We consider a minimal renormalizable non-supersymmetric Grand Unified Theory using fundamental representation 27 for fermions and scalars. The scalar with adjoint representation 78 is also taken for direct breaking of to SM. The proposed model, guided by TeV-scale vector-like fermions and scalar leptoquark, offers successful gauge unification even in the absence of any intermediate symmetry. Embedded with threshold corrections, it is shown to be compatible with the present experimental limit on proton decay lifetime. The unique feature of the model shows that the GUT threshold corrections to the unification mass is controlled by superheavy gauge bosons only, thereby minimizing the uncertainty of the GUT predictions. The scalar leptoquark and vector-like fermions residing in 27 representation can explain flavor physics anomalies like as reported by the LHCb collaboration and the muon anomalous magnetic moment reported by the recent muon experiment at Fermilab. The model can also predict a sub-eV scale neutrino at one-loop level via exchange of W and Z gauge bosons through MRIS mechanism.
我们考虑了一个最小可重正化的非超对称 E6 大统一理论,费米子和标量使用基本表示 27。标量的邻接表示78也用于E6到SM的直接破缺。所提出的模型由 TeV 尺度的类矢量费米子和标量轻夸克引导,即使在没有任何中间对称的情况下也能成功地实现规整统一。嵌入阈值修正后,该模型与目前质子衰变寿命的实验极限相兼容。该模型的独特之处在于,统一质量的 GUT 门限修正仅由超重规玻色子控制,从而最大限度地减少了 GUT 预测的不确定性。驻留在27表征中的标量轻夸克和类矢量费米子可以解释LHCb合作组报告的RD(∗)等味道物理反常现象,以及最近费米实验室μ介子g-2实验报告的μ介子反常磁矩。该模型还可以通过 MRIS 机制,通过 W 和 Z 规玻色子的交换,在一回路水平上预测亚 EV 尺度的中微子。
{"title":"Gauge coupling unification in a minimal non-supersymmetric E6 GUT","authors":"Chandini Dash, Snigdha Mishra, Sudhanwa Patra, Purushottam Sahu","doi":"10.1142/s0217751x24500180","DOIUrl":"https://doi.org/10.1142/s0217751x24500180","url":null,"abstract":"<p>We consider a minimal renormalizable non-supersymmetric <span><math altimg=\"eq-00002.gif\" display=\"inline\" overflow=\"scroll\"><msub><mrow><mi>E</mi></mrow><mrow><mn>6</mn></mrow></msub></math></span><span></span> Grand Unified Theory using fundamental representation 27 for fermions and scalars. The scalar with adjoint representation 78 is also taken for direct breaking of <span><math altimg=\"eq-00003.gif\" display=\"inline\" overflow=\"scroll\"><msub><mrow><mi>E</mi></mrow><mrow><mn>6</mn></mrow></msub></math></span><span></span> to SM. The proposed model, guided by TeV-scale vector-like fermions and scalar leptoquark, offers successful gauge unification even in the absence of any intermediate symmetry. Embedded with threshold corrections, it is shown to be compatible with the present experimental limit on proton decay lifetime. The unique feature of the model shows that the GUT threshold corrections to the unification mass is controlled by superheavy gauge bosons only, thereby minimizing the uncertainty of the GUT predictions. The scalar leptoquark and vector-like fermions residing in 27 representation can explain flavor physics anomalies like <span><math altimg=\"eq-00004.gif\" display=\"inline\" overflow=\"scroll\"><msub><mrow><mi>R</mi></mrow><mrow><msup><mrow><mi>D</mi></mrow><mrow><mo stretchy=\"false\">(</mo><mo>∗</mo><mo stretchy=\"false\">)</mo></mrow></msup></mrow></msub></math></span><span></span> as reported by the LHCb collaboration and the muon anomalous magnetic moment reported by the recent muon <span><math altimg=\"eq-00005.gif\" display=\"inline\" overflow=\"scroll\"><mi>g</mi><mo>−</mo><mn>2</mn></math></span><span></span> experiment at Fermilab. The model can also predict a sub-eV scale neutrino at one-loop level via exchange of <i>W</i> and <i>Z</i> gauge bosons through MRIS mechanism.</p>","PeriodicalId":50309,"journal":{"name":"International Journal of Modern Physics a","volume":"69 1","pages":""},"PeriodicalIF":1.6,"publicationDate":"2024-03-16","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140151508","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 : 2024-03-12DOI: 10.1142/s0217751x24500118
M. Abu-Shady, R. R. Luz, G. X. A. Petronilo, A. E. Santana, R. G. G. Amorim
Using the formalism of generalized fractional derivatives, a two-dimensional nonrelativistic meson system is studied. The mesons are interacting by a Cornell potential. The system is formulated in the domain of the symplectic quantum mechanics by means of the generalized fractional Nikiforov–Uvarov method. The corresponding Wigner function and the energy eigenvalues are then derived. The effect of fractional parameters and with the ground state solution is analyzed through the Wigner function for the charm–anticharm, bottom–antibottom and mesons. One of the fundamental achievements of such Cornell model is the determination of heavy quarkonia mass spectra. We have computed these masses and the present results are in agreement with the experimental data, improving previous theoretical results.
{"title":"On the fractional quark–antiquark confinement and symplectic quantum mechanics","authors":"M. Abu-Shady, R. R. Luz, G. X. A. Petronilo, A. E. Santana, R. G. G. Amorim","doi":"10.1142/s0217751x24500118","DOIUrl":"https://doi.org/10.1142/s0217751x24500118","url":null,"abstract":"<p>Using the formalism of generalized fractional derivatives, a two-dimensional nonrelativistic meson system is studied. The mesons are interacting by a Cornell potential. The system is formulated in the domain of the symplectic quantum mechanics by means of the generalized fractional Nikiforov–Uvarov method. The corresponding Wigner function and the energy eigenvalues are then derived. The effect of fractional parameters <span><math altimg=\"eq-00001.gif\" display=\"inline\" overflow=\"scroll\"><mi>α</mi></math></span><span></span> and <span><math altimg=\"eq-00002.gif\" display=\"inline\" overflow=\"scroll\"><mi>β</mi></math></span><span></span> with the ground state solution is analyzed through the Wigner function for the charm–anticharm, bottom–antibottom and <span><math altimg=\"eq-00003.gif\" display=\"inline\" overflow=\"scroll\"><mi>b</mi><mover accent=\"true\"><mrow><mi>c</mi></mrow><mo accent=\"true\">¯</mo></mover></math></span><span></span> mesons. One of the fundamental achievements of such Cornell model is the determination of heavy quarkonia mass spectra. We have computed these masses and the present results are in agreement with the experimental data, improving previous theoretical results.</p>","PeriodicalId":50309,"journal":{"name":"International Journal of Modern Physics a","volume":"73 1","pages":""},"PeriodicalIF":1.6,"publicationDate":"2024-03-12","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140106119","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 : 2024-03-12DOI: 10.1142/s0217751x24500040
Iver H. Brevik, Moshe M. Chaichian, Amedeo M. Favitta
We analyze the Axion Electrodynamics in a two-dimensional slab of finite width L containing a homogeneous and isotropic dielectric medium with constant permittivity and permeability. We start from the known decomposition of modes in the nonaxion case and then solve perturbatively the governing equations for the electromagnetic fields to which the axions are also coupled. This is a natural approach, since the finiteness of L destroys the spatial invariance of the theory in the z-direction normal to the plates. In this way, we derive the value of the axion-generated rotation angle of the electric and magnetic fields after their passage through the slab, and use the obtained results to calculate the Casimir force between the two conducting plates. Our calculations make use of the same method as previously outlined by [J. S. Høye and I. Brevik, Eur. Phys. J. Plus135, 271 (2020)] for the case of Casimir calculations in chiral media and extend former results on the Casimir force in Axion Electrodynamics.
我们分析了在有限宽度 L 的二维板中的轴子电动力学,该板包含具有恒定介电常数和磁导率的均质各向同性介电介质。我们从已知的非轴子情况下的模式分解出发,然后对轴子也耦合到其中的电磁场的治理方程进行扰动求解。这是一种自然的方法,因为 L 的有限性破坏了理论在板块法线 Z 方向上的空间不变性。通过这种方法,我们可以推导出电场和磁场穿过板后轴心产生的旋转角值,并利用得到的结果计算两块导电板之间的卡西米尔力。我们的计算采用了[J. S. Høye and I. Brevik, Eur. Phys. J. Plus 135, 271 (2020)]先前概述的用于手性介质中卡西米尔计算的相同方法,并扩展了轴子电动力学中卡西米尔力的前人成果。
{"title":"On the Axion Electrodynamics in a two-dimensional slab and the Casimir effect","authors":"Iver H. Brevik, Moshe M. Chaichian, Amedeo M. Favitta","doi":"10.1142/s0217751x24500040","DOIUrl":"https://doi.org/10.1142/s0217751x24500040","url":null,"abstract":"<p>We analyze the Axion Electrodynamics in a two-dimensional slab of finite width <i>L</i> containing a homogeneous and isotropic dielectric medium with constant permittivity and permeability. We start from the known decomposition of modes in the nonaxion case and then solve perturbatively the governing equations for the electromagnetic fields to which the axions are also coupled. This is a natural approach, since the finiteness of <i>L</i> destroys the spatial invariance of the theory in the <i>z</i>-direction normal to the plates. In this way, we derive the value of the axion-generated rotation angle of the electric and magnetic fields after their passage through the slab, and use the obtained results to calculate the Casimir force between the two conducting plates. Our calculations make use of the same method as previously outlined by [J. S. Høye and I. Brevik, <i>Eur. Phys. J. Plus</i> <b>135</b>, 271 (2020)] for the case of Casimir calculations in chiral media and extend former results on the Casimir force in Axion Electrodynamics.</p>","PeriodicalId":50309,"journal":{"name":"International Journal of Modern Physics a","volume":"130 1","pages":""},"PeriodicalIF":1.6,"publicationDate":"2024-03-12","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140106211","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 : 2024-03-09DOI: 10.1142/s0217751x24500155
Andrei T. Patrascu
The holographic principle and its realization as the anti-de Sitter/conformal field theory (AdS/CFT) correspondence leads to the existence of the so-called precursor operators. These are boundary operators that carry nonlocal information regarding events occurring deep inside the bulk and which cannot be causally connected to the boundary. Such nonlocal operators can distinguish nonvacuum-like excitations within the bulk that cannot be observed by any local gauge invariant operators in the boundary. The boundary precursors are expected to become increasingly nonlocal the further the bulk process is from the boundary. Such phenomena are expected to be related to the extended nature of the strings. Standard gauge invariance in the boundary theory equates to quantum error correction which furthermore establishes localization of bulk information. I show that when double field theory quantum error correction prescriptions are considered in the bulk, gauge invariance in the boundary manifests residual effects associated to stringy winding modes. Also, an effect of double field theory quantum error correction is the appearance of positive cosmological constant. The emergence of space–time from the entanglement structure of a dual quantum field theory appears in this context to generalize for de Sitter space–times as well.
{"title":"Cosmological constant as quantum error correction from generalized gauge invariance in double field theory","authors":"Andrei T. Patrascu","doi":"10.1142/s0217751x24500155","DOIUrl":"https://doi.org/10.1142/s0217751x24500155","url":null,"abstract":"<p>The holographic principle and its realization as the anti-de Sitter/conformal field theory (AdS/CFT) correspondence leads to the existence of the so-called precursor operators. These are boundary operators that carry nonlocal information regarding events occurring deep inside the bulk and which cannot be causally connected to the boundary. Such nonlocal operators can distinguish nonvacuum-like excitations within the bulk that cannot be observed by any local gauge invariant operators in the boundary. The boundary precursors are expected to become increasingly nonlocal the further the bulk process is from the boundary. Such phenomena are expected to be related to the extended nature of the strings. Standard gauge invariance in the boundary theory equates to quantum error correction which furthermore establishes localization of bulk information. I show that when double field theory quantum error correction prescriptions are considered in the bulk, gauge invariance in the boundary manifests residual effects associated to stringy winding modes. Also, an effect of double field theory quantum error correction is the appearance of positive cosmological constant. The emergence of space–time from the entanglement structure of a dual quantum field theory appears in this context to generalize for de Sitter space–times as well.</p>","PeriodicalId":50309,"journal":{"name":"International Journal of Modern Physics a","volume":"308 1","pages":""},"PeriodicalIF":1.6,"publicationDate":"2024-03-09","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140108173","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}
Machine learning has blossomed in recent decades and has become essential in many fields. It significantly solved some problems in particle physics — particle reconstruction, event classification, etc. However, it is now time to break the limitation of conventional machine learning with quantum computing. A support-vector machine algorithm with a quantum kernel estimator (QSVM-Kernel) leverages high-dimensional quantum state space to identify a signal from backgrounds. In this study, we have pioneered employing this quantum machine learning algorithm to study the process at the Circular Electron–Positron Collider (CEPC), a proposed Higgs factory to study electroweak symmetry breaking of particle physics. Using 6 qubits on quantum computer simulators, we optimized the QSVM-Kernel algorithm and obtained a classification performance similar to the classical support-vector machine algorithm. Furthermore, we have validated the QSVM-Kernel algorithm using 6-qubits on quantum computer hardware from both IBM and Origin Quantum: the classification performances of both are approaching noiseless quantum computer simulators. In addition, the Origin Quantum hardware results are similar to the IBM Quantum hardware within the uncertainties in our study. Our study shows that state-of-the-art quantum computing technologies could be utilized by particle physics, a branch of fundamental science that relies on big experimental data.
近几十年来,机器学习蓬勃发展,在许多领域都变得不可或缺。它极大地解决了粒子物理学中的一些问题--粒子重构、事件分类等。然而,现在是时候用量子计算打破传统机器学习的局限了。带有量子核估计器的支持向量机算法(QSVM-Kernel)利用高维量子态空间从背景中识别信号。在这项研究中,我们率先采用了这种量子机器学习算法来研究环形电子-正子对撞机(CEPC)上的e+e-→ZH过程,CEPC是拟建的希格斯工厂,用于研究粒子物理的电弱对称破缺。我们使用量子计算机模拟器上的 6 个量子比特优化了 QSVM 内核算法,并获得了与经典支持向量机算法类似的分类性能。此外,我们还在 IBM 和 Origin Quantum 的量子计算机硬件上使用 6 量子比特验证了 QSVM-Kernel 算法:两者的分类性能都接近无噪声量子计算机模拟器。此外,在我们研究的不确定性范围内,Origin Quantum 硬件的结果与 IBM Quantum 硬件相似。我们的研究表明,最先进的量子计算技术可以被粒子物理学这一依赖于大量实验数据的基础科学分支所利用。
{"title":"Application of quantum machine learning in a Higgs physics study at the CEPC","authors":"Abdualazem Fadol, Qiyu Sha, Yaquan Fang, Zhan Li, Sitian Qian, Yuyang Xiao, Yu Zhang, Chen Zhou","doi":"10.1142/s0217751x24500076","DOIUrl":"https://doi.org/10.1142/s0217751x24500076","url":null,"abstract":"<p>Machine learning has blossomed in recent decades and has become essential in many fields. It significantly solved some problems in particle physics — particle reconstruction, event classification, etc. However, it is now time to break the limitation of conventional machine learning with quantum computing. A support-vector machine algorithm with a quantum kernel estimator (QSVM-Kernel) leverages high-dimensional quantum state space to identify a signal from backgrounds. In this study, we have pioneered employing this quantum machine learning algorithm to study the <span><math altimg=\"eq-00001.gif\" display=\"inline\" overflow=\"scroll\"><msup><mrow><mi>e</mi></mrow><mrow><mo>+</mo></mrow></msup><msup><mrow><mi>e</mi></mrow><mrow><mo>−</mo></mrow></msup><mo>→</mo><mi>Z</mi><mi>H</mi></math></span><span></span> process at the Circular Electron–Positron Collider (CEPC), a proposed Higgs factory to study electroweak symmetry breaking of particle physics. Using 6 qubits on quantum computer simulators, we optimized the QSVM-Kernel algorithm and obtained a classification performance similar to the classical support-vector machine algorithm. Furthermore, we have validated the QSVM-Kernel algorithm using 6-qubits on quantum computer hardware from both IBM and Origin Quantum: the classification performances of both are approaching noiseless quantum computer simulators. In addition, the Origin Quantum hardware results are similar to the IBM Quantum hardware within the uncertainties in our study. Our study shows that state-of-the-art quantum computing technologies could be utilized by particle physics, a branch of fundamental science that relies on big experimental data.</p>","PeriodicalId":50309,"journal":{"name":"International Journal of Modern Physics a","volume":"277 1","pages":""},"PeriodicalIF":1.6,"publicationDate":"2024-03-07","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140044625","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 : 2024-03-07DOI: 10.1142/s0217751x23501877
R. Chahri, S. Mouslih, M. Jakha, B. Manaut, S. Taj
In a previous paper, we showed theoretically that the total cross-section of the top-quark pair production by electron–positron annihilation is strongly reduced by the presence of a circularly polarized laser field. In this paper, we present the result for the case of a linearly polarized laser field. This time, the total cross-section is significantly enhanced by the laser field.
{"title":"Top-quark pair production by electron–positron scattering in a linearly polarized laser field","authors":"R. Chahri, S. Mouslih, M. Jakha, B. Manaut, S. Taj","doi":"10.1142/s0217751x23501877","DOIUrl":"https://doi.org/10.1142/s0217751x23501877","url":null,"abstract":"<p>In a previous paper, we showed theoretically that the total cross-section of the top-quark pair production by electron–positron annihilation is strongly reduced by the presence of a circularly polarized laser field. In this paper, we present the result for the case of a linearly polarized laser field. This time, the total cross-section is significantly enhanced by the laser field.</p>","PeriodicalId":50309,"journal":{"name":"International Journal of Modern Physics a","volume":"7 1","pages":""},"PeriodicalIF":1.6,"publicationDate":"2024-03-07","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140044951","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 : 2024-03-06DOI: 10.1142/s0217751x24500064
Gábor Kasza
In high-energy heavy-ion collisions, a nearly perfect fluid, the so-called strongly coupled quark–gluon plasma (QGP), forms. After the short period of thermalization, the evolution of this medium can be described by the laws of relativistic hydrodynamics. The time evolution of the QGP can be understood through direct photon spectra measurements, which are sensitive to the entire period between the thermalization and the freeze-out of the medium. I present a new analytic formula that describes the thermal photon radiation and it is derived from an exact and finite solution of relativistic hydrodynamics with accelerating velocity field. Then I compare my calculations to the most recent nonprompt spectrum of direct photons for at GeV collisions. I have found a convincing agreement between the model and the data, which allows to give an estimate of the initial temperature in the center of the fireball. My results predict hydrodynamic scaling behavior for the thermal photon spectra of high-energy heavy-ion collisions.
{"title":"Describing the thermal radiation in Au+Au collisions at sNN=200 GeV by an analytic solution of relativistic hydrodynamics","authors":"Gábor Kasza","doi":"10.1142/s0217751x24500064","DOIUrl":"https://doi.org/10.1142/s0217751x24500064","url":null,"abstract":"<p>In high-energy heavy-ion collisions, a nearly perfect fluid, the so-called strongly coupled quark–gluon plasma (QGP), forms. After the short period of thermalization, the evolution of this medium can be described by the laws of relativistic hydrodynamics. The time evolution of the QGP can be understood through direct photon spectra measurements, which are sensitive to the entire period between the thermalization and the freeze-out of the medium. I present a new analytic formula that describes the thermal photon radiation and it is derived from an exact and finite solution of relativistic hydrodynamics with accelerating velocity field. Then I compare my calculations to the most recent nonprompt spectrum of direct photons for <span><math altimg=\"eq-00003.gif\" display=\"inline\" overflow=\"scroll\"><mstyle><mtext mathvariant=\"normal\">Au</mtext></mstyle><mo>+</mo><mstyle><mtext mathvariant=\"normal\">Au</mtext></mstyle></math></span><span></span> at <span><math altimg=\"eq-00004.gif\" display=\"inline\" overflow=\"scroll\"><msqrt><mrow><msub><mrow><mi>s</mi></mrow><mrow><mi>N</mi><mi>N</mi></mrow></msub></mrow></msqrt><mo>=</mo><mn>2</mn><mn>0</mn><mn>0</mn></math></span><span></span><span><math altimg=\"eq-00005.gif\" display=\"inline\" overflow=\"scroll\"><mspace width=\".17em\"></mspace></math></span><span></span>GeV collisions. I have found a convincing agreement between the model and the data, which allows to give an estimate of the initial temperature in the center of the fireball. My results predict hydrodynamic scaling behavior for the thermal photon spectra of high-energy heavy-ion collisions.</p>","PeriodicalId":50309,"journal":{"name":"International Journal of Modern Physics a","volume":"194 1","pages":""},"PeriodicalIF":1.6,"publicationDate":"2024-03-06","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140044752","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 : 2024-03-06DOI: 10.1142/s0217751x24500106
Mehdi Sadeghi, Faramaz Rahmani
In this paper, we shall study the phase transition of nonminimal coupling of Einstein–Hilbert gravity and electric field of Yang–Mills type in AdS space–time. We couple the Ricci scalar to the Yang–Mills invariant to obtain a modified theory of gravity. A black brane solution is introduced up to the first order of the term in this model. Then, the phase transition of this solution will be investigated in canonical ensemble. Our investigation shows that only the second-order phase transition behavior is seen in this model. Also, due to the coupling of the Yang–Mills field and Ricci scalar, there are differences with the phase transitions of the usual minimal models. We shall show that in the absence of nonminimal coupling there is not any phase transition.
{"title":"The phase transition of nonminimal Yang–Mills AdS black brane","authors":"Mehdi Sadeghi, Faramaz Rahmani","doi":"10.1142/s0217751x24500106","DOIUrl":"https://doi.org/10.1142/s0217751x24500106","url":null,"abstract":"<p>In this paper, we shall study the phase transition of nonminimal coupling of Einstein–Hilbert gravity and electric field of Yang–Mills type in AdS space–time. We couple the Ricci scalar to the Yang–Mills invariant to obtain a modified theory of gravity. A black brane solution is introduced up to the first order of the term <span><math altimg=\"eq-00001.gif\" display=\"inline\" overflow=\"scroll\"><mi>R</mi><msubsup><mrow><mi>F</mi></mrow><mrow><mi>μ</mi><mi>α</mi></mrow><mrow><mo stretchy=\"false\">(</mo><mi>a</mi><mo stretchy=\"false\">)</mo></mrow></msubsup><msup><mrow><mi>F</mi></mrow><mrow><mo stretchy=\"false\">(</mo><mi>a</mi><mo stretchy=\"false\">)</mo><mi>μ</mi><mi>α</mi></mrow></msup></math></span><span></span> in this model. Then, the phase transition of this solution will be investigated in canonical ensemble. Our investigation shows that only the second-order phase transition behavior is seen in this model. Also, due to the coupling of the Yang–Mills field and Ricci scalar, there are differences with the phase transitions of the usual minimal models. We shall show that in the absence of nonminimal coupling there is not any phase transition.</p>","PeriodicalId":50309,"journal":{"name":"International Journal of Modern Physics a","volume":"271 1","pages":""},"PeriodicalIF":1.6,"publicationDate":"2024-03-06","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140045107","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 : 2024-02-17DOI: 10.1142/s0217751x24500039
J. Klusoň
In this short note, we present analysis of the tachyon kink solution on the world-volume of unstable Dp-brane in general background as the solution of the Hamiltonian equations of motion. We also find Hamiltonian for simplified system of Dp-brane and anti-Dp-brane and study its properties.
{"title":"Canonical description of the tachyon kink in general background and Hamiltonian for Dp-brane-anti-Dp-brane system","authors":"J. Klusoň","doi":"10.1142/s0217751x24500039","DOIUrl":"https://doi.org/10.1142/s0217751x24500039","url":null,"abstract":"<p>In this short note, we present analysis of the tachyon kink solution on the world-volume of unstable Dp-brane in general background as the solution of the Hamiltonian equations of motion. We also find Hamiltonian for simplified system of Dp-brane and anti-Dp-brane and study its properties.</p>","PeriodicalId":50309,"journal":{"name":"International Journal of Modern Physics a","volume":"35 1","pages":""},"PeriodicalIF":1.6,"publicationDate":"2024-02-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140045105","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 : 2024-02-16DOI: 10.1142/s0217751x23501907
Zahra Rezaei, S. Peyman Zakeri
In this paper, we explore the noncommutative space–time to revive the idea that gamma-ray excess in the galactic center may stem from the annihilation of particle dark matter. In the noncommutative theory, the photon spectrum is produced by direct emission during this annihilation wherein a photon can be embed in the final state together with other direct products in new vertices. In the various configurations of dark matter phenomenology, we pursue the most prevalent model known as singlet scalar. Calculating the relevant aspects of the model and determining the parameters phase space, we derive the photon flux in the galactic center. This region, known for its high density and occasional existence of robust magnetic fields, serves as an ideal location for investigating theories that encompass the concept of Lorentz symmetry breaking. Upon comparing our numerical achievements with experimental data, it becomes evident that noncommutative space–time can be a reliable framework to explain the gamma-ray excess.
{"title":"Singlet scalar dark matter in the noncommutative space–time: A viable hypothesis to explain the gamma-ray excess in the galactic center","authors":"Zahra Rezaei, S. Peyman Zakeri","doi":"10.1142/s0217751x23501907","DOIUrl":"https://doi.org/10.1142/s0217751x23501907","url":null,"abstract":"<p>In this paper, we explore the noncommutative space–time to revive the idea that gamma-ray excess in the galactic center may stem from the annihilation of particle dark matter. In the noncommutative theory, the photon spectrum is produced by direct emission during this annihilation wherein a photon can be embed in the final state together with other direct products in new vertices. In the various configurations of dark matter phenomenology, we pursue the most prevalent model known as singlet scalar. Calculating the relevant aspects of the model and determining the parameters phase space, we derive the photon flux in the galactic center. This region, known for its high density and occasional existence of robust magnetic fields, serves as an ideal location for investigating theories that encompass the concept of Lorentz symmetry breaking. Upon comparing our numerical achievements with experimental data, it becomes evident that noncommutative space–time can be a reliable framework to explain the gamma-ray excess.</p>","PeriodicalId":50309,"journal":{"name":"International Journal of Modern Physics a","volume":"17 1","pages":""},"PeriodicalIF":1.6,"publicationDate":"2024-02-16","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140129183","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}