KETERBUKAAN POLITIK DALAM DEMOKRASI PANCASILA: Tinjuan Etika Politik atas Kehidupan Demokrasi di Indonesia

Keterbukaan politik dalam Demokrasi Pancasila merupakan keterbukaan yang berarti umpan balik di mana rakyat sebagai warga negara memiliki hak untuk mengontrol, mengkritik dan memberikan usul serta saran atau dukungan pemerintah. Pemerintahan dalam melaksanakan pemerintahan harus secara terbuka di hadapan publik, agar publik mampu menilai apakah kebijakan pemerintah menjamin hak-hak warga negara dan menegakkan keadilan, ataukah kebijakan itu hanya untuk melestarikan kekuasaan rezim yang sedang berkuasa atau kelompok orang di sekitar kekuasaan. Perjuangan untuk menegakkan keterbukaan politik dalam kehidupan demokrasi Pancasila sangat penting dalam kehidupan demokrasi. Usaha warga negara yang dilakukan merupakan kebijakan dalam rangka membela nilai-nilai yang sangat berhubungan dengan persoalan hak asasi manusia dan kesejahteraan umu

The Glueball in a Chiral Linear Sigma Model with Vector Mesons

We present a two-flavour linear sigma model with global chiral symmetry and (axial-)vector mesons as well as an additional glueball degree of freedom. We study the structure of the well-established scalar resonances f0(1370) and f0(1500): by a fit to experimentally known decay widths we find that f0(1370) is predominantly a \bar{q}q state and f0(1500) is predominantly a glueball state. The overall phenomenology of these two resonances can be well described. Other assignments for our mixed quarkonium-glueball states are also tested, but turn out to be in worse agreement with the phenomenology. As a by-product of our analysis, the gluon condensate is determined.Comment: 8 page

Observation of metastable Aβ amyloid protofibrils by atomic force microscopy

AbstractBackground: Brain amyloid plaque, a diagnostic feature of Alzheimer's disease (AD), contains an insoluble fibrillar core that is composed primarily of variants of the β-amyloid protein (Aβ). As Aβ amyloid fibrils may initiate neurodegeneration, the inhibition of fibril formation is a possible therapeutic strategy. Very little is known about the early steps of the process, however.Results: Atomic force microscopy was used to follow amyloid fibril formation in vitro by the Aβ variants Aβ1-40 and Aβ1-42. Both variants first form small ordered aggregates that grow slowly and then rapidly disappear, while prototypical amyloid fibrils of two discrete morphologies appear. Aβ1-42 aggregates much more rapidly than Aβ1-40, which is consistent with its connection to early-onset AD. We propose that the metastable intermediate species be called Aβ amyloid protofibrils.Conclusions: Aβ protofibrils are likely to be intermediates in the in vitro assembly of Aβ amyloid fibrils, but their in vivo role has yet to be determined. Numerous reports of a nonfibrillar form of Aβ aggregate in the brains of individuals who are predisposed to AD suggest the existence of a precursor form, possibly the protofibril. Thus, stabilization of Aβ protofibrils may be a useful therapeutic strategy

Role of heavy-meson exchange in pion production near threshold

Recent calculations of $s$-wave pion production have severely underestimated the accurately known $pp\rightarrow pp\pi^0$\ total cross section near threshold. In these calculations, only the single-nucleon axial-charge operator is considered. We have calculated, in addition to the one-body term, the two-body contributions to this reaction that arise from the exchange of mesons. We find that the inclusion of the scalar $\sigma$-meson exchange current (and lesser contributions from other mesons) increases the cross section by about a factor of five, and leads to excellent agreement with the data. The results are neither very sensitive to changes in the distorting potential that generates the $NN$ wave function, nor to different choices for the meson-nucleon form factors. We argue that $pp\rightarrow pp\pi^0$\ data provide direct experimental evidence for meson-exchange contributions to the axial current.Comment: 28 Pages, IU-NTC #93-0

Observation of Fano Asymmetry in Raman Spectra of SrTiO3 and Cax Sr1-xTiO3 Perovskite Nanocubes

Bulk SrTi O3 is cubic and not expected to exhibit any first-order Raman scattering. However, nanocubes of SrTi O3 with an edge length of 80±10 nm show strong first-order Raman scattering originating from the breaking of symmetry caused by frozen surface dipoles (local tetragonality) and the presence of nanoscopic polar domains (arising from incorporated impurities). Rapid polarization fluctuations within these nanoscopic ferroelectric regions interfere with a polar phonon, resulting in a Fano-like asymmetric line shape in these SrTi O3 nanocubes, as well as in Ca0.3 Sr0.7 Ti O3 nanocubes

A search for two body muon decay signals

Lepton family number violation is tested by searching for $\mu^+\to e^+X^0$ decays among the 5.8$\times 10^8$ positive muon decay events analyzed by the TWIST collaboration. Limits are set on the production of both massless and massive $X^0$ bosons. The large angular acceptance of this experiment allows limits to be placed on anisotropic $\mu^+\to e^+X^0$ decays, which can arise from interactions violating both lepton flavor and parity conservation. Branching ratio limits of order $10^{-5}$ are obtained for bosons with masses of 13 - 80 MeV/c$^2$ and with different decay asymmetries. For bosons with masses less than 13 MeV/c$^{2}$ the asymmetry dependence is much stronger and the 90% limit on the branching ratio varies up to $5.8 \times 10^{-5}$. This is the first study that explicitly evaluates the limits for anisotropic two body muon decays.Comment: 7 pages, 5 figures, 2 tables, accepted by PR

Cross section and analyzing power of pol{p}p -> pn pi+ near threshold

The cross section and analyzing power of the pol{p}p -> pn pi+ reaction near threshold are estimated in terms of data obtained from the pol{p}p -> d pi+ and pp -> pp pi0 reactions. A simple final state interaction theory is developed which depends weakly upon the form of the pion-production operator and includes some Coulomb corrections. Within the uncertainties of the model and the input data, the approach reproduces well the measured energy dependence of the total cross section and the proton analyzing power at a fixed pion c.m. angle of 90deg, from threshold to T_p = 330 MeV. The variation of the differential cross section with pion angle is also very encouraging.Comment: 20 pages, Latex including 4 eps figure

Measurement of Inverse Pion Photoproduction at Energies Spanning the N(1440) Resonance

Differential cross sections for the process pi^- p -> gamma n have been measured at Brookhaven National Laboratory's Alternating Gradient Synchrotron with the Crystal Ball multiphoton spectrometer. Measurements were made at 18 pion momenta from 238 to 748 MeV/c, corresponding to E_gamma for the inverse reaction from 285 to 769 MeV. The data have been used to evaluate the gamma n multipoles in the vicinity of the N(1440) resonance. We compare our data and multipoles to previous determinations. A new three-parameter SAID fit yields 36 +/- 7 (GeV)^-1/2 X 10^-3 for the A^n_1/2 amplitude of the P_11.Comment: 14 pages, 8 figures, submitted to PR