The charge distribution of nuclear fragments for the nonfissile events of ^^'U at 0.96A GeV in nuclear emulsion is fitted with a power law. The method of scaled factorial moments is used to study fluctuations in the nuclear fragmentations. An intermittent behavior is found in the data, but no clear evidence of critical phenomenon is observed in nuclear fragmentation.PACS numbers: 24.60.Ky The recent studies of intermittency 111 in particle and nuclear collisions have revealed a quite fruitful field of research, and in fact the study of fluctuations has led to interesting insights on physical phenomena. Moreover, the intermittency analysis in terms of scaled factorial moments in relation with percolation models has been shown to be relevant in the study of the nuclear multifragmentation process [2]. In nuclear collisions at lower bombarding energies (<\A GeV) particle production is strongly suppressed and nuclear breakup into fragments dominates. Fragment-size distributions exhibit similar features to those known in percolation models [3]. Thus heavy-ion collisions offer a unique opportunity to study new phases of nuclei. One phase is of a high-density high-temperature region around the quark-gluon plasma (hadron phase transition or a thermal transition at equilibrium). The other phase is the low-density moderatetemperature region near the liquid-gas phase transition, but not at equilibrium-a nonthermal process. One can study the transition by looking at the distribution in composition of the final products. Here we shall look at the nonthermal process.In 1984, we did an analysis of nuclear interactions produced [4] in emulsion from ^^^U projectile at 0.96A GeV, in which 51% of all the 894 interactions were due to lissionlike fragments with a cross section of a^ ==1755 ± 82 mb. Recently, considerable interest has centered around the idea of nuclear multifragmentation, so our interest in the present Letter is to analyze the remaining nonfissile events which broke up into multifragments. When a ^^^U ion passes through the emulsion detector, the interactions in this medium were recorded up to ~ 2.7 cm (corresponding to energy between 960 and 240), where various processes are competing which give rise to different charge spectra of the projectile fragments (PFs). The energy of the produced PFs is high enough to distinguish them easily from the target fragments [5]. In each event the charges of these projectile fragments were determined by a combination of different methods which included grain density, gap density, <5-ray counting, relative track widths, etc. [4]. For projectile fragments of heavy charges which stopped in the stack, we used relations between their thin down track length and the widths [6] which were developed from the data of standard stopping tracks by drawing the profile of their last (150-1000 pm) thin down track lengths with the help of a special Leitz ''discussion tube" and comparing them with the profiles of unknown tracks of different charges. A heavy fragment here is defined as a cluster w...