![]() Kenty C (1950) Role of metastable (3P2) Hg atoms in low current discharges in Hg rare gas mixtures. Wagh SM, Deshpande DA (2011) Revisiting the joshi effect. Joshi SS, Deshmukh GS (1945) Interaction of nitrous oxide and hydrogen in the silent discharge. Joshi SS, Narasimham V (1940) A light effect in chlorine under electrical discharge. Joshi SS (1939) Threshold potentials and reactivity under electrical discharge. Terenin A (1930) Photoionization of salt vapors. ![]() Penning FM (1928) Demonstração de um novo efeito fotoelétrico. doi: 10.1039/C2JM32649Cįoote PD, Moehler FL (1925) Photo-electric ionization of caesium vapor. Shi Y et al (2012) Graphene wrapped LiFePO4/C composites as cathode materials for Li-ion batteries with enhanced rate capability. doi: 10.1039/C1JM10857Cĭaniov V, Rudnev V, Kretov V (2012) Simulation of the heat transfer in the nanocathode. Pitchai R, Thavasi V, Mhaisalkarb SG, Ramakrishna S (2011) Nanostructured cathode materials: a key for better performance in Li-ion batteries. ![]() Yang J et al (2013) LiFePO4–graphene as a superior cathode material for rechargeable lithium batteries: impact of stacked graphene and unfolded graphene. doi: 10.4208/jams.051509.071209aĬhen L, Zhang M, Wei W (2013) Graphene-based composites as cathode materials for lithium ion batteries. Han XL, Chandran H, Misra P (2010) Collisional rate parameters for the 1s 4 energy level of neon 638.3 nm and 650.7 nm transitions from the analyses of the time-dependent optogalvanic signals. Heidenreich A, Jortner J (2010) Effects of the nanoplasma electrons on Coulomb explosion of xenon clusters. Heidenreich A, Last I, Jortner J (2008) Nanoplasma dynamics in Xe clusters driven by ultraintense laser fields. Morsch S, Brown PS, Badyal JPS (2012) Nanoplasma surface electrification. Rai SB, Rai DK (1996) Review article: optogalvanic spectroscopy. We will also briefly touch upon the potential applications of the optogalvanic effect at the nanoscale in fields such as graphene-based nanoelectronics and nanoplasmonics. A comparison between the experimentally recorded optogalvanic signal waveforms and the Monte Carlo fitting routine, along with a discussion related to the variation of the (a i and b j) fitting coefficients as a function of the discharge current, will illustrate the success of our theoretical model. The results presented here will use, for illustrative purposes, the waveforms associated with the laser-excited optogalvanic transitions of neon: 1s 4–2p 3 (607.4 nm), 1s 5–2p 7 (621.7 nm), 1s 3–2p 5 (626.6 nm), 1s 5–2p 8 (633.4 nm) and 1s 5–2p 9 (640.2 nm). The present chapter will focus on transition states of neon in the Fe–Ne hollow cathode lamp. The theoretical model behind the optogalvanic effect will provide insight into the importance of laser optogalvanic spectroscopy as a tool for spectral characterization of the plasma processes and enhanced understanding of the collisional state dynamics associated with the discharge species in hollow cathode lamps. The history of the optogalvanic effect will serve as an introduction to the importance of the phenomena. In this chapter we will discuss the laser optogalvanic effect in a discharge plasma environment, specifically associated with an iron-neon (Fe–Ne) hollow cathode lamp.
0 Comments
Leave a Reply. |
AuthorWrite something about yourself. No need to be fancy, just an overview. ArchivesCategories |