Users wishing to develop and integrate new detector models into the STAR framework will be intersted in the following links:
Tracking Interface (Stv)
Exporting detector hits
Implementing a custom seed finder
ID Truth
ID truth is an ID which enables us to determine which simulated particle was principally responsible for the creation of a hit in a detector, and eventually the physics objects (clusters, points, tracks) which are formed from them. The StHit class has a member function which takes two arguements:
Interface to Starsim
The interface between starsim and reconstruction is briefly outlined here
Information about geometries used in production and which geometries to use in simulations may be found in the following links:
Comparisons between the original AgSTAR model and the new AgML model of the detector may be found here:
AgML Project Overview and Readiness for 2012
HOWTO Use Geometries defined in AgML in STARSIM
AgML geometries are available for use in simulation using the "eval" libraries.
$ starver eval
The geometries themselves are available in a special library, which is setup for backwards compatability with starsim. To use the geometries you load the "xgeometry.so" library in a starsim session, either interactively or in a macro:
starsim> detp geom y2012
starsim> gexe $STAR_LIB/xgeometry.so
starsim> gclos all
HOWTO Use Geometries defined in AgML in the Big Full Chain
AgML geometries may also be used in reconstruction. To access them, the "agml" flag should be provided in the chain being run:
e.g
root [0] .L bfc.C
root [1] bfc(nevents,"y2012 agml ...", inputFile);
Geometry in Preparation: y2012Major changes: 1. Support cone, ftpc, ssd, pmd removed.
2. Inner Detector Support Module (IDSM) added
3. Forward GEM Tracker (FGTD) added
Use of AgML geometries within starsim:
$ starver eval
$ starsim
starsim> detp geom y2012
starsim> gexe $STAR_LIB/xgeometry.so
starsim> gclos all
Use of AgML geometries within the big full chain:
$ root4star
root [0] .L bfc.C
root [1] bfc(0,"y2012 agml ...",inputFile);
|
Current (10/24/2011) configuration of the IDSM with FGT inside -- |
Getting started developing geometries for the STAR experiment with AgML.
Setting up your local environment
You need to checkout several directories and complie in this order:
$ cvs co StarVMC/Geometry $ cvs co StarVMC/StarGeometry $ cvs co StarVMC/xgeometry$ cvs co pams/geometry$ cons +StarVMC/Geometry $ cons
This will take a while to compile, during which time you can get a cup of coffee, or do your laundry, etc...
If you only want to visualize the STAR detector, you can checkout:
$ cvs co StarVMC/Geometry/macros
Once this is done you can visualize STAR geometries using the viewStarGeometry.C macro in AgML 1, and the loadAgML.C macro in AgML 2.0.
$ root.exeroot [0] .L StarVMC/Geometry/macros/viewStarGeometry.C root [1] nocache=true root [2] viewall=true root [3] viewStarGeometry("y2012")root [0] .L StarVMC/Geometry/macros/loadAgML.C root [1] loadAgML("y2016") root [2] TGeoVolume *cave = gGeoManager->FindVolumeFast("CAVE"); root [3] cave -> Draw("ogl"); // ogl uses open GL viewer
Tutorial #1 -- Creating and Placing Volumes
Start by firing up your favorite text editor... preferably something which does syntax highlighting and checking on XML documents. Edit the first tutorial geometries located in StarVMC/Geometry/TutrGeo ...
$ emacs StarVMC/Geometry/TutrGeo/TutrGeo1.xml
This module illustrates how to create a new detector module, how to create and place a simple volume, and how to create and place multiple copies of that volume. Next, we need to attach this module to a geometry model in order to visualize it. Geometry models (or "tags") are defined in the StarGeo.xml file.
$ emacs StarVMC/Geometry/StarGeo.xml
There is a simple geometry, which only defines the CAVE. It's the first geometry tag called "black hole". You can add your detector here...
xxx
$ root.exe
root [0] .L StarVMC/Geometry/macros/viewStarGeometry.C root [1] nocache=true root [2] viewStarGeometry("test","TutrGeo1");
The "test" geometry tag is a very simple geometry, implementing only the wide angle hall and the cave. All detectors, beam pipes, magnets, etc... have been removed. The second arguement to viewStarGeometry specifies which geometry module(s) are to be built and added to the test geometry. In this case we add only TutrGeo1. (A comma-separated list of geometry modules could be provided, if more than one geometry module was to be built).
Now you can try modifying TutrGeo1. Feel free to add as many boxes in as many positions as you would like. Once you have done this, recompile in two steps
$ cons +StarVMC/Geometry $ cons
Tutorial #2 -- A few simple shapes, rotations and reflections
The second tutorial geometry is in StarVMC/Geometry/TutrGeo/TutrGeo2.xml. Again, view it using viewStarGeometry.C
$ root.exe root [0] .L viewStarGeometry.C root [1] nocache=true root [2] viewStarGeometry("test","TutrGeo2")
What does the nocache=true statement do? It instructs viewStarGeometry.C to recreate the geometry, rather than load it from a root file created the last time you ran the geometry. By default, if the macro finds a file name "test.root", it will load the geometry from that file to save time. You don't want this since you know that you've changed the geometry.
The second tutorial illustrates a couple more simple shapes: cones and tubes. It also illustrates how to create reflections. Play around with the code a bit, recompile in the normal manner, then try viewing the geometry again.
Tutorial #3 -- Variables and Structures
AgML provides variables and structures. The third tutorial is in StarVMC/Geometry/TutrGeo/TutrGeo3.xml. Open this up in a text editor and let's look at it. We define three variables: boxDX, boxDY and boxDZ to hold the dimensions of the box we want to create. AgML is case-insensitve, so you can write this as boxdx, BoxDY and BOXDZ if you so choose. In general, choose what looks best and helps you keep track of the code you're writing. Next check out the volume "ABOX". Note how the shape's dx, dy and dz arguements now reference the variables boxDX, boxDY and boxDZ. This allows us to create multiple versions of the volume ABOX. Let's view the geometry and see. $ root.exe root [0] .L StarVMC/Geometry/macros/viewStarGeometry.C root [1] nocache=true root [2] viewStarGeometry("test","TutrGeo3") Launch a new TBrowser and open the "test" geometry. Double click test --> Master Volume --> CAVE --> TUTR. You now see all of the concrete volumes which have been created by ROOT. It should look like what you see at the right. We have "ABOX", but we also have ABO1 and ABO2. This demonstrates the an important concept in AgML. Each <Volume ...> block actually defines a volume "factory". It allows you to create multiple versions of a volume, each differing by the shape of the volume. When the shape is changed, a new volume is created with a nickname, where the last letter in the volume name is replaced by [1 2 3 ... 0 a b c ... z] (then the second to last letter, then the third...). Structures provide an alternate means to define variables. In order to populate the members of a structure with values, you use the Fill statement. Multiple fill statements for a given structure may be defined, providing multiple sets of values. In order to select a given set of values, the <Use ...> operator is invoked. In TutrGeo3, we create and place 5 different tubes, using the data stored in the Fill statements. However, you might notice in the browser that there are only two concrete instances of the tube being created. What is going on here? This is another feature of AgML. When the shape is changed, AgML will look for another concrete volume with exactly the same shape. If it finds it, it will use that volume. If it doesn't, then a new volume is created. There's alot going on in this tutorial, so play around a bit with it. |
Tutorial #4 -- Some more shapes
Abstract: We compare the AgML and AgSTAR descriptions of recent revisions of the STAR Y2005 through Y2011 geometry models. We are specifically interested in the suitability of the AgML model for tracking. We therefore plot the material contained in the TPC vs pseudorapidity for (a) all detectors, (b) the time projection chamber, and (c) the sensitive volumes of the time projection chamber. We also plot (d) the material found in front of the TPC active volumes.
Decription of the PlotsBelow you will find four columns of plots, for the highest revision of each geometry from y2005 to the present. The columns from left-to-right show comparisons of the material budget for STAR and its daughter volumes, the material budgets for the TPC and it's immediate daughter volumes, the material budgets for the active volumes in the TPC, and the material in front of the active volume of the TPC. In the context of tracking, the right-most column is the most important. Each column contains three plots. The top plot shows the material budget in the AgML model. The middle plot, the material budget in the AgSTAR model. The bottom plot shows the difference divided by the AgSTAR model. The y-axis on the difference plot extends between -2.5% and +2.5%. --------------------------------
STAR Y2011 Geometry TagIssues with TpceGeo3a.xml
Issues with PhmdGeo.xml
|
|||
(a) Material in STAR Detector and daughters | (b) Material in TPC and daughters | (c) Material in TPC active volumes | (d) Material in front of TPC active volumes |
STAR Y2010c Geometry TagIssues with TpceGeo3a.xml
Issues with PhmdGeo.xml
|
|||
(a) Material in STAR Detector and daughters | (b) Material in TPC and daughters | (c) Material in TPC active volumes | (d) Material in front of TPC active volumes |
STAR Y2009c Geometry TagIssues with TpceGeo3a.xml
Issues with PhmdGeo.xml
|
|||
(a) Material in STAR Detector and daughters | (b) Material in TPC and daughters | (c) Material in TPC active volumes | (d) Material in front of TPC active volumes |
STAR Y2008e Geometry TagGlobal Issues
Issues with TpceGeo3a.xml
Issues with PhmdGeo.xml
|
|||
(a) Material in STAR Detector and daughters | (b) Material in TPC and daughters | (c) Material in TPC active volumes | (d) Material in front of TPC active volumes |
STAR Y2007h Geometry TagGlobal Issues
Issues with TpceGeo3a.xml
Issues with PhmdGeo.xml
Issues with SVT. |
|||
(a) Material in STAR Detector and daughters | (b) Material in TPC and daughters | (c) Material in TPC active volumes | (d) Material in front of TPC active volumes |
STAR Y2006g Geometry TagGlobal Issues
Note: TpceGeo2.xml does not suffer from the overlap issue in TpceGeo3a.xml |
|||
(a) Material in STAR Detector and daughters | (b) Material in TPC and daughters | (c) Material in TPC active volumes | (d) Material in front of TPC active volumes |
STAR Y2005i Geometry TagGlobal Issues
Issues with TpceGeo3a.xml
Issues with PhmdGeo.xml
|
|||
(a) Material in STAR Detector and daughters | (b) Material in TPC and daughters | (c) Material in TPC active volumes | (d) Material in front of TPC active volumes |
Attached is a comparison of track reconstruction using the Sti tracker, with AgI and AgML geometries as input.
List of default AgML materials and mixtures. To get a complete list of all materials defined in a geometry, execute AgMaterial::List() in ROOT, once the geometry has been created.
[-] Hydrogen: a= 1.01 z= 1 dens= 0.071 radl= 865 absl= 790 isvol= <unset> nelem= 1 [-] Deuterium: a= 2.01 z= 1 dens= 0.162 radl= 757 absl= 342 isvol= <unset> nelem= 1 [-] Helium: a= 4 z= 2 dens= 0.125 radl= 755 absl= 478 isvol= <unset> nelem= 1 [-] Lithium: a= 6.94 z= 3 dens= 0.534 radl= 155 absl= 121 isvol= <unset> nelem= 1 [-] Berillium: a= 9.01 z= 4 dens= 1.848 radl= 35.3 absl= 36.7 isvol= <unset> nelem= 1 [-] Carbon: a= 12.01 z= 6 dens= 2.265 radl= 18.8 absl= 49.9 isvol= <unset> nelem= 1 [-] Nitrogen: a= 14.01 z= 7 dens= 0.808 radl= 44.5 absl= 99.4 isvol= <unset> nelem= 1 [-] Neon: a= 20.18 z= 10 dens= 1.207 radl= 24 absl= 74.9 isvol= <unset> nelem= 1 [-] Aluminium: a= 26.98 z= 13 dens= 2.7 radl= 8.9 absl= 37.2 isvol= <unset> nelem= 1 [-] Iron: a= 55.85 z= 26 dens= 7.87 radl= 1.76 absl= 17.1 isvol= <unset> nelem= 1 [-] Copper: a= 63.54 z= 29 dens= 8.96 radl= 1.43 absl= 14.8 isvol= <unset> nelem= 1 [-] Tungsten: a= 183.85 z= 74 dens= 19.3 radl= 0.35 absl= 10.3 isvol= <unset> nelem= 1 [-] Lead: a= 207.19 z= 82 dens= 11.35 radl= 0.56 absl= 18.5 isvol= <unset> nelem= 1 [-] Uranium: a= 238.03 z= 92 dens= 18.95 radl= 0.32 absl= 12 isvol= <unset> nelem= 1 [-] Air: a= 14.61 z= 7.3 dens= 0.001205 radl= 30400 absl= 67500 isvol= <unset> nelem= 1 [-] Vacuum: a= 14.61 z= 7.3 dens= 1e-06 radl= 3.04e+07 absl= 6.75e+07 isvol= <unset> nelem= 1 [-] Silicon: a= 28.09 z= 14 dens= 2.33 radl= 9.36 absl= 45.5 isvol= <unset> nelem= 1 [-] Argon_gas: a= 39.95 z= 18 dens= 0.002 radl= 11800 absl= 70700 isvol= <unset> nelem= 1 [-] Nitrogen_gas: a= 14.01 z= 7 dens= 0.001 radl= 32600 absl= 75400 isvol= <unset> nelem= 1 [-] Oxygen_gas: a= 16 z= 8 dens= 0.001 radl= 23900 absl= 67500 isvol= <unset> nelem= 1 [-] Polystyren: a= 11.153 z= 5.615 dens= 1.032 radl= <unset> absl= <unset> isvol= <unset> nelem= 2 A Z W C 12.000 6.000 0.923 H 1.000 1.000 0.077 [-] Polyethylene: a= 10.427 z= 5.285 dens= 0.93 radl= <unset> absl= <unset> isvol= <unset> nelem= 2 A Z W C 12.000 6.000 0.857 H 1.000 1.000 0.143 [-] Mylar: a= 12.87 z= 6.456 dens= 1.39 radl= <unset> absl= <unset> isvol= <unset> nelem= 3 A Z W C 12.000 6.000 0.625 H 1.000 1.000 0.042 O 16.000 8.000 0.333
This page was merged with STAR Geometry in simulation & reconstruction and maintained by STAR's librarian.
Retired Simulation Pages kept here.
Immediate action items:
Documentation for the beampipe support geometry description development
After the completion of the 2007 run, the SVT and the SSD were removed from the STAR detector along with there utility lines. The support structure for the beampipe remained, however.
The following drawings describe the structure of the beampipe support as it exists in the late 2007 and probably throughout 2008
Here we present information about our datasets.
Description |
Dataset name
|
Statistics, thousands
|
Status
|
Moved to HPSS
|
Comment
|
---|---|---|---|---|---|
Herwig 6.507, Y2004Y |
rcf1259
|
225
|
Finished
|
Yes
|
7Gev<Pt<9Gev |
Herwig 6.507, Y2004Y |
rcf1258
|
248
|
Finished
|
Yes
|
5Gev<Pt<7Gev |
Herwig 6.507, Y2004Y |
rcf1257
|
367
|
Finished
|
Yes
|
4Gev<Pt<5Gev |
Herwig 6.507, Y2004Y |
rcf1256
|
424
|
Finished
|
Yes
|
3Gev<Pt<4Gev |
Herwig 6.507, Y2004Y |
rcf1255
|
407
|
Finished
|
Yes
|
2Gev<Pt<3Gev |
Herwig 6.507, Y2004Y |
rcf1254
|
225
|
Finished
|
Yes
|
35Gev<Pt<100Gev |
Herwig 6.507, Y2004Y |
rcf1253
|
263
|
Finished
|
Yes
|
25Gev<Pt<35Gev |
Herwig 6.507, Y2004Y |
rcf1252
|
263
|
Finished
|
Yes
|
15Gev<Pt<25Gev |
Herwig 6.507, Y2004Y |
rcf1251
|
225
|
Finished
|
Yes
|
11Gev<Pt<15Gev |
Herwig 6.507, Y2004Y |
rcf1250
|
300
|
Finished
|
Yes
|
9Gev<Pt<11Gev |
Hijing 1.382 AuAu 200 GeV minbias, 0< b < 20fm |
rcf1249
|
24
|
Finished
|
Yes
|
Tracking,new SVT geo, diamond: 60, +-30cm, Y2005D |
Herwig 6.507, Y2004Y |
rcf1248
|
15
|
Finished
|
Yes
|
35Gev<Pt<45Gev |
Herwig 6.507, Y2004Y |
rcf1247
|
25
|
Finished
|
Yes
|
25Gev<Pt<35Gev |
Herwig 6.507, Y2004Y |
rcf1246
|
50
|
Finished
|
Yes
|
15Gev<Pt<25Gev |
Herwig 6.507, Y2004Y |
rcf1245
|
100
|
Finished
|
Yes
|
11Gev<Pt<15Gev |
Herwig 6.507, Y2004Y |
rcf1244
|
200
|
Finished
|
Yes
|
9Gev<Pt<11Gev |
CuCu 62.4 Gev, Y2005C |
rcf1243
|
5
|
Finished
|
No
|
same as 1242+ keep Low Energy Tracks |
CuCu 62.4 Gev, Y2005C |
rcf1242
|
5
|
Finished
|
No
|
SVT tracking test, 10 keV e/m process cut (cf. rcf1237) |
10 J/Psi, Y2005X, SVT out
|
rcf1241
|
30
|
Finished
|
No
|
Study of the SVT material
effect
|
10 J/Psi, Y2005X, SVT in
|
rcf1240
|
30
|
Finished
|
No
|
Study of the SVT material
effect
|
100 pi0, Y2005X, SVT out
|
rcf1239
|
18
|
Finished
|
No
|
Study of the SVT material
effect
|
100 pi0, Y2005X, SVT in
|
rcf1238
|
20
|
Finished
|
No
|
Study of the SVT material
effect
|
CuCu 62.4 Gev, Y2005C |
rcf1237
|
5
|
Finished
|
No
|
SVT tracking test, pilot run |
Herwig 6.507, Y2004Y |
rcf1236
|
8
|
Finished
|
No
|
Test run for initial comparison with Pythia, 5Gev<Pt<7Gev |
Pythia, Y2004Y |
rcf1235
|
100
|
Finished
|
No
|
MSEL=2, min bias |
Pythia, Y2004Y |
rcf1234
|
90
|
Finished
|
No
|
MSEL=0,CKIN(3)=0,MSUB=91,92,93,94,95 |
Pythia, Y2004Y, sp.2 (CDF tune A) |
rcf1233
|
308
|
Finished
|
Yes
|
4<Pt<5, MSEL=1, GHEISHA |
Pythia, Y2004Y, sp.2 (CDF tune A) |
rcf1232
|
400
|
Finished
|
Yes
|
3<Pt<4, MSEL=1, GHEISHA |
Pythia, Y2004Y, sp.2 (CDF tune A) |
rcf1231
|
504
|
Finished
|
Yes
|
2<Pt<3, MSEL=1, GHEISHA |
Pythia, Y2004Y, sp.2 (CDF tune A) |
rcf1230
|
104
|
Finished
|
Yes
|
35<Pt, MSEL=1, GHEISHA |
Pythia, Y2004Y, sp.2 (CDF tune A) |
rcf1229
|
208
|
Finished
|
Yes
|
25<Pt<35, MSEL=1, GHEISHA |
Pythia, Y2004Y, sp.2 (CDF tune A) |
rcf1228
|
216
|
Finished
|
Yes
|
15<Pt<25, MSEL=1, GHEISHA |
Pythia, Y2004Y, sp.2 (CDF tune A) |
rcf1227
|
216
|
Finished
|
Yes
|
11<Pt<15, MSEL=1, GHEISHA |
Pythia, Y2004Y, sp.2 (CDF tune A) |
rcf1226
|
216
|
Finished
|
Yes
|
9<Pt<11, MSEL=1, GHEISHA |
Pythia, Y2004Y, sp.2 (CDF tune A) |
rcf1225
|
216
|
Finished
|
Yes
|
7<Pt<9, MSEL=1, GHEISHA |
Pythia, Y2004Y, sp.2 (CDF tune A) |
rcf1224
|
216
|
Finished
|
Yes
|
5<Pt<7, MSEL=1, GHEISHA |
Pythia special tune2 Y2004Y, GCALOR |
rcf1223
|
100
|
Finished
|
Yes
|
4<Pt<5, GCALOR
|
Pythia special tune2 Y2004Y, GHEISHA |
rcf1222
|
100
|
Finished
|
Yes
|
4<Pt<5, GHEISHA
|
Pythia special run 3 Y2004C |
rcf1221
|
100
|
Finished
|
Yes
|
ENER 200.0, MSEL 2, MSTP (51)=7, MSTP (81)=1, MSTP (82)=1, PARP (82)=1.9, PARP (83)=0.5, PARP (84)=0.2, PARP (85)=0.33, PARP (86)=0.66, PARP (89)=1000, PARP (90)=0.16, PARP (91)=1.0, PARP (67)=1.0 |
Pythia special run 2 Y2004C (CDF tune A) |
rcf1220
|
100
|
Finished
|
Yes
|
ENER 200.0, MSEL 2, MSTP (51)=7, |
Pythia special run 1 Y2004C |
rcf1219
|
100
|
Finished
|
Yes
|
ENER 200.0, MSEL 2, MSTP (51)=7, MSTP (81)=1, MSTP (82)=1, PARP (82)=1.9, PARP (83)=0.5, PARP (84)=0.2, PARP (85)=0.33, PARP (86)=0.66, PARP (89)=1000, PARP (90)=0.16, PARP (91)=1.5, PARP (67)=1.0 |
Hijing 1.382 AuAu 200 GeV central 0< b < 3fm |
rcf1218
|
50
|
Finished
|
Yes
|
Statistics enhancement of rcf1209 with a smaller diamond: 60, +-30cm, Y2004a |
Hijing 1.382 CuCu 200 GeV minbias 0< b < 14 fm |
rcf1216
|
52
|
Finished
|
Yes
|
Geometry: Y2005x
|
Hijing 1.382 AuAu 200 GeV minbias 0< b < 20 fm |
rcf1215
|
100
|
Finished
|
Yes
|
Geometry: Y2004a, Special D decays |
Description | Dataset name | Statistics, thousands | Status | Moved to HPSS | Comment |
---|---|---|---|---|---|
AuAu 200 GeV central | rcf1289 | 1 | Finished | No | upgr06: Hijing, D0 and superposition |
AuAu 200 GeV central | rcf1288 | 0.8 | Finished | No | upgr11: Hijing, D0 and superposition |
AuAu 200 GeV min bias | rcf1287 | 5 | Finished | No | upgr11: Hijing, D0 and superposition |
AuAu 200 GeV central | rcf1286 | 1 | Finished | No | upgr10: Hijing, D0 and superposition |
AuAu 200 GeV min bias | rcf1285 | 6 | Finished | No | upgr10: Hijing, D0 and superposition |
AuAu 200 GeV central | rcf1284 | 1 | Finished | No | upgr09: Hijing, D0 and superposition |
AuAu 200 Gev min bias | rcf1283 | 6 | Finished | No | upgr09: Hijing, D0 and superposition |
AuAu 200 GeV min bias | rcf1282 | 38 | Finished | No | upgr06: Hijing, D0 and superposition |
AuAu 200 GeV min bias | rcf1281 | 38 | Finished | Yes | upgr08: Hijing, D0 and superposition |
AuAu 200 GeV min bias | rcf1280 | 38 | Finished | Yes | upgr01: Hijing, D0 and superposition |
AuAu 200 GeV min bias | rcf1279 | 38 | Finished | Yes | upgr07: Hijing, D0 and superposition |
Extension of 1276: D0 superposition | rcf1278 | 5 | Finished | No | upgr07: Z cut=+-300cm |
AuAu 200 GeV min bias | rcf1277 | 5 | Finished | No | upgr05: Z cut=+-300cm |
AuAu 200 GeV min bias | rcf1276 | 35 | Finished | No | upgr05: Hijing, D0 and superposition |
Pythia 200 GeV + HF | rcf1275 | 23*4 | Finished | No | J/Psi and Upsilon(1S,2S,3S) mix for embedding |
AuAu 200 GeV min bias | rcf1274 | 10 | Finished | No | upgr02 geo tag, |eta|<1.5 (tracking upgrade request) |
Pythia 200 GeV | rcf1273 | 600 | Finished | Yes | Pt <2 (Completing the rcf1224-1233 series) |
CuCu 200 GeV min bias+D0 mix | rcf1272 | 50+2*50*8 | Finished | Yes | Combinatorial boost of rcf1261, sigma: 60, +-30 |
Pythia 200 GeV | rcf1233 | 300 | Finished | Yes | 4< Pt <5 (rcf1233 extension) |
Pythia 200 GeV | pds1232 | 200 | Finished | Yes | 3< Pt <4 (rcf1232 clone) |
Pythia 200 GeV | pds1231 | 240 | Finished | Yes | 2< Pt <3 (rcf1231 clone) |
Pythia 200 GeV | rcf1229 | 200 | Finished | Yes | 25< Pt <35 (rcf1229 extension) |
Pythia 200 GeV | rcf1228 | 200 | Finished | Yes | 15< Pt <25 (rcf1228 extension) |
Pythia 200 GeV | rcf1227 | 208 | Finished | Yes | 11< Pt <15 (rcf1227 extension) |
Pythia 200 GeV | rcf1226 | 200 | Finished | Yes | 9< Pt <11 (rcf1226 extension) |
Pythia 200 GeV | rcf1225 | 200 | Finished | Yes | 7< Pt <9 (rcf1225 extension) |
Pythia 200 GeV | rcf1224 | 212 | Finished | Yes | 5< Pt <7 (rcf1224 extension) |
Pythia 200 GeV Y2004Y CDF_A | rcf1271 | 120 | Finished | Yes | 55< Pt <65 |
Pythia 200 GeV Y2004A CDF_A | rcf1270 | 120 | Finished | Yes | 45< Pt <55 |
CuCu 200 GeV min bias | rcf1266 | 10 | Finished | Yes | SVT study: clams and two ladders |
CuCu 200 GeV min bias | rcf1265 | 10 | Finished | Yes | SVT study: clams displaced |
CuCu 200 GeV min bias | rcf1264 | 10 | Finished | Yes | SVT study: rotation of the barrel |
CuCu 62.4 GeV min bias+D0 mix | rcf1262 | 50*3 | Finished | Yes | 3 subsets: Hijing, single D0, and the mix |
CuCu 200 GeV min bias+D0 mix | rcf1261 | 50*3 | Finished | No | 3 subsets: Hijing, single D0, and the mix |
1 J/Psi over 200GeV minbias AuAu | rcf1260 | 10 | Finished | No | J/Psi mixed with 200GeV AuAu Hijing Y2004Y 60/35 vertex |
Name
System/Energy
Statistics
Status
HPSS
Comment
Site
rcf1290
AuAu200 0<b<3fm, Zcut=5cm
32*5
Done
Yes
Hijing+D0+Lac2+D0_mix+Lac2_mix
rcas
rcf1291
pp200/UPGR07/Zcut=10cm
10
Done
Yes
ISUB = 11, 12, 13, 28, 53, 68
rcas
rcf1292
pp500/UPGR07/Zcut=10cm
10
Done
Yes
ISUB = 11, 12, 13, 28, 53, 68
rcas
rcf1293
pp200/UPGR07/Zcut=30cm
205
Done
Yes
ISUB = 11, 12, 13, 28, 53, 68
rcas
rcf1294
pp500/UPGR07/Zcut=30cm
10
Done
Yes
ISUB = 11, 12, 13, 28, 53, 68
rcas
rcf1295
AuAu200 0<b<20fm, Zcut=30cm
20
Done
Yes
QA run for the Y2007 tag
rcas
rcf1296
AuAu200 0<b<3fm, Zcut=10cm
100*5
Done
Yes
Hijing,B0,B+,B0_mix,B+_mix, Y2007
rcas
rcf1297
AuAu200 0<b<20fm, Zcut=300cm
40
Done
Yes
Pile-up simulation in the TUP studies, UPGR13
rcas
rcf1298
AuAu200 0<b<3fm, Zcut=15cm
100*5
Done
Part
Hijing,D0,Lac2,D0_mix,Lac2_mix, UPGR13
rcas
rcf1299
pp200/Y2005/Zcut=50cm
800
Done
Yes
Pythia, photon mix, pi0 mix
rcas
rcf1300
pp200/UPGR13/Zcut=15cm
100
Done
No
Pythia, MSEL=4 (charm)
rcas
rcf1301
pp200/UPGR13/Zcut=300cm
84
Done
No
Pythia, MSEL=1, wide vertex
rcas
rcf1302
pp200 Y2006C
120
Done
No
Pythia for Spin PWG, Pt(45,55)GeV
rcas
rcf1303
pp200 Y2006C
120
Done
No
Pythia for Spin PWG, Pt(35,45)GeV
rcas
rcf1304
pp200 Y2006C
120
Done
No
Pythia for Spin PWG, Pt(55,65)GeV
rcas
rcf1296
Upsilon S1,S2,S3 + Hijing
15*3
Done
No
Muon Telescope Detector, ext.of 1296
rcas
rcf1306
pp200 Y2006C
400
Done
Yes
Pythia for Spin PWG, Pt(25,35)GeV
rcas
rcf1307
pp200 Y2006C
400
Done
Yes
Pythia for Spin PWG, Pt(15,25)GeV
rcas
rcf1308
pp200 Y2006C
420
Done
Yes
Pythia for Spin PWG, Pt(11,15)GeV
rcas
rcf1309
pp200 Y2006C
420
Done
Yes
Pythia for Spin PWG, Pt(9,11)GeV
rcas
rcf1310
pp200 Y2006C
420
Done
Yes
Pythia for Spin PWG, Pt(7,9)GeV
rcas
rcf1311
pp200 Y2006C
400
Done
Yes
Pythia for Spin PWG, Pt(5,7)GeV
rcas
rcf1312
pp200 Y2004Y
544
Done
No
Di-jet CKIN(3,4,7,8,27,28)=7,9,0.0,1.0,-0.4,0.4
rcas
rcf1313
pp200 Y2004Y
760
Done
No
Di-jet CKIN(3,4,7,8,27,28)=9,11,-0.4,1.4,-0.5,0.6
rcas
rcf1314
pp200 Y2004Y
112
Done
No
Di-jet CKIN(3,4,7,8,27,28)=11,15,-0.2,1.2,-0.6,-0.3
Grid
rcf1315
pp200 Y2004Y
396
Done
No
Di-jet CKIN(3,4,7,8,27,28)=11,15,-0.5,1.5,-0.3,0.4
Grid
rcf1316
pp200 Y2004Y
132
Done
No
Di-jet CKIN(3,4,7,8,27,28)=11,15,0.0,1.0,0.4,0.7
Grid
rcf1317
pp200 Y2006C
600
Done
Yes
Pythia for Spin PWG, Pt(4,5)GeV
Grid
rcf1318
pp200 Y2006C
690
Done
Yes
Pythia for Spin PWG, Pt(3,4)GeV
Grid
rcf1319
pp200 Y2006C
690
Done
Yes
Pythia for Spin PWG, Minbias
Grid
rcf1320
pp62.4 Y2006C
400
Done
No
Pythia for Spin PWG, Pt(4,5)GeV
Grid
rcf1321
pp62.4 Y2006C
250
Done
No
Pythia for Spin PWG, Pt(3,4)GeV
Grid
rcf1322
pp62.4 Y2006C
220
Done
No
Pythia for Spin PWG, Pt(5,7)GeV
Grid
rcf1323
pp62.4 Y2006C
220
Done
No
Pythia for Spin PWG, Pt(7,9)GeV
Grid
rcf1324
pp62.4 Y2006C
220
Done
No
Pythia for Spin PWG, Pt(9,11)GeV
Grid
rcf1325
pp62.4 Y2006C
220
Done
No
Pythia for Spin PWG, Pt(11,15)GeV
Grid
rcf1326
pp62.4 Y2006C
200
Running
No
Pythia for Spin PWG, Pt(15,25)GeV
Grid
rcf1327
pp62.4 Y2006C
200
Running
No
Pythia for Spin PWG, Pt(25,35)GeV
Grid
rcf1328
pp62.4 Y2006C
50
Running
No
Pythia for Spin PWG, Pt(35,45)GeV
Grid
Name | SystemEnergy |
Range | Statistics | Comment |
rcf9001 | pp200, y2007g | 03_04gev | 690k | Jet Study AuAu200(PP200) JLC PWG |
rcf9002 | 04_05gev | 686k | ||
rcf9003 | 05_07gev | 398k | ||
rcf9004 | 07_09gev | 420k | ||
rcf9005 | 09_11gev | 412k | ||
rcf9006 | 11_15gev | 420k | ||
rcf9007 | 15_25gev | 397k | ||
rcf9008 | 25_35gev | 400k | ||
rcf9009 | 35_45gev | 120k | ||
rcf9010 | 45_55gev | 118k | ||
rcf9011 | 55_65gev | 120k | ||
Name | SystemEnergy | Range | Statistics | Comment |
rcf9021 | pp200,y2008 | 03_04 GeV | 690k | Jet Study AuD200(PP200) JLC PWG |
rcf9022 | 04_05 GeV | 686k | ||
rcf9023 | 05_07 GeV | 398k | ||
rcf9024 | 07_09 GeV | 420k | ||
rcf9025 | 09_11 GeV | 412k | ||
rcf9026 | 11_15 GeV | 420k | ||
rcf9027 | 15_25 GeV | 397k | ||
rcf9028 | 25_35 GeV | 400k | ||
rcf9029 | 35_45 GeV | 120k | ||
rcf9030 | 45_55 GeV | 118k | ||
rcf9031 | 55_99 GeV | 120k |
Name | SystemEnergy | Range | Statistics | Comment |
rcf9041 | PP500, Y2009 | 03_04gev | 500k | Spin Study PP500 Spin group(Matt,Jim,Jan) 2.3M evts |
rcf9042 | 04_05gev | 500k | ||
rcf9043 | 05_07gev | 300k | ||
rcf9044 | 07_09gev | 250k | ||
rcf9045 | 09_11gev | 200k | ||
rcf9046 | 11_15gev | 100k | ||
rcf9047 | 15_25gev | 100k | ||
rcf9048 | 25_35gev | 100k | ||
rcf9049 | 35_45gev | 100k | ||
rcf9050 | 45_55gev | 25k | ||
rcf9051 | 55_99gev | 25k | ||
rcf9061 | CuCu200,y2005h | B0_14 | 200k | CuCu200 radiation length budget, Y.Fisyak, KyungEon Choi. |
rcf9062 | AuAu200, y2007h | B0_14 | 150k | AuAu200 radiation length budget Y.Fisyak ,KyungEon Choi |
This page documents the options in geometry.g which define each of the production tags.
This page documents the options in geometry.g which define each of the production tags.
This page documents the options in geometry.g which define each of the production tags.
This page documents the options in geometry.g which define each of the production tags.
This page documents the options in geometry.g which define each of the production tags.
This page documents the options in geometry.g which define each of the production tags.
The attached spreadsheets document the production tags in STARSIM on 11/30/2009. At that time the y2006h and y2010 tags were in development and not ready for production.
.
y2008a full and TPC only material histograms
1 | 2 |
.
2 | |
3 | |
.
111 | |
` |
1 | |
.
. | |
. | |
. | |
The R&D conducted for the inner tracking upgrade required that a few specialized geometry tags be created. For a complete set of geometry tags, please visit the STAR Geometry in simulation & reconstruction page. The below serves as additional documentation and details.
Taxonomy:
The TPC is present in all configuration listed below and the SVT is in none.
Tag |
SSD | IST | HFT | IGT | HPD | Contact Person | Comment | |
---|---|---|---|---|---|---|---|---|
UPGR01 |
+ |
|
+ |
|
||||
UPGR02 |
|
+ |
+ |
|
||||
UPGR03 |
|
+ |
+ |
+ |
|
|||
|
+ |
|
|
+ |
Sevil |
retired | ||
|
+ |
+ |
+ |
+ |
+ |
Everybody |
retired | |
|
+ |
+ |
+ |
Sevil |
retired | |||
UPGR07 |
+ |
+ |
+ |
+ |
|
Maxim |
||
|
+ |
+ |
+ |
+ |
Maxim |
|||
|
+ |
+ |
+ |
Gerrit |
retired Outer IST layer only | |||
UPGR10 |
+ |
+ |
+ |
Gerrit |
Inner IST@9.5cm | |||
UPGR11 |
+ |
+ |
+ |
|
Gerrit |
IST @9.5&@17.0 | ||
|
+ |
+ |
+ |
+ |
+ |
Ross Corliss |
retired UPGR05*diff.igt.radii | |
UPGR13 |
+ |
+ |
+ |
+ |
Gerrit |
UPGR07*(new 6 disk FGT)*corrected SSD*(no West Cone) | ||
UPGR14 | + | + | + | Gerrit | UPGR13 - IST | |||
UPGR15 | + | + | + | Gerrit | Simple Geometry for testing, Single IST@14cm, hermetic/polygon Pixel/IST geometry. Only inner beam pipe 0.5mm Be. Pixel 300um Si, IST 1236umSi | |||
UPGR20 | + | Lijuan | Y2007 + one TOF | |||||
UPGR21 | + | Lijuan | UPGR20 + full TOF |
Eta coverage of the SSD and HFT at different vertex spreads:
Z cut, cm |
eta SSD | eta HFT |
---|---|---|
5 |
1.63 |
2.00 |
10 |
1.72 |
2.10 |
20 |
1.87 |
2.30 |
30 |
2.00 |
2.55 |
Material balance studies for the upgrade: presented below are the usual radiation length plots (as a function of rapidity).
Full UPGR05:
Forward region: the FST and the IGT ONLY:
Below, we plot the material for each individual detector, excluding the forward region to reduce ambiguity.
SSD:
IST:
HPD:
HFT: