APP-IV Introduction to Astro-Particle Physics. Maarten de Jong

Size: px
Start display at page:

Download "APP-IV Introduction to Astro-Particle Physics. Maarten de Jong"

Transcription

1 APP-IV Introduction to Astro-Particl Physics Maartn d Jong 1

2 cosmology in a nut shll Hubbl s law cosmic microwav background radiation abundancs of light lmnts (H, H, )

3 Hubbl s law (199) 1000 vlocity [km/s] pc.6 ly distanc [Mpc]

4 Dopplr ffct Cphid T v L 1+ β λ' = λ0 1 β v c (1 + v ) c λ 0 rd-shift t L = f ( T) Standard candl Vlocity Distanc 4

5 Hubbl s law (II) v= H d Hubbl constant 5

6 xpanding Univrs a(t 1 ) tim a(t ) a(t) = univrsal scal paramtr 6

7 univrsal scal paramtr v= H d H() t = at () a a at () t 7

8 gnralisation of rd-shift obsrvd (t 1 ) mittd (t 0 ) λ' = at ( 1) λ at ( ) 0 λ (1 + z) rd-shift 0 z < 8

9 small rd-shift 1+ z = at ( ) 1 at ( ) = at ( ) at ( ) 1 0 at ( ) 0 at ( ) ( t t ) at ( ) at ( 0) ( t1 t0) c = 1+ at ( ) c 0 d = 1+ H = 1+ c v c z 1 Taylor xpansion Dopplr ffct 9

10 what valu has H today? 1 1 H = h 100 km s Mpc h = obsrvation 10

11 Gravitational forc a m Nwton: M 4 = ρ πa ma = G mm a mmg 1 mmg da ma + = ma = a a constant 1 Kc m 11

12 mmg 1 1 ma = a Kc m ma 1 mmg 1 ( ma ) ( Kc m) a ma = ma a 8πGM Kc 8πGρ Kc = = a π a a a 4 1

13 Fridrich-Lmaîtr-Robrtson-Walkr Enrgy dnsity curvd spac historical 0? H a 8πGρ Kc Λ = = + a a gnral solution of th Einstin quations Mass Enrgy (dividd by c ) homognous and isotropic Univrs 1

14 critical dnsity H 8πGρ Kc Λ = + a K =Λ=0 ρ c = H 8π G usd to normalis particl dnsitis (Ω) in th Univrs 14

15 fat of th Univrs nglct cosmological constant Λ = 0 assum mattr domination Mc non-rlativistic ρ = V mattr consrvd M = constant 15

16 Expansion rat: 8π GMc Kc = 4 π a a a a a GMc = a Kc K = 1 a c K = 0 a 0 K =+ 1 a 0 opn Univrs flat Univrs closd Univrs K = 1, 0, + 1 gnral mtric of homognous, isotropic spac 16

17 fat of th Univrs (Λ = 0) K = 1, opn now K = 0, flat a(t) K = +1, closd t 17

18 Ag of th Univrs K = Λ 0 H = 8π G ρ non-rlativistic mattr = 8π G Mc 4 π a Volum 18

19 a a = 8π G Mc 4 π a try: at () = αt β β 1 αβt = β αt G Mc β α t β α β t = G Mc t β = α = 9G Mc 19

20 Ag of th Univrs (II) a H = = a t t = = 8 11Gyr Gyr H obsrvd 0

21 arly Univrs H 8 = πg ρ 1

22 radiation dominatd volum xpansion rd-shift rlativistic gas: 1 ρ at () at () ρ ρ = a 4 4H a =

23 ρ 8πGρ 4 ρ = try: ρ() t = α t β αβt αt β 1 β βt 8π G = 4 8π G β / 1 β / = 4 α t α t β = α = π G ρ() t t Big Bang!

24 particl dnsity N ( E) dp = π 1 / h p dp E kt g ± 1 numbr of spin stats Numbr of particls pr unit volum in th momntum rang p p + dp Bos-Einstin ± photons (and all othr bosons, i.. spin 0, 1,, ) Frmi-Dirac ± + frmions (spin 1/, /, 5/, ) 4

25 rlativistic gas N ( E) dp = g 1 p dp E / kt π h ± 1 E = pc = hv g hν ( hν) ρν ( ) dν = dhν h / kt π ( hc) ν ± 1 Enrgy pr unit volum in th frquncy rang ν ν + dν 5

26 g hν ( hν) ρν ( ) dν = dhν h / kt π ( hc) ν ± 1 bosons 4 x π dx = x dx frmions 4 x 7 π = x ρ = π 4 ( kt ) 0 ( hc) g ff all particls ar intracting with ach othr 6

27 rlativistic gas xpansion of arly Univrs ρ = π π ( kt ) h c g ff ρ = π G t kt 1 MV t[ s] 7

28 Enrgy dnsity Tmpratur ρ 1 t T 1 t hot Big Bang 8

29 Hubbl constant H 8 πg ( kt ) = ρ 1.66 gff M c h Pl G hc ( M c ) Pl c 4 M Pl c Planck mass GV 9

30 xpanding Univrs At som momnt, photons dcoupld intraction rat xpansion rat Thn, numbr of photons consrvd but Univrs kps xpanding dnsity volum N 1 ( ) d dv ν ν ν = d ν dv = h / kt π ( hc) ν 1 constant 0

31 N ( ν ') dν ' dv ' = N ( ν) dνdv Bos-Einstin distribution T ' = π 1 ν dν dv ( hc) 1 hν / kt 1 (1 + z) ν ' = (1 + z) dν ' dv h(1 + z) ν '/ kt π ( hc) 1 1 ν ' = dν ' (1 + z) dv hν '/ kt ' π ( hc) 1 T = cooling 1 + z dv ' 1

32 cosmic microwav background radiation wavlngth [cm] intnsity photon dnsity distribution T 0 =.7 K frquncy [GHz]

33 Transparncy of th Univrs chargd particls nutral atoms 1 p H γ + + larg photon-mattr cross sction small photon-mattr cross sction Univrs opaqu Univrs transparnt

34 quilibrium non-rlativistic N N, N! γ p 1 + p H + γ chmical potntial µ H = µ p + µ ( µ γ = 0) binding nrgy Q m + m m 1.6 V p H baryon numbr dnsity nb np + nh 4

35 n = g 1 p dp E / kt h 0 π ± 1 kt Q m c i g π 1 h 0 E / kt p dp E mc + p m x p mkt mc / kt x g ( mkt ) = x dx π h 0 5

36 x x x x x dx = x 1 x dx = 1 x 1 dx v ' u = = = = π x ( x ) r dx + y dr rdφ dxdy 6

37 non-rlativistic particl dnsity n = = g ( mkt ) mc / kt π π h 4 mc kt g π ( hc) mc / kt 7

38 diffrnt particl spcis chmical potntial mi c kt ni = g i π ( hc) µ mc i i kt 8

39 photon dnsity g 1 ν N( ν) dν = dν h / kt π ( hc) ν 1 0 dx x x 1 =.404 n γ.404 kt = π hc 9

40 mh c kt nh = g H π ( hc) = µ m c H H kt gh mc mpc kt nn p ggp π ( hc) m c H n n n n µ ( m m m ) c H µ µ p+ + p H kt 0 p p Q Univrs is nutral n p n = g H g g p n p m c kt π ( hc) Q kt 40

41 Ionisation fraction barion / photon ratio X np np = n n + n B p H η B n B n γ n + 1 X nh p H nh = n γ = η B X np nγ np n n γ Saha quation 1 X.404 kt = ηb X π mc Q kt 41

42 limiting cass lim 0 kt X 1 X X 0 Univrs transparnt lim kt Q 1 X X 0 X 1 Univrs opaqu X ( kt ) 0.5? η B ( kt ) numrical calculation 4

43 Ionisation fraction Ionisation fraction transparnt opaqu rd shift 4

44 Ionisation tmpratur T0.7 K z 100 kt = kt (1 + z) 0. V Q = 1 V 0 ηb 1! kt Q / 40 44

45 cross-chck 0.5 = 1 X X.404 ln 0.5 ln ln ( ) B ln kt = + η + + π mc Q kt!

46 Nuclosynthsis 46

47 kt 1 MV t T nutrinos and nuclons in quilibrium T 1 Hlium formation T t 1 t t 47

48 T 1 T T 1 > T < T1 ν ν + n + p + + p + n n p+ + ν nutron dcay 48

49 Q ( M M m ) c 1.9 MV n p kt Q M c p nuclons ar non-rlativistic E Mc + p M m n m p n n n p = Q / kt 49

50 quilibrium intraction rat xpansion rat Γ H dcoupl 50

51 intraction rat pr nuclon dnsity cross sction rlativ vlocity Γ= n σ v 51

52 intraction rat (II) dnsity lctrons & nutrinos ar rlativistic n ν, 1.0 kt = 4 π hc g cross-sction m c s np, σ α ( hc) p p 4 ( M c ) W ν, np, rlativ vlocity lctrons & nutrinos ar rlativistic v c 5

53 intraction rat (III) my guss pν, pnp, kt M Nc +,, ν, ν rlativistic p, n at rst 5

54 quilibrium (II) α M N c 4 ( kt ) ( kt ) 4 W Pl ( M c ) h M c h kt1 0.8 MV m c 511 kv M c 940 MV N 54

55 nutron-proton ratio at t t 1 n ( t) = n (0) n n t / τ r n n Q / kt = 1 n p 0. t / τ nn r () t = np 1+ r r t / τ τ nutron liftim t / τ n ( t) = n (0) + n (0)(1 ) p p n 55

56 T T T > T < T n + p H + γ H + H H + n H + H H + p 4 H + H H + p 4 H + H H + n formation of stabl H nutrons ar savd 56

57 T Q. MV rmindr η B ffctiv tmpratur kt Q / 40 = 0.05 MV 57

58 nutron-proton ratio at t 1MV 1MV t = kt kt1 400 s τ = 896 ± 10 s nutron liftim nn rt ( 1) rt ( ) ( t) = 0.1 np t / τ 1 + rt ( ) rt ( ) 1 1 t / τ 58

59 H mass ratio Y = MH M nn 4 n + n p n 4n H n r = ± 0.01 obsrvd! 1+ r H cosmological origin 59

Cosmology and particle physics

Cosmology and particle physics Cosmology and particl physics Lctur nots Timm Wras Lctur 8 Th thrmal univrs - part IV In this lctur w discuss th Boltzmann quation that allows on to dscrib th volution of procsss in our univrs that ar

More information

Pion condensation with neutrinos

Pion condensation with neutrinos Pion condnsation with nutrinos Or how dos QCD bhav undr high dnsitis of lctron/muon nutrinos Harmn Warringa, Goth Univrsität, Frankfurt Basd on work don with Hiroaki Abuki and Tomas Braunr arxiv:0901.2477

More information

Neutrino Physics. Caren Hagner, Universität Hamburg

Neutrino Physics. Caren Hagner, Universität Hamburg Nutrino Physics Carn Hagnr, Univrsität Hamburg What ar nutrinos? Nutrino mass and mixing Nutrino oscillations Nutrino bams: OPERA Oscillation of acclrator nutrinos Solar Nutrinos: BOREXINO (KamLAND ractor

More information

Contemporary, atomic, nuclear, and particle physics

Contemporary, atomic, nuclear, and particle physics Contmporary, atomic, nuclar, and particl physics 1 Blackbody radiation as a thrmal quilibrium condition (in vacuum this is th only hat loss) Exampl-1 black plan surfac at a constant high tmpratur T h is

More information

Standard Model - Electroweak Interactions. Standard Model. Outline. Weak Neutral Interactions. Electroweak Theory. Experimental Tests.

Standard Model - Electroweak Interactions. Standard Model. Outline. Weak Neutral Interactions. Electroweak Theory. Experimental Tests. Standard Modl - Elctrowak Intractions Outlin ak Nutral Intractions Nutral Currnts (NC) Elctrowak Thory ± and Z and γ Discovry of ± Exprimntal Tsts LEP Z Boson Mass and idth Numbr of Nutrinos ± Boson ±

More information

Derivation of Electron-Electron Interaction Terms in the Multi-Electron Hamiltonian

Derivation of Electron-Electron Interaction Terms in the Multi-Electron Hamiltonian Drivation of Elctron-Elctron Intraction Trms in th Multi-Elctron Hamiltonian Erica Smith Octobr 1, 010 1 Introduction Th Hamiltonian for a multi-lctron atom with n lctrons is drivd by Itoh (1965) by accounting

More information

High Energy Physics. Lecture 5 The Passage of Particles through Matter

High Energy Physics. Lecture 5 The Passage of Particles through Matter High Enrgy Physics Lctur 5 Th Passag of Particls through Mattr 1 Introduction In prvious lcturs w hav sn xampls of tracks lft by chargd particls in passing through mattr. Such tracks provid som of th most

More information

(most) due to long range e m forces i.e. via atomic collisions or due to short range nuclear collisions or through decay ( = weak interactions)

(most) due to long range e m forces i.e. via atomic collisions or due to short range nuclear collisions or through decay ( = weak interactions) Spring 01, P67, YK Monday January 30, 01 8 Obsrvabl particl dtction ffcts ar : (most) du to long rang m forcs i.. via atomic collisions or du to short rang nuclar collisions or through dcay ( = wak intractions)

More information

Antonio Pich. IFIC, CSIC Univ. Valencia.

Antonio Pich. IFIC, CSIC Univ. Valencia. Antonio Pich IFIC, CSIC Univ. Valncia Antonio.Pich@crn.ch Th Standard Modl A. Pich - CERN Summr Lcturs 2005 1. Constitunts & Intractions 2. Quarks 3. Gaug Invarianc 4. Quantum Chromodynamics 5. Elctrowak

More information

HYSTERESIS AND BLEACHING OF ABSORPTION BY ELECTRONS ON HELIUM

HYSTERESIS AND BLEACHING OF ABSORPTION BY ELECTRONS ON HELIUM HYSERESIS AND BLEACHING O ABSORPION BY ELECRONS ON HELIUM D. Ryvkin, 1 M.J. La, and M.I. Dykman 1 1 Dpartmnt of Physics and Astronomy, Michigan Stat Univrsity Royal Holloway, Univrsity of London Dynamics

More information

2. Laser physics - basics

2. Laser physics - basics . Lasr physics - basics Spontanous and stimulatd procsss Einstin A and B cofficints Rat quation analysis Gain saturation What is a lasr? LASER: Light Amplification by Stimulatd Emission of Radiation "light"

More information

PHYSICS 489/1489 LECTURE 7: QUANTUM ELECTRODYNAMICS

PHYSICS 489/1489 LECTURE 7: QUANTUM ELECTRODYNAMICS PHYSICS 489/489 LECTURE 7: QUANTUM ELECTRODYNAMICS REMINDER Problm st du today 700 in Box F TODAY: W invstigatd th Dirac quation it dscribs a rlativistic spin /2 particl implis th xistnc of antiparticl

More information

Why is a E&M nature of light not sufficient to explain experiments?

Why is a E&M nature of light not sufficient to explain experiments? 1 Th wird world of photons Why is a E&M natur of light not sufficint to xplain xprimnts? Do photons xist? Som quantum proprtis of photons 2 Black body radiation Stfan s law: Enrgy/ ara/ tim = Win s displacmnt

More information

BETA DECAY VISUAL PHYSICS ONLINE

BETA DECAY VISUAL PHYSICS ONLINE VISUAL PHYSICS ONLINE BETA DECAY Suppos now that a nuclus xists which has ithr too many or too fw nutrons rlativ to th numbr of protons prsnt for stability. Stability can b achivd by th convrsion insid

More information

26-Sep-16. Nuclear energy production. Nuclear energy production. Nuclear energy production. Nuclear energy production

26-Sep-16. Nuclear energy production. Nuclear energy production. Nuclear energy production. Nuclear energy production Aim: valuat nrgy-gnration rat pr unit mass. Sun: (chck L /M, human ) nrgy-gnration rat producd from fusion of two nucli a + A: nrgy rlasd pr raction raction rat pr unit volum (includs cross sction and

More information

Nuclear reactions The chain reaction

Nuclear reactions The chain reaction Nuclar ractions Th chain raction Nuclar ractions Th chain raction For powr applications want a slf-sustaind chain raction. Natural U: 0.7% of 235 U and 99.3% of 238 U Natural U: 0.7% of 235 U and 99.3%

More information

de/dx Effectively all charged particles except electrons

de/dx Effectively all charged particles except electrons de/dx Lt s nxt turn our attntion to how chargd particls los nrgy in mattr To start with w ll considr only havy chargd particls lik muons, pions, protons, alphas, havy ions, Effctivly all chargd particls

More information

Forces. Quantum ElectroDynamics. α = = We have now:

Forces. Quantum ElectroDynamics. α = = We have now: W hav now: Forcs Considrd th gnral proprtis of forcs mdiatd by xchang (Yukawa potntial); Examind consrvation laws which ar obyd by (som) forcs. W will nxt look at thr forcs in mor dtail: Elctromagntic

More information

Gamma-ray burst spectral evolution in the internal shock model

Gamma-ray burst spectral evolution in the internal shock model Gamma-ray burst spctral volution in th intrnal shock modl in collaboration with: Žljka Marija Bošnjak Univrsity of Rijka, Croatia Frédéric Daign (Institut d Astrophysiqu d Paris) IAU$Symposium$324$0$Ljubljana,$Sptmbr$2016$

More information

On the Hamiltonian of a Multi-Electron Atom

On the Hamiltonian of a Multi-Electron Atom On th Hamiltonian of a Multi-Elctron Atom Austn Gronr Drxl Univrsity Philadlphia, PA Octobr 29, 2010 1 Introduction In this papr, w will xhibit th procss of achiving th Hamiltonian for an lctron gas. Making

More information

ELECTRON-MUON SCATTERING

ELECTRON-MUON SCATTERING ELECTRON-MUON SCATTERING ABSTRACT Th lctron charg is considrd to b distributd or xtndd in spac. Th diffrntial of th lctron charg is st qual to a function of lctron charg coordinats multiplid by a four-dimnsional

More information

fiziks Institute for NET/JRF, GATE, IIT JAM, M.Sc. Entrance, JEST, TIFR and GRE in Physics NUCLEAR AND PARTICLE PHYSICS NET/JRF (JUNE-2011)

fiziks Institute for NET/JRF, GATE, IIT JAM, M.Sc. Entrance, JEST, TIFR and GRE in Physics NUCLEAR AND PARTICLE PHYSICS NET/JRF (JUNE-2011) NUCLEAR AND PARTICLE PHYSICS NET/JRF (JUNE-) 64 Q. Th radius of a 9Cu nuclus is masurd to b 4.8 - cm. (A). Th radius of a 7 Mg nuclus can b stimatd to b.86 - cm (b) 5. - cm (c).6 - cm (d) 8.6 - cm (c)

More information

Radiation Physics Laboratory - Complementary Exercise Set MeBiom 2016/2017

Radiation Physics Laboratory - Complementary Exercise Set MeBiom 2016/2017 Th following qustions ar to b answrd individually. Usful information such as tabls with dtctor charactristics and graphs with th proprtis of matrials ar availabl in th cours wb sit: http://www.lip.pt/~patricia/fisicadaradiacao.

More information

II. The Universe Around Us. ASTR378 Cosmology : II. The Universe Around Us 23

II. The Universe Around Us. ASTR378 Cosmology : II. The Universe Around Us 23 II. The Universe Around Us ASTR378 Cosmology : II. The Universe Around Us 23 Some Units Used in Astronomy 1 parsec distance at which parallax angle is 1 ; 1 pc = 3.086 10 16 m ( 3.26 light years; 1 kpc

More information

6. Cosmology. (same at all points) probably true on a sufficiently large scale. The present. ~ c. ~ h Mpc (6.1)

6. Cosmology. (same at all points) probably true on a sufficiently large scale. The present. ~ c. ~ h Mpc (6.1) 6. 6. Cosmology 6. Cosmological Principle Assume Universe is isotropic (same in all directions) and homogeneous (same at all points) probably true on a sufficiently large scale. The present Universe has

More information

Today. Wave-Matter Duality. Quantum Non-Locality. What is waving for matter waves?

Today. Wave-Matter Duality. Quantum Non-Locality. What is waving for matter waves? Today Wav-Mattr Duality HW 7 and Exam 2 du Thurs. 8pm 0 min rcap from last lctur on QM Finish QM odds and nds from ch.4 Th Standard Modl 4 forcs of Natur Fundamntal particls of Natur Fynman diagrams EM

More information

IYPT 2000 Problem No. 3 PLASMA

IYPT 2000 Problem No. 3 PLASMA IYPT 000 Problm No. 3 PLASMA Tam Austria Invstigat th lctrical conducivity of th flam of a candl. Examin th influnc of rlvant paramtrs, in particular, th shap and polarity of th lctrods. Th xprimnts should

More information

From Classical to Quantum mechanics

From Classical to Quantum mechanics From Classical to Quantum mcanics Engl & Rid 99-300 vrij Univrsitit amstrdam Classical wav baviour Ligt is a wav Two-slit xprimnt wit potons (81-85) 1 On sourc Intrfrnc sourcs ttp://www.falstad.com/matpysics.tml

More information

PAPER 73 PHYSICAL COSMOLOGY

PAPER 73 PHYSICAL COSMOLOGY MATHEMATICAL TRIPOS Part III Wednesday 4 June 2008 1.30 to 4.30 PAPER 73 PHYSICAL COSMOLOGY Attempt no more than THREE questions. There are FOUR questions in total. The questions carry equal weight. STATIONERY

More information

Daniela Kirilova Institute of Astronomy and NAO Bulgarian Academy of Sciences, Sofia, Bulgaria Mihail Chizhov Mariana Panayotova

Daniela Kirilova Institute of Astronomy and NAO Bulgarian Academy of Sciences, Sofia, Bulgaria Mihail Chizhov Mariana Panayotova Standard Modl and Byond Corfu, Sptmbr, 018 Danila Kirilova Institut of Astronomy and NAO Bulgarian Acadmy of Scincs, Sofia, Bulgaria Mihail Chizhov Mariana Panayotova BBN - th dpst rliabl arly Univrs prob

More information

University of Illinois at Chicago Department of Physics. Thermodynamics & Statistical Mechanics Qualifying Examination

University of Illinois at Chicago Department of Physics. Thermodynamics & Statistical Mechanics Qualifying Examination Univrsity of Illinois at Chicago Dpartmnt of hysics hrmodynamics & tatistical Mchanics Qualifying Eamination January 9, 009 9.00 am 1:00 pm Full crdit can b achivd from compltly corrct answrs to 4 qustions.

More information

Exam 1. It is important that you clearly show your work and mark the final answer clearly, closed book, closed notes, no calculator.

Exam 1. It is important that you clearly show your work and mark the final answer clearly, closed book, closed notes, no calculator. Exam N a m : _ S O L U T I O N P U I D : I n s t r u c t i o n s : It is important that you clarly show your work and mark th final answr clarly, closd book, closd nots, no calculator. T i m : h o u r

More information

Precision Standard Model Tests (at JLab)

Precision Standard Model Tests (at JLab) Prcision Standard Modl Tsts (at JLab) Xiaochao Zhng Jun 21st, 2018 Th Standard Modl of Particl Physics How should w sarch for nw physics? Prcision SM tsts at Jffrson Lab Qwak, PVDIS Mollr, 12 GV PVDIS

More information

ECE507 - Plasma Physics and Applications

ECE507 - Plasma Physics and Applications ECE507 - Plasma Physics and Applications Lctur 7 Prof. Jorg Rocca and Dr. Frnando Tomasl Dpartmnt of Elctrical and Computr Enginring Collisional and radiativ procsss All particls in a plasma intract with

More information

Refer to Chapter 8 Kaon system Oscillations and CKM mixing matrix Neutrinos

Refer to Chapter 8 Kaon system Oscillations and CKM mixing matrix Neutrinos Chaptr 1 Rfr to Chaptr 8 Kaon systm Oscillations and CKM mixing matrix Nutrinos " # K 1 = 1 $ K K " # K = 1 $ K K C K = K ; C K = K P K = K ; P K = K % ' & % ' & K andk ar not ignstats of CP : CP K = K

More information

5.62 Physical Chemistry II Spring 2008

5.62 Physical Chemistry II Spring 2008 MIT OpnCoursWar http://ocw.mit.du 5.62 Physical Chmistry II Spring 2008 For information about citing ths matrials or our Trms of Us, visit: http://ocw.mit.du/trms. 5.62 Lctur #7: Translational Part of

More information

Introduction. How did the universe evolve to what it is today?

Introduction. How did the universe evolve to what it is today? Cosmology 8 1 Introduction 8 2 Cosmology: science of the universe as a whole How did the universe evolve to what it is today? Based on four basic facts: The universe expands, is isotropic, and is homogeneous.

More information

5. Equation of state for high densities

5. Equation of state for high densities 5 1 5. Equation of stat for high dnsitis Equation of stat for high dnsitis 5 Vlocity distribution of lctrons Classical thrmodynamics: 6 dimnsional phas spac: (x,y,z,px,py,pz) momntum: p = p x+p y +p z

More information

MASSACHUSETTS INSTITUTE OF TECHNOLOGY Physics Department Physics 8.286: The Early Universe November 12, 2013 Prof. Alan Guth PROBLEM SET 7

MASSACHUSETTS INSTITUTE OF TECHNOLOGY Physics Department Physics 8.286: The Early Universe November 12, 2013 Prof. Alan Guth PROBLEM SET 7 MASSACHUSETTS INSTITUTE OF TECHNOLOGY Physics Department Physics 8.286: The Early Universe November 12, 2013 Prof. Alan Guth PROBLEM SET 7 DUE DATE: Friday, November 15, 2013 READING ASSIGNMENT: Steven

More information

Lecture 2: The First Second origin of neutrons and protons

Lecture 2: The First Second origin of neutrons and protons Lecture 2: The First Second origin of neutrons and protons Hot Big Bang Expanding and cooling Soup of free particles + anti-particles Symmetry breaking Soup of free quarks Quarks confined into neutrons

More information

Chemical Physics II. More Stat. Thermo Kinetics Protein Folding...

Chemical Physics II. More Stat. Thermo Kinetics Protein Folding... Chmical Physics II Mor Stat. Thrmo Kintics Protin Folding... http://www.nmc.ctc.com/imags/projct/proj15thumb.jpg http://nuclarwaponarchiv.org/usa/tsts/ukgrabl2.jpg http://www.photolib.noaa.gov/corps/imags/big/corp1417.jpg

More information

Intro to Nuclear and Particle Physics (5110)

Intro to Nuclear and Particle Physics (5110) Intro to Nuclar and Particl Physics (5110) March 09, 009 Frmi s Thory of Bta Dcay (continud) Parity Violation, Nutrino Mass 3/9/009 1 Final Stat Phas Spac (Rviw) Th Final Stat lctron and nutrino wav functions

More information

Davisson Germer experiment Announcements:

Davisson Germer experiment Announcements: Davisson Grmr xprimnt Announcmnts: Homwork st 7 is du Wdnsday. Problm solving sssions M3-5, T3-5. Th 2 nd midtrm will b April 7 in MUEN E0046 at 7:30pm. BFFs: Davisson and Grmr. Today w will go ovr th

More information

Introduction to the quantum theory of matter and Schrödinger s equation

Introduction to the quantum theory of matter and Schrödinger s equation Introduction to th quantum thory of mattr and Schrödingr s quation Th quantum thory of mattr assums that mattr has two naturs: a particl natur and a wa natur. Th particl natur is dscribd by classical physics

More information

6. The Interaction of Light and Matter

6. The Interaction of Light and Matter 6. Th Intraction of Light and Mattr - Th intraction of light and mattr is what maks lif intrsting. - Light causs mattr to vibrat. Mattr in turn mits light, which intrfrs with th original light. - Excitd

More information

Cosmology. Jörn Wilms Department of Physics University of Warwick.

Cosmology. Jörn Wilms Department of Physics University of Warwick. Cosmology Jörn Wilms Department of Physics University of Warwick http://astro.uni-tuebingen.de/~wilms/teach/cosmo Contents 2 Old Cosmology Space and Time Friedmann Equations World Models Modern Cosmology

More information

The failure of the classical mechanics

The failure of the classical mechanics h failur of th classical mchanics W rviw som xprimntal vidncs showing that svral concpts of classical mchanics cannot b applid. - h blac-body radiation. - Atomic and molcular spctra. - h particl-li charactr

More information

The Friedmann Equation R = GM R 2. R(t) R R = GM R GM R. d dt. = d dt 1 2 R 2 = GM R + K. Kinetic + potential energy per unit mass = constant

The Friedmann Equation R = GM R 2. R(t) R R = GM R GM R. d dt. = d dt 1 2 R 2 = GM R + K. Kinetic + potential energy per unit mass = constant The Friedmann Equation R = GM R R R = GM R R R(t) d dt 1 R = d dt GM R M 1 R = GM R + K Kinetic + potential energy per unit mass = constant The Friedmann Equation 1 R = GM R + K M = ρ 4 3 π R3 1 R = 4πGρR

More information

Cosmology ASTR 2120 Sarazin. Hubble Ultra-Deep Field

Cosmology ASTR 2120 Sarazin. Hubble Ultra-Deep Field Cosmology ASTR 2120 Sarazin Hubble Ultra-Deep Field Cosmology - Da Facts! 1) Big Universe of Galaxies 2) Sky is Dark at Night 3) Isotropy of Universe Cosmological Principle = Universe Homogeneous 4) Hubble

More information

Lecture 2: Cosmological Background

Lecture 2: Cosmological Background Lecture 2: Cosmological Background Houjun Mo January 27, 2004 Goal: To establish the space-time frame within which cosmic events are to be described. The development of spacetime concept Absolute flat

More information

Graduate Students Seminar Paul-Scherrer-Institut. Search for Excited Quarks

Graduate Students Seminar Paul-Scherrer-Institut. Search for Excited Quarks Graduat Studnts Sminar 01.10.2003 Paul-Schrrr-Institut Sarch for Excitd Quarks Jan Bckr Univrsity of Zurich Sarch for Excitd Quarks Framwork Excitd frmions and comositnss Phnomnological framwork Production

More information

Q Q N, V, e, Quantum Statistics for Ideal Gas and Black Body Radiation. The Canonical Ensemble

Q Q N, V, e, Quantum Statistics for Ideal Gas and Black Body Radiation. The Canonical Ensemble Quantum Statistics fo Idal Gas and Black Body Radiation Physics 436 Lctu #0 Th Canonical Ensmbl Ei Q Q N V p i 1 Q E i i Bos-Einstin Statistics Paticls with intg valu of spin... qi... q j...... q j...

More information

Einstein Rosen inflationary Universe in general relativity

Einstein Rosen inflationary Universe in general relativity PRAMANA c Indian Acadmy of Scincs Vol. 74, No. 4 journal of April 2010 physics pp. 669 673 Einstin Rosn inflationary Univrs in gnral rlativity S D KATORE 1, R S RANE 2, K S WANKHADE 2, and N K SARKATE

More information

22/ Breakdown of the Born-Oppenheimer approximation. Selection rules for rotational-vibrational transitions. P, R branches.

22/ Breakdown of the Born-Oppenheimer approximation. Selection rules for rotational-vibrational transitions. P, R branches. Subjct Chmistry Papr No and Titl Modul No and Titl Modul Tag 8/ Physical Spctroscopy / Brakdown of th Born-Oppnhimr approximation. Slction ruls for rotational-vibrational transitions. P, R branchs. CHE_P8_M

More information

Collisions between electrons and ions

Collisions between electrons and ions DRAFT 1 Collisions btwn lctrons and ions Flix I. Parra Rudolf Pirls Cntr for Thortical Physics, Unirsity of Oxford, Oxford OX1 NP, UK This rsion is of 8 May 217 1. Introduction Th Fokkr-Planck collision

More information

When Does The Universe Become Transparent? Last updated 24 June 2007

When Does The Universe Become Transparent? Last updated 24 June 2007 Chaptr 9 Last updatd Jun 007. Introduction In Chaptr 8 w saw that bfor 85,000 yars th majority of th ordinary matrial in th univrs was in th form of fr lctrons and protons. In othr words, th ordinary mattr

More information

PRINCIPLES OF PLASMA PROCESSING Course Notes: Prof. J. P. Chang Part B3: ATOMIC COLLISIONS AND SPECTRA

PRINCIPLES OF PLASMA PROCESSING Course Notes: Prof. J. P. Chang Part B3: ATOMIC COLLISIONS AND SPECTRA Atomic Collisions and Spctra 125 PRINCIPLES OF PLASMA PROCESSING Cours Nots: Prof. J. P. Chang Part B3: ATOMIC COLLISIONS AND SPECTRA I. ATOMIC ENERGY LEVELS Atoms and molculs mit lctromagntic radiation

More information

Weak and Electromagnetic Interactions in Nuclei

Weak and Electromagnetic Interactions in Nuclei Wak and Elctromagntic Intractions in Nucli Toshio Suzuki Nihon Univrsity/CNS CSN Summr School Aug. 8, 7 Intractions Situation Strngth Handling (Cross sctions) EM (lctro- Known modrat (nough) clar magntic)

More information

Preliminary Examination: Astronomy

Preliminary Examination: Astronomy Preliminary Examination: Astronomy Department of Physics and Astronomy University of New Mexico Spring 2017 Instructions: Answer 8 of the 10 questions (10 points each) Total time for the test is three

More information

Exam, FK5024, Nuclear & particle physics, astrophysics & cosmology, October 26, 2017

Exam, FK5024, Nuclear & particle physics, astrophysics & cosmology, October 26, 2017 Exam, FK5024, Nuclear & particle physics, astrophysics & cosmology, October 26, 2017 08:00 13:00, Room FR4 (Oskar Klein Auditorium) No tools allowed except calculator (provided at the exam) and the attached

More information

Cosmology. Assumptions in cosmology Olber s paradox Cosmology à la Newton Cosmology à la Einstein Cosmological constant Evolution of the Universe

Cosmology. Assumptions in cosmology Olber s paradox Cosmology à la Newton Cosmology à la Einstein Cosmological constant Evolution of the Universe Cosmology Assumptions in cosmology Olber s paradox Cosmology à la Newton Cosmology à la Einstein Cosmological constant Evolution of the Universe Assumptions in Cosmology Copernican principle: We do not

More information

Cosmology: Building the Universe.

Cosmology: Building the Universe. Cosmology: Building the Universe. The term has several different meanings. We are interested in physical cosmology - the study of the origin and development of the physical universe, and all the structure

More information

Maxwellian Collisions

Maxwellian Collisions Maxwllian Collisions Maxwll ralizd arly on that th particular typ of collision in which th cross-sction varis at Q rs 1/g offrs drastic siplifications. Intrstingly, this bhavior is physically corrct for

More information

Self-interaction mass formula that relates all leptons and quarks to the electron

Self-interaction mass formula that relates all leptons and quarks to the electron Slf-intraction mass formula that rlats all lptons and quarks to th lctron GERALD ROSEN (a) Dpartmnt of Physics, Drxl Univrsity Philadlphia, PA 19104, USA PACS. 12.15. Ff Quark and lpton modls spcific thoris

More information

MATHEMATICAL TRIPOS Part III PAPER 53 COSMOLOGY

MATHEMATICAL TRIPOS Part III PAPER 53 COSMOLOGY MATHEMATICAL TRIPOS Part III Wednesday, 8 June, 2011 9:00 am to 12:00 pm PAPER 53 COSMOLOGY Attempt no more than THREE questions. There are FOUR questions in total. The questions carry equal weight. STATIONERY

More information

Give the letter that represents an atom (6) (b) Atoms of A and D combine to form a compound containing covalent bonds.

Give the letter that represents an atom (6) (b) Atoms of A and D combine to form a compound containing covalent bonds. 1 Th diagram shows th lctronic configurations of six diffrnt atoms. A B C D E F (a) You may us th Priodic Tabl on pag 2 to hlp you answr this qustion. Answr ach part by writing on of th lttrs A, B, C,

More information

Galaxies 626. Lecture 3: From the CMBR to the first star

Galaxies 626. Lecture 3: From the CMBR to the first star Galaxies 626 Lecture 3: From the CMBR to the first star Galaxies 626 Firstly, some very brief cosmology for background and notation: Summary: Foundations of Cosmology 1. Universe is homogenous and isotropic

More information

Atomic energy levels. Announcements:

Atomic energy levels. Announcements: Atomic nrgy lvls Announcmnts: Exam solutions ar postd. Problm solving sssions ar M3-5 and Tusday 1-3 in G-140. Will nd arly and hand back your Midtrm Exam at nd of class. http://www.colorado.du/physics/phys2170/

More information

Physics 43 HW #9 Chapter 40 Key

Physics 43 HW #9 Chapter 40 Key Pysics 43 HW #9 Captr 4 Ky Captr 4 1 Aftr many ours of dilignt rsarc, you obtain t following data on t potolctric ffct for a crtain matrial: Wavlngt of Ligt (nm) Stopping Potntial (V) 36 3 4 14 31 a) Plot

More information

DARK SECTORS. Flip Tanedo. UC Riverside Particle Theory. 3 Feb 2017 Washington D.C. APS Topical Group on Hadronic Physics

DARK SECTORS. Flip Tanedo. UC Riverside Particle Theory. 3 Feb 2017 Washington D.C. APS Topical Group on Hadronic Physics THE WHYS AND HOWS OF LIFE AFTER WIMPS Flip Tando UC Rivrsid Particl Thory 3 Fb 20 Washington D.C. APS Topical Group on Hadronic Physics 1 Astro + Cosmo: Dark Mattr Exists GALACTIC ROTATION CURVES GRAVITATIONAL

More information

Lecture 11. Neutrino Losses and Advanced Stages of Stellar Evolution - I

Lecture 11. Neutrino Losses and Advanced Stages of Stellar Evolution - I Lctur 11 Nutrino Losss and Advancd Stags of Stllar Evolution - I Th lat stags (> hlium burning) of volution in massiv stars ar charactrizd by hug luminositis, carrid away prdominantly by nutrinos, and

More information

Neutrino Mass and Forbidden Beta Decays

Neutrino Mass and Forbidden Beta Decays NUCLEAR THEORY Vol. 35 016) ds. M. Gaidarov N. Minkov Hron Prss Sofia Nutrino Mass and Forbiddn Bta Dcays R. Dvornický 1 D. Štfánik F. Šimkovic 3 1 Dzhlpov Laboratory of Nuclar Problms JINR 141980 Dubna

More information

Today. Course Evaluations Open. Modern Cosmology. The Hot Big Bang. Age & Fate. Density and Geometry. Microwave Background

Today. Course Evaluations Open. Modern Cosmology. The Hot Big Bang. Age & Fate. Density and Geometry. Microwave Background Today Modern Cosmology The Hot Big Bang Age & Fate Density and Geometry Microwave Background Course Evaluations Open Cosmology The study of the universe as a physical system Historically, people have always

More information

Electromagnetism Physics 15b

Electromagnetism Physics 15b lctromagntism Physics 15b Lctur #8 lctric Currnts Purcll 4.1 4.3 Today s Goals Dfin lctric currnt I Rat of lctric charg flow Also dfin lctric currnt dnsity J Charg consrvation in a formula Ohm s Law vryon

More information

Where k is either given or determined from the data and c is an arbitrary constant.

Where k is either given or determined from the data and c is an arbitrary constant. Exponntial growth and dcay applications W wish to solv an quation that has a drivativ. dy ky k > dx This quation says that th rat of chang of th function is proportional to th function. Th solution is

More information

Division of Mechanics Lund University MULTIBODY DYNAMICS. Examination Name (write in block letters):.

Division of Mechanics Lund University MULTIBODY DYNAMICS. Examination Name (write in block letters):. Division of Mchanics Lund Univrsity MULTIBODY DYNMICS Examination 7033 Nam (writ in block lttrs):. Id.-numbr: Writtn xamination with fiv tasks. Plas chck that all tasks ar includd. clan copy of th solutions

More information

0WAVE PROPAGATION IN MATERIAL SPACE

0WAVE PROPAGATION IN MATERIAL SPACE 0WAVE PROPAGATION IN MATERIAL SPACE All forms of EM nrgy shar thr fundamntal charactristics: 1) thy all tral at high locity 2) In traling, thy assum th proprtis of was 3) Thy radiat outward from a sourc

More information

Pair (and Triplet) Production Effect:

Pair (and Triplet) Production Effect: Pair (and riplt Production Effct: In both Pair and riplt production, a positron (anti-lctron and an lctron (or ngatron ar producd spontanously as a photon intracts with a strong lctric fild from ithr a

More information

Ch. 24 Molecular Reaction Dynamics 1. Collision Theory

Ch. 24 Molecular Reaction Dynamics 1. Collision Theory Ch. 4 Molcular Raction Dynamics 1. Collision Thory Lctur 16. Diffusion-Controlld Raction 3. Th Matrial Balanc Equation 4. Transition Stat Thory: Th Eyring Equation 5. Transition Stat Thory: Thrmodynamic

More information

PAPER 71 COSMOLOGY. Attempt THREE questions There are seven questions in total The questions carry equal weight

PAPER 71 COSMOLOGY. Attempt THREE questions There are seven questions in total The questions carry equal weight MATHEMATICAL TRIPOS Part III Friday 31 May 00 9 to 1 PAPER 71 COSMOLOGY Attempt THREE questions There are seven questions in total The questions carry equal weight You may make free use of the information

More information

Lecture 2. Interaction of Radiation with Matter

Lecture 2. Interaction of Radiation with Matter Lctur Intraction of Radiation with Mattr Dats 14.10. Vorlsung 1 T.Stockmanns 1.10. Vorlsung J.Ritman 8.10. Vorlsung 3 J.Ritman 04.11. Vorlsung 4 J.Ritman 11.11. Vorlsung 5 J.Ritman 18.11. Vorlsung 6 J.

More information

Theory of galaxy formation

Theory of galaxy formation Theory of galaxy formation Bibliography: Galaxy Formation and Evolution (Mo, van den Bosch, White 2011) Lectures given by Frank van den Bosch in Yale http://www.astro.yale.edu/vdbosch/teaching.html Theory

More information

Byeong-Joo Lee

Byeong-Joo Lee OSECH - MSE calphad@postch.ac.kr Equipartition horm h avrag nrgy o a particl pr indpndnt componnt o motion is ε ε ' ε '' ε ''' U ln Z Z ε < ε > U ln Z β ( ε ' ε '' ε ''' / Z' Z translational kintic nrgy

More information

PH300 Modern Physics SP11 Final Essay. Up Next: Periodic Table Molecular Bonding

PH300 Modern Physics SP11 Final Essay. Up Next: Periodic Table Molecular Bonding PH Modrn Physics SP11 Final Essay Thr will b an ssay portion on th xam, but you don t nd to answr thos qustions if you submit a final ssay by th day of th final: Sat. 5/7 It dosnʼt mattr how smart you

More information

Neutrinos are chargeless, nearly massless particles Most abundant particle in the Universe Interact with matter via weak nuclear force

Neutrinos are chargeless, nearly massless particles Most abundant particle in the Universe Interact with matter via weak nuclear force By Wndi Wamlr Nutrinos ar charglss, narly masslss articls Most abundant articl in th Univrs Intract with mattr via wak nuclar forc Narly transarnt to mattr Only known ty of articl that can sca from th

More information

Relativistic effects on the nonlinear propagation of electron plasma waves in dense quantum plasma with arbitrary temperature

Relativistic effects on the nonlinear propagation of electron plasma waves in dense quantum plasma with arbitrary temperature Intrnational Journal of Enginring Rsarch and Dvlopmnt -ISSN: 78-67X, p-issn: 78-8X, www.ijrd.com Volum, Issu 1 (August 1), PP. 51-57 Rlativistic ffcts on th nonlinar propagation of lctron plasma wavs in

More information

Cosmology. Thermal history of the universe Primordial nucleosynthesis WIMPs as dark matter Recombination Horizon problem Flatness problem Inflation

Cosmology. Thermal history of the universe Primordial nucleosynthesis WIMPs as dark matter Recombination Horizon problem Flatness problem Inflation Cosmology Thermal history of the universe Primordial nucleosynthesis WIMPs as dark matter Recombination Horizon problem Flatness problem Inflation Energy density versus scale factor z=1/a-1 Early times,

More information

Schrodinger Equation in 3-d

Schrodinger Equation in 3-d Schrodingr Equation in 3-d ψ( xyz,, ) ψ( xyz,, ) ψ( xyz,, ) + + + Vxyz (,, ) ψ( xyz,, ) = Eψ( xyz,, ) m x y z p p p x y + + z m m m + V = E p m + V = E E + k V = E Infinit Wll in 3-d V = x > L, y > L,

More information

Cosmology: The Origin and Evolution of the Universe Chapter Twenty-Eight. Guiding Questions

Cosmology: The Origin and Evolution of the Universe Chapter Twenty-Eight. Guiding Questions Cosmology: The Origin and Evolution of the Universe Chapter Twenty-Eight Guiding Questions 1. What does the darkness of the night sky tell us about the nature of the universe? 2. As the universe expands,

More information

Relativistic electron microscopy of hadron dynamics

Relativistic electron microscopy of hadron dynamics Impact paramtr analysis in + N + pi+ N 1 Paul Hoyr Univrsity of Hlsinki INT Workshop Novmbr 14-18, 2016 Rlativistic lctron microscopy of hadron dynamics Gold atoms: 3D Th pion: 2D 8 ρπ(b) 6 ρ π (b) [fm

More information

Modeling the Universe A Summary

Modeling the Universe A Summary Modeling the Universe A Summary Questions to Consider 1. What does the darkness of the night sky tell us about the nature of the universe? 2. As the universe expands, what, if anything, is it expanding

More information

Katsushi Arisaka University of California, Los Angeles Department of Physics and Astronomy

Katsushi Arisaka University of California, Los Angeles Department of Physics and Astronomy 11/14/12 Katsushi Arisaka 1 Katsushi Arisaka University of California, Los Angeles Department of Physics and Astronomy arisaka@physics.ucla.edu Seven Phases of Cosmic Evolution 11/14/12 Katsushi Arisaka

More information

Hydrogen Atom and One Electron Ions

Hydrogen Atom and One Electron Ions Hydrogn Atom and On Elctron Ions Th Schrödingr quation for this two-body problm starts out th sam as th gnral two-body Schrödingr quation. First w sparat out th motion of th cntr of mass. Th intrnal potntial

More information

Neutrino Probes of Dark Energy and Dark Matter

Neutrino Probes of Dark Energy and Dark Matter SNOWPAC@Snowbird March 25, 2010 Nutrino Probs of Dark Enrgy and Dark Mattr Shin ichiro Ando California Institut of Tchnology Dark Enrgy and Dark Mattr 2.0 1.5 1.0 No Big Bang SN Most of th nrgy in th Univrs

More information

Chapter 46 Solutions

Chapter 46 Solutions Chapter 46 Solutions 46.1 Assuming that the proton and antiproton are left nearly at rest after they are produced, the energy of the photon E, must be E = E 0 = (938.3 MeV) = 1876.6 MeV = 3.00 10 10 J

More information

Einstein Equations for Tetrad Fields

Einstein Equations for Tetrad Fields Apiron, Vol 13, No, Octobr 006 6 Einstin Equations for Ttrad Filds Ali Rıza ŞAHİN, R T L Istanbul (Turky) Evry mtric tnsor can b xprssd by th innr product of ttrad filds W prov that Einstin quations for

More information

The United States Nuclear Regulatory Commission and Duke University Present: Regulatory and Radiation Protection Issues in Radionuclide Therapy

The United States Nuclear Regulatory Commission and Duke University Present: Regulatory and Radiation Protection Issues in Radionuclide Therapy Th Unitd Stats Nuclar Rgulatory Commission and Duk Univrsity Prsnt: Rgulatory and Radiation Protction Issus in Radionuclid Thrapy Copyright 008 Duk Radiation Safty and Duk Univrsity. All Rights Rsrvd.

More information

neutrinos (ν) } ν energy ~ K ν + proton e + + neutron! e - + proton neutron + ν Freeze-out temperatures

neutrinos (ν) } ν energy ~ K ν + proton e + + neutron! e - + proton neutron + ν Freeze-out temperatures kt ~ mparticle c 2 neutrinos (ν) kt < mparticle c 2 kt > mparticle c 2 Freeze-out temperatures particle /! T (K) time since BB antiparticle 6x10 e 20 sec 1.2x10 μ 1 sec 1x10 p 10 NOTE: after freeze-out,

More information

arxiv: v1 [gr-qc] 25 Jul 2012

arxiv: v1 [gr-qc] 25 Jul 2012 Modifid Amplitud of Gravitational Wavs Spctrum arxiv:1207.5962v1 [gr-qc] 25 Jul 2012 Basm Ghayour and P K Sursh School of Physics, Univrsity of Hydrabad, Hydrabad-500 046. India. E-mail: ph09ph21@uohyd.rnt.in;

More information

You may not start to read the questions printed on the subsequent pages until instructed to do so by the Invigilator.

You may not start to read the questions printed on the subsequent pages until instructed to do so by the Invigilator. MATHEMATICAL TRIPOS Part III Friday 8 June 2001 1.30 to 4.30 PAPER 41 PHYSICAL COSMOLOGY Answer any THREE questions. The questions carry equal weight. You may not start to read the questions printed on

More information