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Slide 1
www.tcm.phy.cam.ac.uk/~gjc29/talks/AustriaTalk2024.pdf7 May 2024: Slide 21. Slide 22. Slide 23. Slide 24. Slide 25. Slide 26. -
Publications: Biology
www.tcm.phy.cam.ac.uk/~bds10/dir/publications_bio.html25 Apr 2024: O. Karin, E. A. Miska and B. D. Simons, Cell Systems 14, 24-40 (2023) | doi: 10.1016/j.cels.2022.12.003 | bioRxiv preprint | pdf | doi: -
FT-E.dvi
www.tcm.phy.cam.ac.uk/impact/FT-E24.pdf16 Apr 2024: RANDOM PROCESSES, SHOT NOISE. AND MORTALITY. • 24 May. SHAPE OF SPIRAL GALLAXIES. • -
FePandatChemplusNIMS
www.phase-trans.msm.cam.ac.uk/2024/FePandatChemplusNIMS.pdf21 Apr 2024: LPBF Laser Scanning Strategies. 21/04/24 70. LPBF Laser Scanning Strategies. 21/04/24 71. ... Common metals and defectsNickel-based superalloys. 21/04/24 79. Common metals and defectsAluminum alloys. -
standardmodel
www.damtp.cam.ac.uk/user/tong/sm/standardmodel6.pdf22 Apr 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/standardmodel5.pdf22 Apr 2024: µ 12Tr GµG. µ. (5.24). The kinetic terms for the fermions are. -
standardmodel
www.damtp.cam.ac.uk/user/tong/sm/standardmodel4.pdf22 Apr 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. -
standardmodel
www.damtp.cam.ac.uk/user/tong/sm/standardmodel3.pdf22 Apr 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/standardmodel2.pdf22 Apr 2024: proportional to. eVScl! 0 as V! 1. (2.24). It’s obvious what’s going on here. -
standardmodel
www.damtp.cam.ac.uk/user/tong/sm/standardmodel1.pdf22 Apr 2024: 1.24). This is our starting point: representations of the Poincaré group are labelled by the.
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