MUST2 SAMURAI_2018 S3-LEB-LPC SUPERNEMO MUGAST EXPAND SCALP GALATRON HiCARI VELO
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New entries since:Thu Jan 1 01:00:00 1970
Status ExpNbr Date Authordown Type Category Target-Source Subject
Fixede793s Sun Mar 14 15:20:47 2021 AdrienOFFLINEGeneralCD2Updated Angular distribution macro
The angular distribution macro has been updated and now produce TWOFNR calculation on the fly.
Feel free to add new plots and play around with the parameter.
MakePlot will produce the distribution using Ex and sigmaEx of the state and Eg and sigmaG of the gamma. Efficiency is automatically taken into account using the efficiency provided by manu.
FIT will perform the TWOFNR calculation using The energy of the state, l and j of the transferred nucleon and J of the formed states. Once the calculation done, it does the fit to the data and extract the C2S.

I found the number strangely small so I suspect we do something wrong.

To run it:
Open a terminal
$> lpcgrit
$> npp MUGAST
$> cd e793s
$> root AngDist.C
Fixede793s Thu Mar 11 01:24:47 2021 Ablaihan, LouisRUNGeneralCD2run 53 screenshots
Screenshots of the run 53
Beam intensity is ~ 7.4 10^5 pps in CATS and 5.3 10^5 in VAMOS
~75% transmition
Dt is ~ 3%
Attachment 1: run53_Scalers.png
run53_Scalers.png
Attachment 2: run53_MM_Impact.png
run53_MM_Impact.png
Attachment 3: run53_Times.png
run53_Times.png
Attachment 4: run53_VAMOS_MWpng
Attachment 5: run53_MM_TY.png
run53_MM_TY.png
Attachment 6: run53_MM_TX.png
run53_MM_TX.png
Attachment 7: run53_MG_TY.png
run53_MG_TY.png
Attachment 8: run53_MG_TX.png
run53_MG_TX.png
Attachment 9: run53_MM_ErawY.png
run53_MM_ErawY.png
Attachment 10: run53_MM_ErawX.png
run53_MM_ErawX.png
Attachment 11: run53_MG_ErawY.png
run53_MG_ErawY.png
Attachment 12: run53_MG_ErawX.png
run53_MG_ErawX.png
Attachment 13: run53_MG_E_TOF.png
run53_MG_E_TOF.png
Attachment 14: run53_MM_dEE.png
run53_MM_dEE.png
Attachment 15: run53_MM_E_TOF.png
run53_MM_E_TOF.png
Attachment 16: run53_MG_impact.png
run53_MG_impact.png
Fixede793s Thu Mar 11 02:50:14 2021 Ablaihan, LouisBEAMGeneralCD2VAMOS transmition
at 2h50 beam intensity reached 1.1x10^6 pps in CATS for 6.5x10^5 pps in VAMOS. The transmition decreased to 60% without any shift of the beam position. Does it come from a loss of efficiency of VAMOS at high counting rate?
Fixede793s Thu Mar 11 04:38:31 2021 Ablaihan, LouisBEAMGeneralCD2Beam stopped due to a equipment tripped in CSS1
Beam stopped 4h30 due to a equipment tripped in CSS1. They are going to fix it. Estimated timing of the intervention ~10/20min.
Beam went back at 4h52 at 3.5x10^5 pps in CATS and 3.0x10^5 pps in VAMOS. transmision ~ 85%
Attachment 1: Scaler_run53_4h30.png
Scaler_run53_4h30.png
Fixede793s Thu Mar 11 05:12:36 2021 Ablaihan, LouisRUNGeneralCD2run 53 new screenshots
Attachment 1: run53_1_MMMG_T.png
run53_1_MMMG_T.png
Attachment 2: run53_1_MM_Impact.png
run53_1_MM_Impact.png
Attachment 3: run53_1_MG_impact.png
run53_1_MG_impact.png
Fixed  Tue Apr 16 12:18:46 2019 AGATAAGATAHardware ATC4 - position 13 HV tripped
- HV tripped around 12h10.
- need access to check the origin
Fixed  Tue Apr 16 13:15:48 2019 AGATAAGATAHardware ATC4 - position 13 HV tripped

set 1500 V at 13h15
Fixed  Wed Apr 17 11:25:29 2019 AGATAAGATAGeneral AGATA background in Coinc with MUST2 with 14O beam
https://lxagata0.ganil.fr:8989/e744/56
http://run-control:8989/e744/56
Pinnede744s Wed Apr 10 11:57:37 2019 A. LemassonOFFLINESoftware VAMOS Conversion HowTo

HOW TO convert a run in VAMOS
  • Do : source $HOME/GoToVamosAna
  • To Convert a Run : MyVAna -d2Ar <RunNr>
  • Otherwise, If you want to convert a single file : MyVAna -d2Ar -f <Infile> <OutFile>
  • Output Root rile is written to : ./RootA/

If you encounter the error on Brho "Could not find the BrhoRef for the run <RunNr> ", Update the ./Calibs/ListBrho.dat file with relevant Brho for RunNr
Fixede744s Thu Apr 11 00:06:50 2019 A. LemassonRUNGeneralN/ARun58
Without Finger 21 kHz -> Reduced to 800 Hz with finger
Attachment 1: XfTFFinger.png
XfTFFinger.png
Attachment 2: run58_Brho_Cats2_14N.png
run58_Brho_Cats2_14N.png
Fixede744s Sun Apr 14 15:05:06 2019 A. LemassonVAMOSHardware Change of Offset in DC Numexo
  • Increasing offset to minimize saturation.
  • Reducing DC Threholds
    • DC0 436 ->355 mV
    • DC1 255 ->255 mV
    • DC2 269 ->269 mV
    • DC3 600 ->433 mV

Attachment 1: DC_NUMEXO_AfterChange.png
DC_NUMEXO_AfterChange.png
Attachment 2: DC_NUMEXO_BeforeChnage.png
DC_NUMEXO_BeforeChnage.png
Fixede744s Mon Apr 15 12:33:52 2019 A. LemassonVAMOSHardware Test Run 127 : Change if IC Shaping
Try to change IC Shaping to solve the pb of Continuous Line in IC0 vs IC1
Change Shaping on all IC during run 126 Change Chan 5-12 from Filter B (3us) to Filter A (1us)
Regarding The line IC0 vs IC1 :
  • If Filter A The y =x line disapear, but the resolution deteriorate (22% compared 9 % in Filter B)
  • No clear effect of the Thresholds of
  • No clear effect of decay time on the resolution

Back to initial conditions of Run 126
Attachment 1: IC_Threshold_BeforeChange_run126.png
IC_Threshold_BeforeChange_run126.png
Attachment 2: IC_Decay_BeforeChange_run127.png
IC_Decay_BeforeChange_run127.png
Attachment 3: IC_CHange_Shaping__run127.png
IC_CHange_Shaping__run127.png
Attachment 4: IC_Shaping_Restore_run127.png
IC_Shaping_Restore_run127.png
Fixede744s Mon Apr 15 15:18:55 2019 A. LemassonVAMOSHardware Optimization of IC Shaping
During Run 129,
1) investigation of the trapezoidal filter of IC
2) The Conclusion is that if we reduce the shaping to 2.5 us we reduce the random line in IC vs IC (At 1e5 in VAMOS : Random Line / Peak is 18.5 % compared to 40% for shaping of 3us)
3) The 2.5us us also optimum for the resolution (oscillation of the abse line after the filter very sensitive to K, with freq of ~500Khz)

/!\ Increasing intensity during the study


Flat Top 1.07 , 320ns k+0.5M

K sigma
0.5 81 530
1.0 236 1038 0.53
1.5 161 1549 0.25
2. 215 2039 0.247
2.5 156 2554 0.1435
3. 260 3082 0.196

Changing N
320 2.5 126 2554 0.116
160 2.5 126 2554 0.116
40 2.5 130 2554 0.119

Chnging Q
2980 40 2.5 130 2554 0.1119
3300 40 2.5 134 2554 0.123

Chnging M

1070 3300 40 2.5 134 2554 0.123
500 2900 40 2.5 145 2554 0.133
750 3000 40 2.5 145 2554 0.133


-> Final Setting is
M Q N K
1070 3200 160 2.5 -> 126/2554 -> 0.116
Attachment 1: IC_Shapingafter_run129.png
IC_Shapingafter_run129.png
Fixede786s Tue Jun 25 15:33:40 2019 A LemassonVAMOSGeneral VAMOS Analysis - Brho
VAMOS Analysis :
VAMOS PID with attached SetAlias.C

Suggestion to change Brho from 1.05 to 0.95 based on the distribution of K ions to optimize acceptance on the K
ions
Attachment 1: dEE_r56.png
dEE_r56.png
Attachment 2: Q_vs_Xf_All_r56.png
Q_vs_Xf_All_r56.png
Attachment 3: Q_vs_Xf_K_r56.png
Q_vs_Xf_K_r56.png
Attachment 4: Brho_E_K_r56.png
Brho_E_K_r56.png
Attachment 5: Q_MQ_K_r56.png
Q_MQ_K_r56.png
Attachment 6: SetAlias.C
char cond[1000];
TTree *t1;
void SetAlias()
{
  gStyle->SetPalette(1);

  t1 = (TTree*) gROOT->FindObject("AD")
;
  t1->SetAlias("fExist_DC_Y","DC0_Y>-1500&&DC1_Y>-1500&&DC2_Y>-1500&&DC3_Y>-1500"); 
  t1->SetAlias("fExist_IC","IC[0]>0&&IC[1]>0&&IC[2]>0&&IC[3]>0"); 

  t1->SetAlias("mT","(T_FPMW_CATS2_C*-1 + 305.3 + -4*(MWTVN==8)-1*(MWTVN==9)-1*(MWTVN==10)-2.2*(MWTVN==11)-0.7*(MWTVN==12)-0.5*(MWTVN==15)-0.6*(MWTVN==16)-1.1*(MWTVN==17)+0.6*(MWTVN==18)-1*(MWTVN==6)-0.5*(MWTVN==5)-0.5*(MWTVN==4)-1.5*(MWTVN==3))*(T_FPMW_CATS1_C>10)");
  t1->SetAlias("mD","D");
  t1->SetAlias("mV","(mD)/mT");
  t1->SetAlias("mBeta","mV/29.9792");
  t1->SetAlias("mGamma","1./sqrt(1.0-mBeta*mBeta)");
  
  t1->SetAlias("mM_Q","Brho/3.107/mBeta/mGamma");
  t1->SetAlias("mM","(mE)/931.5016/(mGamma-1.)");
  t1->SetAlias("mMr","mM_Q*((13.*qmq13+14.*qmq14+15.*qmq15+16.*qmq16))"); 
  t1->SetAlias("mQ","mM/mM_Q");
 
  //t1->SetAlias("mT1","(T_FPMW_HF_C*-1. + 559. + 3*(MWTVN==8))*(T_FPMW_HF_C>10)");
  t1->SetAlias("mT1","1.5+((23.7593+1.03259*MWTV)*(MWTVN==0)+(-9.53168+1.0711*MWTV)*(MWTVN==1)+(-30.486+1.11554*MWTV)*(MWTVN==2)+(-31.1261+1.11624*MWTV)*(MWTVN==3)+(-62.99829+1.1569*MWTV)*(MWTVN==4)+(-47.9021+1.13413*MWTV)*(MWTVN==5)+(-14.3957+1.08086*MWTV)*(MWTVN==6)+(-24.6655+1.1058*MWTV)*(MWTVN==7)+(60.4375+0.981809*MWTV)*(MWTVN==8)+(4.44472+1.06168*MWTV)*(MWTVN==9)+(11.408+1.04492*MWTV)*(MWTVN==10)+(56.8282+0.990287*MWTV)*(MWTVN==11)+(59.6833+0.995356*MWTV)*(MWTVN==12)+(27.6344+1.02846*MWTV)*(MWTVN==13)+(6.02794+1.06554*MWTV)*(MWTVN==14)+(20.1561+1.0342*MWTV)*(MWTVN==15)+(51.0718+1.01008*MWTV)*(MWTVN==16)+(36.5605+1.0391*MWTV)*(MWTVN==17)+(-6.01158+1.09581*MWTV)*(MWTVN==18)+(37.6143+1.00939*MWTV)*(MWTVN==19)+(29.3289+1.01291*MWTV)*(MWTVN==20) + 3*83.4*(GATCONF_MASTER==8)-0*(GATCONF_MASTER==1)-2*83.4*(GATCONF_MASTER==4))");
  t1->SetAlias("mT1","540-2*T_FPMW_CATS2_C");
  t1->SetAlias("mE1","(IC[0]+IC[1]+IC[2]+IC[3]+IC[4])*(IC[0]>0.1&&IC[1]>0.1&&IC[2]>0.1&&IC[3]>0.1)");
  //  t1->SetAlias("mE1","(IC[1]+IC[2]+IC[3])*(IC[1]>1&&IC[2]>1&&IC[3]>1)");
  t1->SetAlias("mdE0","IC[0]*(IC[0]>1)");
  t1->SetAlias("mdE1","IC[0]*(IC[0]>1)+IC[1]*(IC[1]>1)");
  t1->SetAlias("mD1","Path");
  t1->SetAlias("mV1","mD1/(mT1)");
  t1->SetAlias("mBeta1","mV1/29.9792");
  t1->SetAlias("mGamma1","1./sqrt(1.0-mBeta1*mBeta1)");
  
  t1->SetAlias("mM_Q1","Brho/3.107/mBeta1/mGamma1");
  t1->SetAlias("mM1","1.3*(mE1)/931.5016/(mGamma1-1.)");
  t1->SetAlias("mMr","mM_Q*((13.*qmq13+14.*qmq14+15.*qmq15+16.*qmq16))"); 
  t1->SetAlias("mQ1","mM1/mM_Q1");
  t1->SetAlias("ProjD","-174.*1.");
  t1->SetAlias("Xt","TMW1_X+ProjD*tan(TP_Theta/1000.)");
  t1->SetAlias("Yt","TMW1_Y+ProjD*tan(TP_Phi/1000.)");

 
  t1->SetAlias("mT2","540.5-2.*T_FPMW_CATS2_C+2.7*(MWTVN==16)+2.7*(MWTVN==15)+2.9*(MWTVN==14)+2.9*(MWTVN==13)+2.4*(MWTVN==12)+1.3*(MWTVN==11)+1.5*(MWTVN==10)+1.6*(MWTVN==9)-0.6*(MWTVN==8)+2.5*(MWTVN==7)+2.*(MWTVN==6)+1.6*(MWTVN==5)+1.1*(MWTVN==4)-0.6*(MWTVN==3)-1.2*(MWTVN==2)-4.0*(MWTVN==1)");

 //t1->SetAlias("mT2","mT1-TMWT1_MWT2_C+31");
  //  t1->SetAlias("mT2","mT1-4.83");

  t1->SetAlias("mdE2","(IC[0]+IC[1]*(IC[0]>0.1)");

 t1->SetAlias("mE2","0.85*(pow(Xf+450*tan(Tf/1000.),2)*0.0000015*IC[0] + 2.2*IC[0]+1.1*IC[1]*(IC[0]>0.1)+1.34*1.95*IC[2]*(IC[0]>0.1)*(IC[1]>0.1)+3.1*IC[3]*(IC[0]>0.1)*(IC[1]>0.1)*(IC[2]>0.1)+1.05*IC[4]*(IC[0]>0.1)*(IC[1]>0.1)*(IC[2]>0.1)*(IC[3]>0.1)+IC[5]*(IC[0]>0.1)*(IC[1]>0.1)*(IC[2]>0.1)*(IC[3]>0.1)*(IC[4]>0.1))");

 // t1->SetAlias("mE2","0.825*(2.4*IC[0]+IC[1]*(IC[0]>0.1)+1.5*1.95*IC[2]*(IC[0]>0.1)*(IC[1]>0.1)+3.16*IC[3]*(IC[0]>0.1)*(IC[1]>0.1)*(IC[2]>0.1)+1.1*IC[4]*(IC[0]>0.1)*(IC[1]>0.1)*(IC[2]>0.1)*(IC[3]>0.1)+IC[5]*(IC[0]>0.1)*(IC[1]>0.1)*(IC[2]>0.1)*(IC[3]>0.1)*(IC[4]>0.1))");

//t1->SetAlias("mE2","IC[0]+IC[1]*(IC[0]>0.1)+2*IC[2]*(IC[0]>0.1)*(IC[1]>0.1)+2*IC[3]*(IC[0]>0.1)*(IC[1]>0.1)*(IC[2]>0.1)+IC[4]*(IC[0]>0.1)*(IC[1]>0.1)*(IC[2]>0.1)*(IC[3]>0.1)+IC[5]*(IC[0]>0.1)*(IC[1]>0.1)*(IC[2]>0.1)*(IC[3]>0.1)*(IC[4]>0.1)");
   t1->SetAlias("mdE21","(IC[0]+IC[1])*(IC[0]>1&&IC[1]>0.1)");
 t1->SetAlias("mE21","(IC[0]+IC[1]+2*IC[2]+2*IC[3]+IC[4]+IC[5])*(IC[0]>0.1)*(IC[1]>0.1)*(IC[2]>0.1)*(IC[3]>0.1)");
 t1->SetAlias("mD2","Path+5");
  t1->SetAlias("mV2","mD2/(mT2)");
  t1->SetAlias("mBeta2","mV2/29.9792");
  t1->SetAlias("mGamma2","1./sqrt(1.0-mBeta2*mBeta2)");
  
  t1->SetAlias("mM_Q2","Brho/3.105/mBeta2/mGamma2");
  t1->SetAlias("mM2","(mE2)/931.5016/(mGamma2-1.)");
  t1->SetAlias("mQ2","mM2/mM_Q2");
  t1->SetAlias("mMrec","int(mQ2+0.5)*mM_Q2");
  
  t1->SetAlias("Gamma_from_E","mE2/14./931.5016+1");
  t1->SetAlias("Beta_from_E","sqrt(1.-1./pow(Gamma_from_E,2))");
  t1->SetAlias("Brho_from_E","14./8*3.105*Beta_from_E*Gamma_from_E");

  t1->SetAlias("mEM","(3.7*IC[0]+IC[1]+IC[2]+IC[3]*(IC[2]>0.1)+18./55*IC[4]*(IC[3]>0.1&&IC[2]>0.1) + 7.*IC[5]*(IC[4]>0.1&&IC[3]>0.1&&IC[2]>0.1) )*(IC[0]>1&&IC[1]>0.1&&IC[2]>1&&IC[3]>1)");

}


Attachment 7: Mr_K_r56.png
Mr_K_r56.png
Attachment 8: QMQ_K_Gates.png
QMQ_K_Gates.png
Fixede744s Thu Apr 11 00:23:21 2019 Iulian François MarlèneRUNHardwareCH2TAC changes & target
We have inserted the 2nd target CH2 104 um.

We have changed the range of the TAC MUGAST-HF from 1us to 200ns.

TAC VAMOS-CATS1 (in fact CATS2) was not working in the previous run because there was no delay on CATS. We send now CATS DELAY x2, meaning that the delay is 300ns.
   Mon Apr 15 04:34:00 2019      

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