First data from TOTEM experiment at LHC - PowerPoint PPT Presentation

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First data from TOTEM experiment at LHC

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First data from TOTEM experiment at LHC Fabrizio Ferro - INFN Genova TOTEM phyics Total pp cross section Physics with high b* optics Physics with low b* TOTEM ... – PowerPoint PPT presentation

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Title: First data from TOTEM experiment at LHC


1
First data from TOTEM experiment at LHC
  • Fabrizio Ferro - INFN Genova

2
TOTEM phyics
Diffraction soft and hard (with CMS)
3
Total pp cross section
Current models predict for 14 TeV 90 130
mb Aim of TOTEM 1 First year 5
Luminosity independent method
special optics
4
Physics with high b optics
log(t)/Gev2
-t 410-4 0.012
0.3 2.5
  • Total cross section measurement at 5 (1)
  • Elastic scattering 0.0004lttlt 2.5 GeV2
  • Soft diffraction all masses - 65 of
    diffractive protons seen
  • Classification of inelastic events rates
    multiplicity

5
Physics with low b
Single diffraction
ds/dM 0.025ltxlt0.15 1 lt M lt 3 TeV s(M)/M
2 - 5
Acceptance
Central diffraction
ds/dM 200 lt M lt 1000 GeV s(M)/M 2 - 5

Log M(GeV)
Elastic scattering
0.5lt t lt 5 GeV2 s(t) 0.2v t
6
TOTEM detectors
Telescopes
10.5 m
TAS
14 m
Roman Pot stations in the LHC tunnel
RP (147 m)
RP (220m)
7
T1 telescope (1)
2 arms of CSCs for track and vertex
reconstruction 3.1lthlt4.7 - Df2p
  • Both T1 arms on the test line. Ready for
    installation.

8
T1 telescope (2)
Both arms successfully tested with pion and muon
beams Pions on copper target to get many-tracks
events
? reconstructed hits
efficiency
CSC efficiencies with muons ?(triple coincidences)
Longitudinal vertex
Transverse vertex
9
T2 telescope
2 arms of GEMs for tracks and vertex
reconstruction
3.1lthlt4.7 - Df2p
Both arms installed and taking data
10
T2 event at 7 TeV
11
Alignment and vertex reconstruction
Before
RMS1.7cm
RMS3.1m
RMS1.4cm
After
RMS0.8cm
RMS1.0cm
RMS2.3m
12
h distribution
Tracks pointing to vertex Statistical error
only
BeamPipe cone at h5.53
13
TOTEM Roman Pots
14
Roman pot alignment
  • Critical and fundamental for any physics
    measurement
  • To align proton detectors means
  • Resolve misalignments within detector assembly
    ? methods local track
  • Resolve relative positions of the pot


    principal information source motor control (?
    calibration, reliability, )
  • ? method local track based (detector
    overlap)
  • Resolve position of beam (uncertainties and
    variations of optics)
  • ? method profiles from physics events,
    Beam Halo
    Cross-check
    Beam Position Monitors Alignment with
    collimators
  • Resolve left-right position
  • ? method global (elastic) track based

15
Roman Pot alignment (at 20s)
Vertical alignment
sectors 5-6 (IP5 minus side)
sectors 4-5 (IP5 plus side)
Tracks in horizontal pot
Tracks in horizontal pot
preliminary
preliminary
16
Roman Pot alignment (at 20s)
Horizontal alignment
sectors 5-6 (IP5 minus side)
sectors 4-5 (IP5 plus side)
preliminary
preliminary
Halo protons
Tracks in horizontal pot
Tracks in vertical pot
17
Diffractive protons at 7 TeV
preliminary
TOP BOTTOM
Raw distributions, no selection Diffractive
protons background Estimated Dp/p 0.06 -
0.12
preliminary
18
A first elastic scattering candidate
RPs at 25s
Run 1964.004 Event 13682
19
Analysis and data taking still in progress
Data taking with RP at 25s collected 3 M
events with RP only
5 M
RP T2 Data taking with RP at 20s
collected 6 M RP T2 Data taking with
RP at 15s under investigation with the machine
Full set of systematics sources under
investigation - Alignment - Beam position
- Beam divergence - Background from the machine
(halo, beam gas,.....) - Multiple scattering and
material interaction - Optics uncertainty on
the optical functions, crossing angle,
vertex.... and in addition - Estimate
Efficiencies (trigger, track reconstruction....)
- Luminosity - Physics Background Pile-up
20
Summary
  • The TOTEM Detectors installed in the LHC (RP220m
    and T2) have completed the commissioning and are
    presently taking data
  • Once that the 220m RPs will be inserted at their
    nominal position, TOTEM can move on to its physic
    program at low b
  • - high mass Single Central Diffraction
  • - large t elastic scattering (0.65 lt t
    lt 5 GeV2)
  • - forward density of charged particles
  • Precise measurements of elastic, diffractive and
    total cross sections
  • require high b optics and the installation of T1
    and of RP147m
  • - Elastic scattering in a wider t range
  • - Diffractive physics over a larger
    rapidity range 3.1 lth lt 6.5
  • - Single and Central Diffraction at any
    mass
  • - Measurement of stot with a precision of
    5 (1)
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