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SUMMARY:General relativistic solutions in minimal theory of bigravity
DTSTART:20231012T143000Z
DTEND:20231012T160000Z
DTSTAMP:20260914T001603Z
UID:ce46128b-f82b-442c-b69e-2d2b6fb9f6f5
SEQUENCE:1
CREATED:20231006T081455Z
DESCRIPTION: Abstract: We investigate dynamical properties of static and s
 pherically symmetric systems in the self-accelerating branch of the Minima
 l Theory of Bigravity (MTBG).  In the former part\, we study the gravitat
 ional collapse of pressure-less dust and find special solutions\, where\, 
 in both the physical and fiducial sectors\, the exterior and interior spac
 etime geometries are given by the Schwarzschild spacetimes and the Friedma
 nn-Lemaitre-Robertson-Walker universes dominated by pressure-less dust\, r
 espectively\, with specific time slicings. In the case that the Lagrange m
 ultipliers are trivial and have no jump across the matter interfaces in bo
 th the physical and fiducial sectors\, the junction conditions across them
  remain the same as those in general relativity (GR). For simplicity\, we 
 foliate the interior geometry by homogeneous and isotropic spacetimes. We 
 find interesting classes of exact solutions that represent gravitational c
 ollapse in MTBG. In the spatially-flat case\, under a certain tuning of th
 e initial condition\, we find exact solutions of matter collapse in which 
 the two sectors evolve independently. In the spatially-closed case\, once 
 the matter energy densities and the Schwarzschild radii are tuned between 
 the two sectors\, we find exact solutions that correspond to the Oppenheim
 er-Snyder model in GR. In the latter part\, we study odd-parity perturbati
 ons of the Schwarzschild-de Sitter solutions written in the spatially-flat
  coordinates. For the higher-multipole modes $\\ell\\geq2$\, we find that 
 in general the system reduces to that of four physical modes\, where two o
 f them are dynamical and the remaining two are shadowy\, i.e.\, satisfying
  only elliptic equations. In the case that the ratio of the lapse function
 s between the physical and fiducial sectors are equal to a constant determ
 ined by the parameters of the theory\, the two dynamical modes are decoupl
 ed from each other but sourced by one of the shadowy modes.Otherwise\, the
  two dynamical modes are coupled to each other and sourced by the two shad
 owy modes. At least for the cases of collapse described in this paper\, we
  find that the ratio of the lapse functions is determined by the propertie
 s of the collapse itself. On giving appropriate boundary conditions to the
  shadowy modes as to not strongly back-react/influence the dynamics of the
  master variables\, in the high frequency and short wavelength limits\, we
  show that the two dynamical modes do not suffer from ghost or gradient in
 stabilities. 
LAST-MODIFIED:20231006T081455Z
LOCATION:Sala de Seminários do DF\,  Pavilhão de Física\, 2º piso
URL:http://df.vps.tecnico.ulisboa.pt/pt/eventos/general-relativistic-solut
 ions-in-minimal-theory-of-bigravity/
X-ALT-DESC;FMTTYPE=text/html:<p data-block-key="91vkf"><b> Abstract: </b><
 /p><p data-block-key="6s9l3">We investigate dynamical properties of static
  and spherically symmetric systems in the self-accelerating branch of the 
 Minimal Theory of Bigravity (MTBG).  In the former part\, we study the gr
 avitational collapse of pressure-less dust and find special solutions\, wh
 ere\, in both the physical and fiducial sectors\, the exterior and interio
 r spacetime geometries are given by the Schwarzschild spacetimes and the F
 riedmann-Lemaitre-Robertson-Walker universes dominated by pressure-less du
 st\, respectively\, with specific time slicings. <br/><br/>In the case tha
 t the Lagrange multipliers are trivial and have no jump across the matter 
 interfaces in both the physical and fiducial sectors\, the junction condit
 ions across them remain the same as those in general relativity (GR). For 
 simplicity\, we foliate the interior geometry by homogeneous and isotropic
  spacetimes. We find interesting classes of exact solutions that represent
  gravitational collapse in MTBG. <br/><br/>In the spatially-flat case\, un
 der a certain tuning of the initial condition\, we find exact solutions of
  matter collapse in which the two sectors evolve independently. In the spa
 tially-closed case\, once the matter energy densities and the Schwarzschil
 d radii are tuned between the two sectors\, we find exact solutions that c
 orrespond to the Oppenheimer-Snyder model in GR. In the latter part\, we s
 tudy odd-parity perturbations of the Schwarzschild-de Sitter solutions wri
 tten in the spatially-flat coordinates. <br/><br/>For the higher-multipole
  modes $\\ell\\geq2$\, we find that in general the system reduces to that 
 of four physical modes\, where two of them are dynamical and the remaining
  two are shadowy\, i.e.\, satisfying only elliptic equations. In the case 
 that the ratio of the lapse functions between the physical and fiducial se
 ctors are equal to a constant determined by the parameters of the theory\,
  the two dynamical modes are decoupled from each other but sourced by one 
 of the shadowy modes.<br/><br/>Otherwise\, the two dynamical modes are cou
 pled to each other and sourced by the two shadowy modes. At least for the 
 cases of collapse described in this paper\, we find that the ratio of the 
 lapse functions is determined by the properties of the collapse itself. On
  giving appropriate boundary conditions to the shadowy modes as to not str
 ongly back-react/influence the dynamics of the master variables\, in the h
 igh frequency and short wavelength limits\, we show that the two dynamical
  modes do not suffer from ghost or gradient instabilities.<br/> </p>
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