Skip to Content.
Sympa Menu

sphenix-run-l - Re: [Sphenix-run-l] Beam Spot and sPHENIX/INTT Geometry

sphenix-run-l AT lists.bnl.gov

Subject: Commissioning and running of sPHENIX

List archive

Chronological Thread  
  • From: "Sondheim, Walter E" <sondheim AT lanl.gov>
  • To: "Liu, Ming Xiong" <mliu AT lanl.gov>, nouicer <rachid.nouicer AT bnl.gov>, "sphenix-run-l AT lists.bnl.gov" <sphenix-run-l AT lists.bnl.gov>, "SPHENIX MVTX " <sphenix-maps-l AT lists.bnl.gov>
  • Cc: Camelia Mironov <camelia.mironov AT cern.ch>
  • Subject: Re: [Sphenix-run-l] Beam Spot and sPHENIX/INTT Geometry
  • Date: Tue, 18 Jul 2023 01:00:27 +0000

A fascinating plot! Besides the 5.0 mm shift in the beam spot location (X or Y), the amount of background points to adding additional shielding - just my guess.
Cheers,
Walt

Sent with BlackBerry Work
(www.blackberry.com)


From: Liu, Ming Xiong <mliu AT lanl.gov>
Date: Monday, Jul 17, 2023 at 5:59 PM
To: nouicer <rachid.nouicer AT bnl.gov>, sphenix-run-l AT lists.bnl.gov <sphenix-run-l AT lists.bnl.gov>, SPHENIX MVTX <sphenix-maps-l AT lists.bnl.gov>
Cc: Sondheim, Walter E <sondheim AT lanl.gov>, Camelia Mironov <camelia.mironov AT cern.ch>
Subject: Re: [Sphenix-run-l] Beam Spot and sPHENIX/INTT Geometry

Thank you Rachid, cc’d MVTX list,

Very interesting results, I wonder this has anything to do with the high beam background we have seen in MVTX …

 

Ming

 

Ming

 

-----

signature_61897647

 

Dr. Ming Xiong Liu

P-3, MS H846

Physics Division

 

Office: 505.667.7125

Mobile: 505.412.7396

Los Alamos National Laboratory

 

 

From: Sphenix-run-l <sphenix-run-l-bounces AT lists.bnl.gov> on behalf of nouicer <rachid.nouicer AT bnl.gov>
Date: Monday, July 17, 2023 at 5:39 PM
To: "sphenix-tracking-l AT lists.bnl.gov" <sphenix-tracking-l AT lists.bnl.gov>, <sphenix-run-l AT lists.bnl.gov>, "sphenix-intt-l AT lists.bnl.gov" <sphenix-intt-l AT lists.bnl.gov>
Subject: [Sphenix-run-l] Beam Spot and sPHENIX/INTT Geometry

 

Dear Joseph and Tony,

Please see the attached plots which correspond to the RHIC beam spot in X, Y directions obtained by the INTT detector using beam data with magnet-OFF run =20869 taken on 08 July 2023.

We observe that the beam spot coordinates is (0 mm, 5 mm); this means the beam spot is shifted by five mm in Y direction.

Before Stefan shows this plot to CAD, we need to understand is this shift by five mm is due to the beam shift itself, or it is caused by the INTT detector geometry (not fully implemented in our software).

I already provided you with the INTT local survey data (obtained at the lab for each ladder) as well with INTT Global survey data (obtained at the sPHENIXPHENIX IR).  Are these survey data implemented in the present sPHENIX/INTT detector geometry that we are using in our analysis or not?

We would highly appreciated your feedback. 

Sincerely,
Rachid for the INTT Group

-- 
- 
/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/
                                                 /                     /
 Rachid Nouicer                                 /                     /
 Brookhaven National Laboratory                /                     /
                                              /                     /
 Address:                                    /                     /
 Brookhaven National Laboratory (BNL)       /                     /
 Physics Department, Building 510c         /                     /
 20 Pennsylvania Avenue                   /                     /
 Upton, New York, 11973, U.S.A.          /Phone:+1 631 344 8433/
                                        /                     /
 E-mail : rachid.nouicer AT bnl.gov       / Fax:+1 631 344 3253 /
 Web:http://www4.rcf.bnl.gov/~nouicer /                     /
                                     /                     /
/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/ 

_______________________________________________ Sphenix-run-l mailing list Sphenix-run-l AT lists.bnl.gov https://lists.bnl.gov/mailman/listinfo/sphenix-run-l




Archive powered by MHonArc 2.6.24.

Top of Page