Kaonic Atoms Research Workshop at Istituto Nazionale Fisica Nucleare

 
Strange Matter Workshop
Strangeness studies in Italy and Japan
 
Frascati, 16-17 / 10/ 2019
 
Istituto Nazionale Fisica Nucleare - Laboratori Nazionali di Frascati
 
Silicon Drift Detectors for
Kaonic atoms spectroscopy at DA
Φ
NE,
 SIDDHARTA-2 experiment
 
M. Miliucci
On behalf of SIDDHARTA-2 collaboration
 
Marco.Miliucci@lnf.infn.it
 
Frascati, 16/10/2019
 
Kaonic atoms physics at DA
Φ
NE
 
New Silicon Drift Detectors (SDDs) technology
for precision KD measurements
 
SDDs in DA
Φ
NE
 
Conclusions and outlooks
 
Frascati, 16/10/2019
 
Kaonic atoms physics at DA
Φ
NE
 
New Silicon Drift Detectors (SDDs) technology
for precision KD measurements
 
SDDs in DA
Φ
NE
 
Conclusions and outlooks
 
Frascati, 16/10/2019
 
 
Frascati, 16/10/2019
 
DA
Φ
NE
I.N.F.N.– Laboratori Nazionali di Frascati
Frascati, 19/12/2018
Φ 
 K
-
 K
+
 (49.1%)
Monochromatic low-energy K
-
 (~127 MeV/c ; 
Δ
p/p = 0.1%
)
Electromagnetic (
asynchronous
) bkg
Hadronic (syncronous) bkg 
Frascati, 16/10/2019
 
SIDDHARTA 2
 
MC Kaonic deuterium
 
KD yield < 0.1 %
(10 times lower than KH)
 Bazzi et al., Nuclear Physics A 907, 69-77 (2013)
 Bazzi et al., Nuclear Physics A 954, 7–16 (2016)
 
MC Kaonic deuterium
 
ε
 = -800 ± 
30
 eV
Γ = 750 ± 
75
 eV
 
density: 3% (LHD)
detector area: 246 cm
2
 
Same precision as SIDDHARTA,
which gave the most precise
measurement of KH so far
 
KD yield < 0.1 %
 
Frascati, 16/10/2019
 
Kaonic atoms physics at DA
Φ
NE
 
New Silicon Drift Detectors (SDDs) technology
for precision KD measurements
 
SDDs in DA
Φ
NE
 
Conclusions and outlooks
 
Frascati, 16/10/2019
 
[1] P. Rehak at al, Nucl. Instr. Meth. Phys. Res. A235, (1985)
Silicon Drift Chamber (SDC)
 
Frascati, 16/10/2019
 
[1]
 
[2]
3x1 array (SDD:1x1x0.045 cm
3
)
New technology SDD (FBK + PoliMi + LNF)
4x2 array (SDD:0.8x0.8x0.045 cm
3
)
Frascati, 16/10/2019
Linearity
Miliucci et al., Condens. Matter, 4(2) (2019)
Frascati, 16/10/2019
Ti
K
α
Fe
K
α
Cu
K
α
Br
K
α
 
Long time run
 
Ti-Br calibration
 
Fe K
α
 
: 6399.8 ± 0.4 eV
 
ΔE
mean
 = 0.2 ± 0.4 eV
 
Frascati, 16/10/2019
 
Miliucci et al., Condens. Matter, 4(2) (2019)
Energy resolution
        Voltage scan                                   Temperature scan
 
Miliucci et al., Condens. Matter, 4(2) (2019)
Frascati, 16/10/2019
Drift time (temperature scan)
µ: mobility ~ T
-n
Frascati, 16/10/2019
 
Kaonic atoms physics at DA
Φ
NE
 
New Silicon Drift Detectors (SDDs) technology
for precision KD measurements
 
SDDs in DA
Φ
NE
 
Conclusions and outlooks
 
Sharp & Succesfull SIDDHARTINO installation
(April 2019)
 
Frascati, 16/10/2019
SIDDHARTINO top view
He cooling
Frascati, 16/10/2019
 
Frascati, 16/10/2019
 
Frascati, 16/10/2019
 
X-ray tube (35kV,40uA)_SDD 107 ˩
 
Frascati, 16/10/2019
 
X-ray tube (35kV,40uA)_SDD 53 
//
 
Frascati, 16/10/2019
 
Ti
 
Cu
 
Bi
 
Zr
 
Pd
 
Ag
 
Frascati, 16/10/2019
 
Ti
Cu
Zr
 
Bi
Pd
Ag
 
Target
 
Ceramic
 
SDDs response during “DA
Φ
NE Commissioning’’
 
e+
 
/
 e- 
beams
Preliminary
 quantitative considerations
Background from the beam
Normal vs Parallel comparison
 
Frascati, 16/10/2019
 
X-ray tube (35kV,40uA)_SDD 107 ˩
 
Frascati, 16/10/2019
 
X-ray tube (35kV,40uA)_SDD 53 
//
 
Frascati, 16/10/2019
‘‘DA
Φ
NE commissioning’’ bakground
Energy (KeV)
Frascati, 16/10/2019
 
Kaonic atoms physics at DA
Φ
NE
 
New Silicon Drift Detectors (SDDs) technology
for precision KD measurements
 
SDDs in DA
Φ
NE
 
Conclusions and outlooks
 
Frascati, 16/10/2019
Frascati, 16/10/2019
Lab tests 
for 
optimization of new technology Silicon Drift Detectors
optimization of new technology Silicon Drift Detectors
for the SIDDHARTA-2 experiment
:
Linearity & Stabilty (≈eV);
Energy resolution (140 ~ 160 eV @ Mn K
α
)
Time resolution (< 400 ns @ Cu K
α
)
Preliminary 
e+/e- beam 
characterization of Silicon Drift Detectors
characterization of Silicon Drift Detectors
during the DA
Φ
NE commissioning:
Homogeneus background spread over the entire spectra
X-Rays emission of SDDs structural elements activated by the beam,
almost outside the ROI
No significative correlation between the beam direction and the
SDDs positioning
 
THANK YOU
 
Marco.Miliucci@lnf.infn.it
 
Working hard
 
Frascati, 16/10/2019
 
THANK
YOU
 
Frascati, 16/10/2019
 
Marco.Miliucci@lnf.infn.it
Slide Note
Embed
Share

Dive into the world of kaonic atoms physics and the latest advancements in Silicon Drift Detectors technology for precision measurements at the Istituto Nazionale Fisica Nucleare workshops held in Frascati, Italy. Explore the research conducted on strange matter and strangeness studies in Italy and Japan, focusing on the intricate interactions of kaonic atoms and the groundbreaking discoveries made in this field.

  • Kaonic Atoms
  • Physics Research
  • Silicon Drift Detectors
  • INFN Workshop
  • Frascati

Uploaded on Sep 14, 2024 | 0 Views


Download Presentation

Please find below an Image/Link to download the presentation.

The content on the website is provided AS IS for your information and personal use only. It may not be sold, licensed, or shared on other websites without obtaining consent from the author. Download presentation by click this link. If you encounter any issues during the download, it is possible that the publisher has removed the file from their server.

E N D

Presentation Transcript


  1. Istituto Nazionale Fisica Nucleare - Laboratori Nazionali di Frascati Strange Matter Workshop Strangeness studies in Italy and Japan Frascati, 16-17 / 10/ 2019

  2. Silicon Drift Detectors for Kaonic atoms spectroscopy at DA NE, SIDDHARTA-2 experiment M. Miliucci On behalf of SIDDHARTA-2 collaboration Marco.Miliucci@lnf.infn.it Frascati, 16/10/2019

  3. Outline Kaonic atoms physics at DA NE New Silicon Drift Detectors (SDDs) technology for precision KD measurements SDDs in DA NE Conclusions and outlooks Frascati, 16/10/2019

  4. Outline Kaonic atoms physics at DA NE New Silicon Drift Detectors (SDDs) technology for precision KD measurements SDDs in DA NE Conclusions and outlooks Frascati, 16/10/2019

  5. Cascade process strong interaction 1s , 1s KN interaction at threshold Frascati, 16/10/2019

  6. I.N.F.N. Laboratori Nazionali di Frascati ADA e ADONE K-K+(49.1%) Monochromatic low-energy K-(~127 MeV/c ; p/p = 0.1%) Electromagnetic (asynchronous) bkg Hadronic (syncronous) bkg ATLAS NAUTILUS SIDDHARTA Centro di Calcolo DA NE DA NE DAFNE-L BTF FISA FINUDA DEAR e+ e- Auditorium Frascati, 19/12/2018 Frascati, 16/10/2019

  7. KD yield < 0.1 % (10 times lower than KH) Bazzi et al., Nuclear Physics A 907, 69-77 (2013) Bazzi et al., Nuclear Physics A 954, 7 16 (2016) SIDDHARTA 2 MC Kaonic deuterium

  8. MC Kaonic deuterium KD yield < 0.1 % ? = 800?? 1 density: 3% (LHD) detector area: 246 cm2 = -800 30 = 750 75 30 eV 75 eV Same precision as SIDDHARTA, which gave the most precise measurement of KH so far Frascati, 16/10/2019

  9. Outline Kaonic atoms physics at DA NE New Silicon Drift Detectors (SDDs) technology for precision KD measurements SDDs in DA NE Conclusions and outlooks Frascati, 16/10/2019

  10. Silicon Drift Chamber (SDC) Silicon Drift Detector (SDD) RN Back [1] [2] Anode [1] P. Rehak at al, Nucl. Instr. Meth. Phys. Res. A235, (1985) Frascati, 16/10/2019 [2] C. Fiorini et al., IEEE transactions on nuclear science, 47(4) (2000)

  11. New technology SDD (FBK + PoliMi + LNF) SDD ramp & CUBE RESET X-Ray edge 100ns/div 640 s/div 3x1 array (SDD:1x1x0.045 cm3) 4x2 array (SDD:0.8x0.8x0.045 cm3) Frascati, 16/10/2019

  12. Linearity FeK BrK TiK CuK Frascati, 16/10/2019 Miliucci et al., Condens. Matter, 4(2) (2019)

  13. Long time run Ti-Br calibration Fe K : 6399.8 0.4 eV Emean = 0.2 0.4 eV Frascati, 16/10/2019 Miliucci et al., Condens. Matter, 4(2) (2019)

  14. Energy resolution Voltage scan Temperature scan FF = 0.118 0.009 FF = 0.116 0.009 Frascati, 16/10/2019 Miliucci et al., Condens. Matter, 4(2) (2019)

  15. Drift time (temperature scan) : mobility ~ T-n Frascati, 16/10/2019

  16. Outline Kaonic atoms physics at DA NE New Silicon Drift Detectors (SDDs) technology for precision KD measurements SDDs in DA NE Conclusions and outlooks

  17. Sharp & Succesfull SIDDHARTINO installation (April 2019) Frascati, 16/10/2019

  18. SIDDHARTINO top view He cooling SDDs+Veto 2 Beam direction Frascati, 16/10/2019

  19. Frascati, 16/10/2019

  20. Frascati, 16/10/2019

  21. X-ray tube (35kV,40uA)_SDD 107 Frascati, 16/10/2019

  22. X-ray tube (35kV,40uA)_SDD 53 // Frascati, 16/10/2019

  23. Zr Ti Cu Target Zr PdAg Bi Bi Ti Cu Pd Ceramic Ag Frascati, 16/10/2019

  24. SDDs response during DANE Commissioning e+ / e- beams Preliminary quantitative considerations Background from the beam Normal vs Parallel comparison Frascati, 16/10/2019

  25. X-ray tube (35kV,40uA)_SDD 107 Frascati, 16/10/2019

  26. X-ray tube (35kV,40uA)_SDD 53 // Frascati, 16/10/2019

  27. DANE commissioning bakground SDD 107 (normal w.r.t. beam) SDD 53 (parallel w.r.t beam) SDD 107 SDD 53 Frascati, 16/10/2019 Energy (KeV)

  28. Outline Kaonic atoms physics at DA NE New Silicon Drift Detectors (SDDs) technology for precision KD measurements SDDs in DA NE Conclusions and outlooks Frascati, 16/10/2019

  29. Lab tests for optimization of new technology Silicon Drift Detectors for the SIDDHARTA-2 experiment: Linearity & Stabilty ( eV); Energy resolution (140 ~ 160 eV @ Mn K ) Time resolution (< 400 ns @ Cu K ) Preliminary e+/e- beam characterization of Silicon Drift Detectors during the DA NE commissioning: Homogeneus background spread over the entire spectra X-Rays emission of SDDs structural elements activated by the beam, almost outside the ROI No significative correlation between the beam direction and the SDDs positioning Frascati, 16/10/2019

  30. Working hard THANK YOU Marco.Miliucci@lnf.infn.it Frascati, 16/10/2019

  31. THANK YOU Marco.Miliucci@lnf.infn.it Frascati, 16/10/2019

More Related Content

giItT1WQy@!-/#giItT1WQy@!-/#giItT1WQy@!-/#giItT1WQy@!-/#giItT1WQy@!-/#giItT1WQy@!-/#giItT1WQy@!-/#giItT1WQy@!-/#giItT1WQy@!-/#giItT1WQy@!-/#