Again, one can see that T α α β β , as defined above, form s p ( 2 ) -generators and rotate properly q α α . At Q = 0 we get back to the undeformed oscillators. In fact, q α α and T α α β β form the generators of the Lie superalgebra o s p ( 1 | 2 ) , where q α α should be viewed as odd generators. Then, { q α α , q β β } = − − 4 i T α α β β is the part of the defining relations of o s p ( 1 | 2 ) . One (or two) copies of the deformed oscillator relations form a part of the Vasiliev equations where the generators are replaced with fields and the commutation relations are imposed as field equations.