1 / 22

Physics-Based Modeling for TCN Production Rates Calculation

This project aims to calculate the best possible production rates for TCNs using computer codes that simulate particle production and transport. It involves numerical simulation codes such as MCNPX, GEANT, and LCS, and the use of measured or evaluated cross sections. The work includes fine-tuning parameters in the codes, testing with various measurements, and evaluating neutron and cosmic ray fluxes. The results are useful in understanding the production and transport of TCNs.

scecil
Download Presentation

Physics-Based Modeling for TCN Production Rates Calculation

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. Physics-Based ModelingRobert Reedy (UNM), Kyeong Kim (U. Ariz.), and Jozef Masarik(Komensky Univ.) • Objective: Calculate the best possible production rates for TCNs using: • computer codes that numerically simulate particle production and transport • Monte Carlo N Particle eXtended (MCNPX) [Reedy and Kim]; GEANT & LAHET Code System [Masarik]. • the latest measured or evaluated cross sections • Experimental ones for proton reactions; a few measurements or adjusted fits for neutrons. • 6 nuclides: 10Be, 26Al, then 14C, 36Cl, 21Ne, 3He.

  2. Numerical Simulation Codes • MCNPX, GEANT, and LCS codes • extensively developed for nuclear physics; • well tested with many benchmarks; • often used by us for extraterrestrial problems. • Some results by us for terrestrial in situ (and atmospheric) terrestrial cosmogenic nuclides • Not perfectly accurate, but represent fairly well the basic processes involved in the production and transport of primary and secondary particles • Need fine tuning for TCNs.

  3. Work on Codes • Compare codes • Neutron fluxes • Rates for making cosmogenic nuclides • Fine tune parameters in codes • Input cosmic ray spectra – deep space and for different locations on Earth • “Physics” packages in codes • Test with various measurements

  4. Code Work – Compare fluxes • Neutron fluxes using MCNPX and LCS

  5. Code Work, GCR fluxes • Test various galactic cosmic ray spectra • Castagnoli & Lal (1980), Webber & Higbie (2003), others in space and at Earth • Compare input spectra for protons only and both protons and alpha particles using latest versions of MCNPX. • Test physics parameters in the codes • Done for 2 sets by Kim & Reedy (2004) for spallogenic nuclides in meteorite – similar

  6. Code Work, Input spectra • Work by G. W. McKinney et al. (2006) for neutron densities in the Apollo 17 drill core

  7. Code Work, Physics Inputs • Work by G. W. McKinney et al. (2006) for neutron densities in the Apollo 17 drill core

  8. Input GCR energy cutoffs • 1980 vertical cosmic ray cutoff rigidity data were used to then estimate the primary galactic cosmic ray (GCR) spectrum for various geomagnetic latitudes for our MCNPX calculations. [J. Masarik]

  9. Code Work, Terr. GCR Fluxes • Need good GCR spectra for all locations

  10. Code Work, Terr. GCR Fluxes • Gordon et al. (2004) and MCNPX Calc. [Kim]

  11. Code Work, Terr. GCR Fluxes • Gordon et al. (2004) and other calculations

  12. BASICS OF CALCULATIONS OF PRODUCTION RATES • Calculate fluxes (neutrons, protons) in specified target (geometry, composition) and incident cosmic rays. • Calculate production rate at depth d using target composition (i, e.g., SiO2), calculated spectra Φ for particles (k), and cross sections σ for target-element pair (i,j; e.g., O to Be-10, Si to Al-26): • Pj(d) = i Ni k∫σjik(Ek) Φk(Ek,d) dEk

  13. Update Cross Sections • Evaluate measured cross sections for proton-induced reactions • Adjust cross sections for neutron-induced reactions • Use any measured (n,x) cross sections • Adjust using good CN measurements in extraterrestrial and terrestrial samples and artificial targets (natural & accelerators)

  14. CROSS SECTIONS FOR PRODUCTION OF 10Be & 26Al ON TARGET ELEMENTS BY PROTONS

  15. NEUTRON-INDUCEDCROSS SECTIONS • Neutrons dominate (~90-95%) TCN production. • Early work, still used (~20 yrs. ago!): • Use a few measured neutron cross sections (Ne). • Use proton cross sections (Al-26), • Adjust neutron cross sections to fit ET measurements (Be-10, C-14).

  16. Test Calculations • For now, use existing extraterrestrial and some terrestrial measurements • Use new CRONUS results • Refine codes, their inputs (physics packages, input spectra), and reaction cross sections

  17. Preliminary rates for TCNs • from quartz using LCS and [MCNPX]: • Be-10: 5.7, [5.0] • C-14: 18.7, [22.2] • Al-26: 34.3, [36.4] • Close to old rates from Masarik & Reedy [1995]: 5.97, 18.6, and 36.1

  18. Work this year • Papers presented at AMS-10 on TCNs • by Kim, Reedy, & Masarik • Papers submitted to Proc. AMS-10 • Tests using neutron fluxes and Be-10 measured for many locations in southern hemisphere by I. Graham [Kim et al.] • Calculations for the air/ground interface and effects of snow cover [Masarik et al.] (see next 2 images)

  19. Fast and thermal neutron fluxes

  20. Changes due to water (snow)

  21. Future Work • More tests with GEANT (will probably drop LCS as is incorporated in MCNPX and will not be supported. GEANT is entirely different code from LCS/MCNPX. • Fine tune codes and their inputs • Cross section work • Comparisons to improve calculations • Extraterrestrial and other existing data • Terrestrial, especially using CRONUS data

More Related