Testing the neutron generator

Since the last post, the neutron generator has been set-up and checked to see that it works. So what to do with it next? Throw it into a swimming pool!

We plan to run the neutron generator under 5 metres (16ft) of water next to XENON1T, see the figure. For XENON1T, the water acts for two purposes: to shield the detector from environmental neutrons, and to veto any highly energetic cosmic ray muons that interact near the detector.

The XENON1T setup. The neutron generator will be placed directly adjacent to the detector cryostat (centre). Surrounding both will be the support structure and water tank, which of course will be filled with water.

When we ordered the generator, we of course specified that it should be water tight to this depth. However, it’s obvious that we should test it ourselves before putting it next to the detector. This is to see if it leaks under water, if any of the attached cables and hoses are not perfectly sealed. This is also to test that it sinks unaided, as it could have been that air in the hoses made the generator set-up too buoyant.

Rafael and Jacques fiddling with the neutron generator’s high voltage feedthrough before submerged it.

So we contacted the Boilermaker Aquatic Center, the nearest clean body of water we could think of, and they said they would be happy to help. The deep end of the diving pool is 17ft deep, which was more than enough for us. To check for leaks, we put colour saturation desiccant crystals inside the end of each cable, at the point where each cable attaches to the generator. These crystals would then change colour if they were in contact with water. We then went down when the pool was closed, with all cables and hoses attached to test the water tightness and buoyancy. Needless to say, the generator itself was not powered at any point, and so could not produce any neutrons during the test. We then left the generator underwater for an hour, to make completely sure that there was not even a small leak.

The neutron generator being lowered (by Rafael) into the water (where Jacques, Cassie and myself take a swim).

The results of the test were very positive. The generator sank, and the dessicant remained dry inside all cables. In short, everything looks good :)

The generator at the bottom of the diving pool, with Jacques giving a thumbs up: all looking good!

We would like to thank David Fraseur, Terry Huntley and James Barnett at the Boilermaker Aquatic Center for all their help in this test, we couldn’t have done it without you!

Cryostat Arrived

We just received the electropolished cryostat parts for our Xenon Detector and installed them on the frame.

Electropolishing flattens protrusions (but not fill up cavities), and as flattened surface has less area, its outgassing is decreased, so it makes for better vacuum and thus cleaner xenon. And it also makes the surfaces shiny!

So now it’s a game of tightening the ConFlat vacuum flanges. Closing a ConFlat flange takes some caution and time as bolts need to be closed bit by bit in order to prevent one side getting too compressed, blocking other sides from fully closing, and causing leaks. So I’m working around the circle of bolts: After you close a first one, let’s say at 12 o’clock direction, by 1/8, 1/4, or 1/2 a turn, I close the opposite screw, at 6 o’clock, by the same amount, then the one at 1 o’clock, then 7, then 2, etc, following the shape of star, 10-2-7-12-5-11-1-8-4… and always go in a circle either clockwise or counterclockwise.

After a one round of tightening, the bolt at 12 o’clock can be tightened further, so whichever order you go, you’ll need to repeat this a couple of times. This gets rather tedious in a narrow spots like the flanges connecting to the pump in the picture. Well, let’s see how often we will need to re-do them to change their orientation…

See the valve with a black handle? We’ll rotate it down vertically so that the handle can be reached more easily.

Now I hope no more resealing is necessary… At least the ones to the pump as those tight spots…

Unlimited Barns

We know Dark Matter exists. What we don’t know is what it is made of. And what that tells you immediately is that if Dark Matter interacts with us, it will only do so very rarely – otherwise we would have found it long time ago.

To quantify exactly how rarely, physicists use a quantity called the cross-section. If we leave quantum mechanics aside for a moment, the cross-section would be the size of a particle. For example, a pool billiard ball has a radius of a little over an inch. We would attribute to it cross-section of pi times one inch squared, that’s about 3 square inch or, hey, it’s science here, about 20 cm2.

If we go to the largest atoms we know, uranium for example, their nuclei have a radius of about 8 femtometers, that’s 8×10-13cm. Thus, their cross section is about 2×10-24cm2. Clearly, square centimetres are not a convenient unit for nuclear physics. So when physicists at Purdue University were working on the Manhattan project in the 1940s, they were looking for a convenient measure to describe the size of the uranium nucleus. Convenient, and also secretive. With Purdue University being in a pretty rural area back then (it still is in some sense), they called the uranium nucleus “big as a barn”, and so, to this day, the unit barn is defined as being equal to 10-24cm2.

Purdue Campus 1940

Aerial view of the Purdue Campus, 1940, directly adjacent to fields and farms. Image courtesy Purdue University Libraries, Archives and Special Collections from http://earchives.lib.purdue.edu.

Clearly, if you randomly hit the white ball in a game of pool billiard with your queue, it is more likely to hit a coloured ball the bigger these are. In other words, the probability of a scattering to occur grows with the cross-section of the particles that scatter. In the mind-set of quantum mechanics, this concept is generalized: the cross-section is used to indicate the probability of particles scattering with each other.

For example, the probability for a thermal neutron to interact with a helium-3 nucleus, kicking it to its excited level, is 0.00005 barn. The probability for the same neutron to instead react with the helium-3 nucleus and kick out a proton from it is much higher, 5330 barn. Clearly, picturing the cross-section as a geometrical size of the particles can be misleading in these cases. Even so, the barn unit really is convenient in nuclear physics.

As science progressed, particles were discovered that are much less likely to interact with us. If we hit a hydrogen nucleus (a proton) with another proton, the cross-section is about 40 millibarn, or 4×10-26cm2. That’s still nuclear physics. But a typical neutrino coming from the sun will have a cross-section of only 10-41cm2, that’s 10 atto-barn, to hit the proton. At this stage, we enter an area of particle physics where even the nuclear physicist’s unit barn becomes somewhat useless again.

Dark Matter particles interact even less with us. We have searched for Dark Matter particles that would interact with us as “often” as neutrinos do, but with no success. Our current detectors have a sensitivity to detect Dark Matter particles if they interact as rarely as with a cross-section of only 2×10-45cm2. If you’re curious to see how that looks in our research publications, that is available online free to read and shown in the last figure of the paper.

What we are working on is to push this sensitivity further, within the next few years, by another factor of 1000 or so to fully cover the cross-section range where we would expect the cross-section of Dark Matter to be. This requires larger detectors and some clever ideas of how to build and operate them, which is what keeps us busy for the time being. So, back to work.

 

How to Debug a Shipping ;-)

taken from Asterix The Twelve Tasks

Once upon a time in a physics department, some physicist ordered a bunch of resistors. When the package arrived in the lab, the physicist got the second page of the delivery note which indicated that one type of resistor was on back order and would arrive later. When the physicist checked the order, he recognized another type of resistor was also missing. However, because he only got the second page of the delivery note, he actually couldn’t check why the second type of resistor was missing as well. So, he went over to the Physics department secretaries and asked them about the order, and why he did not receive his resistors. They told him that he can only find out what was delivered when he has both pages of the delivery note. The secretaries didn’t have the full delivery notice, but the shipping clerk should have it. When the Physicist went down to the basement in order to talk to him. The shipping clerk said that he only keeps the delivery notices for a few days if something is wrong with the order. Otherwise, they are immediately discarded. In order to locate the missing items, the Physicist could go to the Business Office on the second floor. There, he could get a copy of the delivery notice and check it. After explaining everything to the Purchasing Clerk, she looked into the files of the order and they found the delivery note. Finally, the Physicist and the Purchasing Clerk recognized that the missing part was not even listed on the delivery note. So, the Physicist went back to the secretaries and ask them if it was possible that the company forgot the resistors in the order. After some discussion, they found out that just the simplest solution is the most probable one .…… the resistors were simply not ordered. So, the Physicist filled out a new order form and went down to Rafael’s office to let him sign the second form. He brought the form back to the secretaries and with a little luck he will get his missing parts.

The moral of that story:
One hour walking through the building and finally recognizing that the part simply wasn’t ordered.

That’s life in science as well. ;-)

The Place That Sends You Mad, out of The Twelve Tasks of Asterix

Calibrate all the Things!

Our new neutron generator recently arrived from Germany, after some delay clearing customs. That means we can finally get around to doing the calibration of the neutron generator that is required before we ship it to the Gran Sasso National Laboratory (LNGS) for installation on the XENON1T detector. Of course calibrating the generator is easier said than done. In the next few weeks we will be setting up the generator in the annex next to our lab, while we wait for the neutron detectors we ordered to arrive.

Andy, the English Postdoc, staring in fascination at the fancy packaging of the neutron generator.

Have you read and agreed to the terms of use of this product? Of course we have…

For those of you who are somewhat familiar with different types of radiation, you are probably thinking to yourself,  “Wait did he say they are setting up the neutron generator in the annex next to their lab? Won’t that mean they are going to be permanently destroying their ability to have children?” Well, that is all a matter of what you think of the prospect of having children…, but in all seriousness the answer quite simply is an emphatic no.

Some assembly required…

The neutron generator is a deuterium-deuterium fusion generator. What that means is that the generator has a chamber filled with deuterium gas. The gas is excited by applying high voltage to the chamber and accelerating the deuterium atoms. The deuterium nuclei have sufficient energy so that when they collide, they actually fuse together, producing a nucleus and releasing a high energy neutron. Typically, this reaction produces neutrons with energies of 2.5MeV; for comparison, the more common deuterium-tritium fusion reaction produces 14MeV neutrons.

And here ladies and gentleman we have the business end of the whole affair. Neutrons are produced from a region about halfway down the tube

In addition, the flux we will be running the detector at is so low that one could work, eat, sleep, watch YouTube videos and prove people wrong on the internet in the lab 24/7, and still be subjected to less than 0.1rem per year.  To put that in perspective, the background radiation from cosmic rays, industrial plants, spending all night in front of the TV, eating too many microwave dinners, etc. that the average American receives in a year is 0.6rem per year (Here is a fun website to try and estimate your annual dose). So in conclusion, we won’t be suffering from radiation sickness any time soon, humanity is saved (or not, as the case may be).

But why do we actually need the neutron generator? After all, the purpose of the XENON experiments is to detect Dark Matter. Well, as Shayne described, we expect Dark Matter to scatter off the nucleus of the xenon atoms producing nuclear recoils, which can be distinguished from electronic recoils (how this is done will be subject to a future post, for sure). However, in order to calibrate the XENON1T detector, we need to know what to be looking for when nuclear recoils happen. That is where the neutron generator comes in. Neutrons also scatter of the nuclei. We will be using the neutron generator during calibration runs on the XENON1T detector to introduce a source of neutrons, the energy and flux of which are known, allowing us to identify characteristic patterns in the data which we can associate with nuclear recoils.

Of course, all that is predicated on us actually knowing the flux off neutrons produced by the neutron generator, which is what I will be working on over the weeks to come. That is where the previously mentioned neutron detectors come in, which will be used to quantify the neutron flux produced by the generator at various settings, such as high voltages etc. But wait, there’s more. Because these neutron detectors themselves will have to be calibrated in order for us to use them to calibrate the neutron generator, we… Uh, that will have to wait for my next update in a few weeks.

Annually Modulating Dark Matter?

We don’t really know yet what Dark Matter is made of. This begs the question: is there a tell-tale signature that we may expect from any kind of Dark Matter? Indeed, we can look for annual modulations of possible Dark Matter interactions in our detectors.

We can assume Dark Matter has certain properties by astronomical observations. For example, Dark Matter does not interact with us electromagnetically.  We cannot hold up a magnet and collect Dark Matter, just like we cannot trap it in an electric field.  The only way we can definitely “see” Dark Matter is gravitationally, through methods like gravitational lensing.  Although we can’t actually see the Dark Matter, we can see light bending around it, which produces multiple copies of a galaxy, or even a whole ring of images!

Lensing Cluster Abell 383

The elliptical galaxy in the center is so massive that light bends around it. Many of the oblong images are copies of objects located behind this elliptical galaxy. For example, the ring-like smear towards the bottom of the galaxy is actually one luminous object. This phenomenon is referred to as a partial Einstein ring. (Image courtesy of the Hubble Space Telescope)

This mysterious light-bending substance is all around us.  One popular idea states that Dark Matter is comprised of small particles called WIMPs — Weakly-Interacting Massive Particles. Imagine our galaxy sitting in the middle of a cloud of Dark Matter. Since the Dark Matter does not interact with us much, we would move through this Dark Matter cloud freely. In doing so, we would then encounter a Dark Matter “wind”. Imagine being in a convertible driving on the freeway on a clear, wind-free day. You feel like the wind is blowing in your face. The wind sensation is caused by you moving through the air very quickly, quick enough to feel a “wind”.  The same is true of Dark Matter, we move through it very quickly and would expect to feel a Dark Matter “wind”. The tricky bit is that Dark Matter particles can pass through Earth constantly and we won’t feel them much, due to their feeble interactions.

The Earth moving through the Galaxy. While Earth moves around the Sun, the Sun moves around the Galactic center. To an observer outside our galaxy, we move faster in the summer than in the winter.

 

Just like in the convertible, we move through the Dark Matter with our spaceship, Earth. However, we do not always move through the Dark Matter at the same speed. During the winter, we actually move slower than we do in the summer time. Why is this? Well, on Earth, we orbit the Sun, and the Sun moves around the Galactic center. During the summer we move in the same direction as the Sun, whereas in the winter time we move in the opposite direction. To an observer sitting outside of our galaxy, we move faster in the summer time than in winter, even though we would observe ourselves moving at roughly the same speed during the year, relative to the Sun.

We know that we will feel a constant wind of Dark Matter if we stand still, but we know we are moving at a variable rate, depending on what time of the year it is.  If we can catch Dark Matter particles, we will catch more of them during the summer because there is more of this Dark Matter “wind” than in the summer. Just like in the convertible – The faster you go, the more head wind you experience! If we make a graph of how much Dark Matter we expect to see over the course of years, we expect it to modulate: that’s the the idea of annual modulation.

DAMA signal

This graph represents seven years of data collected by the DAMA experiment. The particles detected had an energy of 2-4 keV. The y-axis is the number of particles detected while the x-axis is the time over which it was collected. The Roman numerals represent the year number. Is this dark matter? You decide! (Figure from Barnabei et al. 2003)

Since we know Dark Matter should modulate the question becomes: does it? Experiments like DAMA and CoGeNT have reported seeing modulated signal rates. However, there are many other things that modulate, including (but not limited to) cosmic rays, temperatures, ground water levels, neutrons and some have even proposed modulating radioactive decay rates. How do we tell all of this modulating background from our modulating Dark Matter signal? Well, these detectors are of course shielded by many layers of different material (including being put under a mountain!), but this is the crux of one of the important research questions we are exploring right now.  Can the signals reported by these experiments actually be due to Dark Matter? While these experiments are meticulously designed and the data is analyzed very carefully, it signals might be confused with some other modulating background. This is the crux of one of our experiments — the Modulation experiment. I will leave the details of that one to a future post, so keep checking back!

Direct Detection of Dark Matter

Dark Matter is hypothesized to account for the vast majority of matter in the Universe. Despite the fact that Dark Matter cannot be observed directly because it does not absorb or emit electromagnetic radiation in any significant quantity, its existence is deduced by the observed gravitational effects on visible matter. Many experiments are in progress to search for the yet undiscovered subatomic particle that make up Dark Matter. These experiments are categorized into three groups: direct detection, the search for Dark Matter particles scattering off nuclei in a detector, indirect detection, the search for Dark Matter decay products, and experiments that aim to produce Dark Matter in particle colliders. Here at Purdue, we are working on the XENON direct dark matter search.

Usually, a direct detection experiment operates in an underground laboratory to shield it from cosmic radiation and reduce background. These laboratories include, just to name a few: the SNOLAB underground laboratory in Sudbury, Ontario; the Canfranc Underground Laboratory in Spain; the Deep Underground Science and Engineering Laboratory in South Dakota; and, of course, the Gran Sasso National Laboratory in Italy which hosts our XENON project. One of two primary types of detector technologies is used in each of these locations are the cryogenic detector or the noble liquid detector. The cryogenic detector, which functions at incredibly low temperatures just fractions of a degree above absolute zero temperature, detects heat from collisions with a crystal absorber. A noble liquid detector looks for scintillation light signals that are emitted from particle collisions with liquid noble elements such as xenon or argon. Liquid noble elements are the preferred target for direct Dark Matter searches. They are easily scalable to targets of variable mass and shield from external background, in addition to allowing discrimination between nuclear recoil and electronic recoil. Liquid xenon is an especially appealing choice in Dark Matter searches because its high mass and large atomic number allow for compact design of detector geometry. A Time Projection Chamber (TPC) is able to reconstruct the 3D position of an interaction within its target volume, permitting a high degree of background rejection.

Particles can interact either with the electron shell of an atom, or with its nucleus. Radioactive backgrounds mostly interact with electrons, causing electronic recoils. Dark Matter on the other hand is expected to be heavier and thus to mostly interact with the nuclei, causing nuclear recoils. Image courtesy of University of California, Berkeley.

In order to be consistent with the state of the early universe, any candidate for a Dark Matter particle should have a small, yet measurable interaction probability, called cross section, with ordinary matter. The cross section between a neutralino particle and nucleon, in particular, is on the order of the electro-weak scale. This interaction combined with the projected range of the mass of a Dark Matter particle, 10-1000 GeV, bestows the name Weakly Interacting Massive Particle (WIMP) to possible Dark Matter particles.

Our planet is colliding every second with a cluster of these particles called the dark halo of the Milky Way galaxy. Cassie will write more about that in the next blog entry. The electro-weak scale is precisely what allows WIMPs to interact with ordinary matter. WIMPs are expected to scatter elastically off atoms, producing nuclear recoils and depositing energy. As such, the goal of direct Dark Matter experiments is to measure the energy deposited in the detector through collisions and discern what types of particles caused them. Tens of thousands of Dark Matter particles may be going through you as you read this post! With our detectors, we try to catch a few of them to be able to study their properties.

Brand New Blog

To celebrate the creation of the new Dark Matters group blog we have a picture that will last for a lifetime. Andy, the Postdoc in our group, always comes to lab dressed in a sport coat, slacks, coloured socks, and just overall nice. While the rest of us come in, well, shorts and t-shirts. We decided to come into lab one day dressed like Andy, and this was the result:
If you don’t know the group, you can tell Andy from his contented expression… Top row: Rafael Lang, Chenglian Zhu (SURF 2012), Cassie Reuter, Katie Davis, David Garand, Jamin Rager (REU 2012), Alex Pan. Bottom row: Greg Pach (REU 2012), Jacques Pienaar, Matthias Kurz, Andy Brown, Lorenz Hruby, Shayne Reichard.