Understand
I consider the two-body decay of a particle at a hadron collider into a visible and an invisible particle, generalizing $W \to e \nu$, where the masses of the decaying particle and the invisible decay particle are, {\em a priori}, unknown.
- I prove that the transverse mass, when maximized over possible kinematic configurations, can be used to determine both of the unknown masses.
- I argue that the proof can be generalized to cover cases such as decays of pair-produced superpartners to the lightest, stable superpartner at the Large Hadron Collider.
Built on
Phil. Mag. 44
R. H. Dalitz, · 1954
Earlier work this paper cites.
Similar
Phys. Lett. B122
G. Arnison et al · 1983
Cited alongside, same era.
W. S. Cho, K. Choi, Y. G. Kim and C. B. Park, arXiv:0709.0288 [hep-ph]
Cited in the paper.
For another possible method of mass determination, see H. C. Cheng, J. F. Gunion, Z. Han, G. Marandella and B. McElrath,
Cited in the paper.
Then
Phys. Lett. B463
C. G. Lester and D. J. Summers, · 2003
Later among the works it cites.
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