scholarly journals Ground State of the Easy-Axis Rare-Earth Kagome LangasitePr3Ga5SiO14

2010 ◽  
Vol 104 (5) ◽  
Author(s):  
A. Zorko ◽  
F. Bert ◽  
P. Mendels ◽  
K. Marty ◽  
P. Bordet
Keyword(s):  
1990 ◽  
Vol 26 (5) ◽  
pp. 320 ◽  
Author(s):  
M. Monerie ◽  
T. Georges ◽  
P.L. Francois ◽  
J.Y. Allain ◽  
D. Neveux

1994 ◽  
Vol 01 (04) ◽  
pp. 649-653 ◽  
Author(s):  
A.J. PATCHETT ◽  
S.S. DHESI ◽  
R.I.R. BLYTH ◽  
S.D. BARRETT

An intense photoemission feature is observed at a binding energy of ~10 eV in the UV photoemission spectra from the (0001) surfaces of bulk single crystals of rare-earth metals. This emission cannot be explained in terms of ground state electronic structure and we have been unable to attribute its existence to the presence of contamination of the surface. We present some evidence that may indicate its origin lies in the creation, by the photoemission process, of a metastable two-hole final state.


2015 ◽  
Vol 10 (4) ◽  
pp. 95-99
Author(s):  
Nikolay Pavlovskii ◽  
Kirill Shaykhutdinov ◽  
Andrey Dubrovskiy ◽  
Mikhail Petrov ◽  
Konstantin Terent’ev ◽  
...  

In this report we investigate changing of magnetic properties of system (La1-zNdz)1.4Sr1.6Mn2O7 during isovalent substitution from lanthanium to neodymium at different concentration z = 0, 0.3. Decreasing of Mn-Mn in-plane distance with increasing z leads to the suppression of the ferromagnetic state that, as expected, tells us about the change of the orbital character eg – electrons with 2 2 3z r d  on the 2 2 . x y d  Also, at high applied magnetic fields metamagnetic transition observed at concentration z = 0.3, it is characterized by a sharp increase of the magnetization and the change of the ground state of the sample from the antiferromagnetic to ferromagnetic.


Materials ◽  
2020 ◽  
Vol 13 (10) ◽  
pp. 2237
Author(s):  
Mowafaq Mohammad Alsardia ◽  
Jaekyung Jang ◽  
Joo Yull Rhee

We explore the influence of pressure on the magnetic ground state of the heavy-fermion antiferromagnet (ferromagnet) CeAuSb 2 (CeAgSb 2 ) using first-principles calculations. The total-energy differences obtained by including the spin-orbit interactions and the on-site Coulomb potential for the Ce-derived 4f-orbitals are necessary to realize the accurate magnetic ground state of CeNMSb 2 (NM: Au and Ag). According to our results, the appearance of a new magnetic phase of CeAuSb 2 (CeAgSb 2 ) at the pressure of 2.1 GPa (3.5 GPa) is due to the rotation of the magnetic easy axis from the <001> to the <100> direction. Additionally, our data confirm that CeAgSb 2 is antiferromagnetic (AFM) above a critical pressure P c , and such a tendency is expected for CeAuSb 2 and remains to be seen. Through the spin-orbit-coupling Hamiltonian and detailed information on the occupation of individual 4f-orbitals of the Ce atom obtained by the electronic-structure calculations, we can deduce the rotation of the magnetic easy axis upon the application of pressure. According to the present and previous studies, the differences among the magnetic properties of CeNMSb 2 (NM: Cu, Ag and Au) compounds are not due to the different noble metals, but due to the subtle differences in the relative position of Ce atoms and, in turn, different occupations of Ce 4f-orbitals.


1991 ◽  
Vol 60 (7) ◽  
pp. 2484-2484 ◽  
Author(s):  
Hidekazu Tanaka ◽  
Soichiro Teraoka ◽  
Eiichiro Kakehashi ◽  
Katsunori Iio ◽  
Kazukiyo Nagata

Nanoscale ◽  
2020 ◽  
Vol 12 (43) ◽  
pp. 22258-22267
Author(s):  
L. Fernandez ◽  
M. Blanco-Rey ◽  
R. Castrillo-Bodero ◽  
M. Ilyn ◽  
K. Ali ◽  
...  

HoAu2, YbAu2 and GdAu2 surface compounds are investigated by electron spectroscopies, microscopy and theory. Yb in YbAu2 reveals a mixed valence character while Gd and Ho are trivalent. HoAu2 is ferromagnetic with an out-of-plane easy axis and TC = 22 K.


Author(s):  
M. A. Noginov ◽  
G. K. Sarkissian ◽  
V. A. Smirnov ◽  
I. A. Shcherbakov

2000 ◽  
Vol 09 (04) ◽  
pp. 309-317 ◽  
Author(s):  
P. C. SOOD ◽  
M. SAINATH ◽  
K. VENKATARAMANIAH

The low-energy two-quasiparticle bandhead energies for the odd-odd Z=101 nucleus 250 Md are evaluated using a zero range residual neutron-proton interaction. The 250Md ground state is seen to have the spin-parity Iπ=0- corresponding to the singlet band from the configuration {p : 7/2[514]⊗n:7/2[624]} in violation of the Gallagher-Moszkowski (GM) coupling rule. The situation here is shown to be almost identical to that for the rare-earth nucleus 166 Ho , which is the only well-established exception to the GM rule known so far. Analysis of the expected low energy spectrum, including the rotational levels, for 250 Md reveals the occurrence of an as-yet-unobserved long-lived high-spin Iπ = 7- isomeric state around (80±30) keV with dominant ε and α decay modes.


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