Reduction of outgassing rate from residual gas analyzers for extreme high vacuum measurements

1996 ◽  
Vol 14 (6) ◽  
pp. 3261-3266 ◽  
Author(s):  
Shu Watanabe ◽  
Masakazu Aono ◽  
Shigeki Kato
2018 ◽  
Vol 25 (1) ◽  
pp. 72-76 ◽  
Author(s):  
Philip Heimann ◽  
Stefan Moeller ◽  
Sergio Carbajo ◽  
Sanghoon Song ◽  
Georgi Dakovski ◽  
...  

For the LCLS-II X-ray instruments, laser power meters are being developed as compact X-ray power diagnostics to operate at soft and tender X-ray photon energies. These diagnostics can be installed at various locations along an X-ray free-electron laser (FEL) beamline in order to monitor the transmission of X-ray optics along the beam path. In addition, the power meters will be used to determine the absolute X-ray power at the endstations. Here, thermopile power meters, which measure average power, and have been chosen primarily for their compatibility with the high repetition rates at LCLS-II, are evaluated. A number of characteristics in the soft X-ray range are presented including linearity, calibrations conducted with a photodiode and a gas monitor detector as well as ultra-high-vacuum compatibility tests using residual gas analysis. The application of these power meters for LCLS-II and other X-ray FEL sources is discussed.


Vacuum ◽  
1987 ◽  
Vol 37 (3-4) ◽  
pp. 335-338 ◽  
Author(s):  
F.M. Mao ◽  
J.M. Yang ◽  
W.E. Austin ◽  
J.H. Heck

1999 ◽  
Vol 70 (3) ◽  
pp. 1880-1884 ◽  
Author(s):  
Shu Watanabe ◽  
Hitoshi Oyama ◽  
Shigeki Kato ◽  
Masakazu Aono

The emission of ions from incandescent solids has been studied by many investigators. The value of e/m , the ratio of the charge to the mass, for the carriers of negative electricity was first measured by Sir J. J. Thomson in the case of a carbon filament heated in a high vacuum. Other observers have since determined the value of this quantity for the negative ions emitted by different incandescent solids, and all agree that the carriers are negatively electrified corpuscles identical in mass from whatever substance they are produced. The investigation of the nature of the carriers of positive electricity emitted by glowing solids presents greater difficulties, owing to the variability of the amount of the positive ionisation produced under different conditions, the causes of which are not yet fully understood. The first measurements of the value of the specific charge of these ions were made by Sir J. J. Thomson, who found e/m = 10 4 /25 for the positive ions from a heated iron wire. Later, experimenting with a strip of platinum foil which had already been heated for some hours in a high vacuum, he obtained the value e/m = 10 4 /27 for the majority of the carriers of positive electricity from that metal. The positive ions thus seem to have the same mass, about 26 times that of the hydrogen atom, in the two cases. This value suggested to Sir J. J. Thomson that they might be molecules of CO or of N 2 , either of which has a mass about 28 times that of the hydrogen atom, so that it would be impossible to distinguish between these two gases by a determination of e/m alone. When a luminous discharge was passed through the residual gas in the tube after the experiments with platinum, the band spectrum of carbon monoxide was obtained, and it was concluded that molecules of this gas acted as the carriers of positive electricity from the glowing metal.


Author(s):  
C. T. Homg ◽  
R. W. Vook

Smooth (111) single crystal Cu films (1200Å) were evaporated on NaCl/mica in an ultra-high vacuum RHEED systemI (base pressure ≤1×10−9 torr) The total residual gas pressure during Cu evaporation was less than 1×10−8 torr. These Cu films served as substrates for thin epitaxial monolayer Ag growth ranging in thickness from 1Å to 20Å, as measured by a quartz thickness monitor. These Ag-Cu bilayers were formed and examined in-situ in the RHEED system.The unusual RHEED patterns first re orted by Gradmann and Krause were observed in the present work up to l0Å of Ag. Beyond 10Å, only Ag and Cu lines plus double diffraction effects were detected. A typical example of the former is given in Fig. 1. The pattern was previously interpreted as due to a two dimensional grid of interfacial dislocations.


Author(s):  
C. T. Horng ◽  
R. W. Vook

Very smooth (111) single crystal Cu films (1200Å) were evaporated on NaCl/mica in an ultra-high vacuum RHEED system at residual gas pressures of less than 1×10−8 torr. These Cu films served as substrates for thin epitaxial monolayer Ag overgrowth. Film thicknesses were measured by a quartz thickness monitor. These Ag-(111)Cu bilayer films were formed and examined in-situ in the RHEED system and subsequently by TEM.


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