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3.4 V-A Coupling of Leptons and Quarks 3.5 CKM Matrix to Describe the Quark Mixing
Advanced Particle Physics: VI. Probing the weak interaction 3.4 V-A coupling of leptons and quarks Reminder u γ µ (1− γ 5 )u = u γ µu L = (u L + u R )γ µu L = u Lγ µu L l ν l ν l l ν l ν In V-A theory the weak interaction couples left-handed lepton/quark currents (right-handed anti-lepton/quark currents) with an universal coupling strength: 2 GF gw = 2 2 8MW Weak transition appear only inside weak-isospin doublets: Not equal to the mass eigenstate Lepton currents: Quark currents: ⎛ν ⎞ ⎛ u ⎞ 1. ⎜ e ⎟ j µ = u γ µ (1− γ 5 )u 1. ⎜ ⎟ j µ = u γ µ (1− γ 5 )u ⎜ − ⎟ eν e ν ⎜ ⎟ du d u ⎝e ⎠ ⎝d′⎠ ⎛ν ⎞ ⎛ c ⎞ 5 2. ⎜ µ ⎟ j µ = u γ µ (1− γ 5 )u 2. ⎜ ⎟ j µ = u γ µ (1− γ )u ⎜ − ⎟ µν µ ν ⎜ ⎟ sc s c ⎝ µ ⎠ ⎝s′⎠ ⎛ν ⎞ ⎛ t ⎞ µ µ 5 3. ⎜ τ ⎟ j µ = u γ µ (1− γ 5 )u 3. ⎜ ⎟ j = u γ (1− γ )u ⎜ − ⎟ τν τ ν ⎜ ⎟ bt b t ⎝τ ⎠ ⎝b′⎠ 3.5 CKM matrix to describe the quark mixing One finds that the weak eigenstates of the down type quarks entering the weak isospin doublets are not equal to the their mass/flavor eigenstates: ⎛d′⎞ ⎛V V V ⎞ ⎛d ⎞ d V u ⎜ ⎟ ⎜ ud us ub ⎟ ⎜ ⎟ ud ⎜ s′⎟ = ⎜Vcd Vcs Vcb ⎟ ⋅ ⎜ s ⎟ ⎜ ⎟ ⎜ ⎟ ⎜ ⎟ W ⎝b′⎠ ⎝Vtd Vts Vtb ⎠ ⎝b⎠ Cabibbo-Kobayashi-Maskawa mixing matrix The quark mixing is the origin of the flavor number violation of the weak interaction. -
Strong Coupling and Quantum Molecular Plasmonics
Strong coupling and molecular plasmonics Javier Aizpurua http://cfm.ehu.es/nanophotonics Center for Materials Physics, CSIC-UPV/EHU and Donostia International Physics Center - DIPC Donostia-San Sebastián, Basque Country AMOLF Nanophotonics School June 17-21, 2019, Science Park, Amsterdam, The Netherlands Organic molecules & light Excited molecule (=exciton on molecule) Photon Photon Adding mirrors to this interaction The photon can come back! Optical cavities to enhance light-matter interaction Optical mirrors Dielectric resonator Veff Q ∼ 1/κ Photonic crystals Plasmonic cavity Veff Q∼1/κ Coupling of plasmons and molecular excitations Plasmon-Exciton Coupling Plasmon-Vibration Coupling Absorption, Scattering, IR Absorption, Fluorescence Veff Raman Scattering Extreme plasmonic cavities Top-down Bottom-up STM ultra high-vacuum Wet Chemistry Low temperature Self-assembled monolayers (Hefei, China) (Cambridge, UK) “More interacting system” One cannot distinguish whether we have a photon or an excited molecule. The eigenstates are “hybrid” states, part molecule and part photon: “polaritons” Strong coupling! Experiments: organic molecules Organic molecules: Microcavity: D. G. Lidzey et al., Nature 395, 53 (1998) • Large dipole moments • High densities collective enhancement • Rabi splitting can be >1 eV (~30% of transition energy) • Room temperature! Surface plasmons: J. Bellessa et al., Single molecule with gap plasmon: Phys. Rev. Lett. 93, 036404 (2004) Chikkaraddy et al., Nature 535, 127 (2016) from lecture by V. Shalaev Plasmonic cavities -
Fundamental Nature of the Fine-Structure Constant Michael Sherbon
Fundamental Nature of the Fine-Structure Constant Michael Sherbon To cite this version: Michael Sherbon. Fundamental Nature of the Fine-Structure Constant. International Journal of Physical Research , Science Publishing Corporation 2014, 2 (1), pp.1-9. 10.14419/ijpr.v2i1.1817. hal-01304522 HAL Id: hal-01304522 https://hal.archives-ouvertes.fr/hal-01304522 Submitted on 19 Apr 2016 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. Distributed under a Creative Commons Attribution| 4.0 International License Fundamental Nature of the Fine-Structure Constant Michael A. Sherbon Case Western Reserve University Alumnus E-mail: michael:sherbon@case:edu January 17, 2014 Abstract Arnold Sommerfeld introduced the fine-structure constant that determines the strength of the electromagnetic interaction. Following Sommerfeld, Wolfgang Pauli left several clues to calculating the fine-structure constant with his research on Johannes Kepler’s view of nature and Pythagorean geometry. The Laplace limit of Kepler’s equation in classical mechanics, the Bohr-Sommerfeld model of the hydrogen atom and Julian Schwinger’s research enable a calculation of the electron magnetic moment anomaly. Considerations of fundamental lengths such as the charge radius of the proton and mass ratios suggest some further foundational interpretations of quantum electrodynamics. -
The Electron-Phonon Coupling Constant
The electron-phonon coupling constant Philip B. Allen Department of Physics and Astronomy, State University of New York, Stony Brook, NY 11794-3800 March 17, 2000 Tables of values of the electron-phonon coupling constants and are given for selected tr elements and comp ounds. A brief summary of the theory is also given. I. THEORETICAL INTRODUCTION Grimvall [1] has written a review of electron-phonon e ects in metals. Prominent among these e ects is sup ercon- ductivity. The BCS theory gives a relation T exp1=N 0V for the sup erconducting transition temp erature c D T in terms of the Debye temp erature .Values of T are tabulated in various places, the most complete prior to c D c the high T era b eing ref. [2]. The electron-electron interaction V consists of the attractive electron-phonon-induced c interaction minus the repulsive Coulombinteraction. The notation is used = N 0V 1 eph and the Coulomb repulsion N 0V is called , so that N 0V = , where is a \renormalized" Coulomb c repulsion, reduced in value from to =[1 + ln! =! ]. This suppression of the Coulomb repulsion is a result P D of the fact that the electron-phonon attraction is retarded in time by an amountt 1=! whereas the repulsive D screened Coulombinteraction is retarded byamuch smaller time, t 1=! where ! is the electronic plasma P P frequency. Therefore, is b ounded ab oveby1= ln! =! which for conventional metals should b e 0:2. P D Values of are known to range from 0:10 to 2:0. -
Dirac's Fine-Structure Formula for an “Abnormally High”
Dirac’s fine-structure formula for an “abnormally high” nuclear charge The solution of an old riddle A. LOINGER Dipartimento di Fisica dell’Università di Milano Via Celoria, 16 − 20133 Milano, Italy Summary. − In Dirac’s fine-structure formula for the hydrogenlike atoms a critical role is played by the square root of the following expression: the unity minus the square of the product of the atomic number by the fine-structure constant (which is approximately equal to 1/137). Indeed, for a fictitious, ideal nucleus for which the above product is greater than or equal to one, the mentioned square root becomes imaginary, or zero. I prove in this Note that the origin of such theoretical “breaking down” is quite simple and is inherent in the special theory of relativity of classical physics. PACS 11.10 − Relativistic wave equations; 03.65 – Semiclassical theories and applications. 1. − The problem As is well known, Dirac’s fine-structure formula for the energy of an electron in the Coulomb field generated by a fixed nuclear charge Ze is as follows: −1 2 2 2 E Z α (1.1) = 1+ , 2 2 m0c 2 2 2 1 2 []nr + (κ − Z α ) 2 where: E = W + m0c is the relativistic total energy; m0 is the rest-mass of the 2 electron; α := e (hc) is the fine-structure constant; nr = 0,1,2,3,... is the radial quantum number; κ = ±1,±2,±3,... is the auxiliary quantum number (according to a Weylian terminology); when nr = 0 , the quantum κ takes only the positive values [1]. -
How the Electron-Phonon Coupling Mechanism Work in Metal Superconductor
How the electron-phonon coupling mechanism work in metal superconductor Qiankai Yao1,2 1College of Science, Henan University of Technology, Zhengzhou450001, China 2School of physics and Engineering, Zhengzhou University, Zhengzhou450001, China Abstract Superconductivity in some metals at low temperature is known to arise from an electron-phonon coupling mechanism. Such the mechanism enables an effective attraction to bind two mobile electrons together, and even form a kind of pairing system(called Cooper pair) to be physically responsible for superconductivity. But, is it possible by an analogy with the electrodynamics to describe the electron-phonon coupling as a resistivity-dependent attraction? Actually so, it will help us to explore a more operational quantum model for the formation of Cooper pair. In particularly, by the calculation of quantum state of Cooper pair, the explored model can provide a more explicit explanation for the fundamental properties of metal superconductor, and answer: 1) How the transition temperature of metal superconductor is determined? 2) Which metals can realize the superconducting transition at low temperature? PACS numbers: 74.20.Fg; 74.20.-z; 74.25.-q; 74.20.De ne is the mobile electron density, η the damping coefficient 1. Introduction that is determined by the collision time τ . In the BCS theory[1], superconductivity is attributed to a In metal environment, mobile electrons are usually phonon-mediated attraction between mobile electrons near modeled to be a kind of classical particles like gas molecules, Fermi surface(called Fermi electrons). The attraction is each of which performs a Brown-like motion and satisfies the sometimes referred to as a residual Coulomb interaction[2] that Langevin equation can glue Cooper pair together to cause superconductivity. -
H20 Maser Observations in W3 (OH): a Comparison of Two Epochs
DePaul University Via Sapientiae College of Science and Health Theses and Dissertations College of Science and Health Summer 7-13-2012 H20 Maser Observations in W3 (OH): A comparison of Two Epochs Steven Merriman DePaul University, [email protected] Follow this and additional works at: https://via.library.depaul.edu/csh_etd Part of the Physics Commons Recommended Citation Merriman, Steven, "H20 Maser Observations in W3 (OH): A comparison of Two Epochs" (2012). College of Science and Health Theses and Dissertations. 31. https://via.library.depaul.edu/csh_etd/31 This Thesis is brought to you for free and open access by the College of Science and Health at Via Sapientiae. It has been accepted for inclusion in College of Science and Health Theses and Dissertations by an authorized administrator of Via Sapientiae. For more information, please contact [email protected]. DEPAUL UNIVERSITY H2O Maser Observations in W3(OH): A Comparison of Two Epochs by Steven Merriman A thesis submitted in partial fulfillment for the degree of Master of Science in the Department of Physics College of Science and Health July 2012 Declaration of Authorship I, Steven Merriman, declare that this thesis titled, `H2O Maser Observations in W3OH: A Comparison of Two Epochs' and the work presented in it are my own. I confirm that: This work was done wholly while in candidature for a masters degree at Depaul University. Where I have consulted the published work of others, this is always clearly attributed. Where I have quoted from the work of others, the source is always given. With the exception of such quotations, this thesis is entirely my own work. -
The Fine Structure Constant
GENERAL ⎜ ARTICLE The Fine Structure Constant Biman Nath The article discusses the importance of the fine structure constant in quantum mechanics, along with the brief history of how it emerged. Al- though Sommerfelds idea of elliptical orbits has been replaced by wave mechanics, the fine struc- ture constant he introduced has remained as an Biman Nath is an important parameter in the field of atomic struc- astrophysicist at the ture. Raman Research Institute, Bengaluru. The values of the constants of Nature, such as Newton’s gravitational constant ‘G’, determine the nature of our Universe. Among these constants, there are a few which are pure numbers and have no units. For example, there is the ‘fine structure constant’, denoted by α, which has a value roughly 1/137. The value of α is related to the electromagnetic force between subatomic charged parti- cles, and essentially determines how an atom holds to- gether its electrons. It is however not obvious why this constant has this par- ticular value. Why 1/137 and not some other value? One might think the question is meaningless, but it is not. If the value of this constant had been slightly smaller or larger, even by as little as 4%, then stars would not have been able to sustain the nuclear reac- tions in their core that produce carbon. As a result, there would not have been any carbon-based lifeforms in our Universe. Therefore, the question why α ≈ 1/137 is not completely irrelevant. Scientists have even wondered if its value remains a con- stant over time. -
Quantum Mechanics of Atoms and Molecules Lectures, the University of Manchester 2005
Quantum Mechanics of Atoms and Molecules Lectures, The University of Manchester 2005 Dr. T. Brandes April 29, 2005 CONTENTS I. Short Historical Introduction : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : 1 I.1 Atoms and Molecules as a Concept . 1 I.2 Discovery of Atoms . 1 I.3 Theory of Atoms: Quantum Mechanics . 2 II. Some Revision, Fine-Structure of Atomic Spectra : : : : : : : : : : : : : : : : : : : : : 3 II.1 Hydrogen Atom (non-relativistic) . 3 II.2 A `Mini-Molecule': Perturbation Theory vs Non-Perturbative Bonding . 6 II.3 Hydrogen Atom: Fine Structure . 9 III. Introduction into Many-Particle Systems : : : : : : : : : : : : : : : : : : : : : : : : : 14 III.1 Indistinguishable Particles . 14 III.2 2-Fermion Systems . 18 III.3 Two-electron Atoms and Ions . 23 IV. The Hartree-Fock Method : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : 24 IV.1 The Hartree Equations, Atoms, and the Periodic Table . 24 IV.2 Hamiltonian for N Fermions . 26 IV.3 Hartree-Fock Equations . 28 V. Molecules : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : 35 V.1 Introduction . 35 V.2 The Born-Oppenheimer Approximation . 36 + V.3 The Hydrogen Molecule Ion H2 . 39 V.4 Hartree-Fock for Molecules . 45 VI. Time-Dependent Fields : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : 48 VI.1 Time-Dependence in Quantum Mechanics . 48 VI.2 Time-dependent Hamiltonians . 50 VI.3 Time-Dependent Perturbation Theory . 53 VII.Interaction with Light : : : : : : : : : : : : : : : : : : : : : : : -
Lattice-QCD Determinations of Quark Masses and the Strong Coupling Αs
Lattice-QCD Determinations of Quark Masses and the Strong Coupling αs Fermilab Lattice, MILC, and TUMQCD Collaborations September 1, 2020 EF Topical Groups: (check all that apply /) (EF01) EW Physics: Higgs Boson Properties and Couplings (EF02) EW Physics: Higgs Boson as a Portal to New Physics (EF03) EW Physics: Heavy Flavor and Top-quark Physics (EF04) EW Physics: Electroweak Precision Physics and Constraining New Physics (EF05) QCD and Strong Interactions: Precision QCD (EF06) QCD and Strong Interactions: Hadronic Structure and Forward QCD (EF07) QCD and Strong Interactions: Heavy Ions (EF08) BSM: Model-specific Explorations (EF09) BSM: More General Explorations (EF10) BSM: Dark Matter at Colliders Other Topical Groups: (RF01) Weak Decays of b and c Quarks (TF02) Effective Field Theory Techniques (TF05) Lattice Gauge Theory (CompF2) Theoretical Calculations and Simulation Contact Information: Andreas S. Kronfeld (Theoretical Physics Department, Fermilab) [email]: [email protected] on behalf of the Fermilab Lattice, MILC, and TUMQCD Collaborations Fermilab Lattice, MILC, and TUMQCD Collaborations: A. Bazavov, C. Bernard, N. Brambilla, C. DeTar, A.X. El-Khadra, E. Gamiz,´ Steven Gottlieb, U.M. Heller, W.I. Jay, J. Komijani, A.S. Kronfeld, J. Laiho, P.B. Mackenzie, E.T. Neil, P. Petreczky, J.N. Simone, R.L. Sugar, D. Toussaint, A. Vairo, A. Vaquero Aviles-Casco,´ J.H. Weber, R.S. Van de Water Lattice-QCD Determinations of Quark Masses and the Strong Coupling αs Quantum chromdynamics (QCD) as a stand-alone theory has 1 + nf + 1 free parameters that must be set from experimental measurements, complemented with theoretical calculations connecting the measurements to the QCD Lagrangian. -
2.5. the Fine Structure of a Hydrogen Atom
Phys460.nb 33 0 0 0= ψ a A H'-H'A ψb = (2.281) 0 0 0 0 0 0 0 0 0 0 ψa A H' ψb - ψ a H'A ψb =A a ψa H' ψb -A b ψa H' ψb =(A a -A b) ψa H' ψb 0 0 If Aa ≠A b, this equation means that ψa H' ψb = 0. 0 0 For this situation, although we have a degeneracy, one can just do non-degenerate perturbation for ψa and ψb (separately) and there will be no singularities at all. 2.5. the fine structure of a hydrogen atom 2.5.1. Relativistic correction In QMI, we solved an ideal model for a hydrogen atom (i.e. a particle in 1/r potential). In a real hydrogen atom, that model missed some of the physics, and one of them is relativistic effects. Q: what is the energy of a particle, if the particle is moving at speed v and the rest mass m. m E=Mc 2 = c2 2 (2.282) 1- v c2 Q: what is the momentum of a particle, if the particle is moving at speed v and the rest mass m. m p =Mv= v 2 (2.283) 1- v c2 As a result, E= p2 c2 +m 2 c4 (2.284) To prove this relation, we start from the r.h.s., p2 c2 +m 2 c4 = v2 2 2 2 2 2 m2 c41- 2 2 2 2 4 2 2 2 2 4 m v m v c c2 m v c +m c -m c v m c m (2.285) c2 +m 2 c4 = + = = = c2 =E v2 v2 v2 v2 v2 1- 2 1- 2 1- 2 1- 2 1- 2 2 c c c c c 1- v c2 This relation between E and p is an very important relation for relativistic physics! Q: what is kinetic energy? A: First, find the energy of a particle when it is not moving p = 0. -
Fine and Hyperfine Structure of the Hydrogen Atom
UNIT 4 Fine and hyperfine structure of the hydrogen atom Notes by N. Sirica and R. Van Wesep Previously, we solved the time-independent Sch¨odingerequation for the Hydro- gen atom, described by the Hamiltonian p2 e2 H = − (1) 2m r Where e is the electron’s charge in your favorite units. However, this is not really the Hamiltonian for the Hydrogen atom. It is non-relativistic and it does not contain spin. In order to completely describe the Hydrogen we would need to use the Dirac equation. We will not introduce that equation here, but we will say a few words about the most important energy level of the relativistic Hydrogen atom, namely the rest mass energy. E = mc2 ≈ 0.5MeV (2) We can compare this to the ground state (ionization) energy we found for the Hamiltonian in 1. 2 E = −Eion ≈ 13.6eV ¿ mc (3) Even though the rest mass energy is so much larger, it appears constant in the non-relativistic regime. Since differences in energy are important, we could ignore it before. The rest mass energy may be large, but it does not enter the world of everyday experience. Regardless, it is fruitful to investigate the relative size of the ionization energy to the rest mass energy. E me4 1 e4 α2 ion = = = (4) mc2 2~2 mc2 2c2~2 2 86 UNIT 4: Fine and hyperfine structure of the hydrogen atom e2 1 Where α = ~c = 137 is a fundamental constant of nature. No one understands it, but it is important that it is small.