Chapter 4. Interaction of Many-Electron Atoms with Electromagnetic Radiation
|
|
- Ernest Tate
- 5 years ago
- Views:
Transcription
1 Cpte 4. Intecton o ny-ecton Atos wt ectognetc Rdton Redng: Bnsden & ocn Cpte 9
2 ny-ecton Atos n n Fed Htonn V t A e p t A e p V t ea p H H Te-ndependent Htonn nt t H Intecton o te to wt te dton ed Te dependent cödnge equton t X t A e V t X t Ψ Ψ q q q X K ~ wek ed t R e e I c W 4 4 ε πε π Tnston te n te dpoe ppoton sopton Ω d c W s 4 ε πε π spontneous esson
3 eecton Rues o ectc poe Tnstons [ ] H negy egensttes poe t eeent * pec coponents ε ε q q ± q ± : eectonc conguton e.g. He s ± y Wgne-ckt teoe q : vecto opeto q Cesc-Godon coecent c q q vnses uness eecton ues o tnstons ± ± pote s ue: toc sttes ust ve opposte pty P e R
4 - coupng: enegy egensttes poe opeto s ndependent o spn. δ q eecton ues o tnstons ± ± ± ± c One eecton tnston ost usu cse : ± ± Hypene stuctue B Cpte 5. H I wee I s te nuce spn ngu oentu. F I Tot ngu oentu o te to nuceus eectons eecton ues o tnstons F ± F F F ±
5 Oscto nd ne tengts k k k k k Oscto stengt < > sopton esson Tos-Rece-Kun su ue k k Tnstons etween two toc sttes nd s c W α α: ne stuctue constnt c W s α wee not syetc
6 ne stengt: syeted c c α α 4 4 I c W c W s π Tnston tes o spontneous esson sopton nd stuted esson ne ntensty o ny tos s W nue o tos n nt sttes e.g. / 5% 5%
7 gnetc poe nd ectc Qudupoe Tnstons poe ppoton t ~ Å π λ 5 Å k k << λ k e k k! k e ˆ ε k ˆ ε W ~ ˆ ε k ˆ ε Tke ~ k eˆ ˆ ε eˆ k ˆ ε k c
8 y p p Fst te [ ] [ ] H H H H p p [ ] [ ] H dt d p H dt d Usng econd te y c c c ~ ~ ~
9 gnetc dpoe tnstons ~ y c Ot gnetc dpoe oent: e e µ µ B µ B : Bo gneton e e e µ IA π π v -e τ π / v Tot gnetc dpoe oentu: e e µ B µ µ µ ~ Repceent o : ~ c c y y dˆ dˆ k ˆ ε µ B c t eeents o tnston y y e k eˆ ˆ ε eˆ
10 eecton ues o tnstons ± ± d ˆ // eˆ : dˆ eˆ : ± Z c Te toc sttes nd ust ve te se pty. Z ~ : even pty tnston seecton ues o - coupng s Z tos coutes wt s ndependent o c n tnstons e owed ony wtn se ne stuctue utpet: cowve o do-equency egon ~. - GH s s tnston / / Two poton esson nd ode petuton tnston o ge Z tos
11 ectc qudupoe tnstons ~ c ~ depends on k // eˆ nd ˆ ε // eˆ. eecton ues o tnstons eectc qudupoe oent ± ± ± ± c Te toc sttes nd ust ve te se pty ~ : even pty tnston seecton ues o - coupng s Z tos ± ± c ± ± One eecton tnston : ± ± ±
12 Oygen to: gound stte conguton s s p 4 P even pty s s p 4 : tnston.4 ev n geen K Buj nd C Zeppen. o Pys. B P H c H c H eecton ue o tnstons etween coponents o ypene stuctue F ± ± F F
13 pect o te Aks Ak ets: K R Cs F cosed se n s Gound stte conguton : s s : s s p 6 s K : s s p 6 s p 6 4s Z- eecton sceenng e V 4πε coe: specy syetc pc ou o enegy eves: n n µ n. u. wee µ n e quntu deects µ n α n* n α
14 sp sees ns n p duse sees nd n p esonnce nes np n s undent sees n n d sodu -nes yeow ceenng: ge Hge n Asopton spect n s np ν R * * n n s n np sson spect Fne stuctue np P λn H j / 5 λn 4 4 P j / P j / j j 4 j λn /
15 pect o Heu nd te Akne ts Heu nd Ak ets: He Be g C B Zn Cd Hg cosed se n s He Gound stte conguton He : s Be : s s g : s s p 6 s One eecton tnston: n s n s n coe: specy syetc C
16 Two eectons ectton s ss p s He s p P p s e He s dpoe dton e utoonton s s p s Rpd pocess: od nd wek spect nes
17 Fne stuctue H ξ pn-ot ntecton: pn-ote ot ntecton: V B µ π µ vnses o snget sttes pn-spn ntecton: pe Tpet sttes o s n wt s Ze n Z V
18 V V X n V n α X X X pn-spn ntecton: wee Z α pn-ot ntecton: α pn-ote ot ntecton: [ ] 4 Z α [ ] 4 Z X α Fo
19 Atos wt eve Optcy Actve ectons Ads to nye epeent spect eecton ues: nue o spect nes o tnstons etween two tes ndè ntev ue - coupng A A [ ] Tot spttng o te te - coupng A A < v Te etve ntenstes o te utpet nes depend ony on ngu oentu ctos. e.g. stongest nes
20 X-Ry pect Z σ n n. u. σ n << n K-se Z X-y Potoesson XP ~. KeV e K α K β cosed se vence eectons -se Auge tnstons -se
21 tk ect -eecton to n sttc uno eectc ed e ˆ e H Intecton enegy : eve stng ng sttes Te-ndependent petuton teoy pty st ode second ode Wgne-ckt teoe: q q B A
22 pttng o sodu -nes A B onnt contuton s o te neest eve o opposte pty to te eve. Gound stte <
23 Zeen ect -eecton to n sttc uno gnetc ed Intecton enegy : B µ B µ BB H µ B B stong ed cse no Zeen eect: B H >> H eˆ spn-ot coupng µ B B Inteedte cse Pscen-Bck eect: H A petuton µ BB A wek ed cse noous Zeen eect: petuton µ B B gµ BB ndè g cto g H << H
ELECTROMAGNETISM. at a point whose position vector with respect to a current element i d l is r. According to this law :
ELECTROMAGNETISM ot-svt Lw: Ths w s used to fnd the gnetc fed d t pont whose poston vecto wth espect to cuent eeent d s. Accodng to ths w : µ d ˆ d = 4π d d The tot fed = d θ P whee ˆ s unt vecto n the
More informationAngular Momentum in Spherical Symmetry
Angu Moentu n Sphec Set Angu Moentu n Sphec Set 6 Quntu Mechncs Pof. Y. F. Chen Angu Moentu n Sphec Set The concept of ngu oentu ps cuc oe n the theedenson 3D Schödnge we equton. The ethod of septon w
More informationAddition of Angular Momentum
Addition of Angula Moentu We ve leaned tat angula oentu i ipotant in quantu ecanic Obital angula oentu L Spin angula oentu S Fo ultielecton ato, we need to lean to add angula oentu Multiple electon, eac
More informationP a g e 5 1 of R e p o r t P B 4 / 0 9
P a g e 5 1 of R e p o r t P B 4 / 0 9 J A R T a l s o c o n c l u d e d t h a t a l t h o u g h t h e i n t e n t o f N e l s o n s r e h a b i l i t a t i o n p l a n i s t o e n h a n c e c o n n e
More informationT h e C S E T I P r o j e c t
T h e P r o j e c t T H E P R O J E C T T A B L E O F C O N T E N T S A r t i c l e P a g e C o m p r e h e n s i v e A s s es s m e n t o f t h e U F O / E T I P h e n o m e n o n M a y 1 9 9 1 1 E T
More informationk p theory for bulk semiconductors
p theory for bu seconductors The attce perodc ndependent partce wave equaton s gven by p + V r + V p + δ H rψ ( r ) = εψ ( r ) (A) 4c In Eq. (A) V ( r ) s the effectve attce perodc potenta caused by the
More informationLecture 1. time, say t=0, to find the wavefunction at any subsequent time t. This can be carried out by
Lectue The Schödinge equation In quantum mechanics, the fundamenta quantity that descibes both the patice-ike and waveike chaacteistics of patices is wavefunction, Ψ(. The pobabiity of finding a patice
More informationCOMP 465: Data Mining More on PageRank
COMP 465: Dt Mnng Moe on PgeRnk Sldes Adpted Fo: www.ds.og (Mnng Mssve Dtsets) Powe Iteton: Set = 1/ 1: = 2: = Goto 1 Exple: d 1/3 1/3 5/12 9/24 6/15 = 1/3 3/6 1/3 11/24 6/15 1/3 1/6 3/12 1/6 3/15 Iteton
More information176 5 t h Fl oo r. 337 P o ly me r Ma te ri al s
A g la di ou s F. L. 462 E l ec tr on ic D ev el op me nt A i ng er A.W.S. 371 C. A. M. A l ex an de r 236 A d mi ni st ra ti on R. H. (M rs ) A n dr ew s P. V. 326 O p ti ca l Tr an sm is si on A p ps
More informationI M P O R T A N T S A F E T Y I N S T R U C T I O N S W h e n u s i n g t h i s e l e c t r o n i c d e v i c e, b a s i c p r e c a u t i o n s s h o
I M P O R T A N T S A F E T Y I N S T R U C T I O N S W h e n u s i n g t h i s e l e c t r o n i c d e v i c e, b a s i c p r e c a u t i o n s s h o u l d a l w a y s b e t a k e n, i n c l u d f o l
More informationρ θ φ δ δ θ δ φ δ φ π δ φ π δ φ π
Physics 6 Fin Ex Dec. 6, ( pts Fou point chges with chge ± q e nged s in Figue. (5 pts. Wht is the chge density function ρ (, θφ,? (,, q ( ( cos ( / + ( ( / / ρ θ φ δ δ θ δ φ δ φ π δ φ π δ φ π b (5 pts.
More informationComplex atoms and the Periodic System of the elements
Complex atoms and the Peodc System of the elements Non-cental foces due to electon epulson Cental feld appoxmaton electonc obtals lft degeneacy of l E n l = R( hc) ( n δ ) l Aufbau pncple Lectue Notes
More information_ J.. C C A 551NED. - n R ' ' t i :. t ; . b c c : : I I .., I AS IEC. r '2 5? 9
C C A 55NED n R 5 0 9 b c c \ { s AS EC 2 5? 9 Con 0 \ 0265 o + s ^! 4 y!! {! w Y n < R > s s = ~ C c [ + * c n j R c C / e A / = + j ) d /! Y 6 ] s v * ^ / ) v } > { ± n S = S w c s y c C { ~! > R = n
More informationExecutive Committee and Officers ( )
Gifted and Talented International V o l u m e 2 4, N u m b e r 2, D e c e m b e r, 2 0 0 9. G i f t e d a n d T a l e n t e d I n t e r n a t i o n a2 l 4 ( 2), D e c e m b e r, 2 0 0 9. 1 T h e W o r
More informationP a g e 3 6 of R e p o r t P B 4 / 0 9
P a g e 3 6 of R e p o r t P B 4 / 0 9 p r o t e c t h um a n h e a l t h a n d p r o p e r t y fr om t h e d a n g e rs i n h e r e n t i n m i n i n g o p e r a t i o n s s u c h a s a q u a r r y. J
More informationA L A BA M A L A W R E V IE W
A L A BA M A L A W R E V IE W Volume 52 Fall 2000 Number 1 B E F O R E D I S A B I L I T Y C I V I L R I G HT S : C I V I L W A R P E N S I O N S A N D TH E P O L I T I C S O F D I S A B I L I T Y I N
More informationPHY121 Formula Sheet
HY Foula Sheet One Denson t t Equatons o oton l Δ t Δ d d d d a d + at t + at a + t + ½at² + a( - ) ojectle oton y cos θ sn θ gt ( cos θ) t y ( sn θ) t ½ gt y a a sn θ g sn θ g otatonal a a a + a t Ccula
More informationTime Evolution of Matter States
Tie Evolution of Matter States W. M. Hetherington February 15, 1 The Tie-Evolution Operat The tie-evolution of a wavefunction is deterined by the effect of a tie evolution operat through the relation Ψ
More informationAn action with positive kinetic energy term for general relativity. T. Mei
An ton wt post nt ny t fo n tty T (Dptnt of Jon Cnt Cn o Unsty Wn H PRO Pop s Rp of Cn E-: to@nn tow@pwn ) Astt: At fst w stt so sts n X: 7769 n tn sn post nt ny oont onton n y X: 7769 w psnt n ton wt
More informationTheorem 1. An undirected graph is a tree if and only if there is a unique simple path between any two of its vertices.
Cptr 11: Trs 11.1 - Introuton to Trs Dnton 1 (Tr). A tr s onnt unrt rp wt no sp ruts. Tor 1. An unrt rp s tr n ony tr s unqu sp pt twn ny two o ts vrts. Dnton 2. A root tr s tr n w on vrtx s n snt s t
More informationNuclear Physics (7 th lecture)
Gaa ecay (cont.) Su ues Nucea Physcs (7 th ectue) Content Measung ethos o the gaa ecay constant Gaa-gaa angua coeaton (utoaty eas.) Nucea oes #: qu o oe Nucea oes #: The Fe-gas oe Gaa-ecay Suay o evous
More informationChapter Runge-Kutta 2nd Order Method for Ordinary Differential Equations
Cter. Runge-Kutt nd Order Metod or Ordnr Derentl Eutons Ater redng ts cter ou sould be ble to:. understnd te Runge-Kutt nd order metod or ordnr derentl eutons nd ow to use t to solve roblems. Wt s te Runge-Kutt
More informationAN ALGEBRAIC APPROACH TO M-BAND WAVELETS CONSTRUCTION
AN ALGEBRAIC APPROACH TO -BAN WAELETS CONSTRUCTION Toy L Qy S Pewe Ho Ntol Lotoy o e Peeto Pe Uety Be 8 P. R. C Att T e eet le o to ott - otool welet e. A yte of ott eto ote fo - otool flte te olto e o
More informationMULTIPOLE FIELDS. Multipoles, 2 l poles. Monopoles, dipoles, quadrupoles, octupoles... Electric Dipole R 1 R 2. P(r,θ,φ) e r
MULTIPOLE FIELDS Mutpoes poes. Monopoes dpoes quadupoes octupoes... 4 8 6 Eectc Dpoe +q O θ e R R P(θφ) -q e The potenta at the fed pont P(θφ) s ( θϕ )= q R R Bo E. Seneus : Now R = ( e) = + cosθ R = (
More informationPHYS 2421 Fields and Waves
PHYS 242 Felds nd Wves Instucto: Joge A. López Offce: PSCI 29 A, Phone: 747-7528 Textook: Unvesty Physcs e, Young nd Feedmn 23. Electc potentl enegy 23.2 Electc potentl 23.3 Clcultng electc potentl 23.4
More informationOH BOY! Story. N a r r a t iv e a n d o bj e c t s th ea t e r Fo r a l l a g e s, fr o m th e a ge of 9
OH BOY! O h Boy!, was or igin a lly cr eat ed in F r en ch an d was a m a jor s u cc ess on t h e Fr en ch st a ge f or young au di enc es. It h a s b een s een by ap pr ox i ma t ely 175,000 sp ect at
More informationMagnetism. 1 Paramagnetism. 2 Magnetic order. Introduction. Technology. Our first contact with magnetism. Plasma spectroscopy, Zeeman effect
agnetm Introducton magnetm nothng new... Paramagnetm agnetc order Our frt contact wth magnetm Technoogy agnetc Reonance Imagng Pama pectrocopy, Zeeman effect Qu. What are the three ource of atomc magnetm
More informationThree-dimensional systems with spherical symmetry
Thee-dimensiona systems with spheica symmety Thee-dimensiona systems with spheica symmety 006 Quantum Mechanics Pof. Y. F. Chen Thee-dimensiona systems with spheica symmety We conside a patice moving in
More informationObjectives. We will also get to know about the wavefunction and its use in developing the concept of the structure of atoms.
Modue "Atomic physics and atomic stuctue" Lectue 7 Quantum Mechanica teatment of One-eecton atoms Page 1 Objectives In this ectue, we wi appy the Schodinge Equation to the simpe system Hydogen and compae
More informationThe Electronic Structure of Atoms
The Electronic Structure of Atoms Classical Hydrogen-like atoms: Atomic Scale: 10-10 m or 1 Å + - Proton mass : Electron mass 1836 : 1 Problems with classical interpretation: - Should not be stable (electron
More informationChapter 8. Linear Momentum, Impulse, and Collisions
Chapte 8 Lnea oentu, Ipulse, and Collsons 8. Lnea oentu and Ipulse The lnea oentu p of a patcle of ass ovng wth velocty v s defned as: p " v ote that p s a vecto that ponts n the sae decton as the velocty
More informationI N A C O M P L E X W O R L D
IS L A M I C E C O N O M I C S I N A C O M P L E X W O R L D E x p l o r a t i o n s i n A g-b eanste d S i m u l a t i o n S a m i A l-s u w a i l e m 1 4 2 9 H 2 0 0 8 I s l a m i c D e v e l o p m e
More informationTHIS PAGE DECLASSIFIED IAW EO IRIS u blic Record. Key I fo mation. Ma n: AIR MATERIEL COMM ND. Adm ni trative Mar ings.
T H S PA G E D E CLA SSFED AW E O 2958 RS u blc Recod Key fo maon Ma n AR MATEREL COMM ND D cumen Type Call N u b e 03 V 7 Rcvd Rel 98 / 0 ndexe D 38 Eneed Dae RS l umbe 0 0 4 2 3 5 6 C D QC d Dac A cesson
More informationTHIS PAGE DECLASSIFIED IAW E
THS PAGE DECLASSFED AW E0 2958 BL K THS PAGE DECLASSFED AW E0 2958 THS PAGE DECLASSFED AW E0 2958 B L K THS PAGE DECLASSFED AW E0 2958 THS PAGE DECLASSFED AW EO 2958 THS PAGE DECLASSFED AW EO 2958 THS
More informationLectures # He-like systems. October 31 November 4,6
Lectue #5-7 7 Octoe 3 oveme 4,6 Self-conitent field Htee-Foc eqution: He-lie ytem Htee-Foc eqution: cloed-hell hell ytem Chpte 3, pge 6-77, Lectue on Atomic Phyic He-lie ytem H (, h ( + h ( + h ( Z Z:
More informationSUPPLEMENTARY INFORMATION
In the format provided by the authors and unedited. NATURE PHYSICS www.nature.com/naturephysics 1 285 x 5 15 5 25 1 1 Ω/µ 3 x C c = 4 6.5 3 µ 2 ε r =7 1.4 9 11 2 1 54 12 1 2 4 12 2 12 µ 2 12 12 12 12 NATURE
More informationNeural Network Introduction. Hung-yi Lee
Neu Neto Intoducton Hung- ee Reve: Supevsed enng Mode Hpothess Functon Set f, f : : (e) Tnng: Pc the est Functon f * Best Functon f * Testng: f Tnng Dt : functon nput : functon output, ˆ,, ˆ, Neu Neto
More informationw x a f f s t p q 4 r u v 5 i l h m o k j d g DT Competition, 1.8/1.6 Stainless, Black S, M, L, XL Matte Raw/Yellow
HELION CARBON TEAM S, M, L, XL M R/Y COR XC Py, FOC U Cn F, 110 T Innn Dn 27. AOS Snn Sy /F Ln, P, 1 1/8"-1 1/2" In H T, n 12 12 M D F 32 FLOAT 27. CTD FIT /A K, 110 T, 1QR, / FIT D, L & Rn A, T Ay S DEVICE
More informationEQUATION SHEETS FOR ELEC
QUTON SHTS FO C 47 Fbuay 7 QUTON SHTS FO C 47 Fbuay 7 hs hυ h ω ( J ) h.4 ω υ ( µ ) ( ) h h k π υ ε ( / s ) G Os (Us > x < a ) Sll s aw s s s Shal z z Shal buay (, aus ) z y y z z z Shal ls ( s sua, s
More informationFI 2201 Electromagnetism
FI 1 Electomgnetism Alexnde A. Isknd, Ph.D. Physics of Mgnetism nd Photonics Resech Goup Electosttics ELECTRIC PTENTIALS 1 Recll tht we e inteested to clculte the electic field of some chge distiution.
More informationChapter 3 Basic Crystallography and Electron Diffraction from Crystals. Lecture 9. CHEM 793, 2008 Fall
Cpte 3 Bsic Cystopy nd Eecton Diffction fom Cysts Lectue 9 Top of tin foi Cyst pne () Bottom of tin foi B Lw d sinθ n Equtions connectin te Cyst metes (,, ) nd d-spcin wit bem pmetes () ( ) ne B Lw d (nm)
More informationFractional Integrals Involving Generalized Polynomials And Multivariable Function
IOSR Joual of ateatcs (IOSRJ) ISSN: 78-578 Volue, Issue 5 (Jul-Aug 0), PP 05- wwwosoualsog Factoal Itegals Ivolvg Geealzed Poloals Ad ultvaable Fucto D Neela Pade ad Resa Ka Deatet of ateatcs APS uvest
More informationkind read i i i i i i
T u Mu P W NNG: Wu 1J1:9 u P OUT, 1J1: 6-10. u u u, u u, u' u u. v v 53:10-1 1' LXX x, u b : P u, N u, v u u u ( P ' "5 v" k ) k z u) ( ( k, u) ku ( u, k k, ub) ( u b u) k ( b Mk u, Ju) 1 J1:9 T Pb- v
More informationRydberg-Rydberg Interactions
Rydbeg-Rydbeg Inteactions F. Robicheaux Aubun Univesity Rydbeg gas goes to plasma Dipole blockade Coheent pocesses in fozen Rydbeg gases (expts) Theoetical investigation of an excitation hopping though
More informationATMO 551a Fall 08. Diffusion
Diffusion Diffusion is a net tanspot of olecules o enegy o oentu o fo a egion of highe concentation to one of lowe concentation by ando olecula) otion. We will look at diffusion in gases. Mean fee path
More information4) Magnetic confinement of plasma
4) Magneti onfineent of plasa Due to the shielding in the plasa, thee is alost no ontol with eleti fields. A ontol is possible with agneti fields, as patiles ae bound to the field lines. This is alled
More informationSlide 1. Quantum Mechanics: the Practice
Slde Quantum Mecancs: te Pactce Slde Remnde: Electons As Waves Wavelengt momentum = Planck? λ p = = 6.6 x 0-34 J s Te wave s an exctaton a vbaton: We need to know te ampltude of te exctaton at evey pont
More informationPhysics 139B Solutions to Homework Set 3 Fall 2009
Physics 139B Solutions to Hoework Set 3 Fall 009 1. Consider a particle of ass attached to a rigid assless rod of fixed length R whose other end is fixed at the origin. The rod is free to rotate about
More informationLesson Ten. What role does energy play in chemical reactions? Grade 8. Science. 90 minutes ENGLISH LANGUAGE ARTS
Lesson Ten What role does energy play in chemical reactions? Science Asking Questions, Developing Models, Investigating, Analyzing Data and Obtaining, Evaluating, and Communicating Information ENGLISH
More informationNXO a Spatially High Order Finite Volume Numerical Method for Compressible Flows
NXO Spty Hgh Ode Fnte Voume Nume Method fo Compebe Fow Jen-Me e Gouez One CFD Deptment Fouth HO CFD Wohop Heon June 4th B of the NXO heme Eue o Nve-Stoe fo pefet g w of tte dof pe e nd pe equton Voume
More informationSoftware Process Models there are many process model s in th e li t e ra t u re, s om e a r e prescriptions and some are descriptions you need to mode
Unit 2 : Software Process O b j ec t i ve This unit introduces software systems engineering through a discussion of software processes and their principal characteristics. In order to achieve the desireable
More information( ) rad ( 2.0 s) = 168 rad
.) α 0.450 ω o 0 and ω 8.00 ω αt + ω o o t ω ω o α HO 9 Solution 8.00 0 0.450 7.8 b.) ω ω o + αδθ o Δθ ω 8.00 0 ω o α 0.450 7. o Δθ 7. ev.3 ev π.) ω o.50, α 0.300, Δθ 3.50 ev π 7π ev ω ω o + αδθ o ω ω
More informationAPPLICATION INSTRUCTIONS FOR THE
APPLICATION INSTRUCTIONS FOR THE SNA KES A ND LA DDERS A DD O N FO R USE WITH THE C HESS, C HEC KERS & BO RDERS LARG E AND NUMBER SET Pro duc t Numb e r: 17-2W-062 SIZE: a ppro xima te ly 19 fe e t e a
More informationPhysics 1501 Lecture 19
Physcs 1501 ectue 19 Physcs 1501: ectue 19 Today s Agenda Announceents HW#7: due Oct. 1 Mdte 1: aveage 45 % Topcs otatonal Kneatcs otatonal Enegy Moents of Ineta Physcs 1501: ectue 19, Pg 1 Suay (wth copason
More information( 1) β function for the Higgs quartic coupling λ in the standard model (SM) h h. h h. vertex correction ( h 1PI. Σ y. counter term Λ Λ.
funon for e Hs uar oun n e sanar moe (SM verex >< sef-ener ( PI Π ( - ouner erm ( m, ( Π m s fne Π s fne verex orreon ( PI Σ (,, ouner erm, ( reen funon ({ } Σ s fne Λ Λ Bn A n ( Caan-Smanz euaon n n (
More informationPHYSICS 272H Electric & Magnetic Interactions
PHYSICS 7H Electic & Magnetic Inteactions Physics couse home page: http://www.physics.pudue.edu/academic-pogams/couses/all_couses.php Blackboad Lean: https://mycouses.pudue.edu/webapps/login/ Couse Content
More informationChapter 3 Basic Crystallography and Electron Diffraction from Crystals. Lecture 11. Chapter 3, CHEM 793, 2011 Fall, L. Ma
Cpte 3 Bsic Cystopy nd Eecton Diffction fom Cysts Lectue Pof. Sectmn: Nobe impossibe witout micoscope Isei ecipient of 0 cemisty Nobe Pize sys oundbein discoey of 'qusicysts' woud e been deyed fo yes witout
More informationDangote Flour Mills Plc
SUMMARY OF OFFER Opening Date 6 th September 27 Closing Date 27 th September 27 Shares on Offer 1.25bn Ord. Shares of 5k each Offer Price Offer Size Market Cap (Post Offer) Minimum Offer N15. per share
More informationV7: Diffusional association of proteins and Brownian dynamics simulations
V7: Diffusional association of poteins and Bownian dynamics simulations Bownian motion The paticle movement was discoveed by Robet Bown in 1827 and was intepeted coectly fist by W. Ramsay in 1876. Exact
More information2 Lecture 2: The Bohr atom (1913) and the Schrödinger equation (1925)
1 Lectue 1: The beginnings of quantum physics 1. The Sten-Gelach expeiment. Atomic clocks 3. Planck 1900, blackbody adiation, and E ω 4. Photoelectic effect 5. Electon diffaction though cystals, de Boglie
More informationOrbital Angular Momentum
Obta Anua Moentu In cassca echancs consevaton o anua oentu s soetes teated b an eectve epusve potenta Soon we w sove the 3D Sch. Eqn. The R equaton w have an anua oentu te whch ases o the Theta equaton
More informationPhotoemission Spectroscopy Fundamental Aspects
Photoemission Spectoscopy Fundamental Aspects G. Stefani Dipatimento di Fisica E. Amaldi, Univesita Roma Te CISM Unita di Riceca di Roma 3 School G. Stefani 1 hν Basic Concepts - E, e K e εˆ E MAX e =
More informationGenerating and characteristic functions. Generating and Characteristic Functions. Probability generating function. Probability generating function
Generating and characteristic functions Generating and Characteristic Functions September 3, 03 Probability generating function Moment generating function Power series expansion Characteristic function
More informationAngular Momentum Properties
Cheistry 460 Fall 017 Dr. Jean M. Standard October 30, 017 Angular Moentu Properties Classical Definition of Angular Moentu In classical echanics, the angular oentu vector L is defined as L = r p, (1)
More informationWeek 10: DTMC Applications Ranking Web Pages & Slotted ALOHA. Network Performance 10-1
Week : DTMC Alictions Rnking Web ges & Slotted ALOHA etwok efonce - Outline Aly the theoy of discete tie Mkov chins: Google s nking of web-ges Wht ge is the use ost likely seching fo? Foulte web-gh s Mkov
More informationI n t e r n a t i o n a l E l e c t r o n i c J o u r n a l o f E l e m e n t a r y E.7 d u, c ai ts is ou n e, 1 V3 1o-2 l6, I n t h i s a r t
I n t e r n a t i o n a l E l e c t r o n i c J o ue rlne am l e not fa r y E d u c a t i o n, 2 0 1 4, 1 37-2 ( 16 ). H o w R e a d i n g V o l u m e A f f e c t s b o t h R e a d i n g F l u e n c y
More informationChapter 5: Your Program Asks for Advice.
Chte 5: You Pogm Asks fo Advce. Pge 63 Chte 5: You Pogm Asks fo Advce. Ths chte ntoduces new tye of ves (stng ves) nd how to get text nd numec esonses fom the use. Anothe Tye of Ve The Stng Ve: In Chte
More information3. Anomalous magnetic moment
3. Anolos gntc ont 3.1 Mgntc ont of th lcton: Dc qton wth lcton colng to lcto-gntc t fld: D A A D ψ 0 cnoncl ont Anstz fo th solton s fo f tcl: t t Χ Φ Φ Χ 0 A 0 A Χ Φ 0 Χ Φ χ ϕ x x 4 Non-ltvstc lt: E,
More informationDoublet structure of Alkali spectra:
Doublet stuctue of : Caeful examination of the specta of alkali metals shows that each membe of some of the seies ae closed doublets. Fo example, sodium yellow line, coesponding to 3p 3s tansition, is
More informationMe n d e l s P e a s Exer c i se 1 - Par t 1
!! Me n d e l s P e a s Exer c i se 1 - Par t 1 TR UE - BR E E D I N G O R G A N I S M S Go a l In this exercise you will use StarGenetics, a genetics experiment simulator, to understand the concept of
More information:9 :9. Public Water Crossings - DE NORTHERN PASS PROJECT. Ashland. Bridgewater
Lgnd ol/ Loction Nothn ss Nothn ss nsission Lins Nub - - - kv Lin Evsouc Lins 5 kv Hight (in ft oss Sction 75-4 -4 5-4 Evsouc 5 kv Lin E5-8 E5- E5- E5-. Rf to Nothn ss nsission LL ublic Wt ossings SE ockt
More informationEinstein Summation Convention
Ensten Suaton Conventon Ths s a ethod to wrte equaton nvovng severa suatons n a uncuttered for Exape:. δ where δ or 0 Suaton runs over to snce we are denson No ndces appear ore than two tes n the equaton
More informationParticle Physics. From Monday: Summary. Lecture 9: Quantum Chromodynamics (QCD) q 2 m 2 Z. !q q!q q scattering
Paticle Physics Lectue 9: Quantum Chomodynamics (QCD)!Colou chage and symmety!gluons!qcd Feynman Rules!! scatteing!jets! 1 Fom Monday: Summay Weak Neutal Cuent Caied by the massive Z-boson: acts on all
More information1 (40) Gravitational Systems Two heavy spherical (radius 0.05R) objects are located at fixed positions along
(40) Gravitational Systes Two heavy spherical (radius 0.05) objects are located at fixed positions along 2M 2M 0 an axis in space. The first ass is centered at r = 0 and has a ass of 2M. The second ass
More informationProblem T1. Main sequence stars (11 points)
Proble T1. Main sequence stars 11 points Part. Lifetie of Sun points i..7 pts Since the Sun behaves as a perfectly black body it s total radiation power can be expressed fro the Stefan- Boltzann law as
More informationThe second law of thermodynamics - II.
Januay 21, 2013 The second law of themodynamics - II. Asaf Pe e 1 1. The Schottky defect At absolute zeo tempeatue, the atoms of a solid ae odeed completely egulaly on a cystal lattice. As the tempeatue
More informationPHYS 601 HW3 Solution
3.1 Norl force using Lgrnge ultiplier Using the center of the hoop s origin, we will describe the position of the prticle with conventionl polr coordintes. The Lgrngin is therefore L = 1 2 ṙ2 + 1 2 r2
More information4πε. me 1,2,3,... 1 n. H atom 4. in a.u. atomic units. energy: 1 a.u. = ev distance 1 a.u. = Å
H atom 4 E a me =, n=,,3,... 8ε 0 0 π me e e 0 hn ε h = = 0.59Å E = me (4 πε ) 4 e 0 n n in a.u. atomic units E = r = Z n nao Z = e = me = 4πε = 0 energy: a.u. = 7. ev distance a.u. = 0.59 Å General results
More informationAgenda Rationale for ETG S eek ing I d eas ETG fram ew ork and res u lts 2
Internal Innovation @ C is c o 2 0 0 6 C i s c o S y s t e m s, I n c. A l l r i g h t s r e s e r v e d. C i s c o C o n f i d e n t i a l 1 Agenda Rationale for ETG S eek ing I d eas ETG fram ew ork
More informationSolutions to problem set ); (, ) (
Solutos to proble set.. L = ( yp p ); L = ( p p ); y y L, L = yp p, p p = yp p, + p [, p ] y y y = yp + p = L y Here we use for eaple that yp, p = yp p p yp = yp, p = yp : factors that coute ca be treated
More informationWhat is this? Jerry Gilfoyle The Hydrogen Atom 1 / 18
What is this? Jey Gilfoyle The Hydogen Atom 1 / 18 What is this? The Hydogen Atom Jey Gilfoyle The Hydogen Atom 1 / 18 What is this? The Hydogen Atom Jey Gilfoyle The Hydogen Atom 1 / 18 What is this?
More informationH STO RY OF TH E SA NT
O RY OF E N G L R R VER ritten for the entennial of th e Foundin g of t lair oun t y on ay 8 82 Y EEL N E JEN K RP O N! R ENJ F ] jun E 3 1 92! Ph in t ed b y h e t l a i r R ep u b l i c a n O 4 1922
More informationCHAPTER 29 ELECTRIC FIELD AND POTENTIAL EXERCISES
HPTER ELETRI FIELD ND POTENTIL EXERISES. oulob Newton l M L T 4 k F.. istnce between k so, foce k ( F ( The weight of boy 4 N 4 N wt of boy So,. foce between chges 4 So, foce between chges.6 weight of
More informationA Tale of Friction Student Notes
Nae: Date: Cla:.0 Bac Concept. Rotatonal Moeent Kneatc Anular Velocty Denton A Tale o Frcton Student Note t Aerae anular elocty: Intantaneou anular elocty: anle : radan t d Tanental Velocty T t Aerae tanental
More informationCharged particle motion in magnetic field
Chaged paticle otion in agnetic field Paticle otion in cued agnetic fieldlines We diide the equation of otion into a elocity coponent along the agnetic field and pependicula to the agnetic field. Suppose
More informationThermodynamics II. Department of Chemical Engineering. Prof. Kim, Jong Hak
Thermodynamcs II Department o Chemca ngneerng ro. Km, Jong Hak .5 Fugacty & Fugacty Coecent : ure Speces µ > provdes undamenta crteron or phase equbrum not easy to appy to sove probem Lmtaton o gn (.9
More information-HYBRID LAPLACE TRANSFORM AND APPLICATIONS TO MULTIDIMENSIONAL HYBRID SYSTEMS. PART II: DETERMINING THE ORIGINAL
UPB Sc B See A Vo 72 I 3 2 ISSN 223-727 MUTIPE -HYBRID APACE TRANSORM AND APPICATIONS TO MUTIDIMENSIONA HYBRID SYSTEMS PART II: DETERMININ THE ORIINA Ve PREPEIŢĂ Te VASIACHE 2 Ace co copeeă oă - pce he
More informationElectric field generated by an electric dipole
Electic field geneated by an electic dipole ( x) 2 (22-7) We will detemine the electic field E geneated by the electic dipole shown in the figue using the pinciple of supeposition. The positive chage geneates
More informationChapter 3 Vector Integral Calculus
hapte Vecto Integal alculus I. Lne ntegals. Defnton A lne ntegal of a vecto functon F ove a cuve s F In tems of components F F F F If,, an ae functon of t, we have F F F F t t t t E.. Fn the value of the
More informationCHAPTER? 29 ELECTRIC FIELD AND POTENTIAL EXERCISES = 2, N = (5.6) 1 = = = = = Newton
Downloe fo HPTER? ELETRI FIELD ND POTENTIL EXERISES. oulob Newton l M L T 4 k F.. istnce between k so, foce k ( F ( The weight of boy 4 N 4 N wt of boy.5 So, foce between chges 4 So, foce between chges
More informationPreliminary Examination - Day 1 Thursday, August 9, 2018
UNL - Department of Physics and Astronomy Preliminary Examination - Day Thursday, August 9, 8 This test covers the topics of Thermodynamics and Statistical Mechanics (Topic ) and Quantum Mechanics (Topic
More informationCHEM Course web page. Outline for first exam period
CHEM 3 Course web page http://web.chemistry.gatech.edu/~barefield/3/chem3a.html Outline for first exam period Atomic structure and periodic properties Structures and bonding models for covalent compounds
More informationPlanar convex hulls (I)
Covx Hu Covxty Gv st P o ots 2D, tr ovx u s t sst ovx oyo tt ots ots o P A oyo P s ovx or y, P, t st s try P. Pr ovx us (I) Coutto Gotry [s 3250] Lur To Bowo Co ovx o-ovx 1 2 3 Covx Hu Covx Hu Covx Hu
More informationMethods for solving the radiative transfer equation. Part 3: Discreteordinate. 1. Discrete-ordinate method for the case of isotropic scattering.
ecture Metos for sov te rtve trsfer equto. rt 3: Dscreteorte eto. Obectves:. Dscrete-orte eto for te cse of sotropc sctter..geerzto of te screte-orte eto for ooeeous tospere. 3. uerc peetto of te screte-orte
More information1 - ELECTRIC CHARGE AND ELECTRIC FIELD Page 1
. Eectc Chge ELECTRIC CHARGE AND ELECTRIC IELD Pge Of most moe thn fundment ptces of mtte, thee most mpotnt e eecton, poton nd neuton. The msses e m e 9. g, m p m n.6 7 g espectvey. Gvtton foce of ttcton
More informationCOMPILATION OF AUTOMATA FROM MORPHOLOGICAL TWO-LEVEL RULES
Kimmo Koskenniemi Re se ar ch Unit for Co mp ut at io na l Li ng ui st ic s University of Helsinki, Hallituskatu 11 SF-00100 Helsinki, Finland COMPILATION OF AUTOMATA FROM MORPHOLOGICAL TWO-LEVEL RULES
More informationSOCKET WELD OR THREADED BODY TYPE (3051SFP FLOWMETER SHOWN THROUGHOUT / 3051CFP, 2051CFP AVAILABLE)
9 10 12 13 14 15 16 RVISION T RVISION O NO. PP' T SI1053953 3/30/17 03/31/17 SRIPTION NOT 10 N RIITION ON ST 10. T 1 - OY INSIONS 2X 1/4" NPT VNT VVS INSIONS IN SIZ 3.4 [86.0] 3.8 [97.0] 4.5 [4.0] 4.7
More informationOn the Navier Stokes equations
On the Navier Stokes equations Daniel Thoas Hayes April 26, 2018 The proble on the existence and soothness of the Navier Stokes equations is resolved. 1. Proble description The Navier Stokes equations
More informationElectrostatic/magnetostatic forces
Eecsc/gnesc ces spes ppc: eneg e ec eneg ce (vec) ve (vec) en ( eneg ) ( snce) ne s cn gve e O ce (n pessue) u cn en snge sp cne s pe e ce spe epe: pe pes eecsc: ppe vge gnesc: cuen I Den. Nekk 00, s upe
More informationEN40: Dynamics and Vibrations. Midterm Examination Tuesday March
EN4: Dynaics and Vibations Midte Exaination Tuesday Mach 8 16 School of Engineeing Bown Univesity NME: Geneal Instuctions No collaboation of any kind is peitted on this exaination. You ay bing double sided
More information