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  • 4.0
    Impact Factor
  • 7.0
    CiteScore
  • 24 days
    Submission to First Decision
  • 5 days
    Acceptance to Publication

Galaxies

Galaxies is an international, peer-reviewed, open access journal on astronomy, astrophysics, and cosmology published bimonthly online by MDPI.

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All Articles (1,247)

  • Article
  • Open Access

We study the Kretschmann invariant K of the post-Newtonian spacetime of a slowly rotating, axially symmetric clump of collisionless matter with a prescribed Miyamoto–Nagai potential, whose metric and matter content to second order in the compactness β were constructed in a companion paper. At O(β2), K is a quadratic form in the Hessian of the potential, with closed-form central and asymptotic values. At O(β3) we show that the static part of K is a closed-form local function of the potential and of the matter fields at every point: the second-order metric functions, which solve a Poisson-type problem and encode the global mass distribution, enter only through the Ricci tensor, that is, only through the local matter. This follows from an exact expression of K for static spacetimes in terms of the tidal tensor of static observers and the local stresses, and holds for any regular prescribed potential. At a centre with isotropic stresses it reduces to , also for composite bulge–disc models. The only non-local contribution at this order is gravitomagnetic; it vanishes at the centre and, for an isotropic rotator, reaches within six scale radii about 10% (round clump) to 40% (thin disc) of the static third-order term. For galaxy-scale compactness, β∼10−6, all relativistic corrections are of relative order 10−7–10−5; the third-order term exceeds 10% of K only for compactness ≳0.04, the regime of relativistic star clusters. A central black hole dominates K within about 25 pc of the centre of a Milky-Way-like bulge–disc model.

Galaxies

21 October 2026

Structure of the third-order invariant, from the closed form (29). (a) Relative third-order correction 
  
    −
    
      K
      
        (
        3
        )
      
    
    /
    
      (
      β
      
        K
        
          (
          2
          )
        
      
      )
    
  
 for 
  
    A
    =
    ε
  
. (b) Share of the gradient and anisotropy terms, 
  
    −
    
      (
      
        K
        ∇
      
      +
      
        K
        π
      
      )
    
    /
    
      |
      
        K
        
          (
          3
          )
        
      
      |
    
  
, for 
  
    A
    =
    ε
  
. (c) The same share along the midplane, the axis and the diagonal 
  
    z
    =
    ρ
  
, as a function of the distance from the centre, for 
  
    ε
    =
    A
  
 (solid) and 
  
    ε
    =
    0.2
    A
  
 (dashed); dotted lines mark the asymptotic values 
  
    1
    /
    3
  
 (axis and diagonal) and 
  
    
      (
      
        A
        2
      
      +
      6
      
        ε
        2
      
      )
    
    /
    
      (
      4
      
        A
        2
      
      +
      4
      A
      ε
      +
      18
      
        ε
        2
      
      )
    
  
 (midplane). Open circles are the values obtained in the original submission from a grid evaluation for 
  
    A
    =
    ε
  
; the two innermost points differ from the closed form by the finite-difference error of that evaluation.
  • Article
  • Open Access

Black Hole Thermodynamics from Macroscopic Vacuum Elasticity

  • Dimitris M. Christodoulou,
  • Demosthenes Kazanas and
  • Silas G. T. Laycock

For the past fifty years, the physical foundations of black hole (BH) thermodynamics have remained widely contested because their original derivations rest at the theoretical intersection of general relativity and quantum field theory (QFT). This work provides an alternative macroscopic formulation by treating the physical vacuum in and around a BH as an elastic continuum strained by the presence of mass. Utilizing Hooke’s law of elasticity, we find that the radial strain at the event horizon of every Schwarzschild BH saturates at the same constant value. Under this principle of universal maximum strain, the laws of BH thermodynamics can be formulated within macroscopic continuum mechanics. This dispenses with the conventional QFT derivation in curved spacetime, paralleling the recent macroscopic descriptions of the Casimir effect. Our calculations are carried out using the Reformulated Planck System (RPS), which relies exclusively on Planck’s constant h. This h-native approach prevents the dimensional contamination of 3D continuum mechanics caused by the 2D geometric factor inherently embedded in Dirac’s reduced constant ℏ, a pivotal misstep first recognized in the iconic definitions of the fine-structure constant α and the gravitational coupling constant αg, which long precluded the identification of the α-dependence of the weak coupling constant αw=α. In BH thermodynamics, this RPS-based approach yields higher Hawking temperatures and lower Bekenstein entropies, both by a factor of 2π.

Galaxies

29 October 2026

  • Article
  • Open Access

This paper examines the thermal properties of a Bardeen-type black hole (BH) embedded in a cloud-of-strings and a quintessence background within the Tsallis non-extensive entropy framework. Within the extended thermodynamic phase space, generalized expressions are derived for the Tsallis thermodynamic temperature, heat capacity, equation of state, Gibbs free energy, and the associated critical parameters. Particular attention is paid to how the cloud-of-strings parameter, the magnetic charge and the quintessence field influence the resulting thermodynamic behaviour. A divergence in the heat capacity marking the boundary of local thermodynamic stability is identified from the heat-capacity analysis. The equation of state is further examined using the standard inflection-point conditions. For the representative parameter set considered in this work, the resulting mathematical critical solution has negative critical temperature and pressure and therefore lies outside the physical thermodynamic domain. Hence, no physically admissible Van der Waals-type critical point is obtained for the chosen parameters. Furthermore, the thermodynamic geometry is investigated using the HPEM metric, whose Ricci scalar provides an independent geometric characterization of the phase-transition structure. The results demonstrate that the cloud-of-strings parameter, magnetic charge, and quintessence field significantly influence the thermodynamic stability and phase structure of the BH, whereas the Tsallis entropy modifies the quantitative thermodynamic behaviour while preserving the overall qualitative phase characteristics.

Galaxies

15 October 2026

  • Article
  • Open Access

Chromosome maps (ChMs) reveal multiple stellar populations in globular clusters (GCs), but radial trends can depend on how overlapping structures are partitioned. We analyse 56 Galactic GCs with Hubble Space Telescope UV Globular Cluster Survey (HUGS) photometry, separating the stability of star-by-star Gaussian-mixture assignments from that of radial statistics. Strict two-family assignments are stable in only 11/55 eligible clusters, whereas the posterior-weighted radial contrast is reproducible for 34/55. In this radial-stability sample, none of four pre-specified broad-family tests shows a robust association with compactness or half-mass relaxation time. By contrast, the label-free absolute median-radius separation between the lowest and highest 30 per cent of normalized ChM pseudocolour increases with compactness (N=34, ρ=0.500, permutation p=0.00256) and remains positive after F814W matching and common-footprint restrictions. Secondary tests show no comparable monotonic ordering with remaining-mass fraction, a present-day dynamical-age proxy, or the atlas-based global second-generation fraction. Larger amplitudes instead occur at greater compactness, higher central density, and shorter core-relaxation time. Because these central variables are strongly collinear, we interpret them as a common structural-state axis rather than unique causal drivers. Thus, the magnitude—not a universal direction—of extreme-tail radial differentiation is linked to present-day central structural state.

Galaxies

9 October 2026

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Galaxies - ISSN 2075-4434