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  • 1
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 81 (1997), S. 1396-1403 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Un-prepoled lead zirconate titanate lanthanum doped-PLZT ferroelectric cathodes have emitted intense current pulses under the action of a high voltage pulse of typically 8 kV/cm for PLZT of 8/65/35 composition and 25 kV/cm for PLZT of 4/95/5 composition. In the experiments described in this paper, the exciting electric field applied to the sample is directed from the rear surface towards the emitting surface. The resulting emission is due to an initial field emission from the metal of the grid deposited over the emitting surface with the consequent plasma formation and the switching of ferroelectric domains. These electrons may be emitted directly form the crystal or from the plasma. This emission requires the material in ferroelectric phase. In fact, PLZT cathodes of the 8/65/35 type, that is with high titanium content, showing ferroelectric-paraelectric phase sequence, emit at room temperature, while PLZT cathodes of the 4/95/5 type, with low titanium content, having antiferro-ferro-paraelectric phase sequence, emit strongly at a temperature higher than 130°C. © 1997 American Institute of Physics.
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  • 2
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 90 (2001), S. 2447-2454 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: With increasing rf power, the electron concentration in the plasma of electron cyclotron resonance (ECR) ion sources is decreasing in comparison to the ion concentration, so that the plasma is charging up positively. When reviewing the basic performance requirements of ECR sources it becomes evident that the direct injection of electrons into the ECR plasma is increasing the electron charge density and the ion current yield. Ferroelectric ceramics was used as very robust, electron emitting cathode material under the heavy-duty conditions inside the plasma chamber of an ECR ion source. The electron emission from the ferroelectric cathode is turned on by a high repetition-rate bipolar pulse of ±1.2 to 1.6 kV amplitude to the electrodes deposited on both sides of the disk-shaped cathode. Lead–barium–zirconium-titanate (30/70/30) cathodes doped with 2 mol % Bi2O3 were installed and tested in the Ar–ion plasma of the ECR ion source CAESAR at INFN-LNS, Catania. The aim was to visibly increase the yield of the ion output current by electron injection. The plasma was heated by rf in continuous mode, while the ferroelectric cathode was pulsed at a repetition rate of 50 to 250 Hz. Pulsed electron injection at 250 Hz led to a noticeable increase of 30% of the Ar8+ output current at a rf power level of 400 W. In addition, magnetohydrodynamic instabilities were damped during and after electron injection. These results strongly encourage further research and development on the application of ferroelectric cathodes for increasing the ion current yield from hot plasma ion sources. © 2001 American Institute of Physics.
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  • 3
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Review of Scientific Instruments 70 (1999), S. 1857-1859 
    ISSN: 1089-7623
    Source: AIP Digital Archive
    Topics: Physics , Electrical Engineering, Measurement and Control Technology
    Notes: A pulse generator with the following characteristics is presented: the voltage ranges in the interval 0.1–6 kV, the maximum delivered current is 150 A, the pulse length ranges within the interval 100–300 ns, the rise time and the decay times are, respectively, 10 and 25 ns on 50 Ω resistive load and the repetition rate is higher than 1 MHz. The circuit has a source capacitor of 10 nF charged at the needed voltage, the capacitor feeds the load through a parallel of two fast and high voltage solid state switches. The nanosecond rise time and the square fashion of the pulse have been accomplished arranging all the components in cylindrical symmetry. A bipolar pulse is obtained coupling two circuits with opposite polarity. © 1999 American Institute of Physics.
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  • 4
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 57 (1985), S. 18-26 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: In this paper the classical theory of the transverse optical klystron is presented. The gain is obtained by solving analytically the Vlasov equation which governs the evolution of the electron beam along the undulator magnet. The initial energy distribution of the electron beam is assumed gaussian. Both the small signal and the saturation regime are investigated.
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  • 5
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 90 (2001), S. 6341-6344 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The emission from ferroelectric cathodes excited by bipolar pulses does not suffer the hysteretic behavior shown with monopolar pulse excitation. This is because the bipolar pulse forces a neat charging–discharging cycle of the whole surface of the sample, and, therefore, the flipping of the polarization. The emission becomes definitely stable, whereas it was erratic in current amplitude, pulse shape and starting time with monopolar excitation. The emission yield of energetic electrons from ferroelectric cathodes of doped lead–titanate–zirconate–lanthanum increased from a few hundreds of milliamperes to some amperes (with current density of 30–50 A/cm2) in passing from monopolar to bipolar voltage pulse excitation. © 2001 American Institute of Physics.
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  • 6
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 89 (2001), S. 1367-1370 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: We describe the photoemission of lanthanum-doped lead zirconate titanate when illuminated with 355 nm radiation, with/without prepoling and with/without the application of a polarizing field. To explain the different behaviors observed, we propose a physical picture based on the defects moving toward the surface and the donor electrons squeezing into a very thin layer at the surface. The model and the experimental results indicate that ferroelectric ceramics could become interesting photoemitters. © 2001 American Institute of Physics.
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  • 7
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 91 (2002), S. 6125-6133 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: We show that properly electroded ceramic disks are strong and robust electron emitters when excited with short voltage pulses. They can operate in two different regimes: (I) a regime at low exciting voltage, ∼0.7 kV per millimeter thickness and (II) a regime at high exciting voltage, ∼2 kV/mm. In the first regime the excitation pulse must be bipolar, positive–negative, the output current results in several tens of milliamperes per cm2. The first positive semiwave charges the cathode surface and the negative semiwave expels the previously accumulated electrons. This behavior of ceramic electroded disks, before as sink and next as source of electrons, is due to the succession of an attractive and then repulsive electron field on the unelectroded zones of the front surface. The two opposite oriented fields are generated by the voltage applied at the rear electrode. In the second regime, the excitation pulse can be either monopolar or bipolar, the emission process is governed by the building up of a plasma sheet as a consequence of the excitation pulse. The high-voltage exciting pulse initiates a discharge, and so the plasma, at the triple metal–insulator–vacuum point because of the strong longitudinal component of the electric field. The plasma cloud expands over the front surface becoming a dynamical electrode. Screening electrons accumulate in front of the sample, either in the plasma sheet or on the front surface of the material. The component of the electric field perpendicular to the surface (due to either the negative semiwave of a bipolar pulse or to the space charge of the huge amount of electrons no longer attracted by bound positive charge) pushes screening electrons out from the cathode. © 2002 American Institute of Physics.
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  • 8
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 87 (2000), S. 4005-4009 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Though present photoemitting cathodes have attained quantum yields, lifetimes, dark currents, and response times as required by high-luminosity accelerators, their use is hampered by their high reactivity to residual gases even in ultra-high-vacuum conditions. Ultrathin (20–200 nm) films of nanostructured sp2 carbon, directly grown on photocathodes by supersonic cluster-beam deposition, besides providing a strongly bound, inert protective coating, are shown to maintain the photoemission efficiency of clean metallic substrate cathodes. Moreover, nanostructured carbon coating is shown to induce strong nonlinearities in photoemission at high intensities, which can be explained as due to the Auger effect. © 2000 American Institute of Physics.
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  • 9
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 85 (1999), S. 8337-8342 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Electron emission from a ceramic disk is due to spontaneous polarization switching induced by a high-voltage pulse applied to the surface electrodes. With a conventional front electrode, emission was erratic as a function of samples and decayed with shot number. On the contrary, when the front electrode consisted of a pattern of unconnected patches contained within a ring, emission was stable. The physics of the two configurations is investigated and a possible interpretation of the two different behaviors is given. © 1999 American Institute of Physics.
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  • 10
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Physics of Plasmas 2 (1995), S. 3488-3493 
    ISSN: 1089-7674
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The free electron laser–peniotron hybrid is studied. It is shown by computer simulations that the free electron laser–peniotron hybrid, with the synchronous condition ω−(kw+k(parallel))v(parallel)−ωc≈0, is a strong interaction, and has an efficiency as high as that of the peniotron. The interaction of the free electron laser–peniotron hybrid is compared with that of the free electron laser–cyclotron hybrid. © 1995 American Institute of Physics.
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