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September 2012

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September 2012. Contin A., Laurenti G., Quadrani L., Bindi V., Palmonari F. Il Sistema TOF dell’esperimento AMS-02 sulla Stazione Spaziale Internazionale : prestazioni nello spazio e ricerca di materia oscura. Nicolo’ Masi Bologna University and INFN. Matter. - PowerPoint PPT Presentation
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Il Sistema TOF dell’esperimento AMS- Il Sistema TOF dell’esperimento AMS- 02 sulla Stazione Spaziale 02 sulla Stazione Spaziale Internazionale: prestazioni nello Internazionale: prestazioni nello spazio e ricerca di materia oscura spazio e ricerca di materia oscura September 2012 Nicolo’ Masi Nicolo’ Masi Bologna University and INFN Contin A., Laurenti G., Quadrani L., Bindi V., Palmonari F.
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Page 1: September 2012

Il Sistema TOF dell’esperimento AMS-02 Il Sistema TOF dell’esperimento AMS-02 sulla Stazione Spaziale Internazionale: sulla Stazione Spaziale Internazionale:

prestazioni nello spazio e ricerca di materia prestazioni nello spazio e ricerca di materia oscuraoscura

September 2012

Nicolo’ MasiNicolo’ Masi Bologna University and INFN

Contin A.,Laurenti G.,Quadrani L.,Bindi V., Palmonari F.

Page 2: September 2012

MatterMatter Anti-MatterAnti-Matter

An Improved Version of AMS-01

An Improved Version of AMS-01

AntimatterAntimatterAstrophysics, Dark Matter

Astrophysics, Dark Matter

StrangeletsStrangelets

Page 3: September 2012

Up in the SkyUp in the Sky

Page 4: September 2012

TOF consists of 4 plastic scintillator TOF consists of 4 plastic scintillator planes, 2 above and 2 below the planes, 2 above and 2 below the magnet.magnet.The counters of adjacent planes are The counters of adjacent planes are orthogonal.orthogonal.The number of counters per plane has The number of counters per plane has been reduced to 8, 8, 10, 8 counters to been reduced to 8, 8, 10, 8 counters to reduce the weight (34 scintillators). reduce the weight (34 scintillators).

Each TOF counter is composed by: Each TOF counter is composed by: • a plastic scintillator a plastic scintillator 1 cm thick and 1 cm thick and around 120 cm long (Eljen-Technology around 120 cm long (Eljen-Technology type: Ej-200), type: Ej-200), • read at both ends by 2 read at both ends by 2 independently powered independently powered photomultiplier tubes photomultiplier tubes (fine-mesh (fine-mesh Hamamatsu R5946 with max spectral Hamamatsu R5946 with max spectral response at 420 nm),response at 420 nm),• connected with transparent light connected with transparent light guidesguides..

Hamamatsu fine-mesh

R5946

On the ISSOn the ISS

Plateau for the trigger efficiency of one counter

Page 5: September 2012

Carbon Beta Resolution: 1.2% -> 48 ps

Longitudinal TOF-Trackercoordinate alignment

Page 6: September 2012
Page 7: September 2012

And physics beginsAnd physics begins

Page 8: September 2012

No Dark Matter Signal!No Dark Matter Signal!Clear Signal!Clear Signal!

….and AMS??….and AMS??

Page 9: September 2012

Primary CR Positron from Dark Matter

Primary CR Positron from Dark Matter

Page 10: September 2012

Light LZP provides

measurable fluxes for AMS-02

Light LZP provides

measurable fluxes for AMS-02

SUSY Wino, Little Higgs, KK Theory,

PBH, Singlet Scalar, Minimal DM…

SUSY Wino, Little Higgs, KK Theory,

PBH, Singlet Scalar, Minimal DM…

With e+ and low energy antideuteron we can probe

With e+ and low energy antideuteron we can probe

Page 11: September 2012

Total Flux High Energy

Antiproton High Energy Signal

from KK particle

Antiproton High Energy Signal

from KK particle

Page 12: September 2012

Discrimination parameter I𝜙 for signal and background: the AMSB Wino MSSM

is the most suitable for AMS-02, both in antiproton and positrons channel

Discrimination parameter I𝜙 for signal and background: the AMSB Wino MSSM

is the most suitable for AMS-02, both in antiproton and positrons channelExpected

clear positron signal from heavy Wino

Expected clear positron

signal from heavy Wino

Page 13: September 2012

The region above the line can be distinguished from the

background.

The region above the line can be distinguished from the

background.

Wide range of the parameter space, including the region BF = 1Wide range of the parameter space, including the region BF = 1

95% C. L. contour within WMAP constraint for Little Higgs Dark

Matter parameters space

95% C. L. contour within WMAP constraint for Little Higgs Dark

Matter parameters space

e+

Page 14: September 2012

Parameters space explorable by AMS-02 in the

antiproton channel

Parameters space explorable by AMS-02 in the

antiproton channel

Goudelis - Antimatter signals of singlet scalar dark matter

Page 15: September 2012

Always promising positron search

Always promising positron search

Page 16: September 2012

Kinetic Energy (GeV)

Page 17: September 2012

The hadronic Low Energy region is realistically obsolete and has been replaced with a High Energy research.

In function of AMS-02 performances, an hadronic research related to very heavy DM particle is ongoing, to restart from PAMELA data. This would be the most significant signal of new particle physics, even cleaner and clearer than the leptonic one.

The positron signal, on the other hand, is of course the fundamental channel for DM study. In terms of intensity of annihilation products fluxes, AMS-02 can see a positron peak for all DM candidates capable of producing e+ beyond 100 GeV.

ConclusionsConclusions

Page 18: September 2012

Antiproton & Antideuteron Search :

Dark Matter Parameters Space for a non-

leptophilic candidate:

Just a little patience!


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