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HADES Collaboration meeting XXII,
FW status for the upcoming HADES beam time Alexander Sadovsky Institute for Nuclear Research RAS, Moscow Readiness of FW to the physics run Some results from Sep-2010 beam test Simulation of : - Reaction plane reconstruction - LVL1 trigger usability? HADES Collaboration meeting XXII, May , 2011 Seillac, France
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HADES Forward Wall, installed: March 2007
Fully operational: summer 2010 Distance to target 7m 140 small 64 middle cells 84 large 2
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AGeV, Sep 2010
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Ni+Ni@1.25 AGeV, Sep 2010 ADC gain saturation Small cell:35
ADC ratio Z2-ratio ratios ratio n/(n-1) (Z(n))2/(Z(n-1))2 “(Z2/Z2)/(ADC/ADC)” /1 = /4 = /9 = /16= /25= /1 = /4 = /9 = /16= /1= /1= /4= /9= Small cell:35 peak ADC Middle cell:168 Large cell:297 A.Taranenko (small, ѳ~0.7o ) peak ADC Lin-Y ADC gain saturation ADC Log-Y ADC
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Ni+Ni@1.25 AGeV, Sep 2010, cell 35 dN/d(ADC) from 1st time peak
spectators with Z=2,3,4 ADC Typical time spectrum (two peaks) dN/d(ADC) from 2nd time peak spectators with Z=1,2,3 Time [ns] ADC Corresponding spectrum of ADC dN/d(ADC) from tails (slow particles) mainly secondaries ADC ADC
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Ni+Ni@1.25 AGeV, Sep 2010, cell 35 Trigger related ? Z1
Time [ns] ADC Time [ns] Time walk: different response for particles with different Z time threshold t1t2 t3 ADC Z1 Z2 Z3 t0 Z1 > Z2 > Z3 t1 < t2 < t3 ADC
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Ni+Ni@1.25 AGeV, Sep 2010, cell 35 Trigger selection of Mult(RPC)==2
Two peaks remain... Time [ns] {(Mult TOF + mult RPC )=2 && Mult TOF<1}
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Conclusions: Simulations SHIELD Au+Au@1.25GeV 20k events by M.Golubeva
FW works, ready for data taking Simulations SHIELD 20k events by M.Golubeva hGeant simulation with full reconstruction by K.Lapidus hydra-8.21, hgeant-8.21, full HADES geometry In simulation FW was placed on 5 meters from target (in real data 7 meters) No LVL1 emulation
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Reconstruction of reaction plane
288 channels scintillator hodoscope located 5 m from the target Reaction plane and centrality determination ⇉ K.Lapidus (CPOD-2010 at JINR) Q > 6 Q > 3 No cut
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Reaction plane reconstr.: Au+Au@1.25GeV/u
no selection 0 < b < 5 no weight Z weight 5 < b < 10 10 < b < 15 43° ⇉ K.Lapidus (HADES coll.meet 2010, GSI)
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FW fired cells distribution Au+Au@1.25AGeV
Selecting spectators by peak at time-of-flight distrib. in FW cells (left ): inside 2sigma (right): outside2sigma Spectators Secondaries y y 100% hits x [cm] x [cm] 16% dN/dx dN/dx Time [ns] Mean =18.1 Sigma=0.87 74% x [cm] Time [ns] x [cm]
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FW multiplicity vs. impact parameter
All hits: no restriction on time-of-flight in FW cells Spectators: restriction on time-of-flight in FW cells
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Number of fired FW cells (S,M,L) vs. b
Small size cells Medium size cells Large size cells b secondaries (top) spectators (bottom) Restriction on time-of-flight at FW cells:
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dN/db for different cut on num. fired cells
Increasing number of small cells fired selects b~9 dN/db b [fm] Increasing number of medium cells fired selects b~8 dN/db b [fm] Increasing number of large cells fired selects b~6 This can be applicable for the off-line analysis. dN/db b [fm]
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Centrality trigger with TOF and FW ?
Centrality selection with multiplicity conditions in FW / TOF dN/db b [fm]
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Forward Wall team NPI Řež: INR Moscow: A.Kugler,
Yu.Sobolev JINR) P.Tlusty, V.Wagner. INR Moscow: O.Busygina, F.Guber, A.Ivashkin, K.Lapidus Exc.Clust.Univ. & TU-Munich) A.Reshetin, A.Sadovsky, E.Usenko.
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Outlook Forward Wall was assembled and fully tested with real data
(2010) and ready for run. Time- and amplitude- parameters of FW were studied. FW response for the reaction was simulated. Possibilities of the FW use for the reaction plane reconstruction and it's potential usability in LVL1 trigger were demonstrated. Multiplicity in separate regions of FW (small, middle, large cells) can be used in off-line analysis for an additional centrality selection
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Backup slides/discussion
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Structure of FW with 288 counters
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Ni+Ni@1.25 @ 1.25 AGeV, Sep 2010 Small cell 35 Middle cell 168
Peak (n+1)/n ratio (Z(n+1))2/(Zn)2 /1=4.00 /4=2.25 /9=1.77 /1=4.00 /4=2.25 /9=1.77 /1=4.00 9/4=2.25 /1=4.00 /4=2.25 /9=1.77 Small cell 35 peak mean-pedestal = charge = 330 = 1030 = 1980 = 2540 Middle cell 168 = 690 = 2030 = 2650 Large cell 297 = 260 = 760 A.Taranenko (small, ѳ~0.7o ) peak charge
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Ni + Ni @ 1.25 AGeV, Sep10 ADC: for all particles ADC:
22ns<Time<31ns for spectators
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Ni AGeV, Sep10 Time: all hits Time: ADC Z=2
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Reaction plane recons. : Au+Au@1.25GeV/u
Cut on Q value helps in suppression of tails and improves the resolution 5 < b < 10 Q > 6 Q > 3 No cut 37o ⇉ K.Lapidus (HADES coll.meet. 2010, GSI)
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Beam 0.9 AGeV, Jun10 Ni AGeV, Sep10
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Multiplicities and immact param. distrib.
All hits, no restriction on time-of-flight in FW cells
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Multiplicities and immact param. distrib.
Spectators hits: restriction on time-of-flight in FW cells for spectators
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dN/db for number of fired S, M, L cells
Small size cells Medium size cells Large size cells b Dependence of number of fired cells (small, medium and large ones) from impact parameter. NB: “hill” of the distribution shifts (no restriction on time-of-flight at FW cells). One may see that large FW cells receive ~20 hits at b=0.
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dN/db for number of fired S, M, L cells
Small size cells Medium size cells Large size cells b Dependence of number of fired cells (small, medium and large ones) from impact parameter. NB: “hill” of the distribution shifts (restriction on time-of-flight for spectators at FW cells ). One may see that large FW cells receive ~8 hits at b=0.
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M(tof), M(rpc) vs M(fw) at different b
Impact parameters range influence to M(tof+rpc) vs M(fw) and M(tof) vs M(fw): spectatrors only (Tfw) dN/db b dN/db b dN/db b
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M(tof), M(rpc) vs M(fw) at different b
Impact parameters range influence to M(tof+rpc) vs M(fw) and M(tof) vs M(fw): all particles dN/db b dN/db b dN/db b
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Ni+Ni@1.25 AGeV, Sep 2010 Small cell:35 Middle cell:168 Large cell:297
Lin-Y Small cell:35 peak ADC Middle cell:168 Large cell:297 A.Taranenko (small, ѳ~0.7o ) peak ADC ADC ratio Z2-ratio (n+1)/n (Z(n+1))2/(Zn)2 /1=4.00 /4=2.25 /9=1.77 /1=4.00 /4=2.25 /9=1.77 /1=4.00 /1=4.00 /4=2.25 /9=1.77 ADC Log-Y ADC
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FW cell: time dependence from particle Z
TRB module has different response for particles with different Z Z1 > Z2 > Z3 t1 < t2 < t3 time threshold t1t2 t3 ADC Z1 Z2 Z3 t0
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Ni+Ni@1.25 AGeV, Sep 2010, cell 35 Time all Adc all Adc, time left
Adc, time right Adc, time tail
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