The sampling imaging electromagnetic calorimeter comprises 44 singlesided silicon sensor planes (380 μ m thick) interleaved with 22 plates of tungsten absorber. Each tungsten layer has a thickness of 0.26 cm, which corresponds to 0.74 X_{0} (radiation lengths), giving a total depth of 16.3 X_{0} ( ~ 0.6 nuclear interaction lengths). Each silicon plane is composed of a 3x3 matrix of (8x8) cm^{2} silicon detectors, each segmented into 32 readout strips with a pitch of 2.4 mm. The orientation of the strips of two consecutive layers is orthogonal and therefore provides twodimensional spatial information..   The frontend is a developed version of a 16 channels CR1 chip with a peaking time of 2 ms, a linear dynamic range between 0.4 and 1200 MIPs, a sensitivity of 5 mV/MIP and a counting rate of 30 kHz. The total number of channels is 4416. The calorimeter has a mass of 110 Kg and a total power consumption of 75 W. 
 The longitudinal and transverse segmentation of the calorimeter, combined with the measurement of the particle energy loss in each silicon strip, allows a rejection power of electrons (in the antiprotons sample) and protons (in the positrons sample) is better than 10^{4} with an efficiency of 90%.
The calorimeter allows also to reconstruct the energy of the electromagnetic shower, providing a measurement of the energy of the incident electrons up to several hundred GeV with a resolution of the order of 5.5%. 
