16,949,103 research outputs found
Understanding the internal structures of the , , and
We investigate the newly observed and based on the
diquark-antidiquark configuration within the framework of QCD sum rules. Both
of them may be interpreted as the -wave tetraquark states
of , but with opposite color structures, which is remarkably similar
to the result obtained in Ref.~\cite{Chen:2010ze} that the and
can be both interpreted as the -wave tetraquark
states of , also with opposite color structures. However, the
extracted masses and these suggested assignments to these states do depend
on these running quark masses where m_s (2 \mbox{ GeV}) = 95 \pm 5 MeV and
GeV. As a byproduct, the masses of the
hidden-bottom partner states of the and are extracted to be
both around 10.64 GeV, which can be searched for in the
invariant mass distribution.Comment: 6 pages, 4 figures. Accepted by Eur. Phys. J.
New molecular candidates: X(1910), X(2200), and X(2350)
Assuming the newly observed resonant structures X(1910), X(2200), and X(2350)
as , , and molecular states respectively,
we compute their mass values in the framework of QCD sum rules. The numerical
results are for state,
for state, and for state, which
coincide with the experimental values of X(1910), X(2200), and X(2350),
respectively. This supports the statement that X(1910), X(2200), and X(2350)
could be , , and molecular candidates
respectively.Comment: 9 pages, 9 eps figures; the name of X(2000) changed to X(1910)
according to the updated data of experiments; more references and discussions
added; accepted for publication in PRD. arXiv admin note: substantial text
overlap with arXiv:1211.2277, arXiv:1201.341
Superparamagnetic relaxation in Cu_{x}Fe_{3-x}O_{4} (x=0.5 and x=1) nanoparticles
The scope of this article is to report very detailed results of the
measurements of magnetic relaxation phenomena in the new
CuFeO nanoparticles and known CuFeO
nanoparticles. The size of synthesized particles is (6.51.5)nm. Both
samples show the superparamagnetic behaviour, with the well-defined phenomena
of blocking of magnetic moment. This includes the splitting of
zero-field-cooled and field-cooled magnetic moment curves, dynamical
hysteresis, slow quasi-logarithmic relaxation of magnetic moment below blocking
temperature. The scaling of the magnetic moment relaxation data at different
temperatures confirms the applicability of the simple thermal relaxation model.
The two copper-ferrites with similar structures show significantly different
magnetic anisotropy density and other magnetic properties. Investigated systems
exhibit the consistency of all obtained results.Comment: 18 pages, 8 figure
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