Grad students can apply now for ComSciCon’18!

Applications are now open for the Communicating Science 2018 workshop, to be held in Boston, MA on June 14-16, 2018!

Graduate students at U.S. and Canadian institutions in all fields of science, technology, engineering, health, mathematics, and related fields are encouraged to apply. The application deadline is March 1st.

Graduate student attendees of ComSciCon’17

As for past ComSciCon national workshops, acceptance to the workshop is competitive; attendance is free and travel support and lodging will be provided to accepted applicants.

Attendees will be selected on the basis of their achievement in and capacity for leadership in science communication. Graduate students who have engaged in entrepreneurship and created opportunities for other students to practice science communication are especially encouraged to apply.

Participants will network with other leaders in science communication and build the communication skills that scientists and other technical professionals need to express complex ideas to the general public, experts in other fields, and their peers. In additional to panel discussions on topics like Science Journalism, Creative & Digital Storytelling, and Diversity and Inclusion in Science, ample time is allotted for networking with science communication experts and developing science outreach collaborations with fellow graduate students.

You can follow this link to submit an application or learn more about the workshop programs and participants. You can also follow ComSciCon on Twitter (@comscicon) and use #comscicon18 !

Our group photo at ComSciCon’17

Longtime Astrobites readers may remember that ComSciCon was founded in 2012 by Astrobites and Chembites authors. Since then, we’ve led five national workshops on leadership in science communication and established a franchising model through which graduate student alums of our program have led sixteen regional and specialized workshops on training in science communication.

We are so excited about the impact ComSciCon has had on the science communication community. You can read more about our programs, the outcomes we have documented, find vignettes about our amazing graduate student attendees, and more in ComSciCon’s 2017 annual report.

The organizers of ComSciCon’17. Can you spot the astronomers?

None of ComSciCon’s impacts would be possible without the generous support of our sponsors. These contributions make it possible for us to offer this programming free of charge to graduate students, and to support their travel to our events. In particular, we wish to thank the American Astronomical Society for being a supporter of both Particlebites and ComSciCon.

If you believe in the mission of ComSciCon, you can support our program to! Visit our webpage to learn more and donate today!

Attendees react to a challenging section of a student’s Pop Talk at ComSciCon’17

It’s A Wrap! Summary of ATLAS Updates from 2016

Article: Latest ATLAS results from Run 2
Authors: Claudia Gemme on behalf of the ATLAS Collaboration
Reference: arXiv:1612.01987 [hep-ex]

2016 certainly has been an…interesting year. There’s been a lot of division, so as the year winds down, this seems like a perfect time to reflect on something we can all get excited about: particle physics! This has been an incredible year for the ATLAS experiment and the LHC in general. Run 2 began in 2015, but really hit its stride this year. The LHC reached a peak luminosity of 1.37 x 1034 cm-2s-1, which exceeds the design luminosity by almost 40%! Additionally, the pile up (number of interactions per bunch crossing) nearly doubled with respect to 2015. From these delivered events, ATLAS was able to record 30 fb-1 of data at 13 TeV center-of-mass energy, with a DAQ (data acquisition) efficiency above 90%.

Before discussing the many analyses being done with this amazing new data set, I’d like to highlight some of the upgrades performed during the long shutdown (2013-2014) that allowed ATLAS to perform so well during Run 2. One of the most important improvements was the addition of the Insertable B-layer (IBL). The IBL is now the innermost part of the inner detector, located only 3.3 cm from the interaction point. The IBL was designed to combat radiation damage to the inner detector; due to its insertable nature, it can eventually be replaced and it shields the other 3 detector layers from the bulk of the radiation damage. Of course, it also allows more tracking points which further improves track reconstruction. There were also extensive improvements to the magnetic and cryogenic systems to provide more powerful cooling and repair damage from Run 1. To deal with the increased data load, the ATLAS DAQ and trigger systems were also upgraded (reminder, triggers are data collection elements that decide which events get stored for analysis and which get thrown out). The High Level Trigger, ATLAS’s only hardware level trigger was updated to output 100kHz of data (previously 75kHz), and the 2 software level triggers were merged into one. This allowed ATLAS DAQ to have an average physics data output of 1kHz, allowing more of the Run 2 events to be processed and stored.

Now, lets talk about ATLAS’s physics program in 2016. A precise understanding of the Standard Model is incredibly important for all particle physics programs. It allows physicists to test theoretical mass and coupling predictions, and to make accurate predictions for background processes in BSM searches. ATLAS improved the precision of many SM measurements in 2016, and a summary of some important cross section measurements is shown in Figure 1. In particular, the measurements of the Z+jets and diboson cross sections were compatible with new next-to-next-leading-order calculations from theorists, confirming theoretical predictions.

Overview of cross-section measurements for a variety of SM processes compared to theoretical expectations

Another major goal of the Run 2 ATLAS physics program was to confirm the discovery of the Higgs Boson and further study it. During Run 1, both ATLAS and CMS found evidence of a Higgs boson with a combined measured mass of 125.09 GeV using the H→gg and H→ZZ*→4l channels. Furthermore, nearly all measured couplings were consistent with SM predictions within 2σ. In Run 2, ATLAS ‘rediscovered’ the Higgs at a compatible mass with a local significance of 10 (compared to 8.6 expected) using the same channels. The Run 2 cross section is slightly higher than the SM prediction, but still compatible within uncertainty. A summary of the cross-section measurements at various energies can be seen in Figure 2. Additionally, ATLAS physicists sought to show conclusive evidence of the H→bb decay channel in Run 2. This decay mode of the Higgs has the largest predicted branching fraction (58%) according to the SM, but has been difficult to measure due to large multi-jet backgrounds. The increased luminosity in Run 2 made studying the similar X+H→bb decay a promising alternative, despite its cross-section being much lower. This decay process is easier to isolate as leptonic decays of the W or Z create a clean signature. However, the measured significance of this decay was only 0.42, compared to a SM expectation of 1.94. The analysis procedure was well validated by measuring SM (W/Z)Z yield, so this large discrepancy is certainly an area for more study in 2017.

Total pp->H cross-sections measured at different center-of-mass energies compared to SM predictions

The final component of the ATLAS physics program is, of course, the many searches for BSM physics. The discovery potential for many of these processes is increased in Run 2 due to the enhanced cross-sections at the larger energy. There are 3 important channels for general BSM searches: diboson, diphoton, and dilepton. Many extensions of the SM predict new heavy particles including heavy neutral Higgs, Heavy Vector Triplet W, and some Gravitons, that could decay into vector-boson pairs. General searches in this channel are done by looking for hadronic decays of the boosted W and Z bosons within a single large-radius jet and using jet substructure properties. Unfortunately, no significant excess is observed. The diphoton channel became the hot topic of 2016, due to a deviation of at least 3σ from the SM only hypothesis seen in both ATLAS and CMS early this year using the 2015 data set. However, this excess was not confirmed with the full 2016 data set, which has 4x more statistics. The largest excess seen by ATLAS in the diphoton channel is now 2.3σ for a mass near 710 GeV. The dilepton final states have excellent sensitivity to a variety of new phenomena and have high signal selection efficiencies. Again, however, the 2016 measurements are consistent with the SM prediction. Lower limits on a resonance mass have been set, enhancing exclusion up to 1 TeV more than in Run 1.

ATLAS physicists also study the infamous SUSY model by looking for signatures of gluinos and squarks (predicted to be the lightest SUSY particles). These particles could be observed in events with high jet multiplicity and lots of missing energy. Once again, no significant excess was found. These results were interpreted within 2 SUSY models, and gluinos with mass up to 1600 GeV were excluded.

So, to conclude, no evidence of BSM physics has been found at ATLAS in Run 2, but the  new limits on some SUSY models and various other BSM phenomena have been improved and can be seen in Figures 3 and 4. Precision measurements of the SM were improved, the detector equipment was updated, and the Higgs was rediscovered, but ATLAS physicists and particle enthusiasts are still hoping for something more exciting. Lest we leave 2016 on a low note, its important to remember that only 50% of ATLAS searches have been updated to the Run 2 energy, so there are still many more channels to be explored. Plus, there are already some modest excesses, as well as the discrepancy in the H→bb measurement. There is certainly more to be discovered as Run 2 continues, so here’s to 2017!

Mass reach of selected ATLAS SUSY searches
Mass reaches of selected non-SUSY BSM searches at ATLAS

References and further reading:

 

Horton Hears a Sterile Neutrino?

Article: Limits on Active to Sterile Neutrino Oscillations from Disappearance Searches in the MINOS, Daya Bay, and Bugey-3 Experiments
Authors:  Daya Bay and MINOS collaborations
Reference: arXiv:1607.01177v4

So far, the hunt for sterile neutrinos has come up empty. Could a joint analysis between MINOS, Daya Bay and Bugey-3 data hint at their existence?

Neutrinos, like the beloved Whos in Dr. Seuss’ “Horton Hears a Who!,” are light and elusive, yet have a large impact on the universe we live in. While neutrinos only interact with matter through the weak nuclear force and gravity, they played a critical role in the formation of the early universe. Neutrino physics is now an exciting line of research pursued by the Hortons of particle physics, cosmology, and astrophysics alike. While most of what we currently know about neutrinos is well described by a three-flavor neutrino model, a few inconsistent experimental results such as those from the Liquid Scintillator Neutrino Detector (LSND) and the Mini Booster Neutrino Experiment (MiniBooNE) hint at the presence of a new kind of neutrino that only interacts with matter through gravity. If this “sterile” kind of neutrino does in fact exist, it might also have played an important role in the evolution of our universe.

Horton hears a sterile neutrino? Source: imdb.com

The three known neutrinos come in three flavors: electron, muon, or tau. The discovery of neutrino oscillation by the Sudbury Neutrino Observatory and the Super-Kamiokande Observatory, which won the 2015 Nobel Prize, proved that one flavor of neutrino can transform into another. This led to the realization that each neutrino mass state is a superposition of the three different neutrino flavor states. From neutrino oscillation measurements, most of the parameters that define the mixing between neutrino states are well known for the three standard neutrinos.

The relationship between the three known neutrino flavor states and mass states is usually expressed as a 3×3 matrix known as the PMNS matrix, for Bruno Pontecorvo, Ziro Maki, Masami Nakagawa and Shoichi Sakata. The PMNS matrix includes three mixing angles, the values of which determine “how much” of each neutrino flavor state is in each mass state. The distance required for one neutrino flavor to become another, the neutrino oscillation wavelength, is determined by the difference between the squared masses of the two mass states. The values of mass splittings m_2^2-m_1^2 and m_3^2-m_2^2 are known to good precision.

A fourth flavor? Adding a sterile neutrino to the mix

A “sterile” neutrino is referred to as such because it would not interact weakly: it would only interact through the gravitational force. Neutrino oscillations involving the hypothetical sterile neutrino can be understood using a “four-flavor model,” which introduces a fourth neutrino mass state, m_4, heavier than the three known “active” mass states. This fourth neutrino state would be mostly sterile, with only a small contribution from a mixture of the three known neutrino flavors. If the sterile neutrino exists, it should be possible to experimentally observe neutrino oscillations with a wavelength set by the difference between m_4^2 and the square of the mass of another known neutrino mass state. Current observations suggest a squared mass difference in the range of 0.1-10 eV^2.

Oscillations between active and sterile states would result in the disappearance of muon (anti)neutrinos and electron (anti)neutrinos. In a disappearance experiment, you know how many neutrinos of a specific type you produce, and you count the number of that type of neutrino a distance away, and find that some of the neutrinos have “disappeared,” or in other words, oscillated into a different type of neutrino that you are not detecting.

A joint analysis by the MINOS and Daya Bay collaborations

The MINOS and Daya Bay collaborations have conducted a joint analysis to combine independent measurements of muon (anti)neutrino disappearance by MINOS and electron antineutrino disappearance by Daya Bay and Bugey-3. Here’s a breakdown of the involved experiments:

  • MINOS, the Main Injector Neutrino Oscillation Search: A long-baseline neutrino experiment with detectors at Fermilab and northern Minnesota that use an accelerator at Fermilab as the neutrino source
  • The Daya Bay Reactor Neutrino Experiment: Uses antineutrinos produced by the reactors of China’s Daya Bay Nuclear Power Plant and the Ling Ao Nuclear Power Plant
  • The Bugey-3 experiment: Performed in the early 1990s, used antineutrinos from the Bugey Nuclear Power Plant in France for its neutrino oscillation observations
Screen Shot 2016-09-12 at 10.22.49 AM
MINOS and Daya Bay/Bugey-3 combined 90% confidence level limits (in red) compared to the LSND and MiniBooNE 90% confidence level allowed regions (in green/purple). Plots the mass splitting between mass states 1 and 4 (corresponding to the sterile neutrino) against a function of the \mu-e mixing angle, which is equivalent to a function involving the 1-4 and 2-4 mixing angles. Regions of parameter space to the right of the red contour are excluded, counting out the majority of the LSND/MiniBooNE allowed regions. Source: arXiv:1607.01177v4.

Assuming a four-flavor model, the MINOS and Daya Bay collaborations put new constraints on the value of the mixing angle \theta_{\mu e}, the parameter controlling electron (anti)neutrino appearance in experiments with short neutrino travel distances. As for the hypothetical sterile neutrino? The analysis excluded the parameter space allowed by the LSND and MiniBooNE appearance-based indications for the existence of light sterile neutrinos for \Delta m_{41}^2 < 0.8 eV^2 at a 95% confidence level. In other words, the MINOS and Daya Bay analysis essentially rules out the LSND and MiniBooNE inconsistencies that allowed for the presence of a sterile neutrino in the first place. These results illustrate just how at odds disappearance searches and appearance searches are when it comes to providing insight into the existence of light sterile neutrinos. If the Whos exist, they will need to be a little louder in order for the world to hear them.

 

Background reading:

Dragonfly 44: A potential Dark Matter Galaxy

Title: A High Stellar Velocity Dispersion and ~100 Globular Clusters for the Ultra Diffuse Galaxy Dragonfly 44

PublicationApJ, v828, Number 1, arXiv: 1606.06291

The title of this paper sounds like some standard astrophysics analyses; but, dig a little deeper and you’ll find – what I think – is an incredibly interesting, surprising and unexpected observation.

The Coma Cluster: NASA, ESA, and the Hubble Heritage Team (STScI/AURA)

Last year, using the WM Keck Observatory and the Gemini North Telescope in Manuakea, Hawaii, the Dragonfly Telephoto Array observed the Coma cluster (a large cluster of galaxies in the constellation Coma – I’ve included a Hubble Image to the left). The team identified a population of large, very low surface brightness (ie: not a lot of stars), spheroidal galaxies around an Ultra Diffuse Galaxy (UDG) called Dragonfly 44 (shown below). They determined that Dragonfly 44 has so few stars that gravity could not hold it together – so some other matter had to be involved – namely DARK MATTER (my favorite kind of unknown matter).

 

The ultra-diffuse galaxy Dragonfly 44. The galaxy consists almost entirely of dark matter. It is surrounded by faint, compact sources. Image credit: Pieter van Dokkum / Roberto Abraham / Gemini Observatory / SDSS / AURA.
The ultra-diffuse galaxy Dragonfly 44. The galaxy consists almost entirely of dark matter. It is surrounded by faint, compact sources. Image credit: Pieter van Dokkum / Roberto Abraham / Gemini Observatory / SDSS / AURA

The team used the DEIMOS instrument installed on Keck II to measure the velocities of stars for 33.5 hours over a period of six nights so they could determine the galaxy’s mass. Observations of Dragonfly 44’s rotational speed suggest that it has a mass of about one trillion solar masses, about the same as the Milky Way. However, the galaxy emits only 1% of the light emitted by the Milky Way. In other words, the Milky Way has more than a hundred times more stars than Dragonfly 44. I’ve also included the Mass-to-Light ratio plot vs. the dynamical mass. This illustrates how unique Dragonfly 44 is compared to other dark matter dominated galaxies like dwarf spheroidal galaxies.

 

 

MLratio
Relation between dynamical mass-to-light ratio and dynamical mass. Open symbols are dispersion-dominated objects from Zaritsky, Gonzalez, & Zabludoff (2006) and Wolf et al. (2010). The UDGs VCC 1287 (Beasley et al. 2016) and Dragonfly 44 fall outside of the band defined by the other galaxies, having a very high M/L ratio for their mass.

What is particularly exciting is that we don’t understand how galaxies like this form.

Their research indicates that these UDGs could be failed galaxies, with the sizes, dark matter content, and globular cluster systems of much more luminous objects. But we’ll need to discover more to fully understand them.

 

 

 

 

 

 

 

 

Further reading (works by the same authors)
Forty-Seven Milky Way-Sized, Extremely Diffuse Galaxies in the Coma Cluster,arXiv: 1410.8141
Spectroscopic Confirmation of the Existence of Large, Diffuse Galaxies in the Coma Cluster: arXiv: 1504.03320