It has been reported on several occasions that, during investigations in a scanning electron microscope (SEM), a reduction of secondary electron (SE) image brightness takes place on cooling high-Tc superconductors from room temperature to liquid nitrogen temperature. The SE image signal shows a continuous and initially slow decrease, then, when the specimen temperature is close to that of liquid nitrogen, a sudden drop (by about 15%) takes place. The effect appears to be reversible. Several hypotheses have been put forward to explain this effect; however, none is entirely satisfactory. Recent experimental results indicate that the effect is related to the residual atmosphere in the specimen chamber. To check this idea, a mass spectrometer was incorporated in an SEM. Combined mass spectroscopy and X-ray spectroscopy have proved that, during cooling, several gases condense on the specimen and form a spurious thin film on its surface, which reduces the SE emission. Subsequent specimen heating produces evaporation of the film, thus restoring the initial brightness of the signal.
Residual pressure effects on SEM/SE YBCO image brightness versus temperature
Monteverde F. T.;
1994
Abstract
It has been reported on several occasions that, during investigations in a scanning electron microscope (SEM), a reduction of secondary electron (SE) image brightness takes place on cooling high-Tc superconductors from room temperature to liquid nitrogen temperature. The SE image signal shows a continuous and initially slow decrease, then, when the specimen temperature is close to that of liquid nitrogen, a sudden drop (by about 15%) takes place. The effect appears to be reversible. Several hypotheses have been put forward to explain this effect; however, none is entirely satisfactory. Recent experimental results indicate that the effect is related to the residual atmosphere in the specimen chamber. To check this idea, a mass spectrometer was incorporated in an SEM. Combined mass spectroscopy and X-ray spectroscopy have proved that, during cooling, several gases condense on the specimen and form a spurious thin film on its surface, which reduces the SE emission. Subsequent specimen heating produces evaporation of the film, thus restoring the initial brightness of the signal.I documenti in IRIS sono protetti da copyright e tutti i diritti sono riservati, salvo diversa indicazione.


