Research

The Aprile Group at Columbia University is on a thrilling quest to directly detect the universe’s hidden matter – dark matter – using sophisticated detectors. We are meticulously searching for tiny whispers of energy, left behind by the incredibly rare collisions between dark matter and the atoms within our detector. Our search occurs deep in underground mines and tunnels, nestled beneath tons of rock—a crucial first line of defence against unwanted interference by cosmic radiation.

While our ultimate goals are shaped by our significant involvement in the international XENON experiment (now operating as XENONnT) and the exciting new DarkSide-20k experiment, we also maintain a vibrant program of local Research and Development here at Columbia. These on-campus efforts allow us to explore innovative detector technologies, refine our analysis techniques, and contribute to the broader field of particle detection.

Ready to dive deeper?

Keep scrolling to learn more about the fascinating world of dark matter, the candidates we’re searching for, and the specifics of our work with XENONnT and DarkSide-20k.

Dark Matter

Have you ever wondered what makes the universe tick? We see stars, galaxies, and planets, but there’s a cosmic mystery lurking in the shadows: dark matter. It’s a mysterious substance, invisible to our telescopes. Yet, we know it’s there, and it plays a crucial role in shaping the universe as we know it. Its presence is felt only through its gravitational pull. However, a wealth of evidence, spanning the vastness of the cosmos down to our own galactic neighborhood, strongly suggests it’s a fundamental ingredient of the universe.

One of the earliest and most compelling clues came from galaxy rotation curves. These are graphs tracking the rotational speed of celestial bodies depending on their distance from a galactic center. When astronomers measured how fast stars orbit the centers of galaxies, they found that stars at the outer edges were moving much faster than they should based on the gravitational force that could be provided by visible matter alone. This suggests that an invisible “halo” of dark matter is enveloping galaxies, providing the extra gravitational pull needed to keep these fast-moving stars from flying off. Intriguingly, we see this same effect even within our own Milky Way galaxy.

Curve showing rotational velocity over distance from the galactic center for the Messier 33 galaxy (from a 1999 paper by Edvige Corbelli and Paolo Salucci)
The Cosmic Microwave Background as seen by the Planck space observatory in 2013.

Looking at even larger scales, the Cosmic Microwave Background, the afterglow of the Big Bang, provides another vital piece of the puzzle. Tiny temperature fluctuations in the Cosmic Microwave Background reveal the seeds of structure formation in the early universe. The patterns we observe in the Cosmic Microwave Background only make sense if there was a significant amount of non-interacting dark matter present, providing the gravitational scaffolding for galaxies and galaxy clusters to eventually form.

The very structure formation we see today, the clustering of galaxies into vast networks, also points to the crucial role of dark matter. Ordinary matter alone wouldn’t have had enough gravity to clump together in the way we observe over the universe’s lifetime. Dark matter, making up a significant portion of the universe’s mass, provided the gravitational “glue” to initiate and accelerate this cosmic assembly.

Graphic taken from the the TNG100-1 run of the IllustrisTNG Project, showing the evolution of the interstellar magnetic field strength in a 10Mpc (comoving) region.

Dark Matter

Hubble Telescope photo of the Abell 2218 galaxy cluster showcasing gravitational lensing.

Another powerful piece of evidence comes from gravitational lensing. Massive objects, like galaxies and galaxy clusters, bend the path of light passing by them. The amount of bending we observe is often far greater than what can be accounted for by the visible matter alone, indicating the presence of a significant amount of unseen dark matter warping spacetime. The image of the Abell 2218 galaxy cluster is a prime example of the kind of distortion caused by the dense mass of these clusters.

Finally, the spectacular phenomenon of merging galaxy clusters provides perhaps the most direct “visual” evidence for dark matter’s separate existence. The case of the merging clusters on the right provides a great example, since the hot matter that has interacted during the collision is clearly visible (red) but the mass of the clusters (blue) seems significantly offset when analyzed with gravitational lensing. When galaxy clusters collide, the ordinary matter (hot gas) interacts and slows down, while the dark matter components can pass right through each other, separating clearly from the visible matter! The best example of this is the “bullet cluster” seen in the image to the right.

Curve showing rotational velocity over distance from the galactic center for the Messier 33 galaxy (from a 1999 paper by Edvige Corbelli and Paolo Salucci)

These independent lines of evidence, from the subtle motions of stars within galaxies to the grand structure of the cosmos, all converge on a compelling picture: our universe is filled with a substantial amount of this mysterious dark matter, a key component that shapes its evolution and structure. Furthermore, the way dark matter interacts gravitationally and the patterns we observe allow us to derive crucial properties that this elusive substance must possess, leading to the development of various theoretical candidates for what dark matter might actually be.

Dark Matter Candidates

Given the enormous range of possibilities, the scientific community is engaged in a broad and diverse search. Experiments like XENONnT and DarkSide-20k are specifically designed with high sensitivity to detect WIMPs, one of the most well-motivated and long-studied dark matter candidates. However, the quest continues across many fronts, exploring all potential signals and pushing the boundaries of our knowledge. To solve this mystery scientists have proposed everything, from new particles to changing our most familiar theories.

Weakly Interacting Massive Particles (WIMPs) are a leading class of dark matter candidates. These hypothetical particles are theorized to interact with normal matter on a scale similar to that of the weak force, one of the fundamental forces of nature, but possibly through new types of interactions that are as weak as or weaker than the standard weak interaction. WIMPs are also predicted to be significantly heavier than standard model particles, with masses potentially ranging from that of a hydrogen atom to several lead atoms. Their mass and potential for weak-scale interactions make them a prime target for direct detection experiments like XENONnT and DarkSide-20k.

QCD axions are hypothetical, extremely light particles proposed to solve a puzzle in the theory of the strong nuclear force (Quantum Chromodynamics, or QCD). Unlike WIMPs, axions would be incredibly light, potentially billions of times lighter than an electron. Despite their tiny mass, if they exist in large enough numbers, they could collectively contribute significantly to the universe's dark matter. Experiments are searching for axions by looking for their very weak interactions with ordinary matter or their potential conversion into photons in strong magnetic fields.

Axion-Like Particles (ALPs) are a broader family of hypothetical light particles that share some properties with the QCD axion but are not necessarily tied to solving the strong force puzzle. Unlike axions, the mass and interaction strength of ALPs are not strictly related, allowing for a wider range of possibilities. These particles could also be very light and, if abundant, contribute to dark matter. Scientists are searching for ALPs through their potential interactions with photons in magnetic fields or their decay into other particles.

Sterile neutrinos are hypothetical, heavier versions of the known neutrinos that earned the name "sterile" because they would not interact via the weak force – the force responsible for radioactive decay – unlike their active counterparts. This lack of standard interactions makes them very difficult to detect. However, they might interact through gravity or by subtly mixing with regular neutrinos. Their existence could explain some mysteries in neutrino physics, and their mass could potentially contribute to the universe's dark matter.

Standard Model neutrinos are fundamental particles known to interact very weakly with other matter. While they are abundant and have a small mass, making them a form of dark matter, they are not considered the primary explanation for the vast majority of dark matter we observe. This is because they are "hot" dark matter – they move at speeds close to the speed of light. Such fast-moving particles would have prevented the formation of the large-scale structures like galaxies that we see in the universe today, which requires "cold," slow-moving dark matter. Therefore, while neutrinos contribute a small fraction to the overall matter density, the bulk of dark matter must be something else.

Primordial black holes (PBHs) are hypothetical black holes that could have formed in the very early universe due to density fluctuations shortly after the Big Bang, unlike stellar black holes that form from the collapse of massive stars. Their mass could range from tiny fractions of a gram to many times the mass of our Sun. If PBHs exist in sufficient numbers within a specific mass range, they could potentially constitute a significant portion, or even all, of the dark matter. Scientists are searching for PBHs through their gravitational effects, such as microlensing (the bending of light from
distant stars) or their potential Hawking radiation.

Massive Compact Halo Objects (MACHOs) are a category of dark matter candidates that, unlike WIMPs and axions, are made of ordinary (baryonic) matter, albeit in a compact and non-luminous form. These could include objects like brown dwarfs, neutron stars, black holes, and even rogue planets. The idea was that a large number of these faint objects residing in the halos of galaxies could collectively account for the missing mass. However, extensive searches using gravitational microlensing have largely ruled out MACHOs as the primary component of dark matter in the mass ranges that would be needed.

WIMPzillas are a class of extremely heavy, hypothetical dark matter particles, with masses potentially ranging from a billion GeV up to the scale of Grand Unified Theories – vastly heavier than typical WIMPs. Unlike standard WIMPs that are often considered thermal relics from the early universe, WIMPzillas are theorized to have been produced non-thermally, possibly through gravitational interactions during or after inflation. Due to their immense mass and potentially very weak interactions, direct detection of WIMPzillas is incredibly challenging, and scientists often look for them indirectly through ultra-high energy cosmic rays produced by their decay.

Modified Gravity refers to a class of theories that propose altering the laws of gravity, as described by Einstein's General Relativity, on large scales, rather than invoking the existence of dark matter. These theories attempt to explain the observed gravitational effects, such as the flat rotation curves of galaxies and the dynamics of galaxy clusters, by changing how gravity behaves at large distances. While some modified gravity theories can explain certain phenomena without dark matter, they often face challenges in explaining other cosmological observations that are well-accounted for by the standard dark matter model, such as the Cosmic Microwave Background and the large-scale structure of the universe.

Info on some leading dark matter theories. Image taken from Beyond the Standard Model by Y. Gouttenoire.

Some of the leading particle contenders in the dark matter race include Weakly Interacting Massive Particles (WIMPs), which are theorized to interact with normal matter on the scale of the weak force – one of the fundamental forces of nature – and are much heavier than known particles, with a typical mass range from that of a hydrogen atom to that of several lead atoms. Other prominent particle candidates include axions, extremely light particles that could have been produced in the early universe, and sterile neutrinos, hypothetical heavier versions of the neutrinos we already know.

Beyond new particles, some scientists are also exploring whether dark matter could be made up of primordial black holes, tiny black holes that might have formed in the very first moments after the Big Bang.

There are even alternative theories that suggest our understanding of gravity itself might need to be modified on large scales (modified gravity), potentially explaining the effects we attribute to dark matter without invoking a new type of particle at all.

Dark Matter Detection Make it, Break it or Shake it

The quest to capture dark matter is on! Researchers are employing three powerful techniques – directly colliding with it, indirectly observing its cosmic footprints, and attempting to forge it in the heart of particle accelerators.

Direct Detection
These experiments aim to observe the very rare collisions between dark matter particles and ordinary matter atoms within highly sensitive detectors. Located deep underground to shield from cosmic rays, these detectors look for the tiny amounts of energy deposited when a dark matter particle interacts with the detector material, such as liquid xenon or argon. A positive signal would provide direct evidence for dark matter particles and allow us to study their properties.
Indirect Detection
This approach searches for the byproducts of dark matter particle annihilation or decay in space. If dark matter particles annihilate or decay, they could produce detectable Standard Model particles like gamma rays, positrons, antiprotons, and neutrinos. Telescopes and detectors on Earth and in space are looking for an excess of these particles coming from regions where dark matter is expected to be abundant, such as the center of our galaxy or dwarf galaxies.
Collider Experiments
High-energy particle colliders, like the Large Hadron Collider (LHC), can potentially create dark matter particles by smashing ordinary particles together at extremely high energies. If dark matter particles are produced, they would likely escape the detector without interacting, leading to an apparent imbalance in energy and momentum in the collision events. Scientists analyze these events to infer the production of invisible particles, which could be dark matter, and study their properties.

Time Projection Chambers

Our most sensitive dark matter detectors, called Dual-Phase Time Projection Chambers (TPCs), use a large amount of very pure, cold liquid, like xenon or argon, with a layer of the same gas above it.

If a dark matter particle bumps into an atom in the liquid, it creates a tiny flash of light and some free electrons. We use an electric field to guide these electrons upwards into the gas. Once in the gas, these electrons create a second, brighter flash of light.

By carefully measuring both the initial tiny flash in the liquid and the later, brighter flash in the gas, along with how long it took the electrons to travel, we can figure out how much energy was deposited and exactly where the “bump” happened within the detector. The ratio of the two light signals also helps us tell what kind of particle caused the interaction, helping us to look specifically for dark matter and ignore other signals. Because these detectors are large and use these dense liquids – for example, liquid xenon is about three times denser than water – they are very good at catching the rare interactions we expect from dark matter.

Two Signals!

Dual-Phase TPCs use noble gases in both liquid and gas forms. A dark matter particle collision with a liquid atom generates two signals:

Scintillation (S1): A prompt flash of light produced by excited atoms at the interaction site in the liquid.

Ionization (S2): Electrons ejected from the interaction in the liquid are drifted into the gas phase by an electric field, where they are accelerated and produce a second, larger flash of light.

Why Bigger is Better!

Detecting dark matter requires catching incredibly rare interactions. Using liquid noble gases allows us to build massive detectors, often weighing several tonnes. A larger detector contains vastly more target atoms for dark matter particles to potentially collide with. This increased target mass directly boosts our experiment’s sensitivity, making it more likely that we will observe one of these elusive interactions. Essentially, a bigger detector gives us a much better chance of seeing a very rare event.

Self-Shielding: A Natural Advantage

Dense liquid noble gases, like xenon, offer a valuable advantage: self-shielding. The outer layers of the liquid act as a natural barrier, absorbing or deflecting some of the background radiation coming from outside the detector. This means the inner part of the detector is shielded by the liquid itself, creating a quieter, radiation-reduced space to search for the faint signals of dark matter interactions, without as much interference from background noise. This built-in protection enhances our ability to detect very rare events.

Pinpointing the Interaction: 3D Event Reconstruction

By precisely measuring the timing and location of the two signals (S1 and S2), we can reconstruct the 3D position of the particle interaction within our detector. Knowing exactly where an event occurred is crucial. It helps us pinpoint potential dark matter signals and, importantly, reject background events that might originate from specific parts of the detector or its surroundings. This 3D information acts like a powerful filter, allowing us to focus on events that are more likely to be the faint signature of a dark matter particle.

The Need for Extreme Purity!

Noble liquids like xenon and argon have a crucial advantage for dark matter detection: they can be purified to an extraordinary degree. This extreme purity is absolutely essential for two key reasons. First, even trace amounts of certain impurities can capture the ionization electrons as they drift through the liquid towards the gas phase. Losing these electrons would distort our signal and hinder our ability to accurately reconstruct the interaction. Second, many impurities can undergo radioactive decay, emitting particles that would create background events within our detector. Unlike external radiation that we can shield against, these internal radioactive decays are much harder to eliminate. Therefore, sophisticated purification and distillation processes are employed to remove virtually all contaminants from the noble liquids, ensuring a pristine and “quiet” environment where the faint signals of dark matter have the best chance of being observed.

Filtering Out the Noise: Background Rejection

Detecting faint dark matter signals is tough because our detectors are constantly hit by other radiation, creating “background noise.” A key way to filter this noise is to look at how particles interact. Many common background events cause interactions with the detector’s electrons, called electronic recoils. However, many dark matter theories predict that WIMPs would primarily interact by directly hitting the nucleus of an atom, causing nuclear recoils. By carefully analyzing the signals in our detector, we can often distinguish between these two types of interactions, allowing us to reject the more common electronic recoil background and focus on the elusive nuclear recoils that might be the signature of dark matter.

XENONnT: Xenon-Based Detection

XENONnT is a state-of-the-art direct detection experiment specifically designed to hunt for Weakly Interacting Massive Particles (WIMPs), one of the most compelling candidates for dark matter. Located 1400 m underground at the Gran Sasso Laboratory (LNGS) in Italy to shield against cosmic backgrounds, XENONnT began operating in 2020 with 8.6 tonnes of xenon. At its core is a 5.9-tonne liquid xenon Time Projection Chamber (TPC), surrounded by a neutron veto (to detect and reject neutron-induced background) and a muon veto (to identify and discard events caused by cosmic muons), all housed within a water tank. This advanced setup is dedicated to detecting the faint signals of dark matter interactions.

From kg to the Multi-Tonne Scale

The search for dark matter with the XENON program has been a journey of increasing scale and sensitivity. It began with the prototype detector XENON10 (15 kg Xe TPC, 2006-2007), pioneered by a group led by Professor Elena Aprile starting in 2002. This was followed by XENON100 (160 kg Xe, 2008-2016) and then the groundbreaking XENON1T (3.2 tonnes Xe, 2015-2018), the first to reach the tonne scale. This continuous development has culminated in the current generation XENONnT using a total of 8.6 tonnes from which 5.9 tonnes are enclosed by the TPC.

The Xenon Target

Xenon is an excellent choice for dark matter detectors due to several key properties. First, its atoms are quite “heavy” (high atomic number (Z = 54) and a range of mass numbers (A = 124 – 136)). This “heaviness” is beneficial because if a dark matter particle bumps into a xenon atom, it’s more likely to leave a detectable signal. Also, these “heavy” atoms are good at blocking other types of radiation that could confuse us. Importantly, because xenon has both even and odd mass number isotopes, it allows scientists to search not only for spin-independent but also for spin-dependent interactions with dark matter particles. Xenon is also a very dense liquid – about 3 times denser than water! This high density means we can pack a lot of it into a relatively small space, increasing the chance of a dark matter particle hitting something. Plus, it stays liquid at a very cold but achievable temperature (around -95 degrees Celsius). When a particle interacts with xenon, it gives off a tiny flash of ultraviolet light that our special light sensors can detect. And importantly, we can clean xenon to an incredible level of purity, removing anything that might interfere with our delicate search or create false signals.

XENONnT TPC: A Closer Look

The heart of the XENONnT experiment is its massive TPC. This cylindrical detector, with structural components made from PTFE (like Teflon), has a diameter of 134 cm and a height of 148 cm, enclosing a substantial 5.9 tonnes of ultra-pure liquid xenon. To observe the tiny flashes of light created when particles interact inside, the TPC is equipped with a total of 494 very sensitive light detectors called photomultiplier tubes (PMTs), which can be thought of as “eyes.” These “eyes” are arranged in two groups: 253 at the top and 241 at the bottom of the detector. This extensive PMT coverage is crucial for precisely measuring the initial scintillation light (S1) and the secondary light signal (S2), allowing scientists to reconstruct the details of particle interactions and distinguish potential dark matter signals from background events.

The Water Tank: Shield and Active Background Veto

The XENONnT detector is encased in a massive water tank, holding 700 tonnes of water doped with Gadolinium (Gd) and standing three stories tall. This serves as a crucial shield against cosmic rays and radioactivity from the surrounding rock deep underground. The water also actively helps us veto unwanted signals. Special light detectors in the water identify muons (energetic cosmic particles) by detecting the Cherenkov light they produce as they pass through. For specifically tagging neutrons, which can mimic dark matter signals, a dedicated neutron veto system encloses a 33-tonne volume around the TPC. This volume, confined by highly reflective panels made of expanded PTFE forming an octagonal prism, also contains the Gd-doped water. When neutrons interact within this veto region, they are captured by the Gadolinium, leading to the emission of detectable Cherenkov light that our detectors can see. By identifying these muons (throughout the tank) and neutrons (within the dedicated veto volume), we can effectively disregard events in the xenon that were likely caused by them, allowing us to focus on the faint potential signals of dark matter.

Purification is Key: Making Xenon Ultra-Clean

Every single piece of material used in XENONnT is meticulously screened for radioactivity to ensure we start out as clean as humanly possible. After carefully shielding our detector from cosmic rays and surrounding rock radioactivity, a crucial challenge remains: tiny impurities dissolved within the liquid xenon itself. These unwanted guests can either “snack” on the precious drifting electrons we’re trying to measure, or worse, they can be radioactive themselves, creating internal background flashes that we can’t shield against, so we must constantly clean and purify our xenon.

One method involves circulating the xenon through special purifiers that remove “electronegative” impurities like oxygen, which would otherwise gobble up our drifting electrons. Radioactive contaminants like krypton and radon are especially problematic because they mimic dark matter signals. For these we use a technique called “cryogenic distillation.” This clever process takes advantage of tiny differences in how easily each substance turns into a gas at very cold temperatures, allowing us to separate and remove the unwanted radioactive elements.

The result of all this effort is truly astounding: the xenon inside the center of our TPC is a billion times less radioactive than the human body! We are incredibly proud to have created what is, to our knowledge, the purest xenon on Earth, giving us the best possible chance to detect the elusive signals of dark matter.

Fine-Tuning Our Vision: The Importance of Calibration

To accurately identify potential dark matter signals, our detector needs to be perfectly “tuned.” This is where calibration comes in – it’s how we meticulously map out how much energy a particle deposits and exactly where it interacts within the xenon, ensuring our measurements are as accurate as possible.

We use various methods to achieve this precision. For external calibration, we place known radioactive materials outside the main xenon volume. For example, we use a neutron “gun” to shoot neutrons into the detector. These neutrons create nuclear recoils (NRs) in the xenon, mimicking the type of signal a WIMP dark matter particle is expected to produce. By studying the detector’s response to these known neutron interactions, we learn to identify potential dark matter signatures.

Even more crucial are internal calibration sources. These are special radioactive gases that can be safely mixed directly into the liquid xenon target for short periods. For instance, we introduce Radon-220 (Rn-220), which then decays to its daughter product Lead-212 (Pb-212). It is the beta decay of Pb-212 that generates electron recoils (ERs) – signals caused by electrons – allowing us to precisely map the detector’s response to these events uniformly throughout the entire xenon volume. Separately, Krypton-83m (Kr-83m), another internal source, is invaluable for understanding how both the light and charge signals are produced and collected, helping us characterize the detector’s fundamental behavior.

By constantly cross-referencing our detector’s responses with these known sources, we ensure our “eyes” (the PMTs) are seeing clearly, and our measurements are as accurate as possible. This meticulous calibration is essential for recognizing the subtle signatures of dark matter and for confidently stating our results.

The Digital Backbone: Data, Control, and Computing

While the TPC is the “eye” of our dark matter search, it needs a sophisticated digital brain and nervous system to function. This complex infrastructure handles everything from continuously monitoring the detector’s environment to capturing every tiny signal, and then processing vast amounts of information.

First, there’s Data Acquisition (DAQ). Think of this as the super-fast nervous system that connects directly to our 494 “eye” (PMT) sensors. Whenever a particle interacts in the xenon and creates those flashes of light, the PMTs convert that light into electrical signals. The DAQ system races to record these signals, timestamping them with extreme precision and converting them into digital data. This process happens constantly, generating a massive stream of raw information – megabytes per second – ready for analysis.

Next, we have Slow Control. This is like the detector’s health monitor and environmental manager. It constantly keeps an eye on critical parameters that affect the detector’s performance, such as the exact temperature and pressure of the liquid xenon, its purity levels, the voltage on our PMTs, and the status of our cryogenic (cooling) systems. Unlike the rapid DAQ, Slow Control works at a slower pace, continuously logging these conditions to ensure the detector operates stably and optimally, and alerting us to any issues.

Finally, all this raw data and environmental information feeds into our powerful Computing Infrastructure. This is where the real “brain” work happens. The enormous volume of data collected by DAQ needs to be stored, processed, and analyzed. High-performance computing clusters meticulously reconstruct each particle interaction, filtering out background noise, and performing complex statistical analyses to search for the elusive dark matter signals. This computing power also handles the storage of petabytes of data, making it accessible for scientists around the globe to collaboratively contribute to the discovery effort. Together, these systems form the indispensable digital backbone that transforms faint physical signals into scientific insights.

Unlocking the Universe's Secrets

While our primary mission with XENONnT is to directly detect dark matter particles, especially WIMPs, this incredibly sensitive detector is also a powerful tool for exploring a wide range of other fundamental mysteries in physics and astrophysics. Its ultra-low background environment and massive xenon target make it uniquely suited for a diverse scientific program.

Beyond WIMPs, XENONnT is searching for other elusive dark matter candidates, such as axions or dark photons, which might interact with our detector in different ways. Finding any of these would be a revolutionary discovery, fundamentally changing our understanding of the universe’s composition.

But the science doesn’t stop at dark matter. XENONnT is also a leading observatory for neutrinos, those famously tiny and ghostly particles. We can study solar neutrinos, which stream from the Sun’s core, offering insights into the nuclear fusion processes powering our star. We also look for a hypothetical, extremely rare nuclear process called neutrinoless double beta decay, which, if observed, would prove neutrinos are their own antiparticles and shed light on why there’s more matter than antimatter in the universe. Furthermore, XENONnT can measure Coherent Elastic Neutrino-Nucleus Scattering (CEvNS), an interaction predicted by the Standard Model, potentially leading to new ways to understand neutrino properties or even test new physics.

In essence, XENONnT is more than just a dark matter hunter; it’s a cutting-edge laboratory probing the very fabric of reality. By pushing the boundaries of sensitivity and cleanliness, it has the potential to reveal entirely new physics beyond our current understanding, opening new windows into the cosmos and the fundamental forces that govern it.

TPC

The Dual-Phase Time Projection Chamber (TPC) is the beating heart of the experiment. Located at the very center of the detector, surrounded by layers of shielding, it is the means by which we hope to eventually "see" dark matter.

Neutron Veto

The water-filled neutron veto is the volume of the detector which surrounds the central TPC. It aims to detect neutrons produced by radioactive impurities in the detector materials and other background neutrons, and thereby enables us to reject them as background.

Muon Veto

The muon veto is the outermost volume of the detector. It uses the Cherenkov light emitted by the muons that pass through it, in order to tag them and reject any muon background events.

DarkSide-20k: Argon-Based Detection

Stepping onto the global stage in the dark matter hunt is DarkSide-20k, a cutting-edge direct detection experiment located, like XENONnT, deep underground at the Gran Sasso Laboratory (LNGS) in Italy. Instead of liquid xenon, DarkSide-20k uses a massive liquid argon Time Projection Chamber (TPC).

The detector’s core contains 50 tonnes of highly purified, depleted liquid argon within its TPC, part of a total of 80 tonnes of depleted argon used in the system. This sensitive region is surrounded by an active 600-tonne liquid argon shield, absorbing background radiation.

This immense setup is designed for extraordinary sensitivity to WIMP dark matter, with projections indicating it will be even more sensitive than XENONnT. DarkSide-20k provides a crucial and complementary search, offering a different technology to cross-check any potential dark matter discovery, which is vital for validating such a groundbreaking find.

The Next-Generation Argon Experiment

DarkSide-20k is the largest and most ambitious experiment to date using liquid argon to directly search for dark matter. It builds directly upon the success of its predecessor, the DarkSide-50 experiment, which successfully demonstrated the power of using ultra-pure underground argon for dark matter searches.

Like its predecessor, DarkSide-20k is located deep underground at the Gran Sasso National Laboratory (LNGS) in Italy, benefiting from the natural shielding of the mountain. It’s currently under construction with operations planned to begin in 2027. Over its ten-year lifespan, DarkSide-20k aims for an unprecedented exposure, making it incredibly sensitive to the elusive dark matter particles known as WIMPs.

A critical goal for DarkSide-20k is to be a nearly “instrumental background-free” detector. This means scientists expect fewer than 0.1 background events to interfere with the WIMP search over the entire planned experiment. This ambitious goal is achieved through several innovative design features.

At the heart of DarkSide-20k is its central Time Projection Chamber (TPC), containing 50 tonnes of specially sourced underground argon (UAr). This TPC is then surrounded by an additional 30 tonnes of UAr in an inner “veto” region, further helping to suppress unwanted signals.

The Heart of DarkSide-20k: Inside the Liquid Argon TPC

At its heart, DarkSide-20k features a large dual-phase Liquid Argon Time Projection Chamber (TPC). It’s built around an octagonal barrel, a precise container about 3.5 meters tall and wide, holding 50 tonnes of ultra-pure underground argon.

The entire active volume is enclosed within an acrylic octagon. Its top and bottom lids are made of pure acrylic and are coated with a thin conductive material (Clevios™). The top lid doubles as the anode, and the bottom lid doubles as the cathode, together establishing the detector’s electric field. The walls of the octagon are also coated with a wavelength shifter, Tetra Phenyl Butadiene (TPB), and highly reflective foil to maximize light collection. Different from xenon, the light produced by argon upon particle interaction is in the far ultraviolet (VUV) range, specifically at 127 nm, which can’t be easily “seen” by standard commercial photo-detectors. Therefore, the TPB coating is essential, as it shifts this VUV light into the visible blue range (around 420 nm), making it detectable.

Along its sides, the acrylic barrel features machined and Clevios-coated conductive rings that form a field cage. These rings, connected by resistors, create a uniform and stable electric drift field of 200 V/cm, ensuring electrons drift upwards.

Both the initial (S1) and secondary (S2) light signals are captured by arrays of highly sensitive Silicon PhotoMultipliers (SiPMs). These advanced sensors are precisely positioned on two “Optical Planes,” located above the anode and below the cathode, to detect every photon.

From Contamination to Clarity: The Argon Story

Like its cousin xenon, argon is a fantastic material for hunting dark matter. It’s a noble gas that becomes a dense liquid when cooled, making it ideal for interactions with particles, and it glows with light when something passes through it. But for such a sensitive dark matter search, there’s a big hurdle: a tiny amount of natural radioactivity in everyday argon.

The main culprit is Atmospheric Argon (AAr). The argon we breathe actually contains a radioactive “cousin” called $^{39}$Ar. This isotope constantly undergoes a type of radioactive decay, creating a steady stream of signals. These signals are a huge problem because their energy looks very similar to what we expect from a dark matter particle, essentially masking any potential dark matter discovery. Every kilogram of atmospheric argon produces about one of these distracting decays every second.

DarkSide-20k’s clever solution is to use Underground Argon (UAr). This special argon is drawn from deep underground wells, like one in Colorado, USA. Because it has been buried for millions of years, it’s been naturally shielded from cosmic rays, which are what produce the troublesome $^{39}$Ar in the first place. This makes underground argon dramatically purer – over 1400 times less radioactive than atmospheric argon!

Once extracted, this already cleaner underground argon gets an extra step of purification. It’s sent to a special facility in Sardinia, Italy, where it’s run through a “cryogenic distillation column.” This process meticulously removes any remaining tiny impurities, ensuring the argon is as pristine as possible.

Using this incredibly low-radioactivity underground argon is the key to DarkSide-20k’s ambitious design. It’s what allows the experiment to achieve its goal of being a nearly “instrumental background-free” detector, meaning the detector itself generates almost no noise to hide a dark matter signal.

Listening to Light: Pulse Shape Discrimination

Beyond simply detecting light signals, DarkSide-20k employs a powerful technique called Pulse Shape Discrimination (PSD). This method is a foundational strength of argon-based detectors and allows us to distinguish between different types of particle interactions based on the unique “fingerprint” of the light pulses they produce.

When a charged particle interacts within the liquid argon, the emitted light isn’t a single, uniform flash. Instead, it’s composed of two distinct parts: a very “fast” component that decays in just 6 nanoseconds, and a “slow” component that lasts much longer, decaying in about 1600 nanoseconds. The ingenious part of PSD lies in how the relative strength of these two components varies depending on the type of particle that caused the interaction, allowing for precise particle identification.

For instance, Nuclear Recoils (NRs), which are the rare events we expect if a WIMP dark matter particle hits an argon nucleus, are highly ionizing and typically produce light pulses dominated by the fast component. In contrast, Electron Recoils (ERs), a significant source of unwanted background caused by electrons or gamma rays, are less ionizing and produce light pulses where the slow component is much more prominent. PSD can also effectively distinguish other heavily ionizing particles, like alpha particles, from potential dark matter signals.

The ability of PSD to powerfully differentiate between nuclear recoils (our potential dark matter signals) and electron recoils (our main background) is absolutely crucial for DarkSide-20k’s incredible sensitivity. When combined with other signal analysis techniques, PSD allows DarkSide-20k to achieve an exceptional electron recoil background rejection factor, essentially filtering out vast amounts of noise. This robust background discrimination is a key element in DarkSide-20k’s design goal of being a nearly “instrumental background-free” experiment, where almost no noise from the detector itself should interfere with the search.

Achieving the Impossible: The Background-Free Design

One of the most ambitious goals of DarkSide-20k is to operate as a nearly “instrumental background-free” detector. This means that during its entire planned operational lifetime – aiming for a massive 200 tonne-year exposure – scientists expect fewer than 0.1 events originating from the detector itself to appear in the crucial WIMP search region. In essence, it aims to be so incredibly clean that virtually no “noise” from the instrument or its surroundings will interfere with the hunt for a dark matter signal.

Achieving this unprecedented level of silence is the result of a multi-pronged strategy, building on several innovations:

Firstly, the use of Underground Argon (UAr) is paramount. As discussed, this specially sourced argon is naturally depleted of the radioactive isotope $^{39}$Ar, which is the dominant intrinsic background in atmospheric argon detectors. By starting with a target material that is already more than 1400 times purer, DarkSide-20k dramatically reduces internal radioactive interference.

Secondly, every single component used in the detector’s construction is rigorously screened for radioactivity. Only materials with the lowest possible levels of inherent radioactivity are selected, ensuring that the detector itself doesn’t introduce unwanted background events.

Thirdly, Pulse Shape Discrimination (PSD) provides an extremely powerful method for background rejection. This technique leverages the unique “fingerprint” of the light pulses produced by different particle interactions in liquid argon. By analyzing the subtle shape of these light signals, DarkSide-20k can effectively distinguish between potential dark matter interactions (nuclear recoils) and common background events (electron recoils), effectively filtering out a vast amount of unwanted noise.

Finally, an elaborate system of shielding and vetoes provides defense against external radiation. The central TPC and its immediate surroundings are encased within a massive 600-tonne active liquid argon shield. This vast volume of argon serves not only as a physical barrier but also actively detects and helps reject particles originating from outside the detector. Additionally, an inner veto region further enhances the capability to identify and reject challenging neutron backgrounds before they can mimic a dark matter signature.

By combining these innovative approaches – ultra-pure target material, meticulous material selection, advanced pulse shape discrimination, and multi-layered shielding – DarkSide-20k is designed to achieve an almost perfect silence, providing an unblemished window into the dark universe.

Exploring the Dark Universe

DarkSide-20k is designed with ambitious scientific goals, primarily focused on the direct detection of dark matter. Its cutting-edge technology and unparalleled background rejection open a wide window for discovery across various frontiers of particle astrophysics.

Its foremost objective is the direct search for Weakly Interacting Massive Particles (WIMPs), a leading candidate for dark matter. With its extraordinary sensitivity and “instrumental background-free” design, DarkSide-20k aims to explore vast uncharted territory in the WIMP mass range, from GeV to TeV scales, pushing the limits of current searches to unprecedented levels.

Beyond traditional WIMPs, DarkSide-20k’s capabilities extend to a broad spectrum of other compelling dark matter candidates. This includes the search for light dark matter, spanning from keV-scale particles (such as warm sterile neutrinos) to GeV-scale candidates, as well as extending sensitivity to very heavy dark matter candidates up to Planck-scale masses.

In addition to its primary dark matter mission, DarkSide-20k will also contribute significantly to neutrino physics. Its vast, ultra-pure liquid argon target and highly sensitive photodetectors will allow it to detect solar neutrino interactions, providing crucial insights into the inner workings of our Sun. Furthermore, it has the potential to observe hundreds of neutrino interactions from a galactic supernova, offering invaluable data on these cataclysmic cosmic events and the production of heavy elements in the universe. Ultimately, DarkSide-20k’s high sensitivity represents a significant step towards reaching the “neutrino floor,” the fundamental limit for direct dark matter searches where neutrino interactions become an unavoidable background.

Local R&D Efforts

Front view of the IMix system for studying the impurity behavior in dual-phase (liquid and gas) xenon
IMix setup at Pupin Hall

IMIX (Impurity Measurements in Xenon), utilizing major components from the original XENON10 detector, precisely tracks impurity behavior in dual-phase (liquid and gas) xenon. By sampling and analyzing both phases with a residual gas analyzer, we determine how impurities distribute between the liquid and gaseous xenon. This small-scale data is crucial for optimizing purification techniques in multi-tonne xenon dark matter detectors.

Photo of the Krypton distillation column itself, non-operational, as received at Columbia's Nevis Labs.
Kr Column at Nevis Labs

A Cryogenic Distillation column was initially used for the XENON100 experiment, successfully removing Krypton from xenon to achieve part-per-trillion levels of contamination. This system has since returned to Columbia, where it is now utilized as a valuable training facility for students.

The Xeclipse system at Columbia, used to test different purifier materials and techniques for the XENONnT experiment
Xeclipse setup at Pupin Hall

Xeclipse (Xenon Cryogenic Liquid Purification Setup) is a prototype liquid-phase purification system at Columbia. Originally serving as a cryogenic and purification demonstrator for XENON1T, it was later used to test different purifier materials and techniques for the XENONnT experiment, featuring a built-in purity monitor.

The DarkSide Radon Trap Test System (DSRTTS) precisely measures how effectively various charcoal materials remove radon from argon in its gas phase.
DSRTTS at Pupin Hall

The DSRTTS (DarkSide Radon Trap Test System) precisely measures how effectively various charcoal materials remove radon from argon in its gas phase. It uses a radon source for injection, a cooling system for precise trap temperature control down to 100K, and a radon detector to monitor removal. This setup can be upgraded to host a liquid argon detector for further studies.

The Outgassing Chamber, a specialized vacuum chamber used to evaluate the purity of detector materials.
Internal view of the outgassing setup

The Outgassing Chamber is a specialized vacuum chamber used to evaluate the purity of detector materials. It houses samples of plastics (like PTFE or acrylic) and, using a Residual Gas Analyzer (RGA), precisely measures impurity diffusion out of the material. Samples can also be cooled to 77K to mimic cryogenic detector temperatures, helping us select materials with minimal outgassing for ultra-low background experiments.

Photo of the now-out-of-comission NERiX setup at the CU lab.
neriX setup at Pupin Hall

NERIX (Nuclear and Electronic Recoils in Xenon) is a dual-phase detector capable of simultaneously measuring light and charge signals from low-energy interactions in liquid xenon. It was designed in the early 2010's to optimize event vertex reconstruction and light detection efficiency. By employing far detector coincidence techniques, NERIX helped characterize the light and charge yields of liquid xenon for different particle types as a function of energy.

Photo of an LXeGRIT flight
LXeGRIT taking flight in Palestine, TX

LXeGRIT (Liquid Xenon Gamma-Ray Imaging Telescope) was a balloon-borne experiment utilizing a liquid xenon TPC. Its purpose was to image gamma-ray emissions from cosmic sources within the 0.15 - 10 MeV energy band, effectively verifying the application of TPC technology for future space missions through three flight campaigns from the Northern Hemisphere.

Photo of the helical resonator from Columbia's ATTA project.
Helical resonator from the ATTA project

ATTA (Atomic Trap Trace Analysis) was a highly sensitive laser-based system. It was designed to trap and count trace isotopes of Krypton found within xenon, reaching an impressive sensitivity on the part-per-trillion level. These tests have concluded, and the system has recently been decommissioned.

IMix

IMIX (Impurity Measurements in Xenon), utilizing major components from the original XENON10 detector, precisely tracks impurity behavior in dual-phase (liquid and gas) xenon. By sampling and analyzing both phases with a residual gas analyzer, we determine how impurities distribute between the liquid and gaseous xenon. This small-scale data is crucial for optimizing purification techniques in multi-tonne xenon dark matter detectors.

Kr Column

A Cryogenic Distillation column was initially used for the XENON100 experiment, successfully removing Krypton from xenon to achieve part-per-trillion levels of contamination. This system has since returned to Columbia, where it is now utilized as a valuable training facility for students.

Xeclipse

Xeclipse (Xenon Cryogenic Liquid Purification Setup) is a prototype liquid-phase purification system at Columbia. Originally serving as a cryogenic and purification demonstrator for XENON1T, it was later used to test different purifier materials and techniques for the XENONnT experiment, featuring a built-in purity monitor.

DSRTTS

The DSRTTS (DarkSide Radon Trap Test System) precisely measures how effectively various charcoal materials remove radon from argon in its gas phase. It uses a radon source for injection, a cooling system for precise trap temperature control down to 100K, and a radon detector to monitor removal. This setup can be upgraded to host a liquid argon detector for further studies.

Outgassing

The Outgassing Chamber is a specialized vacuum chamber used to evaluate the purity of detector materials. It houses samples of plastics (like PTFE or acrylic) and, using a Residual Gas Analyzer (RGA), precisely measures impurity diffusion out of the material. Samples can also be cooled to 77K to mimic cryogenic detector temperatures, helping us select materials with minimal outgassing for ultra-low background experiments.

neriX

NERIX (Nuclear and Electronic Recoils in Xenon) is a dual-phase detector capable of simultaneously measuring light and charge signals from low-energy interactions in liquid xenon. It was designed to optimize event vertex reconstruction and light detection efficiency. By employing far detector coincidence techniques, NERIX helped characterize the light and charge yields of liquid xenon for different particle types as a function of energy.

LXeGRIT

LXeGRIT (Liquid Xenon Gamma-Ray Imaging Telescope) was a balloon-borne experiment utilizing a liquid xenon TPC. Its purpose was to image gamma-ray emissions from cosmic sources within the 0.15 – 10 MeV energy band, effectively verifying the application of TPC technology for future space missions through three flight campaigns from the Northern Hemisphere.

ATTA

ATTA (Atomic Trap Trace Analysis) was a highly sensitive laser-based system. It was designed to trap and count trace isotopes of Krypton found within xenon, reaching an impressive sensitivity on the part-per-trillion level. These tests have concluded, and the system has recently been decommissioned.