Date: Mon, 16 Sep 2013 20:59:49 +0800 (CST)
-----Original E-mail-----
From: yyc2011_at_mail.ustc.edu.cn
Sent Time: 2013-9-12 21:54:41
To: "Anton Lechner" <Anton.Lechner_at_cern.ch>
Cc:
Subject: Re: RE: RE:
Dear Fluka experts,
Please forgive me my bother.I have some problems to consult you.The attachments include two part files.The files which end with _109 consider energy transport cutoff and single scattering.The files which end with _112 don't consider energy transport cutoff and single scattering.The followings are my problems.
1."EMFCUT -0.000001 0.000001 target0 target5"
I think in the input file we only involve the electron transport,not photon.So,there is no need to set the photon transport energy cutoff in the EMFCUT card,right?
2." MULSOPT 1.0 1. 1. 3.GLOBEMF"
According to the Fluka manual,When electrons reach the boundaries,if the electron energy is too small to apply Moliere theory or the step is too short,we can activate the MULSOPT card to set single scattering of the electrons.In the MULSOPT card,I set the number of the electrons single scattering 3.Is my understanding right? On the other hand,Is it necessary to use the MULSOPT card for my problem?
3." USRBDX 101. ELECTRON -31. target5 VOID ebdxf
USRBDX 0.0002 0.000001 300. &"
The primary electron energy is 160KeV,but in the USRBDX card I set the maximum electron energy 200KeV,which exceeds the primary electron energy.Is it reasonable?
4.When use the usxsuw.f code to process the usrbdx file,I can get xx,xx_sum.lis,xx_tab.lis.But how can I get the electron fluence graph in the attachment?Could you tell me in detail?
5.Comparing the one-dimensional and two-dimensional electron distribution diagrams which end with _109 and _112 ,we can find they are so different.But,I don't know which is more reasonable for my problem? What is your opinion?
Thanks for your time.Thanks for any suggestions.
Yours,
Chenyuan
> -----Original E-mail-----
> From: "Anton Lechner" <Anton.Lechner_at_cern.ch>
> Sent Time: 2013-9-6 20:29:38
> To: "yyc2011_at_mail.ustc.edu.cn" <yyc2011_at_mail.ustc.edu.cn>, "fluka-discuss_at_fluka.org" <fluka-discuss_at_fluka.org>
> Cc:
> Subject: RE: RE:
>
> Dear Chenyuan,
>
> I actually used your input file (but, for simplicity, with a 160 keV electron pencil beam instead of a square electron field). Apart from this, I included the physics settings we already discussed:
> EMFCUT -1.0E-06 1.0E-06 target0 target10
> MULSOPT 1.0 1. 1. 3.GLOBEMF
>
> You can then score the fluence spectrum (from region "target10" to "VOID") with USRBDX as follows:
> USRBDX 99.0 ELECTRON -31. target10 VOID ebdxf
> USRBDX 2E-4 1E-6 300. &
>
> Please send replies always to the mailing list.
>
> Cheers, Anton
>
>
>
>
> ________________________________________
> From: yyc2011_at_mail.ustc.edu.cn [yyc2011_at_mail.ustc.edu.cn]
> Sent: 06 September 2013 11:14
> To: Anton Lechner
> Subject: Re: RE:
>
> Dear Anton,
>
> First,thanks for your reply.
> Second,I have a few problems to ask you.The first problem is how can I get the fluence spectrum of electrons exiting the backside of your Be layer.Could you tell me the detailed step to get the fluence spectrum of electrons?The second problem is I want to see your input file about the problem.If you can,Could you send it to me?
>
> Yours,
> Chenyuan
>
>
> > -----Original E-mail-----
> > From: "Anton Lechner" <Anton.Lechner_at_cern.ch>
> > Sent Time: 2013-9-6 15:19:46
> > To: "yyc2011_at_mail.ustc.edu.cn" <yyc2011_at_mail.ustc.edu.cn>, "fluka-discuss_at_fluka.org" <fluka-discuss_at_fluka.org>
> > Cc:
> > Subject: RE:
> >
> > Dear Chenyuan,
> >
> > There was once more no attachment to your Email.
> >
> > Just because your previous input file was running doesn't mean that you have a meaningful result if you don't spend some time thinking about physics model parameters and their impact. You are dealing with electrons of rather lower energies close to the default transport threshold of PRECISIO. For illustration, I attach a plot showing the fluence spectrum of electrons exiting the backside of your Be layer: one curve corresponds to a simulation with a cut of 1 keV (set via EMFCUT) and the other one to a run with the default cut of PRECISIO (100 keV). As you can see, there are striking differences.
> > [just as a remark: even with a cut of 100 keV, one gets some electrons with lower energy in the spectrum; the reason for this is that the energy of some electrons falls below 100 keV only in their last step to the boundary, hence they still appear in the energy spectrum which is scored at the boundary].
> >
> > In summary, I would strongly consider using these cards.
> >
> > Cheers, Anton
> >
> >
> >
> >
> > ________________________________________
> > From: yyc2011_at_mail.ustc.edu.cn [yyc2011_at_mail.ustc.edu.cn]
> > Sent: 02 September 2013 15:01
> > To: fluka-discuss_at_fluka.org
> > Subject:
> >
> > <17652047.3034261377919188455.JavaMail.coremail_at_mailweb>,<30507624.3107761378035584867.JavaMail.coremail_at_mailweb>,<30844077.3141761378087717403.JavaMail.coremail_at_mailweb>
> > Subject: Re: RE: RE: RE: The maximum number of binnings in USRBIN
> > MIME-Version: 1.0
> > Content-Type: multipart/mixed;
> > boundary="----=_Part_768470_18561564.1378126862176"
> > Sender: owner-fluka-discuss_at_mi.infn.it
> >
> > ------=_Part_768470_18561564.1378126862176
> > Content-Type: text/plain; charset=iso-2022-jp
> > Content-Transfer-Encoding: quoted-printable
> >
> > Dear Anton,
> >
> > Thanks for your suggestions.
> >
> > After I disscuss my probelm with you ,I feel very confused.Because before t=
> > his problem,I do some simulations which I think are similar to the input fi=
> > le I sent to you last time.
> >
> > The attachments consist of the input file,the two-dimension graph of elctro=
> > n distribution on the detector plane,and the one-dimension graph of electro=
> > n distribution.In this input file,I don't consider transport cut-off and si=
> > ngle scattering.But the input file runs well.Meanwhile,I think the result i=
> > s what I want. When there are some roughness on the target surface,Is proto=
> > n radiography or electron radiography or X-ray radiography able to diagnose=
> > the tiny roughness on the target surface? This is the problem I want to so=
> > lve.So,Is it really necessary to use EMFCUT card and MULSOPT card? These tw=
> > o cards make the problems become complex.
> > =20
> > Thanks for your time.Thanks for any suggestions.
> >
> > Yours,
> > Chenyuan
> >
> >
> >
> > > -----Original E-mail-----
> > > From: "Anton Lechner" <Anton.Lechner_at_cern.ch>
> > > Sent Time: 2013-9-2 16:13:46
> > > To: "yyc2011_at_mail.ustc.edu.cn" <yyc2011_at_mail.ustc.edu.cn>, "fluka-discuss=
> > _at_fluka.org" <fluka-discuss_at_fluka.org>
> > > Cc:=20
> > > Subject: RE: RE: RE: The maximum number of binnings in USRBIN
> > >=20
> > > Dear Chenyuan,
> > >=20
> > > (1) Indeed you can have many USRBIN scorings in the same simulation, for =
> > different quantities and/or different spatial binnings.
> > >=20
> > > (2) Good.
> > >=20
> > > (3,4) For the scoring, it think you should really ask yourself what you w=
> > ant to get out of the simulation. I know now your physical problem, but I d=
> > on't know what you want to calculate (still, consider my comments below for=
> > the y binning). Concerning the cuts I would say that you should maybe cons=
> > ider adapting them e.g. according to measurement conditions (if this is the=
> > aim of your study). Detection of low-energy electrons can for example be l=
> > imited by the entrance window of a detector (or by a voltage bias applied) =
> > and hence, if you want to reproduce real conditions, I would maybe consider=
> > such detection limits.
> > >=20
> > > (5,6) Your input file crashes. I advice you to at least test it first bef=
> > ore sending it to the mailing list. The problem is with the EMFCUT card: yo=
> > u expressed the electron cut in terms of the total electron energy (WHAT(1)=
> > >0), however I suppose you aimed for the kinetic energy, hence WHAT(1) shou=
> > ld be <0. Secondly, you misplaced the lower and upper region boundary (the =
> > should be on WHAT(4) and (5) and not on (5) and (6)). Finally, I would also=
> > lower the cut for protons. In summary, if you want to apply a cut of 1 keV=
> > , your card should look as follows:
> > > EMFCUT -1.0E-06 1.0E-06 target0 target10
> > >=20
> > > On the other hand, the definition of your MULSOPT seems fine (now you app=
> > ly single scattering close to boundaries, for too short steps and for energ=
> > ies where Moliere theory is not applicable). As you have a very thin layer =
> > only, you might even want to consider applying single scattering in the ent=
> > ire layer (see Example 3 in the MULSOPT entry of the manual) if your CPU ti=
> > mes are still acceptable (you can test that).
> > >=20
> > > Cheers, Anton=20
> > >=20
> > >=20
> > > ________________________________________
> > > From: owner-fluka-discuss_at_mi.infn.it [owner-fluka-discuss_at_mi.infn.it] on =
> > behalf of yyc2011_at_mail.ustc.edu.cn [yyc2011_at_mail.ustc.edu.cn]
> > > Sent: 02 September 2013 04:08
> > > To: fluka-discuss_at_fluka.org
> > > Subject: Re: RE: RE: The maximum number of binnings in USRBIN
> > >=20
> > > Dear Anton,
> > >=20
> > > Thanks for your time.Thanks for your reply.The attachment is my new input=
> > file.
> > >=20
> > > According to your reply,the followings are my questions.
> > >=20
> > > =1B$B!J=1B(B1=1B$B!K=1B(BJudging from your reply=1B$B!$=1B(Bin one input =
> > file,We can have many USRBIN scorings at the same time.In other words,We ca=
> > n get different physical quantities just from one input file.Right?
> > >=20
> > > =1B$B!J=1B(B2=1B$B!K=1B(BI understand what you said.
> > >=20
> > > =1B$B!J=1B(B3=1B$B!K=1B(BI want to get the electrons distribution on the =
> > detector plane.I want to study electron radiography,just like proton radiog=
> > raphy.For each electron energy=1B$B!J=1B(Bthe material is certain=1B$B!K=
> > =1B(B,there is a corresponding range in this material.If the range is too n=
> > ear the total target thickness,the electron beam will become sensitive to =
> > the target thickness.In this case, the electron beam can be used to diagnos=
> > e minute variations about the target thickness.This is what I want to do.
> > >=20
> > > =1B$B!J=1B(B4=1B$B!K!J=1B(B5=1B$B!K!J=1B(B6=1B$B!K=1B(BCould you see my n=
> > ew input file?Could you give me any advice?Perhaps EMFCUT and MULSOPT card =
> > are the key to the problem.I'm very rusty to the two cards.So,I wish you c=
> > ould give me more suggestions and some examples.
> > >=20
> > > Yours,
> > > Chenyuan
> > >=20
> > >=20
> > >=20
> > >=20
> > >=20
> > >=20
> > >=20
> > >=20
> > >=20
> > > > -----Original E-mail-----
> > > > From: "Anton Lechner" <Anton.Lechner_at_cern.ch>
> > > > Sent Time: 2013-9-2 0:29:48
> > > > To: "yyc2011_at_mail.ustc.edu.cn" <yyc2011_at_mail.ustc.edu.cn>, "fluka-discu=
> > ss_at_fluka.org" <fluka-discuss_at_fluka.org>
> > > > Cc:
> > > > Subject: RE: RE: The maximum number of binnings in USRBIN
> > > >
> > > > Dear Chenyuan,
> > > >
> > > > For clarity, I inserted different numbers in your Email below to refer =
> > to your specific questions. Here are my answers:
> > > >
> > > > (1) When saying "number of USRBINs", I mean the number of USRBIN scori=
> > ngs you have in your input file (always counting the USRBIN card and its co=
> > rresponding continuation card as *one* USRBIN) and *independently* which qu=
> > antity you are scoring (energy deposition, fluence, etc.). For example, if =
> > you have following cards in your input file, it means you have two USRBIN s=
> > corings:
> > > > USRBIN 10. ELECTRON -30. 0.4 0.4 0.0221f=
> > luElec
> > > > USRBIN -0.4 -0.4 0.022 40.0 40.0 1.&
> > > > USRBIN 10. POSITRON -30. 0.4 0.4 0.0221f=
> > luPos
> > > > USRBIN -0.4 -0.4 0.022 40.0 40.0 1.&
> > > >
> > > > (2) Let me illustrate this by means of the example given above: each US=
> > RBIN has 40*40*1=3D1600 bins, but since you have two USRBINs your total num=
> > ber of bins is 2*1600=3D3200. This means you need a memory allocation for 3=
> > 200 bins. Of course, if you have further USRBINs, you need to determine the=
> > number of bins for each and add them up in the same way.
> > > >
> > > > (3) This really depends what you actually want to calculate, i.e. what =
> > you intend to learn from the simulation. Just a hint: consider that if your=
> > geometry has a granularity of 6 mm in y and at the same time you have a re=
> > ctangular homogeneous electron field of the same size (covering all 6 mm), =
> > then a 200 um bin size in y will not give you new information for most of t=
> > he (central) bins, but only around the region boundaries. You may want to =
> > consider to use a more fine-grained binning only around boundaries. But I r=
> > epeat myself, I really don't know what you actually want to get out of the =
> > simulation.
> > > >
> > > > (4) I admit that I might have expressed myself not clear enough. It is =
> > not necessarily the difference between incident electron energy and transpo=
> > rt cut-off/production cut which matters, but it is the artificial cut on e=
> > lectrons (in your case mostly on the secondary electrons) which you introdu=
> > ce by having these cuts. As you have a fluence scoring, it will of course c=
> > hange your result if you have lower cuts (since each electron is counted eq=
> > ually independent of its energy). Which cut you should choose once more dep=
> > ends on your physical problem.
> > > >
> > > > (5-6) You did not attach any input file (in this context, please note t=
> > hat the manual is always a very valuable source of information)
> > > >
> > > > Cheers, Anton
> > > >
> > > >
> > > > ________________________________________
> > > > From: owner-fluka-discuss_at_mi.infn.it [owner-fluka-discuss_at_mi.infn.it] o=
> > n behalf of yyc2011_at_mail.ustc.edu.cn [yyc2011_at_mail.ustc.edu.cn]
> > > > Sent: 01 September 2013 13:39
> > > > To: fluka-discuss_at_fluka.org
> > > > Subject: Re: RE: The maximum number of binnings in USRBIN
> > > >
> > > > Dear Anton,
> > > >
> > > > Thanks for your reply in detail.I'm very grateful to you.
> > > >
> > > > I read your mail carefully and I think about your suggestions all the d=
> > ay.But I still have some questions.
> > > >
> > > > First, you say "maximum number of binnings" refers to the number of USR=
> > BINs I can have.What is the meaning?It means we can have many
> > > > usrbins,one of usrbin about energy deposition,one of usrbin about fluen=
> > ce,one of usrbin about neutron balance,and so on.I understand
> > > > it,Right?
> > > > (1)
> > > >
> > > > Second,you say "It is not important how many bins you have per USRBIN, =
> > but how many you have in total for all USRBINs".I don't
> > > > understand what you say.Could you give me a example or a detailed expla=
> > in?
> > > > (2)
> > > >
> > > > Third,you say "your smallest geometric structure is 20 um in x and 6 mm=
> > in y, while you aim for a bin size of less than 1 um in both
> > > > x and y".At this point,I make some changes in my input file.In the new =
> > input file,the smallest geometric structure is still 20 um in
> > > > x and 6 mm in y,but my aim for a bin size of 4 um in x and 200 um in y.=
> > Do you think I was right in doing this?
> > > > (3)
> > > >
> > > > Fourth, my primary electrons energy is 160 KeV.The transport cut-off en=
> > ergy is 100KeV for electrons.You ask me to consider if this
> > > > difference between primary energy and cut is sufficient for my problem.=
> > At this point,I want to know how can I estimate if this
> > > > difference between primary energy and cut is sufficient for my problem"=
> > .
> > > > (4)
> > > >
> > > > Meanwhile,I add the EMFCUT card in my new input file.Please
> > > > see my new input file.And,I will very happy if you give me some suggest=
> > ions.
> > > > (5)
> > > >
> > > > Fifth,you say "if I have such low primary electron energies and um geom=
> > etries, I should consider applying single scattering."In my
> > > > new input file,I add the MULSOPT card.This is the first time I use this=
> > card.Could you see my input file?Is it wrong?Maybe You can
> > > > give me some examples.
> > > > (6)
> > > >
> > > > Thanks for your time.Thanks for any suggestions.
> > > >
> > > > Yours,
> > > > Chenyuan
> > > >
> > > >
> > > >
> > > >
> > > >
> > > >
> > > >
> > > >
> > > > > -----Original E-mail-----
> > > > > From: "Anton Lechner" <Anton.Lechner_at_cern.ch>
> > > > > Sent Time: 2013-8-31 19:30:33
> > > > > To: "yyc2011_at_mail.ustc.edu.cn" <yyc2011_at_mail.ustc.edu.cn>, "fluka-dis=
> > cuss_at_fluka.org" <fluka-discuss_at_fluka.org>
> > > > > Cc:
> > > > > Subject: RE: The maximum number of binnings in USRBIN
> > > > >
> > > > > Dear Chenyuan,
> > > > >
> > > > > You misunderstood the comment in the manual: "maximum number of binni=
> > ngs" refers to the number of USRBINs you can have and not to the number of =
> > bins (see Manual: "A 'binning' is a regular spatial mesh"). The number of b=
> > ins you can have is limited by the memory available for scorings:
> > > > > *) See following answer on the FLUKA discuss list: http://www.fluka.o=
> > rg/web_archive/earchive/new-fluka-discuss/5260.html: the memory allocation =
> > is hard-wired in the library and is 360 MB
> > > > > *) It is not important how many bins you have per USRBIN, but how man=
> > y you have in total for all USRBINs
> > > > > *) Your mesh of 10000*10000*1 occupies 800 MB and is hence far beyond=
> > the limit of allocated memory
> > > > >
> > > > > Apart from this, I have some further comments:
> > > > > *) Even if such a large number of bins would be possible, you should =
> > ask yourself if it would make sense. First, your smallest geometric structu=
> > re is 20 um in x and 6 mm in y, while you aim for a bin size of less than =
> > 1 um in both x and y. Secondly, such a large number of bins would probably =
> > be challenging in terms of statistical error.
> > > > > *) Your primary electrons have an energy of 160 keV, but the transpor=
> > t cut-off and production threshold set by PRECISIO is 100 keV. You should a=
> > sk yourself if this difference between primary energy and cut is sufficien=
> > t for your problem. You can set lower cut values with the EMFCUT card.
> > > > > *) Note that if you have such low primary electron energies and um ge=
> > ometries, you should consider applying single scattering. I also quote the =
> > FLUKA manual: "The minimum recommended energy for PRIMARY electrons is abou=
> > t 50 to 100 keV for low-Z materials and 100-200 keV for heavy materials, un=
> > less the single scattering algorithm is used. Single scattering transport a=
> > llows to overcome most of the limitations at low energy for the heaviest ma=
> > terials at the price of some increase in CPU time."
> > > > >
> > > > > Cheers, Anton
> > > > >
> > > > >
> > > > >
> > > > > ________________________________________
> > > > > From: owner-fluka-discuss_at_mi.infn.it [owner-fluka-discuss_at_mi.infn.it]=
> > on behalf of yyc2011_at_mail.ustc.edu.cn [yyc2011_at_mail.ustc.edu.cn]
> > > > > Sent: 31 August 2013 05:19
> > > > > To: fluka-discuss_at_fluka.org
> > > > > Subject: The maximum number of binnings in USRBIN
> > > > >
> > > > > Dear Fluka experts,
> > > > >
> > > > > I have a question about the maximum number of binnings that I can def=
> > ine in USRBIN.It seems to go wrong when I set the number of
> > > > > binnings=3D10000 or 8000 in my input file.But when I set the number o=
> > f binnings=3D1000,it runs normal. Meanwhile,I note in the Fluka
> > > > > manual"The maximum number of binnings that the user can define is 400=
> > . This value can be changed by modifying the parameter MXUSBN
> > > > > in member USRBIN of the flukapro library or directory and then re-com=
> > piling and linking Fluka." In the manual,It says the maximum
> > > > > number of binnings that the user can define is 400.But when I set the=
> > number of binnings=3D1000,I do not modify the parameter
> > > > > MXUSBN.But the fluka runs normal.The attachments are my input file an=
> > d .out file.Could you help me?
> > > > >
> > > > > Thanks for any suggestions.
> > > > >
> > > > > Yours
> > > > > Chenyuan
> > > > >
> > > >
> > > >
> >
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- application/octet-stream attachment: bjuc_109.inp
(image/jpeg attachment: One_dimensional_electron___distribution_diagram_109.jpg)
(image/jpeg attachment: Two-dimensional_electron___distribution_diagram_109.jpg)
- application/octet-stream attachment: bjuc_112.inp
(image/jpeg attachment: One_dimensional_electron___distribution_diagram_112.jpg)
(image/jpeg attachment: Two-dimensional_electron___distribution_diagram_112.jpg)
- application/pdf attachment: elecfluence.pdf