Each LAC module has a multi layer structure with lead
sheets and scintillator bars, a configuration that provides the best agreement between
good energy resolution and high neutron detection efficiency requirements. It consists of
33 layers, each composed by a 0.20 cm thick lead foil and NE110A plastic scintillator bars
with average width 10 cm and constant thickness 1.5 cm. The module thickness corresponds
to 12.9 radiation lengths and 1.0 adsorption lengths. Teflon sheets with 0.2 mm thickness
separate scintillators from lead while 0.2 mm thick Teflon strips between each pair of
contiguous scintillators bars avoid optical crossover. Each layer is rotated by 90deg
to form a 40*24 matrix of 10*10 cm2 cells.
The
bar width increases going from the inner side toward the outer to guarantee the tapering
required by the CLAS geometry. The surface exposed to particle fluxes is 217*400 cm2.
The module is vertically divided into an inner and an outer part to improve electron/pion
discrimination. Scintillators lying (for the inner and outer part separately) one on top
of the other with the same orientation form 128 different stacks. The electromagnetic
shower originate in the lead sheets and propagate through the layers: the energy adsorbed
in the active material produces a light pulse that is collected at both scintillator ends
with a Lucite light guide coupled to scintillators with an air gap an a 7.0*0.4 cm2
area. Being the coupling area smaller than the scintillator cross section, the remaining
scintillator surface was protected with Teflon to prevent scratches from the aluminum
structure.
The collected light is summed
separately for each stack before a EMI 9945A photomultiplier. Therefore the light pulses
emitted from 8 different scintillators are summed up on a single photomultiplier that is
placed on the top surface of the LAC module several centimeters away from the
scintillators. To reduce photocatode non homogeneity effects, the light guides are glued
together before coupling to photomultiplier. Scintillators placed in the inner and the
outer parts are coupled to different photomultipliers. Monte Carlo simulations showed that
the LAC performances are strongly affected by the efficiency of light transmission and
collection. For this reason, special attention was devoted to the production of high
quality scintillators and light guides whose results have been already reported. In
particular, we selected scintillators with a light attenuation length longer than 300 cm
and light guides that provide about 5 photoelectrons/MeV when coupled to a EMI 9945A PMT.
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