Pioneering Project Research Activity Report 新領域開拓課題 研究業績報告書
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A Bridge Between Nuclear and Particle Physics
Journal of Physics: Conference Series PAPER • OPEN ACCESS Related content - What’s Next for Particle Physics?: Modern hadron spectroscopy: a bridge between Introduction M White nuclear and particle physics. - Light Hadron Spectroscopy at BESIII Jifeng Hu and BESIII Collaboration To cite this article: A. P. Szczepaniak 2018 J. Phys.: Conf. Ser. 1014 012017 - Progress in light hadron spectroscopy at BESIII W C Yan View the article online for updates and enhancements. This content was downloaded from IP address 131.169.5.251 on 15/05/2018 at 23:01 International Workshop "Nuclear Reactions on Nucleons and Nuclei" IOP Publishing IOP Conf. Series: Journal of Physics: Conf. Series 1014 (2018) 012017 doi:10.1088/1742-6596/1014/1/012017 Modern hadron spectroscopy: a bridge between nuclear and particle physics. A. P. Szczepaniak Physics Department, Indiana University, Bloomington, IN 47405, USA, Center for Exploration of Energy and Matter, Indiana University, Bloomington, IN 47403, USA, Theory Center, Thomas Jefferson National Accelerator Facility, Newport News, VA 23606, USA. E-mail: [email protected] Abstract. In this talk I discuss aspects of hadron physics, which soon are expected to shed new light on the fundamental QCD phenomena. In the analysis of hadron reactions and their propertieds I emphasize similarities to the nuclear many body problem. 1. Introduction The vast majority of nuclear phenomena can be understood using protons and neutrons as elementary constituents and the nonrelativistic interactions among them. On the other hand, Quantum Chromodynamics (QCD), which is the underlying theory of nuclear forces, describes the relativistic quarks and gluons as the fundamental degrees of freedom. -
STRANGE MESON SPECTROSCOPY in Km and K$ at 11 Gev/C and CHERENKOV RING IMAGING at SLD *
SLAC-409 UC-414 (E/I) STRANGE MESON SPECTROSCOPY IN Km AND K$ AT 11 GeV/c AND CHERENKOV RING IMAGING AT SLD * Youngjoon Kwon Stanford Linear Accelerator Center Stanford University Stanford, CA 94309 January 1993 Prepared for the Department of Energy uncer contract number DE-AC03-76SF005 15 Printed in the United States of America. Available from the National Technical Information Service, U.S. Department of Commerce, 5285 Port Royal Road, Springfield, Virginia 22161. * Ph.D. thesis ii Abstract This thesis consists of two independent parts; development of Cherenkov Ring Imaging Detector (GRID) system and analysis of high-statistics data of strange meson reactions from the LASS spectrometer. Part I: The CIUD system is devoted to charged particle identification in the SLAC Large Detector (SLD) to study e+e- collisions at ,/Z = mzo. By measuring the angles of emission of the Cherenkov photons inside liquid and gaseous radiators, r/K/p separation will be achieved up to N 30 GeV/c. The signals from CRID are read in three coordinates, one of which is measured by charge-division technique. To obtain a N 1% spatial resolution in the charge- division, low-noise CRID preamplifier prototypes were developed and tested re- sulting in < 1000 electrons noise for an average photoelectron signal with 2 x lo5 gain. To help ensure the long-term stability of CRID operation at high efficiency, a comprehensive monitoring and control system was developed. This system contin- uously monitors and/or controls various operating quantities such as temperatures, pressures, and flows, mixing and purity of the various fluids. -
Snowmass 2021 Letter of Interest: Hadron Spectroscopy at Belle II
Snowmass 2021 Letter of Interest: Hadron Spectroscopy at Belle II on behalf of the U.S. Belle II Collaboration D. M. Asner1, Sw. Banerjee2, J. V. Bennett3, G. Bonvicini4, R. A. Briere5, T. E. Browder6, D. N. Brown2, C. Chen7, D. Cinabro4, J. Cochran7, L. M. Cremaldi3, A. Di Canto1, K. Flood6, B. G. Fulsom8, R. Godang9, W. W. Jacobs10, D. E. Jaffe1, K. Kinoshita11, R. Kroeger3, R. Kulasiri12, P. J. Laycock1, K. A. Nishimura6, T. K. Pedlar13, L. E. Piilonen14, S. Prell7, C. Rosenfeld15, D. A. Sanders3, V. Savinov16, A. J. Schwartz11, J. Strube8, D. J. Summers3, S. E. Vahsen6, G. S. Varner6, A. Vossen17, L. Wood8, and J. Yelton18 1Brookhaven National Laboratory, Upton, New York 11973 2University of Louisville, Louisville, Kentucky 40292 3University of Mississippi, University, Mississippi 38677 4Wayne State University, Detroit, Michigan 48202 5Carnegie Mellon University, Pittsburgh, Pennsylvania 15213 6University of Hawaii, Honolulu, Hawaii 96822 7Iowa State University, Ames, Iowa 50011 8Pacific Northwest National Laboratory, Richland, Washington 99352 9University of South Alabama, Mobile, Alabama 36688 10Indiana University, Bloomington, Indiana 47408 11University of Cincinnati, Cincinnati, Ohio 45221 12Kennesaw State University, Kennesaw, Georgia 30144 13Luther College, Decorah, Iowa 52101 14Virginia Polytechnic Institute and State University, Blacksburg, Virginia 24061 15University of South Carolina, Columbia, South Carolina 29208 16University of Pittsburgh, Pittsburgh, Pennsylvania 15260 17Duke University, Durham, North Carolina 27708 18University of Florida, Gainesville, Florida 32611 Corresponding Author: B. G. Fulsom (Pacific Northwest National Laboratory), [email protected] Thematic Area(s): (RF07) Hadron Spectroscopy 1 Abstract: The Belle II experiment at the SuperKEKB energy-asymmetric e+e− collider is a substantial upgrade of the B factory facility at KEK in Tsukuba, Japan. -
Revealing the Exciton Fine Structure in Lead Halide Perovskite Nanocrystals
nanomaterials Review Revealing the Exciton Fine Structure in Lead Halide Perovskite Nanocrystals Lei Hou 1,2 , Philippe Tamarat 1,2 and Brahim Lounis 1,2,* 1 Université de Bordeaux, LP2N, F-33405 Talence, France; [email protected] (L.H.); [email protected] (P.T.) 2 Institut d’Optique and CNRS, LP2N, F-33405 Talence, France * Correspondence: [email protected] Abstract: Lead-halide perovskite nanocrystals (NCs) are attractive nano-building blocks for photo- voltaics and optoelectronic devices as well as quantum light sources. Such developments require a better knowledge of the fundamental electronic and optical properties of the band-edge exciton, whose fine structure has long been debated. In this review, we give an overview of recent magneto- optical spectroscopic studies revealing the entire excitonic fine structure and relaxation mechanisms in these materials, using a single-NC approach to get rid of their inhomogeneities in morphology and crystal structure. We highlight the prominent role of the electron-hole exchange interaction in the order and splitting of the bright triplet and dark singlet exciton sublevels and discuss the effects of size, shape anisotropy and dielectric screening on the fine structure. The spectral and temporal manifestations of thermal mixing between bright and dark excitons allows extracting the specific nature and strength of the exciton–phonon coupling, which provides an explanation for their remarkably bright photoluminescence at low temperature although the ground exciton state is optically inactive. We also decipher the spectroscopic characteristics of other charge complexes Citation: Hou, L.; Tamarat, P.; whose recombination contributes to photoluminescence. With the rich knowledge gained from these Lounis, B. -
EFB23 Program Sunday 7/Aug
EFB23 program Sunday 7/Aug. 17:00-19:00 Registration and reception at Scandic Aarhus City Auditorium F Auditorium G2 Monday 8/Aug. 8:30-8:55 Registration (in front of Aud. F) 9:00-9:10 Opening 9:10-9:45 Blume D. A new frontier: Few-body systems with spin-momentum coupling 9:45-10:20 Shimoura S. Experimental studies of the tetra-neutron system by using RI-beam 10:20-10:50 Coffee chair: Arlt J. 10:50-11:23 Hen O. Short-range correlations in nuclei 11:23-11:56 Piasetzky E. Measurement of polarization transfered to a proton bound in nuclei 11:56-12:30 Epelbaum E. Recent results in nuclear chiral effective field theory 12:30-14:00 Lunch chair: Kamada H. chair: Viviani M. Faraday waves in coldatom systems with two- and 14:00-14:20 Riisager K. Beta-delayed particle emission from neutron halos Tomio L. three-body interactions Observation of attractive and repulsive polarons in a 14:20-14:40 Refsgaard J. Beta-decay spectroscopy on 12C Jorgensen N.B. Bose-Einstein condensate Role of atomic excitations in search for neutrinoless double beta- Few-body correlations in the spectral response of 14:40-15:00 Amusia M.Ya. decay Levinsen J. impurities coupled to a Bose-Einstein condensate 15:00-15:10 Break Unstable nuclei in dissociation of light stable and radioactive nuclei Calculation of the S-factor $S_{12}$ with the Lorentz 15:10-15:30 Artemenkov D.A. in nuclear track emulsion Leidemann W. integral transform method Integral transform methods: a critical review of kernels for 15:30-15:50 Feldman G. -
Layer Locking Effects in Optical Orientation of Exciton Spin in Bilayer Wse2
LETTERS PUBLISHED ONLINE: 5 JANUARY 2014 | DOI: 10.1038/NPHYS2848 Spin–layer locking effects in optical orientation of exciton spin in bilayer WSe2 Aaron M. Jones1, Hongyi Yu2, Jason S. Ross3, Philip Klement1,4, Nirmal J. Ghimire5,6, Jiaqiang Yan6,7, David G. Mandrus5,6,7, Wang Yao2 and Xiaodong Xu1,3* Coupling degrees of freedom of distinct nature plays a pseudospin up or down, respectively, which corresponds to electri- critical role in numerous physical phenomena1–10. The recent cal polarization. In a layered material with spin–valley coupling and emergence of layered materials11–13 provides a laboratory for AB stacking, such as bilayer TMDCs, both spin and valley are cou- studying the interplay between internal quantum degrees pled to layer pseudospin15. As shown in Fig. 1a, because the lower of freedom of electrons14,15. Here we report new coupling layer is a 180◦ in-plane rotation of the upper layer, the out-of-plane phenomena connecting real spin with layer pseudospins spin splitting has a sign that depends on both valley and layer pseu- in bilayer WSe2. In polarization-resolved photoluminescence dospins. Interlayer hopping thus has an energy cost equal to twice measurements, we observe large spin orientation of neutral the SOC strength λ. When 2λ is larger than the hopping amplitude and charged excitons by both circularly and linearly polarized t?, a carrier is localized in either the upper or lower layer depending excitation, with the trion spectrum splitting into a doublet on its valley and spin state. In other words, in a given valley, the at large vertical electrical field. -
A) Spin-Photon Correlations in Solid-State Systems
A) Spin-photon correlations in solid-state systems A. Imamoglu Quantum Photonics Group, Department of Physics ETH-Zürich Solid-state spins & emitters • Solid-state emitters (artificial atoms) can be used to realize high brightness long-lived single-photon sources: - no need for trapping - easy integration into a directional (fiber-coupled) cavity - up to 109 photons/sec with >70% efficiency • Three different classes of emitters: - rare-earth atoms embedded in a solid matrix (Er in glass) - Deep defects in insulators (NV centers in diamond) - Shallow defects in semiconductors (quantum dots) Note: While the concepts & techniques apply to a wide range of solid-state emitters, we focus on quantum dots Quantum dots & single photons A quantum dot (QD), is a mesoscopic semiconductor structure (~10nm confinement length-scale) consisting of 10,000 atoms and still having a discrete (anharmonic) optical excitation spectrum. -MBE grown InGaAs quantum dot -QDs in monolayer WSe2 Light generation by a quantum dot Resonant laser excitation - Laser excitation - - - - - Light generation by a quantum dot Resonant laser excitation - - Laser excitation - + - - - - electron-hole pair = exciton Light generation by a quantum dot Resonant laser excitation Resonance fluorescence 12000 9000 photon 6000 1X emission 3000 RF (counts/s) 0 - - -20 -10 0 10 20 - - Energy detuning (µeV) - - Quantum dot Spectroscopy From laser Polarization filter To detector Polarization optics NA=0.65 Spot size ≈1µm Magnet Piezo positioner GaAs InGaAs Liquid He GaAs Photon correlations from a single QD (2) : I(t)I(t ) : • Intensity (photon) correlation function: g ( ) 2 I(t) stop pulse • To measure g(2)(), photons from a quantum emitter are single photon detectors sent to a Hanbury-Brown Time-to- Twiss setup amplitude start (voltage) pulse converter • Single quantum emitter driven by a pulsed laser: absence of a center peak indicates that none of the pulses have > 1 photon (Robert, LPN). -
Spin Transport in a Quantum Hall Insulator
applied sciences Article Spin Transport in a Quantum Hall Insulator Azaliya Azatovna Zagitova 1,*, Andrey Sergeevich Zhuravlev 1, Leonid Viktorovich Kulik 1 and Vladimir Umansky 2 1 Institute of Solid State Physics, Russian Academy of Sciences, 142432 Chernogolovka, Russia; [email protected] (A.S.Z.); [email protected] (L.V.K.) 2 Braun Center for Submicron Research, Weizmann Institute of Science, Rehovot 76100, Israel; [email protected] * Correspondence: [email protected] Abstract: A novel experimental optical method, based on photoluminescence and photo-induced resonant reflection techniques, is used to investigate the spin transport over long distances in a new, recently discovered collective state—magnetofermionic condensate. The given Bose–Einstein condensate exists in a purely fermionic system (ν = 2 quantum Hall insulator) due to the presence of a non-equilibrium ensemble of spin-triplet magnetoexcitons—composite bosons. It is found that the condensate can spread over macroscopically long distances of approximately 200 µm. The propagation velocity of long-lived spin excitations is measured to be 25 m/s. Keywords: spintronics; spin transport; excitations; low-dimensional systems; spectroscopy; the Bose–Einstein condensate 1. Introduction The growing interest in spintronics [1,2] has been incited by the prospect of build- Citation: Zagitova, A.A.; Zhuravlev, ing fast, energy-efficient devices utilizing the electron spin. In particular, there has been A.S.; Kulik, L.V.; Umansky, V. Spin rapid development in magnonics [3], which uses spin waves to transport information [4,5]. Transport in a Quantum Hall Magnonic systems are free of many disadvantages of electronic systems associated with Insulator. -
Hadron Spectroscopy, Baryon Spectroscopy and Meson
Integrative Molecular Medicine Image ISSN: 2056-6360 Hadron spectroscopy, baryon spectroscopy and meson spectroscopy comparative study on malignant and benign human cancer cells and tissues under synchrotron radiation Alireza Heidari* Faculty of Chemistry, California South University, 14731 Comet St. Irvine, CA 92604, USA In the current study, we have experimentally and comparatively investigated and compared malignant human cancer cells and tissues before and after irradiating of synchrotron radiation using Hadron spectroscopy, Baryon spectroscopy and Meson spectroscopy. In the current study, we have experimentally and comparatively investigated and compared malignant human cancer cells and tissues before and after irradiating of synchrotron radiation using Hadron spectroscopy, Baryon spectroscopy and Meson spectroscopy. It is clear that malignant human cancer cells and tissues have gradually transformed to benign human cancer cells and tissues under synchrotron radiation with the passing of time (Figures 1-3) [1-198]. It can be concluded that malignant human cancer cells and tissues have gradually transformed to benign human cancer cells and tissues under synchrotron radiation with the passing of time (Figures 1-3) [1- 198]. Figure 2. Baryon spectroscopy analysis of malignant human cancer cells and tissues (a) before and (b) after irradiating of synchrotron radiation in transformation process to benign human cancer cells and tissues with the passing of time [1-198] *Correspondence to: Alireza Heidari, Faculty of Chemistry, California -
Time–Resolved Resonance FT–IR and Raman Spectroscopy And
Global Imaging Insights Image ISSN: 2399-7397 Time–resolved resonance FT–IR and raman spectroscopy and density functional theory investigation of vibronic– mode coupling structure in vibrational spectra of nano- polypeptide macromolecule beyond the multi–dimensional franck–condon integrals approximation and density matrix method Alireza Heidari1,2*, Jennifer Esposito1 and Angela Caissutti1 1Faculty of Chemistry, California South University, 14731 Comet St. Irvine, CA 92604, USA 2American International Standards Institute, Irvine, CA 3800, USA Abstract A macromolecule is a very large molecule, such as protein, commonly created by the polymerization of smaller subunits (monomers). They are typically composed of thousands of atoms or more. The most common macromolecules in biochemistry are biopolymers (nucleic acids, proteins, carbohydrates and lipids) and large non–polymeric molecules (such as lipids and macrocycles). Synthetic macromolecules include common plastics and synthetic fibers as well as experimental materials such as carbon nanotubes. Parameters such as FT –IR and Raman vibrational wavelengths and intensities for single crystal Nano polypeptide macromolecule are calculated using density functional theory and were compared with empirical results. The investigation about vibrational spectrum of cycle dimers in crystal with carboxyl groups from each molecule of acid was shown that it leads to create Hydrogen bonds for adjacent molecules. The current study aimed to investigate the possibility of simulating the empirical values. Analysis of vibrational spectrum of Nano polypeptide macromolecule is performed based on theoretical simulation and FT–IR empirical spectrum and Raman empirical spectrum using density functional theory in levels of HF/6–31G*, HF/6–31++G**, MP2/6–31G, MP2/6– 31++G**, BLYP/6–31G, BLYP/6–31++G**, B3LYP/6–31G and B3LYP6–31–HEG**. -
Hadron Spectroscopyspectroscopy Inin Diffractivediffractive Andand Centralcentral Productionproduction Processesprocesses Atat COMPASSCOMPASS
HadronHadron spectroscopyspectroscopy inin diffractivediffractive andand centralcentral productionproduction processesprocesses atat COMPASSCOMPASS Prometeusz Jasinski for the COMPASS collaboration - Diffraction 2010 - Beyond the qq model Constituent quark model QCD prediction: meson states beyond Color neutral qq systems Hybrids: qqg Quantum numbers (IG) JPC Tetraquarks: (qq)(qq) P=(-1)L+1 C=(-1)L+S G=(-1)I+L+1 → “Spin exotics” JPC multiplets: 0++, 0-+, 1--, 1+-, 1++, 2++, … -- +- -+ +- -+ Forbidden: 0 , 0 , 1 , 2 , 3 , ... Glueballs: gg, ggg Production mechanisms Diffractive Scattering Central Production The COMPASS Spectrometer 2008/2009 The COMPASS Spectrometer 2008/2009 Beam properties Beam properties Beam energy 190 GeV/c² Beam energy 190 GeV/c² Beam composition: - - Beam composition: p -: K -: p = 0.97 : 0.024 : 0.008 p : K : p = 0.97 : 0.024 : 0.008 or + + or p +: K +: p = 0.24 : 0.014 : 0.75 p : K : p = 0.24 : 0.014 : 0.75 Up to 5 x 10⁶ particles/s Up to 5 x 10⁶ particles/s beam The COMPASS Spectrometer 2008/2009 CEDARCEDAR detectors detectors for for beambeam particle particle identification identification The COMPASS Spectrometer 2008/2009 CEDARCEDAR detectors detectors for for beambeam particle particle identification identification Cerenkov Differential counter with Achromatic Ring Focus The COMPASS Spectrometer 2008/2009 RecoilRecoil proton proton detecto detectorr aroundaround 4040 cm cm long long lH2 lH2 target target oror ArrayArray of of solid solid state state discs discs The COMPASS Spectrometer 2008/2009 The COMPASS Spectrometer 2008/2009 Further important upgrades ECALECAL Laser Laser monitoringmonitoring system, system, radhard glass, Sandwich veto radhard glass, Sandwich veto shashlikshashlik modules modules matchingmatching the the spectrometer spectrometer acceptanceacceptance RICHRICH upgrade in 2006 SeveralSeveral tracking tracking upgrade in 2006 detectorsdetectors upgraded: upgraded: coldcold Silicon Silicon stations, stations, PixelPixel GEMs, GEMs, Micromegas,Micromegas, .. -
Lawrence Berkeley National Laboratory Recent Work
Lawrence Berkeley National Laboratory Recent Work Title MEASUREMENTS OP THE MUON-CAPTURE RATE IN He3 AND He4 Permalink https://escholarship.org/uc/item/0wd1f3t9 Author Easterling, Robert John. Publication Date 1964-04-09 eScholarship.org Powered by the California Digital Library University of California UCRL-11004 c.~ .. University of California Ernest 0. lawrence Radiation laboratory TWO-WEEK LOAN COPY This is a library Circulating Copy which may be borrowed for two weeks. For a personal retention copy, call Tech. Info. Dioision, Ext. 5545 MEASUREMENTS OF THE MUON-CAPTURE RATE IN He3 AND He 4 Berkeley. California DISCLAIMER This document was prepared as an account of work sponsored by the United States Government. While this document is believed to contain correct information, neither the United States Government nor any agency thereof, nor the Regents of the University of California, nor any of their employees, makes any warranty, express or implied, or assumes any legal responsibility for the accuracy, completeness, or usefulness of any information, apparatus, product, or process disclosed, or represents that its use would not infringe privately owned rights. Reference herein to any specific commercial product, process, or service by its trade name, trademark, manufacturer, or otherwise, does not necessarily constitute or imply its endorsement, recommendation, or favoring by the United States Government or any agency thereof, or the Regents of the University of California. The views and opinions of authors expressed herein do not necessarily state or reflect those of the United States Government or any agency thereof or the Regents of the University of California. UCRL-11004 .... UNIVERSITY OF CALIFORNIA Lawrence Radiation Laboratory Berkeley, California • AEC Contract No.