Thursday, April 27, 2017

Day 1249

Friday.



1704.08254
On the deuterium abundance and the importance of stellar mass loss in the interstellar and intergalactic medium
van de Voort, Quataert, Faucher-Giguére, Keres, Hopkins, Chan, Feldmann, Hafen

Quantify the gas-phase abundance of D in cosmological zoom-in simulations from the FIRE project.  The cosmic D fraction decreases with time, because mass lost from stars is D-free.  At low metallicity, the simulations confirm that the D abundance is very close to the primordial value.  The D abundance decreases towards higher metallicity, with very small scatter between the D and O abundance.  Compare the sims to existing high-z observations in order to determine a primordial D fraction of (2.549±0.033)e-5 and stress that future observations at higher metallicity can also be used to constrain this value.  At fixed metallicity, the D fraction decreases slightly with decreasing z, due to the increased importance of mass loss from intermediate-mass stars.  Find that the evolution of the average D fraction in a galaxy correlates with its star formation history.  The simulations are consistent with observations of the MW's ISM: the D fraction at the solar circle is 83-92% of the primordial D fraction.  Use the sims to make predictions for future observations.  In particular, the D abundance is lower at smaller galactocenetric radii and in higher mass galaxies, showing that stellar mass loss is more important for fueling SF in these regimes (and can even dominate).  Gas accreting onto galaxies has a D fraction above that of the galaxies' ISM, but below the primordial fraction, because it is a mix of gas accreting from the IGM and gas previously ejected or stripped from galaxies.

Wednesday, April 26, 2017

Day 1248

Wednesday.  Thursday.



1704.07837
Biases from neutrino bias: to worry or not to worry?
Raccanelli, Verde, Villaescusa-Navarro

The relation between the halo field and the matter fluctuation (halo bias), in the presence of massive neutrinos depends on the total neutrino mass, massive neutrinos introduce an additional scale-dependence on the bias which is usually neglected in cosmological analysis.  Investigate the magnitude of the systematic effect on interesting cosmological parameters induced by neglecting this scale dependence, finding that while it is not a problem for current surveys, it is non-negligible for future, denser or deeper ones depending on the neutrino mass, the maximum scale used for the analyses and the details of the nuisance parameters considered.  However there is a simple recipe to account for the bulk of the effect as to make it fully negligible, which is illustrated, and advocate that it should be included in analysis of forthcoming large-scale structure surveys.


1704.07847
A first constraint on the average mass of ultra diffuse galaxies from weak gravitational lensing
Sifón, van der Burg, Hoekstra, Muzzin, Herbonnet

The recent discovery of thousands of UDGs in nearby galaxy clusters has opened a new window into the process of galaxy formation and evolution.  Several scenarios have been proposed to explain the formation history of UDGs ,and their ability to survive in the harsh cluster environments.  A key requirement to distinguish between these scenarios is a measurement of their halo masses which, due to their low surface brightnesses, has proven difficult if one relies on stellar tracers of the potential.  Exploit WL, a technique that does not depend on these baryonic tracers, to measure the average sub halo mass of 784 UDGs selected in 18 clusters at z<0.09.  The sample of UDGs has a median stellar mass <m*>=2e8 Msun and median effective radius <r_eff>=2.8 kpc.  Constrain the average mass of sub haloes within 30 kpc to log m_UCG(r<30kpc)/M_sun < 10.99 at 95% CL, implying an effective viral mass log m_200/M_sun <=11.80, and a lower limit on the stellar mass fraction within 10kpc of 1.0%.   Such mass is consistent with a simple extrapolation of the subhalo-to-stellar mass relation of typical satellite galaxies in massive clusters.  However, the analysis is not sensitive to scatter about this mean mass; the possibility remains that extreme UDGs reside in haloes as massive as the MW.

Monday, April 24, 2017

Day 1247

Tuesday.



1704.06273
Intrinsic Alignment in redMaPPer clusters -- II. Radial alignment of satellites toward cluster centers
Huang, Mandelbaum, Freemen, Chen, Rozo, Rykoff

Study the orientations of satellite galaxies in redMapper clusters constructed from SDSS at 0.1<z<0.35 to determine whether there is any preferential tendency for satellites to point radially toward cluster centers.  Analyze the satellite alignment (SA) signal based on 3 shape measurement methods (re-Gaussianization, deVaucouleurs, and isophotal shapes), which trace galaxy light profiles at different radii.  While no set SA signal is detected using re-Gaussianization shapes across the entire sample, the observed SA signal reaches a statistically significant level when using a subsample of satellites with higher luminosity.  Detect the strongest SA signals using isophotal shapes, followed by the deVaucouleurs shapes, and investigate the impact of noise, systematics, and real physical effects such as isophotal twisting in the comparison between the results based on different shape measurement methods.  After studying the correlation of the SA signal with a total of 17 galaxy and cluster properties, find that the measured SA signal is strongest for satellites with the following characteristics: higher luminosity, smaller distance to the cluster center, rounder in shape, higher bulge fraction in the light profile, distributed preferentially along the major axis directions of their centrals, and residing in clusters with less luminous centrals.  Finally, provide physical explanations for the identified dependencies, and discuss the connection to theories of SA.

Sunday, April 23, 2017

Day 1246

Friday.  Monday.



1704.05843
Properties of the cosmological filament between two clusters: a possible detection of a large-scale accretion shock by $Suzaku$
Akamatsu, et al

Report on the results of a Suzaku observation of the plasma in the filament located between the two massive clusters of galaxies Abell 399 and Abell 401.  Abell 399 (z=0.0724) and 401 (z=0.0737) are expected to be in the initial phase of a cluster merger.  In the region between the two clusters, find a clear enhancement in the temperature of the filament plasma from 4 keV (expected value from a typical cluster temperature profile) to kT~6.5 keV.  The analysis also shows that filament plasma is present out to a radial distance of 15' (1.3 Mpc) from a line connecting the two clusters.  The temperature profile is characterized by an almost flat radial shape with kT~6-7 keV within 10' or ~0.8 Mpc.  Across r=8' from the axis, the temperature of the filament plasma shows a drop from 6.3 keV to 5.1 keV, indicating the presence of a shock front.  The Mach number based on the temperature drop is estimated to be M~1.3.  Also successfully determined the abundance profile up to 15' (1.3 Mpc), showing an almost constant value (Z=0.3 solar) at the cluster outskirt.  Estimated the Compton y-parameter to be ~14.5±1.3e-6, which is in agreement with Planck's results (14-17e-6 on the filament).  The line of sight depth of the filament is ell~1.1 Mpc, indicating that the geometry of filament is likely a pancake shape rather than cylindrical.  The total mass of the filamentary structure is ~7.7e13 Msun.  Discuss a possible interpretation of the drop of X-ray emission at the rim of the filament, which was pushed out by the merging activity and formed by the accretion flow induced by the gravitational force of the filament.


1704.05858
The Hyper Suprime-Cam SSP Survey: Overview and survey design
Aihara, et al

HSC is a wide-field imaging camera on the prime focus of the 8.2m Subaru telescope on the summit of Maunakea.  A team of scientists from Japan, Taiwan and Princeton University is using HSC to carry out a 300-night multi-band imaging survey of the high-latitude sky.  The survey includes 3 layers: the Wide layer will cover 1400 deg^2 in 5 broad bands (grizy), with a 5 sigma point-source depth of r~26.  The Deep layer covers a total of 26 deg^2 in 4 fields, going roughly a magnitude fainter, while the Ultra Deep layer goes almost a magnitude fainter still in 2 pointings of HSC (a total of 3.5 deg^2).  Describe the instrument, the science goals of the survey, and the survey strategy and data processing.  This paper serves as an introduction to a special issue of the Publications of the Astronomical Society of Japan, which includes a large number of technical and scientific papers describing results from the early phases of this survey.

Wednesday, April 19, 2017

Day 1245

Thursday.


1704.05463
Gaia reveals a metal-rich in-situ component of the local stellar halo
Bonaca, Conroy, Wetzel, Hopkins, Keres

Use the first Gaia data release, combined with RAVE and APOGEE spectroscopic surveys, to investigate the origin of halo stars within <~3 kpc from the Sun.  Identify halo stars kinematically, as moving with a relative speed of at least 220 km/s with respect to the local standard of rest.  These stars are in general more metal-poor than the disk, but surprisingly, half of the halo sample is comprised of stars with [Fe/H]>-1.  The orbital directions of these metal-rich halo stars are preferentially aligned with the disk rotation, in sharp contrast with the isotropic orbital distribution of the more metal-poor halo stars.  Find similar properties in the Latte cosmological zoom-in simulation of a Milky Way-like galaxy from the FIRE project.  In Latte, metal-rich halo stars formed primarily inside of the solar circle, while lower-metallicity halo stars preferentially formed in-situ within the Galactic disk rather than having been accreted from satellite systems.  These stars, currently on halo-like orbits, therefore have likely undergone substantial radial migration/heating.

Tuesday, April 18, 2017

Day 1244

Tuesday.  Wednesday.



1704.05380
Hubble Frontier Fields: systematic errors in strong lensing models of galaxy clusters - Implications for cosmography
Acebron, et al

SL by galaxy clusters is a fundamental tool to study DM and constrain the geometry of the Universe.  The HST Frontier Fields program has allowed a significant improvement of mass and magnification measurements but lensing models still have a residual RMS between 0.2" and a few arcsecons, not yet completely understood.  Systematic errors have to be better understood and treated in order to use strong lensing clusters as reliable cosmological probes.  Analysed two simulated HFFs-like clusters from the rubble Frontier Fields Comparison Challenge, Ares and Hera.  Use several estimators (relative bias on magnification, density profiles, ellipticity and orientation) to quantify the goodness of the reconstructions by comparing the multiple models, optimized with the parametric SW Lenstool, with the input models.  Quantified the impact of systematic errors arising, first, from the choice of different density profiles and configuration and, secondly, from the availability of constraints (spectroscopic or photometric redshifts, redshift ranges of the background sources) in the parametric modeling of strong lensing galaxy clusters and therefore on the retrieval of cosmo parameters.  Find that substructures in the outskirts have a significant impact on the position of the multiple images, yielding tighter cosmo contours.  The need for wide-field imaging around massive clusters is thus reinforced.  Show that competitive cosmological constraints can be obtained also with complex multimodal clusters and that photometric redshifts improve the constraints on cosmological parameters when considering a narrow range of (spectroscopic) redshifts for the sources.

Sunday, April 16, 2017

Day 1243

Monday.



1704.04239
The physical origin of log gas depletion times in galaxies
Semenov, Kravtsov, Gnedin

Present a model that elucidates why gas depletion times in galaxies are long compared to the time scales of the processes driving the evolution of the interstellar medium.  Show that global depletion times are not set by any "bottleneck" in the process of gas evolution towards the star-forming state.  Instead, depletion times are long because star-forming gas converts only a small fraction of its mass into stars before it is dispersed by dynamical and feedback processes.  Thus, complete depletion requires that gas transitions between SF and non-SF states multiple times.  The model does not rely on the assumption of equilibrium and can be used to interpret trends of depletion times with the properties of observed galaxies and the parameters of SF and feedback recipes in galaxy simulations.  In particular, the model explains the mechanism by which feedback self-regulates SFR in simulations and makes it insensitive to the local SF efficiency.  Illustrate the model using the results of an isolated L*-sized galaxy simulation that reproduces the observed Kennicutt-Schmidt relation for both molecular and atomic gas.  Interestingly, the relation for molecular gas is close to linear on kilo parsec scales, even though a non-linear relation is adopted in simulation cells.  This difference is due to stellar feedback, which breaks the self-similar scaling of the gas density PDF with the average gas surface density.

Thursday, April 13, 2017

Day 1242

Friday.



1704.03871
Optimized trajectories to the nearest stars using lightweight high-velocity photon sails
Heller, Hippie, Kervella

New means of interstellar travel are now begin considered by various research teams, assuming lightweight spacechips that can be accelerated either via laser or solar radiation to a significant fraction of the speed of light.  Recently demonstrated that gravitational assists can be combined with the deflection from the stellar photon pressure to decelerate an incoming light sail from Earth and either fling it around a star or bring it to rest.  Demonstrate that such a photo gravitational assist is more effective when the star is used as a bumper (i.e. the sail passes "in front of' the star) rather than as a catapult (i.e. the sail passes "behind" or "around" the star).  This increases the maximum deceleration at alpha Can A and B and reduces the travel time of a nominal sail with a mass-to-surface ratio (sigma) similar to graphene (8.6e-4 gram/m^2) from 95 yr to 75 yr.  The maximum possible velocity (v_inf) that can be absorbed upon arrival depends on the required deflection angle from alpha Cen A to B and therefore on the orbital phase of alpha Cen AB.  Here, calculate the resulting variation of the travel times from Earth to Proxima for the next 300 yr.  Then compute the travel times for all stars within about 300 ly with available parallaxes from either Hipparcos or Gaia (about 22,000 in total).  Although alpha Cen is the most nearby star system, find that Sirius A, with a luminosity of 24 solar luminosities, offers the maximum possible declaration in the solar neighborhood, and therefore the shortest possible travel times: 69 yr assuming 12.5%c can be obtained at departure from the solar system.  Sirius A thus offers the opportunity of fly-by exploration plus deceleration into a bound orbit of the companion white dwarf after relatively short times of interstellar travel.

Day 1241

Wednesday.  Thursday.



1704.03461
Baryons still trace dark matter: probing CMB lensing maps for hidden isocurvature
Smith, et al


Compensated isocurvature perturbations (CIPs) are primordial fluctuations that balance baryon and DM isocurvature to leave the total matter density unperturbed.  The effects of CIPs on the CMB anisotropies are similar to those produced by WL of the CMB: smoothing of the power spectrum, and generation of non-Gaussian features.  Previous work considered the CIP effects on the CMB PS but neglected to include the CIP effects on estimates of the lensing potential power spectrum  (though its contribution to the non-Gaussian, connected, part of the CMB trispectrum).  Here, the CIP contribution to the standard estimator for the lensing potential power-spectrum is derived, and along with the CIP contributions to the CMB PS, Planck data is used to place limits on the RMS CIP fluctuations on CMB scales, Delta^2_rms(R_CMB).  The resulting constraint of Delta^2_rms(R_CMB)<4.3e-3 using this new technique improves on past work by a factor of ~3.  Find that for Planck data, the constraints almost reach the ensitivity of the optimal CIP estimator.  The method presented here is currently the most sensitive probe of the amplitude of scale-invariant CIP PS placing an upper limit of A_CIP<0.017 at 95% CL.  Future meausrements of the LS CMB lensing potential power spectrum could probe CIP amplitudes as low as Delta^2_rms(R_CMB)=8e=5 (A_CIP=3.2e-4).



1704.03814
Evidence against a supervoid causing the CMB cold spot
Mackenzie, et al

Report the results of the 2dF-VST ATLAS Cold Spot galaxy redshift survey (2CSz) based on imaging from VST ATLAS and spectroscopy from 2dF AAOmega over the core of the CMB Cold Spot.  Sparsely survey the inner 5deg radius of the Cold Spot to a limit of i_AB<=19.2, sampling ~7000 galaxies at z<0.4.  Found voids at z=0.14,0.26 and 0.30 but they are interspersed with small over-densities and the scale of these voids is insufficient to explain the Cold Spot through the LCDM ISW effect.  Combining with previous data out to z~1, conclude that the CMB Cold Spot could not have been imprinted by a void confined to the inner core of the Cold Spot.  Additionally, find that the 'control' field GAMA G23 shows a similarity in its galaxy redshift distribution to the Cold Spot.  Since the GAMA G23 LoS shows no evidence of a CMB temperature decrement, conclude that the Cold Spot may ave a primordial origin rather than being due to LoS effects.

Monday, April 10, 2017

Day 1240

Thursday.  Friday.  Monday.  Tuesday.



1704.02322
Automated lensing learner - I: an automated strong lensing identification pipeline
Avestruz, Li, Lightman, Collett, Luo

GL directly probes the underlying mass distribution of lensing systems, the high redshift universe, and cosmo models.  The advent of large scale surveys such as LSST and Euclid has promoted a need for automatic and efficient identification of SL systems.  Present (1) a SL identification pipeline and (2) a mock LSST dataset with strong gg-lenses.  In this first application, employ a fast feature extraction method, Histogram of Oriented Gradients (HOG), to capture edge patterns that are characteristic of strong gravitational arcs in gg strong lensing.  Use logistic regression to train a supervised classifier model on the HOG of HST- and LSST-like images.  Use the area under the curve (AUC) of a Receiver Operating CHaractierstic (ROC) curve to assess model performance; AUC=1.0 is an ideal classifier, and AUC=0.5 is no better than randomly guessing.  The best performing models on a training set of 10,000 lens containing images and 10,000 non-lens containing images exhibit an AUC of 0.975 for an HST-like sample.  However, for one exposure of LSST, the model only reaches an AUC of 0.625.  For 10-year mock LSST observations, the AUC improved to 0.809.  Model performance appears to continually improve with the size of the training set.    Models trained on fewer images perform better in absence of the light from the lens galaxy.  However, with larger training data sets, information from the lens galaxy actually improves model performance.  The results demonstrate an efficient and effective method for automatically identifying strong lenses that captures much of the complexity of the arc finding problem.  The linear classifier both runs on a personal laptop and can easily scale to large data sets on a computing cluster, all while using existing open source tools.



1704.02451
Revealing the cosmic web dependent halo bias
Yang et al

Halo bias is one of the key ingredients of the halo models.  It was shown at a given redshift to be only dependent, to the first order, on the halo mass.  In this study, four types of cosmic web environments: clusters, filaments, sheets and voids are defined within a state of the art high resolution N-body simulation  Within those environments, use both halo-dark matter cross-correlation and halo-halo auto correlation functions to probe the clustering properties of haloes.  The nature of the halo bias differs strongly among the four different cosmic web environments described.  With respect to the overall population, haloes in clusters have significantly lower biases in the {1e11.0-1e13.5} Msun/h mass range.  In other environments however, halos show extremely enhanced bases up to a factor 10 in voids for halos of mass 1e12 Msun/h.  Demonstrate for the first time that the cosmic web environment is another first order term tat should be rightfully implemented along with mass in halo bias models.  In addition, age dependence is found to be only significant in clusters and filaments for relatively small halos 1e12.5 Msun/h.


1704.02744
Finding strong lenses in CFHTLS using convolutional neural networks
Jacobs, et al

Train and apply convolutional neural networks, a machine learning technique developed to learn from and classify image data, to CFHTLS imaging for the identification of potential strong lensing systems.  An ensemble of four convolutional neural networks was trained on ims=ages of simulated gg lenses.  The training sets consisted of a total of 62k simulated lenses and 64k non-lens negative examples generated with 2 different methodologies.  The networks were able to learn the features of simulated lenses with accuracy of up to 99.8% and a purity and completeness of 84-100% on a test set of 2000 sims.  An ensemble of trained networks was applied to all of the 171 sq deg of CFHTLS wide field image data, identifying 18k candidates including 63 known and 139 other potential lens candidates.  A second search of 1.4 M early type galaxies selected from the survey catalog as potential deflectors, identified 2465 candidates including 117 previously known lens candidates, 29 confirmed lenses/ high-quality lens candidates, 266 novel probably or potential lenses and 2097 candidates classified as false positives.  For the catalog-based search, estimate a completeness of 21-28% with respect to detectable lenses and a purity of 15%, with a false-positive rate of 1 in 671 images tested.  Predict a human astronomer reviewing candidates produced by the system would identify ~20 probable lenses and 100 possible lenses per hour in a sample selected by the robot.  Convolutional neural networks are therefore a promising tool for use in the search for lenses in current and forthcoming surveys such as DES and LSST.

1704.02970

Spectroscopic confirmation of an ultra-faint galaxy at the epoch of reionization
Hoag, Bradac, Trenti, Treu, et al

Within one billion years of the BB, intergalactic H was ionized by sources emitting UV and higher energy photons .  This was the final phenomenon to globally affect all baryons (visible matter) in the Universe.  It is referred to as cosmic reionization and is an integral component of cosmology.  It is broadly expected that intrinsically faint galaxies were the primary ionizing sources due to their abundance in this epoch.  However, at the highest redshifts (z>7.5; loopback time 13.1 Gyr), all galaxies with spectroscopic confirmations to date are intrinsically bright and, therefore, not necessary representative of the general population.  Report the unequivocal spectroscopic detection of a low luminosity galaxy at z>7.5.  Detected the Ly-alpha emission line at ~10504 AA in two separate observations with MOFIRE on Keck I and independently with the HST slit-less grism spectrograph, implying a source redshift of z=7.640±0.001.  The galaxy is gravitationally magnified by the massive galaxy clusters MACS J1423.8+2404 (z=0.545), with an estimated intrinsic luminosity of M_AB=-19.6±0.2 mag and a stellar mass of M*=3.0+1.5-0.8e8 Msun.  Both are an order of magnitude lower than the 4 other Ly-alpha emitters currently known at z>7.5, making it probably the most distant representative source of reionization found to date.


Tuesday, April 4, 2017

Day 1239

Wednesday.



1704.00729
Quenching of supermassive black hold growth around the apparent maximum mass
Ichikawa, Inayoshi

Recent quasar surveys have revealed that SMBHs rarely exceed a mass of M_BH ~ a few 1e10 Msun during the entire cosmic history.  It has been argued that quenching of the BH growth is caused by a transition of a nuclear accretion disk into an advection dominated accretion flow, with which strong outlaws and/or jets are likely to be associated.  Investigate a relation between the maximum mass of SMBHs and the radio-loudness of quasars with a well-defined sample of 1e5 quasars at 0<z<2, obtained from SDSS DR7 catalog.  Find that the number fraction of the radio-loud (RL) quasars increases above a threshold of M_BH~1e9.5 Msun, independent of their redshifts.  Moreover, the number fraction of RL quasars with lower Eddington ratios (out of the whole RL quasars), indicating lower accretion rates, increases above the critical BH mass.  These observational trends can be natural consequences of the proposed scenario of suppressing BH growth around the apparent maximum mass of ~1e10 Msun.  The ongoing VLS sky survey on radio will allow estimation of the exact number fraction of RL quasars more precisely, which gives further insights to understand quenching processes for BH growth.


1704.00920
Testing approximate predictions of displacements of cosmological dark matter halos
Munari, Monaco, Koda, Kithara, Sefusatti, Borgani

Present a test to quantify how well some approximate methods, designed to reproduce the mildly non-linear evolution of perturbations, are able to reproduce the clustering of DM haloes once the grouping of particles into haloes is defined and kept fixed.  The following methods have been considered: Lagrangian Perturbation Theory (LPT) up to a 3rd order, Truncated LPT, Augmented LPT, MUSCLE and COLA.  The test runs as follows: haloes are defined by applying FoF halo finder to the output of an N-body sim.  The approximate methods are then applied to the same initial conditions of the simulation, producing for all particles displacements from their starting position and velocities.  The position and velocity of each halo are computed by averaging over the particles that belong to that halo, according to the FoF halo finder.  This procedure allows performing a well-posted test of how clustering of the matter density and halo density fields are recovered, without asking to the approximate method an accurate reconstruction of haloes.  Consider the results at z=0, 0.5, 1, and analysed power spectrum in real and z-space, object-by-object difference in position and velocity, density PDF and its moments, phase difference of Fourier modes.  Find that higher LPT orders are generally able to better reproduce the clustering of haloes, while little or no improvement is found for the matter density field when going to 2LPT and 3LPT.  Augmentation provides some improvement when coupled with 2LPT, while its effect is limited when coupled with 3LPT.  Little improvement is brought by MUSCLE with respect to Augmentation.  The more expensive particle-mesh code COLA outperforms all LPT methods.

1704.01054

The effect of Limber and flat-sky approximations on galaxy weak lensing
Lemos, Challinor, Efstathiou

Review the effect of the commonly-used Limber and flat-sky approximation so n the calculation of shear power spectra and correlation functions for galaxy weak lensing.  These approximations are accurate at small scales, but it has been claimed recently that their impact on low multipoles could lead to an increase in the amplitude of the mass fluctuations inferred from surveys such as CFHTLenS, reducing the tension between galaxy WL and the amplitude determined by Planck from observations of the cosmic microwave background.  Here, explore the impact of these approximations on cosmo parameters derived from WL surveys, using CFHTLenS data as a test case.  Conclude that the use of small-angle approximations for cosmo parameter estimation is negligible for current data, and does not contribute to the tension between current WL surveys and Planck.

Day 1238

Monday.  Tuesday.



1704.00069
100 Years of the Cosmological Constant: what's next?
Lahav

The Cosmological Constant Lambda, in different incarnations, has been with us for 100 years.  Many surveys of DE are underway, indicating so far that the data are consistent with a dark energy equation of state of w=-1, i.e. a Lambda term in einstein's equation, although time variation of w is not yet ruled out.  The balls in now back in the theoreticians' court, to explain the physical meaning of Lambda.  Discuss sociological aspects of this field, in particular to what extent the agreement on the cold dark matter + Lambda concordance model is a result of the globalization of research and over-communication.


1704.00258
Quantifying systematics from the shear inversion on weak-lensing peak counts
Lin, Kilbinger

WL peak counts provide a straightforward way to constrain cosmology and results have been shown promising.  However, the importance of understanding and dealing with systematics increases as data quality reaches an unprecedented level.  One of the sources of systematics is the convergence-shear inversion.  This effect, inevitable from observations, is usually neglected by theoretical peak models.  Thus, it could have an impact on cosmological results.  In this letter, study the bias from neglecting they version and find it small but not negligible.  The cosmological dependence of this bias is difficult to model and depends on the filter size.  Also show the evolution of parameter constraints.  Although weak biases arise in individual peak bins, the bias can reach 2sigma for the DE equation of state w0.  Therefore, suggest that the inversion cannot be ignored and that inversion-free approaches, such as aperture mass, would be a more suitable tool to study weak-lensing peak counts.

Sunday, April 2, 2017

Day 1237

Wednesday.  Thursday.  Friday.


1703.09219
Mapping stellar content to dark matter haloes - III. Environmental dependence and conformity of galaxy colors
Zu, Mandelbaum

Recent studies suggest that the quenching properties of galaxies are correlated over several mega-parsecs.  The large-scale "galactic conformity" phenomenon around central galaxies has been regarded as a potential signature of "galaxy assembly bias" or re-heating", both of which interpret conformity as a result of direct environmental effects acting on galaxy formation.  Building on the iHOD halo quenching framework developed in Zu & Mandelbaum (15,16), discover that the fiducial halo mass quenching model, without any galaxy assembly bias, can successfully explain the overall environmental dependence and the conformity of galaxy colors in SDSS, as measured by the mark correlation functions of galaxy colors and the red galaxy fractions around isolated primaries, respectively.  The fiducial iHOD halo quenching mock also correctly predicts the differences in the spatial clustering and galaxy-galaxy lensing signals between the more vs. less red galaxy subsamples, split by the red-sequence ridge-line at fixed stellar mass.  Meanwhile, models that tie galaxy colors fully or partially to halo assembly bias have difficulties in matching all these observables simultaneously.  Therefore, demonstrate that the observed environmental dependence of galaxy colors can be naturally explained by the combination of 1) halo quenching and 2) the variation of halo mass function with environment --- an indirect environmental effect mediated by two separate physical processes.  


1703.09233
Mapping dark matter on the celestial sphere with weak gravitational lensing
Wallis, McEwen, Kitching, Leistedt, Plouviez

Convergence maps of the integrated matter distribution are a key science result from WL surveys.  To date, recovering convergence maps has been performed using a planar approximation of the celestial sphere.  However, with the increasing area of sky covered by DE experiments, such as Euclid, LSST, and WFIRST, this assumption will no longer be valid.  Extend the Kaiser-Squires technique for recovering convergence fields, restricted previously to the plane, to the spherical setting.  Through simulations, study the error introduced by planar approximations.  Moreover, examine how best to recover convergence maps in the planar setting, considering a variety of different projection and defining the local rotations that are required while projecting spin fields such as cosmic shear.  For the sky coverages typical of future surveys, errors introduced by projection effects can be of order tens of percent, exceeding 50% in some cases.  The stereographic projection, which is confirmed and so preserves local angles, is the most effective planar projection.  In any case, these errors can be avoided entirely by recovering convergence fields directly on the celestial sphere.  Apply the spherical Kaiser-Squires mass-mapping method presented to the DES science verification data to recover convergence maps directly on the celestial sphere.