A new approach to suppress ion backflow in multi-GEM structures is suggested.
In this approach, the potential difference applied across the gap between two
adjacent GEMs is reversed compared to the standard configuration. In such a gap
structure, called Electric Gate, a signal transfer from the first to second GEM
is presumably provided by the small residual field still existing at small gate
voltages and connecting the holes of the two GEMs. On the other hand, ion
backflow between the GEMs turned out to be substantially reduced. We also
consider another configuration, called Photoelectric Gate, in which in addition
to the Electric Gate configuration, a CsI photocathode is deposited on the
second GEM. In the Photoelectric Gate, ion backflow through the gap is fully
suppressed and the signal transfer through the gap is provided by the
photoelectric mechanism due to either avalanche scintillations in the first GEM
or proportional scintillations in the electroluminescence gap replacing the
first GEM. The idea of the Electric Gate might find applications in the field
of TPC detectors and gas photomultipliers. The idea of the Photoelectric Gate
is more relevant in the field of two-phase avalanche detectors.Comment: 12 pages, 14 figures. Submitted to JINS