Scientific Realism and Primordial Cosmology
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BABAR Studies Matter-Antimatter Asymmetry in Τ Lepton Decays
BABAR studies matter-antimatter asymmetry in τττ lepton decays Humans have wondered about the origin of matter since the dawn of history. Physicists address this age-old question by using particle accelerators to recreate the conditions that existed shortly after the Big Bang. At an accelerator, energy is converted into matter according to Einstein’s famous energy-mass relation, E = mc 2 , which offers an explanation for the origin of matter. However, matter is always created in conjunction with the same amount of antimatter. Therefore, the existence of matter – and no antimatter – in the universe indicates that there must be some difference, or asymmetry, between the properties of matter and antimatter. Since 1999, physicists from the BABAR experiment at SLAC National Accelerator Laboratory have been studying such asymmetries. Their results have solidified our understanding of the underlying micro-world theory known as the Standard Model. Despite its great success in correctly predicting the results of laboratory experiments, the Standard Model is not the ultimate theory. One indication for this is that the matter-antimatter asymmetry allowed by the Standard Model is about a billion times too small to account for the amount of matter seen in the universe. Therefore, a primary quest in particle physics is to search for hard evidence for “new physics”, evidence that will point the way to the more complete theory beyond the Standard Model. As part of this quest, BABAR physicists also search for cracks in the Standard Model. In particular, they study matter-antimatter asymmetries in processes where the Standard Model predicts that asymmetries should be very small or nonexistent. -
The Belle-II Experiment at Superkekb
Gary S. Varner, Hawai’i The Belle-II Experiment at SuperKEKB Gary S. Varner University of Hawai’i at Manoa Boston (Cambridge), July 26, 2011 Luminosity at the B Factories Gary S. Varner, Hawai’i Fantastic performance much beyond design values! Need O(100x) more data Next generation B-factories Gary S. Varner, Hawai’i SuperKEKB + SuperB 40 times higher luminosity KEKB PEP-II Asymmetric B factories Gary S. Varner, Hawai’i √s=10.58 GeV + - B e e z ~ c Υ(4s) B Υ(4s) B ~ 200m BaBar p(e-)=9 GeV p(e+)=3.1 GeV =0.56 Belle p(e-)=8 GeV p(e+)=3.5 GeV =0.42 Belle II p(e-)=7 GeV p(e+)=4 GeV =0.28 Full Reconstruction Method Gary S. Varner, Hawai’i • Fully reconstruct one of the B’s to – Tag B flavor/charge – Determine B momentum – Exclude decay products of one B from further analysis Decays of interest B BXu l , BK e e+(3.5GeV) (8GeV) BD, Υ(4S) B full reconstruction BD etc. (~0.5%) Offline B meson beam! Powerful tool for B decays with neutrinos “Super” B Factory motivation Gary S. Varner, Hawai’i For details on physics opportunities: See Kay Kinoshita talk 17:20 B factories is SM with CKM right? Thursday, July 28 – Section 5I Super B factories How is the SM wrong? Need much more data (two orders!) because the SM worked so well until now Super B factory e+e- machines running at (or near) Y(4s) will have considerable advantages in several classes of measurements, and will be complementary in many more to LHCb and BESIII Recent update of the physics reach with 50 ab-1 (75 ab-1): Physics at Super B Factory (Belle II authors + guests) hep-ex > arXiv:1002 .5012 SuperB Progress Reports: Physics (SuperB authors + guests) hep-ex > arXiv:1008.1541 TSUKUBA Area (Belle) High Energy Ring (HER) for Electron HER LER How to do it? Interaction Region Low Energy Ring (LER) for Positron Gary S. -
Inflationary Cosmology: from Theory to Observations
Inflationary Cosmology: From Theory to Observations J. Alberto V´azquez1, 2, Luis, E. Padilla2, and Tonatiuh Matos2 1Instituto de Ciencias F´ısicas,Universidad Nacional Aut´onomade Mexico, Apdo. Postal 48-3, 62251 Cuernavaca, Morelos, M´exico. 2Departamento de F´ısica,Centro de Investigaci´ony de Estudios Avanzados del IPN, M´exico. February 10, 2020 Abstract The main aim of this paper is to provide a qualitative introduction to the cosmological inflation theory and its relationship with current cosmological observations. The inflationary model solves many of the fundamental problems that challenge the Standard Big Bang cosmology, such as the Flatness, Horizon, and the magnetic Monopole problems. Additionally, it provides an explanation for the initial conditions observed throughout the Large-Scale Structure of the Universe, such as galaxies. In this review, we describe general solutions to the problems in the Big Bang cosmology carry out by a single scalar field. Then, with the use of current surveys, we show the constraints imposed on the inflationary parameters (ns; r), which allow us to make the connection between theoretical and observational cosmology. In this way, with the latest results, it is possible to select, or at least to constrain, the right inflationary model, parameterized by a single scalar field potential V (φ). Abstract El objetivo principal de este art´ıculoes ofrecer una introducci´oncualitativa a la teor´ıade la inflaci´onc´osmica y su relaci´oncon observaciones actuales. El modelo inflacionario resuelve algunos problemas fundamentales que desaf´ıanal modelo est´andarcosmol´ogico,denominado modelo del Big Bang caliente, como el problema de la Planicidad, el Horizonte y la inexistencia de Monopolos magn´eticos.Adicionalmente, provee una explicaci´onal origen de la estructura a gran escala del Universo, como son las galaxias. -
Superb Report Intensity Frontier Workshop 1 Introduction
SuperB Report Intensity Frontier Workshop 1 Introduction The Standard Model (SM) has been very successful in explaining a wide range of electroweak and strong processes with high precision. In the flavor sector, observation of CP violation in B decays at BABAR and Belle, and the extraordinary consistency between the CKM matrix elements, established the SM as the primary source of CP violation in nature (leading to the 2008 Nobel Prize in physics). However, the remarkable success of the SM in describing all known flavor-physics measurements presents a puzzle to the search for New Physics (NP) at the LHC. New particles below the TeV scale should contribute to low-energy processes through virtual loop diagrams and cause observable effects in the flavor sector. The lack of any such effects suggests that either the NP mass scale is much higher than the TeV scale, or that NP flavor-violating operators are suppressed. In either scenario, flavor physics at the intensity frontier is poised to remain a central element of particle physics research in the coming decades. The INFN-sponsored SuperB project [1–3] in Italy is an asymmetric-energy electron- positron collider in the 10 GeV energy region with an initial design average luminosity of 1036 cm−2s−1, which will deliver up to 75 ab−1 in five years of operation (see Fig. 1 for details) to a new SuperB detector derived from the existing BABAR. A new innovative concept in accelerator design, employing very low-emittance beams and a “crab waist” final focus, makes possible this large increase (100-fold) in instantaneous luminosity over present B Factory colliders with no corresponding increase in power consumption, and similar backgrounds for the detector. -
Phy306 Introduction to Cosmology Homework 3 Notes
PHY306 INTRODUCTION TO COSMOLOGY HOMEWORK 3 NOTES 1. Show that, for a universe which is not flat, 1 − Ω 1 − Ω = , where Ω = Ω r + Ω m + Ω Λ and the subscript 0 refers to the present time. [2] This was generally quite well done, although rather lacking in explanation. You should really define the Ωs, and you need to explain that you divide the expression for t by that for t0. 2. Suppose that inflation takes place around 10 −35 s after the Big Bang. Assume the following simplified properties of the universe: ● it is matter dominated from the end of inflation to the present day; ● at the present day 0.9 ≤ Ω ≤ 1.1; ● the universe is currently 10 10 years old; ● inflation is driven by a cosmological constant. Using these assumptions, calculate the minimum amount of inflation needed to resolve the flatness problem, and hence determine the value of the cosmological constant required if the inflation period ends at t = 10 −34 s. [4] This was not well done at all, although it is not really a complicated calculation. I think the principal problem was that people simply did not think it through—not only do you not explain what you’re doing to the marker, you frequently don’t explain it to yourself! Some people therefore got hopelessly confused between the two time periods involved—the matter-dominated epoch from 10 −34 s to 10 10 years, and the inflationary period from 10 −35 to 10 −34 s. The most common error—in fact, considerably more common than the right answer—was simply assuming that during the post-inflationary epoch 1 − . -
The High Redshift Universe: Galaxies and the Intergalactic Medium
The High Redshift Universe: Galaxies and the Intergalactic Medium Koki Kakiichi M¨unchen2016 The High Redshift Universe: Galaxies and the Intergalactic Medium Koki Kakiichi Dissertation an der Fakult¨atf¨urPhysik der Ludwig{Maximilians{Universit¨at M¨unchen vorgelegt von Koki Kakiichi aus Komono, Mie, Japan M¨unchen, den 15 Juni 2016 Erstgutachter: Prof. Dr. Simon White Zweitgutachter: Prof. Dr. Jochen Weller Tag der m¨undlichen Pr¨ufung:Juli 2016 Contents Summary xiii 1 Extragalactic Astrophysics and Cosmology 1 1.1 Prologue . 1 1.2 Briefly Story about Reionization . 3 1.3 Foundation of Observational Cosmology . 3 1.4 Hierarchical Structure Formation . 5 1.5 Cosmological probes . 8 1.5.1 H0 measurement and the extragalactic distance scale . 8 1.5.2 Cosmic Microwave Background (CMB) . 10 1.5.3 Large-Scale Structure: galaxy surveys and Lyα forests . 11 1.6 Astrophysics of Galaxies and the IGM . 13 1.6.1 Physical processes in galaxies . 14 1.6.2 Physical processes in the IGM . 17 1.6.3 Radiation Hydrodynamics of Galaxies and the IGM . 20 1.7 Bridging theory and observations . 23 1.8 Observations of the High-Redshift Universe . 23 1.8.1 General demographics of galaxies . 23 1.8.2 Lyman-break galaxies, Lyα emitters, Lyα emitting galaxies . 26 1.8.3 Luminosity functions of LBGs and LAEs . 26 1.8.4 Lyα emission and absorption in LBGs: the physical state of high-z star forming galaxies . 27 1.8.5 Clustering properties of LBGs and LAEs: host dark matter haloes and galaxy environment . 30 1.8.6 Circum-/intergalactic gas environment of LBGs and LAEs . -
Discovery at the Large Hadron Collider
Discovery at the Large Hadron Collider Michel Lefebvre University of Victoria ATLAS Canada Collaboration CAP Congress 27 May 2013 Abstract Discovery at the Large Hadron Collider The recent discovery of a new particle is a historic event in our exploration of the fundamental constituents of matter and the interactions between them. To date, the Standard Model of particle physics is extremely successful and accounts for all measured subatomic phenomena. However the postulated Higgs mechanism, from which fundamental particles acquire mass, remains to be verified experimentally. Research at the energy frontier is being carried out at the Large Hadron Collider (LHC), operating at CERN near Geneva since 2010. From 2010 to 2012, the LHC provided proton-proton collisions at a centre of mass energy of 7 to 8 TeV, allowing the exploration of distance scales smaller than a tenth of an attometer. The products of these collisions were successfully recorded by the ATLAS detector, which will be introduced in this lecture, with emphasis on Canadian contributions. The ATLAS physics programme features Standard Model measurements and a rich array of searches for new physics phenomena. The discovery of a new Higgs-like particle and other important results will be presented. The future increase in energy and intensity at the LHC, and the associated ATLAS plans, will also be discussed. These are exciting times indeed for particle physics! Michel Lefebvre, UVic and ATLAS Canada CAP Congress, 27 May 2013 2 Scattering experiment We see through the scatter of -
Introduction to Flavour Physics
Introduction to flavour physics Y. Grossman Cornell University, Ithaca, NY 14853, USA Abstract In this set of lectures we cover the very basics of flavour physics. The lec- tures are aimed to be an entry point to the subject of flavour physics. A lot of problems are provided in the hope of making the manuscript a self-study guide. 1 Welcome statement My plan for these lectures is to introduce you to the very basics of flavour physics. After the lectures I hope you will have enough knowledge and, more importantly, enough curiosity, and you will go on and learn more about the subject. These are lecture notes and are not meant to be a review. In the lectures, I try to talk about the basic ideas, hoping to give a clear picture of the physics. Thus many details are omitted, implicit assumptions are made, and no references are given. Yet details are important: after you go over the current lecture notes once or twice, I hope you will feel the need for more. Then it will be the time to turn to the many reviews [1–10] and books [11, 12] on the subject. I try to include many homework problems for the reader to solve, much more than what I gave in the actual lectures. If you would like to learn the material, I think that the problems provided are the way to start. They force you to fully understand the issues and apply your knowledge to new situations. The problems are given at the end of each section. -
On a Christian Cosmogony Or: Why Not Take Genesis 1 As History and Try to Put Together a Cosmogony That Fits It?
On a Christian Cosmogony or: Why not take Genesis 1 as history and try to put together a cosmogony that fits it? This is an elegantly posed question which is instructive and informative to answer as it stands. Genesis 1 is not history, cannot be history, and was not intended to be history. Cosmo gony ("a theory, system, or account of the creation or generation of the universe" OED,2b) could never be properly historical, and currently we cannot conceive of it as being properly scientific. Cosmo geny ("evolution of the universe", OED) is properly scientific, but is not directly treated in the first Genesis creation account. And even if it were, the proper way to do science is to start with the evidence and to proceed to the conclusion. The suggestion that one should determine a conclusion arbitrarily from a text and then fit the evidence to suit is a shocking distortion of the the proper way to search for truth and should be abhorred by all Christians. Let me unpack this answer so that you can see what I do (and every Christian ought to) believe, and also what I do not (and no Christian should) believe. On Genesis History The first part of the question asserts that the Bible in general and Genesis 1 in particular is historical. This assertion is a very attractive one. In particular, there is absolutely no doubt that Christianity is nothing if not a historical religion. This is made crystal clear in a variety of places. Dr. Luke is explicit about drawing up an account of the things that have been fulfilled among us, just as they were handed down to us by those who from the first were eyewitnesses (Lk.1:1). -
AST4220: Cosmology I
AST4220: Cosmology I Øystein Elgarøy 2 Contents 1 Cosmological models 1 1.1 Special relativity: space and time as a unity . 1 1.2 Curvedspacetime......................... 3 1.3 Curved spaces: the surface of a sphere . 4 1.4 The Robertson-Walker line element . 6 1.5 Redshifts and cosmological distances . 9 1.5.1 Thecosmicredshift . 9 1.5.2 Properdistance. 11 1.5.3 The luminosity distance . 13 1.5.4 The angular diameter distance . 14 1.5.5 The comoving coordinate r ............... 15 1.6 TheFriedmannequations . 15 1.6.1 Timetomemorize! . 20 1.7 Equationsofstate ........................ 21 1.7.1 Dust: non-relativistic matter . 21 1.7.2 Radiation: relativistic matter . 22 1.8 The evolution of the energy density . 22 1.9 The cosmological constant . 24 1.10 Some classic cosmological models . 26 1.10.1 Spatially flat, dust- or radiation-only models . 27 1.10.2 Spatially flat, empty universe with a cosmological con- stant............................ 29 1.10.3 Open and closed dust models with no cosmological constant.......................... 31 1.10.4 Models with more than one component . 34 1.10.5 Models with matter and radiation . 35 1.10.6 TheflatΛCDMmodel. 37 1.10.7 Models with matter, curvature and a cosmological con- stant............................ 40 1.11Horizons.............................. 42 1.11.1 Theeventhorizon . 44 1.11.2 Theparticlehorizon . 45 1.11.3 Examples ......................... 46 I II CONTENTS 1.12 The Steady State model . 48 1.13 Some observable quantities and how to calculate them . 50 1.14 Closingcomments . 52 1.15Exercises ............................. 53 2 The early, hot universe 61 2.1 Radiation temperature in the early universe . -
Inscribing Bodies in Vedic Cosmogony and Samskara Rituals Christine Boulos University of South Florida, [email protected]
University of South Florida Scholar Commons Graduate Theses and Dissertations Graduate School January 2011 From Cosmogony to Anthropogony: Inscribing Bodies in Vedic Cosmogony and Samskara Rituals Christine Boulos University of South Florida, [email protected] Follow this and additional works at: http://scholarcommons.usf.edu/etd Part of the American Studies Commons, Feminist, Gender, and Sexuality Studies Commons, and the Religion Commons Scholar Commons Citation Boulos, Christine, "From Cosmogony to Anthropogony: Inscribing Bodies in Vedic Cosmogony and Samskara Rituals" (2011). Graduate Theses and Dissertations. http://scholarcommons.usf.edu/etd/3715 This Thesis is brought to you for free and open access by the Graduate School at Scholar Commons. It has been accepted for inclusion in Graduate Theses and Dissertations by an authorized administrator of Scholar Commons. For more information, please contact [email protected]. From Cosmogony to Anthropogony: Inscribing Bodies in Vedic Cosmogony and Samskara Rituals by Christine E. Boulos A thesis submitted in partial fulfillment of the requirements for the degree of Master of Arts Department of Religious Studies College of Arts and Sciences University of South Florida Major Professor: Carlos Lopez, Ph.D. Pratyusha Basu, Ph.D. Wei Zhang, Ph.D. Date of Approval: November 1, 2011 Keywords: Judith Butler, performativity, sex, gender mantras Copyright © 2011, Christine E. Boulos DEDICATION This thesis is dedicated to my husband, David. Thank you for supporting me emotionally, physically, and spiritually. You have always made me and my education a priority, whether it was listening patiently as I tried to explain my thoughts and my projects, or spending the weekend with Elijah so I could get two more days in of writing or studying. -
Italy Cancels €1Bn Superb Collider - Physicsworld.Com 30/11/12 20.01
Italy cancels €1bn SuperB collider - physicsworld.com 30/11/12 20.01 This site uses cookies. By continuing to use this site you agree to our use of cookies. To find out more, see our Privacy and Cookies policy. Italy cancels €1bn SuperB collider Nov 28, 2012 11 comments Path not taken: the planned route of SuperB Physics World can confirm rumours that the Italian government is to withdraw €250m from the €1bn SuperB particle accelerator, which was set to be built at the University of Tor Vergata on the outskirts of Rome. The decision, which effectively cancels the project, was made yesterday when Fernando Ferroni, president of the National Institute for Nuclear Physics (INFN), met Italian science minister Francesco Profumo to discuss funding for the project. "Given the difficult economic conditions of the country, the government is willing to confirm the contribution of €250m but not [for] the project," says a government statement, which was released today and seen by Physics World. As outlined in the statement, the INFN, which was set to build SuperB, will keep the €250m but will now spend the money on other projects. The INFN has already appointed two committees to look at what options it has, which includes converting SuperB into a scaled down "tau-charm factory" (called SuperC) or using the money elsewhere. The committees will report by 20 December, with a decision set for early January. Rumours of the funding cancellation first emerged on the blog A Quantum Diaries Survivor, which is written by the CERN-based researcher Tommaso Dorigo. Mystery of antimatter SuperB was designed to produce beams of electrons and positrons inside a linear accelerator to an energy of 6.7 GeV before injecting them into two rings each more than 1 km in circumference, where they would have then been collided to allow the decay of particles such as B mesons.