Issue 
A&A
Volume 600, April 2017



Article Number  A113  
Number of page(s)  11  
Section  Cosmology (including clusters of galaxies)  
DOI  https://doi.org/10.1051/00046361/201629558  
Published online  12 April 2017 
Analysis of a custom support vector machine for photometric redshift estimation and the inclusion of galaxy shape information
Physics Department, University of Richmond 28 Westhampton Way, University of Richmond, VA 23173, USA
email: evan.jones@richmond.edu
Received: 20 August 2016
Accepted: 27 January 2017
Aims. We present a custom support vector machine classification package for photometric redshift estimation, including comparisons with other methods. We also explore the efficacy of including galaxy shape information in redshift estimation. Support vector machines, a type of machine learning, utilize optimization theory and supervised learning algorithms to construct predictive models based on the information content of data in a way that can treat different input features symmetrically, which can be a useful estimator of the information contained in additional features beyond photometry, such as those describing the morphology of galaxies.
Methods. The custom support vector machine package we have developed is designated SPIDERz and made available to the community. As test data for evaluating performance and comparison with other methods, we apply SPIDERz to four distinct data sets: 1) the publicly available portion of the PHAT1 catalog based on the GOODSN field with spectroscopic redshifts in the range z < 3.6, 2) 14 365 galaxies from the COSMOS bright survey with photometric band magnitudes, morphology, and spectroscopic redshifts inside z < 1.4, 3) 3048 galaxies from the overlap of COSMOS photometry and morphology with 3DHST spectroscopy extending to z < 3.9, and 4) 2612 galaxies with fiveband photometric magnitudes and morphology from the Allwavelength Extended Groth Strip International Survey and z < 1.57.
Results. We find that SPIDERz achieves results competitive with other empirical packages on the PHAT1 data, and performs quite well in estimating redshifts with the COSMOS and AEGIS data, including in the cases of a large redshift range (0 < z < 3.9). We also determine from analyses with both the COSMOS and AEGIS data that the inclusion of morphological information does not have a statistically significant benefit for photometric redshift estimation with the techniques employed here.
Key words: techniques: photometric / galaxies: statistics / methods: miscellaneous
© ESO, 2017
1. Introduction
An important challenge for the current and coming era of large multiband extragalactic surveys is obtaining sufficiently accurate photometric redshift estimates and understanding the error properties of these estimates (see e.g. Huterer et al. 2006, for a review). Unlike time consuming spectroscopic redshift determination, photometric redshift estimation (photoz) is subject to significant systematic errors and confusion because the spectral information of a galaxy is limited to the magnitude or flux in a number of wavelength bands. When photozs are used, science goals such as using weak lensing for cosmology are strongly affected by the number of outliers – those objects whose estimated photozs are far from the actual redshifts (e.g. Hearin et al. 2010). In general, data sets with bands extending into those observed by infrared telescopes (e.g. J, H, and K bands) have more accurate photoz estimation and fewer outliers. However, most upcoming large surveys, such as the Large Synoptic Survey Telescope (LSST, Ivezic et al. 2008), will have optical and nearinfrared data only. Reducing the number of, and potentially having a method of identifying, the potential outliers in photoz estimation is an important goal for these projects.
Photoz estimation techniques have traditionally been divided into two main classifications. Socalled “Template fitting” methods, such as the Lephare package as described in Ilbert et al. (2006) and Arnouts et al. (1999), and Bayesian Photometric Redshift (BPZ) as described in Benítez (2000), involve correlating the observed band photometry with model galaxy spectra and redshift, and possibly other model properties. Socalled “Empirical” or “Training set” methods, such as artificial neural networks (e.g. ANNz, Collister & Lahav 2004), boosted decision trees (e.g. ArborZ, Gerdes et al. 2010), regression trees/random forests (e.g. Carliles et al. 2010; Carrasco Kind & Bruner 2013), support vector machines (e.g. Wadadekar 2004), polynomial mapping (e.g. Budavari et al. 2005; Li & Yee 2008), and others develop a mapping from input parameters to redshift with a training set of data in which the actual spectroscopic redshifts are known, then apply the mappings to data for which the redshifts are to be estimated. Both have their drawbacks – template fitting methods require assumptions about intrinsic galaxy spectra or their redshift evolution, and empirical methods require the training set to be “complete” in the sense that it is representative of the target evaluation population in bulk in all characteristics. In a previous work (Singal et al. 2011) we reported on a custom artificial neural network algorithm for photometric redshift determination.
Because of the larger frequency of mergers at higher redshifts and the general evolutionary trend from spiral to elliptical shapes among galaxies, it is a reasonable hypothesis that galaxy morphology and redshift are correlated in such a way that the addition of morphological information could improve photoz estimation. The inclusion of morphological parameters in photoz estimation has been studied using Sloan Digital Sky Survey (SDSS) data by Tagliaferri et al. (2003) with an artificial neural network determination, and by Vince & Csabai (2007) and Way & Srivastava (2006) with other methods. Tagliaferri et al. (2003) find possible modest improvement with the inclusion of shape information, although they restrict their analysis to quite low redshift (z ≤ 0.7) galaxies. Way & Srivastava (2006) consider several empirical methods and show marginal improvement for some methods with the addition of morphological information. Vince & Csabai (2007) claim an improvement of between 1 and 3 percent in the RMS error in photoz determination, however it is not noted whether this result is significant and the method of photoz estimation is not discussed. Singal et al. (2011) considered one of the galaxy test data sets used here which includes a more thorough sample of higher redshift galaxies extending to z ~ 1.57 and found that including galaxy shape information did not result in a statistically significant benefit in the context of a neural network method.
In this work, we evaluate the performance of a custom support vector machine (SVM) package for photoz determination with comparisons to other photoz algorithms, and also explore the efficacy of integrating parameters describing the morphological information of galaxies. The SVM package used in this analysis is developed for the IDL environment by one of the authors (EJ), based largely on algorithmic procedures outlined in Chang & Lin (2011), and has been named SPIDERz (SuPport vector classification for IDEntifying Redshifts)^{1}. It can include additional parameters beyond photometry, such as morphological information, on an equal footing.
Here we follow convention (e.g. Hildebrandt et al. 2010) and define “outliers” as those galaxies where (1)where z_{phot} and z_{spec} are the estimated photoz and actual (spectroscopically determined) redshift of the object. The RMS photoz error in a realization is given by a standard definition (2)where n_{gals} is the number of galaxies in the evaluation set and Σ_{gals} represents a sum over those galaxies. For comparison with other works, we also calculate in certain determinations the RMS error without the inclusion of outlier galaxies, referring to this quantity as the “reduced” RMS or RRMS.
The paper is organized as follows. In Sect. 2 we discuss the SVM model implemented in SPIDERz. In the following sections we perform analyses with four separate test data sets and make comparisons to other photoz methods when possible. In Sect. 3 we discuss the results of testing SPIDERz on the publicly available portion of the PHotoz Accuracy Testing real galaxy data catalog (PHAT1) which spans the redshift range z< 3.6 and provides a useful comparison with other photoz estimation methods. In Sect. 4 we discuss the results of testing SPIDERz on the Cosmic Evolution Survey (COSMOS) bright catalog with 14 365 galaxies spanning z< 1.4 with tenband photometry, spectroscopic redshifts, and seven morphological measurements, highlighting results obtained with differing numbers of bands and the inclusion of morphological information. We perform a similar analysis in Sect. 5 with a catalog of 3048 galaxies spanning a wider redshift range (z< 3.9), which were obtained by combining COSMOS photometry and morphology with 3DHST spectroscopy. In Sect. 6 we discuss the results of testing SPIDERz on a catalog of 2612 galaxies with spectroscopic redshifts, fiveband photometry, and morphological information from the Allwavelength Extended Groth Strip International Survey (AEGIS) in the range z< 1.57, and make a comparison to a neural network determination on this data. We present a summary in Sect. 7.
2. Support vector machine photoz estimation method
2.1. Motivation for use
Support vector machines are a popular statistical machine learning tool that have been successfully applied for a variety of applications (e.g. Hearst et al. 1998). Within astronomy and astrophysics, SVMs have been used in recent works for automated image separation (e.g. Beaumont et al. 2011), galaxy morphological classification (e.g. HuertasCompany et al. 2007) and classification of objects into stellar, galactic, or active galaxy categories using morphology, colors, or spectra (Marton et al. 2016; Malek et al. 2013; Hassan et al. 2013; Solarz et al. 2012; Klement et al. 2011; Peng et al. 2002).
In the case of photoz analysis, the use of SVMs has been reported by Wadadekar (2004) and Wang et al. (2007). Both restricted consideration to lower redshift sources than the present analysis. In the case of the later, the sources are of very low redshift (all z < 0.5 and most z < 0.3). In the case of the former, analyses were restricted to z < 1 sources except in the case of a simulated set.
In SVM photoz determinations, the output of the training algorithm is a mapping from band magnitudes and, in principle, other information such as shape parameters, to redshift. The SVM learning algorithms employed in SPIDERz treat the band magnitudes and other information equally, making it a useful tool for exploring whether additional parameters beyond the band magnitudes, such as morphology in this case, provide additional useful information.
Also, in contrast to an artificial neural network where specific network architecture – such as the number of hidden layers and number of neurons per layer (see e.g. Collister & Lahav 2004) – must be chosen and potentially optimized from a very large set of possibilities, the analogous architecture of an SVM is autonomously optimized during the training process and requires only the predesignation of a kernel function (Burges 1998). Further, SVM training always reaches a global solution, whereas a neural network often has multiple local minima (e.g. Haykin 1999). A comprehensive review of SVM algorithms is presented in e.g. Burges (1998) and Cortes & Vapnik (1995), the latter being coauthored by the originator of the SVM concept.
When considering SVM learning for a continuous variable such as redshift, two approaches are possible – support vector classification (SVC) in which the output is divided into a (possibly large) number of discrete classes, or support vector regression (SVR) where the continuity of the output variable is maintained. We explored both as options with a variety of input scenarios and found that SVC performed significantly better for photoz estimation.
2.2. SPIDERz package and formulation
Fig. 1 Depiction of linearly separable binary class system. For visualization this figure depicts a two dimensional input space, while the input space for photoz determination with SPIDERz is of higher dimension (the dimensions being all band magnitudes plus any other parameters). In this depiction the two classes are filled and open circles. The margin width is equal to where w is a vector perpendicular to the hyperplane as defined in Sect. 2.2. 

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SPIDERz implements a version of SVC. We model SPIDERz on components of the general purpose LibSVM package, a library of support vector machine algorithms available in C++ and Java (Chang & Lin 2011), modified with select customizations for optimization of photoz estimation and implementation in the IDL environment. In addition to providing discrete redshift estimates for each galaxy, SPIDERz can also output photoz probability information (discussed below) and contains supplementary programs for preprocessing galaxy inputs and performing data analysis.
Photoz determination with SPIDERz, and indeed any machine learning algorithm, consists of two main parts: training and evaluation. Inputs in the training process (the training set) are galaxy data consisting of band magnitudes, optional additional parameters (morphological parameters in the case discussed in this work), and known spectroscopic redshifts. The training process outputs a predictive model that can be applied to additional galaxy inputs (the evaluation set) in order to obtain photoz estimates.
We link the galaxies in the training set to their known redshift values by dividing them into redshift bins and assigning each a representative class label. Each galaxy and its corresponding n parameters (band magnitudes and potentially morphological parameters) are represented in ndimensional input space as a galaxy input vector with n coordinates. The objective of the SVC training process is to construct a discriminative hyperplane that linearly separates galaxy vectors in the training set in such a way that maximizes the distance between galaxy vectors from opposing classes. Those vectors located closest to the separating hyperplane are termed support vectors (SVs). For data sets with classes that are not linearly separable by an unbending hyperplane in the ndimensional input space, as turns out to be the case in photoz estimation and most practical scenarios, class separation requires the mapping of input vectors x from input space to a higher Ndimensional feature space with some function φ : x → φ(x). Once an optimal hyperplane solution for the training set is obtained, unlabeled galaxy vectors (those in the evaluation set) are classified according to their location in feature space with respect to the separating hyperplane.
For training a system with m distinct classes (m redshift bins in this case), we use a socalled “one against one” or “pairwise coupling” approach (Hsu & Lin 2002; Knerr et al. 1990) that divides the multiclass system into a series of separate binary classification problems. The hyperplane optimization problem is solved separately for each pair, and the unique hyperplane solutions (also called decision functions) are consolidated and collectively output as a predictive model. In the evaluation process, photoz estimations are obtained by passing each galaxy vector in the evaluation set through the predictive model consisting of the different binary classification problems solved in the training process. If a singlevalued redshift prediction is desired, in the simplest implementation, which we employ in this work, the class to which a particular galaxy is most assigned becomes its final predicted class (or redshift) value (or maximum probability value – see below).
To explore the algorithmic procedures for determining the decision hyperplane in such a binary classification case, let us picture a linearly separable binary class system like the one depicted in Fig. 1. For i = 1,...,l, each input vector x_{i} ∈ R^{2} has an associated class label y_{i} ∈ [ −1,1 ], where y_{i} = 1 for one class of objects and y_{i} = −1 for the other class of objects. The optimal hyperplane is definted as as y_{i}(w·x_{i} + b) = 0, where w is a vector perpendicular to the hyperplane and b is a scalar such that the distance from the origin to the hyperplane is . The following constraint is imposed on the support vectors (SVs), which are the data points located closest to the hyperplane in the space: (3)It is important to note that the dot product w·x_{i} is a distance measure, and since x_{i} and y_{i} are strictly defined, our SV definition is effectively specifying a scale for w and b. Working with these constraints, the decision function indicating the location of data points in this space can be stated as (4)which we can use to define a binary classifier for this system: (5)Once w is specified, this decision function is sufficient to classify objects in the linearly separable two class scheme. As previously discussed, the optimal hyperplane solution is the one in which the margin between SVs of opposing classes is maximized. The form of the decision function sets the width of the margin to , therefore our objective is to minimize ∥ w ∥, or equivalently . Finding an extremum of subject to the constraints imposed on the decision function presents a problem in the calculus of variations with a Lagrangian function (6)for which the minimizing conditions are given by the EulerLagrange equations. Following Cortes & Vapnik (1995) one finds (7)subject to the constraints (8)(9)Thus w can be expressed as a linear combination of SVs, and it’s clear that nonSVs are irrelevant to the optimal hyperplane solution. Finding the optimal hyperplane is now a matter of finding the corresponding α_{i} values for each SV that minimize the Lagrangian of Eq. (6), now with the conditions in Eq. (7) inserted: (10)Let us now consider binary class systems that are not linearly separable in their original input space, like each of the binary classification systems solved by SPIDERz. For such systems, class separation requires mapping galaxy vectors x from an ndimensional input space to a higher Ndimensional feature space with some function φ:x → φ(x). A visualization of such a mapping for a simplified scenario is presented in Fig. 2. Since the Lagrangian stated in Eq. (10) depends on dot products of input vectors living in the same input space, we represent the dot product of mapped vectors with a kernel function: (11)To solve for valid kernel functions that can successfully perform input vector dot products in Ndimensional feature space, Cortes & Vapnik (1995) applied Mercer’s theorem to the HilbertSchmidt theory concerning dot product expansions in Hilbert space, finding that one should use symmetric and positive semidefinite kernel functions of the form: (12)or equivalently, (13)where φ(x_{i})^{T}·φ(x_{j}) is the inner product of the mapped vectors. There are different variants of SVM kernels, however we obtained best results with the radial basis function (RBF) kernel (14)where γ is a scaling factor of the distance measure between input vectors x_{i} and x_{j} in the Ndimensional feature space, and whose value is assigned before training. The RBF kernel, along with other kernels meeting conditions discovered by Cortes & Vapnik (1995), allows the mapping of dot products to feature space to be calculated without explicitly determining the function φ. The free parameter γ determines the topology of the decision surface in the feature space – a low value sets a geometrically complicated boundary while a high value sets a geometrically simpler one with greater potential for misclassifications.
Fig. 2 Conceptual visualization of binary class system which is not linearly separable in the input space (left) but is separable by a hyperplane when mapped to a higher dimensional feature space (right) with some function φ : x → φ(x). 

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Due to the size of the training set and number of galaxy characteristics contained in each training vector, it is not computationally practical to map the galaxy vectors to a feature space in such a way as to obtain a perfect linear separation between classes. Instead we employ a softmargin approach (Cortes & Vapnik 1995) in which a prospective hyperplane solution is not required to inerrantly separate class values, but rather penalized for instances of misclassification during training (mapped inputs falling on the wrong side the separating hyperplane). This consideration is addressed with a cost function (15)where ξ_{i} = 0 if the training vector is correctly classified, and for incorrectly classified training vectors ξ_{i} is the distance from the misclassified point to the margin boundary described by the SVs of the correct class. The cost function is added as an additional term with additional constraints into the Lagrangian of Eq. (6): (16)The EulerLagrange equations then yield conditions that again allow the restatement of the Lagrangian as in Eq. (10) now with the additional constraint that α_{i} = C for the nonzero α_{i}. Thus as C gets larger, a wider range of misclassifications are tolerated and the margin of class separation is larger, but those misclassifications that are not tolerated are penalized more. C is therefore known as a “regularization parameter”.
The training process now requires the minimization of the Lagrangian of Eq. (10) constrained by (17)(18)With the softmargin approach, an optimal classifier is one that limits the number of misclassified input vectors while still maximizing the distance from the separating hyperplane, with the relative importance of each factor having a dependence on the value of C.
This optimization task is a socalled quadratic programming (QP) problem. Our training process solves the QP problem using a decomposition method derived from Platt’s sequential minimal optimization (Platt 1998), which tackles the problem by dividing it into multiple subproblems that can be analytically solved. For this we use the algorithmic solution described in Chang & Lin (2011).
To obtain optimized values of the free parameters γ and C that allow the classifier to construct an optimal separating hyperplane, SPIDERz conducts vfold cross validation (CV) with a parameter grid search. The CV process guards against overfitting the training set as well as approximates the performance of a predictive model on an unknown evaluation set. CV randomly separates training vectors into v subsets of equal size, each of which sequentially serve as a pseudoevaluation set for the predictive model created from a training set comprised of the remaining v1 subsets. Rms error in redshift estimation is calculated during each iteration of CV and serves as the metric of predictive power of a model obtained from training with a particular combination of C and γ values. With a grid search that performs CV using every possible combination of allowed C and γ values within a specified range and iterative step size, the program obtains optimal values of C and γ for each training set by selecting the values associated with the lowest RMS error. To expedite runtime, we first perform a course grid search to identify a rough estimate of optimal parameters, and subsequently perform a fine grid search with a smaller parameter range and step size to achieve greater precision.
With C, γ, and the SVs determined by training, we can obtain a predictive model (with realizations corresponding to each binary pair of classes, as discussed above) and use it to estimate the photozs of galaxies in the evaluation set. For calculating the position of an evaluation vector relative to the separating hyperplane, the kernel function is expressed in terms of support vectors s_{i}(19)and we can state a more precise formulation of the binary classifier introduced in Eq. (5): (20)
2.3. Redshift bins, probabilities, and singlevalued photoz estimates
Once the unique pairwise determinations between m bins of redshift have been made for a particular evaluation galaxy, the combination of these binary class estimates express what amounts to an effective probability distribution function (PDF) for each galaxy, with the relative probability of each bin proportional to the number of times the bin was chosen as the best binary solution. This effective PDF is not continuous, but rather is resolved to the bin width level. Alternately, if one seeks a single value photoz prediction for a galaxy, for reasons of efficiency, simplicity, or to determine performance metrics in a similar way to previous analyses, the most probable (commonly occurring) redshift bin result could be taken as a single valued photoz estimate for the galaxy. For the purposes of the analyses in this work we focus on the later.
Fig. 3 Top: the estimated photoz versus the actual redshift, as determined by SPIDERz, for the AEGIS data set discussed in Sect. 6 with no morphological parameters included. The training set is formed from 700 galaxies and the evaluation set, for which the results are plotted, consists of the remaining 1912 galaxies. “Outliers” in a determination are defined by Eq. (1), shown as those outside of the two diagonal lines. Middle: photozs for the same galaxies, as estimated with the custom neural network as reported in Singal et al. (2011). Bottom: photozs for the same galaxies as estimated with the Lephare template fitting code (Ilbert et al. 2006). The template fitting method has a lower scatter for nonoutliers, but a larger number of outliers than the SVM and neural network for these galaxies. 

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SPIDERz allows users flexibility in redshift bin size. We generally find determinations have increased accuracy and precision when smaller bin sizes are used, however the optimal bin size for any determination will be dependent on the size and nature of the training set and can be approached via trialanderror or approximated with the bin size introduced as an additional parameter in a grid search.
The top panel of Fig. 3 shows the estimated photoz versus spectroscopic redshift for the galaxies in the evaluation set of a particular determination with the AEGIS galaxy data set described in Sect. 6 with no morphological information included. This determination features 700 training galaxies and 1912 evaluation galaxies with a redshift bin size of 0.1. The middle and bottom panel of Fig. 3 also show photoz estimations for the same training and evaluation galaxies with a custom artificial neural network reported in Singal et al. (2011) and as evaluated with the Lephare template fitting method reported in Ilbert et al. (2006). The SPIDERz determination apparently leads to fewer catastrophic outliers than with the Lephare template fitting method or the neural network, although it shows a larger scatter among galaxies for which the photoz estimate is close to the actual redshift. It should be noted that template fitting methods such as LePhare, which consider template spectra evolved over a wide range of redshifts, are at a potential disadvantage when estimating photozs in a limited redshift range relative to empirical methods where the redshift range of the training set would match that of the evaluation set, so it is not necessarily an indication of inferior performance that the LePhare determination has a comparatively higher number of catastrophic outliers (particularly at low spectroscopic redshifts) in this case.
3. Tests with the PHAT1 catalog
In order to obtain a useful comparison with other photoz codes on publicly available data that spans a relatively large redshift range, we first focus on data available from the PHotoz Accuracy Testing (PHAT) program, which was implemented several years ago to test and compare photoz codes (Hildebrandt et al. 2010).
3.1. PHAT1 dataset
At the time of the PHAT program, three spectroscopic and photometric catalogs were assembled, with one (designated PHAT1) based on real galaxy data. PHAT1 featured a catalog of nearly 2000 galaxies with spectroscopic redshifts and 18band photometry from the Great Observatories Origins Deep Survey (GOODS) North field. In the catalogs which were made available, threequarters of the spectroscopic redshifts, chosen at random, were “blinded” to the users with the intention that the users would utilize the other onequarter as the training set and predict the redshifts of the blinded galaxies, with results evaluated by the PHAT authors. As the PHAT program is no longer operational, we did not have the option of evaluating SPIDERz on the blinded galaxies. Therefore, we use only the unblinded galaxies, and to maintain the same proportions of training and evaluation galaxies as in the PHAT program, we use onequarter (chosen at random) as the training set and the remaining threequarters as the evaluation set. For a more straightforward evaluation we also ignore galaxies with missing band magnitudes, which corresponds to the “cleaned sample” analysis reported in Hildebrandt et al. (2010) and results in a set of 374 galaxies with known redshifts ranging from 0.08 < z < 3.6, and thus a training set with 94 galaxies and an evaluation set with 280 galaxies.
3.2. Results with PHAT1 data
Even with this greatly reduced training set size our results on the PHAT1 data are comparable to many other photoz codes. In Table 1 we show the results with SPIDERz along with those from other empirical codes as reported in Table 5 of Hildebrandt et al. (2010). The other empirical codes reported there are the artificial neural network package ANNz (Collister & Lahav 2004), an empirical χ^{2} fitting code (Wolf 2009), a polynomial fit (Li & Yee 2008), and regression trees (Carliles et al. 2010). Results for the eight template fitting codes reported in that work vary from a high of 27.6% outliers and 0.061 reduced RMS to a low of 4.7% outliers and 0.038 reduced RMS. In Table 1 we also show results as reported for the two bestperforming template fitting codes, LePhare (Ilbert et al. 2006) and BPz (Benítez 2000). Figure 4 shows the estimated photoz versus actual redshift results of one particular determination with SPIDERz on the PHAT1 dataset. We note that although the results from a full 18band analysis are reported in Hildebrandt et al. (2010), for a comparison analysis with SPIDERz, we used only 17 bands in our determinations because of a large number of missing values in one band.
Fig. 4 Estimated photoz as determined by SPIDERz versus the actual redshift for the PHAT1 data set discussed in Sect. 3.1 for the case of 14 photometric bands. This determination is with a training set consisting of 94 galaxies chosen at random and an evaluation set consisting of the other 280 galaxies. Outliers are defined by Eq. (1), shown as those outside of the two diagonal lines. This determination results in 15.3% outliers and a reduced RMS of 0.067, which, despite the smaller training set available, is competitive with the results obtained by other empirical methods as shown in Table 1 and discussed in Sect. 3.2. 

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Results for the “cleaned sample” of the PHAT1 catalog with onequarter of galaxies used for training and the remaining threequarters used for evaluation, shown for SPIDERz as determined in this work along with other empirical codes and the two best performing template fitting codes as reported in Hildebrandt et al. (2010).
4. Tests with the COSMOS bright catalog
In order to obtain a data set with a large number of objects, and to investigate the effects of the inclusion of morphological information in photoz determination, we turn to the COSMOS field (e.g. Scoville et al. 2007), where multiband photometry, spectroscopic redshifts, and morphological information are available for a large number of galaxies.
4.1. COSMOS bright data
In particular, we combine photometry from the COSMOS2015 photometric catalog (Laigle et al. 2016), the publicly available portion of the zCOSMOS catalog of spectroscopic redshifts (e.g. Lilly et al. 2009), and the morphological parameters provided by Cassata et al. (2007). Using a 0.5′′ matching criterion for objects, we obtain a catalog of 14 365 galaxies with photometry in u, B, V, r, i, z +, Y, H, J, and Ks bands, seven morphological parameters, and spectroscopic redshifts rated as very secure. By construction all redshifts lie between 0 and 1.4.
Although the COSMOS2015 catalog provides photometry in a large number of optical, infrared, and UV bands, we choose to restrict our analyses to the bands listed above for several reasons. One reason is that outside of those bands the rate of missing photometry is much higher. Another is that with data sets approaching 30 bands of photometry, the distinction between photoz estimation and spectroscopic redshift determination is somewhat muddled, and in any case this does not represent a realistic photometric situation for upcoming large surveys such as LSST, even for subsets which would have infrared survey overlap.
The seven morphological parameters present in the catalog are
 1.
The Petrosian radius R_{P}: the mean radial distance from the center of a galaxy at which the local intensity of the light equals some multiple η of the average intensity of light within the radius:
 2.
The half light radius r_{e}: the radial distance from the center of a galaxy within which half the total light is contained.
 3.
The concentration c: . This parameter defines the central density of the light distribution with radii r_{80} and r_{20} correspondingly 80% and 20% of the total light.
 4.
The asymmetry A: This parameter characterizes the rotational symmetry of the galaxy’s light, with I_{(x,y)} being the intensity at point (x,y) and I_{180(x,y)} being the intensity at the point rotated 180 degrees about the center from (x,y), with B_{180} being the average asymmetry of the background calculated in the same way. It is the difference between object images rotated by 180°.
 5.
The Gini coefficient G: , describes the uniformity of the light distribution, with G = 0 corresponding to the uniform distribution and G = 1 to the case when all flux is concentrated in to one pixel. G is calculated by ordering all pixels by increasing flux X_{i}. is a mean flux and n is the total number of pixels.
 6.
M_{20}: M_{20} = log ΣM_{i}/M_{tot}, is the ratio of the second order moment of the brightest 20% of the galaxy to the total second moment. This parameter is sensitive to the presence of bright offcenter clumps.
 7.
The axial ratio ε: . The values a and b are the semimajor axis and semiminor axis of the galaxy.
These parameters are discussed at greater length in e.g. Scarlata et al. (2007).
4.2. Results with COSMOS bright data
Fig. 5 Estimated photoz as determined by SPIDERz versus the actual redshift for the COSMOS data set discussed in Sect. 4. This determination was performed with tenband photometry and a designated bin size of 0.01. The training and evaluation sets are comprised of 3000 and 11 365 randomly chosen galaxies, respectively. With this small bin size, a relatively large ratio of training set objects is needed in order to adequately bins with training objects. Outliers in a determination are defined by Eq. (1), shown as those outside of the two diagonal lines. The density of points within the lines is quite high – only 2.0% of points lie outside of the lines as outliers. This determination features a reduced RMS error of 0.022. 

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We present several results with the COSMOS bright catalog. First we present results just utilizing the five optical bands u, B, r, i, and z +, which could resemble the default situation for obtaining photometric redshifts from a very large optical survey. We also present results using these five optical bands plus morphological parameters in order to explore whether the inclusion of morphological information can improve photoz estimation in future large optical surveys. For completeness and comparison purposes we also present results utilizing all of the ten photometric bands listed above. Figure 5 shows a plot of estimated photoz versus actual redshift for a particular determination in the tenband case where we have used a small bin size of 0.01 as a demonstration.
In order to quantify the variance for different determinations, we complete six realizations of training and evaluation for every case, each with a randomized training set of 1000 galaxies and an evaluation set of the remaining 13 365 galaxies, and record the number of outliers and RMS errors for the evaluation. Because the membership of the training and evaluation sets is randomized, we obtain slightly varying numbers of outliers and RMS errors with each evaluation. Figure 6 shows the averaged number of outliers and RMS errors for determinations performed using five bands, five bands plus the inclusion of individual shape parameters, five bands plus the inclusion of all shape parameters, and lastly ten bands. We see that the inclusion of shape information does not result in a statistically significant improvement in the fraction of outliers, RMS, or reduced RMS as compared to the fiveband only case. We discuss this further in Sect. 7. As expected, estimates with the tenband case are significantly better than with the fiveband case. We also note that enlarging the training set size beyond 1000 galaxies for this data did not yield an appreciable improvement in either the fraction of outliers or the RMS errors when a binsize of 0.1 was used.
It is potentially interesting to compare the accuracy obtained with SPIDERz to that reported by the COSMOS collaboration’s own photoz analysis on similar data. With the former, in the tenband case, we achieve an average of 1.8% outliers and an average reduced RMS of 0.022. The numbers reported by the latter which most closely correspond to the former are from the “bright spectroscopic redshifts” sample reported by the COSMOS collaboration in Laigle et al. (2016) where they achieve 0.5% outliers and a reduced RMS of 0.007 with a method that is based on the LePhare (Ilbert et al. 2006) template fitting code. However, it must be noted that the results in Laigle et al. (2016) are obtained using up to 30 bands of photometry from ultraviolet to infrared including some quite narrow (<300 Å) bands. The two results then are difficult to compare directly, as the analysis with SPIDERz is disadvantaged by having fewer bands.
5. Tests with the COSMOS and 3DHST overlap data
The COSMOS bright data set discussed in Sect. 4 has the advantage of containing many thousands of galaxies, but the disadvantage of being limited to relatively low redshifts. To obtain a data set of real galaxies with publicly available spectroscopic redshifts that contains higher redshift sources we use spectroscopic redshifts from the 3DHST survey performed with the Hubble Space Telescope and reported in Momcheva et al. (2016) that overlap with COSMOS photometry and morphology. This results in a data set of 3048 galaxies, of which 206 (6.8%) have z> 2 and 537 (17.6%) have z> 1.5. These galaxies have photometry and morphological information as discussed in Sect. 4.1. We note that this is the largest redshift range for which the inclusion of morphological information for photoz determination has been tested, and that potentially morphological information may manifest an advantage in data sets with larger redshift ranges that is not present in narrower ranges.
Fig. 6 Percentage of outliers (top) along with nonreduced (middle) and reduced (bottom) RMS error σ_{Δz/ (1 + z)} in the photoz estimation with the inclusion of different bands and morphological parameters in the COSMOS field data set discussed in Sect. 4 as determined with SPIDERz. The uncertainties represent the standard deviation of the values obtained from different realizations featuring different random compositions of the training and evaluation sets, as discussed in Sect. 4.2. Results are shown for the fiveband case, the cases of five photometric bands plus each individual morphological parameter, the case of five photometric bands plus all morphological parameters, and the ten photometric band case. 

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Fig. 7 Estimated photoz as determined by SPIDERz versus the actual redshift for the COSMOSx3DHST data set discussed in Sect. 5. This determination is with the tenband photometric data and a training set consisting of 1200 galaxies chosen at random and an evaluation set consisting of the other 1848 galaxies, with a bin size of 0.1. Outliers in a determination are defined by Eq. (1), shown as those outside of the two diagonal lines. The density of points within the lines is quite high – only 2.6% of points lie outside of the lines as outliers. This determination features a reduced RMS error of 0.04. 

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As with the COSMOS bright data in Sect. 4.2, for the COSMOSx3DHST data we present several results. First we present results just utilizing the five optical bands u, B, r, i, and z +, which could resemble the default situation for obtaining photometric redshifts from a very large optical survey. We also present results using these five optical bands plus morphological parameters in order to explore whether the inclusion of morphological information can improve photoz estimation in future large optical surveys. For completeness and comparison purposes we also present results utilizing all of the ten photometric bands listed above. Similarly, we complete six realizations of training and evaluation for every case, each with a randomized training set of 1200 of the galaxies and an evaluation set of the remaining 1848 galaxies, and record the number of outliers and the RMS errors for the redshift determination for the evaluation set. For this data we increase the proportion of training set galaxies in an effort to train the model with a greater representation of the relatively scarce highest redshift population. Again, each randomized realization produces a slightly different number of outliers and RMS errors. Figure 7 shows a plot of estimated photoz versus actual redshift for one particular determination in the tenband case. Figure 8 shows the number of outliers and RMS errors for data sets composed of five bands, five bands plus the inclusion of individual shape parameters, five bands plus the inclusion of all shape parameters, and ten bands. We see again that the inclusion of shape information does not result in a statistically significant improvement in the fraction of outliers, RMS, or reduced RMS as compared to the fiveband only case. As expected, estimates with the tenband case are significantly better than with the fiveband case.
We note that SPIDERz performs remarkably well on this data set, including on the high redshift objects, considering that a small fraction of the galaxies are high redshift.
6. Tests with AEGIS data
6.1. AEGIS data
For comparison with previous results obtained with a neural network algorithm (Singal et al. 2011) we also perform tests on observations of the Extended Groth Strip from the the Allwavelength Extended Groth Strip International Survey (AEGIS) data set (Davis et al. 2007), which contains photometric band magnitudes in u, g, r, i, and z bands from the CanadaFranceHawaii Telescope Legacy Survey (CFHTLS, Gwyn 2008), imaging from the Advanced Camera for Surveys on the Hubble Space Telescope (HST/ACS, Koekemoer et al. 2007), and spectroscopic redshifts from the DEEP 2 survey using the DEIMOS spectrograph on the Keck telescope. The limiting i band AB magnitude of the CFHTLS survey is 26.5, while that of HST/ACS is 28.75 in V (F606W) band, and that of DEEP2 is 24.1 in R band.
A total of 2612 galaxies spanning redshifts from 0.01 to 1.57, with a mean redshift of 0.702 and a median of 0.725, and i band magnitudes ranging from 24.43 to 17.62, are in the data set used here. The redshift distribution of this particular set of galaxies arises because of the intentional construction of the portion of DEEP2 spectroscopic catalog within the AEGIS survey to have roughly equal numbers of galaxies below and above z = 0.7; therefore it is not an optimized training set for a generic photometric data evaluation set, although a more optimized training set for any given photometric data evaluation set could be constructed from it.
For shape information we use the following morphological parameters, previously derived in other works from the HST/ACS imaging data in two bands, V (F606W) and I (F814W):

1.
The half light radius r_{e};

2.
The concentration c;

3.
The asymmetry A;

4.
The Gini coefficiet G;

5.
M_{20}; and

6.
The axial ratio ε; all as defined in Sect. 4.1, as well as

7.
The smoothness S: . The smoothness is used to quantify the presence of smallscale structure in the galaxy. It is calculated by smoothing the image with a boxcar of a given width and then subtracting that from the original image. In this case I_{(x,y)} is the intensity at point (x,y) and I_{S(x,y)} is the smoothed intensity at (x,y), while B_{S} is the average smoothness of the background, calculated in the same way. The residual is a measure of the clumpiness due to features such as compact star clusters. In practice, the smoothing scale length is chosen to be a fraction of the Petrosian radius; and

8.
The Sérsic power law index n_{s} where the Sérsic profile has a form Σ(r) = Σ_{e} e^{− k  (r/re)(1 /ns)−1 } (e.g. Graham & Driver 2005), where Σ_{e} is the surface brightness at radius r_{e} and k is defined such that half of the total flux is contained within r_{e}.
Parameters c, A, S, G, and M_{20} are determined in Lotz et al. (2008), while ε, n_{s}, and r_{e} are determined by Griffith et al. (2012) using the Galfit package (Peng et al. 2002; Häussler et al. 2007).
For comparison with a previous result in this case we form principal components of the morphological parameters for this data set. Principal components (e.g. Jolliffe 2002) are the result of a coordinate rotation in a multidimensional space of possibly correlated data parameters into vectors with maximum orthogonal significance. The first principal component is along the direction of maximum variation in the data space, the second is along the direction of remaining maximum variation orthogonal to the first, the third is along the direction of remaining maximum variation orthogonal to both of the first two, and so on. The morphological principal components are given as linear combinations of the eight morphological parameters in Table 1 of Singal et al. (2011).
Fig. 8 Percentage of outliers (top) along with nonreduced (middle) and reduced (bottom) RMS error σ_{Δz/ (1 + z)} in the photoz estimation with the inclusion of different bands and morphological parameters in the COSMOSx3DHST data set discussed in Sect. 5 as determined with SPIDERz. The uncertainties represent the standard deviation of the values obtained from different realizations featuring different random compositions of the training and evaluation sets, as discussed in Sect. 4.2. Results are shown for the five photometric band case, the cases of five photometric bands plus each individual morphological parameter, the case of five photometric bands plus all morphological parameters, and the ten photometric band case. 

Open with DEXTER 
A further discussion of the particular mapping from morphological to principal components is available in Sect. 3 of Singal et al. (2011). As mentioned there the first principal component is well correlated with galaxy type, and correlations persist through several of the other principal components. These correlations hinted that the morphology may provide an additional handle on the photoz estimation, since outliers often occur because a spectral feature (such as a break) of one galaxy type at a given redshift may be seen by the observer to be at the same wavelengths as a spectral feature of another galaxy type at different redshift. Thus it was an intriguing hypothesis that morphological information indicative of galaxy type may help break this degeneracy.
6.2. Results with AEGIS data
As in Sects. 4.2 and 5 we complete six realizations of training and evaluation for every case, for this data with a randomized training set of 700 of the galaxies discussed in Sect. 6.1 and an evaluation set of the remaining 1912 galaxies, and record the number of outliers and the RMS error for the redshift determination for the evaluation set. Here as well because in each realization the membership of the training and evaluation sets varies, each realization for a given input parameter set produces a slightly different number of galaxies in the evaluation set that are outliers and a slightly different RMS error. For comparison, the template fitting results reported by Ilbert et al. (2006) using band photometry only give 5% outliers and a (nonreduced) RMS error of σ_{Δz/ (1 + z)} = .1881 for this sample. This error is dominated by the catastrophic outliers (Fig. 3), and clearly visually drops to below that of SPIDERz if outliers are excluded.
Fig. 9 Percentage of outliers (top) and nonreduced RMS error σ_{Δz/ (1 + z)} (bottom) in the photoz estimation with the inclusion of different individual principal components of the morphological parameters with the AEGIS data set discussed in Sect. 6, shown for SPIDERz (solid lines and star points) and for the custom neural network described in Singal et al. (2011; dashed lines and cross points). The uncertainties represent the standard deviation of the values obtained from different realizations featuring different compositions of the training and evaluation sets, as discussed in Sect. 6.2. 

Open with DEXTER 
Fig. 10 Percentage of outliers (top) and nonreduced RMS error σ_{Δz/ (1 + z)} (bottom) in the photoz estimation with the inclusion of multiple principal components of the morphological parameters with the AEGIS data set discussed in Sect. 6, starting with none, adding the first morphological principal component, then the first and the second principal components, and so on. Results are shown for SPIDERz (solid lines and star points) and for the custom neural network described in Singal et al. (2011, dashed lines and cross points). The uncertainties represent the standard deviation of the values obtained from different realizations featuring different compositions of the training and evaluation sets, as discussed in Sect. 6.2. 

Open with DEXTER 
Figure 9 shows the number of outliers and RMS error for the inclusion of the seven different principal components individually. Figure 10 shows the number of outliers and RMS error for the inclusion of multiple principal components, starting with none, then adding in the first, then adding in the first and second, then adding in the first through third, and so on. We do not show the reduced RMS in this case because it is not available for comparison in the neural network determination. In each figure, the error bars correspond to the standard deviation of the number of outliers or RMS scatter in the different realizations. We note that the last principal component (PC8) should by definition contain minimal significant variation in the morphological parameters, so we do not include it in the analysis.
It is apparent that the SVM algorithm of SPIDERz results in a significant decrease in the number of outliers and RMS error compared to the artificial neural network algorithm previously tested. In addition, the standard deviation for different realizations in the number of outliers is generally smaller with the SVM method, allowing us to determine that adding morphological information in the form of individual principal components of the morphological parameters does not provide a statistically significant decrease in the average number of outliers or the RMS error, while adding multiple principal components increases the number of outliers and the RMS error.
7. Discussion
We have developed a custom SVM classification algorithm for photometric redshift estimation in the IDL environment. The package, SPIDERz, is available to the community. It outputs for each galaxy both an effective distribution of probabilities (in bins of redshift) for each galaxy’s photoz and a singlevalued, most likely predicted photoz bin, with the bin size chosen by the user. In this analysis for practicality of evaluating metrics such as outliers and RMS errors we use only the singlevalued photoz prediction.
We compare results obtained with SPIDERz to those previously reported for other codes with the PHAT1 catalog in Sect. 3.2. We see that SPIDERz performs comparable to other empirical methods on this catalog, noting that as discussed in Sect. 3.1 far fewer training galaxies were available for SPIDERz. On this latter point, having such a reduced number of training galaxies available is a significant disadvantage for SPIDERz or any empirical method in a dataset such as PHAT1 where proportionally few of the galaxies are higher redshift. In the context of SVC as discussed in Sect. 2.2, as the training data in certain redshift bins becomes sparse, there may be insufficient support vectors available for those bins in the binary classifications for effective hyperplane solutions.
SPIDERz can naturally include additional parameters beyond band magnitudes. We note that an SVM is in a sense an unbiased way of determining the relative strength of the correlations of a set of input parameters with the output parameter, and that this SVM algorithm is designed to treat all input parameters on an equal footing, thus providing for a convenient method for investigating the inclusion of additional inputs beyond photometry.
In order to both explore a much larger dataset and examine the effects of the inclusion of morphological parameters on photoz estimation, we form a data set of 14 365 galaxies with photometry, morphological parameters, and spectroscopic redshifts from the COSMOS field as discussed in Sect. 4. We find that while SPIDERz performs relatively well on this data, that the inclusion of morphological information in the form of morphological parameters does not improve the number of outliers or RMS errors in photoz estimation over the case of five optical photometric bands only. As expected, using ten photometric bands reduces the number of outliers and RMS errors considerably relative to five bands.
To study the performance of SPIDERz and the effects of including morphological parameters over a larger redshift range we form a data set of 3048 galaxies from the overlap of COSMOS photometry and morphology with 3DHST spectra as discussed in Sect. 5. We find SPIDERz performs quite well on this data, including on higher redshift galaxies, even though these galaxies form a small fraction of the training set. We again find that the inclusion of morphological information in the form of morphological parameters does not improve the number of outliers or RMS errors in photoz estimation over the case of five optical photometric bands only, and again using ten photometric bands reduces the number of outliers and RMS errors considerably relative to five bands.
For comparison with a previous determination with a neural network algorithm, we also estimate photoz for a data set which consists of 2612 galaxies with five optical band magnitudes, reliable spectroscopic redshifts, and principal components of eight morphological parameters, discussed in Sect. 6. We again find that the inclusion of morphological information does not significantly decrease the number of outliers or RMS error in photoz estimation. Previously Singal et al. (2011) found compatible results with the neural network estimation method. We do note that the inclusion of multiple principal components resulted in a diminished performance in photoz estimation with the neural network algorithm due to the addition of noise while this had less of an effect on the performance of SPIDERz, indicating that perhaps SVMs are less susceptible to the negative effects of adding noise in this situation.
The particular findings regarding the inclusion of shape information thus evidence some robustness in regard to different data sets, consideration of morphological parameters or principal components, and consideration of an SVM or neural network method. We conclude, therefore, that these results are likely applicable to all empirical methods with this redshift range and photometry restricted to the visible and near infrared bands. Any gain that may arise in an empirical photoz determination from correlations between morphology and redshift is overwhelmed by the additional noise introduced. It is likely that any correlations between the morphological parameters and the galaxy type are degenerate to some extent with the correlations between galaxy type and galaxy colors. The possibility remains that under a less inputblind and more complicated scenario where, for example, the regularization parameter for misclassification (see Eq. (15)) varies with the redshift, the additional noise contained in morphological information could be made less consequential. A potentially more straightforward possibility is that morphological information along with probability distribution considerations could be used only to flag galaxies more likely to be catastrophic outliers, which we will explore in a future work.
Available from http://spiderz.sourceforge.net with usage documentation provided there.
Acknowledgments
The authors acknowledge data supplied previously by B. Gerke, M. Shmakova, R.L. Griffith, and J. Lotz. Based in part on observations made with the NASA/ESA Hubble Space Telescope, obtained from the Data Archive at the Space Telescope Science Institute, which is operated by the Association of Universities for Research in Astronomy, Inc., under NASA contract NAS 526555. Funding for the DEEP2 survey has been provided by NSF grants AST0071048, AST0071198, AST0507428, and AST0507483. Some of The data presented herein were obtained at the W. M. Keck Observatory, which is operated as a scientific partnership among the California Institute of Technology, the University of California and the National Aeronautics and Space Administration. The Observatory was made possible by the generous financial support of the W. M. Keck Foundation. The DEEP2 team and Keck Observatory acknowledge the very significant cultural role and reverence that the summit of Mauna Kea has always had within the indigenous Hawaiian community and appreciate the opportunity to conduct observations from this mountain.
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All Tables
Results for the “cleaned sample” of the PHAT1 catalog with onequarter of galaxies used for training and the remaining threequarters used for evaluation, shown for SPIDERz as determined in this work along with other empirical codes and the two best performing template fitting codes as reported in Hildebrandt et al. (2010).
All Figures
Fig. 1 Depiction of linearly separable binary class system. For visualization this figure depicts a two dimensional input space, while the input space for photoz determination with SPIDERz is of higher dimension (the dimensions being all band magnitudes plus any other parameters). In this depiction the two classes are filled and open circles. The margin width is equal to where w is a vector perpendicular to the hyperplane as defined in Sect. 2.2. 

Open with DEXTER  
In the text 
Fig. 2 Conceptual visualization of binary class system which is not linearly separable in the input space (left) but is separable by a hyperplane when mapped to a higher dimensional feature space (right) with some function φ : x → φ(x). 

Open with DEXTER  
In the text 
Fig. 3 Top: the estimated photoz versus the actual redshift, as determined by SPIDERz, for the AEGIS data set discussed in Sect. 6 with no morphological parameters included. The training set is formed from 700 galaxies and the evaluation set, for which the results are plotted, consists of the remaining 1912 galaxies. “Outliers” in a determination are defined by Eq. (1), shown as those outside of the two diagonal lines. Middle: photozs for the same galaxies, as estimated with the custom neural network as reported in Singal et al. (2011). Bottom: photozs for the same galaxies as estimated with the Lephare template fitting code (Ilbert et al. 2006). The template fitting method has a lower scatter for nonoutliers, but a larger number of outliers than the SVM and neural network for these galaxies. 

Open with DEXTER  
In the text 
Fig. 4 Estimated photoz as determined by SPIDERz versus the actual redshift for the PHAT1 data set discussed in Sect. 3.1 for the case of 14 photometric bands. This determination is with a training set consisting of 94 galaxies chosen at random and an evaluation set consisting of the other 280 galaxies. Outliers are defined by Eq. (1), shown as those outside of the two diagonal lines. This determination results in 15.3% outliers and a reduced RMS of 0.067, which, despite the smaller training set available, is competitive with the results obtained by other empirical methods as shown in Table 1 and discussed in Sect. 3.2. 

Open with DEXTER  
In the text 
Fig. 5 Estimated photoz as determined by SPIDERz versus the actual redshift for the COSMOS data set discussed in Sect. 4. This determination was performed with tenband photometry and a designated bin size of 0.01. The training and evaluation sets are comprised of 3000 and 11 365 randomly chosen galaxies, respectively. With this small bin size, a relatively large ratio of training set objects is needed in order to adequately bins with training objects. Outliers in a determination are defined by Eq. (1), shown as those outside of the two diagonal lines. The density of points within the lines is quite high – only 2.0% of points lie outside of the lines as outliers. This determination features a reduced RMS error of 0.022. 

Open with DEXTER  
In the text 
Fig. 6 Percentage of outliers (top) along with nonreduced (middle) and reduced (bottom) RMS error σ_{Δz/ (1 + z)} in the photoz estimation with the inclusion of different bands and morphological parameters in the COSMOS field data set discussed in Sect. 4 as determined with SPIDERz. The uncertainties represent the standard deviation of the values obtained from different realizations featuring different random compositions of the training and evaluation sets, as discussed in Sect. 4.2. Results are shown for the fiveband case, the cases of five photometric bands plus each individual morphological parameter, the case of five photometric bands plus all morphological parameters, and the ten photometric band case. 

Open with DEXTER  
In the text 
Fig. 7 Estimated photoz as determined by SPIDERz versus the actual redshift for the COSMOSx3DHST data set discussed in Sect. 5. This determination is with the tenband photometric data and a training set consisting of 1200 galaxies chosen at random and an evaluation set consisting of the other 1848 galaxies, with a bin size of 0.1. Outliers in a determination are defined by Eq. (1), shown as those outside of the two diagonal lines. The density of points within the lines is quite high – only 2.6% of points lie outside of the lines as outliers. This determination features a reduced RMS error of 0.04. 

Open with DEXTER  
In the text 
Fig. 8 Percentage of outliers (top) along with nonreduced (middle) and reduced (bottom) RMS error σ_{Δz/ (1 + z)} in the photoz estimation with the inclusion of different bands and morphological parameters in the COSMOSx3DHST data set discussed in Sect. 5 as determined with SPIDERz. The uncertainties represent the standard deviation of the values obtained from different realizations featuring different random compositions of the training and evaluation sets, as discussed in Sect. 4.2. Results are shown for the five photometric band case, the cases of five photometric bands plus each individual morphological parameter, the case of five photometric bands plus all morphological parameters, and the ten photometric band case. 

Open with DEXTER  
In the text 
Fig. 9 Percentage of outliers (top) and nonreduced RMS error σ_{Δz/ (1 + z)} (bottom) in the photoz estimation with the inclusion of different individual principal components of the morphological parameters with the AEGIS data set discussed in Sect. 6, shown for SPIDERz (solid lines and star points) and for the custom neural network described in Singal et al. (2011; dashed lines and cross points). The uncertainties represent the standard deviation of the values obtained from different realizations featuring different compositions of the training and evaluation sets, as discussed in Sect. 6.2. 

Open with DEXTER  
In the text 
Fig. 10 Percentage of outliers (top) and nonreduced RMS error σ_{Δz/ (1 + z)} (bottom) in the photoz estimation with the inclusion of multiple principal components of the morphological parameters with the AEGIS data set discussed in Sect. 6, starting with none, adding the first morphological principal component, then the first and the second principal components, and so on. Results are shown for SPIDERz (solid lines and star points) and for the custom neural network described in Singal et al. (2011, dashed lines and cross points). The uncertainties represent the standard deviation of the values obtained from different realizations featuring different compositions of the training and evaluation sets, as discussed in Sect. 6.2. 

Open with DEXTER  
In the text 
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