CKM Unitarity and Neutron Beta Decay Measuring V ud in Neutron Beta Decay

Similar documents
CORRELATION COEFFICIENTS A & B

Neutron lifetime experiment HOPE

Precision Measurements of Neutron Beta Decay with NoMoS at PERC

Investigating Parity Violation in Neutron Decay

UCN supersource at PNPI and fundamental physics program А.P. Serebrov

The Antineutrino Electron Angular Correlation Coefficient a in the Decay of the Free Neutron

* Neutron magnetic storage and neutron lifetime measuring

Neutron ββ-decay Angular Correlations

Present status and future prospects of nedm experiment of PNPI-ILL-PTI collaboration

High-precision studies in fundamental physics with slow neutrons. Oliver Zimmer Institut Laue Langevin

the role of atom and ion traps

TAMU-TRAP facility for Weak Interaction Physics. P.D. Shidling Cyclotron Institute, Texas A&M University

The New Search for a Neutron EDM at the SNS

A new UCN source at TRIUMF for EDM, β decay, gravity etc.

M. Beck. Institut für Physik, Johannes Gutenberg-Universität Mainz for the aspect collaboration. The aspect experiment. an overview and latest results

Victor Ezhov Petersburg Nuclear Physics Institute NRC KI ISINN 2015 May 25-29, Dubna

PENeLOPE. a UCN storage experiment with superconducting magnets for measuring the neutron lifetime

Experiments in Fundamental Neutron Physics

solenoid and time projection chamber for neutron lifetime measurement LINA

The KATRIN experiment

SuperSUN new infrastructure for experiments with ultracold neutrons at ILL

The neutron Electric Dipole Moment

PoS(CKM2016)028. V ud from Nuclear Beta Decays. J.C. Hardy and I.S. Towner

Ultra-Cold Neutrons (UCN) provide unique system to study fundamental neutron properties

Project of ultracold neutron source with superfluid helium at WWR-M reactor (PNPI, Gatchina) and scientific research program А.P.

Adam Tarte Holley. Postdoctoral Fellow Graduate Student Research Assistant Teaching Assistant

Markus Köhli M.Klein, U. Schmidt AG Dubbers

arxiv:nucl-ex/ v1 4 Jan 2007

Fundamental interactions experiments with polarized trapped nuclei

Fundamental Neutron Physics II. Fundamental Neutron Physics III

Institute Laue-Langevin, Grenoble

Nab: a precise measurement of the a and b parameters in neutron decay

Fundamental ESS

POLARIZED 3 He in FUNDAMENTAL PHYSICS with COLD NEUTRONS. Tom Gentile National Institute of Standards and Technology (NIST)

Past searches for kev neutrinos in beta-ray spectra

Neutron Instruments I & II. Ken Andersen ESS Instruments Division

Standard Model and ion traps: symmetries galore. Jason Clark Exotic Beam Summer School July 28 August 1, 2014

Standard Model Theory of Neutron Beta Decay

Plan to search for nnbar at WWR-M reactor

Neutron Beta-Decay. Christopher B. Hayes. December 6, 2012

A quantum bouncing ball gravity spectrometer

KATRIN, an experiment for determination of the -mass: status and outlook DSU2012

Physics with stopped beams at TRIP-TRAP Facility. P.D. Shidling Cyclotron Institute, Texas A&M University

ABSTRACT. (V A) and the Cabibbo-Kobayashi-Maskawa (CKM) quark mixing matrix is unitary. Measuring the

The cryogenic neutron EDM experiment at ILL

Depolarization of ultracold neutrons during their storage in material bottles

Small Angle Neutron Scattering in Different Fields of Research. Henrich Frielinghaus

arxiv: v1 [nucl-ex] 1 Oct 2008

Physics beyond the Standard Model with trapped atoms in the LHC era

Virginia Polytechnic Institute and State University M. Makela, M. Pitt, R.B. Vogelaar

Electroweak Physics: Lecture V

Preparation of facilities for fundamental research with ultracold neutrons at PNPI

Polarization for precision measurements. Torsten Soldner Institut Laue Langevin

Overview of the LEPS facility Recent Results

2017 Nobel Prize in Physics Awarded to LIGO Black Hole Researchers

Sven Schumann. DPG Spring Meeting

ATHENA / AD-1. First production and detection of cold antihydrogen atoms. ATHENA Collaboration. Rolf Landua CERN

The GERmanium Detector Array

Studying Neutron-Induced Reactions for Basic Science and Societal Applications

Neutron Lifetime Measurements

Determination of the Free Neutron Lifetime

Lafont Fabien Roulier Damien Virot Romain

Polarized Ultracold Neutrons: their transport in diamond guides and potential to search for physics beyond the standard model

Current status and future prospects of direct neutrino mass experiments

New Search for Mirror Neutrons at HFIR

Møller Polarimetry for PV Experiments at 12 GeV

Fundamentals of Neutron Physics

Beta decay experiments with separated fragmented beams

Determination of Absolute Neutron Fluence to sub-0.1% uncertainty (and better)

Louis Varriano University of Tennessee, Knoxville P599 PPAC Seminar April 16, 2014

Nab experiment: progress update

Neutronic design of the ESS targetmoderatorreflector. Luca Zanini For the ESS target division and in-kind collaborators

magneto-optically trapped, spin-polarized 37 K

CryoEDM The search for the electric dipole moment of the neutron

High Precision Nuclear Beta Spectroscopy

Measurements of liquid xenon s response to low-energy particle interactions

BSM with Single Nuclear Beta Decays. Alejandro Garcia University of Washington

The Search for the Neutron Electric Dipole Moment

Paul Huffman! Investigating Hadronic Parity Violation Using the γd np Reaction at the Proposed HIGS2 facility at TUNL

Lecture Series: Atomic Physics Tools in Nuclear Physics IV. High-Precision Penning Trap Mass Spectrometry


Status and Neutrino Oscillation Physics Potential of the Hyper-Kamiokande Project in Japan

Electroweak measurements at HERA

Møller Polarimetry for PV Experiments at 12 GeV

Neutrons on a surface of liquid helium.

K.U.Leuven. : an Application of the MYRRHA Accelerator for Nuclear Physics. Piet Van Duppen IKS, KUL, Leuven (BE)

PREX and CREX. R N from Electroweak Asymmetry in Elastic Electron-Nucleus Scattering. Neutron Skin.

Møller Polarimetry on Atomic Hydrogen

Low-spin structure of 210 Bi

Superallowed Fermi Beta Decay

Radiative Corrections in Free Neutron Decays

An option of «UCN pump» for ESS. V.V. Nesvizhevsky. Institut Max von Laue Paul Langevin, 71 av. des Martyrs, Grenoble, France.

1. Physics Motivation

Outline. Charged Leptonic Weak Interaction. Charged Weak Interactions of Quarks. Neutral Weak Interaction. Electroweak Unification

Direct Neutrino Mass Measurement with KATRIN. Sanshiro Enomoto (University of Washington) for the KATRIN Collaboration

Neutron Polarization and polarimetry for precision neutron decay measurments

Weak Decays: theoretical overview

V ud, V us, THE CABIBBO ANGLE, AND CKM UNITARITY Updated March 2012 by E. Blucher (Univ. of Chicago) and W.J. Marciano (BNL)

LEPS Physics HOTTA, Tomoaki (RCNP, Osaka University) on behalf of the LEPS&LEPS2 collaboration

The search for permanent electric dipole moments Klaus Kirch Paul Scherrer Institut and ETH Zürich

Transcription:

CKM Unitarity and Neutron Beta Decay Measuring V ud in Neutron Beta Decay Bastian Märkisch Physik-Department Technische Universität München CKM Matrix Element V ud Effective CC Couplings Neutron Lifetime Neutron Decay Corellations

Neutron Beta-Decay Low energy E p,max = 752 ev E e,max = 782 kev Long lifetime τ = 880.3(1.1) s Only small, precisely known radiative corrections Two free parameters within SM (G F from muon decay) Ratio of coupling constants Quark mixing Axial-vector g A und vector g V Cabibbo-Kobayashi-Maskawa matrix element g g A V 1 2 F 2 R 2 f m c ud ( 1 3 ) 2 G V Vud 5 4 e 3 7

V ud from Neutron Decay from D. Pocanic arxiv:1704.00192v1 Status today: (using PDG 2016 averages) V ud = 0.97585 (18) RC (55) τ (146) λ Future prospects: New experiments: Nab, PERC Penelope / HOPE / τspect / UCNτ / BL3 V ud = 0.97xxx (18) RC (11) τ (8) λ Marciano, Sirlin PRL 96 (2006) Near future (this year s results): acorn, aspect?, UCNA, PERKEO III V ud = 0.97xxx (18) RC (2 22) τ (2 40) λ (new avg lifetime & upcoming PERKEO III result) For comparision: average of 14 nuclei (0 + 0 + ): V ud = 0.97417 (18) RC (9) NS (6) exp J.C. Hardy & I. S. Towner, PRC91, 025501 (2015)

Neutron Classification Cold neutrons moderated in thermal bath (e.g. liquid D 2 ) E ~ 3 mev, T ~ 40 K, v ~ 800 m/s, ~ 0.5nm high flux densities: 2 10 10 s -1 cm -2 density ~10 5 cm - ³ decay rate of up to 10 6 s -1 (typ. correlation measurements) per metre Ultracold neutrons (UCN) E < 300 nev, T ~ 1 mk, v < 7 m/s, > 60nm reflect from surfaces under any incident angle : storable V n < V crit V n V n > V crit Fermi potential ~ 100 nev Gravity ~ 100 nev / m ΔE=m n g Δh Magnetic field ~ 60 nev / Tesla ΔE= μ n B moderate densities: ~30 cm -3 (typ. neutron lifetime, EDM) UCN UCN bottle Material storage and gravity!

Measurement of the neutron lifetime τ n Storage experiments with UCN counting the survivors In-beam experiments with cold neutrons counting the dead 1 τ m t 2 1 - t 1 ln N(t N(t 1 2 ) ) l e,p n β UCN 1 τ m 1 τ β 1 τ wall 1 τ leak τ 1 vacuum... N(t 1 ), N(t 2 ) 1 τ wall μ v eff 0 (experiment) 0 (extrapolation) 1 τm 1 τ β n β dn dt N 0 N τ n 0 e l v τ n relative measurements absolute measurements

Gravitrap at ILL Previous most precise measurement

Neutron Lifetime Measurements 887.7(12) stat (19) sys 877.7(7) stat (3) sys 878.5(7) stat (3) sys 880.5(7) stat (8) sys S=1.9 New avg? 879.4(8) S=1.9

New Gravitrap II Lifetime measurement by fill-and-empty. Massively larger than previous experiment. Running at ILL, Grenoble. Many systematic studies (coating, losses, temperature) Next: Change from LN temperature to LHe cooling (10K) to reduce wall losses.

UCN Magneto-gravitational trap Operated at LANL ~5500 permanent magnets Material: C.-Y. Liu EXA2017

UCN Magneto-gravitational trap Hallbach array R. W. Pattie, et al., arxiv 1707.01817: 877.7(7) stat (3) sys Material: C.-Y. Liu EXA2017

More Neutron Lifetime Exp. TRIGA Mark II HOPE permanent magnet multipole + SC magnet, 8l volume, new UCN source short term goal 2s, long term < 0.3s running at Mainz permanent magnet octupole + SC magnet, 2l volume, new UCN source Goal: 1s -- running at ILL, Grenoble J-PARC TPC Pulsed beam Status: 1% Goal 0.1% NIST BL2: goal 1s BL3: new magnet; goal < 0.3s

2.5 m PENeLOPE (TUM) Magnetic & Gravitational trapping avoids material losses altogether! (HOPE/ILL, Ezhov/ILL, τspect/mainz, UCNτ/LANL, PENeLOPE/TUM): store only one spin-direction PENeLOPE aims at a precision of ± 0.1 s Measure protons and neutrons directly from decay. Also fill-and-empty. absorber movement mechanism proton detector outer pressure vessel helium vessel PENeLOPE light storage walls (electropolished)

Neutron Decay Correlations A Electron p e σ e Neutron Spin J B C Neutrino p ν Proton p p Naviliat-Cuncic and Gonzalez-Alonso, Ann. Phys. 525, 8 9, 600 619 (2013) Dubbers and Schmidt, Rev. Mod. Phys (2012)

Correlation Coefficients e 3 d 1 e 1 3 p E E E 2 2 2 F ud e e 0 e G V 5 de d d 22 p p p p p p 1 a m b E E E A E B E D E E e e n e e e e n e e 2 Jackson, Treiman, Wyld, Nucl. Phys. 4, 1957 Electron p e σ e C A Neutron Spin J B Neutrino p ν Proton p p PERKEO II PERKEO III / PERC Typical current relative precision O(10-2 - 10-3 ) Goal of next generation PERC: O(10-3 - 10-4 ) for some observables 1.2(2.0) 10-4

relative change Determination of = g A /g V = g A /g V A PDG B PDG a PDG -0.1184 0.0010 0.9807 0.0030 C 0.2377 0.0026 0.103 0.004 1.1% 0.3% 1.1% 3.9%

PERKEO III A, B, C, b Heidelberg, TU Wien, TU München, ILL Current Neutron Decay Experiments aspect a Mainz, TU Wien, ILL acorn a NIST UCNA / UCNB A, B, b Los Alamos Nab a, b SNS and PERC

PERKEO: Measuring Beta Asymmetry A Detector 1 Electron Electron angular distribution: v W (, E) 1 Acos c Within Standard Model: g g A V Polarised Neutrons Detector 2 Magnetic field to as quantisation axis Integration over hemispheres: 2 2π detection Experimental asymmetry, polarisation P A exp N N N N 1 2 v c PA cos 1 2

Spectrometer PERKEO III Detector 1 Total length: 8 m ~50.000 decays / sec in the continuous beam Pulsed Neutron Beam electrons B = 150 mt (homogeneous ) B = 90 mt Detector 2 Beam preparation Active volume (~2m) Duty cycle: ~7% Beamstop Velocity Selector Supermirror Polarizer Adiabatic Fast Passage Spin Flipper Mechanical disc chopper

PERKEO III: Pulsed Neutron Beam Sacrifise ~2 orders of magnitude in statistics to address important systematic: background; continuous beam 50.000 s -1 ; pulsed 250 s -1

PERKEO III: Calibration Fits 114 full calibrations in (twice per day) Simultaneous Fit: Χ²/NDF = 1.0 1.3 Free parameters: Non-linearity, gain, PE + norms In addition: Hourly drift measurements ~weekly 2D uniformity scan Green bars indicate fit region

Asymmetry Extraction Result (still blinded): A 1.910 A 4 4.810 3

PERKEO III Error budget Finally, close to being unblinded (inconsistencies in indep. analyses resolved)

New: acorn, NIST Electron-Neutroino Correlation a : Results soon from aspect, Mainz Nab goal: competitive with A New UCNA result Goal of Nab, PERC Δλ/λ ~ O(10-4 ) PDG 2016-1.2723(23)

Proton Electron Radiation Channel (PERC) Magnetic Filter B 1 B 1 B 2 Cryostat B 0 Active volume in a 8 m long neutron-guide, B 0 = 1.5 T: phase space density and statistics Magnetic Filter, B 1 = 6T: phase space, systematics (solid angle, backscatter suppression) B1 212 B 0 Source for specialised spectrometers Aims to improve results by an order of magnitude: 10-4. New Observables. Nucl. Instr. Meth. A 596 (2008) 238 and arxiv:0709.4440

Beam Site Mephisto, FRM II FRM-II, Garching New hall east Reactor Guide hall Atomic egg PERC New hall east Empty new hall Neutron guide: length 40 m, R = 3000 m, m = 2.5 Expected intensity equal to PF1B at ILL (2 10 10 s -1 cm -2 ) Only very few neighbours: low ambient background Easy ground level access, Fixed installation Intermediate Structure Status: All major components of the beam line ready or in production Reactor Core

PERC: Neutron Spin Control O(10-4 ) precision requires neutron spin control on the same level: - polarisation 99.7%: FeSi polarisers Soldner / Petoukhov et al. (ILL) - spin flipper: AFP 100.00% - guide in strong magnetic field: only 10-4 depolarization per bounce allowed - measurement with 3 He spin filters Soldner et al. (ILL) Non-magnetic CuTi mirror m=2 preserves spin direction Production quality (except for the too thin top layer) Large maximum angle of reflection, high reflectivity Reduces neutron losses in PERC by factor > 2: background! (Mildly) backable (>80 C). Beneficial for vacuum conditions. Hollering (TUM), Rebrova / Schmidt (HD)

Status of the PERC Magnet SPP 1491 Closing Convention - B. Märkisch 27

PERC is a Facility Clean source of electrons and protons from neutron decay User System R B spectrometer Wien filter for protons Magnetic spectrometer Electrostatic chopper & p detector MAC-E filter ( aspect ) Electron or proton detector Scintillator, Silicon,

Prospects Tremendous ongoing efforts to improve V ud from neutron decay Lifetime τ Potential new average (including UCNtau + Gravitrap2 results) τ = 879.4(8) s; S = 1.9 Many new experimental results to be expected: UCNtau, HOPE, tauspect, PENeLOPE, Gravitrap2 Current Goal: O(0.1s) Ratio of coupling constants λ New (upcoming) results by acorn, UCNA, PERKEO III, aspect Next generation Nab a 0.1% PERC A 0.05% Long-term future (next decade): cold beam line ANNI at ESS (more than order of magnitude More statistics in pulsed beam) Aerial view ESS construction site September 2015

PERC (Proton Electron Radiation Channel) at FRM II / MLZ B. Märkisch U. Schmidt J. Klenke H. Abele E. Jericha G. Konrad W. Heil O. Zimmer T. Soldner

Wilhelm und Else Heraeus-Seminar Particle Physics with Cold and Ultra-Cold Neutrons Wednesday 24 th Friday 26 th October 2018 Physikzentrum Bad Honnef Scientific Organizers: Hartmut Abele, Atominstitut, TU Wien Bastian Märkisch, TU München

from D. Pocanic arxiv:1704.00192v1

Beam Method: NIST Experiment S. Dewey

Result: 878.5(7) stat (3) sys Measurement cycle measures UCN spectral dependence Small final extrapolation

Observables and Statistics Focus on non-coincident measurements due to high count rates: Polarised neutrons β-asymmetry A A ~ 5 10-4 Proton asymmetry C C ~ 3 10-4 Neutrino asymmetry B B ~ 1 10-3 Weak magnetism f WM from β-asymmetry or polarised spectra > 3 σ Electron C A Proton Neutron Spin B Neutrino a Unpolarised neutrons Correlation a a ~ 5 10-3 from proton spectrum Fierz coefficient b b ~ 1 10-3 from electron spectrum or β-asymmetry Electron helicity h Time for 10 9 events 5 hours (unpolarised) 1 day polarised 98% 2 days polarised 99.7% 25 for pulsed mode

Fierz Interference Term b Sensitive to scalar and tensor couplings within SM: b = 0 Enters decay rate / spectra and asymmetries: Requirement: Calibration etc. independent of neutron data Reach of existing PERKEO III data Δb 3 10-2 from asymmetry. Pending approval by the collaboration. Only 1 out of 4 datasets.

Extra