Gauge anomaly

In this diagram, two particles come in with momenta p₁ and p₂, they interact in some fashion, and then two particles with different momentum (p₃ and p₄) leave.

In theoretical physics, the Mandelstam variables are numerical quantities that encode the energy, momentum, and angles of particles in a scattering process in a Lorentz-invariant fashion. They are used for scattering processes of two particles to two particles. The Mandelstam variables were first introduced by physicist Stanley Mandelstam in 1958.

If the Minkowski Metric is chosen to be $\mathrm {diag} (1,-1,-1,-1)$, the Mandelstam variables $s,t,u$ are then defined by

• $s=(p_{1}+p_{2})^{2}=(p_{3}+p_{4})^{2}\,$
• $t=(p_{1}-p_{3})^{2}=(p_{2}-p_{4})^{2}\,$
• $u=(p_{1}-p_{4})^{2}=(p_{2}-p_{3})^{2}\,$

Where p₁ and p₂ are the four-momenta of the incoming particles and p₃ and p₄ are the four-momenta of the outgoing particles, and we are using Planck units (c=1).

s is also known as the square of the center-of-mass energy (invariant mass) and t is also known as the square of the four-momentum transfer.

Feynman diagrams

The letters $s,t,u$ are also used in the terms s-channel, t-channel, u-channel. These channels represent different Feynman diagrams or different possible scattering events where the interaction involves the exchange of an intermediate particle whose squared four-momentum equals $s,t,u$, respectively.

s-channel	t-channel	u-channel

For example the s-channel corresponds to the particles 1,2 joining into an intermediate particle that eventually splits into 3,4: the s-channel is the only way that resonances and new unstable particles may be discovered provided their lifetimes are long enough that they are directly detectable. The t-channel represents the process in which the particle 1 emits the intermediate particle and becomes the final particle 3, while the particle 2 absorbs the intermediate particle and becomes 4. The u-channel is the t-channel with the role of the particles 3,4 interchanged.

Details

High-energy limit

In the relativistic limit rest mass can be neglected, so for example,

$s=(p_{1}+p_{2})^{2}=p_{1}^{2}+p_{2}^{2}+2p_{1}\cdot p_{2}\approx 2p_{1}\cdot p_{2}\,$

because $p_{1}^{2}=m_{1}^{2}$ and $p_{2}^{2}=m_{2}^{2}.$ It is reminded that by relativistic limit one means that the momentum (speed) is so large that in the relativistic energy-momentum equation the energy becomes essentially the momentum norm (e.g. $E^{2}=\mathbf {p} \cdot \mathbf {p} +{m_{0}}^{2}$ becomes $E^{2}\approx \mathbf {p} \cdot \mathbf {p}$ ).

In summary,

$s\approx \,$	$2p_{1}\cdot p_{2}\approx \,$	$2p_{3}\cdot p_{4}\,$
$t\approx \,$	$-2p_{1}\cdot p_{3}\approx \,$	$-2p_{2}\cdot p_{4}\,$
$u\approx \,$	$-2p_{1}\cdot p_{4}\approx \,$	$-2p_{3}\cdot p_{2}\,$

Addition of

Note that

$s+t+u=m_{1}^{2}+m_{2}^{2}+m_{3}^{2}+m_{4}^{2}\,$

where $m_{i}$ is the mass of particle $i$.

Proof

To prove this, we need to use two facts:

• The square of a particle's four momentum is the square of its mass,

$p_{i}^{2}=m_{i}^{2}\quad \quad \quad \quad \quad \quad \quad \quad \quad \quad \quad (1)\,$

• And conservation of four-momentum,

$p_{1}+p_{2}=p_{3}+p_{4}\,$

$p_{1}=-p_{2}+p_{3}+p_{4}\quad \quad \quad \quad \quad \quad \quad (2)\,$

So, to begin,

$s=(p_{1}+p_{2})^{2}=p_{1}^{2}+p_{2}^{2}+2p_{1}\cdot p_{2}\,$

$t=(p_{1}-p_{3})^{2}=p_{1}^{2}+p_{3}^{2}-2p_{1}\cdot p_{3}\,$

$u=(p_{1}-p_{4})^{2}=p_{1}^{2}+p_{4}^{2}-2p_{1}\cdot p_{4}\,$

First, use (1) to re-write these,

$s=m_{1}^{2}+m_{2}^{2}+2p_{1}\cdot p_{2}\,$

$t=m_{1}^{2}+m_{3}^{2}-2p_{1}\cdot p_{3}\,$

$u=m_{1}^{2}+m_{4}^{2}-2p_{1}\cdot p_{4}\,$

Then add them

$s+t+u\,$	$=3m_{1}^{2}+m_{2}^{2}+m_{3}^{2}+m_{4}^{2}+2p_{1}\cdot p_{2}-2p_{1}\cdot p_{3}-2p_{1}\cdot p_{4}\,$
	$=m_{1}^{2}+m_{2}^{2}+m_{3}^{2}+m_{4}^{2}+2\left(m_{1}^{2}+p_{1}\cdot p_{2}-p_{1}\cdot p_{3}-p_{1}\cdot p_{4}\right)\,$
	$=m_{1}^{2}+m_{2}^{2}+m_{3}^{2}+m_{4}^{2}+2\left(m_{1}^{2}+p_{1}\cdot \left(p_{2}-p_{3}-p_{4}\right)\right)\,$

Then use eq (2) to simplify further,

$s+t+u\,$	$=m_{1}^{2}+m_{2}^{2}+m_{3}^{2}+m_{4}^{2}+2\left(m_{1}^{2}-p_{1}\cdot p_{1}\right)\,$
	$=m_{1}^{2}+m_{2}^{2}+m_{3}^{2}+m_{4}^{2}+2\left(m_{1}^{2}-m_{1}^{2}\right)\,$

So finally,

$s+t+u=m_{1}^{2}+m_{2}^{2}+m_{3}^{2}+m_{4}^{2}\,$

See also

• Feynman diagrams
• Bhabha scattering
• Møller scattering
• Compton scattering

References

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