The simplest schoolboy is now familiar with truths for which Archimedes would have sacrificed his life.
Colloquia
Coffee starts at 12:00 PM and talk starts at 12:15 PM
1. D. Aebisher; D. Bartusik; Y. Liu; Y. Zhao; M. Barahman; Q. Xu; A. M. Lyons; A. Greer "Superhydrophobic Photosensitizers. Mechanistic Studies of 1O2 Generation in the Plastron and Solid/Liquid Droplet Interface" J. Am. Chem. Soc. 2013, 135, 18990-18998.
2. Y. Zhao; Y. Liu; Q. Xu; M. Barahman; D. Bartusik; A. Greer; A. M. Lyons "Singlet Oxygen Generation on Porous Superhydrophobic Surfaces: Effect of Gas Flow and Sensitizer Wetting on Trapping Efficiency" J. Phys. Chem. A 2014, 118, 10364-10371.
3. D. Bartusik; D. Aebisher; A. M. Lyons; A. Greer "Bacterial Inactivation by a Singlet Oxygen Bubbler: Identifying Factors Controlling the Toxicity of 1O2 Bubbles" Environ. Sci. Technol. 2012, 46, 12098-12104.
4. D. Bartusik; D. Aebisher; B. Ghafari; A. M. Lyons; A. Greer "Generating Singlet Oxygen Bubbles: A New Mechanism for Gas-Liquid Oxidations in Water" Langmuir 2012, 28, 3053-3060.
5. R. Choudhury; A. Greer "Synergism Between Airborne Singlet Oxygen and a Trisubstituted Olefin Sulfonate for the Inactivation of Bacteria" Langmuir 2014, 30, 3599-3605.
Space-division multiplexing (SDM), using novel fiber with multiple cores or multiple transverse modes in a large core, is being widely studied as the next wave of fiber optics. Both multicore and multimode approaches have been successfully demonstrated in research, with the throughput of a single multicore fiber exceeding 1 Pb/s. Nonetheless, the challenges facing SDM are numerous and daunting. Multicore fibers are difficult to fabricate, multimode systems are subject to severe inter-modal crosstalk, and successful reduction in the cost per bit will require advanced functional integration of transceivers, amplifiers, mode multiplexers, and other elements of the photonic communications ecosystem. For efficient network operation, flexible lightpath routing is essential, and SDM offers a number of ways to allocate lightpaths among wavelengths and spatial modes. Finally, to assure economic viability at all stages of the SDM introduction, a deployment strategy that supports interworking of SDM and non-SDM sections is needed.
In this talk, I will review the past, present, and future of SDM research, and suggest some criteria for a successful commercial introduction of SDM technology.
Multiple scattering of waves in disordered media is often seen as a nightmare whether it be for communication, imaging or focusing purposes. The ability to control wave propagation through scattering media is thus of fundamental interest in many domains of wave physics, ranging from optics or acoustics to medical imaging or electromagnetism. Thirty years ago, it was shown theoretically that a properly designed combination of incident waves could be fully transmitted through (or reflected by) a disordered medium. Although this remarkable prediction has attracted a great deal of attention, open and closed channels have never been accessed experimentally.
Here, we study the propagation of elastic waves through a disordered elastic waveguide. Thereby, we present experimental measurements of the full S-matrix across a disordered elastic wave guide. To that aim, laser-ultrasonic techniques have been used in order to obtain a satisfying spatial sampling of the field at the input and output of the scattering medium. The unitarity of the S−matrix is investigated and the eigenvalues of the transmission matrix are shown to follow the expected bimodal distribution. Full transmission and reflection of waves propagating through disorder are obtained for the first time experimentally. The wave-fields associated to these open and closed channels are imaged within the scattering medium to highlight the interference effects operating in each case.
In the second part of the talk, we study beam-like states which can be seen as spatio-temporal open / closed channels. To that aim, the eigenstates of the Wigner-Smith time-delay matrix are considered in a regular cavity and a weakly disordered medium. The propagation of the wave-packets associated to these transmitted trajectory-like states is investigated.
In my presentation I will cover the basic principles of artificial photosynthesis and will explain how simple synthetic models may be used to mimic the action of natural photosystems. I will follow with several examples of catalytic transformations relevant to the production of solar fuels such as water oxidation and the reduction of protons and carbon dioxide. In each of these examples the importance of coupling the movement of multiple equivalents of electrons with proton transfer will be emphasized. Also, the modern time-resolved spectroscopy techniques such as pulse radiolysis and laser flash photolysis will be presented as experimental tools for unraveling complex mechanisms of PCET transformations which take place during catalytic cycles.
Inspired by these results we undertook a detailed SHB study of spectral dynamics in several photosynthetic complexes, with the main focus on the CP43 antenna complex [2] of Photosystem II and dimeric Cytochrome b6f [3]. We also developed a unified approach to modeling SHB and spectral hole recovery, at fixed (burn) temperature and upon thermocycling. This approach relies on the argument that in the presence of “spectral memory” (holes recovering mostly due to burnt systems returning to the pre-burn configuration) the barrier distributions encoded into the non-saturated spectral holes and manifesting during the hole recovery differ from the full true barrier distributions. These partial barrier distributions are vastly different for different shapes of the true full distributions, and one can easily distinguish their manifestations. Quantitatively, all complexes we have explored so far exhibit similar barrier distribution parameters, distinct from those of some simple organic glasses. Qualitatively, however, barrier distribution shapes show great variability. Unlike in CP43 [2], the distributions of barriers between protein sub-states involved in light-induced conformational changes (SHB) in Cytochrome b6f are more likely glass-like ~V^(0.5) (V is the barrier height), and not Gaussian.
There is a high degree of correlation between the heights of the barriers in the ground and excited states in the individual pigment-protein systems, as well as nearly perfect spectral memory. Both spectral hole burning and recovery are due to phonon-assisted tunneling associated with the increase of the energy of a scattered phonon. As the latter is unlikely for simultaneously both the hole burning and hole recovery, proteins must exhibit a NPHB mechanism involving diffusion of the free volume towards the pigment. Entities involved in the light-induced conformational changes are characterized by md2 value of about 1.0.10-46 kg.m2. Thus, these entities are protons or, alternatively, small groups of atoms experiencing sub-Å shifts. However, explaining all SHB and recovery data simultaneously, employing just one barrier distribution, requires a drastic decrease in the attempt frequency to about 100 MHz. This decrease may occur due to cooperative effects.
1. Grozdanov, D.; Herascu, N.; Reinot, T.; Jankowiak, R.; Zazubovich, V. J. Phys. Chem. 2010, 114, 3426-3438.
2. Najafi, M., Herascu, N., Seibert, M., Picorel, R., Jankowiak, R., Zazubovich, V., J. Phys. Chem. B 2012, 116, 11780.
3. Najafi, M.; Herascu, N.; Shafiei, G.; Picorel, R.; Zazubovich, V.; J. Phys. Chem. B 2015, 10.1021/acs.jpcb.5b02845
1. D. A. Garanin, E. M. Chudnovsky, and T. C. Proctor, The Role of Vortices in the Three-Dimensional Random-Field XY Model, Europhysics Letters 103, 67009 (2013).
2. D. A. Garanin, E. M. Chudnovsky, and T. C. Proctor, Random-Field XY Model in Three Dimensions, Physical Review B 88, 224418 (2013).
3. T. C. Proctor, D. A. Garanin, and E. M. Chudnovsky, Random Fields, Topology, and the Imry-Ma Argument, Physical Review Letters 112, 097201 (2014).
4. D. A. Garanin and E. M. Chudnovsky, Ordered vs Disordered States of the Random-Field Model in Three Dimensions, European Physics Journal B 88, 81 (2015).
5. T. C. Proctor, E. M. Chudnovsky, and D. A. Garanin, Scaling of Coercivity in a 3d Random Anisotropy Magnet, Journal of Magnetism and Magnetic Materials 384, 181 (2015).
6. T. C. Proctor and E. M. Chudnovsky, Effect of Dilute Random Field on Continuous Symmetry Order Parameter, Physical Review B 91, 140201(R) (2015).
I will report chemical abundances for a sample of M giants in the inner halo of the Milky Way. Abundances are derived for a-elements and neutron capture elements. By analyzing the multi-dimensional abundance space, the formation site of the halo giants – in-situ, kicked-out disk, or accreted – can be assessed. Additionally, I will report results from a study to understand the origin of a diffuse cloud of stars known as Triangulum-Andromeda.
[1] A. P. Slobozhanyuk, A. N. Poddubny, A. J. E. Raaijmakers, C. A. T. van den Berg, A. V. Kozachenko, I. A. Dubrovina, I. V. Melchakova, Yu. S. Kivshar, P. A. Belov, "Enhancement of magnetic resonance imaging with metasurfaces", arXiv:1507.01411 (2015).
