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    Mari Carmen Roldán

    Reissner’s fiber (RF) is a threadlike structure present in the third and fourth ventricles and in the central canal of the spinal cord. RF develops by the assembly of glycoproteins released into the cerebrospinal fluid (CSF) by the... more
    Reissner’s fiber (RF) is a threadlike structure present in the third and fourth ventricles and in the central canal of the spinal cord. RF develops by the assembly of glycoproteins released into the cerebrospinal fluid (CSF) by the subcommissural organ (SCO). SCO cells differentiate early during embryonic development. In chick embryos, the release into the CSF starts at embryonic day 7 (E7). However, RF does not form until E11, suggesting that a factor other than release is required for RF formation. The aim of the present investigation was to establish whether the factor(s) triggering RF formation is (are) intrinsic or extrinsic to the SCO itself. For this purpose, SCO explants from E13 chick embryos (a stage at which RF has formed) were grafted at two different developmental stages. After grafting, host embryos were allowed to survive for 6–7 days, reaching E9 (group 1) and E13 (group 2). In experimental group 1, the secretion released by the grafted SCOs never formed a RF; instead, it aggregated as a flocculent material. In experimental group 2, grafted SCO explants were able to develop an RF-like structure, similar to a control RF. These results suggest that the factor triggering RF formation is not present in the SCO itself, since E13 SCO secretion forms an RF in E13 brains but never develops RF-like structures when placed in earlier developmental environments. Furthermore, the glycoproteins released by implanted SCOs bind specifically to several structures: the apical portion of the mesencephalic floor plate and the choroid plexus of the third and fourth ventricles.
    This is a report of a woman in the fifth decade of life with primary antiphospholipid syndrome and involvement of a heart valve. Diagnosis was reached with echocardiography and serological studies.
    We introduce quantum walks with a time-dependent coin, and show how they include, as a particular case, the generalized quantum walk recently studied by Wojcik et al. {[}Phys. Rev. Lett. \textbf{93}, 180601(2004){]} which exhibits... more
    We introduce quantum walks with a time-dependent coin, and show how they include, as a particular case, the generalized quantum walk recently studied by Wojcik et al. {[}Phys. Rev. Lett. \textbf{93}, 180601(2004){]} which exhibits interesting dynamical localization and quasiperiodic dynamics. Our proposal allows for a much easier implementation of this particular rich dynamics than the original one. Moreover, it allows for an additional control on the walk, which can be used to compensate for phases appearing due to external interactions. To illustrate its feasibility, we discuss an example using an optical cavity. We also derive an approximated solution in the continuous limit (long--wavelength approximation) which provides physical insight about the process.