Feynman Diagram HoodieTWO IN, ONE PHOTON, TWO OUT | Pixelated Physics
Feynman Diagram Hoodie – TWO IN, ONE PHOTON, TWO OUT | Pixelated Physics
- Color
- Black
- Size
- S–5XL
- Made
- To order · shipping times
An electron and a positron meet and annihilate. What comes out is a muon and an antimuon. The tree-level Feynman diagram for e⁺e⁻ → γ* → μ⁺μ⁻, wrapped in its exact 1 + cos²θ angular distribution. Two in, two out. Pixel-art unisex hoodie in black; equation, symbols and sources in the physics panel below.
Size guideS–5XL · inches
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Details
Size & fitS–5XL
Unisex Heavy Blend hoodie (Gildan 18500), classic fit.
| Size | Width | Length | Sleeve |
|---|---|---|---|
| S | 20 | 27 | 33.5 |
| M | 22 | 28 | 34.5 |
| L | 24 | 29 | 35.5 |
| XL | 26 | 30 | 36.5 |
| 2XL | 28 | 31 | 37.5 |
| 3XL | 30 | 32 | 38.5 |
| 4XL | 32 | 33 | 39.5 |
| 5XL | 34 | 34 | 40.5 |
Measurements in inches. Width and length ±1 in, sleeve (from center back) ±0.75 in.
ShippingFree US
Free US shipping. $10 flat shipping outside the US.
Returns & replacements21 days
Every item is printed to order, so we can’t accept returns or exchanges for change of mind, or if you ordered the wrong size or colour.
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∂ The physics
An electron and a positron meet and annihilate. What comes out is a muon and an antimuon.
In between there is a single photon that is never seen. It is virtual: in the centre-of-mass frame it carries the whole collision energy with no momentum, which a real photon cannot do. Richard Feynman’s diagrams, introduced in 1949, turn each such story into one term of the calculation.
At lowest order the answer is short. The muons come out with probability proportional to 1 + cos²θ, twice as likely along the beam line as at right angles to it. That curve is the outline drawn around the diagram.
Time runs up the page. The lines meet at two vertices, each worth a factor of the electric charge.
Two in, one photon, two out.
Equations
| Symbol | Meaning | Unit |
|---|---|---|
| \(\sigma\) | total cross section | \(\mathrm{m^2}\) |
| \(d\sigma/d\Omega\) | differential cross section per solid angle | \(\mathrm{m^2/sr}\) |
| \(\alpha\) | fine-structure constant, about 1/137 | \(\mathrm{1}\) |
| \(s\) | square of the centre-of-mass energy | \(\mathrm{GeV^2}\) |
| \(\theta\) | angle between the outgoing muon and the incoming electron | \(\mathrm{rad}\) |
| \(m_\mu\) | muon mass | \(\mathrm{GeV}\) |
Sources
- Feynman (1949) Space-Time Approach to Quantum Electrodynamics, Phys. Rev. 76, 769 (opens in a new tab)
- Peskin & Schroeder, An Introduction to Quantum Field Theory (1995), Sec. 5.1
- Griffiths, Introduction to Elementary Particles, 2nd ed., Ch. 7
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