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- Timestamp:
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Oct 30, 2016, 10:13:01 PM (7 years ago)
- Author:
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Clarence Wret
- Comment:
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v78
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v79
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| 21 | 21 | Graczyk & Sobczyk (arXiv:0908.2175) and others have resolved the problem in similar ways, often introducing a varying normalisation parameter to the ANL and BNL cross-section distributions separately. Additionally,the normalisation parameters can be correlated between the experiments. This approach does not allow for shape changes in the cross-section, which W&R does. |
| 22 | 22 | |
| | 23 | = Bubble chamber experiments = |
| 23 | 24 | |
| 24 | 25 | == ANL == |
| … |
… |
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| 195 | 196 | * [[Image(SKAT_nu_anu_flux_1985.png, 400px, center)]] |
| 196 | 197 | |
| | 198 | = Nuclear target experiments (2000s+) = |
| | 199 | |
| 197 | 200 | == MiniBooNE == |
| 198 | 201 | |
