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The third family quark mass hierarchy and FCNC in the universal seesaw model 宇宙跷跷板模型中的第三族夸克质量等级和 FCNC
IF 3.5 4区 物理与天体物理 Q1 Physics and Astronomy Pub Date : 2024-08-13 DOI: 10.1093/ptep/ptae127
Takuya Morozumi, Albertus Hariwangsa Panuluh
We present the study of the quark sector of the universal seesaw model with $mathrm{SU(2)_L times SU(2)_R times U(1)_{Y^{prime }}}$ gauge symmetry in the massless case of the two lightest quark families. This model aims to explain the mass hierarchy of the third family quark by introducing a vector-like quark (VLQ) partner for each quark. In this model, we introduce SU(2)L and SU(2)R Higgs doublets. We derive explicitly the Lagrangian for the quark sector, Higgs sector, and kinetic terms of the gauge fields, starting from the Lagrangian, which is invariant under $mathrm{SU(2)_L times SU(2)_R times U(1)_{Y^{prime }}}$ gauge symmetry. At each stage of the symmetry breaking, we present the Lagrangian with the remaining gauge symmetry. Additionally, we investigate the flavor-changing neutral currents (FCNCs) of Higgs (h) and Z-boson in the interaction with the top, heavy top, bottom, and heavy bottom quarks.
我们介绍了在两个最轻夸克族的无质量情况下,具有 $mathrm{SU(2)_L times SU(2)_R times U(1)_{Y^{prime }}$规对称性的通用跷跷板模型的夸克部门的研究。这个模型旨在通过为每个夸克引入一个类矢量夸克(VLQ)伙伴来解释第三族夸克的质量层次。在这个模型中,我们引入了苏(2)L 和苏(2)R 希格斯双特。我们从在 $mathrm{SU(2)_L times SU(2)_R times U(1)_{Y^{prime }}$ 计对称性下不变的拉格朗日出发,明确推导出夸克扇区、希格斯扇区以及规量场的动力学项。在对称性破缺的每个阶段,我们都提出了具有剩余规对称性的拉格朗日。此外,我们还研究了希格斯(h)和 Z 玻色子在与顶、重顶、底和重底夸克相互作用时的变味中性电流(FCNCs)。
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引用次数: 0
Performance of the Fully-equipped Spin Flip Chopper For Neutron Lifetime Experiment at J-PARC 用于 J-PARC 中子寿命实验的全装备自旋翻转斩波器的性能
IF 3.5 4区 物理与天体物理 Q1 Physics and Astronomy Pub Date : 2024-08-10 DOI: 10.1093/ptep/ptae123
K Mishima, G Ichikawa, Y Fuwa, T Hasegawa, M Hino, R Hosokawa, T Ino, Y Iwashita, M Kitaguchi, S Matsuzaki, T Mogi, H Okabe, T Oku, T Okudaira, Y Seki, H E Shimizu, H M Shimizu, S Takahashi, M Tanida, S Yamashita, M Yokohashi, T Yoshioka
To solve the “neutron lifetime puzzle,” where measured neutron lifetimes differ depending on the measurement methods, an experiment with pulsed neutron beam at J-PARC is in progress. In this experiment, neutrons are bunched into 40-cm lengths using a spin flip chopper (SFC), where the statistical sensitivity was limited by the aperture size of the SFC. The SFC comprises three sets of magnetic supermirrors and two resonant spin flippers. In this paper, we discuss an upgrade to enlarge the apertures of the SFC. With this upgrade, the statistics per unit time of the neutron lifetime experiment increased by a factor of 2.8, while maintaining a signal-to-noise ratio of 250–400 comparable to the previous one. Consequently, the time required to reach a precision of 1 s in the neutron lifetime experiment was reduced from 590 to 170 days, which is a significant reduction in time. This improvement in statistic will also contribute to the reduction of systematic uncertainties, such as background evaluation, fostering further advancements in the neutron lifetime experiments at J-PARC.
为了解决 "中子寿命之谜"(测量方法不同,测得的中子寿命也不同),J-PARC 正在进行脉冲中子束实验。在该实验中,使用自旋翻转斩波器(SFC)将中子束成 40 厘米长,统计灵敏度受到 SFC 孔径大小的限制。SFC 由三组磁性超级反射镜和两个共振自旋翻转器组成。本文讨论了扩大 SFC 孔径的升级方案。通过这次升级,中子寿命实验单位时间内的统计量增加了 2.8 倍,同时信噪比保持在 250-400 之间,与以前相当。因此,中子寿命实验达到 1 秒精度所需的时间从 590 天减少到 170 天,大大缩短了时间。统计量的提高还将有助于减少系统不确定性,如背景评估,从而促进 J-PARC 中子寿命实验的进一步发展。
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引用次数: 0
Analytic and Numerical Approaches for Depictive 3-loop Integrals using Sector Decomposition 利用扇形分解描绘三环积分的分析和数值方法
IF 3.5 4区 物理与天体物理 Q1 Physics and Astronomy Pub Date : 2024-08-08 DOI: 10.1093/ptep/ptae122
Elise de Doncker, Tadashi Ishikawa, Kiyoshi Kato, Fukuko Yuasa
Four 3-loop two-point functions are studied analytically and numerically using a simplified sector decomposition method. The coefficients of the ultraviolet divergent part are determined analytically, and those of the finite part are computed numerically. The energy dependence of the integrals is shown explicitly, and a discussion of its behavior is presented.
采用简化扇形分解法对四个三环两点函数进行了分析和数值研究。紫外发散部分的系数是分析确定的,有限部分的系数是数值计算的。明确显示了积分的能量依赖性,并对其行为进行了讨论。
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引用次数: 0
Broad-Band X-Ray Analysis of NGC 3227 NGC 3227 的宽波段 X 射线分析
IF 3.5 4区 物理与天体物理 Q1 Physics and Astronomy Pub Date : 2024-08-08 DOI: 10.1093/ptep/ptae125
Jared Newman, Sachiko Tsuruta, Andrew C Liebmann, Hideyo Kunieda, Yoshito Haba
Previously in Project (A) we carried out analysis of the data obtained by observations of the 1.5 Seyfert galaxy NGC 3227, the two observations performed by XMM-Newton in 2000 and 2006 and six observations by Suzaku in 2008. In the current paper, Project (B), our work was extended to joint XMM-Newton and NuSTAR observations in 2016 as well as a NuSTAR observation in 2017. In Project A a unified model was constructed. The model consists of a hard power law (ΓHard = 1.4 − 1.7) which is interpreted as the Comptonized emission from the corona above an accretion disk. In the high flux states an additional soft excess component dominates, which is consistent with either a power law (ΓSoft = 3.3 − 3.85) or warm Comptonization. These emissions are absorbed by a partial covering material and warm absorbers. A reflection component and several emission lines are also present. In Project B, the model presented in Project A was applied to more recent observations. It was found that this model remains valid. Our conclusion is that this model is consistent, valid with the long observations from 2000 to 2017 and over the broad frequency band from 0.3 keV to 50 keV.
在之前的项目(A)中,我们分析了对1.5塞弗特星系NGC 3227的观测数据,包括XMM-牛顿在2000年和2006年进行的两次观测,以及Suzaku在2008年进行的六次观测。在本文,即项目(B)中,我们的工作扩展到了2016年的XMM-牛顿和NuSTAR联合观测,以及2017年的NuSTAR观测。在项目 A 中,我们构建了一个统一的模型。该模型包括一个硬幂律(ΓHard = 1.4 - 1.7),被解释为来自吸积盘上方日冕的康普顿化发射。在高通量状态下,额外的软过量成分占主导地位,这与幂律(ΓSoft = 3.3 - 3.85)或暖康普顿化一致。这些发射被部分覆盖材料和暖吸收体吸收。此外,还存在反射成分和几条发射线。在项目 B 中,项目 A 中提出的模型被应用于最近的观测。结果发现,该模型仍然有效。我们的结论是,该模型与 2000 年至 2017 年的长期观测结果是一致的,在 0.3 keV 至 50 keV 的宽频带内也是有效的。
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引用次数: 0
Kaluza-Klein Schwinger Effect 卡鲁扎-克莱因-施文格效应
IF 3.5 4区 物理与天体物理 Q1 Physics and Astronomy Pub Date : 2024-08-08 DOI: 10.1093/ptep/ptae124
Yusuke Yamada
We show that electric fields in compactified spaces may produce Kaluza-Klein (KK) particles even when the energy of electric fields is smaller than KK scale. As an illustrating example, we consider a charged massless complex scalar coupled to U(1) gauge theory in $mathbb {R}^{1,3}times {mathbb {S}}^1$ and discuss the effect of background gauge potential along a compact direction. The electric field produces the charged Kaluza-Klein particle non-perturbatively, which we call KK Schwinger effect. We quantitatively show that KK modes can be produced even when the electric field energy is much below the KK scale. The mechanism is rather general and similar phenomena would occur in any compactification models when a gauge potential along compact direction evolves in time and experiences large enough field excursion. We also discuss the subtlety of four dimensional effective theory truncated by KK modes at an initial time, when the electric field is turned on.
我们证明,即使电场的能量小于KK尺度,紧凑空间中的电场也可能产生卡卢扎-克莱因(KK)粒子。作为一个说明性的例子,我们考虑了在 $mathbb {R}^{1,3}times {mathbb {S}}^1$ 中与 U(1) 轨则理论耦合的带电无质量复标量,并讨论了沿紧凑方向的背景轨则势的影响。电场会非微扰地产生带电的卡卢扎-克莱因粒子,我们称之为KK施文格效应。我们定量证明,即使电场能量远低于 KK 尺度,也能产生 KK 模式。这种机制相当普遍,当规电势沿紧凑方向随时间演化并经历足够大的场偏移时,类似现象会发生在任何紧凑模型中。我们还讨论了四维有效理论在电场开启的初始时间被 KK 模式截断的微妙之处。
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引用次数: 0
Distributions of consecutive level spacings of GUE and their ratio: ab initio derivation GUE 的连续级距分布及其比率: Ab initio 推导
IF 3.5 4区 物理与天体物理 Q1 Physics and Astronomy Pub Date : 2024-08-06 DOI: 10.1093/ptep/ptae120
Shinsuke M Nishigaki
In recent studies of many-body localization in nonintegrable quantum systems, the distribution of the ratio of two consecutive energy level spacings, rn = (En + 1 − En)/(En − En − 1) or $tilde{r}_n=min (r_n,r_n^{-1})$, has been used as a measure to quantify the chaoticity, alternative to the more conventional distribution of the level spacings, $s_n=bar{rho }(E_n)(E_{n+1}-E_n)$, as the former unnecessitates the unfolding required for the latter. Based on our previous work on the Tracy-Widom approach to the Jánossy densities, we present analytic expressions for the joint probability distribution of two consecutive eigenvalue spacings and the distribution of their ratio for the Gaussian unitary ensemble (GUE) of random Hermitian N × N matrices at N → ∞, in terms of a system of differential equations. As a showcase of efficacy of our results for characterizing an approach to quantum chaoticity, we contrast them to arguably the most ideal of all quantum-chaotic spectra: the zeroes of the Riemann ζ function on the critical line at increasing heights.
在最近对不可解量子系统中多体局域化的研究中,两个连续能级间距比的分布,rn = (En + 1 - En)/(En - En - 1) 或 $tilde{r}_n=min (r_n,r_n^{-1})$、已被用来量化混沌性,以替代更传统的水平间隔分布,即 $s_n=bar{rho}(E_n)(E_{n+1}-E_n)$,因为前者不需要后者所需的展开。基于我们之前对詹诺西密度的特雷西-维多姆方法的研究,我们用一个微分方程系统给出了两个连续特征值间距的联合概率分布,以及在 N → ∞ 时随机赫米提 N × N 矩阵的高斯单元集合(GUE)的它们的比值分布的解析表达式。为了展示我们的结果在表征量子混沌性方面的功效,我们将它们与所有量子混沌谱中最理想的谱进行了对比:临界线上黎曼ζ函数的零点在高度上不断增加。
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引用次数: 0
An implementation of nuclear many-body wave functions by the superposition of localized Gaussians 通过局部高斯叠加实现核多体波函数
IF 3.5 4区 物理与天体物理 Q1 Physics and Astronomy Pub Date : 2024-08-01 DOI: 10.1093/ptep/ptae119
Masaaki Kimura, Yasutaka Taniguchi
We introduce a new framework for the nuclear structure calculations, which describes the single-particle wave function as a superposition of localized Gaussians. It is a hybrid of the Hartree-Fock and antisymmetrized molecular dynamics models. In the numerical calculations of oxygen, calcium isotopes and 100Sn, the framework shows its potential by significantly improving upon AMD and yielding the results consistent with or even better than Hartree-Fock(-Bogoliubov) calculations based on harmonic oscillator expansions. In addition to the basic equations, general form of the matrix elements are also given.
我们为核结构计算引入了一个新框架,它将单粒子波函数描述为局部高斯的叠加。它是哈特里-福克模型和反对称分子动力学模型的混合体。在氧气、钙同位素和 100Sn 的数值计算中,该框架显示了其潜力,大大改进了 AMD,其结果与基于谐振子展开的 Hartree-Fock(-Bogoliubov)计算结果一致,甚至更好。除基本方程外,还给出了矩阵元素的一般形式。
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引用次数: 0
Systematic effects on lensing reconstruction from a patchwork of CMB polarization maps 从拼凑的 CMB 偏振图重建透镜的系统效应
IF 3.5 4区 物理与天体物理 Q1 Physics and Astronomy Pub Date : 2024-08-01 DOI: 10.1093/ptep/ptae117
Ryo Nagata, Toshiya Namikawa
We investigate the tolerance for systematic errors in lensing analysis applied to a patchwork map of Cosmic Microwave Background polarization. We focus on the properties of the individual polarization maps that comprise the patchwork and discuss the associated calibration residuals that are coherent on those subpatches. We numerically simulate the polarization field modulated as a whole patchwork and apply a suite of lensing analyses to reveal the response of the reconstructed gravitational lensing potential and delensing efficiency. At systematic error levels expected in the near future, we find that it is possible to accurately reconstruct the lensing potential on scales larger than the subpatch size and that there is no severe degradation of the lensing B-mode removal efficiency in the subsequent delensing analysis.
我们研究了应用于宇宙微波背景偏振拼凑图的透镜分析中系统误差的容限。我们重点研究了组成拼凑图的各个偏振图的特性,并讨论了与这些子拼凑图相关的校准残差。我们用数值模拟了作为一个整体拼凑的偏振场调制,并应用一套透镜分析来揭示重建的引力透镜势和脱镜效率的响应。我们发现,在不久的将来,在预计的系统误差水平下,可以在大于子斑尺寸的尺度上准确地重建透镜势,而且在随后的脱透镜分析中,透镜B模去除效率不会严重下降。
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引用次数: 0
Patchwork Conditions for Holographic Nonlinear Responses: A Computational Method of Electric Conductivity and Friction Coefficient 全息非线性响应的拼凑条件:电导率和摩擦系数的计算方法
IF 3.5 4区 物理与天体物理 Q1 Physics and Astronomy Pub Date : 2024-07-31 DOI: 10.1093/ptep/ptae118
Shuta Ishigaki, Shin Nakamura, Kazuaki Takasan
We propose a new method to compute nonlinear transport coefficients in holography, such as nonlinear DC conductivity and nonlinear friction coefficient. The conventional method can be applied only to the models whose action in the gravity dual has the “square-root structure,” i.e., the Dirac-Born-Infeld action of the probe D-branes or the Nambu-Goto action of the probe strings. Our method is applicable to a wider range of holographic models whose action does not have such a square-root structure. We propose a condition to obtain regular physical configurations in the gravity dual in the form of two simultaneous equations, which we call the patchwork condition. Our method also enables us to estimate the effective temperature of the nonequilibrium steady states in a wider range of holographic models. We show that a general model exhibits different effective temperatures for different fluctuation modes.
我们提出了一种新方法来计算全息技术中的非线性传输系数,如非线性直流电导和非线性摩擦系数。传统方法只适用于引力对偶作用具有 "平方根结构 "的模型,即探针 Drane 的 Dirac-Born-Infeld 作用或探针弦的 Nambu-Goto 作用。我们的方法适用于更广泛的全息模型,这些模型的作用不具有这种方根结构。我们提出了在引力对偶中以两个同时方程的形式获得规则物理构型的条件,我们称之为拼凑条件。我们的方法还使我们能够在更广泛的全息模型中估算非平衡稳态的有效温度。我们证明,一般模型在不同的波动模式下会表现出不同的有效温度。
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引用次数: 0
Supersymmetric Expansion Algorithm and Complete Analytical Solution for the Hulthén and Anharmonic Potentials 胡尔特恩势和非谐波势的超对称展开算法和完整解析解
IF 3.5 4区 物理与天体物理 Q1 Physics and Astronomy Pub Date : 2024-07-30 DOI: 10.1093/ptep/ptae115
M Napsuciale, S Rodríguez, M Kirchbach
An algorithm for providing analytical solutions to Schrödinger’s equation with non-exactly solvable potentials is elaborated. It represents a symbiosis between the logarithmic expansion method and the techniques of the supersymmetric quantum mechanics as extended toward non shape invariant potentials. The complete solution to a given Hamiltonian H0 is obtained from the nodeless states of the Hamiltonian H0 and of a set of supersymmetric partners H1, H2, …, Hr. The nodeless states (dubbed “edge” states) are unique and in general can be ground or excited states. They are solved using the logarithmic expansion which yields an infinite system of coupled first order hierarchical differential equations, converted later into algebraic equations with recurrence relations which can be solved order by order. We formulate the aforementioned scheme, termed to as “Supersymmetric Expansion Algorithm” step by step and apply it to obtain for the first time the complete analytical solutions of the three dimensional Hulthén–, and the one-dimensional anharmonic oscillator potentials.
本文阐述了一种为具有非精确可解势能的薛定谔方程提供解析解的算法。它代表了对数展开方法与超对称量子力学技术之间的共生,并扩展到非形状不变势。给定哈密顿 H0 的完整解是从哈密顿 H0 和一组超对称伙伴 H1、H2、......、Hr 的无结点态中获得的。无节点态(被称为 "边缘 "态)是唯一的,一般可以是基态或激发态。我们利用对数展开来求解这些态,从而得到一个无限的耦合一阶层次微分方程系统,然后将其转换为具有递推关系的代数方程,并逐阶求解。我们逐步制定了上述被称为 "超对称展开算法 "的方案,并首次应用它获得了三维胡尔塞恩和一维非谐振子势的完整解析解。
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引用次数: 0
期刊
Progress of Theoretical and Experimental Physics
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