Geometrically frustrated magnetism (GFM) occurs in systems where magnetic cations (spins) are located on a lattice with a triangular geometry and there are antiferromagnetic interactions among them, such that the three neighbouring spins on the triangle cannot be simultaneously antiparallel to each other. The large ground state degeneracy of such systems makes them an interesting platform explore the possible ground states and their entanglements. This proposal seeks to establish if spin ordering occurs in the frustrated systems YCa3(MO)3(BO3)4 (M = Ti3+ and Fe3+) that contain a 2D kagomé type lattice at very low temperatures.