The x<3 experiment. Patricia Solvignon UNH/JLab
|
|
|
- Leona Norman
- 5 years ago
- Views:
Transcription
1 The <3 eperiment Patricia Slvignn UNH/JLab Net generatin nuclear physics with JLab1 and EIC FIU February 10-13, 016
2 E Spkespeple: P. Slvignn (JLab/UNH), J. Arringtn (ANL), D. Day (UVa), D. Higinbtham (JLab) Main physics gals Isspin-dependence Imprved precisin: etract R(T=1/T=0) t 3.8% FSI much smaller (inclusive) and epected t cancel in rati 3N SRCs structure (mmentum-sharing and isspin) Imprved A-dependence in light and heavy nuclei Average f 3 H, 3 He --> A=3 isscalar nucleus Determine isspin dependence --> imprved crrectin fr N>Z nuclei, etraplatin t nuclear matter Abslute crss sectins (and ratis) fr H, 3 H, 3 He: test calculatins f FSI fr simple, well-understd nuclei... Patricia Slvignn
3 : 1.469<Q <1.635 (GeV/c Preliminary Results f E Search fr three-nuclen shrt-range crrelatins in nuclei 3 1 : 1.57<Q <1.386 (GeV/c ) 6 4 Z. Ye, 1, P. Slvignn, 3, 4 P. Aguilera, 5 Z. Ahmed, 6 H. Albataineh, 7 K. Allada, 8 B. Andersn, 9 D. Anez, 10 K. Anil, 11 J. Annand, 1 W. Armstrng, 13 J. Arringtn, 14 T. Averett, 15 T. Badman, 4 H. Baghdasaryan, 1 X. Bai, 16 A σ 4 He / σ3 He rati 4 He/ 3 He Rati: E0019 Data (18 CLAS Data, Q =.7 GeV/c ) 5 : 1.458<Q <1.898 (GeV/c ) 3 : 1.469<Q <1.635 (GeV/c ) 1 : 1.57<Q <1.386 (GeV/c ) T be submitted t PRL (σ1 C /1)/(σ3 He /3) σ 1 C / σ3 He Rati: rati 1 C/ 3 He E0019 Data (18, Q =.7 GeV/c ) 8 :.138<Q <.313 (GeV/c ) 5 : 1.458<Q <1.898 (GeV/c ) 3 : 1.469<Q <1.635 (GeV/c ) 1 : 1.57<Q <1.386 (GeV/c ) 0 15 σ 1 C / σ3 He Rati: FIG.. (Clr nline) The 4 He/ 3 He (tp) and 1 C/ 3 He (bttm) crss sectin ratis at 1, 3, and 5 degrees, alng with results frm CLAS [1] and Hall C (E0-019) [14] measurements. The slid lines crrespnd t a simple crss sectin mdel based n parameterized mmentum distributins. E0019 Data (18, Q =.7 GeV/c ) E :.138<Q <.313 (GeV/c will ) perfrm the average f 3 H, 3 He --> A=3 isscalar nucleus 5 : 1.458<Q <1.898 (GeV/c ) 3 : 1.469<Q <1.635 (GeV/c ) 1 : 1.57<Q <1.386 (GeV/c ) N hint f secnd plateau? Patricia Slvignn 3
4 Onset f Scaling fr <<3 N hint f secnd plateau? Maybe ur Q is t lw?! Patricia Slvignn 4
5 Accessing the cmpnents f Taking deuterium data will allw: the spectral functin 1. Direct measures f the spectral functin in the isspin 1 channel:. Direct measures f the difference f the spectral functin in I=1 and I=0 channels: These results will prvide, in an independent way, a test f the bservatin f small values f (e,e pp)/(e,e pn) ratis. Patricia Slvignn 5
6 Isspin study frm 3 He/ 3 H rati Isspin independent: Simple mean field estimates fr N-SRC n-p (T=0) dminance: σ /3 3 He σ /3 = (σ +1σ ) /3 p n 3 (1σ H p + σ n ) /3 σ p 3σ $ $ $ n 1.40 σ /3 3 H (pn +1nn) /3 = /3 (pn +1pp) /3 =1.0 σ 3 He Inclusive crss sectin calculatin frm M. Sargsian using AV18/UIX dσ/dωde, μb/gev/sr He 3H rati Patricia Slvignn 6
7 3N-cnfiguratin (a) 1 3 etremely large mmentum p 3 = p 1 +p (b) 1 3 Star-cnfiguratin p 1 = p = p 3 (a) yields R( 3 He/ 3 H) 3.0 if nuclen #3 is always the dubly-ccurring nuclen (a) yields R( 3 He/ 3 H) 0.3 if nuclen #3 is always the singly-ccurring nuclen (a) yields R( 3 He/ 3 H) 1.4 if cnfiguratin is isspin-independent, as des (b) R 1.4 implies isspin dependence AND nn-symmetric mmentum sharing Patricia Slvignn 7
8 E : kinematics Beam current: 5 μa, unplarized, Raster interlck Beam energy: 17.5 Days 4.4 GeV [main prductin] QE N 3N Left HRS Right HRS ("parasitic") Left & Right HRS Left HRS running (380 hurs) Q (GeV ) } 6. E =. GeV Patricia Slvignn 8
9 E : kinematics Beam current: 5 μa, unplarized, Raster interlck Beam energy: 17.5 Days 4.4 GeV [main prductin] 1.5 days. GeV [checkut+qe] QE N 3N Left HRS Right HRS ("parasitic") Left & Right HRS Left HRS running (380 hurs) Left+Right HRS running (abut 1 day) Q (GeV ) } 6. E =. GeV Patricia Slvignn 9
10 E : kinematics Beam current: 5 μa, unplarized, Raster interlck Beam energy: 17.5 Days 4.4 GeV [main prductin] 1.5 days. GeV [checkut+qe] QE N 3N Right HRS running ( parasitic ) Eisting 3 H QE data limited Q 0.9 GeV Left HRS Right HRS ("parasitic") Left & Right HRS Left HRS running (380 hurs) Left+Right HRS running (abut 1 day) Q (GeV ) } 6. E =. GeV Patricia Slvignn 10
11 E : prjected results Isspin study f SRC Etractin f GM n % scale uncertainty nt shwn T=0 dminance isspin independence 17.0 (1.48<Q <1.58) 19.0 (1.75<Q <1.88) He/ 3 H H/ 3 He GeV, GeV, GeV, GeV, GeV, 8.5. GeV,. GeV, 6.. GeV, At >, 3 He/ 3 H 1.4 implies isspin dependence AND nn-symmetric mmentum sharing In PWIA, 3 He/ 3 H with 1.5% uncertainty crrespnds t 3% n G M n Patricia Slvignn 11
12 E : Neutrn Magnetic FF Wrld 3 H QE data: Q 0.9GeV This eperiment: 0.6, 0.8, 1.0, 1.4, 1.7,.4,.7 and 3.0 GeV In PWIA, 3 He/ 3 H with 1.5% uncertainty crrespnds t 3% n GM n Limited t Q 1 GeV, where QE peak has minimal inelastic cntributin This is the regin with ~8% discrepancy between the Ankin, Kubn data and the CLAS rati and the Hall A plarized 3 He etractin. Nuclear effects epected t be small, largely cancel in rati Patricia Slvignn 1
13 The Target System Frm D. Meekins (JLab) Main Bdy and Entrance Windw: ASTM B09 AL 7075-T651 Valve assy: SST 316 and Ci f T (0.1 g) ~00 psi at 95K 5 cm lng ID f 1.7mm Vlume = 34 cc Aluminum CF seals Patricia Slvignn 13
14 Tritium Eperiments scheduled t run in February 017 Thank yu Patricia Slvignn 14
NPS Collaboration Meeting
NPS Cllabratin Meeting JLab, Newprt News, VA 21 January 2016 T. Hrn The Neutral-Particle Spectrmeter (NPS) NPS PbWO 4 The NPS is envisined as a facility in Hall C, utilizing the well-understd HMS and the
Short-range NN interactions: Experimental Past and Future
Short-range NN interactions: Experimental Past and Future 7th Workshop of the APS Topical Group on Hadronic Physics Nadia Fomin University of Tennessee February 1 st, 017 Independent Particle Shell Model
The Hall A Tritium Target Physics Program Overview
The Hall A Tritium Target Physics Program Overview Using A=3 Mirror Nuclei to Probe the Nucleon Structure 3H 3He Buddhini Waidyawansa (Argonne National Lab) Hall A & C Summer Collaboration Meeting June
arxiv:hep-ph/ v1 2 Jun 1995
WIS-95//May-PH The rati F n /F p frm the analysis f data using a new scaling variable S. A. Gurvitz arxiv:hep-ph/95063v1 Jun 1995 Department f Particle Physics, Weizmann Institute f Science, Rehvt 76100,
High Momentum Nucleons: where have we been and where are we going
High Momentum Nucleons: where have we been and where are we going Nadia Fomin High Energy Nuclear Physics with Spectator Tagging March 10 th, 015 High momentum nucleons where do they come from? Independent
Measurements with Tritium in Hall A. Patricia Solvignon
Measurements with Tritium in Hall A Patricia Solvignon Users Group Meeting JLab May 29-31, 2013 Outline Tritium target: description and status The MARATHON experiment The x>1 experiment New proposals:
Aircraft Performance - Drag
Aircraft Perfrmance - Drag Classificatin f Drag Ntes: Drag Frce and Drag Cefficient Drag is the enemy f flight and its cst. One f the primary functins f aerdynamicists and aircraft designers is t reduce
Upgrade for SRC/EMC Studies. Stephen Wood
Upgrade for SRC/EMC Studies Stephen Wood Outline Hall C 12 Hardware overview Standard Spectrometers Additional detectors Hall C SRC/EMC/Nuclear-effects physics program Deuteron EMC with LAD Standard Hall
Overview of the SRC/EMC experiments
Overview of the SRC/EMC experiments Donal Day Hall C Winter Meeting 2016 E12-06-105 E12-10-008 PAC Report E12-06-105 (x > 1): Inclusive Scattering from Nuclei at x > 1 in the Quasi-elastic and Deep-inelastic
0νββ decay NMEs in large shell model space with the generator-coordinate method
νββ decay NMEs in large shell mdel space with the generatr-crdinate methd Changfeng Jia Department f Physics Central Michigan University June st @ INT 7-a Generatr Crdinate Methd (). Intrductin... Crrelatins
Latest results from the XENON Program
Rencntres de Mrind 2013 Latest results frm the XENON Prgram Maxime Le Callch, On behalf f the XENON Cllabratin Very High Energy Phenmena in the Universe Rencntres de Mrind 2013, VHEPU The XENON cllabratin:
Tritium Runplan 2017/18. Florian Hauenstein Old Dominion University Hall A collaboration meeting
Tritium Runplan 2017/18 Florian Hauenstein Old Dominion University Hall A collaboration meeting 18.01.17 Tritium Experiments E12-010-103 (MARATHON) Deep Inelastic Scattering to measure F 2n to F 2p ratio,
E : Ratio of the electric form factor in the mirror nuclei 3 He and 3 H (The 3 He 3 H Charge Radius Difference)
E12 14 009: Ratio of the electric form factor in the mirror nuclei 3 He and 3 H (The 3 He 3 H Charge Radius Difference) Luke Myers Hall A Winter Meeting December 9, 2014 Measuring r 2 Absolute methods
Hall C Summer Workshop
Classic Result from (e,e p) Measurements L. Lapikas, Nucl. Phys. A553 (1993) 297. Independent- Par+cle Shell- Model is based upon the assump+on that each nucleon moves independently in an average poten+al
2N and 3N Correlations in Few Body Systems at x > 1
2N and 3N Correlations in Few Body Systems at x > 1 Searching for 3N Correlations at x > 1 Donal Day University of Virginia Next generation nuclear physics with JLab12 and EIC 1 Outline Accepted Notions
Sodium D-line doublet. Lectures 5-6: Magnetic dipole moments. Orbital magnetic dipole moments. Orbital magnetic dipole moments
Lectures 5-6: Magnetic diple mments Sdium D-line dublet Orbital diple mments. Orbital precessin. Grtrian diagram fr dublet states f neutral sdium shwing permitted transitins, including Na D-line transitin
A zz in Quasielastic and Deep Inelastic Scattering at x>1
A zz in Quasielastic and Deep Inelastic Scattering at x> Fantasia on a theme of tensor polarizations Main Motivation: To use Tensor Polarizations to study short range distances in the deuteron & large
and 9 Springer-Verlag 1990
Z. Phys. C Particles and Fields 45, 551 555 (1990) Zeitschrift ~ i c ~ ~r Physik C and 9 Springer-Verlag 1990 Quasielastic nuclen and hypern prductin by neutrins and antineutrins with energies belw 30
Name: Period: Date: ATOMIC STRUCTURE NOTES ADVANCED CHEMISTRY
Name: Perid: Date: ATOMIC STRUCTURE NOTES ADVANCED CHEMISTRY Directins: This packet will serve as yur ntes fr this chapter. Fllw alng with the PwerPint presentatin and fill in the missing infrmatin. Imprtant
SRC Studies using Triple Coincidence A(e,e'pp) & A(e,e'np) reactions
SRC Studies using Triple Coincidence A(e,e'pp) & A(e,e'np) reactions A data-mining project using CLAS EG2 data Meytal Duer Tel-Aviv University July 12, 2018 NPWG meeting, JLab 1 SRC Pair Fraction [%] np-dominance
The basic concept for the NPS is a highly segmented EM calorimeter based on PbWO 4 preceded by a compact sweeping magnet
The Neutral-Particle Spectrmeter (NPS) The NPS is envisined as a facility in Hall C, utilizing the well-understd HMS and the SHMS infrastructure, t allw fr precisin (cincidence) crss sectin measurements
Plans to measure J/ψ photoproduction on the proton with CLAS12
Plans to measure J/ψ photoproduction on the proton with CLAS12 Pawel Nadel-Turonski Jefferson Lab Nuclear Photoproduction with GlueX, April 28-29, 2016, JLab Outline Introduction J/ψ on the proton in CLAS12
Nucleons in the Nuclear Environment
Nucleons in the Nuclear Environment "The next seven years..." John Arrington Argonne National Lab Topic: Study of nucleons (hadrons, quarks) in nuclei 1 - The EMC effect and related measurements 2 - Color
Phys102 Second Major-102 Zero Version Coordinator: Al-Shukri Thursday, May 05, 2011 Page: 1
Crdinatr: Al-Shukri Thursday, May 05, 2011 Page: 1 1. Particles A and B are electrically neutral and are separated by 5.0 μm. If 5.0 x 10 6 electrns are transferred frm particle A t particle B, the magnitude
Tensor Asymmetry A zz Jefferson Lab
Tensor Asymmetry A zz at Jefferson Lab Elena Long Tensor Spin Observables Workshop Jefferson Lab March 11 th, 2014 1 Today s Discussion Overview of the Physics Rates Calculation Experimental Set-up Potential
https://goo.gl/eaqvfo SUMMER REV: Half-Life DUE DATE: JULY 2 nd
NAME: DUE DATE: JULY 2 nd AP Chemistry SUMMER REV: Half-Life Why? Every radiistpe has a characteristic rate f decay measured by its half-life. Half-lives can be as shrt as a fractin f a secnd r as lng
High-energy ea scattering. Spectator nucleon tagging. Future facilities. Energy, luminosity, polarization. Physics objectives with light nuclei
High-energy nuclear physics with spectator tagging A. Deshpande, D. Higinbotham, Ch. Hyde, S. Kuhn, M. Sargsian, C. Weiss Topical Workshop, Old Dominion U., 9 11 March 015 High-energy ea scattering e e
Introductory Thoughts
Flw Similarity By using the Buckingham pi therem, we have reduced the number f independent variables frm five t tw If we wish t run a series f wind-tunnel tests fr a given bdy at a given angle f attack,
E up to Q 2 =13.5
G n M E12-09-019 up to Q 2 =13.5 (GeV/c) 2 by Ratio Method Form factors Combining n & p form factors GMn by ratio method Hall A GMn 1 In one-photon exchange approx. 2 j ien( p f ){ F1 ( Q ) 2 i q F2 (
AP Physics Kinematic Wrap Up
AP Physics Kinematic Wrap Up S what d yu need t knw abut this mtin in tw-dimensin stuff t get a gd scre n the ld AP Physics Test? First ff, here are the equatins that yu ll have t wrk with: v v at x x
Assume that the water in the nozzle is accelerated at a rate such that the frictional effect can be neglected.
1 HW #3: Cnservatin f Linear Mmentum, Cnservatin f Energy, Cnservatin f Angular Mmentum and Turbmachines, Bernulli s Equatin, Dimensinal Analysis, and Pipe Flws Prblem 1. Cnservatins f Mass and Linear
I. Analytical Potential and Field of a Uniform Rod. V E d. The definition of electric potential difference is
Length L>>a,b,c Phys 232 Lab 4 Ch 17 Electric Ptential Difference Materials: whitebards & pens, cmputers with VPythn, pwer supply & cables, multimeter, crkbard, thumbtacks, individual prbes and jined prbes,
Hadron Propagation and Color Transparency at 12 GeV
Hadron Propagation and Color Transparency at 12 GeV Dipangkar Dutta Mississippi State University Hall C Users Meeting Jan 21-22, 2016 Hall C meeting Jan 2016 D. Dutta Hadron propagation in nuclear medium
, which yields. where z1. and z2
The Gaussian r Nrmal PDF, Page 1 The Gaussian r Nrmal Prbability Density Functin Authr: Jhn M Cimbala, Penn State University Latest revisin: 11 September 13 The Gaussian r Nrmal Prbability Density Functin
Probing high-momentum neutrons and protons in asymmetric nuclei
Probing high-momentum neutrons and protons in asymmetric nuclei A data-mining project using JLAB CLAS data Meytal Duer Tel-Aviv University March 8, 017 Workshop on high-density nuclear matter, Weizmann
Nuclear Short Range Correlations
Nuclear Short Range Correlations Larry Weinstein Old Dominion University What are Correlations? Neutron stars EMC effect Hit the correlated pair Spectator correlated pairs np vs pp pairs Summary Elba Workshop,
Three charges, all with a charge of 10 C are situated as shown (each grid line is separated by 1 meter).
Three charges, all with a charge f 0 are situated as shwn (each grid line is separated by meter). ) What is the net wrk needed t assemble this charge distributin? a) +0.5 J b) +0.8 J c) 0 J d) -0.8 J e)
Deeply Virtual Compton Scattering on the Neutron with CLAS12 at 11 GeV
New Research Prpsal t Jeffersn Lab PAC 7 Deeply Virtual Cmptn Scattering n the Neutrn with CLAS1 at 11 GeV A. Fradi, B. Guegan, M. Guidal, S. Nicclai 1,, S. Pisan, D. Skhan Institut de Physique Nucléaire
Part One: Heat Changes and Thermochemistry. This aspect of Thermodynamics was dealt with in Chapter 6. (Review)
CHAPTER 18: THERMODYNAMICS AND EQUILIBRIUM Part One: Heat Changes and Thermchemistry This aspect f Thermdynamics was dealt with in Chapter 6. (Review) A. Statement f First Law. (Sectin 18.1) 1. U ttal
Measurement of Double-polarization Asymmetries in the Quasielastic region: Understanding Polarized 3He as an Effective Polarized Neutron Target
Measurement of Double-polarization Asymmetries in the Quasielastic region: Understanding Polarized 3He as an Effective Polarized Neutron Target Vincent Sulkosky University of Virginia 2015 JLab Users Group
The short-range structure of Nuclei
The short-range structure of Nuclei 1. Beyond the nuclear mean-field the role of Nucleon-Nucleon correlations 2. Review of recent 2-N knockout experiments a) (γ,nn) and (e,e'nn) experiments at Mainz and
Phy 213: General Physics III 6/14/2007 Chapter 28 Worksheet 1
Ph 13: General Phsics III 6/14/007 Chapter 8 Wrksheet 1 Magnetic Fields & Frce 1. A pint charge, q= 510 C and m=110-3 m kg, travels with a velcit f: v = 30 ˆ s i then enters a magnetic field: = 110 T ˆj.
Physics 212. Lecture 12. Today's Concept: Magnetic Force on moving charges. Physics 212 Lecture 12, Slide 1
Physics 1 Lecture 1 Tday's Cncept: Magnetic Frce n mving charges F qv Physics 1 Lecture 1, Slide 1 Music Wh is the Artist? A) The Meters ) The Neville rthers C) Trmbne Shrty D) Michael Franti E) Radiatrs
The CaFe Experiment: Isospin Dependence of Short-Range Nucleon Pairing in Nuclei Proposal to Jefferson Lab PAC 45
PR12-17-005 The CaFe Experiment: Isospin Dependence of Short-Range Nucleon Pairing in Nuclei Proposal to Jefferson Lab PAC 45 F. Hauenstein, C.E. Hyde, M. Khachatryan, H. Szumila-Vance, L.B. Weinstein
Experimental inputs for supernova dynamics
Experimental inputs fr supernva dynamics Francesca Gulminelli - LPC Caen Eric Bnnet Subatech Nantes Beyhan Bastin & Françis de Oliveira Ganil Adriana Raduta IFIN LIA COSMA Type II Supernvae Supernva explsin
Short Range Correlations and the EMC Effect
Short Range Correlations and the EMC Effect Or Hen, Tel-Aviv University Short Range Correlations The EMC Effect and nucleon modification The EMC SRC correlation Implications of the EMC-SRC correlation
The Electric Form Factor of the Neutron for SBS
The Electric Form Factor of the Neutron for SBS Seamus Riordan Stony Brook University seamus.riordan@stonybrook.edu July 1, 16 Seamus Riordan SBS 16 G n E 1/1 G E /G M at high Q - Spin Observables, Pol.
Photoproduction of Mesons off the Deuteron
Phtprductin f Mesns ff the Deutern B. Krusche and I. Jaegle Department f Physics, University f Basel, Ch-456 Basel, Switzerland fr the CBELSA/TAPS cllabratin Phtprductin f mesns ff the deutern has been
Q x = cos 1 30 = 53.1 South
Crdinatr: Dr. G. Khattak Thursday, August 0, 01 Page 1 Q1. A particle mves in ne dimensin such that its psitin x(t) as a functin f time t is given by x(t) =.0 + 7 t t, where t is in secnds and x(t) is
MECHANICS OF SOLIDS TORSION TUTORIAL 2 TORSION OF THIN WALLED SECTIONS AND THIN STRIPS
MECHANICS OF SOLIDS ORSION UORIAL ORSION OF HIN WALLED SECIONS AND HIN SRIPS Yu shuld judge yur prgress by cmpleting the self assessment exercises. On cmpletin f this tutrial yu shuld be able t d the fllwing.
Kinetics of Particles. Chapter 3
Kinetics f Particles Chapter 3 1 Kinetics f Particles It is the study f the relatins existing between the frces acting n bdy, the mass f the bdy, and the mtin f the bdy. It is the study f the relatin between
Checking the resolved resonance region in EXFOR database
Checking the reslved resnance regin in EXFOR database Gttfried Bertn Sciété de Calcul Mathématique (SCM) Oscar Cabells OECD/NEA Data Bank JEFF Meetings - Sessin JEFF Experiments Nvember 0-4, 017 Bulgne-Billancurt,
Phys101 Final Code: 1 Term: 132 Wednesday, May 21, 2014 Page: 1
Phys101 Final Cde: 1 Term: 1 Wednesday, May 1, 014 Page: 1 Q1. A car accelerates at.0 m/s alng a straight rad. It passes tw marks that are 0 m apart at times t = 4.0 s and t = 5.0 s. Find the car s velcity
arxiv: v1 [nucl-th] 25 Oct 2007
![arxiv: v1 [nucl-th] 25 Oct 2007](/thumbs/81/84732583.jpg "arxiv: v1 [nucl-th] 25 Oct 2007")
Clr transparency and shrt-range crrelatins in exclusive pin pht- and electrprductin frm nuclei W. Csyn, M.C. Martínez, and J. Ryckebusch Department f Subatmic and Radiatin Physics, Ghent University, Preftuinstraat
ALE 21. Gibbs Free Energy. At what temperature does the spontaneity of a reaction change?
Name Chem 163 Sectin: Team Number: ALE 21. Gibbs Free Energy (Reference: 20.3 Silberberg 5 th editin) At what temperature des the spntaneity f a reactin change? The Mdel: The Definitin f Free Energy S
Ecology 302 Lecture III. Exponential Growth (Gotelli, Chapter 1; Ricklefs, Chapter 11, pp )
Eclgy 302 Lecture III. Expnential Grwth (Gtelli, Chapter 1; Ricklefs, Chapter 11, pp. 222-227) Apcalypse nw. The Santa Ana Watershed Prject Authrity pulls n punches in prtraying its missin in apcalyptic
Electric Current and Resistance
Electric Current and Resistance Electric Current Electric current is the rate f flw f charge thrugh sme regin f space The SI unit f current is the ampere (A) 1 A = 1 C / s The symbl fr electric current
Chapter 23 Electromagnetic Waves Lecture 14
Chapter 23 Electrmagnetic Waves Lecture 14 23.1 The Discvery f Electrmagnetic Waves 23.2 Prperties f Electrmagnetic Waves 23.3 Electrmagnetic Waves Carry Energy and Mmentum 23.4 Types f Electrmagnetic
Short notes for Heat transfer
Furier s Law f Heat Cnductin Shrt ntes fr Heat transfer Q = Heat transfer in given directin. A = Crss-sectinal area perpendicular t heat flw directin. dt = Temperature difference between tw ends f a blck
Biplots in Practice MICHAEL GREENACRE. Professor of Statistics at the Pompeu Fabra University. Chapter 13 Offprint
Biplts in Practice MICHAEL GREENACRE Prfessr f Statistics at the Pmpeu Fabra University Chapter 13 Offprint CASE STUDY BIOMEDICINE Cmparing Cancer Types Accrding t Gene Epressin Arrays First published:
EXAM #1 PHYSICAL SCIENCE 103 FALLF, 2017
OBJECTIVES 1. Ft Pressure EXAM #1 PHYSICAL SCIENCE 103 FALLF, 2017 Determine the surface area f an bject. Given the weight and surface area, calculate the pressure. 2. Measuring Vlume & Mass Prvided a
Neutron Structure Function from BoNuS
Neutron Structure Function from BoNuS Stephen BültmannB Old Dominion University for the CLAS Collaboration The Structure of the Neutron at Large x The BoNuS Experiment in 005 First Results from the BoNuS
The Electromagnetic Form Factors of the Nucleon
The Electromagnetic Form Factors of the Nucleon Introduction Proton Form Factors Neutron Form Factors Summary September 28, 2006 R. Alarcon @ MIT Symposium e i k r Form factor in quantum mechanics Elastic
Probing Short Range Structure Through the Tensor Asymmetry A zz
Probing Short Range Structure Through the Tensor Asymmetry A zz (TA ) at x>1 zz Elena Long Joint Hall A/C Collaboration Meeting Jefferson Lab June 6 th, 2014 1 Today s Discussion Overview of Physics Motivation
L a) Calculate the maximum allowable midspan deflection (w o ) critical under which the beam will slide off its support.
ecture 6 Mderately arge Deflectin Thery f Beams Prblem 6-1: Part A: The department f Highways and Public Wrks f the state f Califrnia is in the prcess f imprving the design f bridge verpasses t meet earthquake
Probing Dense Nuclear Matter
Probing Dense Nuclear Matter through Inclusive Electron Scattering Donal Day University of Virginia Winter Retreat on Cold Dense Nuclear Matter FIU, Miami, February 15-17, 2007 Outline Introduction Inclusive
This is the author s final accepted version.
Zheng, X. et al. 6) Measurement f target and duble-spin asymmetries fr the e p eπ+n) reactin in the nuclen resnance regin at lw Q. Physical Review C, 944), 456. di:.3/physrevc.94.456) This is the authr
Phys. 344 Ch 7 Lecture 8 Fri., April. 10 th,
Phys. 344 Ch 7 Lecture 8 Fri., April. 0 th, 009 Fri. 4/0 8. Ising Mdel f Ferrmagnets HW30 66, 74 Mn. 4/3 Review Sat. 4/8 3pm Exam 3 HW Mnday: Review fr est 3. See n-line practice test lecture-prep is t
Activity 2 Dimensional Analysis
Activity 2 Dimensinal Analysis Gals! Develp cnversin factrs frm cmmn equalities.! Use cnversin factrs t cnvert between different units f measure.! Apply the cncept f dimensinal analysis t string tgether
AP Statistics Notes Unit Two: The Normal Distributions
AP Statistics Ntes Unit Tw: The Nrmal Distributins Syllabus Objectives: 1.5 The student will summarize distributins f data measuring the psitin using quartiles, percentiles, and standardized scres (z-scres).
Fabrication Thermal Test. Methodology for a Safe Cask Thermal Performance
ENSA (Grup SEPI) Fabricatin Thermal Test. Methdlgy fr a Safe Cask Thermal Perfrmance IAEA Internatinal Cnference n the Management f Spent Fuel frm Nuclear Pwer Reactrs An Integrated Apprach t the Back-End
M.Battaglieri Istituto Nazionale di Fisica Nucleare Genova - Italy. A Forward Photon Tagging Facility for CLAS12
A Forward Photon Tagging Facility for CLAS12 M.Battaglieri Istituto Nazionale di Fisica Nucleare Genova - Italy 1) From CEBAF at 6 GeV 2) From CEBAF at 6 GeV to CEBAF at 12 GeV add Hall D (and beam line)
The Neutron Structure Functions from BoNuS using CLAS
The Neutron Structure Functions from BoNuS using CLAS Keith Griffioen College of William & Mary Helmholtz-Institut Mainz (for the CLAS Collaboration) griff@physics.wm.edu Elba XII Workshop Electron-Nucleus
System size dependence of cluster properties from twoparticle angular correlations in Cu+Cu and Au+Au collisions at sqrt[s_{nn}]=200 GeV
![System size dependence of cluster properties from twoparticle angular correlations in Cu+Cu and Au+Au collisions at sqrt[s_{nn}]=200 GeV](/thumbs/74/70314063.jpg "System size dependence of cluster properties from twoparticle angular correlations in Cu+Cu and Au+Au collisions at sqrt[s_{nn}]=200 GeV")
System size dependence f cluster prperties frm twparticle angular crrelatins in Cu+Cu and Au+Au cllisins at sqrt[s_{nn}]= GeV The MIT Faculty has made this article penly available. Please share hw this
LED Quantity 3 SL-SPOT 3 UH
IP Pb Pb-free RHS CMPLIANT SL-SPTSeries //// high pwer LEDs lighting RDERING INFRMATIN Mdel SL-SPT UH SL-SPT UH SL-SPT UH SL-SPT UH SL-SPT UH FEATURES SPECIFICATIN CLR RANGE SURCE LIFE LED TYPE BEAM ANGLE
UGANDA ADVANCED CERTIFICATE OF EDUCATION INTERNAL MOCK 2016 PURE MATHEMATICS. 3 hours
P/ PURE MATHEMATICS PAPER JULY 0 HOURS UGANDA ADVANCED CERTIFICATE OF EDUCATION INTERNAL MOCK 0 PURE MATHEMATICS hurs INSTRUCTIONS TO CANDIDATES: Attempt ALL the EIGHT questins in sectin A and any FIVE
GAUSS' LAW E. A. surface
Prf. Dr. I. M. A. Nasser GAUSS' LAW 08.11.017 GAUSS' LAW Intrductin: The electric field f a given charge distributin can in principle be calculated using Culmb's law. The examples discussed in electric
Chapter 3: Cluster Analysis
Chapter 3: Cluster Analysis } 3.1 Basic Cncepts f Clustering 3.1.1 Cluster Analysis 3.1. Clustering Categries } 3. Partitining Methds 3..1 The principle 3.. K-Means Methd 3..3 K-Medids Methd 3..4 CLARA
37 Maxwell s Equations
37 Maxwell s quatins In this chapter, the plan is t summarize much f what we knw abut electricity and magnetism in a manner similar t the way in which James Clerk Maxwell summarized what was knwn abut
ECEN 4872/5827 Lecture Notes
ECEN 4872/5827 Lecture Ntes Lecture #5 Objectives fr lecture #5: 1. Analysis f precisin current reference 2. Appraches fr evaluating tlerances 3. Temperature Cefficients evaluatin technique 4. Fundamentals
Power Formulas for Various Energy Resources and Their Application
EP@BHS-TOPIC 2: Energy, UNIT2.2: Energy Cnversin and Efficiency Page 1 UNIT 2.2 Energy Cnversin and Efficiency Purpse Once energy resurces are effectively utilized, cnversin t ther frms f energy is necessary
NPS Collaboration Meeting
NPS Cllabratin Meeting Jeffersn Lab, Newprt News, VA 19 January 2017 Tanja Hrn Histry f NPS Meetings 10 Nvember 2012: Wrkshp n Opprtunities fr DVCS and ther physics with NPS (IPN-Orsay) 14 Nvember 2013:
UNIT 5: ATOMIC THEORY & THE PERIODIC TABLE CHEMISTRY 215, DUFFEY, CHAPTER 4 & SECTION 6.1
UNIT 5: ATOMIC THEORY & THE PERIODIC TABLE CHEMISTRY 215, DUFFEY, CHAPTER 4 & SECTION 6.1 BIG IDEAS (we will tuch n small parts f Chp.5 as well) 4.1 Early Ideas Abut Matter 4.2 Defining the Atm 4.3 Hw
Thermal behavior of Surface Mount Device (SMD) for Spicer case
Thermal behavir f Surface Munt Device (SMD) fr Spicer case Sandip Kumar Saha, Frederik Rgiers, Martine Baelmans sandipkumar.saha@mech.kuleuven.be 3 th Octber 20 Outline Thermal analysis f existing Spicer
Outline. 13./ 16. March Introduction. Photochemistry. Ozone chemistry Chapman model Catalytic cycles
Institute f Applied Physics University f Bern 13./ 16. March 2012 Outline The rle f Ozne hle: what causes what? Culd it be that ClO destrys O 3? Atmsphere as a chemical vessel The can be thught f as a
THE LIFE OF AN OBJECT IT SYSTEMS
THE LIFE OF AN OBJECT IT SYSTEMS Persns, bjects, r cncepts frm the real wrld, which we mdel as bjects in the IT system, have "lives". Actually, they have tw lives; the riginal in the real wrld has a life,
Homework-6 Due:
Applied Optics H-464/564 ECE 594 rtland State niversity A. La Rsa Hmewrk-6 Due: 05-26-2016 1. Quarter wave plates and half wave plates The figures belw shw a calcite crystal plate lcated at the crdinate
Deeply Virtual Compton Scattering off 4. He: New results and future perspectives
Deeply Virtual Compton Scattering off 4 He: New results and future perspectives M. Hattawy (On behalf of the CLAS collaboration) Next generation nuclear physics with JLab12 and EIC 10-13 February 2016,
I. INTRODUCTION JOURNAL OF CHEMICAL PHYSICS VOLUME 115, NUMBER 1 1 JULY 2001
JOURNAL OF CHEMICAL PHYSICS VOLUME 1, NUMBER 1 1 JULY 2001 Phtdissciating methyl vinyl ether t calibrate O ethylene prduct branching and t test prpensity rules fr prduct channel electrnic accessibility
PHYSICAL PROPERTIES OF SEA WATER - TEMPERATURE AND SALINITY
NAME PHYSICAL PROPERTIES OF SEA WATER - TEMPERATURE AND SALINITY I. Sea water temperatures The distributin f surface temperatures fr the majr ceans is shwn in Figure 1. The istherms (lines f equal temperature)
Internal Target Experiments at the MESA accelerator
Jhannes Gutenberg University, Mainz E-mail: merkel@kph.uni-mainz.de The Mainz Supercnducting Energy Recvery Linac (MESA) is a new acceleratr under cnstructin at the University f Mainz. MESA is designed
Multipole Vortices in an ECR Plasma
J. Plasma Fusin Res. SERIES, Vl. 4 (2001) 363-36'l Multiple Vrtices in an ECR Plasma OKAMOTO Atsushi*, ISHIHARA Tatsuz, NAGAOKA Kenichi, YOSHIMURA Shinjit and TANAKA Masayshi y.r Nagya University, Nagya
Inclusive Scattering from Nuclei at x>1 in the quasielastic and deeply inelastic regimes
PR12-06-105 Inclusive Scattering from Nuclei at x>1 in the quasielastic and deeply inelastic regimes J. Arrington (Spokesperson), D.F. Geesaman, K. Hafidi, R. Holt, D.H. Potterveld, P.E. Reimer, P. Solvignon
1 The limitations of Hartree Fock approximation
Chapter: Pst-Hartree Fck Methds - I The limitatins f Hartree Fck apprximatin The n electrn single determinant Hartree Fck wave functin is the variatinal best amng all pssible n electrn single determinants
Lecture 24: Flory-Huggins Theory
Lecture 24: 12.07.05 Flry-Huggins Thery Tday: LAST TIME...2 Lattice Mdels f Slutins...2 ENTROPY OF MIXING IN THE FLORY-HUGGINS MODEL...3 CONFIGURATIONS OF A SINGLE CHAIN...3 COUNTING CONFIGURATIONS FOR
Fundamental Concepts in Structural Plasticity
Lecture Fundamental Cncepts in Structural Plasticit Prblem -: Stress ield cnditin Cnsider the plane stress ield cnditin in the principal crdinate sstem, a) Calculate the maximum difference between the
Revised 2/07. Projectile Motion
LPC Phsics Reised /07 Prjectile Mtin Prjectile Mtin Purpse: T measure the dependence f the range f a prjectile n initial elcit height and firing angle. Als, t erif predictins made the b equatins gerning
RN52-STK2 Starter Kit
The RN52-STK2 Starter Kit has everything yu need t kick-start yur prject and is a great tl fr develpers: Prf f cncept prttypes as well as final cmmercial slutins. fr educatinal use: Natural sciences curses
Lecture 17: Free Energy of Multi-phase Solutions at Equilibrium
Lecture 17: 11.07.05 Free Energy f Multi-phase Slutins at Equilibrium Tday: LAST TIME...2 FREE ENERGY DIAGRAMS OF MULTI-PHASE SOLUTIONS 1...3 The cmmn tangent cnstructin and the lever rule...3 Practical
Inertial Mass of Charged Elementary Particles
David L. Bergan 1 Inertial Mass Inertial Mass f Charged Eleentary Particles David L. Bergan Cn Sense Science P.O. Bx 1013 Kennesaw, GA 30144-8013 Inertial ass and its prperty f entu are derived fr electrdynaic