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First direct observation of time-reversal non-invariance in the neutral-kaon system

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The first observation of time-reversal symmetry violation through a comparison of the probabilities of K 0 transforming into K0 and K 0 into K 0 as a function of the neutral-kaon eigentime t was reported in this article.
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This article is published in Physics Letters B.The article was published on 1998-12-17 and is currently open access. It has received 190 citations till now. The article focuses on the topics: Strangeness.

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Violations of fundamental symmetries in atoms and tests of unification theories of elementary particles

TL;DR: In this article, the authors review the recent progress in atomic parity nonconservation and atomic electric dipole moments (time reversal symmetry violation), with a particular focus on the atomic theory required to interpret the measurements.
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QCD and strongly coupled gauge theories: challenges and perspectives

Nora Brambilla, +53 more
TL;DR: In this paper, the progress, current status, and open challenges of QCD-driven physics, in theory and in experiment, are highlighted, highlighting how the strong interaction is intimately connected to a broad sweep of physical problems, in settings ranging from astrophysics and cosmology to strongly coupled, complex systems in particle and condensed-matter physics, as well as searches for physics beyond the Standard Model.
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Physics at a future Neutrino Factory and super-beam facility

A. Bandyopadhyay, +96 more
TL;DR: The conclusions of the Physics Working Group of the International Scoping Study of a future Neutrino Factory and super-beam facility (the ISS) are presented in this article.

Developments in alkali -metal atomic magnetometry

TL;DR: In this paper, a spin exchange relaxation-free (SERF) magnetometer was proposed to measure all three vector components of the magnetic field in an unshielded environment with comparable sensitivity to other devices.
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Observation of a chiral state in a microwave cavity.

TL;DR: The microwave experiment has been realized to measure the phase difference of the oscillating electric field at two points inside the cavity and it is concluded that the state excited at the singularity has a definitive chirality.
References
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Review of particle physics. Particle Data Group

TL;DR: The Particle Data Group's biennial review as mentioned in this paper summarizes much of Particle Physics, using data from previous editions, plus 1600 new measurements from 550 papers, and lists, evaluates and average measured properties of gauge bosons, leptons, quarks, mesons, and baryons.
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Particle Physics and Introduction to Field Theory

T. D. Lee, +1 more
TL;DR: In this paper, the spin-O field and spin-1/2 field were considered and U1 symmetry and P,C invariance isotropic spin and G parity SU3 symmetry time reversal CPT invariance K-K system vacuum was discussed.
Journal ArticleDOI

Testing CP and CPT violation in the neutral kaon system at a phi factory.

TL;DR: It is demonstrated by means of a global fit to all distributions that, at a {phi} factory with a total integrated luminosity of 10{sup 40} cm{sup {minus}2), it is possible to determine most of the presently measured {ital CP}- and {ital CPT}-violating parameters in the neutral kaon system to a considerably better (statistical) level than that of current measurements.
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The CPLEAR detector at CERN

R. Adler, +175 more
TL;DR: The CPLEAR detector at CERN was used for CP-, T- and CPT-symmetry studies using K 0 and K 0 produced by the annihilation of p's in a hydrogen gas target as mentioned in this paper.
Journal ArticleDOI

Measurement of the CP violation parameter η+− using tagged K0 and K0

R. Adler, +123 more
- 30 Nov 1995 - 
TL;DR: In this paper, the CP violation parameter η+− was determined through the eigentime-dependent asymmetry in the rates of initially tagged K0 and K 0 decaying to π+π−.
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Observation of Time-Reversal Violation in the B-0 Meson System

J. P. Lees, +365 more
Frequently Asked Questions (11)
Q1. What have the authors contributed in "First direct observation of time-reversal non-invariance in the neutral-kaon system" ?

0 the authors report on the first observation of time-reversal symmetry violation through a comparison of the probabilities of K 0 0 0 transforming into K and K into K as a function of the neutral-kaon eigentime t. 

The electron identification efficiency, obtained requiring that less than 2% of pions be misidentified aselectrons, is on the average 85%. 

The inputs to the NN Ž .algorithm are the momentum of the particle, the energy loss in the two scintillators S1, S2 , the number of Ž .photoelectrons in the Cherenkov counter and the time of flight from the decay vertex to the first scintillator S1 . 

TIn order to estimate the effect of an error in the normalization functions, j and h, the authors change the value of the average normalization in the fit procedure by one standard deviation. 

The fitted momenta and vertices resulting from the 6C-fit determine the neutral-kaon lifetime with a precision which ranges from 0.05 t in the short lifetime region to 0.2–0.3 t in the long one. 

SA number of factors that can introduce a distortion of the rates must be considered: detection efficiencies, regeneration effects, background estimation and decay-time resolution. 

In the past, phenomenological studies based on the Bell-Steinberger relation have concluded that CP w xviolation in the neutral-kaon system is dominantly accompanied by CPT invariance and T violation 2 . 

An additional source of systematic error arises from the charge asymmetry in the background, owing to the different probabilities for a pq and a py to be identified as a positron and an electron, respectively. 

The authors note that Im x is given by the value of the asymmetry for shortq Ž . ² exp:lifetimes while 4Re e is determined by the long lifetime values. 

The level of this asymmetry has been determined using pions selected from minimum-bias events and is found to be Ž . ² exp: y33"1 %, leading to an uncertainty in A of "0.02=10 . 

The resulting systematic error on A is foundT to be "0.1=10y3.Ž .The experimentally obtained asymmetry see Section 4.4 is² exp: y3A s 6.6"1.3 "1.0 =10 .Ž .T stat syst Ž . Ž .This value is well compatible with 4Re e see Section 6 .