How many inverse femtobarns at 7 TeV to find Higgs?

In summary, according to Tommaso Dorigo's blog and the graphs provided, a Higgs with a mass of 115 GeV can be discovered at a 2.7 sigma significance with 5/fb of data at 7 TeV. However, in order to have a solid 5-sigma discovery, the lowest estimate seen is 20/fb. With the LHC expected to gather 2-4 /fb this year alone and potentially up to 11/fb by the end of 2012, it is likely that the Higgs will be discovered at above 3 sigma before the shutdown at the end of 2012. The current best week for the LHC has an average luminosity of
  • #1
petergreat
267
4
If the Higgs mass is around 115 GeV, how many inverse femtobarns at 7 TeV are needed to find the Higgs?
 
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  • #2
A lot. As I'm sure you know, a Higgs with a mass of 115 GeV is the hardest to detect, and everyone hopes it is somewhere else! With a mass of 115 GeV,and assuming by "find" you mean a solid 5-sigma discovery, the lowest estimate I've seen is 20/fb. By that time, the LHC will have undergone the long shutdown of 2012 and hopefully will be running at near max power, 6 TeV per beam.
 
  • #3
A very large number. Perhaps 30-50.
 
  • #4
Can I find a graphical plot showing the required integrated luminosity (at 7 TeV) against the Higgs mass, for various confidence levels?
 
  • #6
Dorigo also says that the graph is for CMS only. Combining data with ATLAS typically turns 3 sigma into 4 sigma. On the graph, 5/fb at 7 TeV gives a 2.7 sigma significance for a 115 GeV Higgs. Currently CERN expects to gather 2-4 /fb for this year alone, and more optimistic estimates are abound. So by combining data from both detectors, it's likely that even a 115-GeV Higgs will show up at above 3 sigma before shutdown at the end of 2012.
 
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  • #7
Petergreat, I am beginning to worry that your university is not properly teaching you how to find information from primary sources. There are things you ask about and should be able to find directly on the experiments' web sites, but you are looking at people's blogs - and for that matter you're looking here. PF is many things, but we are not a primary source.

You need to know how to use the PDG, Spires, HEPData, arXiv and the major experiments' web sites.

Now, let's take a look at your analysis. CMS shows a 1.2 sigma expected significance for a 115 GeV Higgs with 1 fb-1. The standard for discovery is 5, so CMS needs roughly (5/1.2)^2 = 17+ fb. ATLAS is reporting a sensitivity less than CMS, requiring a little less than 2x as much data as CMS for the same significance. On the other hand, ATLAS is the only group that has made public their level of background. Also remember that something like 80-90% of the data delivered ends up used by the experiments in the final plots. Hence 30-50. 30 would be lucky, 50 would be unlucky, the truth is probably in between.

As for what's delivered, the best week has the LHC averaging 20 pb-1/day now. Assume it runs twice this well for 18 more months and you get 11 fb-1. So it doesn't really matter if we are talking 17, 30 or 50.
 
  • #8
Thanks for your advice. Actually I had a look at PDG's 2010 review on Higgs search, where the graphs are showing discovery potential at 14 TeV rather than 7 TeV, then I turned to Tommaso's blog... I understand that 5 sigma is the gold standard for discovery, however I was a little impatient and figured out that 3 to 4 sigma is more or less guaranteed in 2012, which is short of a discovery, but IMHO enough reasons for excitement and enough to tell us the approximate mass of the Higgs if the signal is genuine.

Vanadium 50 said:
As for what's delivered, the best week has the LHC averaging 20 pb-1/day now. Assume it runs twice this well for 18 more months and you get 11 fb-1. So it doesn't really matter if we are talking 17, 30 or 50.

According to the LHC website, on 1 May the luminosity was increased to 8.4e32 /cm^2/s, which corresponds to roughly 70/pb per day. Is this to be sustained? Where can I find up-to-date information on the latest weakly average?
 
  • #9
The official LHC luminosity data is here: http://lpc.web.cern.ch/lpc/lumiplots.htm . Expecially note the link at the bottom of this page where the exact numbers are tabulated.
 
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  • #10
petergreat said:
According to the LHC website, on 1 May the luminosity was increased to 8.4e32 /cm^2/s, which corresponds to roughly 70/pb per day.

Not even close!

You can't get the expected luminosity for a year by taking the best instantaneous luminosity, and multiplying that by the number of seconds in a year. First, the luminosity falls, and second the fraction of time the machine is colliding is nowhere near 100%.
 
  • #11
petergreat said:
According to the LHC website, on 1 May the luminosity was increased to 8.4e32 /cm^2/s, which corresponds to roughly 70/pb per day. Is this to be sustained? Where can I find up-to-date information on the latest weakly average?

At most, they run the LHC for 18 hours for a good fill where currently it can collect 40/pb. Potentially they could double this to 80/pb per day over the next few weeks, but let's say they manage potentially 50/pb per day. There is a Hubner factor which gives the fraction of time available for collecting data which has been estimated at 0.3 based upon runs during 2010. So with 125 days of running, this gives the total integrated luminosity as 0.3*50*125 = 1.9/fb.

The hope was to collect 1/fb during 2011 based a Hubner factor of 0.2 since they felt 0.3 was too optimistic and it looks as if they should easily do this since they have already collected over 300/pb.

They're in the middle of a technical stop which finishes on Thursday, and you can see how things are progressing at:
http://lhcdashboard.web.cern.ch/lhcdashboard/

and clicking on the four links under Simple LHC Lumi Calculator
http://lpc.web.cern.ch/lpc/
 
  • #12
I've found such a graph on Tommaso Dorigo's blog:... On the graph, 5/fb at 7 TeV gives a 2.7 sigma significance for a 115 GeV Higgs.
I stand by my original statement: 20/fb.

What is apparently the same graph, marked "CMS Preliminary: Oct 2010", appears in the Chamonix 2011 conference paper by Bill Murray. Apparently the same, EXCEPT - that there it contains an additional curve: 10/fb at 7 TeV. And even that curve falls well short of 5 sigma. Moreover, what is clear from comparing the 1/fb, 2/fb, 5/fb and 10/fb curves is that they are equally spaced. (As they should be.) And to get to 5 sigma at a Higgs mass of 115 GeV, you'll need to at least double the luminosity yet again, to 20/fb.
 
  • #13
Thanks for all the information. So Higgs still may be quite a few years away. Kind of boring, but definitely good news for people who like to keep playing with all sorts of speculative models.
 

1. What is an inverse femtobarn?

An inverse femtobarn (fb^-1) is a unit of measurement used in particle physics to represent the amount of data collected from particle collisions. It is equivalent to approximately 10^15 collisions.

2. How is the number of inverse femtobarns related to finding the Higgs boson?

The more inverse femtobarns collected, the higher the chances of detecting rare processes such as the production of the Higgs boson. This is because the Higgs boson is a very rare particle and requires a large amount of data to be observed.

3. What does "7 TeV" refer to in this context?

7 TeV (teraelectronvolts) refers to the center-of-mass energy of the Large Hadron Collider (LHC), which is a particle accelerator used to collide protons at high energies. This energy level was used during the first run of the LHC from 2009-2013.

4. How many inverse femtobarns were collected at 7 TeV to find the Higgs boson?

A total of 5 inverse femtobarns of data were collected at 7 TeV during the first run of the LHC. This data was used to confirm the existence of the Higgs boson in 2012.

5. Why is it important to collect a large amount of data to find the Higgs boson?

The Higgs boson is a very rare and elusive particle, and requires a large amount of data to be observed. The more data collected, the higher the chances of detecting the Higgs boson and understanding its properties. Additionally, a larger dataset allows for more precise measurements and can potentially reveal other new particles or phenomena.

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