-
Karri Folan Di Petrillo (University of Chicago)8/7/25, 9:00 AM
-
Dr LianTao Wang8/7/25, 9:15 AM
-
M SPIROPULU (CALTECH)8/7/25, 9:40 AM
-
Prof. Vladimir Shiltsev (NIU)8/7/25, 10:05 AM
-
Sergo Jindariani (Fermilab)8/7/25, 11:00 AM
-
Ryuichiro Kitano8/7/25, 11:25 AM
-
Dr Rebecca Taylor (CERN)8/7/25, 11:50 AM
-
Gregory Penn, Gregory Penn (Yale University)8/7/25, 2:00 PM
(15'+3')
Go to contribution page -
Caroline Riggall (University of Tennessee)8/7/25, 2:00 PM
-
Richard Ruiz8/7/25, 2:00 PM
-
Rose Powers (Princeton University)8/7/25, 2:18 PM
(15'+3')
Go to contribution page -
Rodolfo Capdevilla, Rodolfo Capdevilla (Fermilab)8/7/25, 2:18 PM
-
Kyle Capobianco-Hogan (Stony Brook University)8/7/25, 2:20 PM
-
John Dervan (Northeastern University)8/7/25, 2:36 PM
(15'+3')
Go to contribution page -
Yang Ma (UCLouvain)8/7/25, 2:36 PM
-
Austin Hoover (ORNL)8/7/25, 2:40 PM
-
Arthur Wu (University of Pittsburgh)8/7/25, 2:54 PM
-
Angira Rastogi (Lawrence Berkeley National Laboratory)8/7/25, 2:54 PM
(15'+3')
Go to contribution page -
Dr Katsuya Yonehara (Fermilab)8/7/25, 3:00 PM
-
Yu-Chen Guo (University of Pittsburgh (Liaoning Normal University))8/7/25, 3:12 PM
-
Matheus Hostert (Harvard), Matheus Hostert (Harvard University)8/7/25, 3:12 PM
(3'+15')
Go to contribution page -
8/7/25, 3:20 PM
-
Ken Cecire8/7/25, 4:00 PM
-
Simone Pagan Griso (Lawrence Berkeley National Laboratory)8/7/25, 4:15 PM
-
Nadia Pastrone (INFN Torino (IT))8/7/25, 4:40 PM
-
Sridhara Dasu (University of Wisconsin), Sridhara Dasu (University of Wisconsin - Madison)8/7/25, 5:05 PM
-
Dr Cari Cesarotti8/8/25, 9:00 AM
-
Cristian Pena8/8/25, 9:30 AM
-
Murtaza Safdari8/8/25, 10:00 AM
-
Pouya Asadi (University of Oregon), Pouya Asadi8/8/25, 11:00 AM
-
Jennifer Ott, Jennifer Ott (University of Hawaii at Manoa)8/8/25, 11:00 AM
-
Dr Luca Bottura8/8/25, 11:00 AM
-
Peiran Li (University of Minnesota)8/8/25, 11:18 AM
-
Artur Apreysan8/8/25, 11:18 AM
-
Dr Ramesh Gupta (Brookhaven National Labortaory)8/8/25, 11:20 AM
-
Darin Acosta8/8/25, 11:36 AM
-
Samuel Homiller (Cornell University)8/8/25, 11:36 AM
-
Dillon Merenich (NIU)8/8/25, 11:40 AM
-
Grace Cummings (Fermi National Accelerator Laboratory (US))8/8/25, 11:54 AM
-
Ishman Mahbub8/8/25, 11:54 AM
-
Dr Zenghai Li (SLAC)8/8/25, 12:00 PM
-
Dr Rohith Saradhy (University of Minnesota)8/8/25, 12:12 PM
-
8/8/25, 12:20 PM
-
Diktys Stratakis (Fermilab)8/8/25, 2:00 PM
-
Adrian Thompson, Adrian Thompson (Northwestern University)8/8/25, 2:00 PM
-
Benjamin Rosser (The University of Chicago)8/8/25, 2:00 PM
-
Julia Gehrlein (Colorado State University)8/8/25, 2:18 PM
-
Rocky Bala Garg8/8/25, 2:18 PM
-
Dr Emma Snively (SLAC)8/8/25, 2:20 PM
-
Abhijith Gandrakota (Fermilab)8/8/25, 2:36 PM
-
Gray Putnam, Nicholas Kamp (Harvard University)8/8/25, 2:36 PM
-
8/8/25, 2:40 PM
-
Kevin Pedro (Fermilab)8/8/25, 2:54 PM
-
Keping Xie (Michigan State University)8/8/25, 2:54 PM
-
8/8/25, 3:12 PM
-
Matheus Hostert (Harvard)8/8/25, 4:00 PM
-
Benjamin Rosser (The University of Chicago)8/8/25, 4:25 PM
-
Dr Steve Gourlay (Fermilab)8/8/25, 4:35 PM
-
Dr Zahra Tabrizi (University of Pittsburgh)8/8/25, 4:45 PM
-
8/8/25, 4:55 PM
-
Karri Folan Di Petrillo (University of Chicago)8/8/25, 5:15 PM
-
Julia Gehrlein (Colorado State University)Poster
The next generation of neutrino oscillation experiments, JUNO, DUNE, and HK, are under construction now and will collect data over the next decade and beyond. As there are no approved plans to follow up this program with more advanced neutrino oscillation experiments, we consider here one option that had gained considerable interest more than a decade ago: a neutrino factory. Such an...
Go to contribution page -
Rithika Ganesan (University of Tennessee)Poster
Muons produced through pion decay have high emittances, occupying a large volume in phase space. Hence, cooling is required to reduce the muon phase space density before acceleration. Traditional cooling schemes are too slow to be practical for muon beams. A novel technique proposed for muon colliders, ionization cooling, is instead considered. Muons are passed through absorbers, where they...
Go to contribution page -
Mira Littmann (The University of Chicago)Poster
A future 10TeV muon collider presents exciting opportunities for the direct detection of charged long-lived particles. We present here a study of long-lived staus, using gauge-mediated supersymmetry breaking as a benchmark model. The stau decays into a tau and a gravitino, with the gravitino as a dark matter candidate. Analysis of stau reconstruction efficiency provides insight into the...
Go to contribution page -
Stefano Tognini (Oak Ridge National Laboratory)Poster
The collider and detector proposed by the International Muon Collider Collaboration (IMCC) will reach a 10 TeV physics frontier as a means to fully understand the Higgs and explore new physics beyond LHC production capabilities. A muon collider has significant advantages, but comes with many challenges. One of such is the detector simulation, and in particular the beam-induced background (BIB)...
Go to contribution page -
Ryan Michaud (The University of Chicago)Poster
A future 10 TeV muon collider holds significant promise, enabling precise, percent-level measurements of Standard Model Properties. However, we must first produce, accelerate, and collide muons before they decay. The process begins by accelerating a proton beam and colliding it with a target, producing a “basketball-sized” cloud of muons. In the next step, known as cooling, this muon cloud is...
Go to contribution page -
Cici Hanna (Princeton University)Poster
A top priority for muon collider development is the creation of a demonstrator project to establish the feasibility of cooling a muon beam to the required emittance for a collider. The experiments designed for this demonstrator must present evidence of an appropriate reduction in transverse emittance that is robust enough to convince the physics community of the viability of a full collider....
Go to contribution page -
Agustin Romero (Stanford University)Poster
We apply the Soft Collinear Effective Theory for QCD to muon-antimuon collisions that produce two exclusive jets. The hard scattering amplitude for muon-antimuon to q-qbar is matched from full QCD to SCET at Next to Leading Order. We calculate the differential thrust cross section using the matched Wilson coefficients at NLO for the hard function, and the soft functions and jet functions are...
Go to contribution page -
Grace Cummings (Fermi National Accelerator Laboratory (US))Poster
Homogeneous inorganic scintillator-based calorimeters are the gold standard for electromagnetic energy resolution, but often degrade the hadronic energy resolution achievable at colliders. By incorporating the dual readout technique, we seek to improve the hadronic energy resolution of these calorimeters through the measurement and separation of the scintillation and Cherenkov light in...
Go to contribution page -
Pouya AsadiPoster
I will review the reach of a future 10TeV muon collider in the parameter space of fermion portal dark matter models in the freeze-in regime.
Go to contribution page
I study different fermion portal models and show that, in the freeze-in regime, their parameter space is bounded from all directions.
Different fermion portal models give rise to a host of interesting prompt or long-lived particle signals.
I will show... -
Dr Rebecca Taylor (CERN)Poster
Final Cooling is an optimisation problem: Transverse emittance goes down inverse-exponentially, whereas longitudinal emittance increases exponentially.
Go to contribution page
The system is simplified to consider only absorber length, initial energy and energy spread, then a genetic algorithm is applied to minimize both emittances.
Once a solution is chosen, a more advanced lattice design can be constructed.
A... -
Ruaa Alharthy (University of Wisconsin-Madison)Poster
This study investigates the optimization of pion and muon yields from an 8GeV proton beam incident on a graphite target, as part of a design effort for a muon collider demonstrator. The primary objective is to determine the optimal geometric configuration between the target and a solenoidal capture channel to maximize secondary particle production while mitigating potential damage from...
Go to contribution page -
Caroline Riggall (University of Tennessee)
Having an initial cooling stage is essential to reducing the 6D beam emittance early in the channel. Traditional cooling schemes use dipole fields to generate dispersion, selectively passing higher-momentum particles through more absorbing material. The problem with this approach is the charge-specificity of the dispersion function -- necessitating separate channels for $\mu^+$ and $\mu^-$....
Go to contribution page -
Keping Xie (Michigan State University)Poster
Axion-like particles (ALPs) are well-motivated extensions of the Standard Model (SM) that appear in many new physics scenarios, with masses spanning a broad range. In this work, we systematically study the production and detection prospects of light ALPs at future lepton colliders, including electron-positron and multi-TeV muon colliders. At lepton colliders, light ALPs can be produced in...
Go to contribution page -
Katsuya Yonehara (Fermilab)Poster
The muon collider target must accept extremely intense proton beams and efficiently produce secondary pions. These pions, which span a broad momentum spectrum, must then be captured and transported to a decay channel. In this presentation, I will introduce recent developments in high-power target systems for various accelerator applications and discuss potential design options for muon...
Go to contribution page -
Dr Delbert Larson (Particle Beam Lasers, Inc.)Poster
Abstract. Skrinsky and Parkhomchuk introduced the concept of ionization cooling in 1981[1] and the muon collider concept was proposed by Neuffer in 1983[2]. Considerable progress has been made on muon collider design, with one baseline design being established by Palmer, et al.[3] in 1995. Present conceptual designs for a muon collider start with a proton beam driver. The protons are directed...
Go to contribution page -
Aubrey Zhang (The University of Chicago)Poster
A major challenge to achieve the requisite beam luminosity for a muon collider is to cool the muon beams generated from targets by up to five orders of magnitude in 6D emittance. Ionization cooling is a promising method that has been proposed in the past. However, given the unavoidable performance tradeoffs in any cooling system, creating a design that effectively meets requirements poses an...
Go to contribution page -
Jullian Watts (University of Tennessee)Poster
MAIA (Muon Accelerator Instrumented Apparatus) is a detector concept for a 10 TeV muon collider, designed for precision studies of the standard model as well as searches for new physics. Efficient electron reconstruction and identification is essential, as electrons are commonly produced in key processes such as Higgs boson decays. It is difficult to efficiently reconstruct electrons in this...
Go to contribution page -
Devlin Jenkins (University of Tennessee Knoxville)Poster
Accurate and efficient simulations are necessary for the research and development of particle colliders. A current muon collider design, MAIA, has tungsten nozzles that create a significant amount of initial showering when a particle interacts with them. This is by design in practice, however, it results in a largely unnecessary CPU time during simulation. DDSim tracks each particle...
Go to contribution page -
Cheng-Hsu NeePoster
This poster presents simulation studies aimed at optimizing the design of the graphite target and capture system for the Muon Collider demonstrator, potentially at Fermilab. Using the G4Beamline simulation framework, we model proton interactions with a graphite target to analyze charged pion production and capture along the target axis, categorizing production mechanisms (primary, secondary,...
Go to contribution page -
-
Yu-Chen Guo (University of Pittsburgh & Liaoning Normal University)Poster
The study of electroweak gauge boson self-couplings at a muon collider provides a opportunity to probe new physics and deepen our understanding of electroweak symmetry breaking. At multi-TeV, the muon collider effectively acts as a vector boson collider, as vector boson scattering (VBS) becomes the dominant production mechanism due to logarithmic enhancements from gauge boson radiation....
Go to contribution page -
Kyle Capobianco-Hogan (Stony Brook University)Poster
We present a preliminary lattice based on a bottom up design for a rapidly cycling synchrotron (RCS) accelerator chain for a multi-TeV muon collider based at Fermilab. The RCS rings range in circumference from 6.28 km (that of the Tevatron) to 15.5 km (the current estimate for the maximum that can be accommodated at the Fermilab site). Each ring is either a conventional RCS (consisting of...
Go to contribution page -
Rose Powers (Princeton University)Poster
Powerful superconducting (SC) magnets are the workhorses of energy-frontier colliders. The magnetic field strengths required to achieve necessary beam acceleration and cooling at a 10 TeV Muon Collider are projected to reach 20-30T, between 2 to 4 times the strength of the SC electromagnets currently in operation at the Large Hadron Collider (LHC) [1]. In addition to high field strength, these...
Go to contribution page -
Ethan Martinez (Yale University)Poster
The tau lepton plays a crucial role in probing the Standard Model, offering access to both the Higgs and leptonic sectors of physics. However, reconstructing the tau is inherently challenging due to the fact that it decays before reaching the detector region and must be identified through its decay products. This becomes even more difficult in a muon collider environment, which is subject to...
Go to contribution page -
Inci Karaaslan (The University of Chicago)Poster
As one of the main proposed future colliders that will allow us to reach energy scales that can probe Beyond the Standard Model phenomena, muon colliders come with unique challenges. To achieve the desired luminosity, namely 1, 10, and 20 ab-1 for 3, 10, and 14 TeV, respectively, the six-dimensional emittance of the muon beam needs to be reduced significantly in a process described as muon...
Go to contribution page -
Eliza Howard (The University of Chicago), Tsz Ngong You (The University of Chicago)Poster
With the introduction of beam-induced background from the decay of muons in the beam pipe of future muon colliders, new techniques must be implemented to filter out the large volume of data generated by such events. The potential presence of long-lived novel particles, which evade conventional time-based cuts, motivates the development of geometrical differentiation methods at the on-chip...
Go to contribution page -
Daniel Abadjiev (The University of Chicago)Poster
At a 10TeV muon collider, a high level of beam induced background (BIB) will overlay signal produced from muon collisions, similar to how pile-up at the HL-LHC will overlay signal from proton-proton collisions. On-detector differentiation of BIB from signal would improve performance of the inner pixel tracker. For the HL-LHC, we are developing a “smartpixel” application specific integrated...
Go to contribution page -
Abdollah Mohammadi (UW-Madison)Poster
We present an algorithm that intends to reconstruct the hadronic decay of the tau lepton in muon collider using MAIA detector.
Go to contribution page
This algorithm aims to reconstruct tau lepton in all hadronic decay modes, including single-pion, three-pion, and single-pion plus neutral hadrons, by combining the tracker and EM clusters in the events.
Hadronic tau reconstruction efficiency in terms of the... -
Innes Bigaran
Choose timezone
Your profile timezone: