Severity: Warning
Message: file_get_contents(https://...@pubfacts.com&api_key=b8daa3ad693db53b1410957c26c9a51b4908&a=1): Failed to open stream: HTTP request failed! HTTP/1.1 429 Too Many Requests
Filename: helpers/my_audit_helper.php
Line Number: 176
Backtrace:
File: /var/www/html/application/helpers/my_audit_helper.php
Line: 176
Function: file_get_contents
File: /var/www/html/application/helpers/my_audit_helper.php
Line: 250
Function: simplexml_load_file_from_url
File: /var/www/html/application/helpers/my_audit_helper.php
Line: 3122
Function: getPubMedXML
File: /var/www/html/application/controllers/Detail.php
Line: 575
Function: pubMedSearch_Global
File: /var/www/html/application/controllers/Detail.php
Line: 489
Function: pubMedGetRelatedKeyword
File: /var/www/html/index.php
Line: 316
Function: require_once
We follow the evolution of the electronic properties of the titled homologous series when as well as the atomic type of A and M are varied where for = 1, A = Ca, Sr and M = Rh, Ir while for = 3, A = Ca, Sr and M = Rh. The crystal structure of = 1 members is known to be CaRhB-type (), while that of = 3 is CaRhB-type (); the latter can be visualized as a stacking of structural fragments from AMB (6/) and AMB. The metallic properties of the = 1 and 3 members are distinctly different: on the one hand, the = 1 members are characterized by a linear coefficient of the electronic specific heat ≈ 3 mJ mol K, a Debye temperature ≈ 300 K, a normal conductivity down to 2 K and a relatively strong linear magnetoresistivity for fields up to 150 kOe. The = 3 family, on the other hand, exhibits ≈ 18 mJ mol K, ≈ 330 K, a weak linear magnetoresistivity and an onset of superconductivity (for CaRhB, = 4.0 K and = 14.5 kOe, while for SrRh B, = 3.4 K and ≈ 4.0 kOe). These remarkable differences are consistent with the findings of the electronic band structures and density of state (DOS) calculations. In particular, satisfactory agreement between the measured and calculated was obtained. Furthermore, the Fermi level, , of CaRhB lies at almost the top of a pronounced local DOS peak, while that of CaRhB lies at a local valley: this is the main reason behind the differences between the, e.g., superconducting properties. Finally, although all atoms contribute to the DOS at , the contribution of the Rh atoms is the strongest.
Download full-text PDF |
Source |
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http://www.ncbi.nlm.nih.gov/pmc/articles/PMC5090507 | PMC |
http://dx.doi.org/10.1088/1468-6996/14/3/035003 | DOI Listing |
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