All of the results below are from top 10% most central collisions with negative pion assumption
Fiable mt-m0 Bins for abs(zvertex) Ranges in Higher Rapidities
This is just to look at what kind of statistics could be gained from including these reigons.
abs(zVertex) \\ y-> |
.6 |
.8 |
1.0 |
1.2 |
1.4 |
key word |
< 30 |
4-22 |
4-20 |
5-20 |
none |
none |
x |
30-40 |
4-22 |
4-21 |
3-12 |
none |
none |
ttof |
40-50 |
4-21 |
3-19 |
3-13 |
8-13 |
none |
ftof |
50-60 |
4-24 |
3-22 |
3-16 |
6-11 |
none |
ftos |
60-70 |
4-23 |
3-21 |
3-15 |
6-13 |
none |
stos |
70-80 |
4-22 |
3-19 |
3-14 |
5-12 |
none |
stoe |
80-90 |
4-23 |
3-20 |
3-16 |
4-13 |
none |
eton |
90-1000 |
4-22 |
3-19 |
3-14 |
3-12 |
5-9 |
ntoh |
<1000 |
4-22 |
3-19 |
2-17 |
3-12 |
5-9 |
all |
(compare to y=0, abs(zvertex) < 30 has fitable bins 5-28)
Comments
In all cases, the loss of ability to fit is due to kaon contamination.
(ie if we can fix the kaons we can extend our mt-m0 range for all rapidities)
Questions
Why did we cut abs(zvertex) < 30 in the first place?
Is there a way to fix the kaon yields in this range?
Conclusions
Can we get good statistics from higher rapiditiess?
I believe that at least the top 10% centrality data can be extended into y=1.0 without changing the zVertex cut.
If we include all zVertex values we can extend into y=1.2
Is there anything fitable in the relativistic rise?
I looked at the highest mt-m0 bins for all rapidities (bins 30-50) and found no bins which showed fitable seperaion.