記述言語：日本語   掲載種別：研究論文（大学，研究機関等紀要）  

Development of "Let's get hands on a math toolbox" as a "liberal science" subject

DOI： https://doi.org/10.15017/4773092

記述言語：日本語   掲載種別：研究論文（大学，研究機関等紀要）  

Electromotive Force in Electromagnetism

リポジトリ公開URL： http://hdl.handle.net/2324/4363024

記述言語：英語   掲載種別：研究論文（その他学術会議資料等）  

We propose a new approach to Nuclear Effective Field Theory (NEFT) on a lattice on the basis of Renormalization Group (RG) analysis. In order to perform Markov-chain Monte Carlo lattice simulation of NEFT, we introduce auxiliary fields to integrate nucleon field so that its effects are represented as a determinant. The problem is that the determinant becomes complex and cannot be considered as a part of probability distribution function. We introduce a reweighting method, in which the reference determinant is chosen to be optimal in the RG analysis sense: the reference determinant contains only the relevant interactions and the closest to the original determinant. We calculate the standard deviation of the absolute value of the reweighting factor in a simple model, isospin-symmetric S-wave NLO NEFT without pions, and explain why our choice is optimal.

DOI： 10.1007/978-3-030-32357-8_67

記述言語：日本語   掲載種別：研究論文（大学，研究機関等紀要）  

For the purpose of detecting misconception in Newtonian mechanics that students majoring in humanities and social science have, we gave Force Concept Inventory (FCI) test to those who attended the classes of “Physics in Daily Life” in KIKAN Education. We find that they have very low scores for several questions, most of which are closely related to impetus misconception. Principal component analysis of the students’ answers reveals that these questions have large components of the eigenvector corresponding to the largest eigenvalue of the correlation coefficient matrix. Effects of introducing “Basic Physics” into the high school curriculum are briefly discussed.

記述言語：英語   掲載種別：研究論文（学術雑誌）  

We formulate the next-to-leading order nuclear effective field theory without pions in the two-nucleon sector on a spatial lattice, and investigate nonperturbative renormalization group flows in the strong coupling region by diagonalizing the Hamiltonian numerically. The cutoff (proportional to the inverse of the lattice constant) dependence of the coupling constants is obtained by changing the lattice constant with the binding energy and the asymptotic normalization constant for the groundstate being fixed. We argue that the critical line can be obtained by looking at the finite-size dependence of the groundstate energy. We determine the relevant operator and locate the nontrivial fixed point, as well as the physical flow line corresponding to the deuteron in the two-dimensional plane of dimensionless coupling constants. It turns out that the location of the nontrivial fixed point is very close to the one obtained by the corresponding analytic calculation, but the relevant operator is quite different.

DOI： 10.1103/PhysRevC.94.024004

記述言語：英語   掲載種別：研究論文（学術雑誌）  

Low-energy effective field theory describing a nonrelativistic three-body system is analyzed in the Wilsonian renormalization group method. No effective auxiliary field (dimeron) that corresponds to two-body propagation is introduced. The Efimov effect is expected in the case of an infinite two-body scattering length and is believed to be related to the limit cycle behavior in the three-body renormalization group equations (RGEs). If the one-loop property of the RGEs for the nonrelativistic system without the dimeron field, which is essential in deriving RGEs in the two-body sector, persists in the three-body sector, it appears to prevent the emergence of limit cycle behavior. We explain how the multiloop diagrams contribute in the three-body sector without contradicting the one-loop property of the RGEs and derive the correct RGEs, which lead to the limit cycle behavior. The Efimov parameter, s₀, is obtained within a few percent error in the leading orders. We also remark on the correct use of the dimeron formulation. We find rich renormalization group flow structure in the three-body sector. In particular, a novel nontrivial fixed point of the three-body couplings is found when the two-body interactions are absent. We also find, on the two-body nontrivial fixed point, the limit cycle is realized as a loop of finite size in the space of three-body coupling constants when terms with derivatives are included.

DOI： 10.1103/PhysRevD.87.085006

記述言語：英語   掲載種別：研究論文（学術雑誌）  

In order to implement the power counting obtained in the Wilsonian renormalization group (WRG) analysis of nuclear effective field theory (NEFT) including pions, we propose a practical calculational scheme in which the short-distance part of one-pion exchange (S-OPE) is removed and represented as contact terms. A distinctive feature of our scheme is that two regularization schemes are used in combination. The dimensional regularization (DR) is used for diagrams consisting only of contact interactions and a momentum cutoff is implemented for diagrams con-taining the long-distance part of one pion exchange (L-OPE) by introducing a Gaussian damping factor(GDF). The sole purpose of the use of the dimensional regularization is that it considerably simplifies the treatment of nonperturbative part of the scattering amplitude. In the calculation the L-OPE is treated as perturbation and a part of the S-OPE is treated nonperturbatively along with a contact interaction without derivative nonperturbatively. We show the results of the next-To-next-to-leading order(NNLO) calculations for nucleon-nucleon elastic scattering in the S-waves that are fitted to Nijmegen partial wave analysis data.

記述言語：英語   掲載種別：研究論文（国際会議プロシーディングス）  

We perform a Wilsonian renormalization group analysis for the nucleon–nucleon scattering in the
P waves in the nuclear effective field theory including pions, in a similar way to the one done for the S-waves
in our previous paper. We emphasize that the one-pion exchange interaction with large momentum transfer is
of the same order as the leading contact interaction, so that there is no mismatch of the power counting. It is
explicitly shown by obtaining consistent sets of renormalization group equations, that the cutoff dependence
generated by the loop diagrams containing pion exchanges can be compensated by the cutoff dependence of
the coupling constants of the contact interactions.

DOI： 10.1007/s00601-012-0541-9

記述言語：英語   掲載種別：研究論文（国際会議プロシーディングス）  

On the basis of the Wilsonian renormalization group (WRG) analysis of nuclear effective field
theory (NEFT) including pions, we propose a practical calculational scheme in which the short-distance part
of one-pion exchange (S-OPE) is removed and represented as contact terms. The long-distance part of one-
pion exchange (L-OPE) is treated as perturbation. The use of dimensional regularization (DR) for diagrams
consisting only of contact interactions considerably simplifies the calculation of scattering amplitude and
the renormalization group equations. NLO results for nucleon-nucleon elastic scattering in the S-waves are
obtained and compared with experiments. A brief comment on NNLO calculations is given.

DOI： 10.1007/s00601-012-0349-7

記述言語：英語   掲載種別：研究論文（国際会議プロシーディングス）  

We explain how the Wilsonian renormalization group (RG) can determine the power counting of the
nuclear effective field theory (NEFT) including pions. We emphasize that the separation of pion exchange into
the short-distance part and the long-distance part is essential since they behave differently in the RG analysis;
we found that the latter is perturbative whereas the a part of the former is nonperturbative. As for the contact
interactions power counting turns out to be the same as that for pionless NEFT: pion exchange does not affect
the scaling property of contact operators. Our RG equations for NEFT including pions connect smoothly with
those for the pionless NEFT: pions decouple at very low energies as we expect.

DOI： 10.1007/s00601-012-0348-8

記述言語：英語   掲載種別：研究論文（学術雑誌）  

We show how the Apparently Noninvariant Terms (ANTs), which emerge in perturbation theory of nonlinear sigma models, are consistent with the nonlinearly realized symmetry by employing the Ward-Takahashi identity (in the form of an inhomogeneous Zinn-Justin equation). In the literature the discussions on ANTs are confined to the SU(2) case. We generalize them to the U(N) case and demonstrate explicitly at the one-loop level that despite the presence of divergent ANTs in the effective action of the "pions", the symmetry is preserved.

DOI： 10.1143/PTP.123.475

記述言語：英語   掲載種別：研究論文（学術雑誌）  

DOI： 10.1103/PhysRevD.80.029902

記述言語：英語   掲載種別：研究論文（学術雑誌）  

We extend our Wilsonian renormalization group (RG) analysis on the pionless nuclear effective field theory in the two-nucleon sector in two ways; on the one hand, (1) we enlarge the space of operators up to including those of ${\mathcal O}(p-4)$ in the S waves, and, on the other hand, (2) we consider the RG flows in higher partial waves (P and D waves). In the larger space calculations, we find, in addition to nontrivial fixed points, two "fixed lines" and a "fixed surface" which are related to marginal operators. In the higher partial wave calculations, we find similar phase structures to that of the S waves, but there are two relevant directions in the P waves at the nontrivial fixed points and three in the D waves. We explain the physical meaning of the P-wave phase structure by explicitly calculating the low-energy scattering amplitude. We also discuss the relation between the Legendre flow equation which we employ and the RG equation by Birse, McGovern and Richardson, and possible implementation of power divergence subtraction in higher partial waves.

記述言語：英語   掲載種別：研究論文（学術雑誌）  

Apparently noninvariant terms (ANTs) that appear in loop diagrams for nonlinear sigma models are revisited in lattice perturbation theory. The calculations have been done mostly with dimensional regularization so far. In order to establish that the existence of ANTs is independent of the regularization scheme, and of the potential ambiguities in the definition of the Jacobian of the change of integration variables from group elements to "pion" fields, we employ lattice regularization, in which everything (including the Jacobian) is well defined. We show explicitly that lattice perturbation theory produces ANTs in the four-point functions of the pion fields at one-loop and the Jacobian does not play an important role in generating ANTs.

DOI： 10.1103/PhysRevD.79.065037

記述言語：英語   掲載種別：研究論文（学術雑誌）  

We carefully examine one of the derivations of the renormalization group equation (RGE) for the so-called Vl_ow k potential, given by Bogner et al. [nucl-th/0111042]. The derivation, based on the completeness relation of the model space, must be modified if there are bound states. It is however shown that the RGE is unchanged if the bound state wavefunctions in the reduced theory are required to have the same low-momentum components as those in the original theory. Several aspects of the V_{low k} approach are also discussed. harada@phys.kyushu-u.ac.jp.

DOI： 10.1143/PTP.120.741

記述言語：英語   掲載種別：研究論文（学術雑誌）  

We consider an application of Wilsonian Renormalization Group (RG) to the power counting issue in Nuclear Effective Field Theory(NEFT). After reviewing the relevance of scaling dimensions in determining the power counting, we consider the pionless NEFT as the simplest example. The inclusion of the so-called "redundant operators" in a Wilsonian analysis is emphasized.

DOI： 10.1016/j.nuclphysa.2007.03.074

記述言語：英語   掲載種別：研究論文（学術雑誌）  

In a Wilsonian renormalization group (RG) analysis, redundant operators, which may be eliminated by using field redefinitions, emerge naturally. It is therefore important to include them. We consider a nonrelativistic effective theory (the so-called "pionless" nuclear effective field theory) as a concrete example and show that the off-shell amplitudes cannot be renormalized if the redundant operators are not included. The relation between the theories with and without such redundant operators is established in the low-energy expansion. We perform a Wilsonian RG analysis for the off-shell scattering amplitude in the theory with the redundant operator.

DOI： 10.1016/j.physletb.2006.03.072

記述言語：英語   掲載種別：研究論文（学術雑誌）  

DOI： 10.1143/PTP.113.1315

記述言語：英語   掲載種別：研究論文（学術雑誌）  

A self-consistent random phase approximation is proposed as an effective Hamiltonian method in light-front field theory. We apply the general idea to the light-front massive Schwinger model to obtain a new bound state equation and solve it numerically.

DOI： 10.1103/PhysRevD.60.065005

記述言語：英語   掲載種別：研究論文（学術雑誌）  

We present a continuum formulation for θ vacua in the massive Schwinger model on the light front, where θ enters as a background electric field. The effective coupling of the external field is partially screened due to vacuum polarization processes. For small fermion masses and small θ, we calculate the mass of the meson and find agreement with results from bosonization.

記述言語：英語   掲載種別：研究論文（学術雑誌）  

DOI： 10.1103/PhysRevD.57.2460

記述言語：英語   掲載種別：研究論文（学術雑誌）  

DOI： 10.1103/PhysRevD.55.6198

記述言語：英語   掲載種別：研究論文（学術雑誌）  

DOI： 10.1103/PhysRevD.55.4910

記述言語：英語   掲載種別：研究論文（学術雑誌）  

DOI： 10.1103/PhysRevD.54.7656

記述言語：英語   掲載種別：研究論文（学術雑誌）  

The spectrum of the massive Schwinger model in the strong coupling region is obtained by using the light-front Tamm-Dancoff (LFTD) approximation up to and including six-body states. We numerically confirm that the two-meson bound state has a negligibly small six-body component. Emphasis is on the usefulness of the information about states (wave functions). It is used for identifying the three-meson bound state among the states below the three-meson threshold. We also show that the two-meson bound state is well described by the wave function of the relative motion.

DOI： 10.1103/PhysRevD.52.2429

記述言語：英語   掲載種別：研究論文（学術雑誌）  

DOI： 10.1103/PhysRevD.49.4226

記述言語：英語   掲載種別：研究論文（学術雑誌）  

記述言語：英語   掲載種別：研究論文（学術雑誌）  

We calculate three- and four-point functions in super Liouville theory coupled to a super Coulomb gas on world sheets with spherical topology. We first integrate over the zero mode and assume that a parameter takes an integer value. We find the amplitudes, give plausibility arguments in favor of the result, and formally continue the parameter to an arbitrary real number. Remarkably, the result is completely parallel to the bosonic case.

DOI： 10.1103/PhysRevLett.68.1641

記述言語：英語   掲載種別：研究論文（学術雑誌）  

記述言語：英語   掲載種別：研究論文（学術雑誌）  

We show that under a certain assumption systems with second-class constraints can be regarded as gauge-fixed systems with first-class constraints. The massive Yang-Mills theory, a point particle on a sphere and the O(N) symmetric non-linear σ-model are considered as concrete examples.

DOI： 10.1007/BF01565618

記述言語：英語   掲載種別：研究論文（学術雑誌）  

We prove the equivalence of a recently proposed action for chiral bosons coupled to a gauge field to the effective action of chiral QCD₂. We extend the proof to include a one-parameter family of such candidates. We then show that only two values of the parameter are compatible with Lorentz covariance.

DOI： 10.1016/0370-2693(90)91213-U

記述言語：英語   掲載種別：研究論文（学術雑誌）  

記述言語：英語   掲載種別：研究論文（学術雑誌）  

Making use of chiral bosonization, we obtain a fermionic operator solution of the minimal chiral Schwinger model (where the right-handed fermion is absent) and study its physical content in a manifestly covariant operator formalism. We find a free chiral fermion and a free massive scalar as physical asymptotic fields. The existence of a physical asymptotic free chiral fermion distinguishes the chiral Schwinger model from the (vector) Schwinger model and implies that the fermion is not confined. We reconsider the usual chiral Schwinger model and compare it with the minimal one. They are completely consistent.

DOI： 10.1103/PhysRevD.42.4170

記述言語：英語   掲載種別：研究論文（学術雑誌）  

Anomalous gauge theories are considered in the gauge invariant and the gauge non-invariant formulations. We show that the currents which couple to gauge fields are conserved in both formulations. Equal-time commutators for the fermion charge density [(J_L⁰)^a(x),(J_L⁰)^b(y)]_ET are calculated explicitly in the bosonized chiral QCD₂. We emphasize the usefulness of the gauge invariant formulation.

DOI： 10.1016/0550-3213(90)90079-S

記述言語：英語   掲載種別：研究論文（学術雑誌）  

A Comment on the Letter by Srivastava, Phys. Rev. Lett. 63, 2791 (1989).

DOI： 10.1103/PhysRevLett.65.267

記述言語：英語   掲載種別：研究論文（学術雑誌）  

The chiral Schwinger model is reexamined by using chiral bosonization. The Lagrangian is obtained as a gauged Floreanini-Jackiw Lagrangian. We get a bosonic solution which contains one massive free boson and one (free) self-dual field.

DOI： 10.1103/PhysRevLett.64.139

記述言語：英語   掲載種別：研究論文（学術雑誌）  

Two dimensional anomalous non-Abelian gauge theories are studied following the recently-proposed scheme of quantization. The Gauss law operator (GLO) is modified by adding the Wess-Zumino action in the new scheme. By means of an explicit canonical operator construction, we confirm that this modified GLO is time independent and has no commutator anomalies in the two dimensional SU (2) model. Argument for the general validity of this analysis is also presented.

DOI： 10.1007/BF01412579

記述言語：英語   掲載種別：研究論文（学術雑誌）  

Starting from the modified Lagrangian of the bosonized chiral Schwinger model, operator solutions are obtained under three types of gauge fixing conditions. We show that the physical spectrum consists of a massive free boson and a massless excitation. We emphasize that the "longitudinal" component of the gauge field must be treated properly.

DOI： 10.1007/BF01560402

記述言語：英語   掲載種別：研究論文（学術雑誌）  

記述言語：英語   掲載種別：研究論文（学術雑誌）  

記述言語：英語   掲載種別：研究論文（学術雑誌）  

It is shown that there can be a mass generation in the chiral Schwinger model which has recently generated some controversy. Arguments are based on the path-integral formalism and a current regularization scheme which is a variant of the point-splitting regularization.

DOI： 10.1016/0370-2693(86)91234-7

開催年月日： 2018年9月

記述言語：日本語   会議種別：口頭発表（一般）  

開催地：長崎国際大学   国名：日本国  

開催年月日： 2018年7月

記述言語：英語   会議種別：口頭発表（一般）  

開催地：Caen   国名：フランス共和国  

We propose a new approach to Nuclear Effective Field Theory (NEFT) on a lattice on the basis of Renormalization Group (RG)analysis. In order to perform Markov-chain Monte Carlo lattice simulation of NEFT, we introduce auxiliary fields to integrate nucleon field so that its effects are represented as a determinant. The problem is that the determinant becomes complex and cannot be considered as a part of probability distribution function. We introduce a reweighting method, in which the reference determinant is chosen to be optimal in the RG analysis sense: the reference determinant contains only the relevant interactions and the closest to the original determinant. We calculate the standard deviation of the absolute value of the reweighting factor in a simple model, isospin-symmetric S-wave NLO NEFT without pions, and explain why our choice is optimal.

開催年月日： 2017年9月

記述言語：日本語   会議種別：口頭発表（一般）  

開催地：宇都宮大学峰キャンパス   国名：日本国  

繰り込み群の解析を元に、格子上での（パイオンを含まない）核子系有効場理論に対する再加重法の有効性を数値計算に基づいて示す。

開催年月日： 2016年11月

記述言語：日本語   会議種別：口頭発表（一般）  

開催地：福岡大学   国名：日本国  

格子上で定義された（パイオンを含まない）核子系有効場理論に対して、繰り込み群に基づく Re-weighting 法が、より素朴な方法に比べて優れていることを数値計算によって示した。

開催年月日： 2016年9月 - 2016年3月

記述言語：日本語   会議種別：口頭発表（一般）  

開催地：宮崎大学木花キャンパス   国名：日本国  

繰り込み群の解析を元に、格子上での（パイオンを含まない）核子系有効場理論に対する再加重法を提案する。

開催年月日： 2016年9月

記述言語：日本語   会議種別：口頭発表（一般）  

開催地：福岡工業大学   国名：日本国  

九州大学基幹教育科目「身の回りの物理学」における「反転学習」の導入の実践報告。

開催年月日： 2016年9月

記述言語：日本語   会議種別：口頭発表（一般）  

開催地：鹿児島大学   国名：日本国  

九州大学基幹教育科目「身の回りの物理学」におけるピア・インストラクションを活用した授業の実践報告。

開催年月日： 2016年3月

記述言語：日本語   会議種別：口頭発表（一般）  

開催地：東北学院大学泉キャンパス   国名：日本国  

格子上のハミルトニアン対角化によって求めた最低固有状態の固有値と、固有ベクトルから得られるANC(asymptotic normalization constant) を物理量として固定して、繰り込み群の解析を行う。

開催年月日： 2015年9月

記述言語：日本語   会議種別：口頭発表（一般）  

開催地：熊本学園大学   国名：日本国  

高大連携活動の一環として、福岡県立博多青松高校の生徒に対して行った3コマ（100分 x 3回）の講義の実施報告。

開催年月日： 2013年9月

記述言語：日本語   会議種別：口頭発表（一般）  

開催地：高知大学朝倉キャンパス   国名：日本国  

hybrid regularization を用いて、S波の2核子散乱を有効場理論によって記述することができる。

開催年月日： 2013年9月

記述言語：日本語   会議種別：口頭発表（一般）  

開催地：高知大学朝倉キャンパス   国名：日本国  

補助場を用いない Wilson 流くりこみ群の解析を行い、補助場を用いた解析との差について考察した。

開催年月日： 2013年9月

記述言語：日本語   会議種別：口頭発表（一般）  

開催地：九州大学箱崎キャンパス   国名：日本国  

核子系有効場理論は核子とパイオンを基本的な自由度とする強い相互作用の低エネルギー有効場理論である。この理論は本来的に非摂動論的であり、理論に現れる相互作用の性質を理解するためには、非摂動論的繰り込み群による解析が必須である。この講演では、我々のアプローチとその成果について簡単に説明する。

開催年月日： 2013年3月

記述言語：日本語   会議種別：口頭発表（一般）  

開催地：広島大学東広島キャンパス   国名：日本国  

非摂動論的くりこみ群を用いて、2つの p-wave 状態にある同種フェルミオンと、更に質量の異なる第3の粒子からなる系の束縛状態の様子を、質量比をパラメタとして解析する。

開催年月日： 2012年9月

記述言語：日本語   会議種別：口頭発表（一般）  

開催地：京都産業大学   国名：日本国  

ウィルソン流繰り込み群を用いた核子系有効場理論の解析では、パイオンの寄与を短距離部分と長距離部分に分離することが重要であった。この洞察に基づき、実際的な計算において、hybrid 正則化を用いることを提唱する。

開催年月日： 2012年9月

記述言語：英語   会議種別：口頭発表（一般）  

開催地：Centre Paul Langevin (Aussois)   国名：フランス共和国  

We formulate the three-body nonperturbative renormalization group equation without introducing an auxiliary field, known as a dimeron. We show that the Efimov parameter is obtained at the leading order within a 3% error. The previously obtained result with a dimeron has a 40% error. We point out that the previous formulation with dimerons has missing contributions. We also find a nobel nontrivial fixed point.

開催年月日： 2012年8月

記述言語：英語   会議種別：口頭発表（一般）  

開催地：福岡国際会議場   国名：日本国  

We analyze the P-wave nucleon-nucleon scattering including pions in the nonperturbative renormalization group method. Although it has been argued that this channel has an inconsistency of the power counting, we show that there is no such an inconsistency. A set of nonperturbative renormalization group equations is obtained.

開催年月日： 2012年3月

会議種別：口頭発表（一般）  

開催地：関西学院大学西宮上ヶ原キャンパス   国名：日本国  

開催年月日： 2012年3月

会議種別：口頭発表（一般）  

開催地：関西学院大学西宮上ヶ原キャンパス   国名：日本国  

開催年月日： 2011年9月

会議種別：口頭発表（一般）  

開催地：弘前大学文京町キャンパス   国名：日本国  

開催年月日： 2011年9月

会議種別：口頭発表（一般）  

開催地：弘前大学文京町キャンパス   国名：日本国  

開催年月日： 2011年8月 - 2011年9月

会議種別：口頭発表（一般）  

開催地：京都大学基礎物理学研究所   国名：日本国  

開催年月日： 2011年8月

会議種別：口頭発表（一般）  

開催地：International Hall, Sungkyunkwan University   国名：大韓民国  

開催年月日： 2011年8月

会議種別：口頭発表（一般）  

開催地：International Hall, Sungkyunkwan University   国名：大韓民国  

開催年月日： 2011年3月

会議種別：口頭発表（一般）  

開催地：新潟大学五十嵐キャンパス   国名：日本国  

開催年月日： 2010年9月

会議種別：口頭発表（一般）  

開催地：九州工業大学戸畑キャンパス   国名：日本国  

開催年月日： 2010年9月

会議種別：口頭発表（一般）  

開催地：九州工業大学戸畑キャンパス   国名：日本国  

会議種別：口頭発表（一般）  

開催地：東邦大学 (船橋市)   国名：日本国  

Theta vacuum in the massive Schwinger model

会議種別：口頭発表（一般）  

開催地：広島大学 (東広島市)   国名：日本国  

RPA for the light-front massive Schwinger model

開催地：京都大学基礎物理学研究所 (京都市)   国名：日本国  

3 Nucleon Forces From The 1/N_c Expansion Point of View

開催地：京都大学基礎物理学研究所 (京都市)   国名：日本国  

Analysis of Nuclear Effective Theory in terms of Non-Perturbative Renormalization Group

会議種別：口頭発表（一般）  

開催地：九州大学   国名：日本国  

Theta^+ resonance from the 1/N_c point of view

会議種別：口頭発表（一般）  

開催地：九州大学   国名：日本国  

Analysis of Nuclear Effective Theory with Nonperturbative Renormalization Group

会議種別：口頭発表（一般）  

開催地：SPring-8   国名：日本国  

Skyrme Model Revisited: An Effective Theory Approach and Application to the Pentaquarks

会議種別：口頭発表（一般）  

開催地：Santos   国名：ブラジル連邦共和国  

その他リンク： http://www.fb18.com.br/

会議種別：口頭発表（一般）  

開催地：首都大学東京   国名：日本国  

会議種別：口頭発表（一般）  

開催地：北海道大学札幌キャンパス   国名：日本国  

会議種別：口頭発表（一般）  

開催地：岡山理科大学   国名：日本国  

会議種別：口頭発表（一般）  

開催地：大分大学   国名：日本国  

会議種別：口頭発表（一般）  

開催地：近畿大学本部キャンパス   国名：日本国  

会議種別：口頭発表（一般）  

開催地：甲南大学岡本キャンパス   国名：日本国  

会議種別：口頭発表（一般）  

開催地：甲南大学岡本キャンパス   国名：日本国  

記述言語：日本語   掲載種別：記事・総説・解説・論説等（学術雑誌）  

Light-Front Tamm-Dancoff approximation and Relativistic Boundstates

種別：大会・シンポジウム等 

種別：大会・シンポジウム等 

種別：大会・シンポジウム等 

種別：大会・シンポジウム等 

種別：大会・シンポジウム等 

種別：大会・シンポジウム等 

「信州冬の学校」(京都大学基礎物理学研究所地域スクール）講義

企画、引率

対象：幼稚園以下,　小学生,　中学生,　高校生

種別：セミナー・ワークショップ

対象：社会人・一般,　学術団体,　企業,　市民団体,　行政機関

種別：講演会

対象：幼稚園以下,　小学生,　中学生,　高校生

種別：セミナー・ワークショップ

対象：幼稚園以下,　小学生,　中学生,　高校生

種別：セミナー・ワークショップ

対象：幼稚園以下,　小学生,　中学生,　高校生

種別：セミナー・ワークショップ

対象：社会人・一般,　学術団体,　企業,　市民団体,　行政機関

種別：その他

対象：幼稚園以下,　小学生,　中学生,　高校生

種別：セミナー・ワークショップ