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  • Seidel, P. ; Geyer, M.; Lehninger, D.; Schneider, F.; Klemm, V.; Heitmann, J.:.53 (1) (2013), 237-243
 .

    Seidel, P.

    Krupinski, M. ; Kasic, A.; Hecht, T.; Klude, M.; Erben, E.; Heitmann, J.; Mikolajick, T.: Inline-characterization and step coverage optimization of deposited dielectrics in DRAM structures .26 (2), 6478839 (2013), 253-259.

    Krupinski, M.

    Weinreich, W. ; Wilde, L.; Mueller, J.; Sundqvist, J.; Erben, E.; Heitmann, J.; Lemberger, M.; Bauer, A. J.: Structural properties of as deposited and annealed ZrOinfluenced by atomic layer deposition, substrate, and doping .31 (1) (2013), 01A119/1-01A119/9.

    Weinreich, W.

    Haas, S. ; Schneider, F.; Himcinschi, C.; Klemm, V.; Schreiber, G.; Borany, J. von; Heitmann, J.: Ge nanoparticle formation by thermal treatment of rf-sputtered ZrO/ZrGeOsuperlattices .113 (2013), 044303.

    Haas, S.

    Bordihn, S. ; Mertens, V.; Engelhart, P.; Kersten, F.; Mandoc, M.M.; Müller, J.W.; Kessels, W.M.M.: Surface passivation by AlOand a-SiN:H Films Deposited on Wet-Chemically Conditioned Si Surfaces . 1 (6) (2012), P320-P325 .

    Bordihn, S.

    Benner, F. ; Haas, S.; Schneider, F.; Klemm, V.; Schreiber, G.; Borany, J. von; Mikolajick, T.; Heitmann, J.: Silicon and Germanium Nanoclusters Embedded in Zirconium Dioxide Matrices .1 (6) (2012), N135-N138.

    Benner, F.

    Müller, J. ; Polakowski, P.; Olsen, T.; Müller, S.; Schröder, U.; Heitmann, J.: Stabilization of ferroelectric HfO2: The impact of mechanical encapsulation. presentation: E-MRS Strasbourg, Spring Meeting 2012.

    Müller, J.

    Benner, F. ; Haas, S.; Schneider, F.; Klemm, V.; Schreiber, G.; von Borany, J.; Heitmann, J.: Semiconductor Nanocrystals Embedded in High-k Materials . invited presentation: ECS 221st Meeting Seattle 2012, published in:45 (3) (2012) 9-16.

    Weinreich, W. ; Wilde, L.; Müller, J.; Erben, E.; Heitmann, J.; Lemberger, M.; Bauer: Structural properties of ZrOafter deposition and PDA influenced by ALD, substrate, and doping. presentation: ALD conference Dresden
 2012.

    Krupinski, M. ; Kasic, A.; Hecht, T.; Klude, M.; Heitmann, J.; Erben, E.; Mikolajick, T.: Optical characterization of three-dimensional structures within a DRAM capacitor. poster: SPIE München 2011.

    Numerals and numerology

    Numerical coincidences abound, and they are often so remarkable that it is difficult to explain them rationally. Not surprisingly, many people become convinced that these coincidences have irrational explanations. What, for example, should be made of the following similarities (not all of them numerological) between U.S. Presidents Abraham Lincoln and Cheapest Cheap Sale Great Deals Lloyd FOOTWEAR Laceup shoes su YOOXCOM Official Site Outlet Locations Cheap Online N84kFv
    , taken from a far more extensive list in Martin Gardner’s The Magic Numbers of Dr. Matrix (1985)?

    Lincoln was elected president in 1860, Kennedy in 1960.
    Both were assassinated on a Friday.
    Lincoln was killed in Ford’s Theatre; Kennedy was killed riding in a Lincoln convertible made by the Ford Motor Company .
    Both were succeeded by Southern Democrats named Johnson.
    Andrew Johnson was born in 1808, Lyndon Johnson in 1908.
    The first name of Lincoln’s private secretary was John, the last name of Kennedy’s private secretary was Lincoln.
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    was born in 1839, Lee Harvey Oswald in 1939.
    Booth shot Lincoln in a theatre and fled to a warehouse; Oswald shot Kennedy from a warehouse and fled to a theatre.
    and both have 15 letters.
    The first public suggestion that Lincoln should run for president proposed that his running mate should be John Kennedy . ( John Pendleton Kennedy was a Maryland politician.)
    Shift each letter of forward by six letters in the alphabet and you get , the initials of Lee Harvey Oswald.

    One explanation for coincidences of this kind is selective reporting. Anything that fits is kept; anything that does not is discarded. Thus, the coincidence of day of the week for the assassinations is emphasized; the differences in month and number of day in the month are ignored. (Lincoln was assassinated on April 14, Kennedy on November 22.) More subtly, only one choice is made from many possibilities, the one that maintains the numerological pattern. Sometimes the date of birth is used, sometimes the date of election. If those do not work, how about the dates of college graduation, marriage, firstborn child, first election to office, or death? Moreover, some “facts” turn out to be false. The correct birth date for Booth is now thought to be 1838, not 1839, and Booth actually fled to a barn. It is common for coincidences to be exaggerated in this manner. And once one starts looking…Lincoln had a beard. Did Kennedy? No, he was clean-shaven. Do not mention beards, then.

    Many of the coincidences listed here are exaggerations, lies, elaborations chosen from an Tods Gommino pink leather loafers Discount Clearance With Credit Card Inexpensive cyUh4sc
    range of potential targets, or the result of a hidden selective process. Still, a few of the coincidences are quite startling. Although rational explanations exist, a true believer cannot be convinced. It is in this fertile territory that number mysticism thrives.

    Submitted 1 February, 2016; originally announced February 2016.

    arXiv:1601.01737 [, other ] astro-ph.GA

    doi 10.1093/mnras/stx1847

    A Model For Intergalactic Filaments and Galaxy Formation During the First Gigayear

    Authors: A. Gayler Harford , Andrew J. S. Hamilton

    Abstract : We propose a physically based, analytic model for intergalactic filaments during the first gigayear of the universe. The structure of a filament is based upon a gravitationally bound, isothermal cylinder of gas. The model successfully predicts for a cosmological simulation the total mass per unit length of a filament (dark matter plus gas) based solely upon the sound speed of the gas component, co… ▽ More We propose a physically based, analytic model for intergalactic filaments during the first gigayear of the universe. The structure of a filament is based upon a gravitationally bound, isothermal cylinder of gas. The model successfully predicts for a cosmological simulation the total mass per unit length of a filament (dark matter plus gas) based solely upon the sound speed of the gas component, contrary to the expectation for collisionless dark matter aggregation. It argues that the gas, through its hydrodynamic properties, plays a key role in filament structure rather than being a passive passenger in a preformed dark matter potential. The dark matter of a galaxy follows the classic equation of collapse of a spherically symmetric overdensity in an expanding universe. In contrast, the gas usually collapses more slowly. The relative rates of collapse of these two components for individual galaxies can explain the varying baryon deficits of the galaxies under the assumption that matter moves along a single filament passing through the galaxy centre, rather than by spherical accretion. The difference in behaviour of the dark matter and gas can be simply and plausibly related to the model. The range of galaxies studied includes that of the so-called "too big to fail" galaxies, which are thought to be problematic for the standard Lambda-CDM model of the universe. The isothermal-cylinder model suggests a simple explanation for why these galaxies are, unaccountably, missing from the night sky. △ Less

    Submitted 11 June, 2017; v1 submitted 7 January, 2016; originally announced January 2016.

    Comments: 16 pages, 26 figures 18 pages, 27 figures. Changes have been made in response to reviewer's comments

    Journal ref: Mon. Not. Roy. Astron. Soc. 471, 4760-4775 (2017)

    arXiv:1512.02632 [, , other ] math.DG

    The Higgs boson for mathematicians. Lecture notes on gauge theory and symmetry breaking

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