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Sharov, B.V.; Smirnov, O. A.

doi:10.1023/a:1011310819964

Cited by 2 publications

(2 citation statements)

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“…The beam diameter was 2.3 mm. The surface structure of the alloy was ana lyzed by optical (Olympus) and scanning electron (Philips SEM 515) microscopy, measuring the ther mopower [25], PMT 3 microhardness tester equipped with a Vickers indenter, and nanoindentation (Nano Hardness Tester, CSEM) [26]. To study the structurephase composition (character and number of phases, internal stresses, texture), we used X ray diffraction and a Shimadzu XRD 6000 diffractometer (CuK α radiation).…”

Section: Methodsmentioning

confidence: 99%

Properties and structural state of the surface layer in a zirconium alloy modified by a pulsed electron beam and saturated by hydrogen

et al. 2012

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A pulsed action of an electron beam on a Zr-1% Nb zirconium alloy is studied. Alloy samples are irradiated by three 50 μs pulses at an energy density of 15-25 J/cm 2 , a power of (3-6) × 10 4 W/cm 2 , a current density of 10-50 A/cm 2 , and an electron energy of 18 keV. This method of processing is found to modify the surface layer of the alloy without changing the structure-phase state of its volume. This surface modification increases the hydrogen saturation resistance of the alloy.

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Section: Methodsmentioning

confidence: 99%

Properties and structural state of the surface layer in a zirconium alloy modified by a pulsed electron beam and saturated by hydrogen

et al. 2012

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“…The objective of this measurement was to study the effect of absorbed hydrogen on the thermoelectric power as expressed by the Seebeck coefficient [19,20]. The thermopower, an intrinsic property of a material, characterizes the electronic density of states at the Fermi level: the amount of electric charge and the type of charge carrier.…”

Section: Thermopower Measurementsmentioning

confidence: 99%