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Volumn 81, Issue 10, 2010, Pages

Electronic structure and magnetic properties of the spin-gap compound Cu2 ( PO3 ) 2 CH2: Magnetic versus structural dimers

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Indexed keywords


EID: 77954930328     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.81.104416     Document Type: Article
Times cited : (14)

References (53)
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    • eff =4-5 eV
    • eff = 4 - 5 eV.
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    • We obtained J⊥ by averaging the calculated individual exchange integrals. All calculated individual contributions are of similar size between 1 and 2 meV, but have a rather large error bar (∼50% ) due to the small energy differences and the computationally limited size of supercells
    • We obtained J ⊥ by averaging the calculated individual exchange integrals. All calculated individual contributions are of similar size between 1 and 2 meV, but have a rather large error bar (∼ 50 %) due to the small energy differences and the computationally limited size of supercells.
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    • This shift in U is code independent. Although a local orbital and a plane-wave code need different absolute values for U to describe the EFG or the exchange J due to their different basis implementation, the shift in U for both basis schemes is basically the same
    • This shift in U is code independent. Although a local orbital and a plane-wave code need different absolute values for U to describe the EFG or the exchange J due to their different basis implementation, the shift in U for both basis schemes is basically the same.
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    • B T/J from Ref..
    • - (t) = χ (t) J 1 b / N g 2 μ B 2 and t = k B T / J from Ref..
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    • For the fit, we used the parametrized solutions for the AF-AF (Ref.) and the FM-AF (Ref.) alternating chain models.
    • For the fit, we used the parametrized solutions for the AF-AF (Ref.) and the FM-AF (Ref.) alternating chain models.
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    • We measured additional magnetization curves with pulses up to 16 and 32 T. Although the 16 T curve could be perfectly fitted to the low-field SQUID data, the 32 T curve again showed similar discrepancies to the SQUID data as the 60 T data
    • We measured additional magnetization curves with pulses up to 16 and 32 T. Although the 16 T curve could be perfectly fitted to the low-field SQUID data, the 32 T curve again showed similar discrepancies to the SQUID data as the 60 T data.
  • 50
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    • S ≈110 T, which unfortunately is out of reach with the present experimental setup
    • The theoretical curve for the coupled AHC model provides an estimate for the saturation field of μ 0 H S ≈ 110 T, which unfortunately is out of reach with the present experimental setup.


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