exclusive vector meson electroproduction at 12 gev
DESCRIPTION
Exclusive Vector Meson Electroproduction at 12 GeV. Paul Stoler Rensselaer Polytechnic Institute. What do we want to do at 12 GeV ? Approach to the small–size regime Learn about short–range nucleon and meson structure. Is 12 GeV the right energy?. - PowerPoint PPT PresentationTRANSCRIPT
Exclusive Vector Meson Electroproduction
at 12 GeV
Paul Stoler Rensselaer Polytechnic Institute
What do we want to do at 12 GeV?
(a) Approach to the small–size regime
(b) Learn about short–range nucleon and meson structure
Is 12 GeV the right energy?
high xB
valence quarks
low xB
sea quarks
From valence quarks to sea quarks and gluons
From gluon dressed to bare quarks.
(Craig Roberts et al.)
M N =M Ng +M Nq
M μ+,μ+Ni ∝ ea
a∑ Ca dx∫ Hμλ,μλ
i
λ∑ H i(x,ξ,t)
Hμλ ,μλi = dτ db ∫ αS Ψ̂V Fμλ,μλ
i e−S⎡⎣
⎤⎦
GPD’s
Hi =H ,E,H , %E HT ,ET ,HT ,%ET
γL* p → pρ 0
VGGGK
VGG+D
JML
Example of world data
GPD: n=3
γL* p → p φ
s
Example of CLAS 6 GeV date
s
Q2=1-3 GeV2, W=2-3
Jlab 6 GeVJlab 12 GeV
f - ds/dt’
γL* p → p ρ 0 γL
* p → p φ
u =(pi − pp )2 smallt =(pi − pp )2 large
J.P Landsberg, B. Pire, L. Szymanowski
Elastic scattering from proton core in a dressed nucleon.
Backward angle (high -t) electroproduction
Kinematic covered. W ~ 2 4.5 GeV➞
Q2 ~ 1 13 GeV➞ 2
−t’ ~ 0 to > 15 GeV2
Explore the transition from soft physics to the dominance of QCD quarks and gluons
CLAS12 Proposal
γ * + p → p + ρ° γ * + p → p + φ
γ * + p → n + ρ + γ * + p → p + ω
Exclusive Vector Meson Electroproduction with CLAS12
γ * p → φ p φ → K +K − detect epK + and/or epK +K −
φ→ KS0KL
0 KS0 → π +π − detect pπ +π −
γ * p → ρ 0 p ρ 0 → π +π − detect ′e pπ + and ′e π −π +
γ * p → ρ +n ρ + → π + π 0 → π +γ γ
γ * p → ω p ω → π +π −π 0 detect epπ +π −
Meson Decay Modes
Goals of the experiment
dσdt*dφ
=σT +εσL +εσTT cos(2φ* )+ 2ε(ε +1)σLT cosφ
* +h 2ε(ε −1)σL ′Tsinφ*
Goal-obtain information about all 5 structure functions available with polarized beam and unpolarized target
σT + εσ L( ) σ TT σ LT obtained from cos(f) and cos(2f) with h = 0
σT σ L –angular distribution of meson decay products.
Beam spin cross section differences
Δσ = dσuru
dt*dφ −
dσs uu
dt*dφ
σL ′T beam spin asymmetries
Structure Functions:
W (cosθHS) = 38
1−r0004
( ) + 3r0004 −1( )cos
2θHS⎡⎣
⎤⎦
R = σ L
σ L
= 1ε
r0004
1−r0004.
L/T separation
H
Helicity Frame
Simulations
Extensive simulations were carried out for all 4 mesons channels.
In general, statistics are quite good due to large acceptance, high luminosity and efficient PID
Compared with previously successful CLAS 6 GeV r0 r+ f and w experiments, statistics will increase by factor ~102
r0 channel simulations
γ * + p → ρ 0 + p ρ 0 → π + + π −
MM ′e pπ +( ) ⇒ π − IM π +π −
( ) ⇒ ρ 0
MM ′e π +π +( )⇒ p IM π +π +
( )⇒ ρ 0 ← large - t
0.1 xB
Q2
1 GeV2
13 GeV2
0.8
0
ds/d
t ( m
b/G
eV2 )
-t (GeV2)10 20
f simulations
γ * p → φp φ→ K + K −
1. MM ′e pK +( ) ⇒ K −
2.MM ′e K + K −( ) ⇒ p
3.Detect ′e K + K − p( )
⎧
⎨
⎪⎪
⎩
⎪⎪
⎫
⎬
⎪⎪
⎭
⎪⎪
IM K + K −( ) ⇒ φ
γ * p → φp φ→ KS0 KL
0
KS0 → π +π − MM pKS
0( ) → KL
0
Acceptance - e p K+
6 backup slides follow
Statistics•Average acceptance ≃ 10 to 50%. (depending on kinematics)
SystematicsBackground subtraction~ few % (sharp state)Acceptance ~5-10 %
Net: s ~7-12%
Errors on cross sections
Statistics•⇒Statistics: very high•Average acceptance ≃ 10 to 30%. (depending on kinematics)
Systematics Background subtraction: systematics 10%
Net: s ~15%