A calorimetric investigation of RbFeb>2b>Asb>2b> single crystals
详细信息    查看全文
文摘
We present properties of single crystals of the iron pnictide superconductor RbFeb>2b>Asb>2b> grown using a self-flux method. A bulk superconducting transition at on-construct="true" class="math-equation-construct">on-image="true" class="math-equation-image">on-mathml="true" class="math-equation-mathml" style="display:none">org/1998/Math/MathML">b xmlns:w="http://www.wiley.com/namespaces/wiley" xmlns:wiley="http://www.wiley.com/namespaces/wiley/wiley" xmlns:cr="urn://wiley-online-library/content/render" xmlns="http://www.w3.org/1998/Math/MathML">Tcb> on-construct="true" class="math-equation-construct">on-image="true" class="math-equation-image">on-mathml="true" class="math-equation-mathml" style="display:none">org/1998/Math/MathML">o xmlns:w="http://www.wiley.com/namespaces/wiley" xmlns:wiley="http://www.wiley.com/namespaces/wiley/wiley" xmlns:cr="urn://wiley-online-library/content/render" xmlns="http://www.w3.org/1998/Math/MathML">∼o>2.6 K was consistently observed in resistivity, magnetic susceptibility, and specific heat measurements. While the resistivity behaves like a conventional metal at low T, the magnetic susceptibility shows an unusual broad maximum around 80 K in the normal state. A large Sommerfeld coefficient, on-construct="true" class="math-equation-construct">on-image="true" class="math-equation-image">on-mathml="true" class="math-equation-mathml" style="display:none">org/1998/Math/MathML">b xmlns:w="http://www.wiley.com/namespaces/wiley" xmlns:wiley="http://www.wiley.com/namespaces/wiley/wiley" xmlns:cr="urn://wiley-online-library/content/render" xmlns="http://www.w3.org/1998/Math/MathML">γ0b>o xmlns:w="http://www.wiley.com/namespaces/wiley" xmlns:wiley="http://www.wiley.com/namespaces/wiley/wiley" xmlns:cr="urn://wiley-online-library/content/render" xmlns="http://www.w3.org/1998/Math/MathML">=o>om/namespaces/wiley" xmlns:wiley="http://www.wiley.com/namespaces/wiley/wiley" xmlns:cr="urn://wiley-online-library/content/render" xmlns="http://www.w3.org/1998/Math/MathML">127om/namespaces/wiley" xmlns:wiley="http://www.wiley.com/namespaces/wiley/wiley" xmlns:cr="urn://wiley-online-library/content/render" xmlns="http://www.w3.org/1998/Math/MathML" width="thinmathspace">om/namespaces/wiley" xmlns:wiley="http://www.wiley.com/namespaces/wiley/wiley" xmlns:cr="urn://wiley-online-library/content/render" xmlns="http://www.w3.org/1998/Math/MathML" mathvariant="normal">mJo xmlns:w="http://www.wiley.com/namespaces/wiley" xmlns:wiley="http://www.wiley.com/namespaces/wiley/wiley" xmlns:cr="urn://wiley-online-library/content/render" xmlns="http://www.w3.org/1998/Math/MathML">/o>om/namespaces/wiley" xmlns:wiley="http://www.wiley.com/namespaces/wiley/wiley" xmlns:cr="urn://wiley-online-library/content/render" xmlns="http://www.w3.org/1998/Math/MathML">ow>ormal">molKow>2, was observed seemingly a common feature of heavily hole-doped &ldquo;122&rdquo; compounds. In the superconducting state, we analyzed our specific heat data based on the s- and d-wave two-gap models. The presence of the small gap with 2on-construct="true" class="math-equation-construct">on-image="true" class="math-equation-image">on-mathml="true" class="math-equation-mathml" style="display:none">org/1998/Math/MathML">b xmlns:w="http://www.wiley.com/namespaces/wiley" xmlns:wiley="http://www.wiley.com/namespaces/wiley/wiley" xmlns:cr="urn://wiley-online-library/content/render" xmlns="http://www.w3.org/1998/Math/MathML">Δ1b>o xmlns:w="http://www.wiley.com/namespaces/wiley" xmlns:wiley="http://www.wiley.com/namespaces/wiley/wiley" xmlns:cr="urn://wiley-online-library/content/render" xmlns="http://www.w3.org/1998/Math/MathML" stretchy="false">(o>om/namespaces/wiley" xmlns:wiley="http://www.wiley.com/namespaces/wiley/wiley" xmlns:cr="urn://wiley-online-library/content/render" xmlns="http://www.w3.org/1998/Math/MathML">0o xmlns:w="http://www.wiley.com/namespaces/wiley" xmlns:wiley="http://www.wiley.com/namespaces/wiley/wiley" xmlns:cr="urn://wiley-online-library/content/render" xmlns="http://www.w3.org/1998/Math/MathML" stretchy="false">)o>/on-construct="true" class="math-equation-construct">on-image="true" class="math-equation-image">on-mathml="true" class="math-equation-mathml" style="display:none">org/1998/Math/MathML">b xmlns:w="http://www.wiley.com/namespaces/wiley" xmlns:wiley="http://www.wiley.com/namespaces/wiley/wiley" xmlns:cr="urn://wiley-online-library/content/render" xmlns="http://www.w3.org/1998/Math/MathML">kBb>b xmlns:w="http://www.wiley.com/namespaces/wiley" xmlns:wiley="http://www.wiley.com/namespaces/wiley/wiley" xmlns:cr="urn://wiley-online-library/content/render" xmlns="http://www.w3.org/1998/Math/MathML">Tcb>o xmlns:w="http://www.wiley.com/namespaces/wiley" xmlns:wiley="http://www.wiley.com/namespaces/wiley/wiley" xmlns:cr="urn://wiley-online-library/content/render" xmlns="http://www.w3.org/1998/Math/MathML"><o>om/namespaces/wiley" xmlns:wiley="http://www.wiley.com/namespaces/wiley/wiley" xmlns:cr="urn://wiley-online-library/content/render" xmlns="http://www.w3.org/1998/Math/MathML">1 was discussed to account for the large specific heat contribution remaining to low T far below on-construct="true" class="math-equation-construct">on-image="true" class="math-equation-image">on-mathml="true" class="math-equation-mathml" style="display:none">org/1998/Math/MathML">b xmlns:w="http://www.wiley.com/namespaces/wiley" xmlns:wiley="http://www.wiley.com/namespaces/wiley/wiley" xmlns:cr="urn://wiley-online-library/content/render" xmlns="http://www.w3.org/1998/Math/MathML">Tcb>. The large on-construct="true" class="math-equation-construct">on-image="true" class="math-equation-image">on-mathml="true" class="math-equation-mathml" style="display:none">org/1998/Math/MathML">b xmlns:w="http://www.wiley.com/namespaces/wiley" xmlns:wiley="http://www.wiley.com/namespaces/wiley/wiley" xmlns:cr="urn://wiley-online-library/content/render" xmlns="http://www.w3.org/1998/Math/MathML">How>c2ow>b> anisotropy ratio, on-construct="true" class="math-equation-construct">on-image="true" class="math-equation-image">on-mathml="true" class="math-equation-mathml" style="display:none">org/1998/Math/MathML">b xmlns:w="http://www.wiley.com/namespaces/wiley" xmlns:wiley="http://www.wiley.com/namespaces/wiley/wiley" xmlns:cr="urn://wiley-online-library/content/render" xmlns="http://www.w3.org/1998/Math/MathML">ΓHb> = on-construct="true" class="math-equation-construct">on-image="true" class="math-equation-image">on-mathml="true" class="math-equation-mathml" style="display:none">org/1998/Math/MathML">bsup xmlns:w="http://www.wiley.com/namespaces/wiley" xmlns:wiley="http://www.wiley.com/namespaces/wiley/wiley" xmlns:cr="urn://wiley-online-library/content/render" xmlns="http://www.w3.org/1998/Math/MathML">How>c2ow>abbsup>/on-construct="true" class="math-equation-construct">on-image="true" class="math-equation-image">on-mathml="true" class="math-equation-mathml" style="display:none">org/1998/Math/MathML">bsup xmlns:w="http://www.wiley.com/namespaces/wiley" xmlns:wiley="http://www.wiley.com/namespaces/wiley/wiley" xmlns:cr="urn://wiley-online-library/content/render" xmlns="http://www.w3.org/1998/Math/MathML">How>c2ow>cbsup> on-construct="true" class="math-equation-construct">on-image="true" class="math-equation-image">on-mathml="true" class="math-equation-mathml" style="display:none">org/1998/Math/MathML">o xmlns:w="http://www.wiley.com/namespaces/wiley" xmlns:wiley="http://www.wiley.com/namespaces/wiley/wiley" xmlns:cr="urn://wiley-online-library/content/render" xmlns="http://www.w3.org/1998/Math/MathML">∼o> 7 near on-construct="true" class="math-equation-construct">on-image="true" class="math-equation-image">on-mathml="true" class="math-equation-mathml" style="display:none">org/1998/Math/MathML">b xmlns:w="http://www.wiley.com/namespaces/wiley" xmlns:wiley="http://www.wiley.com/namespaces/wiley/wiley" xmlns:cr="urn://wiley-online-library/content/render" xmlns="http://www.w3.org/1998/Math/MathML">Tcb> indicates that the large gap would occupy a highly two-dimensional Fermi surface.

© 2004-2018 中国地质图书馆版权所有 京ICP备05064691号 京公网安备11010802017129号

地址:北京市海淀区学院路29号 邮编:100083

电话:办公室:(+86 10)66554848;文献借阅、咨询服务、科技查新:66554700