Of Particular Significance

Author: Matt Strassler

As someone who has spent several years thinking hard about how to detect “hidden particles” — ones that are not affected by the three forces of the Standard Model, the electromagnetic force and the strong and weak nuclear forces — I am pleased to see the result that just appeared from the APEX experiment, at the Jefferson Laboratory in the US state of Virginia:

http://arxiv.org/PS_cache/arxiv/pdf/1108/1108.2750v1.pdf.

Quoting from [and modifying for non-experts, in italics] the abstract:

  • We present a search at Jefferson Laboratory for new particles, lighter than protons, that are carriers of a new force and that can decay  to electron-positron pairs [recall positron = anti-electron]. Such a particle can be produced by slamming an electron beam into ordinary matter...  Using APEX data, we searched … and found no evidence of such a particle in a certain range of masses and force strengths.  Our findings demonstrate that experiments of this type can explore a new, wide, and important range of masses and strengths for sub-proton-mass forces.

What they’re doing is looking for a particle that is similar to a Z particle, one of the carriers of the weak nuclear force, but that on the one hand (a) exerts a smaller force on ordinary matter than does the weak nuclear force, and on the other hand (b) is lighter in mass than the Z, so the force it exerts dies off more slowly with distance than does the weak nuclear force.   If such a particle were found, it would represent the first new force of nature discovered in many decades!

A competitor experiment from Mainz (called MAMI) reported results a few months ago.  The two experiments are sensitive to a comparable force strength and to slightly different mass ranges.  You can see their results in the figure, which shows the APEX search region in blue and the MAMI search region in green, and other experiments in variants of grey.  These two experiments are probing weaker forces — looking for force carrier particles that are more hidden — than has ever been possible before.

Both of these experiments are still in the very early days; their results come from short, preliminary runs of data-taking.  They both plan to have a much longer run, which should allow them much greater sensitivity to weaker forces and to force carriers of a wider range of masses.  In particular, the unshaded region in the figure, which hasn’t been searched yet, should be entirely covered soon.

I am also pleased because among the leaders on the APEX experiment are three young theorists, Rouven Essig, (a former Rutgers student of my colleague Scott Thomas, and now a Stonybrook faculty member), Natalia Toro and Philip Schuster (two of my  co-authors on a recent paper, and faculty members at the Perimeter Institute), and an experimentalist and professor at nearby New York University, the ubiquitous Kyle Cranmer (who also is on ATLAS and presented that experiment’s result on the search for the Higgs particle a few weeks ago.)

Congratulations, APEX!!!

Picture of POSTED BY Matt Strassler

POSTED BY Matt Strassler

ON August 18, 2011

Ok, folks, after a few days of hard work, I have an article detailing how to look for supersymmetry, one of the most popular theories predicting new phenomena at the Large Hadron Collider.  You may first want to read about the particles of nature  and then about supersymmetry itself.

I’ve tried to take the most common answer to this question — essentially, look for an excess of collisions that produce both high energy quarks and invisible particles — and deconstruct it, showing you what it means at the level of particle physics (what is produced, what decays, how is it detected) and then work backwards to show you what physical assumptions lie underneath this answer.

I hope that once you’ve understood these assumptions, you’ll have a clearer idea what this answer’s strengths and weaknesses are.   And then we can go on, in a future post, to explore what the LHC has and hasn’t said so far about supersymmetry as a property of nature.

As always, comments on clarity and content are welcome!

8/16/11

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POSTED BY Matt Strassler

ON August 16, 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

Here’s an article intended to give a layperson a sense for why so many types of particles — most of them, in fact — decay away almost instantly, forcing us to discover them through various types of trickery.   This is relevant in the search for the Higgs particle, which decays away far too quickly to observe directly. (See the Higgs FAQ, the video clips from my recent public talk, or the article about recent hints of the Higgs for more info.)

Picture of POSTED BY Matt Strassler

POSTED BY Matt Strassler

ON August 4, 2011

On Tuesday, the New York Times had an article on the Higgs particle search.  Not bad, and does quote relevant people, but just a little bit thin on content.  If you want some actual content, try my article on the hints of the Higgs particle.

Also, the article falls into the common mistake of not distinguishing “The Higgs particle” from “The Standard Model Higgs particle.”   One paragraph says

The Higgs boson is the keystone and last undiscovered piece of the so-called Standard Model, a suite of equations that agrees with all the experiments physicists have been able to do so far in the laboratory.  If the Higgs boson does not exist, theorists will have to go back to their blackboards.

If you conflate the general with the specific, you will at some point down the line end up very confused about what the LHC is trying to do and what its results do and don’t mean.  It would be good for the public if the NY Times reporter would read the Higgs FAQ before phrasing a statement like this.  A more correct statement is:

The Standard Model Higgs boson is the keystone and last undiscovered piece of the so-called Standard Model, a suite of equations that agrees with all the experiments physicists have been able to do so far in the laboratory. If the Standard Model Higgs boson does not exist, this will be very exciting for particle physicists, as it will imply (as has been known for decades) that there must be other particles — perhaps multiple Higgs bosons, and/or perhaps other types of particles — that physicists have not yet discovered, but should be able to discover with the LHC.

The spin is pretty different.

And then there’s the generic paragraph about supersymmetry — more or less right, but again with some big missing points.  Well, stay tuned at this website for an article or two on supersymmetry, and what we have and haven’t learned about it from the LHC so far.

Picture of POSTED BY Matt Strassler

POSTED BY Matt Strassler

ON August 4, 2011

Just finished my new article on the hints of a Higgs particle.  I hope you find it useful! I have tried to explain, in largely non-technical terms,

  • how experimentalists at the Large Hadron Collider are looking for the Higgs, using various methods;
  • what makes methods of this type easy or difficult, with analogies;
  • that the current hints of a Higgs particle rely on the more difficult techniques, making it unclear whether we should trust them;
  • that more data over the coming year will bring the simpler techniques into their own, eliminating this problem over time.

I welcome your comments, questions and advice as to how to make this article more transparent to the non-technical reader!

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POSTED BY Matt Strassler

ON July 31, 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

Nice post went up yesterday on the ATLAS experiment’s blog [ATLAS is one of the detectors at the Large Hadron Collider] from Kyle Cranmer (Professor at New York University) ; as I posted on this blog, Kyle gave Friday’s presentation summarizing ATLAS’s results on the search for the Higgs particle.   Kyle is a young star with a special gift for the statistical reasoning that is essential for combining many different measurements together so as to squeeze the maximum knowledge out.  His post has some technical parts, but even if you can’t follow the details I still recommend skimming it for the non-technical insights.

Another  interesting post went up on the Cosmic Variance blog, by John Conway (Professor at UC Davis [and not to be confused with the mathematician John Conway]).  John mentions that ATLAS and CMS (the other big LHC experiment) have observed no sign of quarks being composite (made of other yet smaller things) and have seen no sign of supersymmetry. [I’ll explain supersymmetry on this site soon.]  He then goes on to discuss the Higgs search situation (see also here for my initial take.)  But I disagree quite strongly with what John has to say about the search for supersymmetry; look at comment #9 in reply to his post for my opinion.   John states as a near-fact that we pretty much know now that the super-partners (heavy new particles that are predicted by supersymmetry) of the quarks  are heavier than 1 TeV, but I just put a paper out yesterday with Mariangela Lisanti, Philip Schuster and Natalia Toro that contradicts that statement, arguing that the searches performed so far do not by any means cover all the territory, and suggesting that other search strategies need to be added.   And I know that there is more unexplored territory that we did not even discuss in our current paper.  [I’ll also give a more detailed discussion of our paper’s argument soon.]  This is a key job of particle theorists; make sure all the ground gets covered by the experimentalists before they give up and move on!

Picture of POSTED BY Matt Strassler

POSTED BY Matt Strassler

ON July 28, 2011

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