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Showing papers by "Lloyd Knox published in 2015"


Journal ArticleDOI
TL;DR: In this paper, the authors present results based on full-mission Planck observations of temperature and polarization anisotropies of the CMB, which are consistent with the six-parameter inflationary LCDM cosmology.
Abstract: We present results based on full-mission Planck observations of temperature and polarization anisotropies of the CMB. These data are consistent with the six-parameter inflationary LCDM cosmology. From the Planck temperature and lensing data, for this cosmology we find a Hubble constant, H0= (67.8 +/- 0.9) km/s/Mpc, a matter density parameter Omega_m = 0.308 +/- 0.012 and a scalar spectral index with n_s = 0.968 +/- 0.006. (We quote 68% errors on measured parameters and 95% limits on other parameters.) Combined with Planck temperature and lensing data, Planck LFI polarization measurements lead to a reionization optical depth of tau = 0.066 +/- 0.016. Combining Planck with other astrophysical data we find N_ eff = 3.15 +/- 0.23 for the effective number of relativistic degrees of freedom and the sum of neutrino masses is constrained to < 0.23 eV. Spatial curvature is found to be |Omega_K| < 0.005. For LCDM we find a limit on the tensor-to-scalar ratio of r <0.11 consistent with the B-mode constraints from an analysis of BICEP2, Keck Array, and Planck (BKP) data. Adding the BKP data leads to a tighter constraint of r < 0.09. We find no evidence for isocurvature perturbations or cosmic defects. The equation of state of dark energy is constrained to w = -1.006 +/- 0.045. Standard big bang nucleosynthesis predictions for the Planck LCDM cosmology are in excellent agreement with observations. We investigate annihilating dark matter and deviations from standard recombination, finding no evidence for new physics. The Planck results for base LCDM are in agreement with BAO data and with the JLA SNe sample. However the amplitude of the fluctuations is found to be higher than inferred from rich cluster counts and weak gravitational lensing. Apart from these tensions, the base LCDM cosmology provides an excellent description of the Planck CMB observations and many other astrophysical data sets.

9,745 citations


Journal ArticleDOI
Peter A. R. Ade1, Nabila Aghanim2, Zeeshan Ahmed3, Randol W. Aikin4  +354 moreInstitutions (75)
TL;DR: Strong evidence for dust and no statistically significant evidence for tensor modes is found and various model variations and extensions are probe, including adding a synchrotron component in combination with lower frequency data, and find that these make little difference to the r constraint.
Abstract: We report the results of a joint analysis of data from BICEP2/Keck Array and Planck. BICEP2 and Keck Array have observed the same approximately 400 deg2 patch of sky centered on RA 0h, Dec. −57.5deg. The combined maps reach a depth of 57 nK deg in Stokes Q and U in a band centered at 150 GHz. Planck has observed the full sky in polarization at seven frequencies from 30 to 353 GHz, but much less deeply in any given region (1.2 μK deg in Q and U at 143 GHz). We detect 150×353 cross-correlation in B-modes at high significance. We fit the single- and cross-frequency power spectra at frequencies above 150 GHz to a lensed-ΛCDM model that includes dust and a possible contribution from inflationary gravitational waves (as parameterized by the tensor-to-scalar ratio r). We probe various model variations and extensions, including adding a synchrotron component in combination with lower frequency data, and find that these make little difference to the r constraint. Finally we present an alternative analysis which is similar to a map-based cleaning of the dust contribution, and show that this gives similar constraints. The final result is expressed as a likelihood curve for r, and yields an upper limit r0.05<0.12 at 95% confidence. Marginalizing over dust and r, lensing B-modes are detected at 7.0σ significance.

1,255 citations


Journal ArticleDOI
TL;DR: The Planck 2015 likelihoods as mentioned in this paper describe the 2-point correlations of CMB data, using the hybrid approach employed previously: pixel-based at the low layer and a Gaussian approximation to the distribution of spectra at the higher layer.
Abstract: This paper presents the Planck 2015 likelihoods, statistical descriptions of the 2-point correlations of CMB data, using the hybrid approach employed previously: pixel-based at $\ell<30$ and a Gaussian approximation to the distribution of spectra at higher $\ell$. The main improvements are the use of more and better processed data and of Planck polarization data, and more detailed foreground and instrumental models, allowing further checks and enhanced immunity to systematics. Progress in foreground modelling enables a larger sky fraction. Improvements in processing and instrumental models further reduce uncertainties. For temperature, we perform an analysis of end-to-end instrumental simulations fed into the data processing pipeline; this does not reveal biases from residual instrumental systematics. The $\Lambda$CDM cosmological model continues to offer a very good fit to Planck data. The slope of primordial scalar fluctuations, $n_s$, is confirmed smaller than unity at more than 5{\sigma} from Planck alone. We further validate robustness against specific extensions to the baseline cosmology. E.g., the effective number of neutrino species remains compatible with the canonical value of 3.046. This first detailed analysis of Planck polarization concentrates on E modes. At low $\ell$ we use temperature at all frequencies and a subset of polarization. The frequency range improves CMB-foreground separation. Within the baseline model this requires a reionization optical depth $\tau=0.078\pm0.019$, significantly lower than without high-frequency data for explicit dust monitoring. At high $\ell$ we detect residual errors in E, typically O($\mu$K$^2$); we recommend temperature alone as the high-$\ell$ baseline. Nevertheless, Planck high-$\ell$ polarization allows a separate determination of $\Lambda$CDM parameters consistent with those from temperature alone.

791 citations


Journal ArticleDOI
Lindsey Bleem1, Lindsey Bleem2, B. Stalder3, T. de Haan4, K. A. Aird1, Steven W. Allen5, Steven W. Allen6, Douglas Applegate, Matthew L. N. Ashby3, Mark W. Bautz7, Matthew B. Bayliss3, Bradford Benson1, Bradford Benson8, Sebastian Bocquet9, Mark Brodwin10, John E. Carlstrom, C. L. Chang2, C. L. Chang1, I-Non Chiu9, Hsiao-Mei Cho11, Alejandro Clocchiatti12, T. M. Crawford1, A. T. Crites1, A. T. Crites13, Shantanu Desai9, J. P. Dietrich9, Matt Dobbs4, Matt Dobbs14, R. J. Foley3, R. J. Foley15, William R. Forman3, Elizabeth George16, Michael D. Gladders1, Anthony H. Gonzalez17, N. W. Halverson18, C. Hennig9, Henk Hoekstra19, Gilbert Holder4, W. L. Holzapfel20, J. D. Hrubes1, Christine Jones3, Ryan Keisler6, Ryan Keisler1, Lloyd Knox21, Adrian T. Lee22, Adrian T. Lee20, E. M. Leitch1, Jiayi Liu9, M. Lueker20, M. Lueker13, Daniel M. Luong-Van1, Adam Mantz, Daniel P. Marrone23, Michael McDonald7, Jeff McMahon24, S. S. Meyer1, L. M. Mocanu1, Joseph J. Mohr16, S. S. Murray3, Stephen Padin1, Stephen Padin13, C. Pryke25, Christian L. Reichardt20, Christian L. Reichardt26, Armin Rest27, Jonathan Ruel3, J. E. Ruhl28, Benjamin Saliwanchik28, A. Saro9, J. T. Sayre28, K. K. Schaffer1, K. K. Schaffer29, Tim Schrabback, Erik Shirokoff20, Erik Shirokoff13, Jizhou Song24, Jizhou Song30, Helmuth Spieler22, Spencer A. Stanford31, Spencer A. Stanford21, Z. K. Staniszewski28, Z. K. Staniszewski13, Antony A. Stark3, K. T. Story1, Christopher W. Stubbs3, K. Vanderlinde32, Joaquin Vieira15, Alexey Vikhlinin3, R. Williamson1, R. Williamson13, Oliver Zahn22, Oliver Zahn20, A. Zenteno9 
TL;DR: In this article, the authors presented a catalog of galaxy clusters selected via their Sunyaev-Zel'dovich (SZ) effect signature from 2500 deg^2 of South Pole Telescope (SPT) data.
Abstract: We present a catalog of galaxy clusters selected via their Sunyaev-Zel'dovich (SZ) effect signature from 2500 deg^2 of South Pole Telescope (SPT) data. This work represents the complete sample of clusters detected at high significance in the 2500 deg^2 SPT-SZ survey, which was completed in 2011. A total of 677 (409) cluster candidates are identified above a signal-to-noise threshold of ξ = 4.5 (5.0). Ground- and space-based optical and near-infrared (NIR) imaging confirms overdensities of similarly colored galaxies in the direction of 516 (or 76%) of the ξ > 4.5 candidates and 387 (or 95%) of the ξ > 5 candidates; the measured purity is consistent with expectations from simulations. Of these confirmed clusters, 415 were first identified in SPT data, including 251 new discoveries reported in this work. We estimate photometric redshifts for all candidates with identified optical and/or NIR counterparts; we additionally report redshifts derived from spectroscopic observations for 141 of these systems. The mass threshold of the catalog is roughly independent of redshift above z ~ 0.25 leading to a sample of massive clusters that extends to high redshift. The median mass of the sample is M_(500c(ρcrit)) ~ 3.5 x 10^(14)M_☉ h_(70)^(-1), the median redshift is z_(med) = 0.55, and the highest-redshift systems are at z > 1.4. The combination of large redshift extent, clean selection, and high typical mass makes this cluster sample of particular interest for cosmological analyses and studies of cluster formation and evolution.

573 citations


Book
01 Jan 2015
TL;DR: For example, a future CMB and large-scale structure (LSS) experiments are poised to test the leading paradigm for these earliest moments and to detect the imprints of the inflationary epoch, thereby dramatically increasing our understanding of fundamental physics and the early universe.
Abstract: Fluctuations in the intensity and polarization of the cosmic microwave background (CMB) and the large-scale distribution of matter in the universe each contain clues about the nature of the earliest moments of time. The next generation of CMB and large-scale structure (LSS) experiments are poised to test the leading paradigm for these earliest moments---the theory of cosmic inflation---and to detect the imprints of the inflationary epoch, thereby dramatically increasing our understanding of fundamental physics and the early universe. A future CMB experiment with sufficient angular resolution and frequency coverage that surveys at least 1 of the sky to a depth of 1 uK-arcmin can deliver a constraint on the tensor-to-scalar ratio that will either result in a 5-sigma measurement of the energy scale of inflation or rule out all large-field inflation models, even in the presence of foregrounds and the gravitational lensing B-mode signal. LSS experiments, particularly spectroscopic surveys such as the Dark Energy Spectroscopic Instrument, will complement the CMB effort by improving current constraints on running of the spectral index by up to a factor of four, improving constraints on curvature by a factor of ten, and providing non-Gaussianity constraints that are competitive with the current CMB bounds.

312 citations


Journal ArticleDOI
TL;DR: In this paper, the authors present measurements of secondary cosmic microwave background anisotropies and cosmic infrared background (CIB) fluctuations using data from the South Pole Telescope (SPT) covering the complete 2540 deg 2 SZ survey area.
Abstract: We present measurements of secondary cosmic microwave background (CMB) anisotropies and cosmic infrared background (CIB) fluctuations using data from the South Pole Telescope (SPT) covering the complete 2540 deg^2 SPT-SZ survey area. Data in the three SPT-SZ frequency bands centered at 95, 150, and 220 GHz, are used to produce six angular power spectra (three single-frequency auto-spectra and three cross-spectra) covering the multipole range 2000 2500 at these frequencies. The main contributors to the power spectra at these angular scales and frequencies are the primary CMB, CIB, thermal and kinematic Sunyaev-Zel'dovich effects (tSZ and kSZ), and radio galaxies. We include a constraint on the tSZ power from a measurement of the tSZ bispectrum from 800 deg^2 of the SPT-SZ survey. We measure the tSZ power at 143 GHz to be D^(tSZ)_(3000) = 4.08^(+0.58)_(-0.67) µK^2 and the kSZ power to be D^(kSZ)_(3000) = 2.9 \pm 1.3 µK^2. The data prefer positive kSZ power at 98.1% CL. We measure a correlation coefficient of ξ = 0.113^(+0.057)_(-0.054) between sources of tSZ and CIB power, with ξ < 0 disfavored at a confidence level of 99.0%. The constraint on kSZ power can be interpreted as an upper limit on the duration of reionization. When the post-reionization homogeneous kSZ signal is accounted for, we find an upper limit on the duration Δz < 5.4 at 95% CL.

210 citations


Journal ArticleDOI
TL;DR: In this paper, the B-mode polarization power spectrum (the BB spectrum) from 100 deg^2 of sky observed with SPTpol, a polarization-sensitive receiver currently installed on the South Pole Telescope, was measured in spectral bands centered at 95 and 150 GHz.
Abstract: We present a measurement of the B-mode polarization power spectrum (the BB spectrum) from 100 deg^2 of sky observed with SPTpol, a polarization-sensitive receiver currently installed on the South Pole Telescope. The observations used in this work were taken during 2012 and early 2013 and include data in spectral bands centered at 95 and 150 GHz. We report the BB spectrum in five bins in multipole space, spanning the range 300 ≤ l ≤ 2300, and for three spectral combinations: 95 GHz × 95 GHz, 95 GHz × 150 GHz, and 150 GHz × 150 GHz. We subtract small (<0.5σ in units of statistical uncertainty) biases from these spectra and account for the uncertainty in those biases. The resulting power spectra are inconsistent with zero power but consistent with predictions for the BB spectrum arising from the gravitational lensing of E-mode polarization. If we assume no other source of BB power besides lensed B modes, we determine a preference for lensed B modes of 4.9σ. After marginalizing over tensor power and foregrounds, namely, polarized emission from galactic dust and extragalactic sources, this significance is 4.3σ. Fitting for a single parameter, A_(lens), that multiplies the predicted lensed B-mode spectrum, and marginalizing over tensor power and foregrounds, we find A_(lens) = 1.08 ± 0.26, indicating that our measured spectra are consistent with the signal expected from gravitational lensing. The data presented here provide the best measurement to date of the B-mode power spectrum on these angular scales.

155 citations


Journal ArticleDOI
TL;DR: In this paper, a velocity dispersion-based mass calibration of the South Pole Telescope SZ galaxy cluster sample is presented, which accounts for cluster selection, cosmological sensitivity, and uncertainties in the mass calibrators.
Abstract: We present a velocity dispersion-based mass calibration of the South Pole Telescope SunyaevZel’dovich eect survey (SPT-SZ) galaxy cluster sample. Using a homogeneously selected sample of 100 cluster candidates from 720 deg 2 of the survey along with 63 velocity dispersion ( v) and 16 X-ray YX measurements of sample clusters, we simultaneously calibrate the mass-observable relation and constrain cosmological parameters. Our method accounts for cluster selection, cosmological sensitivity, and uncertainties in the mass calibrators. The calibrations using v and YX are consistent at the 0:6 level, with the v calibration preferring 16% higher masses. We use the full SPTCL dataset (SZ clusters+ v+YX) to measure 8( m=0:27) 0:3 = 0:809 0:036 within a at CDM model. The SPT cluster abundance is lower than preferred by either the WMAP9 or Planck+WMAP9 polarization (WP) data, but assuming the sum of the neutrino masses is P m = 0:06 eV, we nd the datasets to be consistent at the 1.0 level for WMAP9 and 1.5 for Planck+WP. Allowing for larger P m further reconciles the results. When we combine the SPTCL and Planck+WP datasets with information from baryon acoustic oscillations and supernovae Ia, the preferred cluster masses are 1:9 higher than the YX calibration and 0:8 higher than the v calibration. Given the scale of these shifts ( 44% and 23% in mass, respectively), we execute a goodness of t test; it reveals no tension, indicating that the best-t model provides an adequate description of the data. Using the multi-probe dataset, we measure m = 0:299 0:009 and 8 = 0:829 0:011. Within a CDM model we nd P m = 0:148 0:081 eV. We present a consistency test of the cosmic growth rate using SPT clusters. Allowing both the growth index and the dark energy equation of state parameter w to vary, we nd = 0:73 0:28 and w = 1:007 0:065, demonstrating that the expansion and the growth histories are consistent with a

151 citations


Journal ArticleDOI
TL;DR: A first detection of the resulting shifts in the temporal phase of the oscillations is reported, which is inferred from their signature in the cosmic microwave background temperature power spectrum.
Abstract: The unimpeded relativistic propagation of cosmological neutrinos prior to recombination of the baryon-photon plasma alters gravitational potentials and therefore the details of the time-dependent gravitational driving of acoustic oscillations. We report here a first detection of the resulting shifts in the temporal phase of the oscillations, which we infer from their signature in the cosmic microwave background temperature power spectrum.

131 citations


Journal ArticleDOI
TL;DR: The all-sky Planck catalogue of 1227 clusters and cluster candidates (PSZ1) published in March 2013, derived from Sunyaev-Zeldovich (SZ) e ect detections using the first 15.5 months of Planck satellite observations, was updated in this paper.
Abstract: We update the all-sky Planck catalogue of 1227 clusters and cluster candidates (PSZ1) published in March 2013, derived from Sunyaev‐Zeldovich (SZ) e ect detections using the first 15.5 months of Planck satellite observations. addendum, we deliver an updated version of the PSZ1 catalogue, reporting the further confirmation of 86 Planck-discovered clusters. In total, the PSZ1 now contains 947 confirmed clusters, of which 214 were confirmed as newly discovered clusters through follow-up observations undertaken by the Planck Collaboration. The updated PSZ1 contains redshifts for 913 systems, of which 736 ( 80:6%) are spectroscopic, and associated mass estimates derived from the Yz mass proxy. We also provide a new SZ quality flag, derived from a novel artificial neural network classification of the SZ signal, for the remaining 280 candidates. Based on this assessment, the purity of the updated PSZ1 catalogue is estimated to be 94%. In this release, we provide the full updated catalogue and an additional readme file with further information on the Planck SZ detections.

117 citations


Journal ArticleDOI
TL;DR: In this article, the authors present updated constraints on hypothetical light bosons with a two-photon coupling such as axions or axion-like particles (ALPs) and focus on masses and lifetimes where decays happen near big bang nucleosynthesis (BBN).
Abstract: We give updated constraints on hypothetical light bosons with a two-photon coupling such as axions or axion-like particles (ALPs) We focus on masses and lifetimes where decays happen near big bang nucleosynthesis (BBN), thus altering the baryon-to-photon ratio and number of relativistic degrees of freedom between the BBN epoch and the cosmic microwave background's (CMB) last scattering epoch, in particular such that ${N}_{\text{eff}}^{\mathrm{CMB}}l{N}_{\text{eff}}^{\mathrm{BBN}}$ and ${\ensuremath{\eta}}^{\mathrm{CMB}}l{\ensuremath{\eta}}^{\mathrm{BBN}}$ New constraints presented here come from Planck measurements of the CMB power spectrum combined with the latest inferences of primordial $^{4}\mathrm{He}$ and D/H abundances We find that a previously allowed region in parameter space near $m=1\text{ }\text{ }\mathrm{MeV}$ and $\ensuremath{\tau}=100\text{ }\text{ }\mathrm{ms}$, consistent with a QCD axion arising from a symmetry breaking near the electroweak scale, is now ruled out at $g3\ensuremath{\sigma}$ by the combination of $\mathrm{CMB}+D/H$ measurements if only ALPs and three thermalized neutrino species contribute to ${N}_{\text{eff}}$ The bound relaxes if there are additional light degrees of freedom present which, in this scenario, have their contribution limited to $\mathrm{\ensuremath{\Delta}}{N}_{\text{eff}}=11\ifmmode\pm\else\textpm\fi{}03$ We give forecasts showing that a number of experiments are expected to reach the sensitivity needed to further test this region, such as Stage-IV CMB and SUPER-KEKB, the latter a direct test insensitive to any extra degrees of freedom

Journal ArticleDOI
TL;DR: In this article, a measurement of the B$-mode polarization power spectrum (the $BB$ spectrum) from 100 ε-deg 2 of sky observed with SPTpol, a polarization-sensitive receiver currently installed on the South Pole Telescope, is presented.
Abstract: We present a measurement of the $B$-mode polarization power spectrum (the $BB$ spectrum) from 100 $\mathrm{deg}^2$ of sky observed with SPTpol, a polarization-sensitive receiver currently installed on the South Pole Telescope. The observations used in this work were taken during 2012 and early 2013 and include data in spectral bands centered at 95 and 150 GHz. We report the $BB$ spectrum in five bins in multipole space, spanning the range $300 \le \ell \le 2300$, and for three spectral combinations: 95 GHz $\times$ 95 GHz, 95 GHz $\times$ 150 GHz, and 150 GHz $\times$ 150 GHz. We subtract small ($< 0.5 \sigma$ in units of statistical uncertainty) biases from these spectra and account for the uncertainty in those biases. The resulting power spectra are inconsistent with zero power but consistent with predictions for the $BB$ spectrum arising from the gravitational lensing of $E$-mode polarization. If we assume no other source of $BB$ power besides lensed $B$ modes, we determine a preference for lensed $B$ modes of $4.9 \sigma$. After marginalizing over tensor power and foregrounds, namely polarized emission from galactic dust and extragalactic sources, this significance is $4.3 \sigma$. Fitting for a single parameter, $A_\mathrm{lens}$, that multiplies the predicted lensed $B$-mode spectrum, and marginalizing over tensor power and foregrounds, we find $A_\mathrm{lens} = 1.08 \pm 0.26$, indicating that our measured spectra are consistent with the signal expected from gravitational lensing. The data presented here provide the best measurement to date of the $B$-mode power spectrum on these angular scales.

Journal ArticleDOI
TL;DR: In this article, a measurement of the cosmic microwave background (CMB) gravitational lensing potential using data from the first two seasons of observations with SPTpol, the polarization-sensitive receiver currently installed on the South Pole Telescope is presented.
Abstract: We present a measurement of the cosmic microwave background (CMB) gravitational lensing potential using data from the first two seasons of observations with SPTpol, the polarization-sensitive receiver currently installed on the South Pole Telescope. The observations used in this work cover 100 deg^2 of sky with arcminute resolution at 150 GHz. Using a quadratic estimator, we make maps of the CMB lensing potential from combinations of CMB temperature and polarization maps. We combine these lensing potential maps to form a minimum-variance (MV) map. The lensing potential is measured with a signal-to-noise ratio of greater than one for angular multipoles between 100 < L < 250. This is the highest signal-to-noise mass map made from the CMB to date and will be powerful in cross-correlation with other tracers of large-scale structure. We calculate the power spectrum of the lensing potential for each estimator, and we report the value of the MV power spectrum between 100 < L < 2000 as our primary result. We constrain the ratio of the spectrum to a fiducial ΛCDM model to be A_(MV) = 0.92 ± 0.14 (Stat.) ± 0.08 (Sys.). Restricting ourselves to polarized data only, we find A_(POL) = 0.92 ± 0.24 (Stat.) ± 0.11 (Sys.). This measurement rejects the hypothesis of no lensing at 5.9σ using polarization data alone, and at 14σ using both temperature and polarization data.

Journal ArticleDOI
TL;DR: In this article, the authors present measurements of E-mode polarization and temperature-E-mode correlation in the cosmic microwave background using data from the first season of observations with SPTpol, the polarization-sensitive receiver currently installed on the South Pole Telescope (SPT).
Abstract: We present measurements of E-mode polarization and temperature-E-mode correlation in the cosmic microwave background using data from the first season of observations with SPTpol, the polarization-sensitive receiver currently installed on the South Pole Telescope (SPT). The observations used in this work cover 100 deg^2 of sky with arcminute resolution at 150 GHz. We report the E-mode angular auto-power spectrum (EE) and the temperature-E-mode angular cross-power spectrum (TE) over the multipole range 500 < l ≤ 5000. These power spectra improve on previous measurements in the high-l (small-scale) regime. We fit the combination of the SPTpol power spectra, data from Planck, and previous SPT measurements with a six-parameter ΛCDM cosmological model. We find that the best-fit parameters are consistent with previous results. The improvement in high-l sensitivity over previous measurements leads to a significant improvement in the limit on polarized point-source power: after masking sources brighter than 50 mJy in unpolarized flux at 150 GHz, we find a 95% confidence upper limit on unclustered point-source power in the EE spectrum of D_l = l(l + 1) C_l/2π < 0.40 µK^2 at l = 3000, indicating that future EE measurements will not be limited by power from unclustered point sources in the multipole range l < 3600, and possibly much higher in l.

Journal ArticleDOI
TL;DR: In this paper, the authors examined the physical effects of neutrino mass on cosmological observables that make these constraints possible, and also considered how these constraints would be improved to ensure at least a $5σ detection.
Abstract: Our tightest upper limit on the sum of neutrino mass eigenvalues $M_ u$ comes from cosmological observations that will improve substantially in the near future, enabling a detection. The combination of the Baryon Acoustic Oscillation feature measured from the Dark Energy Spectroscopic Instrument and a Stage-IV Cosmic Microwave Background experiment has been forecasted to achieve $\sigma(M_ u) < 1/3$ of the lower limit on $M_ u$ from atmospheric and solar neutrino oscillations \citep{2013arXiv1309.5383A,2012PhRvD..86a3012F}. Here we examine in detail the physical effects of neutrino mass on cosmological observables that make these constraints possible. We also consider how these constraints would be improved to ensure at least a $5\sigma$ detection.

Journal ArticleDOI
TL;DR: In this paper, an all-sky template map of the lensing-induced CMB power spectrum was obtained using a real-space algorithm that minimizes the impact of sky masks.
Abstract: The secondary cosmic microwave background (CMB) $B$-modes stem from the post-decoupling distortion of the polarization $E$-modes due to the gravitational lensing effect of large-scale structures. These lensing-induced $B$-modes constitute both a valuable probe of the dark matter distribution and an important contaminant for the extraction of the primary CMB $B$-modes from inflation. Planck provides accurate nearly all-sky measurements of both the polarization $E$-modes and the integrated mass distribution via the reconstruction of the CMB lensing potential. By combining these two data products, we have produced an all-sky template map of the lensing-induced $B$-modes using a real-space algorithm that minimizes the impact of sky masks. The cross-correlation of this template with an observed (primordial and secondary) $B$-mode map can be used to measure the lensing $B$-mode power spectrum at multipoles up to $2000$. In particular, when cross-correlating with the $B$-mode contribution directly derived from the Planck polarization maps, we obtain lensing-induced $B$-mode power spectrum measurement at a significance level of $12\,\sigma$, which agrees with the theoretical expectation derived from the Planck best-fit $\Lambda$CDM model. This unique nearly all-sky secondary $B$-mode template, which includes the lensing-induced information from intermediate to small ($10\lesssim \ell\lesssim 1000$) angular scales, is delivered as part of the Planck 2015 public data release. It will be particularly useful for experiments searching for primordial $B$-modes, such as BICEP2/Keck Array or LiteBIRD, since it will enable an estimate to be made of the lensing-induced contribution to the measured total CMB $B$-modes.

Journal ArticleDOI
TL;DR: In this article, a low-loss superconducting microstrip made of sputtered Nb and SiOx is presented, and the measured loss tangent of the microstrip is 1-2e-3.
Abstract: Low loss superconducting microstrip is an essential component in realizing 100 kilo-pixel multichroic cosmic microwave background detector arrays. We have been developing a low loss microstrip by understanding and controlling the loss mechanisms. We present the fabrication of the superconducting microstrip, the loss measurements at a few GHz frequencies using half-wavelength resonators, and the loss measurements at 220 GHz frequencies with the superconducting microstrip coupled to slot antennas at one end and to TES detectors at the other end. The measured loss tangent of the microstrip made of sputtered Nb and SiOx is 1-2e-3.