Academic literature on the topic 'Cross section'

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Journal articles on the topic "Cross section"

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Rudstam, Gösta. "Neutron Cross Sections, Volume 2, Neutron Cross Section Curves." Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment 281, no. 1 (August 1989): 250. http://dx.doi.org/10.1016/0168-9002(89)91244-8.

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Katz, Robert. "Cross section." International Journal of Radiation Applications and Instrumentation. Part A. Applied Radiation and Isotopes 41, no. 6 (January 1990): 563–67. http://dx.doi.org/10.1016/0883-2889(90)90040-n.

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Gardner, L., and T. M. Chan. "Cross-section classification of elliptical hollow sections." Steel and Composite Structures 7, no. 3 (June 25, 2007): 185–200. http://dx.doi.org/10.12989/scs.2007.7.3.185.

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Camarda, H. S., T. W. Phillips, and R. M. White. "Neutron total cross section ofCa40and cross section difference ofCa44." Physical Review C 34, no. 3 (September 1, 1986): 810–14. http://dx.doi.org/10.1103/physrevc.34.810.

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Easa, Said M. "Simplifying roadway cross sections without reducing volume accuracy." Canadian Journal of Civil Engineering 16, no. 4 (August 1, 1989): 483–88. http://dx.doi.org/10.1139/l89-078.

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A method for simplifying irregular ground profile of roadway cross sections by a straight line is presented. The presented method does not affect the accuracy of earthwork volume computations. Two types of cross sections are considered: cut (or fill) and transition sections. For a cut (or fill) section, the simplified section is designed such that its area equals that of the original section. This is accomplished by adjusting the least-squares (LS) parameters. Three cases of adjustments that depend on the area of the original section and the unadjusted LS parameters are presented. These cases preserve the section type (cut or fill) and, as much as possible, the general shape of the original section. For a transition section, the simplified section is designed such that its cut and fill areas equal those of the original section. These conditions of equal areas are used to develop formulas for designing the simplified section directly. Application of the method is illustrated by numerical examples. Key words: roadway, cross section, irregular, least squares, linear profile, earthwork volume.
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Gopalakrishnan, V. "Temperature dependence of unshielded cross-sections in multigroup cross-section sets." Annals of Nuclear Energy 27, no. 11 (July 2000): 1029–37. http://dx.doi.org/10.1016/s0306-4549(00)00012-8.

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Pavlovskaia, Е. А., and А. К. Khudoley. "TECTONICS AND GEOLOGICAL STRUCTURE OF THE MAYA-KYLLAKH ZONE (SOUTH VERKHOYANSK REGION) OBTAINED FROM BALANCED CROSS-SECTIONS." Geodynamics & Tectonophysics 15, no. 1 (February 16, 2024): 0742. http://dx.doi.org/10.5800/gt-2024-15-1-0742.

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A technique for balancing cross-sections is used to construct geometrically consistent structural sections through fold-thrust belts. Unlike the predecessor studies, the balanced cross-sections in this study were obtained using the deep seismic sounding and well data and Move Software. Two detailed balanced cross-sections pass through the central part of the South Verkhoyansk region: the 80 km long Yudoma cross-section running along 59°45ʹ N, and the 122 km long Allakh-Yun cross-section within 60°40ʹ – 61°00ʹ N. Both sections are characterized by a thin-skinned structure, "mechanical stratigraphy", emergent leading imbricate fans in the foreland, thick Riphean strata, and eastward dip of the detachment surface. The surface shortening values are ~33 % for the Yudoma cross-section and ~26 % for the Allakh-Yun cross-section, showing an old-to-young-complex decrease from 39 % for the Yudoma cross-section to 19 % for the Allakh-Yun cross-section. On the Yudoma cross-section, the detachment occurs in the Middle Riphean deposits and dips down to 8 km; on the Allah-Yun cross-section, it occurs in the Lower Riphean deposits and dips down to 15 km. The difference in the detachment level may indicate the presence of a ramp between the cross-sections or an inaccurate localization of a ramp between the Central and Kyllakh-Eibeke-Khayata segments. The changes in the geological structure across and along the strike of the orogen are traced; the obtained cross-sections are compared with each other, with other cross-sections across the South and West Verkhoyansk regions, and with the cross-sections through the foreland fold and thrust belts of the Urals, Appalachians, and Cordillera of North America.
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Bates, A. D., R. P. Rassool, E. A. Milne, M. N. Thompson, and K. G. McNeill. "N15photoneutron cross section." Physical Review C 40, no. 2 (August 1, 1989): 506–14. http://dx.doi.org/10.1103/physrevc.40.506.

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McLean, D. J., M. N. Thompson, D. Zubanov, K. G. McNeill, J. W. Jury, and B. L. Berman. "C14photoproton cross section." Physical Review C 44, no. 3 (September 1, 1991): 1137–47. http://dx.doi.org/10.1103/physrevc.44.1137.

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Santini, Thiago, Paolo Rech, Gabriel Luca Nazar, and Flávio Rech Wagner. "Beyond Cross-Section." ACM Transactions on Embedded Computing Systems 15, no. 1 (February 20, 2016): 1–16. http://dx.doi.org/10.1145/2794148.

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Dissertations / Theses on the topic "Cross section"

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Lamo, Ana Rosa. "Cross section distribution dynamics." Thesis, London School of Economics and Political Science (University of London), 1996. http://etheses.lse.ac.uk/1448/.

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This thesis contains four chapters. Each chapter constitutes an empirical exercise in which I apply econometric ideas on studying the dynamics of large cross sections of data (Random Fields). Three of them concern the empirics of convergence and the fourth analyses business cycle fluctuations. The first, "Notes on Convergence Empirics: Some Calculations for Spanish Regions," describes the econometric methods for studying the dynamics of the distributions and how to characterise convergence in this framework, explains why the standard cross-section regression analysis is misleading when testing for convergence and then performs some calculations for regions in Spain. The second chapter, "Dynamics of the Income Distribution Across OECD Countries", considers its baseline hypotheses to be those generated by the Solow growth model. Using sequential conditioning, it studies whether the convergence hypothesis implications can be shown to hold for the OECD economies. It finds that neither absolute nor conditional convergence, in the sense of economies approaching the OECD average, has taken place. The third chapter, "Cross Sectional Firm Dynamics: Theory and Empirical Results", extends ideas of distribution dynamics to a discrete choice setting, and extends the reasoning of Galton's Fallacy to the logit model. It provides evidence of the tendency of firm sizes to converge for the US chemicals sector by analysing dynamically evolving cross-section distributions. Finally, the fourth chapter, "Unemployment in Europe and Regional Labour Fluctuations" applies distribution dynamics ideas to a business cycle setting. It analyses the dynamics of employment for 51 European regions from 1960 to 1990, addressing the issue of whether regional shocks have aggregate effects on unemployment or the opposite. It uses a model for non-stationary evolving distributions to identify idiosyncratic and aggregate disturbances.
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Tosetti, Elisa. "Cross section dependence in panels." Thesis, University of Cambridge, 2009. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.611351.

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Li, Xiang. "Compressive Radar Cross Section Computation." Thesis, Université d'Ottawa / University of Ottawa, 2020. http://hdl.handle.net/10393/40073.

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Compressive Sensing (CS) is a novel signal-processing paradigm that allows sampling of sparse or compressible signals at lower than Nyquist rate. The past decade has seen substantial research on imaging applications using compressive sensing. In this thesis, CS is combined with the commercial electromagnetic (EM) simulation software newFASANT to improve its efficiency in solving EM scattering problems such as Radar Cross Section (RCS) of complex targets at GHz frequencies. This thesis proposes a CS-RCS approach that allows efficient and accurate recovery of under-sampled RCSs measured from a random set of incident angles using an accelerated iterative soft thresh-holding reconstruction algorithm. The RCS results of a generic missile and a Canadian KingAir aircraft model simulated using Physical Optics (PO) as the EM solver at various frequencies and angular resolutions demonstrate good efficiency and accuracy of the proposed method.
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NOVO, MARCELA SILVA. "ARBITRARY CROSS SECTION WAVEGUIDES: ANALYSIS OF MODAL FIELDS AND OF DISCONTINUITIES BETWEEN ARBITRARY CROSS SECTION WAVEGUIDES." PONTIFÍCIA UNIVERSIDADE CATÓLICA DO RIO DE JANEIRO, 2003. http://www.maxwell.vrac.puc-rio.br/Busca_etds.php?strSecao=resultado&nrSeq=3781@1.

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COORDENAÇÃO DE APERFEIÇOAMENTO DO PESSOAL DE ENSINO SUPERIOR
No presente trabalho o método de Rayleigh-Ritz é utilizado na determinação dos campos modais e dos números de onda de corte em guias de onda de seção arbitrária. Inicialmente, o método é aplicado com funções de base polinomiais, sendo a seção transversal do guia aproximada por um polígono convexo. Este tipo de função limitou o número de modos que podem ser calculados, uma vez que polinômios de grau alto geram instabilidades computacionais e overflow. Utilizando a mesma metodologia, os campos modais em guias de onda superquadráticos são analisados. Entretanto, as funções de base polinomiais são substituídas por funções trigonométricas, produzindo um modelo numérico capaz de computar um grande número de modos em um tempo de execução razoável. Os guias superquadráticos constituem uma classe de guias uniformes, incluindo guias circulares, elípticos, quase retangulares e outros de seções intermediárias. Conseqüentemente, eles são úteis na construção de diversos dispositivos em guias de onda, incluindo transições de diferentes seções, tais como circular para elíptica e circular para retangular. O método do casamento de modos é aplicado na determinação da matriz de espalhamento de descontinuidades entre guias superquadráticos. Diversas aplicações numéricas são apresentadas e comparadas com resultados obtidos através de outras técnicas.
In the present work, the modal fields and cutoff wavenumbers of arbitrary cross section waveguides are determined using the Rayleigh-Ritz method. Initially, the method is applied to waveguides with cross section approximated by a convex polygon. Polynomial basis functions are used. Such basis functions limit the number of modes that can be computed, since polynomials of high degree generate computer instabilities and overflow. Using the same methodology, the modal fields of superquadric waveguides are analyzed. Polynomial basis functions are replaced by trigonometric functions, however, producing an efficient numerical model capable of computing a large number of modes with a reasonable computer time. Superquadric waveguides constitute a class of uniform waveguides that include circular, elliptical, almost rectangular waveguides and a series of intermediate cross section waveguides. As a consequence they are quite useful in the construction of several devices, including transitions between waveguides of different cross sections, such as circular to elliptical and circular to rectangular. The mode matching technique is applied to the determination of the scattering matrix of discontinuities between superquadric waveguides. Several numerical applications are presented and compared to results obtained from other techniques.
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Britton, Michael C. "Practical square cross-section helical antennas." Thesis, National Library of Canada = Bibliothèque nationale du Canada, 1999. http://www.collectionscanada.ca/obj/s4/f2/dsk1/tape8/PQDD_0001/MQ43337.pdf.

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Abhakorn, Pongrapeeporn. "The cross-section of stock returns." Thesis, University of York, 2006. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.428059.

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Britton, Michael C. (Michael Charles) Carleton University Dissertation Engineering Electronics. "Practical square cross-section helical antennas." Ottawa, 1999.

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Salvador, Castiñeira Paula. "Neutron-induced fission cross section of 240,242Pu." Doctoral thesis, Universitat Politècnica de Catalunya, 2014. http://hdl.handle.net/10803/284746.

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A recent sensitivity analysis done for the new generation of fast reactors [1] has shown the importance of improved cross section data for several actinides. Among them, the neutron-induced fission cross section of 240,242Pu requires a level of accuracy of 1-3% and 3-5%, respectively, from the current status of 6% and 20%. Moreover, nearly all the measurements in the literature have been done relative to 235U(n,f). Therefore, using other references samples such as 237Np or 238U will provide the scientific community with more valuable data. The work was carried out at the Institute for Reference Materials and Measurements (JRC-IRMM). The Van de Graaff accelerator was used for producing a quasi-monoenergetic neutron flux in the energy range of 0.3MeV to 3MeV. Protons were accelerated thanks to a potential difference. A neutron producing target was placed at the end of the beam line: 7Li(p,n)7Be or T(p,n)3He. Then, a twin Frisch-grid ionization chamber (TFGIC) was used as detector. The setup of the detector consists in a common cathode, two anodes and two grids. In the cathode the sample under study and the reference sample are placed in a back-to-back configuration. Each electrode is connected to a preamplifier, and then to a 100MHz 12 bit waveform digitizer. All raw signals are stored for an offline analysis using C++ under the ROOT framework. All the samples used were produced by the target preparation group at JRC-IRMM. The enrichment of the plutonium samples was of 99.89% for 240Pu and of 99.97% for 242Pu. The plutonium masses were chosen to minimize their alpha activity (0.8MBq for 240Pu and 0.1MBq for 242Pu). Three different reference fission cross sections were employed: 235U(n,f), 238U(n,f) and 237Np(n,f). The mass of all the reference samples used was remeasured by means of low geometry alpha counting or/and by a single grid ionization chamber. The mass uncertainty of each sample was lower than 2%. Results were obtained not only for the neutron-induced fission cross section of 240,242Pu in the region from 0.3 MeV up to 3 MeV, but for the 238U(n,f) cross section and the 237Np(n,f) cross section. The neutron flux from the Van de Graaff was characterized by means of MCNP simulations. A clear influence of the different structures between the neutron producing targets and the deposits was found, specially when the ratios measured involved a fissile sample and a threshold sample. The spontaneous fission of 240,242Pu is, as well, an important correction. Thus, this property was measured independently in this work, reaching an uncertainty lower than 1.3% for both isotopes. More corrections were due to the high electronic threshold needed to not trigger on alpha particles, the fission fragment loss due to the sample thickness, neutron emission anisotropy, etc. On average the results of the 240,242Pu(n,f) cross section are in agreement with previous experimental data, even though the trend is slightly lower than present evaluations. In the case of 242Pu(n,f) cross section the resonance-peak structure at 1.1 MeV could not be reproduced in any case. The results of the 237Np(n,f) cross section show an increase at the plateau region with respect to the ENDF/B-VII.1 evaluation in the same way as the data from Paradela (2010) [2]. The results for the 238U(n,f) cross section show a higher cross section than the ENDF evaluation but in agreement with the present JEFF 3.2 evaluation. [1] Uncertainty and target accuracy assessment for innovative systems using recent covariance data evaluations, Volume 26, 2008, OECD-NEA [2] Paradela, C. et al., Neutron-induced fission cross section of U-234 and Np-237 measured at the CERN Neutron Time-of-Flight (n_TOF) facility.,Physical Review C. 82, 3, 034601 (2010)
Un anàlisi de sensitivitat [1] recent per la nova generació de reactors ràpids va mostrar la importància de millorar les seccions eficaç de varis actínids. Entre ells, la secció eficaç de fissió per neutró induït del 240,242Pu requereix una millora en la seva precisió des d'un 6% a un 1-3% pel 240Pu i des d'un 20% a un 3-5% pel 242Pu. A més, quasi bé totes les dades experimentals disponibles a la literatura han estat determinades relatives a la secció eficaç del 235U(n,f). Per tant, la utilització d'altres isòtops com a referències, tal com el 237Np(n,f) o el 238U(n,f), proveirà a la comunitat científica amb dades valuoses. Aquest treball ha estat realitzat a l'Institute for Reference Materials and Measurements (JRC-IRMM). L'accelerador Van de Graaff disponible al JRC-IRMM s'ha emprat per produir un flux de neutrons quasi mono-energètics en el rang de 0.3 MeV a 3 MeV. Els protons van ser accelerats de fer-los impactar amb una mostra de producció de neutrons: 7Li(p,n)7Be o T(p,n)3He. A continuació, una doble cambra d'ionització amb grid (TFGIC) es va emplaçar com a detector consistent en un càtode, dos ànodes i dos grids. En el càtode es situen la mostra a estudiar i la mostra de referència. Cada un dels elèctrodes és connectat a un preamplificador i, a continuació, a un digitilitzador amb una freqüència de 100 MHz i 12 bit. Les senyals originals són emmagatzemades sense cap tractament previ per a un posterior anàlisi. El tractament de dades es va realitzar mitjançant el codi de programació C++ sota el marc de ROOT. Totes les mostres emprades en aquest experiment s'han produït al grup de preparació de mostres del JRC-IRMM. L'enriquiment de les mostres de plutoni era de 99.89% pel 240Pu (0.8MBq) i del 99.97% pel 242Pu (0.1MBq). La massa de les tres mostres de referència (235U(n,f), 238U(n,f) i 237Np(n,f)) també va ser mesurada. La incertesa de cada massa és inferior al 2%. La principal correcció aplicaca als resultats obtinguts ha estat per la caracterització del flux de neutrons mitjançant el codi de simulació Monte Carlo MCNP. Els resultats de les simulacions han mostrat una clara influència de les diferents estructures emplaçades entre la mostra de producció de neutrons i les mostres de fissió. Altres correccions s¿han realitzat per la fissió espontània del 240,242Pu (mesurada independentment en aquest treball amb una incertesa inferior al 1,3%), la deficiència d'esdeveniments a causa del llindar de detecció, l'eficiència del detector, l'anisotropia en l'emissió dels neutrons, etc. Tot i que el principal objectiu va ser l'obtenció de la secció eficaç de fissió per neutró induït del 240,242Pu en la regió de 0.3 MeV a 3 MeV, resultats addicionals han estat obtinguts per la secció eficaç del 238U(n,f) i el 237Np(n,f). Els resultats obtinguts mostren un acord significatiu entre la secció eficaç del 240,242Pu(n,f) i resultats experimentals anteriors, tot i que la tendència és lleugerament inferior a les avaluacions (ENDF/B-VII.1, JEFF 3.1 i JENDL 4.0) disponibles. En el cas de la secció eficaç del 242Pu(n,f), a més, el pic de ressonància al voltant de 1.1 MeV predit per quasi totes les dades experimentals anteriors i les avaluacions actuals no s'ha reproduït en aquest experiment. Els resultats de la secció eficaç del 237Np(n,f) presenten un increment en la regió plana després del llindar de fissió d'un 5-7% respecte l'avaluació ENDF/B-VII.1, i en concordança amb els resultats obtinguts per Paradela (2010) [2]. Finalment, els resultats de la secció eficaç del 238U(n,f) mostren un increment al voltant d'un 7-9% a la zona plana després del llindar de fissió, aquesta predicció concorda amb l'avaluació JEFF 3.2. [1] Uncertainty and target accuracy assessment for innovative systems using recent covariance data evaluations, Volume 26, 2008, OECD-NEA [2] Paradela, C. et al., Neutron-induced fission cross section of U-234 and Np-237 measured at the CERN Neutron Time-of-Flight (n_TOF) facility.,Physical Review C. 82, 3, 034601 (2010)
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Tesinsky, Milan. "MCNPX Simulations for Neutron Cross Section Measurements." Licentiate thesis, KTH, Reactor Physics, 2010. http://urn.kb.se/resolve?urn=urn:nbn:se:kth:diva-12929.

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This thesis presents MCNPX simulations of the SCANDAL set-up used at the Theodor Svedberg Laboratory for neutron scattering cross-section measurements. The thesis describes processes and data important for the upcoming off-line data analysis. In the experiment, neutrons scattered off the target are converted to protons which are stopped in scintillator crystals. The results of presented simulations include a description of the proton spectra in dependence of the neutron-to-proton conversion angle, calculation of the hit position gates and a study of the converter describing the role of its chemical composition and also the role of other plastic scintillator on the proton spectra.


QC 20100520
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Grijpink, Sjors Johannes Louis Assuerus. "Charged current cross section measurement at HERA." [S.l. : Amsterdam : s.n.] ; Universiteit van Amsterdam [Host], 2004. http://dare.uva.nl/document/72835.

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Books on the topic "Cross section"

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F, Shaeffer John, and Tuley Michael T, eds. Radar cross section. 2nd ed. Boston: Artech House, 1993.

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Knott, Eugene F. Radar Cross Section Measurements. Boston, MA: Springer US, 1993. http://dx.doi.org/10.1007/978-1-4684-9904-9.

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Knott, Eugene F. Radar cross section measurements. New York: Van Nostrand Reinhold, 1993.

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McLane, Victoria. Neutron cross section curves. 4th ed. Boston: Academic Press, 1988.

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1940-, Dunford Charles L., Rose Philip F. 1928-, and Mughabghab S. F. 1934-, eds. Neutron cross section curves. 4th ed. Boston: Academic Press, 1988.

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Casele, Francesco, and Monica Roos. Robert Huff: Cross section. Miami, FL: Letter 16 Press, Inc., 2018.

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Biesty, Stephen. The incredible cross-section book. New York: Knopf, 1992.

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Biesty, Stephen. Egypt in spectacular cross-section. New York: Scholastic Nonfiction, 2005.

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Biesty, Stephen. Egypt in spectacular cross-section. New York: Scholastic Nonfiction, 2005.

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Biesty, Stephen. Rome: In spectacular cross-section. Oxford, Eng: Scholastic Nonfiction, 2003.

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Book chapters on the topic "Cross section"

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Gooch, Jan W. "Cross Section." In Encyclopedic Dictionary of Polymers, 183. New York, NY: Springer New York, 2011. http://dx.doi.org/10.1007/978-1-4419-6247-8_3129.

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Basu, Chinmay. "Cross-Section." In An Introduction to Experimental Nuclear Reactions, 11–18. Boca Raton: CRC Press, 2021. http://dx.doi.org/10.1201/9781003083863-2.

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Paetz gen. Schieck, Hans. "Classical Cross Section." In Nuclear Reactions, 13–38. Berlin, Heidelberg: Springer Berlin Heidelberg, 2014. http://dx.doi.org/10.1007/978-3-642-53986-2_2.

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Mousseau, Joel Allen. "Cross Section Results." In First Search for the EMC Effect and Nuclear Shadowing in Neutrino Nuclear Deep Inelastic Scattering at MINERvA, 137–43. Cham: Springer International Publishing, 2016. http://dx.doi.org/10.1007/978-3-319-44841-1_13.

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Gooch, Jan W. "Crenular Cross Section." In Encyclopedic Dictionary of Polymers, 178. New York, NY: Springer New York, 2011. http://dx.doi.org/10.1007/978-1-4419-6247-8_3060.

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Vayas, Ioannis, John Ermopoulos, and George Ioannidis. "Cross-section design." In Design of Steel Structures to Eurocodes, 75–114. Cham: Springer International Publishing, 2018. http://dx.doi.org/10.1007/978-3-319-95474-5_3.

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Kaltenegger, Lisa. "Absorption Cross Section." In Encyclopedia of Astrobiology, 1. Berlin, Heidelberg: Springer Berlin Heidelberg, 2014. http://dx.doi.org/10.1007/978-3-642-27833-4_8-5.

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Gooch, Jan W. "Triskelion Cross Section." In Encyclopedic Dictionary of Polymers, 770. New York, NY: Springer New York, 2011. http://dx.doi.org/10.1007/978-1-4419-6247-8_12159.

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Kaltenegger, Lisa. "Absorption Cross Section." In Encyclopedia of Astrobiology, 29. Berlin, Heidelberg: Springer Berlin Heidelberg, 2015. http://dx.doi.org/10.1007/978-3-662-44185-5_8.

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Kaltenegger, Lisa. "Absorption Cross Section." In Encyclopedia of Astrobiology, 3–4. Berlin, Heidelberg: Springer Berlin Heidelberg, 2011. http://dx.doi.org/10.1007/978-3-642-11274-4_8.

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Conference papers on the topic "Cross section"

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Condon, Timothy, Bruce Walter, Kavita Bala, and Donald Greenberg. "Prefiltered Cross-Section Occluders." In 2010 18th Pacific Conference on Computer Graphics and Applications (PG). IEEE, 2010. http://dx.doi.org/10.1109/pacificgraphics.2010.23.

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Brown, David A. "Actinide Cross-Section Evaluations." In INTERNATIONAL CONFERENCE ON NUCLEAR DATA FOR SCIENCE AND TECHNOLOGY. AIP, 2005. http://dx.doi.org/10.1063/1.1945040.

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GARRETSON III, HENRY. "RADAR CROSS SECTION TESTING." In 3rd Flight Testing Conference and Technical Display. Reston, Virigina: American Institute of Aeronautics and Astronautics, 1986. http://dx.doi.org/10.2514/6.1986-828.

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GARRETSON, III, H. "Radar cross section testing." In 3rd Flight Testing Conference and Technical Display. Reston, Virigina: American Institute of Aeronautics and Astronautics, 1986. http://dx.doi.org/10.2514/6.1986-9828.

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Berger, M. S. "Threshold cross section measurements." In Physics potential and development of μ. AIP, 1998. http://dx.doi.org/10.1063/1.56395.

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REISERT, Burkard. "Cross-section measurements at Belle." In European Physical Society Europhysics Conference on High Energy Physics. Trieste, Italy: Sissa Medialab, 2010. http://dx.doi.org/10.22323/1.084.0055.

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Del Tutto, Marco. "Cross Section Prospects for MicroBooNE." In The 19th International Workshop on Neutrinos from Accelerators NUFACT2017. Trieste, Italy: Sissa Medialab, 2018. http://dx.doi.org/10.22323/1.295.0068.

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Felcan, Miroslav. "Historical Cross-Section of Arson." In Safe and Secure Society. The College of European and Regional Studies, 2020. http://dx.doi.org/10.36682/ssc_2020/1.

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This work was supported by the Agency for Research and Development under the contract no. APVV-17-0217.Every year fires cause big damage to society, property, environment, buildings and infrastructure and pose a threat to life and health of persons in endangered areas. In most cases arson serves as insurance fraud or cover up any crime (e.g. robbery, embezzlement). However, there may be other reasons, e.g. in the case of the Commission of the European Union, the use of the product in envy, hatred, threats, blackmail, competitive struggle. Or social, political, or ethnic differences. In several cases, arson was used as a so-called 'arson attack'. The false flag, that is, the arsonist used the fire to accuse his enemy and took advantage of the wave of recourse that subsequently was raised against him. The circumstances of the cause and the fire are under investigation. After extinguishing a fire, it is standard procedure to seek and then either confirm, refute or further examine the possibility of intentional formation. In most countries of the world, arson is treated as a crime and seen as harming a stranger or a threat to life.
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Lemoine, F., D. F. Grevey, and A. B. Vannes. "Cross-section modelling laser cladding." In ICALEO® ‘93: Proceedings of the Laser Materials Processing Conference. Laser Institute of America, 1993. http://dx.doi.org/10.2351/1.5058574.

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Shang, Yuping, and Zhongxiang Shen. "Radar cross-section enhancement techniques." In 2017 IEEE International Conference on Computational Electromagnetics (ICCEM). IEEE, 2017. http://dx.doi.org/10.1109/compem.2017.7912846.

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Reports on the topic "Cross section"

1

Kozak, Serhiy, Stefan Nagel, and Shrihari Santosh. Shrinking the Cross Section. Cambridge, MA: National Bureau of Economic Research, November 2017. http://dx.doi.org/10.3386/w24070.

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Kawano, Toshihiko. New Arsenic Cross Section Calculations. Office of Scientific and Technical Information (OSTI), March 2015. http://dx.doi.org/10.2172/1172207.

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Knoll, G. F. [Fast neutron cross section measurements]. Office of Scientific and Technical Information (OSTI), October 1992. http://dx.doi.org/10.2172/6645620.

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Shelley, John, and Philip Bailey. The Cross Section Viewer : a tool for automating geomorphic analysis using cross section data. Coastal and Hydraulics Laboratory (U.S.), January 2018. http://dx.doi.org/10.21079/11681/26284.

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Mattoon, C. M., and P. Oblozinsky. ISSUES IN NEUTRON CROSS SECTION COVARIANCES. Office of Scientific and Technical Information (OSTI), April 2010. http://dx.doi.org/10.2172/1013490.

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Egan, Mark, Stefan Lewellen, and Adi Sunderam. The Cross Section of Bank Value. Cambridge, MA: National Bureau of Economic Research, March 2017. http://dx.doi.org/10.3386/w23291.

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Younes, W., H. C. Britt, and J. B. Wilhelmy. The 237U(n,f) Cross Section. Office of Scientific and Technical Information (OSTI), March 2003. http://dx.doi.org/10.2172/15003856.

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Pruet, J., D. McNabb, and W. Ormand. Cross Section Evaluations for Arsenic Isotopes. Office of Scientific and Technical Information (OSTI), March 2005. http://dx.doi.org/10.2172/15015183.

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Pronskikh, V. S., and N. V. Mokhov. DPA Cross Section Library FermiDPA 1.0. Office of Scientific and Technical Information (OSTI), June 2013. http://dx.doi.org/10.2172/1339146.

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Huang, Burn, and Kingyuen B. Ng. Proton-Helium Elastic Electromagnetic Cross-Section. Office of Scientific and Technical Information (OSTI), November 2015. http://dx.doi.org/10.2172/1352007.

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