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Detection of a neutrino event at the Glashow resonance with IceCube

Christian Haack, TUM

Lu Lu, Tianlu Yuan, UW Madison For the IceCube Collaboration

VLVnT 2021, 21.05.2021

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Christian Haack (TUM) | VLVnT 2021 2

Production of Astrophysical Neutrinos

Accelerator (AGN, SNR, GRB, ..)

p

p

or

ฮณ

๐…

ยฑ

, ๐…

๐ŸŽ

ฮณ ฮณ

Pion Decays

๐œ‹+ โ†’ ๐œ‡+ + ๐œˆ๐œ‡ โ†’ ๐‘’+ + ๐œˆ๐‘’ + ๐œˆ๐œ‡ + าง๐œˆ๐œ‡ ๐œ‹โˆ’ โ†’ ๐œ‡โˆ’ + าง๐œˆ๐œ‡ โ†’ ๐‘’โˆ’ + าง๐œˆ๐‘’ + าง๐œˆ๐œ‡ + ๐œˆ๐œ‡

๐œ‹0 โ†’ ๐›พ๐›พ

e+ฮฝ

DESY

Idealized scenarios

๐‘ + ๐‘ โ†’ ๐‘‹ + เตž

๐œ‹+ 1/3 ๐œ‹โˆ’ 1/3 ๐œ‹0 1/3 ๐‘ + ๐›พ โ†’ ฮ”+ โ†’ เต๐‘ + ๐œ‹0 1/3

๐‘› + ๐œ‹+ 2/3

Interaction of accelerated CR naturally leads to production of neutrinos and gamma rays

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Proton-Proton (๐’‘๐’‘) interactions Idealized scenario:

๐œˆ

๐‘’

: าง๐œˆ

๐‘’

: ๐œˆ

๐œ‡

: าง๐œˆ

๐œ‡

: ๐œˆ

๐œ

: าง๐œˆ

๐œ

= 1: 1: 2: 2: 0: 0

Christian Haack (TUM) | VLVnT 2021 3

Astrophysical Neutrino Production

Proton-Photon (๐’‘๐œธ) interactions Idealized scenario:

๐œˆ

๐‘’

: าง๐œˆ

๐‘’

: ๐œˆ

๐œ‡

: าง๐œˆ

๐œ‡

: ๐œˆ

๐œ

: าง๐œˆ

๐œ

= 1: 0: 1: 1: 0: 0

Neutrino Oscillations

1: 1: 1: 1: 1: 1 14: 4: 11: 7: 11: 7

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The Glashow Resonance

๏‚ง Resonant ๐‘Šโˆ’ -production in ๐‘’าง๐œˆ โˆ’ eโˆ’ interactions at 6.3 PeV neutrino energy (electron at rest)

๐‘’าง๐œˆ + ๐‘’โˆ’ โ†’ ๐‘Šโˆ’ โ†’ แ‰ŠHadrons (67%) Leptons (23%)

๏‚ง > x100 increase over DIS in าง๐œˆ๐‘’ cross section

๏‚ง Not observed experimentally, despite being fundamental Standard Model process

๏‚ง Allows (statistical) measurement of เดฅ๐œˆ๐‘’

๐œˆ๐‘’ ratio -> Handle on astrophysical ๐œˆ production mechanisms

Christian Haack (TUM) | VLVnT 2021 4

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The Glashow Resonance

๏‚ง Resonant ๐‘Šโˆ’ -production in ๐‘’าง๐œˆ โˆ’ eโˆ’ interactions at 6.3 PeV neutrino energy (electron at rest)

๐‘’าง๐œˆ + ๐‘’โˆ’ โ†’ ๐‘Šโˆ’ โ†’ แ‰ŠHadrons (67%) Leptons (23%)

๏‚ง x200 increase over DIS in าง๐œˆ๐‘’ cross section

๏‚ง So far not observed experimentally, despite being fundamental Standard Model process

๏‚ง Allows (statistical) measurement of เดฅ๐œˆ๐‘’

๐œˆ๐‘’ ratio -> Handle on astrophysical ๐œˆ production mechanisms

Christian Haack (TUM) | VLVnT 2021 5

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6

How to Measure the Glashow Resonance

Need good energy resolution:

โ†’ Cascade Events

From conventional event selections expect

~0.2 GR events / year

Solution: Use partially contained events Caveat: Increased contamination by

atmospheric muons

Christian Haack (TUM) | VLVnT 2021

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A Multi-PeV Uncontained Cascade

Event Vertex

The event vertex is outside the

detector and the PMTs closest to the vertex are saturated.

โ‡’ Challenging Reconstruction Best reconstruction achieved by

DirectFit: ABC (Approximate Bayesian Computing) method using event

resimulations.

Time

Early Late

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Event Display

Christian Haack (TUM) | VLVnT 2021 8

Nature 591, 220โ€“224 (2021)

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9 Christian Haack (TUM) | VLVnT 2021

Energy Reconstruction

Reject NC/CC origin with 1% p-value

Nature 591, 220โ€“224 (2021) Nature 591, 220โ€“224 (2021)

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10 Christian Haack (TUM) | VLVnT 2021

Verification via Resimulation

Nature 591, 220โ€“224 (2021)

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Muon Production in Hadronic Cascades

๐‘Š

โˆ’

๐œˆ

๐‘™

๐‘™/๐œˆ

๐‘™

Mesons Muons

Hadronic Cascade (~15m length in ice)

๐‘’

าง๐œˆ ๐‘’

OR

Neutrino DIS

Glashow Resonance

N

Muons canoutrange the

hadronic cascade

Christian Haack (TUM) | VLVnT 2021 11

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12 Christian Haack (TUM) | VLVnT 2021

Early Pulses from Muonic Component

๏‚ง Cherenkov light front propagates with ๐‘/๐‘›

๐‘–๐‘๐‘’

๏‚ง Relativistic muons from hadronic cascade can

โ€œoutrunโ€ cascade light front

๏‚ง Resulting early hit patterns

can be used to reconstruct

muon direction

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13 Christian Haack (TUM) | VLVnT 2021

Early Pulses from Muonic Component

Nature 591, 220โ€“224 (2021)

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14 Christian Haack (TUM) | VLVnT 2021

Angular Reconstruction

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15 Christian Haack (TUM) | VLVnT 2021

Resimulation with Muonic Component

Nature 591, 220โ€“224 (2021) Nature 591, 220โ€“224 (2021)

Pure EM Cascade Hadronic Cascade

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16 Christian Haack (TUM) | VLVnT 2021

Maximum Muon Energy

Number of strings with early hits correlated to leading muon energy

Nature 591, 220โ€“224 (2021)

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Background Probability

Expect less than

๐Ÿ๐ŸŽโˆ’๐Ÿ•

muon events with similar topology.

Energy losses

Muon at Surface

Propagate to detector

Deposit ~6 PeV at reconstructed vertex

Remain with ~25 GeV

Direction is well constrained.

Only possible background topology:

Stopping muon

Christian Haack (TUM) | VLVnT 2021 17

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Background Probability

Expect less than

๐Ÿ๐ŸŽโˆ’๐Ÿ•

muon events with similar topology.

Energy losses

Muon at Surface

Propagate to detector

Deposit ~6 PeV at reconstructed vertex

Remain with ~25 GeV

Direction is well constrained.

Only possible background topology:

Stopping muon

Christian Haack (TUM) | VLVnT 2021 18

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19 Christian Haack (TUM) | VLVnT 2021

The Astrophysical Neutrino Spectrum

Nature 591, 220โ€“224 (2021)

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โ€ข IceCube has detected a multi-PeV uncontained hadronic cascade event

โ€ข Deposited energy is consistent with the expectation from the Glashow Resonance

โ€ข Production via CC constrained at 1% p-value.

โ€ข Muons produced in the hadronic cascade allow independent reconstruction of the event direction

& confirmation of the cascade reconstruction

โ€ข Atmospheric origin excluded at 5๐œŽ

โ€ข What I didnโ€˜t talk about: Early muon reconstruction technique in principle allows to measure the inelasticity of the neutrino interaction โ†’ Further discrimination of CC/GR

โ€ข In the future GR measurements can help constrain astrophysical source scenarios

20 Christian Haack (TUM) | VLVnT 2021

Summary and Outlook

Referencias

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