Petre Badica

Petre Badica

orcid

Research Focus & Metrics

Academic Career Length

32Years (1995-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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7 July 2006 in Physical Review Letters
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Journal Article
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HYH. Q. Yuan
H. Q. Yuan
DAD. F. Agterberg
D. F. Agterberg
NHN. Hayashi
N. Hayashi
PBPetre Badica
Petre Badica
DVD. Vandervelde
D. Vandervelde
MSM. B. Salamon
M. B. Salamon
We investigate the order parameter of noncentrosymmetric superconductors Li2Pd3B and Li2Pt3B via the behavior of the penetration depth λ(T). The low-temperature penetration depth shows BCS-like behavior in Li2Pd3B, while in Li2Pt3B it follows a linear temperature dependence. We propose that broken inversion symmetry and the accompanying antisymmetric spin-orbit coupling, which admix spin-singlet and spin-triplet pairing, are responsible for this behavior. The triplet contribution is weak in Li2Pd3B, leading to a wholly open but anisotropic gap. The significantly larger spin-orbit coupling in Li2Pt3B allows the spin-triplet component to be larger in Li2Pt3B, producing line nodes in the energy gap as evidenced by the linear temperature dependence of λ(T). The experimental data are in quantitative agreement with theory.

8 December 2004 in Physical Review Letters
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Journal Article
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KTK. Togano
K. Togano
PBPetre Badica
Petre Badica
YNY. Nakamori
Y. Nakamori
SOShin−ichi Orimo
Shin−ichi Orimo
HTH. Takeya
H. Takeya
KHK. Hirata
K. Hirata
Superconductivity at about 8 K was observed in the metal-rich Li-Pd-B ternary system. Structural, microstructural, electrical, and magnetic investigations for various compositions proved that the Li2Pd3B compound, which has an antiperovskite cubic structure composed of distorted Pd6B octahedrons, is responsible for the superconductivity. This is the first observation of superconductivity in metal-rich ternary borides containing alkaline metal and Pd as a late transition metal. The compound prepared by arc melting has a high density and is relatively stable in the air. The upper critical fields Hc2(0) estimated by linear extrapolation and the Werthamer-Helfand-Hohenberg theory are 6.2 and 4.8 T, respectively.

1 March 2005 in Journal of the Physical Society of Japan
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Journal Article
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PBPetre Badica
Petre Badica
TKTakaaki Kondo
Takaaki Kondo
KTKazumasa Togano
Kazumasa Togano

1 June 2015 in Composites Part B: Engineering
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Journal Article
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NFN.M. Florea
N.M. Florea
ALA. Lungu
A. Lungu
PBPetre Badica
Petre Badica
LCL. Craciun
L. Craciun
MEMonica Enculescu
Monica Enculescu
Horia  IovuHoria Iovu
Horia Iovu

1 July 2012 in Physica C: Superconductivity and its Applications
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Journal Article
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GAG. Aldica
G. Aldica
DBDan Batalu
Dan Batalu
SPS. Popa
S. Popa
III. Ivan
I. Ivan
PNP. Nita
P. Nita
PBPetre Badica
Petre Badica

29 December 2006 in Physical Review Letters
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Journal Article
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TST. Shimojima
T. Shimojima
KIK. Ishizaka
K. Ishizaka
STS. Tsuda
S. Tsuda
TKT. Kiss
T. Kiss
TYT. Yokoya
T. Yokoya
KTK. Togano
K. Togano
The cobalt oxide superconductor NaxCoO2·yH2O is studied by angle-resolved photoemission spectroscopy. We report the Fermi surface (FS) topology and electronic structure near the Fermi level (EF) in the normal state of NaxCoO2·yH2O. Our result indicates the presence of the hexagonal FS centered at the Γ point, while the small pocket FSs along Γ−K direction are absent, similar to NaxCoO2. The top of the eg′ band, which is expected in band calculations to form the small pocket FSs, extends to within ∼30  meV below EF, closer to EF than in NaxCoO2. We discuss its possible role in superconductivity, comparing with other experimental and theoretical results.