A Novel Tau Signature in Neutrino Telescopes

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April 25, 2006 Doug Cowen, Tyce DeYoung, Soeb Razzaque A Novel Tau Signature in Neutrino Telescopes UHE Tau Neutrino Workshop Beijing, China

description

A Novel Tau Signature in Neutrino Telescopes. UHE Tau Neutrino Workshop Beijing, China. Classic Tau Signature. “Double Bang” Learned & Pakvasa 1995 ν N interaction Tau lepton track ~50 m/PeV (neglecting energy loss) Tau decay. Neutrino flavor. n. t. - PowerPoint PPT Presentation

Transcript of A Novel Tau Signature in Neutrino Telescopes

Page 1: A Novel Tau Signature             in Neutrino Telescopes

April 25, 2006

Doug Cowen, Tyce DeYoung, Soeb Razzaque

A Novel Tau Signature in Neutrino Telescopes

UHE Tau Neutrino WorkshopBeijing, China

Page 2: A Novel Tau Signature             in Neutrino Telescopes

April 25, 2006UHE Tau Neutrino Workshop

Classic Tau SignatureClassic Tau Signature

“Double Bang”Learned & Pakvasa 1995

νN interaction

Tau lepton track ~50 m/PeV

(neglecting energy loss)

Tau decay

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April 25, 2006UHE Tau Neutrino Workshop

Energy Windows by Flavor

Energy Windows by Flavor

(supernovæ) showers vs. tracks

full flavor ID

Neutrino flavor

e

Log(ENERGY/eV)

12 18156 219

e

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April 25, 2006UHE Tau Neutrino Workshop

Alternative SignatureAlternative Signature

“Lollipop” – half double bangBeacom, Bell, Hooper, Pakvasa & Weiler

Dim track

Stops in a big cascade(starting tracks dominated by BG)

Page 5: A Novel Tau Signature             in Neutrino Telescopes

April 25, 2006UHE Tau Neutrino Workshop

Tau Decay ModesTau Decay Modes

Decay mode Branching fraction

• τ → ντ + e + νe 17.8%

• τ → ντ + X (hadronic) ~65%

• τ → ντ + μ + νμ 17.4%

double bang /lollipop

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April 25, 2006UHE Tau Neutrino Workshop

Energy LossesEnergy Losses

Edx

dE

ionization stochastic losses

Particles are detected in neutrino telescopes through energy deposited in the detector

Stochastic energy loss mechanisms:

• Bremsstrahlung• pair production• Photonuclear interactions

ee

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April 25, 2006UHE Tau Neutrino Workshop

Energy Loss Rates Energy Loss Rates

Taus are much dimmer than muonsBremsstrahlung, pair production suppressed by particle mass

At E = 1 PeV: 1 EeV: βμ ~ 5 · 10-6 7 · 10-6

βτ ~ 3.5 · 10-7 9 · 10-7

Page 8: A Novel Tau Signature             in Neutrino Telescopes

Muons are brighter than taus

τ

μ

→ track suddenly brightensCan we see it?

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April 25, 2006UHE Tau Neutrino Workshop

Muonic Tau DecayMuonic Tau Decay

τ → ντ + μ + νμ

Muon energy spectrum in the lab frame:

where

Average muon energy

E

Ex

5943

1 23 xxdx

dn

EE 35.0

(Perl 1992)

Page 10: A Novel Tau Signature             in Neutrino Telescopes

April 25, 2006UHE Tau Neutrino Workshop

Flavor DependenceFlavor Dependence

Muons lose energy by pair production (& brems)

Taus lose through photonuclear interactionsμ τ

Dutta, Reno, Sarcevic, and Seckel

Page 11: A Novel Tau Signature             in Neutrino Telescopes

April 25, 2006UHE Tau Neutrino Workshop

Energy Loss MechanismsEnergy Loss Mechanisms

Bremsstrahlung

Pair production

Photonuclear interactions

ll

ll

ll

γ

e+

e-

hadronicshower

( = μ,τ)l

EMshowers

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April 25, 2006UHE Tau Neutrino Workshop

Hadronic Light YieldHadronic Light Yield

Hadronic showers emit 65-85% of the light of an electromagnetic shower of the same energy

M. Kowalski

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April 25, 2006UHE Tau Neutrino Workshop

Are Photonuclear Losses Quasi-Continuous?

Are Photonuclear Losses Quasi-Continuous?

• Very high energy muons emit pairs, brems so frequently they cannot be resolved

→ Increase overall track brightness

• Tau losses dominated by photonuclear interactions – fewer, brighter events

• If they blur together, increase track brightness

• If they’re distinct, won’t increase “baseline” track brightness

(may reduce event rates)

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April 25, 2006UHE Tau Neutrino Workshop

Photonuclear Energy Loss

Photonuclear Energy Loss

softcomponent

total photonuclearenergy loss

hardcomponent

Bugaev & Shlepin

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April 25, 2006UHE Tau Neutrino Workshop

Photonuclear SpectraPhotonuclear Spectrasoft component

hard component

1 EeV

1 PeV

10 PeV

100 PeV

1 EeV

1 PeV

Peak at10-2 El

Bugaev & Shlepin

= Eshower / Eτ

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April 25, 2006UHE Tau Neutrino Workshop

Quasi-Continuous?Quasi-Continuous?

• Soft component clearly continuous• Hard component:

At 1 PeV,

→ 30 TeV

Mean free path ~ 5 km

At 1 EeV, mean free path ~ 200 m

)103(~

8.5

1058.0

2

7

dv

dv

Ehard

hard

Peak

kmTeV/

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April 25, 2006UHE Tau Neutrino Workshop

Brightness RatioBrightness Ratio

4.3–6.1 2.5–5.0 5.2–6.9 4.1–6.9

0.63–0.79 0.40–0.70 0.72–0.84 0.61–0.84

Quasi-Continuous Non-Continuous

PeV EeV PeV EeV

Ratio:

∆(log10):

Detector resolutions (in log10 E):AMANDA: 0.5ANTARES: 0.3–0.4(Carr & Hallewell)

(ICRC 2003)

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April 25, 2006UHE Tau Neutrino Workshop

Low Energy Taus?Low Energy Taus?

• 1 TeV tau “track:” 5 cm Impossible!

ντ → τ + X μ + νμ + ντ

• Two neutrinos take 2/3 the energy → dim track

• Compare energy of hadronic shower to energy of muon track?

Need to worry about NC/νe background!

MC studies in progress…