Issue 
EPJ Nuclear Sci. Technol.
Volume 2, 2016



Article Number  11  
Number of page(s)  14  
DOI  https://doi.org/10.1051/epjn/e2016500027  
Published online  18 March 2016 
https://doi.org/10.1051/epjn/e2016500027
Regular article
Comparison of SERPENT and SCALE methodology for LWRs transport calculations and additionally uncertainty analysis for crosssection perturbation with SAMPLER module
Institute for Industrial, Radiophysical and Environmental Safety (ISIRYM), Universitat Politècnica de València, Camí de Vera s/n, 46022, Valencia, Spain
^{⁎} email: alabarile@iqn.upv.es
Received:
28
April
2015
Received in final form:
30
October
2015
Accepted:
12
January
2016
Published online:
18
March
2016
In nuclear safety research, the quality of the results of simulation codes is widely determined by the reactor design and safe operation, and the description of neutron transport in the reactor core is a feature of particular importance. Moreover, for the long effort that is made, there remain uncertainties in simulation results due to the neutronic data and input specification that need a huge effort to be eliminated. A realistic estimation of these uncertainties is required for finding out the reliability of the results. This explains the increasing demand in recent years for calculations in the nuclear fields with bestestimate codes that proved confidence bounds of simulation results. All this has lead to the Benchmark for Uncertainty Analysis in Modelling (UAM) for Design, Operation and Safety Analysis of LWRs of the NEA. The UAMBenchmark coupling multiphysics and multiscale analysis using as a basis complete sets of input specifications of boiling water reactors (BWR) and pressurized water reactors (PWR). In this study, the results of the transport calculations carried out using the SCALE6.2 program (TRITON/NEWT and TRITON/KENO modules) as well as Monte Carlo SERPENT code, are presented. Additionally, they have been made uncertainties calculation for a PWR 15 × 15 and a BWR 7 × 7 fuel elements, in two different configurations (with and without control rod), and two different states, Hot Full Power (HFP) and Hot Zero Power (HZP), using the TSUNAMI module, which uses the Generalized Perturbation Theory (GPT), and SAMPLER, which uses stochastic sampling techniques for crosssections perturbations. The results obtained and validated are compared with references results and similar studies presented in the exercise I2 (Lattice Physics) of UAMBenchmark.
© A. Labarile et al., published by EDP Sciences, 2016
This is an Open Access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/4.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.
1 Introduction
This work takes part in the framework of the Organization for Economic Cooperation and Development/Nuclear Energy Agency (OECD/NEA) Benchmark, for Uncertainty Analysis in BestEstimate Modelling (UAM), for Design, Operation and Safety Analysis of LWRs. The groundwork was launched in 2005 with the objective to prepare a benchmark work program with steps (exercises) that would be needed to define the uncertainty and modelling task for the development of uncertainty analysis methodologies, for multiphysics and multiscale simulation. The final goal will create a roadmap along with schedule and organization, for the development and validation of method and codes required for uncertainty and safety analysis in LWR design [1].
Reference systems and scenarios for coupled code analysis are defined to study the uncertainty effects for all stages of the system calculations. Measured data from plant operation and experimental reference data are available for the chosen scenarios. The full chain of uncertainty propagation from basic data, engineering uncertainties, across different scales (multiscale), and physics phenomena (multiphysics) is tested on some benchmark exercises for which experimental data are available and for which the power plant details have been released. The general frame of the OECD UAM LWR Benchmark consists of three phases with different exercises for each phase: Phase 1 (neutronics phase), Phase 2 (core phase) and Phase 3 (system phase). The focus of Phase 1 is on propagating uncertainties in standalone neutronics calculations and consists of the following three exercises:

Exercise I1: “Cell Physic” focused on the derivation of the multigroup microscopic crosssection libraries and associated uncertainties;

Exercise I2: “Lattice Physics” focused on the derivation of the fewgroup macroscopic crosssection libraries and associated uncertainties;

Exercise I3: “Core Physics” focused on the core steady state standalone neutronics calculations and associated uncertainties.
The present paper deals with Cell Physic and Lattice Physics exercises, determining uncertainties associated with basic nuclear data, method and modelling approximation used in lattice physics codes.
This document is structured as follows: the Introduction in Section 1. Section 2 is focused on the description of the codes. The description of the models is shown in Section 3. The results for different codes are presented in Section 4. Finally, the conclusions are shown in Section 5.
2 Codes description
2.1 Transport calculation
In this work, two and threedimensional lattice codes (deterministic and stochastic) were selected to perform transport calculations: SCALE6.2 with TRITON/NEWT and TRITON/KENO modules and SERPENT2.1.22 code.
The SCALE code system [2] is a collection of computational modules whose execution can be linked by various “sequences” to solve a wide variety of applications.
TRITON (Transport Rigor Implemented with Timedependent Operation for Neutronics depletion) is a multipurpose SCALE control module for transport and depletion calculations for reactor physics applications. TRITON is used to provide automated, problemdependent crosssections processing followed by multigroup neutron transport calculation for one, two or threedimensional configuration [3].
NEWT (New ESCbased Weighting Transport code) is a twodimensional (2D) discrete ordinates transport code developed at Oak Ridge National Laboratory. It is based on the Extended Step Characteristic (ESC) approach for spatial discretization in an arbitrary mesh structure. This discretization scheme makes NEWT an extremely powerful and versatile tool for deterministic calculation in realworld nonorthogonal problem domains. The NEWT computer code has been developed to run on SCALE. Thus, NEWT uses AMPXformatted crosssections processed by other SCALE modules [4].
The implemented methodology of these coupled modules of SCALE allows carrying out transport calculation with the computation of energy collapsed and homogenized macroscopic crosssections. In TRITON, NEWT is used to calculate weighted burnupdependent crosssections that are employed to provide localized fluxes used for multiple depletion regions. Additionally, TRITON uses a twopass crosssection update approach to perform fuel assembly burnup calculations and generates a database of crosssections and other burnupdependent physics data that can be used for fullcore analysis [5].
KENO is a functional module in the SCALE system and a Monte Carlo criticality program used to calculate the k_{eff} of threedimensional (3D) system [6]. It uses the SCALE Generalized Geometry Package (SGGP), which offers a powerful geometric representation. KENO was one of the oldest criticality safety analysis tools in SCALE. The primary purpose of its employment in this work is to determine k_{eff} calculations and compare KENO results with TRITON/NEWT and SERPENT2 calculation.
SERPENT is a threedimensional continuousenergy code, based on the Monte Carlo method, for reactor physics burnup calculation [7,8]. The SERPENT project started in 2004 at the VTT Technical Research Centre of Finland. The first version of the code was available to universities and research institutes from 2008 and currently it is still under development. The suggested applications of SERPENT include, among other applications, the spatial homogenization and constant group generation for deterministic reactor calculations and the validation of deterministic lattice transport codes.
2.2 Sensitivity and uncertainty calculation
Sensitivity analysis and propagation of uncertainties of crosssections have been carried out using TSUNAMI and SAMPLER modules.
TSUNAMI2D (Tools for Sensitivity and Uncertainty Analysis Methodology Implementation in Two Dimension) is a SCALE sequence for calculating sensitivity coefficients and response uncertainties to nuclear systems analyses for criticality safety applications. TSUNAMI uses the Generalized Perturbation Theory (GTP) that performs similarity analysis and consolidates experimental and computational results through data adjustment. The uncertainties, resulting from uncertainties in the basic data, are estimated using energydependent crosssectioncovariance matrices [9]. The SAMS module is used to determine the sensitivities of calculated value of k_{eff} and other system responses to the nuclear data used in the calculations as a function of a nuclide, reaction type, and energy. This sensitivity of k_{eff} to the number density is equivalent to the sensitivity of k_{eff} to the total crosssection, integrated over energy. Because the total crosssection sensitivity coefficient tests much of the data used to compute all other sensitivity coefficients, it is considered an adequate test for verification. For each sensitivity coefficient examined by direct perturbation, the k_{eff} of the system is computed first with the nominal values of the input quantities, and then with a selected nominal input value increased by a certain percentage, and then with the nominal value decreased by the same percentage. The direct perturbation sensitivity coefficient of k_{eff} to some input value α is computed as:(1)where α^{+} and α^{−} represent the increased and decreased values, respectively, of the input quantity α, and k_{α+} and k_{α−} represent the corresponding values of k_{eff}.
Statistical uncertainties in the computed values of k_{eff} are propagated to direct perturbation sensitivity coefficients by standard error propagation techniques as:(2)
It is important in sensitivity calculations to ensure that the k_{eff} value of the forward and adjoint solutions closely agree, and typically, the transport calculation of concern is the adjoint calculation. More details of the GPT methodology are provided in the SAMS manual [10].
SAMPLER is a module for statistical uncertainty analysis of any SCALE sequences. The SAMPLER methodology samples probability density functions (pdf) defined by information in the SCALE multigroup covariance library by XUSA program and produces a random sample for the input computational data vector (CDV) that contains all nuclear crosssections used in a transport calculation. After making random perturbations in input data, SAMPLER responses uncertainties are computed by statistical analysis of output responses distribution [11].
The perturbed data vector can be used in any SCALE functional module to perform a single forward solution that computes all the desired perturbed responses. The process is repeated for the specified number of random input samples, and the resulting distribution of output responses from SCALE can be analysed with standard statistical analysis tools to obtain the standard deviations and correlation coefficients for all responses. The typical approach is to assume that the generic multigroup (MG) data pdf is a multivariate normal distribution, which is completely defined by the expected values and covariance matrices for the data. An XSUSA statistical sample consists of a full set of perturbed, infinitely dilute MG data for all groups, reactions, and materials. The SCALE generic multigroup covariance data are given as relative values of the infinitely dilute crosssections, so a random perturbation sample for crosssections σ_{x,g}(∞) corresponds to Δσ_{x,g}(∞)/σ_{x,g}(∞). XSUSA converts these values to a set of multiplicative perturbation factors Q_{x,g} that are applied to the reference data to obtain the altered values:(3)
Subsequently, the multiplicative perturbation factors for all data are preprocessed and stored in a data file for subsequent SCALE calculations [12].
To obtain the uncertainty and correlation coefficient, all parameters are randomly perturbed for each calculation, and the uncertainties and correlations are determined. Mathematically, the uncertainty in an individual output parameter k is determined as:(5)where Δk^{exp}(i) is the uncertainty in system i due to uncertainties in the input parameters.
is the ath Monte Carlo (MC) sample of system i, where all uncertain input parameters have been randomly varied within the specified distribution.
The covariance between two systems, i and j, is determined as shown in equation (6).(6)
The correlation coefficient between systems i and j can be determined from equations (5) and (6) as:(7)
3 Model description
Two main LWR types have been selected for this study, based on previous benchmark experience and available data:

Pressurized Water Reactor (PWR)  Three Mile Island 1 (TMI1);

Boiling Water Reactor (BWR)  Peach Bottom 2 (PB2).
Both models have been analyzed at Hot Full Power (HFP) and Hot Zero Power (HZP) conditions.
Additionally, the two models have been designed with and without control rod.
The different fuel pin cell geometry and reference configuration are schematized in Figures 1 and 2.
SCALE calculations use the Extended Step Characteristic (ESC) approach. The entire problem domain is mapped regarding a set of finite cells. Cells sharing a given side share the value of the angular flux on that side. Once the angular flux has been determined for all sides of the cell for the given direction, it is possible to use a neutron balance to compute the average value of the angular flux within the cell. The process is then repeated for all direction. Numerical quadrature can then be used to determine the average scalar flux in each cell in the problem domain and can be used to determine fission and scattering reaction rates and to update the value of average cell source. In this way, the spatial discretization in SCALE allows to obtain satisfactory results.
The propagation of the crosssections uncertainties across lattice physics is the main purpose of this exercise. To achieve that, in UAMBenchmark instructions there are defined two assembly design for the models studied (a PWR and a BWR) [13]. These assemblies are shown in Figures 3 and 4 while Table 1 shows both fuel assemblies data.
As a result of implementing both fuel assemblies in TRITON/NEWT code for transport calculation, the layout outputs for both types of assemblies have been obtained, as shown in Figures 5 and 6.
There are different methodologies used in our calculation of this work. These methods cover the deterministic approach (TRITON/NEWT) and Monte Carlo methodology (TRITON/KENO and SERPENT), as well as the Generalized Perturbation Theory (TSUNAMI) to stochastic sampling techniques (SAMPLER).
Fig. 1 The configuration of PB2 BWR unit cell. 
Fig. 2 The configuration of TMI1 PWR unit cell. 
Fig. 3 PB2 BWR assembly design. 
Fig. 4 TMI1 PWR assembly design. 
Fuel assembly data for the test cases of Exercises I2.
Fig. 5 BWR and PWR without control rod 2D assembly. 
Fig. 6 BWR and PWR with control rod 2D assembly. 
4 Results
In this section, the results of transport calculation with TRITON/NEWT, SERPENT2 and TRITON/KENO are presented, as well as the sensitivity analysis and propagation of uncertainties results that were performed using TSUNAMI and SAMPLER modules. All calculations were carried out for four assemblies models (like shown in Figs. 5 and 6) and two different states (HFP and HZP), with a total of eight configurations for this test case in UAMBenchmark, Exercise I2.
4.1 TRITON/NEWT and SERPENT2 results
Results for the k_{eff} and crosssection values are summarized in this section. The aim is to compare TRITON/NEWT and SERPENT2 results with the average of Benchmark participation values. In the TRITON/NEWT modules, the 238group nuclear data library collapse was used. Otherwise, the computation with the SERPENT2.1.22 code was carried out with two libraries, JEFF3.1 and ENDF/BVII, to compare results with SCALE (ENDF/BVII.1 library).
The output values compared in this paper are listed in Table 2. Comparison of TRITON/NEWT and SERPENT2 are carried out for the multiplication factor (k_{eff}), the Absorption crosssection, the Fission crosssection, the Diffusion crosssection and the Flux. All crosssection values are presented for both groups, Fast and Thermal.
In Tables 3 and 4, the first column shows the output values compared in this paper, the second one are the reference values found in UAMBenchmark results. The third and fourth columns represent TRITON/NEWT calculations and its error with UAMBenchmark references. Subsequently, the results of SERPENT2 calculations and their comparison with TRITON/NEWT and UAMBenchmark values are presented.
The reference values adopted in these tables have been calculated as an average of all submitted results of all benchmark participants, referring to the last submission of 2013.
It should be considered that each participant uses their own code, and this can introduce errors due to the different methodology of each code, but the objective of the benchmark program takes into account these discrepancies.
Therefore, in this work, we calculated the average results of all participants and it is intended to calculate the error between our simulation against SCALE and SERPENT codes.
It is evident from Table 3 that there is good agreement between TRITON/NEWT and reference values, especially for the unrodded configurations. There is a slight recurring discrepancy in the flux value (in both groups, one and two), but it is assumed to be because of different normalization methods of implemented codes in this benchmark exercise.
In Table 3, comparing the SERPENT2.1.22 results with TRITON/NEWT and UAMBenchmark, it can be seen a good agreement in both models (BWR and PWR) as has been observed for SCALE results. The slight differences, especially in flux and diffusion coefficient results, can be due to the different methodologies (Monte Carlo) implemented in SERPENT code. In fact, in order to obtain most accurate results, the option B1 was adopted in SERPENT calculation while this option is not available in the SCALE beta version used in this work.
Additionally, we have compared SERPENT calculations using both JEFF3.1 and ENDF/BVII libraries, and the JEFF3.1 results are more close to TRITON/NEWT values despite TRITON/NEWT uses the ENDF/BVII library.
Even though the slight differences comparing SERPENT with validated and reference results, it could be a good transport calculation code, ongoing testing and validation.
With the aim to show a clearest exposition of the results, the standard deviations in SERPENT, which are lower than 30 pcm for all cases presented, are avoided in Tables 3 and 4.
Table 4 shows good agreement between TRITON/NEWT and reference values like it was presented in Table 3. Comparing SERPENT2 results with TRITON/NEWT and UAMBenchmark, the results are similar, as shown in PWR configuration in Table 3.
Even though a different approach is used in the SERPENT code, there is an acceptable agreement between SERPENT2 and TRITON/NEWT and Benchmark values. In this case, JEFF3.1 library results are a little bit better comparing with ENDF/BVII library.
As a conclusion, it is important to give relevance to the short computational times in transport calculation for SERPENT code that was found faster than TRITON/NEWT code. In fact, in SERPENT calculation they have simulated 50,000 particles and 350 cycles in which the first 50 cycles were discarded because of its low statistical weight.
For all exercises, it was used a cluster composed of four blocks with 18 servers equipped with two processors Intel Xeon E54620 8c/16T and with a RAM of 64 GB DDR3, and 2 × interfaces 1 0 GbE.
A comparison of the total computational time between SERPENT and TRITON/NEWT calculations, for PWR_HFP_unrodded configuration, returns:

SERPENT total computational time (seconds): 935;

TRITON/NEWT total computational time (seconds): 1358.
Parameter list to compare  Exercise I2.
Comparison of crosssection values of PWR Benchmark configuration exercises I2.
Comparison of crosssection values of BWR Benchmark configuration exercises I2.
4.2 TRITON/KENO and SERPENT2 results
From TRITON/KENO calculation, the best estimate system of k_{eff} in 3D Monte Carlo methodology is obtained, and it is possible to compare these results with deterministic values as shown in Table 5. In this table, the first column shows TRITON/KENO results, the k_{eff} values obtained in TRITON/NEWT figured in the second column, and its error with TRITON/KENO was finally reported.
Analysing Table 5 is possible to corroborate a good agreement through both SCALE models since the largest error calculated has been 0.45%.
Comparison of KENO and NEWT k_{eff} assembly results.
4.3 TSUNAMI2D results
TSUNAMI module is very useful for sensitivity analysis and propagation of uncertainties of crosssections. TSUNAMI employs the Generalized Perturbation Theory and determines the sensitivities coefficient for each nuclide. Furthermore, the sensitivity coefficients for total reaction for each nuclide and mixture can be calculated with this module.
A list of four major contributors to the uncertainty in k_{eff} by individual energy covariance matrices is presented in Figure 7 for BWR calculations and in Figure 8 for PWR calculations.
In both figures, it is possible to find out that the list of major contributors does not vary greatly from case to case, and for all cases uranium seems to be responsible for the uncertainty of k_{eff}. In particular, ^{238}U_{n,γ}, ^{235}U_{nubar}, ^{238}U_{n,n’}, are present at the top of contributors list.
Finally, looking at these results is possible to wise up the relative standard deviation due to crosssection covariance data. The relative standard deviation has been close to 0.50% in all cases, for both BWRs and PWRs calculations.
Likewise, it is interesting to analyse the sensitivity profiles of these major contributors, as shown in Figures 9 and 10. The sensitivity per unit lethargy profiles looks similar, with peaks ranging from 0.28 to 0.35. Sensitivity at Hot Full Power state has emerged greater than sensitivity at Hot Zero Power state, for all cases of study. Moreover, sensitivity profile varies only slightly from case to case, and they do not lead to changes in the uncertainty of the k_{eff}. Figures 9 and 10 represent BWRs and PWRs calculations, respectively.
Fig. 7 Most important contributor to uncertainty in k_{eff} (%Δk/k) in BWRs. 
Fig. 8 Most important contributor to uncertainty in k_{eff} (%Δk/k) in PWRs. 
Fig. 9 Sensitivity profiles of most important contributor to uncertainty in k_{eff}, BWRs cases. 
Fig. 10 Sensitivity profiles of most important contributor to uncertainty in k_{eff}, PWRs cases. 
4.4 SAMPLER results
SAMPLER calculation provides not only estimates for the expected values of the data but also covariance data describing the correlated uncertainty. SAMPLER repeats perturbation steps for a specified number of samples to obtain a distribution of results that can be converted to a standard deviation and correlation coefficients. The SCALE Criticality Safety Analysis Sequence (CSAS) with the 238group nuclear data library was used for the computations.
Based on the Wilks’ approach [14], the sample size for double tolerance limits with a 95% of uncertainty and with 95% of statistical confidence for the output variables is equal to 146 samples [15], which is the number of runs performed in this work.
To provide information on sampling convergence, layout response of SAMPLER results is presented. For every case run within SAMPLER, any number of responses can be extracted. For instance, the histogram plots that indicate the distribution of the k_{eff} and some crosssection computed values for these benchmark exercises are listed below. Figure 11 shows histogram results of BWR with control rod, at hot zero power state (HZP). The k_{eff} and two crosssections (fission and flux) values for the fast and thermal group are represented.
While Figure 12 shows PWR histogram results, in unrodded configuration and at hot full power state (HFP).
In the same way, are represented the k_{eff} and fission, and flux crosssection results for the fast and thermal group.
According to the print flag set by the user, SAMPLER also prints a list of tables with interesting information, like average values and standard deviation, correlation matrices, and covariance matrices and so on. Another of interesting results of perturbed variables in SAMPLER layout is the running average, which represent average values and standard deviation for samples of the population during simulation.
Moreover, in SAMPLER response it is possible to see that samples population are closer to the average value and almost entirely within its standard deviation, this is shown in the figures below. According to Wilks’ theory, more than 95% of reliability is reached with 146 samples.
Figure 13 shows samples population with averaged values and standard deviation of BWR with control rod configuration, at hot zero power state (HZP). The k_{eff} and two crosssections (fission and flux) values, for the fast and thermal group, are represented. While Figure 14 shows PWR results of samples population with averaged values and standard deviation, in unrodded configuration and at hot full power state (HFP). In the same way, are represented the k_{eff} and fission and flux crosssection results, for the fast and thermal group.
Fig. 11 Histogram plot for k_{eff} and two crosssection calculations, for BWR HZP rodded case. 
Fig. 12 Histogram plot for k_{eff} and two crosssection calculations, for PWR HFP unrodded case. 
Fig. 13 Samples population for k_{eff} and two crosssection calculations (fission and flux), for BWR_HZP with control rod. 
Fig. 14 Samples population for k_{eff} and two crosssection calculations (fission and flux), for PWR_HFP without control rod. 
5 Conclusions
This work has been carried out in the framework of UAMBenchmark Exercise I1 Cell Physics and I2 Lattice Physics. The two test cases (PB2 BWR and TMI1 PWR) have been analyzed in two different configurations and two different states, with the objective of quantifying the uncertainty in all step calculation and propagate uncertainties in the LWR whole system.
Transport calculations have been analyzed with the deterministic code TRITON/NEWT and stochastic code SERPENT2.1.22 with the aim of comparing k_{eff} and crosssections results between both codes and with UAMBenchmark reference values.
Sensitivity calculations have been performed with TSUNAMI module, which uses Generalized Perturbation Theory, and SAMPLER for the perturbed crosssection with stochastic sampling techniques.
The following significant conclusions can be highlighted:

TRITON/NEWT is a solid, validated code that has performed well the UAMBenchmark calculations but spent more computational times comparing against the SERPENT2 results. Even though the slight differences comparing SERPENT with validated and reference results, this code could be a good transport calculation code, ongoing testing and validation;

TSUNAMI module was adopted to estimate sensitivity and uncertainty analysis, the impact of the uncertainties in the basic nuclear data on the calculation of the multiplication factor and microscopic and macroscopic crosssections. Uncertainties were found to be ≈0.5% on k_{eff}. The particular ^{238}U_{n,γ}, ^{235}U_{nubar}, ^{238}U_{n,n’} were found to be the most important contributors to the uncertainty in these exercises. The deterministic solutions were compared with SAMPLER response, and good agreement was found for this exercise.
Acknowledgments
This work contains findings produced within the OECD/NEA UAMBenchmark.
This work has been supported by the Generalitat Valenciana under GRISOLIA/2013/A/006 (037) subvention and partially under Project PROMETEOII/008.
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Cite this article as: Antonella Labarile, Nicolas Olmo, Rafael Miró, Teresa Barrachina, Gumersindo Verdú, Comparison of SERPENT and SCALE methodology for LWRs transport calculations and additionally uncertainty analysis for crosssection perturbation with SAMPLER module, EPJ Nuclear Sci. Technol. 2, 11 (2016)
All Tables
All Figures
Fig. 1 The configuration of PB2 BWR unit cell. 

In the text 
Fig. 2 The configuration of TMI1 PWR unit cell. 

In the text 
Fig. 3 PB2 BWR assembly design. 

In the text 
Fig. 4 TMI1 PWR assembly design. 

In the text 
Fig. 5 BWR and PWR without control rod 2D assembly. 

In the text 
Fig. 6 BWR and PWR with control rod 2D assembly. 

In the text 
Fig. 7 Most important contributor to uncertainty in k_{eff} (%Δk/k) in BWRs. 

In the text 
Fig. 8 Most important contributor to uncertainty in k_{eff} (%Δk/k) in PWRs. 

In the text 
Fig. 9 Sensitivity profiles of most important contributor to uncertainty in k_{eff}, BWRs cases. 

In the text 
Fig. 10 Sensitivity profiles of most important contributor to uncertainty in k_{eff}, PWRs cases. 

In the text 
Fig. 11 Histogram plot for k_{eff} and two crosssection calculations, for BWR HZP rodded case. 

In the text 
Fig. 12 Histogram plot for k_{eff} and two crosssection calculations, for PWR HFP unrodded case. 

In the text 
Fig. 13 Samples population for k_{eff} and two crosssection calculations (fission and flux), for BWR_HZP with control rod. 

In the text 
Fig. 14 Samples population for k_{eff} and two crosssection calculations (fission and flux), for PWR_HFP without control rod. 

In the text 
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