Of Particular Significance

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Working hard at Canada’s Perimeter Institute, that is.   Longer posts are on hold for a couple of days while some friends and I stuff our brains with the details of as many ATLAS and CMS papers as we can handle.  We’ve gotten through fifteen or so, I suppose, on several topics.  Already I have learned a lot about the Higgs searches and the supersymmetry-like searches, which eventually will make their way onto these pages.   There are many devils in the details…  In the meantime, in case you’re interested, I did a small update to the article on the  implications of current data for Higgs particles of various types.

Picture of POSTED BY Matt Strassler

POSTED BY Matt Strassler

ON September 5, 2011

I’ve started a new article [click here] that tries to lay out the scientific implications of the Large Hadron Collider searches for the Higgs particle, as of early September 2011.   It’s a work in progress, so there will be more to come.  So far I’ve considered the implications for the Standard Model itself [recall the Standard Model consists of the known elementary particles and the simplest possible Higgs field and particle], and for variations on the Standard Model in which nature has a few extra types of particles that we don’t know about yet.  I’ll get to more complex cases, including supersymmetry and its five Higgs particles, later.  But I’ll bet that you will already be shocked at how different is the case of the Standard Model itself, which is easy to discuss succinctly, from even the simplest variants of the Standard Model.

Picture of POSTED BY Matt Strassler

POSTED BY Matt Strassler

ON September 2, 2011

Restructured the post: My preliminary discussion is first, the updates from the talks are now at the end.  The take-away message from the LHC talks:

The most interesting point here is that ATLAS and CMS [crudely] taken together exclude all regions for the Standard Model Higgs particle except

  • below 145 GeV,
  • the range 288-296 GeV, and
  • above 464 GeV.

Since precision measurements of other quantities in nature indirectly make the region above 464 GeV very unlikely, and even that small window around 290 is probably excluded when the two experimental results are combined properly, we are probably down to the region 115 — 145 GeV for the Standard Model Higgs.

Not much change in the Higgs hint at 140… some details have shifted, but they went by too fast.  It needs a closer look. But don’t expect any real news.  [Update: the significance of the hint has gone down a bit — but is this due just to the new data or have the analyses changed?  Also, from the past month’s data, CMS saw no additional two-lepton/two-antilepton events in that mass range  (at Grenoble they reported two events at 142 GeV.)]

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8/22/11 10:30 Mumbai time

The search for the Higgs particle — a ripple in the Higgs field, the field which is on average non-zero and provides the mass for the known elementary particles — continues at the Tevatron and Large Hadron Collider. We will probably get some new information within an hour or so.

Right now, the focus is on the search for the simplest possible Higgs particle — the one that goes by the name of Standard Model Higgs and arises from the simplest possible type of Higgs field. There are searches also going on for somewhat more complicated possibilities — Higgs particles that decay in unusual ways, or several types of Higgs particles, etc.   But the first task of the experiments is to find the Standard Model Higgs particle, if it is there in nature, or rule it out, forcing us to look for something more complex.

Last month, we heard (a) that the Standard Model Higgs is probably not heavy (its mass-energy [E=m c-squared] probably does not lie in the range above 150 GeV and below about 450, though there are still some gaps in the coverage), and (b) there is a hint of a Standard Model Higgs particle around 140 GeV, although this could also be a more complicated non-standard Higgs particle at masses somewhat lower (perhaps 115-130 GeV.)

But as I emphasized in this detailed article, there are two types of searches for the Standard Model Higgs particle: some simple ones, easy to interpret, that take a while, and difficult ones that require less data but are subject to more subtleties. That hint at 140 relies on a very difficult technique, and so there is some question as to whether it might be an artifact of some type.

We will be watching today at the conference in Mumbai to see the updates on both the easy and the difficult searches. If the experiments really do update their results from the Grenoble conference by including more data, we should see (1) a firmer exclusion of a heavy Standard Model Higgs, except — if it is actually there! or if there is a statistical fluke — at one or two points where there will be a slight hint of a Higgs; (2) an update of the easier search strategies, which could be quite interesting indeed, as there may be enough data now for them to be useful; and (3) probably very little new on the more difficult search strategy, because there are probably internal studies being done to check the methodology, and they may not be complete. The hints seen in the more difficult strategies will still be there, but I suspect they will continue for now to rest on somewhat uncertain ground.

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8/22/11 10:45 Mumbai time

[Right now we have an introductory theory talk by Abdelhak Djouadi, from France.  Why the theorist gets 35 minutes and the ATLAS and CMS experimental talks — the real data! — get only 20 minutes each is beyond me.  The ATLAS talk will be given by Aleandro Nisati from Italy (with whom I had the pleasure to work briefly), and the CMS talk by Vivek Sharma from the U.S.A.  And the Tevatron talk, combining CDF and D0 data, will be given by Marco Verzocchi, also from the U.S.A.]

Update 1: 11:39 ATLAS talk — Excellent!  the full data set is being used for the two-lepton/two-antilepton search!  [Nothing special in two-photon signature.]  11:53 EXACTLY as was predicted above… nice improvement in exclusion in heavy mass region, except for a few gaps; no real change in the Higgs hint below 150.  I think at 95%: excluded 146-232, 256-282, 296-464 GeV.  Striking: 99% exclusion of Standard Model Higgs between 160-220 and 300-420 GeV.

Update 2: 12:07 CMS talk (not quite all the recorded data I think) [in two-photon signature, some excess at 140 GeV, but I think ATLAS did not see one there; presumably just statistical fluctuation] 12:20 And AGAIN, exactly as predicted from CMS.

The most interesting point here is that ATLAS and CMS [crudely] taken together exclude all regions except below 145 GeV, 288-296 GeV, and above 464 GeV.

12:51 The Tevatron (CDF and D0 experiments) reports exclusion of the Standard Model Higgs in these ranges

  • Observed: 100-109 and 156-177 GeV
  • Expected: 100-108 and 148-181 GeV

Since observed is weaker than expected at the low end of the upper range, that means that there is a tiny hint of a Higgs below 150 or so, so this result isn’t in conflict with the LHC hint at around 140 GeV.  But we wouldn’t expect Tevatron to be as sensitive as the LHC experiments to a 140 GeV Higgs, if there is one.

Most interesting result from Tevatron: both CDF and D0 see an excess of events consistent with a supersymmetric Higgs particle in the mass range 120-150 GeV, in a production mechanism that is absent in the Standard Model.  However this is a tough measurement and it is hard to know whether to trust this… and the excesses are not that large.   (Experts: this is b-quark plus Higgs, where Higgs decays to b-quark and b-antiquark.  Note b-quark-plus-Higgs where Higgs decays to tau-lepton and tau-antilepton is not observed at the corresponding expected rate, so this Higgs would have to be exotic in at least one other way if this were a real signal.)

Picture of POSTED BY Matt Strassler

POSTED BY Matt Strassler

ON August 22, 2011

The Lepton-Photon 2011 conference in Mumbai is just getting ready to start.  Unlike the EuroPhysics conference in Grenoble last month, the number of experimental talks is small — and the talks are short.   So it’s all going to go by very fast.  We’ll get our full dose of Higgs searches at the  Large Hadron Collider (LHC) and Tevatron this morning (Monday), and searches for other types of novel phenomena (including top quark physics, supersymmetry, extra dimensions, etc.) tomorrow.  And then the topics will switch to other types of experiments (neutrinos, dark matter, collisions of heavy ions, and cosmic rays), until Saturday.

Although in principle the amount of data collected at the LHC has roughly doubled between Grenoble and Mumbai — a great achievement — you should not assume that the LHC experimentalists have had sufficient time to analyze it all.   In fact many studies presented in Grenoble did not use anywhere near the full amount of data that they had back then — I expect we will see many of those studies updated in Mumbai, but probably only for half the current data.  So there will be only a few results, I suspect, that use all the data.  Some of the Higgs studies might be among them, so that will be quite interesting.  We are likely, if Higgs results with more data are presented, to see more of the heavy-Higgs region excluded by the data than we saw at Grenoble.  We are unlikely to see anything clearly pointing toward discovery at this point — the hints will probably shift but remain hints for now.  I think we would probably need to double the data again first before things become clear.  But that will happen soon enough; by the end of the fall, perhaps?

Stay tuned for more news today….

8/21/11

Picture of POSTED BY Matt Strassler

POSTED BY Matt Strassler

ON August 21, 2011

Once you’ve read about the elementary particles of the Standard Model of particle physics — what we know about the world so far — you might want to learn something about supersymmetry — a speculative idea, whose proponents hope it will resolve several important puzzles about our world.   I’ll get back to the puzzles, and whether and how supersymmetry might solve them, soon.  Today’s article talks a bit about what this symmetry is, what its consequences are for particle physics, why an important bit of trickery is needed to hide the symmetry from obvious view, and how that trickery changes the particle physics implications.

As part of this article, I’ve put up a post about the difference between fermions and bosons.  So those of you who have wondered Why is the Higgs particle called the `Higgs boson’?  now get a chance to find out!

Picture of POSTED BY Matt Strassler

POSTED BY Matt Strassler

ON August 12, 2011

A couple of days ago I posted an elementary article on the elementary particles — an introduction to the particles of the Standard Model of Particle Physics, focusing on how they interact with one another.

Now I have an article for you on how drastically the particles and forces would be rearranged if the Higgs field were zero  in nature.   It’s pretty remarkable, actually, if you’ve never seen it before!  A surprising underlying organization emerges in this imaginary zero-Higgs-field world.  And by looking at how things differ between the real world and this imaginary one, it is possible to glean some insights into how the Higgs field is able to give mass to the known particles, and how it thereby determines the properties of the weak nuclear force.    And you can also learn about a number of interesting issues that continue to puzzle particle physicists.

Hope you enjoy it!

Picture of POSTED BY Matt Strassler

POSTED BY Matt Strassler

ON August 11, 2011

Today’s new article on the known types of particles attempts to set forth the particles of nature in a couple of different ways, ones that I hope will give you insights into why particle physicists categorize the particles the way they do.

The article describes the particles of the Standard Model of Particle Physics, which consists of all the known apparently-elementary particles and the simplest possible Higgs particle.   The name Standard Model just means: this is the simplest set of equations that can fit all the data we have gathered over decades, and that repeatedly makes correct detailed predictions for new experiments (despite occasional hints to the contrary, for instance this one, which unfortunately have tended to vanish over time.)

Sometimes this collection of types of particles is called the Particle Zoo.    Is there some hidden structure that underlies it?

Soon I’ll provide another post showing how this somewhat disorganized array of particles would have been much more simply organized were it not for the Higgs field.  What is the secret story behind this wily Higgs field?!

Picture of POSTED BY Matt Strassler

POSTED BY Matt Strassler

ON August 9, 2011

Ok, the third video clip from my talk at the Secret Science club from March 2011 is now uploaded for your enjoyment.  [But watch the other two clips first, it will make it a lot easier to follow!]  Learn how to find the Higgs particle!  (Or at least the easier ways — an explanation of the harder techniques, some of which are important in the current hints of a Higgs signal, and further details on the easier techniques, will be posted very soon.)

Attentive viewers will notice that in one of my plots of simulated data the Higgs particle has a mass between 140 and 150 GeV.  I promise you 🙂 I had no advanced warning of this month’s hints!!  […which happen currently to favor this regime…]

Picture of POSTED BY Matt Strassler

POSTED BY Matt Strassler

ON July 29, 2011

Correction below — a couple of readers pointed out that I had read a misquote of what Rolf Heuer, director general of CERN, had actually said.  I’ve updated the post to reflect what he said and why he said it, though the main point of the post doesn’t change at all.

I’ve left the EuroPhysics conference … With 400 talks, and a hundred or so from the Tevatron and the Large Hadron Collider, it was information overload.

There are two more days of summary talks at the conference, and tomorrow (Wednesday) afternoon there will be a bit more on the Higgs particle search.  A combination of the DZero and CDF Tevatron results will be presented, and perhaps a preliminary combination of the ATLAS and CMS results at LHC.  [I won’t be there, so don’t look for the update as it happens…]  The combinations can be done roughly in your head by looking at the various experiments separately, so there should be no surprises.

The one thing I want to remind you, in case the press makes a big deal out of what is said on Wednesday, is that what has been done so far to obtain a hint of a Higgs signal involves a very difficult measurement.   [Soon I’ll write an explanation of what I mean by this, but for now you can read more about this here. ]  The experimentalists are well aware of that, and say so both in public and in private.   I believe I saw the director general of the CERN laboratory quoted as saying this will all be cleared up by the end of the year.  UPDATE: This was indeed what I saw, but what I saw was itself a misquote; Heuer actually said “it” will be cleared up by the end of next year.   Either statement is true, depending on what “it” is.

  • If “it” means finding or excluding the Standard Model Higgs particle (remember that’s not the most general Higgs particle, see the Higgs FAQ) then that may not be fully settled until late next year — though in saying “end of next year” Heuer is being suitably conservative.
  • If “it” means figuring out if the current hint of a Higgs particle signal is a mirage or something real, that is probably something that will start to be settled between this December and next June.

Either way, [and here we return to the original post]  notice what this also implies: this [meaning the current hints] will not be cleared up much before the end of the year.  Science requires patient work, especially when the methods are challenging and fraught with subtleties. (more…)

Picture of POSTED BY Matt Strassler

POSTED BY Matt Strassler

ON July 26, 2011

A second video excerpt from my public talk “A Ring of Truth”, given last March, is now available.  I have put a link to it on the “Movie Clips” page.  This excerpt explains briefly why the Higgs is important (even to you), what the Higgs field does in nature, and how particle physicists make and detect rare particles.   [Things will be clearer if you watch excerpt 1 before watching excerpt 2.]

Picture of POSTED BY Matt Strassler

POSTED BY Matt Strassler

ON July 23, 2011

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