Anisotropic magnetic property of single crystals <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mi>R</mml:mi><mml:msub><mml:mrow><mml:mi mathvariant="normal">V</mml:mi></mml:mrow><mml:mn>6</mml:mn></mml:msub><mml:msub><mml:mrow><mml:mi>Sn</mml:mi></mml:mrow><mml:mn>6</mml:mn></mml:msub></mml:math> <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mo>(</mml:mo><mml:mi>R</mml:mi><mml:mo>=</mml:mo><mml:mi mathvariant="normal">Y</mml:mi><mml:mo>,</mml:mo><mml:mo> </mml:mo><mml:mi>Gd</mml:mi><mml:mtext>−</mml:mtext><mml:mi>Tm</mml:mi><mml:mo>,</mml:mo><mml:mo> </mml:mo><mml:mi>Lu</mml:mi><mml:mo>)</mml:mo></mml:math>
Why this work is in the frame
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Bibliographic record
Abstract
${R\mathrm{V}}_{6}{\mathrm{Sn}}_{6}$ $(R=\mathrm{Y}, \mathrm{Gd}\text{\ensuremath{-}}\mathrm{Tm}, \mathrm{Lu})$ single crystals are synthesized by the Sn-flux method and their physical properties are characterized by magnetization, resistivity, and specific heat measurements. Powder x-ray diffraction patterns of all samples can be well indexed with the hexagonal ${\mathrm{HfFe}}_{6}{\mathrm{Ge}}_{6}$-type structure, where rare-earth atoms form hexagonal layers and vanadium atoms form kagome layers. At high temperatures, magnetic susceptibility measurements of moment-bearing rare-earth ions $(R=\mathrm{Gd}\text{\ensuremath{-}}\mathrm{Tm})$ follow Curie-Weiss behavior. Effective moments estimated from the polycrystalline average of magnetic susceptibility curves are consistent with the values for free ${R}^{3+}$ ions. Strong magnetic anisotropy due to crystalline electric field effects is observed for moment-bearing rare-earth ions, except ${\mathrm{GdV}}_{6}{\mathrm{Sn}}_{6}$. The easy magnetization direction is determined to be the $c$ axis for $R=\mathrm{Tb}\text{\ensuremath{-}}\mathrm{Ho}$ and $ab$ plane for $R=\mathrm{Er}$ and Tm. The vanadium ions in ${R\mathrm{V}}_{6}{\mathrm{Sn}}_{6}$ possess no magnetic moment. The compounds for $R=\mathrm{Y}$ and Lu exhibit typical characteristics of paramagnetic metals. At low temperatures, the magnetic ordering is confirmed from magnetization, specific heat, and resistivity: the highest ${T}_{N}=4.9$ K for ${\mathrm{GdV}}_{6}{\mathrm{Sn}}_{6}$ and the lowest ${T}_{N}=2.3$ K for ${\mathrm{HoV}}_{6}{\mathrm{Sn}}_{6}$. No magnetic ordering is observed down to 1.8 K for $R=\mathrm{Er}$ and Tm. A slight deviation of the magnetic ordering temperature from the de Gennes scaling suggests the dominant Ruderman-Kittel-Kasuya-Yosida exchange interaction between rare-earth moments in metallic ${R\mathrm{V}}_{6}{\mathrm{Sn}}_{6}$ compounds.
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Full frame distilled prediction
Teacher imitationNot calibrated prevalence, not ground truth. Human validation pending. Learned from the 10,348 direct Codex labels and 10,348 direct Gemma labels. Candidate is the union of thresholded teacher heads; consensus is their intersection. These outputs are machine_predicted_unvalidated and are not human labels or direct frontier model labels.
Codex and Gemma teacher scores by category
| Category | Codex | Gemma |
|---|---|---|
| Metaresearch | 0.011 | 0.008 |
| Meta-epidemiology (narrow) | 0.007 | 0.013 |
| Meta-epidemiology (broad) | 0.003 | 0.012 |
| Bibliometrics | 0.004 | 0.008 |
| Science and technology studies | 0.011 | 0.009 |
| Scholarly communication | 0.011 | 0.009 |
| Open science | 0.014 | 0.014 |
| Research integrity | 0.011 | 0.010 |
| Insufficient payload (model declined to judge) | 0.487 | 0.015 |
Machine scores (provisional)
The two teacher heads of the student model, read on this work. A score orders the frame for review; it never asserts a category, and the validation status ships verbatim with every row.
Baseline scores from an immature model (maturity gate not passed, 7 training rounds). Scores rank; they never assert a category.
score_only:v0-immature-baseline · verbatim from the scoring run: score_only means the number may rank works, and no category label ships from it