obtain with SE. The conventional BSE detection means have been adapted to operate in the gaseous conditions of the ESEM. The BSE having a high energy are self-propelled to the corresponding detector without significant obstruction by the gas molecules. Already, annular or quadrant solid-state detectors have been employed for this purpose but their geometry is not easily adaptable to the requirements of ESEM for optimum operation. As a result, no much use has been reported of these detectors on genuine ESEM instruments at high pressure. The "Robinson" BSE detector is tuned for operation up to around 100 Pa at the usual working distance of conventional SEM for the suppression of specimen charging, whilst electron collection at the short working distance and high pressure conditions make it inadequate for the ESEM. However, plastic scintillating materials being easily adaptable have been used for BSE and made to measure according to the strictest requirements of the system. Such work culminated in the use of a pair of wedge-shaped detectors saddling a conical PLA1 and abutting to its rim, so that the dead detection space is reduced to a minimum, as shown in the accompanying figure of optimum BSE detectors. The photon conduction is also optimized by the geometry of the light pipes, whilst the pair of symmetrical detectors allow the separation of topography (signal subtraction) and atomic number contrast (signal addition) of the specimen surface to be displayed with the best ever signal-to-noise-ratio. This scheme has further allowed the use of color by superimposing various signals in a meaningful way. These simple but special detectors became possible in the conditions of ESEM, since bare plastic does not charge by the BSE. However, a very fine wire mesh with appropriate spacing has been proposed as a GDD when gas is present and to conduct negative charge away from the plastic detectors when the gas is pumped out, towards a universal ESEM. Furthermore, since the associated electronics involve a photomultiplier with a wide frequency response, true TV scanning rates are readily available. This is an essential attribute to maintain with an ESEM that enables the examination of processes in situ in real time. In comparison, no such imaging has been reported with the electron avalanche mode of the GDD yet. The use of scintillating BSE detectors in ESEM is compatible with the GDD for simultaneous SE detection, in one way by replacing the top plane