I have tried the Python 3 version of Flair. Flair builds OK but the
geoviewer make fails as:
geometryobject.cc:40:10: fatal error: Python.h: No such file or directory
40 | #include <Python.h>
A portion of the compile instruction shows:
-I/usr/include/tcl8.6 -I-I/usr/include/python2.7
-I/usr/include/x86_64-linux-gnu/python2.7
The equivalent line for python2 (which works for me) is
-I/usr/include/tcl8.6 -I/usr/include/python2.7
Note the double "-I" switch before the reference to python2.7.
Is this a mistake? I don't know my way around the make file well enough to
fix it.
Thanks,
Carl
On Sun, Jun 5, 2022 at 11:16 AM <alfredo.ferrari_at_mi.infn.it> wrote:
> ear FLUKA users
>
> Fluka-2021.2.6, a respin of Fluka-2021.2, is now available on the
> Fluka web site (www.fluka.org).
>
> An experimental port of flair-2.3 to python3 is also available, together
> with the already available python2 version. The python3 compatible files
> are called flair...2.3-0bpy3..., see www.fluka.org/flair/download.html,
> let us know if there are (likely) problems.
>
> The Fluka respin addresses a few issues, among them:
>
> - an issue with scoring K0/K0bar/Kshort/Klong: the USRYIELD estimator
> when used on a boundary crossing was assuming a 50%-50% split into Kshort
> and Klong which is correct at production (the other use of USRYIELD)
> but not at boundary crossing. Now the proper mix between Kshort and
> Klong is used. For the other estimators, USRBDX, USRTRACK, USRBIN,
> the Kshort, Klong, K0, and K0bar had to be scored separately (they kept
> for scoring their production identity), thus, for example, in order to
> esitmate Kshort one had to add the proper fraction of K0/K0bar,
> accessing the internal variables giving the Kshort fraction.
> Now life has been made easier for these estimators as well, doing the
> proper summing internally (thanks to Anna Ferrari for pointing out this);
>
> - a rare issue in (anti)hyperon quasielastic scattering (an array
> out of bound could have occurred);
>
> - an issue with electron-nuclear reactions on heavy nuclei;
>
> - an incorrect exprapolation for the hadron-nucleus elastic cross sections
> at
> extremely high energies;
>
> - a very rare crash in Dpmjet-3;
>
> - a typo in the pre-computed compounds;
>
> - a general strengthening of many routines with respect to rounding issues
> when run at very high energies;
>
> - a general cleanup and rationalization of several routines/commons;
>
> - the AUXSCORE description on the manual was out-of-sync with the current
> status of the option.
>
>
> All users are urged to update to the latest respin.
>
> The FLUKA developers
>
> The external data files did not change, see below.
>
> The following Fluka files are available, *PLEASE NOTE
> fluka2021.2-data.tar.gz
> DID NOT CHANGE, HENCE YOU DO NOT NEED TO DOWNLOAD IT AGAIN*
>
> Rpm's:
>
> fluka-2021.2-6.x86_64.rpm (Linux, gfortran-11.3, 64
> bit)
> fluka-2021.2-6.i686.rpm (Linux, g77, 32 and 64 bit)
>
> Tar files:
>
> fluka2021.2-data.tar.gz (Data, required by all other
> tar files, UNCHANGED wrt
> fluka2021.2.4/5)
> fluka2021.2-linux-gfor64bitAA.tar.gz (Linux, gfortran-11.3, 64
> bit)
> fluka2021.2-linux-gfor64bit-10.3-AA.tar.gz (Linux, gfortran-10.3, 64
> bit)
> fluka2021.2-linux-gfor64bit-9.4-AA.tar.gz (Linux, gfortran-9.4, 64
> bit)
> fluka2021.2-linux-gfor64bit-8.5-AA.tar.gz (Linux, gfortran-8.5, 64
> bit)
> fluka2021.2-linuxAA.tar.gz (Linux, g77, 32 and 64
> bit)
> fluka2021.2-mac-gfor64bit-10.3-AA.tar.gz (Mac , gfortran-10.2, 64
> bit)
> fluka2021.2-mac-gfor64bit-9.4-AA.tar.gz (Mac , gfortran-9.4, 64
> bit)
> fluka2021.2-mac-gfor64bit-8.5-AA.tar.gz (Mac , gfortran-8.5, 64
> bit)
> fluka2021.2-linux-gfor64bit-9.4-glibc2.17-AA.tar.gz
> (Linux, gfortran-9.4,
> glibc-2.17, 64 bit)
>
> The gfortran-8 version for MAC is no longer provided, since we suppose
> everybody has moved at least to gfortran-9. If this is a problem please let
> us know and we'll try to provide a gfortran-8 version for Mac as well
>
>
>
> __________________________________________________________________________
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>
>
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Received on Mon Jun 06 2022 - 22:09:25 CEST