2014
DOI: 10.1088/1742-6596/508/1/012007
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Basic features of electromagnetic pulse generated in a laser-target chamber at 3-TW laser facility PALS

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Cited by 26 publications
(35 citation statements)
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“…The signal acquisitions carried out by linear monopole antenna [31] and super wide-band antenna [32] placed both inside the interaction chamber, above the target at 30cm from it, and protected by a thick stainless-steel slab, as from Fig.5(c), are shown in Fig.5(a) and in Fig.5(b), respectively. It is well known that it is very difficult to get reliable measurements of EMP by conductive probes when high intensity and energetic lasers are used [1][2][3][4][5][6][7][8][9][10]12]. In fact, big fluctuations were present shot by shot on the measurements, due to background noise on the oscilloscopes caused by bad EMC-shielding of the scope and by spurious coupling of EMP with outside conductor of the coaxial cables.…”
Section: Methods and Resultsmentioning
confidence: 99%
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“…The signal acquisitions carried out by linear monopole antenna [31] and super wide-band antenna [32] placed both inside the interaction chamber, above the target at 30cm from it, and protected by a thick stainless-steel slab, as from Fig.5(c), are shown in Fig.5(a) and in Fig.5(b), respectively. It is well known that it is very difficult to get reliable measurements of EMP by conductive probes when high intensity and energetic lasers are used [1][2][3][4][5][6][7][8][9][10]12]. In fact, big fluctuations were present shot by shot on the measurements, due to background noise on the oscilloscopes caused by bad EMC-shielding of the scope and by spurious coupling of EMP with outside conductor of the coaxial cables.…”
Section: Methods and Resultsmentioning
confidence: 99%
“…In fact, big fluctuations were present shot by shot on the measurements, due to background noise on the oscilloscopes caused by bad EMC-shielding of the scope and by spurious coupling of EMP with outside conductor of the coaxial cables. To resolve these problems, it was necessary to use a delay line to clean the signals, as described in references [33,34]. Fig.…”
Section: Methods and Resultsmentioning
confidence: 99%
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“…In particular, the requirements needed to measure the energy and the flux of laser-driven beams are: radiation hardness (>10 12 p/bunch), fast charge collection, due to the intense proton pulse duration of about 10 ns and good signal-to-noise ratio, due to the huge electromagnetic pulse (EMP) which characterizes the laser environment [23]. Moreover, considering the high laser repetition rate (1-10 Hz) at ELIMAIA, the use of detectors able to give online shot-to-shot information of the beam parameters, as energy and intensity, is fundamental in order to monitor and control continuously the beam for applications.…”
Section: Diagnostics Systemmentioning
confidence: 99%
“…As one can see from the inset in Figure 12, the EMP is characterized by frequency components from few hundreds of MHz up to 2 GHz. Based on the frequency analysis, the significant noise signal results from the EMP propagation inside the interaction chamber [33,34] and seems to be predominant with respect to the charge signal, affecting the measurement of the total collected charge. Nevertheless, the cumulative integration of the FC signal, as shown in Figure 13, reveals the presence of a charge contribution that, although very small, can be separated by the huge EMP noise contribution [27].…”
Section: On-line Beam Diagnostics and Dosimetrymentioning
confidence: 99%