Fetching the paper…
Reading the bibliography…
We argue that the effective theory describing the long-wavelength dynamics of black branes is the same effective theory that describes the dynamics of biophysical membranes.
P. Canham, Journal of Theoretical Biology 26
1970
Earlier work this paper cites.
W. Helfrich, Z. Naturforsch. C 28
1973
Earlier work this paper cites.
U. Seifert, Advances in Physics 46
1997
Earlier work this paper cites.
G. Policastro, D. Son, and A. Starinets, Phys.Rev.Lett. 87
2001
Earlier work this paper cites.
R. Capovilla, J. Guven, and J. A. Santiago, Journal of Physics A: Mathematical and General 36
2003
Earlier work this paper cites.
R. Emparan, T. Harmark, V. Niarchos, N. A. Obers, and M. J. Rodriguez, JHEP 10
2007
Earlier work this paper cites.
S. Bhattacharyya, V. E. Hubeny, S. Minwalla, and M. Rangamani, JHEP 0802
2008
Earlier work this paper cites.
R. Emparan, T. Harmark, V. Niarchos, and N. A. Obers, Phys. Rev. Lett. 102
2009
Earlier work this paper cites.
R. Emparan, T. Harmark, V. Niarchos, and N. A. Obers, JHEP 03
2010
Cited alongside, same era.
R. Emparan, T. Harmark, V. Niarchos, and N. A. Obers, JHEP 04
2010
Cited alongside, same era.
J. Armas, J. Camps, T. Harmark, and N. A. Obers, JHEP 1202
2012
Cited alongside, same era.
J. Armas, J. Gath, and N. A. Obers, Phys. Rev. Lett. 109
2012
Cited alongside, same era.
N. Banerjee, J. Bhattacharya, S. Bhattacharyya, S. Jain, S. Minwalla, et al. , JHEP 1209
2012
Cited alongside, same era.
2013
Later among the works it cites.
J. Armas and N. A. Obers, Phys.Rev. D87
2013
Later among the works it cites.
B. Kleihaus, J. Kunz, and E. Radu, Phys.Lett. B718
2013
Later among the works it cites.
2014
Closest in time.
Z. Tu and Z. Ou-Yang, Advances in Colloid and Interface Science 208
2014
Closest in time.
alphaXiv searches the wider corpus for related work and actual follow-ups.
alphaXiv is searching for related work…
K. Jensen, M. Kaminski, P. Kovtun, R. Meyer, A. Ritz, et al. , Phys.Rev.Lett. 109
2012
Cited alongside, same era.
J. Camps and R. Emparan, JHEP 1203
2012
Cited alongside, same era.
Derivatives of the thickness r 0 r_{0} can be exchanged by derivatives of the fluid velocity [ 5 , 6 ] . Furthermore, the black branes can also be rotating on transverse directions in which case one also must take into account contributions due the extrinsic twist potential ω a i j {\omega_{a}}^{ij} [ 5 , 6 ]
Cited in the paper.
This equilibrium condition is related to the one found previously in [ 5 ] via the field redefinition R → R + ( n + 1 ) ( n + 4 ) n 2 ( n + 2 ) ξ ( n ) r 0 ε R\to R+\frac{(n+1)(n+4)}{n^{2}(n+2)}\xi(n)r_{0}\varepsilon
Cited in the paper.
Our analytic results cannot be compared to D = 6 D=6 black rings because in D = 6 D=6 back reaction corrections dominate over finite thickness corrections [ 3 ]
Cited in the paper.
J. Armas and T. Harmark, To appear
Cited in the paper.
2014
Closest in time.
O. J. Dias, J. E. Santos, and B. Way, JHEP 1407
2014
Closest in time.