AIDA GELINA BRIKEN nToF CRIB ISOLDE CIRCE nTOFCapture DESPEC DTAS EDI_PSA 179Ta CARME StellarModelling DCF K40
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  ID Date Author Subject
  82   Tue Mar 18 13:28:30 2025 EmmanuelB10 and LiF data with Fast Fourier Transform

Attached is the B10 and LiF data with Fast Fourier Transform and varying time constants.

  81   Wed Feb 12 13:51:02 2025 CLWexpected counts B and Li

The rootfiles countsB.root and countsLi.root contain histograms of count spectra that would be expected at n_TOF for a 10B and a 6Li target, respectively. The units in y are arbitrary. This can be used to check, if we can reproduce the expected trend with our Li and B measurements. So the histograms called "counts" can be directly compared to the histograms called "energy" in Sili_deed.c (they should have the same binning). You need to scale the histogram to get a decent overlap. You can use this also to estimate the neutron energy calibration - the thermal bump at low energy will give you a good idea of the flight path length. Structure at high energy will give you a better idea on the offset.

The files 6Li_endf.root and 10B_endf.root are the original cross section files, and countrate_calc.C is the file used to produce the count spectra.

 

  80   Mon Sep 16 12:36:45 2024 TD34-way IDC to 37-way D connector ribbon cables
The 2x sets of 34-way IDC to 37-way D connctor ribbon cables used at GSI for the two-alpha decay measurement have been located - see attachments 1-4.

They have been packed for shipment to CERN and delivered to stores for shipment. Awaiting quotation and P&M PO.
  79   Sat Sep 14 09:30:40 2024 TDNeutron beam profile
Neutron beam profile - film exposure overnight 12/13.9.24
  78   Thu Sep 12 15:26:30 2024 NickEAR2 Periodic Noise
  76   Thu Sep 12 11:07:29 2024 Nick40K Borrowed Items

We borrowed from n_TOF:

1x O-ring for circular side-flanges on the chamber (the borrowed part has a small green marker cross on it)

10x LIMO-to-BNC connectors (BNC female) from electronics lab outside EAR1

  74   Tue Apr 16 12:24:01 2024 EmmanuelMWD amplitude (dE and E)
  73   Mon Mar 25 12:57:30 2024 ClwAdapters for ntof setup

10 new Adapters for lemo to bnc on my desk

  72   Thu Dec 7 09:48:23 2023 EmmanuelMWDdetector and User Input

MWDdetector and UserInput

  71   Mon Oct 2 08:53:06 2023 EmmanuelEmpty Frame

An empty frame (on the top) was placed on Friday night.

  70   Thu Sep 28 15:32:16 2023 EmmanuelLiF sample in

We switched from 10B target (number 1) to LiF target (number 3). We planned to take this measurement for one day.

  69   Wed Sep 27 09:54:06 2023 Emmanuel10B sample in

We switched from Aluminium target to Boron Target (number 1) on Tuesday (26th of Sept.). The Aluminium target was placed in the material room by the RP. We will change to LiF (number 3) on Thursday (28th of Sept.)

  68   Tue Sep 5 16:09:45 2023 EmmanuelDrop in gain for DEED 14

Dear all,

There was an issue with one of the strips of the deltaE detector (DEED 14), for run216644. The gain dropped to almost a factor of 3. Find attached.

Somehow, it was fixed, but still lags, when compared to other strips of deltaE. This was tested for a more recent run, run216651. Find attached.

I also checked a bit older run (run216637) and they look similar.. Find attached. Maybe we should figure out if this will be a problem for the DEED14 strips.

 

NOTE: The plots have the run number at the top-center.

 

Emmanuel Odusina

 

 

  67   Mon Aug 21 12:08:59 2023 TDRAL108 +/-15V PSU test - JCMB 21.8.23
PSU Calex

Setup, PSU and ac mains filter - attachments 1-3


DSO ch#1 +15V AC/1M, ch#2 -15V AC/1M - y: 50mV/div x: 100ns, 200ns, 1us, 2us, 10us/div

Without ac mains filter - attachments 4-8



DSO ch#1 +15V AC/1M, ch#2 -15V AC/1M - y: 10mV/div x: 100ns, 200ns, 1us, 2us, 10us/div

With ac mains filter - attachments 9-13

Conclusion - Claud Lyons Ltd STF Series Surge & Transient Power Filter produces c. x 2 attenuation of HF noise transients
  66   Sat Aug 19 14:14:26 2023 TDRAL108 +/-15V PSU test - JCMB 18.8.23
PSU Calex

Setup and PSU details - attachments 1-3

DSO ch#1 +15V AC/1M, ch#2 -15V AC/1M - y: 20mV/div x: 100ns, 200ns, 1us, 2us, 10us, 20us & 100us/div - attachments 4-10
  65   Thu Aug 17 10:26:51 2023 Nikolay SosninData Processing

To run raw2root on LXPLUS, you will need to add the following line to your .bashrc, performed using

gedit ~/.bashrc &

then paste line at the bottome of the file

export LD_LIBRARY_PATH=$LD_LIBRARY_PATH:/afs/cern.ch/user/n/ntofuser/public

then save and close the gedit (a linux text editor similar to Windows Notepad). Text file .bashrc is responsible for setting correct paths to various system settings when you log in. The line above sets correct libraries for raw2root from the n_TOF official directories.

 

The old version of raw2root which I use is stored in a directory on EOS accessible via LXPLUS:

cd /eos/home-n/nsosnin/public/raw2root

If you examine the contents of the directory using command ls, there will be two folders: ntoflib and prg. The relative location of these folders on your system should always be the same, and you do not need to do anything in the ntoflib directory, so we can explore the next directory

cd prg && ls

Command cd means change directory and ls is list contents, double-& chains commands in a sequence. Your terminal should now display two more directories: detector and raw2root. detector is a list of codes for various detector types, examine its contents with ls detector. We use MWDdetector.cc and its library header file MWDdetector.h. All the filters are defined and can be changed in MWDdetector.cc, which is a C++ code. You can browse and change its contents with gedit. raw2root codes, however, are run from the raw2root directory, so let's change to it

cd raw2root && ls

When you list the contents of this directory there will be many files, none of which you need to edit. There will also be a directory called Traces, which I created as the default location for signal traces to be written, if relevant sections of MWDdetector.cc are uncommented (discussed below). If you are happy with the contents of MWDdetector.cc, you need to re-compile raw2root. Using C++ code, unlike some others, is a two-step process: compilation and execution. Various bits of code in raw2root and its libraries are put together into one executable file called raw2root during compilation stage, and then the code can be run by executing the executable. To compile raw2root, you need to be in its directory, which you can check by typing in

pwd

which should then display /eos/home-n/nsosnin/public/raw2root/prg/raw2root and if you it displays something else, use

cd /eos/home-n/nsosnin/public/raw2root/prg/raw2root

To compile raw2root in this directory use

make clean && make proper && make

The code will start compiling and do so for a while. It will display some warnings associated with other older n_TOF codes. There should, however, be no errors. If there are errors, something went wrong in MWDdetector.cc, so try troubleshooting it by Googling the errors (the line with the error will also display two numbers, something like error: MWDdetector.cc:1211:45, and the the second number is the line where the problem occurred). C++ errors are a dark art though, so feel free to contact me for help.

If the compilation displays no errors (woo!), the code compiled successfully. To test it, two things are needed: UserInput file and .raw.finished file. UserInput file called UserInput_Silicons.h, which I use, is already stored in that directory. If you examine it with gedit, you will see lines with detector names and numbers and the filtering parameters. The parameters are read in at the top of MWDdetector.cc in order, so you can follow the variables they are read into throughout the code to figure out which parameter does what (this is not an easy task!).

.raw.finished files are binary data files with detector signal traces, which raw2root filters and makes into ROOT files. These need to be downloaded from CERN servers (I left two example ones in the directory though). While the experiment is running these are stored, but will eventually be deleted, so if they don't download, contact me on staging data (i.e. writing it onto servers again after deletion). To download such a binary file for this experiment to the directory you are in use

xrdcp xroot://eosctapublicdisk.cern.ch//eos/ctapublicdisk/archive/ntof/2023/EAR2/26Al_DSSSD/216408/stream1/run216408_1_s1.raw.finished .

Here, xrdcp command is CERN's own copying command, which takes data from the directory listed in the command. I have highlighted above in yellow the bits you may need to change in the command. The first two are simply run number. The last one is the data segment. n_TOF data within a run are subdivided into 20 proton bunch segments, so one such .raw.finished file that you download contains 20 bunches (which is a very small amount of data, so if you need mass_processing, contact me or Fran (francisco.garcia.infantes@cern.ch) at n_TOF). You can download different segments by changing this number. Bunches 1-20 are in segment 0, bunches 21-40 in segment 1, etc.

Once you have downloaded the file of interest execute raw2root with command

./raw2root -p UserInput_Silicons.h -f run216408_1_s1.raw.finished -r rootout.root

This will run for some time, applying settings from UserInput to filters in MWDdetector.cc, and running the filters over data in the .raw.finished file. This will produce an output file called rootout.root, but feel free to change the name in the command to whatever you like, otherwise you will just keep overwriting the old files. This output file will have the amplitudes, times etc. of all the extracted signals listed, but it will not produce traces, as that is not standard raw2root functionality, and requires my code, which I added to MWDdetector.cc

To print traces, open MWDdetector.cc using

gedit ../detector/MWDdetector.cc &

Note, ".." on Linux means "previous directory", so the command above will leave raw2root directory, go to detector directory and open the code. In this code, uncomment (i.e. remove // or /* or */ characters in C++) from lines 310-312, 441, 442, 465 and 529. This will now print trace ROOT files into the Traces directory. Warning: this runs very slowly, as it's a lot of data being written to disk!

The if() statment on line 465 allows you to gate on specific bunches and detectors for producing traces. The contents of histograms inside the output files can be understood in terms of what MWDdetector.cc does by reading the lines 514-522 of that code. This should be everything you need to get started with processing traces and filtering outputs. Good luck!

  64   Tue Aug 15 11:41:27 2023 TD, NSMonday 14 August - vacuum chamber pressure
08.35 Vacuum chamber pressure OK - see attachment 1
  63   Tue Aug 15 10:17:39 2023 TD, NSRAL108 +/-15V PSU test at EAR2, n_TOF Monday 14 August
On the morning of Monday 14 August 2x RAL108 +/-15V PSUs were borrowed from the Edinburgh equipment in the ISOLDE hall to check whether the same transient 
noise is observed at the +/-15V PSU outputs.


PSU #2 Farnell MX2

Setup - attachment 1

DSO ch#1 +15V AC/1M, ch#2 -15V AC/1M - y: 50mV/div x: 1us, 500ns, 250ns & 25us/div - attachments 2-5



PSU #1 Coutant HSC15-3.0

Setup - attachment 6

DSO ch#1 +15V AC/1M, ch#2 -15V AC/1M - y: 50mV/div x: 25us/div - attachment 7


Conclusion

Observe same amplitude and HF structure with all 3x RAL108 +/-15V PSUs
  62   Mon Aug 14 11:00:13 2023 TDRAL108 +/-15V PSU test in ISOLDE hall
This morning 2x RAL108 +/-15V PSUs were borrowed from the Edinburgh equipment in the ISOLDE hall to check whether the same transient noise is observed at the +/-15V PSU 
outputs - this was confirmed. See https://elog.ph.ed.ac.uk/nToF/63

Following this test the same 2x RAL108 +/-15V PSUs were tested in the ISOLDE hall ( 19" rack adjacent to the HIE-ISOLDE GP scattering chamber ). 


PSU #1 Coutant HSC15-3.0

Setup and PSU details - attachments 1-4

DSO ch#1 +15V AC/1M, ch#2 -15V AC/1M - y: 5mV/div x: 400ns, 4us & 40us/div - attachments 5-7


PSU #2 Farnell MX2

Setup and PSU details - attachments 8-10

DSO ch#1 +15V AC/1M, ch#2 -15V AC/1M - y: 5mV/div x: 400ns, 4us & 40us/div - attachments 11-13


Conclusion 

The noise of the 2x RAL108 +/-15V PSUs differed somewhat ( frequency and structure of HF transients ) from each other in the ISOLDE test.

Compared to the EAR2, n_TOF test the amplitudes were c. 10x smaller and the HF transient frequency and structure differed.

This appears to confirm that the primary problem is the ac mains power in EAR2, n_TOF - input and/or output filtering is required.
  61   Sat Aug 12 09:24:19 2023 Nikolay Sosnin26Al Protons

Here is a Google spreadsheet for counting protons for the runs:

https://docs.google.com/spreadsheets/d/1INX8G9GAu-M70SdZdz55qXnMZNXKXLW7xfFH-eaLuQw/edit?usp=sharing

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