セミナー 2024年

Ryan Hill, The university of Edinburgh

Variance-Reduction Techniques for Disconnected Isospin-Breaking QED Corrections

Hybrid On-site: Kenkyu Honkan Seminar room 321, 322 Online: Zoom
Sub-percent calculations of an increasing number of physical observables are within the reach of modern Lattice QCD. In order to achieve such precision, we must include the (typically) O(1%) corrections from isospin-breaking contributions in our calculations. These corrections include disconnected diagrams, which can be prohibitively expensive to resolve using standard techniques. In this talk, I will discuss ongoing efforts to calculate several disconnected topologies relevant at O(alpha) to e.g. Kl2 decays, on RBC-UKQCD physical-point domain-wall ensembles, following on from exploratory calculations [1]. We make use of the ‘split-even’ estimator [1, 2], which can improve statistical errors by an order of magnitude or more, and explore the use of a distance-splitting technique [1] to take advantage of the dominant short-distance behaviour of some topologies. These techniques are applicable beyond disconnected diagrams, and might improve statistical errors in many contractions involving noisy loop estimators. I will explore the potential to make great improvements on the statistical error of our previous result for rare K+->Pi+l+l- decays [3] using these techniques.

[1] Harris, T., Gülpers, V., Portelli, A., Richings, J. Efficiently unquenching QCD+QED at O(alpha) PoS LATTICE2022 (2023). https://arxiv.org/abs/1903.10447
[2] Giusti, L., Harris, T., Nada, A. et al. Frequency-splitting estimators of single-propagator traces. Eur. Phys. J. C 79, 586 (2019). https://doi.org/10.1140/epjc/s10052-019-7049-0
[3] Boyle, P. A., Erben, F., Flynn, J. M., Gülpers, V., Hill, R. C., Hodgson, R., Jüttner, A., Ó hÓgáin, F., Portelli, A., Sachrajda, C. T. Simulating rare kaon decays K+->Pi+l+l- using domain wall lattice QCD with physical light quark masses. Phys. Rev. D 107 (2023) L011503. https://link.aps.org/doi/10.1103/PhysRevD.107.L011503

Rahool Kumar, IPMU

Machine learning the Higgs-top CP measurement at the LHC

Hybrid On-site: Kenkyu Honkan Seminar room 321, 322 Online: Zoom
The conventional approach to LHC analysis involves comparing the measured data to Monte Carlo simulations. These simulations start at the hard-scattering level, where the potential for new physics is maximal, and proceed through various stages, including showering, hadronization, and detector response. Unfortunately, each stage introduces complexities, resulting in a convoluted representation of the true underlying physics at the simulated detector level. Events measured at the LHC detector are also somewhat convoluted versions of the true underlying physics due to various latent effects. Eliminating these convolutions is essential for a direct comparison between theoretical predictions and measured data, which can be achieved through the process of ‘Unfolding’, where measured events are directly mapped to the hard-scattering level.

Yuri Michinobu, YITP

Species bound and its moduli dependence

Hybrid On-site: Kenkyu Honkan Seminar room 321, 322 Online: Zoom
The species bound, a swampland conjecture, suggests that the cutoff of quantum gravity in an effective field theory coupled to a number of light fields is significantly lower than the Planck scale. Notably, the species bound offers insights into the interior of the moduli space. In this talk, I will review recent progress in this direction (2303.13580,2212.10286). I will begin by introducing the notion of the species bound and then discuss constraints on its dependence on moduli. Additionally, I will explain the connection to black hole entropy, which serves as a
non-trivial check of the constraint.

Adil Jueid, Institute for Basic Science

[cancelled] Dark matter triggering flavor changing neutral current decays of the top quark

Hybrid On-site: Kenkyu Honkan Seminar room 321, 322 Online: Zoom
In this talk, I will discuss a possible connection between dark matter (DM) and one-loop induced top quark FCNC decays. In a simplified t-channel DM model that extends the SM with one colored scalar mediator and one right-handed fermion both odd under an ad-hoc Z_2 symmetry, I will show that that moderate to large rates of the top quark FCNC decays are possible while respecting the existing constraints. Then I will discuss the phenomenological implications at hadron colliders (HL-LHC and FCC-hh) of four phenomenologically viable scenarios.

Tokiro Numasawa, ISSP

Gauging Spacetime Inversions

Hybrid On-site: Kenkyu Honkan Seminar room 321, 322 Online: Zoom
Spacetime inversion symmetries such as parity and time reversal play a central role in physics, but they are usually treated as global symmetries.
In quantum gravity there are no global symmetries, so any spacetime inversion symmetries must be gauge symmetries.
In particular this includes CRT symmetry (in even dimensions usually combined with a rotation to become CPT), which in quantum field theory is always a symmetry and seems likely to be a symmetry of quantum gravity as well.
In this talk, we will discuss what it means to gauge a spacetime inversion symmetry and explain some of the more unusual consequences of doing this.
In particular, I will argue that the gauging of CRT is automatically implemented by the sum over topologies in the Euclidean gravity path integral, that in a closed universe the Hilbert space of quantum gravity must be a real vector space, and that in Lorentzian signature manifolds which are not time-orientable must be included as valid configurations of the theory.

Tetsuo Hyodo, Tokyo Metropolitan University

[KEK-JAEA Joint Seminar] Femtoscopy for Exotic Hadrons and Nuclei

Hybrid On-site: Kenkyu Honkan Seminar room 321, 322 Online: Zoom
In high-energy collision experiments, the momentum distribution of hadron pairs reveals correlations arising from hadron interactions and quantum statistics. Traditionally, femtoscopy has been used to derive emission source information from these correlations. Recently, these techniques have also facilitated new methods to assess hadron
interactions, as exemplified by the ALICE collaboration’s significant advancements at the LHC. This talk will cover the fundamental theoretical methods for calculating momentum correlation functions and discuss recent applications to antikaon-nucleon systems and hypernuclei, with a look toward future research at J-PARC.

References:
[1] S. Cho et al., ExHIC collaboration, Prog. Part. Nucl. Phys. 95, 279 (2017).
[2] Y. Kamiya, T. Hyodo, K. Morita, A. Ohnishi, W. Weise, Phys. Rev. Lett. 124, 132501 (2020).
[3] A. Jinno, Y. Kamiya, T. Hyodo, A. Ohnishi, arXiv:2403.09126 [nucl-th]

Kiyoharu Kawana, KIAS

Fine-Tuning as Quantum Phase Transition Point

Online (Zoom)
We discuss analogy between statistical mechanics and quantum field theory from the point of view of fine-tuning problem. In the former, (first-order) phase transition (PT) point spans a finite parameter space in micro-canonical ensemble, while it is literally a point and looks like a fine-tuning of parameters in canonical ensemble.
In this talk, I would like to point out that similar picture holds in quantum field theory. As concrete examples, we discuss free scalar theory and \phi^4 theory and show that gapless point (m^2=0) is typically realized in micro- canonical ensemble. Then, as a phenomenological application, we show that the Higgs alignment in the two Higgs doublet model can be realized in the micro-canonical picture without imposing any symmetries.

George T. Fleming, FNAL

Matching Curved Lattices to Anisotropic Tangent Planes

Hybrid On-site: Kenkyu Honkan Seminar room 321, 322 Online: Zoom
Radial quantization would be the ideal formalism for studying strongly-coupled near-conformal quantum field theories but it requires the ability to perform lattice calculations on static, curved manifolds, specifically a very long cylinder whose cross section is a sphere. Smoothly discretizing the surface of a sphere requires a graph with unequal edge lengths. The geometry of such graphs is well understood since 1961 using Regge Calculus. But, lattice quantum field theories are defined in terms of couplings which appear in the action rather than edge lengths and so the relationship between couplings and lengths must be determined dynamically. A simple example is computing the ratio of spatial to temporal lattice spacings in anisotropic lattice QCD. I will discuss our conjecture that computing anisotropic lattice spacing ratios on affine transformations of regular flat lattices is sufficient to determine coupling assignments on curved lattices.

Takuya Okuda, Univ. of Tokyo

Measurement-based quantum simulation of lattice gauge theories and anomaly inflow

Hybrid On-site: Kenkyu Honkan Seminar room 321, 322 Online: Zoom
Quantum simulation of lattice gauge theories is expected to become a major application of quantum computers in the future. So far, most efforts have focused on the scheme based on quantum circuits. In this talk, I will advocate an alternative scheme inspired by measurement-based quantum computation. The Trotterized discrete time evolution of a Hamiltonian lattice gauge theory is driven by adaptive single-qubit measurements on an entangled resource state tailored for the simulated theory. The resource state itself has interesting physical properties and is in a symmetry-protected topological (SPT) phase protected by higher-form symmetries. We demonstrate an anomaly inflow mechanism between the simulated theory and the resource state by computing the gauge transformations of defect-dependent partition functions. The resource state can also be used to prove Kramers-Wannier-Wegner dualities of various lattice models. Based on arXiv:2210.10908 and 2402.08720 with Sukeno and Parayil Mana.

Masashi Kawahira, YITP

Batalin–Vilkovisky formalism and theta term

Hybrid On-site: Kenkyu Honkan Seminar room 321, 322 Online: Zoom
Quantum field theories (QFTs) describe a lot of physical phenomena in our world. And giving a mathematical definition of QFTs is a long-standing problem. There are several mathematical formulations: Wightman formulation, Osterwalder–Schrader formulation and Atiya-Segal formulation. And each of them cover different aspects of QFTs. Recently, Costello and their collabolators formulate QFTs by using factorization algbras. This formulaion cover a lot of classes of QFTs: TQFTs, 2d CFTs and perturbative QFTs. And they reproduce various results such as asymptotic freedom in non-Abelian gauge theories. Factorization algbras can be given by Batalin–Vilkovisky quantization (BV quantization) of the Lagrangian. However the original BV quantizations are perturbative and they do not have non-perturbative effects like instanton. In this talk, we propose BV quantizations which include instanton effects in compact scalar theory. In modern language, it is a BV formulation of ℤ gauging.
1 2 3 4

ページ先頭へ戻る