April 27, 2015

  • Date:26SundayApril 201529WednesdayApril 2015

    Cortical Development in Health and Disease

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    Time
    08:00 - 18:00
    Location
    David Lopatie Conference Centre
    Kimmel Auditorium
    Chairperson
    Orly Reiner
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  • Date:27MondayApril 2015

    Pearlman Lecture - "Exploring Complex Chemical Systems"

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    Time
    11:00 - 12:30
    Location
    Gerhard M.J. Schmidt Lecture Hall
    Lecturer
    Prof. Leroy (Lee) Cronin
    School of Chemistry, University of Glasgow
    Organizer
    Faculty of Chemistry
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    DetailsShow full text description of How do high nuclearity inorganic and supramolecular assembli...»
    How do high nuclearity inorganic and supramolecular assemblies form? Can understanding the minimal information content of the structures help us understand their assembly? Is there a general route to explore the mechanism and how can one given compound dominate from a combinatorial explosion of possibilities? In our current work we are using new approaches to probability theory and template design to explore the possibility of using high probability templates to assemble low probability structures with 1000s of atoms in a single molecule. Take the example of a recent molecule discovered in our laboratory: A palladium oxometalate {Pd84}-ring cluster 3.3 nm in diameter; [Pd84O42(OAc)28(PO4)42]70- ({Pd84} ≡ {Pd12}7) which is formed in water just by mixing two reagents at room temperature and can be observed in solution within a few days mixing and crystallised with a week, see Figure 1. The key question is how could a ring as large as the {Pd84} spontaneously form and crystallize within the period of days. Indeed the state space for the molecule, just considering the unique arrangements of distinct 84 Pd atoms, ignoring symmetry, gives an upper limit on the combinatorial space of 84! = 3.3 × 10126. It is therefore perhaps safe to assume that the structure therefore did not ‘spontaneously’ form by random chance, but a series of templating events, combined with the correct kinetics, allowed this cluster to be selected from the vast envelope of possible structures available in solution. In this lecture I will propose a new theory that may explain the mechanism of self-assembly of gigantic systems, as well as an approach to understand and use the information content of complex molecular structures.
    Colloquia
  • Date:27MondayApril 2015

    Chirality and Polarity: Two Mechanisms for Microstructure Formation in Soft Materials

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    Time
    14:15
    Location
    Edna and K.B. Weissman Building of Physical Sciences
    Room A
    Lecturer
    Jonathan Selinger
    Kent State University
    Organizer
    Department of Physics of Complex Systems
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    AbstractShow full text abstract about From liquid crystals to biological membranes, many soft mate...»
    From liquid crystals to biological membranes, many soft materials exhibit order in the molecular orientation. This order may be uniform across the material, or it may have some systematic modulation. In this talk, we survey mechanisms for the formation of modulated structures. Many of these structures arise from chirality (left-right asymmetry), which induces a favored twist. On macroscopic scale, this favored twist leads to cholesteric liquid crystals (with helical modulation), blue phases (with cubic lattices of double twist), and twisted membranes. We point out that related structures can arise from polarity (vector asymmetry), which induces a favored splay or bend. We compare and contrast polar structures with chiral structures, and show how each can be observed in experiments.

    Lecture