From 82517fc6eba72e73090dda58018acea9061d9ef7 Mon Sep 17 00:00:00 2001
From: himyss <ivanmuzalevskij@gmail.com>
Date: Tue, 7 Nov 2023 18:51:53 +0300
Subject: [PATCH] data added
---
tetra.tex | 11 ++++++-----
1 file changed, 6 insertions(+), 5 deletions(-)
diff --git a/tetra.tex b/tetra.tex
index 1e3e956..338a68d 100644
--- a/tetra.tex
+++ b/tetra.tex
@@ -29,15 +29,16 @@ This work is dedicated to the results on the $^2$H($^8$He,$^6$Li) reaction studi
\section{Experiment}
-ACCULINNA-2 facility, FLNR, JINR, produced 26\,AMeV $^{8}$He and focused it on the cryogenic deuterium target.
-The experiment was dedicated to $^{7}$H studies, see Ref.\ \cite{Muzalevskii:2021}, but the detection system allowed to measure the product of the $^2$H($^8$He,$^6$Li)4n reaction and further neutron decay.
+
+ACCULINNA-2 facility, FLNR, JINR, produced the 26\,AMeV $^{8}$He beam with intensity $\approx10^{5}$\,pps.
+This beam was focused on the cryogenic gaseous deuterium 27\,K target with a temperature of 27\,K equipped with stainless steel and mylar windows.
+Initially, the experiment was dedicated to $^{7}$H studies, see Ref.\ \cite{Muzalevskii:2021}, but the detection system allowed to measure the product of the $^2$H($^8$He,$^6$Li)4n reaction and further neutron decay.
The employed detector system is widely described in Ref.\ \cite{Muzalevskii:2021}.
The beam particles were identified by two plastic scintillators, which allowed to measure the energy of the projectile from its time-of-flight (ToF).
%The particle identification (PID) of the beam was performed by the dE-ToF
%For the beam particle identification and its energy determination two plastic scintillators were used.
-The trajectories the beam projectiles were tracked by two pairs of multi-wire proportional chambers.
-The cryogenic target was filled with a deuterium gas at 27\,K of atmospheric pressure.
+The motion vector of were reconstructed by two pairs of multi-wire proportional chambers.
The special run with the empty target cell was conducted to estimate the background conditions, which had $\approx$16\% of the total $^8$He beam time.
Detection of the charged reaction products was realized by $\Delta E$-$E$ telescopes.
@@ -121,7 +122,7 @@ The latter will not also increase statistics but also will allow to study neutro
\section{Acknowledgement}
%Institute of Physics of Silesian University in Opava
-We also acknowledge the principal support of this work by the Russian Science
+We acknowledge the principal support of this work by the Russian Science
Foundation grant No.\ 22-12-00054. The authors are grateful to
Profs.\ Yu.Ts.\ Oganessian and S.N.\ Dmitriev for the long-term support and
development of this activity. We acknowledge important contribution of Prof.\
--
2.18.1