平成３０年度
京都大学大学院理学研究科

Ｄ３発表会アブストラクト（平成３１年１月２１日）

物

理

学

第

二

分

野

Ｄ３ 発 表 会
日時

平成３１年１月２１日（月） ９時～

場所

理学研究科５号館 ５２５号室

発表時間

１５分＋５分（質問）《目次》

1 . Gravitational Wave Emission from Rapidly Rotating Very
Massive Stars

打田晴輝（９：００）

2 . Model-independent study on the internal structure of
exotic hadrons

神谷有輝（９：２０）

3 . Kinematics of Conformal Field Theory and Diagrams in
AdS Space京野秀紀（９：４０）

4 . Weyl invariance of string theories in generalized
supergravity backgrounds

坂本純一（１０：００）5 . KL→π0νν崩壊探索における背景事象の研究篠原智史（１０：２０）6 . Phases of Supersymmetric Gauge Theories
on the Three-Sphere清水

数馬（１０：４０）7 . MeVガンマ線望遠鏡ETCC気球実験SMILE-2+

竹村泰斗（１１：００）8 . 宇宙重力波干渉計を用いた短周期連星パルサーの観測に向けて西野裕基（１１：２０）9 . The Gluon Wigner Distribution with the gluon saturation
effects

午

午

萩原

慶一

（１１：４０）

後

10 . Development of a high pressure Xe gas TPC
for 0νββ decay search潘

11 . 大質量星形成における輻射フィードバックの多次元効果

福島肇（１３：２０）

12 .

松野

秀昭

（１３：４０）13 . Quantum Entanglement, Fidelity Susceptibility, andScrambling from AdS/CFT correspondence

宮地

真路（１４：００）14 . Gamow-Teller transitions in the light N=Z odd-odd nuclei

森田皓之（１４：２０）15 . Functional-renormalization-group aided
density-functional theory- ab-inito description of ground and excited states ofquantum many-body systems -横田猛（１４：４０）

16

OのE0 遷移と12C+αクラスター構造晟（１３：００）Gravitational Wave Emission from
Rapidly Rotating Very Massive Stars
基礎物理学研究所 宇宙グループ 打田晴輝
Abstract We compute gravitational waves emitted by the collapse of a rotating very massive star (VMS)
core leading directly to a black hole in axisymmetric numerical-relativity simulations. We find thatgravitational waves will be one of the targets for the third-generation detectors such as Einstein
Telescope.
© 2019 Department of Physics, Kyoto University

Gravitational collapse induced by pair instability (PI) is one of the final fates of very massive stars (VMSs) withmass ≳100M☉. Several observations suggest the existence of VMSs in the universe (e.g., [1]). However, theirformation and evolution process are still highly unknown. It is suggested that when a rotating VMS collapses to a
BH, strong gravitational waves would be emitted [2,3]. If the signal from this event can be observed, we canobtain the information about the internal structure of the VMS, which is considered to be of great use forunderstanding the nature of VMSs. Also, if the detected signal is from the Population III (PopIII) VMS, we canalso obtain the information about the nature of the PopIII stars, which are closely related to the evolution of theuniverse. To study the observability and properties of gravitational waves from this event, we perform
axisymmetric numerical relativity simulations of the gravitational collapse of a rotating PopIII VMS.
We select a progenitor star with the initial mass of MZAMS=320 M☉ (ZAMS: zero-age main sequence) androtating rigidly with the rotation velocity of 50% of the Kepler rotation at its surface. One-dimensional (1D)stellar evolution calculation is performed from the ZAMS stage until the central temperature reaches ~109.2 K
including the effects of hydrodynamical instabilities on the transport of angular momentum. At this stage, we map
the resulting 1D stellar evolution model onto two-dimensional (2D) grids for axisymmetric gravitational collapse
simulations as an initial condition. To consider the cases where the angular velocity is decreased due to otheradditional angular momentum transport mechanisms, we simulate several rotation models for which the angularvelocity is multiplied by a factor of 0.1-0.8.
We find that gravitational waves are composed of a short precursor and ringdown oscillation associated with theformed BH for all the models. The peak strain amplitude and the corresponding frequency of the axisymmetricmode of gravitational waves are ~10-22 and ≈300-600Hz for an event at the distance of D=50Mpc. Suchgravitational waves will be detectable only for D≲10Mpc by the second generation detectors, advanced LIGO,
advanced VIRGO, and KAGRA, even if the designed sensitivities for these detectors are achieved. However, thethird-generation detectors such as Einstein Telescope will be able to detect such gravitational waves for an eventup to D~100Mpc.

References[1] Crowther, P. A., et al., MNRAS, 458, 624 (2016)[2] M. Shibata et al., ApJ, 818, 157 (2016)[3] H. Uchida et al., ArXiv e-prints, 1809.10502 (2018)

Model-independent study on theinternal structure of exotic hadrons
基礎物理学研究所

原子核理論グループ

神谷有輝

Abstract To investigate the internal structure of exotic hadrons, we develop a method to distinguish theorigin of an eigenstate from the positions of the poles and zeros of the scattering amplitude. Applying themethod to 𝐼 = 0 𝐾𝑁-𝜋𝛴 amplitude, we discuss the structure of the Λ 1405 baryon.
© 2019 Department of Physics, Kyoto University

One of the most significant achievements in recent hadron physics is the discovery of many candidatesof exotic hadron states, which are not assigned to the simple 𝑞𝑞 meson nor 𝑞𝑞𝑞 baryon. By identifying theirinternal structure and acquiring the knowledge of the favored quark configuration, the understanding of the
non-perturbative region of the Quantum Chromo Dynamics (QCD) can be gradually deepened.
To identify a candidate of the exotics, we have to consider the various possible structures that areconsistent with its quantum numbers. However, it is very difficult to distinguish which model description is
the most appropriate to describe the internal structure of hadrons because of the model dependence. To avoid
the theoretical uncertainty, we need to discuss the structure based on the quantities that can be uniquelydetermined from the experimental observables. As such quantities, the on-shell scattering amplitude of thetwo-body scattering is the fundamental physical quantity which has the abundant information on the eigenstate.
Thus, by deriving the relation between the on-shell scattering amplitude and the structure of the eigenstate, we
can develop the method to investigate the exotic hadron candidates without model dependence.
In this talk, we discuss the relation between the analytic structure of the scattering amplitude and theorigin of an eigenstate. We introduce the zero coupling limit (ZCL) of the coupled-channel amplitude and weshow that the origin of the eigenstate is distinguished from the behavior of the eigenstate pole in the ZCL.
Based on the topological nature of the phase of the scattering amplitude, it is shown that if the eigenstate has
the hidden channel origin, the pole must encounter with the Castillejo–Dalitz–Dyson (CDD) zero [1-2], which
is defined as the zero of the scattering amplitude, in the ZCL. We show that the origin of the eigenstate can be
distinguished by analyzing the positions of the poles and CDD zeros. As an application to the candidate of theexotic hadrons, we discuss the structure of the Λ 1405 baryon. From the positions of the poles and zeros of
the isospin 𝐼 = 0 𝐾𝑁-𝜋𝛴 amplitude, we conclude that the origin of the high-mass (low-mass) pole of theΛ 1405 baryon is in the 𝐾𝑁 (𝜋𝛴) channel [3].
References[1] L. Castillejo, R. H. Dalitz, and F. J. Dyson, Phys. Rev. 101, 453 (1956).
[2] G. F. Chew and S. C. Frautschi, Phys. Rev. 124, 264 (1961).
[3] Y. Kamiya and T. Hyodo, Phys. Rev. D97 no.5, 054019 (2018).

Kinematics of Conformal Field Theory
and Diagrams in AdS Space
素粒子論研究室

京野秀紀

Abstract We discuss kinematic aspects of d-dimensional Euclidean conformal field theory and diagramsin (d+1)-dimensional Euclidean AdS space. Through an orthogonal basis called the conformal partial
wave, conformal block decompositions of four-point functions and four-point diagrams are systematicallyobtained. We will show some examples and applications.
© 2019 Department of Physics, Kyoto University

Conformal field theories (CFTs) appear in various places in theoretical physics, for example, string
theory, critical phenomena, etc. In such theories, the d-dimensional Poincare symmetry is enhanced tothe conformal symmetry which is described by SO(1,d+1). Due to the enhanced symmetry, thedynamics of theories is strongly restricted. The attempt to constrain CFTs under some physicalassumptions is called the conformal bootstrap. It is known that this approach works very well in twodimensions in which the conformal symmetry is enhanced further to the Virasoro symmetry.
Recently, there are some developments in (d>2)-dimensional CFT. In CFT, the conformal symmetry
restricts correlation functions, and two- and three-point functions are determined completely except foran overall constant. The first non-trivial quantities are four-point functions, and they are usually
analyzed by expanding them in terms of building blocks called the conformal blocks. In [1], it is foundthat the conformal blocks are characterized as eigenfunctions of the conformal Casimir equation, andthe explicit form of conformal block is derived. Based on this result, numerical approaches forconformal bootstrap are developed in this decade [2].
Another recently discussed concept is the conformal partial wave (CPW) introduced as an orthogonalbasis for the eigenfunctions of the conformal Casimir equation. Thanks to the orthogonality, CPW gives
us a systematic way to obtain the conformal block expansion of any four-point functions. This
procedure is packaged as the so-called OPE inversion formula. This formula can also be applied to fourpoint diagrams in (d + 1)-dimensional Euclidean AdS space, and then CPW is lifted to AdS space andcan be interpreted as a bulk diagram. There, a harmonic function in AdS space plays an essential role,
and we can see that the orthogonality of CPW comes from properties of the harmonic function. The
application to AdS diagrams would be useful not only to investigate the AdS/CFT correspondence, butalso as a technique to calculate CFT four-point functions.
In this talk, we introduce the inversion formula and see how the method works using some simple
correlation function and AdS diagrams. We will also mention the crossing kernel which is the innerproduct between CPWs in different channels. Through the crossing kernel, for example, t-channel
exchange diagrams or conformal blocks can be decomposed into s-channel CPWs. We will discuss theactual calculation of crossing kernel and possible applications to bootstrap approaches. This talk isbased on my recent works [3-5].
References[1] F. Dolan and H. Osborn, Nucl.Phys.B 628, 491 (2004).
[2]D. Poland, S. Rychkov and A. Vichi, [arXiv:1805.04405][3] H. Y. Chen, E. J. Kuo and H. Kyono, JHEP 1705, 070 (2017).
[4] H. Y. Chen, E. J. Kuo and H. Kyono, Nucl.Phys.B 931, 291 (2018).
[5] H. Y. Chen and H. Kyono, in preparation.

Weyl invariance of string theories
in generalized supergravity backgrounds
素粒子論研究室

坂本純一

Abstract A recent important progress of string theory is the discovery of generalized supergravity.
Remarkably, the equations of motion can be reproduced from the requirement of the kappa-symmetry.
However, the quantum consistency is not clear. In this talk, we discuss the Weyl invariance of a bosonicstring in generalized supergravity backgrounds.
© 2019 Department of Physics, Kyoto University

A recent important progress of string theory is the discovery of generalized supergravity [1,2]. The novel
effective theory was originally discovered in the recent study of ingerable deformations of the AdS5×S5superstring [1]. The characteristic feature of this theory is that the equations of motion contains a Killing vector
field I. The Killing vector I generates the trace of the non-geometric Q-flux, so that many solutions of generalized
supergravity can be regarded as T-folds [3].
The remarkable fact is that the equations of motion of generalized supergravity can be reproduced from therequirement of the kappa-symmetry in the Green-Swartz formalism. Originally, it is well known that the on-shell
constraints of type II supergravity ensure the kappa-symmetry of the string sigma model in the Green-Swartz
formulation [4,5]. Furthermore, it had been conjectured that the kappa-symmetry requires the type II supergravity
equations. However, after about thirty years, Tseytlin and Wulff [2] had reproduced the equations of motion oftype II generalized supergravity by solving the kappa-symmetry constraints on spacetime fields. In this way, an
old fundamental problem of string theory had been resolved.
The kappa-symmetry is a local fermionic symmetry to obtain the correct fermionic on-shell degrees of freedomof the Green-Swartz superstring theory. Therefore, the Tseytlin-Wulff’s result indicates the classical consistency ofa string in generalized supergravity backgrounds. However, at the quantum level, it is not clear that string theory
can be consistently defined on such backgrounds.
In this talk, we consider the Weyl invariance of bosonic string theory on generalized supergravity backgrounds.
An important observation in [6] is that the Double Field Theory, a T-duality manifest formulation of the massless
sector of string theory, can reproduce both the usual and generalized supergravity from a single action. By using
this result, we construct a possible counterterm to cancel the Weyl anomaly of a bosonic string in generalized
supergravity backgrounds [6]. This is a generalization of the Fradkin-Tseytlin term, and the modified term ischaracterized by the Killing vector I in the generalized supergravity equations. We further show that thecounterterm is definitely local [7]. In this sense, the usual supergravity backgrounds and the generalized
supergravity backgrounds can be treated on an equal footing in string theory.
References[1] G. Arutyunov, S. Frolov, B. Hoare, R. Roiban and A. A. Tseytli, Nucl. Phys. B903, 262-303 (2016).
[2] A.A. Tseytlin and L. Wulff, JHEP 1606, 174 (2016).
[3] J. J. Fernandez-Melgarejo, J. Sakamoto, Y. Sakatani and K. Yoshida, JHEP 1712, 108 (2017).
[4] M. T. Grisaru, P. S. Howe, L. Mezincescu, B. Nilsson and P. K. Townsend, Phys. Lett. 162B, 116 (1985).
[5] E. Bergshoeff, E. Sezgin and P. K. Townsend, Phys. Lett. 169B, 191 (1986).
[6] J. Sakamoto, Y. Sakatani and K. Yoshida, PTEP 2017, no. 5, 053B07 (2017).
[7] J. J. Fernandez-Melgarejo, J. Sakamoto, Y. Sakatani and K. Yoshida, hep-th/1811.10600 (2018).

KL→π0νν崩壊探索における背景事象の研究
高エネルギー研究室

篠原智史

Abstract The KOTO experiment aims to observe the CP-violating rare decay, KL→π0νν, at J-PARC. We
took data in 2016-2018 with a new barrel photon veto detector. We present the analysis status for the data
including the neutron induced background with a large amount of control sample.
© 2019 Department of Physics, Kyoto University

CP 対称性の破れは素粒子物理における標準理論の枠組みで説明される (小林・益川理論)。しかし、現在の物質優勢宇宙を説明するまでには至っておらず、標準理論を超えた新たな物理 (新物理) の寄与が必要である。KL→π0νν崩壊は CP 対称性を直接破る崩壊モードで、標準理論で予測される崩壊分岐
比は 3.0×10−11 と非常に小さく、分岐比の理論的な不定性も 1%程度と小さく抑えられている [1]。このため、新物理が崩壊に寄与していた場合の変化を大きく捉えることが可能である。
KOTO 実験は KL→π0νν崩壊の探索を目的とした実験であり、茨城県東海村に位置する大強度陽子加速器施設 (J-PARC) で行われている。KOTO 実験は 2013 年に物理ランを開始し実験感度 1.3×10−8 を達成
した [2]。2015 年の物理ランでは 2013 年の実験感度を約 10 倍更新した結果を発表し [3]、 2016 年以
降も 2017 年,2018 年と物理ランを行って 2015 年物理ランの約 1.5 倍多いデータを取得している。
KL→π0νν崩壊の終状態はπ0 の崩壊による２つのγと観測されないνである。信号事象の同定は、２つのγを CsI カロリメータで検出し、その他には何も検出されないということを veto 検出器で全崩
壊領域を覆い保証することで行う。
KOTO 実験における KL→π0νν崩壊探索の背景事象は、KL 崩壊由来と中性子反応由来の事象の２つに大別される。KL 由来の背景事象は、veto 可能なγが２つしかない KL→2π0 崩壊の背景事象を抑えることが鍵である。この KL→2π0 崩壊背景事象を 1/3 に削減するデザインの円筒型光子検出器(インナーバレル)が 2015 年の物理ラン後にインストールされ (Fig. 1)、2016 年以降の物理ランを行った。
中性子由来の背景事象は中性子が CsI カロリメータに入射し、反応を起こしてクラスターを生成後に再び中性子が放出され別のクラスターを生成することで背景事象となる。2015 年の物理解析では中性子
背景事象を評価するためのコントロールサンプルの統計量が少ないことが問題になっていた。このため、
2016,2017,2018 年の物理ランでは中性子コントロールサンプルを 2015 年解析の統計量の約 9 倍多く取得した。
本講演では上記の新しい円筒型光子検出器、中性子コントロールサンプルを用いて 2016,2017,2018
年以降に取得した物理データの背景事象の研究について報告する。

 (IB)IBCV

13.5X0and→18.5X
Fig. 1. Schematic view of KOTO :detectors
new barrel
photon veto detector (IB).
0References[1] A. J. Buras, et al. , Journal of High Energy Physics 11, 033 (2015).
[2] J. K. Ahn et al., PTEP, 021C01 (2017).
[3] J. K. Ahn et al. (KOTO collabolation) arXiv:1810.09655

Phases of Supersymmetric Gauge Theories
on the Three-Sphere
基礎物理学研究所素粒子論グループ

清水数馬

Abstract Three-dimensional supersymmetric gauge theory has been studied and provided us many
interesting results. This is mainly due to recent development of localization techniques. We found that
results from a localization technique cannot be interpreted by following flat-space intuition and discussed
them in relation to the flat-space point of view.
© 2019 Department of Physics, Kyoto University

Three-dimensional supersymmetric gauge theory has been studied in various contexts such as understanding
non-perturbative effects of gauge theories, which are necessary to understand strongly coupled theory represented
by the low energy physics of the quantum chromodynamics (QCD). The recent development of localization
techniques for supersymmetric field theory enables us to approach its non-perturbative aspects because for somequantities, the techniques reduce the path integral needed to calculate their expectation value to an ordinary
finite-dimensional integral. As a result, many new and interesting results have been obtained. However, a
localization technique usually requires a supersymmetric theory to be defined on a compact manifold to avoid
infrared divergence. Therefore, the results from localization techniques should not be interpreted by following
flat-space intuition, in particular, for non-conformal theory. However, there is little research which discusses
results obtained from the localization methods for non-conformal theory in viewpoints mentioned above. In ourrecent works [1,2,3,4,5], we found that the results from a localization technique cannot be interpreted by directly
following flat-space intuition and discussed them in relation to the flat-space point of view.
In this presentation, I would like to talk about my work [5]. In my work, we investigated the general behavior of
the partition function in the infinite mass limit through considering mass-deformed supersymmetric QCD. In theinfinite limit, results obtained from a localization technique can be associated with those in flat space. Thus, we
attempt to interpret the partition function in the flat-space language. In particular, mass-deformed supersymmetric
QCD provides us to a simpler partition function and then, is suitable for achieving our goal. We found that in theinfinite mass limit a point of the flat-space vacuum moduli space can dominantly contribute to the partition
function and it corresponds to that of the effective theory at the point. This vacuum selection does not always
agree with flat-space intuition. This result leads us to understand the problem that which flat-spacesupersymmetric vacua survive after coupling the curved background geometry and to shed lights understanding
our previous results in [1,2,3], in which the partition function of a mass-deformed Chern-Simons theory(mass-deformed ABJM theory [6,7]) exhibits such a singular behavior in terms of the flat-space supersymmetricvacua,

References[1] T. Nosaka, K. Shimizu and S. Terashima, JHEP 1603, 063 (2016).
[2] T. Nosaka, K. Shimizu and S. Terashima, JHEP 1703 (2017) 121.
[3] M. Honda, T. Nosaka, K. Shimizu and S. Terashima, arXiv:1807.08874 [hep-th].
[4] K. Shimizu and S. Terashima, JHEP 1811 (2018) 064.
[5] K. Shimizu, accepted in Journal of High Energy Physics.
[6] O. Aharony, O. Bergman, D. L. Jafferis and J. Maldacena, JHEP 0810 (2008) 091[7] J. Gomis, D. Rodriguez-Gomez, M. Van Raamsdonk and H. Verlinde, JHEP 0809, 113 (2008)

MeV ガンマ線望遠鏡 ETCC 気球実験 SMILE-2+
宇宙線研究室竹村泰斗

Abstract We developed a new ETCC for SMILE-2+, which has the effective area of 0.5 cm2 for 662 keV.
We launched SMILE-2+ balloon on April, 2018 at Australia and observed Crab nebula during 5 hours. By
the quick analysis, we obtained an excess of 4 at the detection of Crab nebula.
© 2019 Department of Physics, Kyoto University

MeV ガンマ線天文学は、核ガンマ線から元素プロセスの様相、遠方 GRB 観測により初代星の情報、炭素、酸素の励起ガンマ線観測により粒子加速の解明、など様々な宇宙・天体現象の情報が得られると期待されている。しかし、MeV ガンマ線天文学は、1991 年に打ち上げられた CGRO 衛星の COMPTEL[1]以降全天望遠鏡は存在せず、停滞しているのが現状である。この停滞は、宇宙線と衛星筐体の相互作用により発生する大量のバックグラウンドが取り除けないことや、既存の望遠鏡の Point Spread Function(PSF)が大きく広がっていることに起因している。そこで我々はこの問題を解決すべく電子飛跡検出型コンプトンカメラ(ETCC)[2,3]を開発している。ETCC は電子飛跡情報により到来ガンマ線の方向を一意に再構成する。これにより、既存の MeV ガンマ線望遠鏡では成しえなかった正確かつ 10 度程度の PSF(50%include @662 keV)を ETCC は有しており、この PSF により注目領域外からのバックグラウンドを 2 桁以上取り除く。
ETCC の MeV ガンマ線望遠鏡としての天体観測能力を実証すべく、sub-MeV において明るいかに星雲と銀河中心電子陽電子消滅線をターゲットとして 2018 年 4 月 7 日、豪州にて気球実験 SMILE-2+を実施した。しかし、従来の ETCC は 300 keV 以上のガンマ線に対して有効面積が急減し SMILE-2+には不適であった。SMILE-2+用の望遠鏡として、ガス領域から逃げ出す高エネルギー電子事象(escaped electron
event)(図 1)を測定可能とする改良を加えた新しい ETCC の設計、作製、試験[4]を 2017 年に行った。
SMILE-2+ ETCC は地上試験の結果、662 keV のガンマ線において有効面積~0.5 cm2(図 2)、PSF ~15 度の観測要求を満たす値を示した。SMILE-2+気球は高度 39 km、約 26 時間水平浮遊し、浮遊時間のほとんどにおいて ETCC システムは健全に動作し、かに星雲を約 5 時間、銀河中心を約 8 時間観測することに成功した。その後 ETCC システムと観測データを無事回収した。かに星雲の初期解析の結果、200-400 keV
において 4の有意度を得た(図 3)。気球実験により得られたガンマ線計数率と、ETCC の地上試験から求めた性能値から推定した計数率は一致している。本発表では SMILE-2+ ETCC の地上試験と SMILE-2+フラ
イト、かに星雲解析の初期成果について発表する。また、本発表における地上試験、かに星雲解析は従来解析 fully contained e- event のみを取り扱ったものである。
かに星雲領域
注目領域外
かに星雲領域-注目領域
外 推定値

energy [keV]

図 2 SMILE-2+ ETCC 有効面積 図 3 SMILE-2+気球実験により得られたかに星雲からのガンマ
References
線の計数率[1] V. Schonfelder, et al, A&ASS, Vol. 143 (2000), 145-179.
[2] T. Tanimori, et al., ApJ, 810(1), (2015) p. 28.
[3] T. Tanimori, et al., Scientific Reports, 7, (2017) p. 41511.
[4] 竹村泰斗, 他, 2017 年大気球シンポジウム, isas17-sbs-026
図 1 二つの解析手法

宇宙重力波干渉計を用いた短周期連星パルサーの観測に向けて
天体核研究室西野裕基

Abstract We propose a strategy to detect radio pulses from a short-period Galactic neutron star binary. The Laser
Interferometer Space Antenna has the potential to detect such a binary and could offer precise information on thesky position and binary parameters. These data could assist radio pulsar surveys significantly.
© 2019 Department of Physics, Kyoto University

連星中性子星は2つの中性子星からなる連星で、我々の銀河系内でこれまでに10例以上が電波で検出されている。特に軌道周期が短い連星中性子星は、軌道運動に対する一般相対論的な効果を測定可能で、一般相対論の検証などに用いられてきた。これまでに発見されている最も短い軌道周期の連星中性子星はPSR J1946+2052の1.88時間であるが[1]、より短い軌道周期の連星を見つけることができれば重力理論への制限や中性子星の強い磁気圏同士の相互作用を調べる試金石となることが期待される。LIGO-Virgoの観測チームによって、この近傍の宇宙での連星中性子星合体率が、誤差は大きいものの、1540 Gpc -3 year /0と推定されている[2]。我々の銀河系に相当する大きさの銀河が近傍宇宙に約0.01 Mpc /3の密度で存在するという推定を用いれば[3]、1つの銀河あたり連星中性子星の合体率はおよそ1.5 × 10/5 year /0 と考えられる。これから銀河系内の連星中性子星の数を見積もると、軌道周期が10分以下の連星中性子星がO(10)程度は存在すると期待される。軌道周期が10分程度の連星中性子星はおよそ3ミリヘルツの重力波を放出する。これは2030年代の運用に向けて計画中の宇宙重力波干渉計
The Laser Interferometer Space Antenna (LISA)で主な観測対象となる周波数帯でもある。例えば、
地球から10 kpc離れた1.4-1.4太陽質量の連星中性子星ならば、2年間の観測でLISAは信号雑音比200程度で重力波を検出する能力を有する予定である。このような高い信号雑音比で観測すれば、連星の方向や連星パラメータを極めて精度よく決定することが可能である。連星中性子星の形成過程を考慮す
ると、これらの連星の一方は磁場が弱く電波放出の活動性も穏やかであるのみならずビーミング率が高いパルサーである可能性が高いため、電波望遠鏡による観測も期待できる。
そこで、LISAを用いて短周期パルサーを発見する戦略について議論する[4]。まず、LISAの重力波解析で連星の方向がわかれば、全天探査と比べ必要な観測時間を大幅に減らすことができる。それだけではなく、短周期連星の電波パルスはDoppler効果による不鮮明化のために信号雑音比が下がってしまうことが考えられる。LISAによる軌道運動の位相の情報を用いることで、電波パルスの変調を補正しコヒーレントに足し上げることが可能となる。そのため、これまでに発見できなかったような暗いパルサーであっても高い信号雑音比で電波パルスを検出できるようになる。LISAと同時期に運用される可能性が高いSquare Kilometer Array (SKA)はアンテナ面積が100万平方メートルにも達する世界最高性能の電波干渉計となる予定である[5]。LISAの情報を最大限に利用してSKAでパルサー探査を行うことで、銀河系内にある軌道周期が10分以下の連星中性子星を発見できると期待できる。
References[1]Stovall, K., Freire, P.C.C., Chatterjee, S., et al. 2018, ApJL, 854, L22.
[2]Abbott, B.P., Abbott, R., Abbott, T.D., et al. 2017, Physical Review Letters, 119, 161101.
[3]Kalogera, V., Narayan, R., Spergel, D.N., & Taylor, J.H. 2001, ApJ, 556, 340.
[4]Kyutoku, K., Nishino, Y., & Seto, N. 2019, MNRAS, 483, 2615.
[5]Smits, R., Kramer, M., Stappers, B., et al. 2009, A&A, 493, 1161.

The Gluon Wigner Distribution
with the gluon saturation effects
Nuclear Theory Group

Yoshikazu Hagiwara

Abstract We investigate the gluon phase space distribution, called the gluon Wigner distribution, of thenucleon/nucleus at small Björken x. We also show how to access the gluon Wigner distribution frommeasurements.
© 2019 Department of Physics, Kyoto University

To understand the detailed structure of the nucleon, it is strongly required to investigate themulti-dimensional parton distribution functions. Recently, the Wigner functions, which are phasespace distribution functions of the parton depending on both position and momentum, have beenstudied. These Wigner functions are called the generating functions of the parton distributionfunctions because all the parton distribution functions are obtained by integrating or fixing theparameters in the Wigner function.
In high energy scattering, it is often the case that the Björken variable x is small. In the small
x region, the number of gluons is large, and the interior of the nucleon/nucleus is filled with thegluons. In this situation, the effects of the recombination process of gluons cannot be negligible andthe number of gluons becomes saturated inside the nucleon/nucleus. This phenomenon is called
gluon saturation. It is possible to incorporate the gluon saturation effects into the scattering
amplitude by solving the rapidity evolution equation, called the Balitsky-Kovchegov equation (BKequation) or B-JIMWLK equation. Then it is important and urgent tasks to know the small-x
behavior of multi-dimensional parton distribution functions.
It has been shown that a Wigner distribution can be described by quark and anti-quarkpair(dipole)-nucleon scattering amplitudes. To obtain the Wigner distribution, we need to solve theimpact parameter dependent BK equation. We have found that we can regard the BK equation as
an equation with only one variable, incorporating the SO(3) symmetry of the BK equation, and we
can have accurate solutions. We have evaluated the dipole Wigner distribution using thesesolutions and investigated its properties [1]. As a result of my calculation, we confirmed that thesefunctions have a positive peak at the momentum characteristic of gluon saturation physics.
In what kind of scattering process are the Wigner distributions obtained? It has been suggested that the
Wigner distributions can be obtained approximately from the di-jet production in deep inelastic scattering of thenucleon so far. We have shown that the Wigner distribution can be constructed from the scattering cross section of
the ultra-peripheral diffractive di-jet production [2]. The momentum transfer is very small in this scattering
process, so it is possible to establish a one to one correspondence between the cross section and the Wigner
distribution. This can be studied at the LHC.

References[1] Y. Hagiwara, Y. Hatta and T. Ueda, Phys. Rev. D 94, no. 9, 094036 (2016)[2] Y. Hagiwara, Y. Hatta, R. Pasechnik, M. Tasevsky and O. Teryaev, Phys. Rev. D 96, no. 3, 034009 (2017)

Development of a high pressure Xe gas TPC
for 0νββ decay search
高エネルギー物理学研究室

潘 晟

Abstract We are developing a high-pressure Xe gas TPC for neutrinoless double beta decay search. Ourdetector has a unique cellular readout structure which uses electroluminescence light to detect ionization
signals with high energy resolution. We developed a small size prototype detector and evaluated our
detector concept. We are going to develop a large size prototype detector to get know-how ofenlargement.
© 2019 Department of Physics, Kyoto University

ニュートリノがマヨラナ性を持つか否かという問いは現代物理学に残されている重要な問いのひとつであり、物質優勢宇宙やニュートリノの質量起源を解明するための大きな鍵となっている[1][2]。ニュー
トリノのマヨラナ性を確かめられるほぼ唯一の手段がニュートリノレス二重ベータ崩壊の観測である
が、我々は高圧キセノンガスを用いた Time Projection Chamber(TPC)を用いてこれを探索することを目指している。セル化された検出面内で電離電子をエレクトロルミネッセンス光に変換して信号を読み出す機構が最大の特徴であり、これによって一次荷電粒子の飛跡再構成および高いエネルギー分解能でのエネルギー測定が可能となる。我々のエネルギー分解能の目標は 136Xe の二重ベータ崩壊の Q 値である
2.4 MeV で 0.5%(FWHM)である。また、高圧ガスを用いることで大質量の崩壊核を容易に達成できる。
現在、我々は試作検出器を用いた原理検証および性能評価を行っている。原理検証のための試作機として、検出領域：φ10cm×9cm の円柱体積を持つ小型 TPC を製作し運用および性能評価を行った。キセノンを 4 気圧および 8 気圧封入し、122 keV と 356 keV のガンマ線を照射して性能評価行った[3]。356 keVのピークに対しては、2.58%(FWHM)のエネルギー分解能を得た(Fig.1)。他のピークから得られたエネル
ギー分解能と組み合わせることで、Q 値に外挿して 0.8～1.7%(FWHM)@2.4 MeV のエネルギー分解能が達成できる見込みであることを示した。
また、大型化に向けた研究としてφ50cm×50cm 程度の大型試作機の開発を行っている。小型試作機では信号読み出し機構のセル間隔は 7.5mm ピッチであったが、大型化に伴ってピッチの拡大を試みた。初めに 13mm ピッチのセルの読み出し機構を製作し、小型試作機を用いてテストを行った。13mm ピッチでは十分な性能を示すことができなかったが、得られたデータと詳細なシミュレーションを比較すること
で検出器の理解を深めることに成功した(Fig.2)。この結果を元にピッチの最適化を行った。

Fig.1 Spectrum of number of photons.

Fig.2 EL gain (NET) : data and simulation

References[1] T.Yanagita, Prog. Theor. Phys. 64 (3): 1103–1105 (1980)[2] M. Fukugita and T. Yanagida. Phys. Lett. B 174: 45-47 (1986)[3] S.Ban and K.D.Nakamura et al. Nuclear Instrumental and Methods A 875 : 185-192 (2017)

大質量星形成における
輻射フィードバックの多次元効果
天体核研究室福島 肇

Abstract We performed 2D radiation-hydrodynamics simulations for massive star formation. We findthat low-metal stars are more massive than solar metal stars in the cases with spherically symmetricaccretions or accretion rates larger than 4×10-3 Myr-1.
© 2019 Department of Physics, Kyoto University

大質量星形成では、原始星質量増加に伴い光度も大きくなり、輻射フィードバックが質量降着に影響を与える可能性がある。銀河系における大質量星形成では、ダスト粒子が受ける輻射圧により質量降着が抑制される[1,2]。一方、初代星形成では、ガス中にダスト粒子が含まれないため、HII 領域形成で生じる圧力差により質量降着が抑制される(UV フィードバック)[3,4]。これらの中間金属量を持つ低金属量星については、どちらの輻射フィードバックが支配的であるか知られていなかった。また、大質量星
質量の金属量依存性についても議論が続いている段階である。
本研究では、輻射圧および UV フィードバックの両方を含みかつ金属量依存性まで考慮した 2 次元輻
射流体コードを開発した。このコードは、公開コードである「PLUTO」に非平衡化学、輻射輸送、星進化やα粘性を加えたコードとなっている。得られた各雲質量に対する星形成効率は下図に示す。最初に、
雲質量が 250Mの場合において、1 次元球対称計算を行った。金属量が 1Zの場合には、輻射圧により原始星質量が 30Mで質量降着が止められてしまう。一方、金属量が 10-2Zの場合には、フィードバックは有効とならず、大部分のガスは落下する。２次元計算では、原始星周囲に降着円盤が形成される効果により、1Zにおいて星は 150Mとより大質量となる。逆に、10-2Zでは 160 Mと UV フィードバックの強度は弱まり、太陽金属量の場合とほぼ同程度の質量をもつ星が形成される。また、雲質量の増加について、500, 103Mの場合に計算を行った。1Zの場合には星形成効率は図に示すように 0.5 と一定であるが、10-2Zの場合には星質量の増加に伴い星形成効率も増加している。これは、降着率が 4×10-3 Myr-1
を超えることで、原始星半径の膨張・有効温度の低下が起こり、UV フィードバックが弱くなるためである。本研究により、高降着率や球対称に近い降着を伴う星形成では UV フィードバックの影響が小さくなるため、低金属量星形成ではより大質量星が形成されることがわかった。

Fig 1. The star formation efficiencies for various cloud masses.
Circles and Squares correspond to 1D and 2D simulations.
References[1] Wolfire M. G., Cassinelli J. P., 1987, ApJ, 319, 850[2] McKee C. F., Tan J. C., 2008, ApJ, 681, 771[3] Hosokawa T., Omukai K., Yoshida N., Yorke H. W., 2011, Science, 334, 1250

16

O の E0 遷移と 12C+クラスター構造
原子核理論研究室

松野秀昭

Abstract In 16O, the 0+ energy levels and the E0 transition matrix elements from the ground state areinvestigated. The E0 transition is found out to be sensitive to the intrinsic spin structure and weakcoupling structure of 12C+α cluster states.
© 2019 Department of Physics, Kyoto University

本研究は 16O の E0 遷移と 12C+クラスター構造に関する研究である．E0 遷移は元々重い原子核の構
造，或いは巨大共鳴が現れる高エネルギー領域における現象として注目されていた．しかし，12C において基底状態 01+から 3クラスター構造を持つ 02+状態への E0 遷移が大きいこと，また 11B における
11
B(d,d’)実験と反対称化分子動力学による理論計算から 11B の 3/23-状態は基底状態 3/21-からの E0 遷移が大きく，12C の 02+状態と似たような 2+t クラスター構造を持つことから，E0 遷移は軽い核のクラスター構造と関係すると主張されている[1]．
16
O について，その第一励起状態の角運動量とパリティは J=0+ (02+)である．この負パリティ状態はシ
ェル模型による 0p 閉殻構造から 1s0d 軌道への 1-particle and 1-hole 励起では説明できないものであり，
mysterious zero plus state と呼ばれていたが，現在では 12C+クラスター構造を持つことがよく知られている[2]．16O の基底状態からの E0 遷移強度が(,’)散乱によって測定[3]され，平均場理論に基づく乱雑位相近似計算[4]と比較されている．これによると，乱雑位相近似計算は高エネルギー領域における実験値を再現するが，低エネルギー領域に現れる遷移強度のピークを再現することができない．一方で，クラスター構造を仮定すると 16O の基底状態から低エネルギー領域に存在する励起状態への E0 遷移を説明できる[5]．しかし，文献[5]は 4クラスター模型による計算であり，模型計算にクラスターの崩れの効
果は取り込まれていない．
本研究では，特に 12C+クラスター構造の 12C 部分に着目して 16O の基底状態からの E0 遷移とクラス
ター構造の関係を調べた[6]．本研究では核子の交換に関する反対称化の操作を完全に行った微視的模型
で 12C クラスター部分の 3構造 12C(3)とクラスターが崩れた 0p3/2 閉殻構造 12C(0p3/2)の両方を扱った
上で，基底状態からの E0 遷移を計算した．また，12C 部分の回転を考慮して 12C+クラスターを弱結合的に扱った場合と 4クラスターが正三角錐型に配置された場合を比較した．
本研究により以下の 2 つの知見が得られた．第 1 に 12C クラスター部分が 3構造である 12C(3)+ク
ラスター構造に対して 12C クラスター部分が 0p3/2 閉殻的である 12C(0p3/2) +クラスター構造を加えて計算を行うことで，01+状態から 02+状態への E0 遷移が抑制されることが分かった．これは E0 遷移がスピン S を変化させない為，スピンが 0 の 0p 閉殻的な構造を持つ 01+状態からの E0 遷移は，スピンが 0 の
12C(3)+クラスター構造を持つ 02+状態には起こりやすいが，有限のスピンを持つ 12C(0p3/2) +クラスタ
ー構造が混ざると 02+状態と 01+状態のスピン構造に差が生じるからである．第 2 に 0p 閉殻的な構造を持つ基底状態からの E0 遷移は 4クラスターが正三角錐型に配置された構造に対して起こりやすく，4
クラスターが正三角錐型に配置された場合の計算に対して 12C 部分の回転を考慮して 12C+クラスター
を弱結合的に扱うと模型空間に 4クラスターが平面的に配置された構造が取り込まれ，基底状態からのE0 遷移が抑制されることが分かった．クラスターを弱結合的に扱うことはエネルギー準位を正確に記述するのに必要であるだけでなく，基底状態からの E0 遷移を正しく表すにも必要である．本研究の結果
は Progress of Theoretical and Experimental Physics 誌に掲載されている[6]。
References[1] T. Kawabata et al., Phys. Lett. B 646, 6 (2007).
[2] H. Horiuchi and K. Ikeda, Prog. Theor. Phys. 40, 277 (1968).
[3] Y.-W. Lui, H. L. Clark, and D. H. Youngblood, Phys. Rev. C 64, 064308 (2001).
[4] Z. Ma, N. Van Giai, H. Toki, and M. L’Huillier, Phys. Rev. C 55, 2385 (1997).
[5] T. Yamada, Y. Funaki, H. Horiuchi, K. Ikeda, and A. Tohsaki, Prog. Theor. Phys. 120, 1139 (2008).
[6] H. Matsuno et al., Prog. Theor. Exp. Phys. 2017, 063D01 (2017).

Quantum Entanglement, Fidelity Susceptibility, and Scramblingfrom AdS/CFT correspondence
Yukawa Institute for Theoretical Physics

Masamichi Miyaji

Abstract I consider several quantum information theoretic quantities and phenomena from the viewpointof AdS/CFT correspondence. First I will consider fidelity susceptibility, which measures the distance
between states, and propose its counterpart in gravity. Then I apply fidelity susceptibility to scrambling,and show how fidelity susceptibility can capture scrambling. Finally, I will consider entangling anddisentangling operations in CFT, and study their counter part in gravity, and effects on CFT states .
© 2019 Department of Physics, Kyoto University

In this thesis, I will study several phenomena and quantities which are intimately related to quantum information
theory, using AdS/CFT correspondence. AdS/CFT correspondence is the conjecture on the equivalence between
quantum gravity on Anti de Sitter(AdS) space and quantum field theory on the boundary of AdS.
I will first study fidelity susceptibility, which measures distance between quantum states, using AdS/CFT
correspondence. I will propose a holographic dual of fidelity susceptibility, is given by the volume of maximal
volume bulk time slice, anchored from the boundary time slice. This proposal enables us to compute fidelity
susceptibility of states which evolve non trivially in time.
Then I will apply fidelity susceptibility to study the phenomenon called scrambling. When the initial excitation iscompletely mixed with the environment, we call the excitation is scrambled. I will show that the particularconfiguration of fidelity susceptibility can capture scrambling, and I will describe how this picture is consistent withthe proposed holographic dual of fidelity susceptibility.
Finally, I will consider non local operation in both CFT and gravity. Such operation corresponds to changing
entanglement structure. And I will also study how entanglement structure and averaged null energy are changed bysuch non local operations in CFT, and also how the dual gravity evolves in time.

Fig. 1. Maximal volume time slice inShock wave geometry.
Shock wave geometry. .

Fig.2. Propagation of null energy density after
entangling operation in CFT.

References[1]Miyaji, Numasawa, Shiba, Takayanagi, Watanabe “Distance between Quantum States and Gauge-Gravity
Duality”, Phys. Rev. Lett 115 (2015)[2]Miyaji, “Butterflies from Information Metric”, JHEP 1609 (2016) 002[3]Miyaji, “Time Evolution after Double Trace Deformation”, JHEP 1810 (2018)074

Gamow-Teller transitions in the light N=Z odd-odd nuclei

原子核理論研究室

森田皓之

Abstract I have investigated the Gamow-Teller transitions in the light N=Z odd-odd nuclei by using theantisymmetrized molecular dynamics. These GT transitions occur between the two-nucleon pairs such as
neutron-neutron and proton-neutron pairs which restore SU(4) symmetry. The important point is that the
proton-neutron pairs spatially develop and make cluster structures.
© 2019 Department of Physics, Kyoto University

N=Z odd-odd nuclei are singular subjects in nuclear physics. There are competing isovector (T=1) andisoscalar (T=0) states in the low-lying spectra, where isovector and isoscalar proton-neutron correlations play
important roles.
The recent studies of the mean-field calculations and the experiments have found the strong
Gamow-Teller (GT) strengths near the isobaric analog state in the low-lying regions. These states are called
low-energy super Gamow-Teller (LeSGT) transitions which correspond to degeneracy of isovector andisoscalar states of the proton-neutron pairs, that is, SU(4) symmetry in the nuclei.
These phenomena have been limitedly discussed for the pf-shell nuclei. It is expected to expand the idea tothe lighter nuclei. However, the mean-field methods are not stable for describing clustering phenomena
which are broadly found in the light nuclei.
In this talk, I show a new framework which can deal with proton-neutron correlations and clustering in thesame footing. I call this method isospin projected antisymmtrized molecular dynamics (Tβγ-AMD) [1].
By using this method, I have investigated the Gamow-Teller transitions between the N=Z+2 nuclei to the
N=Z odd-odd nuclei in the p-shell [2]. I have found the strong Gamow-Teller transitions exhausting 50% of
the sum-rule in 6He(01+1)→6Li(11+0), 10Be(01+1)→10B(11+0), and 14C(01+1)→14N(12+0). In these states, theisoscalar proton-neutron pairs make the low-lying spectra in the final states of 6Li(11+0), 10B(11+0), and14
N(12+0). These pairs show clustering nature which play important role to realize SU(4) symmetry.
I have also applied the Tβγ-AMD to 22Na comparing with 10B and comprehensively investigated SU(4)symmetry in the light deformed N=Z odd-odd nuclei [3]. The proton-neutron pairs are formed at surfaces ofthe prolately deformed cores (20Ne=16O+α, 8Be=2α) in both nuclei. I have obtained the Gamow-Teller
strengths 22Ne(01+1) →22Na(11,2+0) whose summation exhausts 50% of the sum-rule value, but the strengths
are fragmented into the half. This indicates that SU(4) symmetry of the proton-neutron pairs is broken as aresult of spin-orbit interactions on quadrupole deformations. In fact, 22Na(11,2+0) have different K-quanta,
which are defined in the deformed state, with K=0 and K=1. Each state contains proton-neutron pair with
anti-aligned spin (Sz=0) and with aligned spin (Sz=1), respectively.
References[1] H. Morita and Y. Kanada-En’yo, Prog. Theor. Exp. Phys. 2016, 103D02 (2016).
[2] H. Morita and Y. Kanada-En'yo, Phys. Rev. C 96, 044318 (2017)[3] H. Morita and Y. Kanada-En'yo, Phys. Rev. C 98, 034307 (2018)

Functional-renormalization-group aided
density-functional theory- ab-inito description of ground and excited states ofquantum many-body systems 原子核理論研究室

横田猛

Abstract We formulate the functional-renormalization-group aided density-functional theory (FRG-DFT)
for infinite homogeneous matter. The applications of the FRG-DFT to infinite nuclear matter andtwo-dimensional homogeneous electron gas are presented. These demonstrations show that the FRG-DFT
describes ground and excited states in a unified manner and is applicable to more-than-one-dimensional
realistic models.
© 2019 Department of Physics, Kyoto University

The functional renormalization group (FRG) is a fundamental tool in the field theory. One of recent significant
developments regarding the FRG is an attempt to employ it for the formulation of the density functional theory(DFT) [1,2], which we call the functional-renormalization-group aided density-functional theory (FRG-DFT). The
FRG-DFT is expected to become a powerful approach for the fundamental problems of the DFT such as the
microscopic determination of the energy density functional and the analyses of excited states involving thelarge-amplitude collective dynamics.
In this presentation, our works on the FRG-DFT toward the unified description of the ground and excited states
in realistic models are presented. Together with my collaborators, I formulate the FRG-DFT for infinite
homogeneous matters [3] and apply it to two models [3-5].
In the first application, we calculate the equation of state (EOS) [3] and the density-density spectral function [4]of the one-dimensional homogeneous matter composed of spinless Fermions with a non-local interaction showing
a short-range repulsion and a long-range attraction like the nuclear force. We find that the saturation energy
extracted from the EOS coincides with that obtained from the Monte Carlo (MC) calculation within a few percent.
Moreover, the spectral function is found to reproduce a notable feature of the non-linear Tomonaga-Luttinger
liquid that the spectral function has singularities at the edge of its support on the lower-energy side. Thisapplication is the first study in which the ground and excited states are analyzed in a unified manner with the
FRG-DFT.
The second application is the analysis of the two-dimensional homogeneous electron gas (2DHEG) [5]. This is
the first example in which a more-than-one-dimensional realistic model is analyzed. The correlation energies arecalculated for various Wigner-Seitz radii and found to completely reproduce the exact result in the high-density
limit. In the finite density case, we find that the result with the FRG-DFT shows good agreement with the MC
results in the higher-density case, although the discrepancy between FRG-DFT and MC results becomes larger as
the system becomes dilute.
Our results suggest that the FRG-DFT is a promising method which is applicable to more-than-one-dimensional
realistic quantum many-body systems and realizes the unified description of the ground and excited states.
References[1] J. Polonyi and K. Sailer. E, Phys. Rev. B66:155113 (2002).
[2] A. Schwenk and J. Polonyi, In 32nd International Workshop on Gross Properties of Nuclei and Nuclear
Excitation: Probing Nuclei and Nucleons with Electrons and Photons (Hirschegg 2004) Hirschegg, Austria,
January 11-17, 2004, pages 273-282 (2004).
[3] T. Yokota, K. Yoshida, and T. Kunihiro, Phys. Rev. C, in press, arXiv:1803.07439.
[4] T. Yokota, K. Yoshida, and T. Kunihiro, PTEP Letter, in press, arXiv:1810.00422.
[5] T. Yokota, T. Naito, arXiv:1812.00588.