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arXiv 2009.05640gr-qcastro-ph.COhep-phhep-th
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引力背景中标量快子不稳定性的存在性和增长率

Scalar tachyonic instabilities in gravitational backgrounds: Existence and growth rate

L. Perivolaropoulos, F. Skara

摘要:

众所周知,Klein Gordon(KG)方程$\Box Φ+ m^2Φ=0$在平坦的Minkowski时空中具有大尺度上的快子不稳定模($m^2<m_{cr}^2=0$),在$k=0$上获得了最大增长率$Ω_{F}(m)= \vert m \vert$.我们在具有质量$M$、电荷$Q$、宇宙学常数$Λ>0$和多重视界的Reissner-Nordström-deSitter(RN-dS)背景时空中研究了这些不稳定性。通过求解KG方程之间的事件和宇宙学视野的范围内,使用乌龟坐标$r_*$,我们确定了新兴的薛定谔类Regge-Wheeler方程对应的不稳定性的束缚态。我们发现,临界值$m_{cr}$,使$m^2<m_{cr}^2$的束缚态和不稳定性出现,仍然等于平坦的空间值$m_{cr}=0$的背景度量参数的所有值,尽管局部负性质的Regge-Wheeler潜在的$m=0$。然而,对于背景度量($Ω(Q/M,M^2 Λ, mM)< \vert m \vert$)的所有参数值,与平坦情况相比,$m^2<0$的快子不稳定性的增长率$Ω$显著降低。在$Q=0$和宇宙视界几乎等于事件视界($ξ\equiv 9M^2 Λ\simeq 1$)的近极端Schwarzschild-deSitter(SdS)黑洞的情况下,快子不稳定性的寿命增加是最大的。不稳定性增长延迟的物理原因似乎是宇宙学视界的存在,它倾向于缩小龟坐标中Regge-Wheeler势的负范围。

英文摘要:

It is well known that the Klein Gordon (KG) equation $\Box Φ+ m^2Φ=0$ has tachyonic unstable modes on large scales ($k^2<\vert m \vert^2$) for $m^2<m_{cr}^2=0$ in a flat Minkowski spacetime with maximum growth rate $Ω_{F}(m)= \vert m \vert$ achieved at $k=0$. We investigate these instabilities in a Reissner-Nordström-deSitter (RN-dS) background spacetime with mass $M$, charge $Q$, cosmological constant $Λ>0$ and multiple horizons. By solving the KG equation in the range between the event and cosmological horizons, using tortoise coordinates $r_*$, we identify the bound states of the emerging Schrodinger-like Regge-Wheeler equation corresponding to instabilities. We find that the critical value $m_{cr}$ such that for $m^2<m_{cr}^2$ bound states and instabilities appear, remains equal to the flat space value $m_{cr}=0$ for all values of background metric parameters despite the locally negative nature of the Regge-Wheeler potential for $m=0$. However, the growth rate $Ω$ of tachyonic instabilities for $m^2<0$ gets significantly reduced compared to the flat case for all parameter values of the background metric ($Ω(Q/M,M^2 Λ, mM)< \vert m \vert$). This increased lifetime of tachyonic instabilities is maximal in the case of a near extreme Schwarzschild-deSitter (SdS) black hole where $Q=0$ and the cosmological horizon is nearly equal to the event horizon ($ξ\equiv 9M^2 Λ\simeq 1$). The physical reason for this delay of instability growth appears to be the existence of a cosmological horizon that tends to narrow the negative range of the Regge-Wheeler potential in tortoise coordinates.

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