Measurements status and plans of the TOTEM experiment

  • Slides: 30
Download presentation
Measurements, status and plans of the TOTEM experiment at the LHC Fabrizio Ferro INFN

Measurements, status and plans of the TOTEM experiment at the LHC Fabrizio Ferro INFN Genova

TOTEM physics (in a glance) 2 TOTEM (main) physics goals are the measurement of

TOTEM physics (in a glance) 2 TOTEM (main) physics goals are the measurement of the total, elastic and inelastic proton-proton cross sections at several energies and the study of the diffractive processes Elastic scattering Total p-p cross section Forward particle production b Diffraction ICPPA 2017 F. Ferro - INFN Genova October-17

TOTEM at the LHC TOTEM is installed at IP 5 together with CMS 3

TOTEM at the LHC TOTEM is installed at IP 5 together with CMS 3 IP 5 ICPPA 2017 F. Ferro - INFN Genova October-17

Experimental apparatus (Run 1) Inelastic telescopes and proton tagging detectors 4 Inelastic telescopes CMS

Experimental apparatus (Run 1) Inelastic telescopes and proton tagging detectors 4 Inelastic telescopes CMS T 1: T 2: T 1 T 2 IP 5 Roman Pots (inside LHC tunnel) ICPPA 2017 RP (147 m) F. Ferro - INFN Genova RP (220 m) October-17

Inelastic telescopes Inelastic event counting, charged multiplicity, rapidity gaps 5 Roman Pot dets. Detection

Inelastic telescopes Inelastic event counting, charged multiplicity, rapidity gaps 5 Roman Pot dets. Detection of the leading protons Roman pot stations in the LHC tunnel at 147 m and 220 m from IP (both sides) 10 edgeless (<50 mm) Si micro strip detectors per pot T 1 § 5 CSC planes § 3. 1<|h|<4. 7 § Df = 2 p T 2 § 10 GEM planes § 5. 3<|h|<6. 5 § Df = 2 p ICPPA 2017 Resolution ~15 mm F. Ferro - INFN Genova Horizontal pot Vertical pots BPM October-17

Proton reconstruction and beam optics (x*, y*): vertex position (θx*, θy*): emission angle: t

Proton reconstruction and beam optics (x*, y*): vertex position (θx*, θy*): emission angle: t ≈ −p 2(θx*2 + θy*2) 6 ξ = Δp/p: momentum loss (elastic case: ξ = 0) Lx, Ly: effective lengths (sensitivity to scattering angle) vx, vy: magnifications (sensitivity to vertex position) Dx : dispersion (sensitivity to momentum loss); Dy ~ 0: Reconstruction of proton kinematics inverting the transport equation [New J. Phys. 16 (2014) 103041] Excellent beam optics understanding needed ICPPA 2017 F. Ferro - INFN Genova October-17

Proton acceptance Acceptance for elastic and diffractive protons depends on LHC optics and TOTEM

Proton acceptance Acceptance for elastic and diffractive protons depends on LHC optics and TOTEM running scenario (e. g. approach to the beam) t ≈ −p 2 Θ∗ 2: four-momentum transfer squared; ξ = Δp/p: fractional momentum loss typically 7 |t| > O(1 Ge. V 2) |t| > O(10− 2 Ge. V 2) |t| > few 10− 4 Ge. V 2 Elastic scattering: special case with ξ = 0 ICPPA 2017 F. Ferro - INFN Genova October-17

Elastic scattering: data sets vs t ranges 8 analysis ongoing [EPJC 76 (2016) 661]

Elastic scattering: data sets vs t ranges 8 analysis ongoing [EPJC 76 (2016) 661] [to be published] [EPL 96 (2011) 21002] [EPL 101 (2013) 21002] [NPB 899 (2015) 527 -546] [EPL 95 (2011) 41001] analysis ongoing ICPPA 2017 F. Ferro - INFN Genova October-17

Elastic scattering at 7 Te. V 9 Comparison with models ICPPA 2017 F. Ferro

Elastic scattering at 7 Te. V 9 Comparison with models ICPPA 2017 F. Ferro - INFN Genova October-17

Elastic scattering at 13 Te. V 10 ICPPA 2017 F. Ferro - INFN Genova

Elastic scattering at 13 Te. V 10 ICPPA 2017 F. Ferro - INFN Genova October-17

Elastic scattering trends Diffractive slope parameter B Diffractive dip position 11 Dip position decreases

Elastic scattering trends Diffractive slope parameter B Diffractive dip position 11 Dip position decreases with increasing s ICPPA 2017 F. Ferro - INFN Genova October-17

Elastic scattering at low t Usually called the “exponential region” The peak at “first

Elastic scattering at low t Usually called the “exponential region” The peak at “first glance” Peak is fitted with a polynomial exponential 12 Difference wrt pure exponential Simple exponential ruled out with a significance of 7. 2 s Differences of the order of ~1%. Very high statistics and very good control of systematics. ICPPA 2017 F. Ferro - INFN Genova [NPB 899 (2015) 527] October-17

Elastic scattering: measurement of r @13 Te. V expected soon 13 Totem direct measurement

Elastic scattering: measurement of r @13 Te. V expected soon 13 Totem direct measurement at 8 Te. V: ρ = 0. 12 ± 0. 03 Indirect measurement done at 7 Te. V First pp measurement of r since ISR era Results at 13 Te. V expected soon Requested run at 900 Ge. V to fill the gap Sensitivity to Odderon (JPC=1 --) states ICPPA 2017 F. Ferro - INFN Genova October-17

Total pp cross section: measurements 2. 76 Te. V Luminosity independent σtot = (84.

Total pp cross section: measurements 2. 76 Te. V Luminosity independent σtot = (84. 7 ± 3. 3) mb using ρ = 0. 145 [COMPETE] 14 7 Te. V Luminosity independent σtot = (98. 0 ± 2. 5) mb using ρ = 0. 14[COMPETE] r independent σtot = (99. 1 ± 4. 3) mb From elastic scattering only σtot = (98. 3 ± 2. 8) mb σtot = (98. 6 ± 2. 2) mb 8 Te. V Luminosity independent σtot = (101. 7 ± 2. 9) mb σtot = (101. 5 ± 2. 1) mb Different extrapolations to the optical point σtot = (102. 9 ± 2. 3) mb 13 Te. V Results expected soon, analysis ongoing ICPPA 2017 F. Ferro - INFN Genova October-17

Total pp cross section: measurements zoom 7 and 8 Te. V 15 2. 76

Total pp cross section: measurements zoom 7 and 8 Te. V 15 2. 76 Te. V CDF E 710 S-dependence compatible with ln 2 s growth Run and measurements at 0. 9 Te. V expected in late 2017 ICPPA 2017 F. Ferro - INFN Genova October-17

Charged-particle pseudorapidity density 16 T 2 with displaced vertex MC tuning in the forward

Charged-particle pseudorapidity density 16 T 2 with displaced vertex MC tuning in the forward region Valuable information for Cosmic Ray physics simulations CMS Measurements done with T 2 and CMS central detector ICPPA 2017 T 2 F. Ferro - INFN Genova October-17

Single diffraction (preliminary) 17 PRELIMINARY Estimated uncertainties: DB~15%, Ds~20% s. SD = 6. 5

Single diffraction (preliminary) 17 PRELIMINARY Estimated uncertainties: DB~15%, Ds~20% s. SD = 6. 5 ± 1. 3 mb in the range 3. 4 Ge. V < Mdiff < 1. 1 Te. V Preliminary results. Not all corrections included ICPPA 2017 F. Ferro - INFN Genova October-17

Central Exclusive Production (with CMS) 18 CMS and TOTEM work together to performs CEP

Central Exclusive Production (with CMS) 18 CMS and TOTEM work together to performs CEP studies CMS-TOTEM Trigger information are exchanged and data can be merged offline Central exclusivity can be verified via rapidity gaps and forward proton tagging selection rules for system X: JPC = 0++, 2++, … (PP, gg) JPC = 1 -- (g. P) ICPPA 2017 F. Ferro - INFN Genova October-17

Central Exclusive Production (with CMS) Low mass resonances and glueballs 19 At low (x

Central Exclusive Production (with CMS) Low mass resonances and glueballs 19 At low (x ~ 10 -3 – 10 -4) LHC becomes (a sort of) gluon-gluon collider and CEP is ideal for glueball production CEP with MX ~ 1 – 4 Ge. V produced very purely from gg 0++(2++) glueball candidates: f 0 (f 2) resonances in 1. 3 -1. 8 Ge. V(> 2 Ge. V) mass range Strategy: determine s. CEP of glueball candidates characterize their decays: p+p-, K+K-, r 0 r 0… CMS+TOTEM advantages: Good reconstruction of charged-particle-only events using dedicated low p. T tracking Good particle ID and mass resolution (s(M) ~ 30 Me. V) using CMS tracker RP protons from TOTEM to assure exclusivity (p. T, RP ~ p. T, tracker , vtx. RP ~vtxtracker) CMS+TOTEM 2015: L = 0. 4 pb-1 of high b* with dedicated low mass CEP trigger ICPPA 2017 F. Ferro - INFN Genova October-17

High luminosity proton detector physics CTPPS: CMS-TOTEM Precision Proton Spectrometer 20 Exclusive Production: photon-photon

High luminosity proton detector physics CTPPS: CMS-TOTEM Precision Proton Spectrometer 20 Exclusive Production: photon-photon fusion gluon-gluon fusion in colour-singlet state (JPC = 0++, 2++. . . ) CERN-LHCC-2014 -021 Tracking detectors + timing detectors in the Roman Pots Exclusive WW Exclusive dijets Inclusive missing mass/missing energy ICPPA 2017 F. Ferro - INFN Genova October-17

CTPPS setup in a snapshot 21 Currently taking data, first results being published See

CTPPS setup in a snapshot 21 Currently taking data, first results being published See e. g. : http: //cds. cern. ch/record/2265781? ln=en ICPPA 2017 F. Ferro - INFN Genova October-17

Conclusions TOTEM has taken data at the LHC at 2. 76, 7, 8 and

Conclusions TOTEM has taken data at the LHC at 2. 76, 7, 8 and 13 Te. V 22 Elastic pp scattering s-dependence of forward slope: acceleration at s ~ 3 Te. V ? non-exponentiality at low t Coulomb-nuclear interference at very low t: sensitivity to Odderon contribution Total cross section s-dependence generally compatible with ln 2 s growth non-negligible differences (mainly) in sinel probably related to MC corrections Preliminary measurements of single diffractive cross sections Measurement of charged d. N/dh multiplicity: MC tuning, CR impact CEP Low mass resonances and glueballs: public results expected soon High luminosity CEP CTPPS: new detectors for present and future data taking in nominal LHC runs ICPPA 2017 F. Ferro - INFN Genova October-17

Thank you!

Thank you!

References 24 • Measurement of Elastic pp Scattering at sqrt(s) = 8 Te. V

References 24 • Measurement of Elastic pp Scattering at sqrt(s) = 8 Te. V in the Coulomb-Nuclear Interference Region - Determination of the rho Parameter and the Total Cross-Section CERN-PH-EP-2015 -325, Eur. Phys. J. C 76 (2016) 661 • Evidence for Non-Exponential Elastic Proton-Proton Differential Cross-Section at Low |t| and sqrt(s) = 8 Te. V by TOTEM CERN-PH-EP-2015 -083, Nucl. Phys. B 899 (2015) 527 -546 • Measurement of the forward charged particle pseudorapidity density in pp collisions at sqrt(s) = 8 Te. V using a displaced interaction point CERN-PH-EP-2014 -260 Eur. Phys. J. C 75 (2015) 126 • LHC Optics Determination with Proton Tracks Measured in the Roman Pots Detectors of the TOTEM Experiment CERN-PH-EP-2014 -066 , New J. Phys. 16 (2014) 103041 • Measurement of pseudorapidity distributions of charged particles in proton-proton collisions at sqrt(s) = 8 Te. V by the CMS and TOTEM experiments CERN-PH-EP-2014 -063 ar. Xiv: 1405. 0722 EPJC 74 (2014) 3053 • Performance of the Totem Detectors at the LHC CERN-PH-EP-2013 -173 ar. Xiv: 1310. 2908 [physics. ins-det] Int. J. Mod. Phys. A • Double diffractive cross-section measurement in the forward region at LHC CERN-PH-EP-2013 -170 Phys. Rev. Lett. 111 (2013) 262001 • A luminosity-independent measurement of the proton-proton total cross-section at sqrt s = 8 Te. V CERN-PH-EP-2012 -354 Phys. Rev. Lett. 111, 012001 (2013) • Luminosity-independent measurements of total, elastic and inelastic cross-sections at sqrt s = 7 Te. V CERN-PH-EP-2012 -353, EPL 101 (2013) 21004 • Measurement of proton-proton inelastic scattering cross-section at sqrt s = 7 Te. V CERN-PH-EP-2012 -352, EPL 101 (2013) 21003 • Measurement of proton-proton elastic scattering and total cross-section at sqrt s = 7 Te. V CERN-PH-EP-2012 -239, EPL 101 (2013) 21002, Hep. Data • Measurement of the forward charged particle pseudorapidity density in pp collisions at sqrt s = 7 Te. V with the TOTEM experiment CERN-PH-EP-2012 -106, EPL 98 (2012) 31002 • First measurements of the total proton-proton cross section at the LHC energy of sqrt s = 7 Te. V CERN-PH-EP-2011 -158, EPL 96 (2011) 21002 • Proton-proton elastic scattering at the LHC energy of sqrt s = 7 Te. V CERN-PH-EP-2011 -101, EPL 95 (2011) 41001, Hep. Data ICPPA 2017 F. Ferro - INFN Genova October-17

25 Back up slides ICPPA 2017 F. Ferro - INFN Genova October-17

25 Back up slides ICPPA 2017 F. Ferro - INFN Genova October-17

Elastic scattering in the CNI region tmin = 6∙ 10 -4 Ge. V 2

Elastic scattering in the CNI region tmin = 6∙ 10 -4 Ge. V 2 26 Data available at 8 and 13 Te. V CNI with constant B and constant hadronic phase (labelled ”SWY”) excluded by TOTEM 8 Te. V data Usage of most common CNI formula, simplified West-Yennie (SWY) not valid ICPPA 2017 F. Ferro - INFN Genova October-17

Total pp cross section: strategies 27 �� ���� and �� ������ from ���� /d��

Total pp cross section: strategies 27 �� ���� and �� ������ from ���� /d�� �� ���� inclusive of low mass diffraction ICPPA 2017 F. Ferro - INFN Genova October-17

Diffractive event topology 28 ICPPA 2017 F. Ferro - INFN Genova October-17

Diffractive event topology 28 ICPPA 2017 F. Ferro - INFN Genova October-17

29 ICPPA 2017 F. Ferro - INFN Genova October-17

29 ICPPA 2017 F. Ferro - INFN Genova October-17

30 ICPPA 2017 F. Ferro - INFN Genova October-17

30 ICPPA 2017 F. Ferro - INFN Genova October-17