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.

Here is a daily protocol of temperatures and vacuum pressure
T_12 is the set value of the 1st and 2nd controller device
T_34 is the set value of the 3rd and 4th controller device 
T_56 is the set value of the 5th and 6th controller device
T_sens is the temperature measured by the sensor close to the detector

day   date        P_setup    T_sens  T_12   T_34   T_56   comment
1     tue 28.08.  1e-6 mbar  ~100°   ~120°  ~120°  ~120°  carefull start
2     wed 29.08.  3e-7 mbar  ~121°   ~180°  ~150°  ~150°  T_sens reached ~126° during NEG-pump conditioning
3     thu 30.08.  6e-7 mbar  ~124°   ~185   ~150°  ~175°  readjusted T_56, outgassing a bit increased
7     mon 02.09.  5e-9 mbar   ~80°                        during cooldown
9     wed 04.09.  2e-10mbar   ~30°                        after cooldown, NexTorr Pump active     

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
that there is no scattering at the edges (maybe worth a GEANT4?). The slit position is at -3cm from the beam, the vertical
length is 7cm (centralized). The following channels are combined in the
simulation:

-8AMeV:
  Rutherford
  pg channel, 5cascade model. Photon emission is treated isotropically
  pn channel, including: -->gs, -->1-->gs, -->2-->gs, -->3-->gs, -->3-->1-->gs, -->4-->1-->gs, -->5-->3-->gs,
-->5-->3-->1-->gs, -->5-->4-->1-->gs decay chains with their weights. Neutron and photon emission is treated isotropically.

-7AMeV:
  Rutherford
  pg channel, 4cascade model. Photon emission is treated isotropically

-4AMeV:
  Rutherford
  pg channel, 3cascade model. Photon emission is treated isotropically


The detector position is -2.5cm from the beam in the radial direction and centered vertically with a 45° tilt. 
The cross section values for pg and pn, the pn channel mixing, and the pg cascade number is based on TALYS simulations.
The other two input parameters are the luminosity and the measurement time. For the simulation, a little
pessimistic (or realistic?) scenario is taken: L = 10^24 cm-2s-1, and t = 10^4 s. From this values, from the N=CS*L*t
equation, the pg counts (based on the TALYS
cross sections) are the following: 8AMeV ~267, 7AMeV ~163, 4AMeV ~5! This means that to reach the Gamow-window
energies is challenging, but with a well-working scraper it is not impossible to reach.


As it is visible, the 8AMeV 118Te(p,g) case is very similar to the 7AMeV 124Xe case. The p,n threshold is
somewhere ~7.5MeV.

# 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
 52 118 te118 pg 20  1.5  3.04  1.46  2.21  -0.01
 52 118 te118 pg 20  2.0  3.71  1.82  2.68  -0.01
 52 118 te118 pg 20  2.5  4.32  2.16  3.10  -0.02
 52 118 te118 pg 20  3.0  4.85  2.44  3.47  -0.06
 52 118 te118 pg 20  3.5  5.35  2.73  3.79  -0.12
 52 118 te118 pg 20  4.0  5.79  2.97  4.08  -0.19
 52 118 te118 pg 20  5.0  6.55  3.38  4.61  -0.35

source: https://journals.aps.org/prc/supplemental/10.1103/PhysRevC.81.045807

save point: lxg1275:/datalocal1/e127/predata/prerun005

start: 23.10.19 - 11:40 
stopp: 23.10.19 - ~13:30

DAQ setup:
32 ADC channels
 ch. 1-16 (section 0) >> x-strips
 ch. 17-32 (section1) >> y-strips
32 TDC channels
 ch. 1-16 (section 0) >> x-strips
 ch. 17-32 (section1) >> y-strips
32 scaler channels 
 (not used)

Detector setup:
bias -30V
MixedAlpha source in center

the DAQ located in
../esrdaq_2018/r4l-58_dev/

currently includes
2x MADC
2x Caen V775 TDC
2x Caen V830 Scaler




> The DAQ located in 
> 
> ../esrdaq_2018/r4l-58/ 
> currently includes the readout of
> MADC
> Caen 775 TDC
> Caen 830 Scaler
> MDPP-16
> 
> ../esrdaq_2018/r4l-58_rewind/
> is without the MDPP-16:
> MADC
> Caen 775 TDC
> Caen 830 Scaler

save point: lxg1275:/datalocal1/e127/predata/prerun007

start: Fr 25.10.19 - 16:35 
stopp: 

DAQ setup:
64 ADC channels
 ch. 01-64 (ADC0) >> empty
 ch. 33-48 (ADC1 - section0) >> x-strips
 ch. 49-64 (ADC1 - section1) >> y-strips
32 TDC channels
 ch. 01-64 (TDC0) >> empty
 ch. 33-48 (TDC1 - section0) >> x-strips
 ch. 49-64 (TDC1 - section1) >> y-strips
64 scaler channels 
 (not used)

Detector setup:
bias -30V
MixedAlpha source in center

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.

The vacuum on the detector side went up from 2e-10 mbar to about 5e-9 mbar.
On the ring side it was 3e-11 mbar befor and 1e-10 mbar after movement.

The extreme positions possible (Endlage) are:

max out: -10613 
max in: -7

These are the absolute positions in units of 0.1 mm

It has to be noted that after bakeout a realignment of the detector was needed in order to have it centered in vertical dimension. However, this realignment has been only slight turns of the base flange alignment screws. In detail, the two inner "Sechskantschrauben" below the bellow have been loosed slightly, while the outer two have been tightend. Additionally, the small "Madenschraube" on the outside has been loosend by 1/4 turn.
In result the detector could be raised in vertical position by about ~5mm (jugded by eye).

The effect of small turning on the screws is extreme on the detector position! Be careful when re-adjusting.

To move the detector remotely from the HKR:
-go to a desktop of a HKR computer
-right click: "App Launcher PRO"
(-you have to give some password at this point?)
-within the program go to "Development->ProHelper"
-write the name of our slow control unit in the field Nomen: "GE01DD4AS"
-There are 4rows, the middle two called: "Read props", "Write props"

-In "Read props" open "rposiabss" -> if you hit here the refresh button it will show only the SET position
-In "Read props" open "rposiabsi" -> if you hit here the refresh button it will show the REAL-TIME position of the detector

-In "Write props" open "wposiabss" -> here you can set the absolute position of our detector (one click is already enough to execute the command).
 most OUT of the ring  position: -10613 [0.1mm] in absolute
 most IN into the ring  position: -7 [0.1mm] in absolute
 The value can have as big step size as we want contrary to relative movement, when you are limited to something like 20cm.

To close the program just simply hit the "x" buttons.

This is a brief how-to about getting the DSSSD set up with stored beam and target in the ESR.

The main goals
1. adjust timing signals to TDC-range
2. adjust energy signals to ADC-range
3. optimize energy resolution

The signal chain is the following:

det [32ch.] > preamp [2x16ch] > 2x MSCF shapers [16ch]

with these HV values the 6 channels are roughly gain matched, such that the 7.83 MeV Po-decay is around channel 5000.

https://docs.google.com/spreadsheets/d/14m8WcCq1erx6HqWJRK7TLbCx121IkjqGa5l-frf4YjI/edit#gid=0

To find a good Si position, we need to follow a procedure similar to this:

1. Si in max-in position
2. find distance of beam by scraping with detector from inside 
--> zero position
3. from this zero, we need to set a distance of about 1.5 cm to the inside (as shown in the sketch below)

It is likely that this position is not compatible with the complete ESR cycle (e.g. we scrape beam with det. during deceleration).
The solution is to move the beam closer to the detector after deceleration. There are two feasible methods to do this:

A. make a local bump in the dipole
--> check new zero and det. position again, as sketched above
--> in 2016 this method didn't allow to go close enough to the detector, eventually we used:

B. global orbit change (by magnet ramp) + target bump (to keep overlap)
--> this takes a bit more time to set up and also the cycle will be longer at low energies (critical due to life-time)
--> method A is preferred, but might not be strong enough

This needs to be checked and repeated for each new beam setting.

The BaF2 detectors planned to be installed at the target induce an additional background in the x-ray detectors sitting below inside the target chamber. 
We made test measurements with an x-ray detector for estimating the background in the region of interest for our K-REC measurements (35 to 50 keV).

For the interval [35-50 keV]:
Normal background level: 0.065 (s*keV)^-1
BaF2 in 5cm distance:    0.078 (s*keV)^-1
This is an increase by about 22%

Assuming an increase by 100% induced by 6 BaF2 in the vincinity of the Ge-detectors this seems acceptable.

However additional BaF-induced peaks are also visible at ~30 keV and ~60 keV. While these are not in the region of interest for the K-REC, we need to be aware of them!

spectra are available on the Frankfurt exp-astro Server at /home/glorius/e127/

• r4l-58 - VME cpu (RIO)
  our DAQ runs on this computer
  access from lxg1275 via ssh litv-exp@r4l-58
  the current DAQ directory is /esr/usr/litv-exp/2020_e127/r4l-58
  from lxg-machines the DAQ dir can also be accessed via the mount point at /lynx/Lynx/esr/usr/litv-exp/2020_e127/r4l-58
  
  
• lxg1275 - main DAQ handler
  used for communication with the DAQ and primary data writing/streaming
  access from any lxg via ssh litv-exp@lxg1275
  primary data folder: /data.local3/e127/lmd/
  local backup folder: /data.local2/e127/lmd_backup/
  
  
• lxg1299 - online monitoring
  used for the R3Broot online monitor server
  access from any lxg via ssh litv-exp@lxg1299
  online data: /data.local3/e127/online/
  
  
• atpnu004 - slow control
  used for remote access to SpecAmps (MesyTec Shapers), Si-HV (caen) and picoscopes
  access from any lxg via E127_nuc or ssh litv-exp@atpnuc004
  screen sessions: mesy_ioc (shapers), caen_ioc (Si HV)
  access screens by screen -x mesy_ioc or screen -x caen_ioc (exit with [Ctrl-a d])
  access vnc session for picoscopes on any lxg: E127_vnc or vncviewer atpnuc004:1
  
  
• apraspi001 - slow control 2
  used for remote access to the BaF HV crate
  access from any lxg via ssh litv-exp@apraspi001
  local access to HV control by telnet: telnet 169.254.93.160 1527
  
  
• lxg0188 - 1st backup node
  used for direct backup of the written data (invoked automatically by stopping a run)
  backup dir: /data.local2/E127_lmd/
  
  
• kronos.hpc.gsi.de - 2nd backup node
  used for secondary backup of lmd-data on lxg0188 (chronjob every 4 hours)
  backup dir: /lustre/ap/litv-exp/2020-03-17_E127_jglorius
  

• E127_daq or /data.local1/e127/scripts/E127_start_gui.sh
  this is the GUI to control the DAQ
  available on lxg1275 only with litv-exp user
  only one instance of this GUI can run at the same time!
  
  
• E127_unpack or /u/litv-exp/unpacker/unpackexps/e127/e127
  this is the unpacker for the current DAQ
  available on any lxg with litv-exp user
  to unpack lmd-files to root-file: E127_unpack infile01.lmd infile02.lmd --ntuple=RAW,outfile.root
  
  
• E127_epics or epicsfind; medm -x /u/litv-exp/e127/medm/e127.adl
  this is the GUI for slow control of Si HV and amplifiers (MesyTec Shapers)
  available on any lxg with litv-exp user
  
  
• E127_rates or /u/litv-exp/e127/UDP/build_cc_x86_64-linux-gnu_4.9.2_debug/udp_reader --trig --rate
  this is the UDP reader for detector and trigger rates
  available on lxg1275 only with litv-exp user
  
  
  
  
  
  

Here you can find the digital version of the E127 beam time manual.