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List of publications H.K. Moffatt May 24, 2024 Curriculum ...
www.damtp.cam.ac.uk/user/hkm2/HKM_publications.pdf18 Jun 2024: Fluid Dyn. 24 (1-4, SI), 209–215. PDF. 2009. 169. Moffatt, H. ... PDF. 4. Publications: H.K.Moffatt May 24, 2024. 167. Moffatt, H. K. & -
Quantum Mechanics David Tong Department of Applied Mathematics and ...
www.damtp.cam.ac.uk/user/tong/qm/qm.pdf26 Jun 2024: 2.1.2 The Infinite Potential Well 24. 2.1.3 The Gaussian Wavepacket 27. ... 24 –. easy to deal with. The Schrödinger equation equation is. -
Stephen J. Cowley, DAMTP, University of Cambridge
www.damtp.cam.ac.uk/user/sjc1/8 Jun 2024: 2.24. To worship gods that are not yours, that is toadyism. -
Stephen J. Cowley: University Committees
www.damtp.cam.ac.uk/user/sjc1/Council/Committees.html8 Jun 2024: 01/01/17-. 31/12/20). ;. the Governance Review Working Group. (24/04/17-. 31/12/20. );. the Pensions Advisory Group. (May 2017 - December 2020, also October 2010 - December 2014). ... elected. 01/01/24-. 31/12/27 and. 01/01/11-. 31/12/14. , co-opted. -
John Hinch - Homepage
www.damtp.cam.ac.uk/user/hinch/publications/index.shtml10 Jun 2024: Guazzelli & L. Oger NATO-ASI E 287, 1-24. Reproduced as a special edition du journal du G.d.R de P.M.H.C. -
Book Reviews | SIAM Review | Vol. 65, No. 4 | Society for Industrial…
www.damtp.cam.ac.uk/user/lauga/papers/BookReview_SIAM.pdf25 Jun 2024: Murphy), Mehrshad Sadria, 1196. Dow. nloa. ded. 06/2. 5/24. to 1. ... Highlights include a con-. Dow. nloa. ded. 06/2. 5/24. to 1. -
E.J.Hinch, 12 March 2024 Publications by E.J. Hinch 1. ...
www.damtp.cam.ac.uk/user/hinch/publications/pubs.pdf10 Jun 2024: Fluid Mech. 76, 187–208. 24. Hinch, E.J. 1976 Mechanical models of dilute polymer solutions for strong flowsin Proc. ... Guazzelli & L. Oger NATO-ASI E 287, 1–24. Repro-duced as a special edition du journal du G.d.R de P.M.H.C. -
standardmodel
www.damtp.cam.ac.uk/user/tong/sm/standardmodel3.pdf26 Jun 2024: V (r) =g2s. 4rT AcaT? Adb. (3.24). – 99 –. We’ve still got those colour indices to deal with. ... the result (3.24).) Consider the operator. SA = T A(R1) 1 1 T A(R2). -
standardmodel
www.damtp.cam.ac.uk/user/tong/sm/standardmodel7.pdf26 Jun 2024: 255 –. Figure 24. A colour coded description of the possible ordering of neutrino masses. ... The two possibilities are shown in Figure 24. Given the pattern seen in all other. -
5. When Gravity is Weak The elegance of the ...
www.damtp.cam.ac.uk/user/tong/gr/five.pdf31 May 2024: 1 1. 2He. i!t. (5.24). where, as we mentioned previously, we should take the real part of the right-hand-side. ... S1(0)2 S2(0)2 = R2. The solutions (5.24) tell us how these geodesics evolve. -
BMC_talk_mjc
www.damtp.cam.ac.uk/user/mjc249/talks/rigged_DMD_manchester.pdf18 Jun 2024: 𝑒𝑗 𝑒𝑗1. 𝑈 =. Back to the shift! . 24. 0 1. ... Slide 24: Back to the shift! Slide 25: Back to the shift! -
2 A Quantum Particle in One Dimension There is ...
www.damtp.cam.ac.uk/user/tong/qm/qm2.pdf26 Jun 2024: d2h. dy22ydh. dy+ (Ẽ 1)h = 0 (2.26). You can check that this is indeed satisfied by our earlier solution (2.24) with h = 1. ... We learn that the. Gaussian wavefunction (2.24) that we guessed earlier is actually the lowest energy. -
Quantum Mechanics David Tong Department of Applied Mathematics and ...
www.damtp.cam.ac.uk/user/tong/qm/qm1.pdf26 Jun 2024: 2.1.2 The Infinite Potential Well 24. 2.1.3 The Gaussian Wavepacket 27. -
cosmo
www.damtp.cam.ac.uk/user/tong/cosmo/one.pdf26 Jun 2024: Zrmax(t). 0. drp1 kr2/R2. = c a(t). Zt. 0. dt0. a(t0)(1.24). ... Indeed,. mathematically it could be that the integral on the left-hand side of (1.24) does not. -
5. Chiral Symmetry Breaking In this section, we discuss ...
www.damtp.cam.ac.uk/user/tong/gaugetheory/5chisb.pdf26 Jun 2024: For example, we. have. m2K+. m2K0. m2. =mu mdmu md. (5.24). ... corrections, we can generalise (5.24) to. (m2K m2K0) (m2 m20). m20. -
Preprint typeset in JHEP style - HYPER VERSION Michaelmas ...
www.damtp.cam.ac.uk/user/tong/gr/one.pdf31 May 2024: should identify. g00(x) 1. 2(x). c2. (1.24). where (x) is the Newtonian gravitational field. ... 1.24) but with a linear gravitational potential of the kind that we would invoke for. -
PUBLICATION LIST -- J
www.damtp.cam.ac.uk/user/tsm/jrw_publist1.pdf3 Jun 2024: Mech. Phys. Solids 24 (1976) 225-238. 43. F. J. Sabina and J. ... Mech. Phys. Solids, 40. (1992) 1671-1681. 126. J. R. Willis, “Asymptotic analysis of crack bridging by ductile fibres”, Composites 24 (1993). -
Vector CalculusUniversity of Cambridge Part IA Mathematical Tripos…
www.damtp.cam.ac.uk/user/tong/vc/vc1.pdf12 Jun 2024: 1.3.3 An Application: Work and Potential Energy 24. 1.3.4 A Subtlety 25. ... 24 –. We learn that a conservative force, one that can be written as (1.18), has a conserved. -
6. Large N Non-Abelian gauge theories are hard. We ...
www.damtp.cam.ac.uk/user/tong/gaugetheory/6n.pdf26 Jun 2024: The gluon exchange is now. 1N2. (6.24). but there are order N3 triplets of quarks, so again the total amplitude scales as N. ... 6N2. X. i 6=j 6=k. V3(xij, xjk). where xij = xi xj and the coecients in front of the potentials are taken from (6.23)and (6.24 -
cosmo
www.damtp.cam.ac.uk/user/tong/cosmo/two.pdf26 Jun 2024: integral as. n 4. (2)3 eµ. Z 1. 0. dp p2ep2/2m =. mkBT. 22. 3/2eµ (2.24). Let’s try to interpret this. Read naively, it seems to tell ... anti-aligned to give 3 dierent spin 1 states. With these two amendments, our expression for the number density (2 -
3. Introducing Riemannian Geometry We have yet to meet ...
www.damtp.cam.ac.uk/user/tong/gr/three.pdf31 May 2024: Claim:. d? F =? J , rµF µ = J (3.24). -
Preprint typeset in JHEP style - HYPER VERSION Michaelmas ...
www.damtp.cam.ac.uk/user/tong/gr/gr.pdf31 May 2024: should identify. g00(x) (1. 2Φ(x). c2. )(1.24). where Φ(x) is the Newtonian gravitational field. ... 1.24) but with a linear gravitational potential Φ of the kind that we would invoke for. -
Preprint typeset in JHEP style - PAPER VERSION June ...
www.damtp.cam.ac.uk/user/tong/tasi/tasi.pdf31 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. -
4 A Quantum Particle in Three Dimensions We will ...
www.damtp.cam.ac.uk/user/tong/qm/qm4.pdf26 Jun 2024: 0 for all S(r) and R(r) (4.24). This is clearly satisfied if R and S are finite at the origin. -
munich_talk_mjc
www.damtp.cam.ac.uk/user/mjc249/talks/rigged_DMD_munich.pdf10 Jun 2024: Slide 24: Spectral measures goes to diagonalisation. Slide 25: Spectral measures goes to dynamics. -
Preprint typeset in JHEP style - HYPER VERSION 2018 ...
www.damtp.cam.ac.uk/user/tong/gaugetheory/1em.pdf26 Jun 2024: Instead, both (1.23) and (1.24) are best thought of as integrating the 2-form Fµ over. ... Armed with (1.23) and (1.24), we see that, at least for this specific example,. -
Preprint typeset in JHEP style - HYPER VERSION 2018 ...
www.damtp.cam.ac.uk/user/tong/gaugetheory/gt.pdf26 Jun 2024: in (1.24) because E = (0,0,E) lies parallel to the side of the torus, not perpendicular. ... Instead, both (1.23) and (1.24) are best thought of as integrating the 2-form Fµν over. -
2. Introducing Di↵erential Geometry Gravity is geometry. To fully ...
www.damtp.cam.ac.uk/user/tong/gr/two.pdf31 May 2024: S T)µ1.µp1.r1.q1.s. = Sµ1.µp1.qT1.r. 1.s (2.24). Given an (r, s) tensor T , we can also construct a tensor of lower rank (r -
4. The Einstein Equations It is now time to ...
www.damtp.cam.ac.uk/user/tong/gr/four.pdf31 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. Lattice Gauge Theory Quantum field theory is hard. ...
www.damtp.cam.ac.uk/user/tong/gaugetheory/4lattice.pdf26 Jun 2024: 4.24). with @ = @t @x. The equations of motion tell us @ = @ = 0. ... moving fermion. The chiral symmetry of the action (4.24) means that the left- and right-handed. -
8. Quantum Field Theory on the Plane In this ...
www.damtp.cam.ac.uk/user/tong/gaugetheory/83d.pdf26 Jun 2024: group, means that the theory admits fluxes (8.24) and gauge transformations (8.25). ... a derivative of the Chern-Simons term (2.24). (It also arose in the same context when. -
cosmo
www.damtp.cam.ac.uk/user/tong/cosmo/three.pdf26 Jun 2024: 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. Black Holes Black holes are among the most ...
www.damtp.cam.ac.uk/user/tong/gr/six.pdf31 May 2024: 6. Black Holes. Black holes are among the most enigmatic objects in the universe. They are described. by deceptively simple solutions to the Einstein equations, yet hold a host of insights. and surprises, from the meaning of causal structure, to -
7. Quantum Field Theory on the Line In this ...
www.damtp.cam.ac.uk/user/tong/gaugetheory/72d.pdf26 Jun 2024: 4i. 1 log. i. 2UV. iv2. (7.24). where, to reach the second line, we’ve Taylor expanded in /2UV. , ... 2. This is the same kind of integral that we met in (7.24) when solving the 2d CPN1. -
standardmodel
www.damtp.cam.ac.uk/user/tong/sm/standardmodel6.pdf26 Jun 2024: 6.24). Of these, U(1)3 acts on V22, leaving the overall sum 1 2 3 4 unchanged. -
standardmodel
www.damtp.cam.ac.uk/user/tong/sm/standardmodel4.pdf26 Jun 2024: Tr T ART BR. =1. 2I(R)AB. (4.24). The Dynkin index is related to the quadratic Casimir C(R), which we previously defined. -
J. Fluid Mech. (2024), vol. 988, A11, doi:10.1017/jfm.2024.260 Fast…
www.damtp.cam.ac.uk/user/hinch/publications/JFM988_A11.pdf31 May 2024: They solvedtheir lubrication equations (24)–(32), again by an expansion in a small Deborah numberWe 1, going to the first correction. ... p/. (1. c). p 1. De. H = 21/22. 23/24. Figure 1. -
standardmodel
www.damtp.cam.ac.uk/user/tong/sm/standardmodel1.pdf26 Jun 2024: 1.24). This is our starting point: representations of the Poincaré group are labelled by the. -
2. Yang-Mills Theory Pure electromagnetism is a free theory ...
www.damtp.cam.ac.uk/user/tong/gaugetheory/2ym.pdf26 Jun 2024: where. Kµ = µtr. A@A. 2i. 3AAA. (2.24). This means that, as in the Maxwell case, the theta term does not change the. ... derivative (2.24), the temporal component was K0 = 42W. For now, the key property of W(A) that we will need is. -
standardmodel
www.damtp.cam.ac.uk/user/tong/sm/standardmodel2.pdf26 Jun 2024: proportional to. eVScl! 0 as V! 1. (2.24). It’s obvious what’s going on here. -
J. Fluid Mech. (2024), vol. 988, A10, doi:10.1017/jfm.2024.223 Flow…
www.damtp.cam.ac.uk/user/hinch/publications/JFM988_A10.pdf10 Jun 2024: Received 10 October 2023; revised 27 December 2023; accepted 24 February 2024). ... F(Z, ζ ) = 13ζ. Z0. H(Z̃) dZ̃. (3.25). We note that solutions (3.24) satisfy the matching conditions between theinner and outer regions. -
3. Anomalies We learn as undergraduates that particles come ...
www.damtp.cam.ac.uk/user/tong/gaugetheory/3anom.pdf26 Jun 2024: p. Figure 24:. to be conserved if we deform the theory, provided that both. ... not Grassmann-valued) four-component spinors n satisfying. i /Dn = nn (3.24). -
G-Adaptive mesh refinement - leveraging graphneural networks and…
www.damtp.cam.ac.uk/user/gam37/preprints/preprint_g-adaptive_mesh_refinement.pdf11 Jun 2024: There has been a proliferation of architectures inspiredby spectral graph theory [11], convolutional (GCN) [24], message passing (MPNN) [15] and atten-tional (GAT) [40] approaches. ... 24] T. N. Kipf and M. Welling. Semi-Supervised Classification with -
Vector Calculus University of Cambridge Part IA Mathematical Tripos…
www.damtp.cam.ac.uk/user/tong/vc/vc.pdf12 Jun 2024: 1.3.3 An Application: Work and Potential Energy 24. 1.3.4 A Subtlety 25. ... 24 –. We learn that a conservative force, one that can be written as (1.18), has a conserved.
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