Lead Projectile Fragmentation on Aluminum Target: Improved Experimental Results ()
1. Introduction
Nuclear projectile fragmentation at relativistic energies provides an insight into some aspects of nuclear structure, especially the peripheral structure of the nucleus. In central and peripheral nuclear collisions, the fragmentation process leads to the emission of fragments with a wide range of masses. Experimental results on fragmentation properties of relativistic energy projectiles are relevant for nuclear physics, cosmic ray physics and astrophysics. Fragmentation cross sections are required to understand and evaluate composition of the cosmic rays propagation through the interstellar medium [1,2]. At relativistic energy, projectile fragmentation on different targets has been studied by a number of authors using both active and passive detection techniques [3-8].
CR-39 (C12H18O7) nuclear track detectors are manufactured by Intercast Europe Co. of Parma Italy. These detectors have been used for the study of different projectiles and targets interaction at relativistic energy [9-13]. Previously, we have presented 158 A GeV fragmentation [10,11] studies on Bi and Cu targets using the most sensitive CR-39 track detector. In this paper, we present Pb projectile fragmentation on Al target using the welloptimized experiments with the experience of previous experiments. Optimized experimental etching conditions provided the improved results compared with our previous investigations in a way that odd-even effect has been observed in a clear and consistent manner over the observed range of fragments of 158 A GeV Pb nuclei (Z = 63 - 81) in comparison with our previous reports [10,11]. This is an important observation which is achieved through optimization of experimental conditions details of which are given in sections 2 and 3. Section 2 is about experimental detail and explains the methodology employed for detector calibration and calculation charge changing cross sections. Results are discussed in section 3 whereas the last section contains conclusions.
2. Experiments
A stack containing Al target sandwiched with CR-39 detector sheets of the size (10 cm × 10 cm × 1 mm) was exposed to 158A GeV Pb ions at SPS beam of CERN. The exposure was performed at normal incidence with a fluence of about 1500 ions/cm2. The total number of lead ions in the stack was about 7.8 × 104 distributed in eight spills. In the exposure stack four CR-39 sheets were placed upstream the target and almost 39 sheets downstream the target. In order to avoid multifragmentation, appropriate gaps were provided in the detectors placed downstream the target in the stack, size of the gaps was nearly 2 cm between the detector foils placed close to the target and gaps were increased as the stack length.
In order to scan, we selected one CR-39 sheet upstream the target and other two downstream the target (one close to the target and other from last pairs in the stack). These detectors were etched in 4 N KOH aqueous solution at 45˚C for 72 h.
In order to improve and implement appropriate etching conditions a considerable emphasis was given to the important factors contributing in the etching process, the concentration of active etching molecules in the etching solution an effective and continuous stirring was maintained using a calibrated motorized stirring system during the etching process to produce a sort of convection in the etching bath to avoid buildup etch products produced from detector surface in developing tracks. The variation in the temperature was not more than ±1˚C to maintain control and stability. Concentration of etchant was kept effectively constant under specific etching conditions by minimizing the water evaporation from the etching solution during the etching.
After etching process the beam ions and the fragments registered in the detector placed after the target appeared as etched cones on both sides of the detectors. The detectors were scanned using optical microscope at a magnification of 400 ×. Using the built-in cone height measuring unit of optical microscope the cone lengths of track events have been measured with an accuracy of ±1 m. Well optimized experimental procedures and precautions, especially for the chemical etching, were adopted throughout the experiments and track measurements. Bases of such procedures and precautions are described elsewhere in detail [11].
3. Results and Discussion
3.1. Charge Identification and Detector Calibration
The etched cones of vertically incident beam particles and the fragments are of circular shape and completely black in direct illumination. The background objects are shallow and appear as black circular objects with a brighter centre are not considered. Target fragments can be resolved based on their short range. The central brightness can be used to separate particle tracks from background. Figure 1 shows the distribution of cone height for beam ions and the fragments registered in a detector placed after the target. The ionizing particles traversing through an insulating material create a narrow path of intense damage on an atomic scale [12].
The damaged region in the detector can be revealed and enlarged by treating with a proper chemical reagent to become visible under an optical microscope. During the etching process, the track etch rate vT exceeds the bulk etch rate vB producing a conical etch-pit at the point
Figure 1. Average cone heights distribution of Pb ions and the fragments produced in interaction with the target observed using CR-39 detector placed after the Al target, arrows indicate charge (atomic number) assigned to peak.
of entrance and exit of the particle. The size and shape of such cones depend on the energy loss of the incident particle; the measurement of the cone base area or heights allows, through an appropriate calibration, to determine the characteristics of the particle.
The focused surface of the opening of the etch-pits looks like a dark, circular of well defined diameter. The CR-39 detectors, placed upstream the targets registered the total number of incident Pb ions and detectors placed after the target recorded both the survived Pb ions and the fragments produced in the interaction of Pb ions with the target. Since the beam exposure is normally incident to the detector surface, the beam ions and the fragments produced as a result of fragmentation almost maintain their longitudinal velocity along the direction of beam ions and a sequence of etch cones is produced on the subsequent detector surfaces.
At relativistic energies the base area of the post etching cones depends only on charge Z, therefore peaks of measured etched cone heights correspond to different charges. This method is applicable as long as the projectile peak and the fragment peaks are clearly separated. It is reported in [13] that the etched cone diameter is sensitive to low Z ions, and cone height to high Z ions. The average values of the cone heights distribution observed in both the detectors is displayed in the form of well separated peaks, which are assigned to a charge value 63 £ Z £ 82 by counting downward beginning with the beam peak Z = 82 (we assume the charge assigned to the fragment as the atomic number of the fragment. In reality, charge of the fragment can be lower than the atomic number Z in a particular case when fragments have lowered their energy and collected electrons from the target which reduces their charge from the maximum possible charge. For the simplicity the atomic number of fragments is shown in Figure 1.
The charge resolution is related to cone height resolution. In view of different units of these quantities relative charge resolution is equated to relative length resolution using the relation
(1)
where 
is the standard deviation in the length of individual peaks assigned to charge value. The plot of charge Z verses cone lengths L is shown in Figure 2. The ratio 
is the slope of the plot.
The energy deposited by the charged particle to form the latent track is the Restricted Energy Loss (REL).The response of the detectors to relativistic ions is characterized by the correlation of parameter
, and REL from the calibration curve. Since track etch rate vT is a function of REL ,which depends on the charge and energy of the incident projectile ion, for relativistic energy ions the REL remains approximately constant therefore, it is considered that the diameter and length of etched cone are function of ion charge only as reported by [14].
The cylindrical cone length L is related to etch rate ratio ‘p’ through the equation
(2)
where‘t’ is etching time. The track etch rate (
) of the
Figure 2. Correlation plot of the charges to the mean etched cone lengths measured in detector placed after the target.
cones produced in the detector can be calculated from the relation,
(3)
where L is the cone height, t is the etching time and 
is the bulk etch rate of the detector measured by the change in the thickness of the detector before and after etching of the detector. The refractive index of the CR-39 was experimentally determined and was used for the determination of the total height of cones.
For the resolution of higher charges the cone heights are associated with different charges. The charge values of fragments with almost identical 
are associated with specific REL values while the lengths are converted to ‘p’ values using Equation (3).
The relation between REL and ‘p’ is specific to the etching condition, because the value of ‘p’ is experimentally measured for the given etching conditions when unknown ion interacts on the detector, it is, therefore, possible to assign it an REL value. The REL vs. p graph as shown in Figure 3 constitute a calibration curve. The function REL defined as
(4)
For particles with ßc > 10–2 c, the REL is a fraction of the electronic energy loss, leading to δ rays with energies lower than Emax, with Emax= 200 eV for CR-39 [15]. If the REL of a particle passing through a stack of detectors
Figure 3. The calibration curve of reduced etch rate p vs REL value. The uncertainties in bulk etch rate measurement yield error in the reduced etch rate p. The points are the experimental data and the line is the fit to the data point. The fitted equation is valid in the REL range ~ 4200 - 7000 MeV cm2/g under present etching conditions.
is constant along its trajectory and the same etching conditions are applied to all the detectors in the stack, the track etching rate vT is constant and identical cones are formed on all crossed detector surfaces.
Figure 4 shows the track length and charge resolutions for the fragments of 158 A GeV Pb projectiles produced in collisions of the projectile beam with Al target. The dotted horizontal line shows the mean values of track length and charge resolutions. We have also analyzed the distributions of track length (Figure 5(a) and charge resolutions (Figure 5(b)). Values of 
and squared regression coefficients R2 for the Gaussian fits on both distributions are given in the respective plots in Figure 4. Peak values of the Gaussian fits on track length and charge resolutions in Figure 4 agree well with the respective arithmatic mean values in Figure 4.