Pub Date : 2024-08-14DOI: 10.1134/s1547477124700742
A. S. Batova, D. L. Pilinskaya, E. B. Dushanov, E. A. Nasonova, A. N. Bugai
Abstract
This work aims at mathematically simulating the repair process of double-strand DNA breaks induced by rare ionizing radiation. A mathematical simulation of several stages of the cellular response to irradiation has been carried out: (i) Chinese hamster cells of the V79 line in the stationary phase of culture growth to the action of 250 keV X-ray irradiation and (ii) human carcinoma cells in the exponential phase of culture growth to (gamma )-Co(^{{60}}) irradiation. The induction and repair of DNA double-strand breaks and the kinetics of formation of incorrectly repaired DNA double-strand breaks are studied. The simulation data are compared with experimental values.
摘要 这项工作旨在对稀有电离辐射诱导的双链 DNA 断裂的修复过程进行数学模拟。对细胞对辐照反应的几个阶段进行了数学模拟:(i)处于培养生长静止期的中国仓鼠 V79 系细胞对 250 keV X 射线辐照的反应;(ii)处于培养生长指数期的人类癌细胞对 (γ )-Co(^{{60}}) 辐照的反应。研究了 DNA 双链断裂的诱导和修复以及错误修复的 DNA 双链断裂的形成动力学。模拟数据与实验值进行了比较。
{"title":"Repair Kinetics of DNA Double-Strand Breaks in Mammalian Cells under Photon Irradiation","authors":"A. S. Batova, D. L. Pilinskaya, E. B. Dushanov, E. A. Nasonova, A. N. Bugai","doi":"10.1134/s1547477124700742","DOIUrl":"https://doi.org/10.1134/s1547477124700742","url":null,"abstract":"<h3 data-test=\"abstract-sub-heading\">Abstract</h3><p>This work aims at mathematically simulating the repair process of double-strand DNA breaks induced by rare ionizing radiation. A mathematical simulation of several stages of the cellular response to irradiation has been carried out: (i) Chinese hamster cells of the V79 line in the stationary phase of culture growth to the action of 250 keV X-ray irradiation and (ii) human carcinoma cells in the exponential phase of culture growth to <span>(gamma )</span>-Co<span>(^{{60}})</span> irradiation. The induction and repair of DNA double-strand breaks and the kinetics of formation of incorrectly repaired DNA double-strand breaks are studied. The simulation data are compared with experimental values.</p>","PeriodicalId":730,"journal":{"name":"Physics of Particles and Nuclei Letters","volume":"8 1","pages":""},"PeriodicalIF":0.5,"publicationDate":"2024-08-14","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142176685","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}
Pub Date : 2024-08-14DOI: 10.1134/s1547477124700894
A. A. Provorov
Abstract
Characteristic identities for (2)- and (3)-split Casimir algebra operators (D(2,1;alpha )) in representations (a{{d}^{{ otimes 2}}}) and (a{{d}^{{ otimes 3}}}) are found; projectors onto the invariant subspaces of these representations are constructed, and formulas for their supertraces are derived. All formulas agree with the universal description of subrepresentations of representations (a{{d}^{{ otimes 2}}}) and (a{{d}^{{ otimes 3}}}) of basic classical Lie superalgebras in terms of Vogel parameters.
{"title":"Split Casimir Operator of Algebra $$D(2,1;alpha )$$ in Representations $$a{{d}^{{ otimes 2}}}$$ and $$a{{d}^{{ otimes 3}}}$$ and Vogel Parameterization","authors":"A. A. Provorov","doi":"10.1134/s1547477124700894","DOIUrl":"https://doi.org/10.1134/s1547477124700894","url":null,"abstract":"<h3 data-test=\"abstract-sub-heading\">Abstract</h3><p>Characteristic identities for <span>(2)</span>- and <span>(3)</span>-split Casimir algebra operators <span>(D(2,1;alpha ))</span> in representations <span>(a{{d}^{{ otimes 2}}})</span> and <span>(a{{d}^{{ otimes 3}}})</span> are found; projectors onto the invariant subspaces of these representations are constructed, and formulas for their supertraces are derived. All formulas agree with the universal description of subrepresentations of representations <span>(a{{d}^{{ otimes 2}}})</span> and <span>(a{{d}^{{ otimes 3}}})</span> of basic classical Lie superalgebras in terms of Vogel parameters.</p>","PeriodicalId":730,"journal":{"name":"Physics of Particles and Nuclei Letters","volume":"22 1","pages":""},"PeriodicalIF":0.5,"publicationDate":"2024-08-14","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142176698","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}
Pub Date : 2024-08-14DOI: 10.1134/s1547477124700924
A. G. Kharlamov, T. A. Kharlamova, V. N. Zhabin, A. S. Kupich
Abstract
The contribution of the direct interaction vertex to the (Z to {{l}^{ + }}{{l}^{ - }}gamma ) process is extracted on basis of a measurement of differential distributions over the invariant mass ({{l}^{ pm }}gamma ) at the ATLAS detector. Models of CP-violating effective interaction and CP-preserving effective interaction are considered. The direct vertex can be seen as an effective description of loop corrections within the Standard Model. The contribution of the direct vertex in the CP-preserving model lead to ({text{Br}}left( {Z to {{e}^{ + }}{{e}^{ - }}gamma } right) = left( {3.81 pm 0.53} right) times {{10}^{{ - 5}}},)({text{Br}}left( {Z to {{mu }^{ + }}{{mu }^{ - }}gamma } right) = left( {3.99 pm 0.47} right) times {{10}^{{ - 5}}}.) Adding an effective model to predictions of the modern PowHeg+PHOTOS and Sherpa 2.2 generators significantly improves the agreement with experimental results. The significance of the additive was 5 and 4.7 standard deviations for PowHeg+PHOTOS and Sherpa 2.2, respectively. The PowHeg+PHOTOS generator with the effective interaction additive describes the experimental data slightly better than other generators with the same type of effective additive.
Abstract The contribution of the direct interaction vertex to the (Z to {{l}^{ + }}{{l}^{ - }}gamma) process is extracted on basis of a measurement of differential distributions over the invariant mass ({{l}^{ pm }}gamma) at the ATLAS detector.考虑了违反CP的有效相互作用模型和保留CP的有效相互作用模型。直接顶点可以看作是对标准模型中环路修正的有效描述。在CP保留模型中,直接顶点的贡献导致({text{Br}}left( {Z to {{e}^{ + }}{{e}^{ - }}gamma } right) = left( {3.81 pm 0.53} right) times {{10}^{ - 5}}},)({text{Br}}left( {Z to {{mu }^{ + }}{{mu }^{ - }}gamma } right) = left( {3.99 pm 0.47} right) times {{10}^{ - 5}}}.)在现代 PowHeg+PHOTOS 和 Sherpa 2.2 发生器的预测中加入有效模型,可以显著提高与实验结果的一致性。在 PowHeg+PHOTOS 和 Sherpa 2.2 中,添加剂的显著性分别为 5 和 4.7 个标准差。使用有效相互作用添加剂的 PowHeg+PHOTOS 生成器对实验数据的描述略好于使用同类有效添加剂的其他生成器。
{"title":"Contribution of the Direct Interaction Vertex to the Z → l+l–γ Process","authors":"A. G. Kharlamov, T. A. Kharlamova, V. N. Zhabin, A. S. Kupich","doi":"10.1134/s1547477124700924","DOIUrl":"https://doi.org/10.1134/s1547477124700924","url":null,"abstract":"<h3 data-test=\"abstract-sub-heading\">Abstract</h3><p>The contribution of the direct interaction vertex to the <span>(Z to {{l}^{ + }}{{l}^{ - }}gamma )</span> process is extracted on basis of a measurement of differential distributions over the invariant mass <span>({{l}^{ pm }}gamma )</span> at the ATLAS detector. Models of CP-violating effective interaction and CP-preserving effective interaction are considered. The direct vertex can be seen as an effective description of loop corrections within the Standard Model. The contribution of the direct vertex in the CP-preserving model lead to <span>({text{Br}}left( {Z to {{e}^{ + }}{{e}^{ - }}gamma } right) = left( {3.81 pm 0.53} right) times {{10}^{{ - 5}}},)</span> <span>({text{Br}}left( {Z to {{mu }^{ + }}{{mu }^{ - }}gamma } right) = left( {3.99 pm 0.47} right) times {{10}^{{ - 5}}}.)</span> Adding an effective model to predictions of the modern PowHeg+PHOTOS and Sherpa 2.2 generators significantly improves the agreement with experimental results. The significance of the additive was 5 and 4.7 standard deviations for PowHeg+PHOTOS and Sherpa 2.2, respectively. The PowHeg+PHOTOS generator with the effective interaction additive describes the experimental data slightly better than other generators with the same type of effective additive.</p>","PeriodicalId":730,"journal":{"name":"Physics of Particles and Nuclei Letters","volume":"77 1","pages":""},"PeriodicalIF":0.5,"publicationDate":"2024-08-14","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142176699","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}
Pub Date : 2024-08-14DOI: 10.1134/s1547477124701292
O. Yu. Ponomareva, S. V. Sumnikov, R. N. Vasin, E. A. Korneeva, N. Yu. Samoylova
Abstract
Prussian white is the promising cathode material for rechargeable sodium ion batteries. Here we study phase transitions in commercial Prussian White powder with particle size up to ~10 μm, which was chemically enriched with sodium, and synthesized sodium-enriched Prussian White with particle size of ~1 μm. X-ray diffraction was used to track structural changes during heating up to 250°C. Both powders were found to undergo the transformation of initial rhombohedral phase to dehydrated rhombohedral phase through a formation of cubic phase. Smaller particle size of the synthesized powder leads to more effective dehydration, which decreases temperatures of all phase transitions by ≈10°C compared to commercial Na-enriched Prussian White.
{"title":"Phase Transformations in Na-Rich Prussian White Cathode Materials with Different Morphology","authors":"O. Yu. Ponomareva, S. V. Sumnikov, R. N. Vasin, E. A. Korneeva, N. Yu. Samoylova","doi":"10.1134/s1547477124701292","DOIUrl":"https://doi.org/10.1134/s1547477124701292","url":null,"abstract":"<h3 data-test=\"abstract-sub-heading\">Abstract</h3><p>Prussian white is the promising cathode material for rechargeable sodium ion batteries. Here we study phase transitions in commercial Prussian White powder with particle size up to ~10 μm, which was chemically enriched with sodium, and synthesized sodium-enriched Prussian White with particle size of ~1 μm. X-ray diffraction was used to track structural changes during heating up to 250°C. Both powders were found to undergo the transformation of initial rhombohedral phase to dehydrated rhombohedral phase through a formation of cubic phase. Smaller particle size of the synthesized powder leads to more effective dehydration, which decreases temperatures of all phase transitions by ≈10°C compared to commercial Na-enriched Prussian White.</p>","PeriodicalId":730,"journal":{"name":"Physics of Particles and Nuclei Letters","volume":"107 1","pages":""},"PeriodicalIF":0.5,"publicationDate":"2024-08-14","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142176848","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}
Pub Date : 2024-08-14DOI: 10.1134/S1547477124700900
Ye. Hambardzumyan, Yu. Kharlov
ALICE3 is a next-generation heavy-ion experiment at the LHC, a successor of the ALICE experiment. It opens a high-precision domain to the strongly interacting matter studies. A set of ALICE3 measurements requires electron identification with high efficiency and purity, which will be performed using several complementing experimental techniques. Feasibility of electron identification using electromagnetic calorimeter clusters matched with tracks reconstructed in the central tracker is studied withing the ALICE3 simulation and analysis framework. Electron identification criteria are optimized against efficiency and hadron contamination suppression and applied to charmonium (1P) reconstruction in pp collisions via the ({{chi }_{{cJ}}} to J{text{/}}psi + gamma ) decay channel. Feasibility to reconstruct the charmonium states in pp collisions at the ALICE3 is discussed.
ALICE3 是在大型强子对撞机上进行的下一代重离子实验,是 ALICE 实验的继承者。它为强相互作用物质研究开辟了一个高精度领域。ALICE3 的一系列测量需要高效率和高纯度的电子识别,这将通过几种辅助实验技术来实现。在 ALICE3 模拟和分析框架内,研究了使用与中央跟踪器重建的轨迹相匹配的电磁量热计集群进行电子识别的可行性。根据效率和强子污染抑制对电子识别标准进行了优化,并通过({chi }_{cJ}} to J{text{/}}psi + gamma )衰变通道应用于pp对撞中的粲(1P)重建。讨论了在ALICE3的pp对撞中重建粲态的可行性。
{"title":"Electron Identification with the Electromagnetic Calorimeter and Its Application for Charmonia Studies in the Experiment ALICE3 at the LHC","authors":"Ye. Hambardzumyan, Yu. Kharlov","doi":"10.1134/S1547477124700900","DOIUrl":"10.1134/S1547477124700900","url":null,"abstract":"<p>ALICE3 is a next-generation heavy-ion experiment at the LHC, a successor of the ALICE experiment. It opens a high-precision domain to the strongly interacting matter studies. A set of ALICE3 measurements requires electron identification with high efficiency and purity, which will be performed using several complementing experimental techniques. Feasibility of electron identification using electromagnetic calorimeter clusters matched with tracks reconstructed in the central tracker is studied withing the ALICE3 simulation and analysis framework. Electron identification criteria are optimized against efficiency and hadron contamination suppression and applied to charmonium (1P) reconstruction in pp collisions via the <span>({{chi }_{{cJ}}} to J{text{/}}psi + gamma )</span> decay channel. Feasibility to reconstruct the charmonium states in pp collisions at the ALICE3 is discussed.</p>","PeriodicalId":730,"journal":{"name":"Physics of Particles and Nuclei Letters","volume":"21 4","pages":"642 - 645"},"PeriodicalIF":0.4,"publicationDate":"2024-08-14","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142411672","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}
Pub Date : 2024-08-14DOI: 10.1134/S1547477124700705
V. O. Galkin, E. M. Savchenko
Masses of the ground and excited states of asymmetric fully heavy tetraquarks with open charm and/or bottom are calculated within the relativistic quark model, based on the quasipotential approach and QCD, and diquark-antidiquark picture of tetraquarks. The relativistic diquark-antidiquark interaction quasipotential takes into account the internal structure of the diquark and all spin-dependent and spin-independent relativistic corrections. It is shown, that there is a significant mixing between the asymmetric in flavor states of tetraquarks with the same total momentum-parity (({{J}^{P}})), but different full spins of the tetraquark ((S)) within the same excitation. The calculated masses of such tetraquarks are compared with the fall-apart decay thresholds into a pair of heavy mesons. The states that could be observed as narrow resonances are determined.
{"title":"Relativistic Description of Asymmetric Fully Heavy Tetraquarks","authors":"V. O. Galkin, E. M. Savchenko","doi":"10.1134/S1547477124700705","DOIUrl":"10.1134/S1547477124700705","url":null,"abstract":"<p>Masses of the ground and excited states of asymmetric fully heavy tetraquarks with open charm and/or bottom are calculated within the relativistic quark model, based on the quasipotential approach and QCD, and diquark-antidiquark picture of tetraquarks. The relativistic diquark-antidiquark interaction quasipotential takes into account the internal structure of the diquark and all spin-dependent and spin-independent relativistic corrections. It is shown, that there is a significant mixing between the asymmetric in flavor states of tetraquarks with the same total momentum-parity (<span>({{J}^{P}})</span>), but different full spins of the tetraquark (<span>(S)</span>) within the same excitation. The calculated masses of such tetraquarks are compared with the fall-apart decay thresholds into a pair of heavy mesons. The states that could be observed as narrow resonances are determined.</p>","PeriodicalId":730,"journal":{"name":"Physics of Particles and Nuclei Letters","volume":"21 4","pages":"597 - 600"},"PeriodicalIF":0.4,"publicationDate":"2024-08-14","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142411684","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}
Pub Date : 2024-08-14DOI: 10.1134/S1547477124700584
N. A. Avdeev, P. I. Dyadina
In this work, accretion onto spherically symmetric black hole in hybrid metric-Palatini (f(R))-gravity was studied within the framework of the Novikov–Thorn model. The average energy flux from the disk surface was numerically obtained for two cases: (V = 0) and (V = - frac{{{{mu }^{2}}}}{2}{{phi }^{2}} + frac{zeta }{4}{{phi }^{4}}). We also note that in each considered case, the prediction of the theory for this quantity are compared with similar result for the Schwarzschild black hole.
在这项工作中,在诺维科夫-索恩(Novikov-Thorn)模型的框架内研究了在混合度量-帕拉蒂尼(f(R))引力下球面对称黑洞的吸积问题。通过数值计算得到了两种情况下来自圆盘表面的平均能量通量:(V = 0) and (V = - frac{{{{mu }^{2}}}}{2}{{phi }^{2}}+ frac{zeta }{4}{{phi }^{4}}).我们还注意到,在所考虑的每种情况下,理论对这个量的预测都与施瓦兹柴尔德黑洞的类似结果进行了比较。
{"title":"Accretion in a Hybrid Metric-Palatini f(R)-Gravity onto Spherically Symmetric Black Holes","authors":"N. A. Avdeev, P. I. Dyadina","doi":"10.1134/S1547477124700584","DOIUrl":"10.1134/S1547477124700584","url":null,"abstract":"<p>In this work, accretion onto spherically symmetric black hole in hybrid metric-Palatini <span>(f(R))</span>-gravity was studied within the framework of the Novikov–Thorn model. The average energy flux from the disk surface was numerically obtained for two cases: <span>(V = 0)</span> and <span>(V = - frac{{{{mu }^{2}}}}{2}{{phi }^{2}} + frac{zeta }{4}{{phi }^{4}})</span>. We also note that in each considered case, the prediction of the theory for this quantity are compared with similar result for the Schwarzschild black hole.</p>","PeriodicalId":730,"journal":{"name":"Physics of Particles and Nuclei Letters","volume":"21 4","pages":"561 - 563"},"PeriodicalIF":0.4,"publicationDate":"2024-08-14","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142411760","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}
Pub Date : 2024-08-14DOI: 10.1134/S1547477124700936
I. S. Tiurin
The K+ → π0µ+νγ(Kµ3γ) and K+ → π0e+νγ (Ke3γ) decays are measured with OKA detector at the RF-separated 17.7 GeV/c momentum kaon beam from the U-70 synchrotron. The data obtained corresponds to the value of 2.62 × 1010 “live” kaons passing to the decay volume. The ratios of Br(Kµ3γ)/Br(Kµ3) and Br(Ke3γ)/Br(Ke3) are measured. The T-odd correlation ξπμγ (ξπeγ), which is the mixed product of the momenta of µ+(e+), π0, and γ in the kaon rest frame, is measured. The asymmetry of the distribution in ξ is characterized by the ratio Aξ = (N+ − N−)/(N+ + N−), where N+(−) is the number of events with positive (negative) ξ. The values of Aξ for Kµ3γ and for Ke3γ is obtained.
{"title":"K+ → π0µ+νγ and K+ → π0e+νγ Decays: Recent Results from the “OKA” Experiment","authors":"I. S. Tiurin","doi":"10.1134/S1547477124700936","DOIUrl":"10.1134/S1547477124700936","url":null,"abstract":"<p>The <i>K</i><sup>+</sup> → π<sup>0</sup>µ<sup>+</sup>νγ(<i>K</i><sub>µ3γ</sub>) and <i>K</i><sup>+</sup> → π<sup>0</sup><i>e</i><sup>+</sup>νγ (<i>K</i><sub><i>e</i>3γ</sub>) decays are measured with OKA detector at the RF-separated 17.7 GeV/<i>c</i> momentum kaon beam from the U-70 synchrotron. The data obtained corresponds to the value of 2.62 × 10<sup>10</sup> “live” kaons passing to the decay volume. The ratios of Br(<i>K</i><sub>µ3γ</sub>)/Br(<i>K</i><sub>µ3</sub>) and Br(<i>K</i><sub><i>e</i>3γ</sub>)/Br(<i>K</i><sub><i>e</i>3</sub>) are measured. The T-odd correlation ξ<sub>πμγ</sub> (ξ<sub>π<i>e</i>γ</sub>), which is the mixed product of the momenta of µ<sup>+</sup>(<i>e</i><sup>+</sup>), π<sup>0</sup>, and γ in the kaon rest frame, is measured. The asymmetry of the distribution in ξ is characterized by the ratio <i>A</i><sub>ξ</sub> = (<i>N</i><sub>+</sub> − <i>N</i><sub>−</sub>)/(<i>N</i><sub>+</sub> + <i>N</i><sub>−</sub>), where <i>N</i><sub>+(−)</sub> is the number of events with positive (negative) ξ. The values of <i>A</i><sub>ξ</sub> for <i>K</i><sub>µ3γ</sub> and for <i>K</i><sub><i>e</i>3γ</sub> is obtained.</p>","PeriodicalId":730,"journal":{"name":"Physics of Particles and Nuclei Letters","volume":"21 4","pages":"650 - 653"},"PeriodicalIF":0.4,"publicationDate":"2024-08-14","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142411678","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}
Pub Date : 2024-08-14DOI: 10.1134/S1547477124701036
V. Kuskov
In this overview, recent results of the ALICE collaboration on neutral meson and direct photon production are reported. The invariant cross section of ({{pi }^{0}}) and (eta ) meson production in pp collisions (sqrt s = 13) TeV are measured and compared to pQCD calculations. The direct photon production and two-photons HBT correlations in Pb–Pb (sqrt {{{s}_{{NN}}}} = 5.02) TeV are presented as well.
{"title":"Recent Neutral Meson and Direct Photon Measurements with ALICE","authors":"V. Kuskov","doi":"10.1134/S1547477124701036","DOIUrl":"10.1134/S1547477124701036","url":null,"abstract":"<p>In this overview, recent results of the ALICE collaboration on neutral meson and direct photon production are reported. The invariant cross section of <span>({{pi }^{0}})</span> and <span>(eta )</span> meson production in <i>pp</i> collisions <span>(sqrt s = 13)</span> TeV are measured and compared to pQCD calculations. The direct photon production and two-photons HBT correlations in Pb–Pb <span>(sqrt {{{s}_{{NN}}}} = 5.02)</span> TeV are presented as well.</p>","PeriodicalId":730,"journal":{"name":"Physics of Particles and Nuclei Letters","volume":"21 4","pages":"676 - 679"},"PeriodicalIF":0.4,"publicationDate":"2024-08-14","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142411627","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}
Pub Date : 2024-08-14DOI: 10.1134/S1547477124700638
G. Punetha
In order to better understand the dynamics of the quark-hadron phase transition in the presence of a magnetic field, the thermal behaviour of the non-perturbative QCD vacuum has been examined. The dynamical configuration of the resulting dual QCD vacuum and its flux tube configuration have been explored in order to investigate the non-perturbative properties of QCD. Within the context of dual QCD-based hadronic bag, which ensures the critical parameters and the accompanying critical sites for quark-hadron phase transition, related thermodynamic quantities and equation of state (EoS) to define quark matter have also been studied in presence of magnetic field.
{"title":"Effect of Magnetic Field on Dual QCD Quark-Hadron Phase Transition","authors":"G. Punetha","doi":"10.1134/S1547477124700638","DOIUrl":"10.1134/S1547477124700638","url":null,"abstract":"<p>In order to better understand the dynamics of the quark-hadron phase transition in the presence of a magnetic field, the thermal behaviour of the non-perturbative QCD vacuum has been examined. The dynamical configuration of the resulting dual QCD vacuum and its flux tube configuration have been explored in order to investigate the non-perturbative properties of QCD. Within the context of dual QCD-based hadronic bag, which ensures the critical parameters and the accompanying critical sites for quark-hadron phase transition, related thermodynamic quantities and equation of state (EoS) to define quark matter have also been studied in presence of magnetic field.</p>","PeriodicalId":730,"journal":{"name":"Physics of Particles and Nuclei Letters","volume":"21 4","pages":"577 - 580"},"PeriodicalIF":0.4,"publicationDate":"2024-08-14","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142411668","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}