Academic literature on the topic 'Photoelectric effect'

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Journal articles on the topic "Photoelectric effect"

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Cortel, Adolf. "Simple Photoelectric Effect." Physics Teacher 44, no. 5 (2006): 310–11. http://dx.doi.org/10.1119/1.2195405.

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Aseyev, S. A., B. N. Mironov, D. G. Poydashev, A. A. Ischenko, and E. A. Ryabov. "“Anomalous” Photoelectric Effect in the Ultrafast Electron Diffraction Method." JETP Letters 119, no. 7 (2024): 495–500. http://dx.doi.org/10.1134/s0021364024600745.

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Electron-pulse probing of fast laser-induced processes has allowed the direct observation of the structural dynamics in matter with a high spatiotemporal resolution. A thin gold film has appeared to be a convenient photocathode, and photoelectron emission has been induced by femtosecond ultraviolet radiation with a photon energy of about 4.65–4.75 eV (in particular, $$\hbar $$ω $$ \cong $$ 4.65 eV for the third harmonic of the Ti:sapphire laser). For the linear photoelectric effect, this energy contradicts the reference work function WAu$$ \cong $$ 5.1–5.3 eV of pure metal. Reasons for such contradiction have been analyzed and good agreement with experimental data has been reached with a model proposed for the generation of photoelectron pulses.
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P. Opeil, C., R. C.Albers, K. B. Blagoev, et al. "Photoelectric Effect in Uranium." Journal of the Physical Society of Japan 75, Suppl (2006): 56–57. http://dx.doi.org/10.1143/jpsjs.75s.56.

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Bancong, Hartono, Ana Dhiqfaini Sultan, Subaer Subaer, and Muris Muris. "Development and Students’ Perception on Teaching Aids of Photoelectric Effect Experiment Using Leds." Jurnal Pendidikan Fisika 7, no. 3 (2019): 253–61. http://dx.doi.org/10.26618/jpf.v7i3.2332.

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The photoelectric effect experiment generally uses a very sophisticated and expensive apparatus. Some high schools and even universities in Indonesia cannot afford to conduct this experiment because of the high price of the apparatus. The purpose of this study was to develop a user-friendly, and cost-effective teaching aids which can be used to demonstrate the concepts of modern physics related to the photoelectric effect. The stages of this study employed the Four-D model, namely define, design, develop, and disseminate. Based on experts and practitioner evaluation, the developed teaching aids and practicum devices of photoelectric effect experiment were found to be valid and reliable. The results of the experiment by using this developed teaching aids of the photoelectric effect showed that there is a linear relationship between the stopping potential and the frequency of light emitted by the LED. These results are consistent with Millikan's experimental results, the first physicist who succeed in proving Einstein's hypothesis of the photoelectric effect, that in the photoelectric effect the stopping potential does not depend on the intensity of light but depends only on the frequency of light. In this study, the Planck’s constant value obtained is 6.408x10-34 J.s. Although this value is slightly smaller than the accepted value of Planck's constant that is 6.626x10-34 J.s, it is good enough considering the instrumental error occurred during the measurement of current and voltage. Furthermore, the students’ perception of the developed teaching aids and practicum devices of the photoelectric effects experiment are 74.9% (good) and 80.2% (very good), respectively. This indicates that the photoelectric effect experiment teaching aids and practicum devices that have been developed can be used to demonstrate and prove the concepts of modern physics related to the photoelectric phenomena correctly.Keywords: Teaching Aids, Photoelectric Effect, Students’ Perception
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He, Bo, Jing Xu, HuanPo Ning, et al. "Preparation and Optoelectrical Properties of p-CuO/n-Si Heterojunction by a Simple Sol–Gel Method." International Journal of Nanoscience 16, no. 05n06 (2017): 1750013. http://dx.doi.org/10.1142/s0219581x17500132.

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The Cuprous oxide (CuO) thin film was prepared on texturized Si wafer by a simple sol–gel method to fabricate p-CuO/n-Si heterojunction photoelectric device. The novel sol–gel method is very cheap and convenient. The structural, optical and electrical properties of the CuO film were studied by X-ray diffraction (XRD), Scanning Electron Microscope (SEM), X-ray photoelectron spectroscopy (XPS), UV–Vis spectrophotometer and Hall effect measurement. A good nonlinear rectifying behavior is obtained for the p-CuO/n-Si heterojunction. Under reverse bias, good photoelectric behavior is obtained.
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Chen, Chun Xiao, and Chang Geng Zhang. "New demonstration of photoelectric effect." Physics Teacher 37, no. 7 (1999): 442. http://dx.doi.org/10.1119/1.880346.

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De Ninno, Giovanni, Jonas Wätzel, Primož Rebernik Ribič, et al. "Photoelectric effect with a twist." Nature Photonics 14, no. 9 (2020): 554–58. http://dx.doi.org/10.1038/s41566-020-0669-y.

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Hirohashi, Ryo, Toyohide Tanaka, Yoshihiro Koshijima, and Masafumi Kamiyama. "Photoelectric Effect of Metallophthalocyanine Derivatives." Bulletin of the Chemical Society of Japan 62, no. 10 (1989): 3359–61. http://dx.doi.org/10.1246/bcsj.62.3359.

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Sokolowski, Andrzej. "Teaching the photoelectric effect inductively." Physics Education 48, no. 1 (2012): 35–41. http://dx.doi.org/10.1088/0031-9120/48/1/35.

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Goldader, Jeffrey. "Tweaking “Simple Photoelectric Effect” Demo." Physics Teacher 44, no. 7 (2006): 406. http://dx.doi.org/10.1119/1.2353568.

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Dissertations / Theses on the topic "Photoelectric effect"

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MULERI, FABIO. "Expectations and perspectives of X-ray photoelectric polarimetry." Doctoral thesis, Università degli Studi di Roma "Tor Vergata", 2009. http://hdl.handle.net/2108/816.

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La polarimetria è l'ultima branca dell'Astronomia nella banda dei raggi X ancora inesplorata. Nonostante un vasto interesse testimoniato da un'estesa letteratura, il suo sviluppo è stato impedito dalla mancanza di dispositivi la cui sensibilità giustificasse l'inserimento di polarimetri X a bordo delle missioni spaziali moderne. Ciononostante nuovi strumenti basati sull'effetto fotoelettrico, capaci di risolvere le tracce dei fotoelettroni in un gas, offrono oggi la possibilità di colmare il divario tra aspettative teoriche e gli scarsi risultati ad oggi raggiunti: in questo ambito, uno dei progetti più avanzati è il Gas Pixel Detector (GPD), sviluppato in Italia dall'INFN di Pisa e dall'INAF/IASF di Roma. Questa tesi ha contribuito dell'inserimento del GPD a bordo delle prossime missioni in differenti aspetti. Innanzitutto è stata misurata la risposta dello strumento a radiazione polarizzata di alcuni keV, ovvero nell'intervallo energetico di massima sensibilità, grazie ad una sorgente di calibrazione basata sulla diffrazione di Bragg a circa 45 gradi. Quest'ultima, insieme a sorgenti radioattive e a tubi a raggi X, è stata montata su un sistema meccanico, progettato e costruito in modo tale che lo strumento in esame potesse essere spostato, inclinato e ruotato rispetto al fascio incidente. Questo rende disponibile una struttura per la completa caratterizzazione del GPD (e di altri strumenti): prime e preliminari misure di calibrazione sono state effettuate grazie ad essa e sono di seguito presentate. Infine ho calcolato la sensibilità del GPD nel caso in cui esso sia posto nel piano focale di telescopi progettati per le prossime missioni spaziali, come PolariX e IXO, e ho discusso ulteriori applicazioni del GPD e dei polarimetri fotoelettrici in generale. In particolare, sono presentati il possibile utilizzo di questi dispositivi come strumenti a grande campo di vista o e quello come rivelatori sensibili fino ad energie di decine di keV.<br>Polarimetry is the last unexplored branch of X-ray Astronomy. Despite a wide interest proved by an extended literature, its development has suffered the lack of instruments which could assure a sufficient sensitivity to justify the inclusion of X-ray polarimeters on-board modern missions. Nevertheless new devices based on photoelectric absorption, which are able to image the track of photoelectrons in a gas mixture, offer today the possibility to fill the gap between theoretical expectations and the current meagre results: in this regard, one of the most advanced project is the GPD (Gas Pixel Detector), developed in Italy by INFN of Pisa and INAF/IASF of Rome. This work of thesis contributed to the use of the GPD on-board future space missions from different points of view. The response of the instrument to polarized radiation at a few keV, namely in the energy range of maximum sensitivity, was measured thanks to a calibration source based on Bragg diffraction at nearly 45 degrees. This source, together with radioactive unpolarized sources and X-ray tubes, were also interfaced with a mechanical assembly which was designed and built allowing for the movement, the inclination and the rotation of the instrument with respect to the incident beam. This makes available a facility for the complete characterization of the GPD (and other instruments) and the first and preliminary systematic measurements of calibration are presented. I also derive the scientific performances of the GPD when the instrument is placed in the focal plane of realistic X-ray telescopes planned for future missions, such as PolariX or IXO, and discuss some further applications of the GPD and of the photoelectric polarimeters in general. In particular the possible use of these devices as large field of view instruments or at energies up to tens of keV are presented.
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Басов, Андрій Геннадійович, Андрей Геннадьевич Басов, Andrii Hennadiiovych Basov та О. Калінін. "Цифровий навчальний комплекс "фотоефект"". Thesis, Видавництво СумДУ, 2010. http://essuir.sumdu.edu.ua/handle/123456789/21092.

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Fanis, Alberto De. "Double photoionization of alkaline earth atoms and photoelectron spectroscopy of reactive intermediates." Thesis, University of Southampton, 2000. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.327255.

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De, Beer Isabella Constance. "Experiences of learners when a computer simulation is used to aid teaching the photoelectric effect." Diss., University of Pretoria, 2013. http://hdl.handle.net/2263/40532.

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This study explores the use of computer simulations to supplement learning in Science lessons, specifically the photoelectric effect. This study uses the Felder and Silverman Learning Style Model (FSLSM) as a theoretical framework to investigate the use of simulations as it provides a useful lens through which to explore the consistent way in which a person learns regardless of the teaching method or content learnt. Using this theoretical framework, this research investigates the experiences of learners with different learning styles when an interactive computer simulation is used to aid teaching the photoelectric effect in Physical Science. This case study used qualitative data collected from 17 computer literate Grade 12 learners in three different classes at a secondary school in Nelspruit, Mpumalanga. Analysis of the data collected in this study shows that when the simulation is used in Science, the learning experience of the learners is enhanced. Positive experiences for all four the Dimensions in the FSLSM could be indentified when the ICS was used and this could be linked to specific learning styles. Sensory and Intuitive learners enjoyed conducting the experiment that would normally require unsafe conditions and that the experiment could be set up quickly and with ease. The different dimension brought about by using the ICS was enjoyed by Intuitive learners. The visualisation of the abstract physical systems enhanced the learning for Visual and Verbal learners, whilst Global and Sequential learners felt that they gained a deeper understanding of the photoelectric phenomenon by using the ICS. Reflective learners enjoyed the precision of their pseudo-experimental data, but the Active learners felt that they did not understand the graphs given in the ICS. The interactive control variables and the fact that the learners had an option to work in either a group or on their own, benefitted both Active and Reflective learners.<br>Dissertation (MEd)--University of Pretoria, 2013.<br>gm2014<br>Science, Mathematics and Technology Education<br>unrestricted
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Sabbatucci, Lorenzo <1986&gt. "Fundamental and Applied Aspects of X-Ray Spectrometry: Detector Influence and Photoelectric Effect Cross-Sections." Doctoral thesis, Alma Mater Studiorum - Università di Bologna, 2016. http://amsdottorato.unibo.it/7473/1/Sabbatucci_Lorenzo_tesi.pdf.

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The first part of this work reports the elementary theory of the atomic photoeffect presented in a form that is suited for practical numerical calculation. A detailed derivation of subshell cross sections for both excitation and ionization, comprising the angular distributions of emitted photoelectrons, is presented taking into account the effect of the polarization of the photons. The theoretical formulas have been implemented in a computer program PHOTACS that calculates tables of excitation and ionization cross sections for any element and subshell. Numerical calculations are practicable for excitations to final states with the principal quantum number up to about 20 and for ionization by photons with energy up to about 2 MeV. The effect of the finite width of atomic energy levels is accounted for by convolving the calculated subshell cross section with a Lorentzian profile. The second part of this work reports unfolding strategies for correcting a radiation measurement from the effects of the detector-pulse handling circuitry system. These strategies comprise the correction from the effects of pulse pile-up (PPU) and the detector response function (DRF). A first principles balance equation for second order PPU is derived and solved for the particular case of rectangular pulse shape. A Monte Carlo (MC) strategy is then implemented in the code MCPPU (Multi-shape pulse pile-up correction) allowing handling more general cases. Regarding the DRF, computed with deterministic or MC codes, it is presented the new tool RESOLUTION which introduces in the computed DRF the effects of energy resolution and incomplete charge collection. In the end the computer program UMESTRAT (Unfolding Maximum Entropy STRATegy) is presented in an updated version which include a new constrain to the total number of photons of the spectrum, which can be easily determined by inverting the diagonal efficiency matrix.
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Sabbatucci, Lorenzo <1986&gt. "Fundamental and Applied Aspects of X-Ray Spectrometry: Detector Influence and Photoelectric Effect Cross-Sections." Doctoral thesis, Alma Mater Studiorum - Università di Bologna, 2016. http://amsdottorato.unibo.it/7473/.

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The first part of this work reports the elementary theory of the atomic photoeffect presented in a form that is suited for practical numerical calculation. A detailed derivation of subshell cross sections for both excitation and ionization, comprising the angular distributions of emitted photoelectrons, is presented taking into account the effect of the polarization of the photons. The theoretical formulas have been implemented in a computer program PHOTACS that calculates tables of excitation and ionization cross sections for any element and subshell. Numerical calculations are practicable for excitations to final states with the principal quantum number up to about 20 and for ionization by photons with energy up to about 2 MeV. The effect of the finite width of atomic energy levels is accounted for by convolving the calculated subshell cross section with a Lorentzian profile. The second part of this work reports unfolding strategies for correcting a radiation measurement from the effects of the detector-pulse handling circuitry system. These strategies comprise the correction from the effects of pulse pile-up (PPU) and the detector response function (DRF). A first principles balance equation for second order PPU is derived and solved for the particular case of rectangular pulse shape. A Monte Carlo (MC) strategy is then implemented in the code MCPPU (Multi-shape pulse pile-up correction) allowing handling more general cases. Regarding the DRF, computed with deterministic or MC codes, it is presented the new tool RESOLUTION which introduces in the computed DRF the effects of energy resolution and incomplete charge collection. In the end the computer program UMESTRAT (Unfolding Maximum Entropy STRATegy) is presented in an updated version which include a new constrain to the total number of photons of the spectrum, which can be easily determined by inverting the diagonal efficiency matrix.
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Dogan, M. "Correlation studies of simultaneous excitation-ionization in helium." Thesis, University of Newcastle Upon Tyne, 1999. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.297499.

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Harmer, Stuart William. "Enhanced absorptance photocathodes." Thesis, University of Sussex, 2000. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.311348.

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This thesis addresses one of the major limiting factors in the performance of photomultipliers, that is that the photocathodes employed often only absorb a small fraction, typically less than 25%, of the power in the incident light. Current photocathodes are almost exclusively planar and the starting point of the thesis is the mathematical modelling of both, semitransparent and reflective planar photocathodes. The analysis shows that the absorptance of semitransparent photocathodes increases for light incident beyond the critical angle needed for Attenuated Total Internal Reflection (ATIR). Reflective type planar photocathodes could certainly have their absorptance enhanced by use of silver rather than nickel substrates, as increases in absorptance of 2-3 times are possible for red light. The proposed method for remedying the inherent loss in sensitivity of photomultipliers caused by the non-total absorption of light in the photocathode was to employ a ridged substrate in the photocathode. The ridged substrate, glass or metal for semitransparent and reflective type photocathodes respectively, allows the light multiple interactions with the photoemissive layer. In the case of semitransparent photocathodes ATIR would mean no power is transmitted for those interactions that take place beyond the critical angle of incidence. The mathematical modelling and subsequent analysis of ridged photocathodes show enhanced absorptance (20-30 fold improvements are certainly achievable), especially for light in the red end of the operating spectral range. Further gains in quantum efficiency can follow by the reduction of the optimum photocathode thickness, resulting from the structure, while maintaining high absorptance. Some subwavelength structures are also modelled and analysed to ascertain whether this route could be used to improve the absorptance of photocathodes, the results are inconclusive but generally indicate anti-reflective, rather than absorbing properties. Finally the extremely sparse nature of published permitivity data has been rectified by our own measurements for the permitivities of certain photocathodes over a wide wavelength range.
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Jackson, Stacey Michael. "Optical characterisation of cubic silicon carbide." Thesis, University of Surrey, 1998. http://epubs.surrey.ac.uk/842961/.

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The varied properties of Silicon Carbide (SiC) are helping to launch the material into many new applications, particularly in the field of novel semiconductor devices. In this work, the cubic form of SiC is of interest as a basis for developing integrated optical components. Here, the formation of a suitable SiO2 buried cladding layer has been achieved by high dose oxygen ion implantation. This layer is necessary for the optical confinement of propagating light, and hence optical waveguide fabrication. Results have shown that optical propagation losses of the order of 20 dB/cm are obtainable. Much of this loss can be attributed to mode leakage and volume scattering. Mode leakage is a function of the effective oxide thickness, and volume scattering related to the surface layer damage. These parameters have been shown to be controllable and so suggests that further reduction in the waveguide loss is feasible. Analysis of the layer growth mechanism by RBS, XTEM and XPS proves that SiO2 is formed, and that the extent of formation depends on implant dose and temperature. The excess carbon generated is believed to exit the oxide layer by a number of varying mechanisms. The result of this appears to be a number of stable Si-C-O intermediaries that form regions to either depth extreme of the SiO2 layer. Early furnace tests suggest a need to anneal at temperatures approaching the melting point of the silicon substrate, and that the quality of the virgin material is crutial in controlling the resulting oxide growth.
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Santhanakrishna, Anand Kumar. "Piezoelectric ZnO Nanowires as a Tunable Interface Material for Opto-Electronic Applications." Scholar Commons, 2019. https://scholarcommons.usf.edu/etd/7926.

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Organic electronic devices are sustainable alternatives to the conventional electronics, due to their advantages of low cost, mechanical flexibility and wide range of applications. With the myriad list of organic materials available today, the opportunities to imagine new innovative devices are immense. Organic electronic devices such as OLEDs (organic light emitting diode), OPVs (Organic photovoltaics) and OFETs (organic field effect transistors) are among the leading device categories. Although OLED’s have been a huge commercial success, other categories are not lagging. Radical thinking is necessary to improve on the current performances of these devices. One such thinking is to combine the versatile ZnO (Zinc Oxide) material to organic semiconductors. This can be achieved by exploiting the dual nature of ZnO’s semiconducting and piezoelectric property. Many devices have used ZnO in combination with organic semiconductors for applications ranging from sensors, photovoltaics, OFET’s, memory and many others. The goal of the work is to incorporate the piezoelectric nature of hydrothermally grown ZnO nanowires for Opto-electronic applications. Although the initial research work was done on incorporating the piezo effect of bulk grown ZnO nanowires in improving the efficiency of an OPV, we discovered a unique memory effect in this device by incorporating ZnO nanowires in an inverted organic photovoltaic architecture. The device switched between a rectifying response in dark to resistive behavior under illumination with a finite transition time and was reversible. Since then we decided to explore few of the opto-electronic applications of this technology. The synthesis and characterization of crystalline ZnO nanowires, nanoforest and planar ZnO nanofilm are reported along with the application of these ZnO nanostructures in optoelectronic devices. Noncentro symmetry of crystalline ZnO nanostructures makes it an excellent candidate to be used as piezo functional material and these nanostructures are characterized using electrochemical cell containing ZnO electrode as the working electrode. ZnO nanostructures like nanowires, nanoforest and planar nanofilm are similarly characterized for piezo property using electrochemical technique. Different devices require distinguishing physical and electrical properties of ZnO nanostructures, hence morphology, effect of pre-strain, surface area, surface coverage and thickness of these nanostructures were evaluated for its piezoresponse. It is shown that it was possible to obtain similar piezoresponse among different ZnO nanostructures in addition to taking advantage of the structural benefits among various categories of nanostructures as per requirement. The presented research can be used as the proof-of-the-concept that ZnO nanostructures can be designed and fabricated with a prestrain to adjust the piezo response of the material under external forces. Therefore, the structure with the prestrain can be employed in various electronic and optical devices where the piezo voltage can be used for adjusting the energy band bending at an interface.
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Books on the topic "Photoelectric effect"

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Pilipovich, V. A. Fotoėlektricheskie preobrazovateli v sistemakh opticheskoĭ obrabotki informat͡s︡ii. "Navuka i tėkhnika,", 1990.

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Borghesi, Giovanni Andrea. Una nuova teoria della struttura nucleare: La materia è energia apparentemente immobile e l'energia è materia che risolve questo suo stato di apparente immobilità. Giardini, 1990.

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M, Marshall J., and Dimova-Malinovska D, eds. Photovoltaic and photoactive materials: Properties, technology, and applications. Kluwer Academic, 2002.

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United States. National Aeronautics and Space Administration., ed. A rare gas optics-free absolute photon flux and energy analyzer for solar and planetary observations: Final report. Dept. of Physics and Space Sciences Center, University of Southern California, 1994.

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United States. National Aeronautics and Space Administration., ed. A rare gas optics-free absolute photon flux and energy analyzer for solar and planetary observations: Final report. Dept. of Physics and Space Sciences Center, University of Southern California, 1994.

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United States. National Aeronautics and Space Administration., ed. A rare gas optics-free absolute photon flux and energy analyzer for solar and planetary observations: Final report. Dept. of Physics and Space Sciences Center, University of Southern California, 1994.

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W, Liemohn M., Moore T. E, and United States. National Aeronautics and Space Administration., eds. Photoelectron effects on the self-consistent potential in the collisionless polar wind. National Aeronautics and Space Administration, 1997.

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W, Liemohn M., Moore T. E, and United States. National Aeronautics and Space Administration., eds. Photoelectron effects on the self-consistent potential in the collisionless polar wind. National Aeronautics and Space Administration, 1997.

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1942-, Thompson Michael, ed. Auger electron spectroscopy. Wiley, 1985.

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Ferguson, I. F. Auger microprobe analysis. A. Hilger, 1989.

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Book chapters on the topic "Photoelectric effect"

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Wheaton, Bruce R. "Photoelectric Effect." In Compendium of Quantum Physics. Springer Berlin Heidelberg, 2009. http://dx.doi.org/10.1007/978-3-540-70626-7_143.

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Weik, Martin H. "photoelectric effect." In Computer Science and Communications Dictionary. Springer US, 2000. http://dx.doi.org/10.1007/1-4020-0613-6_13988.

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Weik, Martin H. "external photoelectric effect." In Computer Science and Communications Dictionary. Springer US, 2000. http://dx.doi.org/10.1007/1-4020-0613-6_6667.

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Dodd, John N. "The Photoelectric Effect." In Atoms and Light: Interactions. Springer US, 1991. http://dx.doi.org/10.1007/978-1-4757-9331-4_12.

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Weik, Martin H. "photoelectric-effect detector." In Computer Science and Communications Dictionary. Springer US, 2000. http://dx.doi.org/10.1007/1-4020-0613-6_13989.

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Weik, Martin H. "internal photoelectric effect." In Computer Science and Communications Dictionary. Springer US, 2000. http://dx.doi.org/10.1007/1-4020-0613-6_9421.

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Weik, Martin H. "external photoelectric effect detector." In Computer Science and Communications Dictionary. Springer US, 2000. http://dx.doi.org/10.1007/1-4020-0613-6_6668.

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Weik, Martin H. "extrinsic internal photoelectric effect." In Computer Science and Communications Dictionary. Springer US, 2000. http://dx.doi.org/10.1007/1-4020-0613-6_6696.

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Grometstein, Alan A. "The Photoelectric Effect (1902)." In The Roots of Things. Springer US, 1999. http://dx.doi.org/10.1007/978-1-4615-4877-5_6.

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Weik, Martin H. "internal photoelectric-effect detector." In Computer Science and Communications Dictionary. Springer US, 2000. http://dx.doi.org/10.1007/1-4020-0613-6_9422.

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Conference papers on the topic "Photoelectric effect"

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Fiolhais, Manuel. "Photoelectric Effect and Relativity." In 2023 Photonics & Electromagnetics Research Symposium (PIERS). IEEE, 2023. http://dx.doi.org/10.1109/piers59004.2023.10221264.

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Eberly, J. H., Phay J. Ho, R. Panfili, and S. L. Haan. "A completely classical photoelectric effect?" In Frontiers in Optics. OSA, 2004. http://dx.doi.org/10.1364/fio.2004.fma1.

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Shaw, Ping-Shine, Shaul Hanany, Yee Liu, et al. "Vectorial photoelectric effect at 2.69 keV." In San Diego, '91, San Diego, CA, edited by D. P. Siddons. SPIE, 1991. http://dx.doi.org/10.1117/12.50578.

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Gong, BingXin. "The Classical Electrodynamics Approach To Explain The Photoelectric Effect And The Photoelectric Emission." In Frontiers in Optics. OSA, 2005. http://dx.doi.org/10.1364/fio.2005.jwa14.

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Gong, BingXin. "The classical electrodynamics approach to explain the photoelectric effect and the photoelectric emission." In ICO20:Biomedical Optics, edited by Gert von Bally and Qingming Luo. SPIE, 2006. http://dx.doi.org/10.1117/12.667466.

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Miaja, Luis, Guido Saathoff, Chifong Lei, et al. "Laser-Assisted Photoelectric Effect on Pt(111)." In International Conference on Ultrafast Phenomena. OSA, 2006. http://dx.doi.org/10.1364/up.2006.thd18.

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Miaja, Luis, Guido Saathoff, Chifong Lei, et al. "The laser-assisted photoelectric effect on surfaces." In 2006 Conference on Lasers and Electro-Optics and 2006 Quantum Electronics and Laser Science Conference. IEEE, 2006. http://dx.doi.org/10.1109/cleo.2006.4628955.

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Frejlich, Jaime, Ivan de Oliveira, Jesiel F. Carvalho, William R. Araújo, Marc Georges, and Thizy Cedric. "Photoelectric Conversion Effect in Non-Photovoltaic Photorefractive Materials." In Latin America Optics and Photonics Conference. OSA, 2014. http://dx.doi.org/10.1364/laop.2014.lm1a.1.

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Foong, S. K., P. Lee, D. Wong, Y. P. Chee, Boonchoat Paosawatyanyong, and Pornrat Wattanakasiwich. "On the Conceptual Understanding of the Photoelectric Effect." In INTERNATIONAL CONFERENCE ON PHYSICS EDUCATION: ICPE-2009. AIP, 2010. http://dx.doi.org/10.1063/1.3479845.

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Khots, Boris, and Dmitriy Khots. "Photoelectric effect from observer's mathematics point of view." In 10TH INTERNATIONAL CONFERENCE ON MATHEMATICAL PROBLEMS IN ENGINEERING, AEROSPACE AND SCIENCES: ICNPAA 2014. AIP Publishing LLC, 2014. http://dx.doi.org/10.1063/1.4904614.

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