear physics Atomic ad uclear physics X-ray physics X-ray eergy spectroscopy LD Physics Leaflets P6.3.5.4 Ivestigatio of the characteristic spectra as a fuctio of the elemet's atomic umber: K-lies Objects of the experimet

More information

Stellar Helium Burning. He-Burning in massive Stars

Stellar Helium Burning. He-Burning in massive Stars Stellar lium Burig -Burig i massive Stars -burig is igited o the ad ashes of the precedig hydroge burig phase! Most importat reactio -triple alpha process 3 12 C 7.96 MeV Eergy productio i helium burig

More information

Physics 2D Lecture Slides Lecture 22: Feb 22nd 2005

Physics 2D Lecture Slides Lecture 22: Feb 22nd 2005 Physics D Lecture Slides Lecture : Feb d 005 Vivek Sharma UCSD Physics Itroducig the Schrodiger Equatio! (, t) (, t) #! " + U ( ) "(, t) = i!!" m!! t U() = characteristic Potetial of the system Differet

More information

Hydrogen (atoms, molecules) in external fields. Static electric and magnetic fields Oscyllating electromagnetic fields

Hydrogen (atoms, molecules) in external fields. Static electric and magnetic fields Oscyllating electromagnetic fields Hydroge (atoms, molecules) i exteral fields Static electric ad magetic fields Oscyllatig electromagetic fields Everythig said up to ow has to be modified more or less strogly if we cosider atoms (ad ios)

More information

1. Szabo & Ostlund: 2.1, 2.2, 2.4, 2.5, 2.7. These problems are fairly straightforward and I will not discuss them here.

1. Szabo & Ostlund: 2.1, 2.2, 2.4, 2.5, 2.7. These problems are fairly straightforward and I will not discuss them here. Solutio set III.. Szabo & Ostlud:.,.,.,.5,.7. These problems are fairly straightforward ad I will ot discuss them here.. N! N! i= k= N! N! N! N! p p i j pi+ pj i j i j i= j= i= j= AA ˆˆ= ( ) Pˆ ( ) Pˆ

More information

Lecture 6. Semiconductor physics IV. The Semiconductor in Equilibrium

Lecture 6. Semiconductor physics IV. The Semiconductor in Equilibrium Lecture 6 Semicoductor physics IV The Semicoductor i Equilibrium Equilibrium, or thermal equilibrium No exteral forces such as voltages, electric fields. Magetic fields, or temperature gradiets are actig

More information

17 Phonons and conduction electrons in solids (Hiroshi Matsuoka)

17 Phonons and conduction electrons in solids (Hiroshi Matsuoka) 7 Phoos ad coductio electros i solids Hiroshi Matsuoa I this chapter we will discuss a miimal microscopic model for phoos i a solid ad a miimal microscopic model for coductio electros i a simple metal.

More information

Chapter 5 Vibrational Motion

Chapter 5 Vibrational Motion Fall 4 Chapter 5 Vibratioal Motio... 65 Potetial Eergy Surfaces, Rotatios ad Vibratios... 65 Harmoic Oscillator... 67 Geeral Solutio for H.O.: Operator Techique... 68 Vibratioal Selectio Rules... 7 Polyatomic

More information

STRUCTURE OF ATOM MODULE - 7 OBJECTIVES. Notes

STRUCTURE OF ATOM MODULE - 7 OBJECTIVES. Notes 4 STRUCTURE OF ATOM So far you have studied about mechaical, thermal, electrical ad magetic properties of matter. Have you ever thought as to why do differet materials have differet properties? That is,

More information

Office: JILA A709; Phone ;

Office: JILA A709; Phone ; Office: JILA A709; Phoe 303-49-7841; email: weberjm@jila.colorado.edu Problem Set 5 To be retured before the ed of class o Wedesday, September 3, 015 (give to me i perso or slide uder office door). 1.

More information

1. Hydrogen Atom: 3p State

1. Hydrogen Atom: 3p State 7633A QUANTUM MECHANICS I - solutio set - autum. Hydroge Atom: 3p State Let us assume that a hydroge atom is i a 3p state. Show that the radial part of its wave fuctio is r u 3(r) = 4 8 6 e r 3 r(6 r).

More information

Lecture # 07: Flow Visualization techniques: Shadowgraph and Schlieren

Lecture # 07: Flow Visualization techniques: Shadowgraph and Schlieren AerE 311L & AerE343L Lecture Notes Lecture # 07: Flow Visualizatio techiques: Shadowgraph ad Schliere Dr. Hui H Hu Departmet of Aerospace Egieerig owa State Uiversity Ames, owa 50011, U.S.A AerE311L: Lab#01

More information

The Quantum Oscillatory Modulated Potential I The Hydrogen Atom

The Quantum Oscillatory Modulated Potential I The Hydrogen Atom Joural of Moder Physics 3 597-63 http://dx.doi.org/.436/jmp..378 Published Olie July (http://www.scirp.org/joural/jmp) The Quatum Oscillatory Modulated Potetial I The Hydroge Atom Waldemar Woley Filho

More information

The Pendulum. Purpose

The Pendulum. Purpose The Pedulum Purpose To carry out a example illustratig how physics approaches ad solves problems. The example used here is to explore the differet factors that determie the period of motio of a pedulum.

More information

ATOMIC STRUCTURE (ADVANCED) FOUNDATION BUILDER (OBJECTIVE) By law of conservation of mass and change the missing particle in neutron

ATOMIC STRUCTURE (ADVANCED) FOUNDATION BUILDER (OBJECTIVE) By law of conservation of mass and change the missing particle in neutron . (A) Li? e 6 ATOMIC STRUCTURE (ADVANCED) FOUNDATION BUILDER (OBJECTIVE) By law of coservatio of mass ad cage te missig particle i eutro. (D) e ratio lies i te sequece p l M Particle Cage Mass + + + p

More information

Total number of nucleons: mass number 238 Number of protons: atomic number 92U

Total number of nucleons: mass number 238 Number of protons: atomic number 92U 9 The Nucleus Protos Neutros Nucleos Total umber of ucleos: mass umber 8 Number of protos: atomic umber 9U Isotopes: idetical atomic umbers differet mass umbers same chemical properties differet uclear

More information

PHYS-3301 Lecture 9. CHAPTER 5 Wave Properties of Matter and Quantum Mechanics I. 5.3: Electron Scattering. Bohr s Quantization Condition

PHYS-3301 Lecture 9. CHAPTER 5 Wave Properties of Matter and Quantum Mechanics I. 5.3: Electron Scattering. Bohr s Quantization Condition CHAPTER 5 Wave Properties of Matter ad Quatum Mecaics I PHYS-3301 Lecture 9 Sep. 5, 018 5.1 X-Ray Scatterig 5. De Broglie Waves 5.3 Electro Scatterig 5.4 Wave Motio 5.5 Waves or Particles? 5.6 Ucertaity

More information

Semiconductors a brief introduction

Semiconductors a brief introduction Semicoductors a brief itroductio Bad structure from atom to crystal Fermi level carrier cocetratio Dopig Readig: (Sedra/Smith 7 th editio) 1.7-1.9 Trasport (drift-diffusio) Hyperphysics (lik o course homepage)

More information

AIT. Blackbody Radiation IAAT

AIT. Blackbody Radiation IAAT 3 1 Blackbody Radiatio Itroductio 3 2 First radiatio process to look at: radiatio i thermal equilibrium with itself: blackbody radiatio Assumptios: 1. Photos are Bosos, i.e., more tha oe photo per phase

More information

reactions / Fission Classification of nuclear reactions

reactions / Fission Classification of nuclear reactions Classiicatio o uclear reactios reactios / Fissio Geeralities Liquid-drop picture Chai reactios Mass distributio Fissio barrier Double issio barrier Ater the scissio poit Time scale i issio Neutro-iduced

More information

ATOMIC STRUCTURE (MAIN) FOUNDATION BUILDER (OBJECTIVE) By law of conservation of mass and change the missing particle in neutron

ATOMIC STRUCTURE (MAIN) FOUNDATION BUILDER (OBJECTIVE) By law of conservation of mass and change the missing particle in neutron . (A) Li? e 6 4 ATOMIC STRUCTURE (MAIN) FOUNDATION BUILDER (OBJECTIVE) By law of coservatio of mass ad cage te missig particle i eutro. (D) e ratio lies i te sequece p l M Particle Cage Mass + + 4 0 +

More information

Preliminary Examination - Day 1 Thursday, May 12, 2016

Preliminary Examination - Day 1 Thursday, May 12, 2016 UNL - Departmet of Physics ad Astroomy Prelimiary Examiatio - Day Thursday, May, 6 This test covers the topics of Quatum Mechaics (Topic ) ad Electrodyamics (Topic ). Each topic has 4 A questios ad 4 B

More information

Repetition: Refractive Index

Repetition: Refractive Index Repetitio: Refractive Idex (ω) κ(ω) 1 0 ω 0 ω 0 The real part of the refractive idex correspods to refractive idex, as it appears i Sellius law of refractio. The imagiary part correspods to the absorptio

More information

Information Theory Model for Radiation

Information Theory Model for Radiation Joural of Applied Mathematics ad Physics, 26, 4, 6-66 Published Olie August 26 i SciRes. http://www.scirp.org/joural/jamp http://dx.doi.org/.426/jamp.26.487 Iformatio Theory Model for Radiatio Philipp

More information

Lecture 5-2: Polytropes. Literature: MWW chapter 19

Lecture 5-2: Polytropes. Literature: MWW chapter 19 Lecture 5-2: Polytropes Literature: MWW chapter 9!" Preamble The 4 equatios of stellar structure divide ito two groups: Mass ad mometum describig the mechaical structure ad thermal equilibrium ad eergy

More information

genius PHYSICS Atomic structure 1

genius PHYSICS Atomic structure 1 geius PHYSICS tomic structure Importat tomic Models. () Thomso's model J.J. Thomso gave the first idea regardig structure of atom. ccordig to this model. (i) atom is a solid sphere i which etire ad positive

More information

Lecture 25 (Dec. 6, 2017)

Lecture 25 (Dec. 6, 2017) Lecture 5 8.31 Quatum Theory I, Fall 017 106 Lecture 5 (Dec. 6, 017) 5.1 Degeerate Perturbatio Theory Previously, whe discussig perturbatio theory, we restricted ourselves to the case where the uperturbed

More information

Solids - types. correlates with bonding energy

Solids - types. correlates with bonding energy Solids - types MOLCULAR. Set of sigle atoms or molecules boud to adjacet due to weak electric force betwee eutral objects (va der Waals). Stregth depeds o electric dipole momet No free electros poor coductors

More information

Accuracy of TEXTOR He-beam diagnostics

Accuracy of TEXTOR He-beam diagnostics Accuracy of TEXTOR He-beam diagostics O. Schmitz, I.L.Beigma *, L.A. Vaishtei *, A. Pospieszczyk, B. Schweer, M. Krychoviak, U. Samm ad the TEXTOR team Forschugszetrum Jülich,, Jülich, Germay *Lebedev

More information

Acknowledgments. Line Resolved Spectra. Outline. Continuum Processes ATOMIC PROCESSES IN. Spectral Line Intensities. Spectral Line Intensities (2/2)

Acknowledgments. Line Resolved Spectra. Outline. Continuum Processes ATOMIC PROCESSES IN. Spectral Line Intensities. Spectral Line Intensities (2/2) ATOMIC PROCESSES IN PLASMAS IAEA Advaced School o Plasma Spectroscopy ICTP, March 2015 Ackowledgmets I am greatly idebted to Prof. J. L. Schwob from whom I leared most of what I kow about laboratory plasma

More information

Physics 232 Gauge invariance of the magnetic susceptibilty

Physics 232 Gauge invariance of the magnetic susceptibilty Physics 232 Gauge ivariace of the magetic susceptibilty Peter Youg (Dated: Jauary 16, 2006) I. INTRODUCTION We have see i class that the followig additioal terms appear i the Hamiltoia o addig a magetic

More information

ADDITIONAL NON-COULOMB ELECTRON-ELECTRON INTERACTION IN MULTIELECTRON SYSTEMS Каvеrа V.V. Krasnodar, Russia

ADDITIONAL NON-COULOMB ELECTRON-ELECTRON INTERACTION IN MULTIELECTRON SYSTEMS Каvеrа V.V. Krasnodar, Russia ADDITIONAL NON-COULOMB ELECTRON-ELECTRON INTERACTION IN MULTIELECTRON SYSTEMS Каvеrа V.V. Krasodar, Russia E-mail: vad809@rambler.ru Abstract. The author suggests a approach based o the separatio of total

More information

Chem Discussion #13 Chapter 10. Correlation diagrams for diatomic molecules. Key

Chem Discussion #13 Chapter 10. Correlation diagrams for diatomic molecules. Key Chem 101 017 Discussio #13 Chapter 10. Correlatio diagrams for diatomic molecules. Key 1. Below is a plot of the first 10 ioizatio eergies for a sigle atom i 3 rd row of the periodic table. The x- axis

More information

Lecture 13: Laser-Induced Fluorescence: Two-Level Model

Lecture 13: Laser-Induced Fluorescence: Two-Level Model Lecture 3: Laser-Iduced Fluorescece: Two-Level Model. Itroductio ad backgroud. Typical experimetal setup 3. Sigal level (steady & pulsed) 4. Two-level model 5. Detectio limits (pulsed laser) 6. Characteristic

More information

A Brief Introduction to the Physical Basis for Electron Spin Resonance

A Brief Introduction to the Physical Basis for Electron Spin Resonance A Brief Itroductio to the Physical Basis for Electro Spi Resoace I ESR measuremets, the sample uder study is exposed to a large slowly varyig magetic field ad a microwave frequecy magetic field orieted

More information

INVESTIGATION OF RADIOACTIVE EQUILIBRIUM AND MEASURING THE HALF-LIFE OF 137m Ba

INVESTIGATION OF RADIOACTIVE EQUILIBRIUM AND MEASURING THE HALF-LIFE OF 137m Ba Vilius Uiversity Faculty of Physics Departmet of Solid State Electroics Laboratory of Applied Nuclear Physics Experimet No. 5 INVESTIGATION OF RADIOACTIVE EQUILIBRIUM AND MEASURING THE HALF-LIFE OF 37m

More information

Does God Play Dice with Universe: The Hydrogen Atomic model of Bohr and de Broglie

Does God Play Dice with Universe: The Hydrogen Atomic model of Bohr and de Broglie Does God Play Dice with Uiverse: The Hydroge Atomic model of Bohr ad de Broglie Pavel S. Kameov, Faculty of Physics, Uiversity of Sofia, Sofia-1164, Bulgaria I memory of Luis de Broglie 1. Itroductio.

More information

Lecture 1 Probability and Statistics

Lecture 1 Probability and Statistics Wikipedia: Lecture 1 Probability ad Statistics Bejami Disraeli, British statesma ad literary figure (1804 1881): There are three kids of lies: lies, damed lies, ad statistics. popularized i US by Mark

More information

The Transition Dipole Moment

The Transition Dipole Moment The Trasitio Dipole Momet Iteractio of Light with Matter The probability that a molecule absorbs or emits light ad udergoes a trasitio from a iitial to a fial state is give by the Eistei coefficiet, B

More information

The Transition Dipole Moment

The Transition Dipole Moment The Trasitio Dipole Momet Iteractio of Light with Matter The probability that a molecule absorbs or emits light ad udergoes a trasitio from a iitial to a fial state is give by the Eistei coefficiet, B

More information

Matsubara-Green s Functions

Matsubara-Green s Functions Matsubara-Gree s Fuctios Time Orderig : Cosider the followig operator If H = H the we ca trivially factorise this as, E(s = e s(h+ E(s = e sh e s I geeral this is ot true. However for practical applicatio

More information

Miscellaneous Notes. Lecture 19, p 1

Miscellaneous Notes. Lecture 19, p 1 Miscellaeous Notes The ed is ear do t get behid. All Excuses must be take to 233 Loomis before oo, Thur, Apr. 25. The PHYS 213 fial exam times are * 8-10 AM, Moday, May 6 * 1:30-3:30 PM, Wed, May 8 The

More information

Lecture #1 Nasser S. Alzayed.

Lecture #1 Nasser S. Alzayed. Lecture #1 Nasser S. Alzayed alzayed@ksu.edu.sa Chapter 6: Free Electro Fermi Gas Itroductio We ca uderstad may physical properties of metals, ad ot oly of the simple metals, i terms of the free electro

More information

Complex Analysis Spring 2001 Homework I Solution

Complex Analysis Spring 2001 Homework I Solution Complex Aalysis Sprig 2001 Homework I Solutio 1. Coway, Chapter 1, sectio 3, problem 3. Describe the set of poits satisfyig the equatio z a z + a = 2c, where c > 0 ad a R. To begi, we see from the triagle

More information

2C09 Design for seismic and climate changes

2C09 Design for seismic and climate changes 2C09 Desig for seismic ad climate chages Lecture 02: Dyamic respose of sigle-degree-of-freedom systems I Daiel Grecea, Politehica Uiversity of Timisoara 10/03/2014 Europea Erasmus Mudus Master Course Sustaiable

More information

is completely general whenever you have waves from two sources interfering. 2

is completely general whenever you have waves from two sources interfering. 2 MAKNG SENSE OF THE EQUATON SHEET terferece & Diffrctio NTERFERENCE r1 r d si. Equtio for pth legth differece. r1 r is completely geerl. Use si oly whe the two sources re fr wy from the observtio poit.

More information

Kinetics of Complex Reactions

Kinetics of Complex Reactions Kietics of Complex Reactios by Flick Colema Departmet of Chemistry Wellesley College Wellesley MA 28 wcolema@wellesley.edu Copyright Flick Colema 996. All rights reserved. You are welcome to use this documet

More information

Optics. n n. sin. 1. law of rectilinear propagation 2. law of reflection = 3. law of refraction

Optics. n n. sin. 1. law of rectilinear propagation 2. law of reflection = 3. law of refraction Optics What is light? Visible electromagetic radiatio Geometrical optics (model) Light-ray: extremely thi parallel light beam Usig this model, the explaatio of several optical pheomea ca be give as the

More information

ELECTRICAL PROPEORTIES OF SOLIDS

ELECTRICAL PROPEORTIES OF SOLIDS DO PHYSICS ONLINE ELECTRICAL PROPEORTIES OF SOLIDS ATOMIC STRUCTURE ucleus: rotos () & electros electros (-): electro cloud h h DE BROGLIE wave model of articles mv ELECTRONS IN ATOMS eergy levels i atoms

More information

MODERN PHYSICS. Contents. Theory Exercise Exercise Exercise Exercise Answer Key

MODERN PHYSICS. Contents. Theory Exercise Exercise Exercise Exercise Answer Key MODERN PHYSICS Cotets Topic Page No. Teory 0-03 Exercise - 04 - Exercise - - 5 Exercise - 3 5-4 Exercise - 4 4-5 Aswer Key 6-7 Syllabus Potoelectric effect ; Bor s teory of ydroge like atoms ; Caracteristic

More information

Chapters 31 Atomic Physics

Chapters 31 Atomic Physics Chapters 31 Atomic Physics 1 Overview of Chapter 31 Early Models of the Atom The Spectrum of Atomic Hydrogen Bohr s Model of the Hydrogen Atom de Broglie Waves and the Bohr Model The Quantum Mechanical

More information

The Wave Function and Quantum Reality

The Wave Function and Quantum Reality The Wave Fuctio ad Quatum Reality Sha Gao Uit for History ad Philosophy of Sciece & Cetre for Time, SOPHI Uiversity of Sydey, Sydey, NSW 006, Australia Abstract. We ivestigate the meaig of the wave fuctio

More information

Hilbert Space Methods Used in a First Course in Quantum Mechanics

Hilbert Space Methods Used in a First Course in Quantum Mechanics Hilbert Space Methods Used i a First Course i Quatum Mechaics Victor Poliger Physics/Mathematics Bellevue College 03/07/3-04//3 Outlie The Ifiite Square Well: A Follow-Up Timelie of basic evets Statistical

More information

Zumdahl (pp [atomic properties] ), [ionic radii] )

Zumdahl (pp [atomic properties] ), [ionic radii] ) Chemistry 1B-AL Fall 2016 advetures lectures 7-8 Zumdahl (pp. 571-582 [atomic properties] ), 606-609 [ioic radii] ) 1 Chemistry 1B AL Electroic Structure ad Periodic Properties of Atoms 2 Zumdahl (pp.

More information

LIGHT ION REACTION MECHANISM

LIGHT ION REACTION MECHANISM Proceedigs of the 1983 RCNP Iteratioal Symposium o LIGHT ION REACTION MECHANISM 16-20 MAY, 1983 Edited by H. Ogata, T. Kammuri ad I. Katayama RESEARCH CENTER FOR NUCLEAR PHYSICS OSAKA UNIVERSITY IBARAKI,

More information

EE 485 Introduction to Photonics Photon Optics and Photon Statistics

EE 485 Introduction to Photonics Photon Optics and Photon Statistics Itroductio to Photoics Photo Optics ad Photo Statistics Historical Origi Photo-electric Effect (Eistei, 905) Clea metal V stop Differet metals, same slope Light I Slope h/q ν c/λ Curret flows for λ < λ

More information

Particle nature of light & Quantization

Particle nature of light & Quantization Particle nature of light & Quantization A quantity is quantized if its possible values are limited to a discrete set. An example from classical physics is the allowed frequencies of standing waves on a

More information

CHAPTER 8 SYSTEMS OF PARTICLES

CHAPTER 8 SYSTEMS OF PARTICLES CHAPTER 8 SYSTES OF PARTICLES CHAPTER 8 COLLISIONS 45 8. CENTER OF ASS The ceter of mass of a system of particles or a rigid body is the poit at which all of the mass are cosidered to be cocetrated there

More information

h p L= mvr = n atomic absorption and emission of light 1889 Rydberg generalized to other H emission lines: (Z ) n (ev) 1 2 ke Z E= mv -

h p L= mvr = n atomic absorption and emission of light 1889 Rydberg generalized to other H emission lines: (Z ) n (ev) 1 2 ke Z E= mv - atomic absorption and emission of light 1889 Rydberg generalized to other H emission lines: mv r n r.53 Z ke Z = r (A) * (Z ) E n -13.6 (ev) n h p o L= mvr = n 1 ke Z E= mv - r Mosley's Law E E f n E n1

More information

Casimir-Polder shifts on quantum levitation states 1

Casimir-Polder shifts on quantum levitation states 1 Casimir-Polder shifts o quatum levitatio states 1 Pierre-Philippe Crépi Laboratoire Kastler Brossel supervised by S. Reyaud, R. Guérout ad N. Cherroret With discussios with V. V. Nesvizhevsky ad A. Yu.

More information

Radiative Lifetimes of Rydberg States in Neutral Gallium

Radiative Lifetimes of Rydberg States in Neutral Gallium Vol. 115 (2009) ACTA PHYSICA POLONICA A No. 3 Radiative Lifetimes of Rydberg States i Neutral Gallium M. Yildiz, G. Çelik ad H.Ş. Kiliç Departmet of Physics, Faculty of Arts ad Sciece, Selçuk Uiversity,

More information

SOLUTIONS: ECE 606 Homework Week 7 Mark Lundstrom Purdue University (revised 3/27/13) e E i E T

SOLUTIONS: ECE 606 Homework Week 7 Mark Lundstrom Purdue University (revised 3/27/13) e E i E T SOUIONS: ECE 606 Homework Week 7 Mark udstrom Purdue Uiversity (revised 3/27/13) 1) Cosider a - type semicoductor for which the oly states i the badgap are door levels (i.e. ( E = E D ). Begi with the

More information

CHM 424 EXAM 2 - COVER PAGE FALL

CHM 424 EXAM 2 - COVER PAGE FALL CHM 44 EXAM - COVER PAGE FALL 007 There are six umbered pages with five questios. Aswer the questios o the exam. Exams doe i ik are eligible for regrade, those doe i pecil will ot be regraded. coulomb

More information

Outline 24. QUANTUM PHYSICS. Liew Sau Poh. Objectives. Objectives. Objectives. Objectives Photon. Objectives

Outline 24. QUANTUM PHYSICS. Liew Sau Poh. Objectives. Objectives. Objectives. Objectives Photon. Objectives Outlie 4. QUNTUM PHYSICS Liew Sau Poh 4. Photos 4. Wave-particle duality 4.3 tomic structure 4.4 X-rays 4.5 Naosciece Objectives (a) describe importat observatios i photoelectric emissio experimets (b)

More information

Electric dipole moment of nuclei

Electric dipole moment of nuclei Electric dipole momet of uclei I collaboratio with odoka Yamaaka (ithes Group, RIKE) E. Hiyama (RIKE), T. Yamada (Kato Gakui Uiv.), Y. Fuaki (RIKE) 2016/03/02 RIKE Itroductio CP violatio of Stadard model

More information

This presentation was created for the students of technical lyceum originally.

This presentation was created for the students of technical lyceum originally. Electro cloud This presetatio was created for the studets of techical lyceum origially. Some years ago the presetatio was itroduced durig a sciece lessos for studets i appreticeship course because of their

More information