Proposal for a Topical Collaboration in Nuclear Theory for The
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Leptogenesis in Realistic SO(10) Models
Physics Letters B 651 (2007) 195–207 www.elsevier.com/locate/physletb Leptogenesis in realistic SO(10) models Xiangdong Ji a,b, Yingchuan Li a,∗, R.N. Mohapatra a,S.Nasria,YueZhangb a Department of Physics, University of Maryland, College Park, MD 20742, USA b Institute for Theoretical Physics, Peking University, Beijing, China Received 16 May 2007; received in revised form 4 June 2007; accepted 10 June 2007 Available online 13 June 2007 Editor: T. Yanagida Abstract We study the origin of baryonic matter via leptogenesis in realistic SO(10) models, in particular, in a new lopsided mass matrix model introduced recently by three of the authors. It is shown that the model generates sufficient baryon asymmetry in addition to fitting to fermion masses and mixing. We compare this result with other realistic SO(10) models. © 2007 Elsevier B.V. All rights reserved. 1. Introduction One of the most fundamental questions in modern cosmology is where the baryon number asymmetry in today’s Universe comes from. It is an attractive idea to assume that it arises dynamically in a symmetric big-bang model through C and CP violating processes out of thermal equilibrium. Of the several proposals that use this scenario, leptogenesis [1] has emerged as one of the most interesting scenarios for baryon generation. Here the baryon number is produced through the so-called sphaleron processes from a residual lepton number density left over from an early stage of the universe through lepton number violating decays of right-handed neutrinos. Such connection is extremely interesting since the same heavy right-handed neutrinos are also important ingredients for understanding the small left-handed neutrino masses through the so-called see-saw mechanism [2]. -
Topics in Heavy Particle Effective Theories
Topics in Heavy Particle Effective Theories Thesis by Matthew P. Dorsten In Partial Fulfillment of the Requirements for the Degree of Doctor of Philosophy California Institute of Technology Pasadena, California 2006 (Defended May 25, 2006) ii c 2006 Matthew P. Dorsten All Rights Reserved iii Acknowledgments Many thanks to my advisor, Mark Wise, for his guidance, physics-related and otherwise. I would also like to thank my collaborators on the physics projects described here: Christian Bauer, Sean Fleming, Sonny Mantry, Mike Salem, and Iain Stewart. I acknowledge the support of a Graduate Research Fellowship from the National Science Foundation and the Department of Energy under Grant No. DE-FG03-92ER40701. Above all I must thank Rebecca, who helped me get through the whole thing. iv Abstract This thesis gives several applications of effective field theory to processes involving heavy particles. The first is a standard application of heavy quark effective theory to exclusive B decays. It involves two new sum rules discovered by Le Yaouanc et al. by applying the operator product expansion to the nonforward matrix element of a time-ordered product of b c currents. They lead to the constraints σ2 > 5ρ2/4 and σ2 > 3(ρ2)2/5 + 4ρ2/5 → on the curvature of the B¯ D(∗) Isgur-Wise function, both of which imply the absolute → lower bound σ2 > 15/16 when combined with the Uraltsev bound ρ2 > 3/4 on the slope. This thesis calculates order αs corrections to these bounds, increasing the accuracy of the resultant constraints on the physical form factors. The second application involves matching SCETI onto SCETII at one loop. -
Bamboomc--A Geant4-Based Simulation Program for the Pandax Experiments
Prepared for submission to JINST BambooMC – A Geant4-based simulation program for the PandaX experiments Xun Chen 0,1,1 Chen Cheng2 Mengting Fu3 Franco Giuliani0 Jianglai Liu 0,1,4,2 Xiaoying Lu 5 Xiangdong Ji 6,3 Zhicheng Qian0 Hao Qiao3 Qiuhong Wangℎ Jingkai Xia0 Pengwei Xie0 Yukun Yao0 Hongguang Zhang0 0INPAC and School of Physics and Astronomy, Shanghai Jiao Tong University, MOE Key Lab for Particle Physics, Astrophysics and Cosmology, Shanghai Key Laboratory for Particle Physics and Cosmology, Shanghai 200240, China 1Shanghai Jiao Tong University Sichuan Research Institute, Chengdu 610213, China 2School of Physics, Sun Yat-Sen University, Guangzhou 510275, China 3School of Physics, Peking University, Beijing 100871, China 4Tsung-Dao Lee Institute, Shanghai 200240, China 5 School of Physics and Key Laboratory of Particle Physics and Particle Irradiation (MOE), Shandong University, Jinan 250100, China 6Department of Physics, University of Maryland, College Park, Maryland 20742, USA ℎKey Laboratory of Nuclear Physics and Ion-beam Application (MOE), Institute of Modern Physics, Fudan University, Shanghai 200433, China E-mail: [email protected] Abstract: The purpose of the PandaX experiments is to search for the possible events resulted from dark matter particles, neutrinoless double beta decay or other rare processes with xenon detectors. Understanding the energy depositions from backgrounds or calibration sources in these detectors is very important. The program of BambooMC is created to perform the Geant4-based Monte Carlo simulation, providing reference information for the experiments. We introduce the design and features of BambooMC in this report. The running of the program depends on a configuration file, which combines different detectors, event generators, physics lists and analysis packs together in one simulation. -
SU(3) Chiral Symmetry in Non-Relativistic Field Theory
SU Chiral Symmetry in NonRelativistic Field Theory Thesis by Stephen M Ouellette In Partial Fulllment of the Requirements for the Degree of Do ctor of Philosophy I T U T E O T F S N T I E C A I H N N R O O 1891 L F O I L G A Y C California Institute of Technology Pasadena California Submitted January ii Acknowledgements I recognize three groups of p eople to whom I owe a particular debt of gratitude for the ability to nish the work of this thesis First and foremost are my partnerinlife Heather Frase my parents and my siblings Their unconditional love supp ort and pa tience have b een the glue which holds myworld together Also I wanttoacknowledge my mentors Mark WiseRyoichi Seki and Ubira jara van Kolck and my former ocemate Iain Stewart for the encouragementandvaluable insights they oered during our discus sions To those four p eople I oweeverything that I know ab out the practice of scientic inquiry Finally I want to thank the p eople of the Caltech Theoretical High Energy Physics group and a host of other characters Adam Leib ovich Erik Daniel Torrey Lyons for making my exp erience at Caltechenjoyable as well as educational iii Abstract Applications imp osing SU chiral symmetry on nonrelativistic eld theories are con sidered The rst example is a calculation of the selfenergy shifts of the spin decuplet baryons in nuclear matter from the chiral eective Lagrangian coupling o ctet and de cuplet baryon elds Sp ecial attention is paid to the selfenergy of the baryon near the saturation densityofnuclear matter We nd contributions -
Model-Independent Approaches to QCD and B Decays Christian Arnesen
Model-Independent Approaches to QCD and B Decays by Christian Arnesen Submitted to the Department of Physics in partial fulfillment of the requirements for the degree of Doctorate of Philosophy at the MASSACHUSETTS INSTITUTE OF TECHNOLOGY May 2007 @ Christian Arnesen, MMVII. All rights reserved. The author hereby grants to MIT permission to reproduce and distribute publicly paper and electronic copies of this thesis document in whole or in part. A uthor ......... .. .................. Department of Physics May 30, 2007 Certified by.......... Iain W. Stewart Assistant Professor Thesis Supervisor Accepted by ........... whomaa eytak MASSACHLSEMI TMiTUTE• OF TECHNOLOGBY Associate Department Head foY Education OCT 0 9 2008 LIBRARIES ARCHIVES Model-Independent Approaches to QCD and B Decays by Christian Arnesen Submitted to the Department of Physics on May 30, 2007, in partial fulfillment of the requirements for the degree of Doctorate of Philosophy Abstract We investigate theoretical expectations for B-meson decay rates in the Standard Model. Strong-interaction effects described by quantum chromodynamics (QCD) make this a challenging endeavor. Exact solutions to QCD are not known, but an arsenal of approximation techniques have been developed. We apply effective field theory methods, in particular the sophisticated machinery of the soft-collinear effec- tive theory (SCET), to B decays with energetic hadrons in the final state. SCET separates perturbative interactions at the scales mb and V/mbAQcD from hadronic physics at AQCD by expanding in ratios of these scales. After a review of SCET, we construct a complete reparametrization-invariant basis for heavy-to-light currents in SCET at next-to-next-to-leading order in the power-counting expansion. -
Factorization at the LHC: from Pdfs to Initial State Jets (Ph. D. Thesis)
Factorization at the LHC: From PDFs to Initial State Jets by Wouter J. Waalewijn Submitted to the Department of Physics in partial fulfillment of the requirements for the degree of Doctor of Philosophy in Physics at the MASSACHUSETTS INSTITUTE OF TECHNOLOGY June 2010 c Massachusetts Institute of Technology 2010. All rights reserved. Author............................................................................ Department of Physics May 12, 2010 Certified by........................................................................ Iain W. Stewart Associate Professor Thesis Supervisor arXiv:1104.5164v1 [hep-ph] 27 Apr 2011 Accepted by....................................................................... Krishna Rajagopal Associate Department Head for Education 2 Factorization at the LHC: From PDFs to Initial State Jets by Wouter J. Waalewijn Submitted to the Department of Physics on May 12, 2010, in partial fulfillment of the requirements for the degree of Doctor of Philosophy in Physics Abstract New physics searches at the LHC or Tevatron typically look for a certain number of hard jets, leptons and photons. The constraints on the hadronic final state lead to large logarithms, which need to be summed to obtain reliable theory predictions. These constraints are sensitive to the strong initial-state radiation and resolve the colliding partons inside initial- state jets. We find that the initial state is properly described by \beam functions". We introduce an observable called \beam thrust" τB, which measures the hadronic radiation relative to the beam axis. By requiring τB 1, beam thrust can be used to impose a central jet veto, which is needed to reduce the large background in H WW `ν`ν¯ ! ! from tt¯ W W b¯b. We prove a factorization theorem for \isolated" processes, pp XL ! ! where the hadronic final state X is restricted by τB 1 and L is non-hadronic. -
17. SCET Multipole Expansion the Following Content Is Provided Under a Creative Commons License
MITOCW | 17. SCET Multipole Expansion The following content is provided under a Creative Commons license. Your support will help MIT OpenCourseWare continue to offer high quality educational resources for free. To make a donation or view additional materials from hundreds of MIT courses, visit MIT OpenCourseWare at ocw.mit.edu. IAIN STEWART: All right, so this is where we got to last time. So we were on the road to deriving the leading order SCET Lagrangian. We said that there were some things that we had to deal with, in particular expanding it. And we started out, as a first step, getting rid of two of the components of the field that we said are not going to be ones that we project onto in the high energy limit. And that led us to this Lagrangian right here, but we haven't yet expanded it. We haven't yet separated the ultra soft and collinear momenta or the ultra soft and collinear gauge fields. And so in order to do that, I argued that you have to make multipole expansion. And I talked a little bit about what the multipole expansion would look like in position space. And then I said, it's better for us to do it in momentum space. And we started to do that. And we're going to continue to do that today. So first of all, let's just go to momentum space. So I've called the field here-- since it's not the final field that we want, I introduced a crummy notation for it, Cn hat. -
Publishing Index 20 2
A SUPPLEMENT TO NATURE PUBLISHING INDEX 202 CHINA Based on the Nature Publishing Index nature.asia/publishing-index nature.asia/publishing-index-china 30 May 2013 © 2013 Macmillan Publishers Limited. All rights reserved Ghent , Belgium Sacramento, USA Shenzhen, China June 25 - 28 September 12 -13 October 30 - November 1 The 2nd The 2nd International Conference International Conference th on Genomics in on Genomics in the The 8 International Conference Europe Americas on Genomics Co-organizer : VIB Co-organizer : UC DAVIS Co-organizer : GigaScience Join Us for 2013 International Conference on Genomics Over the past seven years, the International Conference on Genomics (ICG) has been one of the top grade gathering of global thought leaders in genomics featuring latest advancements in genomic-related fields. This year, BGI continues to hold series ICG conferences, including ICG-8, ICG Americas-II, and ICG Eu- rope-II. These gatherings will be an excellent opportunity to exchange your research experience and latest discoveries, as well as the new insights into future development of life science. Scan this QR code to visit www.icg-2013.org for more information! Organizer : [email protected] +86-755-25273340 PUBLISHING INDEX 2012 CHINA A SUPPLEMENT TO NATURE inners and losers. It is in these terms that PUBLISHING INDEX 202 CONTENTS CHINA regular rankings like the Nature Publishing Index (NPI) are often perceived, with the rise Wof one institution, city or country inevitably leading to 2 A LARGER SLICE OF THE PIE the slide of another. A broad look at another year of Yet this might be too simplistic a picture. -
Neutrino Physics with JUNO
Home Search Collections Journals About Contact us My IOPscience Neutrino physics with JUNO This content has been downloaded from IOPscience. Please scroll down to see the full text. 2016 J. Phys. G: Nucl. Part. Phys. 43 030401 (http://iopscience.iop.org/0954-3899/43/3/030401) View the table of contents for this issue, or go to the journal homepage for more Download details: IP Address: 134.107.3.78 This content was downloaded on 23/02/2016 at 13:12 Please note that terms and conditions apply. Journal of Physics G: Nuclear and Particle Physics J. Phys. G: Nucl. Part. Phys. 43 (2016) 030401 (188pp) doi:10.1088/0954-3899/43/3/030401 Technical Report Neutrino physics with JUNO Fengpeng An1, Guangpeng An2,QiAn3, Vito Antonelli4, Eric Baussan5, John Beacom6, Leonid Bezrukov7, Simon Blyth8, Riccardo Brugnera9, Margherita Buizza Avanzini10, Jose Busto11, Anatael Cabrera12, Hao Cai13, Xiao Cai2, Antonio Cammi14,15, Guofu Cao2, Jun Cao2, Yun Chang16, Shaomin Chen17, Shenjian Chen18, Yixue Chen19, Davide Chiesa14,20, Massimiliano Clemenza14,20, Barbara Clerbaux21, Janet Conrad22, Davide D’Angelo4, Hervé De Kerret12, Zhi Deng17, Ziyan Deng2, Yayun Ding2, Zelimir Djurcic23, Damien Dornic11, Marcos Dracos5, Olivier Drapier10, Stefano Dusini24, Stephen Dye25, Timo Enqvist26, Donghua Fan27, Jian Fang2, Laurent Favart21, Richard Ford4, Marianne Göger-Neff28, Haonan Gan29, Alberto Garfagnini9, Marco Giammarchi4, Maxim Gonchar30, Guanghua Gong17, Hui Gong17, Michel Gonin10, Marco Grassi2, Christian Grewing31, Mengyun Guan2, Vic Guarino23, Gang Guo32, Wanlei -
Effective Field Theory Iain Stewart Lecture Notes
Effective Field Theory Iain Stewart Lecture Notes Saner Edwin equalises expectably or urge irrationally when Roarke is unbreathing. Antefixal Davidde aftermarls sisterless some vitality Claire after translates abducted sustainedly. Hymie flammed trickily. Intent Samson cachinnate some quadriplegic Workshop on Effective Field Theory Techniques in Gravitational Wave Physics Carnegie. Introduction To Soft Collinear Effective Theory Lecture Notes. What are talking best online physics courses Quora. Whence the Effectiveness of Effective Field Theories PhilSci. IZ Rothstein and IW Stewart An Effective Field Theory for Forward Scattering and. Feynman Path Integrals Theory and Applications in the Fields of Quantum Mechanics Statistical Mechanics and Quantum Field Theory Lecture notes for the. That gravitational effective field theories can be constrained by infrared. Advanced Quantum Field Theory David Schaich. Kierkegaard Free Online Video Jon B Stewart University of Copenhagen. However not new engineers lack capital necessary skills to effectively find and. The inverse problem in Galois theory effective computation of Galois groups algebraic. Kierkegaard Free Online Video Jon B Stewart University of Copenhagen. Anderson Malcolm Bonjour Filipe Gregory Ruth and Stewart John 1997. Lecture 24 SCET-II Effective Field Theory by Iain Stewart Video. Of the higgs boson and iain stewart has applied effective field theory methods to. Harsh Mathur Physics on the prize in Physics Phoebe Stewart Pharmacology on the prize in. Solutions Manual Galois Theory Stewart Share content Buy Ltd. Freeman John Dyson FRS 15 December 1923 2 February 2020 was a British-American theoretical and mathematical physicist mathematician and statistician known outside his works in quantum field theory. Note that moose are already breaking the EFT rules in comparison FULL THEORY before we. -
Soft-Collinear Effective Field Theory } Thomas Becher Bern University
C1 s } 1 C b Ca } } 2 Soft-Collinear Effective Field Theory } Thomas Becher Bern University CUSOC Graduate2 Course, EPFL, Nov. 2015 Tools for QFT computations Expansion Expansion in in the interaction scale ratios: strength: Effective Field perturbation Theories theory Toy models: Numerical solvable models methods: SUSY theories lattice simulations AdS/CFT Jet physics at the LHC Many scale hierarchies! ps pT M E m ⇤ Jet Jet out proton ⇠ QCD → Soft-Collinear Effective Theory (SCET) Outline of the course • Invitation: perturbative QCD and effective field theory • The method of regions • a simple example • Scalar Sudakov form factor • Introduction to perturbative QCD / introduction to EFT • Scalar SCET • factorization for the scalar Sudakov form factor in d=6 • Generalization to QCD Outline […] • Sudakov form factor in QCD • Resummation by RG evolution • Drell-Yan process near partonic threshold • Factorization for generic Drell-Yan • Factorization constraints on infrared divergences in n-point amplitudes • Factorization and resummation for cone-jet processes (1508.06645 with Neubert, Rothen and Shao). Literature A few selected original references are: Original SCET papers (using the label formalism): • C.W. Bauer, S. Fleming, D. Pirjol and I.W. Stewart, An effective field theory for collinear and soft gluons: Heavy to light decays, PRD 63, 114020 (2001) [hep-ph/0011336] • C.W. Bauer, S. Fleming, D. Pirjol and I.W. Stewart, Soft-Collinear Factorization in Effective Field Theory, PRD 65, 054022 (2002) [hep-ph/0109045] SCET in position space: • M. Beneke, A.P. Chapovsky, M. Diehl and T. Feldmann,``Soft- collinear effective theory and heavy-to-light currents beyond leading power,'' Nucl. -
Effective Field Theory
Effective Field Theory Iain Stewart MIT Nuclear Physics 2007 Long Range Plan Joint Town Meeting on QCD Jan, 2007 Effective Field Theories of QCD ChPT HTL NRQCD cc states pions large T large HDET unstable density particle top quark QCD energetic EFT hadrons SCET jets nuclear SCET single nucleon forces bd states NNEFT Heavy Hadron HQET ChPT Arrows: Effective theories describe infrared limits of QCD m ChPT π 1 π Λ ! talks by D. Kaplan, D. Phillips, p H. Griesshammer 1 Λ ! Effective Field Theories of QCD ChPT HTL NRQCD cc states pions large T large HDET unstable density particle top quark QCD energetic EFT hadrons SCET jets nuclear SCET single nucleon forces bd states NNEFT Heavy Hadron HQET ChPT Arrows: Effective theories describe infrared limits of QCD Q Soft-Collinear Effective hard probes Theory (SCET) Λ 1 • Q ! Effective Field Theories of QCD ChPT HTL NRQCD cc states pions large T large HDET unstable density particle top quark QCD energetic EFT hadrons SCET jets nuclear SCET single nucleon forces bd states NNEFT Heavy Hadron HQET ChPT Lattice QCD a Chiral EFT ’s g L QCD, π Nuclei 1 mπ− q a, L, QCD Q perturbative 1 F (Q2) = dxdy H(x, y) φ(x) φ(y) Q2 SCET Λ ! QCD non-perturbative 2 ChPT mπ f µ (4) = tr ∂ Σ∂ Σ† + v tr m†Σ+m Σ† + (L ) L 8 µ q q L i ! " ! " Lattice & EFT - extrapolations Symanzik’s Effective Field Theory Symanzik’s EffeχctiSBvewFieithldWTilsheonoQryuarks ! −1 Near continuum a ΛQCD, lattice action described by a continuum effective fieldFtehremorioy n Discretization ! W−1ilson solves the doubling radically with second Near continuum a Λ2 QCD, lattice a1 ction describ1ed by a 2 2 0 1 2 Sy−manzik’s Effective Field Theory Symanzik Action: SSymanzik = S + a S + a Sder+iv.a.t.ive Go (m = 0) = iγµ a sin(pµa) + a sin (pµa/2) FecormniotinnuDumLisactetricefefetizdctiscriavtioeetizafientilodnt(hsheoortrryange) in χPT? Operators in EFT respect symmetries of laCttihceir−a1al ctsymionmetry1 recovered only in the continuum limit Naive discretization G (m = 0) = iγµ sin(p2µa) Symanzik Action: SSymanziko = S0 + a S1a + a S2 + .