Representations of the Poincare group

In summary, relativistic quantum field theories have unitary representations of the Poincare group for all particles. For massive particles, there are scalar, spinor, and vector representations with a defined spin and dimension. For massless particles, spin is replaced by helicity with a dimension of 1 and helicity values of +1 and -1. However, for tachyons with m² < 0, their energy would require them to move faster than the speed of light, making them unphysical. This can be seen in a simple model of quantizing Klein-Gordon scalar fields. The traditional argument against tachyons is that they violate causality.
  • #1
tom.stoer
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Hello,

in relativistic quantum field theories all particles are members of (unitary) representations of the Poincare group. For massive particles m² > 0 one gets the usual scalar / spinor / vector representations with spin J = 0, 1/2, 1, 3/2, ... and dim. rep. = 2J+1. For massless particles m² = 0 the spin is no longer defined in the usual sense (angular momentum in rest frame does not make sense) and is replaced by helicity. Again one finds the usual representations with dim. rep. = 1 and helicity = +1 and -1, respectively.

Question: what happens for m² < 0? how do the representations look like and why are they unphysical?
 
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  • #2
These are the famous tachyons. As m is the energy in the rest frame, tachyons would have to move with speeds higher than c for their energy to be real valued.
 
  • #3
You can try and go through a simple model where m^2<0 (for instance try quantizing the Klein-Gordon scalar fields with this assumption). All sorts of odd things occur. This was a final exam problem in my QFT class.

An interesting read of the simplest tachyon field is by http://prola.aps.org/abstract/PR/v159/i5/p1089_1. You might find it enlightening.

But to answer your question about why they are unphysical- the traditional argument is they violate causality.
 

1. What is the Poincare group?

The Poincare group is a mathematical concept that represents the symmetries of Minkowski space, which is a mathematical model of space-time in physics. It includes translations, rotations, and boosts (Lorentz transformations) that preserve the interval between events in space-time.

2. Why are representations of the Poincare group important?

Representations of the Poincare group are important because they allow us to understand how physical quantities and objects behave under the symmetries of space-time. This is crucial in the study of fundamental particles and their interactions, as well as in the development of theories such as special relativity and quantum field theory.

3. How are representations of the Poincare group classified?

Representations of the Poincare group are classified by their dimension and by their behavior under the symmetries of space-time. They can be either finite-dimensional or infinite-dimensional, and can be further classified as either unitary or non-unitary representations.

4. What is the significance of the spinor representation in the Poincare group?

The spinor representation is significant because it describes how spin-1/2 particles, such as electrons, transform under the symmetries of space-time. This representation is important in understanding the behavior of particles at high speeds and in the development of quantum field theories.

5. How are representations of the Poincare group used in physics?

Representations of the Poincare group are used in physics to study the behavior of particles and fields under the symmetries of space-time. They are also used in the development of theories such as special relativity and quantum field theory, and in the prediction and interpretation of experimental results in particle physics and cosmology.

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