Itinerant Magnetism in Metallic CuFe2Ge2
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{"title"=>"Itinerant magnetism in metallic CuFe2Ge2", "type"=>"journal", "authors"=>[{"first_name"=>"K. V.", "last_name"=>"Shanavas", "scopus_author_id"=>"12795006800"}, {"first_name"=>"David J.", "last_name"=>"Singh", "scopus_author_id"=>"7403593794"}], "year"=>2015, "source"=>"PLoS ONE", "identifiers"=>{"pui"=>"603466308", "arxiv"=>"1412.5254", "doi"=>"10.1371/journal.pone.0121186", "scopus"=>"2-s2.0-84961322780", "issn"=>"19326203", "sgr"=>"84961322780"}, "id"=>"aa71aa1c-5cac-3a3f-a100-94f293909f1a", "abstract"=>"Theoretical calculations are performed to understand the electronic structure and magnetic properties of CuFe$_2$Ge$_2$. The band structure reveal large electron density $N(E_F)$ at the Fermi level suggesting strong itinerant character of magnetism. The Fermi surface is dominated by two dimensional sheet like structures, with potentially strong nesting between them. The magnetic ground state appears to be ferromagnetic along $a$ and antiferromagnetic in other directions. The results show that CuFe$_2$Ge$_2$ is an antiferromagnetic metal, with similarities to the Fe-based superconductors; such as magnetism with substantial itinerant character and coupling between magnetic order and electrons at the Fermi energy.", "link"=>"http://www.mendeley.com/research/itinerant-magnetism-metallic-cufe2ge2", "reader_count"=>6, "reader_count_by_academic_status"=>{"Researcher"=>3, "Student > Ph. D. Student"=>3}, "reader_count_by_user_role"=>{"Researcher"=>3, "Student > Ph. D. Student"=>3}, "reader_count_by_subject_area"=>{"Materials Science"=>1, "Physics and Astronomy"=>4, "Chemistry"=>1}, "reader_count_by_subdiscipline"=>{"Materials Science"=>{"Materials Science"=>1}, "Chemistry"=>{"Chemistry"=>1}, "Physics and Astronomy"=>{"Physics and Astronomy"=>4}}, "group_count"=>0}

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Figshare

  • {"files"=>["https://ndownloader.figshare.com/files/1987463"], "description"=>"<p>For different magnetic ordering patterns studied (see text), the resulting magnetic moments <i>m</i>, energies and density at the Fermi surface <i>N</i>(<i>E</i><sub><i>F</i></sub>) in units of eV<sup>−1</sup> per formula unit. The energy of paramagnetic case (NSP) is taken to be zero.</p><p>Magnetic properties from GGA.</p>", "links"=>[], "tags"=>["antiferromagnetic", "CuFe 2Ge", "electron", "fermi", "Metallic CuFe 2Ge", "Magnetism"], "article_id"=>1354907, "categories"=>["Uncategorised"], "users"=>["K. V. Shanavas", "David J. Singh"], "doi"=>"https://dx.doi.org/10.1371/journal.pone.0121186.t001", "stats"=>{"downloads"=>0, "page_views"=>4, "likes"=>0}, "figshare_url"=>"https://figshare.com/articles/_Magnetic_properties_from_GGA_/1354907", "title"=>"Magnetic properties from GGA.", "pos_in_sequence"=>0, "defined_type"=>3, "published_date"=>"2015-03-25 03:58:36"}
  • {"files"=>["https://ndownloader.figshare.com/files/1987462"], "description"=>"<p>The high symmetry points are marked in the first panel. Seven bands with Fe-<i>d</i> character cross Fermi level and bands numbered as 1, 3, 4, 5 have strong Fe<sub>1</sub> character and bands 2, 6, 7 have strong Fe<sub>2</sub> character.</p>", "links"=>[], "tags"=>["antiferromagnetic", "CuFe 2Ge", "electron", "fermi", "Metallic CuFe 2Ge", "Magnetism"], "article_id"=>1354906, "categories"=>["Uncategorised"], "users"=>["K. V. Shanavas", "David J. Singh"], "doi"=>"https://dx.doi.org/10.1371/journal.pone.0121186.g006", "stats"=>{"downloads"=>0, "page_views"=>25, "likes"=>0}, "figshare_url"=>"https://figshare.com/articles/_Calculated_Fermi_surfaces_of_CuFe_2_Ge_2_/1354906", "title"=>"Calculated Fermi surfaces of CuFe<sub>2</sub>Ge<sub>2</sub>.", "pos_in_sequence"=>0, "defined_type"=>1, "published_date"=>"2015-03-25 03:58:36"}
  • {"files"=>["https://ndownloader.figshare.com/files/1987457"], "description"=>"<p>It shows the orthorhombic unitcell containing two formula units.</p>", "links"=>[], "tags"=>["antiferromagnetic", "CuFe 2Ge", "electron", "fermi", "Metallic CuFe 2Ge", "Magnetism"], "article_id"=>1354901, "categories"=>["Uncategorised"], "users"=>["K. V. Shanavas", "David J. Singh"], "doi"=>"https://dx.doi.org/10.1371/journal.pone.0121186.g001", "stats"=>{"downloads"=>0, "page_views"=>17, "likes"=>0}, "figshare_url"=>"https://figshare.com/articles/_The_crystal_structure_of_CuFe_2_Ge_2_/1354901", "title"=>"The crystal structure of CuFe<sub>2</sub>Ge<sub>2</sub>.", "pos_in_sequence"=>0, "defined_type"=>1, "published_date"=>"2015-03-25 03:58:36"}
  • {"files"=>["https://ndownloader.figshare.com/files/1987461"], "description"=>"<p>Contributions from the <i>d</i> states of Fe<sub>1</sub> and Fe<sub>2</sub> ions near the Fermi level from the non-magnetic calculation show that all states contribute significantly to the density of states. The crystallographic axes are taken as the coordinate system for calculation.</p>", "links"=>[], "tags"=>["antiferromagnetic", "CuFe 2Ge", "electron", "fermi", "Metallic CuFe 2Ge", "Magnetism"], "article_id"=>1354905, "categories"=>["Uncategorised"], "users"=>["K. V. Shanavas", "David J. Singh"], "doi"=>"https://dx.doi.org/10.1371/journal.pone.0121186.g005", "stats"=>{"downloads"=>1, "page_views"=>19, "likes"=>0}, "figshare_url"=>"https://figshare.com/articles/_Partial_density_of_states_for_Fe_d_states_/1354905", "title"=>"Partial density of states for Fe-<i>d</i> states.", "pos_in_sequence"=>0, "defined_type"=>1, "published_date"=>"2015-03-25 03:58:36"}
  • {"files"=>["https://ndownloader.figshare.com/files/1987459"], "description"=>"<p>The bottom panel zooms in on the states close to Fermi level which is set to 0 eV. The orbital character of the bands are shown by colored symbols in the top right panel. States close to Fermi level are dominated by Fe-3<i>d</i> states.</p>", "links"=>[], "tags"=>["antiferromagnetic", "CuFe 2Ge", "electron", "fermi", "Metallic CuFe 2Ge", "Magnetism"], "article_id"=>1354903, "categories"=>["Uncategorised"], "users"=>["K. V. Shanavas", "David J. Singh"], "doi"=>"https://dx.doi.org/10.1371/journal.pone.0121186.g003", "stats"=>{"downloads"=>2, "page_views"=>21, "likes"=>0}, "figshare_url"=>"https://figshare.com/articles/_Electronic_band_structure_of_CuFe_2_Ge_2_in_the_non_magnetic_phase_calculated_using_GGA_/1354903", "title"=>"Electronic band structure of CuFe<sub>2</sub>Ge<sub>2</sub> in the non-magnetic phase calculated using GGA.", "pos_in_sequence"=>0, "defined_type"=>1, "published_date"=>"2015-03-25 03:58:36"}
  • {"files"=>["https://ndownloader.figshare.com/files/1987460"], "description"=>"<p>Cu-<i>d</i> states are below the fermi level while Fe-<i>d</i> and Ge-<i>p</i> are partially occupied. Not shown are Fe and Cu <i>s</i> states, that are empty.</p>", "links"=>[], "tags"=>["antiferromagnetic", "CuFe 2Ge", "electron", "fermi", "Metallic CuFe 2Ge", "Magnetism"], "article_id"=>1354904, "categories"=>["Uncategorised"], "users"=>["K. V. Shanavas", "David J. Singh"], "doi"=>"https://dx.doi.org/10.1371/journal.pone.0121186.g004", "stats"=>{"downloads"=>0, "page_views"=>63, "likes"=>0}, "figshare_url"=>"https://figshare.com/articles/_Total_and_partial_density_of_states_DOS_for_the_non_magnetic_calculation_/1354904", "title"=>"Total and partial density of states (DOS) for the non-magnetic calculation.", "pos_in_sequence"=>0, "defined_type"=>1, "published_date"=>"2015-03-25 03:58:36"}
  • {"files"=>["https://ndownloader.figshare.com/files/1987458"], "description"=>"<p>Fe<sub>1</sub> (middle layer) are octahedrally coordinated. The atomic distances are marked in Angstrom.</p>", "links"=>[], "tags"=>["antiferromagnetic", "CuFe 2Ge", "electron", "fermi", "Metallic CuFe 2Ge", "Magnetism"], "article_id"=>1354902, "categories"=>["Uncategorised"], "users"=>["K. V. Shanavas", "David J. Singh"], "doi"=>"https://dx.doi.org/10.1371/journal.pone.0121186.g002", "stats"=>{"downloads"=>2, "page_views"=>10, "likes"=>0}, "figshare_url"=>"https://figshare.com/articles/_The_projection_of_CuFe_2_Ge_2_unitcell_on_to_ac_plane_/1354902", "title"=>"The projection of CuFe<sub>2</sub>Ge<sub>2</sub> unitcell on to <i>ac</i> plane.", "pos_in_sequence"=>0, "defined_type"=>1, "published_date"=>"2015-03-25 03:58:36"}

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Relative Metric

{"start_date"=>"2015-01-01T00:00:00Z", "end_date"=>"2015-12-31T00:00:00Z", "subject_areas"=>[]}
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