HyCal reconstruction: current situation and future tasks . V. Mochalov, IHEP (Protvino)
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1Brookhaven National Laboratory2University of California- Berkeley3Pennsylvania State University4IHEP, Protvino5Stony Brook University6Texas A&M University7Utrecht, the Netherlands
8Zagreb University
FMS status - June 2007F.Bieser2, L.Bland1, E. Braidot7, R.Brown1, H.Crawford2, A.Derevshchikov4, J.Drachenberg6, J.Engelage2, L.Eun3, M.Evans3, D.Fein3, C.Gagliardi6, S.Hepplemann3, E.Judd2, V.Kravtsov4, J. Langdon5, Yu.Matulenko4, A.Meschanin4, C.Miller5, D.Morozov4, M.Ng2, L.Nogach4, S.Nurushev4, A.Ogawa1, H. Okada1, J. Palmatier3, T.Peitzmann7, S. Perez5, C.Perkins2, M.Planinic8, N.Poljak8, G.Rakness3, A.Vasiliev4, N.Zachariou5
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Three Highlighted Objectives In STAR Forward Meson Spectrometer Proposal
[hep-ex/0502040]
1. A d(p)+Aud(p)+Au+X+X measurement of the parton model gluon density distributions xg(x) in gold gold nucleinuclei for 0.001< 0.001< xx <0.1 <0.1. For 0.01<x<0.1, this measurement tests the universality of the gluon distribution.
2. Characterization of correlated pion cross sections as a function of Q2 (pT
2) to search for the onset of gluon saturation effects associated with macroscopic macroscopic gluon fields. gluon fields. (again d-Au)(again d-Au)
3. Measurements with transversely polarized transversely polarized protonsprotons that are expected to resolve the origin of resolve the origin of the large transverse spin asymmetriesthe large transverse spin asymmetries in reactions for forward forward production. production. (polarized (polarized pp)pp)
DOE milestone
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FPD -> FMS
The FPD originated as a test cell for the EEMC and has evolved into a 2mx2m forward spectrometer providing new physics results with each run
Run-5 FPDRun-6 FPD++Run-7 FMS
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Any difference between p+p and d+Au?
Kharzeev, Levin, McLerran gives physics picture (NPA748, 627)
Color glass condensate predicts that the back-to-back correlation from p+p should be suppressed
Frankfurt and Strikman:Frankfurt and Strikman:Explains our RExplains our RdAudAu result with result with black center nucleusblack center nucleus (>10% energy loss) (>10% energy loss)
and only peripheral events contributing to leading pion production.and only peripheral events contributing to leading pion production.Also explain suppression of away jet with combinatorics.Also explain suppression of away jet with combinatorics.
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How do we tell if there is a CGC?
ln(1/x) and the scale (Q) is taken as pT
Require two (jets) in FMS probes smallest x gluons in Au nucleus (largest )Look for broadening or disappearance of peak as pT decreases
pT decreasing
We will map the Q2 - X space
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FMS for d-Au saturation physicsFMS for d-Au saturation physicsp+p and d+Au ++X correlations with forward
hep-ex/0502040p+p in PYTHIA d+Au in HIJING
Conventional shadowing will change yield, but not angular correlation. Saturation will change yield and modify the angular correlation.
Sensitive down to xg ~ 10-3 in pQCD scenario; few x 10-4 in CGC scenario.
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The STAR FMS is a ~2m x 2m lead-glass wall west of the STAR interaction point viewing collisions through the hole in the STAR magnet poletip. In conjunction with the barrel and endcap EMC, the addition of the FMS realizes a “full-acceptance detector” with electromagnetic calorimetry for -1 < < +4
STAR Forward Meson Spectrometer (FMS)Lead-glass calorimeter / STATUS
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d+Au +X at 200 GeV
pT dependence of d+Au π0 cross section at <η> = 4.0 is best described by a LO CGC calculation.
(Dumitru, Hayashigaki, and Jalilian-Marian, NPA 765, 464)
nucl-ex/0602011
STARSTAR
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π0 AN at √s=200 GeV – xF-dependence
• AN at positive xF grows with increasing xF
• AN at negative xF is consistent with zero
• Run 6 data at <η>=3.7 are consistent with the existing measurements
• Small errors of the data points allow quantitative comparison with theory predictions
• Theory expects the reverse dependence on η
Phys.Rev.D74:114013,2006Phys.Rev.D74:114013,2006..
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A-single- study using PythiaHiromi Okada
What is Ex point for R=Nall/N
direct=1? With VETO, Without VETO (VETO: Large cells)
Pythia condition:• MSELL=0,• MSUB=(11,12,13,28,53,68,81,82,86,87,88,89,92,93,94,95,1,2) and
(14,18,29,114,115). inelastic=41.12 [mb]
• CKIN(5)=1,CKIN(6)=1,CKIN(3)=0,CKIN(4)=-1. Select “A single events”
• Acceptance: FPD++ small cells• VETO FPD++ large cells (See page 2)
Results Without VETO EX=43 GeV (Intersecting point of black and pink histograms in page 3) With VETO EX=26 GeV (This value can be improved
by better choices for "acceptance" and "veto“).
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Single photon acceptance
Acceptance (Small cells)
Veto (Large cells)
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A single events in acceptance (FPD++ inner cells)
from 0 (Without VETO) from (Without VETO)
Direct-
43 GeV E from 0 (With VETO)
L=0.9 pb-1
3.81010 calls
WITHOUT VETO
Pythia simulation
Intersecting point of black and pink histograms
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Cell details
Large Cells / 788 in total
(5.8cm)2 x 60.2 cm lead glass
18.75 radiation lengths
XP2202 photomultiplier
5.8cm
60.2 cm
Small Cells / 476 in total
(3.8cm)2 x 45 cm lead glass
18 radiation lengths
FEU84 + XP2972 photomultipliers
170 small cells prior to wrapping
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STAR Forward Meson Spectrometer (FMS)Lead-glass calorimeter / STATUS
Detectors are stacked on the west platform in two movable halves. This view is of the south FMS half, as seen through the retracted west poletip.
Schematic of the FMS as seen from the interaction point. The small-cell inner calorimeter has 476 detectors and the large cell outer calorimeter has 788 detectors.
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High Voltage Systems
Large cells / 788 in total
XP2202 phototube powered by Zener-diode-stabilized resistive voltage divider, with high-voltage delivered by
four 256-channel LeCroy 1440 main frames
Small cells viewed by FEU-84 224 in total
Cockcroft-Walton system for FEU-84 designed/built by Steve Heppelman,
Len Eun, et al. at Penn State University
Small cells view by XP2972252 in total
Existing phototubes and bases courtesy of Yale University, from AGS-E864
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Up to16 controllers of either type
Up to16 PSU bases
Up to16 Yale bases
PC
USB to I2C
Light-tight, ventilated enclosure (half of FMS)+9V/2.4A
+30V/1.2A
-6/0.5A
as in E864
Two PC-controlled 256-channel Cockcroft-Walton control systems designed/built by Steve Heppelmann, Len Eun, et al. (Penn State) for small-cell inner calorimeter HV control
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PSU controllers
Master controller
Yale controllers
Yale bases PSU bases
Resistive bases
High-voltage systems as implemented in north FMS half
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Electronics and TriggerHank Crawford, Fred Bieser, Jack Engelage, Eleanor Judd, Chris Perkins, et al.
(UC Berkeley/SSL)
QT8 daughter card QT32 with 4 QT8 daughter cards
Readout of 1264 channels of FMS provided by QT boards. Each board has
• 32 analog inputs
• 12-bit ADC / channel
• 5-bit TDC / channel
• five FPGA for data and trigger
• operates at 9.38 MHz and higher harmonics
• produces 32 bits for each RHIC crossing for trigger
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South FMS rack, servicing 632 detectors
QT1 Crate 1/12 QT boards
QT2 Crate 12 QT boards
FMS Crate 16 DSM boards
Present Status
• 37/48 QT boards mounted in 9U VME in STAR Wide Angle Hall;
• all QT boards ready for installation;
• QT2,QT3,QT4 crates connected to phototubes and tested operational;
• Trigger connections completed; tests after run ends.
North FMS rack, servicing 632 detectors
QT3 Crate 12 QT boards
QT4 Crate 12 QT boards
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Commissioning of FMS during Run 7Ready for Production Now and in Run 8
• completed: cell-by-cell scans of HV to check HV and signal connections
• completed: quadrant-by-quadrant total-energy measurements
• completed: initial timing for QT electronics
Au Au FMS Commissioning Au Au FMS Commissioning
Cell multiplicityCell multiplicity
Summed Energy (ADC cnts)Summed Energy (ADC cnts)
QT gate
North Large Cell
Row-2 / Col-11
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QT status
Currently have 3/4 of QTs operating. Expect to add final 1/4 next week.
Have verified sensitivity as <0.25 pC/count
Have verified absence of correlated noise; single channel rms~0.6 cts
Linear over full range to <1%
Expect to test L0 trigger capabilities this week
Building multi-LED programmable system for testing trigger pattern capability - for use this summer
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Future
We expect to explore at least two upgrades to the FMSTo allow us to investigate forward π0 production and theExpected asymmetries using the 250 GeV pp beamsAnd to explore QCD Drell-Yan processes producing charged Leptons.Both of these concepts require a position sensitive detector at the front of the FMS; the second requires tracking through a magnetic field.