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9 May 2024: S Babak, JG Baker, MJ Benacquista, NJ Cornish, SL Larson, I Mandel, ST McWilliams, A Petiteau, EK Porter, EL Robinson, M Vallisneri, A Vecchio, M Adams, KA Arnaud, A Blaut, M

9 May 2024: Beyond the Standard Model Physics at the HL-LHC and HE-LHC. XC Vidal, M D'Onofrio, PJ Fox, R Torre, KA Ulmer, A Aboubrahim, A Albert, J Alimena, BC Allanach,

13 Mar 2019: δ(r a). Show that the phase shifts are given by. tan δl = kλa2[jl(ka)]. ... 2. 1 kλa2jl(ka)nl(ka). [Hint: The δ-function leads to two continuity conditions at r = a.

9 May 2024: MR Bate, SH Lubow, GI Ogilvie, KA Miller. (2003). (doi: 10.48550/arxiv.astro-ph/0301154).

9 May 2024: KA Bacik, S Lovett, C-CP Caulfield, NM Vriend. – Phys Rev Lett.

9 May 2024: KA Bacik, S Lovett, C-CP Caulfield, NM Vriend. – Phys Rev Lett.

7 Apr 2021: m!2 = 2 eika eika. = 4sin2. ka. 2. We find the dispersion relation! = ... 2 =. mM. hm M. p(m M)2 4mM cos2(ka). i. The resulting dispersion relation is sketched in Figure 74 in the first Brillouin zone.

10 Apr 2011: Trapping and Wiggling: Elastohydrodynamics of Driven Microfilaments. Chris H. Wiggins, D. Riveline,# A. Ott,# and Raymond E. Goldstein. Department of Physics, Princeton University, Princeton, New Jersey 08544 USA; #Institut Curie, Section de

19 Oct 2013: #"$ %'&)(,.-0/$1#(23547684:9 ;8< = >?9A@B9DCFE7;8<G9IH 4KJ L59NM. OPRQST U U U U V W XY XY X X X XZ XY XY X. X XU XU. [#[T U U U U]_)]_)a.bc)_edXU XZ X X XZ X X XU XZ X f b)ghd. XZ X XZ X X Xi. [)jT U U U Uk]_l]DmBnoDdXi Xi XZ XU XZ X XU XZ XZ XZ X

26 Jul 2013: with similar viscosities (, ) and densities (, ),(b) dimensionless membrane-viscous number, Me U=KA, for two fluids separated by an elastic membrane(thickness t, area modulus KA, density m, bending stiff-ness ... f 2= is an intrinsic viscocapillary