TY - INPR A1 - Pikovskij, Arkadij T1 - Comment on "Asymptotic Phase for Stochastic Oscillators" T2 - Physical review letters Y1 - 2015 U6 - https://doi.org/10.1103/PhysRevLett.115.069401 SN - 0031-9007 SN - 1079-7114 VL - 115 IS - 6 PB - American Physical Society CY - College Park ER - TY - INPR A1 - Bürger, Gerd T1 - Comment on "Bias correction, quantile mapping, and downscaling: revisiting the inflation issue" T2 - Journal of climate N2 - In a recent paper, Maraun describes the adverse effects of quantile mapping on downscaling. He argues that when large-scale GCM variables are rescaled directly to small-scale fields or even station data, genuine small-scale covariability is lost and replaced by uniform variability inherited from the larger scales. This leads to a misrepresentation mainly of areal means and long-term trends. This comment acknowledges the former point, although the argument is relatively old, but disagrees with the latter, showing that grid-size long-term trends can be different from local trends. Finally, because it is partly incorrectly addressed, some clarification is added regarding the inflation issue, stressing that neither randomization nor inflation is free of unverified assumptions. KW - Climate change KW - Statistics KW - Climate variability Y1 - 2014 U6 - https://doi.org/10.1175/JCLI-D-13-00184.1 SN - 0894-8755 SN - 1520-0442 VL - 27 IS - 4 SP - 1819 EP - 1820 PB - American Meteorological Soc. CY - Boston ER - TY - INPR A1 - Föhlisch, Alexander A1 - de Groot, F. M. F. A1 - Odelius, Michael A1 - Techert, Simone A1 - Wernet, P. T1 - Comment on "state-dependent electron delocalization dynamics at the solute-solvent interface: soft-x-ray absorption spectroscopy and lambda b initio calculations" T2 - Physical review letters Y1 - 2014 U6 - https://doi.org/10.1103/PhysRevLett.112.129302 SN - 0031-9007 SN - 1079-7114 VL - 112 IS - 12 PB - American Physical Society CY - College Park ER - TY - INPR A1 - Henkel, Carsten A1 - Pieplow, Gregor T1 - Reply to Comment on 'Fully covariant radiation force on a polarizable particle' T2 - New journal of physics : the open-access journal for physics N2 - We argue that the theories of Volokitin and Persson (2014 New J. Phys. 16 118001), Dedkov and Kyasov (2008 J. Phys.: Condens. Matter 20 354006), and Pieplow and Henkel (2013 New J. Phys. 15 023027) agree on the electromagnetic force on a small, polarizable particle that is moving parallel to a planar, macroscopic body, as far as the contribution of evanescent waves is concerned. The apparent differences are discussed in detail and explained by choices of units and integral transformations. We point out in particular the role of the Lorentz contraction in the procedure used by Volokitin and Persson, where a macroscopic body is 'diluted' to obtain the force on a small particle. Differences that appear in the contribution of propagating photons are briefly mentioned. KW - applied classical electromagnetism KW - fluctuation phenomena KW - random processes KW - noise KW - Brownian motion KW - mechanical effects of light Y1 - 2014 U6 - https://doi.org/10.1088/1367-2630/16/11/118002 SN - 1367-2630 VL - 16 PB - IOP Publ. Ltd. CY - Bristol ER - TY - INPR A1 - Hilczer, Börn A1 - Gerhard, Reimund A1 - Scott, James F. T1 - Special Issue of Ferroelectrics in Honor of S. B. Lang T2 - Ferroelectrics Y1 - 2014 U6 - https://doi.org/10.1080/00150193.2014.964099 SN - 0015-0193 SN - 1563-5112 VL - 472 IS - 1 SP - VII EP - VIII PB - Routledge, Taylor & Francis Group CY - Abingdon ER - TY - INPR A1 - Gerhard, Reimund T1 - Sidney Lang - his collaboration with the University of Potsdam T2 - Ferroelectrics Y1 - 2014 U6 - https://doi.org/10.1080/00150193.2014.967090 SN - 0015-0193 SN - 1563-5112 VL - 472 IS - 1 SP - 5 EP - 5 PB - Routledge, Taylor & Francis Group CY - Abingdon ER - TY - INPR A1 - Scherf, Ullrich A1 - Tian, He T1 - Organic electronics/optics for an energetic life T2 - Advanced materials Y1 - 2012 U6 - https://doi.org/10.1002/adma.201104917 SN - 0935-9648 VL - 24 IS - 5 SP - 576 EP - 579 PB - Wiley-Blackwell CY - Malden ER - TY - INPR A1 - Acharya, B. S. A1 - Actis, M. A1 - Aghajani, T. A1 - Agnetta, G. A1 - Aguilar, J. A1 - Aharonian, Felix A. A1 - Ajello, M. A1 - Akhperjanian, A. G. A1 - Alcubierre, M. A1 - Aleksic, J. A1 - Alfaro, R. A1 - Aliu, E. A1 - Allafort, A. J. A1 - Allan, D. A1 - Allekotte, I. A1 - Amato, E. A1 - Anderson, J. A1 - Angüner, Ekrem Oǧuzhan A1 - Antonelli, L. A. A1 - Antoranz, P. A1 - Aravantinos, A. A1 - Arlen, T. A1 - Armstrong, T. A1 - Arnaldi, H. A1 - Arrabito, L. A1 - Asano, K. A1 - Ashton, T. A1 - Asorey, H. G. A1 - Awane, Y. A1 - Baba, H. A1 - Babic, A. A1 - Baby, N. A1 - Baehr, J. A1 - Bais, A. A1 - Baixeras, C. A1 - Bajtlik, S. A1 - Balbo, M. A1 - Balis, D. A1 - Balkowski, C. A1 - Bamba, A. A1 - Bandiera, R. A1 - Barber, A. A1 - Barbier, C. A1 - Barcelo, M. A1 - Barnacka, Anna A1 - Barnstedt, Jürgen A1 - Barres de Almeida, U. A1 - Barrio, J. A. A1 - Basili, A. A1 - Basso, S. A1 - Bastieri, D. A1 - Bauer, C. A1 - Baushev, Anton N. A1 - Becerra Gonzalez, J. A1 - Becherini, Yvonne A1 - Bechtol, K. C. A1 - Tjus, J. Becker A1 - Beckmann, Volker A1 - Bednarek, W. A1 - Behera, B. A1 - Belluso, M. A1 - Benbow, W. A1 - Berdugo, J. A1 - Berger, K. A1 - Bernard, F. A1 - Bernardino, T. A1 - Bernlöhr, K. A1 - Bhat, N. A1 - Bhattacharyya, S. A1 - Bigongiari, C. A1 - Biland, A. A1 - Billotta, S. A1 - Bird, T. A1 - Birsin, E. A1 - Bissaldi, E. A1 - Biteau, Jonathan A1 - Bitossi, M. A1 - Blake, S. A1 - Blanch Bigas, O. A1 - Blasi, P. A1 - Bobkov, A. A. A1 - Boccone, V. A1 - Boettcher, Markus A1 - Bogacz, L. A1 - Bogart, J. A1 - Bogdan, M. A1 - Boisson, Catherine A1 - Boix Gargallo, J. A1 - Bolmont, J. A1 - Bonanno, G. A1 - Bonardi, A. A1 - Bonev, T. A1 - Bonifacio, P. A1 - Bonnoli, G. A1 - Bordas, Pol A1 - Borgland, A. W. A1 - Borkowski, Janett A1 - Bose, R. A1 - Botner, O. A1 - Bottani, A. A1 - Bouchet, L. A1 - Bourgeat, M. A1 - Boutonnet, C. A1 - Bouvier, A. A1 - Brau-Nogue, S. A1 - Braun, I. A1 - Bretz, T. A1 - Briggs, M. S. A1 - Bringmann, T. A1 - Brook, P. A1 - Brun, Pierre A1 - Brunetti, L. A1 - Buanes, T. A1 - Buckley, J. H. A1 - Buehler, R. A1 - Bugaev, V. A1 - Bulgarelli, A. A1 - Bulik, Tomasz A1 - Busetto, G. A1 - Buson, S. A1 - Byrum, K. A1 - Cailles, M. A1 - Cameron, R. A. A1 - Camprecios, J. A1 - Canestrari, R. A1 - Cantu, S. A1 - Capalbi, M. A1 - Caraveo, P. A. A1 - Carmona, E. A1 - Carosi, A. A1 - Carr, John A1 - Carton, P. H. A1 - Casanova, Sabrina A1 - Casiraghi, M. A1 - Catalano, O. A1 - Cavazzani, S. A1 - Cazaux, S. A1 - Cerruti, M. A1 - Chabanne, E. A1 - Chadwick, Paula M. A1 - Champion, C. A1 - Chen, Andrew A1 - Chiang, J. A1 - Chiappetti, L. A1 - Chikawa, M. A1 - Chitnis, V. R. A1 - Chollet, F. A1 - Chudoba, J. A1 - Cieslar, M. A1 - Cillis, A. N. A1 - Cohen-Tanugi, J. A1 - Colafrancesco, Sergio A1 - Colin, P. A1 - Calome, J. A1 - Colonges, S. A1 - Compin, M. A1 - Conconi, P. A1 - Conforti, V. A1 - Connaughton, V. A1 - Conrad, Jan A1 - Contreras, J. L. A1 - Coppi, P. A1 - Corona, P. A1 - Corti, D. A1 - Cortina, J. A1 - Cossio, L. A1 - Costantini, H. A1 - Cotter, G. A1 - Courty, B. A1 - Couturier, S. A1 - Covino, S. A1 - Crimi, G. A1 - Criswell, S. J. A1 - Croston, J. A1 - Cusumano, G. A1 - Dafonseca, M. A1 - Dale, O. A1 - Daniel, M. A1 - Darling, J. A1 - Davids, I. A1 - Dazzi, F. A1 - De Angelis, A. A1 - De Caprio, V. A1 - De Frondat, F. A1 - de Gouveia Dal Pino, E. M. A1 - de la Calle, I. A1 - De La Vega, G. A. A1 - Lopez, R. de los Reyes A1 - De Lotto, B. A1 - De Luca, A. A1 - de Mello Neto, J. R. T. A1 - de Naurois, M. A1 - de Oliveira, Y. A1 - de Ona Wilhelmi, E. A1 - de Souza, V. A1 - Decerprit, G. A1 - Decock, G. A1 - Deil, C. A1 - Delagnes, E. A1 - Deleglise, G. A1 - Delgado, C. A1 - Della Volpe, D. A1 - Demange, P. A1 - Depaola, G. A1 - Dettlaff, A. A1 - Di Paola, A. A1 - Di Pierro, F. A1 - Diaz, C. A1 - Dick, J. A1 - Dickherber, R. A1 - Dickinson, H. A1 - Diez-Blanco, V. A1 - Digel, S. A1 - Dimitrov, D. A1 - Disset, G. A1 - Djannati-Ataï, A. A1 - Doert, M. A1 - Dohmke, M. A1 - Domainko, W. A1 - Prester, Dijana Dominis A1 - Donat, A. A1 - Dorner, D. A1 - Doro, M. A1 - Dournaux, J-L. A1 - Drake, G. A1 - Dravins, D. A1 - Drury, L. A1 - Dubois, F. A1 - Dubois, R. A1 - Dubus, G. A1 - Dufour, C. A1 - Dumas, D. A1 - Dumm, J. A1 - Durand, D. A1 - Dyks, J. A1 - Dyrda, M. A1 - Ebr, J. A1 - Edy, E. A1 - Egberts, Kathrin A1 - Eger, P. A1 - Einecke, S. A1 - Eleftheriadis, C. A1 - Elles, S. A1 - Emmanoulopoulos, D. A1 - Engelhaupt, D. A1 - Enomoto, R. A1 - Ernenwein, J-P A1 - Errando, M. A1 - Etchegoyen, A. A1 - Evans, P. A1 - Falcone, A. A1 - Fantinel, D. A1 - Farakos, K. A1 - Farnier, C. A1 - Fasola, G. A1 - Favill, B. A1 - Fede, E. A1 - Federici, S. A1 - Fegan, S. A1 - Feinstein, F. A1 - Ferenc, D. A1 - Ferrando, P. A1 - Fesquet, M. A1 - Fiasson, A. A1 - Fillin-Martino, E. A1 - Fink, D. A1 - Finley, C. A1 - Finley, J. P. A1 - Fiorini, M. A1 - Firpo Curcoll, R. A1 - Flores, H. A1 - Florin, D. A1 - Focke, W. A1 - Foehr, C. A1 - Fokitis, E. A1 - Font, L. A1 - Fontaine, G. A1 - Fornasa, M. A1 - Foerster, A. A1 - Fortson, L. A1 - Fouque, N. A1 - Franckowiak, A. A1 - Fransson, C. A1 - Fraser, G. A1 - Frei, R. A1 - Albuquerque, I. F. M. A1 - Fresnillo, L. A1 - Fruck, C. A1 - Fujita, Y. A1 - Fukazawa, Y. A1 - Fukui, Y. A1 - Funk, S. A1 - Gaebele, W. A1 - Gabici, S. A1 - Gabriele, R. A1 - Gadola, A. A1 - Galante, N. A1 - Gall, D. A1 - Gallant, Y. A1 - Gamez-Garcia, J. A1 - Garcia, B. A1 - Garcia Lopez, R. A1 - Gardiol, D. A1 - Garrido, D. A1 - Garrido, L. A1 - Gascon, D. A1 - Gaug, M. A1 - Gaweda, J. A1 - Gebremedhin, L. A1 - Geffroy, N. A1 - Gerard, L. A1 - Ghedina, A. A1 - Ghigo, M. A1 - Giannakaki, E. A1 - Gianotti, F. A1 - Giarrusso, S. A1 - Giavitto, G. A1 - Giebels, B. A1 - Gika, V. A1 - Giommi, P. A1 - Girard, N. A1 - Giro, E. A1 - Giuliani, A. A1 - Glanzman, T. A1 - Glicenstein, J. -F. A1 - Godinovic, N. A1 - Golev, V. A1 - Gomez Berisso, M. A1 - Gomez-Ortega, J. A1 - Gonzalez, M. M. A1 - Gonzalez, A. A1 - Gonzalez, F. A1 - Gonzalez Munoz, A. A1 - Gothe, K. S. A1 - Gougerot, M. A1 - Graciani, R. A1 - Grandi, P. A1 - Granena, F. A1 - Granot, J. A1 - Grasseau, G. A1 - Gredig, R. A1 - Green, A. A1 - Greenshaw, T. A1 - Gregoire, T. A1 - Grimm, O. A1 - Grube, J. A1 - Grudzinska, M. A1 - Gruev, V. A1 - Gruenewald, S. A1 - Grygorczuk, J. A1 - Guarino, V. A1 - Gunji, S. A1 - Gyuk, G. A1 - Hadasch, D. A1 - Hagiwara, R. A1 - Hahn, J. A1 - Hakansson, N. A1 - Hallgren, A. A1 - Hamer Heras, N. A1 - Hara, S. A1 - Hardcastle, M. J. A1 - Harris, J. A1 - Hassan, T. A1 - Hatanaka, K. A1 - Haubold, T. A1 - Haupt, A. A1 - Hayakawa, T. A1 - Hayashida, M. A1 - Heller, R. A1 - Henault, F. A1 - Henri, G. A1 - Hermann, G. A1 - Hermel, R. A1 - Herrero, A. A1 - Hidaka, N. A1 - Hinton, J. A1 - Hoffmann, D. A1 - Hofmann, W. A1 - Hofverberg, P. A1 - Holder, J. A1 - Horns, D. A1 - Horville, D. A1 - Houles, J. A1 - Hrabovsky, M. A1 - Hrupec, D. A1 - Huan, H. A1 - Huber, B. A1 - Huet, J. -M. A1 - Hughes, G. A1 - Humensky, T. B. A1 - Huovelin, J. A1 - Ibarra, A. A1 - Illa, J. M. A1 - Impiombato, D. A1 - Incorvaia, S. A1 - Inoue, S. A1 - Inoue, Y. A1 - Ioka, K. A1 - Ismailova, E. A1 - Jablonski, C. A1 - Jacholkowska, A. A1 - Jamrozy, M. A1 - Janiak, M. A1 - Jean, P. A1 - Jeanney, C. A1 - Jimenez, J. J. A1 - Jogler, T. A1 - Johnson, T. A1 - Journet, L. A1 - Juffroy, C. A1 - Jung, I. A1 - Kaaret, P. A1 - Kabuki, S. A1 - Kagaya, M. A1 - Kakuwa, J. A1 - Kalkuhl, C. A1 - Kankanyan, R. A1 - Karastergiou, A. A1 - Kaercher, K. A1 - Karczewski, M. A1 - Karkar, S. A1 - Kasperek, Aci. A1 - Kastana, D. A1 - Katagiri, H. A1 - Kataoka, J. A1 - Katarzynski, K. A1 - Katz, U. A1 - Kawanaka, N. A1 - Kellner-Leidel, B. A1 - Kelly, H. A1 - Kendziorra, E. A1 - Khelifi, B. A1 - Kieda, D. B. A1 - Kifune, T. A1 - Kihm, T. A1 - Kishimoto, T. A1 - Kitamoto, K. A1 - Kluzniak, W. A1 - Knapic, C. A1 - Knapp, J. w A1 - Knoedlseder, J. A1 - Koeck, F. A1 - Kocot, J. A1 - Kodani, K. A1 - Koehne, J. -H. A1 - Kohri, K. A1 - Kokkotas, K. A1 - Kolitzus, D. A1 - Komin, N. A1 - Kominis, I. A1 - Konno, Y. A1 - Koeppel, H. A1 - Korohoda, P. A1 - Kosack, K. A1 - Koss, G. A1 - Kossakowski, R. A1 - Kostka, P. A1 - Koul, R. A1 - Kowal, G. A1 - Koyama, S. A1 - Koziol, J. A1 - Kraehenbuehl, T. A1 - Krause, J. A1 - Krawzcynski, H. A1 - Krennrich, F. A1 - Krepps, A. A1 - Kretzschmann, A. A1 - Krobot, R. A1 - Krueger, P. A1 - Kubo, H. A1 - Kudryavtsev, V. A. A1 - Kushida, J. A1 - Kuznetsov, A. A1 - La Barbera, A. A1 - La Palombara, N. A1 - La Parola, V. A1 - La Rosa, G. A1 - Lacombe, K. A1 - Lamanna, G. A1 - Lande, J. A1 - Languignon, D. A1 - Lapington, J. A1 - Laporte, P. A1 - Lavalley, C. A1 - Le Flour, T. A1 - Le Padellec, A. A1 - Lee, S. -H. A1 - Lee, W. H. A1 - Leigui de Oliveira, M. A. A1 - Lelas, D. A1 - Lenain, J. -P. A1 - Leopold, D. J. A1 - Lerch, T. A1 - Lessio, L. A1 - Lieunard, B. A1 - Lindfors, E. A1 - Liolios, A. A1 - Lipniacka, A. A1 - Lockart, H. A1 - Lohse, T. A1 - Lombardi, S. A1 - Lopatin, A. A1 - Lopez, M. A1 - Lopez-Coto, R. A1 - Lopez-Oramas, A. A1 - Lorca, A. A1 - Lorenz, E. A1 - Lubinski, P. A1 - Lucarelli, F. A1 - Luedecke, H. A1 - Ludwin, J. A1 - Luque-Escamilla, P. L. A1 - Lustermann, W. A1 - Luz, O. A1 - Lyard, E. A1 - Maccarone, M. C. A1 - Maccarone, T. J. A1 - Madejski, G. M. A1 - Madhavan, A. A1 - Mahabir, M. A1 - Maier, G. A1 - Majumdar, P. A1 - Malaguti, G. A1 - Maltezos, S. A1 - Manalaysay, A. A1 - Mancilla, A. A1 - Mandat, D. A1 - Maneva, G. A1 - Mangano, A. A1 - Manigot, P. A1 - Mannheim, K. A1 - Manthos, I. A1 - Maragos, N. A1 - Marcowith, Alexandre A1 - Mariotti, M. A1 - Marisaldi, M. A1 - Markoff, S. A1 - Marszalek, A. A1 - Martens, C. A1 - Marti, J. A1 - Martin, J-M. A1 - Martin, P. A1 - Martinez, G. A1 - Martinez, F. A1 - Martinez, M. A1 - Masserot, A. A1 - Mastichiadis, A. A1 - Mathieu, A. A1 - Matsumoto, H. A1 - Mattana, F. A1 - Mattiazzo, S. A1 - Maurin, G. A1 - Maxfield, S. A1 - Maya, J. A1 - Mazin, D. A1 - Mc Comb, L. A1 - McCubbin, N. A1 - McHardy, I. A1 - McKay, R. A1 - Medina, C. A1 - Melioli, C. A1 - Melkumyan, D. A1 - Mereghetti, S. A1 - Mertsch, P. A1 - Meucci, M. A1 - Michalowski, J. A1 - Micolon, P. A1 - Mihailidis, A. A1 - Mineo, T. A1 - Minuti, M. A1 - Mirabal, N. A1 - Mirabel, F. A1 - Miranda, J. M. A1 - Mirzoyan, R. A1 - Mizuno, T. A1 - Moal, B. A1 - Moderski, R. A1 - Mognet, I. A1 - Molinari, E. A1 - Molinaro, M. A1 - Montaruli, T. A1 - Monteiro, I. A1 - Moore, P. A1 - Moralejo Olaizola, A. A1 - Mordalska, M. A1 - Morello, C. A1 - Mori, K. A1 - Mottez, F. A1 - Moudden, Y. A1 - Moulin, Emmanuel A1 - Mrusek, I. A1 - Mukherjee, R. A1 - Munar-Adrover, P. A1 - Muraishi, H. A1 - Murase, K. A1 - Murphy, A. A1 - Nagataki, S. A1 - Naito, T. A1 - Nakajima, D. A1 - Nakamori, T. A1 - Nakayama, K. A1 - Naumann, C. L. A1 - Naumann, D. A1 - Naumann-Godo, M. A1 - Nayman, P. A1 - Nedbal, D. A1 - Neise, D. A1 - Nellen, L. A1 - Neustroev, V. A1 - Neyroud, N. A1 - Nicastro, L. A1 - Nicolau-Kuklinski, J. A1 - Niedzwiecki, A. A1 - Niemiec, J. A1 - Nieto, D. A1 - Nikolaidis, A. A1 - Nishijima, K. A1 - Nolan, S. A1 - Northrop, R. A1 - Nosek, D. A1 - Nowak, N. A1 - Nozato, A. A1 - O'Brien, P. A1 - Ohira, Y. A1 - Ohishi, M. A1 - Ohm, S. A1 - Ohoka, H. A1 - Okuda, T. A1 - Okumura, A. A1 - Olive, J. -F. A1 - Ong, R. A. A1 - Orito, R. A1 - Orr, M. A1 - Osborne, J. A1 - Ostrowski, M. A1 - Otero, L. A. A1 - Otte, N. A1 - Ovcharov, E. A1 - Oya, I. A1 - Ozieblo, A. A1 - Padilla, L. A1 - Paiano, S. A1 - Paillot, D. A1 - Paizis, A. A1 - Palanque, S. A1 - Palatka, M. A1 - Pallota, J. A1 - Panagiotidis, K. A1 - Panazol, J. -L. A1 - Paneque, D. A1 - Panter, M. A1 - Paoletti, R. A1 - Papayannis, Alexandros A1 - Papyan, G. A1 - Paredes, J. M. A1 - Pareschi, G. A1 - Parks, G. A1 - Parraud, J. -M. A1 - Parsons, D. A1 - Arribas, M. Paz A1 - Pech, M. A1 - Pedaletti, G. A1 - Pelassa, V. A1 - Pelat, D. A1 - Perez, M. D. C. A1 - Persic, M. A1 - Petrucci, P-O A1 - Peyaud, B. A1 - Pichel, A. A1 - Pita, S. A1 - Pizzolato, F. A1 - Platos, L. A1 - Platzer, R. A1 - Pogosyan, L. A1 - Pohl, M. A1 - Pojmanski, G. A1 - Ponz, J. D. A1 - Potter, W. A1 - Poutanen, J. A1 - Prandini, E. A1 - Prast, J. A1 - Preece, R. A1 - Profeti, F. A1 - Prokoph, H. A1 - Prouza, M. A1 - Proyetti, M. A1 - Puerto-Gimenez, I. A1 - Puehlhofer, G. A1 - Puljak, I. A1 - Punch, M. A1 - Pyziol, R. A1 - Quel, E. J. A1 - Quinn, J. A1 - Quirrenbach, A. A1 - Racero, E. A1 - Rajda, P. J. A1 - Ramon, P. A1 - Rando, R. A1 - Rannot, R. C. A1 - Rataj, M. A1 - Raue, M. A1 - Reardon, P. A1 - Reimann, O. A1 - Reimer, A. A1 - Reimer, O. A1 - Reitberger, K. A1 - Renaud, M. A1 - Renner, S. A1 - Reville, B. A1 - Rhode, W. A1 - Ribo, M. A1 - Ribordy, M. A1 - Richer, M. G. A1 - Rico, J. A1 - Ridky, J. A1 - Rieger, F. A1 - Ringegni, P. A1 - Ripken, J. A1 - Ristori, P. R. A1 - Riviere, A. A1 - Rivoire, S. A1 - Rob, L. A1 - Roeser, U. A1 - Rohlfs, R. A1 - Rojas, G. A1 - Romano, Patrizia A1 - Romaszkan, W. A1 - Romero, G. E. A1 - Rosen, S. A1 - Lees, S. Rosier A1 - Ross, D. A1 - Rouaix, G. A1 - Rousselle, J. A1 - Rousselle, S. A1 - Rovero, A. C. A1 - Roy, F. A1 - Royer, S. A1 - Rudak, B. A1 - Rulten, C. A1 - Rupinski, M. A1 - Russo, F. A1 - Ryde, F. A1 - Sacco, B. A1 - Saemann, E. O. A1 - Saggion, A. A1 - Safiakian, V. A1 - Saito, K. A1 - Saito, T. A1 - Saito, Y. A1 - Sakaki, N. A1 - Sakonaka, R. A1 - Salini, A. A1 - Sanchez, F. A1 - Sanchez-Conde, M. A1 - Sandoval, A. A1 - Sandaker, H. A1 - Sant'Ambrogio, E. A1 - Santangelo, A. A1 - Santos, E. M. A1 - Sanuy, A. A1 - Sapozhnikov, L. A1 - Sarkar, S. A1 - Sartore, N. A1 - Sasaki, H. A1 - Satalecka, K. A1 - Sawada, M. A1 - Scalzotto, V. A1 - Scapin, V. A1 - Scarcioffolo, M. A1 - Schafer, J. A1 - Schanz, T. A1 - Schlenstedt, S. A1 - Schlickeiser, R. A1 - Schmidt, T. A1 - Schmoll, J. A1 - Schovanek, P. A1 - Schroedter, M. A1 - Schultz, C. A1 - Schultze, J. A1 - Schulz, A. A1 - Schure, K. A1 - Schwab, T. A1 - Schwanke, U. A1 - Schwarz, J. A1 - Schwarzburg, S. A1 - Schweizer, T. A1 - Schwemmer, S. A1 - Segreto, A. A1 - Seiradakis, J. -H. A1 - Sembroski, G. H. A1 - Seweryn, K. A1 - Sharma, M. A1 - Shayduk, M. A1 - Shellard, R. C. A1 - Shi, J. A1 - Shibata, T. A1 - Shibuya, A. A1 - Shum, E. A1 - Sidoli, L. A1 - Sidz, M. A1 - Sieiro, J. A1 - Sikora, M. A1 - Silk, J. A1 - Sillanpaa, A. A1 - Singh, B. B. A1 - Sitarek, J. A1 - Skole, C. A1 - Smareglia, R. A1 - Smith, A. A1 - Smith, D. A1 - Smith, J. A1 - Smith, N. A1 - Sobczynska, D. A1 - Sol, H. A1 - Sottile, G. A1 - Sowinski, M. A1 - Spanier, F. A1 - Spiga, D. A1 - Spyrou, S. A1 - Stamatescu, V. A1 - Stamerra, A. A1 - Starling, R. A1 - Stawarz, L. A1 - Steenkamp, R. A1 - Stegmann, Christian A1 - Steiner, S. A1 - Stergioulas, N. A1 - Sternberger, R. A1 - Sterzel, M. A1 - Stinzing, F. A1 - Stodulski, M. A1 - Straumann, U. A1 - Strazzeri, E. A1 - Stringhetti, L. A1 - Suarez, A. A1 - Suchenek, M. A1 - Sugawara, R. A1 - Sulanke, K. -H. A1 - Sun, S. A1 - Supanitsky, A. D. A1 - Suric, T. A1 - Sutcliffe, P. A1 - Sykes, J. A1 - Szanecki, M. A1 - Szepieniec, T. A1 - Szostek, A. A1 - Tagliaferri, G. A1 - Tajima, H. A1 - Takahashi, H. A1 - Takahashi, K. A1 - Takalo, L. A1 - Takami, H. A1 - Talbot, C. A1 - Tammi, J. A1 - Tanaka, M. A1 - Tanaka, S. A1 - Tasan, J. A1 - Tavani, M. A1 - Tavernet, J. -P. A1 - Tejedor, L. A. A1 - Telezhinsky, Igor O. A1 - Temnikov, P. A1 - Tenzer, C. A1 - Terada, Y. A1 - Terrier, R. A1 - Teshima, M. A1 - Testa, V. A1 - Tezier, D. A1 - Thuermann, D. A1 - Tibaldo, L. A1 - Tibolla, O. A1 - Tiengo, A. A1 - Tluczykont, M. A1 - Todero Peixoto, C. J. A1 - Tokanai, F. A1 - Tokarz, M. A1 - Toma, K. A1 - Torii, K. A1 - Tornikoski, M. A1 - Torres, D. F. A1 - Torres, M. A1 - Tosti, G. A1 - Totani, T. A1 - Toussenel, C. A1 - Tovmassian, G. A1 - Travnicek, P. A1 - Trifoglio, M. A1 - Troyano, I. A1 - Tsinganos, K. A1 - Ueno, H. A1 - Umehara, K. A1 - Upadhya, S. S. A1 - Usher, T. A1 - Uslenghi, M. A1 - Valdes-Galicia, J. F. A1 - Vallania, P. A1 - Vallejo, G. A1 - van Driel, W. A1 - van Eldik, C. A1 - Vandenbrouke, J. A1 - Vanderwalt, J. A1 - Vankov, H. A1 - Vasileiadis, G. A1 - Vassiliev, V. A1 - Veberic, D. A1 - Vegas, I. A1 - Vercellone, S. A1 - Vergani, S. A1 - Veyssiere, C. A1 - Vialle, J. P. A1 - Viana, A. A1 - Videla, M. A1 - Vincent, P. A1 - Vincent, S. A1 - Vink, J. A1 - Vlahakis, N. A1 - Vlahos, L. A1 - Vogler, P. A1 - Vollhardt, A. A1 - von Gunten, H. P. A1 - Vorobiov, S. A1 - Vuerli, C. A1 - Waegebaert, V. A1 - Wagner, R. A1 - Wagner, R. G. A1 - Wagner, S. A1 - Wakely, S. P. A1 - Walter, R. A1 - Walther, T. A1 - Warda, K. A1 - Warwick, R. A1 - Wawer, P. A1 - Wawrzaszek, R. A1 - Webb, N. A1 - Wegner, P. A1 - Weinstein, A. A1 - Weitzel, Q. A1 - Welsing, R. A1 - Werner, M. A1 - Wetteskind, H. A1 - White, R. A1 - Wierzcholska, A. A1 - Wiesand, S. A1 - Wilkinson, M. A1 - Williams, D. A. A1 - Willingale, R. A1 - Winiarski, K. A1 - Wischnewski, R. A1 - Wisniewski, L. A1 - Wood, M. A1 - Woernlein, A. A1 - Xiong, Q. A1 - Yadav, K. K. A1 - Yamamoto, H. A1 - Yamamoto, T. A1 - Yamazaki, R. A1 - Yanagita, S. A1 - Yebras, J. M. A1 - Yelos, D. A1 - Yoshida, A. A1 - Yoshida, T. A1 - Yoshikoshi, T. A1 - Zabalza, V. A1 - Zacharias, M. A1 - Zajczyk, A. A1 - Zanin, R. A1 - Zdziarski, A. A1 - Zech, Alraune A1 - Zhao, A. A1 - Zhou, X. A1 - Zietara, K. A1 - Ziolkowski, J. A1 - Ziolkowski, P. A1 - Zitelli, V. A1 - Zurbach, C. A1 - Zychowski, P. T1 - Introducing the CTA concept T2 - Astroparticle physics N2 - The Cherenkov Telescope Array (CTA) is a new observatory for very high-energy (VHE) gamma rays. CTA has ambitions science goals, for which it is necessary to achieve full-sky coverage, to improve the sensitivity by about an order of magnitude, to span about four decades of energy, from a few tens of GeV to above 100 TeV with enhanced angular and energy resolutions over existing VHE gamma-ray observatories. An international collaboration has formed with more than 1000 members from 27 countries in Europe, Asia, Africa and North and South America. In 2010 the CTA Consortium completed a Design Study and started a three-year Preparatory Phase which leads to production readiness of CTA in 2014. In this paper we introduce the science goals and the concept of CTA, and provide an overview of the project. KW - TeV gamma-ray astronomy KW - Air showers KW - Cherenkov Telescopes Y1 - 2013 U6 - https://doi.org/10.1016/j.astropartphys.2013.01.007 SN - 0927-6505 SN - 1873-2852 VL - 43 IS - 2 SP - 3 EP - 18 PB - Elsevier CY - Amsterdam ER - TY - INPR A1 - Guasti, Giovanna A1 - Engbert, Ralf A1 - Krampe, Ralf T. A1 - Kurths, Jürgen T1 - Phase transitions, complexity, and stationarity in the production of polyrhythms N2 - Contents: 1 Introduction 2 Experiment 3 Data 4 Symbolic dynamics 4.1 Symbolic dynamics as a tool for data analysis 4.2 2-symbols coding 4.3 3-symbols coding 5 Measures of complexity 5.1 Word statistics 5.2 Shannon entropy 6 Testing for stationarity 6.1 Stationarity 6.2 Time series of cycle durations 6.3 Chi-square test 7 Control parameters in the production of rhythms 8 Analysis of relative phases 9 Discussion 10 Outlook T3 - NLD Preprints - 57 Y1 - 2000 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:kobv:517-opus-14933 ER - TY - INPR A1 - Schumacher, Jörg A1 - Seehafer, Norbert T1 - Bifurcation analysis of the plane sheet pinch N2 - A numerical bifurcation analysis of the electrically driven plane sheet pinch is presented. The electrical conductivity varies across the sheet such as to allow instability of the quiescent basic state at some critical Hartmann number. The most unstable perturbation is the two-dimensional tearing mode. Restricting the whole problem to two spatial dimensions, this mode is followed up to a time-asymptotic steady state, which proves to be sensitive to three-dimensional perturbations even close to the point where the primary instability sets in. A comprehensive three-dimensional stability analysis of the two-dimensional steady tearing-mode state is performed by varying parameters of the sheet pinch. The instability with respect to three-dimensional perturbations is suppressed by a sufficiently strong magnetic field in the invariant direction of the equilibrium. For a special choice of the system parameters, the unstably perturbed state is followed up in its nonlinear evolution and is found to approach a three-dimensional steady state. T3 - NLD Preprints - 56 Y1 - 1999 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:kobv:517-opus-14926 ER - TY - INPR A1 - Demircan, Ayhan A1 - Scheel, Stefan A1 - Seehafer, Norbert T1 - Heteroclinic behavior in rotating Rayleigh-Bénard convection N2 - We investigate numerically the appearance of heteroclinic behavior in a three-dimensional, buoyancy-driven fluid layer with stress-free top and bottom boundaries, a square horizontal periodicity with a small aspect ratio, and rotation at low to moderate rates about a vertical axis. The Prandtl number is 6.8. If the rotation is not too slow, the skewed-varicose instability leads from stationary rolls to a stationary mixed-mode solution, which in turn loses stability to a heteroclinic cycle formed by unstable roll states and connections between them. The unstable eigenvectors of these roll states are also of the skewed-varicose or mixed-mode type and in some parameter regions skewed-varicose like shearing oscillations as well as square patterns are involved in the cycle. Always present weak noise leads to irregular horizontal translations of the convection pattern and makes the dynamics chaotic, which is verified by calculating Lyapunov exponents. In the nonrotating case, the primary rolls lose, depending on the aspect ratio, stability to traveling waves or a stationary square pattern. We also study the symmetries of the solutions at the intermittent fixed points in the heteroclinic cycle. T3 - NLD Preprints - 55 Y1 - 1999 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:kobv:517-opus-14914 ER - TY - INPR A1 - Volosevich, Alexandra V. A1 - Meister, Claudia-Veronika T1 - Nonlinear interaction of Farley-Buneman waves N2 - The nonlinear interaction of waves excited by the modified two-stream instability (Farley-Buneman instability) is considered. It is found that, during the linear stage of wave growth, the enhanced pressure of the high-frequency part of the waves locally generates a ponderomotive force. This force acts on the plasma particles and redistributes them. Thus an additional electrostatic polarization field occurs, which influences the low-frequency part of the waves. Then, the low-frequency waves also cause a redistribution of the high-frequency waves. In the paper, a self-consistent system of equations is obtained, which describes the nonlinear interaction of the waves. It is shown that the considered mechanism of wave interaction causes a nonlinear stabilization of the high-frequency waves’ growth and a formation of local density structures of the charged particles. The density modifications of the charged particles during the non-linear stage of wave growth and the possible interval of aspect angles of the high-frequency waves are estimated. T3 - NLD Preprints - 52 Y1 - 1998 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:kobv:517-opus-14851 ER - TY - INPR A1 - Maaß, Peter A1 - Pereverzev, Sergei V. A1 - Ramlau, Ronny A1 - Solodky, Sergei G. T1 - An adaptive discretization for Tikhonov-Phillips regularization with a posteriori parameter selection N2 - The aim of this paper is to describe an efficient strategy for descritizing ill-posed linear operator equations of the first kind: we consider Tikhonov-Phillips-regularization χ^δ α = (a * a + α I)^-1 A * y ^δ with a finite dimensional approximation A n instead of A. We propose a sparse matrix structure which still leads to optimal convergences rates but requires substantially less scalar products for computing A n compared with standard methods. T3 - NLD Preprints - 48 Y1 - 1998 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:kobv:517-opus-14739 ER - TY - INPR A1 - Braun, Robert A1 - Feudel, Fred A1 - Guzdar, Parvez T1 - The route to chaos for a two-dimensional externally driven flow N2 - We have numerically studied the bifurcations and transition to chaos in a two-dimensional fluid for varying values of the Reynolds number. These investigations have been motivated by experiments in fluids, where an array of vortices was driven by an electromotive force. In these experiments, successive changes leading to a complex motion of the vortices, due to increased forcing, have been explored [Tabeling, Perrin, and Fauve, J. Fluid Mech. 213, 511 (1990)]. We model this experiment by means of two-dimensional Navier-Stokes equations with a special external forcing, driving a linear chain of eight counter-rotating vortices, imposing stress-free boundary conditions in the vertical direction and periodic boundary conditions in the horizontal direction. As the strength of the forcing or the Reynolds number is raised, the original stationary vortex array becomes unstable and a complex sequence of bifurcations is observed. Several steady states and periodic branches and a period doubling cascade appear on the route to chaos. For increasing values of the Reynolds number, shear flow develops, for which the spatial scale is large compared to the scale of the forcing. Furthermore, we have investigated the influence of the aspect ratio of the container as well as the effect of no-slip boundary conditions at the top and bottom, on the bifurcation scenario. T3 - NLD Preprints - 46 Y1 - 1998 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:kobv:517-opus-14717 ER - TY - INPR A1 - Lukaschewitsch, Michael T1 - Geoelectrical conductivity problems on unbounded domains N2 - This paper deals with the electrical conductivity problem in geophysics. It is formulated as an elliptic boundary value problem of second order for a large class of bounded and unbounded domains. A special boundary condition, the so called "Complete Electrode Model", is used. Poincaré inequalities are formulated and proved in the context of weighted Sobolev spaces, leading to existence and uniqueness statements for the boundary value problem. In addition, a parameter-to-solution operator arising from the inverse conductivity problem in medicine (EIT) and geophysics is investigated mathematically and is shown to be smooth and analytic. T3 - NLD Preprints - 45 Y1 - 1998 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:kobv:517-opus-14704 ER - TY - INPR A1 - Seehafer, Norbert A1 - Schumacher, Jörg T1 - Resistivity profile and instability of the plane sheet pinch N2 - The stability of the quiescent ground state of an incompressible, viscous and electrically conducting fluid sheet, bounded by stress-free parallel planes and driven by an external electric field tangential to the boundaries, is studied numerically. The electrical conductivity varies as cosh–2(x1/a), where x1 is the cross-sheet coordinate and a is the half width of a current layer centered about the midplane of the sheet. For a <~ 0.4L, where L is the distance between the boundary planes, the ground state is unstable to disturbances whose wavelengths parallel to the sheet lie between lower and upper bounds depending on the value of a and on the Hartmann number. Asymmetry of the configuration with respect to the midplane of the sheet, modelled by the addition of an externally imposed constant magnetic field to a symmetric equilibrium field, acts as a stabilizing factor. T3 - NLD Preprints - 44 Y1 - 1998 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:kobv:517-opus-14686 ER - TY - INPR A1 - Rüdiger, Sten A1 - Feudel, Fred A1 - Seehafer, Norbert T1 - Dynamo bifurcations in an array of driven convection-like rolls N2 - The bifurcations in a three-dimensional incompressible, electrically conducting fluid with an external forcing of the Roberts type have been studied numerically. The corresponding flow can serve as a model for the convection in the outer core of the Earth and is realized in an ongoing laboratory experiment aimed at demonstrating a dynamo effect. The symmetry group of the problem has been determined and special attention has been paid to symmetry breaking by the bifurcations. The nonmagnetic, steady Roberts flow loses stability to a steady magnetic state, which in turn is subject to secondary bifurcations. The secondary solution branches have been traced until they end up in chaotic states. T3 - NLD Preprints - 43 Y1 - 1998 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:kobv:517-opus-14678 ER - TY - INPR A1 - Engbert, Ralf A1 - Scheffczyk, Christian A1 - Krampe, Ralf-Thomas A1 - Rosenblum, Mikhael A1 - Kurths, Jürgen A1 - Kliegl, Reinhold T1 - Tempo-induced transitions in polyrhythmic hand movements N2 - We investigate the cognitive control in polyrhythmic hand movements as a model paradigm for bimanual coordination. Using a symbolic coding of the recorded time series, we demonstrate the existence of qualitative transitions induced by experimental manipulation of the tempo. A nonlinear model with delayed feedback control is proposed, which accounts for these dynamical transitions in terms of bifurcations resulting from variation of the external control parameter. Furthermore, it is shown that transitions can also be observed due to fluctuations in the timing control level. We conclude that the complexity of coordinated bimanual movements results from interactions between nonlinear control mechanisms with delayed feedback and stochastic timing components. T3 - NLD Preprints - 41 Y1 - 1997 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:kobv:517-opus-14380 ER - TY - INPR A1 - Seehafer, Norbert A1 - Schumacher, Jörg T1 - Squire‘s theorem for the magnetohydrodynamic sheet pinch N2 - The stability of the quiescent ground state of an incompressible viscous fluid sheet bounded by two parallel planes, with an electrical conductivity varying across the sheet, and driven by an external electric field tangential to the boundaries is considered. It is demonstrated that irrespective of the conductivity profile, as magnetic and kinetic Reynolds numbers (based on the Alfvén velocity) are raised from small values, two-dimensional perturbations become unstable first. T3 - NLD Preprints - 40 Y1 - 1997 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:kobv:517-opus-14628 ER - TY - INPR A1 - Scheel, Stefan A1 - Seehafer, Norbert T1 - Bifurcation to oscillations in three-dimensional Rayleigh-Bénard convection N2 - Three-dimensional bouyancy-driven convection in a horizontal fluid layer with stress-free boundary conditions at the top and bottom and periodic boundary conditions in the horizontal directions is investigated by means of numerical simulation and bifurcation-analysis techniques. The aspect ratio is fixed to a value of 2√2 and the Prandtl number to a value of 6.8. Two-dimensional convection rolls are found to be stable up to a Rayleigh number of 17 950, where a Hopf bifurcation leads to traveling waves. These are stable up to a Rayleigh number of 30 000, where a secondary Hopf bifurcation generates modulated traveling waves. We pay particular attention to the symmetries of the solutions and symmetry breaking by the bifurcations. T3 - NLD Preprints - 39 Y1 - 1997 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:kobv:517-opus-14370 ER -