What is the Invariant Mass of Two Perpendicular Photons?

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Discussion Overview

The discussion revolves around the invariant mass of two photons traveling perpendicular to each other, exploring the implications of their momentum and energy in different frames of reference. Participants examine theoretical frameworks and mathematical formulations related to invariant mass in the context of special relativity.

Discussion Character

  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants propose that the invariant mass of a system of two perpendicular photons should be zero, but express hesitation about whether this is always the case.
  • Others argue that only a system of photons traveling in the same direction has zero invariant mass, suggesting that introducing a photon in a different direction results in a non-zero invariant mass.
  • A participant outlines a general method for finding invariant mass by choosing an inertial frame with zero total momentum, but another participant challenges the applicability of this method when the invariant mass is zero.
  • One participant presents a mathematical formulation for the invariant mass of two photons, emphasizing the importance of the angle between their momenta and correcting the equation to include the square of energy.
  • Another participant questions a specific mathematical step regarding the sine function in the derivation, suggesting a potential error in the formulation.
  • There is a discussion about the equivalence of different mathematical expressions for the invariant mass, with some participants confirming the correctness of their formulations.

Areas of Agreement / Disagreement

Participants express differing views on the invariant mass of two perpendicular photons, with no consensus reached on whether it is always zero or if it can be non-zero depending on the configuration of the photons.

Contextual Notes

Some mathematical steps remain unresolved, particularly regarding the correct formulation of the invariant mass and the implications of different angles between the photon momenta. The discussion highlights the complexity of applying theoretical frameworks to specific cases.

rashida564
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TL;DR
Two photons travels perpendicular to each other find their invariant mass
I think since Esystem=(PsystemC)^2 + (Minvariant C^2)^2. Then the invariant mass of the system should be zero, but I am hesitated with this is it always the case that photon that travels perpendicular to each other have zero invariant mass
 
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rashida564 said:
Summary:: Two photons travels perpendicular to each other find their invariant mass

I think since Esystem=(PsystemC)^2 + (Minvariant C^2)^2. Then the invariant mass of the system should be zero, but I am hesitated with this is it always the case that photon that travels perpendicular to each other have zero invariant mass
Only a system of photons that travel in the same direction has zero invariant mass. As soon as you add a single photon traveling in a different direction, the invariant mass will be non-zero.

Edit: Your equation should also contain E^2, not E.
 
The general recipe for finding the invariant mass of a system works here: Choose an inertial frame in which the total momentum is zero; the energy in that frame is the rest energy; invariant mass is then calculated from ##E=mc^2##.

If the two photons are moving in the same direction then there is no frame in which the momentum is zero and then this recipe cannot be used.
 
Nugatory said:
The general recipe for finding the invariant mass of a system works here: Choose an inertial frame in which the total momentum is zero; the energy in that frame is the rest energy; invariant mass is then calculated from ##E=mc^2##.

I disagree, since it is not applicable when the invariant mass is zero, it cannot be a general recipe. Instead, I would compute the invariant mass from the relation provided by the OP (apart from the missing square), ##E^2 = (\vec pc)^2 + m^2 c^4##. For the two-photon system, it is simple enough to compute the total energy and the momenta given the photons' directions and energies.
 
The total mass of a system is given by
$$m^2 c^2=P_{\mu} P^{\mu}=s,$$
where ##P_{\mu}## is the total momentum. For two photons you have
$$s=(q_1+q_2)^2=q_1^2 + q_2^2 + 2 q_1 \cdot q_2=2 q_1 \cdot q_2$$
From this you get
$$m^2=\frac{2}{c^2} q_1 \cdot q_2.$$
Now
$$q_1=(|\vec{q}_1|,\vec{q}_1), \quad q_2 = (\vec{q}_2,\vec{q}_2)$$
and thus [EDIT: Corrected in view of #6]
$$m^2 = \frac{2}{c^2} (|\vec{q}_1| |\vec{q}_2|-\vec{q}_1 \cdot \vec{q}_2)=\frac{2}{c^2} |\vec{q}_1| |\vec{q}_2| (1-\cos \vartheta),$$
where ##\vartheta \in [0,\pi]## is the angle between ##\vec{q}_1## and ##\vec{q}_2##. Thus you always get a well defined ##m^2>0## always.
 
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vanhees71 said:
The total mass of a system is given by
...
and thus
$$m^2 = \frac{2}{c^2} (|\vec{q}_1| |\vec{q}_2|-\vec{q}_1 \cdot \vec{q}_2)=\frac{2}{c^2} |\vec{q}_1| |\vec{q}_2| \sin^2 \vartheta,$$
where ##\vartheta \in [0,\pi]## is the angle between ##\vec{q}_1## and ##\vec{q}_2##. Thus you always get a well defined ##m^2>0## always.
Shouldn’t sin2 be (1 - cos ), i.e. not squared, in the last step? Note, with yours, parallel and anti parallel would be the same, which is incorrect.

Otherwise, love the derivation.
 
##\frac{4}{c^2}|\vec q_1||\vec q_2|\sin^2 \frac{\vartheta}{2}##?
 
SiennaTheGr8 said:
##\frac{4}{c^2}|\vec q_1||\vec q_2|\sin^2 \frac{\vartheta}{2}##?
That’s, of course, equivalent to what I wrote.
 
Yes, just guessing that that's what @vanhees71 meant to write.
 
  • #10
Of course you are right. It's a typo (I've corrected it also in the original posting).
 

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