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An Intermediate Luminosity GRB 210210A: The early onset of the external forward shock in the X-ray? 中等亮度 GRB 210210A:X射线中外部前向冲击的早期开始?
Pub Date : 2024-09-07 DOI: arxiv-2409.04871
Rahul Gupta, A. K. Ror, S. B. Pandey, J. Racusin, M. Moss, A. Aryan, N. Klingler, A. J. Castro-Tirado
We have analyzed the prompt and afterglow characteristics of the intermediateluminosity burst ``GRB 210210A". Our prompt emission analysis indicates thatGRB 210210A is among the softest long GRBs detected by the Swift-BAT. Thetime-integrated prompt emission spectrum of GRB 210210A is aptly described by apower law function with an exponential cutoff. The spectral peak energy(E$_{p,z}$) in rest-frame and the E$_{rm gamma, iso}$ for this GRB marginallysatisfy the 2$sigma$ Amati correlation, a common feature observed inlow/intermediate luminosity GRBs. Notably, an early bump is observed in theSwift-XRT light curve (a rare feature); the optical afterglow light curve, onthe other hand, appears to follow a power law decay. However, due to the lackof sufficient early optical observations, we cannot completely rule out thepossibility of an early bump in the optical light curve. For the bump observedin the early X-ray light curve, we calculated parameters such as peak time,rise time, decay time, and bulk Lorentz factor ($Gamma_{0}$ $sim$ 156), whichperfectly satisfy the correlation between the parameters of the onset of theafterglow in GRBs. Both the optical and X-ray (including our observations)light curves exhibit a chromatic break in the late afterglow. Based on theprompt and afterglow parameters, we confirm that the intermediate luminosityGRB 210210A favors a collapsar scenario and is possibly powered by a magnetar.
我们分析了中等亮度爆发 "GRB 210210A "的瞬发和余辉特征。我们的瞬时发射分析表明,GRB 210210A是斯威夫特-BAT探测到的最软的长GRB之一。GRB 210210A的时间积分瞬时发射光谱可以用指数截止的幂律函数来恰当地描述。该GRB的静帧光谱峰值能量(E$_{p,z}$)和E$_{rm gamma, iso}$略微满足2$sigma$ Amati相关性,这是在低/中等光度GRB中观测到的常见特征。值得注意的是,在Swift-XRT光曲线中观测到了一个早期凸起(一个罕见的特征);另一方面,光学余辉光曲线似乎遵循了一个幂律衰减。然而,由于缺乏足够的早期光学观测数据,我们无法完全排除光学光曲线中出现早期凸起的可能性。对于在早期X射线光曲线中观测到的凸起,我们计算了峰值时间、上升时间、衰减时间和体洛伦兹因子($Gamma_{0}$ $sim$ 156)等参数,这些参数完全符合GRB余辉开始的参数之间的相关性。光学和X射线(包括我们的观测)光曲线在晚期余辉中都表现出色度断裂。根据起始参数和余辉参数,我们确认中等光度的GRB 210210A倾向于坍缩星方案,并且可能是由磁星驱动的。
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引用次数: 0
A precessing stellar disk model for superorbital modulations of the gamma-ray binary LS I+61$^{circ}$ 303 伽马射线双星LS I+61$^{circ}$ 303的超轨道调制的前冲恒星盘模型
Pub Date : 2024-09-07 DOI: arxiv-2409.04818
A. M. Chen, J. Takata, Y. W. Yu
Gamma-ray binary LS I+61$^{circ}$ 303 consists of a neutron star orbitingaround a Be star with a period of $P_{rm orb}simeq26.5 {rm d}$. Apart fromorbital modulations, the binary shows long-term flux variations with asuperorbital period of $P_{rm sup}simeq4.6 {rm yrs}$ as seen in nearly allwavelengths. The origin of this superorbital modulation is still not wellunderstood. Under the pulsar wind-stellar outflow interaction scenario, wepropose that the superorbital modulations of LS I+61$^{circ}$ 303 could becaused by the precession of the Be disk. Assuming X-rays arise from synchrotronradiation of the intrabinary shock, we develop an analytical model to calculateexpected flux modulations over the orbital and superorbital phases. Theasymmetric two-peak profiles in orbital light curves and sinusoidal-likelong-term modulations are reproduced under the precessing disk scenario. Theobserved orbital phase drifting of the X-ray peak and our fitting of long-termX-ray data indicate that the neutron star is likely orbiting around the starwith a small eccentricity and periastron phase around $Phi_{rm p}sim0.6$. Wecompare the Corbet diagrams of LS I+61$^{circ}$ 303 with other Be/X-raybinaries and the linear correlation in the $P_{rm sup}-P_{rm orb}$ diagramsuggests that the precession of the Be disk in LS I+61$^{circ}$ 303 is inducedby the tidal torque of its neutron star companion.
伽马射线双星LS I+61$^{circ}$ 303由一颗围绕Be星运行的中子星组成,其周期为$P_{rm orb}simeq26.5 {rm d}$。除了轨道调制之外,该双星还显示出长期的通量变化,其上轨道周期为$P_{/rm sup}simeq4.6 {rm yrs}$,几乎在所有波长上都能看到。这种超轨道调制的起源还没有得到很好的理解。在脉冲星风-恒星外流相互作用的假设下,我们推测LS I+61$^{circ}$ 303的超轨道调制可能是由Be盘的前向运动引起的。假设X射线来自于双内冲击的同步辐射,我们建立了一个分析模型来计算轨道和超轨道阶段的预期通量调制。轨道光曲线中的不对称双峰剖面和正弦-长周期调制在前冲圆盘情景下得以重现。观测到的X射线峰的轨道相位漂移和我们对长期X射线数据的拟合表明,这颗中子星很可能是以很小的偏心率围绕恒星运行的,其周天体相位大约为$Phi_{rm p}sim0.6$。我们将LS I+61$^{circ}$ 303的科贝图与其他Be/X-射线双星进行了比较,$P_{rm sup}-P_{rm orb}$图中的线性相关表明,LS I+61$^{circ}$ 303中Be盘的前倾是由其中子星伴星的潮汐力矩引起的。
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引用次数: 0
A Deeper Look into eFEDS AGN Candidates in Dwarf Galaxies with Chandra 用钱德拉深入观测矮星系中的 eFEDS AGN 候选者
Pub Date : 2024-09-06 DOI: arxiv-2409.04514
Adonis A. Sanchez, Amy E. Reines, Akos Bogdan, Ralph P. Kraft
The ability to accurately discern active massive black holes (BHs) in nearbydwarf galaxies is paramount to understanding the origins and processes of"seed" BHs in the early Universe. We present Chandra X-ray Observatoryobservations of a sample of three local dwarf galaxies (M$_{*}$ $leqslant 3times 10^{9}$ M$_odot$, z $leqslant$ 0.15) previously identified ascandidates for hosting active galactic nuclei (AGN). The galaxies were selectedfrom the NASA-Sloan Atlas (NSA) with spatially coincident X-ray detections inthe eROSITA Final Equatorial Depth Survey (eFEDS). Our new Chandra data revealthree X-ray point sources in two of the target galaxies with luminositiesbetween log(L$_{rm text{2-10 keV}}$ [erg s$^{-1}$]) = 39.1 and 40.4. Ourresults support the presence of an AGN in these two galaxies and a ULX in oneof them. For the AGNs, we estimate BH masses of $M_{rm BH} sim 10^{5-6}M_odot$ and Eddington ratios on the order of $sim 10^{-3}$.
要想了解早期宇宙中 "种子 "黑洞的起源和过程,就必须能够准确地分辨出附近矮星系中活跃的大质量黑洞(BHs)。我们展示了钱德拉X射线天文台(Chandra X-ray Observatory)对三个本地矮星系(M$_{*}$ $leqslant 3times 10^{9}$ M$_odot$,z $leqslant$ 0.15)样本的观测结果,这三个矮星系以前曾被确定为活动星系核(AGN)的候选宿主。这些星系是从NASA-Sloan图集(NSA)中挑选出来的,在eROSITA最终赤道深度巡天(eFEDS)中有空间重合的X射线探测。我们最新的钱德拉数据在其中两个目标星系中发现了三个X射线点源,其光度介于log(L$_{rm text{2-10 keV}}$ [erg s$^{-1}$]) = 39.1和40.4之间。我们的研究结果支持在这两个星系中存在一个AGN,在其中一个星系中存在一个ULX。对于AGN,我们估计其BH质量为$M_{/rm BH}sim 10^{5-6}M_odot$,爱丁顿比为 $sim 10^{-3}$。
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引用次数: 0
ZTF SN Ia DR2: The diversity and relative rates of the thermonuclear SN population ZTF SN Ia DR2:热核SN群体的多样性和相对速率
Pub Date : 2024-09-06 DOI: arxiv-2409.04200
G. Dimitriadis, U. Burgaz, M. Deckers, K. Maguire, J. Johansson, M. Smith, M. Rigault, C. Frohmaier, J. Sollerman, L. Galbany, Y. -L. Kim, C. Liu, A. A. Miller, P. E. Nugent, A. Alburai, P. Chen, S. Dhawan, M. Ginolin, A. Goobar, S. L. Groom, L. Harvey, W. D. Kenworthy, S. R. Kulkarni, B. Popovic, R. L. Riddle, B. Rusholme, T. E. Muller-Bravo, J. Nordin, J. H. Terwel, A. Townsend
The Zwicky Transient Facility SN Ia Data Release 2 (ZTF SN Ia DR2) containsmore than 3,000 Type Ia supernovae (SNe Ia), providing the largest homogeneouslow-redshift sample of SNe Ia. Having at least one spectrum per event, thisdata collection is ideal for large-scale statistical studies of thephotometric, spectroscopic and host-galaxy properties of SNe Ia, particularlyof the more rare "peculiar" subclasses. In this paper, we first present themethod we developed to spectroscopically classify the SNe in the sample, andthe techniques we used to model their multi-band light curves and explore theirphotometric properties. We then show a method to distinguish between the"peculiar" subtypes and the normal SNe Ia. We also explore the properties oftheir host galaxies and estimate their relative rates, focusing on the"peculiar" subtypes and their connection to the cosmologically useful SNe Ia.Finally, we discuss the implications of our study with respect to theprogenitor systems of the "peculiar" SN Ia events.
兹威基瞬变设施SN Ia数据第2版(ZTF SN Ia DR2)包含了3000多个Ia型超新星(SNe Ia),提供了最大的同质低红移SNe Ia样本。由于每个事件至少有一个光谱,这个数据集非常适合对Ia型SNe的光度、光谱和宿主星系特性进行大规模统计研究,尤其是对比较罕见的 "奇特 "亚类进行研究。在本文中,我们首先介绍了我们开发的对样本中的SNE进行光谱分类的方法,以及我们用来模拟其多波段光曲线和探索其光度特性的技术。然后,我们展示了一种区分 "奇特 "亚型和正常偶发 Ia 的方法。最后,我们讨论了我们的研究对 "奇特 "SNe Ia 事件的原星系的影响。
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引用次数: 0
Multi-epoch leptohadronic modeling of neutrino source candidate blazar PKS 0735+178 候选中微子源炽星 PKS 0735+178 的多频谱七重建模
Pub Date : 2024-09-06 DOI: arxiv-2409.04165
A. Omeliukh, S. Garrappa, V. Fallah Ramazani, A. Franckowiak, W. Winter, E. Lindfors, K. Nilsson, J. Jormanainen, F. Wierda, A. V. Filippenko, W. Zheng, M. Tornikoski, A. Lähteenmäki, S. Kankkunenand, J. Tammi
The origin of the astrophysical neutrino flux discovered by IceCube remainslargely unknown. Several individual neutrino source candidates were observed.Among them is the gamma-ray flaring blazar TXS 0506+056. A similar coincidenceof a high-energy neutrino and a gamma-ray flare was found in blazar PKS0735+178. By modeling the spectral energy distributions of PKS 0735+178, weexpect to investigate the physical conditions for neutrino production duringdifferent stages of the source activity. We analyze the multi-wavelength dataduring the selected periods of time. Using numerical simulations of radiationprocesses in the source, we study the parameter space of one-zone leptonic andleptohadronic models and find the best-fit solutions that explain the observedphoton fluxes. We show the impact of model parameter degeneracy on theprediction of the neutrino spectra. We show that the available mutli-wavelengthdata are not sufficient to predict the neutrino spectrum unambiguously. Still,under the condition of maximal neutrino flux, we propose a scenario in which0.2 neutrino events are produced during the 50 days flare.
冰立方发现的天体物理中微子通量的来源在很大程度上仍然是未知的。在观测到的几个候选中微子源中,有一个是伽马射线耀斑星TXS 0506+056。在耀斑星 PKS0735+178 中也发现了类似的高能中微子和伽马射线耀斑的巧合。通过对PKS 0735+178的光谱能量分布进行建模,我们期望研究中微子在源活动的不同阶段产生的物理条件。我们分析了选定时间段内的多波长数据。通过对源内辐射过程的数值模拟,我们研究了单区轻子和轻电子模型的参数空间,并找到了能够解释观测到的光子通量的最佳拟合解。我们展示了模型参数退化对中微子光谱预测的影响。我们表明,现有的多波长数据不足以明确地预测中微子谱。尽管如此,在中微子通量最大的条件下,我们提出了在50天耀斑期间产生0.2个中微子事件的设想。
{"title":"Multi-epoch leptohadronic modeling of neutrino source candidate blazar PKS 0735+178","authors":"A. Omeliukh, S. Garrappa, V. Fallah Ramazani, A. Franckowiak, W. Winter, E. Lindfors, K. Nilsson, J. Jormanainen, F. Wierda, A. V. Filippenko, W. Zheng, M. Tornikoski, A. Lähteenmäki, S. Kankkunenand, J. Tammi","doi":"arxiv-2409.04165","DOIUrl":"https://doi.org/arxiv-2409.04165","url":null,"abstract":"The origin of the astrophysical neutrino flux discovered by IceCube remains\u0000largely unknown. Several individual neutrino source candidates were observed.\u0000Among them is the gamma-ray flaring blazar TXS 0506+056. A similar coincidence\u0000of a high-energy neutrino and a gamma-ray flare was found in blazar PKS\u00000735+178. By modeling the spectral energy distributions of PKS 0735+178, we\u0000expect to investigate the physical conditions for neutrino production during\u0000different stages of the source activity. We analyze the multi-wavelength data\u0000during the selected periods of time. Using numerical simulations of radiation\u0000processes in the source, we study the parameter space of one-zone leptonic and\u0000leptohadronic models and find the best-fit solutions that explain the observed\u0000photon fluxes. We show the impact of model parameter degeneracy on the\u0000prediction of the neutrino spectra. We show that the available mutli-wavelength\u0000data are not sufficient to predict the neutrino spectrum unambiguously. Still,\u0000under the condition of maximal neutrino flux, we propose a scenario in which\u00000.2 neutrino events are produced during the 50 days flare.","PeriodicalId":501343,"journal":{"name":"arXiv - PHYS - High Energy Astrophysical Phenomena","volume":"45 1","pages":""},"PeriodicalIF":0.0,"publicationDate":"2024-09-06","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142206564","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
GRB 221009A: the B.O.A.T Burst that Shines in Gamma Rays GRB 221009A:闪耀着伽马射线的B.O.A.T爆发
Pub Date : 2024-09-06 DOI: arxiv-2409.04580
M. AxelssonFermi LAT collaboration, M. AjelloFermi LAT collaboration, M. ArimotoFermi LAT collaboration, L. BaldiniFermi LAT collaboration, J. BalletFermi LAT collaboration, M. G. BaringFermi LAT collaboration, C. BartoliniFermi LAT collaboration, D. BastieriFermi LAT collaboration, J. Becerra GonzalezFermi LAT collaboration, R. BellazziniFermi LAT collaboration, B. BerenjiFermi LAT collaboration, E. BissaldiFermi LAT collaboration, R. D. BlandfordFermi LAT collaboration, R. BoninoFermi LAT collaboration, P. BruelFermi LAT collaboration, S. BusonFermi LAT collaboration, R. A. CameronFermi LAT collaboration, R. CaputoFermi LAT collaboration, P. A. CaraveoFermi LAT collaboration, E. CavazzutiFermi LAT collaboration, C. C. CheungFermi LAT collaboration, G. ChiaroFermi LAT collaboration, N. CibrarioFermi LAT collaboration, S. CipriniFermi LAT collaboration, G. CozzolongoFermi LAT collaboration, P. Cristarella OrestanoFermi LAT collaboration, M. CrnogorcevicFermi LAT collaboration, A. CuocoFermi LAT collaboration, S. CutiniFermi LAT collaboration, F. D'AmmandoFermi LAT collaboration, S. De GaetanoFermi LAT collaboration, N. Di LallaFermi LAT collaboration, A. DineshFermi LAT collaboration, R. Di TriaFermi LAT collaboration, L. Di VenereFermi LAT collaboration, A. DomínguezFermi LAT collaboration, S. J. FeganFermi LAT collaboration, E. C. FerraraFermi LAT collaboration, A. FioriFermi LAT collaboration, A. FranckowiakFermi LAT collaboration, Y. FukazawaFermi LAT collaboration, S. FunkFermi LAT collaboration, P. FuscoFermi LAT collaboration, G. GalantiFermi LAT collaboration, F. GarganoFermi LAT collaboration, C. GasbarraFermi LAT collaboration, S. GermaniFermi LAT collaboration, F. GiacchinoFermi LAT collaboration, N. GigliettoFermi LAT collaboration, M. GilibertiFermi LAT collaboration, R. GillFermi LAT collaboration, F. GiordanoFermi LAT collaboration, M. GirolettiFermi LAT collaboration, J. GranotFermi LAT collaboration, D. GreenFermi LAT collaboration, I. A. GrenierFermi LAT collaboration, S. GuiriecFermi LAT collaboration, M. GustafssonFermi LAT collaboration, M. HashizumeFermi LAT collaboration, E. HaysFermi LAT collaboration, J. W. HewittFermi LAT collaboration, D. HoranFermi LAT collaboration, T. KayanokiFermi LAT collaboration, M. KussFermi LAT collaboration, A. LavironFermi LAT collaboration, J. LiFermi LAT collaboration, I. LiodakisFermi LAT collaboration, F. LongoFermi LAT collaboration, F. LoparcoFermi LAT collaboration, L. LorussoFermi LAT collaboration, B. LottFermi LAT collaboration, M. N. LovelletteFermi LAT collaboration, P. LubranoFermi LAT collaboration, S. MalderaFermi LAT collaboration, D. MalyshevFermi LAT collaboration, A. ManfredaFermi LAT collaboration, G. Martí-DevesaFermi LAT collaboration, R. MartinelliFermi LAT collaboration, I. Martinez CastellanosFermi LAT collaboration, M. N. MazziottaFermi LAT collaboration, J. E. McEneryFermi LAT collaboration, I. MereuFermi LAT collaboration, M. MeyerFermi LAT collaboration, P. F. MichelsonFermi LAT collaboration, N. MirabalFermi LAT collaboration, W. MitthumsiriFermi LAT collaboration, T. MizunoFermi LAT collaboration, P. Monti-GuarnieriFermi LAT collaboration, M. E. MonzaniFermi LAT collaboration, T. MorishitaFermi LAT collaboration, A. MorselliFermi LAT collaboration, I. V. MoskalenkoFermi LAT collaboration, M. NegroFermi LAT collaboration, R. NiwaFermi LAT collaboration, N. OmodeiFermi LAT collaboration, M. OrientiFermi LAT collaboration, E. OrlandoFermi LAT collaboration, D. PanequeFermi LAT collaboration, G. PanzariniFermi LAT collaboration, M. PersicFermi LAT collaboration, M. Pesce-RollinsFermi LAT collaboration, V. PetrosianFermi LAT collaboration, R. PilleraFermi LAT collaboration, F. PironFermi LAT collaboration, T. A. PorterFermi LAT collaboration, G. PrincipeFermi LAT collaboration, J. L. RacusinFermi LAT collaboration, S. RainòFermi LAT collaboration, R. RandoFermi LAT collaboration, B. RaniFermi LAT collaboration, M. RazzanoFermi LAT collaboration, S. RazzaqueFermi LAT collaboration, A. ReimerFermi LAT collaboration, O. ReimerFermi LAT collaboration, F. RydeFermi LAT collaboration, M. Sánchez-CondeFermi LAT collaboration, P. M. Saz ParkinsonFermi LAT collaboration, D. SeriniFermi LAT collaboration, C. SgròFermi LAT collaboration, V. SharmaFermi LAT collaboration, E. J. SiskindFermi LAT collaboration, G. SpandreFermi LAT collaboration, P. SpinelliFermi LAT collaboration, D. J. SusonFermi LAT collaboration, H. TajimaFermi LAT collaboration, D. TakFermi LAT collaboration, J. B. ThayerFermi LAT collaboration, D. F. TorresFermi LAT collaboration, J. ValverdeFermi LAT collaboration, G. ZaharijasFermi LAT collaboration, S. LesageFermi GBM collaboration, M. S. BriggsFermi GBM collaboration, E. BurnsFermi GBM collaboration, S. BalaFermi GBM collaboration, P. N. BhatFermi GBM collaboration, W. H. ClevelandFermi GBM collaboration, S. DalessiFermi GBM collaboration, C. de BarraFermi GBM collaboration, M. GibbyFermi GBM collaboration, M. M. GilesFermi GBM collaboration, R. HamburgFermi GBM collaboration, B. A. HristovFermi GBM collaboration, C. M. HuiFermi GBM collaboration, D. KocevskiFermi GBM collaboration, B. MailyanFermi GBM collaboration, C. MalacariaFermi GBM collaboration, S. McBreenFermi GBM collaboration, S. PoolakkilFermi GBM collaboration, O. J. RobertsFermi GBM collaboration, L. ScottonFermi GBM collaboration, P. VeresFermi GBM collaboration, A. von KienlinFermi GBM collaboration, C. A. Wilson-HodgeFermi GBM collaboration, J. WoodFermi GBM collaboration
We present a complete analysis of Fermi Large Area Telescope (LAT) data ofGRB 221009A, the brightest Gamma-Ray Burst (GRB) ever detected. The burstemission above 30 MeV detected by the LAT preceded by 1 s the low-energy (< 10MeV) pulse that triggered the Fermi Gamma-Ray Burst Monitor (GBM), as has beenobserved in other GRBs. The prompt phase of GRB 221009A lasted a few hundredseconds. It was so bright that we identify a Bad Time Interval (BTI) of 64seconds caused by the extremely high flux of hard X-rays and soft gamma rays,during which the event reconstruction efficiency was poor and the dead timefraction quite high. The late-time emission decayed as a power law, but theextrapolation of the late-time emission during the first 450 seconds suggeststhat the afterglow started during the prompt emission. We also found thathigh-energy events observed by the LAT are incompatible with synchrotronorigin, and, during the prompt emission, are more likely related to an extracomponent identified as synchrotron self-Compton (SSC). A remarkable 400 GeVphoton, detected by the LAT 33 ks after the GBM trigger and directionallyconsistent with the location of GRB 221009A, is hard to explain as a product ofSSC or TeV electromagnetic cascades, and the process responsible for its originis uncertain. Because of its proximity and energetic nature, GRB 221009A is anextremely rare event.
我们对费米大面积望远镜(LAT)探测到的最亮伽马射线暴(GRB)GRB 221009A的数据进行了全面分析。LAT探测到的30MeV以上的爆发系统比触发费米伽玛射线暴监测器(GBM)的低能量(< 10MeV)脉冲早1秒,这在其他伽玛射线暴中也有观察到。GRB 221009A 的激发阶段持续了几百秒。它是如此明亮,以至于我们发现了一个长达64秒的坏时间间隔(Bad Time Interval,BTI),这是由极高的硬X射线和软伽马射线通量造成的,在此期间,事件重建效率很低,死时间分数相当高。晚期发射呈幂律衰减,但对前 450 秒的晚期发射进行的外推法表明,余辉是在早期发射时开始的。我们还发现,LAT 观测到的高能事件与同步加速器起源不符,而更有可能与同步加速器自康普顿(SSC)外成分有关。在GBM触发33 ks后,LAT探测到了一个引人注目的400 GeV光子,其方向与GRB 221009A的位置一致,但很难解释为SSC或TeV电磁级联的产物,其起源过程也不确定。由于GRB 221009A距离很近,能量很高,因此是一个极其罕见的事件。
{"title":"GRB 221009A: the B.O.A.T Burst that Shines in Gamma Rays","authors":"M. AxelssonFermi LAT collaboration, M. AjelloFermi LAT collaboration, M. ArimotoFermi LAT collaboration, L. BaldiniFermi LAT collaboration, J. BalletFermi LAT collaboration, M. G. BaringFermi LAT collaboration, C. BartoliniFermi LAT collaboration, D. BastieriFermi LAT collaboration, J. Becerra GonzalezFermi LAT collaboration, R. BellazziniFermi LAT collaboration, B. BerenjiFermi LAT collaboration, E. BissaldiFermi LAT collaboration, R. D. BlandfordFermi LAT collaboration, R. BoninoFermi LAT collaboration, P. BruelFermi LAT collaboration, S. BusonFermi LAT collaboration, R. A. CameronFermi LAT collaboration, R. CaputoFermi LAT collaboration, P. A. CaraveoFermi LAT collaboration, E. CavazzutiFermi LAT collaboration, C. C. CheungFermi LAT collaboration, G. ChiaroFermi LAT collaboration, N. CibrarioFermi LAT collaboration, S. CipriniFermi LAT collaboration, G. CozzolongoFermi LAT collaboration, P. Cristarella OrestanoFermi LAT collaboration, M. CrnogorcevicFermi LAT collaboration, A. CuocoFermi LAT collaboration, S. CutiniFermi LAT collaboration, F. D'AmmandoFermi LAT collaboration, S. De GaetanoFermi LAT collaboration, N. Di LallaFermi LAT collaboration, A. DineshFermi LAT collaboration, R. Di TriaFermi LAT collaboration, L. Di VenereFermi LAT collaboration, A. DomínguezFermi LAT collaboration, S. J. FeganFermi LAT collaboration, E. C. FerraraFermi LAT collaboration, A. FioriFermi LAT collaboration, A. FranckowiakFermi LAT collaboration, Y. FukazawaFermi LAT collaboration, S. FunkFermi LAT collaboration, P. FuscoFermi LAT collaboration, G. GalantiFermi LAT collaboration, F. GarganoFermi LAT collaboration, C. GasbarraFermi LAT collaboration, S. GermaniFermi LAT collaboration, F. GiacchinoFermi LAT collaboration, N. GigliettoFermi LAT collaboration, M. GilibertiFermi LAT collaboration, R. GillFermi LAT collaboration, F. GiordanoFermi LAT collaboration, M. GirolettiFermi LAT collaboration, J. GranotFermi LAT collaboration, D. GreenFermi LAT collaboration, I. A. GrenierFermi LAT collaboration, S. GuiriecFermi LAT collaboration, M. GustafssonFermi LAT collaboration, M. HashizumeFermi LAT collaboration, E. HaysFermi LAT collaboration, J. W. HewittFermi LAT collaboration, D. HoranFermi LAT collaboration, T. KayanokiFermi LAT collaboration, M. KussFermi LAT collaboration, A. LavironFermi LAT collaboration, J. LiFermi LAT collaboration, I. LiodakisFermi LAT collaboration, F. LongoFermi LAT collaboration, F. LoparcoFermi LAT collaboration, L. LorussoFermi LAT collaboration, B. LottFermi LAT collaboration, M. N. LovelletteFermi LAT collaboration, P. LubranoFermi LAT collaboration, S. MalderaFermi LAT collaboration, D. MalyshevFermi LAT collaboration, A. ManfredaFermi LAT collaboration, G. Martí-DevesaFermi LAT collaboration, R. MartinelliFermi LAT collaboration, I. Martinez CastellanosFermi LAT collaboration, M. N. MazziottaFermi LAT collaboration, J. E. McEneryFermi LAT collaboration, I. MereuFermi LAT collaboration, M. MeyerFermi LAT collaboration, P. F. MichelsonFermi LAT collaboration, N. MirabalFermi LAT collaboration, W. MitthumsiriFermi LAT collaboration, T. MizunoFermi LAT collaboration, P. Monti-GuarnieriFermi LAT collaboration, M. E. MonzaniFermi LAT collaboration, T. MorishitaFermi LAT collaboration, A. MorselliFermi LAT collaboration, I. V. MoskalenkoFermi LAT collaboration, M. NegroFermi LAT collaboration, R. NiwaFermi LAT collaboration, N. OmodeiFermi LAT collaboration, M. OrientiFermi LAT collaboration, E. OrlandoFermi LAT collaboration, D. PanequeFermi LAT collaboration, G. PanzariniFermi LAT collaboration, M. PersicFermi LAT collaboration, M. Pesce-RollinsFermi LAT collaboration, V. PetrosianFermi LAT collaboration, R. PilleraFermi LAT collaboration, F. PironFermi LAT collaboration, T. A. PorterFermi LAT collaboration, G. PrincipeFermi LAT collaboration, J. L. RacusinFermi LAT collaboration, S. RainòFermi LAT collaboration, R. RandoFermi LAT collaboration, B. RaniFermi LAT collaboration, M. RazzanoFermi LAT collaboration, S. RazzaqueFermi LAT collaboration, A. ReimerFermi LAT collaboration, O. ReimerFermi LAT collaboration, F. RydeFermi LAT collaboration, M. Sánchez-CondeFermi LAT collaboration, P. M. Saz ParkinsonFermi LAT collaboration, D. SeriniFermi LAT collaboration, C. SgròFermi LAT collaboration, V. SharmaFermi LAT collaboration, E. J. SiskindFermi LAT collaboration, G. SpandreFermi LAT collaboration, P. SpinelliFermi LAT collaboration, D. J. SusonFermi LAT collaboration, H. TajimaFermi LAT collaboration, D. TakFermi LAT collaboration, J. B. ThayerFermi LAT collaboration, D. F. TorresFermi LAT collaboration, J. ValverdeFermi LAT collaboration, G. ZaharijasFermi LAT collaboration, S. LesageFermi GBM collaboration, M. S. BriggsFermi GBM collaboration, E. BurnsFermi GBM collaboration, S. BalaFermi GBM collaboration, P. N. BhatFermi GBM collaboration, W. H. ClevelandFermi GBM collaboration, S. DalessiFermi GBM collaboration, C. de BarraFermi GBM collaboration, M. GibbyFermi GBM collaboration, M. M. GilesFermi GBM collaboration, R. HamburgFermi GBM collaboration, B. A. HristovFermi GBM collaboration, C. M. HuiFermi GBM collaboration, D. KocevskiFermi GBM collaboration, B. MailyanFermi GBM collaboration, C. MalacariaFermi GBM collaboration, S. McBreenFermi GBM collaboration, S. PoolakkilFermi GBM collaboration, O. J. RobertsFermi GBM collaboration, L. ScottonFermi GBM collaboration, P. VeresFermi GBM collaboration, A. von KienlinFermi GBM collaboration, C. A. Wilson-HodgeFermi GBM collaboration, J. WoodFermi GBM collaboration","doi":"arxiv-2409.04580","DOIUrl":"https://doi.org/arxiv-2409.04580","url":null,"abstract":"We present a complete analysis of Fermi Large Area Telescope (LAT) data of\u0000GRB 221009A, the brightest Gamma-Ray Burst (GRB) ever detected. The burst\u0000emission above 30 MeV detected by the LAT preceded by 1 s the low-energy (< 10\u0000MeV) pulse that triggered the Fermi Gamma-Ray Burst Monitor (GBM), as has been\u0000observed in other GRBs. The prompt phase of GRB 221009A lasted a few hundred\u0000seconds. It was so bright that we identify a Bad Time Interval (BTI) of 64\u0000seconds caused by the extremely high flux of hard X-rays and soft gamma rays,\u0000during which the event reconstruction efficiency was poor and the dead time\u0000fraction quite high. The late-time emission decayed as a power law, but the\u0000extrapolation of the late-time emission during the first 450 seconds suggests\u0000that the afterglow started during the prompt emission. We also found that\u0000high-energy events observed by the LAT are incompatible with synchrotron\u0000origin, and, during the prompt emission, are more likely related to an extra\u0000component identified as synchrotron self-Compton (SSC). A remarkable 400 GeV\u0000photon, detected by the LAT 33 ks after the GBM trigger and directionally\u0000consistent with the location of GRB 221009A, is hard to explain as a product of\u0000SSC or TeV electromagnetic cascades, and the process responsible for its origin\u0000is uncertain. Because of its proximity and energetic nature, GRB 221009A is an\u0000extremely rare event.","PeriodicalId":501343,"journal":{"name":"arXiv - PHYS - High Energy Astrophysical Phenomena","volume":"13 1","pages":""},"PeriodicalIF":0.0,"publicationDate":"2024-09-06","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142206560","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
Self-lensing flares from black hole binaries IV: the number of detectable shadows 来自黑洞双星的自透镜耀斑 IV:可探测到的阴影数量
Pub Date : 2024-09-06 DOI: arxiv-2409.04583
Kevin Park, Chengcheng Xin, Jordy Davelaar, Zoltan Haiman
Sub-parsec supermassive black hole (SMBH) binaries are expected to be commonin active galactic nuclei (AGN), as a result of the hierarchical build-up ofgalaxies via mergers. While direct evidence for these compact binaries islacking, a few hundred candidates have been identified, most based on theapparent periodicities of their optical light-curves. Since these signaturescan be mimicked by AGN red-noise, additional evidence is needed to confirmtheir binary nature. Recurring self-lensing flares (SLF), occurring wheneverthe two BHs are aligned with the line of sight within their Einstein radii,have been suggested as additional binary signatures. Furthermore, in manycases, lensing flares are also predicted to contain a "dip", whenever thelensed SMBH's shadow is comparable in angular size to the binary's Einsteinradius. This feature would unambiguously confirm binaries and additionallyidentify SMBH shadows that are spatially unresolvable by high-resolution VLBI.Here we estimate the number of quasars for which these dips may be detectableby LSST, by extrapolating the quasar luminosity function to faint magnitudes,and assuming that SMBH binaries are randomly oriented and have mass-ratiosfollowing those in the Illustris simulations. Under plausible assumptions aboutquasar lifetimes, binary fractions, and Eddington ratios, we expect tens ofthousands of detectable flares, of which several dozen contain measurable dips.
超大质量黑洞(SMBH)双星预计在活动星系核(AGN)中很常见,这是星系通过合并分层堆积的结果。虽然缺乏这些紧凑型双星的直接证据,但已经确定了几百个候选者,大部分是基于其光学光曲线的明显周期性。由于这些特征可以被 AGN 红噪模仿,因此需要更多的证据来证实它们的双星性质。每当两个黑体在它们的爱因斯坦半径范围内与视线对齐时,就会发生重复出现的自透镜耀斑(SLF),这被认为是额外的双星特征。此外,在许多情况下,当被光照的 SMBH 的影子的角尺寸与双星的爱因斯坦半径相当时,光照耀斑也被预测为包含 "凹陷"。在这里,我们通过将类星体光度函数外推到微弱等级,并假设SMBH双星是随机定向的,其质量比与Illustris模拟中的质量比相同,来估算LSST可能探测到这些凹陷的类星体数量。根据对类星体寿命、双星比例和爱丁顿比的合理假设,我们预计会有数万个可探测到的耀斑,其中几十个包含可测量的凹陷。
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引用次数: 0
ZTF SN Ia DR2: Overview ZTF SN Ia DR2:概述
Pub Date : 2024-09-06 DOI: arxiv-2409.04346
Mickael Rigault, Mathew Smith, Ariel Goobar, Kate Maguire, Georgios Dimitriadis, Umut Burgaz, Suhail Dhawan, Jesper Sollerman, Nicolas Regnault, Marek Kowalski, Melissa Amenouche, Marie Aubert, Chloé Barjou-Delayre, Julian Bautista, Josh S. Bloom, Bastien Carreres, Tracy X. Chen, Yannick Copin, Maxime Deckers, Dominique Fouchez, Christoffer Fremling, Lluis Galbany, Madeleine Ginolin, Matthew Graham, Mancy M. Kasliwal, W. D'Arcy Kenworthy, Young-Lo Kim, Dylan Kuhn, Frank F. Masci, Tomas Müller-Bravo, Adam Miller, Joel Johansson, Jakob Nordin, Peter Nugent, Igor Andreoni, Eric Bellm, Marc Betoule, Mahmoud Osman, Dan Perley, Brodie Popovic, Philippe Rosnet, Damiano Rosselli, Florian Ruppin, Robert Senzel, Ben Rusholme, Tassilo Schweyer, Jacco H. Terwel, Alice Townsend, Andy Tzanidakis, Avery Wold, Josiah Purdum, Yu-Jing Qin, Benjamin Racine, Simeon Reusch, Reed Riddle, Lin Yan
We present the first homogeneous release of several thousand Type Iasupernovae (SNe Ia), all having spectroscopic classification, and spectroscopicredshifts for half the sample. This release, named the "DR2", contains 3628nearby (z < 0.3) SNe Ia discovered, followed and classified by the ZwickyTransient Facility survey between March 2018 and December 2020. Of these, 3000have good-to-excellent sampling and 2667 pass standard cosmology light-curvequality cuts. This release is thus the largest SN Ia release to date,increasing by an order of magnitude the number of well characterizedlow-redshift objects. With the "DR2", we also provide a volume-limited (z <0.06) sample of nearly a thousand SNe Ia. With such a large, homogeneous andwell controlled dataset, we are studying key current questions on SN cosmology,such as the linearity SNe Ia standardization, the SN and host dependencies, thediversity of the SN Ia population, and the accuracy of the current light-curvemodeling. These, and more, are studied in detail in a series of articlesassociated with this release. Alongside the SN Ia parameters, we publish ourforce-photometry gri-band light curves, 5138 spectra, local and global hostproperties, observing logs, and a python tool to ease use and access of thesedata. The photometric accuracy of the "DR2" is not yet suited for cosmologicalparameter inference, which will follow as "DR2.5" release. We nonethelessdemonstrate that the multi-thousand SN Ia Hubble Diagram has a typical 0.15 magscatter.
我们首次发布了数千个I型超新星(SNe Ia),所有样本都有光谱分类和一半样本的光谱红移。这次发布的样本被命名为 "DR2",包含了 2018 年 3 月至 2020 年 12 月间由兹威基瞬变设施巡天发现、跟踪和分类的 3628 个近邻(z < 0.3)Ia SNe。其中,3000个具有良好到优秀的采样,2667个通过了标准宇宙学光曲线质量切割。因此,这次发布是迄今为止规模最大的一次SN Ia发布,使特性良好的低红移天体的数量增加了一个数量级。通过 "DR2",我们还提供了近千个SNe Ia的体积限制(z <0.06)样本。有了这样一个庞大、均质和良好控制的数据集,我们就可以研究当前有关SN宇宙学的关键问题,如SNe Ia的线性标准化、SN与宿主的相关性、SN Ia群体的多样性以及当前光曲线建模的准确性。与此次发布相关的一系列文章将对这些问题以及更多问题进行详细研究。除了SN Ia参数之外,我们还发布了我们的测力光度gri波段光曲线、5138光谱、局部和全局宿主属性、观测日志以及一个python工具,以方便使用和访问这些数据。DR2 "的光度精度还不适合用于宇宙学参数推断,这将在 "DR2.5 "发布后进行。尽管如此,我们还是证明了数以千计的 SN Ia 哈勃图具有典型的 0.15 马格散射。
{"title":"ZTF SN Ia DR2: Overview","authors":"Mickael Rigault, Mathew Smith, Ariel Goobar, Kate Maguire, Georgios Dimitriadis, Umut Burgaz, Suhail Dhawan, Jesper Sollerman, Nicolas Regnault, Marek Kowalski, Melissa Amenouche, Marie Aubert, Chloé Barjou-Delayre, Julian Bautista, Josh S. Bloom, Bastien Carreres, Tracy X. Chen, Yannick Copin, Maxime Deckers, Dominique Fouchez, Christoffer Fremling, Lluis Galbany, Madeleine Ginolin, Matthew Graham, Mancy M. Kasliwal, W. D'Arcy Kenworthy, Young-Lo Kim, Dylan Kuhn, Frank F. Masci, Tomas Müller-Bravo, Adam Miller, Joel Johansson, Jakob Nordin, Peter Nugent, Igor Andreoni, Eric Bellm, Marc Betoule, Mahmoud Osman, Dan Perley, Brodie Popovic, Philippe Rosnet, Damiano Rosselli, Florian Ruppin, Robert Senzel, Ben Rusholme, Tassilo Schweyer, Jacco H. Terwel, Alice Townsend, Andy Tzanidakis, Avery Wold, Josiah Purdum, Yu-Jing Qin, Benjamin Racine, Simeon Reusch, Reed Riddle, Lin Yan","doi":"arxiv-2409.04346","DOIUrl":"https://doi.org/arxiv-2409.04346","url":null,"abstract":"We present the first homogeneous release of several thousand Type Ia\u0000supernovae (SNe Ia), all having spectroscopic classification, and spectroscopic\u0000redshifts for half the sample. This release, named the \"DR2\", contains 3628\u0000nearby (z < 0.3) SNe Ia discovered, followed and classified by the Zwicky\u0000Transient Facility survey between March 2018 and December 2020. Of these, 3000\u0000have good-to-excellent sampling and 2667 pass standard cosmology light-curve\u0000quality cuts. This release is thus the largest SN Ia release to date,\u0000increasing by an order of magnitude the number of well characterized\u0000low-redshift objects. With the \"DR2\", we also provide a volume-limited (z <\u00000.06) sample of nearly a thousand SNe Ia. With such a large, homogeneous and\u0000well controlled dataset, we are studying key current questions on SN cosmology,\u0000such as the linearity SNe Ia standardization, the SN and host dependencies, the\u0000diversity of the SN Ia population, and the accuracy of the current light-curve\u0000modeling. These, and more, are studied in detail in a series of articles\u0000associated with this release. Alongside the SN Ia parameters, we publish our\u0000force-photometry gri-band light curves, 5138 spectra, local and global host\u0000properties, observing logs, and a python tool to ease use and access of these\u0000data. The photometric accuracy of the \"DR2\" is not yet suited for cosmological\u0000parameter inference, which will follow as \"DR2.5\" release. We nonetheless\u0000demonstrate that the multi-thousand SN Ia Hubble Diagram has a typical 0.15 mag\u0000scatter.","PeriodicalId":501343,"journal":{"name":"arXiv - PHYS - High Energy Astrophysical Phenomena","volume":"203 1","pages":""},"PeriodicalIF":0.0,"publicationDate":"2024-09-06","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142206580","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
Asymptotic-state prediction for fast flavor transformation in neutron star mergers 中子星合并中快速味道转换的渐近态预测
Pub Date : 2024-09-06 DOI: arxiv-2409.04405
Sherwood Richers, Julien Froustey, Somdutta Ghosh, Francois Foucart, Javier Gomez
Neutrino flavor instabilities appear to be omnipresent in dense astrophysicalenvironments, thus presenting a challenge to large-scale simulations ofcore-collapse supernovae and neutron star mergers (NSMs). Subgrid models offera path forward, but require an accurate determination of the local outcome ofsuch conversion phenomena. Focusing on "fast" instabilities, related to theexistence of a crossing between neutrino and antineutrino angulardistributions, we consider a range of analytical mixing schemes, including anew, fully three-dimensional one, and also introduce a new machine learning(ML) model. We compare the accuracy of these models with the results of severalthousands of local dynamical calculations of neutrino evolution from theconditions extracted from classical NSM simulations. Our ML model shows goodoverall performance, but struggles to generalize to conditions from a NSMsimulation not used for training. The multidimensional analytic model performsand generalizes even better, while other analytic models (which assumeaxisymmetric neutrino distributions) do not have reliably high performances, asthey notably fail as expected to account for effects resulting from stronganisotropies. The ML and analytic subgrid models extensively tested here areboth promising, with different computational requirements and sources ofsystematic errors.
中微子味道不稳定性似乎在高密度天体物理环境中无处不在,因此给大规模模拟核坍缩超新星和中子星合并(NSMs)带来了挑战。子网格模型提供了一条前进的道路,但需要准确确定这种转换现象的局部结果。我们重点研究了与中微子和反中微子角分布交叉有关的 "快速 "不稳定性,考虑了一系列分析混合方案,包括一种新的、完全三维的方案,还引入了一种新的机器学习(ML)模型。我们将这些模型的准确性与根据经典 NSM 模拟提取的条件对中微子演化进行的数千次局部动力学计算的结果进行了比较。我们的 ML 模型显示出良好的总体性能,但在泛化未用于训练的 NSM 模拟条件时却很吃力。多维分析模型的性能和泛化效果更好,而其他分析模型(假定中微子分布是不对称的)的性能并不可靠,因为它们在解释强各向异性产生的影响时明显失败。这里广泛测试的 ML 子网格模型和解析子网格模型都很有前途,但它们的计算要求和系统误差来源各不相同。
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引用次数: 0
Triple trouble with PSR J1618-3921: Mass measurements and orbital dynamics of an eccentric millisecond pulsar PSR J1618-3921 的三重麻烦:偏心毫秒脉冲星的质量测量和轨道动力学
Pub Date : 2024-09-05 DOI: arxiv-2409.03615
K. Grunthal, V. Venkatraman Krishnan, P. C. C. Freire, M. Kramer, M. Bailes, S. Buchner, M. Burgay, A. D. Cameron, C. -H. R. Chen, I. Cognard, L. Guillemot, M. E. Lower, A. Possenti, G. Theureau
PSR J1618-3921 is one of five known millisecond pulsars (MSPs) in eccentricorbits (eMPSs) located in the Galactic plane, whose formation is poorlyunderstood. Earlier studies of these objects revealed significant discrepanciesbetween observation and predictions from standard binary evolution scenarios ofpulsar-Helium white dwarf binaries. We conducted observations with the L-bandreceiver of the MeerKAT radio telescope and the UWL receiver of the ParkesMurriyang radio telescope between 2019 and 2021. These data were added toarchival observations. We perform an analysis of this joint 23-year-dataset. Weuse the recent observations to give a brief account of the emission propertiesof J1618-3921, including a Rotating Vector model fit of the linear polarisationposition angle of the pulsar. The long timing baseline allowed for a highlysignificant measurement of the rate of advance of periastron of $dot{omega}$.We can only report a low significance detection of the orthometric Shapirodelay parameters $h_3$ and $varsigma$, leading to mass estimates of the totaland individual binary masses. We detect an unexpected change in the orbitalperiod of, which is an order of magnitude larger and carries an opposite signto what is expected from Galactic acceleration and the Shklovskii effect. Wealso detect a significant second derivative of the spin frequency. Furthermore,we report an unexpected, abrupt change of the mean pulse profile in June 2021with unknown origin. We propose that the anomalous $dot{P_b}$ and $ddot{f}$indicate an additional varying acceleration due to a nearby mass, i.e., theJ1618-3921 binary system is likely part of a hierarchical triple. This findingsuggests that at least some eMSPs might have formed in triple star systems.Although the uncertainties are large, the binary companion mass is consistentwith the $P_b$ - $M_{WD}$ relation.
PSR J1618-3921 是位于银河系平面的五颗已知偏心轨道毫秒脉冲星(MSPs)之一,人们对它们的形成过程知之甚少。对这些天体的早期研究表明,观测结果与脉冲星-氦白矮星双星的标准双星演化方案的预测结果之间存在巨大差异。我们利用 MeerKAT 射电望远镜的 L 波段接收器和 ParkesMurriyang 射电望远镜的 UWL 接收器在 2019 年至 2021 年期间进行了观测。这些数据被添加到历史观测数据中。我们对这个 23 年的联合数据集进行了分析。我们利用最近的观测数据简要介绍了 J1618-3921 的发射特性,包括脉冲星线性偏振位置角的旋转矢量模型拟合。我们只能报告对正交沙皮罗延迟参数$h_3$和$varsigma$的低显著性探测,从而得出双星总质量和单个质量的估计值。我们探测到了一个意想不到的轨道周期变化,它比银河加速度和什克洛夫斯基效应所预期的要大一个数量级,并且具有相反的意义。我们还探测到了自旋频率的重要二阶导数。此外,我们还报告了 2021 年 6 月平均脉冲轮廓的意外突变,其原因不明。我们认为,反常的$dot{P_b}$和$dot{f}$表明由于附近质量的存在而产生了额外的变化加速度,也就是说,J1618-3921双星系统很可能是分层三重系统的一部分。尽管不确定性很大,但双星伴星质量与$P_b$ - $M_{WD}$关系是一致的。
{"title":"Triple trouble with PSR J1618-3921: Mass measurements and orbital dynamics of an eccentric millisecond pulsar","authors":"K. Grunthal, V. Venkatraman Krishnan, P. C. C. Freire, M. Kramer, M. Bailes, S. Buchner, M. Burgay, A. D. Cameron, C. -H. R. Chen, I. Cognard, L. Guillemot, M. E. Lower, A. Possenti, G. Theureau","doi":"arxiv-2409.03615","DOIUrl":"https://doi.org/arxiv-2409.03615","url":null,"abstract":"PSR J1618-3921 is one of five known millisecond pulsars (MSPs) in eccentric\u0000orbits (eMPSs) located in the Galactic plane, whose formation is poorly\u0000understood. Earlier studies of these objects revealed significant discrepancies\u0000between observation and predictions from standard binary evolution scenarios of\u0000pulsar-Helium white dwarf binaries. We conducted observations with the L-band\u0000receiver of the MeerKAT radio telescope and the UWL receiver of the Parkes\u0000Murriyang radio telescope between 2019 and 2021. These data were added to\u0000archival observations. We perform an analysis of this joint 23-year-dataset. We\u0000use the recent observations to give a brief account of the emission properties\u0000of J1618-3921, including a Rotating Vector model fit of the linear polarisation\u0000position angle of the pulsar. The long timing baseline allowed for a highly\u0000significant measurement of the rate of advance of periastron of $dot{omega}$.\u0000We can only report a low significance detection of the orthometric Shapiro\u0000delay parameters $h_3$ and $varsigma$, leading to mass estimates of the total\u0000and individual binary masses. We detect an unexpected change in the orbital\u0000period of, which is an order of magnitude larger and carries an opposite sign\u0000to what is expected from Galactic acceleration and the Shklovskii effect. We\u0000also detect a significant second derivative of the spin frequency. Furthermore,\u0000we report an unexpected, abrupt change of the mean pulse profile in June 2021\u0000with unknown origin. We propose that the anomalous $dot{P_b}$ and $ddot{f}$\u0000indicate an additional varying acceleration due to a nearby mass, i.e., the\u0000J1618-3921 binary system is likely part of a hierarchical triple. This finding\u0000suggests that at least some eMSPs might have formed in triple star systems.\u0000Although the uncertainties are large, the binary companion mass is consistent\u0000with the $P_b$ - $M_{WD}$ relation.","PeriodicalId":501343,"journal":{"name":"arXiv - PHYS - High Energy Astrophysical Phenomena","volume":"58 1","pages":""},"PeriodicalIF":0.0,"publicationDate":"2024-09-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142206585","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
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arXiv - PHYS - High Energy Astrophysical Phenomena
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