# The European Physical Journal C

The European Physical Journal C > 2019 > 79 > 8 > 1-40

The European Physical Journal C > 2019 > 79 > 8 > 1-11

*n*-excited black holes. We show that the $$n=0$$ n=0 black hole is stable against full perturbations,...

The European Physical Journal C > 2019 > 79 > 8 > 1-10

*s*-wave $$\Lambda {\bar{K}}$$ ΛK¯ or $$\Sigma {\bar{K}}$$ ΣK¯ bound state. Based on this molecule picture, we establish the Bethe–Salpeter equations for $$\Xi (1620)$$ Ξ(1620) in the ladder and instantaneous approximations. We solve the Bethe–Salpeter equations for the $$\Lambda {\bar{K}}$$ ΛK¯ and $$\Sigma {\bar{K}}$$...

The European Physical Journal C > 2019 > 79 > 8 > 1-11

The European Physical Journal C > 2019 > 79 > 8 > 1-8

*f*(

*T*) gravity in

*N*-dimensions, where $$f(T)=T+\alpha T^{2}$$ f(T)=T+αT2 . These solutions are nontrivial extensions of the solutions presented in Lemos (Phys Lett B 353:46–51. arXiv:gr-qc/9404041, 1995) and Awad (Class Quantum Gravity 20:2827–2834. arXiv:hep-th/0209238, 2003) in the context of general relativity...

The European Physical Journal C > 2019 > 79 > 8 > 1-38

The European Physical Journal C > 2019 > 79 > 8 > 1-34

The European Physical Journal C > 2019 > 79 > 8 > 1-17

The European Physical Journal C > 2019 > 79 > 8 > 1-23

*SO*(4) and

*SO*(3) symmetries corresponding...

The European Physical Journal C > 2019 > 79 > 8 > 1-31

The European Physical Journal C > 2019 > 79 > 8 > 1-26

The European Physical Journal C > 2019 > 79 > 8 > 1-18

The European Physical Journal C > 2019 > 79 > 8 > 1-3

The European Physical Journal C > 2019 > 79 > 8 > 1-8

The European Physical Journal C > 2019 > 79 > 8 > 1-18

*SL*(5). The embedding tensor in $$\mathbf {15}$$ 15 representation leads to $$CSO(p,q,5-p-q)$$...

The European Physical Journal C > 2019 > 79 > 8 > 1-9

The European Physical Journal C > 2019 > 79 > 8 > 1-14

*x*evolution that appear in the literature. We find that all of them generate the same leading anti-collinear poles in Mellin space which agree with BFKL up to NLL order and up to NNLL in $$N=4$$ N=4 sYM. The coefficients of subleading poles vanish up to NNLL order for all constraints and we prove...

The European Physical Journal C > 2019 > 79 > 8 > 1-6

The European Physical Journal C > 2019 > 79 > 8 > 1-17

The European Physical Journal C > 2019 > 79 > 8 > 1-5