Freeze out (or, why are these people just standing around?)

Dark matter appears to explain the bulk of matter in our cosmos. While it has clearly been observed to exert influence over normal matter – nuclei, electrons, light – through gravitation, it has never been observed through any other interaction. Dark matter does not appear to directly emit light, nor respond to light; it has never been conclusively observed to scatter off a nucleus in a terrestrial detector, so far ruling out interactions through the strong or weak nuclear forces. A great deal of effort is therefore spent speculating on its properties, in order to design experiments that can measure them.

I’ve been thinking about freeze out, a property of particles which is often exploited in order to make statements about dark matter. “Freeze out” is when a particle species is unable to interact with itself or other matter because either the probability of an interaction is very small or because the likelihood of running into other matter is very small, or both. One can think of freeze out in a very human way.

Let’s consider a social situation, in which you are invited to a party where you don’t know anybody (except maybe the host). Let’s also consider a parameter, your “social cross-section”, which simply is a measure of how willing you are to approach a complete stranger and begin, then sustain, a conversation.

At the beginning, the party is hot. People are densely packed, the music is loud and thumping, you’re walking around with a drink in your hand and bumping into complete strangers. If you have a high social cross-section, you’ll take every bump and jab as a chance to flash a smile and start a conversation. With a sufficiently high social cross-section, you’ll dance with people and even as the party cools off (time goes on, people leave, the music gets less interesting) you’ll continue to stick with party-goers and socialise. You’ll keep meeting up with people, running into them, dancing, forming small social cliques of equally interactive people. Even when the party is completely wound down, you’ll stick with the hard-core types, the most social – maybe even go and have an after-party somewhere else. A high social cross-section can overcome the cooling effect on the party, allowing people to stick together and form new relationships despite a thinning population density at the party.

Consider instead a person with a low social cross-section. They may be comfortable starting a conversation but not sustaining it past small-talk. They certainly don’t like to dance, unless they really get prodded into it. Maybe they really don’t even like to start conversations but they feel obliged to go to the party because of the host. So they go, and the party starts off real hot. They get bumped and jostled, drink spilling, and maybe they flash a smile and start a conversation. But the interactions are weak and rare, sustained in frequency only by the density of the people at the party. Eventually the party cools, people start leaving, high social cross-section folks are cliquing and grouping. The low cross-section people are off by themselves, tapping a foot by the side of the dance floor or standing by the buffet, but not forming new relationships.

This is dark matter, and this is how dark matter “freezes out” of interactions. When the party is hopping, it almost doesn’t matter what your cross-section is. You’re caught up in the fray, forced to interact by the sheer number density of party-goers. But as the party cools and the crowd thins, the inclination to interact remains the same but the opportunity drops precipitously. Now imagine a party where 85% of the party-goers left over when the cooling happens are low cross-section types. That’s our universe. High cross-section people are forced to clump and group in between the low cross-section types, forming little groups in this sea of non-interacting people. Welcome to our cosmos. Nerds rule!

Of course, the trick here is that it’s possible that the low cross-section types are only low on verbal and physical communication. Imagine a party where the low cross-section types are super-techy, and prefer to interact through social media. They’re standing around, mobile phones out and tapping away on their Facebook or Twitter streams, while the high cross-section people have phones put away and are gabbing and laughing and dancing. “This party is lame,” tweets one low cross-section type. “Let’s leave,” types another. “But the dip is good and the beer is free,” says a third. “Good call, let’s stay,” says a fourth. They are actually communicating all the time but the talkers are unaware, because they are not tapped into this social stream.

The promise of studying the dark sector, dark matter and all of its friends, is that we might tap into how they communicate with one another. Maybe every now and then one of the low cross-section types laughs at a Tweet, and a nearby high cross-section type hears them and asks, “What’s so funny?” “Oh, it’s just that my friend PwnN00bs1984 noticed that girl in the corner is so drunk she is mistaking some random guy for the guy she came in with.” “That IS funny,” says the high cross-section type, suddenly exposed to a whole conversation going on behind the scenes.

Let’s hope that eventually, we find a way to tap into the dark sector’s own little conversation. Maybe, then, we’ll figure out what 85% of these people are doing at this party.

Accelerate for America

I was recently a participant in a welcome event for pre-med students at SMU. The event started with a panel discussion, including members of the science faculty at SMU. It ended with a social event outside the auditorium. Jodi and I participated in the social event (the panel discussion was packed and well underway by the time we showed up) and met a bunch of pre-med undergraduates. Several of them were interested in what they would get out of taking physics (one made the common remark about having a bad experience in high school physics). Jodi and I took a holistic approach – discuss the exciting reasons for doing physics, but emphasize the applications of physics across boundaries.

For instance, I enjoyed mentioning the role that subatomic particle accelerators play in modern cancer treatment. The statistic we used to bring to Washington D.C. was that 11,000 cancer patients every day are treated with medical accelerators. I mentioned the fact that subatomic charged particles are attractive because some of them can penetrate the body, doing little damage as they enter, and then dump all of their energy into the tumor. It’s like a guided missile for cancer.

There was definitely surprise from some of the students that physics plays this role. It was a pleasure to take this opportunity to start broadening them a little. Maybe they’ll take physics and hate it, or maybe they won’t take it at all. But the truth is that physics, like many other sciences, plays a central role in our lives. From medical imaging using antimatter (PET scans) to cancer therapies, physics is in all sorts of places. Let’s not forget the central role that classical mechanics plays in sports medicine (Newton, after all, can teach us a lot about bone breaking, shock and impulse on joints, and many other mechanical stresses on the body).

I learned today about www.acceleratorsamerica.org,  a website devoted to promoting a symposium about accelerators and their role in the future of the U.S. From manufacturing to medicine, particle accelerators are playing an increasing and important role in our world. How does the U.S. remain viable in the development of this technology? These and other questions linger over this enterprise.

The first patient to receive radiation therapy from the medical linear accelerator at Stanford.
The first patient to receive radiation therapy from the medical linear accelerator at Stanford.

I like to look back at a haunting but uplifting photograph that a good friend of mine showed me many years ago. In it, a small boy is seen sitting, almost casually, under the watchful eye of a particle accelerator [1]. The black and white photo is of the first person ever treated by a particle accelerator in the Western Hemisphere. The article referenced here tells us,

[Henry] Kaplan and [Edward] Ginzton, PhD, professor of electrical engineering and of physics, developed the first medical linear accelerator in the Western Hemisphere, installed at Stanford-Lane Hospital in San Francisco. In January 1956 the machine was ready to be used on their first patient, a boy with retinoblastoma in his one remaining eye after surgeons had removed the tumor in the other eye. Destroying the tumor while sparing the eye would have been impossible with earlier, less-focused radiation sources.

“I will never forget the puzzled look on the face of the garage owner down on Fillmore Street when I asked him to borrow a heavy-duty automobile jack,” recalled Kaplan in the book. “I explained that it was to carry a large block of lead with a pinhole in it, to enable us to position that pinhole day after day for six weeks directly opposite the tumor in the boy’s eye while missing the lens and cornea.”

As in all things in learning, don’t forget that learning in a narrow lane won’t give you the creativity you need to do great things. Expanding yourself a little, challenging your educational comfort zone, leads to greatness. If physics kept to physics, biology to biology, chemistry to chemistry, how many important medical procedures and treatments would have been missed? How many lives lost?

A little physics can go a long way. Heck, it might save a life.

[1] http://news-service.stanford.edu/news/2007/april18/med-accelerator-041807.html

To CERN: messages from today, messages from 1980

Next week (June 2-6), I will be at CERN for the first time in many years (and to kickoff my many visits to come!). I am attending the ATLAS Collaboration Physics Week, a four-day event centering on ATLAS physics analysis. I am excited to be heading to the new Mecca of particle physics, the new global hub that will soon define the frontier of collider physics.

In the spirit of that new frontier, I had a very interesting conversation today at lunch. A senior SLAC theoretical physicist started discussing the very interesting evidence that he thinks is mounting for significant contributions to the proton from charm and bottom quarks. Called “intrinsic charm” or “intrinsic bottom”, these contributions mark the ultimate in quantum mechanics. In the classical physics view of the proton, the quarks rattle around inside glued together by the strong force. Quantum mechanics, which accurately described the proton and crushes the classical picture, instead tells us that the proton is mostly NOT the three quarks that define it. It’s mostly gluons, and in fact those gluons are constantly producing pairs of virtual particles that flit in and our of existence and contribute significant structure to the proton. Even in that latter picture, the basis of all computation, there are assumptions about how much you can ignore charm and bottom that may be proving to be wrong.

That more common view sees the contribution of intrinsic charm and bottom as negligible. But, in the high energy environment of leading hadron colliders – the Tevatron and soon the LHC – that picture may be incorrect (c.f. [1,2]). In fact, a recent D0 preliminary result [3] suggest that the proton/anti-proton collision debris close to the beamline (at large rapidity) exhibit behavior that greatly differs from the leading calculations of these collisions. These calculations are provided in the Coordinated Theoretical-Experimental QCD (CTEQ) parton distribution functions (PDFs) [4]. The D0 authors state that the version of CTEQ PDFs used in their comparison do not include the Tevatron Run II data results, so they represent a pre-Run-II picture of QCD at hgh energy. Their data suggests that picture needs updating.

The picture painted at lunch today was of this rich universe of phenomena lurking just inside this deceptively simple picture of the proton. Looking back at some papers on this, I also realize that we are entering an era where these ideas that seemed, perhaps, so far off in 1980 (ala [1]) are on our doorstep now, demanding attention. In the fight to understand the Standard Model, so that we can see beyond it, such issues will become more and more critical.

[1] S.J. Brodsky, P. Hoyer, C. Peterson and N. Sakai. Phys. Lett. B 93 (1980)

[2] http://arxiv.org/abs/hep-ph/0508126

[3] http://www-d0.fnal.gov/Run2Physics/WWW/results/prelim/QCD/Q14/

[4] http://www.phys.psu.edu/~cteq/