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schedule
https://www.dpmms.cam.ac.uk/~rbdt2/NAGR/NAGR_schedule_cont.pdf9 Nov 2023: 15:00. 15:05. 15:10. 15:15. 15:20. 15:25. 15:30. 15:35. Wednesday 11/Oct:. Tousif Islam (KITP, UC Santa Barbara)Connection between linear perturbation theory and -
Characteristic classes and K-theoryOscar Randal-Williams…
https://www.dpmms.cam.ac.uk/~or257/teaching/notes/Kthy_short.pdf18 Jan 2023: c1(L) = c1(γ1,n1C ) 1 1 c1(γ. 1,n1C ). 20 Chapter 2 Characteristic classes. -
Characteristic classes and K-theoryOscar Randal-Williams…
https://www.dpmms.cam.ac.uk/~or257/teaching/notes/Kthy_long.pdf13 Mar 2023: ci(E) = (1)ici(E). 20 Chapter 2 Characteristic classes. Example 2.8.5. Over CPnCPn consider the line bundle L := π1 (γ1,n1C )π2 (γ. -
Nonlinear aspects GR @ Princeton
https://www.dpmms.cam.ac.uk/~rbdt2/NAGR/NAGR_16_Bonga.pdf9 Nov 2023: Equal mass l=2,4,6,. are only non-zero. Notation: ωlmn ωln. For l=2, possible quadratic modes are ω20 x 20 and ω20 x 40 possible versions with overtones. -
Geometric inverse problems with emphasis on two dimensions Gabriel ...
https://www.dpmms.cam.ac.uk/~gpp24/GIP2D_driver.pdf1 Feb 2023: 1.4 The Funk transform1.4 The Funk transform 20. 2 Radial sound speeds2 Radial sound speeds 26.
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