Alessandro Drago
Current Organizations / Institutes
The organizations/institutes from the scholar's latest article
Research Subjects
Research Interests
Alessandro Drago has a total of 759 co-authors. Here are the top co-authors by number of shared publications:
- Giuseppe Pagliara
Department of Physics and Earth Science, University of Ferrara, 44122 Ferrara, Italy
16 shared publications - Francesco Di Clemente
Department of Physics University of Houston 77204 Houston TX USA
11 shared publications - Andrea Lavagno
Department of Applied Science and Technology, Politecnico di Torino, 10129 Torino, Italy
9 shared publications - Mirco Guerrini
Department of Physics and Earth Science, University of Ferrara, 44122 Ferrara, Italy
6 shared publications Giuseppe Pagliara
5 shared publications- Valentina Mantovani Sarti
Technische Universität München
4 shared publications
Latest Publications
- 9 October 2026
- Published by Elsevier in Journal of Subatomic Particles and Cosmology
- Vol. 6
Strange quark matter as dark matter
- 9 October 2026
- Published by Elsevier in Journal of Subatomic Particles and Cosmology
- Vol. 6
Strange quark matter as dark matter
- Open Access
- 8 October 2026
- Published by Elsevier in SSRN Electronic Journal
Cosmological QCD phase transition investigation with state of the art lattice QCD equation of state
We compute the full cosmic trajectories of the early Universe across the QCD phase diagram from $T\simeq500,\mathrm{MeV}$ to $30,\mathrm{MeV}$, assuming $\beta$-equilibrated matter. The trajectories are obtained by simultaneously enforcing baryon-number, electric-charge, and lepton-flavor conservation and are closed with a state-of-the-art lattice-QCD equation of state based on a fourth-order Taylor expansion in the chemical potentials. The construction combines the latest $(2+1)$-flavor lattice susceptibilities with charm-quark contributions, yielding a consistent $(2+1+1)$-flavor equation of state. Comparisons with an ideal quark--gluon plasma and a hadron-resonance gas are used to isolate interaction effects. We analyze both flavor-symmetric configurations, $(\ell_e=\ell_\mu=\ell_\tau=\ell/3)$, and strongly flavor-asymmetric cases with small total lepton asymmetry, $|\ell|\lesssim10^{-2}$, but potentially large individual flavor asymmetries. Increasing $|\ell|$ systematically shifts the cosmic trajectories toward larger baryon chemical potential $\mu_B$ and more negative electric-charge chemical potential $\mu_Q$. In $\tau$--$\mu$ asymmetric configurations, a non-monotonic ``bounce'' appears once the $\tau$ chemical potential reaches the $\tau$-lepton mass threshold, producing a local maximum in $\mu_B(T)$ whose position depends on $\ell_\tau$. By contrast, $\mu$--$e$ asymmetric configurations approach a limiting trajectory and do not develop such a maximum. These results establish, for each temperature, an upper bound on the baryon chemical potential attainable through lepton-flavor asymmetry alone. Assuming the QCD critical end point retains only a modest dependence on $\mu_Q$ relative to present lattice estimates obtained at $\mu_Q=0$, all trajectories explored, including extreme flavor-asymmetric cases, remain on the crossover side of the phase diagram. Thus, even substantial individual lepton-flavor asymmetries are unlikely to drive the early Universe into a first-order QCD transition unless the critical region is shifted to significantly lower values of $\mu_B/T$ by nonzero $\mu_Q$. Our analysis therefore constrains the QCD-era relic of standard cosmology to the conventional chiral crossover scenario, while also estimating the baryon and lepton asymmetries required for trajectories that would pass substantially closer to the QCD critical point.- 8 October 2026
- Published by Elsevier in SSRN Electronic Journal
Open AccessCosmological QCD phase transition investigation with state of the art lattice QCD equation of state
We compute the full cosmic trajectories of the early Universe across the QCD phase diagram from $T\simeq500,\mathrm{MeV}$ to $30,\mathrm{MeV}$, assuming $\beta$-equilibrated matter. The trajectories are obtained by simultaneously enforcing baryon-number, electric-charge, and lepton-flavor conservation and are closed with a state-of-the-art lattice-QCD equation of state based on a fourth-order Taylor expansion in the chemical potentials. The construction combines the latest $(2+1)$-flavor lattice susceptibilities with charm-quark contributions, yielding a consistent $(2+1+1)$-flavor equation of state. Comparisons with an ideal quark--gluon plasma and a hadron-resonance gas are used to isolate interaction effects. We analyze both flavor-symmetric configurations, $(\ell_e=\ell_\mu=\ell_\tau=\ell/3)$, and strongly flavor-asymmetric cases with small total lepton asymmetry, $|\ell|\lesssim10^{-2}$, but potentially large individual flavor asymmetries. Increasing $|\ell|$ systematically shifts the cosmic trajectories toward larger baryon chemical potential $\mu_B$ and more negative electric-charge chemical potential $\mu_Q$. In $\tau$--$\mu$ asymmetric configurations, a non-monotonic ``bounce'' appears once the $\tau$ chemical potential reaches the $\tau$-lepton mass threshold, producing a local maximum in $\mu_B(T)$ whose position depends on $\ell_\tau$. By contrast, $\mu$--$e$ asymmetric configurations approach a limiting trajectory and do not develop such a maximum. These results establish, for each temperature, an upper bound on the baryon chemical potential attainable through lepton-flavor asymmetry alone. Assuming the QCD critical end point retains only a modest dependence on $\mu_Q$ relative to present lattice estimates obtained at $\mu_Q=0$, all trajectories explored, including extreme flavor-asymmetric cases, remain on the crossover side of the phase diagram. Thus, even substantial individual lepton-flavor asymmetries are unlikely to drive the early Universe into a first-order QCD transition unless the critical region is shifted to significantly lower values of $\mu_B/T$ by nonzero $\mu_Q$. Our analysis therefore constrains the QCD-era relic of standard cosmology to the conventional chiral crossover scenario, while also estimating the baryon and lepton asymmetries required for trajectories that would pass substantially closer to the QCD critical point. - Open Access
- 18 August 2026
- Published by Elsevier in SSRN Electronic Journal
Strange quark matter as dark matter
Forty years after Witten's proposal, we reassess whether dark matter can be made of strangelets, macroscopic clusters of up, down and strange quarks. Using a state-of-the-art lattice QCD equation of state, we show that in standard cosmology the cosmic trajectory cannot reach the QCD critical end point, so that strangelet formation cannot rely on a first-order transition. We propose an alternative path near the crossover, combining strong quark correlations, a chemical-mechanical instability in the hadronic phase and color superconductivity. Partial evaporation then fixes the ordinary-to-dark matter ratio and a mass spectrum peaking at $A\sim10^{35}-10^{40}$. Unlike primordial black holes, strangelets do not undergo Hawking evaporation and can populate masses below $10^{17}\,\mathrm{g}$. Lunar seismometry, motivated by the unidentified Apollo shallow moonquakes, is a promising probe.- 18 August 2026
- Published by Elsevier in SSRN Electronic Journal
Open AccessStrange quark matter as dark matter
Forty years after Witten's proposal, we reassess whether dark matter can be made of strangelets, macroscopic clusters of up, down and strange quarks. Using a state-of-the-art lattice QCD equation of state, we show that in standard cosmology the cosmic trajectory cannot reach the QCD critical end point, so that strangelet formation cannot rely on a first-order transition. We propose an alternative path near the crossover, combining strong quark correlations, a chemical-mechanical instability in the hadronic phase and color superconductivity. Partial evaporation then fixes the ordinary-to-dark matter ratio and a mass spectrum peaking at $A\sim10^{35}-10^{40}$. Unlike primordial black holes, strangelets do not undergo Hawking evaporation and can populate masses below $10^{17}\,\mathrm{g}$. Lunar seismometry, motivated by the unidentified Apollo shallow moonquakes, is a promising probe. - Open Access
- 29 July 2026
- Published by Elsevier in Journal of High Energy Astrophysics
- Vol. 55
Is the coexistence of strange quark stars and hadronic stars favored by astrophysical data? A Bayesian analysis
- 29 July 2026
- Published by Elsevier in Journal of High Energy Astrophysics
- Vol. 55
Open AccessIs the coexistence of strange quark stars and hadronic stars favored by astrophysical data? A Bayesian analysis
- 15 January 2026
- Published by American Physical Society (APS) in Physical Review D
- Vol. 113 (2)
Cosmic trajectories calculation with a state of the art lattice QCD equation of state
- 15 January 2026
- Published by American Physical Society (APS) in Physical Review D
- Vol. 113 (2)
Cosmic trajectories calculation with a state of the art lattice QCD equation of state
- 4 October 2025
- Published by Elsevier in Journal of High Energy Astrophysics
- Vol. 50
On the formation of strange quark stars from supernova in compact binaries
- 4 October 2025
- Published by Elsevier in Journal of High Energy Astrophysics
- Vol. 50
On the formation of strange quark stars from supernova in compact binaries
- Open Access
Role of Thermal Fluctuations in Nucleation of Three-Flavor Quark Matter
We present a framework that aims to investigate the role of thermal fluctuations in matter composition and color superconductivity in the nucleation of three-flavor deconfined quark matter in the typical conditions of high-energy astrophysical systems related to compact stars. It is usually assumed that the flavor composition is locally fixed during the formation of the first seed of deconfined quark matter, since a weak interaction acts too slowly to re-equilibrate flavors. However, the matter composition fluctuates around its average equilibrium values at the typical temperatures of high-energy astrophysical processes. Here, we extend our previous two-flavor nucleation formalism to a three-flavor case. We develop a thermodynamic framework incorporating finite-size effects and thermal fluctuations in the local composition to compute the nucleation probability as the product of droplet formation and composition fluctuation rates. Moreover, we discuss the role of color superconductivity in nucleation, arguing that it can play a role only in systems larger than the typical coherence length of diquark pairs. We found that thermal fluctuations in the matter composition led to lowering the potential barrier between the metastable hadronic phase and the stable quark phase. Moreover, the formation of diquark pairs reduced the critical radius and thus the potential barrier in the low baryon density and temperature regime.
Open AccessRole of Thermal Fluctuations in Nucleation of Three-Flavor Quark Matter
We present a framework that aims to investigate the role of thermal fluctuations in matter composition and color superconductivity in the nucleation of three-flavor deconfined quark matter in the typical conditions of high-energy astrophysical systems related to compact stars. It is usually assumed that the flavor composition is locally fixed during the formation of the first seed of deconfined quark matter, since a weak interaction acts too slowly to re-equilibrate flavors. However, the matter composition fluctuates around its average equilibrium values at the typical temperatures of high-energy astrophysical processes. Here, we extend our previous two-flavor nucleation formalism to a three-flavor case. We develop a thermodynamic framework incorporating finite-size effects and thermal fluctuations in the local composition to compute the nucleation probability as the product of droplet formation and composition fluctuation rates. Moreover, we discuss the role of color superconductivity in nucleation, arguing that it can play a role only in systems larger than the typical coherence length of diquark pairs. We found that thermal fluctuations in the matter composition led to lowering the potential barrier between the metastable hadronic phase and the stable quark phase. Moreover, the formation of diquark pairs reduced the critical radius and thus the potential barrier in the low baryon density and temperature regime.
- Open Access
On the formation of strange quark stars from supernova in compact binaries
Strange quark stars (SQSs), namely compact stars entirely composed of deconfined quark matter, are characterized by similar masses and compactness to neutron stars (NSs) and have been theoretically proposed to exist in the Universe since the 1970s. However, multiwavelength observations of compact stars in the last 50 years have not yet led to an unambiguous SQS identification. This article explores whether SQSs could form in the supernova (SN) explosion of an evolved star (e.g., carbon-oxygen, or Wolf-Rayet) occurring in a binary with the companion being a neutron star (NS). The collapse of the iron core of the evolved star generates a newborn NS and the SN explosion. Part of the ejected matter accretes onto the NS companion as well as onto the newborn NS via matter fallback. The accretion occurs at hypercritical (highly super-Eddington) rates, transferring mass and angular momentum to the stars. We present numerical simulations of this scenario and demonstrate that the density increase in the NS interiors during the accretion process may induce quark matter deconfinement, suggesting the possibility of SQS formation. We discuss the astrophysical conditions under which such a transformation may occur and possible consequences.
Open AccessOn the formation of strange quark stars from supernova in compact binaries
Strange quark stars (SQSs), namely compact stars entirely composed of deconfined quark matter, are characterized by similar masses and compactness to neutron stars (NSs) and have been theoretically proposed to exist in the Universe since the 1970s. However, multiwavelength observations of compact stars in the last 50 years have not yet led to an unambiguous SQS identification. This article explores whether SQSs could form in the supernova (SN) explosion of an evolved star (e.g., carbon-oxygen, or Wolf-Rayet) occurring in a binary with the companion being a neutron star (NS). The collapse of the iron core of the evolved star generates a newborn NS and the SN explosion. Part of the ejected matter accretes onto the NS companion as well as onto the newborn NS via matter fallback. The accretion occurs at hypercritical (highly super-Eddington) rates, transferring mass and angular momentum to the stars. We present numerical simulations of this scenario and demonstrate that the density increase in the NS interiors during the accretion process may induce quark matter deconfinement, suggesting the possibility of SQS formation. We discuss the astrophysical conditions under which such a transformation may occur and possible consequences.
- Open Access
Role of thermal fluctuations in nucleation of three-flavor quark matter
We present a framework that aims to investigate the role of thermal fluctuations of the matter composition and color-superconductivity in the nucleation of three-flavor deconfined quark matter in the typical conditions of high-energy astrophysical systems related to compact stars. It is usually assumed that the flavor composition is locally fixed during the formation of the first seed of deconfined quark matter since weak interaction acts too slowly to re-equilibrate flavors. However, the matter composition fluctuates around its average equilibrium values at the typical temperatures of high-energy astrophysical processes. Here, we extend our previous two-flavor nucleation formalism to a three-flavor case. We develop a thermodynamic framework incorporating finite-size effects and thermal fluctuations of local composition to compute the nucleation probability as the product of droplet formation and composition fluctuation rates. Moreover, we discuss the role of color-superconductivity in nucleation, arguing that it can play a role only in systems larger than the typical coherence length of diquark pairs. We found that thermal fluctuations of the matter composition lead to lowering the potential barrier between the metastable hadronic phase and the stable quark phase. Moreover, the formation of diquark pairs reduces the critical radius and thus the potential barrier in the low baryon density and temperature regime.
Open AccessRole of thermal fluctuations in nucleation of three-flavor quark matter
We present a framework that aims to investigate the role of thermal fluctuations of the matter composition and color-superconductivity in the nucleation of three-flavor deconfined quark matter in the typical conditions of high-energy astrophysical systems related to compact stars. It is usually assumed that the flavor composition is locally fixed during the formation of the first seed of deconfined quark matter since weak interaction acts too slowly to re-equilibrate flavors. However, the matter composition fluctuates around its average equilibrium values at the typical temperatures of high-energy astrophysical processes. Here, we extend our previous two-flavor nucleation formalism to a three-flavor case. We develop a thermodynamic framework incorporating finite-size effects and thermal fluctuations of local composition to compute the nucleation probability as the product of droplet formation and composition fluctuation rates. Moreover, we discuss the role of color-superconductivity in nucleation, arguing that it can play a role only in systems larger than the typical coherence length of diquark pairs. We found that thermal fluctuations of the matter composition lead to lowering the potential barrier between the metastable hadronic phase and the stable quark phase. Moreover, the formation of diquark pairs reduces the critical radius and thus the potential barrier in the low baryon density and temperature regime.
- Open Access
- 20 January 2025
- Published by Oxford University Press (OUP) in Monthly Notices of the Royal Astronomical Society
- Vol. 537 (2) , 1056-1069
Strange quark matter as dark matter: 40 yr later, a reappraisal
Forty years ago Witten suggested that dark matter could be composed of macroscopic clusters of strange quark matter. This idea was very popular for several years, but it dropped out of fashion once lattice quantum chromodynamics calculations indicated that the confinement/deconfinement transition, at small baryonic chemical potential, is not first order, which seemed to be a crucial requirement in order to produce large clusters of quarks. Here, we revisit the conditions under which strangelets can be produced in the Early Universe. We discuss the impact of an instability in the hadronic phase separating a low density, positive-strange-charge phase from a high-density phase with a negative strange charge. This second phase can rapidly stabilize by forming colour-superconducting gaps. The strangelets then undergo partial evaporation. In this way, we obtain distributions of their sizes in agreement with the observational constraints and we discuss the many astrophysical and cosmological implications of these objects. Finally, we examine the most promising techniques to detect this type of strangelets. We also show that strangelets can exist with masses $\lesssim $1017 g, while primordial black holes are ruled out in that mass range, allowing us to distinguish between these two dark matter candidates.
- 20 January 2025
- Published by Oxford University Press (OUP) in Monthly Notices of the Royal Astronomical Society
- Vol. 537 (2) , 1056-1069
Open AccessStrange quark matter as dark matter: 40 yr later, a reappraisal
Forty years ago Witten suggested that dark matter could be composed of macroscopic clusters of strange quark matter. This idea was very popular for several years, but it dropped out of fashion once lattice quantum chromodynamics calculations indicated that the confinement/deconfinement transition, at small baryonic chemical potential, is not first order, which seemed to be a crucial requirement in order to produce large clusters of quarks. Here, we revisit the conditions under which strangelets can be produced in the Early Universe. We discuss the impact of an instability in the hadronic phase separating a low density, positive-strange-charge phase from a high-density phase with a negative strange charge. This second phase can rapidly stabilize by forming colour-superconducting gaps. The strangelets then undergo partial evaporation. In this way, we obtain distributions of their sizes in agreement with the observational constraints and we discuss the many astrophysical and cosmological implications of these objects. Finally, we examine the most promising techniques to detect this type of strangelets. We also show that strangelets can exist with masses $\lesssim $1017 g, while primordial black holes are ruled out in that mass range, allowing us to distinguish between these two dark matter candidates.