current projects in the zeus collaboration
DESCRIPTION
Current Projects in the ZEUS collaboration. Mónica L. Vázquez Acosta. Max Planck Institute, Munich, 09.05.2005. HERA: ep Collider. H1: ep interactions. 920 GeV protons 27.5 GeV positrons. HERMES: polarised e + fixed target. HERA-B: p beam+fixed target. ZEUS: ep interactions. - PowerPoint PPT PresentationTRANSCRIPT
Current Projects in the ZEUS collaboration
Mónica L. Vázquez AcostaMónica L. Vázquez Acosta
Max Planck Institute, Munich, 09.05.2005
Current Projects in the ZEUS Collaboration, Mónica L. Vázquez Acosta (NIKHEF) Max-Planck Intitute MunichMax-Planck Intitute Munich, 09/05, 2005 - 2
HERA: ep ColliderHERA: ep ColliderHERA: ep ColliderHERA: ep Collider
H1: ep interactions
HERA-B: p beam+fixed target
HERMES: polarised e + fixed target
ZEUS: ep interactions
920 GeV protons27.5 GeV positrons
Current Projects in the ZEUS Collaboration, Mónica L. Vázquez Acosta (NIKHEF) Max-Planck Intitute MunichMax-Planck Intitute Munich, 09/05, 2005 - 3
Measures taken:• Additional collimators far upstream of IPs• Additional pump near IP
HERA-II no longer current-limited due to backgrounds
Background problems in HERA-II solved!Background problems in HERA-II solved!Background problems in HERA-II solved!Background problems in HERA-II solved!
Shutdown 2003
mea
sure
of
bac
kgr
oun
d
positron beam current2001: Luminosity upgrade & new silicon detector (MVD)2002-2003: background struggle
Current Projects in the ZEUS Collaboration, Mónica L. Vázquez Acosta (NIKHEF) Max-Planck Intitute MunichMax-Planck Intitute Munich, 09/05, 2005 - 4
ZEUS Gated Luminosity ZEUS Gated Luminosity ZEUS Gated Luminosity ZEUS Gated Luminosity
ZEUS gated: 43.7 pb-1
ZEUS gated: 48.36 pb-1
plot 09/03/05
Most ZEUS data is good MicroVertexDetector(MVD) data
Efficiency loss due to: Bad conditions in the initial tuning after luminosity is declared, which prevents to switch on the tracking chambers DAQ problems which now have been solved
Current Projects in the ZEUS Collaboration, Mónica L. Vázquez Acosta (NIKHEF) Max-Planck Intitute MunichMax-Planck Intitute Munich, 09/05, 2005 - 5
Radiation Monitor SystemRadiation Monitor SystemRadiation Monitor SystemRadiation Monitor System
zx-Querschnitt
4x2 PIN diodes 4x2 PIN diodes
-100 cm
110 cm
BMVDFMVD
z=160 cm -120 cm
-130 cm
4 RadFET
X
Z
4 RadFET8 RadFET
8 RadFET
Silicon PIN diodes Instantaneous dose rate from signal current Automatic dump system Bulk damage from offset leakage-current
Radiation Field Effect Transistors (RadFETs) Monitor surface damage from shift in threshold voltage
Current Projects in the ZEUS Collaboration, Mónica L. Vázquez Acosta (NIKHEF) Max-Planck Intitute MunichMax-Planck Intitute Munich, 09/05, 2005 - 6
Silicon pin diodes: fast radiation monitorSilicon pin diodes: fast radiation monitorSilicon pin diodes: fast radiation monitorSilicon pin diodes: fast radiation monitor
Threshold alarm: 1000 nA ~ 0.02 kRadThreshold dump: 4000 nA ~ 0.08 kRrad Forgiveness rate: 10 nA/s : allows short-term increase during injection and small constant background
25 kRad expected dose in the MVD by end of HERAII Front end chips tested up to 300 kRads
Maximumfill level
ffill Isignal = Idiode - Ileakage
fforgiveness
Actualfill level
bucket overflow beam dump
Dump signal to HERA
Current Projects in the ZEUS Collaboration, Mónica L. Vázquez Acosta (NIKHEF) Max-Planck Intitute MunichMax-Planck Intitute Munich, 09/05, 2005 - 7
Silicon Pin Diodes: leakage currentsSilicon Pin Diodes: leakage currentsSilicon Pin Diodes: leakage currentsSilicon Pin Diodes: leakage currents
Diodes on ring inside,closest to beamline
ShutdownProton beam-loss accident
Long term increase and annealing of leackage currentSubtract pedestal before each fill
Current Projects in the ZEUS Collaboration, Mónica L. Vázquez Acosta (NIKHEF) Max-Planck Intitute MunichMax-Planck Intitute Munich, 09/05, 2005 - 8
RADFETs: integrated doseRADFETs: integrated doseRADFETs: integrated doseRADFETs: integrated dose
Steady increase during beam operationStep like increase from single beam-loss accidentsValues expected higher in rear than in MVD (-0.3m) due to: backscatter in C5 collimator synchrotron radiation and off momentum positrons
Dos
e (k
Rad
)
MVD (-0.6m) REAR (-1.7m)C5 (-1m) FORWARD (1.3m)
Current Projects in the ZEUS Collaboration, Mónica L. Vázquez Acosta (NIKHEF) Max-Planck Intitute MunichMax-Planck Intitute Munich, 09/05, 2005 - 9
Radiation damage in the MVDRadiation damage in the MVDRadiation damage in the MVDRadiation damage in the MVD
No evidence of significant radiation damage
- Mean signal size stable
- Uncontrolled proton beam loss (4 Nov 03)
caused 10% drop in signal
- Big effort of HERA to reduce the risk
to <1 till end of running
- Noise shows a shallow slope
- Corresponds to 6 kRad in 500 days
on innermost cylinder
Detector in good shape
- Bad channels stable <2%
Current Projects in the ZEUS Collaboration, Mónica L. Vázquez Acosta (NIKHEF) Max-Planck Intitute MunichMax-Planck Intitute Munich, 09/05, 2005 - 10
The MVD is there ...The MVD is there ...The MVD is there ...The MVD is there ...
All vertices in the XY plane with -25 cm < Z < 25 cm The interactions in the material of the beampipe and the MVD are clearly seen
Ladders 3% Xo
Current Projects in the ZEUS Collaboration, Mónica L. Vázquez Acosta (NIKHEF) Max-Planck Intitute MunichMax-Planck Intitute Munich, 09/05, 2005 - 11
MVD Alignment with cosmic muonsMVD Alignment with cosmic muonsMVD Alignment with cosmic muonsMVD Alignment with cosmic muons
うQ’
Q
P
P
MVD alignmentminimize the difference betweenthe expected track position andthe measured hit position
cosmic track reconstruct as 2 tracks
0ZThe mismatch distribution has a width of 97 m after alignment
Before alignment
After alignment
Current Projects in the ZEUS Collaboration, Mónica L. Vázquez Acosta (NIKHEF) Max-Planck Intitute MunichMax-Planck Intitute Munich, 09/05, 2005 - 12
Impact parameter resolution from cosmicsImpact parameter resolution from cosmicsImpact parameter resolution from cosmicsImpact parameter resolution from cosmics
cosmic track reconstruct as 2 tracks
0Z
Difference of two independent tracks so divide by √2 : 83/pt + 47 m
This satisfies the design criterium of an impact parameter resolution of 100 m
After MVD alignment
Current Projects in the ZEUS Collaboration, Mónica L. Vázquez Acosta (NIKHEF) Max-Planck Intitute MunichMax-Planck Intitute Munich, 09/05, 2005 - 13
Tracking quantities in ep DIS dataTracking quantities in ep DIS dataTracking quantities in ep DIS dataTracking quantities in ep DIS data
Tracking quantities are well describedThe point of distance of closest approach is well described
Current Projects in the ZEUS Collaboration, Mónica L. Vázquez Acosta (NIKHEF) Max-Planck Intitute MunichMax-Planck Intitute Munich, 09/05, 2005 - 14
DD++: charm: charm taggingtagging with the MVDwith the MVDDD++: charm: charm taggingtagging with the MVDwith the MVD
The combinatorial background is reduced by a factor 45 and the signal by a factor 2.7
Submitted to ICHEP2004
Current Projects in the ZEUS Collaboration, Mónica L. Vázquez Acosta (NIKHEF) Max-Planck Intitute MunichMax-Planck Intitute Munich, 09/05, 2005 - 15
Event display of a DIS DEvent display of a DIS D++ candidate candidateEvent display of a DIS DEvent display of a DIS D++ candidate candidate
Q2 = 160 GeV2
pt(D+)=5.1 GeV
Current Projects in the ZEUS Collaboration, Mónica L. Vázquez Acosta (NIKHEF) Max-Planck Intitute MunichMax-Planck Intitute Munich, 09/05, 2005 - 16
Charm semileptonic decays in DISCharm semileptonic decays in DISCharm semileptonic decays in DISCharm semileptonic decays in DIS
Charm tagging: detect charmed mesons BR(c→D*) = 2.6 % detect e- BR(c→e-) = 9.6 %
Q2
Electron tagging using: CAL clusters with a matched track & dEdx CAL deposit requirementEEMC/ETOT>0.9 ("electron sample")EEMC/ETOT<0.4 ("hadron sample") → Estimate background
Current Projects in the ZEUS Collaboration, Mónica L. Vázquez Acosta (NIKHEF) Max-Planck Intitute MunichMax-Planck Intitute Munich, 09/05, 2005 - 17
Charm semileptonic decays in DISCharm semileptonic decays in DISCharm semileptonic decays in DISCharm semileptonic decays in DIS
HERA-I 99-00 data
Results to be made preliminary for EPS05
Current Projects in the ZEUS Collaboration, Mónica L. Vázquez Acosta (NIKHEF) Max-Planck Intitute MunichMax-Planck Intitute Munich, 09/05, 2005 - 18
Jet production in charged current DIS Jet production in charged current DIS Eur.Phys.J.C31: 149-164, 2003Eur.Phys.J.C31: 149-164, 2003
Jet production in charged current DIS Jet production in charged current DIS Eur.Phys.J.C31: 149-164, 2003Eur.Phys.J.C31: 149-164, 2003
Test flavour changing electroweak theory and QCD in one type of events
Current Projects in the ZEUS Collaboration, Mónica L. Vázquez Acosta (NIKHEF) Max-Planck Intitute MunichMax-Planck Intitute Munich, 09/05, 2005 - 19
Jet Substructure: mean subjet multiplicityJet Substructure: mean subjet multiplicityJet Substructure: mean subjet multiplicityJet Substructure: mean subjet multiplicity
(th.)(syst.)(stat.)0.0052 0.1202)(Mα 0.00650.0053
0.00600.0019ZS
QCD does not distinguish if W (CC) or (NC) is exchanged
NC CC
The kT algorithm is reapplied to particles assigned to jet until distances between clusters:
2jetTcutij Eyd
HERA physics is excitingbut the LHC is calling ...