Spectra of electrons reflected from targets |
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Experimental
setup |
The stainless steel vacuum chamber withstands
bake-out up to 300°C. The vacuum system is oil-free: preliminary
pumping- by turbo-molecular pump; finally during experiment - by means
of two magneto-discharge pumps (with the turbo-molecular pump cut off).
Residual pressure during the experiment is kept below 10-6 Pa
with no hydrocarbons found with mass spectrometry. The probing electron beam of energy E0 is variable between 3 and 30 keV. The electron beam current is kept at a level of 125 mkA. Virtually no heating of target appears. The experiment geometry is such that the energy analyzer receives electrons reflected from the target surface at the angle J= 135° (that is 45° to the target’s normal). The energies of reflected electrons are detected by a 180° spherical electrostatic energy analyzer with a resolution DE/E0 = 0.8%. The voltage applied to the analyzer plates varies between 0 to 4 kV. The electrons passed through the analyzer proceed into a Faraday cup. The Faraday cup current (10-12 to 10-10A) is registered by an electrometric amplifier with an absolute resolution of 10-13A. Nb/Si and Nb/Al/Nb/Si targets have been prepared
on a Si(100) phosphorus-doped, 4.5 Ohm cm substrates using Leybold
L560 magnetron sputtering system (Moscow State University), at a
base pressure level of 2 10-5Pa. Before deposition
substrates were sputter cleaned in glow discharge of Ar at a
pressure of 0.5Pa for 150s. Subsequently, the sputtering of Nb and
Al has been carried out at Ar pressure of 1 Pa. The thicknesses of
the Nb and Al layers have been measured with a Taylor–Hobsen
profilometer and, independently, using the Michelson interferometry
method. Multiple measurements showed an error within 10%. The rates
of Nb and Al evaporation were found to be 2.34 and 0.16 nm/s,
respectively. |