the implication of bicep2 : alternative interpretations on its results seokcheon lee (kias) @ snu...
TRANSCRIPT
The Implication of BICEP2: Alternative Interpretations on its
results
Seokcheon Lee (KIAS)@ SNU SeminarApr. 10th. 2014
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OUTLINE
• Cosmic Microwave Background Physics– Temperature Anisotropies– Polarization
• Implication of Background Imaging Cosmic Extragalac-
tic Polarization2– Data– Interpretation– Constraints on Inflation Models– Alternative Interpretations on its results
• Conclusions2014-04-10 SNU SEMINAR ( 이석천 / 고등과학원 )
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CMB Physics: Temperature Anisotropies
• The Universe was in thermal equilib-rium when the last scattering hap-pened
• We obtain the blackbody spectrum with average T = 2.725 K
• Last Scattering : when the photon is decoupled with electron2014-04-10 SNU SEMINAR ( 이석천 / 고등과학원 )
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CMB Physics: Temperature Anisotropies
• This is much colder than the H ionization energy (13.6 eV)
• After LS, the photon freely propagates to us (exception reionization)
• What we see is the fossil of the standing wave be-tween photon and baryon
• Deviation from Average T : Ensemble Average of this small deviation is called Temperature Power Spectrum
2014-04-10 SNU SEMINAR ( 이석천 / 고등과학원 )
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CMB Physics: Temperature Anisotropies
• Measure the anisotropy of T
• Measuring the directional difference of T (average doesn’t work)
2014-04-10 SNU SEMINAR ( 이석천 / 고등과학원 )
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CMB Physics: Temperature Anisotropies
• General solution
Ωcr2014-04-10 SNU SEMINAR ( 이석천 / 고등과학원 )
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CMB Physics: T-E-B contaminations
• Temptation to measure 150-200 GHz
2014-04-10 SNU SEMINAR ( 이석천 / 고등과학원 )
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Polarization: How to generate E & B-mode ?
• Generating E-mode (linear polariza-tion) – From both scalar and tensor perturba-
tions
2014-04-10 SNU SEMINAR ( 이석천 / 고등과학원 )
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B-mode Polarization: How to generate B-mode ?
• Generating B-mode – From tensor perturbation (h)– From converting E-mode into B-mode
(Gravitational lensing, Birefringence, primordial magnetic field)
2014-04-10 SNU SEMINAR ( 이석천 / 고등과학원 )
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B-mode Polarization : Why Important
• E & B modes around hot and cold spots
• Gravitational wave : Unique (?) channel to generate B-mode
2014-04-10 SNU SEMINAR ( 이석천 / 고등과학원 )
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CMB Physics: Temperature and Polariza-
tion
N = ln[ ((10E16 GeV)/(10E-4 eV))] = 29 * ln[10] = 67
2014-04-10 SNU SEMINAR ( 이석천 / 고등과학원 )
Limited by cosmic variance if only consider T : Knox & Turner (94) r < 0.1
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Implication of BICEP2: why BICEP2 ?
• Ground based telescope @ south pole / starting from Nov. 2005
• Frequencies : 100 (BICEP1), 150 GHz (BICEP2) / 26cm aperture
• Bolometer / 512 antenna (will be up-dated to 2560 antenna)
• Fig from BICEP
2014-04-10 SNU SEMINAR ( 이석천 / 고등과학원 )
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Why BICEP ? II• Comparison for CMB polarization ex-
periments (G : ground, HEMT : High-Electron-
Mobility-Transistor, TES : Transition Edge Sensors)NAME BEGIN BASIS/LOC
Frequency Amplifier Targets
AMiBA 2002 G/Hawaii 86-102 Interfer-ometer
SZ, Pol
BICEP 2005 G/South Pole
100, 150 Bolome-ter
Large scale Pol
CBI (DASI) 2002-2008 (99-03)
G/Chille (SP)
26-36 HEMT Small scale
QUaD 2005-2007
G/ SP 100, 150 Bolome-ter
Small scale Pol
EBEX Future Ballon/Antarctica
150-450 Bolome-ter
Inflation GW
POLAR-BEAR
2011 G/Chille 150 Antenna-Coupled TES
Lensed B
Qubic Future G/ 97,150,230
Bolome-ter / TES
Interme-diate B
SPOrt Future Space Pol
SPT 2006 G/SP 90, 150, 220
Pol
SPIDER 2011 Balloon 90,150,220
Bolome-ter
Large scale Pol
Planck 2009 Space 30-857 HEMT/Bo-lometer
2014-04-10 SNU SEMINAR ( 이석천 / 고등과학원 )
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Foreground Removal: Contaminations
• Contamination sources & Sensitivity
2014-04-10 SNU SEMINAR ( 이석천 / 고등과학원 )
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Problems in Foreground Remove
• Not much is known about the polarization of fore-grounds
• Understanding and removing foregrounds are critical for Polarization detection
• Independent Component Analysis (ICA) used in T• None of studies take into account the impact of fore-
grounds in the presence of lensing and instrumental systematics
• Lack of a polarized dust map (BICEP relies on Planck data for this)– BICEP considered several models (FDS, BSS, LSA, PSM,
DDM1 p.12)– Important because this affects the result of r (Fig. 6 & 11)
2014-04-10 SNU SEMINAR ( 이석천 / 고등과학원 )
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Constraints on Inflation Models I
• Slow roll parame-ters
• Observable quanti-ties in terms of slow roll parame-ters to first order (Liddle & Lyth 00)
2014-04-10 SNU SEMINAR ( 이석천 / 고등과학원 )
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Constraints on Inflation models
• Prefer simple inflation? Rule out many r < 10E-5 models?
• Not really, it can’t have large running index
• Does BICEP2 confirm large r if we trust their data? (assume their systematic is correct)
2014-04-10 SNU SEMINAR ( 이석천 / 고등과학원 )
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Alternative Interpretations
• Many alternative ideas are possible (r = 0.1 still work)– Any other mechanism to create large
scale B-mode in addition to GW?– Lowering the scalar amplitude As
(Peloso et.al 1403.4596)– Primordial Magnetic field (Bonvin et.al
1403.6768)– Alleviate Bunch Davies vacuum (Collins
et.al 1403.4592)
• Cause the blue tilt nT > 1– Strongly against this, because it costs
changes in Temperature power spectrum (however it’s still consistent with error limit of T
2014-04-10 SNU SEMINAR ( 이석천 / 고등과학원 )
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Conclusions
• BICEP2 shows the first B-mode signal (still need to investigate the origin of this signal)
• It might show that we are under the right track to understand the Universe
• For the data interpretation, we still need to understand many others– Need better control for foreground contamination– Need to suspect for alternative interpretations
and mechanism
• Stay tune for KECK and PLANCK
2014-04-10 SNU SEMINAR ( 이석천 / 고등과학원 )