1 / 23

Tentative polarized solid Targets for CERN Projects

Tentative polarized solid Targets for CERN Projects. Fall meeting of the GDR PH-QCD 18 – 21 October 2011, IPN Orsay. Technical Constraints - Beam - Target - FoM.

irish
Download Presentation

Tentative polarized solid Targets for CERN Projects

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript

  1. Tentative polarized solid Targets for CERN Projects Fall meeting of the GDR PH-QCD 18 – 21 October 2011, IPN Orsay Technical Constraints - Beam - Target - FoM Dynamic Polarization - Principle - Frozen Spin Targets - NMR Static Polarization - Principle - HD Polarization Dynamic Polarization of HD for Hadron Physics From HD to DT for future “Fusion Power Plants” J-P DIDELEZ

  2. Target heating and damages Compass 50 µW 15 mK 1 nA = ±1 mW = ±10E10 p/s 5×10E8 p/s = ± 50 µW Limit before damages ±10E15 p/cm2 Run duration < 23 days

  3. HD radiation 0.30 moderate ?

  4. Figure of Merit (FoM) FoM = ρ k (f P) 2 t -1~ ρ k (f P) 2 ρstands for the density of the material k corresponds to the ratio of the volume occupied by the material to the volume of the target cell f is the dilution factor BUTANOL C4H9OH H H H H H – C – C – C – C – O – H H H H H f = 1 if free protons can be identified f = 1/4.2 if target protons can be identified f = 1/7.4 if target nucleons cannot be identified AFTER HD 0.14 H :~0.9 D :~0.3 0.95 0.95 12 12.8 9.3 28.9 30.00

  5. Dynamic Nuclear Polarization (DNP) T = 1 K

  6. COMPASS 6LiD Polarized Target Since 2011, NH3 is used as polarization material.

  7. Polarization measurement by NMR NH3 ND3 ΔP/P = 3% ΔP/P = 8%

  8. Static Polarization of HD B/T > 1500 Dilution Refrigerator 10 mK and 17 T (B/T = 1700)

  9. Dynamic Polarization of HD IDEAL Target 70 K Shield Liquid 4He (4.2 K) Saddle coils Micro Wave PolarizedHD or D2 NMR Coils Liquid 3He (0.5 K) Solenoid Coil

  10. Inertial Fusion induced by Laser, Gain = Efus /Ein Mauro TEMPORAL DTCS G = 0.05 DTCS × 2 G = 76 Polarized DTCS = DTCS × 1.5 → G = 4

  11. Conclusions • Several polarized targets could be used for • future CERN projects. - The best FoM is obtained with 6LiD or HD material. - Static polarization of HD is still problematic (TJNaF, Spring-8) - Dynamic polarization of HD should be revisited for Hadronic Physics fundamental research Thermonuclear Fusion power plants THE REAL PROBLEM IS TO FIND A GOOD TEAM TO BUILD A POLARIZED TARGET !

  12. Evolution du Temps de Relaxation Spin-Réseau Des Protons en fonction du vieillissement du HD

  13. HYDILE Target 70 K Shield Liquid 4He (4.2 K) Saddle coils Al Wires PolarizedHD NMR Coils Liquid 3He (0.5 K) Solenoid Coil

  14. HYDILE

  15. Proton NMR Signal 0.016 0.014 0.012 0.01 0.008 Signal (Volt) 0.006 0.004 0.002 0 41.78 41.8 41.82 41.84 41.86 41.88 41.9 41.92 -0.002 -0.004 -0.006 Frequency (MHz)

  16. Dispositif de Distillation Suivi des concentrations Spectromètre de masse quadripolaire Résultat de la distillation Colonne de distillation Distillateur DNP = Échantillon pour la polarisation dynamique Statique = Échantillon pour la polarisation statique

  17. HD Target: NMR Measurements Field = 0.85 T – Temperature = 1.8 K Sample 1 [H2] = 2.0 10-4 [D2] = 1.7 10-3 Sample 2 [H2] = 6 10-4 [D2] = 9.0 10-4 T1D T1D Back conversion at room temp. for 5 hours is 30% T1H T1H Temps de Relaxation du HD distillé en fonction des concentrations en ortho-H2

More Related