Of Particular Significance

Blog – Of Particular Significance

Ok, today I’ve posted the article you’ve been waiting for: What does the LHC have to say, so far, about supersymmetry? [Here’s an article about supersymmetry and what it predicts, and another about standard ways to look for signs of it at the Large Hadron Collider, under certain assumptions; if you want to review the known particles and forces first, you can read about them here.]

If you’ve been reading the press, you may have seen statements such as “the air is getting thin for supersymmetry” or “we’re painting supersymmetry into a corner”. And recently on Cosmic Variance some broad statements about supersymmetry being in serious trouble were made by experimentalist John Conway (before being somewhat watered down after I raised an objection.)

[Update: in response to a comment posted below, I reread this post, and I see that indeed I did not, in the original version, give enough words attesting to the tremendous progress that has been made.  So let me state clearly: what the LHC and the ATLAS and CMS experiments have achieved, in the supersymmetry-aimed searches made public so far, is fantastic.   They have wiped not only many variants of supersymmetry, but also variants of many other speculative ideas, off the map.   And I don’t mean in any way to downplay this… just to try to put it in proper perspective.  To do so better, I also added a sentence after the list of assumptions below.]

A number of experimentalists seem to have (and, in their public statements, give) the impression that most supersymmetry theorists, faced with an apparent disaster, are rushing around in circles desperately trying to think of new ways that supersymmetry might have escaped notice. This view also seems to be showing up on various blogs. This is a profound misconception, one that history clearly contradicts. Rather than a picture of universally panicked theorists trying to figure out how to save their favorite theory, the image should be of a number of theorists sitting calmly in their chairs, saying, “we knew this situation was a reasonable possibility — and we’ve been trying to alert you to it for a very long time.” The statements have been in the scientific literature for years.

Many theorists, including myself [and let me emphasize that I am not a huge proponent of supersymmetry, though I have worked on it and do view it as a serious contender as a theory of nature] have been saying for years that the main search strategies planned at the LHC would be insufficient to cover large regions of the supersymmetric continent. Important papers on this subject go back into the 1990s and a good chunk of the last decade. Here is the point. The bulk of the search strategy used at the LHC to find supersymmetry rests upon three assumptions.

  1. in any process, the number of superpartners can only change by an even number;
  2. the lightest superpartner [which is stable, by assumption 1]  is a superpartner of a particle we know (and therefore, to avoid conflict with other data, an undetectable neutralino or sneutrino);
  3. the superpartners that are affected by the strong nuclear force are significantly heavier than the other superpartners of known particles.

These assumptions are not unreasonable, and there are strong arguments in their favor, especially for assumption 1 and to a degree assumption 3 (described here).  But we must keep in mind that if we relax any one of those assumptions,  the limits on supersymmetry from current LHC data become much weaker. If you want to read more details about how this works, you can click here, though you will find it useful to read today’s article first unless you already know a lot about the subject.  Or click on the figure below (taken from this post, which also explains why these assumptions are often made) to understand how these assumptions lead to the prediction of “jets and missing energy” on which the most powerful search strategies — including the ones we’ll hear about at this week’s conference in Mumbai — are all based.

The logical chain that leads particle physicists to look for supersymmetry in the standard way. SP and LSP stand for "superpartner'' and "lightest superpartner".

So until you hear a consensus building, you should be cautious in making too much of statements that supersymmetry, as a part of nature and a solution to the hierarchy problem, is in serious trouble.  The truth is that certain variants of supersymmetry — ones based on certain assumptions that might be wrong — are indeed strongly constrained by current data.  Others, simply put, are not.  In short, we have a long way to go.

8/19/11

Picture of POSTED BY Matt Strassler

POSTED BY Matt Strassler

ON August 19, 2011

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

Picture of POSTED BY Matt Strassler

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

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