New idea for the target detector: SuperFGD

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Presentation transcript:

New idea for the target detector: SuperFGD Davide Sgalaberna “Neutrino Near Detector” Workshop, Tokai 20/5/17

FGD-like detector X-Y plastic scintillator bars (1cm2 cross section) Need tracks crossing at least 4 transversal layers Need at least 6 hits: >5cm track length (not ideal for protons) Reconstruction not reliable at |cosƟ|<0.3 Ambiguity in 3D track reconstruction Not optimized for a accurate measurement of e+e- conversion in FV No low energy protons From TN-245 Need a full 3D detector (no XY bars) to obtain a precise 4π acceptance Also need a very good PID --> proton/pion separation is very important (WAGASCI not optimal for PID) A water target is useful only if we can do still a very good job OK

FGD-like detector X-Y plastic scintillator bars (1cm2 cross section) Need tracks crossing at least 4 transversal layers Need at least 6 hits: >5cm track length (not ideal for protons) Reconstruction not reliable at |cosƟ|<0.3 Ambiguity in 3D track reconstruction Not optimized for a accurate measurement of e+e- conversion in FV No low energy protons OK Need a full 3D detector (no XY bars) to obtain a precise 4π acceptance Also need a very good PID --> proton/pion separation is very important (WAGASCI not optimal for PID) A water target is useful only if we can do still a very good job

Goals Fully active plastic scintillator detector 4pi acceptance track reconstruction Provide 3D reconstruction, i.e. 3 projections-2D (FGD has 2 projections): ability to solve the track hits ambiguity Fine granularity --> track reconstruction down to 300 MeV/c or below for protons Very good PID --> high light yield

SuperFGD Idea of Davide Sgalaberna and Andrea Longhin 1cm 1cm Standard plastic scintillator Light collected by 3 fibers --> Tot # of p.e. ~x3 than (needs teste) Each cube coated with TiO2 to keep light entrapped inside the cube --> may expect better light yield than long plastic bar (needs test) 1 particle interaction (energy released) would produce light collected in the 3 fibers at the same time --> 1 track interaction = 1 hit!!!

SuperFGD Idea of Davide Sgalaberna and Andrea Longhin 1cm 1cm Standard plastic scintillator Light collected by 3 fibers --> Tot # of p.e. ~x3 than (needs teste) Each cube coated with TiO2 to keep light entrapped inside the cube --> may expect better light yield than long plastic bar (needs test) 1 particle interaction (energy released) would produce light collected in the 3 fibers at the same time --> 1 track interaction = 1 hit!!!

SuperFGD 1 cm3 Possible cross talks: - between cubes through the coating: should be same as standard plastic scintillator bars Cross talk along the fiber holes is not a problem: - light has same direction as the one collected by the fiber transported toward the fiber-end - should be limited given the small hole size Tests needed to confirm the expectation

Tracking How easy is separating tracks? Not a real 3D detector but we have 3 projections (XY, XZ, YZ) It should be enough to solve the ambiguity of several tracks in the same XZ layer X X X X X X X X Z Y X X X = hit in MPPC - = WLS fiber X X X

Simulation of SuperFGD Muon particle gun: Ekin=400 MeV, Along Z axis # of p.e. / cm (MIP) ~ 30-40 p.e. / fiber ~x2 than FGD because of new MPPC But we have 3 fibers / cm3 --> ~100 p.e./cm Expect very good PID (>~100 p.e. / cm for MIP) and tracking (1cm on the single hit, better than FGD, FGD3D or water- WAGASCI)

Simulation of SuperFGD Gamma particle gun: Ekin=400 MeV Gamma is well detected inside the target and visible in all the projections

Mechanical constraints For 1.8x0.6x1.3 m3, ~1.5 tons: Size cube 1 cm3 1.5 cm3 2 cm3 # of channels channels ~42k ~18.7k ~10.5k # of cubes 180x60x130 ~1.4M 120x40x87~420k 90x65x30 ~175k fiber length ~42km ~18.7km ~10km Discussed with Franck Cadoux (mechanical engineer at UniGe): 1) cut standard plastic scintillator bars in many cubes 2) coating on each cube, put in a bath of TiO2 3) make holes by drilling on XYZ 4) gluing cubes is not needed: cubes inside a box closed by screw 5) when assembling pull the fibers inside all the holes with standard techniques used by electricians: take a rigid row with the fiber glued on one end and pull through all the holes. Steps 1), 2) and 3) should be done in serie by a company. More expensive costs probably still dominated by the electronics Approximative cost is ~2-3M$ (dominated by electronics)

Conclusions SuperFGD seems a good idea for: - fully active detector - 4π acceptance - good tracking - good PID Production not as simple as FGD-like detector, but possible Many things should be tested to check its real behavior Best would be a small prototype (e.g. 5x5x5 cm3) for test beam - 125 cubes - 75 readout channels Low costs. Pieces (e.g. plastic, fibers, MPPC) could be recycled Joint efforts of different institutes my reduce costs even more

BACKUP

Option 1: Fully active WAGASCI WAGASCI structure + LS (also Water-based LS) Need WLS fiber immersed in LS REFLECTIVE COATING WLS FIBERS Z Y X 3 WLS fibers for each scintillator bar In order to let the fibers going for ~2m 3D --> small holes (1-2mm) in crossing bars

Option 1: Fully active WAGASCI X Z - Since in Z we don’t have a - This bars need (Z) needs a WLS on both sides --> interaction in LS gives automatically 2 hits along Z --> this coordinate is defined - Same as WAGASCI reconstruction but only for Z coordinate

B.Quilan - HK collaboration meeting – ND session (2016/01/31) ~17E/ch 1JPY ~ 121E ~ 112$ ~33E/ch Cost of Fully active WAGASCI ~ WAGASCI x 2 1target (2x2x0.6 m3 - 1cm3 cube) --> ~64k channels --> $ ~3-4M Prices are getting lower --> estimation is conservative and may be lower by 2