Neutron Skin Effects in Mirror Energy Differences: The Case of

Energy differences between analogue states in the T=1/2 ^{23}Mg-^{23}Na mirror nuclei have been measured along the rotational yrast bands. This allows us to search for effects arising from isospin-symmetry-breaking interactions (ISB) and/or shape changes. Data are interpreted in the shell model framework following the method successfully applied to nuclei in the f_{7/2} shell. It is shown that the introduction of a schematic ISB interaction of the same type of that used in the f_{7/2} shell is needed to reproduce the data. An alternative novel description, applied here for the first time, relies on the use of an effective interaction deduced from a realistic charge-dependent chiral nucleon-nucleon potential. This analysis provides two important results: (i) The mirror energy differences give direct insight into the nuclear skin; (ii) the skin changes along the rotational bands are strongly correlated with the difference between the neutron and proton occupations of the s_{1/2} "halo" orbit.

Neutron Skins and Halo Orbits in the sd and pf Shells.

The strong dependence of Coulomb energies on nuclear radii makes it possible to extract the latter from calculations of the former. The resulting estimates of neutron skins indicate that two mechanisms are involved. The first one-isovector monopole polarizability-amounts to noting that when a particle is added to a system it drives the radii of neutrons and protons in different directions, tending to equalize the radii of both fluids independently of the neutron excess. This mechanism is well understood and the Duflo-Zuker (small) neutron skin values derived 14 years ago are consistent with recent measures and estimates. The alternative mechanism involves halo orbits whose huge sizes tend to make the neutron skins larger and have a subtle influence on the radial behavior of sd and pf shell nuclei. In particular, they account for the sudden rise in the isotope shifts of nuclei beyond N=28 and the near constancy of radii in the A=40-56 region. This mechanism, detected here for the first time, is not well understood and may well go beyond the Efimov physics usually associated with halo orbits.

Observation of 54Ni: cross-conjugate symmetry in f7/2 mirror energy differences.

Gamma decays from excited states up to Jpi=6+ in the N=Z-2 nucleus 54Ni have been identified for the first time. Level energies are compared with those of the isobars 54Co and 54Fe and of the cross-conjugate nuclei of mass A=42. The good but puzzling f7/ cross-conjugate symmetry in mirror and triplet energy differences is analyzed. Shell model calculations reproduce the new data but the necessary nuclear charge-dependent phenomenology is not fully explained by modern nucleon-nucleon potentials.

1/f noise and very high spectral rigidity.

It was recently pointed out that the spectral fluctuations of quantum systems are formally analogous to discrete time series, and therefore their structure can be characterized by the power spectrum of the signal. Moreover, it is found that the power spectrum of chaotic spectra displays a 1/f behavior, while that of regular systems follows a 1/f2 law. This analogy provides a link between the concepts of spectral rigidity and antipersistence. Trying to get a deeper understanding of this relationship, we have studied the correlation structure of spectra with high spectral rigidity. Using an appropriate family of random Hamiltonians, we increase the spectral rigidity up to hindering completely the spectral fluctuations. Analyzing the long range correlation structure a neat power law 1/f has been found for all the spectra, along the whole process. Therefore, 1/f noise is the characteristic fingerprint of a transition that, preserving the scale-free correlation structure, hinders completely the fluctuations of the spectrum.

The spectra of mixed 3He-4He droplets.

The diffusion Monte Carlo technique is used to calculate and analyze the excitation spectrum of 3He atoms bound to a cluster of 4He atoms by using a previously determined optimum filling of single-fermion orbits with well-defined orbital angular momentum L, spin S, and parity quantum numbers. The study concentrates on the energies and shapes of the three kinds of states for which the fermionic part of the wave function is a single Slater determinant: maximum L or maximum S states within a given orbit, and fully polarized clusters. The picture that emerges is that of systems with strong shell effects, whose binding and excitation energies are essentially determined by averages over configuration at fixed number of particles and spin, i.e., by the monopole properties of an effective Hamiltonian.

Unusual isospin-breaking and isospin-mixing effects in the A=35 mirror nuclei.

Excited states have been studied in 35Ar following the 16O(24Mg,1alpha1n)35Ar fusion-evaporation reaction at 60 MeV using the Ge-detector array GASP. A comparison with the mirror nucleus 35Cl shows two remarkable features: (i) A surprisingly large energy difference for the 13/2(-) states, in which the hitherto overlooked electromagnetic spin-orbit term is shown to play a major role, and (ii) a very different decay pattern for the 7/2(-) states, which provides direct evidence of isospin mixing.

Three-body monopole corrections to realistic interactions.

It is shown that a very simple three-body monopole term can solve practically all the spectroscopic problems-in the p, sd, and pf shells-that were hitherto assumed to need drastic revisions of the realistic potentials.

Isobaric multiplet yrast energies and isospin nonconserving forces.

The isovector and isotensor energy differences between yrast states of isobaric multiplets in the lower half of the pf region are quantitatively reproduced in a shell model context. The isospin nonconserving nuclear interactions are found to be at least as important as the Coulomb potential. Their isovector and isotensor channels are dominated by J=2 and J=0 pairing terms, respectively. The results are sensitive to the radii of the states, whose evolution along the yrast band can be accurately followed.

Spectroscopy with random and displaced random ensembles.

Because of the time reversal invariance of the angular momentum operator J2, the average energies and variances at fixed J for random two-body Hamiltonians exhibit odd-even- J staggering that may be especially strong for J = 0. It is shown that upon ensemble averaging over random runs, this behavior is reflected in the yrast states. Displaced (attractive) random ensembles lead to rotational spectra with strongly enhanced B(E2) transitions for a certain class of model spaces. It is explained how to generalize these results to other forms of collectivity.

Coulomb energy differences in t = 1 mirror rotational bands in (50)Fe and (50)Cr.

Gamma rays from the N = Z-2 nucleus (50)Fe have been observed, establishing the rotational ground state band up to the state J(pi) = 11+ at 6.994 MeV excitation energy. The experimental Coulomb energy differences, obtained by comparison with the isobaric analog states in its mirror (50)Cr, confirm the qualitative interpretation of the backbending patterns in terms of successive alignments of proton and neutron pairs. A quantitative agreement with experiment has been achieved by exact shell model calculations, incorporating the differences in radii along the yrast bands, and properly renormalizing the Coulomb matrix elements in the pf model space.

Molecular mechanisms underlying carotenogenesis in the chromoplast: multilevel regulation of carotenoid-associated genes

In nature, carotenoid function and mode of action are highly determined by the neighboring protein and lipid molecules. Therefore an understanding of the proteins' involvement in carotenoid sequestration would be of great help in elucidating carotenoid function in vivo. Based on a study of the expression of chromoplast-specific carotenoid-associated genes from cucumber corolla (CHRC and CHRD), a working model is presented wherein two major regulatory factors control carotenoid sequestration within the chromoplasts: (i) floral tissue-specific transcriptional regulators of chromoplasto- genesis; and (ii) post-transcriptional regulators related to the amount/type of sequestered carotenoids. This model is supported by the major role transcriptional regulation was found to play in the temporal and spatial expression of the CHRC gene, and by the fact that phytohormones such as gibberellic acid (GA3), abscisic acid and ethylene also acted as transcriptional regulators of CHRC expression. The primary response to GA3 was localized within the CHRC promoter to a 290 bp fragment. Furthermore, we demonstrated strong down-regulation of CHRC expression at post-transcriptional and translational/post-translational levels resulting from inhibition of carotenoid biosynthesis, thus revealing a close link between carotenoid biosynthetic and sequestration machineries.

Genetic engineering for cut-flower improvement.

The application of modern biotechnological approaches to cut flowers has clearly become instrumental and rewarding for the floriculture industry. In recent years, several gene-transfer procedures have been developed for some of the major commercial cut flowers. Using Agrobactrium or microprojectile bombardment, several basic protocols are now available. However, despite the great progress and interest in gene transfer to these crops, their transformation is routine in only a limited number of laboratories, and its application is still considered to be an "art form". This review summarizes the reported gene-transfer procedures for the main cut-flower crops, with an emphasis on the unique factors of each method and the recent progress in introducing new traits of horticultural interest into these species.

Adventitious shoot regeneration from leaf explants of Gypsophila paniculata L.

Adventitious shoots were successfully regenerated from leaf explants of Gypsophila paniculata L. The efficiency of shoot regeneration for cv. Arbel was tested on 18 media based on Murashige and Skoog basal medium containing different concentrations of thidiazuron or 6-benzylaminopurine in combination with naphthaleneacetic acid. Both explant age and that of the cuttings used as leaf donors affected the regeneration efficiency. The highest efficiency of adventitious shoot regeneration was obtained with the oldest leaves originating from the youngest cutting analyzed; on thidiazuron-containing medium, shoots regenerated on average from 67% of the leaves, with an average of seven shoots per explant. This regeneration procedure was suitable for all six commercial cultivars studied. Regenerated shoots elongated, rooted and successfully acclimatized to the greenhouse where they were grown to flowering.