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REACTIONS WITH LIGHT NUCLEI
Nuclear reactions group: Cracow - Kiev - Warsaw
Andrzej Sołtan Institute of Nuclear Studies, ul. Hoża 69, 00-681 Warsaw, Poland
K.Rusek, S. Yu. Mezhevych
Institute of Nuclear Research, Prospect Nauki 47, 03680 Kiev, Ukraine
A.T.Rudchik, V.M. Kyryanchuk, A.V. Mokhnach,
O.A. Momotyuk, Val.M. Pirnak, O. Ponkratenko, V. Romanyshyn,
A.A. Rudchik
H.Niewodniczański Institute of Nuclear Physics, ul. Radzikowskiego 152,
31-342 Cracow, Poland
A. Budzanowski, B.Czech, S.Kliczewski, R. Siudak, I.Skwirczyńska
Kharkiv State University, 61077 Kharkiv, Ukraine
E.Koshchy
Heavy Ion Laboratory of Warsaw University, ul. Pasteura 5A, 02-093 Warsaw, Poland
T. Czosnyka, J. Choiński, A. Stolarz
Military University of Technology, ul. Kaliskiego 2, 00-908 Warsaw, Poland
L.Głowacka
Contact: Krzysztof Rusek, Krzysztof.Rusek(at)fuw.edu.pl
Nuclear reactions are the main source of experimental information
on the structure of nuclei, mechanisms of nuclear processes and
properties of nucleus-nucleus interaction. This information, for
instance, may be obtained from the theoretical analysis of angular
distributions of the measured reaction products. The present
theoretical models used for such an analysis are parameterized, and
the parameters describing nuclear structure, mechanisms of reactions
and nucleus-nucleus interactions are closely related to each
other. Therefore, for the reliable determination of these parameters a
broad set of experimental data is demanded for reactions with
different nuclei in the entrance and exit channels and at different
energies. Thus, obtaining new experimental data remains an urgent task
in nuclear physics.
We perform experiments with the 10B3+, 11B2+,
12C2+, 14N3+ and 18O4+
ion beams, accelerated at Warsaw Cyclotron
U-200P up to an energy of 5-10 MeV/A, which are scattered from the
6,7Li, 9Be, 12,13,14C targets.
The experimentally obtained angular
distributions of the reaction products are analyzed by means of the
coupled-reaction-channels method, and the parameters describing the
structure of the nuclei, mechanisms of nuclear reactions and
nucleus-nucleus interactions are deduced. We start with the
investigation of the elastic and inelastic scattering in order to
obtain a reliable set of optical model parameters describing the
nucleus-nucleus interaction in the entrance channel, which are then
employed in the calculations of different transfer processes leading
to the production of the experimentally observed nuclei in the exit
reaction channels.
EXPERIMENTAL SETUP "SYRENA" AT WARSAW CYCLOTRON
The setup is located in section "B" of the experimental hall of the
Heavy Ion Laboratory of Warsaw University. The picture of the
scattering chamber is shown in Fig.1. In the center of the chamber a
frame with targets is fixed on a movable rod. The scattering chamber
has two movable platforms on which the detectors are
mounted. Three-channel ΔE-E spectrometer, with the gas-filled
ionization chamber serving as the ΔE - detector, is mounted on the
lower platform (see Fig.2). At the backward side of the ionization
chamber silicon E-detectors (approx. 500 μm), stopping the reaction products,
are mounted. Angular separation between the channels is 9.5o. On the
upper platform the second ΔE-E spectrometer consisted of the silicon
ΔE (approx. 60 μm) and E (approx. 500 μm) detectors is placed.
Figure 1: Scattering chamber of the experimental setup "SYRENA".
Figure 2: The scattering chamber in the inside.
In Fig.3 a typical two-dimensional energy spectrum of the 7Li(12C,X)
reaction products at Elab(12C) = 115 MeV registered at Θlab
= 15o by
the silicon ΔE-E spectrometer is shown. Very good energy resolution of
the detectors leads to a good separations between Li, Be, B, C and N
isotopes.
Figure 3: ΔE-E spectrum of the
7Li(12C,X) reaction products.
RESULTS OBTAINED USING THE BEAM FROM THE WARSAW CYCLOTRON
So far we have published five papers (see the list below). They
contain new experimental data sets as well as many interesting
conclusions drawn from the data analyses. As an example we present in
Fig. 4 the angular distribution of the inelastically scattered 11B
from 14C target leading to the excitation of the 7.012 MeV (2+)
excited state of 14C. The curves present results of the
coupled-channels calculations. Collective model of the target nucleus
was assumed. The short dashed curve was obtained assuming the positive
quadrupole deformation (β2 = +0.2) of 14C,
while the solid curve was
obtained with the negative quadrupole deformation (β2 = -0.2.).
Figure 4: The results of the calculations compared to the experimental data.
BIBLIOGRAPHY
(The experimental data obtained at Warsaw Cyclotron serves as the
experimental material for four PhD theses as well as two
DSc dissertations)
- A.T.Rudchik, A.Budzanowski, V.K.Chernievsky, B.Czech, L.Glowacka,
S.Kliczewski, A.V.Mokhnach, O.A.Momotyuk, S.E.Omelchuk, V.M.Pirnak,
K.Rusek, R.Siudak, I.Skwirczynska, A.Szczurek, L.Zemlo,
The 11B + 12C Elastic and Inelastic Scattering at
Elab(11B) = 49 MeV and Energy
Dependence of the 11B + 12C Interaction,
Nucl.Phys. A695, 51 (2001)
- S.Yu.Mezhevych, K.Rusek,
Quadrupole deformation of 11B (3/2-,
5.02 MeV) excited states from 11B + 12C scattering,
Acta Phys.Pol. B34, 2415 (2003)
- A.T.Rudchik, V.M.Kyryanchuk,
A.Budzanowski, V.K.Chernievsky, B.Czech, T.Czosnyka, A.V.Glowacka,
S.Kliczewski, E.I.Koshchy, S.Yu.Mezhevych, A.V.Mokhnach, K.Rusek,
S.B.Sakuta, R.Siudak, I.Skwirczynska, A.Szczurek, L.Zemlo,
Mechanism of large angle enhancement of the 9Be+11B scattering,
Nucl.Phys. A714, 391 (2003)
- S.Yu.Mezhevych, K.Rusek, A.T.Rudchik,
A.Budzanowski, V.K.Chernievsky, B.Czech, J.Choinski, L.Glowacka,
S.Kliczewski, E.I.Koshchy, V.M.Kyryanchuk, A.V.Mokhnach, A.A.Rudchik,
S.B.Sakuta, R.Siudak, I.Skwirczynska, A.Szczurek, L.Zemlo,
The 13C +
11B elastic and inelastic scattering and isotopic effects in the
12,13C + 11B scattering, Nucl.Phys. A724, 29 (2003)
- V.M.Kyryanchuk, A.T.Rudchik, A.Budzanowski, V.K.Chernievsky,
T.Czosnyka, B.Czech, L.Glowacka, S.Kliczewski, E.I.Koshchy,
S.Yu.Mezhevych, A.V.Mokhnach, K.Rusek, S.B.Sakuta, R.Siudak,
I.Skwirczynska, A.Szczurek, L.Zemlo,
One-nucleon transfer reaction
9Be(11B, 10B)10Be and optical potential for the
10B + 10Be
interaction,
Nucl.Phys. A726, 231 (2003)
- S.Yu.Mezhevych, K.Rusek,
A.T.Rudchik, A.Budzanowski, B.Czech, J.Choinski, L.Glowacka,
S.Kliczewski, E.I.Koshchy, V.M.Kyryanchuk, A.V.Mokhnach, A.A.Rudchik,
S.B.Sakuta, R.Siudak, I.Skwirczynska, A.Szczurek,
Structure of 14C
from 11B + 14C scattering, submitted to Nucl.Phys. A
- A.A.Rudchik,
A.T.Rudchik, A.Budzanowski, A.Szczurek, B.Czech, T.Czosnyka,
J.Choinski, L.Glowacka, S.Kliczewski, E.I.Koshchy, S.Yu.Mezhevych,
A.V.Mokhnach, O.A.Momotyuk, Val.M.Pirnak, R.Siudak, I.Skwirczynska,
Mechanism of 12C(11B,15N)8Be
reaction and 8Be + 15N optical model
potential, submitted to Eur. Phys. J. A
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