my involvement in the spin and parity programs at jlab ... · my involvement in the spin and parity...
TRANSCRIPT
My involvement in the Spin and Parity Programs at JLab, and beyond
Introduction — nucleon structure and electron scatteringThree types of Deep Inelastic Scattering (DIS) and some completed/future experiments at JLabResearch opportunitiesWhat does it take to achieve a Ph.D.?
Xiaochao ZhengOctober 1, 2010
d2
d dE '= Mott [F1Q
2 ,F 2 Q2 ,]
Exploring Nucleon Structure Using EM Probe
The cross section:
For pointlike target
k=E,k
k '=E',k '
q= , q
W 2=P ' 2
Q 2=−q 2
P=M,0
➔ Elastic – the nucleus appears as a rigid body
➔ Quasielastic – individual nucleon appears as a rigid body; nucleus = incoherent sum of nucleons
(quasi-) elastic — rigid body
Q2=2MT
Q2=2MN
Exploring Nucleon Structure Using EM Probe (cont.)
Nucleon form factors well measured
1W2GeV
1W2GeV
➔ Resonance region – quarks inside the nucleon react coherently
resonances — certain excitations of the internal structure
Exploring Nucleon Structure Using EM Probe (cont.)
For resonances, typically use phenomenological models to study N-N* transition amplitudes and polarizations.
Deep Inelastic Scattering (DIS):Quarks start to react incoherentlyStart to see constituents of the nucleon
Exploring Nucleon Structure Using EM Probe (cont.)
For DIS, perturbation theory starts to work, can test perturbative QCD.
Current Knowledge of Nucleon Unpolarized Structure (after 40 years of study)
● Phys. Rev. D 66, 010001 (2002)
d2
d dE '= Mott [F1Q
2 ,F 2 Q2 ,]
After 39 years of DIS experiments, the unpolarized structure of the nucleon is reasonably well understood (for moderate xBj region).
F1x =12 ei
2[qi x ] in the QuarkParton Model and the
infinite momentum frame (IMF)
(P ∞)
Current Knowledge of Nucleon Unpolarized Structure (after 40 years of study)
Polarized DIS (1980~present)
Scattering cross section is spindependent (imaging throwing two small magnets together)
Longitudinal
Transverse
d 2
d dE '−
d2
d dE '∝ point−like [ ' g1x , Q2
' g2 x , Q2]
d 2
d dE '−
d2
d dE '∝ point−like [ ' ' g1x ,Q2 ' ' g2 x , Q2]
N SN SS N N S vs.
Polarized Structure Function and the Nucleon Spin Structure
in QPM and the infinite momentum frame:
g1x = 12 ei
2[q i
x −qi
x] = 1
2 ei
2[ qi x ]
The integral of g1(x) over x describes how much of the nucleon's spin is carried by quarks' spin
But do we really understand strong interaction?
To do this, we must understand the nucleon structure from the theory of strong interaction (QCD).
SQ2
=4
11−2 n f /3ln Q2/ 2
Because strong interaction is highly non-perturbative, it is very difficult to predict the value of structure functions from QCD.
Data vs. Theory – How do we test QCD?For most cases, QCD cannot predict the value of structure functions because of their nonperturbative nature.However, the large x region provides a handful of exceptions:
F2p/F2
n and d/uA1
p, A1n , or u/u and d/d
A1 =1/2− 3/2
1/2 3/2
2 =Q2
2=
4 M2 x2
Q2
Virtual photon asymmetry:
A1 =g1−
2 g2
F1
≈g1
F1.at large Q2
At large x, valence quarks dominate, a relatively clean/easy region to
study/model the nucleon
The 6 GeV Hall A Measurement (21 PAC days, 2001)
HHC not valid,quark OAM?
(1) SU(6)(2)(2) CQMCQM(3) LSS(BBS)(4) BBS(5) Bag
Model(6) Duality(7) LSS 2001(8) Statistical
Model(9) Chiral
Soliton
(1)CQM (2)LSS(BBS):pQCD+HHC(3)Statistical Model (4)LSS 2001
(Deutron data not shown: E143, E155, SMC)
X. Zheng et al., Phys. Rev. Lett. 92, 012004 (2004); Phys. Rev. C 70, 065207 (2004)
(1)
(9)
(8)
(7)
(2)
(6)
(4)(3)(6)(5) (1)
(1)
(2)
(2)
(3)
(3)
(4)
(4)
Polarized DIS and Nucleon Spin StructureH. Avakian, S. Brodsky, A. Deur, F. Yuan,
Phys. Rev. Lett.99:082001(2007)Figure credit: A. Deur
Future Experiments after the 11 GeV JLab Upgrade
Fully approved in August 2010, rated A.There are in fact two experiments, one in Hall A, one in Hall C.
Expected ResultsCombined results from Hall C (neutron) and B (proton) 11 GeV experiments
EM observables — σ, A... (polarized beam + polarized target)
hadron structure, strong interaction and its standard model (QCD);
Weak observables — parity violating asymmetries (APV)(polarized beam + unpolarized target)
study hadron structure elastic scattering: strange form factors A4, G0, HAPPEX, SAMPLEDIS: nonperturbative effects, CSV etc... PVDIS
test the standard model of electroweak interaction Qweak
Parity Violating DIS
ALR≡
r−
l
r
l≈
Q2
M Z2≈120 ppm
at Q2=1GeV /c2
N SS N vs.
From Ad can extract C1,2q and sin2W.
For a deuterium target
In the SM, tree level
Ad = 540 ppmQ2 2C1u [1RC x ]−C1d [1RS x ]Y 2 C2u−C2dRV x
5RS x4RC x
C1d=gAe gV
d=
12−
23
sin2W
C1u=gAe gV
u=−
12
43
sin2W
C2d=gVe gA
d=
12−2 sin2
W
C2u=gVe gA
u=−
122sin2
W
Test of EW Standard Model Using PVDIS
1970's, result from SLAC E122 consistent with sin2W=1/4, confirmed the Standard Model prediction;Development in experimental technique allows to search for new physics
JLab 6 GeV Experiment 08011
E08011 ran OctDec 2009
Used 105A, 6 GeV, 85% polarized beam on a 20cm LD2 target;
Two Hall A High Resolution Spectrometers detect scattered electrons;
Customerized DAQ built by UVa group
Measure Ad at Q2=1.10 and 1.90 GeV2 to about 34% (stat.);
Cospokesperson & contact: X. ZhengCospokesperson: P.E. Reimer, R. Michaels
Students: Diancheng Wang, Xiaoyan Deng, Huaibo Ding, Kai Panpostdoc: Ramesh Subedi
●ANL, Calstate, FIU, Jlab, Kentucky, U. of Ljubljana (Slovenia), MIT, UMD, UMass, UNH, Universidad Nacional Autonoma de Mexico, Rutgers, Smith C., Syracuse, UVa, W&M
Current Knowledge on C1,2q
MIT/ Bates
SLAC/Prescott
R. Young (PVES)
R. Young (combined)
PDG best fit
Cs APV
PDG best fit
SAMPLE
SLAC/ Prescott
all are 1 limit
Best: (2C2uC2d) = 0.24
C2u
+C2d
1.25
1.5
1.75
1.0
0.75
0.5
0.25
0
0.25
-0.5
-0.75
C2uC2d
- 0.25 0.50.250- 0.5
0.10
0.125
0.15
0.175
C1uC1d
- 0.4- 0.6- 0.8
C1u
+C1d
Tl APV
Qweak (expected)
MIT/ Bates
SLAC/Prescott
R. Young (PVES)
R. Young (combined)
PDG best fit
Cs APV
SAMPLE
SLAC/ Prescott
all are 1 limit
Best: (2C2uC2d) = 0.24
C2u
+C2d
1.25
1.5
1.75
1.0
0.75
0.5
0.25
0
0.25
-0.5
-0.75
C2uC2d
- 0.25 0.50.250- 0.5
0.10
0.125
0.15
0.175
C1uC1d
- 0.4- 0.6- 0.8
C1u
+C1d
Tl APV
The 6 GeV E08011
PDG best fit
Expected: JLab 6 GeV PVDIS E08011 (assuming small hadronic effects and a 4% stat error on Ad)
Qweak (expected)
Hall A large acceptance “solenoid” device: PR09012
Measure Ad to 1% for a wide range of (x,Q2,y), clean separation of New Physics (via C2q and sin2W), HT and CSV possible;
Extract d/u at large x from PVDIS on a proton target, free of nuclear effects;Other hadronic physics study possible: A1
n at large x, Semiinclusive DIS.
Two approaches:
Hall C “baseline” SHMS+HMS: PR1207102 (P.E. Reimer, XC. Z, K. Paschke,
1% on Ad, extraction of C2q, sin2W (if highertwists and CSV are negligible);
PVDIS Program at JLab 12 GeV
(conditionally approved)
Hall A large acceptance “solenoid” device: PR10007 fully approved
Measure Ad to 1% for a wide range of (x,Q2,y), clean separation of New Physics (via C2q and sin2W), HT and CSV possible;
Extract d/u at large x from PVDIS on a proton target, free of nuclear effects;Other hadronic physics study possible: A1
n at large x, Semiinclusive DIS.
Two approaches:
Hall C “baseline” SHMS+HMS: PR1207102 (P.E. Reimer, XC. Z, K. Paschke)
1% on Ad, extraction of C2q, sin2W (if highertwist and CSV are negligible);
PVDIS Program at JLab 11 GeV
Projected PVDIS Measurement with SOLID@11 GeV
figure from K. Kumar, Seattle 2009 EIC Workshop EW talks
Projected PVDIS Measurement with SOLID@11 GeV
figure from K. Kumar, Seattle 2009 EIC Workshop EW talks
Ongoing 6 GeV Physics Program
Measurement of neutron asymmetry A1n in the valence quark
region at JLab 12 GeV
Flagship experimentMay be one of the first experiments to run (~2014?)
SOLID program (2015 or later)
PVDIS at 11 GeV — ultimate goal: clean separation of New Physics and CSV
A1n, d/u measurements, SIDIS, etc.
Research Opportunities
Frontiers of Nuclear Science“Building on the foundation of the recent past, nuclear science is focused on three broad but highly related research frontiers: (1) QCD and its implications and predictions (1) QCD and its implications and predictions for the state of matter in the early universe, for the state of matter in the early universe, quark confinement, the role of gluons, and quark confinement, the role of gluons, and the structure of the proton and neutron;the structure of the proton and neutron; (2) the structure of atomic nuclei and nuclear astrophysics, which addresses the origin of the elements, the structure and limits of nuclei, and the evolution of the cosmos; and (3) developing a New Standard Model of (3) developing a New Standard Model of nature's fundamental interactions, and nature's fundamental interactions, and understanding its implications for the origin understanding its implications for the origin of matter and the properties of neutrinos and of matter and the properties of neutrinos and nuclei.nuclei.”
A few words (slides) beyond the exact research topic
How a life towards your Ph.D. will feel like?
It's not like course work, there is no homework, no scheduled assignments, no TA/instructor to tell you what to do everyday.There is no midterm or final
It's not like course work, there is no homework, no scheduled assignments, no TA/instructor to tell you what to do everyday.There is no midterm or final
If you want to solve a problem, you need to go out and ask! Most of time, you have to define the problem yourself.If you want to know if what you are doing is leading towards your Ph.D., you need to sit down and think!There is no “after-midterm” or “after-final” vacation time to look forward to. You are facing years of hard work.Could be more complicated if you are also bothered by other questions, such as ... ...
How a life towards your Ph.D. will feel like?How a life towards your Ph.D. will feel like?
It's not like course work, there is no homework, no scheduled assignments, no TA/instructor to tell you what to do everyday.There is no midterm or final
If you want to solve a problem, you need to go out and ask! Most of time, you have to define the problem yourself.If you want to know if what you are doing is leading towards your Ph.D., you need to sit down and think!There is no “after-midterm” or “after-final” vacation time to look forward to. You are facing years of hard work.Could be more complicated if you are also bothered by other questions, such as ... ...
No wonder most of people I know said the few years leading to their Ph.D are the “darkest time” of their life.
How a life towards your Ph.D. will feel like?How a life towards your Ph.D. will feel like?
The Basics
A Doctor of Philosophy degree, abbreviated Ph.D., is the highest academic degree anyone can earn. Because earning a Ph.D. requires extended study and intense intellectual effort, less than one percent of the population attains the degree. Society shows respect for a person who holds a Ph.D. by addressing them with the title ``Doctor''.
To earn a Ph.D., one must accomplish two things. First, one must master a specific subject completely. Second, one must extend the body of knowledge about that subject.
A Few Questions To Ask
1. Do you want a research career?
even if you are planning a industrial/financial position, keep in mind what the people there are looking for?
2. Do you want an academic position?
3. Do you have what it takes?
It is difficult for an individual to assess their own capabilities. The following guidelines and questions may be of help.
Intelligence;
Time;
Creativity;
Intense curiosity;
Adaptability;
Problem-solving skills;
Self-Motivation;
Competitiveness;
Maturity.
A few warnings:Students sometimes enroll in a Ph.D. program for the wrong reasons. After a while, such students find that the requirements overwhelm them. Before starting one should realize that a Ph.D. is not:
Prestigious in itselfA guarantee of respect for all your opinions
A goal in itselfA job guarantee
A practical way to impress your family or friendsSomething you can “try” to find out how smart you are
The only research topic you will ever pursueEasier than entering the work force
Better than the alternativesA way to make more money
The good news:
Despite all our warnings, we are proud that we earned Ph.D. degrees and proud of our research accomplishments. If you have the capability and interest, a research career can bring rewards unequaled in any other profession. You will meet and work with some of the brightest people on the planet. You will reach for ideas beyond your grasp, and in so doing extend your intellectual capabilities. You will solve problems that have not been solved before. You will explore concepts that have not been explored. Working on research will become sheer joy (without saying it loud). You may enjoy your work so much that you look forward to every day ahead of you, and you may not want to retire, ever.