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High Temperature Material Processes: An International Quarterly of High-Technology Plasma Processes

Publication de 4  numéros par an

ISSN Imprimer: 1093-3611

ISSN En ligne: 1940-4360

The Impact Factor measures the average number of citations received in a particular year by papers published in the journal during the two preceding years. 2017 Journal Citation Reports (Clarivate Analytics, 2018) IF: 0.4 The Immediacy Index is the average number of times an article is cited in the year it is published. The journal Immediacy Index indicates how quickly articles in a journal are cited. Immediacy Index: 0.1 The Eigenfactor score, developed by Jevin West and Carl Bergstrom at the University of Washington, is a rating of the total importance of a scientific journal. Journals are rated according to the number of incoming citations, with citations from highly ranked journals weighted to make a larger contribution to the eigenfactor than those from poorly ranked journals. Eigenfactor: 0.00005 The Journal Citation Indicator (JCI) is a single measurement of the field-normalized citation impact of journals in the Web of Science Core Collection across disciplines. The key words here are that the metric is normalized and cross-disciplinary. JCI: 0.07 SJR: 0.198 SNIP: 0.48 CiteScore™:: 1.1 H-Index: 20

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SIMULATION OF PHASE TRANSITIONS INDUCED IN CdTe BY PULSED LASER RADIATION

Volume 18, Numéro 4, 2014, pp. 291-298
DOI: 10.1615/HighTempMatProc.2015015699
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RÉSUMÉ

Numerical simulation of the processes of melting and solidification under the action of nanosecond ruby laser on CdTe is carried out with account for the diffusion of components in the melt and their evaporation from the surface. It is shown that intense cooling of the surface of the material as a result of the evaporation of cadmium atoms leads to the formation of a nonmonotonic profile of the temperature field with a maximum temperature in the semiconductor at a distance of ~20 nm from the surface. The value of the threshold energy density required for the melt exit on the surface may exceed the energy density required for the formation of the latent melt layer by about 15−20%.

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