Physical Review DPub Date : 2025-02-13DOI: 10.1103/physrevd.111.044039
Diganta Bandopadhyay, Christopher J. Moore
{"title":"Searching for stellar-origin binary black holes in LISA Data Challenge 1b: Yorsh","authors":"Diganta Bandopadhyay, Christopher J. Moore","doi":"10.1103/physrevd.111.044039","DOIUrl":"https://doi.org/10.1103/physrevd.111.044039","url":null,"abstract":"This paper reports the first search for stellar-origin binary black holes within the LISA Data Challenges (LDC). The search algorithm and the LDC datasets, both previously described elsewhere, are only summarized briefly; the primary focus here is to present the results of applying the search to the challenge of data. The search employs a hierarchical approach, leveraging semicoherent matching of template waveforms to the data using a variable number of segments, combined with a particle swarm algorithm for parameter space exploration. The computational pipeline is accelerated using graphics processing unit (GPU) hardware. The results of two searches using different models of the LISA response are presented. The most effective search finds all five sources in the data challenge with injected signal-to-noise ratios ≳</a:mo>12</a:mn></a:math>. Rapid parameter estimation is performed for these sources. <jats:supplementary-material> <jats:copyright-statement>Published by the American Physical Society</jats:copyright-statement> <jats:copyright-year>2025</jats:copyright-year> </jats:permissions> </jats:supplementary-material>","PeriodicalId":20167,"journal":{"name":"Physical Review D","volume":"79 6 1","pages":""},"PeriodicalIF":5.0,"publicationDate":"2025-02-13","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143417298","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"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}
Physical Review DPub Date : 2025-02-13DOI: 10.1103/physrevd.111.034019
Shohini Bhattacharya, Renaud Boussarie, Yoshitaka Hatta
{"title":"Exploring orbital angular momentum and spin-orbit correlations for gluons at the Electron-Ion Collider","authors":"Shohini Bhattacharya, Renaud Boussarie, Yoshitaka Hatta","doi":"10.1103/physrevd.111.034019","DOIUrl":"https://doi.org/10.1103/physrevd.111.034019","url":null,"abstract":"In our previous work [S. Bhattacharya , ], we introduced a pioneering observable aimed at experimentally detecting the orbital angular momentum (OAM) of gluons. Our focus was on the longitudinal double spin asymmetry observed in exclusive dijet production during electron-proton scattering. We demonstrated the sensitivity of the cos</a:mi>ϕ</a:mi></a:math> angular correlation between the scattered electron and proton as a probe for gluon OAM at small <c:math xmlns:c=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><c:mi>x</c:mi></c:math> and its intricate interplay with gluon helicity. This current work provides a comprehensive exposition, diving further into the aforementioned calculation with added elaboration and in-depth analysis. We reveal that, in addition to the gluon OAM, one also gains access to the spin-orbit correlation of gluons. We supplement our work with a detailed numerical analysis of our observables for the kinematics of the Electron-Ion Collider. In addition to dijet production, we also consider the recently proposed semi-inclusive diffractive deep inelastic scattering process, which potentially offers experimental advantages over dijet measurements. Finally, we investigate quark-channel contributions to these processes and find an unexpected breakdown of collinear factorization. <jats:supplementary-material> <jats:copyright-statement>Published by the American Physical Society</jats:copyright-statement> <jats:copyright-year>2025</jats:copyright-year> </jats:permissions> </jats:supplementary-material>","PeriodicalId":20167,"journal":{"name":"Physical Review D","volume":"21 1","pages":""},"PeriodicalIF":5.0,"publicationDate":"2025-02-13","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143418362","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"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}
Physical Review DPub Date : 2025-02-12DOI: 10.1103/physrevd.111.043030
Connor Stratman, Tongyan Lin
{"title":"Daily modulation of low-energy nuclear recoils from sub-GeV dark matter","authors":"Connor Stratman, Tongyan Lin","doi":"10.1103/physrevd.111.043030","DOIUrl":"https://doi.org/10.1103/physrevd.111.043030","url":null,"abstract":"At sufficiently low nuclear recoil energy, the scattering of dark matter (DM) in crystals gives rise to single phonon and multiphonon excitations. In anisotropic crystals, the scattering rate into phonons modulates over each sidereal day as the crystal rotates with respect to the DM wind. This gives a potential avenue for directional detection of DM. The daily modulation for single phonons has previously been calculated. Here we calculate the daily modulation for multiphonon excitations from DM in the mass range 1 MeV–1 GeV. We generalize previous multiphonon calculations, which made an isotropic approximation, and implement results in the DarkELF package. We find daily modulation rates up to 1%–10% for an Al</a:mi>2</a:mn></a:msub>O</a:mi>3</a:mn></a:msub></a:math> target and DM mass below 30 MeV, depending on the recoil energies probed. We obtain similar results for SiC, while modulation in Si, GaAs, and <d:math xmlns:d=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><d:mrow><d:msub><d:mrow><d:mi>SiO</d:mi></d:mrow><d:mrow><d:mn>2</d:mn></d:mrow></d:msub></d:mrow></d:math> is negligible. <jats:supplementary-material> <jats:copyright-statement>Published by the American Physical Society</jats:copyright-statement> <jats:copyright-year>2025</jats:copyright-year> </jats:permissions> </jats:supplementary-material>","PeriodicalId":20167,"journal":{"name":"Physical Review D","volume":"63 1","pages":""},"PeriodicalIF":5.0,"publicationDate":"2025-02-12","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143393519","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"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}
Physical Review DPub Date : 2025-02-12DOI: 10.1103/physrevd.111.043029
Badal Bhalla, Benjamin V. Lehmann, Kuver Sinha, Tao Xu
{"title":"Three-body exchanges with primordial black holes","authors":"Badal Bhalla, Benjamin V. Lehmann, Kuver Sinha, Tao Xu","doi":"10.1103/physrevd.111.043029","DOIUrl":"https://doi.org/10.1103/physrevd.111.043029","url":null,"abstract":"The abundance of massive primordial black holes has historically been constrained by dynamical probes. Since these objects can participate in hard few-body scattering processes, they can readily transfer energy to stellar systems and, in particular, disrupt wide binaries. However, disruption is not the only possible outcome of such few-body processes. Primordial black holes could also participate in exchange processes, in which one component of a binary system is ejected and replaced by the black hole itself. In this case, the remaining object in the binary would dynamically appear to have an invisible companion. We study the rate of exchange processes for primordial black holes as a component of dark matter and evaluate possible mechanisms for detecting such binaries. We find that many such binaries plausibly exist in the Solar neighborhood and show that this process can account for observed binary systems whose properties run counter to the predictions of isolated binary evolution. <jats:supplementary-material> <jats:copyright-statement>Published by the American Physical Society</jats:copyright-statement> <jats:copyright-year>2025</jats:copyright-year> </jats:permissions> </jats:supplementary-material>","PeriodicalId":20167,"journal":{"name":"Physical Review D","volume":"54 1","pages":""},"PeriodicalIF":5.0,"publicationDate":"2025-02-12","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143401467","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"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}
Physical Review DPub Date : 2025-02-12DOI: 10.1103/physrevd.111.035010
Zeren Simon Wang, Yu Zhang, Wei Liu
{"title":"Long-lived sterile neutrinos from an axionlike particle at Belle II","authors":"Zeren Simon Wang, Yu Zhang, Wei Liu","doi":"10.1103/physrevd.111.035010","DOIUrl":"https://doi.org/10.1103/physrevd.111.035010","url":null,"abstract":"Axionlike particles (ALPs) can be produced in meson decays via tree-level quark-flavor-violating couplings, and decay to a pair of sterile neutrinos if also coupled to them. Such light sterile neutrinos are necessarily long-lived and may give rise to striking signatures of displaced vertices (DVs) at terrestrial experiments. In this work, we study the prospect of the ongoing Belle II experiment for detecting the sterile neutrinos from the ALP, leveraging the O</a:mi>(</a:mo>10</a:mn>10</a:mn></a:msup>)</a:mo></a:math> <f:math xmlns:f=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><f:mi>B</f:mi></f:math>-mesons projected to be produced at the experiment with an integrated luminosity of <h:math xmlns:h=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><h:mrow><h:mn>50</h:mn><h:mtext> </h:mtext><h:mtext> </h:mtext><h:msup><h:mrow><h:mi>ab</h:mi></h:mrow><h:mrow><h:mo>−</h:mo><h:mn>1</h:mn></h:mrow></h:msup></h:mrow></h:math>. We propose search strategies for one or two DVs, and perform Monte-Carlo simulations in order to estimate the sensitivity reach of Belle II to active-sterile-neutrino mixing <j:math xmlns:j=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><j:mo stretchy=\"false\">|</j:mo><j:msub><j:mi>V</j:mi><j:mrow><j:mi>e</j:mi><j:mi>N</j:mi></j:mrow></j:msub><j:msup><j:mo stretchy=\"false\">|</j:mo><j:mn>2</j:mn></j:msup></j:math> as functions of the sterile-neutrino mass. Signatures include a selected list of sterile-neutrino final states, for which we estimate an <n:math xmlns:n=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><n:mi mathvariant=\"script\">O</n:mi><n:mo stretchy=\"false\">(</n:mo><n:mn>1</n:mn><n:mo stretchy=\"false\">)</n:mo></n:math> or lower background level. Our results show that the proposed search strategies can probe values of <s:math xmlns:s=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><s:mo stretchy=\"false\">|</s:mo><s:msub><s:mi>V</s:mi><s:mrow><s:mi>e</s:mi><s:mi>N</s:mi></s:mrow></s:msub><s:msup><s:mo stretchy=\"false\">|</s:mo><s:mn>2</s:mn></s:msup></s:math> up to about two orders of magnitude beyond the existing bounds, for ALP mass over 4 GeV and sterile-neutrino mass above the <w:math xmlns:w=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><w:mi>D</w:mi></w:math>-meson threshold. Compared to the one-DV search, the two-DV one, despite its weaker sensitivities as a result of double exponential suppression of the sterile-neutrino decay positions, possesses the advantage of possible full reconstruction of the signal event allowing for pinning down the masses of the sterile neutrino and the ALP, if a discovery is made. <jats:supplementary-material> <jats:copyright-statement>Published by the American Physical Society</jats:copyright-statement> <jats:copyright-year>2025</jats:copyright-year> </jats:permissions> </jats:supplementary-material>","PeriodicalId":20167,"journal":{"name":"Physical Review D","volume":"35 1","pages":""},"PeriodicalIF":5.0,"publicationDate":"2025-02-12","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143401503","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"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}
Physical Review DPub Date : 2025-02-12DOI: 10.1103/physrevd.111.036019
J. Andrade, Rodolfo Casana, E. da Hora
{"title":"BPS chiral vortices in Maxwell-Higgs electrodynamics","authors":"J. Andrade, Rodolfo Casana, E. da Hora","doi":"10.1103/physrevd.111.036019","DOIUrl":"https://doi.org/10.1103/physrevd.111.036019","url":null,"abstract":"We investigate the existence of Bogomol’nyi-Prasad-Sommerfield (BPS) structures in Maxwell-Higgs electrodynamics immersed in a chiral medium. The medium has its electromagnetic properties controlled by both a Chern-Simons term and a neutral scalar field. We implement the Bogomol’nyi-Prasad-Sommerfield technique and minimize the corresponding total energy. As a consequence, we get the BPS potential and the self-dual equations whose solutions saturate the Bogomol’nyi bound. In such a context, we look for vortices in two chiral media. The first one engenders localized configurations with an exponential decay similar to that of the standard Abrikosov-Nielsen-Olesen solutions. The second medium generates delocalized profiles whose tail follows a power-law decay. In both cases, we discuss the effects on the shape of the field profiles due to the chiral medium. <jats:supplementary-material> <jats:copyright-statement>Published by the American Physical Society</jats:copyright-statement> <jats:copyright-year>2025</jats:copyright-year> </jats:permissions> </jats:supplementary-material>","PeriodicalId":20167,"journal":{"name":"Physical Review D","volume":"47 1","pages":""},"PeriodicalIF":5.0,"publicationDate":"2025-02-12","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143401511","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"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}
Physical Review DPub Date : 2025-02-12DOI: 10.1103/physrevd.111.034017
Jens O. Andersen, Martin Kjøllesdal Johnsrud, Qing Yu, Hua Zhou
{"title":"Chiral perturbation theory and Bose-Einstein condensation in QCD","authors":"Jens O. Andersen, Martin Kjøllesdal Johnsrud, Qing Yu, Hua Zhou","doi":"10.1103/physrevd.111.034017","DOIUrl":"https://doi.org/10.1103/physrevd.111.034017","url":null,"abstract":"We present recent results in three-flavor chiral perturbation theory at finite isospin μ</a:mi>I</a:mi></a:msub></a:math> and strangeness <c:math xmlns:c=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><c:msub><c:mi>μ</c:mi><c:mi>S</c:mi></c:msub></c:math> chemical potentials at zero temperature. The tree-level spectrum for the mesons and gauge bosons in the pion-condensed phase is derived. The phase diagram to <e:math xmlns:e=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><e:mi mathvariant=\"script\">O</e:mi><e:mo stretchy=\"false\">(</e:mo><e:msup><e:mi>p</e:mi><e:mn>2</e:mn></e:msup><e:mo stretchy=\"false\">)</e:mo></e:math> in the <j:math xmlns:j=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><j:msub><j:mi>μ</j:mi><j:mi>I</j:mi></j:msub><j:mi>–</j:mi><j:msub><j:mi>μ</j:mi><j:mi>S</j:mi></j:msub></j:math> plane is mapped out with and without electromagnetic effects. The phase diagram consists of a vacuum phase and three Bose-condensed phases with condensates of <l:math xmlns:l=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><l:msup><l:mi>π</l:mi><l:mo>±</l:mo></l:msup></l:math>, <n:math xmlns:n=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><n:msup><n:mi>K</n:mi><n:mo>±</n:mo></n:msup></n:math>, and <p:math xmlns:p=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><p:msup><p:mi>K</p:mi><p:mn>0</p:mn></p:msup><p:mo>/</p:mo><p:msup><p:mover accent=\"true\"><p:mi>K</p:mi><p:mo stretchy=\"false\">¯</p:mo></p:mover><p:mn>0</p:mn></p:msup></p:math>, respectively. Including electromagnetic interactions, the charged Bose-condensed phases become Higgs phases via the Higgs mechanism. We calculate the pressure, energy density, isospin density, and speed of sound in the pion-condensed phase to <t:math xmlns:t=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><t:mi mathvariant=\"script\">O</t:mi><t:mo stretchy=\"false\">(</t:mo><t:msup><t:mi>p</t:mi><t:mn>4</t:mn></t:msup><t:mo stretchy=\"false\">)</t:mo></t:math>. The results are compared with recent lattice simulations and the agreement is very good for isospin chemical potentials up to approximately 180 MeV. Moreover, by integrating out the <y:math xmlns:y=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><y:mi>s</y:mi></y:math>-quark, we show that the thermodynamic quantities can be mapped onto their two-flavor counterparts with renormalized parameters. The breaking of the U(1) symmetry in the Bose-condensed phases gives rise to a Goldstone boson, whose dispersion is linear for small momenta. We use Son’s prescription to construct an effective theory for the Goldstone mode in the pion-condensed phase, which is valid for momenta p</ab:mi>≪</ab:mo>μ</ab:mi>I</ab:mi></ab:msub></ab:math>. It is shown that its damping rate is of order <cb:math xmlns:cb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><cb:msup><cb:mi>p</cb:mi><cb:mn>5</cb:mn></cb:msup></cb:math> in the nonrelativistic limit, which is Beliaev’s result for a dilute Bose gas. It is also shown that in the nonrel","PeriodicalId":20167,"journal":{"name":"Physical Review D","volume":"8 1","pages":""},"PeriodicalIF":5.0,"publicationDate":"2025-02-12","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143401509","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"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}
Physical Review DPub Date : 2025-02-12DOI: 10.1103/physrevd.111.036020
Wen Yin, Junya Yoshida
{"title":"Undulators are ALP factories","authors":"Wen Yin, Junya Yoshida","doi":"10.1103/physrevd.111.036020","DOIUrl":"https://doi.org/10.1103/physrevd.111.036020","url":null,"abstract":"Axionlike particles (ALPs), hypothetical particles, are known to be produced through axion-photon conversion in the presence of a stationary external magnetic field that is strong enough. Devices such as undulators and wigglers, which are used widely for photon production, e.g., in synchrotron radiation facilities, inherently possess strong magnetic fields, making them potential sources for ALP production without introducing additional light source or magnetic fields. In this paper, we establish formalisms and formulas for studying ALP production in the ALP-photon-charged current system based on quantum field theory. We demonstrate that ALP production is inevitable in any undulator with the standard designs due to the electron Coulomb potential as well as a “photon resonance” effect depending on the ALP mass. In particular, ALPs are predominantly produced in a direction slightly misaligned with the photons’ main direction. We propose placing detectors in the desired directions during operations of the originally planned experiments as an efficient approach to simultaneously probing ALPs. The calculation methods and formulas developed in this study are applicable to ALP production from other environments and productions of other particles beyond the standard model relevant to synchrotron radiations. <jats:supplementary-material> <jats:copyright-statement>Published by the American Physical Society</jats:copyright-statement> <jats:copyright-year>2025</jats:copyright-year> </jats:permissions> </jats:supplementary-material>","PeriodicalId":20167,"journal":{"name":"Physical Review D","volume":"63 1","pages":""},"PeriodicalIF":5.0,"publicationDate":"2025-02-12","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143401504","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"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}
Physical Review DPub Date : 2025-02-12DOI: 10.1103/physrevd.111.l041701
Oleg Antipin, Jahmall Bersini, Francesco Sannino
{"title":"Exact results for scaling dimensions of neutral operators in scalar conformal field theories","authors":"Oleg Antipin, Jahmall Bersini, Francesco Sannino","doi":"10.1103/physrevd.111.l041701","DOIUrl":"https://doi.org/10.1103/physrevd.111.l041701","url":null,"abstract":"We determine the scaling dimension Δ</a:mi>n</a:mi></a:msub></a:math> for the class of composite operators <d:math xmlns:d=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><d:msup><d:mi>ϕ</d:mi><d:mi>n</d:mi></d:msup></d:math> in the <f:math xmlns:f=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><f:mi>λ</f:mi><f:msup><f:mi>ϕ</f:mi><f:mn>4</f:mn></f:msup></f:math> theory in <h:math xmlns:h=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><h:mi>d</h:mi><h:mo>=</h:mo><h:mn>4</h:mn><h:mo>−</h:mo><h:mi>ε</h:mi></h:math> taking the double scaling limit <j:math xmlns:j=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><j:mi>n</j:mi><j:mo stretchy=\"false\">→</j:mo><j:mi>∞</j:mi></j:math> and <m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><m:mi>λ</m:mi><m:mo stretchy=\"false\">→</m:mo><m:mn>0</m:mn></m:math> with fixed <p:math xmlns:p=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><p:mi>λ</p:mi><p:mi>n</p:mi></p:math> via a semiclassical approach. Our results resum the leading power of <r:math xmlns:r=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><r:mi>n</r:mi></r:math> at any loop order. In the small <t:math xmlns:t=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><t:mi>λ</t:mi><t:mi>n</t:mi></t:math> regime we reproduce the known diagrammatic results and predict the infinite series of higher-order terms. For intermediate values of <v:math xmlns:v=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><v:mi>λ</v:mi><v:mi>n</v:mi></v:math> we find that <x:math xmlns:x=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><x:msub><x:mi mathvariant=\"normal\">Δ</x:mi><x:mi>n</x:mi></x:msub><x:mo>/</x:mo><x:mi>n</x:mi></x:math> increases monotonically approaching a (</ab:mo>λ</ab:mi>n</ab:mi>)</ab:mo>1</ab:mn>/</ab:mo>3</ab:mn></ab:mrow></ab:msup></ab:math> behavior in the <eb:math xmlns:eb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><eb:mi>λ</eb:mi><eb:mi>n</eb:mi><eb:mo stretchy=\"false\">→</eb:mo><eb:mi>∞</eb:mi></eb:math> limit. We further generalize our results to neutral operators in the <hb:math xmlns:hb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><hb:msup><hb:mi>ϕ</hb:mi><hb:mn>4</hb:mn></hb:msup></hb:math> in <jb:math xmlns:jb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><jb:mi>d</jb:mi><jb:mo>=</jb:mo><jb:mn>4</jb:mn><jb:mo>−</jb:mo><jb:mi>ε</jb:mi></jb:math>, <lb:math xmlns:lb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><lb:msup><lb:mi>ϕ</lb:mi><lb:mn>3</lb:mn></lb:msup></lb:math> in <nb:math xmlns:nb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><nb:mi>d</nb:mi><nb:mo>=</nb:mo><nb:mn>6</nb:mn><nb:mo>−</nb:mo><nb:mi>ε</nb:mi></nb:math>, and <pb:math xmlns:pb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><pb:msup><pb:mi>ϕ</pb:mi><pb:mn>6</pb:mn></pb:msup></pb:math> in <rb:math xmlns:rb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><rb:mi>d</rb:mi><rb:mo>=</rb:mo><rb:mn>3</rb:mn><rb:mo>−</rb:mo><rb:mi>ε</rb:mi></rb:math> theories wi","PeriodicalId":20167,"journal":{"name":"Physical Review D","volume":"66 1","pages":""},"PeriodicalIF":5.0,"publicationDate":"2025-02-12","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143401505","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"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}
Physical Review DPub Date : 2025-02-12DOI: 10.1103/physrevd.111.044036
Guglielmo Faggioli, Maarten van de Meent, Alessandra Buonanno, Aldo Gamboa, Mohammed Khalil, Gaurav Khanna
{"title":"Testing eccentric corrections to the radiation-reaction force in the test-mass limit of effective-one-body models","authors":"Guglielmo Faggioli, Maarten van de Meent, Alessandra Buonanno, Aldo Gamboa, Mohammed Khalil, Gaurav Khanna","doi":"10.1103/physrevd.111.044036","DOIUrl":"https://doi.org/10.1103/physrevd.111.044036","url":null,"abstract":"In this work, we test an effective-one-body radiation-reaction force for eccentric planar orbits of a test mass in a Kerr background, which contains third-order post-Newtonian (PN) nonspinning and second-order PN spin contributions. We compare the analytical fluxes connected to two different resummations of this force, truncated at different PN orders in the eccentric sector, with the numerical fluxes computed through the use of frequency- and time-domain Teukolsky-equation codes. We find that the different PN truncations of the radiation-reaction force show the expected scaling in the weak gravitational-field regime, and we observe a fractional difference with the numerical fluxes that is <</a:mo>5</a:mn>%</a:mo></a:math>, for orbits characterized by eccentricity <c:math xmlns:c=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><c:mn>0</c:mn><c:mo>≤</c:mo><c:mi>e</c:mi><c:mo>≤</c:mo><c:mn>0.7</c:mn></c:math>, central black-hole spin <e:math xmlns:e=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><e:mo>−</e:mo><e:mn>0.99</e:mn><e:mi>M</e:mi><e:mo>≤</e:mo><e:mi>a</e:mi><e:mo>≤</e:mo><e:mn>0.99</e:mn><e:mi>M</e:mi></e:math> and fixed orbital-averaged quantity <g:math xmlns:g=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><g:mi>x</g:mi><g:mo>=</g:mo><g:mo stretchy=\"false\">⟨</g:mo><g:mi>M</g:mi><g:mi mathvariant=\"normal\">Ω</g:mi><g:msup><g:mo stretchy=\"false\">⟩</g:mo><g:mrow><g:mn>2</g:mn><g:mo>/</g:mo><g:mn>3</g:mn></g:mrow></g:msup><g:mo>=</g:mo><g:mn>0.06</g:mn></g:math>, corresponding to the mildly strong-field regime with semilatera recta <l:math xmlns:l=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><l:mn>9</l:mn><l:mi>M</l:mi><l:mo><</l:mo><l:mi>p</l:mi><l:mo><</l:mo><l:mn>17</l:mn><l:mi>M</l:mi></l:math>. Our analysis provides useful information for the development of spin-aligned eccentric models in the comparable-mass case. <jats:supplementary-material> <jats:copyright-statement>Published by the American Physical Society</jats:copyright-statement> <jats:copyright-year>2025</jats:copyright-year> </jats:permissions> </jats:supplementary-material>","PeriodicalId":20167,"journal":{"name":"Physical Review D","volume":"19 1","pages":""},"PeriodicalIF":5.0,"publicationDate":"2025-02-12","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143401506","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"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}