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  2. LargeDUniversal

    www.damtp.cam.ac.uk/research/hep/files/conferences/EurostringTalks/Emparan.pdf
    6 Feb 2019: Finite energy of Hawking radn: 𝑟0 𝐿𝑃𝑙𝑎𝑛𝑐𝑘 𝐷2. Black hole perturbations.
  3. General Relativity

    www.damtp.cam.ac.uk/user/hsr1000/part3_gr_lectures.pdf
    12 Oct 2022: Mathematical Tripos Part III. General Relativity. Harvey Reall. CONTENTS. Contents. 1 Manifolds and tensors 4. 1.1 Introduction 4. 1.2 Differentiable manifolds 5. 1.3 Smooth functions 8. 1.4 Curves and vectors 9. 1.5 Covectors 14. 1.6 Abstract index
  4. The projective to Einstein correspondence and a kink on a wormhole

    www.damtp.cam.ac.uk/user/md327/alice_thesis.pdf
    30 Nov 2019: The projective to Einsteincorrespondence and a kink on a. wormhole. Alice Claire Waterhouse. Supervisor: Dr. Maciej Dunajski. Department of Applied Mathematics and Theoretical PhysicsUniversity of Cambridge. This dissertation is submitted for the
  5. EuroStrings2015.key

    www.damtp.cam.ac.uk/research/hep/files/conferences/EurostringTalks/Dabholkar.pdf
    6 Feb 2019: What is the exact quantum generaliza"on of the celebrated Bekenstein-‐Hawking formula? ... Bekenstein-‐Hawking-‐Wald entropy. ATISH DABHOLKAR QUANTUM ENTROPY OF BLACK HOLES. Compu@ng Quantum Entropy.
  6. , 20120576, published 2 January 2013469 2013 Proc. R. ...

    www.damtp.cam.ac.uk/user/md327/skyrmion_proc.pdf
    14 Aug 2013: doi:10.1098/rspa.2011.0616)3. Gibbons GW, Hawking SW. 1979 Classification of gravitational instanton symmetries.
  7. Preprint typeset in JHEP style - HYPER VERSION January ...

    www.damtp.cam.ac.uk/user/tong/string/string.pdf
    30 May 2023: Preprint typeset in JHEP style - HYPER VERSION January 2009. String TheoryUniversity of Cambridge Part III Mathematical Tripos. Dr David Tong. Department of Applied Mathematics and Theoretical Physics,. Centre for Mathematical Sciences,. Wilberforce
  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: This is often called the Bunch-Davies vacuum or Hartle-Hawking state. Excited states are then obtained by actingwith creation operators on this vacuum.
  9. 6 Oct 2014: Gibbons–Hawking background, are new. The octonionic instanton equation illustrates rather nicely the effects of the lack.
  10. Op#cal Conduc#vity from a Holographic La8ce Based on work ...

    www.damtp.cam.ac.uk/user/tong/talks/optical.pdf
    7 Jun 2012: Boundary field theory d=21. • Bulk d=31 black hole • Hawking radia#on = finite temperature • Electrically charged (Reissner-‐Nordstrom) = finite density.
  11. C:\Documents and Settings\Maciej Dunajski\My…

    www.damtp.cam.ac.uk/user/md327/PDElecture_old.pdf
    3 Jun 2008: Exercise. Implement the change of coordinates at the level of ĝ given by (hatted versionof) (1.2) to show that it is equivalent to the Gibbons–Hawking form.

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