We have measured the specific heat, C, of the easy-axis triangular lattice antiferromagnet CsNiCb in order to investigate the critical behavior associated with a multicritical point when the chiral symmetry is induced by an external magnetic field B. Critical exponents a determined from C are close to zero for two successive zero-field transitions, while a =0.25 ±0.08 near the multicritical point at 7^ ~ 4.48 K and BM « 2.25 T, and a =0.37 ±0.08 at the high-field phase boundary (Z?=6 T) far away from BMThe observed crossover from ordinary XY behavior for B < BM to n =3 chiral behavior at BM and finally to n =2 chiral behavior for B^>BM is in very good agreement with recent theoretical predictions.PACS numbers: 75.40.Cx, 65.40.Hq, 75.50.Ee The critical behavior near second-order phase transitions is described by a set of critical exponents. These are, e.g., a, /3, /, and v, for the specific heat, the order parameter, the susceptibility, and the correlation length, respectively. The renormalization group theory suggests that for short-range interaction all second-order phase transitions should belong to universality classes which are characterized only by the dimensionality of the system, d, and the number of components of the order parameter, n. Each universality class is associated with certain values of the critical exponents. The universality hypothesis has been well established and experimentally confirmed. Recently Kawamura pointed out that not only n is relevant, but the complete symmetry of the order parameter [1], This leads to new universality classes for magnetic systems which exhibit certain noncollinear spin structures characterized by a new degree of freedom, the chirality. These chiral universality classes have critical exponents that differ remarkably from the exponents [2] of ordinary three-dimensional universality classes. The difference is largest for a, which has a value close to zero for the conventional classes while systems with chirality have rather large positive values leading to distinctly different forms of the specific-heat anomaly at the critical temperature.Magnetic structures with chiral degeneracy are commonly found in hexagonal ABX3 compounds, where the magnetic B ions form chains along the c axis and a triangular lattice in the basal plane. The intrachain coupling in these substances is usually much larger than the interchain coupling. This gives rise to a quasi-one-dimensional magnetic behavior in an intermediate temperature range, while at low temperatures the small interchain coupling leads to three-dimensionally ordered states. In the case of antiferromagnetic coupling, the triangular spin arrangement essentially causes a noncollinear magnetic structure due to frustration effects. If the anisotropy of the magnetic ions is of easy-plane type CYF-like), the spins form a 120° structure in the basal plane, and the antiferromagnetic phase transition belongs to the n = 2 chiral universality class, whereas for systems without single-ion anisotropy, the transition is governed by th...