Total pp cross section measurements at 2, 7, 8 and 57 TeV

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1 Total pp cross section measurements at 2, 7, 8 and 57 TeV A) One (out of several) theoretical framework B) Topologies of events in σ tot C) Direct measurement of σ inel : 1) cosmic-ray experiments 2) collider experiments D) The art of elastic scattering E ) Results: σ Tot, σ SD, σ DD F ) Implication of the new results LISHEP 18 March 2013 N. Cartiglia, INFN Turin. 1

2 Let s set the scale The total cross section is dominated by soft processes mb If you were to eliminate every process below the first line (even the Higgs, the first AND the second one..!) the value of the total cross section would be the same If R 1 = R 2 = cm (one fermi)! σ ~ cm 2 = 100 mb LISHEP 18 March 2013 N. Cartiglia, INFN Turin. 2

3 Scattering of composite particles The cross section between composite particles has a much more complex dependence from the center-of-mass energy, and it s not calculable. Let s consider a proton. It contains: - valence quarks - sea quarks - gluons These define the particle to be a proton Mostly SU(3) color symmetric, common to protons and anti-protons (almost true..) What part is controlling the total cross section? LISHEP 18 March 2013 N. Cartiglia, INFN Turin. 3

4 pp vs pbarp cross section At low energy σ is different: valence quarks need to be important here At high energy σ is the same: only sea quarks and gluons can contribute LISHEP 18 March 2013 N. Cartiglia, INFN Turin. 4

5 LISHEP 18 March 2013 N. Cartiglia, INFN Turin. 5

6 Theoretical framework: Regge Theory Regge Theory, and derivations, is the language used to describe the total cross sections of hadron-hadron scattering. The value of the total cross section depends on the exchanges of many particles. 1) Particles, when plotted in the mass (t) - spin plane, form lines, called trajectories. 2) You cannot exchange a single particle, you exchange all the particles on the trajectory. p Plot of spins of families of particles against their squared masses: α(t) α t Intercept p? Trajectory exchange The function α(t) is called a Regge trajectory LISHEP 18 March 2013 N. Cartiglia, INFN Turin. 6

Contribution of each trajectory to σ All known particles lie on trajectories such as: α(t) α + α t Each trajectory contributes to σ according to: σ TOT (s) = Im A(s,t = 0) = s α 1 And

7 Contribution of each trajectory to σ All known particles lie on trajectories such as: α(t) α + α t Each trajectory contributes to σ according to: σ TOT (s) = Im A(s,t = 0) = s α 1 And therefore the prediction for the total cross section is: α smaller than 1!! So, it should decrease with s. However. σ TOT (s) = s α(0) 1 = s -1/2 LISHEP 18 March 2013 N. Cartiglia, INFN Turin. 7

8 Overview of hadronic cross sections pp πp pk pn The cross section is raising at high energy: every process requires a trajectory with LISHEP the same 18 March positive 2013 exponent: s 0.08 N...something Cartiglia, INFN Turin. is clearly missing 8

9 The advent of the Pomeron Intercept larger than one! A trajectory without known particles Intercept larger than one V. Gribov introduced, within Regge theory, a vacuum pole (Pomeron with α(0) ~ 1.1) in order to have a constant (or rising) total cross section. 9 LISHEP 18 March 2013 N. Cartiglia, INFN Turin. 9

10 The problem with the Pomeron trajectory The exchanged particles (poles) on Reggeon an pion trajectories offer guidance on how to write the scattering amplitude A(s) There is little spectroscopic guidance from the pomeron trajectory, as it has no particles. Pomerons exchange contribute as: σ TOT (s) = Im A(s,t = 0) ~ s ε (simple pole) σ TOT (s) = Im A(s,t = 0) ~ ln(s) (double pole) σ TOT (s) = Im A(s,t = 0) ~ ln 2 (s) (triple pole) The COMPETE collaboration has scanned a large selection of models compared with all available experimental data points and has produced a comprehensive set of predictions. σ COMPETE tot (7 TeV) = 98 ± 5 mb σ COMPETE tot (8 TeV) = 101 ± 5 mb LISHEP 18 March 2013 N. Cartiglia, INFN Turin

Regge Theory: master formula pre-lhc Three large families of parametrization: To infinity σ TOT (s) = c + α s -0.5 + β s 0.08 σ TOT (s) = c + α s -0.

11 Regge Theory: master formula pre-lhc Three large families of parametrization: To infinity σ TOT (s) = c + α s β s 0.08 σ TOT (s) = c + α s γ ln 2 (s) (most favorite COMPETE prediction) σ TOT (s) = c + α s β ln(s) + γ ln 2 (s) Reggeon decrease Pomeron increase QCD: exchange of valence quark QCD: exchange of sea quark and gluons, glueballs.. But no high-m 11 diffraction! LISHEP 18 March 2013 N. Cartiglia, INFN Turin. 11

12 The Rise of the gluons As measured at HERA, the gluon PDFs experience a very strong rise as the energy increases. If the pomeron is related to gluons, it s reasonable to assume a modification of the pomeron term: the cross section will start rising more rapidly at higher energy. LISHEP 18 March 2013 N. Cartiglia, INFN Turin. 12

13 2-pomeron formula for higher energy In a simple model (DL, Cudel et al.) an additional term called hardpomeron can be introduced in σ TOT to account for this effect. It gives a steeper energy behavior: σ TOT (s) = α s β s γ s 0.45 (2 simple poles) Hard pomeron contribution DL for LHC: σ TOT ( s = 7) = mb LISHEP 18 March 2013 N. Cartiglia, INFN Turin. σ TOT ( s = 14) = mb 13

14 Total cross section and elastic scattering At small t, elastic scattering is governed by an exponential law. Elastic scattering probes the proton at a distance b ~ 1/ t dσ EL dt = Ae B t p p p p t Solid: Total spectrum, sum of 3 contributions Different models predicts different t spectrum and contributions The proton is made of different layers, each contributing differently to the cross section (3) (1) (2) (3) t > ~ 4 GeV 2 Elastic scattering on valence quark (1) t < ~ 1 GeV 2 ~ 0.2 fm Scattering between qqbar condensate >~ 0.4 fm (2) t ~1-4 GeV 2 Exchange of vector mesons LISHEP 18 March 2013 N. Cartiglia, INFN Turin. 14

15 Monte Carlo models: RFT vs. pqcd QGSJET 01, QGSJET II SIBYLL PHOJET EPOS RFT based models Soft QCD σ Tot, σ El, σ Inel, σ SD, σ DD Extended to ~ Λ QCD Extended to Hard QCD pqcd based models PYTHIA HERWIG SHERPA LISHEP 18 March 2013 N. Cartiglia, INFN Turin. 15

$Topologies of events in σ tot TOTAL cross section means measuring everything We need to measure every kind of events, in the full rapidity range: σ Tot = σ elastic +σ diffractive (σ SD +σ DD +.$

16 Topologies of events in σ tot TOTAL cross section means measuring everything We need to measure every kind of events, in the full rapidity range: σ Tot = σ elastic +σ diffractive (σ SD +σ DD +...)+σ Elastic: two-particle final state, very low p t, at very high rapidity.! Very difficult, needs dedicated detectors near the beam Diffractive: Single, Double, Central diffractions, gaps everywhere.! Quite difficult, some events have very small mass, difficult to distinguish diffraction from standard QCD. Everything else: jets, multi-particles, Higgs.! Easy LISHEP 18 March 2013 N. Cartiglia, INFN Turin. 16

17 The very difficult part: elastic scattering Need dedicated experiments able to detect scattered particles very closed to the beam line: pp! pp Far p Sector 45 (220m) Near p p ~ 150 m p ~ 5 mm Sector 56 (220m) Near Far Top Top BLM Horizontal BPM IP5 BPM Horizontal BLM Bottom Bottom LHC Roman Pot and silicon detector LISHEP 18 March 2013 N. Cartiglia, INFN Turin. 17

18 The difficult part: pomeron exchange Pomeron exchange is a synonym of colour singlet exchange (diffraction) Many different topologies to measure Importance of very low mass events LISHEP 18 March 2013 N. Cartiglia, INFN Turin. 18

$The easy part: everything else The non-diffractive inelastic events are$

19 The easy part: everything else The non-diffractive inelastic events are usually not difficult to detect: LISHEP 18 March 2013 N. Cartiglia, INFN Turin. 19

Direct measurement of parts of σ TOT : cosmic-ray and collider experiments In cosmic-ray experiments (AUGER just completed its analysis), the shower is seen from below.

20 Direct measurement of parts of σ TOT : cosmic-ray and collider experiments In cosmic-ray experiments (AUGER just completed its analysis), the shower is seen from below. Using models, the value of σ inel (p-air) is inferred, and then using a technique based on the Glauber method, σ inel (pp) is evaluated. In collider experiments (currently ALICE, ATLAS, CMS, and LHC ), the detector covers a part of the possible rapidity space. The measurement is performed in that range, and then it might be extrapolated to σ inel. LISHEP 18 March 2013 N. Cartiglia, INFN Turin. 20 η

21 We want to measure the point of impact Cosmic-ray shower The actual measurement is done on the ground, with Cherenkov light and muon detectors. What is measured is only loosely connected with the impact point LISHEP 18 March 2013 N. Cartiglia, INFN Turin. 21

22 Cosmic-ray experiments: the method to measure σ inel - The path before interaction, X 1, is a function of the p-air cross section. - The experiments measure the position of the maximum of the shower, Xmax - Use MC models to related X max to X 1, and then σ (p-air) LISHEP 18 March 2013 N. Cartiglia, INFN Turin. 22

23 Auger: the measurement The position of the air shower maximum, at fixed energy, X max, is sensitive to the cross section LISHEP 18 March 2013 N. Cartiglia, INFN Turin. 23

24 Auger: p-air cross section AGASA Ne/Nµ Technique Fly s Eye X max tail AUGER X max tail HiRes X max tail EAS-TOP Ne/Nµ Technique LISHEP 18 March 2013 N. Cartiglia, INFN Turin. 24

25 LISHEP 18 March 2013 N. Cartiglia, INFN Turin. 25

26 The Glauber model The p-air cross section is interpreted as the convolution of effects due to many nucleons LISHEP 18 March 2013 N. Cartiglia, INFN Turin. 26

27 Auger: pp cross section LISHEP 18 March 2013 N. Cartiglia, INFN Turin. 27

Collider experiments: measure σ inel by counting number of vertexes 7 8 4 5 6 2 3 1 How

28 Collider experiments: measure σ inel by counting number of vertexes How to use pile-up events to your advantage LISHEP 18 March 2013 N. Cartiglia, INFN Turin. 28

29 Pileup Analysis Technique The probability of having n pileup depends only on the visible σ(pp) cross section: If we count the number of pile-up events as a function of luminosity L, we can measure σ vis (pp). For an accurate measurement we need a large luminosity interval. LISHEP 18 March 2013 N. Cartiglia, INFN Turin. 29

30 Probability of n extra vertices depends upon σ P(n vertexes ) = (Lσ )n vertexes n vertexes! e ( Lσ ) Fit to σ LISHEP 18 March 2013 N. Cartiglia, INFN Turin. 30

31 Measurement of σ Inel using pile-up vertices P(n vertexes ) = (Lσ )n vertexes Extract σ assuming the pile-up follows a Poisson distribution n vertexes! e ( Lσ ) [mb] σ inel Total inelastic CMS - HF based CMS - Vtx based ATLAS TOTEM ALICE PYTHIA 6 CMS pp s = 7 TeV > 3 tracks > 2 tracks > 1 track ξ> PYTHIA 8 PYTHIA 8 + MBR PHOJET EPOS 1.99 QGSJET 01 QGSJET II-03 QGSJET II-04 SIBYLL 2.1 LISHEP 18 March 2013 N. Cartiglia, INFN Turin. 31

32 Collider experiments: measure σ inel by counting number of events The total inelastic proton-proton cross section is obtained by measuring the number of times opposite beams of protons hit each other and leave some energy in the most Hadronic Forward calorimeter (HF) E HF > 5 GeV is converted, using MC correction, into M x > 15 GeV (M 2 x /s = ξ > 5 * 10-6 ) LISHEP 18 March 2013 N. Cartiglia, INFN Turin. 32

33 Hadronic Forward Activity: analysis technique 1) p p 2) p p 1) Count the number of times (i.e. the luminosity, Ldt ) in which there could have been scattering, for example using beam monitors that signal the presence of both beams. 2) Measure the number of times there was a scattering, for example measuring a minimum energy deposition in the detector 3) Correct for detection efficiency ε 4) Correct for the possibility of having more than one scattering (pileup) Fpu. σ Inel = N Event F pu ε Ldt LISHEP 18 March 2013 N. Cartiglia, INFN Turin. 33 This method works only at low luminosity

34 Coverage of pileup and HF measurements Very small masses, invisible part What is escaping? >1 tracks All events? E>5 GeV LISHEP 18 March 2013 N. Cartiglia, INFN Turin. 34

35 Rapidity coverage and low mass states The difficult part of the measurement is the detection of low mass states (M x ). A given mass M x covers an interval of rapidity: Δη = - ln (M x2 /m p ) M x [GeV] Δη ξ = M x2 /s Escape ξ = M x2 /s characterizes the reach of a given measurement. LISHEP 18 March 2013 N. Cartiglia, INFN Turin. 35

36 A different method: σ TOT measured via optical theorem Optical theorem: elastic scattering at t =0! σ TOT B t dσ EL / dt = Ae t ρ = Ref el t=0 / Imf el t=0 LISHEP 18 March 2013 N. Cartiglia, INFN Turin. 36

37 Three basic type of results: 1) Elastic scattering Results 2) Comparison of the total value of the cross section between data and parameterizations as a function of the center-of-mass energy 3) Comparison of the value of parts of the cross section (elastic, diffractive, soft) with hadronic models (for example MCs) of pp interactions. LISHEP 18 March 2013 N. Cartiglia, INFN Turin. 37

38 TOTEM: pp cross section at 7 TeV Elastic cross section: σ el = 25.4±1.1 mb B = 19.9 GeV -2 Using the optical theorem: t -7.8 σ TOT = 98.6 mb ± 2.2 mb t dip = 0.53 GeV 2 And then: σ inel = σ TOT σ el EPL 96 (2011) To be published σ inel = 73.1 mb ± 1.3 mb LISHEP 18 March 2013 N. Cartiglia, INFN Turin. 38 Karsten Eggert p. 38

39 σ tot, σ inel, and σ el σ tot COMPETE (7 TeV) = 98 ± 5 mb σ tot COMPETE (8 TeV) = 101 ± 5 mb σ tot 2-pomeron (8 TeV) ~ 125 ± 5 mb σ tot TOTEM (7 TeV) = 98.6 ± 2.8 mb σ tot TOTEM (8 TeV) = ± 2.9 mb 133 ± 29 mb Auger 92 ± 14 mb σ inel TOTEM (7 TeV) = 73.1 ± 1.3 mb σ inel TOTEM (8 TeV) = 74.7 ± 1.7 mb σ el TOTEM (7 TeV) = 25.4 ± 1.1 mb σ el TOTEM (8 TeV) = 27.1 ± 1.4 mb σ el / σ tot (7 TeV) = ± σ el / σ tot (8 TeV) = ± 0.01 σ el / σ inel (7 TeV) = ± σ el / σ inel (8 TeV) = ± LISHEP 18 March 2013 N. Cartiglia, INFN Turin. 39

40 Compilation of inelastic pp cross section Auger LISHEP 18 March 2013 N. Cartiglia, INFN Turin. 40

41 σ inel for specific final states LHC experiments have measured the cross section for specific final states. These results are really useful to distinguish the importance of the various processes that are making up σ tot Very few models predict concurrently the correct values of σ for specific final states and σ Tot [mb] σ inel CMS pp s Total inelastic CMS - HF based CMS - Vtx based ATLAS TOTEM ALICE PYTHIA 6 > 3 tracks > 2 tracks > 1 track ξ>5 10 = 7 TeV -6 PYTHIA 8 PYTHIA 8 + MBR PHOJET EPOS 1.99 QGSJET 01 QGSJET II-03 QGSJET II-04 SIBYLL 2.1 LISHEP 18 March 2013 N. Cartiglia, INFN Turin. 41

42 Summary and outlook - I The study of the total cross section and its components is very active. A large set of new results have been presented in the last year: σ Tot (7 TeV), σ El (7 TeV), σ Ine (7 TeV), σ SD (7 TeV), σ DD (7 TeV) σ Tot (8 TeV), σ El (8 TeV), σ Ine (8 TeV) B slope and dip position of elastic scattering at 7 TeV σ Tot (57 TeV), σ Inel (57 TeV) σ Mx>15 (7 TeV), σ >1trk (7 TeV), σ 2trk (7 TeV), σ 3trk (7 TeV) LISHEP 18 March 2013 N. Cartiglia, INFN Turin. 42

43 Summary and outlook - II The value of the total cross section σ tot TOTEM (8 TeV) = ± 2.9 mb is well reproduced by the preferred COMPETE fits, σ tot COMPETE (8 TeV) = 101 ± 5 mb ( ~ ln 2 (s) ) while the 2-pomeron prediction, σ tot 2-pomeron (8 TeV) ~ 125 ± 5 mb, is disfavored. Commonly used MCs such as PYTHIA do not reproduce correctly the sub-components of the total cross section. LHC data at 7 & 8 TeV, together with cosmic-ray results, are becoming more and more precise, and they are constraining the available models. A very interesting contact is happening: measurements at LHC detectors are used to constrain cosmic-ray models, as finally collider energies are high enough: the extrapolation between 14 GeV and AUGER is the same as Tevatron! LHC. Please invite me back in 3 years, 14 TeV in 2015!! LISHEP 18 March 2013 N. Cartiglia, INFN Turin. 43

44 Reference 1. Several talks from the TOTEM home page: 2. Donnachie & Landshoff: 3. AUGER: 4. ALICE results, ISVHECRI 2012, Berlin, August D Enteria et al, Constraints from the first LHC data on hadronic event generators for ultra-high energy cosmic-ray physics 6. ATLAS 7. COMPETE collaboration (and reference in the linked page): 8. Many articles from the 13th Int. Conf. on Elastic and Diffractive Scattering CERN, confid=41547&view=standard&showdate=all&showsession=all&detaillevel =contribution LISHEP 18 March 2013 N. Cartiglia, INFN Turin. 44

45 EXTRA LISHEP 18 March 2013 N. Cartiglia, INFN Turin. 45

46 Experimental reach of t and β* Beam angular spread: σ(θ) ~ (1/β * ) Low t requires very small angular spread! very large β * October 24-25, 2012: β * : 11 " 90 " 500 " 1000m de- squeeze in 45 minutes Elastic cross section 2012: β * = 1000m Distance to beam < 1mm t-range for β*= 1km RPs at 3σ, ε = 2.4 µm β* = 1000m 2011: β* = 90m LISHEP 18 March 2013 N. Cartiglia, INFN Turin t / GeV 2

47 The Coulomb peak at t = 0 The t slope changes as a function of t value. Do no use: Coulomb part We need to measure this part Measurement of ρ by studying the Coulomb Nuclear interference region down to t ~ 6 x 10-4 GeV 2 LISHEP 18 March 2013 N. Cartiglia, INFN Turin. 47

48 Measuring ρ using the Coulomb part From Marco Bozzo LISHEP 18 March 2013 N. Cartiglia, INFN Turin. 48

Experimental coverage of rapidity ATLAS and CMS measure up to η = +- 5, which means they can reach values as low as ξ > 5 * 10-6 (Mx ~ 17 GeV) LHC detectors coverage ALICE covers -3.7 < η < 5.

49 Experimental coverage of rapidity ATLAS and CMS measure up to η = +- 5, which means they can reach values as low as ξ > 5 * 10-6 (Mx ~ 17 GeV) LHC detectors coverage ALICE covers -3.7 < η < 5.1 TOTEM has two detectors: T1: 3.1 < η < 4.7, T2: 5.3 < η < 6.5, ξ > 2 * 10-7 (Mx ~ 3.4 GeV) Main problem: from σ inel vis to the total value σ inel Solutions: 1) Don t do it 2) Put large error bars LISHEP 18 March 2013 N. Cartiglia, INFN Turin. 49

TOTEM: t-distribution of pp elastic scattering at @ 7 TeV The t-distribution measured by TOTEM was not predicted

50 TOTEM: t-distribution of pp elastic scattering 7 TeV The t-distribution measured by TOTEM was not predicted by any of the dynamical models of the proton LISHEP 18 March 2013 N. Cartiglia, INFN Turin. 50 Karsten Eggert p. 50

51 Predictions for 14 TeV (pre-lhc) J. R. Cudell: The measurement of the total cross section at the LHC will tell us a lot about the analytic structure of the amplitude, as there is a variety of predictions that span the region from 90 to 230 mb: σ tot > 200 mb: the only unitarisation scheme able to accommodate such a large number is the U matrix. It basically predicts the same inelastic cross section as more standard schemes, but the elastic cross section is much larger, and accounts for the difference. 120 mb < σ tot < 160 mb: this would be a clear signal for a two-pomeron model, and would also tell us about the unitarisation scheme. σ tot 110 mb: this is the standard prediction not only of the COMPETE fits, but also of many models based on a simple eikonal and only one pomeron pole. σ tot < 100 mb: this would indicate either the validity of double-pole parametrisations, or that of unitarisation schemes in which multiple-pomeron vertices are important. LISHEP 18 March 2013 N. Cartiglia, INFN Turin. 51

52 Cross Section Bounds Problem: the infinite rise of the cross section violates unitarity. The predictions have incorporated various processes and unitarity constrains that tame the rise of the value of the cross section. This process is called unitarization Froissart-Martin bound: σ TOT (s) <π/m 2 πlog 2 (s) However it s not a big deal for LHC: σ TOT < 4.3 barns Pumplin bound: σ El (s) < ½ σ TOT (s) σ El (s) ~ s 2ε σ Tot (s) ~ s ε At high energy: s 2ε > s ε Two-pomeron model without and with simple unitarization models LISHEP 18 March 2013 N. Cartiglia, INFN Turin. 52

53 TOTEM: Shrinkage and σ el / σ 7 TeV The shrinkage of the forward peak continues, the proton becomes larger and larger. The elastic component is becoming more important with energy B [GeV 2 ] pp, Ref. [8] p p, Ref. [8] TOTEM this publication el/ tot [%] pp p p TOTEM this publication p 10 4 s [GeV] p 4 s [GeV] LISHEP 18 March 2013 N. Cartiglia, INFN Turin. 53 Karsten Eggert p. 53

Elastic and inelastic cross section measurements with the ATLAS detector

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