Neutrinos. Overview. Pauli postulates Neutrino Discovery of neutrino flavours. Neutrino Interactions. Neutrino mass. Neutrino oscillations

Size: px
Start display at page:

Download "Neutrinos. Overview. Pauli postulates Neutrino Discovery of neutrino flavours. Neutrino Interactions. Neutrino mass. Neutrino oscillations"

Transcription

1 Nutrnos Ovrvw Paul postulats Nutrno Dscovry of nutrno flavours Elctron, muon and tau nutrnos Nutrno Intractons Cross sctons Nutrno mass Drct masurmnt Nutrno oscllatons Lpton flavour volaton Formalsm Solar nutrnos Homstak, Supr-K and SNO Atmosphrc nutrnos Supr-K Dscovry of Nutrno Mass nutrno oscllatons Cosmology Nuclar and Partcl Physcs Franz Muhm

2 Paul s Lttr Partcl Physcs n 930 Only 3 knowns fundamntal partcls: -, p, γ Contnuous nrgy spctrum of - n bta dcay A Z X A Z X ν Paul postulats Nutrno Dar radoactv Lads and Gntlman dsprat rmdy to sav th law of consrvaton of nrgy that thr could xst nutrons Paul n bta dcay a nutron s mttd n addton to th lctron 934 nam - nutrno cond by Frm 93 nutron dscovrd by Chadwck Nuclar and Partcl Physcs Franz Muhm

3 Nutrno Intractons Nutrnos pont-lk lptons do not ntract strongly, no colour charg charg Q = 0 no lctromagntc ntractons Only wak ntractons by couplng to W ± and Z 0 Expct vry small dtcton rats I hav don a trrbl thng. I hav postulatd a partcl that cannot b dtctd. Paul Invrs Bta Dcay ν n p ν p n Cross scton σ 44 Eν ( ν p n ) 5 0 cm MV Man Fr Path 60 lght yars of watr for MV ant-nutrno λ = 6 0 nσ 9 cm 60 lght yars n = Z N A = ν n 0 ntracts whn crossng th arth Rqur hug rats as nutrno sourcs A 3 cm -3 Nuclar and Partcl Physcs Franz Muhm 3

4 Dscovry of Nutrnos Elctron Nutrno ν dscovrd 956 by Ant-nutrno sourc Rns and Cowan Nuclar ractor --- ant-ν flux s - Targt and Dtctor l lqud scntllator Watr and Cadmum Chlord Dtcton of ant-nutrno annhlats wth atomc - ν n Cd racton dlayd by 0 s p n ncd Cd Dlayd concdncs only producd by sgnal Muon Nutrno ν 96 at Brookhavn by Pon bam Ldrmann, Stnbrgr, Schwartz Iron absorbr --- only muons survv π - bam obsrv π ν ν n don't s ν n p p ν ν and ν ar dffrnt Tau Nutrno ν τ 000 at Frmlab - Donut p on tungstn targt produc D s msons D s τ τ τ ν ν N τ X τ ν ν τ γ Cd Nuclar and Partcl Physcs Franz Muhm 4 π ν p n ν p n γγ *

5 Nutrno Physcs Nutrno Sourcs Natural radoactvty.g. rocks Cosmc rays httng th atmosphr Nuclar ractors Partcl acclrators Sun - nuclar fuson ractor 4 p 4 H ν 6.7 MV Flux on arth ~0 cm - s - 00 bllons/sc through your fngr nal Nutrno Mass No apparnt rason for nutrno to b masslss all othr frmons hav mass Drct mass masurmnts Bta dcay nrgy spctrum dγ GF = 3 de π dγ de E ( E E ) 0 E 0 E E Kur plot lnar H H Endpont modfd by rsoluton and non-zro ν mass Trtum Bta Dcay Mass m(ν ) < 3 V Nutrno Oscllatons No apparnt rason for nutrnos not to oscllat nto ach othr 3 3 ν Nuclar and Partcl Physcs Franz Muhm 5

6 Nutrno Oscllatons Lpton flavour consrvaton L, L, L τ ar consrvd sparatly Nutrnos wth mass can mx wak gnstats ar lnar suprpostons of mass gnstats L, L, L τ not absolutly consrvd L, L, L τ Volaton too small to obsrv BF < 0-40 Nutrno flavours Easy to undrstand, can b xpandd to 3 gnratons ν cosθ snθ ν = ν snθ cosθ ν Tm voluton ν ( t) = ν (0)xp E t ( ) ( t) ν ( t) = ν (0)xp E Intnsty I(t) for ntal ν bam I Nutrno nrgy E and mass dffrnc m E ν = p E m p m p Nutrno Oscllaton Probablts P P E >> m ( ) ( E E ) cos θ sn θ 4sn θ cos θ sn ( t) = Iν (0) ( v v ) = sn t θ sn m Dstanc from sourc L [m], E[MV] and m [V ] Nuclar and Partcl Physcs Franz Muhm 6 m.7 m ( ) [V] L[m] v = sn sn v θ E[MV] m E E.7 m [V] L[m] E[MV] E m / E

7 Solar Nutrnos Standard Solar Modl (SSM) Bahcall Prdcts rats and solar nutrno nrgy spctra pp flux blow 0.4 MV 8 B ν up to 4 MV pp cycl Homstak Exprmnt Frst obsrvd solar nutrnos n 970s 00,000 gallons of Davs clanng flud C Cl 4 Masurmnt ν 37 Cl 37 Ar 0.5 Ar atoms/day.56±0.3 SNU SSM prdcton.5 Ar atoms/day 7.7±.3 SNU Puzzl - What s wrong? Exprmnt, SSM, Nutrnos SNU = ntracton 0 36 targt atoms/sc Nuclar and Partcl Physcs Franz Muhm 7

8 Solar Nutrnos II Supr-Kamokand 50,000 tons of watr,,000 phototubs undrground nsd a mn n Japan, startd 997 ν Dtcton Elastc scattrng ν ν Drctonal snstvty Masurmnts (0.465 ± ) x SSM ν dfntly from sun Sgnal from cntr of sun Puzzl - What s wrong? Homstak xprmnt confrmd Exprmnt, SSM, Nutrnos Nuclar and Partcl Physcs Franz Muhm 8

9 Solar Nutrnos III SNO --- Sudbury Nutrno Obsrvatory 000 tons of havy watr (D O) 0,000 photo multplrs tubs Snstvty SNO s abl to masur ν but also ν and ν τ (ν =,,τ ) Chargd Elastc Nutral currnt (CC) scattrng (ES) currnt (NC) ν D ν ν D n p ν - Chargd Currnt - Nutral Currnt p p ν Masurmnts 003 rsults 3% of SSM 00% of SSM 3 % of solar ν s arrv as ν at arth 00% of solar ν s dtctd f ν and ν τ ar ncludd Puzzl - What s wrong? Exprmnt, SSM, Nutrnos Nutrno Oscllatons ν chang to ν n flght Nuclar and Partcl Physcs Franz Muhm 9

10 Atmosphrc Nutrnos Cosmc Rays Protons ht nucl n uppr part of atmosphr Producng chan of partcls copous sourc of nutrnos Man dcay squnc π ν and π ν ν ν ν ν Expct ν for ach ν ~990 st ndcatons for too fw ν Supr-Kamokand Can dscrmnat ν from ν N X ν N ν Rcol muon producs clan rng Rcol - producs fuzzy rng X ν N X ν N X Nuclar and Partcl Physcs Franz Muhm 0

11 Atmosphrc Nutrnos II Masurmnts 998 Supr-Kamokand Obsrv sgnfcant dfct of ν and agrmnt for ν Nutrno Dsapparanc ν travrsng th arth. arrvng at th dtctor from blow dsappar Nutrno Oscllatons Atmosphrc nutrnos ν chang to ν τ n flght Frst Evdnc for Nutrno Oscllatons Nuclar and Partcl Physcs Franz Muhm

12 Dscovry of Nutrno Mass Atmosphrc Nutrno Oscllatons Atmosphrc ν chang nto ν τ Oscllaton P v vτ = sn probablty Ft data for bst valus of mass dffrnc m 3 and mxng angl θ τ Fnd θ τ 45 0 and m V Nutrnos hav Mass Solar Nutrno Oscllatons Supr-Kamokand, SNO Kamland ractor ant-ν Fnd θ 33 0 and Nutrno mass m V Mnmum m ν ~ 0.05 V scnaros Cosmology Bg Bang larg nr. of nutrnos Nutrnos ar hot dark mattr canddats Suprnova 987A Kamokand and IMB Obsrvd ~ 0 nutrnos.7 m [V] L[m] ( ) ( ) τ sn θ τ E[MV] Nuclar and Partcl Physcs Franz Muhm

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

Lecture 14. Relic neutrinos Temperature at neutrino decoupling and today Effective degeneracy factor Neutrino mass limits Saha equation

Lecture 14. Relic neutrinos Temperature at neutrino decoupling and today Effective degeneracy factor Neutrino mass limits Saha equation Lctur Rlc nutrnos mpratur at nutrno dcoupln and today Effctv dnracy factor Nutrno mass lmts Saha quaton Physcal Cosmoloy Lnt 005 Rlc Nutrnos Nutrnos ar wakly ntractn partcls (lptons),,,,,,, typcal ractons

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

CHAPTER 33: PARTICLE PHYSICS

CHAPTER 33: PARTICLE PHYSICS Collg Physcs Studnt s Manual Chaptr 33 CHAPTER 33: PARTICLE PHYSICS 33. THE FOUR BASIC FORCES 4. (a) Fnd th rato of th strngths of th wak and lctromagntc forcs undr ordnary crcumstancs. (b) What dos that

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

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

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

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

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

sin VALUE LIMIT IN DOUBLE CHOOZ EXPERIMENT Pi-Jung Chang

sin VALUE LIMIT IN DOUBLE CHOOZ EXPERIMENT Pi-Jung Chang sn 3 VALU LIMIT IN DOUBL CHOOZ XPRIMNT P-Jung Chang OUTLIN Dscovry nutrno Nutrno oscllaton Doubl Chooz xprnt Dtctor structur Nutrno sourc Backgrounds Systc uncrtants Uncrtants n Doubl Chooz xprnt Snstvty

More information

WEAK INTERACTION STUDIES WITH 6 HE A. GARCIA UNIVERSITY OF WASHINGTON

WEAK INTERACTION STUDIES WITH 6 HE A. GARCIA UNIVERSITY OF WASHINGTON WEK INERION SUDIES WIH 6 HE. GRI UNIERSIY OF WSHINGON h Wak Intracton or pont-lk partcl dcays H `ctor `xal h Wak Intracton or nuclons H onsrvd currnt Not consrvd WM q q Ignor propagator (q

More information

Neutrino Oscillations Hint at a New Fundamental Interaction

Neutrino Oscillations Hint at a New Fundamental Interaction Nutrino Oscillations Hint at a Nw Fundamntal Intraction Mario Evraldo d Souza Dpartamnto d Física, Univrsidad Fdral d Srgip, São Cristóvão, Srgip, Brazil Abstract It is suggstd that nutrino oscillations

More information

Discovery of first elementary particles

Discovery of first elementary particles Lptons Discovry of first lmntary particls Known particls at th nd of th 30 s Elctron Proton Photon Nutron Positron Muon Pion Nutrino: a particl whos xistnc was hypotsizd without a discovry! Faraday, Goldstin,

More information

Chapter. 3 Wave & Particles I

Chapter. 3 Wave & Particles I Announcmnt Cours wbpag http://highnrgy.phys.ttu.du/~sl/2402/ Txtbook PHYS-2402 Lctur 8 Quiz 1 Class avrag: 14.2 (out of 20) ~ 70% Fb. 10, 2015 HW2 (du 2/19) 13, 17, 23, 25, 28, 31, 37, 38, 41, 44 Chaptr.

More information

Phys 774: Nonlinear Spectroscopy: SHG and Raman Scattering

Phys 774: Nonlinear Spectroscopy: SHG and Raman Scattering Last Lcturs: Polaraton of Elctromagntc Wavs Phys 774: Nonlnar Spctroscopy: SHG and Scattrng Gnral consdraton of polaraton Jons Formalsm How Polarrs work Mullr matrcs Stoks paramtrs Poncar sphr Fall 7 Polaraton

More information

N eu trino ()scilla tion

N eu trino ()scilla tion N u trino ()scilla tion Siddhshwar Lal Oscillation as a quantum mchanical phnomnon btwn a nutral particl and its anti particl was first nvisagd in 1955 to undrstand th KO - KO problm. In th study of nuclar

More information

September 23, Honors Chem Atomic structure.notebook. Atomic Structure

September 23, Honors Chem Atomic structure.notebook. Atomic Structure Atomic Structur Topics covrd Atomic structur Subatomic particls Atomic numbr Mass numbr Charg Cations Anions Isotops Avrag atomic mass Practic qustions atomic structur Sp 27 8:16 PM 1 Powr Standards/ Larning

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

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

M. Cobal, PIF 2006/7. Leptoni

M. Cobal, PIF 2006/7. Leptoni Ltoni Frmions: th lmntary layrs Th lmntary articl familis: frmions Why 3 familis? Ar thr mor? 1st gnration 2nd gnration 3rd gnration Imossibil visualizzar l'immagin. La mmoria dl comutr otrbb ssr insufficint

More information

0 +1e Radionuclides - can spontaneously emit particles and radiation which can be expressed by a nuclear equation.

0 +1e Radionuclides - can spontaneously emit particles and radiation which can be expressed by a nuclear equation. Radioactivity Radionuclids - can spontanously mit particls and radiation which can b xprssd by a nuclar quation. Spontanous Emission: Mass and charg ar consrvd. 4 2α -β Alpha mission Bta mission 238 92U

More information

Neutrinos are one of the fundamental particles and have only week interaction. Neutrino has a zero mass, a zero charge and a spin 1/2.

Neutrinos are one of the fundamental particles and have only week interaction. Neutrino has a zero mass, a zero charge and a spin 1/2. Vladimir Kravtsov Particls of th Standard Modl Within th SM thr ar 3 diffrnt familis of particls. Each lpton has a nutrino associatd with it. Nutrinos ar on of th fundamntal particls and hav only wk intraction.

More information

11 Neutrino astronomy. introduc)on to Astrophysics, C. Bertulani, Texas A&M-Commerce 1

11 Neutrino astronomy. introduc)on to Astrophysics, C. Bertulani, Texas A&M-Commerce 1 11 Neutrino astronomy introduc)on to Astrophysics, C. Bertulani, Texas A&M-Commerce 1 11.1 The standard solar model As we discussed in stellar evolution III, to obtain a reliable model for the sun, we

More information

Exact formula of 3 flavor ν oscillation probability and its application to high energy astrophysical ν

Exact formula of 3 flavor ν oscillation probability and its application to high energy astrophysical ν Exact formula of 3 flavor ν oscillation probability and its application to high nrgy astrophysical ν Osamu Yasuda Tokyo Mtropolitan nivrsity 1-16 16-5 at Miami5 Contnts 1. Introduction 1.1 Status of ν

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

Recent Discoveries in Neutrino Physics

Recent Discoveries in Neutrino Physics Recent Discoveries in Neutrino Physics Experiments with Reactor Antineutrinos Karsten Heeger http://neutrino.physics.wisc.edu/ Karsten Heeger, Univ. of Wisconsin NUSS, July 13, 2009 Standard Model and

More information

The DELPHI experiment at the LEP accelerator at the CERN laboratory

The DELPHI experiment at the LEP accelerator at the CERN laboratory Th DELPHI xprimnt at th LEP acclrator at th CERN laboratory Part 1. Th LEP acclrator Part 2. Th DELPHI xprimnt Part 3. Particl physics rsarch at LEP Th LEP acclrator Th study of collisions btwn lctrons

More information

Search for the Dark Photon at Belle for 0.27 < m A < 3 GeV/c 2

Search for the Dark Photon at Belle for 0.27 < m A < 3 GeV/c 2 Sarch for th Dark Photon at Bll for.7 < m A < 3 GV/c Igal Jagl Univrsity of Hawai i at Mānoa for th Bll Collaboration QCD, Montpllir, 6 Juillt BELLE Igal Jagl (UH) Sarch for th Dark photon at Bll QCD /

More information

Low-energy QED tests (and what we can learn from them)

Low-energy QED tests (and what we can learn from them) Low-nrgy QED tsts (and what w can larn from thm) (0γ) 2γ (4γ) (1γ) 3γ (5γ) Indirct Sarchs for Nw Physics at th tim of LHC Flornc, March 2010 Andrzj Czarncki U. of Albrta & CERN Outlin Gyromagntic factors

More information

Aspects on Neutrino (Mass-) and Mixing

Aspects on Neutrino (Mass-) and Mixing Aspcts on Nutrino (Mass-) and Mixing Carn Hagnr, Univrsität Haburg Introduction: nutrino ass and ixing Nutrino Oscillation (I): u tau ixing atosphric nutrinos prsnt nutrino ba xprints: MINOS (NuMi ba:

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

Solar spectrum. Nuclear burning in the sun produce Heat, Luminosity and Neutrinos. pp neutrinos < 0.4 MeV

Solar spectrum. Nuclear burning in the sun produce Heat, Luminosity and Neutrinos. pp neutrinos < 0.4 MeV SOLAR NEUTRINOS Solar spectrum Nuclear burning in the sun produce Heat, Luminosity and Neutrinos pp neutrinos < 0.4 MeV Beryllium neutrinos 0.86 MeV Monochromatic since 2 body decay 2 kev width due to

More information

Radial Cataphoresis in Hg-Ar Fluorescent Lamp Discharges at High Power Density

Radial Cataphoresis in Hg-Ar Fluorescent Lamp Discharges at High Power Density [NWP.19] Radal Cataphorss n Hg-Ar Fluorscnt Lamp schargs at Hgh Powr nsty Y. Aura, G. A. Bonvallt, J. E. Lawlr Unv. of Wsconsn-Madson, Physcs pt. ABSTRACT Radal cataphorss s a procss n whch th lowr onzaton

More information

1- Summary of Kinetic Theory of Gases

1- Summary of Kinetic Theory of Gases Dr. Kasra Etmad Octobr 5, 011 1- Summary of Kntc Thory of Gass - Radaton 3- E4 4- Plasma Proprts f(v f ( v m 4 ( kt 3/ v xp( mv kt V v v m v 1 rms V kt v m ( m 1/ v 8kT m 3kT v rms ( m 1/ E3: Prcntag of

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

ITER Performance Study with the Presence of Internal Transport Barrier

ITER Performance Study with the Presence of Internal Transport Barrier J. Plasma Fuson Rs. SERIES, Vol. 8 (9) IER Prformanc Study wth th Prsnc of Intrnal ransport arrr hawatcha Onjun Plasma and Fuson Rsarch Unt, Srndhorn Intrnatonal Insttut of chnology, hammasat Unvrsty,

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

Oklahoma State University. Solar Neutrinos and their Detection Techniques. S.A.Saad. Department of Physics

Oklahoma State University. Solar Neutrinos and their Detection Techniques. S.A.Saad. Department of Physics Oklahoma State University Solar Neutrinos and their Detection Techniques S.A.Saad Department of Physics Topics to be covered Solar Neutrinos Solar Neutrino Detection Techniques Solar Neutrino Puzzle and

More information

CHAPTER 4. The First Law of Thermodynamics for Control Volumes

CHAPTER 4. The First Law of Thermodynamics for Control Volumes CHAPTER 4 T Frst Law of Trodynacs for Control olus CONSERATION OF MASS Consrvaton of ass: Mass, lk nrgy, s a consrvd proprty, and t cannot b cratd or dstroyd durng a procss. Closd systs: T ass of t syst

More information

Structure of the Atom. Thomson s Atomic Model. Knowledge of atoms in Experiments of Geiger and Marsden 2. Experiments of Geiger and Marsden

Structure of the Atom. Thomson s Atomic Model. Knowledge of atoms in Experiments of Geiger and Marsden 2. Experiments of Geiger and Marsden CHAPTER 4 Structur of th Atom 4.1 Th Atomic Modls of Thomson and Ruthrford 4. Ruthrford Scattring 4.3 Th Classic Atomic Modl 4.4 Th Bohr Modl of th Hydrogn Atom 4.5 Succsss & Failurs of th Bohr Modl 4.6

More information

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

Chemical Engineering 412

Chemical Engineering 412 Chical Enginring 4 Introductory Nuclar Enginring Lctur 6 Nuclar Radiation Typs Ky oints Typs of cay Na roprtis athatical scriptions Cavats cay Charts (KNOW HOW TO USE!) Nuclar Equation for cay -Valus for

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

Moon Moon Devi. INO.

Moon Moon Devi. INO. Moon Moon Dvi. INO. Plan of Th Talk: Motivation. Nutrino intractions and cross sctions. Diffrnt Exprimnts to masur nutrino cross sctions Dscriptions. Rsults. Conclusion. Motivation: To study nuclon structur.

More information

DO PHYSICS ONLINE FROM QUANTA TO QUARKS HIGH ENERGY PARTICLE PHYSICS

DO PHYSICS ONLINE FROM QUANTA TO QUARKS HIGH ENERGY PARTICLE PHYSICS DO PHYSICS ONLINE FROM QUANTA TO QUARKS HIGH ENERGY PARTICLE PHYSICS THE STANDARD MODEL OF MATTER Th Quanta to Quarks option consists of a numbr of parts, som of which concrn th "Standard Modl" of subatomic

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

Physics 256: Lecture 2. Physics

Physics 256: Lecture 2. Physics Physcs 56: Lctur Intro to Quantum Physcs Agnda for Today Complx Numbrs Intrfrnc of lght Intrfrnc Two slt ntrfrnc Dffracton Sngl slt dffracton Physcs 01: Lctur 1, Pg 1 Constructv Intrfrnc Ths wll occur

More information

Constituents of the Atom

Constituents of the Atom 1 Constitunts of th Atom To b know th constitunts of th atom with thir masss and chargs To b abl to calculat th spcific charg of th constitunts To b abl to xplain what isotops and ions ar Th Nuclar Modl

More information

Ερωτήσεις και ασκησεις Κεφ. 10 (για μόρια) ΠΑΡΑΔΟΣΗ 29/11/2016. (d)

Ερωτήσεις και ασκησεις Κεφ. 10 (για μόρια) ΠΑΡΑΔΟΣΗ 29/11/2016. (d) Ερωτήσεις και ασκησεις Κεφ 0 (για μόρια ΠΑΡΑΔΟΣΗ 9//06 Th coffcnt A of th van r Waals ntracton s: (a A r r / ( r r ( (c a a a a A r r / ( r r ( a a a a A r r / ( r r a a a a A r r / ( r r 4 a a a a 0 Th

More information

??? Dynamic Causal Modelling for M/EEG. Electroencephalography (EEG) Dynamic Causal Modelling. M/EEG analysis at sensor level. time.

??? Dynamic Causal Modelling for M/EEG. Electroencephalography (EEG) Dynamic Causal Modelling. M/EEG analysis at sensor level. time. Elctroncphalography EEG Dynamc Causal Modllng for M/EEG ampltud μv tm ms tral typ 1 tm channls channls tral typ 2 C. Phllps, Cntr d Rchrchs du Cyclotron, ULg, Blgum Basd on slds from: S. Kbl M/EEG analyss

More information

A=P=E M-A=N Alpha particle Beta Particle. Periodic table

A=P=E M-A=N Alpha particle Beta Particle. Periodic table Nam Pr. Atomic Structur/Nuclar Chmistry (Ch. 3 & 21) OTHS Acadmic Chmistry Objctivs: Undrstand th xprimntal dsign and conclusions usd in th dvlopmnt of modrn atomic thory, including Dalton's Postulats,

More information

Physics 2D Lecture Slides Lecture 14: Feb 1 st 2005

Physics 2D Lecture Slides Lecture 14: Feb 1 st 2005 Physics D Lctur Slids Lctur 14: Fb 1 st 005 Vivk Sharma UCSD Physics Compton Effct: what should Happn Classically? Plan wav [f,λ] incidnt on a surfac with loosly bound lctrons intraction of E fild of EM

More information

Status of Solar Neutrino Oscillations

Status of Solar Neutrino Oscillations Status of Solar Neutrino Oscillations With many thanks to Dave Wark - RAL/ University of Sussex and Stephen Brice - Fermilab The Solar Neutrino Problem Next three plots adapted from http://www.sns.ias.edu/~jnb/

More information

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

APP-IV Introduction to Astro-Particle Physics. Maarten de Jong APP-IV Introduction to Astro-Particl Physics Maartn d Jong 1 cosmology in a nut shll Hubbl s law cosmic microwav background radiation abundancs of light lmnts (H, H, ) Hubbl s law (199) 1000 vlocity [km/s]

More information

Fine Structure Calculation of Energy Levels, Oscillator Strengths and Lifetimes in Se-Like Ions

Fine Structure Calculation of Energy Levels, Oscillator Strengths and Lifetimes in Se-Like Ions ISSN: 77-75 ISO 9:8 Crtfd Intrnatonal Journal of Engnrng and Innovatv Tchnology (IJEIT) Volum, Issu 6, Dcmbr Fn Structur Calculaton of Enrgy Lvls, Oscllator Strngths and Lftms n S-Lk Ions M. Mossad, Abr

More information

Magnetic Neutron Scattering

Magnetic Neutron Scattering Magntc utron Scattrng Martn Rottr Insttut für Physkalsch Chm, Unvrstät Wn Martn Rottr ESY Wntr School 005 Contnts Introucton: utrons an Magntsm Elastc Magntc Scattrng Inlastc Magntc Scattrng Martn Rottr

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

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

Neutrino Physics: Lecture 1

Neutrino Physics: Lecture 1 Neutrino Physics: Lecture 1 Overview: discoveries, current status, future Amol Dighe Department of Theoretical Physics Tata Institute of Fundamental Research Feb 1, 2010 Plan of the course Omnipresent

More information

Physics 2D Lecture Slides. Oct 21. UCSD Physics. Vivek Sharma

Physics 2D Lecture Slides. Oct 21. UCSD Physics. Vivek Sharma Physics D Lctur Slids Oct 1 Vivk Sharma UCSD Physics Modrn Viw of Photolctric Effct E = hf = KE+ ϕ Is h sam in Photolctric Effct as in BBQ Radiation? Slop h = 6.66 x 10-34 JS Einstin Nobl Priz! No mattr

More information

Geo-neutrinos Status and Prospects

Geo-neutrinos Status and Prospects Go-nutrinos Status and Prospcts Applid Antinutrino Physics Octobr 01 ν + Stv Dy Hawaii Pacific Univrsity Univrsity of Hawaii p u u d W d u d n Outlin Earth nrgy balanc Aq = Mh Mc( T/ t) Radiognic hat/go-nutrinos

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

Radio-chemical method

Radio-chemical method Neutrino Detectors Radio-chemical method Neutrino reactions: n+ν e => p+e - p+ν e => n+e + Radio chemical reaction in nuclei: A N Z+ν e => A-1 N(Z+1)+e - (Electron anti-neutrino, right) (Z+1) will be extracted,

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

Study of Dynamic Aperture for PETRA III Ring K. Balewski, W. Brefeld, W. Decking, Y. Li DESY

Study of Dynamic Aperture for PETRA III Ring K. Balewski, W. Brefeld, W. Decking, Y. Li DESY Stud of Dnamc Aprtur for PETRA III Rng K. Balws, W. Brfld, W. Dcng, Y. L DESY FLS6 Hamburg PETRA III Yong-Jun L t al. Ovrvw Introducton Dnamcs of dampng wgglrs hoc of machn tuns, and optmzaton of stupol

More information

Andre Schneider P621

Andre Schneider P621 ndr Schnidr P61 Probl St #03 Novbr 6, 009 1 Srdnicki 10.3 Vrtx for L 1 = gχϕ ϕ. Th vrtx factor is ig. ϕ ig χ ϕ igur 1: ynan diagra for L 1 = gχϕ ϕ. Srdnicki 11.1 a) Dcay rat for th raction ig igur : ynan

More information

Discovery of the Neutrino Mass-I. P1X* Frontiers of Physics Lectures October 2004 Dr Paul Soler University of Glasgow

Discovery of the Neutrino Mass-I. P1X* Frontiers of Physics Lectures October 2004 Dr Paul Soler University of Glasgow -I P1X* Frontiers of Physics Lectures 19-0 October 004 Dr Paul Soler University of Glasgow Outline 1. Introduction: the structure of matter. Neutrinos:.1 Neutrino interactions. Neutrino discovery and questions.3

More information

Properties and types of water. Properties of water

Properties and types of water. Properties of water PART 3 Proprtis and typs of watr Proprtis of watr Chmical form: H 2 O Physical stats: gas (vapor) liquid (watr) solid (ic, snow) Molcular structur: On oxygn atom and two hydrogn atoms ar arrangd as in

More information

Arturo R. Samana* in collaboration with Carlos Bertulani*, & FranjoKrmpotic(UNLP-Argentina) *Department of Physics Texas A&M University -Commerce 07/

Arturo R. Samana* in collaboration with Carlos Bertulani*, & FranjoKrmpotic(UNLP-Argentina) *Department of Physics Texas A&M University -Commerce 07/ Comparison of RPA-lik modls in Nurino-Nuclus Nuclus Procsss Aruro R. Samana* in collaboraion wih Carlos Brulani* & FranjoKrmpoicUNLP-Argnina *Dparmn of Physics Txas A&M Univrsiy -Commrc 07/ 0/008 Aomic

More information

Physics of Very High Frequency (VHF) Capacitively Coupled Plasma Discharges

Physics of Very High Frequency (VHF) Capacitively Coupled Plasma Discharges Physcs of Vry Hgh Frquncy (VHF) Capactvly Coupld Plasma Dschargs Shahd Rauf, Kallol Bra, Stv Shannon, and Kn Collns Appld Matrals, Inc., Sunnyval, CA AVS 54 th Intrnatonal Symposum Sattl, WA Octobr 15-19,

More information

ST 524 NCSU - Fall 2008 One way Analysis of variance Variances not homogeneous

ST 524 NCSU - Fall 2008 One way Analysis of variance Variances not homogeneous ST 54 NCSU - Fall 008 On way Analyss of varanc Varancs not homognous On way Analyss of varanc Exampl (Yandll, 997) A plant scntst masurd th concntraton of a partcular vrus n plant sap usng ELISA (nzym-lnkd

More information

Chapter 8: Electron Configurations and Periodicity

Chapter 8: Electron Configurations and Periodicity Elctron Spin & th Pauli Exclusion Principl Chaptr 8: Elctron Configurations and Priodicity 3 quantum numbrs (n, l, ml) dfin th nrgy, siz, shap, and spatial orintation of ach atomic orbital. To xplain how

More information

DIS-Parity. Search for New Physics Through Parity Violation In Deep Inelastic Electron Scattering. The Physics Case

DIS-Parity. Search for New Physics Through Parity Violation In Deep Inelastic Electron Scattering. The Physics Case DIS-Parity Sarch for Nw Physics Through Parity Violation In Dp Inlastic Elctron Scattring Th Physics Cas R. Arnold for th DIS-Parity Collaboration Exprimnt Plan by Stv Rock will follow 12 Jun 2003 DIS-Parity

More information

The Death of Stars - II.

The Death of Stars - II. Th Dath of Stars - II. Larning Objctivs! How can w us H-R diagrams to masur th ag of star clustrs (and hnc th ag of our Univrs)?! Why do high and low mass stars volv diffrntly? How ar havy lmnts such as

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

New Muon Lifetime and the Fermi Coupling Constant G F. Kevin Giovanetti James Madison University

New Muon Lifetime and the Fermi Coupling Constant G F. Kevin Giovanetti James Madison University Nw Muon Liftim and th Frmi Coupling Constant G F Kvin Giovantti Jams Madison Univrsity HallC mting, JLAB, Aug 10, 007 a µ = g µ / Prcision FUNDAMENTAL Muon Phyiscs SYMMETRIES Prcision Masurmnts of Standard

More information

Neutrino Experiments: Lecture 2 M. Shaevitz Columbia University

Neutrino Experiments: Lecture 2 M. Shaevitz Columbia University Neutrino Experiments: Lecture 2 M. Shaevitz Columbia University 1 Outline 2 Lecture 1: Experimental Neutrino Physics Neutrino Physics and Interactions Neutrino Mass Experiments Neutrino Sources/Beams and

More information

Searching for chirality flipping interactions in nuclear beta decay. Presentation to REU Students July 2015

Searching for chirality flipping interactions in nuclear beta decay. Presentation to REU Students July 2015 Sarching for chirality flipping intractions in nuclar bta dcay Prsntation to REU Studnts July 015 Wak intractions in nucli: a prob to sarch for nw physics Aljandro Garcia Univrsity of Washington Whil th

More information

Particle Physics WS 2012/13 ( )

Particle Physics WS 2012/13 ( ) Particle Physics WS 2012/13 (22.1.2013) Stephanie Hansmann-Menzemer Physikalisches Institut, INF 226, 3.101 Reminder: No lecture this Friday 25.01.2012 2 Neutrino Types and Sources Neutrinos are only detected

More information

Neutrino oscillation experiments: Recent results and implications

Neutrino oscillation experiments: Recent results and implications Title transparency Neutrino oscillation experiments: Recent results and implications W. Hampel MPI Kernphysik Heidelberg Motivation for talk On the way from the Standard Model to String Theory: appropriate

More information

Laboratorio di Fisica delle Particelle COSMIC MUONS. Giorgia Albani Daniele Cortinovis Alessandra Gaeta Davide Rozza

Laboratorio di Fisica delle Particelle COSMIC MUONS. Giorgia Albani Daniele Cortinovis Alessandra Gaeta Davide Rozza Laboratorio di Fisica dll Particll COSMIC MUONS Giorgia Albani Danil Cortinovis Alssandra Gata David Rozza Rlazion di laboratorio di: Giorgia Albani, Danil Cortinovis, Alssandra Gata, David Rozza ABSTRACT

More information

SOLAR NEUTRINO PROBLEM SOLVED

SOLAR NEUTRINO PROBLEM SOLVED Fakulteta za matematiko in fiziko Oddelek za fiziko Jadranska 19 1000 Ljubljana UROŠ BOROVŠAK SOLAR NEUTRINO PROBLEM SOLVED ADVISOR dr. TOMAŽ PODOBNIK Ljubljana, April 2, 2003 Abstract Since the end of

More information

Chart of Elementary Particles

Chart of Elementary Particles Chart of Elementary Particles Chart of Elementary Particles Better Chart! Better Chart! As of today: Oscillation of 3 massive active neutrinos is clearly the dominant effect: If neutrinos have mass: For

More information

Phy213: General Physics III 4/10/2008 Chapter 22 Worksheet 1. d = 0.1 m

Phy213: General Physics III 4/10/2008 Chapter 22 Worksheet 1. d = 0.1 m hy3: Gnral hyscs III 4/0/008 haptr Worksht lctrc Flds: onsdr a fxd pont charg of 0 µ (q ) q = 0 µ d = 0 a What s th agntud and drcton of th lctrc fld at a pont, a dstanc of 0? q = = 8x0 ˆ o d ˆ 6 N ( )

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

Neutrinos: What we ve learned and what we still want to find out. Jessica Clayton Astronomy Club November 10, 2008

Neutrinos: What we ve learned and what we still want to find out. Jessica Clayton Astronomy Club November 10, 2008 Neutrinos: What we ve learned and what we still want to find out Jessica Clayton Astronomy Club November 10, 2008 Neutrinos, they are very small, they have no charge and have no mass, and do not interact

More information

Review of Solar Neutrinos. Alan Poon Institute for Nuclear and Particle Astrophysics & Nuclear Science Division Lawrence Berkeley National Laboratory

Review of Solar Neutrinos. Alan Poon Institute for Nuclear and Particle Astrophysics & Nuclear Science Division Lawrence Berkeley National Laboratory Review of Solar Neutrinos Alan Poon Institute for Nuclear and Particle Astrophysics & Nuclear Science Division Lawrence Berkeley National Laboratory Solar Neutrinos pp chain: 4p + 2e 4 He + 2ν e + 26.7

More information

Alpha and beta decay equation practice

Alpha and beta decay equation practice Alpha and bta dcay quation practic Introduction Alpha and bta particls may b rprsntd in quations in svral diffrnt ways. Diffrnt xam boards hav thir own prfrnc. For xampl: Alpha Bta α β alpha bta Dspit

More information

The Standard Model Lagrangian

The Standard Model Lagrangian Th Standard Modl aranian Elmntary Particl Physics Stron Intraction Fnomnoloy Dio Bttoni Acadmic ar - D. Bttoni Fnomnoloia Intrazioni Forti Dirac Formalism m i j Consrvd Currnt i i i 5 i m Gau Invarianc

More information

The Weak Interaction: A Drama in Many Acts

The Weak Interaction: A Drama in Many Acts Th Wak Intraction: A Drama in Many Acts 1890 s: Rontgn discovrs rays Thought Uranium salts wr affctd by th sun but rainy Paris soon hlpd showing othrwis. 190 s: Pauli proposs To xplain continuous spctrum:

More information

IV. e + e annihilation experiments 1. Experimental methods Discovery of the Tau-Lepton 5. hadrons 6. Hadronic resonances

IV. e + e annihilation experiments 1. Experimental methods Discovery of the Tau-Lepton 5. hadrons 6. Hadronic resonances IV. annihilation xprimnts 1. Exprimntal mthods. 3. 4. Discovry of th Tau-Lpton 5. (γ ) µ µ (γ ) hadrons 6. Hadronic rsonancs Lit.: H.U Martyn, Tst of QED in Quantum Elctrodynamics, T.Kinoshita (d.) 1.

More information

HERA - Structure of Matter and QCD

HERA - Structure of Matter and QCD HERA - Structur of Mattr and QCD p Contnts 5 yar running of HERA and H/ZEUS Elctrowak rsults Structur of th proton Katsuo Tokushuku (KEK, ZEUS) DESY/HERA HERA 99-7 H ZEUS HERA: (7.5GV lctron 9GVproton)

More information

PHYSICS 2150 EXPERIMENTAL MODERN PHYSICS. Lecture 3 Statistical vs. Systematic Errors,Rejection of Data; Weighted Averages

PHYSICS 2150 EXPERIMENTAL MODERN PHYSICS. Lecture 3 Statistical vs. Systematic Errors,Rejection of Data; Weighted Averages PHYSICS 150 EXPERIMENTAL MODERN PHYSICS Lctur 3 Statistical vs. Systmatic Errors,Rjction of Data; Wightd Avrags SO FAR WE DISCUSS STATISTICAL UNCERTAINTY. NOW WHAT ABOUT UNCERTAINTY INVOLVED WITH MEASUREMENT

More information

ACOUSTIC WAVE EQUATION. Contents INTRODUCTION BULK MODULUS AND LAMÉ S PARAMETERS

ACOUSTIC WAVE EQUATION. Contents INTRODUCTION BULK MODULUS AND LAMÉ S PARAMETERS ACOUSTIC WAE EQUATION Contnts INTRODUCTION BULK MODULUS AND LAMÉ S PARAMETERS INTRODUCTION As w try to vsualz th arth ssmcally w mak crtan physcal smplfcatons that mak t asr to mak and xplan our obsrvatons.

More information

UNIT1: Experimental Evidences of Neutrino Oscillation Atmospheric and Solar Neutrinos

UNIT1: Experimental Evidences of Neutrino Oscillation Atmospheric and Solar Neutrinos UNIT1: Experimental Evidences of Neutrino Oscillation Atmospheric and Solar Neutrinos Stefania Ricciardi HEP PostGraduate Lectures 2016 University of London 1 Neutrino Sources Artificial: nuclear reactors

More information

1. Neutrino Oscillations

1. Neutrino Oscillations Neutrino oscillations and masses 1. Neutrino oscillations 2. Atmospheric neutrinos 3. Solar neutrinos, MSW effect 4. Reactor neutrinos 5. Accelerator neutrinos 6. Neutrino masses, double beta decay 1.

More information

Deconfinement phase transition in SU(3)/Z3 QCD (adj) via the gauge theory/affine XY-model duality

Deconfinement phase transition in SU(3)/Z3 QCD (adj) via the gauge theory/affine XY-model duality Dconfnmnt phas transton n SU(3)/Z3 QCD (adj) va th gaug thory/affn XY-modl dualty MOHAMED ABER UIVERSITY OF TOROTO TH W O R K S H O P O O - P E R T U R B A T I V E Q C D M.A., Erch Popptz, Mthat Unsal

More information

Chapter 3. r r. Position, Velocity, and Acceleration Revisited

Chapter 3. r r. Position, Velocity, and Acceleration Revisited Chapter 3 Poston, Velocty, and Acceleraton Revsted The poston vector of a partcle s a vector drawn from the orgn to the locaton of the partcle. In two dmensons: r = x ˆ+ yj ˆ (1) The dsplacement vector

More information

Neutrino Oscillations

Neutrino Oscillations Neutrino Oscillations Elisa Bernardini Deutsches Elektronen-Synchrotron DESY (Zeuthen) Suggested reading: C. Giunti and C.W. Kim, Fundamentals of Neutrino Physics and Astrophysics, Oxford University Press

More information

Jones vector & matrices

Jones vector & matrices Jons vctor & matrcs PY3 Colást na hollscol Corcagh, Ér Unvrst Collg Cork, Irland Dpartmnt of Phscs Matr tratmnt of polarzaton Consdr a lght ra wth an nstantanous -vctor as shown k, t ˆ k, t ˆ k t, o o

More information