World Premier International Research Center Initiative (WPI) FY2012 WPI Project Progress Report (Post-Interim Evaluation)
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Atsuto Suzuki
Atsuto Suzuki (KEK : High Energy Accelerator Research Organization) 1 2 1. Quark Flavor Project 2. Lepton Flavor Project 3. Energy Frontier Project 4. Non-Accelerator Project 5. Summary 3 In 2008 4 Quest for International Linear Collider Quest for Unifying Birth-Evolution (ILC) Matter and Force of Universe Scientific Activities Beyond Standard Physics Lepton CP Asymmetry Technology Innovations Power-Upgrade Talented Human Resources SuperKEKB J-PARC KEK-B Quark CP Asymmetry LHC [Origin of Matter] nt Quest for Neutrinos nm Quest for 6 Quarks ne [Origin of Force] Higgs Particle [Origin of Mass] e-/e+ Collider KEKB -> SuperKEKB SCC RF(HER) Belle Detector 8 GeV e- 3.5 GeV e+ 1036 SuperKEKB Ares RF ) 1 - 50 times higher s cavity 2 - luminosity e+ source Peak Luminosity Luminosity (cm Peak TRISTAN 6 15 countries, 400 collaborators # of papers : 315 # of citations : 13,309 CPV: caused by a single phase of CKM matrix7 Standard Model X(3872) Z(4430) SM quar k lept on Bgdg transition BgD*tn Upgrade KEKB to SuperKEKB with x 50 performance 8 KEKB upgrade to SuperKEKB Colliding bunches IR with by*=0.3mm SC final focus system e-(2.6A) SuperKEKB Low emittance lattice Add RF systems for e+(3.6A) higher beam current Damping ring for low emittance positron injection Positron NEG pumps capture section LER beampipe to suppress photoelectron instability Beam SR Target: L = 8x1035/cm2/s 9 Belle II Detector (in comparison with Belle) EKLM Module 0 @ITEP Aerogel- RICH Bell SVD: 4 DSSD lyrs g 2 DEPFET lyrs + 4 DSSD lyrs CDC: small cell, long lever arm Bell II ACC+TOF g TOP+A-RICH ECL: waveform sampling (+pure CsI for end-caps) KLM: RPC g Scintillator +MPPC(end-caps) Inconsistency in unitarity triangle? B -> fKs J-PARC Facility (KEK/JAEA) Linac 3 GeV RCS Neutrino Beams (to Kamioka) Materials and Life Experimental Facility (n, m) Hadron Exp. -
Arxiv:0711.0760V3 [Hep-Th]
DBI N-flation John Ward1 Department of Physics and Astronomy, University of Victoria, Victoria BC, V8P 1A1, Canada Abstract We investigate DBI inflation using N multiple branes and show how the configuration is equivalent to a single wrapped D5-brane with flux. We then show how 1/N corrections can be implemented, and we examine the sound speed and levels of non-Gaussianities in two distinct cases. For models with constant warping we find that the non-Gaussian amplitude is bounded from above (as a function of γ). For AdS backgrounds we find that the signature is generally large and positive, although is no longer globally defined over the full phase space. We then investigate an inflationary mechanism using a representation cascade, whereby the transition from a reducible representation to the irrep drives inflation. arXiv:0711.0760v3 [hep-th] 26 Nov 2007 [email protected] 1 Introduction In the absence of any direct test of string theory, cosmology remains the best laboratory with which to test string theoretic models [1]. Over the past few years we have witnessed cosmology become a precision science, with COBE, WMAP and SDSS [2] providing crucial support for the flatness of the universe, the existence of dark energy and for a period of cosmic inflation. Whilst the dark energy puzzle remains an outstanding problem for theoretical physics in general [3], inflation has been a carefully developed paradigm with many explicit models. Unfortunately as far as inflationary model building is concerned, there are still many problems to be resolved. Particularly since many of the models suffer from super-Planckian VEV’s for the inflaton field [1], and therefore find themselves in a region where quantum gravity effects are non-negligible. -
Is There Eternal Inflation in the Cosmic Landscape ?
Is there eternal inflation in the cosmic landscape ? Henry Tye Cornell University hep-th/0611148 ArXiv:0708.4374 [hep-th] with Qing-Guo Huang, ArXiv:0803.0663 [hep-th] with Dan Wohns and Yang Zhang, ArXiv:0811.3753 [hep-th] IPMU, 04/01/09 Expansion of the universe k ρm ρr H2 =Λ+ + + a2 a3 a4 • a(t) = the cosmic scale factor ~ size of universe • H = Hubble constant =(da/dt)/a • Λ = dark energy ~ cosmological constant ~ effective potential • k = curvature • ρm = matter density at initial time • ρr = radiation density at initial time • H = constant ⇒ a = eHt Inflation BRIEF ARTICLE THE AUTHOR 1 (1) d = s(Λc)/ξ +1 ∼ ∼ 1 ∼ −1/4 (2) ξ s(Λs) Λs ms (3) d>60 BRIEF ARTICLE (4) T (n) " T0/n THE AUTHOR 4 (5) Γ = msT (6) n ∼ 1/Hs 1 Eternal Inflation Ht 3 3Ht (7) (1) a(t) " e → V = a(t) " e τ > 1/H Suppose the universe is sitting at a local minimum, with a ln L (2)lifetime longer than the Hubble lntime:g ∼− L = −e Then the number of Hubble patches will increase −Si (3) exponentially. Even after some Hubble patchesαi have∼ e decayed, there would be many remaining Hubble patches (4) that continue to inflate. |βij| < αi (5) Eternal inflation impliesφi = thatϕi/f i somewhere in the universe (outside our horizon),d −1 (6) Γt ∼ n Γ0 inflation is still happening today. T (A → B)T (B → C) (7) T (A → C)= ∼ T0/2 T (A → B)+T (B → C) −S (8) ΓA→B = ΓB→C = Γ0 ∼ e 2 (9) ΓA→C ∼ ΓA→BΓB→C = Γ0 1 1 2 (10) tA→C = tA→B + tB→C = + ∼ → → 1 ΓA B ΓB C Γ0 Γ0 (11) Γ → = A C 2 −S (12) Γ(1) = Γ0 ∼ e − (13) Γ(2) ∼ e 2S − (14) Γ(2) ∼ e S − (15) Γ(n) ∼ e S (16) +H2φ2 2 2 (17) H = U/3MP 1 Flux compactification in Type II string theory where all moduli of the 6-dim. -
The Minimal Supersymmetric Leptogenesis∗
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by CERN Document Server August 3, 1999 IASSNS-HEP-99/69 LBNL-44042 hep-ph/9908223 The Minimal Supersymmetric Leptogenesis∗ Takeo Moroi1 and Hitoshi Murayama2,3 1School of Natural Sciences, Institute for Advanced Study Princeton, New Jersey 08540 2Theoretical Physics Group Ernest Orlando Lawrence Berkeley National Laboratory University of California, Berkeley, California 94720 and 3Department of Physics University of California, Berkeley, California 94720 Abstract We reanalyze the supersymmetric leptogenesis model by one of the ˜ authors (HM) and Yanagida based on L = Hu flat direction in detail. We point out that the appropriate amount of baryon asymmetry can be generated in this model with the neutrino mass matrix consistent with the atmospheric neutrino oscillation and solutions to the solar neutrino problem, preferably the small angle MSW solution. The reheating temperature can be low enough to avoid the cosmological gravitino problem. This model is the minimal one because it does not rely on any new physics beyond supersymmetry and Majorana neutrino masses. ∗This work was supported in part by the U.S. Department of Energy under Con- tracts DE-AC03-76SF00098, in part by the National Science Foundation under grants PHY-95-13835 and PHY-95-14797. TM was also supported by the Marvin L. Goldberger Membership. HM was also supported by Alfred P. Sloan Foundation. 1. Introduction Cosmic baryon asymmetry has been one of the biggest puzzles in mod- ern cosmology. It is hoped to understand it in terms of microscopic physics and evolution of Universe, if the well-known Sakharov’s three conditions are satisfied: (1) existence of baryon-number violation, (2) existence of CP vio- lation, and (3) departure from thermal equilibrium. -
Submitted Proposal
Trimmed version of the CNAP PFC proposal to the NSF (page numbers refer to those in the upper right-hand corners) 1 NSF coverpage 2 Project Summary 3 Executive Summary 6 Prior Accomplishments 11 Major Activities Introduction 13 MA1: Neutrino Phenomenology 21 MA2: Neutrino Technology 31 MA3: Neutrino Frontier 41 Education, Development and Outreach 44 Shared Facilities 47 Collaboration with other sectors 49 International Collaboration 50 Seed Funding and Emerging Areas 51 Management 55 Institutional and Other Commitments 56 NSF Summary Table 57 References 64 Abbreviated Biographical Information 73 Center Budget Justification 81 Letter from NC Museum of Natural Sciences 82 List of Supporting Letters 1 COVER SHEET FOR PROPOSAL TO THE NATIONAL SCIENCE FOUNDATION PROGRAM ANNOUNCEMENT/SOLICITATION NO./CLOSING DATE/if not in response to a program announcement/solicitation enter NSF 08-1 FOR NSF USE ONLY NSF 07-567 01/30/08 NSF PROPOSAL NUMBER FOR CONSIDERATION BY NSF ORGANIZATION UNIT(S) (Indicate the most specific unit known, i.e. program, division, etc.) PHY - PHYSICS FRONTIER CENTER DATE RECEIVED NUMBER OF COPIES DIVISION ASSIGNED FUND CODE DUNS# (Data Universal Numbering System) FILE LOCATION 003137015 EMPLOYER IDENTIFICATION NUMBER (EIN) OR SHOW PREVIOUS AWARD NO. IF THIS IS IS THIS PROPOSAL BEING SUBMITTED TO ANOTHER FEDERAL TAXPAYER IDENTIFICATION NUMBER (TIN) A RENEWAL AGENCY? YES NO IF YES, LIST ACRONYM(S) AN ACCOMPLISHMENT-BASED RENEWAL 546001805 NAME OF ORGANIZATION TO WHICH AWARD SHOULD BE MADE ADDRESS OF AWARDEE ORGANIZATION, INCLUDING -
Observational Cosmology - 30H Course 218.163.109.230 Et Al
Observational cosmology - 30h course 218.163.109.230 et al. (2004–2014) PDF generated using the open source mwlib toolkit. See http://code.pediapress.com/ for more information. PDF generated at: Thu, 31 Oct 2013 03:42:03 UTC Contents Articles Observational cosmology 1 Observations: expansion, nucleosynthesis, CMB 5 Redshift 5 Hubble's law 19 Metric expansion of space 29 Big Bang nucleosynthesis 41 Cosmic microwave background 47 Hot big bang model 58 Friedmann equations 58 Friedmann–Lemaître–Robertson–Walker metric 62 Distance measures (cosmology) 68 Observations: up to 10 Gpc/h 71 Observable universe 71 Structure formation 82 Galaxy formation and evolution 88 Quasar 93 Active galactic nucleus 99 Galaxy filament 106 Phenomenological model: LambdaCDM + MOND 111 Lambda-CDM model 111 Inflation (cosmology) 116 Modified Newtonian dynamics 129 Towards a physical model 137 Shape of the universe 137 Inhomogeneous cosmology 143 Back-reaction 144 References Article Sources and Contributors 145 Image Sources, Licenses and Contributors 148 Article Licenses License 150 Observational cosmology 1 Observational cosmology Observational cosmology is the study of the structure, the evolution and the origin of the universe through observation, using instruments such as telescopes and cosmic ray detectors. Early observations The science of physical cosmology as it is practiced today had its subject material defined in the years following the Shapley-Curtis debate when it was determined that the universe had a larger scale than the Milky Way galaxy. This was precipitated by observations that established the size and the dynamics of the cosmos that could be explained by Einstein's General Theory of Relativity. -
Instructions to Authors
www.elsevier.com/locate/physletb Instructions to authors Aims and Scope Physics Letters B ensures the rapid publication of letter-type communications in the fields of Nuclear Physics, Particle Physics and Astrophysics. Articles should influence the physics community significantly. Submission Electronic submission is strongly encouraged. The electronic file, accompanied by a covering message, should be e-mailed to one of the Editors indicated below. Easy submission via the LANL-preprint server is certainly possible; please visit http://www.elsevier.com/locate/plbsubmission. If electronic submission is not feasible, submission in print is possible, but it will delay publication. In the latter case manuscripts (one original + two copies), accompanied by a covering letter, should be sent to one of the following Editors: L. Alvarez-Gaumé, Theory Division, CERN, CH-1211 Geneva 23, Switzerland, E-mail address: Luis.Alvarez-Gaume@CERN. CH Theoretical High Energy Physics (General Theory) J.-P. Blaizot, ECT*, Strada delle Tabarelle, 266, I-38050 Villazzano (Trento), Italy, E-mail address: [email protected]. FR Theoretical Nuclear Physics M. Cvetic,ˇ David Rittenhouse Laboratory, Department of Physics, University of Pennsylvania, 209 S, 33rd Street, Philadelphia, PA 19104-6396, USA, E-mail address: [email protected] Theoretical High Energy Physics M. Doser, EP Division, CERN, CH-1211 Geneva 23, Switzerland, E-mail address: [email protected] Experimental High Energy Physics D.F. Geesaman, Argonne National Laboratory, 9700 South Cass Avenue, Argonne, IL 60439, USA, E-mail address: [email protected] Experimental Nuclear Physics H. Georgi, Department of Physics, Harvard University, Cambridge, MA 02138, USA, E-mail address: Georgi@PHYSICS. -
Annual Report 2010 Report Annual IPMU ANNUAL REPORT 2010 April 2010 April – March 2011March
IPMU April 2010–March 2011 Annual Report 2010 IPMU ANNUAL REPORT 2010 April 2010 – March 2011 World Premier International Institute for the Physics and Mathematics of the Universe (IPMU) Research Center Initiative Todai Institutes for Advanced Study Todai Institutes for Advanced Study The University of Tokyo 5-1-5 Kashiwanoha, Kashiwa, Chiba 277-8583, Japan TEL: +81-4-7136-4940 FAX: +81-4-7136-4941 http://www.ipmu.jp/ History (April 2010–March 2011) April • Workshop “Recent advances in mathematics at IPMU II” • Press Release “Shape of dark matter distribution” • Mini-Workshop “Cosmic Dust” May • Shaw Prize to David Spergel • Press Release “Discovery of the most distant cluster of galaxies” • Press Release “An unusual supernova may be a missing link in stellar evolution” June • CL J2010: From Massive Galaxy Formation to Dark Energy • Press Conference “Study of type Ia supernovae strengthens the case for the dark energy” July • Institut d’Astrophysique de Paris Medal (France) to Ken’ichi Nomoto • IPMU Day of Extra-galactic Astrophysics Seminars: Chemical Evolution August • Workshop “Galaxy and cosmology with Thirty Meter Telescope (TMT)” September • Subaru Future Instrumentation Workshop • Horiba International Conference COSMO/CosPA October • The 3rd Anniversary of IPMU, All Hands Meeting and Reception • Focus Week “String Cosmology” • Nishinomiya-Yukawa Memorial Prize to Eiichiro Komatsu • Workshop “Evolution of massive galaxies and their AGNs with the SDSS-III/BOSS survey” • Open Campus Day: Public lecture, mini-lecture and exhibits November -
CHINA and LATIN AMERICA Economic and Trade Cooperation in the Next 10 Years
Advance Information CHINA AND LATIN AMERICA Economic and Trade Cooperation in the Next 10 Years By Zhenxing Su (China Academy of Social Sciences, China) Translated by Hongling Zhao (Beijing Institute of Technology, China) Key Features: Pub Date: May 2017 • Features solid argumentation and substantial evidences Binding: Hardcover • Contains historical materials, analyses current situation and predicts the future trends ISBN: 978-981-3202-28-3 of relationship between China and Latin America Price: £123 Description: Page Extent: 500pp The international financial crisis in 2008 marked the beginning of important changes in the international economic system. The emerging market economies are increasingly Type: Monograph becoming a driving force for the global economic growth. Under such circumstances, the Main Subject: Asian Studies Sino–Latin American economic and trade cooperation has entered a new period of historical Sub-subjects: China Studies; opportunity. Based on the economic development trend and the adjustment of policy, this Asian Economies; Asian Politics/ book explores the prospect for Sino–Latin American economic and trade cooperation. It Society; International Relations; tracks the development path for this cooperation in the next 10 years by analyzing resource International Economics; General endowment, industrial structure, economic system, development pattern, basic economic Economics; Developmental policy, economic environment, economic and trade relations between China and Latin Economics America. BIC: KCLT Author: BISAC: BUS069020; POL011020; Su Zhenxing studied Russian in the Beijing Foreign Language College for one year from 1959 POL024000 to 1960. From 1960 to 1964, he studied Spanish at the department of western languages and Keywords: China; Latin America; literature in Peking University. He is a Researcher and PhD student advisor at the Institute of Economic Cooperation; Trade Latin American Studies of the Chinese Academy of Social Sciences. -
Sky and Telescope
sizingup Inflation By Steve Nadis in january 1980, a young Stanford physicist named Alan Guth unveiled a brilliant idea that had just one drawback: it didn’t work. At the time, Guth (now a professor at MIT) was fully aware of this shortcoming, yet he was convinced of the idea’s impor- tance nevertheless. History shows his faith to have been well placed. Unlike most 25-year-old ideas that don’t quite work, this one, which Guth called “inflation,” was not dis- carded long ago. Instead, the notion of a fleeting yet explosive growth spurt in the universe’s earliest mo- ments has become a cornerstone of modern cosmology. University of Chicago astrophysicist Michael Turner goes further, calling inflation “the most important idea in cosmology since the Big Bang.” 32 November 2005 Sky & Telescope What put the bang in the Big Bang? A physical force whose nature remains cloaked in mystery. S&T illustration by Casey B. Reed Sky & Telescope November 2005 33 psizing up inflation When Guth first conceived of inflation, he doubted that were delayed by “supercooling,” so that it occurred at a lower the idea would be rigorously tested within his lifetime. But temperature than otherwise would have been the case (just inflation has already passed numerous observational hur- as supercooled water turns to ice well below its normal dles with flying colors. Now, with the age of “precision cos- freezing point). Late one night in December 1979, Guth mology” upon them, astronomers hope to see whether this discovered another consequence of supercooling: it would powerful idea holds up to even closer scrutiny. -
Why the Cosmological Constant Is So Small? a String Theory Perspective
i \9-Tye" | 2018/3/9 | 22:36 | page 1803 | #1 i i i ADV. THEOR. MATH. PHYS. Volume 21, Number 7, 1803{1818, 2017 Why the cosmological constant is so small? A string theory perspective S.-H. Henry Tye (with Yoske Sumitomo and Sam Wong) With no free parameter (except the string scale MS), dynami- cal flux compactification in Type IIB string theory determines both the cosmological constant (vacuum energy density) Λ and the Planck mass MP in terms of MS, thus yielding their relation. Following elementary probability theory, we find that a good frac- tion of the meta-stable de Sitter vacua in the cosmic string theory landscape tend to have an exponentially small cosmological con- stant Λ compared to either the string scale MS or the Planck scale 4 4 MP , i.e., Λ MS MP . Here we illustrate the basic stringy idea with a simple scalar field φ3 (or φ4) model coupled with fluxes to show how this may happen and how the usual radiative insta- bility problem is bypassed (since there are no parameters to be fine-tuned). These low lying semi-classical de Sitter vacua tend to be accompanied by light scalar bosons/axions, so the Higgs boson mass hierarchy problem may be ameliorated as well. 1. Introduction Cosmological data strongly indicates that our universe has a vanishingly small positive cosmological constant Λ (or vacuum energy density) as the dark energy, −122 4 (1.1) Λ ∼ 10 MP −1=2 19 where the Planck mass MP = GN ' 10 GeV. Such a small Λ is a major puzzle in physics.1 In general relativity, Λ is a free arbitrary parameter one can introduce, so its smallness can be accommodated but not explained within quantum field theory. -
Looking Back Over 27 Years of Grant-In-Aid Recidivism by Dr
KAKENHI ESSAY SERIES No.14(Feb2009) Looking Back over 27 Years of Grant-in-Aid Recidivism By Dr. Atsuto Suzuki, Director General, High Energy Accelerator Research Organization (KEK) Looking back over the evolution of my research, I couldn’t have cut myself off from Grants-in-Aid even if I had tried. Among the results the program has yielded has been the ability to acquire budgets for well-equipped facilities and to pioneer new fields of research. My initial contact with the Grant-in-Aid Program took place when I moved from the University of Tokyo to the High Energy Accelerator Research Organization (KEK). Over a 27-year period from 1982 through 2008, I have in both the capacities as a principal and collaborating investigator received support every year from the program. I have listed below these many Grant-in-Aid supported projects. From FY 1982-1984: Specially Promoted Research, titled “Verification of Grand Unified Theory; Nucleon Decay Experiment, Using Water Cherenkov Detector” (Representative: Koshiba Masatoshi) This grant helped foster the Kamiokande (Kamioka nuclear decay) facility and its experiments. The objective of Kamiokande was to verify the Grand Unified Theory by detecting and elucidating the nucleon decay phenomenon. From FY 1985-1986: Basic Research (A), titled “Proton Decay Experiment” (Representative: Teruhiro Suda) This was the most discouraging period in the operation of Kamiokande, as great difficulty was being experienced in detecting nucleon decay and the future of the facility seemed bleak. Then, Dr. Koshiba detected the solar neutrino, so plans were initiated to retool the Kamiokande devices. From FY 1986-1987: Basic Research (A), titled “Observation of Solar Neutrinos” (Representative: Yoji Totsuka) Through a process of trial and error the Kamiokande facility was reconstructed.