|  Wed Nov  6 14:13:53 2019, Jan, Laszlo, Detectors, DSSSD - 1st movement - realignment, | 
| We moved the new detector installation for the first time slowly into the dipole chamber. The alignement seems to be pefect, no distortion or vertical movement of the detector-arm was observed from the window flange.
 
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|  Fri Oct 25 16:34:51 2019, Jan, Runs, prerun007 - MixedAlpha, | 
| save point: lxg1275:/datalocal1/e127/predata/prerun007 
 start: Fr 25.10.19 - 16:35
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|  Fri Jun  7 15:57:41 2019, Jan, DAQ, DAQ with & without MDPP-16, | 
| The DAQ located in 
 ../esrdaq_2018/r4l-58/
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|  Wed Oct 23 15:35:29 2019, Jan, DAQ, DAQ with & without MDPP-16, | 
| the DAQ located in ../esrdaq_2018/r4l-58_dev/
 
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|  Wed Oct 23 14:51:43 2019, Jan, Laszlo, DAQ, VME modules & main.cfg,   | 
| Here is the current list of VME modules in our DRASI daq including HW addresses: 
 Slot    <module>        [HW addr.]
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|  Wed Oct 23 11:40:29 2019, Jan, Runs, prerun005 - MixedAlpha, | 
| save point: lxg1275:/datalocal1/e127/predata/prerun005 
 start: 23.10.19 - 11:40
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|  Wed Sep 25 13:58:24 2019, Laszlo, General, Gamow window energies for 118Te(p,g),   | 
| # Z   A   Iso Re Rc   T9 upper width mxpos  shift 52 118 te118 pg 20  0.5  1.39  0.58  1.06  -0.01
 52 118 te118 pg 20  1.0  2.27  1.04  1.69  -0.01
 | 
|  Wed Sep 25 13:03:46 2019, Laszlo, Analysis, simulations on 118Te+p,  11x   | 
| I have made some simulations at 8AMeV, 7AMeV and 4AMeV energies for the main 118Te + p reaction channels. For the Rutherford simulations credits to Yuanming! For each energy there are 3 simulations: without the scraper, with the
 scraper (online), scraper (online) + E-truncation (offline). The scraper is treated as an "ideal scraper" meaning
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|  Thu Aug 29 10:02:22 2019, Jan, Detectors, bakeout at ESR setup,   | 
| The bakeout for our detector setup has started on the evening of 27.08.2019 We have a temperature sensor in the vacuum next to the detector.
 The goal is to maximize bakeout temperature, while not going above 125°C at the detector/sensor.
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|  Fri Aug  9 13:43:15 2019, Laszlo, Simulations, pn channel simulations for 111Sn(p,g)112Sb experiment,  12x   | 
| The p,n channel opening for 111Sn beam is at 5.8895 MeV/u beam energy. Therefore, when choosing 6MeV/u, 7MeV/u, 8MeV/u beam energies, there is not much kinetic energy left for the excitation of the 111Sb nucleus --> there
 can be "less" nuclear levels populated above groundstate of 111Sb. These "less" states can be handled explicitly
 | 
|  Fri Aug  9 13:14:09 2019, Laszlo, , pn channel simulations for 111Sn(p,g)112Sb experiment, | 
| The p,n channel opening for the 111Sn+p reaction is at 5.8895 MeV/u beam energy. Therefore, when choosing as 6MeV/u, 7MeV/u, 8MeV/u beam energies, there is not much kinetic energy left for the outgoing neutron --> there are "less" nuclear levels populated above groundstate in 111Sb, they can be handled
 explicitly. My simulations are based on TALYS results. The following steps did I made:
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|  Tue Jul 23 10:46:29 2019, Laszlo, Analysis, 124Xe pg peak fit using mixed cascade simulation,  7x   | 
| This entry is the continuation of the cascade effects on the pg peak shape entry: 
 https://exp-astro.physik.uni-frankfurt.de:8080/E108/475
 | 
|  Tue Jul  9 15:26:59 2019, Yuanming Xing, Simulations, Simulated Rutherford scattering distribution on detector,     | 
| Simulated Rutherford scattering distribution on detector 
 Beam: 111Sn
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|  Mon Jul  8 14:57:07 2019, Yuanming Xing, Detectors, The measurement of the tilting angle,   | 
| As shown in the figure, the detector is tilted by a certain angle which is about 45 degree. The tilted angle is defined as angle B.
 We measured angle A using the vertical laser line (red) and papers with a straight line edge. So we can marked
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|  Fri Jun 28 14:06:28 2019, Jan, General, CAD of (p,g) setup, | 
|  | 
|  Tue Jun 25 21:19:50 2019, Laszlo, Simulations, MOCADI input parameters,    | 
| initial BEAM input parameters for MOCADI are based on: - https://web-docs.gsi.de/~weick/mocadi/download/esr-exl-test.in --> twist parameters (ratio of X/A and B/Y)
 - M. Steck et al, Electron cooling experiments at the ESR, NIM A 532 (2004) 357-365 --> epsilon_x = 5·10^-7
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|  Tue Jun 11 10:13:56 2019, Jan, Runs, prerun003 - MixedAlpha, | 
| save point: lxg1275:/datalocal1/e127/predata/prerun004 ~10min run
 
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|  Fri Jun  7 14:39:36 2019, Jan, Detectors, Pt100 installation & readout,    | 
| The new detector holder incorporates a Pt100 temperature sensor, which is UHV compatible. The Pt-resistor is read out via 4 wires. These wires are integrated into the D-SUB connector of the detector. The new wires use the pins as shown in the attached picture
 "det_connector.png".
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|  Fri Jun  7 14:28:09 2019, Jan, Runs, prerun003 - MixedAlpha,   | 
| save point: lxg1275:/datalocal1/e127/predata/prerun003 
 ~20min run
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|  Fri Jun  7 13:52:32 2019, Jan, Runs, prerun002 - MixedAlpha,   | 
| save point: lxg1275:/datalocal1/e127/predata/prerun002 
 ~20min run
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|  Fri Jun  7 10:18:23 2019, Jan, Runs, prerun001 - MixedAlpha,   | 
| save point: lxg1275:/datalocal1/e127/predata/prerun001-root 
 ~2h run
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