with the transverse momentum vector ${\vec {p}}_{T}=(p_{x},p_{y})$. It is easy to see that for vanishing mass ($m=0$) the three quantities are the same: $E_{T}=p_{T}=m_{T}$.
The transverse mass is used together with the rapidity, transverse momentum and polar angle in the parameterization of the four-momentum of a single particle:

These are also the definitions that are used by the software package ROOT, which is commonly used in high energy physics.

Transverse mass in two-particle systemsedit

Hadron collider physicists use another definition of transverse mass (and transverse energy), in the case of a decay into two particles. This is often used when one particle cannot be detected directly but is only indicated by missing transverse energy. In that case, the total energy is unknown and the above definition cannot be used.

where $\phi$ is the angle between the daughters in the transverse plane.
The distribution of $M_{T}$ has an end-point at the invariant mass $M$ of the system with $M_{T}\leq M$. This has been used to determine the $W$ mass at the Tevatron.

Referencesedit

J.D. Jackson (2008). "Kinematics" (PDF). Particle Data Group. - See sections 38.5.2 ($m_{T}$) and 38.6.1 ($M_{T}$) for definitions of transverse mass.

J. Beringer; et al. (Particle Data Group) (2012). "Review of Particle Physics". Physical Review D. 86 (1): 010001. Bibcode:2012PhRvD..86a0001B. doi:10.1103/PhysRevD.86.010001. hdl:10481/34377. - See sections 43.5.2 ($m_{T}$) and 43.6.1 ($M_{T}$) for definitions of transverse mass.