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@article{
 title = {Investigation of the spin glass transition in a low U doped YRu 2 Si 2 sample},
 type = {article},
 year = {2003},
 identifiers = {[object Object]},
 pages = {4613-4621},
 volume = {15},
 websites = {http://stacks.iop.org/0953-8984/15/i=26/a=311?key=crossref.33f47e8e83acc6b9884a1000b9d8f85b},
 month = {7},
 day = {9},
 id = {216a58ab-2352-31cf-9921-692d5d53f230},
 created = {2016-12-15T10:02:47.000Z},
 file_attached = {false},
 profile_id = {12182ba0-f80b-33ff-8da5-1813b38b682d},
 group_id = {60cbc7ed-7d3c-385a-96b0-5920f1dfe2f9},
 last_modified = {2017-03-14T16:39:15.352Z},
 read = {false},
 starred = {false},
 authored = {false},
 confirmed = {true},
 hidden = {false},
 citation_key = {Ocko2003a},
 private_publication = {false},
 abstract = {We have made extensive studies of a dilute U doped YRu2Si2 alloy using several experimental techniques such as ac and dc magnetic susceptibility, dc resistivity and microstructural investigations. The real part of the ac susceptibility shows a maximum at around 6.75 K for f = 7 Hz. With increasing frequency, the temperature of this maximum increases while, at the same time, the magnitude of the maximum decreases, which is a typical spin glass behaviour. The magnitude of the imaginary part shows frequency-dependent behaviour too. We show that most of the imaginary part of the susceptibility, at least over the range of the frequencies we used, comes from the conduction electrons. Zero-field cooling and field cooling dc magnetization measurements also indicate the presence of a spin glass transition at about the same temperature. We also found that relaxation processes below the freezing temperature show ln(t + to) behaviour. We discuss our findings in light of the origin of the spin glass behaviour and compare them with other similar studies.},
 bibtype = {article},
 author = {Očko, M and Drobac, Đ. and Park, J-G and Samardzija, Z and Zadro, K},
 journal = {Journal of Physics: Condensed Matter},
 number = {26}
}