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@let@token Dynamical Black Hole Entropy
https://www.dpmms.cam.ac.uk/~rbdt2/NAGR/NAGR_07_Wald.pdf9 Nov 2023: cross-sections C1 and C2 yieldsκ. 2π[δSC2 δSC1 ] =. ξaδCa =. δTabξ. akbhdV dn2x. where ka is the tangent to the affinely parametrized generatorsof the horizon. ... Since. ka =1. κVξa. this is equivalent to. V2SvNV 2. 2πκ. -
HX1Lycée Louis le Grand 2015-2016 Chimie Classe de Mathématiques ...
https://www.dpmms.cam.ac.uk/~aptm3/docs/lecture-notes/Chimie-Sup.pdf31 Aug 2023: d’acidité :. Ka =[H3O+] [A – ]. [HA]. On note de plus pKa = log Ka. ... HB][HA][B – ] =. Ka,AKa,B. , d’où pK = pKa,B pKa,A. -
The density of integral quadratic forms having ak-dimensional totally …
https://www.dpmms.cam.ac.uk/~taf1000/papers/isotropic-subspaces.pdf22 Jan 2024: ρp(k,2k 1) =. aQp/(Qp)2P2k1(d(Q) = (1)ka,c(Q) = (1,a)k);. ρp(k,2k 2) = 1P2k2(d(Q) = (1)k1,c(Q) = 1). ... This gives four Qp-equivalence classes of forms, with invariants d(Q) = (1)ka andc(Q) = (1,a)k. -
Algebraic TopologyOscar Randal-Williams…
https://www.dpmms.cam.ac.uk/~or257/teaching/notes/at.pdf31 Jan 2024: Algebraic TopologyOscar Randal-Williams. https://www.dpmms.cam.ac.uk/or257/teaching/notes/at.pdf. 1 Introduction 11.1 Some recollections and conventions. 21.2 Cell complexes. 3. 2 Homotopy and the fundamental group 42.1 Homotopy. 42.2 Paths. 72.3 -
GLOBAL SECTIONS OF EQUIVARIANT LINE BUNDLES ON THE p-ADIC ...
https://www.dpmms.cam.ac.uk/~sjw47/Drinfeld.pdf20 Dec 2023: GLOBAL SECTIONS OF EQUIVARIANT LINE BUNDLES ON. THE p-ADIC UPPER HALF PLANE. KONSTANTIN ARDAKOV AND SIMON WADSLEY. Abstract. Let F be a finite extension of Qp, let F be Drinfeld’s upper half-plane over F and let G0 the subgroup of GL2(F ) -
The Ward Correspondence and StationaryAxisymmetric Spacetimes…
https://www.dpmms.cam.ac.uk/~gt306/mp1.pdf16 Jan 2024: 4cK. cηab. (14). The general solution to eq. (14) is. Ka = Ta Labxb Rxa xbxbSa 2Sbxbxa,. -
HX1Lycée Louis le Grand 2015-2016 Physique Classe de Mathématiques ...
https://www.dpmms.cam.ac.uk/~aptm3/docs/lecture-notes/Physique-Sup.pdf31 Aug 2023: On a donc ici Epe = 12 kA2 cos2(ωt φ). Au final, on obtient Em = Ec Epe = 12 kA. ... 2. On s’intéresse aux valeurs moyennes des différentes formes d’énergie. On a :. ⟨Ec⟩ =12 kA. 2〈sin2(ωt φ). 〉et ⟨Epe⟩ =. 12 kA. 2〈cos2(ωt φ). -
HX1Lycée Louis le Grand 2015-2016 Mathématiques Classe de…
https://www.dpmms.cam.ac.uk/~aptm3/docs/lecture-notes/Mathematiques-Sup.pdf31 Aug 2023: HX1Lycée Louis le Grand 2015-2016. Mathématiques. Classe de Mathématiques Supérieures. Cours de Véronique Lods. Notes de Alexis Marchand. Table des matières. 1 Complexes 1I Définition de C. 1II Conjugaison et module. 1III Étude de U = {z C, -
MP∗2Lycée Louis le Grand 2016-2017 Mathématiques Classe de…
https://www.dpmms.cam.ac.uk/~aptm3/docs/lecture-notes/Mathematiques-Spe.pdf31 Aug 2023: MP2Lycée Louis le Grand 2016-2017. Mathématiques. Classe de Mathématiques Spéciales. Cours de Yves Duval. Notes de Alexis Marchand. Table des matières. 1 Suites Réelles et Complexes 1I Bornes supérieures et bornes inférieures. 1II Suites
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