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BEGIN:VEVENT
SUMMARY:Unified equation of state probing compact stars
DTSTART:20250312T170000Z
DTEND:20250312T190000Z
DTSTAMP:20260916T130801Z
UID:5d323077-edf5-4e8b-bf12-43c692dcf136
SEQUENCE:2
CREATED:20250310T120726Z
DESCRIPTION:Meeting ID: 971 1964 8836Passcode Zoom (se necessária): 13463
 1The equation of state (EoS) of neutron stars plays a crucial role in dete
 rmining their internal composition and observable properties. In this stud
 y\, we construct an EoS\, incorporating a 1st order phase transition from 
 hadronic to quark matter using a Maxwell construction\, and apply it for m
 odelling both static and rotating neutron stars. In the quark matter phase
 \, we consider the effects of vector repulsion and color superconductivity
 \, which significantly alter the stiffness of the EoS and the onset of the
  deconfinement phase transition\, respectively.Our results in the static c
 ase provide very good agreement with the astrophysical constraints extract
 ed from the gravitational wave (GW) signal GW170817 and even the subsolar-
 mass compact object HESS J1731-347. For non-vanishing rotational velocitie
 s\, we compare our outcomes with a collection of measurements of the most 
 recent millisecond pulsar (MSP) measurements and again find consistency wi
 th the observational data. Additionally\, we developed a model of accretio
 n matter onto rotating hybrid stars with finite magnetic. The model predic
 ts a set of measurable parameters that can be verified by future data.Furt
 hermore\, we apply an alternative approach for unified treatment of quark-
 hadron matter\, i.e. the framework of quarkyonic matter. We for the first 
 time introduce the effects of color superconductivity in the quark gluon p
 lasma to the framework of quarkyonic matter. In upcoming publications\, we
  will examine the impact of colour superconductivity in quarkyonic matter 
 and compare it to the Maxwell construction of the 1st order phase transiti
 on.
LAST-MODIFIED:20250310T120738Z
LOCATION:Sala de Formação Avançada do DF (2-8.11) + Zoom (Formato Híbr
 ido)
URL:http://df.vps.tecnico.ulisboa.pt/pt/eventos/unified-equation-of-state-
 probing-compact-stars/
X-ALT-DESC;FMTTYPE=text/html:<p data-block-key="6ax9g">Meeting ID: 971 196
 4 8836<br/>Passcode Zoom (se necessária): 134631</p><p data-block-key="rn
 7">The equation of state (EoS) of neutron stars plays a crucial role in de
 termining their internal composition and observable properties. In this st
 udy\, we construct an EoS\, incorporating a 1st order phase transition fro
 m hadronic to quark matter using a Maxwell construction\, and apply it for
  modelling both static and rotating neutron stars. In the quark matter pha
 se\, we consider the effects of vector repulsion and color superconductivi
 ty\, which significantly alter the stiffness of the EoS and the onset of t
 he deconfinement phase transition\, respectively.<br/></p><p data-block-ke
 y="em4uh">Our results in the static case provide very good agreement with 
 the astrophysical constraints extracted from the gravitational wave (GW) s
 ignal GW170817 and even the subsolar-mass compact object HESS J1731-347. F
 or non-vanishing rotational velocities\, we compare our outcomes with a co
 llection of measurements of the most recent millisecond pulsar (MSP) measu
 rements and again find consistency with the observational data. Additional
 ly\, we developed a model of accretion matter onto rotating hybrid stars w
 ith finite magnetic. The model predicts a set of measurable parameters tha
 t can be verified by future data.<br/></p><p data-block-key="cto6f">Furthe
 rmore\, we apply an alternative approach for unified treatment of quark-ha
 dron matter\, i.e. the framework of quarkyonic matter. We for the first ti
 me introduce the effects of color superconductivity in the quark gluon pla
 sma to the framework of quarkyonic matter. In upcoming publications\, we w
 ill examine the impact of colour superconductivity in quarkyonic matter an
 d compare it to the Maxwell construction of the 1st order phase transition
 .</p><p data-block-key="69t7o"></p>
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