F i n a l C i r c u l a r (revised 99/7/9) International Workshop on Atomic Collisions and Atomic Spectroscopy with Slow Antiprotons

Size: px
Start display at page:

Download "F i n a l C i r c u l a r (revised 99/7/9) International Workshop on Atomic Collisions and Atomic Spectroscopy with Slow Antiprotons"

Transcription

1 F i n a l C i r c u l a r (rvisd 99/7/9) Intrnational Workshop on Atomic Collisions and Atomic Spctroscopy with Slow Antiprotons July 19-21, 1999, Tsurumi, Yokohama, Kanagawa, Japan Th Intrnational Workshop on Atomic Collisions and Atomic Spctroscopy with Slow Antiprotons will b hld from July 19 to 21, Th Workshop is organizd by Th Antimattr Scinc Projct, Univrsity of Tokyo, Th Cntr for CERN rlatd Atomic and Nuclar Physics of th Danish Natural Scinc Rsarch Council, and RIKEN. Workshop Schdul & Sit: July 18 th : Wlcom Drink: 19:30-21:30, Room Sumir, 3 rd floor of th Nw Towr of Sinagawa Princ Hotl Rgistration Dsk: 18:00-21:30, th sam room as th Wlcom Drink July 19 th : Bus from Shinagawa Princ Hotl to Tsurumi Girls High School: 8:00 Rgistration Dsk: 9:00-16:00, at Tsurumi Girls High School Scintific Program: 9:00-16:00 at Tsurumi Girls High School Social Program (Zaznkai): 16:10- at Sojiji-Tmpl Bus from Tsurumi Girls High School to Shinagawa Princ Hotl (for thos who do NOT join th Social Program at Sojiji): 16:10 July 20 th : Bus from Shinagawa Princ Hotl to Tsurumi Girls High School (for thos who do not join th Social Program at Sojiji): 8:00 Rgistration Dsk: 9:00-17:00, at Tsurumi Girls High School Scintific Program:9:00-17:20 at Tsurumi Girls High School Bus from Tsurumi Girls High School to Shinagawa Princ Hotl: 17:30 Workshop Banqut: 19:00-21:00 at Room Aso, 6 th floor of th Nw Towr of Sinagawa Princ Hotl July 21 st : Scintific Program:9:00-12:30 at Room Aso, 6 th floor of th Nw Towr of Sinagawa Princ Hotl

2 Accommodation: For thos who rsrvd a room at Shinagawa Princ Hotl: All th rooms for pbar99 attnds ar rsrvd at "Nw Towr" of th Hotl. Room Rat Singl Twin With Brakfast Without Brakfast 9,800 9,200 (srvic charg includd, tax not includd) Th wb sit of th hotl is 17,800 16,300

3 Transportation: From Narita Airport to Shinagawa Princ Hotl: (1)Dirct Connction by Limousin Bus ( (2)From Narita Airport to Nippori by Kisi Railway Lin (about 1 hour), from Nippori to Shinagawa by Yamanot Lin (about 20 minuts), and a coupl of minuts walk to th Hotl (othr possibilitis could b found at /accss_ /accss_indx.html) From Shinagawa Princ Hotl to Tsurumi Girls High School: (1) By th chartrd bus: Th bus will lav th Hotl on 8:00. All th Workshop attnds who ar intrstd in ar xpctd to prsnt at th "Front Srvic" of th Hotl (1 st floor of th Nw Towr) bfor 7:55. (2) By Train: JR Kihin-Tohoku Lin from Shinagawa Station to Tsurumi Station (about 15min.) From JR Tsurumi Station to Tsurumi Girls High School: Follow th rd dottd lin drawn in th map attachd in th nxt pag Rgistration Dsk: Th rgistration dsk will opn from 18:00, July 18 th (Sunday) at Sumir (th room for Wlcom Drink) at 3 rd floor of th Shinagawa Princ Hotl. Th rgistration f ( 20,000) must b paid at th dsk. W can only accpt Japans Yn in cash. Th rgistration f includs th abstract book, coff during coff brak, and all th Social Programs. Th rgistration f for th accompanying prson(s) is 10,000, which includs all th Social Program.

4 To Shinagawa Tokyo Tsurumi Station Tsurumi Girls High School sojiji rcption To Yokohama slop Gat Hospital

5 Intrnational Advisory Board: J.Burgdorfr, J.S.Cohn, R.Hayano, M.H.Holzschitr, D.Horvath, M.Inokuti, H.Knudsn, K.Komaki, T.Yamazaki, Y.Yamazaki, Organizing Committ: R.Hayano, H.Knudsn, K.Komaki, T.Yamazaki, Y.Yamazaki Workshop Chairman: Kn-ichiro Komaki Addrss of Corrspondnc: Yasunori Yamazaki or Ms. Chikako Kuramochi (Workshop scrtary) Antiproton Workshop, Institut of Physics, Univrsity of Tokyo, Komaba 3-8-1, Komaba, Mguro-ku, Tokyo, , Japan, tl: , fax: wb: In cas of mrgncy: Scintific Program ( slid projctors ar NOT availabl) July 19 th, morning sssion I: K.Komaki (30min): Antimattr Scinc with Slow Antiprotons H.Knudsn(30min): Exprimntal data on ionization and nrgy loss for antiprotons colliding with mattr P.Krstic (30min): Ionization of ions and atoms by slow antiprotons A.Igarashi(15min): Ionization of atomic hydrogn with antiprotons July 19 th, morning sssion II: R.Hayano (30min): Lasr spctroscopy of protonium J.S.Cohn (30min): Isotop ffcts on antiproton captur M.Fujiwara (30min): Muon catalyzd fusion studis with a muonic hydrogn bam at TRIUMF K.Ohtsuki (20min): + July 19, aftrnoon sssion: K.Fin (40min): Nonnutral plasmas and antihydrogn production T.Ichioka (30min): Status rport on th ASACUSA antiproton trapping systm H.Totsuji (30min) : Two-Componnt Nonquilibrium Nonnutral Plasma in Pnning-Malmbrg Trap

6 July 20 th, morning sssion I M.Hori(30min): High-prcision, two-photon lasr spctroscopy of antiprotonic hlium atoms and othr xprimnts using ultra-low dnsity targts Y.Kino (30min): Non-Adiabatic High-Prcision Calculation of Antiprotonic Hlium Atomcul and Dtrmination of Antiproton Mass V. I.Korobov (30min): Spctroscopy of th antiprotonic atomcul T.Koik(20min): Nuclar absorption procss in antiprotonic hlium atoms July 20 th, morning sssion II: G.Ya.Kornman (30min): Collisions of antiprotonic atomculs with H atoms D.Bakalov (30min): Dnsity shift and broadning of th transition lins in antiprotonic hlium T.Azuma (20min) : Dos a solvatd antiproton xist? July 20 th, aftrnoon sssion I: H.Schmidt-Bocking (30min): Comparison of multi-diffrntial ionization cross sctions in fast antiproton and proton on Hlium collisions --- A proposal for futur studis with a tabl sizd PBAR-storag ring C.D.Lin (30min): Ionization of H and H atoms by antiprotons rvisitd A.Kovr (30min): Post Collision Intraction at Proton, Antiproton - Atom Collisions July 20 th, aftrnoon sssion II: R.Schuch (20min): An accurat masurmnt of th p mass using highly chargd ions in a Pnning trap E.Mornzoni (30min): A nw low nrgtic muon bam and its applications N.Kabachnik (20min): Channling of slow antiprotons July 21 st, morning sssion I: M.Holzschitr (30min): Tsts of CPT, Lorntz Invarianc and th WEP with Antihydrogn R.Schuch (20min): Making Hbar by rcombination in a Pnning trap S.Schipprs (30min): Rcombination of H-lik ions with lctrons: a tsting ground for th formation of antihydrogn? P.Frolich (20min): Hydrogn - Antihydrogn Collisions July 21 st, morning sssion II: Panl Discussion: Antihydrogn Production & Spctroscopy M.Inokuti (20min): Concluding Rmarks

7 Mor dtails on Zaznkai: July 19 th A Spcial Lctur & Zaznkai at Sojiji Tmpl (Th sam campus as th Workshop sit) 16:10-18:15 Mal Prparation 18:15-19:05 Spcial Lctur: Zn Gardn as an Expansion of Mind by Mr. Shunmyo Masuno (Zn Prist, Gardn Architct, Visiting Prof. of British Columbia Univ.) 19:15-20:05 Dharma Talk by Mr. Dosho Saikawa (Zn Prist of Sojiji Tmpl) 20:15 Zazn Sssion 20:45 Explanation and Instruction of Morning Srvic 21:00 Light out 20 th 3:30 Wak up 4:00 Morning Zazn Sssion 5:00 Morning Srvic/ Crmony 7:00 Brakfast 8:00 Tour of Sojiji, or a discussion about Zazn Not for Zaznkai Attnds: Bring 1)writing matrials, 2)comfortabl cloths for Zn practic, 3)a tooth brush, 4)a hand towl, 5)an umbrlla, 6) socks (prfrably whit) You could join just th lctur without having practic. In this cas, howvr, thr is no bus transportation srvic from Sojiji to Shinagawa Princ Hotl on you way back. Som Usful Information Travl information on Japan: Accss from Narita Airport: /accss_ /accss_indx.html Limousin bus timtabl from Narita Airport to th hotl:

8 Workshop Rgistration Form Plas fill th rgistration form blow and snd it to th following addrss prfrably via at your arlist convninc but NOT latr than Jun 10 th to: Yasunori Yamazaki or Ms.Chikako Kuramochi Antiproton Workshop Institut of Physics, Univrsity of Tokyo, Komaba 3-8-1, Komaba, Mguro-ku, Tokyo, , Japan tl: fax: Your mail or fax should b acknowldgd soon. If you do not har from us within a wk, plas snd your mail to yasunori@postman.rikn.go.jp Family Nam First and Middl Nams Titl Institution Addrss City Zip Cod Country Phon Fax E- mail Nam(s) of Accompanying Prson(s)

9 Morning sssion(1) Morning sssion(2) Aftrnoon Sssion(1) Aftrnoon Sssion(2) Evning Sssion 18 th 19 th 19:30- Wlcom drink at Shinagawa Princ Hotl 9:00-10:45 (T.Yamazaki) 11:10-13:00 (H.Knudsn) 14:20-16:00 (A.Mohri) 16:00- K.Komaki (30min) R.Hayano (30min) K.Fin (40min) Antimattr Scinc with Slow Antiprotons c Lasr spctroscopy of protonium l Nonnutral plasmas and antihydrogn production H.Knudsn(30min) o J.S.Cohn (30min) u T.Ichioka (30min) Exprimntal data on ionization and nrgy loss for Isotop ffcts on antiproton captur Status rport on th ASACUSA antiproton trapping antiprotons colliding with mattr ff n M.Fujiwara (30min) systm P.Krstic (30min) Muon catalyzd fusion studis with a muonic c H.Totsuji (30min) Ionization of ions and atoms by slow antiprotons hydrogn bam at TRIUMF h Two-Componnt Nonquilibrium Nonnutral Plasma in Z a z n k a i at Sojiji A.Igarashi(15min) Ionization of atomic hydrogn with antiprotons K.Ohtsuki (20min) Antiprotonic lithium atom ; formation, nrgy lvls and stability Pnning-Malmbrg Trap 20 th 9:00-10:50 (J.Eads) 11:20-12:40 14:00-15:30 (N.Toshima) 16:00-17:10 19:00- M.Hori(30min) High-prcision, two-photon lasr spctroscopy of antiprotonic hlium atoms and othr xprimnts using ultra-low dnsity targts Y.Kino (30min) Non-Adiabatic High-Prcision Calculation of Antiprotonic Hlium Atomcul and Dtrmination of Antiproton Mass V. I.Korobov (30min) Spctroscopy of th antiprotonic atomcul T.Koik(20min) Nuclar absorption procss in antiprotonic hlium atoms c o ff (T.Watanab) G.Ya.Kornman (30min) Collisions of antiprotonic atomculs with H atoms D.Bakalov (30min) Dnsity shift and broadning of th transition lins in antiprotonic hlium T.Azuma (20min) Dos a xist? solvatd antiproton 9:00-10:40 (D.Horvath) 11:00-12:30 (J.Eichlr) 21 st M.Holzschitr (30min) Tsts of CPT, Lornz Invarianc and th WEP with Antihydrogn R.Schuch (20min) Making Hbar by rcombination in a Pnning trap S.Schipprs (30min) Rcombination of H-lik ions with lctrons: a tsting ground for th formation of anti-hydrogn? P.Frolich (20min) Hydrogn - Antihydrogn Collisions c o ff l u n c h Panl Discussion Antihydrogn Production & Spctroscopy M.Inokuti (20min) Concluding Rmarks H.Schmidt-Bocking (30min) Comparison of multi-diffrntial ionization cross sctions in fast antiproton and proton on Hlium collisions --- A proposal for futur studis with a tabl sizd PBAR-storag ring C.D.Lin (30min) Ionization of H and H atoms by antiprotons rvisitd A.Kovr (30min) Post Collision Intraction at Proton, Antiproton - Atom Collisions c o ff (M.Kamimura) R.Schuch (20min) An accurat masurmnt of th p mass using highly chargd ions in a Pnning trap E.Mornzoni (30min) A nw low nrgtic muon bam and its applications N.Kabachnik (20min) Channling of slow antiprotons Banqut at Shinagawa Princ Hotl

10

by g-factor Measurements

by g-factor Measurements Intrnational Bound-Stat Acclrator Quantum Facility Elctrodynamics for Bams in Strong of Ions and Filds Antiprotons Byond at Darmstadt th Furry Pictur by g-factor Masurmnts Wolfgang Quint GSI Darmstadt

More information

The mechanisms of antihydrogen formation

The mechanisms of antihydrogen formation Th mchanisms of antihydrogn formation E.Lodi Rizzini, L.Vnturlli, N.Zurlo, (ATHENA Collaboration) Prsntd by L.Vnturlli Brscia Univrsity & INFN (Italy) 2.5 cm 10 4 pbars 10 8 + 3T 1 Antihydrogn Exprimnts

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

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

ph People Grade Level: basic Duration: minutes Setting: classroom or field site

ph People Grade Level: basic Duration: minutes Setting: classroom or field site ph Popl Adaptd from: Whr Ar th Frogs? in Projct WET: Curriculum & Activity Guid. Bozman: Th Watrcours and th Council for Environmntal Education, 1995. ph Grad Lvl: basic Duration: 10 15 minuts Stting:

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

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

THE MTV EXPERIMENT FROM T-VIOLATION TO LORENTZ-VIOLATION. Jiro Murata Rikkyo University for the MTV collaboration INPC2016, Sydney, Sep 11-16, 2016

THE MTV EXPERIMENT FROM T-VIOLATION TO LORENTZ-VIOLATION. Jiro Murata Rikkyo University for the MTV collaboration INPC2016, Sydney, Sep 11-16, 2016 THE MTV EXPERIMENT FROM T-VIOLATION TO LORENTZ-VIOLATION Jiro Murata Rikkyo Univrsity for th MTV collaboration INPC2016 Sydny Sp 11-16 2016 Rikkyo J. Murata Y. Nakaya Y. Totsuka S. Tanaka R. Tanuma T.

More information

Background: We have discussed the PIB, HO, and the energy of the RR model. In this chapter, the H-atom, and atomic orbitals.

Background: We have discussed the PIB, HO, and the energy of the RR model. In this chapter, the H-atom, and atomic orbitals. Chaptr 7 Th Hydrogn Atom Background: W hav discussd th PIB HO and th nrgy of th RR modl. In this chaptr th H-atom and atomic orbitals. * A singl particl moving undr a cntral forc adoptd from Scott Kirby

More information

Wolfgang Quint GSI Darmstadt and Univ. Heidelberg. Fundamental Constants Meeting, Eltville, Germany, February 2015, Wolfgang Quint

Wolfgang Quint GSI Darmstadt and Univ. Heidelberg. Fundamental Constants Meeting, Eltville, Germany, February 2015, Wolfgang Quint Intrnational Improvd Acclrator Dtrmination Facility for of Bams th of Ions Elctron and Antiprotons Mass in at Darmstadt Atomic Mass Units Wolfgang Quint GSI Darmstadt and Univ. Hidlbrg Intrnational Acclrator

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

Brief on APSCO Data Sharing Service Platform Project

Brief on APSCO Data Sharing Service Platform Project Brif on APSCO Data Sharing Srvic Platform Projct Bijing China, Novmbr, 2012 Origin - Originally, this projct proposal was put forward during th First Exprt Group Mting on Futur Plan (EGMFP-1) of Spac Activitis

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

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

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

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

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

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

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

Precise Masses of particles

Precise Masses of particles /1/15 Physics 1 April 1, 15 Ovrviw of topic Th constitunts and structur of nucli Radioactivity Half-lif and Radioactiv dating Nuclar Binding Enrgy Nuclar Fission Nuclar Fusion Practical Applications of

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

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

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

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

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

Classical Magnetic Dipole

Classical Magnetic Dipole Lctur 18 1 Classical Magntic Dipol In gnral, a particl of mass m and charg q (not ncssarily a point charg), w hav q g L m whr g is calld th gyromagntic ratio, which accounts for th ffcts of non-point charg

More information

State-space behaviours 2 using eigenvalues

State-space behaviours 2 using eigenvalues 1 Stat-spac bhaviours 2 using ignvalus J A Rossitr Slids by Anthony Rossitr Introduction Th first vido dmonstratd that on can solv 2 x x( ( x(0) Th stat transition matrix Φ( can b computd using Laplac

More information

orbiting electron turns out to be wrong even though it Unfortunately, the classical visualization of the

orbiting electron turns out to be wrong even though it Unfortunately, the classical visualization of the Lctur 22-1 Byond Bohr Modl Unfortunatly, th classical visualization of th orbiting lctron turns out to b wrong vn though it still givs us a simpl way to think of th atom. Quantum Mchanics is ndd to truly

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

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

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

(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

The pn junction: 2 Current vs Voltage (IV) characteristics

The pn junction: 2 Current vs Voltage (IV) characteristics Th pn junction: Currnt vs Voltag (V) charactristics Considr a pn junction in quilibrium with no applid xtrnal voltag: o th V E F E F V p-typ Dpltion rgion n-typ Elctron movmnt across th junction: 1. n

More information

Continuous probability distributions

Continuous probability distributions Continuous probability distributions Many continuous probability distributions, including: Uniform Normal Gamma Eponntial Chi-Squard Lognormal Wibull EGR 5 Ch. 6 Uniform distribution Simplst charactrizd

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

Physics 2D Lecture Slides Lecture 12: Jan 28 th 2004

Physics 2D Lecture Slides Lecture 12: Jan 28 th 2004 Brian Wcht, th TA, is away this wk. I will substitut for his offic hours (in my offic 3314 Mayr Hall, discussion and PS sssion. Pl. giv all rgrad rqusts to m this wk (only) Quiz 3 Will Covr Sctions.1-.5

More information

Molecular Orbitals in Inorganic Chemistry

Molecular Orbitals in Inorganic Chemistry Outlin olcular Orbitals in Inorganic Chmistry Dr. P. Hunt p.hunt@imprial.ac.uk Rm 167 (Chmistry) http://www.ch.ic.ac.uk/hunt/ octahdral complxs forming th O diagram for Oh colour, slction ruls Δoct, spctrochmical

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

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

ECE602 Exam 1 April 5, You must show ALL of your work for full credit.

ECE602 Exam 1 April 5, You must show ALL of your work for full credit. ECE62 Exam April 5, 27 Nam: Solution Scor: / This xam is closd-book. You must show ALL of your work for full crdit. Plas rad th qustions carfully. Plas chck your answrs carfully. Calculators may NOT b

More information

(Upside-Down o Direct Rotation) β - Numbers

(Upside-Down o Direct Rotation) β - Numbers Amrican Journal of Mathmatics and Statistics 014, 4(): 58-64 DOI: 10593/jajms0140400 (Upsid-Down o Dirct Rotation) β - Numbrs Ammar Sddiq Mahmood 1, Shukriyah Sabir Ali,* 1 Dpartmnt of Mathmatics, Collg

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

What makes laser light special? Lasers. Lasers. Laser history. Lasers are everywhere! Review of atom discharge lamps. So how do we make laser light?

What makes laser light special? Lasers. Lasers. Laser history. Lasers are everywhere! Review of atom discharge lamps. So how do we make laser light? Lasrs Lasrs What is diffrnt/spcial about lasr light. How dos a lasr work. - rviw atomic discharg lamps. - how light intracts with atoms - how ths idas ar usd to mak lasr. "You know, I hav on simpl rqust.

More information

4E : The Quantum Universe. Lecture 5, April 5 Vivek Sharma

4E : The Quantum Universe. Lecture 5, April 5 Vivek Sharma 4E : Th Quantum Univrs Lctur 5, April 5 Vivk Sharma modphys@hpmail.ucsd.du An X-ray Tub from 0 th Cntury Xray Th High Enrgy Acclrator of 1900s: producd nrgtic light : X Ray, gav nw optic to subatomic world

More information

Overview. Flood Risk in NSW FLOODING, FLOOD MODELLING AND FLOOD MAPPING COMMUNICATION CHALLENGES. Floodplain Risk Management Process

Overview. Flood Risk in NSW FLOODING, FLOOD MODELLING AND FLOOD MAPPING COMMUNICATION CHALLENGES. Floodplain Risk Management Process Sydny Coastal Council Group and Survying and Spatial Scincs Institut Sydny s Intgratd Spatial Futur Customs Hous Th Barnt Long Room Wdnsday 9 Dcmbr 2009 FLOODING, FLOOD MODELLING AND FLOOD MAPPING COMMUNICATION

More information

PHY 114 A General Physics II 11 AM-12:15 PM TR Olin 101. Plan for Lecture 4:

PHY 114 A General Physics II 11 AM-12:15 PM TR Olin 101. Plan for Lecture 4: PHY 114 A Gnral Physics II 11 AM-1:15 PM TR Olin 101 Plan for Lctur 4: 1. Introuction to th lctric potntial.rlationship btwn th lctric potntial an th lctric fil 1/31/01 PHY 114 A Spring 01 -- Lctur 4 1

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

A central nucleus. Protons have a positive charge Electrons have a negative charge

A central nucleus. Protons have a positive charge Electrons have a negative charge Atomic Structur Lss than ninty yars ago scintists blivd that atoms wr tiny solid sphrs lik minut snookr balls. Sinc thn it has bn discovrd that atoms ar not compltly solid but hav innr and outr parts.

More information

The influence of electron trap on photoelectron decay behavior in silver halide

The influence of electron trap on photoelectron decay behavior in silver halide Th influnc of lctron trap on photolctron dcay bhavior in silvr halid Rongjuan Liu, Xiaowi Li 1, Xiaodong Tian, Shaopng Yang and Guangshng Fu Collg of Physics Scinc and Tchnology, Hbi Univrsity, Baoding,

More information

MCB137: Physical Biology of the Cell Spring 2017 Homework 6: Ligand binding and the MWC model of allostery (Due 3/23/17)

MCB137: Physical Biology of the Cell Spring 2017 Homework 6: Ligand binding and the MWC model of allostery (Due 3/23/17) MCB37: Physical Biology of th Cll Spring 207 Homwork 6: Ligand binding and th MWC modl of allostry (Du 3/23/7) Hrnan G. Garcia March 2, 207 Simpl rprssion In class, w drivd a mathmatical modl of how simpl

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

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

Random Access Techniques: ALOHA (cont.)

Random Access Techniques: ALOHA (cont.) Random Accss Tchniqus: ALOHA (cont.) 1 Exampl [ Aloha avoiding collision ] A pur ALOHA ntwork transmits a 200-bit fram on a shard channl Of 200 kbps at tim. What is th rquirmnt to mak this fram collision

More information

SPH4U Electric Charges and Electric Fields Mr. LoRusso

SPH4U Electric Charges and Electric Fields Mr. LoRusso SPH4U lctric Chargs an lctric Fils Mr. LoRusso lctricity is th flow of lctric charg. Th Grks first obsrv lctrical forcs whn arly scintists rubb ambr with fur. Th notic thy coul attract small bits of straw

More information

Machine Detector Interface Workshop: ILC-SLAC, January 6-8, 2005.

Machine Detector Interface Workshop: ILC-SLAC, January 6-8, 2005. Intrnational Linar Collidr Machin Dtctor Intrfac Workshop: ILCSLAC, January 68, 2005. Prsntd by Brtt Parkr, BNLSMD Mssag: Tools ar now availabl to optimiz IR layout with compact suprconducting quadrupols

More information

1-loop effects of MSSM particles in Higgs productions at the ILC

1-loop effects of MSSM particles in Higgs productions at the ILC 1-loop ffcts of MSSM particls in Higgs productions at th ILC Yusaku Kouda, Tadashi Kon, Masato Jimbo A, Yoshimasa Kurihara B, Tadashi Ishikawa B, Kiyoshi Kato C, and Masaaki Kuroda D, Siki Univ., Chiba

More information

Pipe flow friction, small vs. big pipes

Pipe flow friction, small vs. big pipes Friction actor (t/0 t o pip) Friction small vs larg pips J. Chaurtt May 016 It is an intrsting act that riction is highr in small pips than largr pips or th sam vlocity o low and th sam lngth. Friction

More information

eksguyky lq[kkfm+;k fo'ofo ky;] mn;iqj MOHANLAL SUKHADIA UNIVERSITY : UDAIPUR

eksguyky lq[kkfm+;k fo'ofo ky;] mn;iqj MOHANLAL SUKHADIA UNIVERSITY : UDAIPUR S. No. 1 2 3 4 5 6 7 8 9 10 11 12 13 14 ksguyky lq[kkfm+;k fo'ofo ky;] mn;iqj No. F. /MLSU/Rctt./27/3-A Datd :.08.27 DETAILED ADVERTISEMENT FOR VARIOUS NON TEACHING POSTS Onlin Applications ar invitd for

More information

+ f. e f. Ch. 8 Inflation, Interest Rates & FX Rates. Purchasing Power Parity. Purchasing Power Parity

+ f. e f. Ch. 8 Inflation, Interest Rates & FX Rates. Purchasing Power Parity. Purchasing Power Parity Ch. 8 Inlation, Intrst Rats & FX Rats Topics Purchasing Powr Parity Intrnational Fishr Ect Purchasing Powr Parity Purchasing Powr Parity (PPP: Th purchasing powr o a consumr will b similar whn purchasing

More information

Lecture 37 (Schrödinger Equation) Physics Spring 2018 Douglas Fields

Lecture 37 (Schrödinger Equation) Physics Spring 2018 Douglas Fields Lctur 37 (Schrödingr Equation) Physics 6-01 Spring 018 Douglas Filds Rducd Mass OK, so th Bohr modl of th atom givs nrgy lvls: E n 1 k m n 4 But, this has on problm it was dvlopd assuming th acclration

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

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

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

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

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

Computing and Communications -- Network Coding

Computing and Communications -- Network Coding 89 90 98 00 Computing and Communications -- Ntwork Coding Dr. Zhiyong Chn Institut of Wirlss Communications Tchnology Shanghai Jiao Tong Univrsity China Lctur 5- Nov. 05 0 Classical Information Thory Sourc

More information

San José State University Aerospace Engineering AE 138 Vector-Based Dynamics for Aerospace Applications, Fall 2016

San José State University Aerospace Engineering AE 138 Vector-Based Dynamics for Aerospace Applications, Fall 2016 San José Stat Univrsity Arospac Enginring AE 138 Vctor-Basd Dynamics for Arospac Applications, Fall 2016 Instructor: Offic Location: Email: Offic Hours: Class Days/Tim: Classroom: Prof. J.M. Huntr E272F

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

Diffractive Dijet Production with Leading Proton in ep Collisions at HERA

Diffractive Dijet Production with Leading Proton in ep Collisions at HERA Diffractiv Dijt Production with Lading Proton in p Collisions at HERA JHEP [arxiv:150.01683] Radk Žlbčík Charls Univrsity Eric 015 Diffraction Th scattrd proton stays intact Exchang with vacuum quantum

More information

PoS(INPC2016)185. The MTV Experiment: from T Violation To Lorentz Violation

PoS(INPC2016)185. The MTV Experiment: from T Violation To Lorentz Violation Th MTV Exprimnt: from T Violation To Lorntz Violation 1, H. Baba 2, J.A. Bhr 3, F. Goto 4, S. Inaba 1, H. Kawamura 5, M. Kitaguchi 4, C.D.P Lvy 3, H. Masuda 1, Y. Nakaya 1, K. Ninomiya 1, J. Onishi 1,

More information

第 1 回バイオメトリクス研究会 ( 早稲田大学 ) THE INSTITUTE OF ELECTRONICS, INFORMATION AND COMMUNICATION ENGINEERS Proceedings of Biometrics Workshop Wol

第 1 回バイオメトリクス研究会 ( 早稲田大学 ) THE INSTITUTE OF ELECTRONICS, INFORMATION AND COMMUNICATION ENGINEERS Proceedings of Biometrics Workshop Wol TH INSTITUT OF LCTRONICS, INFORMATION AND COMMUNICATION NGINRS Procdings of Biomtrics Workshop Wolf Lamb,, 244-0817 292 153-8505 4-6-1 113-8656 7-3-1 -mail: {takao.murakami.nr,knta.takahashi.bw}@hitachi.com,

More information

A new idea to search for charged lepton flavor violation using a muonic atom

A new idea to search for charged lepton flavor violation using a muonic atom Journal of Physics: Confrnc Sris OPEN ACCESS A nw ida to sarch for chargd lpton flavor violation using a muonic atom To cit this articl: Jo Sato 2014 J. Phys.: Conf. Sr. 485 012036 Rlatd contnt - Sarch

More information

Homotopy perturbation technique

Homotopy perturbation technique Comput. Mthods Appl. Mch. Engrg. 178 (1999) 257±262 www.lsvir.com/locat/cma Homotopy prturbation tchniqu Ji-Huan H 1 Shanghai Univrsity, Shanghai Institut of Applid Mathmatics and Mchanics, Shanghai 272,

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

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

Proceedings of the 12th International Conference on Low Energy Antiproton Physics (LEAP216) Downloaded from journals.jps.jp by on 3/23/

Proceedings of the 12th International Conference on Low Energy Antiproton Physics (LEAP216) Downloaded from journals.jps.jp by on 3/23/ Proceedings of the 12th International Conference on Low Energy Antiproton Physics (LEAP216) Downloaded from journals.jps.jp by 128.141.46.242 on 3/23/18 Proc. 12th Int. Conf. Low Energy Antiproton Physics

More information

Atomic Physics. Final Mon. May 12, 12:25-2:25, Ingraham B10 Get prepared for the Final!

Atomic Physics. Final Mon. May 12, 12:25-2:25, Ingraham B10 Get prepared for the Final! # SCORES 50 40 30 0 10 MTE 3 Rsults P08 Exam 3 0 30 40 50 60 70 80 90 100 SCORE Avrag 79.75/100 std 1.30/100 A 19.9% AB 0.8% B 6.3% BC 17.4% C 13.1% D.1% F 0.4% Final Mon. Ma 1, 1:5-:5, Ingraam B10 Gt

More information

Two Products Manufacturer s Production Decisions with Carbon Constraint

Two Products Manufacturer s Production Decisions with Carbon Constraint Managmnt Scinc and Enginring Vol 7 No 3 pp 3-34 DOI:3968/jms9335X374 ISSN 93-34 [Print] ISSN 93-35X [Onlin] wwwcscanadant wwwcscanadaorg Two Products Manufacturr s Production Dcisions with Carbon Constraint

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

How can I control light? (and rule the world?)

How can I control light? (and rule the world?) How can I control light? (and rul th world?) "You know, I hav on simpl rqust. And that is to hav sharks with frickin' lasr bams attachd to thir hads! - Dr. Evil Phys 230, Day 35 Qustions? Spctra (colors

More information

That is, we start with a general matrix: And end with a simpler matrix:

That is, we start with a general matrix: And end with a simpler matrix: DIAGON ALIZATION OF THE STR ESS TEN SOR INTRO DUCTIO N By th us of Cauchy s thorm w ar abl to rduc th numbr of strss componnts in th strss tnsor to only nin valus. An additional simplification of th strss

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

REGISTER!!! The Farmer and the Seeds (a parable of scientific reasoning) Class Updates. The Farmer and the Seeds. The Farmer and the Seeds

REGISTER!!! The Farmer and the Seeds (a parable of scientific reasoning) Class Updates. The Farmer and the Seeds. The Farmer and the Seeds How dos light intract with mattr? And what dos (this say about) mattr? REGISTER!!! If Schrödingr s Cat walks into a forst, and no on is around to obsrv it, is h rally in th forst? sourc unknown Phys 1010

More information

Studies of Turbulence and Transport in Alcator C-Mod Ohmic Plasmas with Phase Contrast Imaging and Comparisons with GYRO*

Studies of Turbulence and Transport in Alcator C-Mod Ohmic Plasmas with Phase Contrast Imaging and Comparisons with GYRO* Studis of Turbulnc and Transport in Ohmic Plasmas with Phas Contrast Imaging and Comparisons with GYRO* L. Lin 1, M. Porkolab 1, E.M. Edlund 1, J.C. Rost 1, M. Grnwald 1, D.R. Mikklsn 2, N. Tsujii 1 1

More information

K

K Alicyclic Chmistry. Lctur 3 Th ovrall strain in cycloalkns can b masurd by th magnitud of th complxation constants with Ag +. Th gratr th angl strain th mor it is rlivd in th π-complx which rducs th π-charactr

More information

Higher order derivatives

Higher order derivatives Robrto s Nots on Diffrntial Calculus Chaptr 4: Basic diffrntiation ruls Sction 7 Highr ordr drivativs What you nd to know alrady: Basic diffrntiation ruls. What you can larn hr: How to rpat th procss of

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

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

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

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

Storage Ring Measurements of the DR Rate of Rotationally Cold H

Storage Ring Measurements of the DR Rate of Rotationally Cold H Storag Ring Masurmnts of th DR Rat of Rotationally Cold H 3 Bn McCall Dpartmnt of Chmistry Dpartmnt of Astronomy Univrsity of llinois at Urbana-Champaign A. J. Hunycutt, R. J. Saykally (Univrsity of California

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

Lecture 2: Discrete-Time Signals & Systems. Reza Mohammadkhani, Digital Signal Processing, 2015 University of Kurdistan eng.uok.ac.

Lecture 2: Discrete-Time Signals & Systems. Reza Mohammadkhani, Digital Signal Processing, 2015 University of Kurdistan eng.uok.ac. Lctur 2: Discrt-Tim Signals & Systms Rza Mohammadkhani, Digital Signal Procssing, 2015 Univrsity of Kurdistan ng.uok.ac.ir/mohammadkhani 1 Signal Dfinition and Exampls 2 Signal: any physical quantity that

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

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

Differential Equations

Differential Equations Prfac Hr ar m onlin nots for m diffrntial quations cours that I tach hr at Lamar Univrsit. Dspit th fact that ths ar m class nots, th should b accssibl to anon wanting to larn how to solv diffrntial quations

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

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

MA 262, Spring 2018, Final exam Version 01 (Green)

MA 262, Spring 2018, Final exam Version 01 (Green) MA 262, Spring 218, Final xam Vrsion 1 (Grn) INSTRUCTIONS 1. Switch off your phon upon ntring th xam room. 2. Do not opn th xam booklt until you ar instructd to do so. 3. Bfor you opn th booklt, fill in

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