Status of the TOTEM Experiment and Latest Results Hubert Niewiadomski on behalf of the TOTEM Collaboration LHCC, 15 June 2011
Download ReportTranscript Status of the TOTEM Experiment and Latest Results Hubert Niewiadomski on behalf of the TOTEM Collaboration LHCC, 15 June 2011
Status of the TOTEM Experiment and Latest Results Hubert Niewiadomski on behalf of the TOTEM Collaboration LHCC, 15 June 2011 Experimental Setup @ IP5 Inelastic telescopes: charged particle & vertex reconstruction in inelastic events T1: 3.1 < < 4.7 T2: 5.3 < < 6.5 IP5 HF (CMS) ~ 10 m ~ 14 m T1 CASTOR (CMS) T2 Roman Pots: measure elastic & diffractive protons close to outgoing beam IP5 RP147 RP220 T1 T2 RP 147 The TOTEM experiment is completely installed and running • • • • • • All Roman Pots at 147 and 220m installed (24 pots) T1 detectors are installed on both sides T2 detectors are installed on both sides Trigger system based on all detectors is running DAQ is running with an event rate capability of 1 kHz Special runs with dedicated b* and bunch structures are prepared Beam based alignment of RPs @220m and data taking (T1,T2,RP220m) (18 May 2011) Beam Loss Data Beam intensity Scraping exercise: RP220 approached the low intensity beam in 10 mm steps RP220 now ready for routine insertions in 2011 RP approach x, y Vert Pot Position (mm) Data taking with RPs @ 220 close to the beams - vertical RPs @ 5σ = 2.2 mm - horizontal RPs @ 7σ = 1 mm - low pile-up Alignment of RP147 planned in August T2 data 2011 Raw data Very good agreement: - left and right side - bunch and active trigger Pythia PhoJet Unfolded Green band after vertex cuts ‘Plus’ and ‘minus’ T2 sides superimposed - Bunch crossing trigger - T2 detector trigger Taken during scraping exercise only low intensity bunches of 1010 p (low pile-up) Low luminosity runs 2010 Preliminary dN/d results (T1) • 3 short periods of data taking with useful conditions for T1 (L = 1028 – 1030 cm–2 s–1): March (2.76 TeV), May (7 TeV) • 25 million events collected with different configurations • Data analysis in progress • T1 ready for physics Distributions (uncorrected) Vertex reconstruction 7 TeV Vertex reconstruction is effected by the CMS magnetic field Symmetric distributions obtained – a good starting point ELASTIC pp SCATTERING t-range: 0.36 – 3 GeV2 Elastic pp scattering • Several runs were taken during 2010 with different distances of the Roman pots to the beam center • The 7 s runs were analyzed • The 18 s runs with a total luminosity of 5.8 pb-1 will follow Luminosity 25 s Integrated luminosity 1.5 nb-1 20 s 185 nb-1 18 s 5800 nb-1 RP dist. Analysed data files 7s p. 9 Karsten Eggert– 9.5 nb-1 important for large t Proton reconstruction • Both angle projections reconstructed: Θx* and Θy* – Θx* from Θx @ RP220 (through dLx/ds) – Θy* from y @ RP220 (through Ly) Θx = dLx/ds Θx* y = Ly Θy* → Excellent optics understanding – Magnet currents measured – Measurements of optics parameters with elastic scatt. • • • Θleft* = Θright* (proton pair collinearity) Proton position ↔ angle correlations Lx=0 determination, coupling corrections → Fine alignment – Alignment between pots with overlapping tracks (1μm) – Alignment with respect to the beam – scraping exercise (20μm) – Mechanical constraints between top and bottom pots (10μm) Track based alignment Cuts and data reduction • Topology Intergrated luminosity : 6.2 nbarn-1 – near and far units – diagonals • Low || selection (3σ) – – – – |xRP,45|<3σx @ Lx,45=0 |xRP,56|<3σx @ Lx,56=0 corr. yRP216,45 yRP220,45 corr. yRP216,56 yRP220,56 • Elastic collinearity (3σ) – θx,45* θx,56* – θy,45* θy,56* Total triggers 5.28M Reconstructed tracks & elastic topology 293k Low || selection 70.2k Collinearity cuts 66.0k showers Diagonals analysed independently Proton tracks of a single diagonal (left-right coincidences) Sector 56 t = -p2 q2 = Dp/p Sector 45 y = Ly Qy x = Lx Qx + D Lx ~ 0 Cuts and data reduction • Topology Intergrated luminosity : 6.2 nbarn-1 – near and far units – diagonals • Low || selection (3σ) – – – – |xRP,45|<3σx @ Lx,45=0 |xRP,56|<3σx @ Lx,56=0 corr. yRP216,45 yRP220,45 corr. yRP216,56 yRP220,56 • Elastic collinearity (3σ) – θx,45* θx,56* – θy,45* θy,56* Total triggers 5.28M Reconstructed tracks & elastic topology 293k Low || selection 70.2k Collinearity cuts 66.0k showers Low = Dp/p cuts |x| < 3σx @ Lx = 0 yRP near,45 yRP far,45 (dLy/ds0) Cuts and data reduction • Topology Intergrated luminosity : 6.2 nbarn-1 – near and far units – diagonals • Low || selection (3σ) – – – – |xRP,45|<3σx @ Lx,45=0 |xRP,56|<3σx @ Lx,56=0 corr. yRP216,45 yRP220,45 corr. yRP216,56 yRP220,56 • Elastic collinearity (3σ) – θx,45* θx,56* – θy,45* θy,56* Total triggers 5.28M Reconstructed tracks & elastic topology 293k Low || selection 70.2k Collinearity cuts 66.0k showers Elastic collinearity cuts Data outside the 3σ cuts used for background estimation Background and resolution determination –– signal –– background –– combined B/S = (8±1)% σ*=17.8mrad (beam divergence) Data Combined background (t) -t [GeV2] Dθx/sqrt(2) Signal to background normalisation (also as a function of Dθy) σ* → t-reconstruction resolution: s (t ) t 0.4 GeV 2 : 14% 2 ps * = : 1 GeV 2 : 8.8% t 3 GeV 2 : 5.1% Signal vs. background (t) |t|=0.4GeV2: B/S = (11±2)% |t|=0.5GeV2: B/S = (19±3)% |t|=1.5GeV2: B/S = (0.8±0.3)% ty-acceptance corrections |t|<0.36GeV2 removed Missing acceptance in θy* Correction error (ty): 0.31 GeV2 : 30% 0.33 GeV2 : 11% 0.35 GeV2 : 2% 0.4 GeV2 : 0.8% 0.5 GeV2 : 0.1% -acceptance correction Total -acceptance correction Accepted (t) t [GeV2] Θ* [rad] 1 2 3 4 5 6 0.33 0.36 0.60 1.00 1.80 3.00 1.65E-04 1.71E-04 2.21E-04 2.86E-04 3.83E-04 4.95E-04 38.6 76.4 162.5 209.8 246.3 269.0 Diagonal 1 12 3 4 No. Accepted (2 diag.) [°] 5 6 Θ* |t|<0.36GeV2 removed Accepted (t) Diagonal 2 Critical at low t-acceptance limit accept. correct. factor 9.3±4.7% 4.7±1.8% 2.2±0.3% 1.7±0.1% 1.5 1.3 Final unfolded distribution | Systematic normalisation uncertainty30% Elastic Scattering – from ISR to Tevatron ISR ~ 1.7 GeV2 ~ 0.7 GeV2 ~1.5 GeV2 Comparison to some models B (t=-0.4 GeV2) tDIP t-n [1.5–2.5 GeV2] 20.2 23.3 0.60 0.51 5.0 7.0 22.0 0.54 8.4 25.3 20.1 0.48 0.72 0.53 ± 0.01 10.4 4.2 23.6 ± 0.5 Better statistics at large t needed 7.8 ± 0.3 Future analyses of existing data 1. RP – 18 s 2010 data (5.8 pbarn-1) – Double Pomeron Exchange, RP +T1 and T2 (2011 data from 6 low L pilots) 2. Inelastic detectors T1 and T2 (data from 2011) – Pseudorapidity distributions (including RP information) – Multiplicity distributions and correlations Future runs 2011 1. RP 220 m fully validated (14 s vert., 17 s horiz. in normal runs): (large-t elastic scattering, β*=1.5 m) 2. RP 147 m beam based alignment with data taking (August) (diffraction) 3. β* = 90 m optics – First MD (done): successful for separated beams – Next MD (28. June): establish collisions and ~1hour data taking for optics diagnostics – Physics starting in August / September • • Low-t (10 -2 GeV2) elastic scattering Total cross-section (extrapolation to t=0 possible) BACKUP Outlook: Measurement of r in the Coulomb-nuclear Interference Region? Aim: get also the last ingredient to stot from measurement rather than theory (eN = 3.75 mm rad) (eN = 1 mm rad) might be possible at sqrt(s)=7 TeV with RPs at 6 s incentive to develop very-high-b* optics before reaching 14 TeV ! e.g. try to use the same optics principle as for 90m and unsqueeze further. OPTICS Optics verification Triplet dLx/ds dLy/ds MQY MQML dLy/ds|s=220m measured by TOTEM Lx Ly s dLy ( ) L ( s ) = L y ( 0) = 0 y 0 d d C1 , with dLy dL ( s ) s y ds (0) = 1 = Ly ( )k ( )d C2 ds 0 s: Lx=0 measured by TOTEM s: Lx(s)==0 determination • Four fits per diagonal, 8 in total, diagonals averaged Top 45 bottom 56, 45 near s=214.463 m Top 45 bottom 56, 45 far s=220 m a=2.229 a=-3.142 Interpolation: Lx(s) = 0 for s = 217.8 m (nominally 222.1m) Θy vs. y, coupling , beam 1 Preliminary fits, fit direction rather needs to be orthogonal, better numbers from Jan’s alignment needed (dLy/ds) / Ly near =3.9210-3 m-1 5 % Nominally: 2.710-3 m-1 Constraint for triplet strenghts matching re14/re34 far=36 mrad5 % Nominally: 0 Constraint for triplet rotation matching Beam 2 • (dLy/ds) / Ly=2.61510-3 m-1 5 % (nominally 1.30410-3 m-1) • re14/re34 far=31.8 mrad 5 % (nominally 0) Matched parameters • Perturbation of (nominal) actual LHC settings – 30 parameters per beam – Magnet positions, rotations, k – Beam energy, displacement, crossing angle, harmonics... • Selected fitted parameters – – – – 6 strengths per beam (MQXA, MQXB, MQXB, MQXA, MQY, MQML) 6 corresponding rotations per beam Mean per beam Total of 26 fitted parameters Constraints • TOTAL of 36 • LHC design constraints (a total of 26): – sigma(k)/k = 0.1% – sigma (rot) = 1mrad – Sigma()/ = 10-3 • Measured constraints of individual arms (a total of 8): – (dLy/ds)/Ly; near unit rotation (coupling); far unit rotation (coupling) – s: Lx==0 (1 m precision) • Measured elastic scattering kinematics constraints between arms (a total of 2): – Ratio of Ly56 / Ly45 (0.2 % precision) – Ratio of (dLx/ds 56) / (dLx/ds 45) (0.5 % precision) Matching solution 56 dLx/ds Ly [m] RP215 RP220 D RP215 D RP220 -0.311962 -0.311962 -2.84% -2.84% 22.1464676 0.0432331 22.6191755 0.0396463 +0.78% +0.81% 45 dLx/ds Ly [m] RP215 RP220 D RP215 D RP220 -0.314508 -0.314508 -4.51% -4.51% 34 33 35 36 2 1 2 3 31 Principle Component Analysis (PCA) ideally should be applied ROT [mrad] 20.3883272 0.0400268 20.6709463 0.0372828 +10.19% +10.79% 2/NDF = 25.8/(36-26)=2.6 (would be lower in correlations are elmininated) Matching results within the LHC tolerance 4 25 5 1.5 32 ROT [mrad] Strong correlations between fitted parameters 24 6 7 1 30 8 28 11 26 12 25 13 24 14 23 15 22 21 20 19 18 17 16 Abs(Pulls) of constraints 3 4 5 22 10 27 2 1 6 9 0 1 1.5 23 0.5 29 26 2 0.5 All constraints 21 7 Fitted parameters 0 20 8 19 9 18 10 17 11 16 15 14 13 12 Abs(Pulls) of fitted parameters ANALYSIS STEPS DETAILED Analytical unfolding Smearing only due to beam divergence Detector resolution negligible (divergence uncertainty) Verified by MC based approach Verified by stringent selection cuts Unfolding verification MC vs. Analytical unfolding Data transformations (after selection cuts) diagonal top 45 bottom 56 alone Raw data Acceptance corrected 4 5 6 1 2 1 – raw data (signal + background) 2 – estimated background 3 3 – estimated background acceptance corrected 4 – raw data acceptance corrected 5 – raw data acceptance corrected - background 6 – final unfolded distribution The Roman Pot System at 220 m and 147 m fully installed TOTAL: 24 pots p. 38 Karsten Eggert– Installation of the RP system at 147 m p. 39 Karsten Eggert–