| ID |
Date |
Author |
Category |
Subject |
|
43
|
Sat Jun 21 22:33:04 2025 |
Peter , Danyal | Detectors | PMTs are switched off | We have switched off all 3 PMTs ! |
|
50
|
Mon Jun 23 01:01:17 2025 |
Carsten | Detectors | CAEN PMT Power supply | Since yesterday, channel 0 of the CAEN PS is dead (no voltage even without cable).
Changed detector south to channel 3. |
|
54
|
Mon Jun 23 18:36:39 2025 |
Wilfried, Simon | Detectors | PMT test with LED | We tested the PMTs again, this time with an UV LED that is mounted at a window close to the XUV detector.
PMT south showed a very clear increase in count rate from about 1 to 50 Hz.
PMT mid also showed a small increase by a few Hz.
For PMT north there was no great change between LED off and on, but we think that the count rate also very slightly increased. Note, that PMT north is also the furthest away from the LED.
Also we saw a difference between single- and multi-photon events at PMT south. |
|
55
|
Tue Jun 24 12:25:34 2025 |
Carsten | Detectors | PMT behaviour - noise / PMT voltages / CFD Threshholds / CAEN Power supply (broken channel resetted) | In position North there is still the "old" 9423B PMT that draws quite some current.
On this detector threre is also some quite substantial noise. Very likely the base is not ok any more. Noise was much lesss for the other two PMTs.
Since position NORTH is the position with the largest sold angle, if there is another break from the accelerator we should exchange it against SOUTH.
It was also difficult to ramp up PMT north ; and I thought that againa channel broke (showing UnV not OVC (Overcurrent)). However, the PS is resetted if
you switch of the whole crate (aka switch the PS off). Before doing so, please ramp down the other channels slowly as intended.
Please leave the PMTs (besides you go in to exhchange the PMTs).
If you ramp pt PMT North (or the same detector at a different position), start with 2400 V and then slowly increase by steps of 50V.
Checked theresholds (but during injections, so in presence of electronic noise from injection). A further adjusted might be done later when we have measurement conditions.
(Or if we have time to exchange the PMTs).
Presently we have the following settings for CAEN:
CH1: Middle 2750 V, Thr 9
CH2: South 2700 V, Thr 7
CH3: North 2800 V, Thr 9 |
|
57
|
Tue Jun 24 17:39:13 2025 |
Carsten, Stefan, Simon, Rima, Nils | Detectors | PMT behaviour - noise / PMT voltages / CFD Threshholds / CAEN Power supply (broken channel resetted) | PMT North and South have been changed:
CFD CH0: Middle Thr 7 / CAEN HV Ch1: 2750 V
CFD CH1: South Thr 8 / CAEN HV Ch2: 2700 V
CFD CH2: North Thr 8 / CAEN HV CH3: 2800 V
MESY CFD Ch4: Thr.17
MESY CFD Ch5: Thr.16
MESY CFD Ch6: Thr.20
| Quote: | In position North there is still the "old" 9423B PMT that draws quite some current.
On this detector threre is also some quite substantial noise. Very likely the base is not ok any more. Noise was much lesss for the other two PMTs.
Since position NORTH is the position with the largest sold angle, if there is another break from the accelerator we should exchange it against SOUTH.
It was also difficult to ramp up PMT north ; and I thought that againa channel broke (showing UnV not OVC (Overcurrent)). However, the PS is resetted if
you switch of the whole crate (aka switch the PS off). Before doing so, please ramp down the other channels slowly as intended.
Please leave the PMTs (besides you go in to exhchange the PMTs).
If you ramp pt PMT North (or the same detector at a different position), start with 2400 V and then slowly increase by steps of 50V.
Checked theresholds (but during injections, so in presence of electronic noise from injection). A further adjusted might be done later when we have measurement conditions.
(Or if we have time to exchange the PMTs).
Presently we have the following settings for CAEN:
CH1: Middle 2750 V, Thr 9
CH2: South 2700 V, Thr 7
CH3: North 2800 V, Thr 9 |
|
|
61
|
Thu Jun 26 18:13:17 2025 |
Jan, Carsten | Detectors | PMT voltages & thresholds | current settings of PMT voltages and thresholds at the CAEN CFD:
PMT South [HV ch2: 2700V] [CFD ch0: 8]
PMT Middle [HV ch1: 2850V] [CFD ch1: 8]
PMT Nord [HV ch3: 2850V] [CFD ch2: 9] |
|
6
|
Wed Jun 11 11:20:23 2025 |
Konstantin, Simon | DAQ | octal gate generator delays | We checked the set delays of the OG 8000 octal gate generator and compared them with the values measured before the Bi-beamtime (see entry 34).
All values match within an uncertainty of <1ns
|
| OG 8000 delay / ns | |
Photodiode North | 62 | |
Photodiode South | 66.2 | |
PMT South | 157.5 | |
PMT Middle | 156.6 | |
PMT North | 159.4 | |
Particle South | 329.8
|
|
|
8
|
Wed Jun 11 17:33:04 2025 |
Carsten, Jan | DAQ | DAQ2 - new computer , new directories (lxg0155 doesn't work reliably) | LXG0155 (used in form er beamtimes) crashes and hangs and hangs eventually.
Lgx0155 is shut-down and is replaced by lxg3113.
For the experiment (DAQ2) still user stoe_exp can be used (Credits - see monitor).
MBS runs on r4l-68 with user atplaser: (/esr/usr/atplaser/) mbsrun/E0052/DAQ2
The data is stored on the ATP NAS (atprfio.gsi.de). (instead of local disk).
In the home directory there is link to access the data (u/stoe_exp/nas/229Th2025 ; ~/nas/229Th2025)
( sshfs -o directport=7777 atprfio.gsi.de:/mnt/raw.data /u/stoe_exp/nas )
For mbs the correct location on atprfio.gsi.de need to be used (cf. @openfile).i.e.
con rfio atprfio -DISK
and
open file /mnt/raw.data/229Th2025/Th25DAQ2_.lmd .
This is the mountpoint in mbs.
The commands @connectdisk and @openfile are adjusted accordingly. |
|
9
|
Thu Jun 12 15:53:13 2025 |
Carsten | DAQ | data directory and backup disk (WDBook2 RAID) | The data of DAQ1 are stored in the following directory and with the following filenames
open file /data.local2/2025_229Th/2025_229ThDAQ1_ -auto -rfio
(from @openfile)
The usual @connectdisk, @openfile @closefile are adapted and can be used.
The WDBook RAID0 disk is attached for backup of the data
/media/atplaser/WDBook2/2025E0052daq1 |
|
10
|
Thu Jun 12 16:27:45 2025 |
Carsten | DAQ | NTCAP directory | On the NTCAP the directory is changed to
Q:/E0052 |
|
11
|
Fri Jun 13 18:14:02 2025 |
Konstantin, Carsten | DAQ | DAQ Folder | Dryrun of DAQs. Folders of the data are:
|
DAQ1 file | DAQ2 file | scan range | laser steps | comment | |
/data.local2/2025_229Th/2025_229ThDAQ1_0090.lmd | /mnt/raw.data/229Th2025/Th25DAQ2_0106.lmd - */Th25DAQ2_0107.lmd | 550.4 - 549.6 | 201 | | |
91 | 108 - 111 | 550.4 - 549.6 | 201 | | |
92 | 112 | 550.4 - 549.6 | 201 | Changed step logic of Medusa back to previous version before the start of this run | |
93 | 113 | 550.4 - 549.6 | 201 | | |
94 | 114 | 550.4 - 549.6 | 201 | | |
95 | 115 - 116 | 550.4 - 549.6 | 201 | | |
96 | 117 | 550.4 - 549.6 | 201 |
|
Data were recorded with a synthesized RF of 1.5MHz |
|
12
|
Mon Jun 16 07:26:01 2025 |
Konstantin | DAQ | Startup of Medusa and DAQ1 | The laser control software (Medusa) is hosted on the Windows PC ATPPC023. First connect via the command
atplaser@lxg1297:~$ xfreerdp /w:2500 /h:1400 /u:atplaser /v:atppc023.campus.gsi.de
You will be asked for the usual "atplaser" password. Please be aware that you're typing on an english keyboard!
Medusa is simply started by the link on the Desktop called "Medusa Laser Control". After startup you will see the main window (Attachment 1).
Please make also sure that the Wavelength meter software is running!!! Otherwise, wavelengths cannot be logged
In the main window different actions can be made (see also Attachment 2):
- Open additional views, options are "Display" (figure of recent values), "MBS Messenger" (connection status with MBS, lower part of Attachment 2), "Devices View" (most recent values of different devices, right part of Attachment 2)
- Make sure that "Make Data Available to MBS" is selected
- Definition of laser scan Parameters. The laser will perform an automated scan between the selected wavelengths. It's possible to define an increment or a number of laser steps as scan parameter. After the laser has received the specified number of rising edges on Trigger port #1 (Do not change the port number, since this corresponds to the Hardware setting!) the laser advances to the next frequency until the number of steps and scan repetitions is completed. There is an option to start the laser scan automatically, when a trigger was received on port #3 (The cabling is done. However, the pulse generation must be provided from SCU sddsc221 channel IO1 of timing receiver tr1 whenever needed).
- The button can be used to start and stop a scan. In some cases there might occur an USB communication error with the laser, which can also be reset by this button.
- IMPORTANT NOTE: Make sure that the FCU is enabled, since otherwise the BBO of the FCU does not follow the wavelength of the laser, which results in NO UV output power.
- After "Make Data Available to MBS" option (see 2.) has been selected, Medusa is awaiting the MBS client to connect.
- View of most recent parameter settings.
The complete startup routine to perform a laser scan is the following:
- Start medusa as described above
- Connect to "r4l-41":
atplaser@lxg1297:~$ ssh atplaser@r4l-41
- Change to the directory of the Th-MBS version:
R4L-41 > cd mbsrun/E0052/DAQ1
- Make a reset (optional):
R4L-41 > resl
- Start mbs:
R4L-41 > mbs
- Once you are in the mbs environment start the acquisition:
mbs > @startup
- Connect to the file server:
mbs > @connectdisk
- Start acquisition:
mbs > sta ac
With this command, the connection to the Medusa server should be established. This can be verified by the line
-R4L-41 :read_meb :connected succesfully to LabView Server.
of the MBS output, and in the MBS Messenger View of Medusa stating
Connected! Established connection to ...
- Open file:
mbs > @openfile
- Press Run-button in the Go4 analysis (must be started beforehand)
- Start laser scan in medusa
- Press Stop-button in the Go4 analysis
- Close file:
mbs > @closefile
As long as nothing crashes (keep fingers crossed), only steps 9-13 need to be repeated for subsequent scans. |
| Attachment 1: MedusaStartup.JPG
|
|
| Attachment 2: Medusa.png
|
|
|
14
|
Mon Jun 16 22:27:01 2025 |
Carsten, Simon | DAQ | Thresholds | We also adjusted the thresholds for the mesytic.
Doing that, we noticed that one of the trafos is broken (5th row, middle).
|
PMT | channel | Threshold
| |
South | 5 | 35
| |
Middle | 6 | 16
| |
North | 7 | 16
|
|
|
16
|
Tue Jun 17 16:33:16 2025 |
Carsten, Simon | DAQ | Gate Q-swtich | The gate generator of the Q-switch signal for the Vuprom TDC was set to 10ms. |
|
18
|
Wed Jun 18 00:33:56 2025 |
Esther, Alexis, Anton, Rodolfo, Carsten | DAQ | R4l-41 | | We have some issues with the RIO computer R4l-41 (DAQ1). We had to switch off completely twice. Only then it reacted properly. Maybe a problem with the network at about 00:00 o'clock? |
|
45
|
Sun Jun 22 18:47:23 2025 |
Carsten, Peter, Marek, Simon | DAQ | PMT and particle detector settings | Final voltages and thresholds for the PMTs and particle detectors before the first scan:
|
Detector | voltage (kV) | threshold (mV) | mesytec
| |
particle detector | 1.35 | 100 | -
| |
PMT north | 2.7 | 10 | 16
| |
PMT mid | 2.65 | 10 | 16
| |
PMT south | 2.7 | 10 | 16
|
All other mesytec thresholds remain unchanged and can be found in entry 7.
Important note: Ch0 of the PMT power supply broke, so we moved PMT north to CH3.
Current setup:
CH1: PMT mid
CH2: PMT south
CH3: PMT north |
|
56
|
Tue Jun 24 15:44:06 2025 |
Konstantin | DAQ | Phase shift in DAQ1 | In the SetParameters.C file is a parameter called fPar->piPhaseOffset. It was shifted from 100 to 50 in order to see ion bunches in the pmt signal and laser pulses in the photodiode signal during the same revolution in the TDC spectrum. Note that this parameter must be taken
into account when setting the window conditions of the arrival time in the SetConditions.C file. |
|
67
|
Fri Jun 27 11:21:25 2025 |
Esther, Konstantin | DAQ | Timing | We cross-checked the timing. Laser pulse is detected at bins 136 (PD-North) and 171 (PD-south), respectively. Therefore, the laser puls is in the electron cooler at 153.5. The revolution period corresponds to 3e8Hz / 1.54315MHz = 194.
The ion bunch must travel 2.5m more than the half of the circumference (108.3m). Taking this into account, the ion bunch must be detected (0.5 + 2.5 / 108.3) * 194 = 101.5 bins later (meaning less) than 153.5.
Finally, we are happy that the timing is still perfect, since the ion bunch arrives at 52. |
|
63
|
Thu Jun 26 21:27:34 2025 |
Carsten, Jan, Simon | Calibration | Timing | We checked the timing (before the start of the measurement cycle documented below).
Timing and measurement window are attached. |
| Attachment 1: Bildschirmfoto_timing_new_2025-06-26_19-00-04.png
|
|
|
26
|
Wed Jun 18 19:05:28 2025 |
Carlo, Zac, Shahab, Ragan | Analysis | PID with rionid | For PID with rionid we used:
- LISE file from last year (attached.
- .npz file from 410 RSA (attached). |
| Attachment 1: Schermata_2025-06-18_alle_19.03.04.png
|
|
| Attachment 2: E142_TEline-ESR_229Th.lpp
|
Version 17.5.18
{============================= Main Part ======================================}
[general]
File = //wsl.localhost/Ubuntu-18.04/home/chenruijiu-ubuntu/experiment/ESR/2022_229Th/E142_TEline-ESR_229Th.lpp
Date = 12-06-2024
Time = 01:29:23
Configuration = GSI/FRS-TA-ESR_2014.lcn
Optionsfile = GSI_FRS_2021.lopt
Title = GSI FRS TA-ESR (2014)
BlockStructure = DSDSMDASDDD
NumberOfBlocks = 11
[settings]
A,Z,Q = 238U 92+ ; Mass ElementName Charge+ Beam
Energy = 555.9 MeV/u
Intensity = 1e+9 pps ; enA,pna,pps,kW
RF frequency = 20 MHz
Bunch length = 1 ns
Settings on A,Z = 229Th ; Mass ElementName Charge+ Beam
[OpticsBeam]
BX = 0.472 (+/-)mm ; one-half the horisontal beam extent (x)
BT = 1.59 (+/-)mrad ; one-half the horisontal beam divergence(x')
BY = 0.245 (+/-)mm ; one-half the vertical beam extent (y)
BF = 2.04 (+/-)mrad ; one-half the vertical beam divergence (y')
BL = 0 (+/-)mm
BD = 0.03 (+/-)% ; one-half of the momentum spread (dp/p)
ShiftX = 0 mm ; beam respect to the spectrometer axis
AngleX = 0 mrad ; beam respect to the spectrometer axis
ShiftY = 0 mm ; beam respect to the spectrometer axis
AngleY = 0 mrad ; beam respect to the spectrometer axis
Scheme Angle = 0 degrees
ShapeX = 1
ShapeT = 1
ShapeY = 1
ShapeF = 1
ShapeL = 1
ShapeD = 1
OptBeam_X = 1 (+/-)mm
OptBeam_T = 30 (+/-)mrad
OptBeam_Y = 1 (+/-)mm
OptBeam_F = 30 (+/-)mrad
OptBeam_L = 0 (+/-)mm
OptBeam_D = 1.5 (+/-)%
[options]
NP simple = 64 ; Number of points in distribution
NP charge states = 16 ; Number of points in distribution
NP wedge = 128 ; Number of points in distribution
Charge states = Yes ; No & Yes
CutEdgeEffect = 1 ; 1-Yes. Default, 0-no - for extended configurations
Prim.beam scatter = 0 ; 0-without, 1-with
Delta peak = 0 ; 0-without, 1-with
BrhoMeanMax = 1 ; 0-Max, 1-Mean
BrhoMeMaLeRi = 3 ; 0-Max, 1-Mean, 2-Left, 3-Right /for fission/
CentralCut = 1 ; 0-no, 1-moderate, 2-strong
[target]
Target contents = 0,4,1,9.012 ; Nomer,Z,Atoms,Mass
Target thickness = 1,1850,1.85,0,0,0 ; State,Thickness,density,angle,SolidGas,..
Target fusion compound = 0
Targ use for Q-states = 1
Target Defect = 0,0.1 ; [0] choice - % or micron at 0 degree, [1]=value;
Degrader contents = 0,6,1,12.011 ; Nomer,Z,Atoms,Mass
Degrader thickness = 0,0,2.26,0,0,0 ; State,Thickness,density,angle,SolidGas,..
Degra use for Q-states = 1
Degrader Defect = 0,0.1 ; [0] choice - % or micron at 0 degree, [1]=value;
[mechanism]
Reaction = 0 ; 0 - fragm, 1 - fusion-resid, 2 - fusion-fission
CalcOther = 1 ; calculate other reactions
V calculation = 5 ; 0 - constant, 1 - Borrel, 2 - Rami, 3-convolution, 4-two body reaction
V_opt/Vbeam = 1 ; default 1
Velocity_exceed = 1 ; 0 - without, 1-with - two-body recations velocity corrections
Binding Energy for Vf/Vp = 8 MeV ; Binding energy for Borrel's expression
Shift for Vf/Vp calc = 0
Prefragment_Rami = 1
Sigma0 = 90 MeV/c ; default 90
SigmaD = 0 MeV/c ; default 200
SigmaM = 87 MeV/c ; default 87
Asymmetry = 0 % ; default 0
Method v-sigma = 0 ; 0 - Goldhaber, 1-Morrissey,2-Friedman,3-Convolution
G_Surface = 0.95 MeV/fm^2
Symmetry around half_Ab = 1
Pfaff pickup correction = 0
ChargeExchangePfaff = 0 ; 1 - exclude, 0-forget
Sigma corr 0 = 0 ; Coulomb energy
Sigma corr 1 = 0 ; Projectile mass
Friedman mode = 2 ; 0-Qgg, 1-Surface, 2-Qgg+Surface
Prefragment_Fri = 1
Coulomb_Friedman = 1
K_Morr = 8 MeV/A ; E/A=8MeV/A default; D.Morrissey coef.
K_MorHalf = 8 MeV/A ; E/A=8MeV/A default at Afrag=Aproj/2; D.Morrissey coef.
AA_fast = 0
AA_Modefast = 3
MethodApf = 2 ; Prefragment search method: 0-N/Z direction, 1 - W*EPAX, 2 - W*CSgeom,
ExcitationApf = 1 ; Excitation energy for APF search: 0 - dSurface, 1 - dA*Ex
BarrierShape = 1 ; 0-classical, 1-quantum mech.
H_omega = 3 MeV ; default 3
Probabilty_CN = 1 ; 0/1 use Prbabilty for CN formation
UseVanishing = 1
VanishMode = 0 ; 0-Sierk, 1-Cohen
NuclPotential = 1 ; 0-Bass, 1-WS
WS_V0 = 105 MeV
WS_R0 = 1.12 fm
WS_a = 0.75 fm
FusDiffuseness = 1
Width Coef = 1 ; default 1; for Leon's charge state distribution
gZt Correction = 1 ; default 1; Leon's C.S.D.
PowerCoefLeon = 0.477 ; default 0.477; Leon's C.S.D.
Cross section = File ; Fit & File
Charge method = 3 ; charge calculations method 0-5
EPAX Cross Section = 4 ; cross section calculations method 0-4
SR Cross Section = 1 ; EPAX for SR 0-2
Energy Loss = 4 ; energy loss calculation method 0-3
Anglular straggling = 1
AngStragInOptics = 0 ; 0-LISE, 1-ATIMA
StragglingCoef1 = 0.217
StragglingCoef2 = 1.12
Energy straggling = 1 ; 0-LISE, 1-ATIMA
EnergyStragMethod = 1 ; 0-integrate, 1-table
EnergyStragShape = 0 ; 0-Gauss, 1-Landau-Vavilov
EquilThickness = 1 ; 0-Charge, 1-Global
MassMethod = 0 ; 0-DB+calcul, 1 + just calcul
MassDataBase = 0 ; 0-A&W, 1-User ME
Mass formula = 2 ; 0-LDM, 1-Myerer, 2: 1+corrections
MassExcessFile = AME2016.lme
UseChargeForEnergy = 2 ; 0-No, 1-Yes, 2-Auto
EnergyValueAuto = 30 ; default value 30 MeV/u
EquilibriumMode = 0 ; 0-Equil, 1-NonEquil
UB_Global = 70 ; default 70 MeV/u
MinZ_Global = 29 ; default Z>=29
ChargeStateOptim = 1 ; 0-No, 1-Yes
ZmQ_AfterReactn = 0 ; default 0 (full stripped)
EPAX_p_Norm = 1
EPAX_p_Un = 1.65
EPAX_p_Up0 = 1.788
EPAX_p_Up1 = 0.004721
EPAX_p_Up2 = -1.303e-5
EPAX_p_H = 1
[fission]
FisAngDistShape = 0 ; 0-isotropic; 1-anisotropic
FisMomCutForAngDist = 2 ; 0-dont use; 1-use just MatrixKinematics; 2-use for all; (default 2)
OddEvenCorrections = 1 ; 0-dont use; 1-use
PostScissionEvaporation = 1 ; 0-dont use; 1-use
DeexcitFunctionPoints = 0 ; 0- average deexcitation energy; 1- 3 points; 2 - manually
FisEXmanually = 20 ; Excitation energy manually
FisCSmanually = 1000 ; Cross section manually
FisTXEmethod = 0 ; 0-from Edissipated, 1 from Q-value
Fis_f = 0.0035 ; default 0.0045
FisEXsigma = 5.5 MeV ; default 5.5
FisCS_Global = 1e-12
FisCS_TKE = 1e-8
FisBeta1 = 0.625 ; deformation of light fragment
FisBeta2 = 0.625 ; deformation of heavy fragment
FisTKE_d = 2 fm ; d-param in Wilkins formula
FisBetaFit = 1 ; 0-manual, 1-fit
N0 = 83 ; default 82
dU0 = -2.65 ; default -2.5
C0 = 0.7 ; default 1.4
cpol0 = 0.65 ; default 0.65
width0 = 0.63 ; default 0.63
N1 = 90 ; default 90
dU1 = -3.8 ; default -5.5
C1 = 0.15 ; default 0.16
cpol1 = 0.55 ; default 0.55
width1 = 0.97 ; default 0.97
[charge_suppression]
FragInd = 1e-3
FragTotal = 1e-5
BeamInd = 1e-12
BeamTotal = 1e-15
[convolution]
Convolution mode = 1 ; 0-Qgg, 1-Surface, 2-E* per Abraded nucleon
Sigma_0 = 91.5
Sigma_1 = 91.5
Sigma_2 = 160
CoefConv_0 = 3.344
CoefConv_1 = 3
CoefConv_2 = 1
ShiftConv_0 = 0.1581
ShiftConv_1 = 0.1487
ShiftConv_2 = -1
[evaporation]
NP evaporation = 32 ; Number of points in distribution
NPevapFis = 8 ; Number of points in distribution
EvapMethod = 2
StateDensityMode = 2 ; 0, 1+pairing, 2+shell
EvapUnstableNuclei = 1 ; 0 - only stable,1 +unstable
Tunnelling = 1
AvoidUnboundCS = 1
ProtectedChannels = 1
R_Evaporation = 5.7 fm ; correction for the effective Coulomb barrier
Mode_Apf_manual = 0 ; 1-manual, 0-auto
Energy_in_T = 2 ; default 2
EvaporationVelocity = 0 ; 0 - quality, 1 -fast
DeltaOddEvenEvap = 12
DeltaOddEvenFission = 14
BreakupTemperature250 = 4.7
BreakupTemperature150 = 5.9
BreakupTemperature050 = 8
BreakupDiffuseness = 0.05
DissipationKramers = 0
DissipationStepFunction = 1
DissipationBeta = 1 ; default 2.0
mode_1n = 1
mode_2n = 0
mode_1p = 1
mode_2p = 0
mode_a = 1
mode_d = 0
mode_t = 0
mode_3he = 0
mode_fis = 1
mode_brk_up = 1
mode_gamma = 0
[fission_barrier]
FissionBarrierFactor = 1
FissionBarrierMode = 1 ; #0-4
OddEvenCorrections = 1
ShellCorrections = 1
FB_InOutMax = 2 ; #0-2 - in/out/max
ModeForUser = 1 ; #0-2
NdeltaOddEven = 2.5
ZdeltaOddEven = 9
[excitation_energy]
AbrasionModel = 0 ; 0-Geometrical, 1-Exponential
GeomAA_Correction = 1 ; 0 - don't use,1 - use -default
Thermalization = 0
ThermaTimeCoef = 3e+0 ; 2.1e-22 MeV *s/e(t)
AbraExpSlope = 0.363
Friction = 0 ; 0 - off,1 - on
Ev_A_SigmaCoef = 9.6
G_FrictionCoef1 = 6.5
G_FrictionCoef2 = 0.5
G_FactorCoef1 = 1.5
G_FactorCoef2 = 2.5
DepthHole = 40
EnergyCoef_CB0 = 0
EnergyCoef_CB1 = 27
EnergyCoef_CB2 = 0
SigmaCoef_CB0 = 0
SigmaCoef_CB1 = 18
SigmaCoef_CB2 = 0
D_MeanTemp = 13
DN_MeanTemp = 0
DZ_MeanTemp = 0
LN_median = 20
LN_variance = 20
LN2_median = 0
LN2_variance = 0
AA_factor = 1
ApplyLimitTemp = 0
[evapauto]
tun_a0 = -0.61392
tun_a1 = 0.44559
tun_a2 = 0.12008
A_Bound = 300
A_Pairing = 1
[plot]
Start target = Detector ; Detector & RF
Start of TOF = T1
Stop of TOF = M1
dE-detector-1st = M1
dE-detector-2nd = M1
TKE-detector = M1
X-detector = M1
Y-detector = M1
Tilting = M1
Stopper = M2
RO_Wedge = W1
ConditionBlock = A0
Plot threshold = 1e-10 pps ; minimal value for plot scale
Shift of TOF for RF = 0 ns ; for dE-TOF plot with RF
Fraction of RF trigger = 1
UseCondition = 0
TKE_calibration = 1,1,0,MeV
[cs_file]
UserDiffCS = 0 ; Number of User Diff CS saved in this file
AppendOverwrite = 1
AttachedInside = 1
ShowCSinPlot = 1
Chi2 = 1
[sec_reactions]
NP sec.reactions = 32 ; Number of points in distribution
Secondary reactions = 0
fiss_FilterUse0 = 1
fiss_FilterUse1 = 1
fiss_FilterUse2 = 1
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| Attachment 3: RSA01-2025.06.18.18.06.02.162.tiq_spectrum.npz
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| Attachment 4: Schermata_2025-06-18_alle_19.32.53.png
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