Associated with the Bondi coordinates is a (Bondi) null tetrad system, (). The first tetrad vector is the tangent to the geodesics of the constant null surfaces given by [44]
The second null vector is normalized so that: In Bondi coordinates, we have [44] for functions and to be determined, and with and . At , is tangent to the null generators of .The tetrad is completed with the choice of a complex null vector , which is itself orthogonal to both and , initially tangent to the constant cuts at and parallel propagated inward on the null geodesics. It is normalized by
Once more, in coordinates, we have [44] for some and to be determined. All other scalar products in the tetrad are to vanish.With the tetrad thus defined, the contravariant metric of the spacetime is given by
In terms of the metric coefficients , , , and , the metric can be written as: Thus, the spacetime metric is determined from the metric coefficients.There remains the issue of both coordinate and tetrad freedom, i.e., local Lorentz transformations. Most of the time we work in one arbitrary but fixed Bondi coordinate system, though for special situations more general coordinate systems are used. The more general transformations are given, essentially, by choosing an arbitrary slicing of , written as with labeling the slices. To keep conventional coordinate conditions unchanged requires a rescaling of . It is also useful to be able to shift the origin of by with arbitrary .
The tetrad freedom of null rotations around , performed in the neighborhood of , will later play a major role. For an arbitrary function on , the null rotation about the vector [44] is given by
Eventually, by the appropriate choice of the function , the new null vector, , can be made into the tangent vector of an asymptotically shearfree NGC.
The second type of tetrad transformation is the rotation in the tangent plane, which keeps and fixed:
This latter transformation provides motivation for the concept of spin weight. A quantity is said to have spinweight if, under the transformation, Equation (17), it transforms asAn example would be to take a vector on , say , and form the spinweightone quantity, .
Comment: For later use we note that has spin weight, .
For each , spin functions can be expanded in a complete basis set, the spin harmonics, or spin tensor harmonics, .
A third tetrad transformation, the boosts, are given by
These transformations induce the idea of conformal weight, an idea similar to spin weight. Under a boost transformation, a quantity, , will have conformal weight ifSphere derivatives of spinweighted functions are given by the action of the operators and its conjugate operator , defined by [17]
where the function is the conformal factor defining the sphere metric,

most often taken as

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