Stellar Helium Burning. He-Burning in massive Stars

Size: px
Start display at page:

Download "Stellar Helium Burning. He-Burning in massive Stars"

Transcription

1 Stellar lium Burig -Burig i massive Stars -burig is igited o the ad ashes of the precedig hydroge burig phase! Most importat reactio -triple alpha process 3 12 C 7.96 MeV Eergy productio i helium burig eutro productio i helium burig Ucertaities i the weak s-process

2 Stellar Evolutio of Massive Stars m/m log time util core collapse [y]

3 Critical Reactios i -burig O helium fuel produced i precedig hydroge burig Oxyge-16 Eergy source i stellar burig Eergy release determied by associated reactio rates

4 etwork for stellar lium burig C C O O O C C C e e O O O O C C dt d dt d dt d dt d = = = =

5 budace evolutio i stellar core Declie of time-scale icrease i 12 C 16 O equilibrium 12 C/ 16 O Rapid declie i. time [s]

6 The case of: 3- ad 12 C 16 O Reactio rates determied by strog resoaces ad E2 direct capture cotributios sigifyig strog alpha cluster state cofiguratios i the T=0 uclei alog the reactio path! θ 2 1 θ MeV MeV MeV MeV MeV MeV MeV MeV 2 θ θ θ Be 12 C 16 O

7 The Reactio as two step process r first step! = Q=0.092 MeV 8 Be 0 8 Be 12 C 8 Be T 1/2 8 Be = s Γ =6.8 ev pure cluster cofiguratio fast capture equilibrium betwee capture ad decay pplicatio of Saha Equatio For calculatig 8 Be equilibrium: π µ kt Be = h 3/ 2 e Q kt

8 Example for 8 Be equilibrium abudace: Case of typical -burig: T=0.1GK T 9 =0.1; =10 5 g/cm 3 8 Be = / 2 T T9 e Be.10 = i i 8 Be ~ oe 8 Be ucleus for 3 10 particles

9 Resoat capture o 8 Be secod step! The Hoyle resoace! E R =0.287MeV 7.65 MeV 0 Q=7.367 MeV 8 Be e e - σv = ω µ T 3/ 2 e E T R.39 MeV 2 ω = 2J 1 ω = Γi Γ Γ 9 tot out MeV ± 12% 12 C 0 Decay by sequetial E2 trasitios or iteral e e - pair coversio

10 12 C C 16 O the Holy Grail Level ad Iterferece Structure betwee 1 - levels E1 ad 2 states ad direct capture E2. Ucertaity i low eergy extrapolatio

11 R-matrix aalysis Complex resoace structure iterferig broad resoaces Parameters from probig 16 O compoud ucleus through elastic scatterig β-delayed -decay resoat capture -trasfer reactio photo-dissociatio 12 C 12 C Bochum D 16 β 12 C ale TRIUMF L 12 C 16 O Caltech Müster Quees Stuttgart Bochum 12 C 7 Lit 16 O UM TUL 16 O 12 C HIS

12 R-matrix fit examples E1-term E2-term S E1 80 kev bar S E2 85 kev-bar From Kuz et al. PRL

13 12 C 16 O reactio rate = T 2/3 9 S eff [ MeV b] e / 3 T 9 cm s 3 S eff 0.17 [ MeV b] T 2/3 9 e / 3 T 9 cm s 3 Oly very crude estimate! E-T depedecy eeds to be cosidered!

14 16 O 20 e rate ad Oly a few sigle resoaces o strog o-resoat term i the excitatio curve observed! o-resoat direct capture E2 compoet expected. o-resoat M1 compoet most likely too weak to be of relevace?

15 ew results E2 Direct Reactio Compoet 1e-12 1e06 1e-13 1e05 ormalized ield 1e- 1e-15 1e-16 1e-17 Resoaces S-Factor MeV-bar Ceter of Mass Eergy MeV 10 1e Ceter of Mass Eergy MeV 1e-13 ormalized ield 1e- 1e-15 Upper Limits S eff 2. 8 MeV bar 1e-16 1e-17 Resoaces ad E2 Direct Capture Ceter of Mass Eergy MeV ppreciable o resoat compoet which eeds to be implemeted as DC reactio rate cotributio.

16 Reactio Rates for 12 C 16 O & 16 O 20 e 1.0E00 reactio rate [ccm/s mol] 1.0E E E E E E-30 Gamow Rage 16 O 20 e 12 C 16 O temperature [GK] 12 C 16 O rate domiates over the 16 O 20 e rate at the typical -burig temperatures T~ GK.

17 Cosequeces of the 12 C 16 O ad 16 O 20 e reactio rates! O Late Stellar Evolutio determies Carbo ad/or Oxyge phase = / i i i C Type Ia Superova cetral carbo burig of C/O white dwarf M =13 M 1.0 CF CF e.1e.3e.5e Time s Type II Superova shock-frot ucleosythesis i C ad shells of pre-superova star

18 Stellar eutro Sources i massive Stars Fβ ν O e or e T-depedet icrease of -productio

19 Reactio etwork for -sources e e x O O e e e e F F O O O p F F F F F dt d dt d dt d dt d dt d β β β λ λ λ = = = = = eutro productio through e 25 Mg depeds o reactio rates of this sequece

20 Example: e 25 Mg e 25 Mg low eergy resoaces? The potetial existece of low eergy resoaces causes cosiderable ucertaity i reactio rate

21 Two chael problems! Extrapolatio to lower eergies Impact of the e brach The MeV state is a proouced cluster state i 26 Mg! re there uboud cluster states above the threshold? re there uboud cluster states below the -threshold?

22 eutro productio β β β β λ λ λ λ e e e x e e x e e e e F F O O O F F F dt d dt d dt d dt d dt d dt d = = = = = = = = = eutro flux depeds o seed abudace from H burig ad reactio rate ad brachig coditios i alpha capture sequece!

23 Measuremet with gas target Low eergy beam ito exteded e gas-target

24 eutro Detector rray Gas-cell target Combiatio with udergroud muo shieldig ecessary for reductio of muo iduced eutros

25 Complemetary -trasfer studies i 26 Mg Q = MeV? Q = MeV Observatioal evidece for cluster cofiguratio ear the threshold of 26 Mg at MeV! Recet studies with better resolutio by Ugalde et al cofirmed more resoaces.

26 Reactio Rate Limits ad Ucertaities

27 Weak s-process β β λ λ e e x Z Z dt d dt d ± ± = = Leads to ~100

28 budace evolutio i weak s-process

29 Weak-s-process abudaces CRE lower limit CRE upper limit Large ucertaities i the fial weak s-process abudace distributio due to the ucertaities i the e rates. This traslates ito ucertaity for: Weak s-process abudaces Seed material for p-process ad p-process abudaces LEPP or secod r-process

30 From s- to p-process FZ Karlsruhe LSCE/LL _ToF/CER OREL/ORL s-process build up of elemets ear =100 depedig o eutro flux ad -capture reactio rates TOMKI Demokritos/DTL Bochum FZ Karlsruhe otre Dame TU Darmstadt s-process build up of seed isotopes High photo flux required high temperature eviromets uclear ucertaities associated with the uclear structure i the Z=50 =50 closed shell regio.

31 Possible impact o seed coditios i ext burig sequece ucleosythesis for Z 12 eutro productio lower limit 20 M upper limit lower limit upper limit e for Carbo burig as secod s-process site -productio for s-process

32 The low eergy cross sectio of 13 C 16 O Direct measuremet Brue et al Drotleff et al Strog idicatio of subthreshold state! Idirect trasfer studies 13 C 6 Lid 17 O Kuboo et al Keeley et al Johso et al Hamache et al 2008 Ucertaities: -3 kev 1/2 subthreshold state -90 kev 3/2 subthreshold state First C results idicate a weaker resoace stregth as suggested by direct S-factor extrapolatio secod C study icreases value!

33 Low-eergy low-backgroud Experimet with π BaF 2 -array - beam eutro detectio through the coversio of eutros through Cd with -detectio i surroudig BaF 2 array! ctive shieldig techiques; Pulse shape aalysis; eutro backgroud 0.0 /s il et al. 2008

34 Fit predictios for 13 C S-factor Fits of all possible reactio chaels 13 C 16 O 16 O 13 C 13 C 13 C 16 O 16 O 13 C 13 C 16 O 16 O This work il et al LPH EERG [kev] Low eergy extrapolatio i good agreemet with the C predictios!

Structure and evolution of AGB stars

Structure and evolution of AGB stars Structure ad evolutio of AGB stars M bol T eff The mai s-process s i AGB stars H 12 C(p,γ) 13 N(β + υ) 13 C 13 C(α,) He-flash eutro source 13 C(α,) 16 dy 13 dt dy dt C = Y = x 13 Y C X Y 4 Y He ρ N ρ N

More information

He-Burning in massive Stars

He-Burning in massive Stars He-Burning in massive Stars He-burning is ignited on the He and ashes of the preceding hydrogen burning phase! Most important reaction -triple alpha process 3 + 7.6 MeV Red Giant Evolution in HR diagram

More information

Lecture 23: Origin of the Elements 2 Hertzsprung Russell Diagram

Lecture 23: Origin of the Elements 2 Hertzsprung Russell Diagram Lecture 23: Origi of the Elemets 2 Hertzsprug Russell Diagram Temperature, size ad lumiosity We kow that for objects that are approximately blackbodies Hotter thigs are brighter. o Eergy radiated per uit

More information

Physics Methods in Art and Archaeology

Physics Methods in Art and Archaeology Physics Methods i Art ad Archaeology Michael Wiescher PHYS 78 Archaeologist i the 90ties Somewhere i South America 80 years later --- i the Valley of the Kigs, gypt Physics Tools & Techology Dager & Adveture

More information

Experimental and theoretical problems:

Experimental and theoretical problems: Workshop o Nuclear Physics, Beijig, September 211 2 t p 6 He 5 H Experimetal ad theoretical problems: We ca ot rely o the theory predictios Reactio mechaism affects the shape of the spectra The overlappig

More information

The power of analytical spectroscopy

The power of analytical spectroscopy The power of aalytical spectroscopy Daiila et al. J. Rama Spectr. 33, 807 (00) Reflected light Red lake varish UV light Rama spectrum Lead white ciabar Caput mortuum Byzatie Ico (AD Our 534), Lady, Our

More information

Physics Oct Reading

Physics Oct Reading Physics 301 21-Oct-2002 17-1 Readig Fiish K&K chapter 7 ad start o chapter 8. Also, I m passig out several Physics Today articles. The first is by Graham P. Collis, August, 1995, vol. 48, o. 8, p. 17,

More information

Primer: Nuclear reactions in Stellar Burning

Primer: Nuclear reactions in Stellar Burning Primer: Nuclear reactions in Stellar Burning Michael Wiescher University of Notre Dame The difficulty with low temperature reaction rates CNO reactions in massive main sequence stars He burning reactions

More information

Helium Production in Big Bang 10 Nov. Objectives

Helium Production in Big Bang 10 Nov. Objectives Helium Productio i Big Bag 10 Nov Homework 8 is o agel. Due oo o Mo, 15 Nov. Homework 9 will be due Fri, 19 Nov at start of class. No late aers. Covered o Test 3 (22 Nov). Log assigmet. Start early. He

More information

Resonance self-shielding in the epi-thermal region

Resonance self-shielding in the epi-thermal region Resoace self-shieldig i the epi-thermal regio Workshop o Nuclear Data for Activatio Aalysis Trieste, Italy, 7 18 March 005 P. Schillebeeckx, K. Volev ad M. Moxo peter.schillebeeckx@cec.eu.it EC JRC IRMM,

More information

LIGHT ION REACTION MECHANISM

LIGHT ION REACTION MECHANISM Proceedigs of the 1983 RCNP Iteratioal Symposium o LIGHT ION REACTION MECHANISM 16-20 MAY, 1983 Edited by H. Ogata, T. Kammuri ad I. Katayama RESEARCH CENTER FOR NUCLEAR PHYSICS OSAKA UNIVERSITY IBARAKI,

More information

Recent Results from T2K

Recent Results from T2K Recet Results from T2K Alessadro Bravar o behalf of the T2K Collaboratio TAU 2016 Beijig Sept. 22, 16 The T2K Experimet 11 coutries ~500 members 2 JPARC - accelerator complex NA61 hadroproductio far detector

More information

arxiv: v1 [nucl-th] 26 Jan 2018

arxiv: v1 [nucl-th] 26 Jan 2018 Beyod the eutro-drip lie: two-eutro decay of uboud uclei arxiv:1801.08673v1 [ucl-th] 26 Ja 2018 K. Hagio 1,2 ad H. Sagawa 3,4 1 Departmet of Physics, Tohoku Uiversity, Sedai, 980-8578, Japa 2 Research

More information

Electric dipole moment of nuclei

Electric dipole moment of nuclei Electric dipole momet of uclei I collaboratio with odoka Yamaaka (ithes Group, RIKE) E. Hiyama (RIKE), T. Yamada (Kato Gakui Uiv.), Y. Fuaki (RIKE) 2016/03/02 RIKE Itroductio CP violatio of Stadard model

More information

ABSTRACT 1. INTRODUCTION

ABSTRACT 1. INTRODUCTION Iwamura, Y., T. Itoh, ad M. SakaNo. Nuclear Products ad Their Time Depedece Iduced by Cotiuous Diffusio of Deuterium Through Multi-layer Palladium Cotaiig Low Work Fuctio Material. i 8th Iteratioal Coferece

More information

INT 2006: First stars... Neutrinos & Supernova Nucleosynthesis. With C. Fröhlich G. Martinez-Pinedo F.-K. Thielemann

INT 2006: First stars... Neutrinos & Supernova Nucleosynthesis. With C. Fröhlich G. Martinez-Pinedo F.-K. Thielemann INT 2006: First stars... Neutrios & Superova Nucleosythesis M. Liebedörfer Uiversity of Basel superova as ucleosythesis site emergece of p-rich ejecta ucleosythesis i p-rich ejecta uder the ifluece of

More information

Miscellaneous Notes. Lecture 19, p 1

Miscellaneous Notes. Lecture 19, p 1 Miscellaeous Notes The ed is ear do t get behid. All Excuses must be take to 233 Loomis before oo, Thur, Apr. 25. The PHYS 213 fial exam times are * 8-10 AM, Moday, May 6 * 1:30-3:30 PM, Wed, May 8 The

More information

Di-neutron correlations and pair transfer

Di-neutron correlations and pair transfer Di-eutro correlatios ad pair trasfer M. Matsuo (Niigata U.) with Y. Serizawa (Niigata U.) K. Mizuyama (Jyvaskyla) Based o PRC7 (005) 06436 PRC73 (006) 044309 NPA788 (007) 307c ArXiv:0809.9 Paper i preparatio.

More information

Nuclear Data Needs for. in HFIR. M.T. Pigni and I.C. Gauld. 238Pu Production Targets. Oak Ridge National Laboratory Oak Ridge, TN

Nuclear Data Needs for. in HFIR. M.T. Pigni and I.C. Gauld. 238Pu Production Targets. Oak Ridge National Laboratory Oak Ridge, TN Nuclear Data Needs for Productio Targets i FIR M.T. Pigi ad I.C. Gauld Oak Ridge Natioal aoratory Oak Ridge, TN Nuclear Data Needs ad Capailities for Applicatios awrece Berkley Natioal aoratory 27-29 May

More information

Measurement uncertainty of the sound absorption

Measurement uncertainty of the sound absorption Measuremet ucertaity of the soud absorptio coefficiet Aa Izewska Buildig Research Istitute, Filtrowa Str., 00-6 Warsaw, Polad a.izewska@itb.pl 6887 The stadard ISO/IEC 705:005 o the competece of testig

More information

reactions / Fission Classification of nuclear reactions

reactions / Fission Classification of nuclear reactions Classiicatio o uclear reactios reactios / Fissio Geeralities Liquid-drop picture Chai reactios Mass distributio Fissio barrier Double issio barrier Ater the scissio poit Time scale i issio Neutro-iduced

More information

THERMAL ENERGY REGION

THERMAL ENERGY REGION 245 CM FISSION CROSS SECTION MEASUREMENT IN THE THERMAL ENERGY REGION O. SEROT * CEA-Cadarache, DEN/DER/SPRC/LEPh, at. 230, F-13108 Sait Paul lez Durace, Frace C. WAGEMANS, S. VERMOTE Departmet o Physics

More information

Coherent and incoherent DVCS and π 0 production on 4 He

Coherent and incoherent DVCS and π 0 production on 4 He Coheret ad icoheret DVCS ad π 0 productio o 4 He S. Stepaya (JLAB) Nucleo ad Resoace Structure with Hard Exclusive Processes IPN-ORSAY, May 29 31, 2017 Outlie 2 DVCS ad p 0 productio o spi ad isospi zero

More information

All Excuses must be taken to 233 Loomis before 4:15, Monday, April 30.

All Excuses must be taken to 233 Loomis before 4:15, Monday, April 30. Miscellaeous Notes The ed is ear do t get behid. All Excuses must be take to 233 Loomis before 4:15, Moday, April 30. The PYS 213 fial exam times are * 8-10 AM, Moday, May 7 * 8-10 AM, Tuesday, May 8 ad

More information

The Wave Function and Quantum Reality

The Wave Function and Quantum Reality The Wave Fuctio ad Quatum Reality Sha Gao Uit for History ad Philosophy of Sciece & Cetre for Time, SOPHI Uiversity of Sydey, Sydey, NSW 006, Australia Abstract. We ivestigate the meaig of the wave fuctio

More information

PHYS-3301 Lecture 7. CHAPTER 4 Structure of the Atom. Rutherford Scattering. Sep. 18, 2018

PHYS-3301 Lecture 7. CHAPTER 4 Structure of the Atom. Rutherford Scattering. Sep. 18, 2018 CHAPTER 4 Structure of the Atom PHYS-3301 Lecture 7 4.1 The Atomic Models of Thomso ad Rutherford 4.2 Rutherford Scatterig 4.3 The Classic Atomic Model 4.4 The Bohr Model of the Hydroge Atom 4.5 Successes

More information

CUMULATIVE DAMAGE ESTIMATION USING WAVELET TRANSFORM OF STRUCTURAL RESPONSE

CUMULATIVE DAMAGE ESTIMATION USING WAVELET TRANSFORM OF STRUCTURAL RESPONSE CUMULATIVE DAMAGE ESTIMATION USING WAVELET TRANSFORM OF STRUCTURAL RESPONSE Ryutaro SEGAWA 1, Shizuo YAMAMOTO, Akira SONE 3 Ad Arata MASUDA 4 SUMMARY Durig a strog earthquake, the respose of a structure

More information

Multicomponent-Liquid-Fuel Vaporization with Complex Configuration

Multicomponent-Liquid-Fuel Vaporization with Complex Configuration Multicompoet-Liquid-Fuel Vaporizatio with Complex Cofiguratio William A. Sirigao Guag Wu Uiversity of Califoria, Irvie Major Goals: for multicompoet-liquid-fuel vaporizatio i a geeral geometrical situatio,

More information

Hydrogen (atoms, molecules) in external fields. Static electric and magnetic fields Oscyllating electromagnetic fields

Hydrogen (atoms, molecules) in external fields. Static electric and magnetic fields Oscyllating electromagnetic fields Hydroge (atoms, molecules) i exteral fields Static electric ad magetic fields Oscyllatig electromagetic fields Everythig said up to ow has to be modified more or less strogly if we cosider atoms (ad ios)

More information

NUCLEATION 7.1 INTRODUCTION 7.2 HOMOGENEOUS NUCLEATION Embryos and nuclei CHAPTER 7

NUCLEATION 7.1 INTRODUCTION 7.2 HOMOGENEOUS NUCLEATION Embryos and nuclei CHAPTER 7 CHAPER 7 NUCLEAION 7.1 INRODUCION I this text, we focus our attetio o crystallie solids that form from the melt. he process begis with the creatio of a cluster of atoms of crystallie structure, which may

More information

Frank Laboratory of Neutron Physics, JINR, Dubna, Russia. Institute of Heavy Ion Physics, Peking University, Beijing, P.R. China. 1.

Frank Laboratory of Neutron Physics, JINR, Dubna, Russia. Institute of Heavy Ion Physics, Peking University, Beijing, P.R. China. 1. SYSTEMATICS OF (,α) CROSS SECTIONS FOR 4-6 MeV NEUTRONS G.Khuukhekhuu 1, Yu.M.Gledeov, Guohui Zhag 3, M.V.Sedysheva, J.Mukhsaikha 1, M.Odsure 1 1) Nuclear Research Ceter, Natioal Uiversity of Mogolia,

More information

Towards a high-intensity source of stellar-energy/epithermal neutrons

Towards a high-intensity source of stellar-energy/epithermal neutrons LiLiT@SARAF: expectatios ad limitatios Michael Paul for the LiLiT collaboratio (Hebrew U- Soreq NRC) Towards a high-itesity source of stellar-eergy/epithermal eutros Nuclear astrophysics eed good quality

More information

PHYS-3301 Lecture 5. CHAPTER 3 The Experimental Basis of Quantum. 3.8: Compton Effect. 3.8: Compton Effect. Sep. 11, 2018

PHYS-3301 Lecture 5. CHAPTER 3 The Experimental Basis of Quantum. 3.8: Compton Effect. 3.8: Compton Effect. Sep. 11, 2018 CHAPTER 3 The Experimetal Basis of Quatum PHYS-3301 Lecture 5 Sep. 11, 2018 3.1 Discovery of the X Ray ad the Electro 3.2 Determiatio of Electro Charge 3.3 Lie Spectra 3.4 Quatizatio 3.5 Blackbody Radiatio

More information

Physics 201 Final Exam December

Physics 201 Final Exam December Physics 01 Fial Exam December 14 017 Name (please prit): This test is admiistered uder the rules ad regulatios of the hoor system of the College of William & Mary. Sigature: Fial score: Problem 1 (5 poits)

More information

REAL-TIME MONITORING OF POWER AND NEUTRON CAPTURE CROSS SECTION IN NUCLEAR RESEARCH REACTOR

REAL-TIME MONITORING OF POWER AND NEUTRON CAPTURE CROSS SECTION IN NUCLEAR RESEARCH REACTOR D5 REAL-TIME MONITORING OF POWER AND NEUTRON CAPTURE CROSS SECTION IN NUCLEAR RESEARCH REACTOR D.A.P. PALMA Brazilia Nuclear Eergy Commissio (CNEN), Rio de Jaeiro, Brazil A.Z. MESQUITA, R.M.G.P. SOUZA

More information

Rate Analysis or a Possible Interpretation of Abundances

Rate Analysis or a Possible Interpretation of Abundances Rate Aalysis or a Possible Iterpretatio of Abudaces Berze High School/Gyögyösi Berze agy Jáos Gimázium H-00 Gyögyös, Kossuth u.., Hugary E-mail: kiss-m@chello.hu Heavy elemets are formed i ucleosythesis

More information

Review Sheet for Final Exam

Review Sheet for Final Exam Sheet for ial To study for the exam, we suggest you look through the past review sheets, exams ad homework assigmets, ad idetify the topics that you most eed to work o. To help with this, the table give

More information

Principle Of Superposition

Principle Of Superposition ecture 5: PREIMINRY CONCEP O RUCUR NYI Priciple Of uperpositio Mathematically, the priciple of superpositio is stated as ( a ) G( a ) G( ) G a a or for a liear structural system, the respose at a give

More information

Lecture-04 Big-Bang Nucleosysthesis

Lecture-04 Big-Bang Nucleosysthesis Lecture-04 Big-Bag Nucleosysthesis Pig He ITP.CAS.CN 2006.03.04 http://power.itp.ac.c/~hep/cosmology.htm 1 Basic Ideas of Nucleosythesis H, He, Li, Light-elemets are produced by big-bag ucleosysthesis

More information

A Brief Introduction to the Physical Basis for Electron Spin Resonance

A Brief Introduction to the Physical Basis for Electron Spin Resonance A Brief Itroductio to the Physical Basis for Electro Spi Resoace I ESR measuremets, the sample uder study is exposed to a large slowly varyig magetic field ad a microwave frequecy magetic field orieted

More information

Universal physics of two neutrons with one flavored meson

Universal physics of two neutrons with one flavored meson Uiversal physics of two eutros with oe flavored meso U. Raha a, Y. Kamiya b, S.-I. Ado c, T. Hyodo b a IIT Guwahati, Idia, b YITP, Kyoto Uiv. c Sumoo Uiv., Korea 2017, Mar 13th 1 Cotets Cotets Itroductio

More information

True Nature of Potential Energy of a Hydrogen Atom

True Nature of Potential Energy of a Hydrogen Atom True Nature of Potetial Eergy of a Hydroge Atom Koshu Suto Key words: Bohr Radius, Potetial Eergy, Rest Mass Eergy, Classical Electro Radius PACS codes: 365Sq, 365-w, 33+p Abstract I cosiderig the potetial

More information

Kinetics of Complex Reactions

Kinetics of Complex Reactions Kietics of Complex Reactios by Flick Colema Departmet of Chemistry Wellesley College Wellesley MA 28 wcolema@wellesley.edu Copyright Flick Colema 996. All rights reserved. You are welcome to use this documet

More information

ANALYSIS OF EXPERIMENTAL ERRORS

ANALYSIS OF EXPERIMENTAL ERRORS ANALYSIS OF EXPERIMENTAL ERRORS All physical measuremets ecoutered i the verificatio of physics theories ad cocepts are subject to ucertaities that deped o the measurig istrumets used ad the coditios uder

More information

Why? The atomic nucleus. Radioactivity. Nuclear radiations. The electrons and the nucleus. Length scale of the nature

Why? The atomic nucleus. Radioactivity. Nuclear radiations. The electrons and the nucleus. Length scale of the nature The atomic ucleus. Radioactivity. Nuclear radiatios László Smeller Why? Medical alicatios of the uclear radiatio: - Nuclear imagig - Radiotheray Legth scale of the ature m meter me -3 millimeter size of

More information

Name Solutions to Test 2 October 14, 2015

Name Solutions to Test 2 October 14, 2015 Name Solutios to Test October 4, 05 This test cosists of three parts. Please ote that i parts II ad III, you ca skip oe questio of those offered. The equatios below may be helpful with some problems. Costats

More information

13 Synthesis of heavier elements. introduc)on to Astrophysics, C. Bertulani, Texas A&M-Commerce 1

13 Synthesis of heavier elements. introduc)on to Astrophysics, C. Bertulani, Texas A&M-Commerce 1 13 Synthesis of heavier elements introduc)on to Astrophysics, C. Bertulani, Texas A&M-Commerce 1 The triple α Reaction When hydrogen fusion ends, the core of a star collapses and the temperature can reach

More information

Probability, Expectation Value and Uncertainty

Probability, Expectation Value and Uncertainty Chapter 1 Probability, Expectatio Value ad Ucertaity We have see that the physically observable properties of a quatum system are represeted by Hermitea operators (also referred to as observables ) such

More information

a b c d e f g h Supplementary Information

a b c d e f g h Supplementary Information Supplemetary Iformatio a b c d e f g h Supplemetary Figure S STM images show that Dark patters are frequetly preset ad ted to accumulate. (a) mv, pa, m ; (b) mv, pa, m ; (c) mv, pa, m ; (d) mv, pa, m ;

More information

Solids - types. correlates with bonding energy

Solids - types. correlates with bonding energy Solids - types MOLCULAR. Set of sigle atoms or molecules boud to adjacet due to weak electric force betwee eutral objects (va der Waals). Stregth depeds o electric dipole momet No free electros poor coductors

More information

ON INTRINSIC LOCALIZED MODES, BREATHERS AND QUODONS. Helsinki, Accelerator Laboratory, Friday, June 12, 2015.

ON INTRINSIC LOCALIZED MODES, BREATHERS AND QUODONS. Helsinki, Accelerator Laboratory, Friday, June 12, 2015. ON INTRINSIC LOCALIZED MODES, BREATHERS AND QUODONS What are they? Why do they exist? Where do they exist? Do they exist i crystals? ILMs i germaium? Quodos i mica muscovite? Jua FR Archilla Uiversidad

More information

I. Motivation. II. ACCULINNA separator

I. Motivation. II. ACCULINNA separator Neutro detectio array based o stilbee scitillators. Grzegorz Kamiski Flerov Laboratory of Nuclear Reactios FLNR JINR, theme 03-5-1094-2010/2014, 6 I. Motivatio Neutro detectors are used extesively at almost

More information

Chapter 5 Vibrational Motion

Chapter 5 Vibrational Motion Fall 4 Chapter 5 Vibratioal Motio... 65 Potetial Eergy Surfaces, Rotatios ad Vibratios... 65 Harmoic Oscillator... 67 Geeral Solutio for H.O.: Operator Techique... 68 Vibratioal Selectio Rules... 7 Polyatomic

More information

Topic 18: Composite Hypotheses

Topic 18: Composite Hypotheses Toc 18: November, 211 Simple hypotheses limit us to a decisio betwee oe of two possible states of ature. This limitatio does ot allow us, uder the procedures of hypothesis testig to address the basic questio:

More information

Accuracy of TEXTOR He-beam diagnostics

Accuracy of TEXTOR He-beam diagnostics Accuracy of TEXTOR He-beam diagostics O. Schmitz, I.L.Beigma *, L.A. Vaishtei *, A. Pospieszczyk, B. Schweer, M. Krychoviak, U. Samm ad the TEXTOR team Forschugszetrum Jülich,, Jülich, Germay *Lebedev

More information

Evaluation of Natural Radioactivity Levels for Structural Material Used in the Construction of the Neutrino Detector

Evaluation of Natural Radioactivity Levels for Structural Material Used in the Construction of the Neutrino Detector World Joural of Nuclear Sciece ad Techology, 215, 5, 43-56 Published Olie Jauary 215 i SciRes. http://www.scirp.org/joural/wjst http://dx.doi.org/1.4236/wjst.215.515 Evaluatio of Natural Radioactivity

More information

1. Hydrogen Atom: 3p State

1. Hydrogen Atom: 3p State 7633A QUANTUM MECHANICS I - solutio set - autum. Hydroge Atom: 3p State Let us assume that a hydroge atom is i a 3p state. Show that the radial part of its wave fuctio is r u 3(r) = 4 8 6 e r 3 r(6 r).

More information

LINEAR REGRESSION ANALYSIS. MODULE IX Lecture Multicollinearity

LINEAR REGRESSION ANALYSIS. MODULE IX Lecture Multicollinearity LINEAR REGRESSION ANALYSIS MODULE IX Lecture - 9 Multicolliearity Dr Shalabh Departmet of Mathematics ad Statistics Idia Istitute of Techology Kapur Multicolliearity diagostics A importat questio that

More information

Propagation of Cathode-Directed Streamer Discharges in Air

Propagation of Cathode-Directed Streamer Discharges in Air Propagatio of Cathode-Directed Streamer Discharges i Air Yuriy Serdyuk Associate Professor High Voltage Egieerig Chalmers Uiversity of Techology SE-41296 Gotheburg, Swede E-mail: yuriy.serdyuk@chalmers.se

More information

FACULTY OF MATHEMATICAL STUDIES MATHEMATICS FOR PART I ENGINEERING. Lectures

FACULTY OF MATHEMATICAL STUDIES MATHEMATICS FOR PART I ENGINEERING. Lectures FACULTY OF MATHEMATICAL STUDIES MATHEMATICS FOR PART I ENGINEERING Lectures MODULE 5 STATISTICS II. Mea ad stadard error of sample data. Biomial distributio. Normal distributio 4. Samplig 5. Cofidece itervals

More information

C(p, ) 13 N. Nuclear reactions generate energy create new isotopes and elements. Notation for stellar rates: p 12

C(p, ) 13 N. Nuclear reactions generate energy create new isotopes and elements. Notation for stellar rates: p 12 Iroducio o sellar reacio raes Nuclear reacios geerae eergy creae ew isoopes ad elemes Noaio for sellar raes: p C 3 N C(p,) 3 N The heavier arge ucleus (Lab: arge) he ligher icomig projecile (Lab: beam)

More information

Outlook. Motivation How to overcome experimental difficulties for Actinides σ(n,γ) ( 3 He,pγ) as a surrogate :

Outlook. Motivation How to overcome experimental difficulties for Actinides σ(n,γ) ( 3 He,pγ) as a surrogate : M. iche G. Boutoux B. urado G. Barreau N. Capella I. Compais S. Czajkowski D. Dassie B. Haas L. Mathieu. Bauge 2.M. Daugas 2 T. Faul 2 L. Gaudefroy 2 V. Meot 2 P. Morel 2 N. Pillet 2 O. Roig 2. Taieb 2

More information

Lecture XX: The equation of state of dense matter

Lecture XX: The equation of state of dense matter Lecture XX: The equatio of state of dese matter Christopher M. Hirata Caltech M/C 350-17, Pasadea CA 91125, USA (Dated: Jauary 20, 2012) I. OVERVIEW Thus far we have ivestigated the relativistic equatios

More information

Mechatronics. Time Response & Frequency Response 2 nd -Order Dynamic System 2-Pole, Low-Pass, Active Filter

Mechatronics. Time Response & Frequency Response 2 nd -Order Dynamic System 2-Pole, Low-Pass, Active Filter Time Respose & Frequecy Respose d -Order Dyamic System -Pole, Low-Pass, Active Filter R 4 R 7 C 5 e i R 1 C R 3 - + R 6 - + e out Assigmet: Perform a Complete Dyamic System Ivestigatio of the Two-Pole,

More information

Limitation of Applicability of Einstein s. Energy-Momentum Relationship

Limitation of Applicability of Einstein s. Energy-Momentum Relationship Limitatio of Applicability of Eistei s Eergy-Mometum Relatioship Koshu Suto Koshu_suto19@mbr.ifty.com Abstract Whe a particle moves through macroscopic space, for a isolated system, as its velocity icreases,

More information

5.76 Lecture #33 5/08/91 Page 1 of 10 pages. Lecture #33: Vibronic Coupling

5.76 Lecture #33 5/08/91 Page 1 of 10 pages. Lecture #33: Vibronic Coupling 5.76 Lecture #33 5/8/9 Page of pages Lecture #33: Vibroic Couplig Last time: H CO A A X A Electroically forbidde if A -state is plaar vibroically allowed to alterate v if A -state is plaar iertial defect

More information

NEUTRON FLUX MEASUREMENT UTILIZING CAMPBELL TECHNIQUE

NEUTRON FLUX MEASUREMENT UTILIZING CAMPBELL TECHNIQUE Iteratioal Coferece Nuclear Eergy i Cetral Europe 000 Golf Hotel, Bled, Sloveia, September 11-14, 000 NEUTRON FLUX MEASUREMENT UTILIZING CAMPBELL TECHNIQUE Marti Kropík Departmet of Nuclear Reactors Faculty

More information

PHYS-3301 Lecture 9. CHAPTER 5 Wave Properties of Matter and Quantum Mechanics I. 5.3: Electron Scattering. Bohr s Quantization Condition

PHYS-3301 Lecture 9. CHAPTER 5 Wave Properties of Matter and Quantum Mechanics I. 5.3: Electron Scattering. Bohr s Quantization Condition CHAPTER 5 Wave Properties of Matter ad Quatum Mecaics I PHYS-3301 Lecture 9 Sep. 5, 018 5.1 X-Ray Scatterig 5. De Broglie Waves 5.3 Electro Scatterig 5.4 Wave Motio 5.5 Waves or Particles? 5.6 Ucertaity

More information

Response Variable denoted by y it is the variable that is to be predicted measure of the outcome of an experiment also called the dependent variable

Response Variable denoted by y it is the variable that is to be predicted measure of the outcome of an experiment also called the dependent variable Statistics Chapter 4 Correlatio ad Regressio If we have two (or more) variables we are usually iterested i the relatioship betwee the variables. Associatio betwee Variables Two variables are associated

More information

Unusual statistics of interference effects in neutron scattering from compound nuclei

Unusual statistics of interference effects in neutron scattering from compound nuclei PHYSICAL REVIEW C, VOLUME 6, 46 Uusual statistics of iterferece effects i eutro scatterig from compoud uclei J. C. Beregut, V. V. Flambaum, ad G. F. Gribaki* School of Physics, Uiversity of New South Wales,

More information

Final Exam. Curve of the Binding Energy. Natural radioactivity

Final Exam. Curve of the Binding Energy. Natural radioactivity Fial Exam Wed 3/17 from 3:00pm-5:59 York 2622 Will cover all the course material icludig the last week 25 questios multiple choice. You are allowed to brig 2 sheets of paper with equatios o both sides.

More information

Introduction to Astrophysics Tutorial 2: Polytropic Models

Introduction to Astrophysics Tutorial 2: Polytropic Models Itroductio to Astrophysics Tutorial : Polytropic Models Iair Arcavi 1 Summary of the Equatios of Stellar Structure We have arrived at a set of dieretial equatios which ca be used to describe the structure

More information

Observations of Large Scale Sidereal Anisotropy in 1 and 11 TeV Cosmic Rays from the MINOS Experiment

Observations of Large Scale Sidereal Anisotropy in 1 and 11 TeV Cosmic Rays from the MINOS Experiment Observatios of Large Scale Sidereal Aisotropy i 1 ad 11 ev Cosmic Rays from the MINOS Experimet Jeffrey de Jog Oxford Uiversity For the MINOS Collaboratio August 12 th,2011 32 d ICRC Beijig, Chia Presetatio

More information

Total number of nucleons: mass number 238 Number of protons: atomic number 92U

Total number of nucleons: mass number 238 Number of protons: atomic number 92U 9 The Nucleus Protos Neutros Nucleos Total umber of ucleos: mass umber 8 Number of protos: atomic umber 9U Isotopes: idetical atomic umbers differet mass umbers same chemical properties differet uclear

More information

5. Quantum Nature of the Nano-world ( Fundamental of. Quantum mechanics)

5. Quantum Nature of the Nano-world ( Fundamental of. Quantum mechanics) 5. Quatu Nature of the Nao-world Fudaetal of What is the defiitio of aoaterials?? Quatu echaics i Origial: quatu size effect where the electroic properties of solids are altered with great reductios i

More information

Jaynes-Cummings Model

Jaynes-Cummings Model Jayes-Cummigs Model The JC model plays a importat role i atom-field iteractio. It is a fully quatized model ad yet aalytically solvable. It describes the iteractio betwee a two-level atom ad a quatized

More information

5.61 Fall 2013 Problem Set #3

5.61 Fall 2013 Problem Set #3 5.61 Fall 013 Problem Set #3 1. A. McQuarrie, page 10, #3-3. B. McQuarrie, page 10, #3-4. C. McQuarrie, page 18, #4-11.. McQuarrie, pages 11-1, #3-11. 3. A. McQuarrie, page 13, #3-17. B. McQuarrie, page

More information

Free Radical Polymerization

Free Radical Polymerization Free Radical Polymerizatio Referece: Aspe Polymers: Uit Operatios ad Reactio Models, Aspe Techology, Ic., 2013. 1. Itroductio The free-radical bulk/solutio polymerizatio model is applicable to bulk ad

More information

Filter banks. Separately, the lowpass and highpass filters are not invertible. removes the highest frequency 1/ 2and

Filter banks. Separately, the lowpass and highpass filters are not invertible. removes the highest frequency 1/ 2and Filter bas Separately, the lowpass ad highpass filters are ot ivertible T removes the highest frequecy / ad removes the lowest frequecy Together these filters separate the sigal ito low-frequecy ad high-frequecy

More information

CEE 522 Autumn Uncertainty Concepts for Geotechnical Engineering

CEE 522 Autumn Uncertainty Concepts for Geotechnical Engineering CEE 5 Autum 005 Ucertaity Cocepts for Geotechical Egieerig Basic Termiology Set A set is a collectio of (mutually exclusive) objects or evets. The sample space is the (collectively exhaustive) collectio

More information

2 1. The r.s., of size n2, from population 2 will be. 2 and 2. 2) The two populations are independent. This implies that all of the n1 n2

2 1. The r.s., of size n2, from population 2 will be. 2 and 2. 2) The two populations are independent. This implies that all of the n1 n2 Chapter 8 Comparig Two Treatmets Iferece about Two Populatio Meas We wat to compare the meas of two populatios to see whether they differ. There are two situatios to cosider, as show i the followig examples:

More information

Office: JILA A709; Phone ;

Office: JILA A709; Phone ; Office: JILA A709; Phoe 303-49-7841; email: weberjm@jila.colorado.edu Problem Set 5 To be retured before the ed of class o Wedesday, September 3, 015 (give to me i perso or slide uder office door). 1.

More information

Recent Experimental Results in ADITYA Tokamak

Recent Experimental Results in ADITYA Tokamak Recet Experimetal Results i ADITYA Tokamak R. Jha ad the ADITYA Team Istitute for Plasma Research, Bhat, Gadhiagar-382 428, INDIA e-mail:rjha@ipr.res.i Abstract. Recet studies o measuremets of edge turbulece

More information

Each copy of any part of a JSTOR transmission must contain the same copyright notice that appears on the screen or printed page of such transmission.

Each copy of any part of a JSTOR transmission must contain the same copyright notice that appears on the screen or printed page of such transmission. Quatum Iterferece i the Cotrol of Molecular Processes Author(s): P. Brumer ad M. Shapiro Source: Philosophical Trasactios: Mathematical, Physical ad Egieerig Scieces, Vol. 355, No. 1733, Highlights i Quatum

More information

11TH INTERNATIONAL SYMPOSIUM ON PARTICLE IMAGE VELOCIMETRY - PIV15 Santa Barbara, California, Sept , 2015

11TH INTERNATIONAL SYMPOSIUM ON PARTICLE IMAGE VELOCIMETRY - PIV15 Santa Barbara, California, Sept , 2015 11TH INTERNATIONAL SYMPOSIUM ON PARTICLE IMAGE VELOCIMETRY - PIV15 Sata Barbara, Califoria, Sept. 14-16, 2015 ABSTRACT HELE-SHAW RHEOMETRY BY MEANS OF PARTICLE IMAGE VELOCIMETRY Sita Drost & Jerry Westerweel

More information

Simona Malace University of South Carolina

Simona Malace University of South Carolina Simoa Malace Uiversity of South Carolia i collaboratio with Y. Kah, W. Melitchouk, S.A. Kulagi, C. Keppel MENU010, May 31 Jue 4, 010 Williamsburg, VA Outlie New metho : etract from uclear Applicatio of

More information

Material Balances on Reactive Processes F&R

Material Balances on Reactive Processes F&R Material Balaces o Reactive Processes F&R 4.6-4.8 What does a reactio do to the geeral balace equatio? Accumulatio = I Out + Geeratio Cosumptio For a reactive process at steady-state, the geeral balace

More information

Comprehensive Bridge Health Evaluation Method Based on Information Fusion

Comprehensive Bridge Health Evaluation Method Based on Information Fusion MATEC Web of Cofereces 82, 03003 (2016) DOI: 10.1051/ mateccof/20168203003 Comprehesive Bridge Health Evaluatio Method Based o Iformatio Fusio Li-pig Li 1,a, We-xia Dig 2 ad Xiao-li Lu 3 1 Faculty of Egieerig,

More information

The improvement of the volume ratio measurement method in static expansion vacuum system

The improvement of the volume ratio measurement method in static expansion vacuum system Available olie at www.sciecedirect.com Physics Procedia 32 (22 ) 492 497 8 th Iteratioal Vacuum Cogress The improvemet of the volume ratio measuremet method i static expasio vacuum system Yu Hogya*, Wag

More information

Atomic Physics 4. Name: Date: 1. The de Broglie wavelength associated with a car moving with a speed of 20 m s 1 is of the order of. A m.

Atomic Physics 4. Name: Date: 1. The de Broglie wavelength associated with a car moving with a speed of 20 m s 1 is of the order of. A m. Name: Date: Atomic Pysics 4 1. Te de Broglie wavelegt associated wit a car movig wit a speed of 0 m s 1 is of te order of A. 10 38 m. B. 10 4 m. C. 10 4 m. D. 10 38 m.. Te diagram below sows tree eergy

More information

Why? The atomic nucleus. Radioactivity. Nuclear radiations. Length scale of the nature. The electrons and the nucleus

Why? The atomic nucleus. Radioactivity. Nuclear radiations. Length scale of the nature. The electrons and the nucleus The atomic ucleus. Radioactivity. Nuclear radiatios László Smeller Why? Medical alicatio of uclear radiatio: Nuclear imagig Radiotheray Legth scale of the ature m meter me -3 millimeter size of letters

More information

All Excuses must be taken to 233 Loomis before 4:15, Monday, April 30.

All Excuses must be taken to 233 Loomis before 4:15, Monday, April 30. Miscellaeous Notes The ed is ear do t get behid. All Excuses must be take to 233 Loomis before 4:15, Moday, April 30. The PHYS 213 fial exam times are * 8-10 AM, Moday, May 7 * 8-10 AM, Tuesday, May 8

More information

Strangeness in nuclei and matter: the importance of three-body forces

Strangeness in nuclei and matter: the importance of three-body forces Strageess i uclei ad matter: the importace of three-body forces Diego Loardoi I collaboratio with: Alessadro Lovato, AL Stefao Gadolfi, LAL Fracesco Pederiva, UiT Fracesco Catalao, UiT ECT*, Villazzao

More information

Nuclear Level Density Calculation of Astrophysical Reactions

Nuclear Level Density Calculation of Astrophysical Reactions IOSR Joural of pplied Pysics (IOSR-JP) e-issn: 2278-4861.Volume 8, Issue 4 Ver. I (Jul. - ug. 2016), PP 43-52 www.iosrjourals.org Nuclear Leel Desity Calculatio of stropysical Reactios med. Selma 1, Hamsa

More information

Radiative Lifetimes of Rydberg States in Neutral Gallium

Radiative Lifetimes of Rydberg States in Neutral Gallium Vol. 115 (2009) ACTA PHYSICA POLONICA A No. 3 Radiative Lifetimes of Rydberg States i Neutral Gallium M. Yildiz, G. Çelik ad H.Ş. Kiliç Departmet of Physics, Faculty of Arts ad Sciece, Selçuk Uiversity,

More information

Time-Domain Representations of LTI Systems

Time-Domain Representations of LTI Systems 2.1 Itroductio Objectives: 1. Impulse resposes of LTI systems 2. Liear costat-coefficiets differetial or differece equatios of LTI systems 3. Bloc diagram represetatios of LTI systems 4. State-variable

More information

Modification of Arrhenius Model for Numerical Modelling of Turbulent Flames

Modification of Arrhenius Model for Numerical Modelling of Turbulent Flames J. Basic. Appl. Sci. Res., (5)480-486, 01 01, TextRoad Publicatio ISSN 090-4304 Joural of Basic ad Applied Scietific Research www.textroad.com Modificatio of Arrheius Model for Numerical Modellig of Turbulet

More information

Numerical Methods for Ordinary Differential Equations

Numerical Methods for Ordinary Differential Equations Numerical Methods for Ordiary Differetial Equatios Braislav K. Nikolić Departmet of Physics ad Astroomy, Uiversity of Delaware, U.S.A. PHYS 460/660: Computatioal Methods of Physics http://www.physics.udel.edu/~bikolic/teachig/phys660/phys660.html

More information

Nernst Equation. Nernst Equation. Electric Work and Gibb's Free Energy. Skills to develop. Electric Work. Gibb's Free Energy

Nernst Equation. Nernst Equation. Electric Work and Gibb's Free Energy. Skills to develop. Electric Work. Gibb's Free Energy Nerst Equatio Skills to develop Eplai ad distiguish the cell potetial ad stadard cell potetial. Calculate cell potetials from kow coditios (Nerst Equatio). Calculate the equilibrium costat from cell potetials.

More information

Manifestation of Multiparton Dynamics in Dense Nuclear Matter

Manifestation of Multiparton Dynamics in Dense Nuclear Matter D+Au ad Au+Au Reactios at RHIC: Maifestatio of Multiparto Dyamics i Dese Nuclear Matter Iva Vitev Iowa State Uiversity, Ames, IA 50011 INT First Three Years at RHIC Jue 09, 003 Istitute for Nuclear Theory,

More information