A critical review of experiments on deuterium retention in displacement-damaged tungsten as function of damaging dose
T Schwarz-Selinger
Abstract:Experimental results from the literature on the evolution of deuterium retention in displacement-damaged tungsten as a function of damaging dose are presented. Except for a few outliers, retention is generally found to increase with the presence of displacement damage. However, total retention results scatter by three orders of magnitude for similar exposure temperatures and are difficult to compare, because they depend on experiment-specific parameters such as the irradiation energy used to produce the displa… Show more
“…There is little literature regarding Li-D co-depositions in a D plasma environment and with in-situ diagnostics. Tabares et al [16] exposed tungsten plates to lithium-seeded deuterium plasma at temperatures between 130 • C-600 • C. The measured Li and D content were below the NRA detection limit, for all but one case, at 130 • C. In this case the D/Li ratio was less than 10 −4 , which is similar to retention rates of D in W at this temperature [17]. Krat et al [18] conducted magnetron sputtering with D 2 onto a Li target, capturing both D and Li on a molybdenum substrate.…”
The vapor-box is a liquid metal based design to cope with the demanding conditions of the divertor. This design relies on the recirculation of lithium by evaporation and condensation. An issue to this approach is the safety risks of Li-D/T formation and co-deposition on both the vapor-box walls - leading to possible recirculation impedance- and on the first wall leading to unacceptable tritium retention. Additively manufactured tungsten Capillary Porous Structure (CPS) samples filled with Li were exposed to high heat flux D plasmas in the linear plasma device Magnum-PSI and Li-D co-deposition was measured as a function of substrate temperature, estimated to be in the range 200-428 ${^\circ}$C and distance between 25-85 mm to the plasma beam center. The D:Li ratio was determined via in-situ ion beam diagnostics (NRA and EBS) and the spectra analyzed simultaneously to maximise the precision of the measurement. The experimental results approach close to the theoretical maximum at 40:60 D:Li ratio and the thickness of the deposited films was 0.02 - 3.2 $\mu$m. For witness plate temperatures above 400 ${^\circ}$C Li films under 150 nm in thickness were deposited and show lower D:Li ratios, as low as 5:95 D:Li ratio. At these temperatures the evaporation rate from the WPs is close to the deposition rate, and the decomposition pressure for LiD becomes comparable to the operational pressure in the vessel during the discharge. SOLPS-ITER simulations were also conducted to complement the experimental data. The results were used to narrow the range of CPS surface temperature to between $650-700$^{\circ}$C and determined that the D$^{+}$ plasma is largely replaced by Li$^{+}$ plasma close to the target surface. Further, the redeposition ratio of the lithium on the CPS surface is determined to be around 80$\%$, which matches well with the value determined from a quartz crystal microbalance. Due to limitations in the modeling of neutral interactions with Li coated surfaces, the SOLPS-ITER modeling does not well recreate the observed Li and D deposition layers on the WPs, indicating that this aspect of the modeling in Eirene needs improvement to accurately model plasmas containing significant quantities of Li. However, SOLPS-ITER simulations should be extended to include LiD molecules and improve the accuracy of heat flux towards the target to improve the comparison with experimental data.
“…There is little literature regarding Li-D co-depositions in a D plasma environment and with in-situ diagnostics. Tabares et al [16] exposed tungsten plates to lithium-seeded deuterium plasma at temperatures between 130 • C-600 • C. The measured Li and D content were below the NRA detection limit, for all but one case, at 130 • C. In this case the D/Li ratio was less than 10 −4 , which is similar to retention rates of D in W at this temperature [17]. Krat et al [18] conducted magnetron sputtering with D 2 onto a Li target, capturing both D and Li on a molybdenum substrate.…”
The vapor-box is a liquid metal based design to cope with the demanding conditions of the divertor. This design relies on the recirculation of lithium by evaporation and condensation. An issue to this approach is the safety risks of Li-D/T formation and co-deposition on both the vapor-box walls - leading to possible recirculation impedance- and on the first wall leading to unacceptable tritium retention. Additively manufactured tungsten Capillary Porous Structure (CPS) samples filled with Li were exposed to high heat flux D plasmas in the linear plasma device Magnum-PSI and Li-D co-deposition was measured as a function of substrate temperature, estimated to be in the range 200-428 ${^\circ}$C and distance between 25-85 mm to the plasma beam center. The D:Li ratio was determined via in-situ ion beam diagnostics (NRA and EBS) and the spectra analyzed simultaneously to maximise the precision of the measurement. The experimental results approach close to the theoretical maximum at 40:60 D:Li ratio and the thickness of the deposited films was 0.02 - 3.2 $\mu$m. For witness plate temperatures above 400 ${^\circ}$C Li films under 150 nm in thickness were deposited and show lower D:Li ratios, as low as 5:95 D:Li ratio. At these temperatures the evaporation rate from the WPs is close to the deposition rate, and the decomposition pressure for LiD becomes comparable to the operational pressure in the vessel during the discharge. SOLPS-ITER simulations were also conducted to complement the experimental data. The results were used to narrow the range of CPS surface temperature to between $650-700$^{\circ}$C and determined that the D$^{+}$ plasma is largely replaced by Li$^{+}$ plasma close to the target surface. Further, the redeposition ratio of the lithium on the CPS surface is determined to be around 80$\%$, which matches well with the value determined from a quartz crystal microbalance. Due to limitations in the modeling of neutral interactions with Li coated surfaces, the SOLPS-ITER modeling does not well recreate the observed Li and D deposition layers on the WPs, indicating that this aspect of the modeling in Eirene needs improvement to accurately model plasmas containing significant quantities of Li. However, SOLPS-ITER simulations should be extended to include LiD molecules and improve the accuracy of heat flux towards the target to improve the comparison with experimental data.
“…Data from the work of Pec ˇovnik et al [11] has been used to evaluate the annealing parameters (A 0 and E A ). To evaluate the damaging parameters (K and n max,Φ ), unpublished data from T. Schwarz-Selinger was used that was generated following the procedure outlined in [31].…”
Section: Damaged Induced Trap Model Definitionmentioning
A damage-induced hydrogen trap creation model is proposed, and parameters for tungsten are identified using experimental data. The methodology for obtaining these parameters using thermo-desorption analysis spectra data is outlined. Self-damaged and optionally annealed tungsten samples have undergone TDS analysis, which has been analysed to identify the properties of extrinsic traps induced by the damage and to determine how they evolve with damage and annealing temperature. A parametric study investigated the impact of the damage rate and temperature on tritium inventories in tungsten. Tritium transport simulations have been performed with FESTIM considering a 1D model of a 2 mm sample of tungsten with damage rates and temperatures varying from 0–
10
2
dpa/fpy and 600–1300 K, respectively. The results show that after 24 h simultaneous exposure to neutron damage at
10
2
dpa/FPY and tritium implantation at 700 K, tritium inventories can increase by up to four orders of magnitude when damaged at a rate of
10
2
dpa/FPY compared to undamaged, defect-free tungsten, increasing further to five orders of magnitude after one full power year. The time taken to reach retention saturation shows the need for kinetic models of trapping properties on time scales relevant to reactor operation. The trap-creation model parameterisation procedure can be used to investigate neutron damage effects on other fusion-relevant materials such as EUROFER, Inconel and more.
“…11,12 Furthermore, the research on the retention of hydrogen and isotopes on the surface holds significant potential for nuclear fusion energy. 13,14 Tokamak reactors commonly employ hydrogen and isotopes as fuel sources, and the interaction of these species in the plasma state on the inner walls of the reactor has garnered significant attention in current studies. 15−18 Moreover, hydrogen storage assisted by plasma has garnered attention from several research groups.…”
Section: Introductionmentioning
confidence: 99%
“…H 2 and D 2 are commonly applied to passivate Si substrates in the microelectronic industry to prevent contamination, such as H 2 O, which is present in the base pressure of standard vacuum vessels. − Additionally, passivation finds various applications in thin film technologies, serving as anticorrosive protection and interface functionalization and creating hard coatings. − Passivation of dangling bonds is crucial in hydrogenated amorphous silicon materials. , Furthermore, the research on the retention of hydrogen and isotopes on the surface holds significant potential for nuclear fusion energy. , Tokamak reactors commonly employ hydrogen and isotopes as fuel sources, and the interaction of these species in the plasma state on the inner walls of the reactor has garnered significant attention in current studies. − Moreover, hydrogen storage assisted by plasma has garnered attention from several research groups. , To control the physical–chemical mechanisms of passivation, factors like the surface state, temperature, and sticking coefficient must be taken into consideration. − …”
This study presents a comparison of H 2 and D 2 passivation on Si(100) under simultaneous Xe + ion bombardment. The impact of Xe + ions causes significant damage to the substrate surface, leading to an increase in H 2 (D 2 ) retention as Si−H (Si−D) bonds. The ion bombardment conditions are precisely controlled using a Kaufman ion gun. The atomic concentrations on the surface of the sample were investigated by quasi-in situ X-ray photoelectron spectroscopy. A simple methodology is employed to estimate the H (D) chemical concentration and the cover ratio of the sample, with regard to the oxygen concentration through residual water chemisorption present in the vacuum vessel. Differences in passivation are expected when using H 2 or D 2 atmospheres because their retained scission energies and physisorption properties differ. The results indicate an increase of the sticking coefficient for D 2 and H 2 under the ion bombardment. It is also found that the flux of H 2 (D 2 ) impinging on the surface contributes to play an important role in the whole process. Finally, a model is proposed to describe the phenomenon of the passivation of Si under Xe + ion bombardment in the presence of H 2 (D 2 ).
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