Neutrinos from the Sun
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Radiochemical Solar Neutrino Experiments, "Successful and Otherwise"
BNL-81686-2008-CP Radiochemical Solar Neutrino Experiments, "Successful and Otherwise" R. L. Hahn Presented at the Proceedings of the Neutrino-2008 Conference Christchurch, New Zealand May 25 - 31, 2008 September 2008 Chemistry Department Brookhaven National Laboratory P.O. Box 5000 Upton, NY 11973-5000 www.bnl.gov Notice: This manuscript has been authored by employees of Brookhaven Science Associates, LLC under Contract No. DE-AC02-98CH10886 with the U.S. Department of Energy. The publisher by accepting the manuscript for publication acknowledges that the United States Government retains a non-exclusive, paid-up, irrevocable, world-wide license to publish or reproduce the published form of this manuscript, or allow others to do so, for United States Government purposes. This preprint is intended for publication in a journal or proceedings. Since changes may be made before publication, it may not be cited or reproduced without the author’s permission. DISCLAIMER This report was prepared as an account of work sponsored by an agency of the United States Government. Neither the United States Government nor any agency thereof, nor any of their employees, nor any of their contractors, subcontractors, or their employees, makes any warranty, express or implied, or assumes any legal liability or responsibility for the accuracy, completeness, or any third party’s use or the results of such use 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 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 its contractors or subcontractors. -
PP and CNO-Cycle Nucleosynthesis: Kinetics and Numerical Modeling of Competitive Fusion Processes
University of Tennessee, Knoxville TRACE: Tennessee Research and Creative Exchange Supervised Undergraduate Student Research Chancellor’s Honors Program Projects and Creative Work 5-2012 PP and CNO-Cycle Nucleosynthesis: Kinetics and Numerical Modeling of Competitive Fusion Processes Matt Torrico [email protected] Follow this and additional works at: https://trace.tennessee.edu/utk_chanhonoproj Part of the Physical Processes Commons, and the Plasma and Beam Physics Commons Recommended Citation Torrico, Matt, "PP and CNO-Cycle Nucleosynthesis: Kinetics and Numerical Modeling of Competitive Fusion Processes" (2012). Chancellor’s Honors Program Projects. https://trace.tennessee.edu/utk_chanhonoproj/1557 This Dissertation/Thesis is brought to you for free and open access by the Supervised Undergraduate Student Research and Creative Work at TRACE: Tennessee Research and Creative Exchange. It has been accepted for inclusion in Chancellor’s Honors Program Projects by an authorized administrator of TRACE: Tennessee Research and Creative Exchange. For more information, please contact [email protected]. PP and CNO-Cycle Nucleosynthesis: Kinetics and Numerical Modeling of Competitive Fusion Processes M.N. TorricoA, M.W. GuidryA,B A Department of Physics and Astronomy, University of Tennessee, Knoxville, TN 37996, USA B Physics Division, Oak Ridge National Laboratory, Oak Ridge, TN 37831, USA Signed on 21 April 2012 Abstract The very history of matter (and hence Man) is exquisitely coupled to the nuclear fusion processes that power the Sun and other stars. The fusion of hydrogen into helium and other thermonuclear fusion processes (collectively called nucleosynthesis processes) provides us with not only the energy to carry on our lives, but the very materials that constitute our very bodies and our world. -
Quiz 1 Feedback! Queries & Concerns Earth's Magnetic Field/Shield Quiz
Quiz 1 Feedback! Queries & Concerns • There is no protection on Earth from solar radiation. 1. What usually happens to energetic charged particles from the Sun when they approach the Earth? ! – Fortunately, this is not true! The Earths atmosphere absorbs high- energy electromagnetic radiation (such as X-rays from solar flares). !There is a continual flow of particles from the outer layers As for the energetic charged particles flowing from the Sun, the of the Sun, sometimes called the solar wind. We are Earths magnetic field provides a shield against them. Instead of protected from them by the Earths magnetic field, traveling straight through and hitting the Earth, they are redirected which deflects them away (changes their direction) so to travel along the field lines that bend around the Earth. that they dont hit the Earth head-on. Some of the particles – The ongoing, relatively thin flow of particles from the Sun is called travel along the field lines to the Earths magnetic poles, the solar wind. CMEs are rare, occasional events where a lot of where they collide with molecules in the atmosphere, mass is expelled in a short period of time. causing the Northern and Southern lights, the aurorae. – Some particles follow the field lines to the Earths magnetic poles; (Aside: The light is produced when electrons within the when they hit the upper atmosphere in the polar regions, they molecules are knocked up to higher energy states, and produce a glow we call the Northern/Southern Lights or aurorae. then fall back down, emitting photons of light.)! – Other particles are trapped in doughnut-shaped regions called the Van Allen belts. -
A Half-Century with Solar Neutrinos*
REVIEWS OF MODERN PHYSICS, VOLUME 75, JULY 2003 Nobel Lecture: A half-century with solar neutrinos* Raymond Davis, Jr. Department of Physics and Astronomy, University of Pennsylvania, Philadelphia, Pennsylvania 19104, USA and Chemistry Department, Brookhaven National Laboratory, Upton, New York 11973, USA (Published 8 August 2003) Neutrinos are neutral, nearly massless particles that neutrino physics was a field that was wide open to ex- move at nearly the speed of light and easily pass through ploration: ‘‘Not everyone would be willing to say that he matter. Wolfgang Pauli (1945 Nobel Laureate in Physics) believes in the existence of the neutrino, but it is safe to postulated the existence of the neutrino in 1930 as a way say that there is hardly one of us who is not served by of carrying away missing energy, momentum, and spin in the neutrino hypothesis as an aid in thinking about the beta decay. In 1933, Enrico Fermi (1938 Nobel Laureate beta-decay hypothesis.’’ Neutrinos also turned out to be in Physics) named the neutrino (‘‘little neutral one’’ in suitable for applying my background in physical chemis- Italian) and incorporated it into his theory of beta decay. try. So, how lucky I was to land at Brookhaven, where I The Sun derives its energy from fusion reactions in was encouraged to do exactly what I wanted and get paid for it! Crane had quite an extensive discussion on which hydrogen is transformed into helium. Every time the use of recoil experiments to study neutrinos. I imme- four protons are turned into a helium nucleus, two neu- diately became interested in such experiments (Fig. -
Resolving the Solar Neutrino Problem
FEATURES Resolving the solar neutrino problem: Evidence for massive neutrinos in the Sudbury Neutrino Observatory Karsten M. Heeger for the SNO collaboration ............................................................................................................................................................................................................................................................ The solar neutrino problem are not features of the Standard Model of particle physics. In or more than 30 years, experiments have detected neutrinos quantum mechanics, an initially pure flavor (e.g. electron) can Pproduced in the thermonuclear fusion reactions which power change as neutrinos propagate because the mass components that the Sun. These reactions fuse protons into helium and release neu made up that pure flavor get out of phase. The probability for trinos with an energy of up to 15 MeY. Data from these solar neutrino oscillations to occurmayeven be enhanced in the Sun in neutrino experiments were found to be incompatible with the an energy-dependent and resonant manner as neutrinos emerge predictions of solar models. More precisely, the flux ofneutrinos from the dense core of the Sun. This effect of matter-enhanced detected on Earthwas less than expected, and the relative intensi neutrino oscillations was suggested by Mikheyev, Smirnov, and ties ofthe sources ofneutrinos in the sun was incompatible with Wolfenstein (MSW) and is one of the most promising explana those predicted bysolar models. By the mid-1990's the data -
Helioseismology, Solar Models and Solar Neutrinos
Helioseismology, solar models and solar neutrinos G. Fiorentini Dipartimento di Fisica, Universit´adi Ferrara and INFN-Ferrara Via Paradiso 12, I-44100 Ferrara, Italy E-mail: fi[email protected] and B. Ricci Dipartimento di Fisica, Universit´adi Ferrara and INFN-Ferrara Via Paradiso 12, I-44100 Ferrara, Italy E-mail: [email protected] ABSTRACT We review recent advances concerning helioseismology, solar models and solar neutrinos. Particularly we shall address the following points: i) helioseismic tests of recent SSMs; ii)the accuracy of the helioseismic determination of the sound speed near the solar center; iii)predictions of neutrino fluxes based on helioseismology, (almost) independent of SSMs; iv)helioseismic tests of exotic solar models. 1. Introduction Without any doubt, in the last few years helioseismology has changed the per- spective of standard solar models (SSM). Before the advent of helioseismic data a solar model had essentially three free parameters (initial helium and metal abundances, Yin and Zin, and the mixing length coefficient α) and produced three numbers that could be directly measured: the present radius, luminosity and heavy element content of the photosphere. In itself this was not a big accomplishment and confidence in the SSMs actually relied on the success of the stellar evoulution theory in describing many and more complex evolutionary phases in good agreement with observational data. arXiv:astro-ph/9905341v1 26 May 1999 Helioseismology has added important data on the solar structure which provide se- vere constraint and tests of SSM calculations. For instance, helioseismology accurately determines the depth of the convective zone Rb, the sound speed at the transition radius between the convective and radiative transfer cb, as well as the photospheric helium abundance Yph. -
An Introduction to Solar Neutrino Research
AN INTRODUCTION TO SOLAR NEUTRINO RESEARCH John Bahcall Institute for Advanced Study, Princeton, NJ 08540 ABSTRACT In the ¯rst lecture, I describe the conflicts between the combined standard model predictions and the results of solar neutrino experi- ments. Here `combined standard model' means the minimal standard electroweak model plus a standard solar model. First, I show how the comparison between standard model predictions and the observed rates in the four pioneering experiments leads to three di®erent solar neutrino problems. Next, I summarize the stunning agreement be- tween the predictions of standard solar models and helioseismological measurements; this precise agreement suggests that future re¯nements of solar model physics are unlikely to a®ect signi¯cantly the three solar neutrino problems. Then, I describe the important recent analyses in which the neutrino fluxes are treated as free parameters, independent of any constraints from solar models. The disagreement that exists even without using any solar model constraints further reinforces the view that new physics may be required. The principal conclusion of the ¯rst lecture is that the minimal standard model is not consistent with the experimental results that have been reported for the pioneering solar neutrino experiments. In the second lecture, I discuss the possibilities for detecting \smok- ing gun" indications of departures from minimal standard electroweak theory. Examples of smoking guns are the distortion of the energy spectrum of recoil electrons produced by neutrino interactions, the de- pendence of the observed counting rate on the zenith angle of the sun (or, equivalently, the path through the earth to the detector), the ratio of the flux of neutrinos of all types to the flux of electron neutrinos 1 (neutral current to charged current ratio), and seasonal variations of the event rates (dependence upon the earth-sun distance). -
19910023712.Pdf
SOLAR ASTRONOMY IX-1 Solar Astronomy 59-el N91-38026 Table of Contents 0. Executive Summary ................................ page 2 1. An Overview of Modern Solar Physics ......................... page 5 1.1 General Perspectives .............................. page 5 1.2 Frontiers and Goals for the 1990s ........................ page 8 1.2.1 The Solar Interior ............................ page 8 1.2.2 The Solar Surface ............................ page 9 1.2.3 The Outer Solar Atmosphere: Corona and Heliosphere ............ page 9 1.2.4 The Solar-Stellar Connection ....................... page 10 2. Ground-Based Solar Physics ............................. page 11 2.1 Introduction ................................. page 11 2.2 Status of Major Projects and Facilities ...................... page 11 2.3 A Prioritized Ground-based Program for the 1990s ................. page 12 2.3.1 Prerequisites .............................. page 12 2.3.2 Prioritization .............................. page 12 2.3.3 The Major Initiative: Solar Magnetohydrodynamics, and the LEST ....... page 12 2.3.3.1 The Large Earth-based Solar Telescope (LEST) ............ page 14 2.3.3.2 Infrared Facility Development .................... page 15 2.3.4 Moderate Initiatives ........................... page 15 2.3.5 Interdisciplinary Initiatives ........................ page 18 2.4 Conclusions and Summary ........................... page 20 3. Space Observations For Solar Physics ......................... page 20 3.1 Introduction ................................. page 20 3.2 -
Lecture 7: "Basics of Star Formation and Stellar Nucleosynthesis" Outline
Lecture 7: "Basics of Star Formation and Stellar Nucleosynthesis" Outline 1. Formation of elements in stars 2. Injection of new elements into ISM 3. Phases of star-formation 4. Evolution of stars Mark Whittle University of Virginia Life Cycle of Matter in Milky Way Molecular clouds New clouds with gravitationally collapse heavier composition to form stellar clusters of stars are formed Molecular cloud Stars synthesize Most massive stars evolve He, C, Si, Fe via quickly and die as supernovae – nucleosynthesis heavier elements are injected in space Solar abundances • Observation of atomic absorption lines in the solar spectrum • For some (heavy) elements meteoritic data are used Solar abundance pattern: • Regularities reflect nuclear properties • Several different processes • Mixture of material from many, many stars 5 SolarNucleosynthesis abundances: key facts • Solar• Decreaseabundance in abundance pattern: with atomic number: - Large negative anomaly at Be, B, Li • Regularities reflect nuclear properties - Moderate positive anomaly around Fe • Several different processes 6 - Sawtooth pattern from odd-even effect • Mixture of material from many, many stars Origin of elements • The Big Bang: H, D, 3,4He, Li • All other nuclei were synthesized in stars • Stellar nucleosynthesis ⇔ 3 key processes: - Nuclear fusion: PP cycles, CNO bi-cycle, He burning, C burning, O burning, Si burning ⇒ till 40Ca - Photodisintegration rearrangement: Intense gamma-ray radiation drives nuclear rearrangement ⇒ 56Fe - Most nuclei heavier than 56Fe are due to neutron -
Chapter 15--Our
2396_AWL_Bennett_Ch15/pt5 6/25/03 3:40 PM Page 495 PART V STELLAR ALCHEMY 2396_AWL_Bennett_Ch15/pt5 6/25/03 3:40 PM Page 496 15 Our Star LEARNING GOALS 15.1 Why Does the Sun Shine? • Why was the Sun dimmer in the distant past? • What process creates energy in the Sun? • How do we know what is happening inside the Sun? • Why does the Sun’s size remain stable? • What is the solar neutrino problem? Is it solved ? • How did the Sun become hot enough for fusion 15.4 From Core to Corona in the first place? • How long ago did fusion generate the energy we 15.2 Plunging to the Center of the Sun: now receive as sunlight? An Imaginary Journey • How are sunspots, prominences, and flares related • What are the major layers of the Sun, from the to magnetic fields? center out? • What is surprising about the temperature of the • What do we mean by the “surface” of the Sun? chromosphere and corona, and how do we explain it? • What is the Sun made of? 15.5 Solar Weather and Climate 15.3 The Cosmic Crucible • What is the sunspot cycle? • Why does fusion occur in the Sun’s core? • What effect does solar activity have on Earth and • Why is energy produced in the Sun at such its inhabitants? a steady rate? 496 2396_AWL_Bennett_Ch15/pt5 6/25/03 3:40 PM Page 497 I say Live, Live, because of the Sun, from some type of chemical burning similar to the burning The dream, the excitable gift. -
Pp-Chain and CNO Cycle
10 – pp-chain and CNO cycle introduc)on to Astrophysics, C. Bertulani, Texas A&M-Commerce 1 pp chain reaction in the Sun introduc)on to Astrophysics, C. Bertulani, Texas A&M-Commerce 2 10.1 - Hydrogen burning – ppI chain As a star forms from a giant cloud in the interstellar medium (protostar), density and temperature increase in its center. Fusion of hydrogen (1H) is the first long term nuclear energy source that can ignite. With only hydrogen available (for example, a first generation star) the ppI chain (see previous slide) is the only possible sequence of reactions. (other reaction chains require catalyst nuclei). The ppI chain proceeds as follows: 2 Step 1: p + p → He This does not work because 2He is unstable + (10.1) p + p → d + e + ve 3 (10.2) Step 2: d + p → He d d 4 He This does not work because the d abundance is + → too low. d + p leads to rapid destruction of d. 3 4 Step 3: He + p → Li Does not work because 4Li is unstable 3 He + d → 4 He + n Does not work because d abundance is too low 3 He + 3 He → 4 He + 2p (10.3) Last reaction is OK because Y3He gets large as there is no other rapid destruction. introduc)on to Astrophysics, C. Bertulani, Texas A&M-Commerce 3 10.1.1 - S-factors for the pp chain All reactions in the pp-chain are charge-dependent. The cross section has the form given by Eq. (9.49) which can be cast in the form b − where 1 E σ ∝ e (10.4) A1A2 E b 31.28 Z Z A1/2 keV A = = 1 2 (10.5) A1 + A2 (10.6) Typical units for S(E) are keV barn. -
The History and Impact of the CNO Cycles in Nuclear Astrophysics
Phys. Perspect. 20 (2018) 124–158 Ó 2018 Springer International Publishing AG, part of Springer Nature 1422-6944/18/010124-35 https://doi.org/10.1007/s00016-018-0216-0 Physics in Perspective The History and Impact of the CNO Cycles in Nuclear Astrophysics Michael Wiescher* The carbon cycle, or Bethe-Weizsa¨cker cycle, plays an important role in astrophysics as one of the most important energy sources for quiescent and explosive hydrogen burning in stars. This paper presents the intellectual and historical background of the idea of the correlation between stellar energy production and the synthesis of the chemical elements in stars on the example of this cycle. In particular, it addresses the contributions of Carl Friedrich von Weizsa¨cker and Hans Bethe, who provided the first predictions of the carbon cycle. Further, the experimental verification of the predicted process as it developed over the following decades is discussed, as well as the extension of the initial carbon cycle to the carbon- nitrogen-oxygen (CNO) multi-cycles and the hot CNO cycles. This development emerged from the detailed experimental studies of the associated nuclear reactions over more than seven decades. Finally, the impact of the experimental and theoretical results on our present understanding of hydrogen burning in different stellar environments is presented, as well as the impact on our understanding of the chemical evolution of our universe. Key words: Carl Friedrich von Weizsa¨cker; Hans Bethe; Carbon cycle; CNO cycle. Introduction The energy source of the sun and all other stars became a topic of great interests in the physics community in the second half of the nineteenth century.