ID |
Date |
Author |
Category |
Subject |
54
|
Wed Jun 12 21:21:15 2024 |
Yuri | Detectors | NTCap started |
Fcenter - 244.6 MHz
BW - 10 MHz |
67
|
Thu Jun 13 14:56:09 2024 |
Stefan Schippers | Accelerator | Estimated beam lifetime: About 150 s |
Estimate of storage lifetime using my code 'hydrocal':
ion mass in u ...................................: 229
ion nuclear charge ..............................: 90
ion charge state ................................: 89
beam energy in MeV ..............................: 45501.1
beam energy in MeV/u ............................: 198.695
beam beta .......................................: 0.566309
beam rigidity in T m.............................: 5.4944
ring circumference in m .........................: 108.36
ring acceptance in mrad .........................: 2
ring temperature in °C ..........................: 25
ring vacuum pressure in mbar ....................: 3e-11
residual gas density in m^-3 ....................: 7.28767e+11
residual gas composition
Z %
1 93.43
6 2.23
7 0.75
8 3.29
18 0.3
cooler length in m ..............................: 2.5
electron current in A ...........................: 0.2
magnetic expansion factor .......................: 1
electron-beam diameter in mm ....................: 50.8
electron density in cm^-3 .......................: 3.62844e+06
cooler cathode temperature in meV ...............: 110
cooling energy in eV ............................: 109000
space_charge (0th iteration) in eV ..............: 44.3477
space_charge (1st iteration) in eV ..............: 44.341
transverse temperature in meV ...................: 110
longitudinal temperature in meV .................: 0.2
RR nmin .........................................: 1
RR lmin .........................................: 0
RR nele [no. electrons in subshell (nmin,lmin)] .: 1
RR nmax .........................................: 128
RR enhancement factor ...........................: 2.5
RR alpha in cm^3 s^-1 ...........................: 8.04602e-08
beam lifetime due to multiple scattering in s ...: 1.86e+06
beam lifetime due to single scattering in s .....: 7.51886e+07
beam lifetime due to charge capture in s ........: 3.5516e+06
beam lifetime due to stripping in s .............: 1e+99
beam lifetime due to recombination in cooler in s: 148.466
beam lifetime with electron cooling in s ........: 148.46
beam lifetime without electron cooling in s .....: 1.20121e+06
detector count rates for 1E6 stored ions and a residual gas pressure of 3e-11 mbar:
recombination detector from ecool (Hz) ....: 4575.41
recombination detector from res.gas (Hz) ....: 0.0545666
total rate on recombination detector (Hz) ....: 4575.46
ionization detector from res.gas (Hz) ....: 1.93798e-94 |
6
|
Wed May 29 10:54:21 2024 |
Shahab, Jan | General | Gas Target Events with new timing system |
Using the new timing system, it is possible to grab any events as pulses, but also as long inter event gates under GENESYS. Many instances of GENESYS can be running on ACO computers, so that there is no conflict, if an instance is running in main control room or another in ESR-Messhütte.
GENESYS Settings:
Inter-Event for 162 up and 163 down, signaling the gas target cycle. The signal can either be:
- Controlled automatically by the control system (sub chain patterns)
- Set to manual operation during setup or experiment.
"activating" the condition in GENESYS by clicking on the small "A" button in the condition. (B) us achieved by "deactivating" the condition in GENESYS, by clicking again on the "A", it turns into a "-". After this, it is possible to manually set the level "hi" or "low" on the left box. As a result a orange bar goes up and down as an indicator. Any time you can switch to automatic change by pressing on "-" again.
Using this new timing system, the old hardware in the main control room is not needed anymore.
Additional Information:
In the old experiments, we used the new control system events but still using the old hardware in the main control room. Please see:
https://elog.gsi.de/esr/E121/13 |
32
|
Fri Jun 7 17:10:45 2024 |
Sebastian | General | XUV LED |
Maximum XUV LED Voltage: 6.5V |
79
|
Wed Jun 26 11:59:12 2024 |
Ruijiu, Shahab, Carsten | Analysis | Prepare plots for Thomas's presentation |
data:
(env_OnlineDataAnalysisSystem) litv-exp@lxbk0497:/lustre/astrum/experiment_data/2024-05_E018/OnlineDataAnalysisSystem/data/iq/IQ_2024-06-
12_21-47-54$
The root file is at:
(env_OnlineDataAnalysisSystem) litv-exp@lxbk0497:/lustre/astrum/experiment_data/2024-05_E018/OnlineDataAnalysisSystem/data/iq/IQ_2024-06-
12_21-47-54$ root filtered_spectrum_670_750.root
The figure below shows the interface of the program "combine_injection". You can combine any tdms file with this program. To run this
program, you need to log in to the server /luster/astrum/, and activate the conda environment. Then type the command "combine_injection" at
the terminal. You will see the interface. |
71
|
Thu Jun 13 18:48:26 2024 |
Ruijiu Chen, David, Shahab, Yuri | Analysis | The ion identification of 229Th is correct. |
Harmonic: 124.0 , Bp: 7.796046 [Tm]
ion fre[Hz] yield [pps]
------------------------------------------------------------
237U+92 243732740.7822311819 8.6164e+03
237Np+92 243732858.1891748905 1.9672e+02
224Ac+87 243759120.6575988531 1.7025e+03
229Pa+89 243784072.1343108118 2.5529e+03
229Th+89 243784111.0000000000 3.3883e+03
234Pa+91 243807737.9699291289 2.4721e+03
234Np+91 243807852.4158236086 1.7745e+01
The strongest line is 229Th+89/229Pa+89. The yield and frequency of 229Pa+89 and 229Th+89 are very close to each other. We needed to
install Al target to suppress Pa as much as possible. Al gives a better ratio of h-like to he-like than Be. Two peaks at left
side are 237U+92/237Np+92 and 224Ac+87. One peak at right side is
234Pa+91/234Np+91.
Note added 2024-06-14 (Carsten): a) We will not produce Np, this is an artifact of Lise, b) relative intensities are for injection only. Line intensities for 237U/224Ac/234Pa are substantially lower after cooling/HF/deceleration. |
62
|
Thu Jun 13 12:37:14 2024 |
Ruijiu Chen, David | Analysis | Lifetime of beam in center of mass is 193 s. |
|
63
|
Thu Jun 13 13:29:47 2024 |
Ruijiu Chen, David | Analysis | Lifetime of beam during June 12 22:00- June 13 0:00 |
|
64
|
Thu Jun 13 14:20:36 2024 |
Ruijiu Chen, David | Analysis | Lifetime of beam during June 13 4:30:7:00 |
|
65
|
Thu Jun 13 14:35:27 2024 |
Ruijiu Chen, David | Analysis | Lifetime of beam during June 13 7:00~9:00 |
|
66
|
Thu Jun 13 14:41:22 2024 |
Ruijiu Chen, David | Analysis | Lifetime of beam during June 13 9:00~11:00 |
|
7
|
Fri May 31 15:53:06 2024 |
Ruijiu Chen | DAQ | run NTCAP system |
NTCAP is working again.
Connect the RF cable and the scaler cables to NTCAP system.
The map of signal is recorded in following link.
https://elog.gsi.de/esr/E0018/2
Test it with IQ rate of 10 MSamples/s.
E0052/IQ_2024-05-31_15-04-34
E0052/SC_2024-05-31_15-04-34 |
40
|
Mon Jun 10 11:59:12 2024 |
Ruijiu Chen | Analysis | The ion identification of spectrum recorded on 2022 |
The simulated frequency is given in simulation_result.out. The yield is calculated by LISE file. The LISE file is attached here also. |
46
|
Wed Jun 12 01:51:51 2024 |
RuiJiu, David | Analysis | ID |
The preliminary identification has been thoroughly checked using the RionID software. We have confirmed that the identification is accurate.
Attached can be found the simulation file with each of the expected ions, their revolutions frequencies in the 125th harmonic and expected yield from the LISE file attached.
Also attached are some figures from RionID that highlight the region of interest for the 124th and 125th harmonics. The center frequency of the 245 MHz resonator is closer to the 124th harmonic for 229Th+89 which is located at 244.769 MHz.
If necessary, we can slightly shift the resonator curve to higher frequencies to fine-tune the signal-to-noise ratio for 229Th+89. |
70
|
Thu Jun 13 18:38:24 2024 |
Rodolfo Sanchez, Julian Palmes, Sebastian Klammes | Laser | Laser Dye change - new MRC settings - scraper checks of laser beam |
We changed the dye at ~3pm.
After some fine adjustements of the laser we had to change the MRC settings, because the laser position changed.
Therefore we checked the position of the laser with the T-Scrapers with the settings from post 49 "First Scraper Scan".
New settings of MRC and screen pic is attached.
The position of the laser on the screen is now the 'same' as yesterday (see attachement). |
3
|
Thu Apr 25 16:34:05 2024 |
Rodolfo | Laser | Efficiency of Fluorescein27 |
The figure below shows the efficiency of Fluorescein27 vs. Wavelength. Each point was averaged over 500 laser shots.
Dye Laser: Sirah, Cobra Strech.
- Solvent: Ethanol + H2O.
- Concentration Oszillator: 0.4 g + 0,2 g/l NaOH.
- Concentration Main Amplifier: (1/8) Concentration Oscillator .
Pump Laser: InnoLas, SpitLight 1500-30
- Seeding energy: 550 mJ / Pulse.
Note. Dye was mixed on 28.04.2022 |
5
|
Wed May 29 09:49:30 2024 |
Rodolfo | Laser | Laser-beam profile |
Using a telescope (Plan-concave lens -500 mm and Plan-convex lens +1000 mm) after the pulsed-dye laser system we got the following laser-beam profile at the Electron-Cooler's position. Dye Laser @ 550 nm / 275 nm |
15
|
Mon Jun 3 18:24:44 2024 |
Rodolfo | Detectors | PMT arrangement |
The picture shows the actual configuration of the PMTs.
We are using a 4-Channel High-Voltage supply. The channels are labeled according to the PMTs names.
The suggested operation voltages are:
- PMT Nord (Type 9423, SN. 652): -2600 V
- PMT Mitte (Type 9423, SN. 653): -2500 V
- PMT Süd (Type 9422, SN. 1049): -1750 V |
16
|
Mon Jun 3 19:42:06 2024 |
Rodolfo | Laser | Laser-beam through E-Cooler |
UV-laser beam is now going through the Electron-Cooler.
Telescope settings:
- Plan concave lens -500 mm
- Plan convex lens + 1000 mm
- Distance between the both linses: 535 mm
- Position at Long Travel Stage: 60,0 mm |
17
|
Tue Jun 4 22:54:02 2024 |
Rodolfo | Detectors | PMT - Manufacture - Test Result Data |
|