|
1.
|
|
|
Recent advances and perspectives of the high precision laser metrology
/ Batusov, V (Dubna, JINR) ; Budagov, J (Dubna, JINR) ; Glagolev, V (Dubna, JINR) ; Lyablin, M (Dubna, JINR) ; Shirkov, G (Dubna, JINR) ; Gayde, J Ch (CERN) ; Di Girolamo, B (CERN) ; Mainaud Durand, H (CERN) ; Mergelkuhl, D (CERN) ; Nessi, M (CERN) et al.
The laser-based metrology presents new means and opens possibilities in solving
tasks where achievement of a high precision survey is of the principal signiˇcance
necessity.
The extended laser ˇducial line (coordinate axis) is necessary for precision
alignment of basic structure units of large-scale accelerators, for precision assembly
of subdetectors when mounting large spectrometric complexes, for online control of
space stability of particle detectors during the data taking period.
The high sensitivity laser inclinometers open the new possibilities for ground
motion control and for accelerator (collider) beam space stabilization essential for
achievement of stable high intensity (luminosity) at the interaction area.
The investigation has been performed at the Dzhelepov Laboratory of Nuclear
Problems, JINR..
E13-2014-21.
-
2014. - 17 p.
Fulltext
|
|
|
2.
|
The precision laser inclinometer long-term measurement in thermo-stabilized conditions (First Experimental Data)
/ Azaryan, N (Dubna, JINR) ; Batusov, V (Dubna, JINR) ; Budagov, J (Dubna, JINR) ; Glagolev, V (Dubna, JINR) ; Lyablin, M (Dubna, JINR) ; Trubnikov, G (Dubna, JINR) ; Shirkov, G (Dubna, JINR) ; Gayde, J -Ch (CERN) ; Di Girolamo, B (CERN) ; Mergelkuhl, D (CERN) et al.
The Precision Laser Inclinometer was tested at thermo-stabilized conditions and the ground angular stability of 1 μrad (observation during 24 h) and 7nrad (observation during 60 min) was measured..
Springer, 2015 - 4 p.
- Published in : Phys. Part. Nucl. Lett. 12 (2015) 532-535
|
|
|
3.
|
The ATLAS Detector Positioning System (ADEPO) to Control Moving Parts During ATLAS Closure
/ Gayde, J -C (CERN) ; Mergelkhul, D (CERN) ; Raymond, M (CERN) ; Dönszelmann, M (Nijmegen U.) ; Daakir, M (Paris-Est U.) ; Batusov, V (Dubna, JINR)
ATLAS is one of two general-purpose detectors at CERN’s Large Hadron Collider (LHC). It is 46 m long, 25 m wide and 25 m in height and has a total mass of 7000 tons. [...]
2016 - 6 p.
- Published in : (2016)
Fulltext: PDF;
In : International Workshop on Accelerator Alignment, Grenoble, France, 3 - 7 Oct 2016
|
|
|
4.
|
Comparative analysis of earthquakes data recorded by the innovative Precision Laser Inclinometer instruments and the classic Hydrostatic Level System
/ Azaryan, N (Dubna, JINR) ; Batusov, V (Dubna, JINR) ; Budagov, J (Dubna, JINR) ; Glagolev, V (Dubna, JINR) ; Lyablin, M (Dubna, JINR) ; Trubnikov, G (Dubna, JINR) ; Shirkov, G (Dubna, JINR) ; Gayde, J -Ch (CERN) ; Di Girolamo, B (CERN) ; Herty, A (CERN) et al.
The Hydrostatic Level System (HLS) data and the Precision Laser Inclinometer (PLI) instruments data have been comparatively analyzed in the event of surface angular oscillations induced by earthquakes. The comparative data analysis has shown an agreement on the arrival and stop time of earthquakes. [...]
2017 - 13 p.
- Published in : Phys. Part. Nucl. Lett. 14 (2017) 480-492
|
|
|
5.
|
The laser reference line method and its comparison to a total station in an ATLAS like configuration
/ Batusov, V (Dubna, JINR) ; Budagov, J (Dubna, JINR) ; Lyablin, M (Dubna, JINR) ; Gayde, J -Ch (CERN) ; Girolamo, B (CERN) ; Mergelkuhl, D (CERN) ; Nessi, M (CERN)
A new type of measuring system, the Laser Reference Line, is proposed as a metrological tool and can be used within limited space to ensure a precise installation along an axis on the ATLAS interaction point. A simplified ATLAS like beam pipe mock-up is used for this test. [...]
2014 - 10 p.
- Published in : Phys. Part. Nucl. Lett. 11 (2014) 299-308
|
|
|
6.
|
|
|
7.
|
The calibration of the Precision Laser Inclinometer
/ Batusov, V (Dubna, JINR) ; Budagov, J (Dubna, JINR) ; Lyablin, M (Dubna, JINR) ; Shirkov, G (Dubna, JINR) ; Gayde, J -Ch (CERN) ; Mergelkuhl, D (CERN)
The calibration methods of the two-coordinate Precision Laser Inclinometer are presented. For the inclinometer studied sample of the, the calibration coefficients 630 ± 70 and 531 ± 66 μrad/V have been determined by two independent methods..
2015 - 5 p.
- Published in : Phys. Part. Nucl. Lett. 12 (2015) 819-823
- Published in : Phys. Elem. Part. At. Nucl. Lett.: 12 (2015) , no. 7, pp. 1272-1278
|
|
|
8.
|
The sensitivity limitation by the recording ADC to Laser Fiducial Line and Precision Laser Inclinometer
/ Batusov, V (Dubna, JINR) ; Budagov, J (Dubna, JINR) ; Lyablin, M (Dubna, JINR) ; Shirkov, G (Dubna, JINR) ; Gayde, J-Ch (CERN) ; Mergelkuhl, D (CERN)
For metrology set-ups using a laser beam (The Laser Fiducial Line, the Precision Laser Inclinometer) the recording noise has been determined. This noise is limiting the measurement precision of the beam displacement Δx and consequently the precision Δψ of measurement of the beam inclination angle. [...]
2015 - 6 p.
- Published in : Phys. Part. Nucl. Lett. 12 (2015) 813-818
- Published in : Phys. Elem. Part. At. Nucl. Lett.: 12 (2015) , no. 7, pp. 1264-1271
|
|
|
9.
|
Mechanical construction and installation of the ATLAS tile calorimeter
/ Abdallah, J. (Valencia U., IFIC) ; Adragna, P (INFN, Pisa ; Pisa U.) ; Alexa, C (Bucharest, IFIN-HH) ; Alves, R (LIP, Coimbra ; Coimbra U.) ; Amaral, P (CERN ; LIP, Lisbon ; Lisbon U.) ; Ananiev, A (LIP, Lisbon) ; Anderson, K (Illinois U., Chicago) ; Andresen, X (CERN ; LIP, Lisbon ; Lisbon U.) ; Antonaki, A (Athens U.) ; Batusov, V (Dubna, JINR) et al.
/ATLAS Tile Calorimeter Community
This paper summarises the mechanical construction andinstallation of the Tile Calorimeter for the ATLASexperiment at the Large Hadron Collider in CERN, Switzerland. The TileCalorimeter is a sampling calorimeter using scintillator as the sensitivedetector and steel as the absorber and covers the central region of the ATLASexperiment up to pseudorapidities ±1.7. [...]
2013 - 27 p.
- Published in : JINST 8 (2013) T11001
IOP Open Access article: PDF;
|
|
|
10.
|
|