Pub Date : 2024-07-04DOI: 10.1016/j.newast.2024.102274
Syed Mudassir Syed Iqbal , G.U. Khapekar , S.H. Shekh , A. Dixit
we explored the holographic dark energy model using Hubble’s Horizon as the infrared (IR) cut-off in Locally Rotationally Symmetric (LRS) Bianchi type-I, considering the gravity framework in our analysis. In order to solve the field equations, we assume a relation and volumetric power law expansion (where is constant). we have expressed various crucial cosmological parameters in terms of the redshift and depicted them graphically to enhance our understanding of the expansion and evolution of the universe like holographic dark energy density (), holographic dark energy pressure (), equation of state parameter () , total energy density parameter () etc. Also, we analyzed the stability of the universe in our model through the squared speed of sound test and its validity by energy conditions. Ultimately, our model indicates that the universe is currently in an expanding phase, exhibiting an accelerating phase, closely approaching a flat geometry, and its behavior resembles that of a quintessence dark energy model.
我们探索了全息暗能量模型,将哈勃地平线(Hubble's Horizon)作为局部旋转对称(LRS)边奇 I 型的红外(IR)截止点,并在分析中考虑了引力框架。为了求解场方程,我们假设了一个关系和体积幂律膨胀(其中为常数)。我们用红移表示了各种关键的宇宙学参数,并用图形描述了它们,以加深我们对宇宙膨胀和演化的理解,如全息暗能量密度()、全息暗能量压力()、状态方程参数()、总能量密度参数()等。此外,我们还通过声速平方检验分析了我们模型中宇宙的稳定性及其在能量条件下的有效性。最终,我们的模型表明,宇宙目前正处于膨胀阶段,表现出加速阶段,接近于平面几何,其行为类似于五元暗能量模型。
{"title":"LRS Bianchi type-I with Hubble’s horizon as IR cut-off in f(R) gravity","authors":"Syed Mudassir Syed Iqbal , G.U. Khapekar , S.H. Shekh , A. Dixit","doi":"10.1016/j.newast.2024.102274","DOIUrl":"10.1016/j.newast.2024.102274","url":null,"abstract":"<div><p>we explored the holographic dark energy model using Hubble’s Horizon as the infrared (IR) cut-off in Locally Rotationally Symmetric (LRS) Bianchi type-I, considering the <span><math><mrow><mi>f</mi><mrow><mo>(</mo><mi>R</mi><mo>)</mo></mrow></mrow></math></span> gravity framework in our analysis. In order to solve the field equations, we assume a relation <span><math><mrow><mi>F</mi><mo>∝</mo><mspace></mspace><msup><mrow><mi>a</mi></mrow><mrow><mi>m</mi></mrow></msup></mrow></math></span> and volumetric power law expansion (where <span><math><mi>m</mi></math></span> is constant). we have expressed various crucial cosmological parameters in terms of the redshift <span><math><mi>z</mi></math></span> and depicted them graphically to enhance our understanding of the expansion and evolution of the universe like holographic dark energy density (<span><math><msub><mrow><mi>ρ</mi></mrow><mrow><mi>Λ</mi></mrow></msub></math></span>), holographic dark energy pressure (<span><math><msub><mrow><mi>p</mi></mrow><mrow><mi>Λ</mi></mrow></msub></math></span>), equation of state parameter (<span><math><mi>ω</mi></math></span>) , total energy density parameter (<span><math><mi>Ω</mi></math></span>) etc. Also, we analyzed the stability of the universe in our model through the squared speed of sound test and its validity by energy conditions. Ultimately, our model indicates that the universe is currently in an expanding phase, exhibiting an accelerating phase, closely approaching a flat geometry, and its behavior resembles that of a quintessence dark energy model.</p></div>","PeriodicalId":54727,"journal":{"name":"New Astronomy","volume":"113 ","pages":"Article 102274"},"PeriodicalIF":1.9,"publicationDate":"2024-07-04","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141587749","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-07-02DOI: 10.1016/j.newast.2024.102275
Eugene Oks
In attempts to resolve the neutron lifetime puzzle, there was suggested a hypothetical decay of neutrons into some unspecified dark matter (DM) particles. Later there were performed studies on how the hypothetical decay of neutrons would affect neutron stars. Recently it was shown that with the allowance for the second solution of Dirac equation for hydrogen atoms, the theoretical branching ratio (BR) for the two-body decay of neutrons (compared to their three-body decay) is amplified by a factor of 3300 from 0.000004. So, the BR becomes about 1.3% in the excellent agreement with the “experimental” BR = (1.15 ± 0.27)% required for reconciling the two distinct experimental values of the neutron lifetime: one from the beam experiments, another from the trap experiments. This meant that the two-body decay of neutrons in the beam experiments (that count only the protons) plays a much more sizable part in the overestimation of the lifetime of neutrons in these experiments than previously thought. Hydrogen atoms corresponding to the second solution of Dirac equations are called the second flavor of hydrogen atoms (SFHA) by the analogy with the flavors of quarks. The existence of the SFHA is evidenced by four different types of atomic/molecular experiments. The primary feature of the SFHA is that due to having only the s-states, they do not emit or absorb the electromagnetic radiation (except for the 21 cm line): they are practically dark. The SFHA became a candidate for a part of DM for the first time after the SFHA-based successful qualitative and quantitative explanation of the perplexing observation by Bowman et al. of the anomalous absorption in the redshifted 21 cm line from the early Universe. In the present paper we analyzed how this neutron decay into the SFHA affects neutron stars. We showed that old neutron stars could very slowly generate the new specific, described in detail baryonic DM in the form of the SFHA. Some old neutron stars would release it into their tiny atmospheres, while some other old neutron stars would release it into the interstellar medium. Besides, mergers of a neutron star with another neutron star or with a black hole, accompanied by the ejection of neutron-rich material, can also lead to the formation of SFHA as the ejecta cools down. This is another interesting aspect of the multi-messenger astronomy focused on studying these mergers through the gravitational waves they generate. These mechanisms of generating new baryonic DM in the universe should have the fundamental importance. We point out the indirect observational evidence of the continuing generation of new baryonic DM. We hope that our results will stimulate a further research in this direction.
{"title":"New results on the two-body decay of neutrons shed new light on neutron stars","authors":"Eugene Oks","doi":"10.1016/j.newast.2024.102275","DOIUrl":"10.1016/j.newast.2024.102275","url":null,"abstract":"<div><p>In attempts to resolve the neutron lifetime puzzle, there was suggested a hypothetical decay of neutrons into some <em>unspecified</em> dark matter (DM) particles. Later there were performed studies on how the hypothetical decay of neutrons would affect neutron stars. Recently it was shown that with the allowance for the second solution of Dirac equation for hydrogen atoms, the theoretical branching ratio (BR) for the two-body decay of neutrons (compared to their three-body decay) is amplified by a factor of 3300 from 0.000004. So, the BR becomes about 1.3% in the excellent agreement with the “experimental” BR = (1.15 ± 0.27)% required for reconciling the two distinct experimental values of the neutron lifetime: one from the beam experiments, another from the trap experiments. This meant that the two-body decay of neutrons in the beam experiments (that count only the protons) plays a much more sizable part in the overestimation of the lifetime of neutrons in these experiments than previously thought. Hydrogen atoms corresponding to the second solution of Dirac equations are called the second flavor of hydrogen atoms (SFHA) by the analogy with the flavors of quarks. The existence of the SFHA is evidenced by four different types of atomic/molecular experiments. The primary feature of the SFHA is that due to having only the s-states, they do not emit or absorb the electromagnetic radiation (except for the 21 cm line): they are practically <em>dark</em>. The SFHA became a candidate for a part of DM for the first time after the SFHA-based successful qualitative and quantitative explanation of the perplexing observation by Bowman et al. of the anomalous absorption in the redshifted 21 cm line from the early Universe. In the present paper we analyzed how this neutron decay into the SFHA affects neutron stars. We showed that old neutron stars could very slowly generate the new <em>specific, described in detail</em> baryonic DM in the form of the SFHA. Some old neutron stars would release it into their tiny atmospheres, while some other old neutron stars would release it into the interstellar medium. Besides, mergers of a neutron star with another neutron star or with a black hole, accompanied by the ejection of neutron-rich material, can also lead to the formation of SFHA as the ejecta cools down. This is another interesting aspect of the multi-messenger astronomy focused on studying these mergers through the gravitational waves they generate. These mechanisms of generating new baryonic DM in the universe should have the fundamental importance. We point out the indirect observational evidence of the continuing generation of new baryonic DM. We hope that our results will stimulate a further research in this direction.</p></div>","PeriodicalId":54727,"journal":{"name":"New Astronomy","volume":"113 ","pages":"Article 102275"},"PeriodicalIF":1.9,"publicationDate":"2024-07-02","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141587750","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-06-30DOI: 10.1016/j.newast.2024.102272
Absos Ali Shaikh , Faizuddin Ahmed , Mousumi Sarkar
<div><p>The objective of this article is to study topologically charged Eddington-inspired Born–Infeld (briefly, EiBI) gravity spacetime. It is proved that the topologically charged EiBI spacetime executes different types of pseudosymmetry, viz. Ricci generalized pseudosymmetry as <span><math><mrow><mi>R</mi><mi>⋅</mi><mi>R</mi><mo>=</mo><mi>Q</mi><mrow><mo>(</mo><mi>S</mi><mo>,</mo><mi>R</mi><mo>)</mo></mrow></mrow></math></span>, Ricci generalized projectively pseudosymmetry as <span><math><mrow><mi>P</mi><mi>⋅</mi><mi>R</mi><mo>=</mo><mfrac><mrow><mn>2</mn></mrow><mrow><mn>3</mn></mrow></mfrac><mi>Q</mi><mrow><mo>(</mo><mi>S</mi><mo>,</mo><mi>R</mi><mo>)</mo></mrow></mrow></math></span>, pseudosymmetry due to conformal curvature as <span><math><mrow><mi>C</mi><mi>⋅</mi><mi>C</mi><mo>=</mo><mo>−</mo><mfrac><mrow><mrow><mo>(</mo><msup><mrow><mi>r</mi></mrow><mrow><mn>2</mn></mrow></msup><msup><mrow><mi>α</mi></mrow><mrow><mn>2</mn></mrow></msup><mo>+</mo><mn>2</mn><mi>ϵ</mi><msup><mrow><mi>α</mi></mrow><mrow><mn>2</mn></mrow></msup><mo>−</mo><msup><mrow><mi>r</mi></mrow><mrow><mn>2</mn></mrow></msup><mo>)</mo></mrow></mrow><mrow><mn>6</mn><msup><mrow><mi>r</mi></mrow><mrow><mn>4</mn></mrow></msup></mrow></mfrac><mi>Q</mi><mrow><mo>(</mo><mi>g</mi><mo>,</mo><mi>C</mi><mo>)</mo></mrow></mrow></math></span> and pseudosymmetry due to conharmonic curvature as <span><math><mrow><mi>K</mi><mi>⋅</mi><mi>K</mi><mo>=</mo><mo>−</mo><mfrac><mrow><mrow><mo>(</mo><msup><mrow><mi>α</mi></mrow><mrow><mn>2</mn></mrow></msup><mo>−</mo><mn>1</mn><mo>)</mo></mrow></mrow><mrow><mn>2</mn><msup><mrow><mi>r</mi></mrow><mrow><mn>2</mn></mrow></msup></mrow></mfrac><mi>Q</mi><mrow><mo>(</mo><mi>g</mi><mo>,</mo><mi>K</mi><mo>)</mo></mrow></mrow></math></span>. Also, we have exhibited the linear dependence of <span><math><mrow><mi>Q</mi><mrow><mo>(</mo><mi>g</mi><mo>,</mo><mi>C</mi><mo>)</mo></mrow></mrow></math></span> and <span><math><mrow><mi>Q</mi><mrow><mo>(</mo><mi>S</mi><mo>,</mo><mi>C</mi><mo>)</mo></mrow></mrow></math></span> on the difference <span><math><mrow><mo>(</mo><mi>C</mi><mi>⋅</mi><mi>R</mi><mo>−</mo><mi>R</mi><mi>⋅</mi><mi>C</mi><mo>)</mo></mrow></math></span>. Moreover, it is exhibited that the topologically charged EiBI spacetime is an Einstein manifold of level 3, 2-quasi Einstein, conformal 2-forms are recurrent, Ricci 1-forms are recurrent and generalized Roter type. As a special case, we have acquired the geometric structures of point-like global monopole (briefly, PGM) spacetime and topologically charged Ellis Bronnikov Wormhole (briefly, TCEBW) spacetime. Also, we have explored that the topologically charged EiBI spacetime possesses almost <span><math><mi>η</mi></math></span>-Ricci-Yamabe soliton, almost <span><math><mi>η</mi></math></span>-Ricci soliton, and for a certain condition it admits almost Ricci soliton. Further, it is also verified that such a spacetime reveals generalized curvature inheritance and for a particular condition it admits
{"title":"Curvature related geometrical properties of topologically charged EiBI-gravity spacetime","authors":"Absos Ali Shaikh , Faizuddin Ahmed , Mousumi Sarkar","doi":"10.1016/j.newast.2024.102272","DOIUrl":"10.1016/j.newast.2024.102272","url":null,"abstract":"<div><p>The objective of this article is to study topologically charged Eddington-inspired Born–Infeld (briefly, EiBI) gravity spacetime. It is proved that the topologically charged EiBI spacetime executes different types of pseudosymmetry, viz. Ricci generalized pseudosymmetry as <span><math><mrow><mi>R</mi><mi>⋅</mi><mi>R</mi><mo>=</mo><mi>Q</mi><mrow><mo>(</mo><mi>S</mi><mo>,</mo><mi>R</mi><mo>)</mo></mrow></mrow></math></span>, Ricci generalized projectively pseudosymmetry as <span><math><mrow><mi>P</mi><mi>⋅</mi><mi>R</mi><mo>=</mo><mfrac><mrow><mn>2</mn></mrow><mrow><mn>3</mn></mrow></mfrac><mi>Q</mi><mrow><mo>(</mo><mi>S</mi><mo>,</mo><mi>R</mi><mo>)</mo></mrow></mrow></math></span>, pseudosymmetry due to conformal curvature as <span><math><mrow><mi>C</mi><mi>⋅</mi><mi>C</mi><mo>=</mo><mo>−</mo><mfrac><mrow><mrow><mo>(</mo><msup><mrow><mi>r</mi></mrow><mrow><mn>2</mn></mrow></msup><msup><mrow><mi>α</mi></mrow><mrow><mn>2</mn></mrow></msup><mo>+</mo><mn>2</mn><mi>ϵ</mi><msup><mrow><mi>α</mi></mrow><mrow><mn>2</mn></mrow></msup><mo>−</mo><msup><mrow><mi>r</mi></mrow><mrow><mn>2</mn></mrow></msup><mo>)</mo></mrow></mrow><mrow><mn>6</mn><msup><mrow><mi>r</mi></mrow><mrow><mn>4</mn></mrow></msup></mrow></mfrac><mi>Q</mi><mrow><mo>(</mo><mi>g</mi><mo>,</mo><mi>C</mi><mo>)</mo></mrow></mrow></math></span> and pseudosymmetry due to conharmonic curvature as <span><math><mrow><mi>K</mi><mi>⋅</mi><mi>K</mi><mo>=</mo><mo>−</mo><mfrac><mrow><mrow><mo>(</mo><msup><mrow><mi>α</mi></mrow><mrow><mn>2</mn></mrow></msup><mo>−</mo><mn>1</mn><mo>)</mo></mrow></mrow><mrow><mn>2</mn><msup><mrow><mi>r</mi></mrow><mrow><mn>2</mn></mrow></msup></mrow></mfrac><mi>Q</mi><mrow><mo>(</mo><mi>g</mi><mo>,</mo><mi>K</mi><mo>)</mo></mrow></mrow></math></span>. Also, we have exhibited the linear dependence of <span><math><mrow><mi>Q</mi><mrow><mo>(</mo><mi>g</mi><mo>,</mo><mi>C</mi><mo>)</mo></mrow></mrow></math></span> and <span><math><mrow><mi>Q</mi><mrow><mo>(</mo><mi>S</mi><mo>,</mo><mi>C</mi><mo>)</mo></mrow></mrow></math></span> on the difference <span><math><mrow><mo>(</mo><mi>C</mi><mi>⋅</mi><mi>R</mi><mo>−</mo><mi>R</mi><mi>⋅</mi><mi>C</mi><mo>)</mo></mrow></math></span>. Moreover, it is exhibited that the topologically charged EiBI spacetime is an Einstein manifold of level 3, 2-quasi Einstein, conformal 2-forms are recurrent, Ricci 1-forms are recurrent and generalized Roter type. As a special case, we have acquired the geometric structures of point-like global monopole (briefly, PGM) spacetime and topologically charged Ellis Bronnikov Wormhole (briefly, TCEBW) spacetime. Also, we have explored that the topologically charged EiBI spacetime possesses almost <span><math><mi>η</mi></math></span>-Ricci-Yamabe soliton, almost <span><math><mi>η</mi></math></span>-Ricci soliton, and for a certain condition it admits almost Ricci soliton. Further, it is also verified that such a spacetime reveals generalized curvature inheritance and for a particular condition it admits ","PeriodicalId":54727,"journal":{"name":"New Astronomy","volume":"112 ","pages":"Article 102272"},"PeriodicalIF":1.9,"publicationDate":"2024-06-30","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141587603","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-06-29DOI: 10.1016/j.newast.2024.102271
B. Gürol , A.-Y. Zhou
We present the discovery of Doradus-type pulsations in the eclipsing binary TIC 140736015. We obtained the physical and geometrical parameters of this detached eclipsing binary hosting a pulsating component. Based on the Transiting Exoplanet Survey Satellite (TESS) observation and Gaia DR3 data of TIC 140736015, we refined the light elements of the system using analysis and found that the eclipse times varied with a period of days, probably linked to the multiperiodic pulsational nature. We showed that essentially, only secondary eclipse is seen in the phased light curve. The frequency analysis using the out-of-eclipse data reveals that all the pulsational frequencies are located in the region lower than . After removing the pulsational variation from the observations we analysed the residual light curve together with the radial velocity data obtained from Gaia DR3 and find the masses and radii of the primary and secondary components as , and , , respectively. Regarding the location of the components on the Hertzsprung–Russell diagram both components can be a Dor/solar-like pulsator.
{"title":"Pulsational and eclipsing nature of TIC 140736015","authors":"B. Gürol , A.-Y. Zhou","doi":"10.1016/j.newast.2024.102271","DOIUrl":"10.1016/j.newast.2024.102271","url":null,"abstract":"<div><p>We present the discovery of <span><math><mi>γ</mi></math></span> Doradus-type pulsations in the eclipsing binary TIC 140736015. We obtained the physical and geometrical parameters of this detached eclipsing binary hosting a pulsating component. Based on the Transiting Exoplanet Survey Satellite (<em>TESS</em>) observation and Gaia DR3 data of TIC 140736015, we refined the light elements of the system using <span><math><mrow><mo>(</mo><mi>O</mi><mo>−</mo><mi>C</mi><mo>)</mo></mrow></math></span> analysis and found that the eclipse times varied with a period of <span><math><mrow><mo>∼</mo><mn>2048</mn></mrow></math></span> days, probably linked to the multiperiodic pulsational nature. We showed that essentially, only secondary eclipse is seen in the phased light curve. The frequency analysis using the out-of-eclipse data reveals that all the pulsational frequencies are located in the region lower than <span><math><mrow><mn>5</mn><mspace></mspace><msup><mrow><mi>d</mi></mrow><mrow><mo>−</mo><mn>1</mn></mrow></msup></mrow></math></span>. After removing the pulsational variation from the observations we analysed the residual light curve together with the radial velocity data obtained from Gaia DR3 and find the masses and radii of the primary and secondary components as <span><math><mrow><msub><mrow><mi>M</mi></mrow><mrow><mn>1</mn></mrow></msub><mo>=</mo><mn>1</mn><mo>.</mo><mn>429</mn><mo>±</mo><mn>0</mn><mo>.</mo><mn>022</mn></mrow></math></span> <span><math><msub><mrow><mi>M</mi></mrow><mrow><mo>⊙</mo></mrow></msub></math></span>, <span><math><mrow><msub><mrow><mi>M</mi></mrow><mrow><mn>2</mn></mrow></msub><mo>=</mo><mn>1</mn><mo>.</mo><mn>402</mn><mo>±</mo><mn>0</mn><mo>.</mo><mn>022</mn></mrow></math></span> <span><math><msub><mrow><mi>M</mi></mrow><mrow><mo>⊙</mo></mrow></msub></math></span>and <span><math><mrow><msub><mrow><mi>R</mi></mrow><mrow><mn>1</mn></mrow></msub><mo>=</mo><mn>1</mn><mo>.</mo><mn>685</mn><mo>±</mo><mn>0</mn><mo>.</mo><mn>001</mn></mrow></math></span> <span><math><msub><mrow><mi>R</mi></mrow><mrow><mo>⊙</mo></mrow></msub></math></span>, <span><math><mrow><msub><mrow><mi>R</mi></mrow><mrow><mn>2</mn></mrow></msub><mo>=</mo><mn>1</mn><mo>.</mo><mn>393</mn><mo>±</mo><mn>0</mn><mo>.</mo><mn>001</mn></mrow></math></span> <span><math><msub><mrow><mi>R</mi></mrow><mrow><mo>⊙</mo></mrow></msub></math></span>, respectively. Regarding the location of the components on the Hertzsprung–Russell diagram both components can be a <span><math><mi>γ</mi></math></span> Dor/solar-like pulsator.</p></div>","PeriodicalId":54727,"journal":{"name":"New Astronomy","volume":"113 ","pages":"Article 102271"},"PeriodicalIF":1.9,"publicationDate":"2024-06-29","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141587604","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-06-29DOI: 10.1016/j.newast.2024.102270
S. Adalalı , E. Soydugan
In this study, new CCD photometric observations and photometric analysis of BK Vul and V699 Cep systems, which are classified as contact binaries in the literature, are presented. For the V699 Cep, the TESS light curve was also used in the photometric analysis. We determined the basic astrophysical parameters of the BK Vul and V699 Cep systems from photometric analysis using the Wilson–Devinney method. Due to the lack of spectroscopic data for both systems in the literature, these absolute parameters were approximately calculated as to be = 0.73 , = 1.39 and = 1.09 for BK Vul, and = 0.36 , = 2.40 and = 1.33 for V699 Cep after estimating the mass of the primary component. The period decrease rate (dP/dt) and cyclic variation period of BK Vul were determined from the analysis as -3.86 day yr−1 and 27 yrs., respectively. The evolutionary status of components of both systems were discussed.
{"title":"First photometric study of W UMa-type binary systems: BK Vul and V699 Cep","authors":"S. Adalalı , E. Soydugan","doi":"10.1016/j.newast.2024.102270","DOIUrl":"https://doi.org/10.1016/j.newast.2024.102270","url":null,"abstract":"<div><p>In this study, new CCD photometric observations and photometric analysis of BK Vul and V699 Cep systems, which are classified as contact binaries in the literature, are presented. For the V699 Cep, the <em>TESS</em> light curve was also used in the photometric analysis. We determined the basic astrophysical parameters of the BK Vul and V699 Cep systems from photometric analysis using the Wilson–Devinney method. Due to the lack of spectroscopic data for both systems in the literature, these absolute parameters were approximately calculated as to be <span><math><msub><mrow><mi>M</mi></mrow><mrow><mn>2</mn></mrow></msub></math></span> = 0.73 <span><math><msub><mrow><mi>M</mi></mrow><mrow><mo>⊙</mo></mrow></msub></math></span>, <span><math><msub><mrow><mi>R</mi></mrow><mrow><mn>1</mn></mrow></msub></math></span> = 1.39 <span><math><msub><mrow><mi>R</mi></mrow><mrow><mo>⊙</mo></mrow></msub></math></span> and <span><math><msub><mrow><mi>R</mi></mrow><mrow><mn>2</mn></mrow></msub></math></span> = 1.09 <span><math><msub><mrow><mi>R</mi></mrow><mrow><mo>⊙</mo></mrow></msub></math></span> for BK Vul, and <span><math><msub><mrow><mi>M</mi></mrow><mrow><mn>2</mn></mrow></msub></math></span> = 0.36 <span><math><msub><mrow><mi>M</mi></mrow><mrow><mo>⊙</mo></mrow></msub></math></span>, <span><math><msub><mrow><mi>R</mi></mrow><mrow><mn>1</mn></mrow></msub></math></span> = 2.40 <span><math><msub><mrow><mi>R</mi></mrow><mrow><mo>⊙</mo></mrow></msub></math></span> and <span><math><msub><mrow><mi>R</mi></mrow><mrow><mn>2</mn></mrow></msub></math></span> = 1.33 <span><math><msub><mrow><mi>R</mi></mrow><mrow><mo>⊙</mo></mrow></msub></math></span> for V699 Cep after estimating the mass of the primary component. The period decrease rate (<em>dP/dt</em>) and cyclic variation period of BK Vul were determined from the <span><math><mrow><mi>O</mi><mo>−</mo><mi>C</mi></mrow></math></span> analysis as -3.86 <span><math><mrow><mo>×</mo><mn>1</mn><msup><mrow><mn>0</mn></mrow><mrow><mo>−</mo><mn>7</mn></mrow></msup></mrow></math></span> day yr<sup>−1</sup> and 27 yrs., respectively. The evolutionary status of components of both systems were discussed.</p></div>","PeriodicalId":54727,"journal":{"name":"New Astronomy","volume":"112 ","pages":"Article 102270"},"PeriodicalIF":1.9,"publicationDate":"2024-06-29","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141541503","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-06-25DOI: 10.1016/j.newast.2024.102262
Angel Castro , Raúl Michel , Noel Castro Segura , Diego Altamirano , Carlos Tejada , Joel Herrera , Enrique Colorado , Gerardo Sierra , Liliana Altamirano-Dévora , Juan Echevarría , Rasjied Sloot , Rudy Wijnands , Iván Zavala , David Rojas , Juan V. Hernández Santisteban , Federico Vincentelli , Javier A. Hernández-Landa , Song Wang , Melissa Fuentes , Poshak Gandhi , Francisco Valenzuela
OPTICAM is a triple-band optical system developed for the 2.1 m telescope of the National Astronomical Observatory in the Sierra de San Pedro Mártir (OAN-SPM). Partial engineering tests were conducted in 2019, with the complete system experiencing its first light in March 2022. The system incorporates two beam splitters, enabling simultaneous observations on three channels. Users can choose three out of the five available filters from the SDSS filter set (), covering the wavelength range from 320 to 1000 nm. It offers an effective field of view of approximately 4.7, 4.7, and 5.6 arcminutes in each of its arms, respectively. Due to its design and capabilities, OPTICAM is suitable for coordinated observations with other ground-based and space-based observatories. This document presents the final instrument design and the current system status. Some of the optical tests carried out are described. We also present the results of scientific observations conducted during its first light and first year of operations.
{"title":"First light simultaneous triple-channel optical observations of the OPTICAM system at the OAN-SPM","authors":"Angel Castro , Raúl Michel , Noel Castro Segura , Diego Altamirano , Carlos Tejada , Joel Herrera , Enrique Colorado , Gerardo Sierra , Liliana Altamirano-Dévora , Juan Echevarría , Rasjied Sloot , Rudy Wijnands , Iván Zavala , David Rojas , Juan V. Hernández Santisteban , Federico Vincentelli , Javier A. Hernández-Landa , Song Wang , Melissa Fuentes , Poshak Gandhi , Francisco Valenzuela","doi":"10.1016/j.newast.2024.102262","DOIUrl":"10.1016/j.newast.2024.102262","url":null,"abstract":"<div><p>OPTICAM is a triple-band optical system developed for the 2.1 m telescope of the National Astronomical Observatory in the Sierra de San Pedro Mártir (OAN-SPM). Partial engineering tests were conducted in 2019, with the complete system experiencing its first light in March 2022. The system incorporates two beam splitters, enabling simultaneous observations on three channels. Users can choose three out of the five available filters from the SDSS filter set (<span><math><mrow><msup><mrow><mi>u</mi></mrow><mrow><mo>′</mo></mrow></msup><msup><mrow><mi>g</mi></mrow><mrow><mo>′</mo></mrow></msup><msup><mrow><mi>r</mi></mrow><mrow><mo>′</mo></mrow></msup><msup><mrow><mi>i</mi></mrow><mrow><mo>′</mo></mrow></msup><msup><mrow><mi>z</mi></mrow><mrow><mo>′</mo></mrow></msup></mrow></math></span>), covering the wavelength range from 320 to 1000 nm. It offers an effective field of view of approximately 4.7, 4.7, and 5.6 arcminutes in each of its arms, respectively. Due to its design and capabilities, OPTICAM is suitable for coordinated observations with other ground-based and space-based observatories. This document presents the final instrument design and the current system status. Some of the optical tests carried out are described. We also present the results of scientific observations conducted during its first light and first year of operations.</p></div>","PeriodicalId":54727,"journal":{"name":"New Astronomy","volume":"112 ","pages":"Article 102262"},"PeriodicalIF":1.9,"publicationDate":"2024-06-25","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141587605","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-06-08DOI: 10.1016/j.newast.2024.102263
Marco Immanuel B. Rivera , Reinabelle C. Reyes
The future space-borne Laser Interferometer Space Antenna (LISA) is expected to detect gravitational waves (GW) from Extreme Mass Ratio Inspiral (EMRI) binaries which may live in nontrivial environments such as accretion disks. In this work, we apply the Fisher matrix Principal Component Analysis (PCA) method to assess how well LISA observations can jointly constrain the source parameters and environmental densities around EMRIs. Specifically, we calculate the Fisher matrix from the post-Newtonian parameters of an EMRI binary embedded in a fluid with a constant density profile. We determine that the most dominant measurable parameter combination is dominated by contributions from environmental effects, namely, gravitational drag, accretion, and gravitational pull (in order of contribution). The proposed reparameterization of the PN parameters can be used to improve the power and efficiency of future detection and parameter estimation methods.
未来的星载激光干涉仪空间天线(LISA)有望探测到来自极端质量比激发(EMRI)双星的引力波(GW),这些双星可能生活在吸积盘等非简单环境中。在这项工作中,我们应用费舍尔矩阵主成分分析(PCA)方法来评估 LISA 观测能在多大程度上共同约束 EMRI 周围的源参数和环境密度。具体来说,我们根据嵌入恒定密度曲线流体中的 EMRI 双星的后牛顿参数计算费雪矩阵。我们确定,最主要的可测量参数组合是由环境效应贡献的,即引力拖拽、吸积和引力(按贡献大小排序)。提议的 PN 参数重新参数化可以用来提高未来探测和参数估计方法的功率和效率。
{"title":"Measurable parameter combinations of environmentally-dephased EMRI gravitational-wave signals","authors":"Marco Immanuel B. Rivera , Reinabelle C. Reyes","doi":"10.1016/j.newast.2024.102263","DOIUrl":"10.1016/j.newast.2024.102263","url":null,"abstract":"<div><p>The future space-borne Laser Interferometer Space Antenna (LISA) is expected to detect gravitational waves (GW) from Extreme Mass Ratio Inspiral (EMRI) binaries which may live in nontrivial environments such as accretion disks. In this work, we apply the Fisher matrix Principal Component Analysis (PCA) method to assess how well LISA observations can jointly constrain the source parameters and environmental densities around EMRIs. Specifically, we calculate the Fisher matrix from the post-Newtonian parameters of an EMRI binary embedded in a fluid with a constant density profile. We determine that the most dominant measurable parameter combination is dominated by contributions from environmental effects, namely, gravitational drag, accretion, and gravitational pull (in order of contribution). The proposed reparameterization of the PN parameters can be used to improve the power and efficiency of future detection and parameter estimation methods.</p></div>","PeriodicalId":54727,"journal":{"name":"New Astronomy","volume":"112 ","pages":"Article 102263"},"PeriodicalIF":2.0,"publicationDate":"2024-06-08","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141393619","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-06-04DOI: 10.1016/j.newast.2024.102261
R. Torres , T. Grismayer , F. Cruz , R.A. Fonseca , L.O. Silva
We present ab initio global general-relativistic Particle-in-cell (GR-PIC) simulations of compact millisecond neutron star magnetospheres in the axisymmetric aligned rotator configuration. We investigate the role of GR and plasma supply on the polar cap particle acceleration efficiency – the precursor of coherent radio emission – employing a new module for the PIC code OSIRIS, designed to model plasma dynamics around compact objects with fully self-consistent GR effects. We provide a detailed description of the main sub-algorithms of the novel PIC algorithm, including a charge-conserving current deposit scheme for curvilinear coordinates. We demonstrate efficient particle acceleration in the polar caps of compact neutron stars with denser magnetospheres, numerically validating the spacelike current extension provided by force-free models. We show that GR relaxes the minimum required poloidal magnetospheric current for the transition of the polar cap to the accelerator regime, thus justifying the observation of weak pulsars beyond the expected death line. We denote that spin-down luminosity intermittency and radio pulse nullings for older pulsars might arise from the interplay between the polar and outer gaps. Also, narrower radio beams are expected for weaker low-obliquity pulsars.
我们介绍了对轴对称对齐转子构型的紧凑型毫秒中子星磁层进行的全局广义相对论粒子入胞(GR-PIC)模拟。我们利用 PIC 代码 OSIRIS 的一个新模块研究了 GR 和等离子体供应对极盖粒子加速效率(相干射电发射的前兆)的作用,该模块旨在利用完全自洽的 GR 效应模拟紧凑天体周围的等离子体动力学。我们详细介绍了新型 PIC 算法的主要子算法,包括曲线坐标的电荷守恒电流沉积方案。我们证明了粒子在具有较密集磁层的紧凑中子星极盖中的高效加速,从数值上验证了无力模型所提供的类似于空间的电流扩展。我们表明,GR 放松了极盖过渡到加速器机制所需的最小极磁层电流,从而证明了在预期死亡线之外观测到弱脉冲星是合理的。我们指出,较老脉冲星的自旋下降光度间歇和射电脉冲无效可能是由于极隙和外隙之间的相互作用造成的。另外,较弱的低倾脉冲星的射电波束预计会更窄。
{"title":"OSIRIS-GR: General relativistic activation of the polar cap of a compact neutron star","authors":"R. Torres , T. Grismayer , F. Cruz , R.A. Fonseca , L.O. Silva","doi":"10.1016/j.newast.2024.102261","DOIUrl":"https://doi.org/10.1016/j.newast.2024.102261","url":null,"abstract":"<div><p>We present ab initio global general-relativistic Particle-in-cell (GR-PIC) simulations of compact millisecond neutron star magnetospheres in the axisymmetric aligned rotator configuration. We investigate the role of GR and plasma supply on the polar cap particle acceleration efficiency – the precursor of coherent radio emission – employing a new module for the PIC code OSIRIS, designed to model plasma dynamics around compact objects with fully self-consistent GR effects. We provide a detailed description of the main sub-algorithms of the novel PIC algorithm, including a charge-conserving current deposit scheme for curvilinear coordinates. We demonstrate efficient particle acceleration in the polar caps of compact neutron stars with denser magnetospheres, numerically validating the spacelike current extension provided by force-free models. We show that GR relaxes the minimum required poloidal magnetospheric current for the transition of the polar cap to the accelerator regime, thus justifying the observation of weak pulsars beyond the expected death line. We denote that spin-down luminosity intermittency and radio pulse nullings for older pulsars might arise from the interplay between the polar and outer gaps. Also, narrower radio beams are expected for weaker low-obliquity pulsars.</p></div>","PeriodicalId":54727,"journal":{"name":"New Astronomy","volume":"112 ","pages":"Article 102261"},"PeriodicalIF":2.0,"publicationDate":"2024-06-04","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S1384107624000757/pdfft?md5=4b7e74c6e0596423df64b16f4a75d011&pid=1-s2.0-S1384107624000757-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141291525","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-06-03DOI: 10.1016/j.newast.2024.102258
W.H. Elsanhoury
<div><p>Here, we report the kinematical parameters of inner-halo hot subdwarfs located within <span><math><mrow><mo>(</mo><mrow><mi>d</mi><mo>≤</mo><mn>15</mn><mrow><mspace></mspace><mtext>kpc</mtext></mrow></mrow><mo>)</mo></mrow></math></span> at high Galactic latitudes <span><math><mrow><mo>(</mo><mrow><msup><mrow><mi>b</mi></mrow><mi>o</mi></msup><mo>≥</mo><mn>20</mn></mrow><mo>)</mo></mrow></math></span>. The study included three program stars for one of the extreme He-rich groups (<em>e</em>He-1) with eccentricity (<em>e</em>= 0.65) and the z-component of the angular momentum (J<sub>z</sub> = 4288.66 kpc km <em>s</em><sup>−1</sup>), the inner halo program I with 121 points <span><math><mrow><mo>(</mo><mrow><msub><mi>T</mi><mtext>eff</mtext></msub><mo>≥</mo><mn>24</mn><mo>,</mo><mn>000</mn></mrow><mo>)</mo></mrow></math></span> and their subsections, i.e. inner halo program II (sdB; 79 points) with <span><math><mrow><mo>(</mo><mrow><mn>40</mn><mo>,</mo><mn>000</mn><mo>≥</mo><msub><mi>T</mi><mtext>eff</mtext></msub><mo>≥</mo><mn>24</mn><mo>,</mo><mn>000</mn></mrow><mo>)</mo></mrow></math></span> and inner halo program III (sdO; 42 points) with <span><math><mrow><mo>(</mo><mrow><mn>80</mn><mo>,</mo><mn>000</mn><mo>≥</mo><msub><mi>T</mi><mtext>eff</mtext></msub><mo>≥</mo><mn>40</mn><mo>,</mo><mn>000</mn></mrow><mo>)</mo></mrow></math></span>. First, we calculated the spatial velocities (<span><math><mrow><mover><mi>U</mi><mo>¯</mo></mover><mo>,</mo><mrow><mspace></mspace><mover><mi>V</mi><mo>¯</mo></mover></mrow><mo>,</mo><mrow><mspace></mspace><mover><mi>W</mi><mo>¯</mo></mover></mrow><mo>;</mo><mrow><mspace></mspace><mtext>km</mtext><mspace></mspace></mrow><msup><mrow><mi>s</mi></mrow><mrow><mo>−</mo><mn>1</mn></mrow></msup><mrow><mo>)</mo></mrow></mrow></math></span> along the Galactic coordinates (i.e., 25.73 ± ± 5.07, 28.79 ± 5.37, −14.51 ± 3.81) and their dispersion velocities <span><math><mrow><mo>(</mo><mrow><msub><mi>σ</mi><mn>1</mn></msub><mo>,</mo><mspace></mspace><msub><mi>σ</mi><mn>2</mn></msub><mo>,</mo><mspace></mspace><msub><mi>σ</mi><mn>3</mn></msub><mo>;</mo><mrow><mspace></mspace><mtext>km</mtext><mspace></mspace></mrow><msup><mrow><mi>s</mi></mrow><mrow><mo>−</mo><mn>1</mn></mrow></msup></mrow><mo>)</mo></mrow></math></span> = (161.94 ± 12.73, 140.31 ± 11.85, 101.57 ± 10.08) and subsequently their subsections sdB and sdO. Second, we calculated the vertex longitudes <span><math><mrow><mo>(</mo><msub><mi>l</mi><mn>2</mn></msub><mo>)</mo></mrow></math></span> and the Solar motion <span><math><mrow><mo>(</mo><mrow><msub><mi>S</mi><mo>⊙</mo></msub><mo>=</mo><mn>41.24</mn><mrow><mspace></mspace><mspace></mspace></mrow><mn>6.42</mn><mrow><mspace></mspace><mtext>km</mtext><mspace></mspace></mrow><msup><mrow><mi>s</mi></mrow><mrow><mo>−</mo><mn>1</mn></mrow></msup></mrow><mo>)</mo></mrow></math></span> as well as their subsections. Finally, based on the kinematic relation of the ratio <span><math><mrow><mo>(</mo><mrow><msub><mi>σ</mi
{"title":"Kinematical and ellipsoidal properties of the inner-halo hot subdwarfs observed in Gaia DR3 and LAMOST DR7","authors":"W.H. Elsanhoury","doi":"10.1016/j.newast.2024.102258","DOIUrl":"https://doi.org/10.1016/j.newast.2024.102258","url":null,"abstract":"<div><p>Here, we report the kinematical parameters of inner-halo hot subdwarfs located within <span><math><mrow><mo>(</mo><mrow><mi>d</mi><mo>≤</mo><mn>15</mn><mrow><mspace></mspace><mtext>kpc</mtext></mrow></mrow><mo>)</mo></mrow></math></span> at high Galactic latitudes <span><math><mrow><mo>(</mo><mrow><msup><mrow><mi>b</mi></mrow><mi>o</mi></msup><mo>≥</mo><mn>20</mn></mrow><mo>)</mo></mrow></math></span>. The study included three program stars for one of the extreme He-rich groups (<em>e</em>He-1) with eccentricity (<em>e</em>= 0.65) and the z-component of the angular momentum (J<sub>z</sub> = 4288.66 kpc km <em>s</em><sup>−1</sup>), the inner halo program I with 121 points <span><math><mrow><mo>(</mo><mrow><msub><mi>T</mi><mtext>eff</mtext></msub><mo>≥</mo><mn>24</mn><mo>,</mo><mn>000</mn></mrow><mo>)</mo></mrow></math></span> and their subsections, i.e. inner halo program II (sdB; 79 points) with <span><math><mrow><mo>(</mo><mrow><mn>40</mn><mo>,</mo><mn>000</mn><mo>≥</mo><msub><mi>T</mi><mtext>eff</mtext></msub><mo>≥</mo><mn>24</mn><mo>,</mo><mn>000</mn></mrow><mo>)</mo></mrow></math></span> and inner halo program III (sdO; 42 points) with <span><math><mrow><mo>(</mo><mrow><mn>80</mn><mo>,</mo><mn>000</mn><mo>≥</mo><msub><mi>T</mi><mtext>eff</mtext></msub><mo>≥</mo><mn>40</mn><mo>,</mo><mn>000</mn></mrow><mo>)</mo></mrow></math></span>. First, we calculated the spatial velocities (<span><math><mrow><mover><mi>U</mi><mo>¯</mo></mover><mo>,</mo><mrow><mspace></mspace><mover><mi>V</mi><mo>¯</mo></mover></mrow><mo>,</mo><mrow><mspace></mspace><mover><mi>W</mi><mo>¯</mo></mover></mrow><mo>;</mo><mrow><mspace></mspace><mtext>km</mtext><mspace></mspace></mrow><msup><mrow><mi>s</mi></mrow><mrow><mo>−</mo><mn>1</mn></mrow></msup><mrow><mo>)</mo></mrow></mrow></math></span> along the Galactic coordinates (i.e., 25.73 ± ± 5.07, 28.79 ± 5.37, −14.51 ± 3.81) and their dispersion velocities <span><math><mrow><mo>(</mo><mrow><msub><mi>σ</mi><mn>1</mn></msub><mo>,</mo><mspace></mspace><msub><mi>σ</mi><mn>2</mn></msub><mo>,</mo><mspace></mspace><msub><mi>σ</mi><mn>3</mn></msub><mo>;</mo><mrow><mspace></mspace><mtext>km</mtext><mspace></mspace></mrow><msup><mrow><mi>s</mi></mrow><mrow><mo>−</mo><mn>1</mn></mrow></msup></mrow><mo>)</mo></mrow></math></span> = (161.94 ± 12.73, 140.31 ± 11.85, 101.57 ± 10.08) and subsequently their subsections sdB and sdO. Second, we calculated the vertex longitudes <span><math><mrow><mo>(</mo><msub><mi>l</mi><mn>2</mn></msub><mo>)</mo></mrow></math></span> and the Solar motion <span><math><mrow><mo>(</mo><mrow><msub><mi>S</mi><mo>⊙</mo></msub><mo>=</mo><mn>41.24</mn><mrow><mspace></mspace><mspace></mspace></mrow><mn>6.42</mn><mrow><mspace></mspace><mtext>km</mtext><mspace></mspace></mrow><msup><mrow><mi>s</mi></mrow><mrow><mo>−</mo><mn>1</mn></mrow></msup></mrow><mo>)</mo></mrow></math></span> as well as their subsections. Finally, based on the kinematic relation of the ratio <span><math><mrow><mo>(</mo><mrow><msub><mi>σ</mi","PeriodicalId":54727,"journal":{"name":"New Astronomy","volume":"112 ","pages":"Article 102258"},"PeriodicalIF":2.0,"publicationDate":"2024-06-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141291524","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-06-01DOI: 10.1016/j.newast.2024.102259
Gopal Sardar, Subenoy Chakraborty
In the present work we consider three modified Chevallier–Polarski–Linder (CPL) models with considering non-cold dark matter in the background of homogeneous and isotropic FLRW space–time model. From the observational data set ((Pantheon+)+BAO+HST) we find that all the parameters involved in the models having equation of dark energy state (Model II) and (Model III) do not depend on . We also find that for all the models equation of state for dark matter is almost same and observe that Model I is more preferable than the other two proposed models.
{"title":"Observational constraints on modified CPL models considering non-cold dark matter","authors":"Gopal Sardar, Subenoy Chakraborty","doi":"10.1016/j.newast.2024.102259","DOIUrl":"10.1016/j.newast.2024.102259","url":null,"abstract":"<div><p>In the present work we consider three modified Chevallier–Polarski–Linder (CPL) models with considering non-cold dark matter in the background of homogeneous and isotropic FLRW space–time model. From the observational data set ((Pantheon+)+BAO+HST) we find that all the parameters involved in the models having equation of dark energy state <span><math><mrow><msub><mrow><mi>ω</mi></mrow><mrow><mi>d</mi><mi>e</mi></mrow></msub><mo>=</mo><msub><mrow><mi>ω</mi></mrow><mrow><mn>0</mn></mrow></msub><mo>+</mo><msub><mrow><mi>ω</mi></mrow><mrow><mn>1</mn></mrow></msub><mfrac><mrow><mi>a</mi></mrow><mrow><msup><mrow><mrow><mo>(</mo><mn>1</mn><mo>+</mo><mi>a</mi><mo>)</mo></mrow></mrow><mrow><mi>p</mi></mrow></msup></mrow></mfrac></mrow></math></span> (Model II) and <span><math><mrow><msub><mrow><mi>ω</mi></mrow><mrow><mi>d</mi><mi>e</mi></mrow></msub><mo>=</mo><msub><mrow><mi>ω</mi></mrow><mrow><mn>0</mn></mrow></msub><mo>+</mo><msub><mrow><mi>ω</mi></mrow><mrow><mn>1</mn></mrow></msub><mfrac><mrow><mn>1</mn><mo>−</mo><mi>a</mi></mrow><mrow><msup><mrow><mrow><mo>(</mo><mn>1</mn><mo>+</mo><mi>a</mi><mo>)</mo></mrow></mrow><mrow><mi>p</mi></mrow></msup></mrow></mfrac></mrow></math></span> (Model III) do not depend on <span><math><mi>p</mi></math></span>. We also find that for all the models equation of state for dark matter is almost same and observe that Model I is more preferable than the other two proposed models.</p></div>","PeriodicalId":54727,"journal":{"name":"New Astronomy","volume":"112 ","pages":"Article 102259"},"PeriodicalIF":2.0,"publicationDate":"2024-06-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141277508","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}