KEK-PH Lectures and Workshops 2021

Asia/Tokyo
Description

"KEK-PH lectures and workshops" is a form of KEK-PH workshop series at the time of Covid-19.

The annual KEK Theory Meeting on Particle Physics Phenomenology (KEK-PH) covers many topics in Particle Physics and Cosmology, from the Standard Model and models beyond it to particle cosmology and astrophysics. At the time of Covid-19, the KEK theory center is organizing an on-line lecture and workshop series, "KEK-PH lectures and workshops 2021."


6th KEK-PH + 2nd KEK-COSMO joint mini-workshop

This time the KEK Theory Center is organizing the phenomenology and cosmology-themed mini workshop, the 6th KEK-PH and the 2nd KEK-Cosmo, which is mainly made up of contribution talks by young researchers held on 9th and 10th, March, 2022.  Prior to the session of the contributed talks, on the morning of the 9th, we are going to hold a special invited talk by Prof. Wei Xue (U of Florida) about the structure formation by axion.
 
Program: 
 
Plenary session
Mar. 9th (Wed.) 11:05-12:00:  
Prof. Wei Xue (University of Florida), "Resonant excitation of the axion field during the QCD phase transition"
 

Short talk sessions

 Mar. 9th (Wed.) 13:30-16:55 and Mar. 10th (Thu.) 11:00-16:55

We invite the following young researchers to give talks:

Yoshihiko Abe (Kyoto U.), "Origin of pseudo-Nambu-Goldstone dark matter"

Kazuki Enomoto (Osaka U), "Electroweak baryogenesis in the three-loop neutrino mass model with dark matter"

Motoko Fujiwara (Nagoya U), "Electroweakly interacting spin-1 dark matter and its phenomenology"

Yu Hamada (KEK), "Electroweak-Skyrmion as Asymmetric Dark Matter"

Minxi He (KEK), "Reheating after Mixed Higgs-R^2 Inflation"

Asuka Ito (TITech), "Searching for axion dark matter/gravitational waves with magnons"

Naoya Kitajima (Tohoku U.), "Parametric resonance instability of the QCD axion"

* In the short talk sessions, all topics (including those not related with the plenary talk) are welcome. Also, contributions from students, postdocs and faculty staffs are all welcome.

 

Registration dead line:  
23rd (Wed.) Feb. 18:00 (JST), to apply for a short talk

8th (Tue.) Mar. 18:00 (JST), only for your participation

Zoom link will be sent to the registered e-mail address.

 

 

The 5th KEK-PH on "Jet Physics"

In the search for new physics at the LHC experiment, jet is often produced from heavy particle decays. By studying the jet structure, we can reconstruct particles with high momentum, such as W, Z, top, and H, and increase the sensitivity to new physics. In "KEK-PH Jet Physics", we will discuss recent theoretical developments, the latest data from the ATLAS and CMS experiments, and the expected sensitivity at the HL-LHC from both theoretical and experimental perspectives.
 
Program: 
 
Invited talks
 
Nov. 30th (Tue.)
16:15-17:00:  Prof. Takuya Nobe (ICEPP, Tokyo), "Jet physics with ATLAS"
17:00-18:00:  Prof. Gavin Salam (Oxford), "Jets through the LHC era"
 
Dec. 1st (Wed.)
10:00-10:45: Prof. Cristina Mantilla (FermiLab), "Boosted jet physics in CMS" 
 

 

The 4th KEK-PH on "New Ideas in Particle Physics"

We are now preparing a workshop on "New ideas in particle physics," on Nov. 16 and 17. This time, it is a joint workshop with Florida State University (co-organizer: Kosaku Tobioka). The topics cover cosmological solutions to the naturalness problems, swampland conjectures, as well as quantum gravity effects on low energy physics.

Program

https://conference-indico.kek.jp/event/141/timetable/#day-2021-11-16

Invited talks

First day:
16th (Tue.), Nov. 16:00-19:15 (JST)

  • Michael Geller (Tel Aviv U.), "Crunching Naturalness" 
  • Raffaele D'Agnolo (IPhT, Saclay), "Aspects of Cosmological Selection of the Weak Scale"
  • Gia Dvali (Munich U., ASC and Munich, Max Planck Inst.), "S-matrix exclusion of de Sitter landscape, and naturalness"
  • Matthew McCullough (CERN), "Gegenbauer Goldstones"

Second day:
17th (Wed.), Nov. 9:00-12:30 (JST)

  • Surjeet Rajendran (Johns Hopkins U.), "A Causal Framework for Non Linear Quantum Mechanics"
  • Anson Hook (Maryland U.), "Solving the naturalness puzzle using old ideas"
  • Yuta Hamada (Harvard U.), "Brane Probes, Finiteness and Distance Conjecture"
  • Tom Rudelius (UC, Berkeley), "Consequences of No Global Symmetries in Quantum Gravity"

Registration dead line:  

15th (Mon.) Nov. 18:00 (JST)

Zoom link will be sent to the registered e-mail address.

Sponsor:
Grant-in-Aid for Scientific Research on Innovative Areas (18H05542), Japan
Scientific Research A (19H00689), Japan
Scientific Research B (21H01086), Japan


The 3rd KEK-PH + 1st KEK-Cosmo joint workshop on "Primordial Black Holes"

Convener(s): Kazunori Kohri and Kyohei Mukaida (KEK/Theory)

Program

https://conference-indico.kek.jp/event/141/timetable/#day-2021-10-19
 

Invited talks

First invited talk:
19th (Tue.), Oct. 16:00-17:30 (JST):

Dr. Gabriele Franciolini (Geneva U), "Primordial Black Holes and Gravitational Wave Observations"

Second invited talk:
20th (Wed.), Oct. 16:00-17:30 (JST): 

Dr.  Christian Byrnes (Sussex U), "Primordial black holes as a LIGO-Virgo and dark matter candidate"

Zoom link will be sent to the registered e-mail address.

Short talks

19th (Tue.), Oct. 13:30-15:30: 

13:30 - 13:55: Marcos Flores (UCLA), "Primordial Black Holes from Long-Range Scalar Forces and Scalar Radiative Cooling"

14:00 - 14:25: Yuichiro Tada (Nagoya U), "Primordial black holes in peak theory with a non-Gaussian tail"

14:30 - 14:55: Tomohiro Harada (Rikkyo U), "Spins of primordial black holes formed in the radiation-dominated phase of the universe: first-order effect"

15:00 - 15:25: Qianhang Ding (HKUST), "Ultrahigh-energy Gamma Rays and Gravitational Waves from Primordial Exotic Stellar Bubbles"

Registration deadlines:


28th (Tue.),  Sep. 17:00 (JST): to apply for a short talk
18th (Mon.), Oct. 17:00 (JST): only for your participation

 


2nd KEK-PH on "Next Generation Accelerators"

Program

https://conference-indico.kek.jp/event/141/timetable/#day-2021-06-23

Invited talks

First talk:
June 23 16:00-17:30: Prof. Mitsuhiro Yoshida (Accelerator Laboratory, KEK), "
Future laser and beam driven high gradient accelerator technology"

Registration dead line: June 21 (Mon.)  June 22 (Tue.) 17:00(JST)

Second talk:
June 30 16:00-17:30: Prof.
Daniel Schulte (CERN), "Muon Collider"

Registration dead line: June 29 (Tue.) 17:00(JST)

Zoom link will be sent to the registered e-mail address.


1st KEK-PH on "Muon g-2"

Program

https://conference-indico.kek.jp/event/141/timetable/#day-2021-05-11

Invited talks

May 11 17:00-18:30: Dr. Massimo Passera (INFN, Padua), "Muon g-2 and Δα connection"

May 19 17:00-18:30: Prof. Christoph Lehner (Regensburg U. and Brookhaven Natl. Lab.), "Consistency of the hadronic vacuum polarization between lattice QCD and the R-ratio"


Organizers: Motoi Endo, Amon Furuichi, Toru Goto, Yu Hamada, Minxi He, Takahisa Igata, Ryuichiro Kitano, Kazunori Kohri, Takahiko Matsubara, Ryutaro Matsudo, Satoshi Mishima, Kyohei Mukaida, Kazunori Nakayama, Mihoko M. Nojiri, Hajime Otsuka, Yutaka Sakamura, Kengo Shimada, Hiromasa Takaura, Yuko Urakawa


Participants
  • Ahmed Hammad
  • Aiichi Iwazaki
  • Aine Kobayashi
  • Akihiro Doi
  • Akimasa ISHIKAWA
  • Akio Sugamoto
  • Akio Tomiya
  • Akira Matsumoto
  • Akira Yamamoto
  • Akitoshi Ueda
  • Albert Escrivà
  • Alessandro Parisi
  • ALESSANDRO VALENTI
  • Alexander Kusenko
  • Alexander Prygarin
  • Amjad Ashoorioon
  • Amon Furuichi
  • Amon Furuichi
  • Aoto Tanaka
  • Apriadi Salim Adam
  • Apriadi Salim Adam
  • Asuka Ito
  • Asuka Ito
  • Atsushi Hinata
  • Atsushi Horikoshi
  • Atsushi Nakamura
  • Atsushi Nishizawa
  • Atsuya Niki
  • Atsuya Niki
  • Atsuya Niki
  • Atsuyuki Yamada
  • Bing Sun
  • Bruno Scheihing
  • Ce Zhang
  • Cendikia Abdi
  • Chao Chen
  • Chengcheng Han
  • Chisato Ikuta
  • Chongzhi Li
  • Chul Kim
  • Chulmoon Yoo
  • daigo shimoguchi
  • Daiki Ueda
  • Daisuke Jido
  • Daisuke Nomura
  • Daisuke Takahashi
  • Daisuke Yokoyama
  • Dan Kondo
  • Dan Kondo
  • Dan Kondo
  • Dan Kondo
  • Daniel Jeans
  • Daniele Teresi
  • Denny Lane Sombillo
  • Dimitrios Giataganas
  • Dong Woo Kang
  • Edoardo Spezzano
  • Eigo Shintani
  • eiji hayashi
  • Eung Jin Chun
  • Eung Jin Chun
  • Fathiyya Izzatun Az Zahra
  • Francesca Borzumati
  • Fumihiro Takayama
  • Genta Sato
  • Georgiy Razuvaev
  • Guillem Domenech
  • Hajime Otsuka
  • Haruka Asada
  • Haruki Takahashi
  • Haruki Takahashi
  • Haruki Takahashi
  • Haruki Takahashi
  • Haruki Takahashi
  • Hidenori Fukaya
  • Hiroaki Sugiyama
  • Hiroaki Sugiyama
  • Hiroki Hoshina
  • Hiroki Sakamoto
  • Hiromasa Takaura
  • Hiromasa Takaura
  • Hiromasa Takaura
  • Hiromasa TAKAURA
  • Hiromasa Takaura
  • Hiromichi Kichimi
  • Hiroto Shibuya
  • Hirotsugu Fujii
  • Hiroyasu Ego
  • Hiroyuki Ishida
  • Hiroyuki Ishida
  • Hiroyuki Ishida
  • Hiroyuki Ishida
  • Hisakazu Minakata
  • Howard Haber
  • Hrishabh Bharadwaj
  • Ibuki Terashima
  • Ilia Musco
  • isamu nakamura
  • Issaku Kanamori
  • Jihun Kim
  • JINHEUNG KIM
  • Joe Sato
  • Joe Sato
  • Junichi Tanaka
  • Junichiro Kawamura
  • Junichiro Kawamura
  • Junji Hisano
  • Junji Hisano
  • Junji Hisano
  • Junpei Shirai
  • Juntaro Wada
  • Jurina Nakajima
  • Kai Murai
  • Kai Murai
  • Kaoru Hagiwara
  • Katsuhiko Ishida
  • KATSUHIKO SATO
  • Katsumasa Ikematsu
  • Katsuo Tokushuku
  • Kayoung Ban
  • Kaz Kohri
  • Kaz Kohri
  • Kaz Kohri
  • Kazuhiro Tanaka
  • Kazuhiro Tobe
  • Kazuhito Suzuki
  • Kazuki Enomoto
  • Kazuki Enomoto
  • Kazuki Tanaka
  • Kazumichi SUMI
  • Kazunari Shima
  • Kazunori Itakura
  • Kazunori Itakura
  • Kazunori Itakura
  • Kazunori Kohri
  • Kazunori Kohri
  • Kazunori Nakayama
  • Kazunori Nakayama
  • kazuo Fujikawa
  • Kazutaka SUMISAWA
  • Kei Sano
  • Kei Yamamoto
  • Kei Yamamoto
  • Kei Yamamoto
  • Kei Yamamoto
  • Kei-Ichi Kondo
  • Kei-Ichi Kondo
  • Keiichi Watanabe
  • Keiichi Watanabe
  • Keiko Nagao
  • Keiko Nagao
  • Keiko Nagao
  • Keiko Nagao
  • Keisho Hidaka
  • Keisho Hidaka
  • Keisho Hidaka
  • Keiya Ishiguro
  • Ken-ichi Hikasa
  • Ken-ichi Okumura
  • Kengo Kikuchi
  • Kengo Shimada
  • Kengo Shimada
  • Kengo Shimada
  • Kengo Shimada
  • Kengo Shimada
  • Kenichi Saikawa
  • kenji kadota
  • kenji kadota
  • kenji kadota
  • Kenji Kadota
  • Kensuke Akita
  • Kentarou Mawatari
  • Kentarou Mawatari
  • Kentarou Mawatari
  • Kentarou Mawatari
  • Kentarou Mawatari
  • Kentarou Mawatari
  • Kento Asai
  • Kento Asai
  • Kento Asai
  • Kento Asai
  • Kento Asai
  • Ki-ichiro Sato
  • Kimihiro Nomura
  • Kimiko Yamashita
  • Kimiko Yamashita
  • Kimiko Yamashita
  • Kingman Cheung
  • Kiyoharu Kawana
  • Kiyoharu Kawana
  • Kiyoharu Kawana
  • Kiyoharu Kawana
  • Kiyoshi Higashijima
  • Kodai Sakurai
  • Kohei Kamada
  • Kohsaku Tobioka
  • Kohsaku Tobioka
  • Koichi Hamaguchi
  • Koichi Hamaguchi
  • Koichi Hattori
  • Koichi Hirano
  • Koichi Hirano
  • Koichiro Shimomura
  • Koji Ishiwata
  • Koji Tsumura
  • Kolahal Bhattacharya
  • Koutarou Kyutoku
  • Kunihiro Nagano
  • Kyohei Mukaida
  • Kyohei Mukaida
  • Kyohei Mukaida
  • Kyohei Mukaida
  • Lakmin Wickremasinghe
  • Leonardo Darini
  • luigi delbuono
  • Lukas Berns
  • Makiko Nio
  • Marcos Flores
  • Mario Reig
  • Masaharu Tanabashi
  • Masahiro Kuze
  • Masahiro Kuze
  • Masahiro Yamaguchi
  • Masahito Ogata
  • Masahito Yamazaki
  • Masahito Yamazaki
  • Masahito Yamazaki
  • Masahito Yoshii
  • Masaki Yamada
  • Masako Bando
  • Masashi Aiko
  • Masashi Otani
  • Masashi Yokoyama
  • Masato Aoki
  • Masayasu Hasegawa
  • Masha Baryakhtar
  • Matsuo Sato
  • Maura Ramirez
  • Megumi Endo
  • Michihisa Takeuchi
  • Michihisa Takeuchi
  • Michio Hashimoto
  • Michio Hashimoto
  • Michiyasu Nagasawa
  • Miho Shimada
  • Mihoko Nojiri
  • Mihoko Nojiri
  • Mihoko Nojiri
  • Mihoko Nojiri
  • Minuk Choi
  • Minxi He
  • Minxi He
  • Minxi He
  • Misao Sasaki
  • Mitsuaki Hirasawa
  • Mitsuhiro Yoshida
  • Mitsuru Kakizaki
  • motohiko Yoshimura
  • Motoi ENDO
  • Motoi ENDO
  • Motoi ENDO
  • Motoi Endo
  • Motoi ENDO
  • Motoi ENDO
  • Motokazu Abe
  • Motoko Fujiwara
  • Motoko Fujiwara
  • Muhammad Abdul Rehman
  • Muhammad Farooq
  • Nagomi Uchida
  • Nao HIGASHI
  • Naohiro Osamura
  • Naoki Kawai
  • Naoki Yamamoto
  • Naoki Yamatsu
  • Naoto Nishimura
  • Naoto Nishimura
  • Naotoshi Okamura
  • Naoya Kitajima
  • Naoya Ukita
  • naoyuki haba
  • naoyuki haba
  • Natsumi Nagata
  • Natsumi Nagata
  • Natsumi Nagata
  • Nicholas J. Benoit
  • Nobuhiro Maekawa
  • Nobuhito Maru
  • Nobuhito Maru
  • Nobuyoshi Ohta
  • Noriaki Kitazawa
  • norikazu yamada
  • Noriko Yamasaki
  • Norimi Yokozaki
  • Norisuke Sakai
  • Nosratollah Jafari Sonbolabadi
  • Osamu Sato
  • Peiwen Wu
  • Percy Cáceres
  • Pyungwon Ko
  • Pyungwon Ko
  • Qianhang Ding
  • Ramy Fitrah Izzah
  • Ramy Fitrah Izzah
  • Raymundo Ramos
  • Raymundo Ramos
  • Rinto Kuramochi
  • Rui Zhang
  • Ryo Kitamura
  • Ryo Nagai
  • Ryo Namba
  • Ryodai Kawaguchi
  • Ryosuke Sato
  • Ryotaro Ishikawa
  • Ryotaro Ishikawa
  • Ryu Sawada
  • Ryuichiro Hada
  • Ryuichiro Kitano
  • Ryuichiro Kitano
  • Ryuichiro Kitano
  • Ryusuke Jinno
  • Sadaharu Uehara
  • Saeid Foroughi-Abari
  • Samuel Homiller
  • Sanket Dave
  • Satoshi Mishima
  • Satoshi Mishima
  • Satoshi Mishima
  • Satoshi Mishima
  • Satoshi Mishima
  • Satsuki Nishimura
  • Satsuki Nishimura
  • Satsuki Oda
  • Saurabh Kumar Shukla
  • Seong Chan Park
  • Seong Chan Park
  • Seongchan Park
  • Shameran Mahmud
  • Shao-Feng (韶锋) Ge (葛)
  • Shao-Feng (韶锋) Ge (葛)
  • Shi Pi
  • Shigeki Hirose
  • Shigeki Matsumoto
  • Shigemi Ohta
  • shigeo ohkubo
  • Shih-Yen Tseng
  • Shihwen Hor
  • Shihwen Hor
  • Shihwen Hor
  • Shimpei Endo
  • Shin-ichiro Kanematsu
  • Shinta Kasuya
  • Shinta Kasuya
  • Shintaro Eijima
  • Shintaro Eijima
  • Shintaro Eijima
  • Sho Iwamoto
  • Shogo Nishiyama
  • Shohei Aoyama
  • Shohei Nishida
  • Shohei Nishida
  • Shohei Okawa
  • Shohei Okawa
  • Shoichi Aritome
  • Shoichi Ichinose
  • Shoichi Kawamoto
  • Shoichi Kawamoto
  • Shota Nakagawa
  • Shota Nakagawa
  • Shun Arai
  • Shun-ichiro Koh
  • Shunsuke Taniwaki
  • Shuntaro Aoki
  • Shuntaro Aoki
  • shunyu yao
  • Shunzo Kumano
  • Shunzo Kumano
  • Shunzo Kumano
  • Shuto Nomazaki
  • Sinya Aoki
  • So Chigusa
  • So Chigusa
  • So Chigusa
  • So Chigusa
  • SooJin Lee
  • Sri Aditya Gadam
  • Suho Kim
  • Sunchan Jeong
  • Suvam Maharana
  • Suyong Choi
  • Syuhei Iguro
  • Syuhei Iguro
  • Taehyun Jung
  • Taisuke Katayose
  • Takahiko Matsubara
  • Takahiro Kubota
  • Takahiro Terada
  • Takahiro Terada
  • Takahiro Terada
  • Takahiro Ueda
  • Takahiro Yoshida
  • Takahiro Yoshida
  • Takahiro Yoshida
  • Takanao Tsuyuki
  • Takao Yamaki
  • Takashi Hamana
  • Takashi Kaneko
  • Takashi Mori
  • Takashi Toma
  • Takashi Yamanaka
  • Takashi Yamanaka
  • Takashi Yoshimoto
  • Takehiko Asaka
  • Takemichi Okui
  • Takeru Monobe
  • Takeshi Chiba
  • Takeshi Chiba
  • Takeshi Chikamatsu
  • Takeshi Chikamatsu
  • Takeshi Chikamatsu
  • Takeshi Kobayashi
  • Takeshi Yamazaki
  • Takumi Doi
  • Takumi Kuwahara
  • Takumi Kuwahara
  • Takumi Kuwahara
  • Takuya Kamitani
  • Takuya Morozumi
  • Takuya Yoda
  • Tamaki Murokoshi
  • TANABE Yoshihiro
  • Tatsumi Aoyama
  • Teppei Kitahara
  • Teppei Kitahara
  • Teppei Kitahara
  • Teppei Kitahara
  • Teruhiko Kawano
  • Teruhiko Kawano
  • Teruhiko Kawano
  • Tetsufumi Hirano
  • Tetsuo Shidara
  • Tetsuo Shindou
  • Tetsuo Shindou
  • Tetsutaro Higaki
  • Tetsutaro Higaki
  • Tetsutaro Higaki
  • Tetsutaro Higaki
  • Tetsuyuki Yukawa
  • Tevong You
  • Thanaporn Sichanugrist
  • Tommaso Scirpa
  • Tomohiro Fujita
  • Tomohiro Harada
  • Tomoya Nagai
  • Tomoya Nagai
  • Tomoya Nagai
  • Tomoya Nagai
  • Tomoya Naito
  • Toru Goto
  • Toru Goto
  • Toru Harada
  • Toshi Sumida
  • Toshifumi Yamada
  • Toshiyuki Morii
  • Toshiyuki Morii
  • Toshiyuki Morii
  • Toshiyuki Morii
  • TRIPURARI SRIVASTAVA
  • Tsunayuki Matsubara
  • Tsutomu Ishikawa
  • Tsutomu Mibe
  • Tsutomu Sakai
  • Tsutomu Yanagida
  • Valerio De Luca
  • Vazha Loladze
  • Vomna Mohan
  • Wakutaka Nakano
  • Won Jun
  • Yasuhiro Sekino
  • Yasuhiro Shimizu
  • Yasuhiro Shimizu
  • Yasuhiro Shimizu
  • Yasuhiro Shimizu
  • Yasuhiro Shimizu
  • Yasuhito Kaminaga
  • Yasuhito Sakaki
  • Yasuki Tachibana
  • Yasumichi Aoki
  • Yasutaka Koga
  • Yen Chin Ong
  • Ying-li Zhang
  • Yingbo Ji
  • Yoichi Kazama
  • Yoshiharu Kawamura
  • Yoshihiko Abe
  • Yoshihiko Abe
  • Yoshihiko Abe
  • Yoshihiko Abe
  • Yoshihiro SHIGEKAMI
  • Yoshiki Kanazawa
  • Yoshiki Uchida
  • Yoshiki Uchida
  • Yoshiki Uchida
  • Yoshiki Uchida
  • Yoshiki Uchida
  • yoshinori enomoto
  • Yoshio Kuramoto
  • Yoshitaka Bando
  • Yoshitaka KUNO
  • Yoshiyuki Inoue
  • Yosuke Honda
  • Yosuke Imamura
  • Yu Hamada
  • Yu HAMADA
  • Yu HAMADA
  • Yu Zhou
  • Yudong Luo
  • Yuga Nakazawa
  • Yuga Nakazawa
  • Yuhma Asano
  • Yuichiro Tada
  • Yuk Kei Kong
  • Yuk Kei Kong
  • Yuki Adachi
  • Yuki Adachi
  • Yukihiro Kanda
  • Yuko Urakawa
  • Yuma FURUTA
  • Yun-Long Zhang
  • Yusei Bando
  • Yusuke Takeuchi
  • Yusuke Takeuchi
  • Yuta Hamada
  • Yuta Hiranuma
  • Yuta Okazaki
  • Yutaka Ookouchi
  • Yutaro Iiyama
  • Yutaro Sato
  • Yuto Minami
  • Yuuiti Sendouda
  • Yuuka Kanakubo
  • Yuuka Kanakubo
  • Zhen Liu
  • Zheng-Gang Chen
    • KEK-PH Muon g-2
      Convener: Motoi ENDO
      • 1
        Muon g-2 and Δα connection

        The Muon g-2 experiment at Fermilab has recently confirmed Brookhaven's earlier measurement of the muon anomalous magnetic moment aμ. This new result increases the discrepancy Δaμ with the Standard Model (SM) prediction and strengthens its "new physics" interpretation as well as the quest for its underlying origin. In this talk I will review the SM prediction of the muon g-2, focusing on some of the latest developments, and discuss the connection of the discrepancy Δaμ to precision electroweak predictions via their common dependence on hadronic vacuum polarization effects.

        Speaker: Dr Massimo Passera (INFN, Padua)
    • KEK-PH Muon g-2
      Convener: Motoi ENDO
      • 2
        Consistency of the hadronic vacuum polarization between lattice QCD and the R-ratio

        I will review the current status of data-driven R-ratio as well as lattice QCD determinations of the hadronic vacuum polarization. I will then discuss universality tests within the lattice QCD community and the consistency with data-driven results based on the R-ratio. The talk will also present expected progress in the coming years.

        Speaker: Prof. Christoph Lehner (Regensburg U. and Brookhaven Natl. Lab.)
    • KEK-PH Next Generation Accelerators
      • 3
        Future laser and beam driven high gradient accelerator technology

        Recent high gradient accelerator technologies will be introduced. Most popular high gradient accelerator is the laser plasma wakefield accelerator and it reaches up to 100 GV/m level. However it is currently low repetition rate and difficult for the cascading acceleration. On the other hand, there are another accelerator technologies to realize the high repetition and the cascading acceleration based on the THz wave. The main issue for the THz accelerator is the efficient THz generation driven by high power laser or the electron beam. Further recent high power laser technologies are also introduced.

        Speaker: Prof. Mitsuhiro Yoshida (Accelerator Laboratory, KEK)
    • KEK-PH Next Generation Accelerators
      • 4
        Muon Collider

        A muon collider provides a unique path to a high-energy, high-luminosity lepton collider that combines precision measurements and discovery potential. The talk will introduce the scheme and highlight some key challenges. It will also introduce the new collaboration that plans to develop the concept.

        Speaker: Prof. Daniel Schulte (CERN)
    • The KEK-PH + KEK-Cosmo joint workshop on "Primordial Black Holes": Short talks
      Convener: Dr Kazunori Kohri (KEK)
      • 5
        Primordial Black Holes from Long-Range Scalar Forces and Scalar Radiative Cooling

        Primordial black holes (PBHs) are a natural consequence of long-range scalar forces in the early Universe. These forces can lead to the formation of halos of heavy particles, Q-balls or oscillons even during the radiation dominated era. This same force removes energy and angular momentum from virialized systems via scalar radiation, leading to the subsequent formation of black holes. We will discuss two scenarios which result in the formation of PBHs. First, we consider heavy fermions interacting via a light scalar mediator. This scenario relates the mass of the dark-sector particles to the masses and abundance of dark matter PBHs in a way that can explain why dark matter and ordinary matter have similar mass densities. Second, we consider interactions among SUSY Q-balls. The mass and abundance of PBHs in this scenario are naturally explained by the SUSY breaking scale. Lastly, we will comment on the expected PBH spins from this formation mechanism in comparison to other earlier models.

        Speaker: Mr Marcos Flores (UCLA)
      • 6
        Primordial black holes in peak theory with a non-Gaussian tail

        In this work, we update the peak theory for the estimation of the primordial black hole (PBH) abundance,
        particularly by implementing the critical behavior in the estimation of the PBH mass and employing the averaged compaction function for the PBH formation criterion to relax the profile dependence.
        We apply our peak theory to a specific non-Gaussian feature called the exponential tail, which is characteristic in ultra slow-roll models of inflation. With this type of non-Gaussianity, the probability of a large perturbation is not suppressed by the Gaussian factor but decays only exponentially, so the PBH abundance is expected to be much enhanced.
        Not only do we confirm this enhancement even compared to the case of the corresponding nonlinearity parameter $f_\mathrm{NL}=5/2$, but also we find that the resultant PBH mass spectrum has a characteristic maximal mass which is not seen in the simple Press--Schechter approach.

        Speaker: Dr Yuichiro Tada (Nagoya U)
      • 7
        Spins of primordial black holes formed in the radiation-dominated phase of the universe: first-order effect

        The standard deviation of the initial values of the nondimensional Kerr parameter a∗ of primordial black holes (PBHs) formed in the radiation-dominated phase of the universe is estimated to the first order of perturbation for the narrow power spectrum. Evaluating the angular momentum at turn around based on linearly extrapolated transfer functions and peak theory, we obtain the expression. This implies that for M≃MH, where MH is the horizon mass at the horizon entry, the higher the probability of the PBH formation, the larger the standard deviation of the spins, while PBHs of M≪MH formed through near-critical collapse may have larger spins than those of M≃MH. In comparison to the previous estimate, the new estimate has the explicit dependence on the ratio M/MH and no direct dependence on the current dark matter density. On the other hand, it suggests that the first-order effect can be numerically comparable to the second-order one.

        Speaker: Prof. Tomohiro Harada (Rikkyo U)
      • 8
        Ultrahigh-energy Gamma Rays and Gravitational Waves from Primordial Exotic Stellar Bubbles

        We put forward a novel class of exotic celestial objects that can be produced through phase transitions occurred in the primordial Universe. These objects appear as bubbles of stellar sizes and can be dominated by primordial black holes (PBHs). We report that, due to the processes of Hawking radiation and binary evolution of PBHs inside these stellar bubbles, both electromagnetic and gravitational radiations can be emitted that are featured on the gamma-ray spectra and stochastic gravitational waves (GWs). Our results reveal that, depending on the mass distribution, the exotic stellar bubbles consisting of PBHs provide not only a decent fit for the ultrahigh-energy gamma-ray spectrum reported by the recent LHAASO experiment, but also predict GW signals that are expected to be tested by the forthcoming GW surveys.

        Speaker: Mr Qianhang Ding (HKUST)
      • 3:30 PM
        Break
    • The KEK-PH + KEK-Cosmo joint workshop on "Primordial Black Holes": 1st Invited Talk
      Convener: Dr Mukaida Kyohei (KEK)
      • 9
        Primordial Black Holes and Gravitational Wave Observations

        Primordial Black Holes might comprise a significant fraction of dark matter in the Universe and can give rise to observable signatures at current and future gravitational wave experiments. First, we review the PBH model and discuss how accretion and clustering may affect the properties of PBH binaries. Second, we confront the PBH model with LIGO/Virgo data showing its upsides and shortcomings, by also including state-of-the-art astrophysical models in a multi-population inference. Finally, we discuss how 3G detectors, such as Einstein Telescope and Cosmic Explorer, may be able to discover a PBH population by searching for high redshift merger events.

        Speaker: Dr Gabriele Franciolini (Geneva U)
    • The KEK-PH + KEK-Cosmo joint workshop on "Primordial Black Holes": 2nd Invited Talk
      Convener: Kazunori KOHRI (KEK/Theory)
      • 10
        Primordial black holes as a LIGO-Virgo and dark matter candidate

        Although black holes can be the remnants of dead stars, it is also possible that some are primordial. Such primordial black holes are the unique dark matter candidate which is not a new type of particle, and they could also explain some of the unexpected properties of the black hole mergers that LIGO and Virgo have detected. I will summarise the evidence and (fine-tuning) challenges behind this claim, including a new Bayesian model comparison between astrophysical and primordial black holes.
        I will also discuss the interesting coincidence of scales between the LIGO events, Chandrasekhar limit and the horizon mass during the QCD transition in the early universe, and the wavelength of gravitational waves on which NANOGrav may (potentially) have detected a stochastic gravitational wave background.

        Speaker: Dr Christian Byrnes (Sussex U)
    • KEK-PH New Ideas in Particle Physics: 1st day
      • 11
        Crunching Naturalness
        Speaker: Michael Geller (Tel Aviv U.)
      • 12
        Aspects of Cosmological Selection of the Weak Scale
        Speaker: Raffaele D'Agnolo (IPhT, Saclay)
      • 5:30 PM
        Break
      • 13
        S-matrix exclusion of de Sitter landscape, and naturalness
        Speaker: Gia Dvali (Munich U., ASC and Munich, Max Planck Inst.)
      • 14
        Gegenbauer Goldstones
        Speaker: Matthew McCullough (CERN)
    • KEK-PH New Ideas in Particle Physics: 2nd day
      • 15
        A Causal Framework for Non Linear Quantum Mechanics
        Speaker: Surjeet Rajendran (Johns Hopkins U.)
      • 16
        Solving the naturalness puzzle using old ideas
        Speaker: Anson Hook (Maryland U.)
      • 10:45 AM
        Break
      • 17
        Brane Probes, Finiteness and Distance Conjecture
        Speaker: Yuta Hamada (Harvard U.)
      • 18
        Consequences of No Global Symmetries in Quantum Gravity
        Speaker: Tom Rudelius (UC, Berkeley)
    • KEK-PH Jet Physics
      Convener: Nojiri Mihoko
      • 19
        Jet physics with ATLAS

        New physics searches using jet substructure are actively performed at the LHC era. There are several new techniques with ATLAS to extract the substructure information more precisely. A new particle-flow algorithm, unified-flow objects (UFOs), is recently developed to improve the resolution of the substructure variables. On top of that, to identify boosted W/Z/top/H decaying to hadrons, as well as unknown new particles which form the characteristic jet substructure, some new approaches are introduced, using some machine-learning techniques and/or new substructure representatives e.g. Lund-plane variables. The modeling of the jet substructure is an important key to improve the sensitivity. In this talk, I will summarize recent developments of the ATLAS jet substructure, and the status of the new physics searches using it.

        Speaker: Prof. Takuya Nobe
      • 20
        Jets through the LHC era

        In this talk I will give a personal view of some of the major theoretical advances that have been made in jet physics through the LHC era so far. Topics that I will touch on will include the development of infrared safe jet finders, essential for quantitative interpretation of LHC data; the development of the field of jet substructure to identify hadronic decays of boosted electroweak bosons; and progress towards the use of complete event information in interpreting the underlying scattering dynamics of high-energy collisions.

        Speaker: Prof. Gavin Salam
    • KEK-PH Jet Physics
      Convener: Nojiri Mihoko
      • 21
        Boosted jet physics in CMS

        Many measurements and searches at the Large Hadron Collider need to identify highly boosted particles that decay to hadronic final states. The decay products of these particles will be closely collimated and reconstructed into one single large-radius jet. One can then use jet substructure and deep learning approaches to learn information about the radiation pattern inside the jet and mitigate combinatorial backgrounds. For example, graph neural networks can be trained to take the unordered set of jet constituent particles as inputs and infer attributes of the jet. These jet tagging methods are then calibrated to reflect their tagging efficiency in data and the uncertainties on the calibration will vary depending on the complexity of the final state. In this talk, I will review the latest jet tagging techniques in CMS, their calibration methods and its usage in searches for boosted heavy resonances with 13 TeV LHC data.

        Speaker: Prof. Cristina Mantilla
    • KEK-PH + KEK-COSMO joint mini-workshop: Lecture
      Convener: Yuko Urakawa (KEK)
    • KEK-PH + KEK-COSMO joint mini-workshop: First afternoon session
      Convener: Noaya Kitajima
    • 2:55 PM
      Break
    • KEK-PH + KEK-COSMO joint mini-workshop: Second afternoon session
      Convener: Minxi He
      • 26
        Parametric resonance instability of the QCD axion
        Speaker: Naoya Kitajima (Tohoku University)
      • 27
        Cosmological effects of Peccei-Quinn symmetry breaking on QCD axion dark matter
        Speaker: Shota Nakagawa (Tohoku University)
      • 28
        Origin of pseudo-Nambu-Goldstone dark matter
        Speaker: Yoshihiko Abe (Kyoto University)
    • KEK-PH + KEK-COSMO joint mini-workshop: Morning session
      Convener: Yu Hamada
      • 29
        Dark radiation abundance in axion-SU(2) model
        Speaker: Masahito Ogata (University of Toyama)
      • 30
        Searching for axion dark matter/gravitational waves with magnons
        Speaker: Asuka Ito (Tokyo Institute of Technology)
    • 12:00 PM
      Break
    • KEK-PH + KEK-COSMO joint mini-workshop: First afternoon session
      Convener: Motoi Endo
    • 2:55 PM
      Break
    • KEK-PH + KEK-COSMO joint mini-workshop: Second afternoon session
      Convener: Ryutaro Matsudo
      • 34
        Electroweakly interacting spin-1 dark matter and its phenomenology
        Speaker: Motoko Fujiwara (Nagoya University)
      • 35
        Chiral Composite Asymmetric Dark Matter
        Speaker: Keiichi Watanabe (The University of Tokyo, ICRR)
      • 36
        Electroweak-Skyrmion as Asymmetric Dark Matter
        Speaker: Yu Hamada (KEK)