baryon, heavy stable particle and strange meson production in ep-collisions
DESCRIPTION
XII International Conference on Hadron Spectroscopy Frascati , October 8 th -12 th , 2007. Baryon, Heavy Stable Particle and Strange Meson Production in ep-Collisions. Karin Daum – Wuppertal on behalf of the H1 and ZEUS collaborations. Outline: HERA & kinematics at HERA - PowerPoint PPT PresentationTRANSCRIPT
Karin Daum
Hadron07, Frascati, Oct., 11th 2007 1
Baryon, Heavy Stable Particle and Strange Meson Production in ep-Collisions
Karin Daum – Wuppertal
on behalf of theH1 and ZEUS
collaborations
XII International Conference on Hadron SpectroscopyFrascati, October 8th-12th, 2007
Outline:
• HERA & kinematics at HERA• Charged particle fragmentation function• Proton & Deuteron production• Strange particle production• Bose Einstein correlations• Conclusions
Karin Daum
Hadron07, Frascati, Oct., 11th 2007 2
The HERA accelerator
DESYHamburg-Germany Protons 920 GeV
Electrons 27.6 GeV
Results based on HERA-I data (~120 pb-1)- 3 times more to come
Karin Daum
Hadron07, Frascati, Oct., 11th 2007 3
HERA kinematics
E = 27.6 GeVe E = 920 (820)GeVp
ep-Kinematics:
√s = 300-318 GeV (energy c.m.)
Q2=-q2 (photon virtuality)
x=xBJ (fraction of proton momentum carried by the struck quark)
2 kinematic regimes :Q² 0 GeV² : Photoproduction (p)Q² > 1 GeV² : Electroproduction (DIS)
Dh(xp,)FFq
Fragmentation process:
xp (fraction of quark momentum carried by the hadron)
(energy scale of the quark)
h = PDF M.E. FF
Karin Daum
Hadron07, Frascati, Oct., 11th 2007 4
Models for ep scattering
Dh(xp,)FFq
h = PDF M.E. FF
How well do we understand
particle production?
PYTHIA for pLEPTO for DIS
LO ME+
Parton showers+
String fragmentation
Hadrons
ARIADNE for DIS
Color dipol model (CDM)
+String fragmentation
Karin Daum
Hadron07, Frascati, Oct., 11th 2007 5
Charged particle fragmentation function
Dh(xp,)FFq
±
K±
pdK0
s
h = PDF M.E. FF
H1
Inclusive fragmentation function:No distinction between ±, K±, p
Restricted to 100<Q²<10000 GeV²
Suppresses HO QCD effects not present in e+e-
(e.g. boson-gluon-fusion, ISR)
Use a reference frame closest tothe situation in e+e-: (Breit-Frame)
Energy scales: ep-collisions: =Q/2 e+e--annihilation: =s/2=Ebeam
Karin Daum
Hadron07, Frascati, Oct., 11th 2007 6
Charged particle fragmentation function
(ep)=Q/2, (e+e-)=s/2
Steep fall with Q at large xp
Depletion due to gluon radiation
Steep rise with Q at small xp
Population due to gluon splitting
Overall agreement with e+e-
except at large Q + small xp
Karin Daum
Hadron07, Frascati, Oct., 11th 2007 7
Charged particle fragmentation function
(ep)=Q/2
Comparison with NLO QCD predictions based on different fragmentation functions extracted from e+e- data
Quite different QCD predictions
Strong scaling violations in data
- All calculations fail to
describe them!
Karin Daum
Hadron07, Frascati, Oct., 11th 2007 8
Charged particle fragmentation function
ZEUS prel.
HERA-I + HERA-II: 0.5 fb-1
very good agreement with H1 but 10 times more statistics
Karin Daum
Hadron07, Frascati, Oct., 11th 2007 9
Production of protons and deuterons
Dh(xp,)FFq
±
K±
pd
K0s
h = PDF M.E. FF
ZEUS DIS: Q²>1 GeV²
Coalescence Model:
Baryons uncorrelated &inv. cross section same for p and n
Relates proton to deuteron production:
Coalescence parameter B2
(defines region of nucleon overlap): - Same for deuteron & anti-deuteron? - Process dependent?
Ed d3σd Ep d3σp
σtot dpd3 σtot dpp
3 =B2( )2
Karin Daum
Hadron07, Frascati, Oct., 11th 2007 10
σinv(d) 10-3·σinv (p)
σinv(d) ≠ σinv(d)
Production of protons and deuterons
Not expected fromcoalescence model
Karin Daum
Hadron07, Frascati, Oct., 11th 2007 11
Coalescence parameter B2
Coalescence parameter B2 depends on - primary process - centre-of-mass energy (less dependent in scattering off
protons)
B2(d)=(3.32±0.34 )10-2GeV2
B2(d)=(0.89±0.14 )10-2GeV2
+1.13-1.15
+0.19-0.20
Karin Daum
Hadron07, Frascati, Oct., 11th 2007 12
Strange particle production
Dh(xp,)FFq
±
K±
pdK0
s
h = PDF M.E. FF
ZEUS
Different regimes is ep-kinematic:
1. DIS: Q²>25 GeV² 2. DIS: 5<Q²<25 GeV²
3. p: Q²≈0, 2 jets, ET > 5 GeV acts as a quasi-real target may get internal structure (resolves into partons)
Distinction of direct from resolved via observable x calculated from the two jets:
x≈1 direct x«1 resolved
jet
Due to the s-quark mass ms
fragmentation into K0s, is
suppressed w.r.t. , p
Strangeness suppression factor s
Karin Daum
Hadron07, Frascati, Oct., 11th 2007 13
Strange particle production (DIS)
ARIADNE s=0.3 (CDM) overall reasonable – but shapes not so goodARIADNE s=0.22 systematically too small (from previous result)
LEPTO s=0.3 (PS) fails
5<Q²<25 GeV² Q²>25 GeV² 5<Q²<25 GeV² Q²>25 GeV²
pT pTpTpT
Karin Daum
Hadron07, Frascati, Oct., 11th 2007 14
Strange particle production p
PYTHIA reasonable in pt and PYTHIA off in shape of x (small x)
Resolved Intact (direct)
x x
pT pT
Karin Daum
Hadron07, Frascati, Oct., 11th 2007 15
Strange baryon-to-meson ratio
Model in DIS (ARIADNE) s=0.3 quite good (10%)
Model in p (PYTHIA) off in all distributions
p
Resolved Intact (direct)
x
pT pT
pT
DIS 5<Q²<25 GeV² Q²>25 GeV²
- especially @ small x
for x=1 same baryon-to-meson ratio as in DIS and e+e-
Karin Daum
Hadron07, Frascati, Oct., 11th 2007 16
Bose-Einstein correlations for K±K±, Ks
Ks 0 0
Identical bosons prefer to be produced close in phase space
Distance in phase space characterized by: r = source size of particle emission Q12 = distance in 4-momentum space
= -(p1-p2)2
Correlation function (static Gaussian source):R(Q12) = 1 + exp(-r2Q2
12)
experimentally:
R(Q12) =
Double ratio (reduced sensitivity to models)
R(Q12) =
P(Q12)
Pref(Q12)
P(Q12)data
Pmix(Q12)data
P(Q12)MCnoBEC
Pmix(Q12)MCnoBEC
Karin Daum
Hadron07, Frascati, Oct., 11th 2007 17
Bose-Einstein correlations for K±K±, Ks
Ks 0 0
Q12 Q12
R(Q
12)
=0.37±0.07+0.09-0.08 =0.70±0.19+0.47
-0.53
r=0.57±0.09+0.15-0.08 r=0.63±0.09+0.11
-0.08
Bose-Einstein correlations clearly established for K±K± pairsMarginal for Ks Ks pairs due background from f0(980) Ks Ks
Consistent results on source radius
0 0 0 0
Karin Daum
Hadron07, Frascati, Oct., 11th 2007 18
Bose-Einstein correlations
Consistent results on r: - ep (DIS) vs. e+e-
- K±K± vs. Ks Ks
- Kaons vs. charged particles
0 0
Karin Daum
Hadron07, Frascati, Oct., 11th 2007 19
Charged particle fragmentation function in ep collisions
shows significant scaling violations agrees reasonably with e+e- annihilation data NLO QCD calculations fail to describe scaling violations
Deuteron/Anti-deuteron production invariant d(d) cross section 1/1000 of p(p) coalescence parameter B2 (nucleon overlap) not universal
Strange particle production in ep collisions reasonably described in DIS with s=0.3 (LEP tuning) model fails to describe (Λ+Λ)/K0
s in resolved p consistent (Λ+Λ)/K0
s ratios in DIS, direct p and e+e-
a single parameter s not sufficient
Bose-Einstein correlations established for K±K± and K0
s K0s in DIS
consistent source radii for all processes & boson pairs
Conclusions
Karin Daum
Hadron07, Frascati, Oct., 11th 2007 20
Production of protons and deuterons
d/p in DIS (ZEUS)same as in p (H1)
p/p 1
d/d « 1
Karin Daum
Hadron07, Frascati, Oct., 11th 2007 21
Strange-to-light meson ratio
Data prefer strangeness suppression factor 0.3 in DIS and p
Range of T consistent with values obtained in e+e-
pT
DIS p
pT
N(Ks0)
Nch
T=
Karin Daum
Hadron07, Frascati, Oct., 11th 2007 22
Possible f0(980) contribution in Ks Ks 0 0
Simultaneous fit of MC with BEC and Flatté for f0(980)