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University of Washington Ultracold Gases • the scattering length a is a variable parameter in experiments with ultracold gases (Feshbach resonances) • study BEC-BCS
116 ANEXO II – BILAG II – ANHANG II – ΠΑΡΑΡΤΗΜΑ II – ANNEX II – ANNEXE II – ALLEGATO II – BIJLAGE II – ANEXO II – LIITE II – BILAGA II – PRÍLOHA…
On the dynamics of periodically perturbed quantum systems Consider a system of n ODEs 𝑑 𝑑𝑡 𝜓 𝑡 = 𝐴 𝑡 𝜓 𝑡 , 𝜓:ℝ ⟶ 𝑀𝑛×1 ℂ where 𝐴:ℝ…
Planetesimal Formation in the Dead Zone of Protoplanetary Disks: Hubble Fellow Symposium, STScI, 03/10/2014 Xuening Bai Institute for Theory and Computation, Harvard-Smithsonian…
DAN BURGHELEA AND STEFAN HALLER Abstract. We consider vector fields X on a closed manifold M with rest points of Morse type. For such vector fields we define the property
Dynamics of Eutrophication and OligotrophicationEutrophication and Oligotrophication Processes in the Seto Inland Sea and their relationships to the Satoumi concept Tetsuo
Dark Matter Superfluidity & Galactic DynamicsJune 12, 2018 Dark Matter Distribution N-body simulations reveal universal density profile: Navarro, Frenk, White ’96
evol_rmjoint work with Gernot Akemann and Mario Kieburg arxiv:1809.05905 Z.Burda April 29th - May 3rd, Kraków Outline • WSR = width-to-spacing ratio • kernel
Car-Parrinello Molecular DynamicsEric J. Bylaska HPCC Group Moral: “A man dreams of a miracle and wakes up with loaves of bread” Erich Maria Remarque Molecular
A620_Dynamics_2017_revised.pptToday! • Non-spherical potential! • Virial theorm! • Time scales- collisionless systems ! ! For more detail on some of this material
Peter Sarnak Mahler Lectures 2011 Mobius Randomness and Dynamics n ≥ 1, µ(n) = (−1)t if n = p1p2 · · · pt distinct, 0 if n has a square
Causality and relativistic fluid dynamicsStefan Florchinger (Heidelberg U.) based on: Stefan Floerchinger & Eduardo Grossi, Causality of fluid dynamics for high-energy
Slide 1 / 103 Dynamics in Two Dimensions Slide 2 / 103 · Newton's Three Laws of Motion · Inertial Reference Frames · Mass vs. Weight · Forces we studied: weight / gravity…
STRUCTURAL DYNAMICS, VOL. 9 Computational Dynamics Søren R. K. Nielsen λ λ1 λ2 λ3 µkµk−1 µk+1 P (λ) y(λ) = P (µk) + ( P (µk) − P (µk−1) ) λ − µk µk…
Whiskered invariant tori for fibered dynamics We consider fibered holomorphic dynamics generated by the skew product over the translation Tω: F : Td ˆ Cn Ñ Td ˆ Cn Fpθ…
Slide 1 Slide 2 Body Size and Scaling Size Matters in Physiology Slide 3 Living Organisms Come in a Huge Range of Sizes! Pleuropneumonia-like organisms (Mycoplasma) –0.1…
“Chaotic Rotation in the Three-Body Coorbital Problem” Alexandre C.M. Correia IMCCE / Observatoire de Paris gr@av group meeting March 5th, 2014 - Aveiro Philippe Robutel…
and Cholesterol Biosynthesis and Cholesterol Biosynthesis • Most acetyl CoA from β-oxidation is routed through the TCA cycle • Excess is used to synthesize
International Journal of Radiation Oncology biology physics www.redjournal.org Physics Contribution 4p Noncoplanar Stereotactic Body Radiation Therapy for Head-and-Neck Cancer:…
Ketone Body Formation; Fatty acid and Cholesterol Biosynthesis Ketone Body Formation; Fatty acid and Cholesterol Biosynthesis • Most acetyl CoA from β-oxidation is routed…