“Mandelstam variables”的意思、由来-开放百科全书

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Mandelstam variables

释义

Feynman diagrams
Details
Relativistic limit Sum Proof
See also
References

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 , the Mandelstam variables are then defined by

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 relativistic 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 are also used in the terms s-channel (space-channel), t-channel (time-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 , 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

Relativistic limit

In the relativistic limit, the momentum (speed) is large, so using the relativistic energy-momentum equation, the energy becomes essentially the momentum norm (e.g. becomes ). The rest mass can also be neglected.

So for example,

because and

Thus,

Sum

Note that

where is the mass of particle .

Proof

To prove this, we need to use two facts:

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

And conservation of four-momentum,

So, to begin,

Then adding the three while inserting squared masses leads to,

Then note that the last four terms add up to zero using conservation of four-momentum,

So finally,

References

{{cite journal | last = Mandelstam | first = S. | title = Determination of the Pion-Nucleon Scattering Amplitude from Dispersion Relations and Unitarity | journal = Physical Review | volume = 112 | year = 1958 | pages = 1344 | url = http://dbserv.ihep.su/hist/owa/hw.part2?s_c=MANDELSTAM+1958 | archive-url = https://web.archive.org/web/20000528212400/http://dbserv.ihep.su/hist/owa/hw.part2?s_c=MANDELSTAM+1958 | dead-url = yes | archive-date = 2000-05-28 | doi = 10.1103/PhysRev.112.1344 | bibcode = 1958PhRv..112.1344M | issue = 4 }}
{{cite book |author1=Halzen, Francis |authorlink1 = Francis Halzen |author2=Martin, Alan | authorlink2 = Alan Martin (physicist) |title=Quarks & Leptons: An Introductory Course in Modern Particle Physics | publisher=John Wiley & Sons | year=1984 | isbn=0-471-88741-2}}
{{cite book | author=Perkins, Donald H. | title=Introduction to High Energy Physics |edition=4th | publisher=Cambridge University Press | year=2000 | isbn=0-521-62196-8 }}

2 : Kinematics (particle physics)|Quantum field theory

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Feynman diagrams

Details

Relativistic limit

Sum

Proof

See also

References