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The existence of a stable vacuum at the end point of the condensation process depends on a modulus representation under the gauge group.
Its high current operation of intermediate charge state ions requires stable vacuum pressures < 10-12 mbar under dynamic machine conditions which are only achievable when the whole beam pipe is used as an huge cryopump.
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The mobility was very stable in vacuum by exhibiting 2% variation after 6 h stress even under the high gate bias stress of VGS = − 20 V.
Experimental results indicate that the coating is highly stable in vacuum at 500 °C for 100 h with a good solar selectivity of 0.92/0.11.
While the trans conformers in glycine-like coordination are the most stable in vacuum, conformers in all coordination modes are predicted within 15 kJ mol−1 in aqueous solution.
These films are thermally stable after vacuum annealing at 600 °C, the main structural changes being related to a defect annihilation and crystal recovery, leading to the development of a net tensile stress.
The chemisorbed layer consists of a mixture of species related to CH3CN and acetamide (CH3CONH2), contains about θ = 0.15 molecules per surface Pt atom is stable in vacuum and in solution over a wide range of electrode potentials, is replaced only slowly by other strong adsorbates such as iodide and lacks long-range order in the absence of anions such as iodide.
To keep the surface stable, ultra-high vacuum is needed.
The films remain stable under high vacuum conditions.
Still, both Branchina and Ellis say that based on other arguments, they suspect that something does make the vacuum stable.
The investigation indicates that this ionic liquid is highly stable in a vacuum and under argon flow.
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