scholarly journals Measurement of the charged pion mass using a low-density target of light atoms

2016 ◽  
Vol 130 ◽  
pp. 01022 ◽  
Author(s):  
M. Trassinelli ◽  
D.F. Anagnostopoulos ◽  
G. Borchert ◽  
A. Dax ◽  
J.-P. Egger ◽  
...  
2020 ◽  
Vol 2020 (9) ◽  
Author(s):  
Masayasu Hasegawa

Abstract We aim to show the effects of the magnetic monopoles and instantons in quantum chromodynamics (QCD) on observables; therefore, we introduce a monopole and anti-monopole pair in the QCD vacuum of a quenched SU(3) by applying the monopole creation operator to the vacuum. We calculate the eigenvalues and eigenvectors of the overlap Dirac operator that preserves the exact chiral symmetry in lattice gauge theory using these QCD vacua. We then investigate the effects of magnetic monopoles and instantons. First, we confirm the monopole effects as follows: (i) the monopole creation operator makes the monopoles and anti-monopoles in the QCD vacuum. (ii) A monopole and anti-monopole pair creates an instanton or anti-instanton without changing the structure of the QCD vacuum. (iii) The monopole and anti-monopole pairs change only the scale of the spectrum distribution without affecting the spectra of the Dirac operator by comparing the spectra with random matrix theory. Next, we find the instanton effects by increasing the number density of the instantons and anti-instantons as follows: (iv) the decay constants of the pseudoscalar increase. (v) The values of the chiral condensate, which are defined as negative numbers, decrease. (vi) The light quarks and the pseudoscalar mesons become heavy. The catalytic effect on the charged pion is estimated using the numerical results of the pion decay constant and the pion mass. (vii) The decay width of the charged pion becomes wider than the experimental result, and the lifetime of the charged pion becomes shorter than the experimental result. These are the effects of the monopoles and instantons in QCD.


Author(s):  
D. F. Anagnostopoulos ◽  
M. Augsburger ◽  
G. Borchert ◽  
D. Chatellard ◽  
P. El-Khoury ◽  
...  

2020 ◽  
Vol 9 ◽  
pp. 308
Author(s):  
D. F. Anagnostopoulos, et al.

X-ray transitions in pionic nitrogen were measured using a curved crystal spectrometer. From the transition energy, calibrated with the help of the copper Ka1,2 electronic transition, a value for the charged pion mass of (139.57071± 0.00053) MeV/c2 was deduced. In order to reduce the uncertainty of the charged pion mass in the level of 1 ppm, we propose the determination of pionic transition energy based on the more precisely known energies and line shapes of muonic transitions.


2021 ◽  
Vol 62 (3) ◽  
Author(s):  
M. Hori ◽  
H. Aghai-Khozani ◽  
A. Sótér ◽  
A. Dax ◽  
D. Barna

AbstractWe review recent experiments carried out by the PiHe collaboration of the Paul Scherrer Institute (PSI) that observed an infrared transition of three-body pionic helium atoms by laser spectroscopy. These measurements may lead to a precise determination of the charged pion mass, and complement experiments of antiprotonic helium atoms carried out at the new ELENA facility of CERN.


2016 ◽  
Vol 759 ◽  
pp. 583-588 ◽  
Author(s):  
M. Trassinelli ◽  
D.F. Anagnostopoulos ◽  
G. Borchert ◽  
A. Dax ◽  
J.-P. Egger ◽  
...  
Keyword(s):  

Author(s):  
G. L. Borchert ◽  
B. Manil ◽  
D. Anagnostopoulos ◽  
J. P. Egger ◽  
D. Gotta ◽  
...  

Author(s):  
Manfred Daum ◽  
Peter-R. Kettle

The most precise value for the \pi^0π0 mass was obtained from the measurement of the mass difference m_{\pi^-}-m_{\pi^0} = 4.593\,64(48)mπ−−mπ0=4.59364(48),MeV/c^22 in the charge exchange reaction \pi^-π−p \rightarrow \pi^0→π0n at PSI. With the most precise charged pion mass value, m_{\pi^+} = 139.570\,21(14)mπ+=139.57021(14),MeV/c^22 and the validity of the CPT theorem (m_{\pi^-} = m_{\pi^+}mπ−=mπ+), a value m_{\pi^0} = 134.976\,57(50)mπ0=134.97657(50),MeV/c^22 is obtained. The measurements also revealed, for the first time, evidence of an unexpectedly large contribution from Coulomb de-excitation states during the pionic atom cascade.


1996 ◽  
Vol 53 (11) ◽  
pp. 6065-6077 ◽  
Author(s):  
K. Assamagan ◽  
Ch. Brönnimann ◽  
M. Daum ◽  
H. Forrer ◽  
R. Frosch ◽  
...  

Author(s):  
P.J. Killingworth ◽  
M. Warren

Ultimate resolution in the scanning electron microscope is determined not only by the diameter of the incident electron beam, but by interaction of that beam with the specimen material. Generally, while minimum beam diameter diminishes with increasing voltage, due to the reduced effect of aberration component and magnetic interference, the excited volume within the sample increases with electron energy. Thus, for any given material and imaging signal, there is an optimum volt age to achieve best resolution.In the case of organic materials, which are in general of low density and electric ally non-conducting; and may in addition be susceptible to radiation and heat damage, the selection of correct operating parameters is extremely critical and is achiev ed by interative adjustment.


Sign in / Sign up

Export Citation Format

Share Document