kara hoffman, the university of maryland. the antarctic muon and neutrino array

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Kara Hoffman, the University of Maryland

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Page 1: Kara Hoffman, the University of Maryland. the Antarctic Muon and Neutrino Array

Kara Hoffman, the University of Maryland

Page 2: Kara Hoffman, the University of Maryland. the Antarctic Muon and Neutrino Array

the Antarctic Muon and Neutrino Array

Page 3: Kara Hoffman, the University of Maryland. the Antarctic Muon and Neutrino Array

IceTop

InIce

Air shower detetor

threshold ~ 300 TeV

70-80 Strings ,

60 Optical Modules

17 m between Modules

125 m between Strings

2005-2006: 8 strings

AMANDA

19 Strings

677 Modules

2006-2007: 13

strings

2007-2008: 18 strings

2008-2009: 19 strings

59 out of 86 strings operating

2004-2005: 1 string2004-2005: 1 string

DeepCore6 additional strings ,

60 Optical Modules

7 or 10 m between Modules

72 m between Strings

Page 4: Kara Hoffman, the University of Maryland. the Antarctic Muon and Neutrino Array

Neutrino flavor

Log(ENERGY/eV)

12 18156 219

e

e

supernovaeFull flavor ID

Showers vs tracks

IceCube flavor ID,direction, energy

IceCube triggered,partial reconstruction

TeV PeV

Page 5: Kara Hoffman, the University of Maryland. the Antarctic Muon and Neutrino Array

Veryclearice

Dust concentration

Ereco= 500 TeV

Page 6: Kara Hoffman, the University of Maryland. the Antarctic Muon and Neutrino Array

Median angular resolution:(zenith angle averaged) MPE SPEE-1.5 ν – spectrum: 1.2° 2.4°E-2 ν – spectrum: 1.3° 1.7°

Filter level- 40 string configurationFilter level- 40 string configuration

•Angular resolution improves with detector size.•More sophisticated filtering includes a single iteration of a likelihood.

•Improved techniques improve angular resolution at high energies.

Page 7: Kara Hoffman, the University of Maryland. the Antarctic Muon and Neutrino Array

Existence of the moon confirmed!

deficit of events from direction of moon in the IceCube 40-stringdetector (3 months of data) confirms pointing accuracy.

Validates pointing capabilities:

Angular resolution:– IceCube 22 < 1.5°– IceCube 80 < 1°

Page 8: Kara Hoffman, the University of Maryland. the Antarctic Muon and Neutrino Array

e+e-

pair-creationbremsstrahlung

photo-nuclear

•New variables are a stronger function of energy.•Use information contained in the waveform instead of simply counting the number of hit phototubes.

Page 9: Kara Hoffman, the University of Maryland. the Antarctic Muon and Neutrino Array

Sky map with first 22 strings of the IceCube detector

Hottest spot found at r.a. 153º , dec. 11ºpre-trial p-value: 7x 10-7 (4.8 )

est. nSrcEvents = 7.7 est. = 1.65Accounting for all trials, p-value for analysis is 1.34% (2.2 ).

At this significance level, consistent with fluctuation of background.

galactic plane

5114 neutrino candidates in 276 days livetime!new unbinned search methodnew unbinned search method

energy variables usedenergy variables used

Page 10: Kara Hoffman, the University of Maryland. the Antarctic Muon and Neutrino Array

• 3.8 yr livetime• 95% of RA-randomized skymaps have maximum

significance > 3.38 σ → Not significant

Significance

3yr max significance: 3.73 1.5

Max Significanceδ=54o, α=11.4h 3.38

5yr max significance: 3.74 2.8

arXiv:0809.1646

6595 candidate events6595 candidate events

Page 11: Kara Hoffman, the University of Maryland. the Antarctic Muon and Neutrino Array
Page 12: Kara Hoffman, the University of Maryland. the Antarctic Muon and Neutrino Array

•Earth becomes neutrino absorbing at high energies.

•High flux from atmospheric muons inhibits search above horizon.

•Background from atmospheric neutrinos irreducible over all sky.

•Use energy related variables to discriminate against softer atmospheric spectrum.

Page 13: Kara Hoffman, the University of Maryland. the Antarctic Muon and Neutrino Array

search in 2.5 degree bins

background calculation from same declination band

large irreducible background just below the horizon

Coordinates: Dec. 1.00°, RA 103.5° (6.9 h)P-value: 2.9x10-5 (pre-trial prob.)Bin content: 8 events with 1.2 expected (109 in dec. band)

The trial-corrected probability for a random excess of the same or larger valueanywhere in the sky from 390,000 scrambled maps: 37.4 %, i.e. not significant.

Page 14: Kara Hoffman, the University of Maryland. the Antarctic Muon and Neutrino Array

Down-going (sin(δ)<0 )90% energy interval:50 TeV – 300 PeV

Up-going ( sin(δ)>0 )90% energy interval:8 TeV – 5 PeV

Down-going (sin(δ)<0 )90% energy interval:790 TeV – 5 EeV

Up-going (sin(δ)>0 )90% energy interval:32 TeV – 0.8 EeV

E-2E-2

E-1.5E-1.5

In the PeV regime, point source searches can be extended above the horizon!Energy dependent variables invaluable!

Page 15: Kara Hoffman, the University of Maryland. the Antarctic Muon and Neutrino Array

•Look for spatial and temporal coincidences with satellite observations-low background search

•New satellites, Swift, GLAST, improve observations

•cascade searches (triggered and rolling) yield flux limits that are 1-2 orders of magnitude higher

Cascade(Trig & Roll)

Cascade(Rolling)

search

WB03

WB03

MN06

MN06

R03bR03b

R03aR03a 400 bursts400 bursts

Page 16: Kara Hoffman, the University of Maryland. the Antarctic Muon and Neutrino Array

•IceCube will be sensitive to Waxman Bahcall fluxes within 1 year of full detector operation (~70 bursts)!

•IceCube will be sensitive to Waxman Bahcall fluxes within 1 year of full detector operation (~70 bursts)!

22 string detector configuration

•gains come from inclusion of energy variables and grb weighting

Page 17: Kara Hoffman, the University of Maryland. the Antarctic Muon and Neutrino Array

•Detector was running in test mode• (9 out of 22 strings taking data)• Expect 0.1 events for Γ = 300• No neutrino candidate near GRB coordinates

➞ 90% upper flux limit

•Would expect ~1 event from similar burst in IceCube 80-strings

GRB080319BGRB080319B

March 19, 06:12:49 UT (duration ~70 s)• Position: RA = 217.9°, Dec = +36.3°• Brightest (optical) GRB ever observed•z = 0.94 (DA = 1.6 Gpc)

Page 18: Kara Hoffman, the University of Maryland. the Antarctic Muon and Neutrino Array

•Coincident triggers are selected for further CPU intensive reconstructions. If coming from same direction in the sky, an alert is sent to the ROTSE array.

•Quality cuts, time and space windows are set to allow ~30 random coincidences per year.

•4o angular window•100 ns time window•1.85ox1.85o ROTSE fov well matched to IC psf

•Increased sensitivity to transients•Supernova (id: rising lightcurve)•Gamma-Ray Burst (id: afterglow)•Gamma-Dark Bursts (id: orphan afterglows)

Page 19: Kara Hoffman, the University of Maryland. the Antarctic Muon and Neutrino Array

search for neutrinos from unresolved point sources

Energy related variables help distinguish atmospheric background from harder astrophysical flux.

Page 20: Kara Hoffman, the University of Maryland. the Antarctic Muon and Neutrino Array

bb

WW

•annihilating in the gravity well of the Sun•indirect detection

HZW

ll

qq

,,

~~

±

→→→ χχ L

•Sun sinks maximally 23o

below the horizon at the South Pole-horizontal events very important

•Deep core enhancement under construction will greatly enhance sensitivity- see talk by Doug Cowen.

104 days livetime with 22 string configuration

bbWW

Page 21: Kara Hoffman, the University of Maryland. the Antarctic Muon and Neutrino Array

•atmospheric neutrino measurement important as background for other analyses•look for nonstandard neutrino oscillations•survival probability depends on energy and length of chord in the Earth•VLI introduces velocity eigenstates distinct from mass and flavor•new mixing angle and phase

• SuperK+K2K limit*: δc/c < 1.9 10-27 (90%CL)

• This analysis: δc/c < 2.8 10-27 (90%CL)

• IceCube: sensitivity of δc/c ~ 10-28

Up to 700K atmospheric in 10 years

• SuperK+K2K limit*: δc/c < 1.9 10-27 (90%CL)

• This analysis: δc/c < 2.8 10-27 (90%CL)

• IceCube: sensitivity of δc/c ~ 10-28

Up to 700K atmospheric in 10 years

Limits on Violation of Lorentz Invariance assuming maximal mixing:

Page 22: Kara Hoffman, the University of Maryland. the Antarctic Muon and Neutrino Array

λ >> l

l is the length of the bunch

Add coherently!

power proportional to the square of the shower energy

•Ongoing R&D for a future GZK energy neutrino detector focuses on radio Askaryan and acoustic detection.

•Propagation of sound and RF in cold ice are being studied using in situ measurements.

•Optimal technologies and array configurations under investigation.

pressure v. time

Page 23: Kara Hoffman, the University of Maryland. the Antarctic Muon and Neutrino Array

instrumented depth:•80 m - 500 mper string:• 7 sensors• 7 transmitters

Retrofit hardware developed for RICE, IceCube, and ANITA

•reuse IceCube hardware for time stamping, communications•use ANITA digitization•four antennas placed vertically along a string provide for up/down discrimination•deployments at 250m and 1400m

Transmitter:• ring shaped piezo ceramiccoated in resin• HV generator

Cold ice is the only medium in which acoustic, radio, and optical detection methods may be used simultaneously!

Sensor:• 3 channels / sensor• pre-amplifier• analogue signal transmission• steel pressure housing

Page 24: Kara Hoffman, the University of Maryland. the Antarctic Muon and Neutrino Array

250m1 low f channel

250m

250m

1400m

1400m1 low f channel

1400mTx only

Clusters consist of 4 receivers and 1 transmitter unless otherwise indicated

Deployed in 06-07 and 08-09 austral summers

Retrofit hardware developed for RICE, IceCube, and ANITA

RICE array

Radio

Acoustic

3 clusters installed 06-07 austral summer

1 string with improved hardware installed 07-08 austral summer

Page 25: Kara Hoffman, the University of Maryland. the Antarctic Muon and Neutrino Array

time

time

time

time

radio frequency

Page 26: Kara Hoffman, the University of Maryland. the Antarctic Muon and Neutrino Array

•2008-2009 season successful with the addition of 19 new IceCube 2008-2009 season successful with the addition of 19 new IceCube strings bringing the total to 59.strings bringing the total to 59.

•Many analyses of the 22 string configuration complete, thanks to data Many analyses of the 22 string configuration complete, thanks to data filtering at the Pole and subsequent satellite transmission. Analyses filtering at the Pole and subsequent satellite transmission. Analyses using 40 strings will be available shortly.using 40 strings will be available shortly.

•Analysis techniques are continually refined as we gain operational Analysis techniques are continually refined as we gain operational knowledge- improved analysis sensitivity.knowledge- improved analysis sensitivity.

•1 cubic kilometer (80 strings) will be instrumented by 2011.1 cubic kilometer (80 strings) will be instrumented by 2011.

•Efforts are underway to develop the technology to build a GZK scale Efforts are underway to develop the technology to build a GZK scale neutrino detector after IceCube is complete.neutrino detector after IceCube is complete.

•See talk by Doug Cowen about a low energy enhancement that is See talk by Doug Cowen about a low energy enhancement that is already being implemented.already being implemented.

Page 27: Kara Hoffman, the University of Maryland. the Antarctic Muon and Neutrino Array

USA: Bartol Research Institute, Delaware University of California, Berkeley University of California, Irvine Pennsylvania State University Clark-Atlanta University Ohio State University Georgia Tech University of Maryland University of Alabama, Tuscaloosa University of Wisconsin-Madison University of Wisconsin-River Falls Lawrence Berkeley National Lab. University of Kansas Southern University and A&M

College, Baton Rouge University of Alaska, Anchorage

Sweden: Uppsala Universitet Stockholm Universitet

UK: Oxford University

Belgium: Université Libre de Bruxelles Vrije Universiteit Brussel Universiteit Gent Université de Mons-Hainaut

Germany: DESY-Zeuthen Universität Mainz Universität Dortmund Universität Wuppertal Humboldt Universität MPI Heidelberg RWTH Aachen

Japan: Chiba University

New Zealand: University of Canterbury33 institutions, ~250 members

http://icecube.wisc.edu

Netherlands: Utrecht University

Switzerland: EPFL

Page 28: Kara Hoffman, the University of Maryland. the Antarctic Muon and Neutrino Array

P (Ei | =2)

P (Ei | =3)

Patm (Ei)