Difference between revisions of "Elong-13-05-01-HERMES-Match"
(New page: ==Matching HERMES F<sub>1</sub><sup>d</sup>, dA<sub>zz</sub><sup>d</sup>, and db<sub>1</sub><sup>d</sup>== I wanted to double-check the code against the HERMES data, but this required a fe...) |
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==Matching HERMES F<sub>1</sub><sup>d</sup>, dA<sub>zz</sub><sup>d</sup>, and db<sub>1</sub><sup>d</sup>== | ==Matching HERMES F<sub>1</sub><sup>d</sup>, dA<sub>zz</sub><sup>d</sup>, and db<sub>1</sub><sup>d</sup>== | ||
− | I wanted to double-check the code against the HERMES data, but this required a few extra steps. First, using the values for | + | I wanted to double-check the code against the HERMES data, but this required a few extra steps. First, using the values for $A_{zz}^d$ and $b_{1}^d$ that they measured, along with the formula $b_1^d = -\frac{3}{2}A^d_{zz}F^d_1$, I found what they were using for $F^d_1$. The $F^d_1$ they're using is per nucleon, and for HERMES' two highest ''x'' points (the rest are inaccessible to the Bosted code because for 0.012<''x''<0.063, 16.75<''W''<sup>2</sup><42.87, which is outside the ''W'' range that the code can handle) they match the code relatively well: |
{| class="wikitable" style="text-align:center; border-collapse:collapse;" border="1" | {| class="wikitable" style="text-align:center; border-collapse:collapse;" border="1" | ||
− | | style="width: 100px;" | <''x''> || style="width: 100px;" | ''Q''<sup> 2</sup> || style="width: 100px;" | HERMES | + | | style="width: 100px;" | <''x''> || style="width: 100px;" | ''Q''<sup> 2</sup> || style="width: 100px;" | HERMES $F_1^d$ || style="width: 100px;" | Bosted $\frac{F_1^d}{A_d}$ |
|- | |- | ||
| 0.128 || 2.33 || 1.018 || 0.620 (Outside Bosted "Good" range) | | 0.128 || 2.33 || 1.018 || 0.620 (Outside Bosted "Good" range) | ||
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|} | |} | ||
− | This means that the way I was calculating the error | + | This means that the way I was calculating the error $\delta b_1^d=\frac{3}{2}\delta A_{zz}^d F_1^d$ was off by a factor of $A_d=2$. This was corrected. |
− | Including the 1/2 term in the polarized cross-section (to stay consistent with HERMES' terminology), then | + | Including the 1/2 term in the polarized cross-section (to stay consistent with HERMES' terminology), then $\delta A_{zz}^d = \frac{2}{f\cdot P_{zz}\sqrt{N_{\mathrm{Tot}}}}$ where $P_{zz}=0.9$, $N_{\mathrm{Tot}} = 3,200,000$ and $f=0.5$. |
Looking at points from the HERMES data, I get:<br> | Looking at points from the HERMES data, I get:<br> | ||
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[[Image:2013-05-01-HERMES.png]] | [[Image:2013-05-01-HERMES.png]] | ||
− | The lowest point in | + | The lowest point in $\delta b_1^d$ doesn't match because of the difference in $F_1^d$ noted above, although I'm not sure why I get a smaller error on the highest point in $\delta A_{zz}$. However, you may want to take these results with a grain of salt since this was all input using the SHMS code as I don't have code set up for the HERMES detector. |
Latest revision as of 13:49, 18 October 2023
Matching HERMES F1d, dAzzd, and db1d
I wanted to double-check the code against the HERMES data, but this required a few extra steps. First, using the values for $A_{zz}^d$ and $b_{1}^d$ that they measured, along with the formula $b_1^d = -\frac{3}{2}A^d_{zz}F^d_1$, I found what they were using for $F^d_1$. The $F^d_1$ they're using is per nucleon, and for HERMES' two highest x points (the rest are inaccessible to the Bosted code because for 0.012<x<0.063, 16.75<W2<42.87, which is outside the W range that the code can handle) they match the code relatively well:
<x> | Q 2 | HERMES $F_1^d$ | Bosted $\frac{F_1^d}{A_d}$ |
0.128 | 2.33 | 1.018 | 0.620 (Outside Bosted "Good" range) |
0.248 | 3.11 | 0.496 | 0.486 |
0.452 | 4.69 | 0.161 | 0.171 |
This means that the way I was calculating the error $\delta b_1^d=\frac{3}{2}\delta A_{zz}^d F_1^d$ was off by a factor of $A_d=2$. This was corrected.
Including the 1/2 term in the polarized cross-section (to stay consistent with HERMES' terminology), then $\delta A_{zz}^d = \frac{2}{f\cdot P_{zz}\sqrt{N_{\mathrm{Tot}}}}$ where $P_{zz}=0.9$, $N_{\mathrm{Tot}} = 3,200,000$ and $f=0.5$.
Looking at points from the HERMES data, I get:
The lowest point in $\delta b_1^d$ doesn't match because of the difference in $F_1^d$ noted above, although I'm not sure why I get a smaller error on the highest point in $\delta A_{zz}$. However, you may want to take these results with a grain of salt since this was all input using the SHMS code as I don't have code set up for the HERMES detector.