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1

SOEZIMA, Hiroyoshi. "Electron probe micro analysis." Hyomen Kagaku 10, no. 10 (1989): 710–17. http://dx.doi.org/10.1380/jsssj.10.710.

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2

Lewis, R. A. "Gas analysis by electron probe." Micron and Microscopica Acta 16, no. 4 (1985): 271–75. http://dx.doi.org/10.1016/0739-6260(85)90051-6.

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3

KENNEDY, R. V., and J. E. ALLEN. "The floating potential of spherical probes and dust grains. Part 1. Radial motion theory." Journal of Plasma Physics 67, no. 4 (2002): 243–50. http://dx.doi.org/10.1017/s0022377802001691.

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A theoretical analysis of spherical probes in plasmas is presented. It is assumed that the probe is at floating potential, that ion motion with respect to the probe is radial and that the electrons are Maxwellian. The analysis shows that as probe radius divided by Debye length tends to zero, the ratio of floating potential to electron temperature also goes to zero.
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4

Keenan IV, James A., and William A. Lamberti. "Quantitative Electron Probe Analysis of Zeolites." Microscopy and Microanalysis 10, S02 (2004): 486–87. http://dx.doi.org/10.1017/s1431927604885854.

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5

Somlyo, A. P., and Avril V. Somlyo. "Electron Probe Analysis and Cell Physiology." Proceedings, annual meeting, Electron Microscopy Society of America 43 (August 1985): 2–5. http://dx.doi.org/10.1017/s0424820100117169.

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Electron probe x-ray microanalysis (EPMA) of rapidly frozen tissues is a uniquely powerful method for dealing with a large class of general problems in cell physiology, as it is suitable for measuring, under direct vision, the elemental composition of cells and cell organelles. EPMA can reach a spatial resolution of at least 10nm, and its practically attainable sensitivity (for Ca) is 0.3mmol Ca/kg dry wt. Therefore, the composition of mitochondria and of other organelles, as small as the endoplasmic reticulum (ER), can be quantitated with EPMA. The most extensive applications of EPMA to cell
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6

LECHENE, C. "Electron-Probe Analysis of Cultured Cells." Annals of the New York Academy of Sciences 483, no. 1 Recent Advanc (1986): 270–83. http://dx.doi.org/10.1111/j.1749-6632.1986.tb34532.x.

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7

MATSUMOTO, Keisaku, and Takao HIRAJIMA. "Modal analysis using scanning electron probe microanalyzer." Japanese Magazine of Mineralogical and Petrological Sciences 35, no. 2 (2006): 97–108. http://dx.doi.org/10.2465/gkk.35.97.

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8

Ul-Hamid, Anwar, Hani M. Tawancy, Abdul-Rashid I. Mohammed, Said S. Al-Jaroudi, and Nureddin M. Abbas. "Quantitative WDS analysis using electron probe microanalyzer." Materials Characterization 56, no. 3 (2006): 192–99. http://dx.doi.org/10.1016/j.matchar.2005.11.007.

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9

Jurek, Karel, and Ondrej Gedeon. "Analysis of alkali-silicate glasses by electron probe analysis." Spectrochimica Acta Part B: Atomic Spectroscopy 58, no. 4 (2003): 741–44. http://dx.doi.org/10.1016/s0584-8547(02)00288-4.

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10

Bell, David C., Anthony J. Garratt-Reed, and Linn W. Hobbs. "RDF Analysis of Radiation-Amorphized SiC using a field Emission Scanning Electron Microscope." Microscopy and Microanalysis 4, S2 (1998): 700–701. http://dx.doi.org/10.1017/s143192760002362x.

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AbstractFast electrons are a particularly useful chemical and structural probe for the small sample volumes associated with ion- or fast electron-irradiation-induced amorphization, because of their much stronger interaction with matter than for X-rays or neutrons, and also because they can be readily focused to small probes. Three derivative signals are particularly rich in information: the angular distribution of scattered electrons (which is utilized in both diffraction and imaging studies); the energy loss spectrum of scattered electrons (electron energy loss spectroscopy, or EELS); and the
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11

Scheinfein, Michael R., John Unguris, Daniel T. Pierce, and Robert J. Celotta. "Surface Magnetic Microstructural Analysis using Scanning Electron Microscopy with Polarization Analysis (SEMPA)." Proceedings, annual meeting, Electron Microscopy Society of America 48, no. 1 (1990): 216–17. http://dx.doi.org/10.1017/s042482010017983x.

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High resolution imaging of magnetic microstructure has important ramifications for both fundamental studies of magnetism and the technology surrounding the magnetic recording industry. In SEMPA, a focused beam of electrons excites secondary electrons on a ferromagnet's surface. The secondaries leave the solid with an electron spin polarization which is characteristic of the net spin density in the ferromagnet. This is related directly to the sample magnetization. By scanning the beam and analyzing the secondary electron spin polarization at each point, a magnetization map of the ferromagnet's
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12

Cliff, G., and P. B. Kenway. "The future of AEM: Toward atom analysis." Proceedings, annual meeting, Electron Microscopy Society of America 47 (August 6, 1989): 200–201. http://dx.doi.org/10.1017/s0424820100152975.

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The ultimate goal of analytical electron microscopy (AEM) is a minimum detection limit, MDL, of one atom! Utilising the small probes and the high current densities attainable using a field emission gun, FEG, in a scanning transmission electron microscope, STEM, the MDL is at present 100 atoms. This discussion will show that an MDL of 1 atom could be achieved with existing engineering technology available on the current generation of AEM instrumentation.Indeed if AEM was like hi-fi an AEM analyst could today combine features of different microscopes to build an AEM capable of atom detection!The
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13

Wu, Ryan J., Anudha Mittal, Michael L. Odlyzko, and K. Andre Mkhoyan. "Simplifying Electron Beam Channeling in Scanning Transmission Electron Microscopy (STEM)." Microscopy and Microanalysis 23, no. 4 (2017): 794–808. http://dx.doi.org/10.1017/s143192761700068x.

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AbstractSub-angstrom scanning transmission electron microscopy (STEM) allows quantitative column-by-column analysis of crystalline specimens via annular dark-field images. The intensity of electrons scattered from a particular location in an atomic column depends on the intensity of the electron probe at that location. Electron beam channeling causes oscillations in the STEM probe intensity during specimen propagation, which leads to differences in the beam intensity incident at different depths. Understanding the parameters that control this complex behavior is critical for interpreting exper
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14

Somlyo, Andrew P. "Cell calcium measurement with electron probe and electron energy loss analysis." Cell Calcium 6, no. 1-2 (1985): 197–212. http://dx.doi.org/10.1016/0143-4160(85)90044-2.

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15

Darznek, S. A., V. B. Mityukhlyaev, P. A. Todua, and M. N. Filippov. "Electron Probe X-Ray Spectral Analysis of Nanoparticles." Inorganic Materials 54, no. 14 (2018): 1412–16. http://dx.doi.org/10.1134/s0020168518140054.

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16

Suzuki, M., T. Kaneyama, E. Watanabe, M. Naruse, and Y. Kokubo. "An Application of 200kV Ultrahigh Resolution Analytical Electron Microscope." Proceedings, annual meeting, Electron Microscopy Society of America 48, no. 2 (1990): 98–99. http://dx.doi.org/10.1017/s0424820100134089.

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A 200 kV ultrahigh resolution analytical electron microscope (UHRAEM), JEM-2010, enables both ultrahigh resolution imaging with a theoretical point resolution of 0.194 nm and nm-area analysis. In this paper, its preliminary data for x-ray analysis (Energy Dispersive X ray Spectroscopy: EDS) and its application data will be shown.An objective lens polepiece has been designed to minimize the spherical aberration coefficient (Cs) of the prefield and thereby increase the probe current in small probe size for nm-area EDS analysis. Measured values of Cs and chromatic aberration coefficient (Cc) are
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17

Small, JA, and JT Armstrong. "Improving the Analtical Accuracy in the Analysis of Particles by Employing Low Voltage Analysis:." Microscopy and Microanalysis 6, S2 (2000): 924–25. http://dx.doi.org/10.1017/s1431927600037119.

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The energy of the electron beam, in conventional electron probe microanalysis, is generally in the range of 15-25 keV which provides the necessary overvoltage to excite efficiently the K and L x-ray lines for elements with atomic numbers in the range of about 5-83. One of the primary microanalytical methods for obtaining compositional information on particles is X-ray analysis in the electron probe and these same voltage criteria have been applied to the procedures developed for this purpose. The main difference in analytical procedures for bulk samples and particles is that corrections have t
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18

EGURO, Toru, Toru MAEDA, Masaaki OGAWA, Kazuaki YONEMOTO, Hisayoshi TANAKA, and Ichiroh KATSUUMI. "Electron Probe Micro-Analysis of a Contact Probe after Er:YAG Laser Tooth Ablation." Dental Materials Journal 22, no. 1 (2003): 80–86. http://dx.doi.org/10.4012/dmj.22.80.

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19

McGibbon, A. J., and S. J. Pennycook. "Direct retrieval of crystal structures by maximum-entropy analysis of incoherent Z-contrast images." Proceedings, annual meeting, Electron Microscopy Society of America 52 (1994): 916–17. http://dx.doi.org/10.1017/s0424820100172310.

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Z-contrast imaging of crystalline specimens in a scanning transmission electron microscope (STEM) can provide directly interpretable images of crystal structures at atomic resolution with strong compositional sensitivity. The key feature of the technique is that, by recording images using high-anglethermally diffuse scattered electrons, the resultant image is incoherent, and can be interpreted as aconvolution between the incident electron probe and the projected crystal structure of the specimen. Consequently, the technique is ideally suited to the application of deconvolution routines which e
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20

LeFurgey, A., and P. Ingram. "Calcium measurements with electron probe X-ray and electron energy loss analysis." Environmental Health Perspectives 84 (March 1990): 57–73. http://dx.doi.org/10.1289/ehp.908457.

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21

Na, Byung-Keun, Kwang-Ho You, Dae-Woong Kim, Hong-Young Chang, Shin-Jae You, and Jung-Hyung Kim. "Cutoff probe using Fourier analysis for electron density measurement." Review of Scientific Instruments 83, no. 1 (2012): 013510. http://dx.doi.org/10.1063/1.3680103.

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22

Jensen, O. Mejlhede, A. M. Coats, and F. P. Glasser. "Chloride ingress profiles measured by electron probe micro analysis." Cement and Concrete Research 26, no. 11 (1996): 1695–705. http://dx.doi.org/10.1016/s0008-8846(96)00158-5.

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23

Warner, Ronald R., Mark C. Myers, and Dennis A. Taylor. "Electron Probe Analysis of Human Skin: Element Concentration Profiles." Journal of Investigative Dermatology 90, no. 1 (1988): 78–85. http://dx.doi.org/10.1111/1523-1747.ep12462576.

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24

Hashimoto, T., and D. C. Joy. "The nano-probe profile of the hf-2000 field-emission TEM." Proceedings, annual meeting, Electron Microscopy Society of America 50, no. 2 (1992): 1208–9. http://dx.doi.org/10.1017/s0424820100130675.

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The probe profile is as important as the probe size for nano-meter area X-ray analysis. Assuming the electron distribution of the probe as the Gaussian, the probe size d is usually defined as the full width half maximum (FWHM) of the probe distribution, which is suitable for SEM/STEM resolution. However, for the X-ray analysis of thin specimens, the full width tenth maximum (FWTM) which contains 90 % of the incident electrons, and thus 90 % of the × rays generated, is more suitable. For a Gaussian probe FWTM = 1.82 × FWHM. Recent electron microscopes with higher than 200 kV acceleration voltag
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25

Willich, Peter, and Kirsten Schiffmann. "Electron probe microanalysis of borophosphosilicate coatings." Proceedings, annual meeting, Electron Microscopy Society of America 48, no. 2 (1990): 226–27. http://dx.doi.org/10.1017/s0424820100134739.

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Planarization and passivation of integrated circuits by use of borophosphosilicate glass (BPSG) is of considerable technological interest. BPSG is prepared by chemical vapour deposition and electron probe microanalysis (EPMA) offers the possibility of non-destructive characterization in respect of composition and film thickness. Particular difficulties of EPMA are due to the insulating character of BPSG in combination with the demand for analysis of ultra-light elements (B and O). However, EPMA of BPSG also demonstrates the accuracy of recent bulk and thin film data processing when based on re
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26

Dillé, John E., Douglas C. Bittel, Kathleen Ross, and J. Perry Gustafson. "Preparing plant chromosomes for scanning electron microscopy." Genome 33, no. 3 (1990): 333–39. http://dx.doi.org/10.1139/g90-052.

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The scanning electron microscope may be useful in the analysis of plant chromosomes treated with in situ hybridization, especially when the probes and (or) chromosomes are near or beyond the resolution of the light microscope. Usual methods of plant chromosome preparation are unsuitable for scanning electron microscope observation as a result of cellular debris, which also interferes with probe hybridization. A method is described whereby protoplasts are obtained from fixed root tips by enzymatic digestion and applied to slides in a manner that produces little or no cellular debris overlying t
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27

Small, John A., and Matthew A. Calderone. "Accuracies associated with the automated electron probe analysis of particulate populations." Proceedings, annual meeting, Electron Microscopy Society of America 50, no. 2 (1992): 1494–95. http://dx.doi.org/10.1017/s0424820100132108.

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The analysis of large numbers of particles by automated scanning electron microscopy/ electron probe (ASEM) has been used in conjunction with multivariate analysis algorithms to classify atmospheric particles into different groups based on size, shape, and elemental composition. These groups or clusters and the number of particles belonging to each are often used to develop source apportionment for the sampled aerosol.There are several limitations particularly with the compositional analysis aspects of the automated routines that may limit the information that can be obtained from the sample.
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28

McNeil, J. P., J. E. Carter, C. W. Boudreaux, F. McDonald, J. A. Tucker, and J. A. C. King. "Electron Probe Microanalysis Of Spironolactone Bodies." Microscopy and Microanalysis 5, S2 (1999): 1288–89. http://dx.doi.org/10.1017/s1431927600019760.

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Spironolactone bodies (SB) were first described in 1963 by Janigan. These laminated, whorled structures are seen in cells of the adrenal zona glomerulosa in patients treated with the drug spironolactone. Spironolactone is an aldosterone antagonist. Hyperaldosteronism may result from excess production by the adrenal cortex. By both light microscopy and transmission electron microscopy (TEM), SB have a distinctive, laminated appearance. Kovacs, et al. observed that SB are composed of cellular constituents. To our knowledge, SB have not been analyzed using scanning electron microscopy (SEM) and e
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29

Laakso, H., T. L. Aggson, and R. F. Pfaff. "Plasma gradient effects on double-probe measurements in the magnetosphere." Annales Geophysicae 13, no. 2 (1995): 130–46. http://dx.doi.org/10.1007/s00585-995-0130-z.

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Abstract. The effects on double-probe electric field measurements induced by electron density and temperature gradients are investigated. We show that on some occasions such gradients may lead to marked spurious electric fields if the probes are assumed to lie at the same probe potential with respect to the plasma. The use of a proper bias current will decrease the magnitude of such an error. When the probes are near the plasma potential, the magnitude of these error signals, ∆E, can vary as ∆E ~ Te(∆ne/ne)+0.5∆Te, where Te is the electron temperature, ∆ne/ne the relative electron density vari
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Tsuji, Kouichi, Kesami Saito, Katsuhiko Asami, Kazuaki Wagatsuma, Filip Delalieux, and Zoya Spolnik. "Localized thin-film analysis by grazing-exit electron probe microanalysis." Spectrochimica Acta Part B: Atomic Spectroscopy 57, no. 5 (2002): 897–906. http://dx.doi.org/10.1016/s0584-8547(02)00020-4.

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31

Tsuji, Kouichi, Kazuaki Wagatsuma, Rik Nullens, and René E. Van Grieken. "Grazing Exit Electron Probe Microanalysis for Surface and Particle Analysis." Analytical Chemistry 71, no. 13 (1999): 2497–501. http://dx.doi.org/10.1021/ac990075p.

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32

Wang, Frank Cheng-Yu. "Submicrometer phase chemical composition analysis with an electron probe microanalyzer." X-Ray Spectrometry 23, no. 5 (1994): 203–7. http://dx.doi.org/10.1002/xrs.1300230504.

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33

Walsh, L. G., and J. M. Tormey. "Cellular compartmentation in ischemic myocardium: indirect analysis by electron probe." American Journal of Physiology-Heart and Circulatory Physiology 255, no. 4 (1988): H929—H936. http://dx.doi.org/10.1152/ajpheart.1988.255.4.h929.

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Electron probe microanalysis (EPMA) was carried out directly on myocardial cells and on the myofibrils and the mitochondria within them. A third subcellular compartment, which contains sarcoplasmic reticulum (SR), was measured indirectly. The percent of the total cell calcium content that resides within this "hidden" compartment was calculated from cell data minus weighted myofibril and mitochondria data. This approach was applied to control, ischemic, and reperfused myocardium, and other elements were also quantified. We found that the calcium content of this third compartment is little chang
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34

Ho, R., Z. Jia, A. P. Somlyo, and Z. Shao. "Improved precision of quantitating calcium in biological electron probe analysis." Journal of Microscopy 204, no. 1 (2001): 61–68. http://dx.doi.org/10.1046/j.1365-2818.2001.00941.x.

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35

LeFurgey, Ann, Peter Ingram, and Lazaro J. Mandel. "Heterogeneity of calcium compartmentation: Electron probe analysis of renal tubules." Journal of Membrane Biology 94, no. 2 (1986): 191–96. http://dx.doi.org/10.1007/bf01871198.

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36

Bassell, Gary, and Robert H. Singer. "Ultrastructural analysis of the spatial distribution of MRNA." Proceedings, annual meeting, Electron Microscopy Society of America 50, no. 1 (1992): 552–53. http://dx.doi.org/10.1017/s0424820100123167.

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We have been investigating the spatial distribution of nucleic acids intracellularly using in situ hybridization. The use of non-isotopic nucleotide analogs incorporated into the DNA probe allows the detection of the probe at its site of hybridization within the cell. This approach therefore is compatible with the high resolution available by electron microscopy. Biotinated or digoxigenated probe can be detected by antibodies conjugated to colloidal gold. Because mRNA serves as a template for the probe fragments, the colloidal gold particles are detected as arrays which allow it to be unequivo
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37

León, Gloria, Charles Fiori, Pradeep Das, et al. "Electron probe analysis and biochemical characterization of electron-dense granules secreted by Entamoeba histolytica." Molecular and Biochemical Parasitology 85, no. 2 (1997): 233–42. http://dx.doi.org/10.1016/s0166-6851(97)02833-8.

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38

Isabell, Thomas C., and Paul E. Fischione. "Plasma Cleaning for Electron Microscopy." Microscopy and Microanalysis 4, S2 (1998): 872–73. http://dx.doi.org/10.1017/s143192760002448x.

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Specimen contamination and amorphous irradiation damage severely limit the ability to perform accurate electron microscope analysis of materials, especially as specimen areas of interest decrease in size. To analyze smaller areas of interest, electron probe sizes have decreased, while probe currents have increased. The combination of these two factors results in an increase in the amount of carbonaceous contamination formed on the specimen under the electron beam. Recently, the use of low energy plasmas has been shown to be effective in preventing such contamination from occurring (1-3). For T
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39

Anstis, Geoffrey R. "The 1s-State Analysis Applied to High-Angle, Annular Dark-Field Image Interpretation—When Can We Use It?" Microscopy and Microanalysis 10, no. 1 (2004): 4–8. http://dx.doi.org/10.1017/s1431927604040255.

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A small probe centered on an atomic column excites the bound and unbound states of the two-dimensional projected potential of the column. It has been argued that, even when several states are excited, only the 1sstate is sufficiently localized to contribute a signal to the high-angle detector. This article shows that non-1sstates do make a significant contribution for certain incident probe profiles. The contribution of the 1sstate to the thermal diffuse scattering is calculated directly. Sub-Ångstrom probes formed by Cs-corrected lenses excite predominantly the 1sstate and contributions from
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40

Deconihout, B., P. Pareige, D. Blavette, A. Bostel, and A. Menand. "The Tomographic Atom Probe: A New Dimension In Material Analysis." Microscopy and Microanalysis 4, S2 (1998): 78–79. http://dx.doi.org/10.1017/s1431927600020511.

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Today material science requires the use of increasingly powerful tools in material analysis. The last twenty years have witnessed the development of a number of analytical techniques. However, among these techniques, only a few allow observation and analysis of materials at the nanometer level ; one can mention scanning transmission electron microscopy coupled with electron energy loss spectrometry (STEM-EELS), SIMS and atom-probe techniques. In the STEM combined with electron energy loss spectrometry the spatial resolution can be better than one nanometer on a wide scanning area. However the
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41

Cooper, Bridgette, Přemysl Kolorenč, Leszek J. Frasinski, Vitali Averbukh, and Jon P. Marangos. "Analysis of a measurement scheme for ultrafast hole dynamics by few femtosecond resolution X-ray pump–probe Auger spectroscopy." Faraday Discuss. 171 (2014): 93–111. http://dx.doi.org/10.1039/c4fd00051j.

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Ultrafast hole dynamics created in molecular systems as a result of sudden ionisation is the focus of much attention in the field of attosecond science. Using the molecule glycine we show through ab initio simulations that the dynamics of a hole, arising from ionisation in the inner valence region, evolves with a timescale appropriate to be measured using X-ray pulses from the current generation of SASE free electron lasers. The examined pump–probe scheme uses X-rays with photon energy below the K edge of carbon (275–280 eV) that will ionise from the inner valence region. A second probe X-ray
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42

Nakamura, N., K. Anno та S. Kono. "Structure analysis of the single-domain surface by μ-probe Auger electron diffraction and μ-probe reflection high energy electron diffraction". Surface Science Letters 256, № 1-2 (1991): A534. http://dx.doi.org/10.1016/0167-2584(91)91169-w.

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43

West, Paul E., Sid Marchesse-Rugona, and Zhuoning Li. "Fractal analysis with scanning probe microscopy." Proceedings, annual meeting, Electron Microscopy Society of America 50, no. 2 (1992): 1046–47. http://dx.doi.org/10.1017/s0424820100129863.

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Surface roughness determined qualitatively by direct visualization can be correlated to several physical properties. However, finding a suitable method of quantifying surface roughness, until recently, has been difficult. The concept of Fractal Dimension, recently popularized by Mandelbrot(1982) has been extremely successful in quantifying surface roughness and relating it to such measurable physical properties such as; cleanability, catalytic activity, rate of corrosion, and even flavor.Atomic Force Microscopes permit direct three dimensional measurements of surface microstructure. AFM images
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44

Vincent, R. "Analysis of multiple diffraction contrast." Proceedings, annual meeting, Electron Microscopy Society of America 45 (August 1987): 48–51. http://dx.doi.org/10.1017/s0424820100125270.

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Transmission microscopy of modern alloys, ceramics and semiconductor/metal contact/insulator assemblies often discloses unfamiliar crystalline compounds, either uncharted on the relevant phase diagrams (if available) or metastable. Although the standard technigues of convergent beam electron diffraction (CBED) are sufficient to establish the space group, further progress towards defining the contents of the unit cell requires at least some qualitative estimate of the structure factors F, which are obscured by the varieties of multiple diffraction paths followed by electrons. However, modern an
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45

Escaig-Haye, F., V. Grigoriev, G. Peranzi, P. Lestienne, and J. G. Fournier. "Analysis of human mitochondrial transcripts using electron microscopic in situ hybridization." Journal of Cell Science 100, no. 4 (1991): 851–62. http://dx.doi.org/10.1242/jcs.100.4.851.

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Human mitochondrial transcripts have been examined at the ultrastructural level. After contact with ultrathin sections of a human lymphoid cell line (CEM) embedded in Lowicryl K4M, biotinylated mitochondrial probes yield specific hybrids identified by a colloidal gold immunocytochemistry marker that visualizes rRNA and mRNA coding for respiratory chain polypeptides CO II, CO III and ATPase-6. The mitochondrial transcripts are preferentially located close to the inner membrane, particularly the cristae, suggesting that intra-organelle protein synthesis is intimately associated with the mitochon
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46

Matthews, Mike B., Stuart L. Kearns, and Ben Buse. "Electron Beam-Induced Carbon Erosion and the Impact on Electron Probe Microanalysis." Microscopy and Microanalysis 24, no. 6 (2018): 612–22. http://dx.doi.org/10.1017/s1431927618015398.

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AbstractElectron beam-induced carbon contamination is a balance between simultaneous deposition and erosion processes. Net erosion rates for a 25 nA 3 kV beam can reduce a 5 nm C coating by 20% in 60 s. Measurements were made on C-coated Bi substrates, with coating thicknesses of 5–20 nm, over a range of analysis conditions. Erosion showed a step-like increase with increasing electron flux density. Both the erosion rate and its rate of change increase with decreasing accelerating voltage. As the flux density decreases the rate of change increases more rapidly with decreasing voltage. Time-depe
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47

Reznik, P. L., V. M. Zamyatin, and V. S. Mushnikov. "Thermal analysis and electron probe microanalysis of the AK6 aluminum alloy." Russian Journal of Non-Ferrous Metals 54, no. 1 (2013): 62–65. http://dx.doi.org/10.3103/s1067821213010173.

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GE, Xiangkun, Mingkuan QIN, and Guang FAN. "Study and Application of Electron Probe Micro-analysis Dating for Uraninite." Acta Geologica Sinica - English Edition 88, s2 (2014): 1345–46. http://dx.doi.org/10.1111/1755-6724.12381_5.

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Poeml, Philipp, Karen Wright, Hirokazu Ohta, Luca Capriotti, and Jason Harp. "Comparison of Two Irradiated Metallic Fuels by Electron Probe Micro-analysis." Microscopy and Microanalysis 26, S2 (2020): 874. http://dx.doi.org/10.1017/s1431927620016153.

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Fernando, Sujatha S. E. "Pseudomelanosis duodeni: A case report with electron-probe X-ray analysis." Pathology 22, no. 3 (1990): 169–72. http://dx.doi.org/10.3109/00313029009063559.

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