AIDA GELINA BRIKEN nToF CRIB ISOLDE CIRCE nTOFCapture DESPEC DTAS EDI_PSA 179Ta CARME StellarModelling DCF K40
  BRIKEN, Page 15 of 21  ELOG logo
ID Date Author Subject
  134   Tue Nov 8 02:49:19 2016 PV, LiuSpecification of the dE silicon detector
The specification and picture of the dE silicon detector is shown in the attached photos.
The detector  has an effective area of 134 x 123 mm and  320 micrometer  thick
There are 26 vertical strips. They are combined into 2 readout channels (top and bottom which respect to the orientation of the detector in BRIKEN)
Attachment 1: spec_de_1.jpg
spec_de_1.jpg
Attachment 2: spec_de_2.jpg
spec_de_2.jpg
Attachment 3: IMG_1340.JPG
IMG_1340.JPG
  133   Mon Nov 7 14:17:23 2016 BRIKEN collaborationPicture of shift schedule
Attachment 1: IMG_20161107_183105.jpg
IMG_20161107_183105.jpg
  131   Mon Nov 7 13:44:26 2016 Alvaro, Ale, Jorge, JoseRunning Gasific and run protocol
Preliminary
Attachment 1: GasificShort.pdf
GasificShort.pdf GasificShort.pdf GasificShort.pdf GasificShort.pdf
  130   Mon Nov 7 13:15:07 2016 Alvaro, Ale, Jorge, JoseBackground
Background measurement overnight.

Start: 23:27 (07/11/2016)
Stop: 07:52 (08/11/2016)
ROOT file: 161108_0751_Overnight.root


The spectra have a terrible aspect!

This is consequence of DACQ crashing because LN2 filling!
Attachment 1: 161108_0751_Overnight_BRIKEN.pdf
161108_0751_Overnight_BRIKEN.pdf
  129   Mon Nov 7 13:11:42 2016 Alvaro, Ale, Jose, JorgeNew directory and Config file
For second part of Takechi's run:

Directory: /data/1611Commissioning/161107Parasitic
Config File: 161107Conf_BrikenFull.xlsx
Attachment 1: 161107Conf_BrikenFull.xlsx
  128   Mon Nov 7 09:05:09 2016 IrisDraft for Run sheet
Attached is the draft for the paper run sheet (version 2). If something is missing, please let me know.
Attachment 1: Run_sheet-Nov16-v2.pdf
Run_sheet-Nov16-v2.pdf
Attachment 2: Run_sheet-Nov16-v2.docx
  127   Mon Nov 7 09:04:10 2016 Phong,Liu,Ale,JoseNew AIDA plastic calibration
To have a range of about 200 MeV

Ortec671 Gain from x20 to x5 (fine gain : x0.5)
HV from 1500V to 1300V
60Co-> 10 mV

Root file: 161107_1800_AIDAplasticCalib.root

calibration a1= 0.001 MeV/units
Attachment 1: 161107_1800_AIDAplasticCalib.pdf
161107_1800_AIDAplasticCalib.pdf
  126   Mon Nov 7 06:55:01 2016 NTB, SGHPGe Fill line to D4 replaced

HPGe fill line to D4 replaced only small leak (overflow) once Ge is full.

Solenoid was also wrapped to no effect. AIDA DAQ still stops writing.

Boron sheet and extra polyethylene were placed back on top.

 

 

  125   Mon Nov 7 05:36:20 2016 Alenew calibration for F11
new calibration for F11

Using a value of 70 MeV energy loss and the file 161107_0833_Overnight.root
We obtained new peak positions: for V1A7C3 peak at 5398 (F11 right), for V1A7C4 (F11 left) peak at 6060

F11_rigth (V1A7C3): 0.01297
F11_left (V1A7C4): 0.01155
  124   Mon Nov 7 04:49:57 2016 Tain, AleAIDA plastic (veto) and Si de calibration
AIDA plastic (veto) and Si de calibration

For the calibration the Compton edge of the spectrum seen in the detectors was used.
There is a large uncertainty in that determination, since the spectra are not so clear in terms of shape.

For the spectra V1A7C13_EFIR (Si de, top) the channel position is 12900 units

For the spectra V1A7C14_EFIR (Si de, bottom) the channel position is 12950 units

For the spectra V1A7C9_EFIR (AIDA plastic) the channel position is 10425 units

These corresponds to the following calibration factors using 0.9 MeV as the Compton energy from Co source:

V1A7C13_EFIR (Si de, top): 6.976744E-5
V1A7C14_EFIR (Si de, bottom): 6.949807E-5
V1A7C9_EFIR (AIDA plastic): 8.633094E-5
  123   Mon Nov 7 04:37:33 2016 Phong,Liu,...Si de and AIDA plastic calibration
60Co source placed close to the detectors:

ROOT files: 
161107_1221_SiDetCalibration.root
161107_1237_AIDAPlasticCalibration.root
  122   Mon Nov 7 02:39:55 2016 AlePhoto of the white board with the details on the cards and preamps at B1F
Photo of the white board with the details on the cards and preamps at B1F
Attachment 1: New_Doc_160_2.pdf
New_Doc_160_2.pdf
  121   Sun Nov 6 23:35:42 2016 Tain et al.Overnight measurement: Ca isotopes
First 50,49,48Ca beam and then 47,46,45Ca beam
C-6mm IN and OUT

New Configuration file: 161107Conf_BrikenFull.xlsx

Start: 00:43
Stop: 08:33
Tmeas:12883.1 s


ROOT file: 161107_0833_Overnight.root

There is a change of gain for F11_PL_R and F11_PL_L

Rates:
F11R: 1150 cps / 950 cps
BRIKEN: 70->40 cps / 45->25 cps
VPLT: 34->12 cps / 34->12 cps
VPLB: 6->2 cps / 6->2 cps

Counts:
RateF11R: 1.41342e+07
RateBRIKEN: 697082. (4.9 neutrons/100 particles)
Corr_BR_F11R: 632710 (91%)
Estimated background: 5153.24
RateVPLT: 376233.
Corr_BR_VPLT: 213977 (315)
Attachment 1: 161107_0833_Overnight_Rates.pdf
161107_0833_Overnight_Rates.pdf
Attachment 2: 161107_0833_Overnight_F11.pdf
161107_0833_Overnight_F11.pdf
Attachment 3: 161107_0833_Overnight_CorrBRF11R.pdf
161107_0833_Overnight_CorrBRF11R.pdf
  120   Sun Nov 6 07:16:59 2016 Tain et al.58Ni on F7 CH2 F11 empty/C6mm
CH2 target at F7 in
Start with Empty at F11
Change to C-6mm at F11 later

Start: 16:16
Stop: 17:25

Change to C-6mm at 16:47 (at 544E6 ms in Timestamp units)

ROOT file: 161106_1725_58Ni_F7CH2.root

Rates:
F11R: 2000 cps
BRIKEN: 20 cps -> 35 cps
VPLT: 16 cps -> 40 cps
VPLB: 1.5 cps -> 5.5 cps

Figures Rate BRIKEN (red) Rate V_PL_T (blue)

Counts:
RateF11R: 8006721

RateBRIKEN: 111089 (1.4 neutron/100 particles)

Corr_BR_F11R: 108817 (98%)

RateBRVPLT: 115440

Corr_BR_VPLT: 21486 (19%)

RateBRVPLB: 16109
Attachment 1: 161106_1725_58Ni_F7CH2_Rates.pdf
161106_1725_58Ni_F7CH2_Rates.pdf
Attachment 2: 161106_1725_58Ni_F7CH2_RatesRings.pdf
161106_1725_58Ni_F7CH2_RatesRings.pdf
  119   Sun Nov 6 06:39:23 2016 Tain et al.58Ni on F11 C-6mm
58Ni in F11 C-6mm (later empty)
F7 CH2 target out (F5 CH2 target in)
Thresholds in V_PL_* lowered from 20MeV to 1MeV

Start: 15:37
Stop: 1609

ROOT file: 

They put the empty position of the F11 target ladder 
at 15:48. 
BRIKEN neutron count rate was reduced by a factor 2!
Also veto plastic det.
 
Rates:
F3: 4000 cps
F11_PL_R: 1350 cps
BRIKEN: 23 cps -> 14 cps
VPLT: 28 cps -> 12 cps
VPLB: 4 cps -> 1 cps

ROOT File: 161106_1609_58Ni_F11_empty.root

Figures Rate BRIKEN (red) Rate V_PL_T (blue)

Counts:
RateF11R: 2512767

RateBRIKEN: 30363 (1.2 neutron/100 particles)

Corr_BR_F11R: 29176 (96%)

RateBRVPLT: 31275

Corr_BR_VPLT: 5424 (17%)

RateBRVPLB: 3764
Attachment 1: 161106_1609_58Ni_F11_empty_Rates.pdf
161106_1609_58Ni_F11_empty_Rates.pdf
  118   Sun Nov 6 06:27:49 2016 Tain et al.58Ni on F11 C-6mm in
New calibration in V_PL_T and V_PL_R (Energyx1/2)

Start: 15:15
Stop: 15:35

File: 161106_1535_58Ni_F11_C6mm.root

Rates
F11_PL_R: 1300 cps
BRIKEN: 22 cps
V_PL_T: 7 cps
V_PL_B: 0.3 cps
  117   Sun Nov 6 03:12:55 2016 Alvaro,JorgeOvernight measurement
Measurement during beam production
and measurement with F7 CH2 out, 
F11 C-tar in/out, F7 CH2 in C-target out/in

START: 02:45
STOP: 12:47

ROOT file: 161106_1247_Overnight.root
  116   Sat Nov 5 17:07:27 2016 Tain, Alvaro, Jorge62Ni in F7
62Ni beam in F7 ON CH2 target

Strat with C target ladder in F11 in empty position.
They changed to C 6mm after a while (5-10min) but we 
didnt realized that!

THERE ARE NO APPRECIABLE DIFFERENCES WITH THE C-TARGET IN OR OUT!

DLT: 161106_0210_62Ni_F7_empty_002.dlt
Start: 02:10
Stop: 02:32
tlife: 1292.80 s

ROOT file: 161106_0232_62Ni_F7_empty.root

Rates at 2:19
F3: 2800 cps
F11: 1200 cps
BRIKE: 32 cps
VPLT: 17 cps
VPLR: 1 cps

Counts:
RateBRIKEN: 47703 (36.9 cps)

RateF11R: 1688270 (1305.90 cps)

Corr_BR_F11R: 47603 
(all neutrons are correlated with a particle going through F11)

RateBRVPLT: 23826 (18.43 cps)
Corr_BR_VPLT: 7557 
(15.8% of the neutrons are correlated with a particle 
going through plastic veto top) 

RateBRVPLB: 1865 (1.44 cps)
(the rate is 12.8 times smaller than top detector)
Attachment 1: 161106_0232_62Ni_F7_empty_Rates.pdf
161106_0232_62Ni_F7_empty_Rates.pdf
Attachment 2: 161106_0232_62Ni_F7_empty_F11.pdf
161106_0232_62Ni_F7_empty_F11.pdf
Attachment 3: 161106_0232_62Ni_F7_empty_CorrBRF11R.pdf
161106_0232_62Ni_F7_empty_CorrBRF11R.pdf
Attachment 4: 161106_0232_62Ni_F7_empty_VPL.pdf
161106_0232_62Ni_F7_empty_VPL.pdf
Attachment 5: 161106_0232_62Ni_F7_empty_CorrBRVPL.pdf
161106_0232_62Ni_F7_empty_CorrBRVPL.pdf
  115   Sat Nov 5 16:27:13 2016 Tain,Ale,Jorge,Alvaro62Ni beam in F11 empty target
Empty position of the target ladder at F11
(hole is smaller than beam size)

CH2 target at F7 is OUT

DLT 161106_0126_62Ni_F11_empty_001

Start: 01:26
Stop: 01:40

NO ROOT FILE!!

At 01:32:
Rate at F3: 2600 cps
Rate at F11: 850 cps
Rate at BRIKEN: 13 n/s
Rate at VPLT: 3 cps
Rate at VPLB: 0.1 cps
  114   Sat Nov 5 15:07:11 2016 Tain, Ale62Ni beam on F11 C-6mm
62Ni on 6 mm C target between MUSICs

The background before was 0.36 neutrons/s
Now it is around 10 n/s
With 3100 counts/s at F3 we have of the order of 25 neutrons/s
There is an slightly higher than 10 factor between the rate of 
the plastic top and bottom (13 cts/s vs 1ct/s).
Rate at F11 (plastic) 900 cts/s.

We start a proper measurement with DLT
Reset Timestamp

They will measure with 6mm C target (between MUSICS) for 
about 45 minutes and then 15 min without target.
CH2 target at F7 is OUT (beam going directly to F11).

DLT: 161106_0026_62Ni_F11_C6mm_000
Run: 000

Start: 00:27
Stop: 01:17
tlife=3007 s

At 00:37
Rate at F3: 3000 cps
Rate at F11: 900 cps
Rate at BRIKEN: 25 n/s
Rate at VPLT:13 cps
Rate at VPLB: 0.8 cps

Root File: 161106_0117_62Ni_F11_C6mm.root


Figure with rates: F11 (black), BRIKEN (red), Clovers (green)
V_PL_T (blue), V_PL_B (pink)

Figure with F11 spectra: Right (red), Left (blue)

Figure with time correlation between F11 and BRIKEN
The number of correlations (integrated spectrum minus flat background)
is 73063 very close the number of detected neutrons 73899
The difference 833 agrees well with the expected number of background
neutrons. That is: for every neutron detected in BRIKEN there was an 
ion passing through F11 (!?).
There is a funny double structure in the first 20 microsec.
94% of the neutrons are detected within 200microsec

Figure with the spectra of Veto plastics Top (red) and
bottom (blue). There are 7.5 times more counts in T than in B.
One can see in the Top peaks at 3MeV and 12MeV 
(corrected from 6 and 25 MeV: wrong calibration!!)
and show signals up to very high energy (GeV)

Figure with the time correlation between Veto Plastics and BRIKEN
Top (red) Bottom (blue). There is a time correlation with Top veto plastic
for 15% of the neutrons in BRIKEN (11440). There  are 18 times less 
correlations with the Bottom plastic. 
WARNING: The correlation was done for signals above "20MeV"
in the V_PL_T spectra i.e. only including the second bump"
Attachment 1: 161106_0117_62Ni_F11_C6mm_Rates.pdf
161106_0117_62Ni_F11_C6mm_Rates.pdf
Attachment 2: 161106_0117_62Ni_F11_C6mm_F11.pdf
161106_0117_62Ni_F11_C6mm_F11.pdf
Attachment 3: 161106_0117_62Ni_F11_C6mm_CorrBRF11R.pdf
161106_0117_62Ni_F11_C6mm_CorrBRF11R.pdf
Attachment 4: 161106_0117_62Ni_F11_C6mm_VPL.pdf
161106_0117_62Ni_F11_C6mm_VPL.pdf
Attachment 5: 161106_0117_62Ni_F11_C6mm_CorrBRVPL.pdf
161106_0117_62Ni_F11_C6mm_CorrBRVPL.pdf
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