Title: First data from TOTEM experiment at LHC
1First data from TOTEM experiment at LHC
- Fabrizio Ferro - INFN Genova
2TOTEM phyics
Diffraction soft and hard (with CMS)
3Total pp cross section
Current models predict for 14 TeV 90 130
mb Aim of TOTEM 1 First year 5
Luminosity independent method
special optics
4Physics 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
5Physics 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
6TOTEM detectors
Telescopes
10.5 m
TAS
14 m
Roman Pot stations in the LHC tunnel
RP (147 m)
RP (220m)
7T1 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.
8T1 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
9T2 telescope
2 arms of GEMs for tracks and vertex
reconstruction
3.1lthlt4.7 - Df2p
Both arms installed and taking data
10T2 event at 7 TeV
11Alignment and vertex reconstruction
Before
RMS1.7cm
RMS3.1m
RMS1.4cm
After
RMS0.8cm
RMS1.0cm
RMS2.3m
12h distribution
Tracks pointing to vertex Statistical error
only
BeamPipe cone at h5.53
13TOTEM Roman Pots
14Roman 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
15Roman 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
16Roman 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
17Diffractive protons at 7 TeV
preliminary
TOP BOTTOM
Raw distributions, no selection Diffractive
protons background Estimated Dp/p 0.06 -
0.12
preliminary
18A first elastic scattering candidate
RPs at 25s
Run 1964.004 Event 13682
19Analysis 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
20Summary
- 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)