  We consider localized anomalies in six dimensional Z_n orbifolds. We give a
very simple expression for the contribution of a bulk fermion to the fixed
point gauge anomaly that is independent of the order n of the orbifold twist.
We show it can be split into three terms, two of which are canceled by bulk
fermions and Green-Schwarz four forms respectively. The remaining anomaly
carries an integer coefficient and hence can be canceled by localized fermions
in suitable representations. We present various examples in the context of
supersymmetric theories. Also we point out that the six-dimensional
gravitational symmetries generally have localized anomalies that require
localized four-dimensional fields to transform nontrivially under them.
