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  1. Results that match 1 of 2 words

  2. Rebound and scattering of motile Chlamydomonas algae in confined…

    www.damtp.cam.ac.uk/user/lauga/papers/192.pdf
    8 Jul 2021: Cells interact with their surroundingsthrough complex hydrodynamic and steric interactions.21,22 Rigidboundaries, free surfaces and other obstacles in suspensions areknown to strongly affect swimming behaviour.23,24 Relevantcomplex media include
  3. 23 Apr 2021: Particle PhysicsCERN Lectures. David Tong. Department of Applied Mathematics and Theoretical Physics,. Centre for Mathematical Sciences,. Wilberforce Road,. Cambridge, CB3 OBA, UK. http://www.damtp.cam.ac.uk/user/tong/particlephysics.html.
  4. 5 When Gravity is Weak‣ General Relativity by David Tong

    www.damtp.cam.ac.uk/user/tong/gr/grhtml/S5.html
    16 Oct 2021: 5 When Gravity is Weak. 5 When Gravity is Weak. The elegance of the Einstein field equations ensures that they hold a special place in the hearts of many physicists. However, any fondness you may feel for these equations will be severely tested if
  5. cosmo

    www.damtp.cam.ac.uk/user/tong/cosmo/three.pdf
    18 Apr 2021: 1. ar v̇ = Ḣ. 1. arv̇. Take the gradient of (3.24) to get. ... 1.24). In such a situation, it would make little sense to talk about perturbations with.
  6. J. Fluid Mech. (2021), vol. 916, A17, doi:10.1017/jfm.2021.181…

    www.damtp.cam.ac.uk/user/lauga/papers/190.pdf
    8 Jul 2021: Received 13 May 2020; revised 18 February 2021; accepted 24 February 2021). ... Ω. , (2.23). where. A = 6ζ‖ 4Δζ (φ21 φ22 ) O(φ4), (2.24)B = 4Δζ (φ1 φ2) 83 Δζ (φ31 φ32 ) O(φ4), (2.25).
  7. Lecture Notes on Cosmological Soft Theorems Enrico Pajera aDepartment …

    www.damtp.cam.ac.uk/user/ep551/notes_cosmo_soft_theorems.pdf
    16 Apr 2021: D : (3 ττ ) kiki , (4.24)b K : (3 ττ ) 2biki b kkiki 2kikibjkj. ... R|comoving R =A. 2. (5.24). The metric then takes the form.
  8. Field Theory in Cosmology (Part III) Enrico Pajer Contents ...

    www.damtp.cam.ac.uk/user/ep551/field_theory_in_Cosmology.pdf
    15 Apr 2021: M2Plä. a= 1. 6(ρ 3p). (1.24). Second, by taking the time derivative of the Friedmann equation and using the continuityequation to get rid of ρ̇, we can find the ... ̇K = ä2K. ȧ3ä (ρ 3p) (1 3w) , (1.27). where in the second step I used the
  9. Convex optimization and quantum information theory

    www.damtp.cam.ac.uk/user/hf323/qip2021_tutorial_cvxqi.pdf
    22 Apr 2021: 23/82. 24/82. Hilbert’s question. Are all nonnegative polynomials sums of squares?
  10. Morphoelasticity of large bending deformations of cell sheets during…

    www.damtp.cam.ac.uk/user/gold/pdfs/morpho_bending.pdf
    22 Feb 2021: A theory ofnon-Euclidean plates [23] has been developed in parallel.Apart from a general geometric theory of morphoelastic sur-faces [24], studies of morphoelastic shells have remained. ... 1 εκsζ 0 ζ0,ζ. (24). The elastic deformation gradient is,
  11. Part III - Classical and Quantum Solitons

    www.damtp.cam.ac.uk/user/examples/3P11e.pdf
    20 Apr 2021: The quantities we are interested in are vortices. 24. 2 Vortices III Classical and Quantum Solitons.

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