IceCube Collaboration’s scientific contributions

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Publications (93)


Figure 1: Left: a plot of the binned Monte Carlo event distribution, binned in the space of reconstructed log energy (log 10 (í µí°¸∕GeV)) and the cosine of the reconstructed declination angle (cos í µí¼ƒ). The color scale indicates the number í µí± of events in each bin. To generate this distribution, all nuisance parameters are held at their prior central value. Right: in contrast, a pull plot that compares another Monte Carlo event distribution with the one on the left, assuming the prior central values of all nuisance parameters, with the exception of DOMEfficiency, which has been increased by two times its prior width. The color scale indicates the pull value comparing a new bin count í µí± +2í µí¼Ž with í µí±. The deficit in the bottom rows of the pull plot is due to the DOMEfficiency shifting lower energy events to higher energies, and these rows contain the lowest energy events in the sample.
Figure 3: The result of minimization for a single fit, comparing the best-fit and initial value of the nuisance parameters, using í µí¼Ž, the number of prior standard deviations away from the prior value. The parameter astroPivot has a uniform prior, and no influence on the shape of the flux, and therefore little effect on the likelihood. Hence there is no preferred value to be recovered.
GollumFit: An IceCube Open-Source Framework for Binned-Likelihood Neutrino Telescope Analyses
  • Preprint
  • File available

June 2025

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1 Read

IceCube Collaboration

We present GollumFit, a framework designed for performing binned-likelihood analyses on neutrino telescope data. GollumFit incorporates model parameters common to any neutrino telescope and also model parameters specific to the IceCube Neutrino Observatory. We provide a high-level overview of its key features and how the code is organized. We then discuss the performance of the fitting in a typical analysis scenario, highlighting the ability to fit over tens of nuisance parameters. We present some examples showing how to use the package for likelihood minimization tasks. This framework uniquely incorporates the particular model parameters necessary for neutrino telescopes, and solves an associated likelihood problem in a time-efficient manner.

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Fast Low Energy Reconstruction using Convolutional Neural Networks

IceCube is a Cherenkov detector instrumenting over a cubic kilometer of glacial ice deep under the surface of the South Pole. The DeepCore sub-detector lowers the detection energy threshold to a few GeV, enabling the precise measurements of neutrino oscillation parameters with atmospheric neutrinos. The reconstruction of neutrino interactions inside the detector is essential in studying neutrino oscillations. It is particularly challenging to reconstruct sub-100 GeV events with the IceCube detectors due to the relatively sparse detection units and detection medium. Convolutional neural networks (CNNs) are broadly used in physics experiments for both classification and regression purposes. This paper discusses the CNNs developed and employed for the latest IceCube-DeepCore oscillation measurements. These CNNs estimate various properties of the detected neutrinos, such as their energy, direction of arrival, interaction vertex position, flavor-related signature, and are also used for background classification.


Measurement of the inelasticity distribution of neutrino-nucleon interactions for 80 GeV<Eν<560 GeV\mathbf{80~GeV<E_{\nu}<560~GeV} with IceCube DeepCore

February 2025

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18 Reads

IceCube Collaboration

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M. Ackermann

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V. Aushev

We report a measurement of the inelasticity distribution in the scattering of neutrinos of energy 8056080-560 GeV off nucleons, which is sensitive to the inclusive differential cross section. This analysis is based on a sample of atmospheric muon neutrinos detected in the IceCube sub-array DeepCore during 2012-2021, and is the first such measurement in this energy range. Our measurement extends to energies where accelerator data is not available, hence we compare our results to predictions from perturbative QCD calculations, finding good agreement.


FIG. 1. Differential upper limit (90 % CL) on the neutrino flux. The differential limit is compared to the IceCube 9 year result [23], the limit by Auger [58], and cosmogenic neutrino flux models [10, 11, 13, 20] and a UHE astrophysical model [53]. The model from [20] assumes γ = 2.5, Emax = 10 20 eV, m = 3.4 and a 10 % proton fraction. The Auger limit is re-scaled to all-flavor, decade-wide bins for comparison.
FIG. 3. Constraints on the proton fraction (fp) of UHECRs as a function of source evolution parameter m at 90 % CL based on the non-observation of UHE neutrinos in this study. The excluded region is shown for the two source evolution models SE1(z) (blue) and SE2(z) (orange).
A search for extremely-high-energy neutrinos and first constraints on the ultra-high-energy cosmic-ray proton fraction with IceCube

February 2025

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51 Reads

We present a search for the diffuse extremely-high-energy neutrino flux using 12.6 years of IceCube data. The non-observation of neutrinos with energies well above 10PeV10 \, \mathrm{PeV} constrains the all-flavor neutrino flux at 1018eV10^{18} \, \mathrm{eV} to a level of E2Φνe+νμ+ντ108GeVcm2s1sr1E^2 \Phi_{\nu_e + \nu_\mu + \nu_\tau} \simeq 10^{-8} \, \mathrm{GeV} \, \mathrm{cm}^{-2} \, \mathrm{s}^{-1} \, \mathrm{sr}^{-1}, the most stringent limit to date. Using this data, we constrain the proton fraction of ultra-high-energy cosmic rays (UHECRs) above 30EeV\simeq 30 \, \mathrm{EeV} to be 70\lesssim 70\,% (at 9090\,% CL) if the cosmological evolution of the sources is comparable to or stronger than the star formation rate. This result complements direct air-shower measurements by being insensitive to uncertainties associated with hadronic interaction models. It is the first such result to disfavor the ``proton-only" hypothesis for UHECRs using neutrino data.



Search for Galactic core-collapse supernovae in a decade of data taken with the IceCube Neutrino Observatory

August 2023

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67 Reads

The IceCube Neutrino Observatory has been continuously taking data to search for O(0.5-10) s long neutrino bursts since 2007. Even if a Galactic core-collapse supernova is optically obscured or collapses to a black hole instead of exploding, it will be detectable via the O(10) MeV neutrino burst emitted during the collapse. We discuss a search for such events covering the time between April 17, 2008 and December 31, 2019. Considering the average data taking and analysis uptime of 91.7% after all selection cuts, this is equivalent to 10.735 years of continuous data taking. In order to test the most conservative neutrino production scenario, the selection cuts were optimized for a model based on a 8.8 solar mass progenitor collapsing to an O-Ne-Mg core. Conservative assumptions on the effects of neutrino oscillations in the exploding star were made. The final selection cut was set to ensure that the probability to detect such a supernova within the Milky Way exceeds 99%. No such neutrino burst was found in the data after performing a blind analysis. Hence, a 90% C.L. upper limit on the rate of core-collapse supernovae out to distances of ~ 25kpc was determined to be 0.23/yr. For the more distant Magellanic Clouds, only high neutrino luminosity supernovae will be detectable by IceCube, unless external information on the burst time is available. We determined a model-independent limit by parameterizing the dependence on the neutrino luminosity and the energy spectrum.


FIG. 3. Distribution of the average charge observed by the DOMs for events at Level 5 of the selection (see Sec. III), compared to expectation from simulation of neutrinos, muons and detector noise. Data are shown for the same time period in 2014, before (Pass 1) and after the SPE calibration described in the text (Pass 2).
FIG. 12. Output probability score distribution from the PID algorithm for the different interaction types. Distributions are normalized to better visualize shape differences.
FIG. 13. Reduced chi-square from the SANTA track hypothesis fit.
FIG. 14. Proxy for direction of travel calculated using the uppermost 15 layers of IceCube DOMs. Only events with at least 4 hits in those layers are included in the histograms.
FIG. 19. Example of a hypersurface function in one bin projected on the DOM efficiency dimension. Each data point corresponds to one systematic set. Translucent datapoints are from sets where one or more systematic parameter besides DOM efficiency is off-nominal. Those points are projected along the fitted plane to the nominal point. Several systematic sets have a nominal DOM efficiency of 1.0. The band shows to the standard deviation of the fitted function.
Measurement of Atmospheric Neutrino Mixing with Improved IceCube DeepCore Calibration and Data Processing

April 2023

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92 Reads

We describe a new data sample of IceCube DeepCore and report on the latest measurement of atmospheric neutrino oscillations obtained with data recorded between 2011-2019. The sample includes significant improvements in data calibration, detector simulation, and data processing, and the analysis benefits from a detailed treatment of systematic uncertainties, with significantly higher level of detail since our last study. By measuring the relative fluxes of neutrino flavors as a function of their reconstructed energies and arrival directions we constrain the atmospheric neutrino mixing parameters to be sin2θ23=0.51±0.05\sin^2\theta_{23} = 0.51\pm 0.05 and Δm322=2.41±0.07×103eV2\Delta m^2_{32} = 2.41\pm0.07\times 10^{-3}\mathrm{eV}^2, assuming a normal mass ordering. The resulting 40\% reduction in the error of both parameters with respect to our previous result makes this the most precise measurement of oscillation parameters using atmospheric neutrinos. Our results are also compatible and complementary to those obtained using neutrino beams from accelerators, which are obtained at lower neutrino energies and are subject to different sources of uncertainties.


Figure 1. The spatial distribution of FRBs in equatorial coordinates. The 22 unique, nonrepeating FRBs are shown in red and FRB 121102 is shown in blue. FRB 121102 is an extragalactic source located at a decl. of 33° . 15 (Spitler et al. 2014).
Figure 2. The 90% confidence level upper limits as a function of time-window duration. We assume power-law spectra of E −2 (left) and E −3 (right) for the timeintegrated neutrino fluxes. The Six Year Southern Tracks and All-Sky Tracks analyses used statistically independent events; they are included in addition to our limits. Note that the previous IceCube analyses used symmetric time windows that are centered on the FRB to search for neutrino emission; this analysis only searches for neutrino emission after an FRB has occurred. Hence ΔT is offset by T 2 D  between this analysis and IceCube's previous analyses and the time windows do not
Figure 3. The 90% confidence level upper limits as a function of time windows assuming the best-fit diffuse spectrum (E −2.53 ) measured in cascades (Aartsen et al. 2020a). The "diffuse astrophysical flux constraint" assumes that FRBs are solely responsible for the diffuse neutrino flux. The constraint is calculated by dividing the entire diffuse astrophysical flux equally among 820 homogeneous FRBs. Note that we assume 820 FRBs per day from the CHIME experiment's estimations of the FRB all-sky rate (Amiri et al. 2021).
A Search for Coincident Neutrino Emission from Fast Radio Bursts with Seven Years of IceCube Cascade Events

April 2023

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12 Reads

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11 Citations

The Astrophysical Journal

This paper presents the results of a search for neutrinos that are spatially and temporally coincident with 22 unique, nonrepeating fast radio bursts (FRBs) and one repeating FRB (FRB 121102). FRBs are a rapidly growing class of Galactic and extragalactic astrophysical objects that are considered a potential source of high-energy neutrinos. The IceCube Neutrino Observatory's previous FRB analyses have solely used track events. This search utilizes seven years of IceCube cascade events which are statistically independent of track events. This event selection allows probing of a longer range of extended timescales due to the low background rate. No statistically significant clustering of neutrinos was observed. Upper limits are set on the time-integrated neutrino flux emitted by FRBs for a range of extended time windows.


Figure 4: Spectral energy distribution of NGC 1068. Gray points show publicly available multi-frequency measurements (42). Dark and light green error bars refer to gamma-ray measurements from Fermi-LAT (33, 43) and MAGIC (41), respectively. The solid, dark blue line shows the best-fit neutrino spectrum, and the corresponding blue band covers all powerlaw neutrino fluxes that are consistent with the data at 95% C.L. It is shown in the energy range between 1.5 TeV and 15 TeV where the flux measurement is well constrained. Two theoretical AGN core models are shown for comparison: The light blue shaded region and the gray line show the NGC 1068 neutrino emission models from (44) and (45), respectively. Additional details on the model construction of the light blue shaded region can be found in (46).
Evidence for neutrino emission from the nearby active galaxy NGC 1068

November 2022

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74 Reads

We report three searches for high energy neutrino emission from astrophysical objects using data recorded with IceCube between 2011 and 2020. Improvements over previous work include new neutrino reconstruction and data calibration methods. In one search, the positions of 110 a priori selected gamma-ray sources were analyzed individually for a possible surplus of neutrinos over atmospheric and cosmic background expectations. We found an excess of 7920+2279_{-20}^{+22} neutrinos associated with the nearby active galaxy NGC 1068 at a significance of 4.2σ\,\sigma. The excess, which is spatially consistent with the direction of the strongest clustering of neutrinos in the Northern Sky, is interpreted as direct evidence of TeV neutrino emission from a nearby active galaxy. The inferred flux exceeds the potential TeV gamma-ray flux by at least one order of magnitude.


FIG. 2. Real-only result. Top: The −2∆LLH profile from the fit to data. Blue-shaded regions correspond to the the CL regions determined from the −2∆LLH values. Bottom: Comparison of the 90% CL limits from this analysis to IceCube's previous real-only µτ search [25] and the Super-Kamiokande experiment's inaugural constraints [58].
Strong constraints on neutrino nonstandard interactions from TeV-scale νμ\nu_\mu disappearance at IceCube

January 2022

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26 Reads

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1 Citation

We report a search for nonstandard neutrino interactions (NSI) using eight years of TeV-scale atmospheric muon neutrino data from the IceCube Neutrino Observatory. By reconstructing incident energies and zenith angles for atmospheric neutrino events, this analysis presents unified confidence intervals for the NSI parameter ϵμτ\epsilon_{\mu \tau}. The best-fit value is consistent with no NSI at a p-value of 25.2%. With a 90% confidence interval of 0.0041ϵμτ0.0031-0.0041 \leq \epsilon_{\mu \tau} \leq 0.0031 along the real axis and similar strength in the complex plane, this result is the strongest constraint on any NSI parameter from any oscillation channel to date.


Citations (35)


... With the introduction of the WIMP (Weakly Interacting Massive Particle) scenario [36], the search for DM candidates in the GeV∼TeV mass range became prominent. Despite the recent advancement in DM direct-detection experiments such as LUX [37], XENON-100 [38], PANDAX-II [39,40], XENON-1T [41,42], LZ [43] and indirect-detection experiments such as PAMELA [44,45], AMS-2 [46], Fermi Gamma-ray space Telescope [47] and IceCube [48,49] to name few, there has been no hint of any excess of signal events over the background indicating a DM particle signature. This has led to a highly constraint parameter space for BSM scenarios with a DM candidate detectable at these experiments. ...

Reference:

Singlet-doublet fermionic dark matter in gauge theory of baryons
Search for Neutrinos from Dark Matter Self-Annihilations in the center of the Milky Way with 3 years of IceCube/DeepCore

... Several neutrino detectors, such as IceCube [7], IceCube-Gen2 [8], Baikal-GVD [9], and KM3NeT 2.0 ARCA [10,11], detect Cherenkov light radiation emitted by high-energy charged particles (e.g., muons or taus) to observe astrophysical neutrino interactions. These neutrinos have higher energy than the ones measured in ground-based neutrino DIS experiments like NuTeV [12], CCFR [13], and NOMAD [14]. ...

The IceCube Neutrino Observatory: Instrumentation and Online Systems
  • Citing Preprint
  • December 2016

... Torsion couples naturally to the spin density of matter, resulting in spin-dependent splittings of energy levels [49] and spin oscillations [50]. Neutrinos, on the other hand, play an important role in both cosmology and astrophysics [66,51,52,53,54,55,56,57,58,59,60,61,62,63,64,65,67]. Due to their relatively weak interactions and the large quantities in which they are produced, neutrinos serve as a valuable source of information about the universe. ...

A Search for Coincident Neutrino Emission from Fast Radio Bursts with Seven Years of IceCube Cascade Events

The Astrophysical Journal

... It is known that moving in galaxies and intergalactic space cosmic particles gain energy and accelerate due to various acceleration mechanisms (dynamic mechanism, hydrodynamic mechanism, electromagnetic mechanism, Fermi acceleration mechanism, acceleration due to a strong shock wave etc). For instance, PeV-energy ∼ 10 15 eV antineutrinos was discovered among cosmic particles as a result of observing Glashow resonance [1] in the Ice Cube experiment performed in Antarctica [2]:ν ...

Detection of a particle shower at the Glashow resonance with IceCube
  • Citing Article
  • January 2021

... In the former case, since oscillations are observed by comparing the chargedcurrent (CC) rate of events in near and far detectors, the only effect of (vector) NC NSIs are modifications to the matter potential. This has been used to constrain NC NSI at a variety of long-baseline [15,16], atmospheric [17][18][19][20] and solar neutrino experiments [21]. While oscillation physics provides leading constraints on vector NC NSIs, it cannot probe universal, flavor-diagonal NSIs, as these induce an overall phase in the oscillation amplitude which cancels out in the probability level [22]. ...

Strong constraints on neutrino nonstandard interactions from TeV-scale νμ\nu_\mu disappearance at IceCube

... For instance, in ref. [29], the authors presented the experimental NSI constraints on lepton flavour violating couplings for a Z ′ boson with a mass heavier than the τ lepton. In this paper, we will confront the ATOMKI anomaly and the anomalous magnetic moments of leptons with the NSI constraints reported by the IceCube collaboration [30]. We will show the allowed regions of couplings and the amount of non-universality in the minimal U(1) ′ extension of the SM which satisfy IceCube constraints. ...

All-flavor constraints on nonstandard neutrino interactions and generalized matter potential with three years of IceCube DeepCore data

... First-time findings have more value than second-time findings and subsequent replications (Merton 1957;Stephan 1996). To illustrate, in 2018 IceCube detected a cosmic neutrino from a blazar, laying 4-light years away from Earth (Collaboration 2018). The finding was considered exceptionally valuable because it was only the second source of cosmic neutrinos ever-detected apart from a supernova identified in 1987. ...

Neutrino emission from the direction of the blazar TXS 0506+056 prior to the IceCube-170922A alert
  • Citing Article
  • February 2018

... The interactions of these CRs produce γ-rays and neutrinos (e.g., [566,567]) which contribute to the extragalactic diffuse backgrounds. These backgrounds have been measured with IceCube [568][569][570] and Fermi-LAT [571]. LIRGs have recently emerged as a viable contributor to these backgrounds following a neutrino detection from the LIRG NGC 1068 [381] (see also Section 4.1). ...

Characteristics of the diffuse astrophysical electron and tau neutrino flux with six years of IceCube high energy cascade data

... Auger ANTARES IceCube Figure 8: Measured 14-day all-flavor 90% confidence sensitivity of the ANTARES, IceCube, and Auger experiments to GW170817, and the simulated sensitivity for SPB-2 [36]. ...

Search for High-energy Neutrinos from Binary Neutron Star Merger GW170817 with ANTARES, IceCube, and the Pierre Auger Observatory
  • Citing Article
  • November 2017

... However, as we have shown, the rock muons are also . The IceCube [55] and T2K [56] data at 90% CL are also shown in comparison. The blue dot shows the best fit values from the IceCube data, (sin 2 θ 23 , Δm 2 32 ) = (0.51, 2.31 × 10 −3 eV 2 ) with NH sensitive to the neutrino oscillation parameters, especially in the 2-3 sector. ...

Measurement of Atmospheric Neutrino Oscillations at 6–56 GeV with IceCube DeepCore