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Journal articles on the topic 'Ionization current'

Author: Grafiati

Published: 4 June 2021

Last updated: 18 February 2022

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1

Itoh, Haruo, Susumu Suzuki, and Nobuaki Ikuta. "Ionization Current in N2 Gas." IEEJ Transactions on Fundamentals and Materials 113, no. 1 (1993): 25–31. http://dx.doi.org/10.1541/ieejfms1990.113.1_25.

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2

Itoh, Haruo, Xiao Yong Hu, and Nobuaki Ikuta. "Ionization Current in Ne/Ar Mixtures." IEEJ Transactions on Fundamentals and Materials 108, no. 3 (1988): 125. http://dx.doi.org/10.1541/ieejfms1972.108.125.

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3

Gapeev, Alexei, Alberto Berton, and Daniele Fabris. "Current-controlled nanospray ionization mass spectrometry." Journal of the American Society for Mass Spectrometry 20, no. 7 (July 2009): 1334–41. http://dx.doi.org/10.1016/j.jasms.2009.03.007.

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4

Stoyanov, D. G. "Current-voltage characteristic of parallel-plane ionization chamber with inhomogeneous ionization." Journal of Instrumentation 2, no. 08 (August 24, 2007): P08007. http://dx.doi.org/10.1088/1748-0221/2/08/p08007.

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5

Ifa, Demian R., Chunping Wu, Zheng Ouyang, and R. Graham Cooks. "Desorption electrospray ionization and other ambient ionization methods: current progress and preview." Analyst 135, no. 4 (2010): 669. http://dx.doi.org/10.1039/b925257f.

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6

Brancaccio, Franco, Mauro S. Dias, and Marina F. Koskinas. "Automatic system for ionization chamber current measurements." Applied Radiation and Isotopes 61, no. 6 (December 2004): 1339–42. http://dx.doi.org/10.1016/j.apradiso.2004.03.001.

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7

Paracchini, C., and V. Dallacasa. "Impact ionization current in semi-insulating GaAs." Solid State Communications 69, no. 1 (January 1989): 49–52. http://dx.doi.org/10.1016/0038-1098(89)90024-0.

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8

Van, V., M. J. Deen, J. Kendall, D. S. Malhi, S. Voinigescu, and M. Schrofer. "DC extraction of the base and emitter resistances in polysilicon-emitter npn BJTs." Canadian Journal of Physics 74, S1 (December 1, 1996): 172–76. http://dx.doi.org/10.1139/p96-853.

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Five DC techniques of extracting the base and emitter resistances of polysilicon-emitter npn bipolar junction transistors (BJTs) are presented and compared. The five techniques include three previously published techniques and two new techniques, constant base current and IB–IE plane fitting. Application of the five methods to a 0.8 × 16 μm2 npn BJT shows that all but the method of impact ionization yield comparable Rc and Rbb values at high currents. The impact ionization method, which extracts Rc and Rbb in the impact ionization region and at low base currents, yields markedly different Rc and Rbb values, indicating that the values of the parasitic resistances depend on the current range over which the extraction is performed. Thus the choice of which method is best to use depends on the current range over which Rc and Rbb are to be measured, and the validity of the assumptions used in the method when applied to the device.

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9

Mah, K. R., F. W. Dalby, and C. W. Barnard. "Polarization dependence of resonant multiphoton ionizations on 1S0 and 1,3D2 states in atomic mercury." Canadian Journal of Physics 66, no. 1 (January 1, 1988): 1–6. http://dx.doi.org/10.1139/p88-001.

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The polarization dependences of some resonant multiphoton ionizations in atomic mercury have been measured with a broadband (bandwidth ≈ 1.5 cm−1) multimode dye laser at moderate light intensities (≈ 500 MW∙cm−2). The multiphoton processes studied were the absorption of four photons to a resonant 1S0, 1D2, or 3D2 level by one-photon ionization. Complete saturation of the one-photon ionization step results in the ionization of all atoms excited to the resonant level. Because of the saturation of the ionization step, the polarization dependence of the four-photon excitation to the resonant level is measured. The theory developed by Dalby et al. is shown to give good agreement with the experiment when it is used to calculate the polarization dependence of the multiphoton transition to the resonant level. For the 6d1D2 resonance, distortions in the polarization dependence and an unusual linewidth dependence on the light polarization were observed. We relate these observations to the alternating current Stark effect and to the production of the third harmonic of the laser light in the focal volume.

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10

Suzuki, Susumu, Haruo Itoh, Hisashi Sekizawa, and Nobuaki Ikuta. "Ionization Current in N₂ Gas." IEEJ Transactions on Fundamentals and Materials 114, no. 12 (1994): 880–85. http://dx.doi.org/10.1541/ieejfms1990.114.12_880.

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11

Suzuki, Susumu, Haruo Itoh, Hisashi Sekizawa, and Nobuaki Ikuta. "Ionization Current in N₂ Gas." IEEJ Transactions on Fundamentals and Materials 115, no. 1 (1995): 44–49. http://dx.doi.org/10.1541/ieejfms1990.115.1_44.

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12

Suzuki, Susumu, Haruo Itoh, Hisashi Sekizawa, and Nobuaki Ikuta. "Ionization Current in N₂ Gas." IEEJ Transactions on Fundamentals and Materials 115, no. 9 (1995): 799–805. http://dx.doi.org/10.1541/ieejfms1990.115.9_799.

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13

Itoh, Haruo, and Nobuaki Ikuta. "Ionization Current in N₂ Gas." IEEJ Transactions on Fundamentals and Materials 111, no. 5 (1991): 410–16. http://dx.doi.org/10.1541/ieejfms1990.111.5_410.

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14

Suzuki, Susumu, Haruo Itoh, Hisashi Sekizawa, and Nobuaki Ikuta. "Ionization Current in N₂ Gas." IEEJ Transactions on Fundamentals and Materials 113, no. 6 (1993): 453–60. http://dx.doi.org/10.1541/ieejfms1990.113.6_453.

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15

Suzuki, Susumu, Haruo Itoh, Hisashi Sekizawa, and Nobuaki Ikuta. "Ionization Current in N₂ Gas." IEEJ Transactions on Fundamentals and Materials 118, no. 10 (1998): 1125–31. http://dx.doi.org/10.1541/ieejfms1990.118.10_1125.

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16

Chau, Quan. "Investigating and modeling impact ionization current in MOSFETs." Solid-State Electronics 94 (April 2014): 66–71. http://dx.doi.org/10.1016/j.sse.2014.02.009.

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17

Lee, Hong-Wei, and Aaron R. Hawkins. "Solid-state current amplifier based on impact ionization." Applied Physics Letters 87, no. 7 (August 15, 2005): 073511. http://dx.doi.org/10.1063/1.2031929.

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18

Kapustin, Vladimir, and A. Korgaviy. "Ion Current Composition of Surface-ionization thermoemitter ions." Журнал технических исследований 2, no. 4 (November 24, 2016): 1. http://dx.doi.org/10.12737/23025.

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19

SATO, M. "ION CURRENT CHARACTERISTICS OF Ar FIELD IONIZATION SOURCE." Le Journal de Physique Colloques 48, no. C6 (November 1987): C6–183—C6–188. http://dx.doi.org/10.1051/jphyscol:1987630.

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20

Choueiri, Edgar Y., and Thomas M. Randolph. "Ionization front in a high-current gas discharge." Physics of Plasmas 14, no. 3 (March 2007): 033502. http://dx.doi.org/10.1063/1.2646365.

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21

Schneider, A., S. Popov, G. Sandolache, A. Batrakov, and S. Rowe. "Ionization–Recombination Front in High-Current Vacuum Arc." IEEE Transactions on Plasma Science 39, no. 11 (November 2011): 2844–45. http://dx.doi.org/10.1109/tps.2011.2158590.

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22

Bohne, W., S. Hessler, and G. Röschert. "Beam-current measurement based on residual gas ionization." Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms 113, no. 1-4 (June 1996): 78–80. http://dx.doi.org/10.1016/0168-583x(95)01311-3.

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23

Du, H. W., M. Chen, Z. M. Sheng, and J. Zhang. "Numerical studies on terahertz radiation generated from two-color laser pulse interaction with gas targets." Laser and Particle Beams 29, no. 4 (December 2011): 447–52. http://dx.doi.org/10.1017/s0263034611000577.

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AbstractBased upon the Ammosov-Delone-Krainov ionization model, it is shown that two-color laser interaction with neutral gas generates strong ionization currents, which lead to electromagnetic emission at terahertz frequency when the gas density is at proper values. The emission efficiency depends on the difference of the phases between the fundamental and its second harmonic. The intensity ratio between the two pulses also affects the emission strength. An optimum intensity ratio has been found within our parameter region. The above ionization current theory is in agreement with one-dimensional particle-in-cell simulations with field ionization included.

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24

Christen, Thomas. "Nonequilibrium Phase Transition and Current Filaments in Extrinsic Semiconductors." Zeitschrift für Naturforschung A 49, no. 9 (September 1, 1994): 851–55. http://dx.doi.org/10.1515/zna-1994-0906.

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Abstract A phenomenological model for charge transport in extrinsic semiconductors is presented. For shallow impurities, large saturated impact-ionization coefficient and sufficiently low lattice temperature, the current-field characteristic is S-shaped (SNDC) due to the interplay between impact ionization and scattering of carriers from acoustic phonons, ionized and neutral impurities. The present model provides and explanation of the experimentally observed disappearance of SNDC above a critical lattice temperature. In the region of negative differential conductivity where a current-controlled uniform state is unstable, current filaments are calculated numerically.

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25

Abaye, Daniel A., Irene A. Agbo, and Birthe V. Nielsen. "Current perspectives on supercharging reagents in electrospray ionization mass spectrometry." RSC Advances 11, no. 33 (2021): 20355–69. http://dx.doi.org/10.1039/d1ra00745a.

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26

Nariyama, Nobuteru. "Current saturation in free-air ionization chambers with chopped synchrotron radiation." Journal of Synchrotron Radiation 20, no. 5 (July 3, 2013): 698–704. http://dx.doi.org/10.1107/s0909049513016154.

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Saturation curves for free-air ionization chambers with electrode gap widths of 4.2, 8.4 and 18 mm were obtained for 10 and 15 keV undulator synchrotron radiation thinned with a 230 Hz rotating-disk chopper. Ion recombination in free-air ionization chambers was found to be inversely proportional to the applied electric field, and an expression that satisfactorily reproduced the ion-recombination rate is determined. A comparison of the expressions for continuous and pulsed X-rays revealed that chopped high-intensity X-rays require a higher voltage to attain saturation when the product of the pulse width and electric field exceeds a value that depends on the X-ray energy. This behaviour was observed explicitly for 10 keV X-rays in measurements with the ionization chamber placed before and after the chopper.

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27

Sarver, Scott A., Nishant Chetwani, Norman J. Dovichi, David B. Go, and Carlos A. Gartner. "A Comparison of Alternating Current and Direct Current Electrospray Ionization for Mass Spectrometry." Journal of The American Society for Mass Spectrometry 25, no. 4 (January 25, 2014): 524–29. http://dx.doi.org/10.1007/s13361-013-0809-4.

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28

Hamad, Hassan, Christophe Raynaud, Pascal Bevilacqua, Sigo Scharnholz, and Dominique Planson. "Temperature Dependence of 4H-SiC Ionization Rates Using Optical Beam Induced Current." Materials Science Forum 821-823 (June 2015): 223–28. http://dx.doi.org/10.4028/www.scientific.net/msf.821-823.223.

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The behavior of 4H-SiC power devices in severe environment with varying temperature is a key characteristic indicating their reliability. This paper shows the dependence of the ionization rates of 4H-SiC with respect to temperature. Optical Beam Induced Current (OBIC) measurements have been performed on PN junctions to determine the multiplication coefficient for temperature varying between 100 and 450K. That allows extracting the ionization rates by fitting the curves of multiplication coefficient.

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29

Jin, Qinhan, Wenjun Yang, Aimin Yu, Xiaodan Tian, and Fendi Wang. "Helium direct current discharge ionization detector for gas chromatography." Journal of Chromatography A 761, no. 1-2 (February 1997): 169–79. http://dx.doi.org/10.1016/s0021-9673(96)00800-x.

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30

Higashiyama, Y., and S. Enomoto. "A Current Mode Potential Meter Utilizing α-Ray Ionization." Isotopenpraxis Isotopes in Environmental and Health Studies 24, no. 8 (January 1988): 317–19. http://dx.doi.org/10.1080/10256018808623984.

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31

Chetwani, Nishant, Catherine A. Cassou, David B. Go, and Hsueh-Chia Chang. "Frequency Dependence of Alternating Current Electrospray Ionization Mass Spectrometry." Analytical Chemistry 83, no. 8 (April 15, 2011): 3017–23. http://dx.doi.org/10.1021/ac103189p.

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32

Harris, Glenn A., Asiri S. Galhena, and Facundo M. Fernández. "Ambient Sampling/Ionization Mass Spectrometry: Applications and Current Trends." Analytical Chemistry 83, no. 12 (June 15, 2011): 4508–38. http://dx.doi.org/10.1021/ac200918u.

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33

Sato, Mieko. "Ion current characteristics of an Ar field ionization source." Surface Science Letters 285, no. 3 (April 1993): L525—L527. http://dx.doi.org/10.1016/0167-2584(93)90360-u.

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34

Sato, Mieko. "Ion current characteristics of an Ar field ionization source." Surface Science 285, no. 3 (April 1993): L525—L527. http://dx.doi.org/10.1016/0039-6028(93)90425-j.

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35

Fitzgerald, R., D. E. Bergeron, S. P. Giblin, D. G. Jarrett, S. M. Judge, C. Michotte, H. Scherer, and N. M. Zimmerman. "The next generation of current measurement for ionization chambers." Applied Radiation and Isotopes 163 (September 2020): 109216. http://dx.doi.org/10.1016/j.apradiso.2020.109216.

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36

Курченко, Андрей. "MALDI MASS SPECTROMETRY - IN THE ASSESSMENT OF HUMAN MICROBIOTA. CURRENT STATE AND PERSPECTIVES." Immunology and Allergy: Science and Practice, no. 2 (July 29, 2020): 11–18. http://dx.doi.org/10.37321/immunology.2020.02-02.

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Mass spectrometry is a modern physicochemical method of analysis that allows for a qualitative and quantitative analysis of the composition of a substancebased on the preliminary ionization of its constituent atoms or molecules. One of the new methods of ionization, thanks to which the mass spectrometric study of macromolecules has become widespread, is matrix-activated laser desorption / ionization (MALDI), which is a pulsed laser irradiation of the substance under study mixed with a matrix.Тhe article presents modern data on the use of the MALDI mass- spectrometry method for conducting genus and species-specific identification of microorganisms in the practice of diagnostic laboratories. The advantages of MALDI-TOF identification in comparison with other methods of microbiota research are considered.The place of mass spectrometry in the system of laboratory diagnostics of various pathogens is indicated.

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37

Зольников and Konstantin Zolnikov. "MATHEMATICAL RATIOS TO IONIZATION CURRENT CORRESPONDS TO A DEEP-SUBMICRON TECHNOLOGY." Modeling of systems and processes 7, no. 2 (October 30, 2014): 8–11. http://dx.doi.org/10.12737/6081.

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38

Dittrich, Aleš, Josef Laurin, and Tomáš Zvolský. "Device for Detecting the Level of Ionization of the Fuel Mixture in the Cylinder Petrol Engine." Applied Mechanics and Materials 799-800 (October 2015): 880–84. http://dx.doi.org/10.4028/www.scientific.net/amm.799-800.880.

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The paper is focused on the ionization current measurement in the cylinder SI engine during an engine cycle. Briefly describes the problems and lists reference sources, which are several possible ways of measuring the ionization current during the working cycle. Paper also provides information regarding the proposed scheme of measuring devices and mentions functional test equipment.

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39

Zhang, Yongzheng, and Xiaoqing Zhang. "A Practical Algorithm for Calculating the Impulse Earthing Resistances of Vertical Earthing Electrodes." Journal of Electronics and Advanced Electrical Engineering 1, no. 2 (May 3, 2021): 15–20. http://dx.doi.org/10.47890/jeaee/2020/yongzhengzhang/11120008.

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An algorithm is proposed in this paper for calculating the impulse earthing resistances of vertical earthing electrodes. The proposed algorithm employs the average potential method to derive the formula of the low current earthing resistance. Unlike the previous algorithm, the soil ionization effect under high impulse current is taken into account by introducing a nonlinear characteristic to represent the relationship between the electric field and current density in the ionization zone around the earthing electrode. On the basis of the nonlinear characteristic, the effective radius is evaluated for the equivalent earthing electrode. Then, the impulse earthing resistance can be calculated by substituting the effective radius into the formula of the low current earthing resistance. A comparison is also made between calculated and measured results to confirm the validity of the proposed algorithm. Keywords: Earthing Resistance; Vertical Earthing Electrode; Average Potential Integral; Soil Ionization; Current Density;

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40

Yang, Chris, Anatoly Zharin, and Steven Danyluk. "Surface Characterization with an Ionization Probe." Key Engineering Materials 447-448 (September 2010): 518–23. http://dx.doi.org/10.4028/www.scientific.net/kem.447-448.518.

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This paper discusses the application of an ionizing source coupled with galvanic differences between metals in a measure of the work function difference between the metal surfaces. The electrical field generated from the contact potential difference (CPD) between two electrodes will cause the gaseous ions to discharge at both surfaces, creating a measurable current. The current depends on the surface size, spacing, and ionizing source power. One of the surfaces (probe) can vary in shape and size, and if inert, can be used to obtain the work function or surface potential of the second surface. The ionic current is proportional to ion mobility, ion generation rate, CPD, and the probe size, but inversely proportional to the spacing between the probe and the sample. It is found, as expected, that there is an approximate linear relationship between the ionization probe signal and the work function of the surfaces of metals.

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41

Nielsen, Lars, and Lars Eriksson. "Ionization Current Interpretation for Ignition Control in Internal Combustion Engines." IFAC Proceedings Volumes 29, no. 1 (June 1996): 7814–19. http://dx.doi.org/10.1016/s1474-6670(17)58949-1.

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42

Eriksson, L., and L. Nielsen. "Ionization current interpretation for ignition control in internal combustion engines." Control Engineering Practice 5, no. 8 (August 1997): 1107–13. http://dx.doi.org/10.1016/s0967-0661(97)00103-2.

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43

Debayle, A., and V. T. Tikhonchuk. "Target ionization by a high current relativistic monoenergetic electron beam." Physics of Plasmas 14, no. 7 (July 2007): 073104. http://dx.doi.org/10.1063/1.2749500.

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44

Canali, C., A. Neviani, C. Tedesco, E. Zanoni, A. Centronio, and C. Lanzieri. "Dependence of ionization current on gate bias in GaAs MESFETs." IEEE Transactions on Electron Devices 40, no. 3 (March 1993): 498–501. http://dx.doi.org/10.1109/16.199353.

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45

Mühle, C., K. D. Leible, and P. Spädtke. "Development of the Penning ionization gauge source for higher current." Review of Scientific Instruments 69, no. 2 (February 1998): 1057–59. http://dx.doi.org/10.1063/1.1148632.

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46

Li, Leping, Bing-Xin Yang, and P. M. Johnson. "Alternating-current Stark-effect line shapes in multiphoton ionization spectra." Journal of the Optical Society of America B 2, no. 5 (May 1, 1985): 748. http://dx.doi.org/10.1364/josab.2.000748.

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47

Mihnea, A., P. J. Rudeck, Chun Chen, K. D. Prall, and R. Ghodsi. "Direct observation of secondary ionization current in n-channel MOSFETs." IEEE Transactions on Electron Devices 49, no. 12 (December 2002): 2301–7. http://dx.doi.org/10.1109/ted.2002.805567.

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48

Krinberg, I. A. "Ionization and particle transfer in an expanding current‐carrying plasma." Physics of Plasmas 1, no. 9 (September 1994): 2822–26. http://dx.doi.org/10.1063/1.870520.

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49

Ahedo, E. "Current–voltage response of anodic plasma contactors with external ionization." Physics of Plasmas 3, no. 11 (November 1996): 3875–84. http://dx.doi.org/10.1063/1.871575.

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50

Mokhatri, Mehrdad, and Zulkurnain Abdul-Malek. "The Effect of Grounding Electrode Parameters on Soil Ionization and Transient Grounding Resistance Using Electromagnetic Field Approach." Applied Mechanics and Materials 554 (June 2014): 628–32. http://dx.doi.org/10.4028/www.scientific.net/amm.554.628.

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The soil ionization phenomenon occurs during the dispersion of lightning current into the earth. This phenomenon causes the grounding electrode resistance to be effectively reduced. The extension of the soil ionization depends on the current amplitude along the electrode and the resultant electric field intensity surrounding the electrode. The electrical and physical parameters of the grounding electrode system are found as factors that affect the electric field intensity. In this study the electromagnetic field approach and the soil breakdown theory are taken into account to investigate the effect of the mentioned factors on soil ionization and grounding resistance. Changing the parameters of the grounding electrode system affect the electric field distribution around the electrode. Based on the conditions the grounding electrode resistance was reduced between 12% to 75% by considering the soil ionization effect.

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