Search results for "75"

showing 10 items of 1365 documents

CCDC 706838: Experimental Crystal Structure Determination

2009

Related Article: J.Frey, C.Tock, J.-P.Collins, V.Heitz, J.-P.Sauvage, K.Rissanen|2008|J.Am.Chem.Soc.|130|11013|doi:10.1021/ja801924y

Space GroupCrystallographyCrystal SystemCrystal StructureCell Parameters(4)-bis(mu~2~-38-bis(5-(4-Methoxyphenyl)-2-pyridyl)-47-phenanthroline-NN'N''N''') bis(mu~2~-161922252831515457606366-dodecaoxa-61037417174-hexa-azatridecacyclo-[44.24.4.2$811~2~1215~2~4750~2~6770!1^3236^1^3539^0^472^0^542^-0^740^0^938^0^4373^]-tetraoctaconta-1(71)24(72)5(42)6810121432(80)-3335(79)36384043(73)4446(74)4749676975778183-hexacosaene)-tetra-copper(i)-pseudorotaxane tetrakis(hexafluorophosphate) dichlo romethane tetrahydrofuran dichloromethane unspecified solvateExperimental 3D Coordinates
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CCDC 144174: Experimental Crystal Structure Determination

2001

Related Article: C.Schmidt, T.Straub, D.Falabu, E.F.Paulus, E.Wegelius, E.Kolehmainen, V.Bohmer, K.Rissanen, W.Vogt|2000|Eur.J.Org.Chem.|2001|3937|doi:10.1002/1099-0690(200012)2000:233.0.CO;2-X

Space GroupCrystallographyCrystal SystemCrystal StructureCell Parameters2468-Tetra-n-pentyl-146346546746-octahydroxy-15355575-tetrakis(4-ethyl-13-oxazolidin-3-ylmethyl)-1357-tetra(13)benzenacyclo-octaphane dichloromethane clathrate acetonitrile solvate dihydrateExperimental 3D Coordinates
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CCDC 705736: Experimental Crystal Structure Determination

2009

Related Article: D.Meshcheryakov, V.Bohmer, M.Bolte, V.Hubscher-Bruder, F.Arnaud-Neu|2009|Chem.-Eur.J.|15|4811|doi:10.1002/chem.200802573

Space GroupCrystallographyCrystal SystemCrystal StructureCell Parameters97979898-Tetramethyl-3435191-tetra-t-butyl-153147637995-hexaoxa-6822243840545670728688-dodeca-azapentadecacyclo[91.3.1.1^4549^.0^596^.0^914^.0^1621^.0^2530^.0^3237^.0^4146^.0^4853^.0^5762^.0^6469^.0^7378^.0^8085^.0^8994^]octanonaconta-1(96)2491113161820252729323436414345485052575961646668737577808284899193-hexatriacontaene-72339557187-hexone acetone solvateExperimental 3D Coordinates
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CCDC 161425: Experimental Crystal Structure Determination

2002

Related Article: Qian Yi Li, E.Vogel, A.H.Parham, M.Nieger, M.Bolte, R.Frohlich, P.Saarenketo, K.Rissanen, F.Vogtle|2001|Eur.J.Org.Chem.|2001|4041|doi:10.1002/1099-0690(200111)2001:213.0.CO;2-7

Space GroupCrystallographyCrystal SystemCrystal StructureCell ParametersExperimental 3D Coordinates3172335415561737880838588909395-Hexadecamethyl-2020:3838:5858:7676-tetrakis(pentamethylene)-5152533435363718494-decaazatridecacyclo[70.2.2.2^1619^.2^2124^.2^3437^.2^3942^.2^5457^.2^5962^.2^7275^.1^711^.1^2731^.1^4549^.1^6569^]hexanonaconta-137911(79)1216182123272931(84)34363941454749(89)5054565961656769(94)72747780828587909295-octatriacontaen-614263244526470-octaone chloroform dichloromethane ethyl acetate methanol solvate hydrate
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Pingüí del cap, Pingüino del cabo (VER0000191)

Jackass Penguin (Anglès), Manchot du cap (Francès), Brillenpinguin (Alemany) Gabinet de Vertebrats (Departament de Zoologia), Facultat de Ciències Biològiques (Campus de Burjassot), C/ Doctor Moliner, s/n, Bloque B. 5é plant, Burjassot (Valencia). Armari: 12-1 Valencia Hembra Adulto

Spheniscus demersus (Linnaeus 1758)SphenicidaePingüinos
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Ziemie Prus w trakcie polskiej wojny sukcesyjnej i wojny siedmioletniej

2021

W trakcie licznych konfliktów zbrojnych rozegranych w osiemnastowiecznej Europie Prusy Wschodnie tylko raz były teatrem działań wojennych: latem 1757 r. – zimą 1758 r. Dwukrotnie jednak działania zbrojne toczyły się nad jej granicami, a w latach 1734-1735 przez prowincje pruską przechodziły transporty i oddziały walczących wojsk. Taka postawa nie przyniosła wówczas królowi pruskiemu żadnych korzyści, ale też uchroniła Prusy Wschodnie oraz jego mieszkańców przed ewentualnymi negatywnymi skutkami wojny na terytorium Rzeczpospolitej. Jednak ponad dwadzieścia lat później Prusy Wschodnie nie uniknęły już okrucieństw wojny. Król Fryderyk II atakiem w sierpniu 1756 r. na Saksonię chciał uprzedzić …

Stanisław LeszczyńskiRosjawojna siedmioletnia 1756-1763cesarzowa ElżbietaThe war of 1733-1735Frederick II HohenzollernWojna 1733-1735Frederick William HohenzollernRussiaPrussiaFryderyk II Hohenzollernseven-year war of 1756-1763cesarzowa AnnaEmpress ElisabethPrusyFryderyk Wilhelm HohenzollernEmpress Anna
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Quantitative ergodicity for some switched dynamical systems

2012

International audience; We provide quantitative bounds for the long time behavior of a class of Piecewise Deterministic Markov Processes with state space Rd × E where E is a finite set. The continuous component evolves according to a smooth vector field that switches at the jump times of the discrete coordinate. The jump rates may depend on the whole position of the process. Under regularity assumptions on the jump rates and stability conditions for the vector fields we provide explicit exponential upper bounds for the convergence to equilibrium in terms of Wasserstein distances. As an example, we obtain convergence results for a stochastic version of the Morris-Lecar model of neurobiology.

Statistics and ProbabilitySwitched dynamical systemsDynamical systems theoryMarkov process01 natural sciences34D2393E15010104 statistics & probabilitysymbols.namesakeCouplingPiecewise Deterministic Markov ProcessPosition (vector)60J25FOS: MathematicsState spaceApplied mathematicsWasserstein distance0101 mathematicsMathematicsProbability (math.PR)010102 general mathematicsErgodicityErgodicity[MATH.MATH-PR]Mathematics [math]/Probability [math.PR]Linear Differential EquationsPiecewisesymbolsJumpAMS-MSC. 60J75; 60J25; 93E15; 34D23Vector fieldStatistics Probability and Uncertainty60J75[ MATH.MATH-PR ] Mathematics [math]/Probability [math.PR]Mathematics - Probability
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Simulation of BSDEs with jumps by Wiener Chaos Expansion

2016

International audience; We present an algorithm to solve BSDEs with jumps based on Wiener Chaos Expansion and Picard's iterations. This paper extends the results given in Briand-Labart (2014) to the case of BSDEs with jumps. We get a forward scheme where the conditional expectations are easily computed thanks to chaos decomposition formulas. Concerning the error, we derive explicit bounds with respect to the number of chaos, the discretization time step and the number of Monte Carlo simulations. We also present numerical experiments. We obtain very encouraging results in terms of speed and accuracy.

Statistics and ProbabilityWiener Chaos expansionDiscretizationMonte Carlo methodTime stepConditional expectation01 natural sciences010104 statistics & probabilitybackward stochastic differential equations with jumpsFOS: MathematicsApplied mathematics60H10 60J75 60H35 65C05 65G99 60H070101 mathematicsMathematicsPolynomial chaosApplied MathematicsNumerical analysis010102 general mathematicsMathematical analysista111Probability (math.PR)numerical methodCHAOS (operating system)[MATH.MATH-PR]Mathematics [math]/Probability [math.PR]Modeling and SimulationScheme (mathematics)Mathematics - Probability
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"Table 1" of "Cross Sections for the Reactions e+e- --> K+ K- pi+pi-, K+ K- pi0pi0, and K+ K- K+ K- Measured Using Initial-State Radiation Events"

2013

The cross section for the reaction E+ E- --> K+ K- PI+ PI- measured with ISR data. Statistical errors only.

Strange productionE+ E- ScatteringIntegrated Cross SectionE+ E- --> K+ K- PI+ PI-Exclusive1.4125-4.9875Cross SectionSIG
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"Table 2" of "Cross Sections for the Reactions e+e- --> K+ K- pi+pi-, K+ K- pi0pi0, and K+ K- K+ K- Measured Using Initial-State Radiation Events"

2013

Cross section measurements for the reaction E+ E- --> K*(892)0 K- PI+. Statistical errors only.

Strange productionE+ E- ScatteringIntegrated Cross SectionExclusiveE+ E- --> K*(892)0 K- PI+ + CCCross SectionSIG1.5875-3.9625
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