“…e plasma state has been diagnosed by Kuznetsov, and in our experiment, the plasma state can be determined by the initial gas pressure and discharge voltage based on the results presented in [38]. e initial energy loss ΔE for 100 and 90 keV protons was measured to be 5.02 and 7.73 keV before discharge.…”
Section: Resultsmentioning
confidence: 92%
“…Laser and Particle Beams degree of the plasma are found to be 3.35 * 10 17 cm −2 and 3.75 * 10 17 cm −2 , and 0.76 and 0.44, respectively, at the peak stage of discharge (around 3 μs). e linear free-and boundelectron density can be obtained by ref [38]. Figure 2 shows the free-and bound-electron density (the initial gas pressure was about 0.81 mbar, and the voltage was 3 kV), where n b and n f denote the linear bound-and free-electron density, respectively.…”
Section: Resultsmentioning
confidence: 99%
“…e plasma linear electron density has been determined by the laser interferometry techniques [38]. e length of the gas column in the target is limited to about 220 mm.…”
Energy loss of protons with 90 and 100 keV energies penetrating through a hydrogen plasma target has been measured, where the electron density of the plasma is about 1016 cm−3 and the electron temperature is about 1-2 eV. It is found that the energy loss of protons in the plasma is obviously larger than that in cold gas and the experimental results based on the Bethe model calculations can be demonstrated by the variation of effective charge of protons in the hydrogen plasma. The effective charge remains 1 for 100 keV protons, while the value for 90 keV protons decreases to be about 0.92. Moreover, two empirical formulae are employed to extract the effective charge.
“…e plasma state has been diagnosed by Kuznetsov, and in our experiment, the plasma state can be determined by the initial gas pressure and discharge voltage based on the results presented in [38]. e initial energy loss ΔE for 100 and 90 keV protons was measured to be 5.02 and 7.73 keV before discharge.…”
Section: Resultsmentioning
confidence: 92%
“…Laser and Particle Beams degree of the plasma are found to be 3.35 * 10 17 cm −2 and 3.75 * 10 17 cm −2 , and 0.76 and 0.44, respectively, at the peak stage of discharge (around 3 μs). e linear free-and boundelectron density can be obtained by ref [38]. Figure 2 shows the free-and bound-electron density (the initial gas pressure was about 0.81 mbar, and the voltage was 3 kV), where n b and n f denote the linear bound-and free-electron density, respectively.…”
Section: Resultsmentioning
confidence: 99%
“…e plasma linear electron density has been determined by the laser interferometry techniques [38]. e length of the gas column in the target is limited to about 220 mm.…”
Energy loss of protons with 90 and 100 keV energies penetrating through a hydrogen plasma target has been measured, where the electron density of the plasma is about 1016 cm−3 and the electron temperature is about 1-2 eV. It is found that the energy loss of protons in the plasma is obviously larger than that in cold gas and the experimental results based on the Bethe model calculations can be demonstrated by the variation of effective charge of protons in the hydrogen plasma. The effective charge remains 1 for 100 keV protons, while the value for 90 keV protons decreases to be about 0.92. Moreover, two empirical formulae are employed to extract the effective charge.
“…When the discharging current reaches the maximum at around 3us after discharging, the temporal gradients of the electromagnetic field and the plasma parameters are minimum, and the free electron density in plasma reaches the maximum. The plasma parameters at the peak-discharging time are very well diagnosed, the linear free electron density and the ionization degree are 4.48 • 10 17 /cm 2 and 31%, respectively [30]. So in the following we discuss the data at this time and compare it with our theoretical approaches and others.…”
mentioning
confidence: 83%
“…The typical lifetime of the plasma is several microseconds, which is two orders of magnitude longer than the ion-plasma interaction time in our measurements (It takes 50 ns for the 100 keV/u helium ion passing though the plasma). The plasma parameters were well characterised by means of Mach-Zehnder interferometer [30]. A similar plasma device has been successfully used in the previous experiments in higher energy regime [31].…”
This paper reports the measurement of the energy loss of protons at the energy of 100 keV penetrating a partially ionized hydrogen plasma. The plasma of ne ≈ 1015–16 cm−3; Te ≈ 1–2 eV and lifetime of about 8 µs is created by the hydrogen gas discharge. The experimental results show an increase of a factor of 2.8 in the energy loss, which are in good agreement with the Bethe, Standard Stopping Model, Li–Petrasso and Vlasov models’ predictions within the error limit. The Bethe–Bloch Coulomb logarithm term is found to increase by a factor of 4.0 for free electrons as compared with the situation where bound electrons prevail. The potential application of protons energy loss for diagnosing the electron density in plasma is proposed too.
scite is a Brooklyn-based organization that helps researchers better discover and understand research articles through Smart Citations–citations that display the context of the citation and describe whether the article provides supporting or contrasting evidence. scite is used by students and researchers from around the world and is funded in part by the National Science Foundation and the National Institute on Drug Abuse of the National Institutes of Health.