Proof. [05AP]
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Proof.
Let be the decomposition of into prime cycles and for each let be the irreducible components of with . Then is the decomposition of into prime cycles. Furthermore, the intersection of any two irreducible components of does not contain a Shilov point as it is of lower dimension and hence does not meet the support of the measures of interest. By linearity in the irreducible components we may therefore assume that and are irreducible and reduced. Let be a formal model of with reduced special fibre on which there exist formal models of . Let be a formal model of which exists by paracompactness of , see Remark 3.2. After possibly blowing up, the inclusion induces a morphism ([Bos14, Theorem 8.4.3]). Let . As both measures are discrete it is enough to show that they have the same mass at . Let denote the relative interior of over in the sense of [Ber93, 1.5]. If then by [Ber93, Proposition 1.5.5 (ii)]. Conversely if then there exists an affinoid neighbourhood of in such that is in the relative interior of over . But is also a neighbourhood of in as and therefore . Hence if and only if . If this is not the case then by definition of the measures and Corollary A.4, both of them are zero at . So assume that . Choose a locally finite cover of by open affine formal subschemes and let be the union of all which contain . Then is an open and quasi-compact formal subscheme of . Analogously choose a cover of by open affine formal subschemes. As is quasi-compact, there is a finite subcover of it. Let be the union of the sets in this subcover and add all with . Then also is an open and quasi-compact formal subscheme of and induces a morphism . By [BL93, Corollary 5.4] there is an admissible formal blowing up such that the induced morphism is an open immersion.
Let be an irreducible component of with corresponding divisorial point . Then by definition and hence we may calculate the mass of at using . By Proposition 4.5 iii) we may also use . So let be the irreducible component of corresponding to . Since we see that is an irreducible component of . Additionally, by Corollary A.4, and are proper and hence and it is an irreducible component of . It’s image in is a proper irreducible component of and hence also an irreducible component of . By the same argumentation as above we may use instead of to calculate the mass of at . This shows that the mass of the two measures is equal at in this case.
Conversely, if is an irreducible component of with corresponding divisorial point then by definition. Again we may use to calculate the mass at and we denote the corresponding irreducible component by . Then the closure of in is an irreducible component of with corresponding divisorial point and hence by the above . Therefore and coincide at .
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