MCNP6, the latest and most advanced LANL transport code representing a recent merger of MCNP5 and MCNPX, has been Validated and Verified (V&V) against a variety of intermediate and high-energy experimental data and against results by different versions of MCNPX and other codes. In the present work, we V&V MCNP6 using mainly the latest modifications of the Cascade-Exciton Model (CEM) and of the Los Alamos version of the Quark-Gluon String Model (LAQGSM) event generators CEM03.03 and LAQGSM03.03. We found that MCNP6 describes reasonably well various reactions induced by particles and nuclei at incident energies from 18 MeV to about 1 TeV per nucleon measured on thin and thick targets and agrees very well with similar results obtained with MCNPX and calculations by CEM03.03, LAQGSM03.03 (03.01), INCL4 + ABLA, and Bertini INC + Dresner evaporation, EPAX, ABRABLA, HIPSE, and AMD, used as stand alone codes. Most of several computational bugs and more serious physics problems observed in MCNP6/X during our V&V have been fixed; we continue our work to solve all the known problems before MCNP6 is distributed to the public.PACS. PACS-key discribing text of that key -PACS-key discribing text of that key
IntroductionDuring the past several years, a major effort has been undertaken at the Los Alamos National Laboratory (LANL) to develop the transport code MCNP6 [1,2], the latest and most advanced Los Alamos transport code representing a merger of MCNP5 [3] and MCNPX [4]. The work on MCNP6 is not yet completed; we continue to solve the observed problems in the current version of MCNP6 and to develop and improve it further, with a plan to make it available officially to the users via RSICC at Oak Ridge, TN, USA, during 2011. Before distributing MCNP6 to the public, we must test and validate it on as many test-problems as possible, using reliable experimental data. Extensive Validation and Verification (V&V) of our low energy transport code MCNP5 has been performed and published for many different test-problems involving interactions of neutrons, photons, and electrons with thick and thin targets, therefore V&V of MCNP6 for such problems is important but not very critical. On the other hand, our high-energy transport code, MCNPX, was not tested against experimental data so extensively, especially for high-energy processes induced by protons, and heavy-ions. More important, MCNP6 uses the latest modifications of the Cascade-Exciton Model (CEM) and of the Los Alamos version of the Quark-Gluon String Model (LAQGSM) event generators CEM03.03 and LAQGSM03.03 [5], and they were not tested extensively in MCNPX. This is why it is necessary to V&V MCNP6 at intermediate and high energies, to test how CEM03.03 and LAQGSM03.03 work in MCNP6 and to make sure that the latter properly transports energetic particles and nuclei through the matter.A description of different versions of our CEM and LAQGSM event generators with many useful references may be found in our recent lecture [5]. Let's us recall here only their main assumptions. The basic...