Information entropy and Zipf's law in the field of information theory have been used for studying the disassembly of nuclei in the framework of the isospin dependent lattice gas model and molecular dynamical model. We found that the information entropy in the event space is maximum at the phase transition point and the mass of the cluster show exactly inversely to its rank, i.e. Zipf's law appears. Both novel criteria are useful in searching the nuclear liquid gas phase transition experimentally and theoretically. Hot nuclei can be formed in energetic heavy ion collisions (HIC) and may be highly excited. They deexcite by different decay modes, such as multifragmentation. Experimentally, this kind of multifragment emission was observed to evolve with beam energy (excitation energy, or nuclear temperature, ...). Multiplicity, N imf , of intermediate mass fragment (IMF) rises with the beam energy, reaches a maximum, and finally falls to lower value. This phenomenon of the rise and fall of N imf may be related to the liquid gas phase transition in nuclear matter [1]. The onset of multifragmentation probably indicates the coexistence of liquid and gas phases. The mass distribution of IMF distribution can be expressed as power law with parameter τ . The minimum of τ , τ min , occurs when the liquid gas phase transition takes place [2]. However, τ min can also reveal at supercritical densities along the Kertész line [3] and at some subcritical densities at lower temperature [4]. So it is not possible to determine the phase transition only from N imf and τ min .On the other hand, experimentalists measured the nuclear caloric curves, i.e. the relationship between nuclear temperature and the excitation energy. He-Li isotopic temperature from Albergo thermometer [5] for projectilelike Au spectators seems to exhibit a temperature plateau in the excitation energy range of 3 to 10 MeV/u [6]. This plateau was taken as an indication for a first order nuclear liquid gas phase transition. However, due to the changing mass of Au spectators with excitation energy and the side-feeding effect to measured He-Li isotopic temperature, this conclusion is questionable [7]. Nuclear caloric curves were also surveyed by several groups [8]. However, unfortunately, the sharp signature of liquid gas phase transition in macroscopic systems may be smoothed and blurred due to the small numbers of nucleons in nuclei, and/or the difficulty to perform a direct comparison between the measured "apparent" temperature and the "real" temperature interferes obtaining the real nuclear caloric curve. These factors hamper the * Present Address: Cyclotron Institute, Texas A & M University, College Station, Texas 77801 reaching of a definite conclusion on liquid gas phase transition in nuclei.The extraction of critical exponents and the study of critical behavior in finite-size systems were attempted in [9] and were followed by controversial debates [10]. In this context, it is necessary and meaningful to search for some novel signatures to characterize the nuc...