JAERI-Tech 99-056 the JOINT PROJECT for HIGH-INTENSITY

Total Page:16

File Type:pdf, Size:1020Kb

JAERI-Tech 99-056 the JOINT PROJECT for HIGH-INTENSITY JAERI-Tech KEK Report99-4 99-056 JHF-99-3 THE JOINT PROJECT FOR HIGH-INTENSITY PROTON ACCELERATORS August 1999 The Joint Project Team of JAERI and KEK Japan Atomic Energy Research Institute Mi, u , H*m-{-Jjbmpmftmmutmmmm (1=319-1195 hx, is to This report is issued irregularly. Inquiries about availability of the reports should be addressed to Research Information Division, Department of Intellectual Resources, Japan Atomic Energy Research Institute, Tokai-mura, Naka-gun, Ibaraki-ken, 319-1195, Japan. ©Japan Atomic Energy Research Institute, 1999 JAERI-Tech 99-056 KEK Report 99-4 JHF-99-3 The Joint Project for High-Intensity Proton Accelerators The Joint Project Team of JAERI and KEK* Center for Neutron Science Tokai Research Establishment Japan Atomic Energy Research Institute Tokai-mura, Naka-gun, Ibaraki-ken (Received July 1,1999) Japan Atomic Energy Research Institute (JAERI) and the High Energy Accelerator Research Organization (KEK) agreed to promote the joint project integrating both the Neutron Science Project (NSP) of JAERI and the Japan Hadron Facility Project (JHF) of KEK for comprehensive studies on basic science and technology using high-intensity proton accelerator. This document describes the joint proposal prepared by the Joint Project Team of JAERI and KEK to construct accelerators and research facilities necessary both for the NSP and the JHF at the site of JAERI Tokai Establishment. Keywords : Joint Project, High-Intensity Proton Accelerator, Spallation Neutron Source, Particle Physics, Nuclear Physics, Hadron, Neutrino, Neutron Science, Structural Biology, Material Science, Muon Science, Exotic Nuclear Beams, Nuclear Waste Transmutation •XM.Furusaka*, R.Hino, Y.Ikeda, H.Ikezoe, J.Imazato* Y.Kuno* Y.Miyake* •ju 4< "k "k H.Miyatake , M.Mizumoto, Y.Mori , T.Mukaiyama, T.Nagae , K.Nagamine , S.Nagamiya , N.Niimura, T.Nomura , Y.Oyama, N.Sasamoto, S.Sawada , T.Shibata* H.Takano, M.Takasaki* N.Watanabe, Y.Yamazaki* and H.Yokomizo *: High Energy Accelerator Research Organization (KEK) JAERl-Tech 99-056 KEK Report 994 JHF-99-3 (19 9 r - <t t KP : =r319 1195 tf 01$* JAERl-Tech 99-056 The Joint Project for High-Intensity Proton Accelerators 23-April-1999 The Joint Project Team of JAERI and KEK JAERI-Tech 99-056 This document was compiled and edited by M.Furusaka2>, R.Hino0, Y.Dceda", H.flcezoe", J.Imazato2', Y.Kuno2), Y.Miyake2), H.Miyatake2), M.Mizumoto", Y.Mori2), T.Mukaiyama0, T.Nagae2), K.Nagamine2), S.Nagamiya2), N.Niimura0, T.Nomura2), Y.Oyama", N.Sasamoto", S.Sawada2), T.Shibata2), H.Takano15, M.Takasaki2), N.Watanabe^, Y.Yamazaki2), and H.Yokomizo0. 1): Japan Atomic Energy Research Institute (JAERI) 2): High Energy Accelerator Research Organization (KEK) JAERITech 99-056 CONTENTS 1 OVERVIEW OF THE JOINT PROJECT 1 1.1 THE HIGHEST BEAM POWER IN THE WORLD 1 1.2 ORIGINAL PROPOSALS AT JAERI AND KEK 1 1.2.1 Neutron Science Project at JAERI 1 1.2.2 Japan Hadron Facility (JHF) Project at KEK 3 1.3 ACCELERATORS AND SCIENCE IN THE JOINT PROJECT 4 1.4 ORGANIZATION 6 1.5 INTERNATIONAL RESPONSIBILITY 6 1.6 SITE SELECTION 7 2 RESEARCH FACILITIES AND PROGRAMS 8 2.1 PARTICLE AND NUCLEAR PHYSICS 8 2.1.1 Overview 8 2.1.2 Nuclear Physics 10 a. Hypernuclear Spectroscopy 10 b. Vector Mesons in Nuclei 11 c. Hyperon-Nucleon Scattering 11 d. Hadron Spectroscopy 12 2.1.3 Particle Physics 12 a. Rare K Decays 12 b. Studies of Fundamental Symmetries 12 c. Lepton Flavor Violation 13 d. Neutrino Oscillation 14 e. Fundamental Physics with Neutrons 14 2.1.4 Summary 75 2.2 NEUTRON SCIENCE 17 2.2.1 Introduction 17 2.2.2 Neutron Science 18 a. Overview of Neutron Science 18 b. Structual Biology 19 c. Soft Matter 20 d. Materials Science 21 e. Industrial Applications 22 2.2.3 Neutron Facility 23 a. Overview of Neutron Facility 23 b. Neutron Intensity and Pulse Structure 23 c. Neutron Source R&D 25 (1) JAERl-Tech 99-056 d. Guide line for Spectrometer Design 26 e. User Support Program 26 2.3 MUON SCIENCE 28 2.3.1 Overview 28 2.3.2 Facility Proposal 28 2.3.3 Muon Spin Probe for Condensed Matter Studies 29 2.3.4 Ultra-Slow /J* Source and its Application 31 2.3.5 Muon Catalyzed Fusion and Muonic Atoms 31 2.4 SCIENCE WITH EXOTIC NUCLEAR BEAMS 33 2.4.1 Overview 33 2.4.2 Some Research Subjects 34 a. Reaction mechanism of neutron-rich nuclei 34 b. Study of superheavy elements 34 c. Muonic atoms of unstable nuclei 35 d. Nuclear Astrophysics 35 e. Atom-at-a-time chemistry for heavy elements 35 f. Materials Science 36 2.5 NUCLEAR WASTE TRANSMUTATION 37 2.5.1 Overview 37 2.5.2 Concept of Transmutation System 38 2.5.3 Accelerator-Driven Transmutation Plant 39 2.5.4 Technical Issues for Demonstration of ADS 41 2.5.5 Experimental Facilities for ADS Technology Demonstration 42 2.5.6 International collaboration for ADS development 45 3 ACCELERATOR 47 3.1 INTRODUCTION 47 3.2 ACCELERATOR SCHEME 48 3.3 LINAC 52 3.4 LATTICE DESIGN 60 3.4.1 50-GeV Synchrotron 60 3.4.2 3-GeW Synchrotron 63 3.5 RESEARCH AND DEVELOPMENT FOR THE SYNCHROTRONS 64 3.6 CONCLUSION 67 4 RADIATION SAFETY 69 5 FUTURE EXTENSION OF THE PROJECT 71 5.1 PURPOSE OF THE PHASE 2 UPGRADE 71 (2) JAERI-Tech 99-056 5.2 ACCELERATORS FROM 1 MWTO5 MW 71 5.3 EXAMPLES OF OTHER UPGRADES 74 5.3.7 Particle and Nuclear Physics at Phase 2 74 5.3.2 Neutron Science at Phase 2 75 5.3.3 Muon Science at Phase 2 77 (3) 99-056 OVERVIEW OF THE PROJECT 1 Overview of the Joint Project 1.1 The Highest Beam Power in the World This document describes a new proposal to pursue frontier science in particle physics, nuclear physics, materials science, life science, and nuclear technology, using a new proton accelerator complex at the highest beam power in the world. The plan has been discussed and it is proposed jointly by the High Energy Accelerator Research Organization (KEK) under the Ministry of Education, Science, Sports and Culture (Monbusho) and the Japan Atomic Energy Research Institution (JAERI) under the Science and Technology Agency (STA). Previously, these institutions proposed the Japan Hadron Facility (JHF) at KEK and the Neutron Science Project (NSP) at JAERI, respectively. The present new joint plan, temporarily called the "Joint Project", is based on these two past proposals. It is also proposed that accelerators of this Joint Project be constructed at the JAERI site. The frontiers of accelerator science are in two complimentary directions. One path is towards the highest beam energy, examples for which are LEP (electron + positron collider at 100 GeV each), RHIC (Au + Au collider at 100 GeV per nucleon each), and LHC (proton + antiproton collider at 7 TeV each). The major purpose of these energy-frontier accelerators is to hunt for new particles, for example, in particle physics. The other path is towards the highest beam power. Many new accelerators are based on this philosophy, such as high- intensity electron accelerators that provide intense synchrotron radiation sources. In proton accelerators, the high beam power allows production of a variety of intense secondary particle beams such as kaons, neutrons, muons, neutrinos, antiprotons, and short-lived radioactive nuclear beams. In nuclear and particle physics, an example using these secondary beams is to measure rare processes such as neutrino oscillations and CP violation. In addition, sciences and technologies other than particle and nuclear physics can be carried out by using these secondary beams. These sciences and technologies include a) materials and life sciences with neutron and muon beams, b) accelerator-driven nuclear transmutation of long-lived nuclides in nuclear waste, and c) astrophysics research using radioactive isotope beams. The present proposal represents a major step in the direction of the intensity frontier. 1.2 Original Proposals at JAERI and KEK Before describing the Joint Proposal, the two original proposals are described in this section. 1.2.1 Neutron Science Project at JAERI The Neutron Science Project at JAERI aimed at construction of the world's most powerful spallation neutron source and research facility complex to enhance basic sciences and the accelerator application for transmutation of long-lived nuclides associated with nuclear power generation. The major facilities would be a superconducting proton linac, a 5- MW target station allowing neutron pulses for neutron scattering research, and research facilities for accelerator-driven transmutation technology, neutron physics, materials irradiation, and spallation radioactive ion (RI) beam production for exotic nuclei science. - 1 - OVERVIEW OF THE PROJECT JAERi-Tech 99-056 With an initial power level of 1.5 MW (1.5 GeV, 1mA) on target with the pulse mode, the superconducting linear accelerator complex would be expanded to 8 MW (5 MW) with cw mode (pulse mode), including a test facility with thermal power of 30 MW for demonstrating accelerator-driven transmutation technology. Since one of the major technical challenges of a high-current accelerator resides in the low-energy section, JAERI has been carrying out R&D for ion source, RFQ, and DTL since 1990. In a recent beam test with a 150 mA (peak) ion source and a 2-MeV RFQ, the peak current of 70 mA with a duty factor of 8% was achieved. A hot test model of a DTL for mock-up of the low-energy portion (2 MeV to 100 MeV) was fabricated and tested for high- power and high-duty (50%) operation. Another challenge is the development of a super- conducting linac for accelerating protons.
Recommended publications
  • How to Hack a Turned-Off Computer Or Running Unsigned
    HOW TO HACK A TURNED-OFF COMPUTER, OR RUNNING UNSIGNED CODE IN INTEL ME Contents Contents ................................................................................................................................ 2 1. Introduction ...................................................................................................................... 3 1.1. Intel Management Engine 11 overview ............................................................................. 4 1.2. Published vulnerabilities in Intel ME .................................................................................. 5 1.2.1. Ring-3 rootkits.......................................................................................................... 5 1.2.2. Zero-Touch Provisioning ........................................................................................... 5 1.2.3. Silent Bob is Silent .................................................................................................... 5 2. Potential attack vectors ...................................................................................................... 6 2.1. HECI ............................................................................................................................... 6 2.2. Network (vPro only)......................................................................................................... 6 2.3. Hardware attack on SPI interface ..................................................................................... 6 2.4. Internal file system .........................................................................................................
    [Show full text]
  • Issue #63, July 2000 Starting Our SIXTH Year in Publishing!
    Issue #63, July 2000 Starting our SIXTH year in publishing! 64a Page 1 Wed, Jul 2000 Cover by: Bill Perry [email protected] Published by My Mac Productions 110 Burr St., Battle Creek, MI 49015-2525 Production Staff Tim Robertson • [email protected] Publisher / Creator / Owner Editor-in-Chief Adam Karneboge • [email protected] Webmaster / Contributing Editor Roger Born • [email protected] Website Edior Barbara Bell • [email protected] Director, Public Relations •Jobs & Woz • Inspiration Artwork Created by: •Mike Gorman• [email protected] •Bill Perry• [email protected] •Tim Robertson• [email protected] •Adam Karneboge• [email protected] This Publication was created with: DOCMaker v4.8.4 http://www.hsv.tis.net/~greenmtn & Adobe Acrobat 4.0 http://www.adobe.com 64a Page 2 Wed, Jul 2000 Other Tools: Adobe Photoshop 5.5, 5.0.1 ColorIt! 4.0.1 BBEdit Lite ClarisWorks 5.0 Microsoft Word 98 GraphicConverter Snapz Pro 2.0 SimpleText Netscape Communicator 4.6.1 Internet Explorer 4.5 Eudora Pro 4.0.2 FileMaker Pro 4.0v3 QuickKeys 4.0 and the TitleTrack CD Player (To keep us sane!) Website hosted by Innovative Technologies Group Inc. http://www.inno-tech.com My Mac Magazine ® 1999-2000 My Mac Productions. All Rights Reserved. 64a Page 3 Wed, Jul 2000 http://www.inno-tech.com http://www.smalldog.com http://www.megamac.com 64a Page 4 Wed, Jul 2000 Advertising in My Mac = Good Business Sense! With over 500,000 website visits a month and thousands of email subscribers, You just can't go wrong! Send email to [email protected] for information.
    [Show full text]
  • Intel Management Engine Deep Dive
    Intel Management Engine Deep Dive Peter Bosch About me Peter Bosch ● CS / Astronomy student at Leiden University ● Email : [email protected] ● Twitter: @peterbjornx ● GitHub: peterbjornx ● https://pbx.sh/ About me Previous work: ● CVE-2019-11098: Intel Boot Guard bypass through TOCTOU attack on the SPI bus (Co-discovered by @qrs) Outline 1. Introduction to the Management Engine Operating System 2. The Management Engine as part of the boot process 3. Possibilities for opening up development and security research on the ME Additional materials will be uploaded to https://pbx.sh/ in the days following the talk. About the ME About ME ● Full-featured embedded system within the PCH ○ 80486-derived core ○ 1.5MB SRAM ○ 128K mask ROM ○ Hardware cryptographic engine ○ Multiple sets of fuses. ○ Bus bridges to PCH global fabric ○ Access to host DRAM ○ Access to Ethernet, WLAN ● Responsible for ○ System bringup ○ Manageability ■ KVM ○ Security / DRM ■ Boot Guard ■ fTPM ■ Secure enclave About ME ● Only runs Intel signed firmware ● Sophisticated , custom OS ○ Stored mostly in SPI flash ○ Microkernel ○ Higher level code largely from MINIX ○ Custom filesystems ○ Custom binary format ● Configurable ○ Factory programmed fuses ○ Field programmable fuses ○ SPI Flash ● Extensible ○ Native modules ○ JVM (DAL) Scope of this talk Intel ME version 11 , specifically looking at version 11.0.0.1205 Platforms: ● Sunrise Point (Core 6th, 7th generation SoC, Intel 100, 200 series chipset) ● Lewisburg ( Intel C62x chipsets ) Disclaimer ● I am in no way affiliated with Intel Corporation. ● All information presented here was obtained from public documentation or by reverse engineering firmware extracted from hardware found “in the wild”. ● Because this presentation covers a very broad and scarcely documented subject I can not guarantee accuracy of the contents.
    [Show full text]
  • The Strangeness Magnetic Moment of the Proton in the Chiral Quark Model
    The Strangeness Magnetic Moment of the Proton in the Chiral Quark Model L. Hannelius, D.O. Riska Department of Physics, University of Helsinki, 00014 Finland and L. Ya. Glozman Institute for Theoretical Physics, University of Graz, A-8019 Graz, Austria Abstract The strangeness magnetic moment of the proton is shown to be small in the chiral quark model. The dominant loop contribution is due to kaons. The K∗ loop contributions are proportional to the difference between the strange and light constituent quark masses or −2 mK∗ and therefore small. The loop fluctuations that involve radiative transitions between K∗ mesons and kaons are small, when the cut-off scale in the loops is taken to be close to the chiral symmetry restoration scale. The net loop amplitude contribution to the strangeness magnetic moment of the proton is about −0.05, which falls within the uncertainty range of arXiv:hep-ph/9908393v2 24 Aug 1999 the experimental value. 0 1. Introduction The recent finding by the SAMPLE collaboration that the strangeness magnetic moment s 2 2 of the proton is small, and possibly even positive [1] (GM (Q = 0.1 GeV )=0.23 ± 0.37) was unexpected in view of the fact that the bulk of the many theoretical predictions for this quantity are negative, and outside of the experimental uncertainty range (summaries are given e.g. in refs. [2, 3, 4]). A recent lattice calculation gives −0.36 ± 0.20 for this quantity [5], thus reaffirming the typical theoretical expectation, while remaining outside of the uncertainty range of the empirical value.
    [Show full text]
  • An Introduction to Morphos
    An Introduction to MorphOS Updated to include features to version 1.4.5 May 14, 2005 MorphOS 1.4 This presentation gives an overview of MorphOS and the features that are present in the MorphOS 1.4 shipping product. For a fully comprehensive list please see the "Full Features list" which can be found at: www.PegasosPPC.com Why MorphOS? Modern Operating Systems are powerful, flexible and stable tools. For the most part, if you know how to look after them, they do their job reasonably well. But, they are just tools to do a job. They've lost their spark, they're boring. A long time ago computers were fun, it is this background that MorphOS came from and this is what MorphOS is for, making computers fun again. What is MorphOS? MorphOS is a fully featured desktop Operating System for PowerPC CPUs. It is small, highly responsive and has very low hardware requirements. The overall structure of MorphOS is based on a new modern kernel called Quark and a structure divided into a series of "boxes". This system allows different OS APIs to be used along side one another but isolates them so one cannot compromise the other. To make sure there is plenty of software to begin with the majority of development to date has been based on the A- BOX. In the future the more advanced Q-Box shall be added. Compatibility The A-Box is an entire PowerPC native OS layer which includes source and binary compatibility with software for the Commodore A500 / A1200 etc.
    [Show full text]
  • Basics of Qcd Perturbation Theory
    BASICS OF QCD PERTURBATION THEORY Davison E. Soper* Institute of Theoretical Science University of Oregon, Eugene, OR 97403 ABSTRACT (•• i This is an introduction to the use of QCD perturbation theory, em- I phasizing generic features of the theory that enable one to separate short-time and long-time effects. I also cover some important classes of applications: electron-positron annihilation to hadrons, deeply in- elastic scattering, and hard processes in hadron-hadron collisions. •Supported by DOE Contract DE-FG03-96ER40969. © 1996 by Davison E. Soper. -15- 1 Introduction 2 Electron-Positron Annihilation and Jets A prediction for experiment based on perturbative QCD combines a particular In this section, I explore the structure of the final state in QCD. I begin with the calculation of Feynman diagrams with the use of general features of the theory. kinematics of e+e~ —> 3 partons, then examine the behavior of the cross section The particular calculation is easy at leading order, not so easy at next-to-leading for e+e~ —i- 3 partons when two of the parton momenta become collinear or one order, and extremely difficult beyond the next-to-leading order. This calculation parton momentum becomes soft. In order to illustrate better what is going on, of Feynman diagrams would be a purely academic exercise if we did not use certain I introduce a theoretical tool, null-plane coordinates. Using this tool, I sketch general features of the theory that allow the Feynman diagrams to be related to a space-time picture of the singularities that we find in momentum space.
    [Show full text]
  • Introduction to Storage and Software Systems for Data Analysis
    INTRODUCTION TO STORAGE AND SOFTWARE SYSTEMS FOR DATA ANALYSIS Bob Jacobsen University of California, Berkeley, USA Abstract The Storage and Software Systems for Data Analysis track discusses how HEP physics data is taken, processed and analyzed, with emphasis on the problems that data size and CPU needs pose for people trying to do experimental physics. The role of software engineering is discussed in the context of building large, robust systems that must at the same time be accessible to physicists. We include some examples of existing systems for physics analysis, and raise some issues to consider when evaluating them. This lecture is the introduction to those topics. 1. INTRODUCTION Many modern high-energy physics (HEP) experiments are done by collaborations of hundreds of people. Together, these groups construct and operate complex detectors, recording billions of events and terabytes of data, all toward the goal of “doing physics”. In this note, we provide an introduction to how we currently do this, and raise a number of issues to be considered when thinking about the new systems that are now being built. 2. SCALE OF THE EXPERIMENTS BaBar, CDF and D0 are examples of the large experiments now taking or about to take data in a collider environment. The collaborations that have built these experiments contain 300 to 600 members with varying levels of activity. Almost everybody is considered “familiar” with using computing to do their work, but only a small fraction of the collaboration can be considered as computing professionals. Some of these can even be considered world-class experts in large scale computing.
    [Show full text]
  • Quarkxpress 8.0 Readme Ii
    QuarkXPress 8.0 ReadMe ii Contents QuarkXPress 8.0 ReadMe....................................................................................................3 System requirements.............................................................................................................4 Mac OS.....................................................................................................................................................4 Windows...................................................................................................................................................4 Installing: Mac OS................................................................................................................5 Performing a silent installation.................................................................................................................5 Preparing for silent installation....................................................................................................5 Installing.......................................................................................................................................5 Performing a drag installation..................................................................................................................5 Adding files after installation...................................................................................................................6 Installing: Windows..............................................................................................................7
    [Show full text]
  • Lepton Probes in Nuclear Physics
    L C f' - l ■) aboratoire ATIONAI FR9601644 ATURNE 91191 Gif-sur-Yvette Cedex France LEPTON PROBES IN NUCLEAR PHYSICS J. ARVIEUX Laboratoire National Saturne IN2P3-CNRS A DSM-CEA, CESaclay F-9I191 Gif-sur-Yvette Cedex, France EPS Conference : Large Facilities in Physics, Lausanne (Switzerland) Sept. 12-14, 1994 ££)\-LNS/Ph/94-18 Centre National de la Recherche Scientifique CBD Commissariat a I’Energie Atomique VOL LEPTON PROBES IN NUCLEAR PHYSICS J. ARVTEUX Laboratoire National Saturne IN2P3-CNRS &. DSM-CEA, CESaclay F-91191 Gif-sur-Yvette Cedex, France ABSTRACT 1. Introduction This review concerns the facilities which use the lepton probe to learn about nuclear physics. Since this Conference is attended by a large audience coming from diverse horizons, a few definitions may help to explain what I am going to talk about. 1.1. Leptons versus hadrons The particle physics world is divided in leptons and hadrons. Leptons are truly fundamental particles which are point-like (their dimension cannot be measured) and which interact with matter through two well-known forces : the electromagnetic interaction and the weak interaction which have been regrouped in the 70's in the single electroweak interaction following the theoretical insight of S. Weinberg (Nobel prize in 1979) and the experimental discoveries of the Z° and W±- bosons at CERN by C. Rubbia and Collaborators (Nobel prize in 1984). The leptons comprise 3 families : electrons (e), muons (jt) and tau (r) and their corresponding neutrinos : ve, and vr . Nuclear physics can make use of electrons and muons but since muons are produced at large energy accelerators, they more or less belong to the particle world although they can also be used to study solid state physics.
    [Show full text]
  • Phenomenological Review on Quark–Gluon Plasma: Concepts Vs
    Review Phenomenological Review on Quark–Gluon Plasma: Concepts vs. Observations Roman Pasechnik 1,* and Michal Šumbera 2 1 Department of Astronomy and Theoretical Physics, Lund University, SE-223 62 Lund, Sweden 2 Nuclear Physics Institute ASCR 250 68 Rez/Prague,ˇ Czech Republic; [email protected] * Correspondence: [email protected] Abstract: In this review, we present an up-to-date phenomenological summary of research developments in the physics of the Quark–Gluon Plasma (QGP). A short historical perspective and theoretical motivation for this rapidly developing field of contemporary particle physics is provided. In addition, we introduce and discuss the role of the quantum chromodynamics (QCD) ground state, non-perturbative and lattice QCD results on the QGP properties, as well as the transport models used to make a connection between theory and experiment. The experimental part presents the selected results on bulk observables, hard and penetrating probes obtained in the ultra-relativistic heavy-ion experiments carried out at the Brookhaven National Laboratory Relativistic Heavy Ion Collider (BNL RHIC) and CERN Super Proton Synchrotron (SPS) and Large Hadron Collider (LHC) accelerators. We also give a brief overview of new developments related to the ongoing searches of the QCD critical point and to the collectivity in small (p + p and p + A) systems. Keywords: extreme states of matter; heavy ion collisions; QCD critical point; quark–gluon plasma; saturation phenomena; QCD vacuum PACS: 25.75.-q, 12.38.Mh, 25.75.Nq, 21.65.Qr 1. Introduction Quark–gluon plasma (QGP) is a new state of nuclear matter existing at extremely high temperatures and densities when composite states called hadrons (protons, neutrons, pions, etc.) lose their identity and dissolve into a soup of their constituents—quarks and gluons.
    [Show full text]
  • Inside Track
    Inside Track JOHN C. DVORAK neaking In the Back Door Dept.: to use those pesky legacy apps. A European If you think the battle of plat- If this machine achieves critical mass, consortium forms involves only Linux, it could reignite the dull computer Mac, and Windows, you’re in scene. There is a weird—even freaky— wants to float Sfor a rude awakening. enthusiasm about this project. It’s a a slew of Since 1995, a group of superstars work- community-based movement, which blimps to deliv- ing primarily in Europe has literally means that everything’s free. Tools are er broadband. morphed the architecture of the we-all- free, the OS is free, applications that thought-it-was-dead AmigaOS, probably cost money for other OSs are free for Who says the slickest, tightest code ever put on a MorphOS. The geeks are in high gear. they don’t desktop computer. With seven years of This is much more exciting than the smoke potent clean-room engineering, the new Morph- pedantic Linux world, which can’t seem OS runs on the PowerPC chip, and literal- to consolidate, let alone compete with marijuana in ly thousands of developers worldwide are Microsoft on the desktop. Europe? working with it. The new OS is best It’s not impossible for a new platform showcased in the PowerPC-based Genesi to emerge. Remember how Nintendo works. SkyLinc, from York, England, Pegasos computer, which runs both Mor- and Sega dominated the game scene for wants to position tethered blimps 5,000 phOS and various PPC versions so many years after the collapse of feet in the air over rural areas (with mile- of Linux.
    [Show full text]
  • MINIX 3 Di Alessandro Bottoni
    Mensile edito dall'Associazione di promozione sociale senza scopo di lucro Partito Pirata G Iscrizione Tribunale di Rovereto Tn n° 275 direttore responsabile Mario Cossali p.IVA/CF01993330222 I U G N O 2 0 0 8 anno 1 numero 7 prezzo di vendita: OpenContent (alla soddisfazione del lettore) L’IMMAGINE DEL MINORE E LA SUA TUTELA di Valeria Falcone 7 MINIX 3 di Alessandro Bottoni L'ossimoro dell' anonimato libero La Porta Galleggiante di Miyajima di Alessandro Bottoni Per parlare di anonimato è necessario prima chia- ecc.), lo fa per due motivi principali: 1) denuncia- rire cosa s'intende per un termine ben più re una vicenda che dovrebbe essere conosciuta pervasivo: libertà. Possiamo definire libero il dal pubblico e dalle Forze dell'ordine senza te- pensiero umano, ciò che pensiamo è uno ma di subire ritorsioni a livello personale; 2)non scambio di neuroni confinati all'interno della no- subire alcuna limitazione per la propria espres- stra scatola cranica, dipende da noi tradurli in sione. In entrambi i casi si tratta comunque di parole o lasciarli confinati nel nostro cervello. Al mancanza di libertà, nel primo caso c'è la paura di là del pensiero la libertà scema influenzata da delle conseguenze derivanti da una condizione migliaia di variabili, ambientali, culturali o situazio- oggettiva di inferiorità vera o supposta, nel se- ni contingenti. In qualsiasi società la libertà è poi condo caso per condizionamenti, i più diversi, o limitata dalle regole che permettono di definire per evitare coinvolgimenti personali. In una so- più o meno marcatamente la libertà dei singoli in cietà idilliaca ogni cittadino dovrebbe essere rapporto alla collettività.
    [Show full text]