44 research outputs found
Photonic Band Gaps of Three-Dimensional Face-Centered Cubic Lattices
We show that the photonic analogue of the Korringa-Kohn-Rostocker method is a
viable alternative to the plane-wave method to analyze the spectrum of
electromagnetic waves in a three-dimensional periodic dielectric lattice.
Firstly, in the case of an fcc lattice of homogeneous dielectric spheres, we
reproduce the main features of the spectrum obtained by the plane wave method,
namely that for a sufficiently high dielectric contrast a full gap opens in the
spectrum between the eights and ninth bands if the dielectric constant
of spheres is lower than the dielectric constant of
the background medium. If , no gap is found in the
spectrum. The maximal value of the relative band-gap width approaches 14% in
the close-packed case and decreases monotonically as the filling fraction
decreases. The lowest dielectric contrast for which a
full gap opens in the spectrum is determined to be 8.13. Eventually, in the
case of an fcc lattice of coated spheres, we demonstrate that a suitable
coating can enhance gap widths by as much as 50%.Comment: 19 pages, 6 figs., plain latex - a section on coated spheres, two
figures, and a few references adde
Etched distributed Bragg reflectors as three-dimensional photonic crystals: photonic bands and density of states
The photonic band dispersion and density of states (DOS) are calculated for
the three-dimensional (3D) hexagonal structure corresponding to a distributed
Bragg reflector patterned with a 2D triangular lattice of circular holes.
Results for the Si/SiO and GaAs/AlGaAs systems determine the optimal
parameters for which a gap in the 2D plane occurs and overlaps the 1D gap of
the multilayer. The DOS is considerably reduced in correspondence with the
overlap of 2D and 1D gaps. Also, the local density of states (i.e., the DOS
weighted with the squared electric field at a given point) has strong
variations depending on the position. Both results imply substantial changes of
spontaneous emission rates and patterns for a local emitter embedded in the
structure and make this system attractive for the fabrication of a 3D photonic
crystal with controlled radiative properties.Comment: 8 pages, 5 figures; to appear in Phys. Rev.
Photonic band gaps in materials with triply periodic surfaces and related tubular structures
We calculate the photonic band gap of triply periodic bicontinuous cubic
structures and of tubular structures constructed from the skeletal graphs of
triply periodic minimal surfaces. The effect of the symmetry and topology of
the periodic dielectric structures on the existence and the characteristics of
the gaps is discussed. We find that the C(I2-Y**) structure with Ia3d symmetry,
a symmetry which is often seen in experimentally realized bicontinuous
structures, has a photonic band gap with interesting characteristics. For a
dielectric contrast of 11.9 the largest gap is approximately 20% for a volume
fraction of the high dielectric material of 25%. The midgap frequency is a
factor of 1.5 higher than the one for the (tubular) D and G structures
Search for the Flavor-Changing Neutral Current Decay with the HERA-B Detector
We report on a search for the flavor-changing neutral current decay using events recorded with a dimuon trigger in
interactions of 920 GeV protons with nuclei by the HERA-B experiment. We find
no evidence for such decays and set a 90% confidence level upper limit on the
branching fraction .Comment: 17 pages, 4 figures (of which 1 double), paper to be submitted to
Physics Letters
Measurement of the J/Psi Production Cross Section in 920 GeV/c Fixed-Target Proton-Nucleus Interactions
The mid-rapidity (dsigma_(pN)/dy at y=0) and total sigma_(pN) production
cross sections of J/Psi mesons are measured in proton-nucleus interactions.
Data collected by the HERA-B experiment in interactions of 920 GeV/c protons
with carbon, titanium and tungsten targets are used for this analysis. The
J/Psi mesons are reconstructed by their decay into lepton pairs. The total
production cross section obtained is sigma_(pN)(J/Psi) = 663 +- 74 +- 46
nb/nucleon. In addition, our result is compared with previous measurements
Limits for the central production of Î+ and Îââ pentaquarks in 920-GeV pA collisions
We have searched for Î+(1540) and Îââ(1862) pentaquark candidates in proton-inducedreactions on C, Ti, and W targets at midrapidity and sâ=41.6ââGeV. In 2Ă108 inelastic eventswe find no evidence for narrow (Ïâ5ââMeV) signals in the Î+âpK0S and ÎâââÎâÏâ channels; our 95% C.L. upper limits (UL) forthe inclusive production cross section times branching fraction BâdÏ/dy $y â0 are (4-16) ÎŒb/N for a Î+ mass between 1521 and 1555 MeV,and 2.5ÎŒb/N for the Îââ. The UL of the yield ratio of Î+/Î(1520)<(3-12)% is significantly lower than model predictions.Our UL of BâÎââ/Î(1530)0<4% is at variance with the results that have provided the first evidencefor the Îââ