equation 116.9 eq:expdis-F2-parton
open in the book ·
parts/11-qft-standard-model/18-exp-deep-inelastic.tex:328
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Supports
-
depends_on
phenomenon 116.9
Callan–Gross
¶
- depends_on phenomenon 116.19 The longitudinal cross section is small ¶
- depends_on phenomenon 116.36 The EMC effect ¶
- depends_on phenomenon 116.25 Half the proton momentum is invisible to the photon ¶
- depends_on phenomenon 116.27 The neutrino cross section rises linearly with energy ¶
-
depends_on
phenomenon 116.18
Bjorken scaling
¶
- depends_on phenomenon 116.32 Scaling is violated logarithmically ¶
- depends_on proposition 116.40 The Drell–Yan cross section scales ¶
- depends_on proposition 116.35 The gluon density is measured, not assumed ¶
- depends_on proposition 116.21 What the neutron-to-proton ratio measures ¶
Neighborhood
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Edges
| type | direction | node | provenance | where |
|---|---|---|---|---|
depends_on |
← | Callan–Gross | declared | parts/11-qft-standard-model/18-exp-deep-inelastic.tex:384 |
depends_on |
← | The EMC effect | declared | parts/11-qft-standard-model/18-exp-deep-inelastic.tex:2240 |
depends_on |
← | Half the proton momentum is invisible to the photon | declared | parts/11-qft-standard-model/18-exp-deep-inelastic.tex:1473 |
depends_on |
← | The neutrino cross section rises linearly with energy | declared | parts/11-qft-standard-model/18-exp-deep-inelastic.tex:1617 |
depends_on |
← | Bjorken scaling | declared | parts/11-qft-standard-model/18-exp-deep-inelastic.tex:977 |
depends_on |
← | The Drell–Yan cross section scales | declared | parts/11-qft-standard-model/18-exp-deep-inelastic.tex:2405 |
depends_on |
← | The gluon density is measured, not assumed | declared | parts/11-qft-standard-model/18-exp-deep-inelastic.tex:2133 |
depends_on |
← | What the neutron-to-proton ratio measures | declared | parts/11-qft-standard-model/18-exp-deep-inelastic.tex:1114 |