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  2. Preprint typeset in JHEP style - PAPER VERSION June ...

    www.damtp.cam.ac.uk/user/tong/tasi/tasi.pdf
    31 May 2024: 1.4.1 The Metric on the Higgs Branch 23. 1.4.2 Constructing the Solutions 24. ... in 5 1 dimensions is a sigma-model on a hyperKähler target space [24] which, for.
  3. 4. The Einstein Equations It is now time to ...

    www.damtp.cam.ac.uk/user/tong/gr/four.pdf
    31 May 2024: ṙ2 Ve(r) = E2 (4.24). but this time with the eective potential. ... This tells us that the particle follows a null geodesic. The equation (4.24) gets replaced.
  4. standardmodel

    www.damtp.cam.ac.uk/user/tong/sm/standardmodel1.pdf
    26 Jun 2024: 1.24). This is our starting point: representations of the Poincaré group are labelled by the.
  5. Under consideration for publication in J. Fluid Mech. 1 ...

    www.damtp.cam.ac.uk/user/hinch/publications/HSB3.pdf
    11 Mar 2024: They solved their lubrication equations(24–32), again by an expansion in a small Deborah number We 1, going tothe first correction.
  6. Supplementary Material:Stochastic Voronoi Tessellations as Models for …

    www.damtp.cam.ac.uk/user/gold/pdfs/Srinivasan_etal_SM110324.pdf
    11 Mar 2024: V (X) =i. xi1xi2. xi1xi2. y2dy =1. 24. i. [(xi1 xi)3 (xi xi1)3. ]. ... v. 0.0. 0.5. 1.0. 1.5. 2.0. t = 10000.0000.04Y23.65,1. 2.64Z14.92,24.87. FIG.
  7. 18 Mar 2024: Then, using our previous result (1.24), we have. Tr (1)FeβH =X. ... 24 –. Note that we’re not assuming that all critical points of h correspond to true E = 0.
  8. Preprint typeset in JHEP style - HYPER VERSION Michaelmas ...

    www.damtp.cam.ac.uk/user/tong/kintheory/kintheory.pdf
    22 Feb 2024: 1)f1(r, p. ′2) f1(r, p)f1(r, p2). ](2.24). This is the Boltzmann equation.
  9. standardmodel

    www.damtp.cam.ac.uk/user/tong/sm/standardmodel2.pdf
    26 Jun 2024: proportional to. eVScl! 0 as V! 1. (2.24). It’s obvious what’s going on here.
  10. Preprint typeset in JHEP style - HYPER VERSION January ...

    www.damtp.cam.ac.uk/user/tong/qhe/qhe.pdf
    1 Apr 2024: ψ(x,y) = ψn,k(x mE/eB2,y) (1.24). and the energies are now given by. ... holomorphic and anti-holomorphic derivatives. =1. 2. (. x+ i. y. )and ̄ =. 1. 2. (. x i. y. ). – 24 –. which obey z = ̄z̄ = 1 and z̄ = ̄z = 0.

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