coffee break[only]

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検出器 R＆D

[2] Measurement of electron drift parameters for helium and CF4-based gases (pdf) (html) (翻訳) (reference)
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Reference

[1] The μ-RWELL: A compact, spark protected, single amplification-stage MPGD (pdf) (html) (翻訳) (reference)
M. Poli Lener et al., Nucl. Instr. Meth. A 824 (2016) 565–568.

Reference

The GERDA experiment has been proposed in 2004 as a new 76Ge double-beta decay experiment at LNGS. The GERDA installation is a facility with germanium detectors made out of isotopically enriched material. The detectors are operated inside a liquid argon shield. The experiment is located in Hall A of LNGS.

Upgrade for Phase II of the GERDA Experiment
Eur. Phys. J. C 78 (2018) 388

Improved Limit on Neutrinoless Double-β Decay of 76Ge from GERDA Phase II
Phys. Rev. Lett. 120 (2018) 132503

GERDA Phase II: search for neutrinoless double beta decay
PoS (EPS-HEP2017) 150

Background-free search for neutrinoless double-β decay of 76Ge with GERDA
Nature 544 (2017) 47 (6 April 2017) suppl. material

Limits on uranium and thorium bulk content in Gerda Phase I detectors Astroparticle Physics 91 (2017) 15-21

EXO(web)

test
CUORE

Search for neutrinoless double-beta decay of ¹³⁰Te with CUORE-0
K. Alfonso et al., Phys. Rev. Lett. 115 (2015) 102502. (pdf) (html)

CUORE crystal caliration runs: Results on radioactive contamination and extrapolation to
F. Alessandria et al., Astr. Phys. 35 (2012) 839-849. CUORE background(pdf) (html)

CUORE: a cryogenic underground observatory for rate events
C. Arnaboldi et al., Nucl. Instr. Meth. A 518 (2004) 775-798. (pdf)

NOvA(web)

test
Super Kamiokande(web)

Phys. Rev. D 98, 052006 (2018)(web)<>

Phys. Rev. D 98, 052006 (2018)(web)

IceCube(web)

test
PANDA X(web)

test
CDEX (China Dark matter EXperiment)

(go to web) [1] CDEX Dark Matter Experiment: Status and Prospects (pdf), (arxive)
(翻訳) (reference)
Hao Ma, et al., arXiv:1712.06046 [hep-ex] (2017).

[2] The CDEX Dark Matter Program at the China Jinping Underground Laboratory (pdf), (arxive)
(翻訳) (reference)
Qian Yue, et al., arXiv:1602.02462 [physics.ins-det] (2016)

[2] Cryogenic system of China Dark matter Experiment (CDEX-10) (pdf), (html)
(翻訳) (reference)
Feipeng Ning, et al., Cryogenics, Volume 76, June 2016, Pages 10-15.

DEAP-3600(web)

[1] First results from the DEAP-3600 dark matter search with argon at SNOLAB (pdf), (arxive)
(翻訳) (reference)
P.-A. Amaudruz, et al., arXiv:1707.08042 [astro-ph.CO] (2017)

NEWAGE(web)

[23] Study of Negative-Ion TPC Using μ-PIC for Directional Dark Matter Search (pdf), (html)
(翻訳) (reference)
T. Ikeda, et al., EPJ Web of Conf. 174. 02006 (2018) MPGD2015.

Reference

[2] Development of a low-alpha-emitting μ-PIC for NEWAGE direction-sensitive dark-matter search (pdf) (pdf_arxive) (html) (reference)
H. Takashi, et al., AIP conf. Proc. 1921, 070001 (2018).
　方向感度をもつ暗黒物質探索NEWAGEの低α線放射μ-PICの開発：ダークマター直接探索研究NEWAGEにおいて、従来のTPC(μ-PIC)ではバックグラウンドのα線が材質ポリミドに多かった。なので、新しく低(α線)放射能な素材(エポキシ追加)を使用して、α線量を7.55x10^-2未満まで減らした。今後このμ-PICを使って、低BGでダークマターを探索する。

Reference
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[20] NEWAGE - direction-sensitive dark matter serach experiment (pdf), (html)
(翻訳) (reference)
K. Nakamura et al., Phys. Proc. 61 (2015) 737-741.

Reference

[12] Direction-sensitive dark matter search with gaseous tracking detector NEWAGE-0.3b’(pdf) (html) (翻訳) (reference)
K. Nakamura et al., PTEP 2015, 043F01.
NEWAGEはCF4ガスで満たされたマイクロ・タイム・プロジェクション・チェンバーを用いた方向感度を持つ暗黒物質探索実験である。2008年神岡での我々の最初の地下測定に続いて、我々は感度改善した新しい検出器NEWAGE-0.3b’を開発した。NEWAGE-0.3b’は前回の検出器の標的体積の２倍、低いエネルギー閾値、そしてデータ収集システムを改良した。2013年に神岡地下実験場でNEWAGE-0.3’によって暗黒物質探索に着手した。0.327 kg・daysの暴露は90%C.L.の方向感度・スピン依存性の断面積が200 GeV/c2のWIMPにおいて557 pbの限界値を達成した。最初の地下測定と比べて(relative)、新しい方向感度の限界はファクター約10まで改善され、そしてこの限界値は（我々の）データにとって最高のものです。　

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[18] Direction-sensitive dark matter search results in a surface laboratory (pdf), (html)
(翻訳) (reference)
M. Kimura et al., Phys. Lett. B 654 (2007) 58-64. NEWAGE

Reference

[3] First underground results with NEWAGE-0.3a direction-sensitive dark matter detector(pdf) (html) (翻訳) (reference)
K. Miuchi et al. (NEWAGE Collaboration): Phys. Lett. B 686 (2010) 11.
　神岡地下実験室でNEWAGE-0.3a検出器を用いた暗黒物質直接探索実験が行われた。NEWAGE-0.3aは152 Torr*）のCF4ガスのマイクロ時間プロジェクション・チェンバーである。基準となる体積と標的の質量はそれぞれ20x25x31 cm3と0.0115 kgである。0.524 kg daysの露出で、方向に感度をもつ方法によって改善されたスピンに依存している弱い相互作用する質量をもつ粒子(WIMP)と陽子の断面積の限界は150 GeV/c2のWIMPにおいて5400 pbの新しい記録を達成した。我々は残された背景雑音を研究し、そして取り巻くγ線が残された背景雑音の1/5を分布していることとガスチェンバーの中の放射能汚染が分布していたことがわかった。

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LUX

(web)

"Signal yields, energy resolution, and recombination fluctuations in liquid xenon", Accepted for publication in Phys. Rev. D, December 15, 2016. DOI: 10.1103/PhysRevD.95.012008, arXiv:1610.02076

"Results from a search for dark matter in the complete LUX exposure", Accepted for publication in Phys. Rev. Lett., December 5, 2016. DOI: 10.1103/PhysRevLett.118.021303, arXiv:1608.07648

"Low-energy (0.7-74 keV) nuclear recoil calibration of the LUX dark matter experiment using D-D neutron scattering kinematics", arXiv:1608.05381

"Chromatographic separation of radioactive noble gases from xenon", arXiv:1605.03844

"Results on the Spin-Dependent Scattering of Weakly Interacting Massive Particles on Nucleons from the Run 3 Data of the LUX Experiment", Phys. Rev. Lett, 116:161302, April 2016. DOI: 10.1103/PhysRevLett.116.161302 , arXiv:1602.03489

"Improved WIMP scattering limits from the LUX experiment", Phys. Rev. Lett, 116:161301, April 2016. DOI: 10.1103/PhysRevLett.116.161301, arXiv:1512.03506 Data from Figures 1-3

"Tritium calibration of the LUX dark matter experiment,", Phys. Rev. D, 93:072009, Apr 2016. DOI: 10.1103/PhysRevD.93.072009, arXiv:1512.03133

"FPGA-based Trigger System for the LUX Dark Matter Experiment,", Nucl. Instrum. Meth. A 818 57-67 (May 2016). DOI: 10.1016/j.nima.2016.02.017, arXiv:1511.03541

"Radiogenic and Muon-Induced Backgrounds in the LUX Dark Matter Detector," Astropart. Phys. 62 (2015) 33-46, arXiv:1403.1299

"First results from the LUX dark matter experiment at SURF," Phys. Rev. Lett. 112, 091303. arXiv:1310.8214

"The Large Underground Xenon (LUX) Experiment," Nucl. Instrum. Meth. A 704 111-126 (2013). arXiv:1211.3788

"Technical Results from the Surface Run of the LUX Dark Matter Experiment," arXiv:1210.4569

"An Ultra-Low Background PMT for Liquid Xenon Detectors," arXiv:1205.2272

"Radio-assay of Titanium samples for the LUX Experiment," arXiv:1112.1376

"LUXSim: A Component-Centric Approach to Low-Background Simulations," Nucl. Instrum. Meth. A 675 63 (2012). arXiv:1111.2074

"Data Acquisition and Readout System for the LUX Dark Matter Experiment," Nucl. Instrum. Meth. A 668 1 (2012). arXiv:1108.1836

XMASS

(web) [11] XMASS experiment, dark matter search with liquid xenon detector (pdf), (html)
A. Munamino, Nucl. Inst. Meth. A 623 (2010) 448–450.

[10] XMASS detector (pdf), (html)
K. Abe et al., Nucl. Inst. Meth. A 716 (2013) 78–85.

[9] Direct dark matter search by annual modulation in XMASS-I (pdf), (html)
K. Abe et al., Physics Letters B 759 (2016) 272–276.

[8] Status of the XMASS experiment (pdf), (html)
S. Moriyama, Physics Procedia 61 (2015) 138–143.

[7] Direct Dark Matter Search with XMASS (pdf), (html)
Kazuyoshi Kobayash, Nuclear and Particle Physics Proceedings 273–275 (2016) 361–366.

DAMA/LIBRA NaI LXe

(go to web)
[3] First model independent results from DAMA/LIBRA-phase2 (arxiv)
R. Bernabei, et al., arXiv:1805.10486v1.

[2] DAMA annual modulation and mirror Dark Matter (pdf), (html)
R. CerulliP et al., Eur. Phys. J. C (2017) 77:83.

[1] The DAMA/LIBRA apparatus (pdf), (html)
(翻訳) (reference)
R. Bernabei et al., Nucl. Instr. Meth. A 592 (2008) 297.
　DAMA/LIBRA検出器

Reference

天文物理関連

[3] An absorption profile centred at 78 megahertz in the sly-averaged spectrum (pdf) (html) (翻訳) (reference)
P. Adamson et al. (NOvA Collaboration) Phys. Rev. Lett. 116, 151806 (2016).

Reference

[2] First Measurement of Electron Neutrino Appearance in NOvA (pdf) (html) (翻訳) (reference)
P. Adamson et al. (NOvA Collaboration) Phys. Rev. Lett. 116, 151806 (2016).

Reference

[1] Discovery of a big void in Khufu’s Pyramid by observation of cosmic-ray muons(pdf) (html) (翻訳) (reference)
K. Morishima et al., Nature 24647 (2017).

Reference

ダークマター探索関連

[23] Current status of neutrinoless double-beta decay searches (pdf) (html) (翻訳) (reference)
Reyco Henning, Reviews in Physics 1 (2016) 29–35.
この記事はニュートリノレス二重ベータ崩壊の実験的探索の現在の状況と近い期間の将来を簡単に批評する。ニュートリノレス二重ベータ崩壊の動機と歴史を議論した後で、現在の実験とこれら感度を制限する因子に注目しよう。その後、転換させたニュートリノ質量の階層性(hierarchy)を探索する実験の提案の要求と展望を議論しよう。

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　暗黒物質は宇宙のエネルギー密度の1/4以上を占めていると信じられている。多くの実験が暗黒物質の研究に取り組んできたにも関わらず、この自然の明確な理解が得られていない。暗黒物質の直接探索は暗黒物質と普通のよく知られた物質との弾性散乱によって落としたエネルギーを検出することが狙いだ。今日において究極の暗黒物質の検出器は開発されていない。つまりこの分野において新たな技術の余地がまだあるということだ。この論文では、いくつかの暗黒物質の直接探索のための検出器の要請を批評する。

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ストロンチウム90カウンター開発研究関連

[91] Nutrient analysis of fish and fish products(pdf)(html)
Mark Roe, et al.,Publication DH, GOV.UK, 2013.

[87] Nutrient analysis of fish and fish products(pdf)(html)
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[85] Chemical Reactions and the Composition of Sea Water(pdf)(html)
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[74] Application ofICP-DRC-MStoscreeningtestofstrontiumand plutoniuminenvironmentalsamplesatFukushima(pdf)
[73] ResultsofanEClaboratorycomparisonon ⁴⁰K, ⁹⁰Sr and ¹³⁷Cs indried bilberry powder(pdf)
[72] On-line ion chemistry for the AMS analysis of ⁹⁰Sr and ¹³⁵,¹³⁷Cs(pdf)
[71] An overview of current knowledge concerning the health and environmental consequences of the Fukushima Daiichi Nuclear Power Plant (FDNPP) accident(pdf)
[70] Iodine isotopes in precipitation: Four-year time series variations before and after 2011 Fukushima nuclear accident(pdf)
[69] Fukushima Daiichi Nuclear Plant accident: Atmospheric and oceanic impacts over the five years(pdf)
[68] Deposition of fission and activation products after the Fukushima Dai-ichi nuclear power plant accident(pdf)(html)
　　K. Shozugawa et al., Environmental Pollution 163 (2012) 243-247
　　小豆川勝見(しょうずがわかつみ)
　　東京大学大学院総合文化研究科広域科学専攻
　　環境分析化学研究室(松尾研究室) 助教
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　　要約(pdf)

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[65] 放射性ストロンチウム分析法(pdf), (html)
文部科学省、放射能測定法シリーズ2、平成15年

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[63] Transarterial Y90 radioembolization versus chemoembolization for patients with hepatocellular carcinoma: A meta-analysis(pdf), (html)
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[62] Surveillance of Strontium-90 in Foods after the Fukushima Daiichi Nuclear Power Plant Accident(pdf), (html)
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[61] 70マイクロメートル線量当量率を用いた⁹⁰Sr/⁹⁰Y汚染密度推定法(pdf), (html)
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　　キーワード：放射能、137Cs、
　　Contents>>

pp85137Csの生物学的半減期(年)は年齢(歳)に依存している。
T_b=12.8 (X ^{1/2} + e^-X)
ここでXは年齢
しかし、乳幼児から20歳まで有効.熟年層はむしろ体重が顕著に効いてくる
T_b=6 W^{3/2}
ここでWは体重(kg)
pp89体内の137Cs排泄促進に有効なものはカリウムフェロシアナイドないしナトリウムフェロシアナイドから調製されたプルシアンブルーで験体群の1.2%は4日で投与した137Csの0%に、35.2%の検体は70%の量に減衰したことを観測した。

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[50] Radioactive Cs in the estuary sediments near Fukushima Daiichi Nuclear Power Plant(pdf), (html)
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[49] 家畜のストロンチウム-カルシウム差別率に伴うストロンチウム代謝に関する研究 I (pdf), (html)
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[40] Spectral identiﬁcation of a ⁹⁰Sr source in the presence of masking nuclides using Maximum-Likelihood deconvolution(pdf), (html)
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[6] Determination of the ¹³⁷Cs and ⁹⁰Sr radioisotope activity concentrations found in digestive organs of sheep fed with different feeds (pdf)

[5] Inventory and vertical migration of ⁹⁰Sr fallout and ¹³⁷Cs/⁹⁰Sr ratio in Spanish mainland soils (pdf)

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　　- 翻訳(pdf)
　　- 論文紹介

[2] Cherenkov detector of ⁹⁰Sr based on aerogel as radiator (html)(pdf)

上へ

肺がん、ラドン測定関連

[21] Measurement of radon concentration in super-Kamiokande’s buffer gas(pdf) (html) (arxive) (翻訳) (reference)
Y. Nakano, et al., NIMA 867 (2017) 108.
　スーパーカミオカンデ検出器にバッファー気体として清潔にした(purify)空気のラドン濃度を精密に測定するために、と同じくらい低い固有の(intrinsic)背景雑音を持つラドンに高い感度を持つ検出器を開発した。この論文では、スーパーカミオカンデの上のバッファー気体の測定と監視のための機能の結果と同等な、この検出器の建造(construction)と較正を議論する。2013年3月、バッファー気体内部にラドンを除去するために使用した冷却(chilled)活性炭(activate charcoal)システムをアップグレードした。改善した後、提供したガスのラドン濃度の劇的な減少(reduction)はに低下した。加えて、本来の場所のバッファー気体のラドン濃度は新しいラドン検出器を使用してが測定された。これらの測定に基づいて、スーパーカミオカンデのタンク自身からの汚染からバッファー気体のラドンの支配的な源が発生すると決定できた。　

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D. Nikezic, Radiation Measurements 41 (2006) 101 – 107

[3] Lung Cancer in Never Smokers: A Review(pdf)
] J. Subramanian, R. Govindan, Journal of Clinical Oncology 25 (2007) 561–570

[2] Investigating the role of human papillomavirus in lung cancer (pdf)
E. Argyri, Papillomavirus Research 3 (2017) 7–10
　　要約(pdf)

[1] Radiocesium transfer from hillslopes to the Pacific Ocean after the Fukushima Nuclear Power Plant accident: A review(pdf)

上へ

PET開発関連

[39] Time of flight in PET revisited(pdf), (html)
　　W. W. Moses, et al., IEEE Trans. on Nucl. Sci. 50, 5 (2003)

[38] Prospects for Time-of-Flight PET using LSO Scintillator(pdf), (html)
　　W. W. Moses, et al., IEEE Trans. on Nucl. Sci. 46, 3 (1999)

[37] Evaluation of a high resolution silicon PET insert module(pdf), (html)
　　Milan Grkovski, et al., Nucl. Instr. and Meth. A 788 (2015) 86-94

[36] A compact high resolution flat panel PET detector based on the new 4-side buttable MPPC for biomedical applications(pdf), (html)
　　Qiang Wang, et al., Nucl. Instr. and Meth. A 794 (2015) 151-159

[35] From PET detectors to PET scanners(pdf), (html)
　　J.L. Humm, A. Rosenfeld, A. Del Guerra,
　　European Journal of Nuclear Medicine and Molecular Imaging, 30 (2003), p. 1574

[31] Development of a wavelength-shifting fibre gamma camera (pdf), (html)
　　A. J. Soares et al., Conf. Reco., Nucl. Scie. Symp. (1999) IEEE
　　keyword: PET, CsI(Na), WLSF, gamma camera
　　- 翻訳(pdf)

[30] Performance of cerium-doped Gd₃Al₂Ga₃O₁₂ (GAGG:Ce) scintillator in gamma-ray spectrometry (pdf)

[29] Performance of the AX-PET Demonstrator (pdf)

[28] AX-PET: A novel PET concept with G-APD readout (pdf)

[27] The AX-PET experiment: A demonstrator for an axial Positron Emission Tomograph (pdf)

[26] Development of an ultrahigh-resolution Si-PM-based dual-head GAGG coincidence imaging system (pdf)

[25] A compact and high efficiency GAGG well counter for radiocesium concentration measurements (pdf)

[24] Characterization of GAGG:Ce scintillators with various Al-to-Ga ratio (pdf)

[23] Development of GAGG depth-of-interaction (DOI) block detectors based on pulse shape analysis (pdf)

[22] Sensitivity booster for DOI-PET scanner by utilizing Compton scattering events between detector blocks (pdf)

[21] Qualification test of a MPPC-based PET module for future MRI-PET scanners (pdf),(html)
　　Y. Kurei et al. / Nucl. Instr. and Meth. A 765 (2014) 275-279
　　Keywords:Multi-Pixel Photon Counter (MPPC)
　　Positron Emission Tomography (PET)
　　Magnetic Resonance Imaging (MRI)
　　- 翻訳(pdf)

[20] A novel method for the line-of-response and time-of-flight reconstruction in TOF-PET detectors based on a library of synchronized model signals (pdf), (html)
　　P. Moskal et al. / Nucl. Instr. and Meth. A 775 (2015) 54 - 62
　　Keywords:Scintillator detectors, Positron Emission Tomography, Time-of-flight, J-PET
　　- 翻訳(pdf)
　　- 論文紹介

[18] The Challenge of Detector Designs for PET (pdf)

[17] Novel Geometrical Concept of a High Performance Brain PET Scanner - Principle, Design and Performance Estimates (pdf)

[16] Joint Reconstruction of Image and Motion in Gated Positron Emission Tomography (pdf)

[15] Development of a High Precision Axial 3-D PET for Brain Imaging (pdf)

[14] The AX-PET project: Demonstration of a high resolution axial 3D PET (pdf), (html)
　　keyword: Positron emission tomography, PET, LYSO scintillator, G-APD
　　- 翻訳(pdf)
　　- 論文紹介(pdf)

[13] AX-PET: A novel PET detector concept with full 3D reconstruction (pdf)

[12] GEANT4 studies on the propagation and detection of scintillation light in long thin YAP crystals (pdf)

[11] Wavelength shifter strips and G-APD arrays for the read-out of the z-coordinate in axial PET modules (pdf)

[10] High precision axial coordinate readout for an axial 3-D PET detector module using a wave length shifter strip matrix (pdf)

[9] Recent advances and future advances in time-of-flight PET (pdf)

[8] Optimization of the effective light attenuation length of YAP:Ce and LYSO:Ce crystals for a novel geometrical PET concept (pdf)

[7] Trends in PET imaging (html)(pdf)
　　William W. Moses, Nucl. Instr. and Meth. A 471 (2001) 209 - 214
　　keyword: PET instrumention
　　- 翻訳(pdf)
　　- 論文紹介

[2] Photodetectors for nuclear medical Imaging (pdf 297KB)

[1] The AX-PET demonstrator - Design, construction and characterization (html)(pdf)
　　P. Beltrame et al. / Nucl. Instr. and Meth. A 654 (2011) 546 - 559
　　keyword: Sr-90, Cherenkov radiation, silica aerogel
　　- 翻訳(pdf)
　　- 論文紹介
　　

上へ

ハドロン物理関連

[25] New Limit on the T-Violation Transverse Muon Polarization in K⁺->π⁰e⁺ν decays (pdf) (翻訳) (reference)
M. Abe, et al., Phys. Rev. Lett. 93, 13 (2004) 131601.
KEK-E246 Exp.

Reference

[24] Structure near the K^-+p+p threshold in the in-flight ³He(K^-,Λp)n reaction (pdf) (翻訳) (reference)
Y. Sada, et al., Prog. Theo. Exp. Ohys. 2016 051D01.
J-PARC E15 Exp.

Reference

[23] Experimental study of the radiative decay K⁺->μ⁺νe⁺e^- K⁺->e⁺νe⁺e^- (pdf) (翻訳) (reference)
A. A. Poblaguev et al., Phys. Rev. Lett. 89, 6 (2002) 061803.
BNL-AGS 865 Exp.

Reference

[22] First observation of the decay K⁺->e⁺νμ⁺μ^- (pdf) (翻訳) (reference)
H. Ma et al., Phys. Rev. D 73, 037101 (2006).
BNL-AGS 865 Exp.

Reference

[21] Measurement of K⁺->π⁰π⁰e⁺ν (K00e4) decay using stopped positive kaons (pdf) (翻訳) (reference)
S. Shimizu et al., Phys. Rev. D 70, 037101 (2004).
KEK-E470 Exp.

Reference

[20] T-violation muon polarization in Kμ3 decays (pdf) (翻訳) (reference)
G. Belanger and C. Q. Geng, Phys. Rev. D 44, 9 (1991) 2789.
Theory

Reference

[19] Non-standerd-model CP violation in Kμ3 Decays as a method of probing for new physics (pdf) (翻訳) (reference)
R. Garisto and G. Kane, Phys. Rev. D 44, 7 (1991) 2038.

Reference

[18] Kμ3 Decay: Tests fot Time Reveral and Two-Component Theory (pdf) (翻訳) (reference)
J. J. Sakurai, Phys. Rev. 109, 3 (1958) 980.

Reference

[17] Precise tests of low energy QCD from K_e4 decay properties(pdf) (翻訳) (reference)
J. R. Batley, Eur. Phys. J. C 70 (2010) 635-657.
NA48/2

Reference

[16] K_l3 form factors at order p⁶ of chiral perturbation theory(pdf) (翻訳) (reference)
P. Post and K. Schicher, Eur. Phys. J. C 25 (2002) 427-443.

Reference

[15] New measurement of the K^±->π⁺π^-e^±ν (Ke4) decay branching ratio and hadronic form factors(pdf) (翻訳) (reference)
J. B. Batley, et al., Phys. Lett. B 715 (2012) 105-115.
NA48/2 　

Reference

[14] Study of the K^-->π⁰e^-ν decay (pdf) (翻訳) (reference)
I. V. Ajinenko, et al., Phys. Lett. B 574 (2003) 14-20.

Reference

[13] Dalitz plot density analysis in Kμ3 decay (pdf) (翻訳) (reference)
D. Haidt, et al., Phys. Lett. 29B 10 (1969) 691.
X2 collaboration 　

Reference

[12] Test of CPT and Lorentz symmetry in entangled neutral kaons with the KLOE experiment(pdf) (翻訳) (reference)
D. Babusci et al., Phys. Lett. B 730 (2014) 89-94.
KLOE-2 collaboration 　

Reference

[11] A measurement of the (K⁺→e⁺ν)/(K⁺→μ⁺ν) branching ratio(pdf) (翻訳) (reference)
K. S. Heard et al., Phys. Lett. B 55, 3 (1975) 327-330.
　

Reference

[10] A measurement of K⁺_eνγ decay(pdf) (翻訳) (reference)
K. S. Heard et al., Phys. Lett. B 55, 3 (1975) 324-326.
　

Reference

[9] Measurement of K⁰_L flux at the J-PARC neutral-Kaon beam line(pdf) (翻訳) (reference)
K. Shiomi et al., Nucl. Instr. Meth. A 664 (2012) 264.
KOTO実験　

Reference

[8] Fabirication of silica aerogel with n=1.08 for e⁺/μ⁺ separation in a threshold Cherenkov counter of the J-PARC TREK.E36 experiment(pdf) (翻訳) (reference)
M. Tabata et al., Nucl. Instr. Meth. A 795 (2015) 206.
E36実験シリカエアロゲルチェレンコフ検出器開発　

Reference

[7] A measurement of the K⁺→e⁺ν_eγ structure decay(pdf) (翻訳) (reference)
J. Heintze, et al., Nuclear Physics B 1977.
abst 　

Reference

[6] Analysis of K⁺→e⁺ν_eγ in light-front quark model and chiral perturbation theory of order p⁶ (pdf)(arxiv)(html) (翻訳) (reference)
Chuan-Hung Chen, et al., Phys. Rev. D. 77 (2008) 014004.
abst 　

Reference

[5] Precise measurement of Γ(K → eν(γ))/Γ(K → μν(γ)) and study of K → eνγ(pdf)(html) (翻訳) (reference)
F. Ambrosino et al., Eur. Phys. J. C 64 (2009) 627.
abst 　

Reference

[4] Proposal for J-PARC 30 GeV Proton Synchrotron
　　Gamma-Ray Spectroscopy of Light Λ Hypernuclei II (pdf)
H. Tamura, J-PARC PAC 2010-04 (J-PARC E36)

[3]J-PARC Experimental Proposal
　　Measurement of Γ(K+ → e+ν)/Γ(K+ → μ+ν) and Search for heavy sterile neutrinos using the TREK detector system (pdf)
S. Shimizu, J-PARC PAC 2010-04 (J-PARC E36)

[2] Proposal for an experiment at the 50-GeV PS
　　Measurement of the cross sections of Σp scatterings (pdf)
K. Miwa, J-PARC PAC 2010-12 (J-PARC E40)

[1] REVIEW OF PARTICLE PHYSICS
PHYSICAL REVIEW D 98, 030001 (2018). (pdf)
Chinese Physics C Vol. 40, No. 10 (2016) 100001. (pdf)
Chinese Physics C Vol. 38, No. 9 (2014) 090001. (pdf)

上へ

素粒子研究関連

[5] A view of neutrino studies with the next generation facilities (pdf) (html) (翻訳) (reference)
L. Stanco, Rev. Phys. 1 (2016) 90.
abst 　

Reference

[4] Flavor Physics and CP violation (pdf) (html) (翻訳) (reference)
P. Chang et al., Prog. Part. Nucl. Phys. 97 (2017) 261.
現在のCKM(カボビ・小林・益川)パラダイムは不十分で、すごくたくさんのパラメータを持つ。フレーバー物理とCP破れ研究(FPCP)の主な狙いは標準模型(SM)を超える新物理を明らかにするための追跡である。LHC RUN1の期間の２つのハイライトは混合BsのCPV位相φsとBs->K*0 μ+ μ-崩壊、ここで、途中経過はSMに一致していることがわかっている。さらにB0->K*0 μ+ μ-崩壊のP'5角度変位アノマリーとRK(*)のB->K0 μ+ μ-とB->K0 e+ e-の頻度の比、そしてB->D(*)τν崩壊におけるBaBarアノマリー、これらはZ’, 荷電ヒッグス、レプトクォークを追加した点でこれらのフレーバー過程の考えうる新物理を示唆する。チャームレスハドロニック、セミレプトニック、純粋なレプトニックとradioactive B崩壊は新物理のさらに様々なウィンドウを提供するために継続している。B物理から離れて、K->μγγ, μμμ, eee崩壊とKセクターのε'/ε、μ->e遷移、ミューオンg-2と電子と中性子のダイポール運動量、そして少しのチャーム物理探索が新物理の広範囲帯の先駆者のウィンドウを提供する。最後に、トップクォークtと125 GeVヒッグスボゾンhを巻き込んだ電荷的に中性のフレーバー遷移: t->ch と h->μτ はFPCPへの新たな窓を与える。ここで、P’5アノマリーによって起こさせるまたは関する新たなZ’はトップクォーク過程に類似して現れる、おそらくミューオンg-2または稀なkaon過程のような低エネルギー現象に結合される。特に、我々はフレーバー破れを制御するために区別した対称性がない２つのヒッグスの二重項モデルの新物理の潜在性をSM2として主張する。むしろSMに似ているhの制限を設けて近づけるとして、中性ヒッグスのフレーバー遷移結合(FCNH)は小さい混合角によって抑制されるが、エキゾティック・ヒッグス二重項はFCNH結合を処理する、我々はちょうどこの探索を開始する。LHC Run 2はこの過程を走らせ、そしてBelle II B物理プログラムがもうすぐ開始で、フレーバーとCPVセクターにおいてとても楽しみである。

Reference
[1] F. Zwicky et. al.:Astrophys. J. 86 (1937) 217.
[2] V. C. Rubin et. al.:Astrophys. J. 159 (1970) 379.

[3] Search for Resonant Diphoton Production with the D0 Detector (pdf), (html)
V. M. Abazov et al. (D0 Collaboration): Phys. Rev. Lett. 102, 231801 (2009).

[2] Measurement of the top quark forward-backward production asymmetry and its dependence on event kinematic properties (pdf), (html)
T. Aaltonen et al. (CDF Collaboration) Phys. Rev. D 87, 092002 (2013).

[1] Evidence for D0-bar{D0} Mixing (pdf), (html) (arxive)
M. Starič et al. (Belle Collaboration) Phys. Rev. Lett. 98, 211803 (2007).

上へ

その他

[5] Depolarization of Positive Muon in Condensed Matter (pdf), (html)
　　R. A. Swanson, Phys. Rev. 112, 2 (1958) 580.

[4] Pulsed source of ultra low energy positive muons for near-surface μSR studies(pdf), (html)
　　P. Bakule, et al., Nucl. Instr. Meth. B 266 (2008) 335.

[3] Geant4—a simulation toolkit(pdf), (html)
　　S. Agostinelli et al. / Nuclear Instruments and Methods in Physics Research A 506 (2003) 250-303.

[2] Impact Frequency Estimate of Micron-sized Meteoroids and Debris on Tanpopo Capture Panels on the ISS (pdf), (html)
　　M. Kurihara et al., Procedia Engineering 103 (2015) 334 - 340
　　Keywords: Space debris, ISS, Silica Aerogel

上へ

[1] 光電子増倍管その基礎と応用　3rd Edition
　浜松ホトニクス社 (2007)(pdf)

日本物理学会誌

2016	1	2	3	4	5	6	7	8	9	10
2015	1	2	3	4	5	6	7	8	9	10	11	12
2014	1	2	3	4	5	6	7	8	9	10	11	12
2013	1	2	3	4	5	6	7	8	9	10	11	12
2012	1	2	3	4	5	6	7	8	9	10	11	12

上へ

IEEE Conference Record

IEEE NSS MIC 2014 Conference Record

上へ

卒論・修士・学位論文

神戸大

2018
[0] 矢ヶ部遼太 Direction-sensitive direct dark matter search with a three dimentional tracking gaseiys detector
(manuscript_v0)

千葉大

2017
[1] 伊藤博士 A study and development of real-time strontium-90 counter based on Cherenkov radiation detection. (pdf)

2016
[4] 磯部
[3] 井尻
[2] 兼子奈緒見 WLSFを用いたPET検査用γ線検出器の開発　(pdf)
[1] 小林篤史高性能PET装置用ガンマ線測定器の開発　(pdf)

2015
[2] 上山俊輔
[1] 児玉諭士 J-APRC E36実験のためのスパイラルファイバートラッカーの開発　(pdf)

2014
[5] 大和久耕平
[4] 韓樹林
[3] 雲越大輔クリアファイバーを用いたチェレンコフカウンターの開発　(pdf)
[2] 伊藤博士高汎用性しきい値型粒子識別装置の開発　　(pdf)
[1] 飯島周多郎リアルタイム大面積90Sr検出器の開発　(pdf)

2013
[2] 玉津
[2] 新田
[1] 丸橋健太 ⁹⁰Sr β線即時検出器の開発　(pdf)

2012
[3] 金山沙緒里炭素線治療時に生じる二次粒子の炭素同位体の成分評価に向けたレンジカウンタの開発　(pdf)
[2] 岸
[1] 久保将人 LEPS2 のための WLS fiber と MPPC を用いたエアロゲルチェレンコフカウンターの開発研究

2009
[1] 田端誠 Study of Transparent Silica Aerogel over the Wide Range of Densities
2008
[1] 高屈折率および低屈折率シリカエアロゲルを用いたチェレンコフカウンターによる粒子識別　東海林彰(pdf)

2007
[1] シリカエアロゲルを用いたリングイメージングチェレンコフカウンターの開発倉谷厚志(pdf)

2006
[1] 田端誠気体-液体間の屈折率空白域を埋めるシリカエアロゲルの新製法の研究開発　(pdf)

2002
[1] 斎藤真一 Belle Silica Aerogel Cherenkov検出器の粒子識別能力の向上及びB中間子の再構成に関する研究　(pdf)

2000
[2] 七尾美緒 BELL実験におけるエアロジェルチェレンコフカウンターの粒子識別能力の評価　(pdf)
[1] 海野祐士 PID Performance by BELLE Aerogel Cerenkov Counter 　(pdf)

中央大

1998
BELLE における低屈折率シリカエアロジェルチェレンコフカウンターの研究及び開発大場隆人

京都大

[] J-PARC K1.8ビームラインに用いる粒子識別検出器の開発と性能評価
　京都大学　足立智 (2010)(pdf)

[] T2K実験において用いられる半導体光検出器MPPCの大量測定
　京都大　永井直樹(2009)(pdf)

[] MPPC読み出しによるシンチレーションカウンターを用いた荷電粒子検出
　奈良女子大　木原理美・脇田紗弥佳(2011)(pdf)

[] MPPCの基本特性およびシンチレーションカウンターへの応用
　奈良女子　辻知佳・宮田香織(2008)(pdf)

[] 新型MPPCの性能評価
　信州大　小林秋人　(2011)(pdf)

[] MPPCを用いた小型放射線検出器の開発と性能評価
　信州大　小倉隆義(2011)(pdf)

[] MPPCの安定性能の研究
　信州大　佐久間隆幸(2010)(pdf)

[] MPPCとストリップ型プラスチックシンチレータの研究
　信州大　戸塚俊介(2009)(pdf)

[] MPPCの性能評価方法の研究
　信州大　坪川貴俊(2007)(pdf)

[] Belle II実験用　新型粒子識別装置Aerogel RICHの開発
　首都大　岩田修一(2011)(pdf)

上へ

素粒子原子核物理学実験・放射線測定＆検出器開発・シリカエアロゲル製造