Bibliographies thématiques / Synchrotron Radiatio

Littérature scientifique sur le sujet « Synchrotron Radiatio »

Auteur : Grafiati
Publié le 1 avril 2023

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Articles de revues sur le sujet "Synchrotron Radiatio"

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Henderson, Richard, et Mejd Alsari. « Radiation Sources in Structural Biology ». Scientific Video Protocols 1, no 1 (6 juin 2020) : 1–3. http://dx.doi.org/10.32386/scivpro.000023.

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What is radiation damage? Are electrons more suitable than X-rays in structural biology? Richard Henderson talks about synchrotron radiation and how cryo-EM laboratories are being established at synchrotrons as national research facilities.
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Peter, William, et Anthony L. Peratt. « Thermalization of synchrotron radiation from field-aligned currents ». Laser and Particle Beams 6, no 3 (août 1988) : 493–501. http://dx.doi.org/10.1017/s0263034600005413.

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Three-dimensional plasma simulations of interacting galactic-dimensioned current filaments show bursts of synchroton radiation of energy density 1·2 ×10−13 erg/cm3 which can be compared with the measured cosmic microwave background energy density of 1·5 × 10−13 erg/cm3. However, the synchrotron emission observed in the simulations is not blackbody. In this paper, we analyze the absorption of the synchrotron emission by the current filaments themselves (i.e., self-absorption) in order to investigate the thermalization of the emitted radiation. It is found that a large number of current filaments (>1031) are needed to make the radiation spectrum blackbody up to the observed measured frequency of 100 GHz. The radiation spectrum and the required number of current filaments is a strong function of the axial magnetic field in the filaments.
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Fernandez-Palomo, Cristian, Zacharenia Nikitaki, Valentin Djonov, Alexandros G. Georgakilas et Olga A. Martin. « Non-Targeted Effects of Synchrotron Radiation : Lessons from Experiments at the Australian and European Synchrotrons ». Applied Sciences 12, no 4 (17 février 2022) : 2079. http://dx.doi.org/10.3390/app12042079.

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Studies have been conducted at synchrotron facilities in Europe and Australia to explore a variety of applications of synchrotron X-rays in medicine and biology. We discuss the major technical aspects of the synchrotron irradiation setups, paying specific attention to the Australian Synchrotron (AS) and the European Synchrotron Radiation Facility (ESRF) as those best configured for a wide range of biomedical research involving animals and future cancer patients. Due to ultra-high dose rates, treatment doses can be delivered within milliseconds, abiding by FLASH radiotherapy principles. In addition, a homogeneous radiation field can be spatially fractionated into a geometric pattern called microbeam radiotherapy (MRT); a coplanar array of thin beams of microscopic dimensions. Both are clinically promising radiotherapy modalities because they trigger a cascade of biological effects that improve tumor control, while increasing normal tissue tolerance compared to conventional radiation. Synchrotrons can deliver high doses to a very small volume with low beam divergence, thus facilitating the study of non-targeted effects of these novel radiation modalities in both in-vitro and in-vivo models. Non-targeted radiation effects studied at the AS and ESRF include monitoring cell–cell communication after partial irradiation of a cell population (radiation-induced bystander effect, RIBE), the response of tissues outside the irradiated field (radiation-induced abscopal effect, RIAE), and the influence of irradiated animals on non-irradiated ones in close proximity (inter-animal RIBE). Here we provide a summary of these experiments and perspectives on their implications for non-targeted effects in biomedical fields.
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Pérez, Serge, et Daniele de Sanctis. « Glycoscience@Synchrotron : Synchrotron radiation applied to structural glycoscience ». Beilstein Journal of Organic Chemistry 13 (14 juin 2017) : 1145–67. http://dx.doi.org/10.3762/bjoc.13.114.

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Synchrotron radiation is the most versatile way to explore biological materials in different states: monocrystalline, polycrystalline, solution, colloids and multiscale architectures. Steady improvements in instrumentation have made synchrotrons the most flexible intense X-ray source. The wide range of applications of synchrotron radiation is commensurate with the structural diversity and complexity of the molecules and macromolecules that form the collection of substrates investigated by glycoscience. The present review illustrates how synchrotron-based experiments have contributed to our understanding in the field of structural glycobiology. Structural characterization of protein–carbohydrate interactions of the families of most glycan-interacting proteins (including glycosyl transferases and hydrolases, lectins, antibodies and GAG-binding proteins) are presented. Examples concerned with glycolipids and colloids are also covered as well as some dealing with the structures and multiscale architectures of polysaccharides. Insights into the kinetics of catalytic events observed in the crystalline state are also presented as well as some aspects of structure determination of protein in solution.
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Martin-Garcia, Jose M., Lan Zhu, Derek Mendez, Ming-Yue Lee, Eugene Chun, Chufeng Li, Hao Hu et al. « High-viscosity injector-based pink-beam serial crystallography of microcrystals at a synchrotron radiation source ». IUCrJ 6, no 3 (5 avril 2019) : 412–25. http://dx.doi.org/10.1107/s205225251900263x.

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Since the first successful serial crystallography (SX) experiment at a synchrotron radiation source, the popularity of this approach has continued to grow showing that third-generation synchrotrons can be viable alternatives to scarce X-ray free-electron laser sources. Synchrotron radiation flux may be increased ∼100 times by a moderate increase in the bandwidth (`pink beam' conditions) at some cost to data analysis complexity. Here, we report the first high-viscosity injector-based pink-beam SX experiments. The structures of proteinase K (PK) and A2A adenosine receptor (A2AAR) were determined to resolutions of 1.8 and 4.2 Å using 4 and 24 consecutive 100 ps X-ray pulse exposures, respectively. Strong PK data were processed using existing Laue approaches, while weaker A2AAR data required an alternative data-processing strategy. This demonstration of the feasibility presents new opportunities for time-resolved experiments with microcrystals to study structural changes in real time at pink-beam synchrotron beamlines worldwide.
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Eichhorn, Klaus D. « Single-crystal X-ray diffractometry using synchrotron radiation ». European Journal of Mineralogy 9, no 4 (23 juillet 1997) : 673–92. http://dx.doi.org/10.1127/ejm/9/4/0673.

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Ebrahim, Ali, Tadeo Moreno-Chicano, Martin V. Appleby, Amanda K. Chaplin, John H. Beale, Darren A. Sherrell, Helen M. E. Duyvesteyn et al. « Dose-resolved serial synchrotron and XFEL structures of radiation-sensitive metalloproteins ». IUCrJ 6, no 4 (3 mai 2019) : 543–51. http://dx.doi.org/10.1107/s2052252519003956.

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An approach is demonstrated to obtain, in a sample- and time-efficient manner, multiple dose-resolved crystal structures from room-temperature protein microcrystals using identical fixed-target supports at both synchrotrons and X-ray free-electron lasers (XFELs). This approach allows direct comparison of dose-resolved serial synchrotron and damage-free XFEL serial femtosecond crystallography structures of radiation-sensitive proteins. Specifically, serial synchrotron structures of a heme peroxidase enzyme reveal that X-ray induced changes occur at far lower doses than those at which diffraction quality is compromised (the Garman limit), consistent with previous studies on the reduction of heme proteins by low X-ray doses. In these structures, a functionally relevant bond length is shown to vary rapidly as a function of absorbed dose, with all room-temperature synchrotron structures exhibiting linear deformation of the active site compared with the XFEL structure. It is demonstrated that extrapolation of dose-dependent synchrotron structures to zero dose can closely approximate the damage-free XFEL structure. This approach is widely applicable to any protein where the crystal structure is altered by the synchrotron X-ray beam and provides a solution to the urgent requirement to determine intact structures of such proteins in a high-throughput and accessible manner.
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Bagrov, Vladislav, Anna Kasatkina et Alexey Pecheritsyn. « Effective Angle of Synchrotron Radiation ». Symmetry 12, no 7 (2 juillet 2020) : 1095. http://dx.doi.org/10.3390/sym12071095.

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An exact analytical expression for the effective angle is determined for an arbitrary energy value of a radiating particle. An effective angle of instantaneous power is defined for synchrotron radiation in the framework of classical electrodynamics. This definition explicitly contains the most symmetric distribution of half the total of the instantaneous power of synchrotron radiation. Two exact analytical expressions for the effective angle are considered for the arbitrary energy values of a radiating particle, and the second expression brings to light the exact asymptotics of the effective angle in the ultrarelativistic limit.
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Morgan, Kaye Susannah, David Parsons, Patricia Cmielewski, Alexandra McCarron, Regine Gradl, Nigel Farrow, Karen Siu et al. « Methods for dynamic synchrotron X-ray respiratory imaging in live animals ». Journal of Synchrotron Radiation 27, no 1 (1 janvier 2020) : 164–75. http://dx.doi.org/10.1107/s1600577519014863.

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Small-animal physiology studies are typically complicated, but the level of complexity is greatly increased when performing live-animal X-ray imaging studies at synchrotron and compact light sources. This group has extensive experience in these types of studies at the SPring-8 and Australian synchrotrons, as well as the Munich Compact Light Source. These experimental settings produce unique challenges. Experiments are always performed in an isolated radiation enclosure not specifically designed for live-animal imaging. This requires equipment adapted to physiological monitoring and test-substance delivery, as well as shuttering to reduce the radiation dose. Experiment designs must also take into account the fixed location, size and orientation of the X-ray beam. This article describes the techniques developed to overcome the challenges involved in respiratory X-ray imaging of live animals at synchrotrons, now enabling increasingly sophisticated imaging protocols.
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MIYAHARA, Tsuneaki. « Synchrotron Radiation. II. Synchrotron Radiation. 2. Optics for Synchrotron Radiation. » RADIOISOTOPES 47, no 1 (1998) : 79–84. http://dx.doi.org/10.3769/radioisotopes.47.79.

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Thèses sur le sujet "Synchrotron Radiatio"

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Botez, Cristian E. « Synchrotron x-ray scattering studies of metallic surfaces / ». free to MU campus, to others for purchase, 2002. http://wwwlib.umi.com/cr/mo/fullcit?p3052151.

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Crosbie, Jeffrey. « Synchrotron microbeam radiation therapy ». Monash University. Faculty of Science. School of Physics, 2008. http://arrow.monash.edu.au/hdl/1959.1/64948.

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This thesis presents interdisciplinary, collaborative research in the field of synchrotron microbeam radiation therapy (MRT). Synchrotron MRT is an experimental radiotherapy technique under consideration for clinical use, following demonstration of efficacy in tumour-bearing rodent models with remarkable sparing of normal tissue. A high flux, X-ray beam from a synchrotron is segmented into micro-planar arrays of narrow beams, typically 25 μm wide and with peak-to-peak separations of 200 μm. The radiobiological effect of MRT and the underlying cellular mechanisms are poorly understood. The ratio between dose in the ‘peaks’of the microbeams to the dose in the ‘valleys’, between the microbeams, has strong biological significance. However, there are difficulties in accurately measuring the dose distribution for MRT. The aim of this thesis is to address elements of both the dosimetric and radiobiological gaps that exist in the field of synchrotron MRT. A method of film dosimetry and microdensitometry was adapted in order to measure the peak-to-valley dose ratios for synchrotron MRT. Two types of radiochromic film were irradiated in a phantom and also flush against a microbeam collimator on beamline BL28B2 at the SPring-8 synchrotron. The HD-810 and EBT varieties of radiochromic film were used to record peak dose and valley dose respectively. In other experiments, a dose build-up effect was investigated and the half value layer of the beam with and without the microbeam collimator was measured to investigate the effect of the collimator on the beam quality. The valley dose obtained for films placed flush against the collimator was approximately 0.25% of the peak dose. Within the water phantom, the valley dose had increased to between 0.7–1.8% of the peak dose, depending on the depth in the phantom. We also demonstrated, experimentally and by Monte Carlo simulation, that the dose is not maximal on the surface and that there is a dose build-up effect. The microbeam collimator did not make an appreciable difference to the beam quality. The measured values of peak-to-valley dose ratio were higher than those predicted by previously published Monte Carlo simulation papers. For the radiobiological studies, planar (560 Gy) or cross-planar (2 x 280 Gy or 2 x 560 Gy) irradiations were delivered to mice inoculated with mammary tumours in their leg, on beamline BL28B2 at the SPring-8 synchrotron. Immunohistochemical staining for DNA double strand breaks, proliferation and apoptosis was performed on irradiated tissue sections. The MRT response was compared to conventional radiotherapy at 11, 22 or 44 Gy. The results of the study provides the first evidence for a differential tissue response at a cellular level between normal and tumour tissues following synchrotron MRT. Within 24 hours of MRT to tumour, obvious cell migration had occurred into and out of irradiated zones. MRT-irradiated tumours showed significantly less proliferative capacity by 24 hours post-irradiation (P = 0.002). Median survival times for EMT-6.5 and 67NR tumour-bearing mice following MRT (2 x 560 Gy) and conventional radiotherapy (22 Gy) increased significantly compared to unirradiated controls (P < 0.0005). However, there was markedly less normal tissue damage from MRT than from conventional radiotherapy. MRT-treated normal skin mounts a more coordinated repair response than tumours. Cell-cell communication of death signals from directly irradiated, migrating cells, may explain why tumours are less resistant to high dose MRT than normal tissue.
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Baine, Michael. « Laser undulated synchrotron radiation sources / ». Diss., Connect to a 24 p. preview or request complete full text in PDF format. Access restricted to UC IP addresses, 2000. http://wwwlib.umi.com/cr/ucsd/fullcit?p9956463.

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Krishnamurthy, Satheesh. « Synchrotron radiation studies of nanostructured materials ». Thesis, University of Newcastle Upon Tyne, 2006. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.430334.

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Margaritondo, Giorgio, et Johann Rafelski. « The relativistic foundations of synchrotron radiation ». INT UNION CRYSTALLOGRAPHY, 2017. http://hdl.handle.net/10150/625068.

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Special relativity (SR) determines the properties of synchrotron radiation, but the corresponding mechanisms are frequently misunderstood. Time dilation is often invoked among the causes, whereas its role would violate the principles of SR. Here it is shown that the correct explanation of the synchrotron radiation properties is provided by a combination of the Doppler shift, not dependent on time dilation effects, contrary to a common belief, and of the Lorentz transformation into the particle reference frame of the electromagnetic field of the emission-inducing device, also with no contribution from time dilation. Concluding, the reader is reminded that much, if not all, of our argument has been available since the inception of SR, a research discipline of its own standing.
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Salomon, Felix. « Refraction index modification by synchrotron radiation ». [S.l. : s.n.], 2007. http://nbn-resolving.de/urn:nbn:de:bsz:352-opus-44255.

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Ludwig, Wolfgang. « Development and Applications of Synchrotron Radiation Microtomography ». Diss., lmu, 2001. http://nbn-resolving.de/urn:nbn:de:bvb:19-3447.

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Weaver, Jill Suzanne. « Synchrotron Radiation Studies of Magnetic Thin Films ». Thesis, University of York, 2007. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.485147.

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The purpose of these studies has been to gain a better understanding of the relationships that govern the interfaces of ferromagnetic / ill-V semiconductor heterostructures and other materials. The results here in are expected to promote the development of next generation spin electronic devices which may open the way toward incorporating data processing and storage in a single device through the utilisation of both electron charge and spin. Development ofsuch devices relies a great deal on the quality ofinterface which can be set up between the semiconductor and ferromagnetic structures, as a poor interface leads to difficulty in carrier transport between the materials. Studies into interface magnetism, which can most effectively be carried out using the synchrotron technique of x-ray magnetic circular dichroism (XMCD), have been used to make substantial strides forward in the understanding of the importance of interface quality. It is hoped that these shidies involving synchrotron radiation, predominantly in the area of XMCD, wiJI help the further development ofnew spintronic technologies.
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Thompson, Stephen P. « Studies of cosmic dusts using synchrotron radiation ». Thesis, Keele University, 1991. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.303876.

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Wright, Andrew Edward. « Studies of reactive intermediates with synchrotron radiation ». Thesis, University of Southampton, 1997. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.242644.

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Livres sur le sujet "Synchrotron Radiatio"

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R, Gonzalez-Elipe A., et Muñoz Páez A, dir. Necesidades y perspectivas de uso de la radiación sincrotrón en España. Sevilla : Universidad de Sevilla, 1993.

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Ernest, Fontes, et National Conference on Synchrotron Radiation Instrumentation (10th : 1997 : Cornell University), dir. Synchrotron radiation instrumentation : Tenth US national conference, Ithaca, New York, June 1997. Woodbury, N.Y : American Institute of Physics, 1997.

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Facility, European Synchrotron Radiation. Highlights 2001. Grenoble : ESRF, 2002.

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Facility, European Synchrotron Radiation. Highlights 2001. Grenoble : ESRF, 2002.

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Mobilio, Settimio, Federico Boscherini et Carlo Meneghini, dir. Synchrotron Radiation. Berlin, Heidelberg : Springer Berlin Heidelberg, 2015. http://dx.doi.org/10.1007/978-3-642-55315-8.

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Wiedemann, Helmut. Synchrotron Radiation. Berlin, Heidelberg : Springer Berlin Heidelberg, 2003. http://dx.doi.org/10.1007/978-3-662-05312-6.

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Wiedemann, Helmut. Synchrotron Radiation. Berlin, Heidelberg : Springer Berlin Heidelberg, 2003.

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Bachrach, Robert Z., dir. Synchrotron Radiation Research. Boston, MA : Springer US, 1992. http://dx.doi.org/10.1007/978-1-4615-3280-4.

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1934-, Cox David, Vlieg Elias et Robinson I. K. 1955-, dir. Synchrotron radiation crystallography. London : Academic Press, 1992.

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Gacoin, Marie-Pauline. Les orfèvres de la lumière : Une visite au synchrotron SOLEIL. Paris : Le Pommier, 2010.

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Chapitres de livres sur le sujet "Synchrotron Radiatio"

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Lin, Fanglei. « Electron Polarization ». Dans Polarized Beam Dynamics and Instrumentation in Particle Accelerators, 155–81. Cham : Springer International Publishing, 2022. http://dx.doi.org/10.1007/978-3-031-16715-7_6.

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AbstractThis chapter focuses on the introduction and discussion of electron polarization. In addition to the gyromagnetic ratio, the most different character of electrons compared to protons is that electrons radiate electromagnetic energy in a circular accelerator. A very small correction has to be applied to the electron spin flip to account for the synchrotron radiation. The different instantaneous spin flip probabilities, up to down and down to up, can build up the electron beam polarization state. However, mostly synchrotron radiation tends to disturb the electron orbital motion that is eventually balanced by the radiation damping along an equilibrium orbit. The electron spin motion is described by the modified Thomas-BMT equation with the radiative spin transition term included. Detail of the electron (de)polarization phenomena is described in this chapter. The lecture is extracted from various early theoretical papers, lectures, thesis and presentations (Lee, Accelerator Physics. World Scientific Publishing, 1999; Buon and Koutchouk, Polarization of Electron and Proton Beams. CERN-SL-94-80-AP, 1994; Montague, Phys. Rep. 113(1):1–96, 1984; Lee, Spin Dynamics and Snakes in Synchrotrons. World Scientific Publishing, 1997; Barber and Ripken, Handbook of Accelerator Physics and Engineering, 1st edn. World Scientific Publishing, 2006; Barber, An Introduction to Spin Polarisation in Accelerators and Storage Rings. Cockcroft Institute Academic Training Winter Term, 2014; Mane, Nucl. Instr. Methods Phys. Res. A 292:52–74, 1990; Berglund, Spin-Orbit Maps and Electron Spin Dynamics for the Luminosity Upgrade Project at HERA. DESY-THESIS-2001-044, 2001; Electron-Ion Collider Conceptual Design Report, 2020).
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Rouan, Daniel. « Synchrotron Radiation ». Dans Encyclopedia of Astrobiology, 1645. Berlin, Heidelberg : Springer Berlin Heidelberg, 2011. http://dx.doi.org/10.1007/978-3-642-11274-4_1557.

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Stupakov, Gennady, et Gregory Penn. « Synchrotron Radiation ». Dans Graduate Texts in Physics, 221–30. Cham : Springer International Publishing, 2018. http://dx.doi.org/10.1007/978-3-319-90188-6_18.

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Wiedemann, Helmut. « Synchrotron Radiation ». Dans Particle Accelerator Physics II, 229–68. Berlin, Heidelberg : Springer Berlin Heidelberg, 1999. http://dx.doi.org/10.1007/978-3-642-59908-8_7.

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Perelomov, Askold. « Synchrotron Radiation ». Dans Generalized Coherent States and Their Applications, 289–91. Berlin, Heidelberg : Springer Berlin Heidelberg, 1986. http://dx.doi.org/10.1007/978-3-642-61629-7_27.

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Peratt, Anthony L. « Synchrotron Radiation ». Dans Physics of the Plasma Universe, 205–57. New York, NY : Springer New York, 2014. http://dx.doi.org/10.1007/978-1-4614-7819-5_6.

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Rouan, Daniel. « Synchrotron Radiation ». Dans Encyclopedia of Astrobiology, 2447. Berlin, Heidelberg : Springer Berlin Heidelberg, 2015. http://dx.doi.org/10.1007/978-3-662-44185-5_1557.

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Wiedemann, Helmut. « Synchrotron Radiation ». Dans Particle Accelerator Physics II, 229–68. Berlin, Heidelberg : Springer Berlin Heidelberg, 1995. http://dx.doi.org/10.1007/978-3-642-97550-9_7.

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Peratt, Anthony L. « Synchrotron Radiation ». Dans Physics of the Plasma Universe, 197–252. New York, NY : Springer New York, 1992. http://dx.doi.org/10.1007/978-1-4612-2780-9_6.

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Wiedemann, Helmut. « Synchrotron Radiation ». Dans Particle Accelerator Physics I, 300–336. Berlin, Heidelberg : Springer Berlin Heidelberg, 1999. http://dx.doi.org/10.1007/978-3-662-03827-7_9.

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Actes de conférences sur le sujet "Synchrotron Radiatio"

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Zanini, F. « ARCHAEOLOGICAL APPLICATIONS OF SYNCHROTRON RADIATION AT ELETTRA ». Dans Знаки и образы в искусстве каменного века. Международная конференция. Тезисы докладов [Электронный ресурс]. Crossref, 2019. http://dx.doi.org/10.25681/iaras.2019.978-5-94375-308-4.33.

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The use of synchrotron radiation for the analysis of samples of historical and artistic importance (archaeology, palaeontology, conservation sciences, palaeo-environments) has been increasing over the past years, and experiments related to the study of our cultural heritage (CH) have been routinely performed at many beamlines of Elettra, the Italian synchrotron radiation facility. Fundamental parameters such as the high photon flux, the small source size and the low divergence typical of synchrotrons make it a very efficient source for a range of advanced spectroscopy and imaging techniques, adapted to the dishomogeneity and complexity of the materials under study. The continuous tunability of the source (from infrared to X-rays) is essential for techniques based on a fine tuning of the probing energy to reach high chemical sensitivity such as XANES, EXAFS, STXM, UV/VIS spectrometry. Moreover, the small source size attained in the vertical plane leads to spatial coherence of the photon source itself, giving rise to a series of imaging methods already crucial to the field. The increasing number of scientific publications shows that microfocused hard X-ray spectroscopy (absorption, fluorescence, diffraction), full-field X-ray tomography and infrared spectroscopy are the most popular synchrotron techniques in the field. The Elettra laboratory now offers a platform dedicated to CH researchers in order to support both the proposal application phase and the different steps of the experiment, from sample preparation to data analysis. We will present this activity and the main instrumental setups and experimental techniques in use at Elettra, and describe their impact for the science being applied to ancient materials using synchrotron rad
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Martin, Mike. « Coherent Synchrotron Radiation in Synchrotrons as a Broadband High Power Terahertz Source ». Dans Optical Terahertz Science and Technology. Washington, D.C. : OSA, 2007. http://dx.doi.org/10.1364/otst.2007.tud1.

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TENG, LEE C. « SYNCHROTRON RADIATION ». Dans Selected Lectures of OCPA International Accelerator School 2002. WORLD SCIENTIFIC, 2004. http://dx.doi.org/10.1142/9789812702807_0008.

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Sander, Robert K., et Joe J. Tiee. « Molecular Photoionization and Photofragmentation Studies Using VUV Radiation ». Dans Free-Electron Laser Applications in the Ultraviolet. Washington, D.C. : Optica Publishing Group, 1988. http://dx.doi.org/10.1364/fel.1988.sb4.

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It has long been recognized that studies of molecular processes such as photoionization and photofragmentation can provide valuable spectroscopic and chemical dynamics information that can lead to a detailed mechanistic understanding of the energetics, structure, and reactivity of molecular species. With the availability of high power and tunable lasers in the uv and visible region, substantial progress has been made in recent years in understanding molecular dynamics through photoionization and photofragmentation studies. These works, however, are limited to only a few selected molecules and in some cases involve multiple photon excitation. This is because most molecules undergo these molecular processes at excitation wavelengths shorter than 200 nm (i.e., in the VUV region) where few good laser sources are available. Synchrotron light sources have been applied to similar investigations in the VUV with limited success. The main difficulty appears to be the lack of spectral brightness of synchrotrons, particularly in state-specific photoexcitation studies where both high photon intensity and spectral resolution are essential.
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Tanida, Hajime. « XAFS and Protein Crystallography Beamline BL38B1 at SPring-8 ». Dans SYNCHROTRON RADIATION INSTRUMENTATION : Eighth International Conference on Synchrotron Radiation Instrumentation. AIP, 2004. http://dx.doi.org/10.1063/1.1757840.

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Wang, Q. P. « The Status of NSRL Beamline Construction ». Dans SYNCHROTRON RADIATION INSTRUMENTATION : Eighth International Conference on Synchrotron Radiation Instrumentation. AIP, 2004. http://dx.doi.org/10.1063/1.1757841.

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7

Aghasyan, M. « The First Group of CANDLE Beamlines ». Dans SYNCHROTRON RADIATION INSTRUMENTATION : Eighth International Conference on Synchrotron Radiation Instrumentation. AIP, 2004. http://dx.doi.org/10.1063/1.1757842.

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Ilavsky, Jan. « Versatile USAXS (Bonse-Hart) Facility for Advanced Materials Research ». Dans SYNCHROTRON RADIATION INSTRUMENTATION : Eighth International Conference on Synchrotron Radiation Instrumentation. AIP, 2004. http://dx.doi.org/10.1063/1.1757846.

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Niibe, M. « Characterization Of Light Radiated From 11 m Long Undulator ». Dans SYNCHROTRON RADIATION INSTRUMENTATION : Eighth International Conference on Synchrotron Radiation Instrumentation. AIP, 2004. http://dx.doi.org/10.1063/1.1757862.

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Nakamura, Norio. « An Electron-Beam Profile Monitor Using Fresnel Zone Plates ». Dans SYNCHROTRON RADIATION INSTRUMENTATION : Eighth International Conference on Synchrotron Radiation Instrumentation. AIP, 2004. http://dx.doi.org/10.1063/1.1757854.

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Rapports d'organisations sur le sujet "Synchrotron Radiatio"

1

Wiedemann, Helmut. Synchrotron Radiation. Office of Scientific and Technical Information (OSTI), août 2003. http://dx.doi.org/10.2172/815294.

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2

Liu, James C. Radiation Protection at Synchrotron Radiation Facilities. Office of Scientific and Technical Information (OSTI), octobre 2001. http://dx.doi.org/10.2172/798880.

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3

Donahue, R. J. ALS synchrotron radiation shielding. Office of Scientific and Technical Information (OSTI), octobre 1995. http://dx.doi.org/10.2172/186725.

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4

Winick, Herman. Future Synchrotron Radiation Sources. Office of Scientific and Technical Information (OSTI), juillet 2003. http://dx.doi.org/10.2172/813270.

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5

Liu, J. Radiation Safety System for Stanford Synchrotron Radiation Laboratory. Office of Scientific and Technical Information (OSTI), mars 2004. http://dx.doi.org/10.2172/826762.

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6

Zholents, A. A., et M. S. Zolotorev. Femto-second pulses of synchrotron radiation. Office of Scientific and Technical Information (OSTI), juillet 1995. http://dx.doi.org/10.2172/110718.

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7

Jenkins, Theodore M., et W. Ralph Nelson. Synchrotron Radiation in the Collider ARCS. Office of Scientific and Technical Information (OSTI), juillet 2014. http://dx.doi.org/10.2172/1146414.

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8

Venturini, Marco. Coherent Synchrotron Radiation in Storage Rings. Office of Scientific and Technical Information (OSTI), décembre 2002. http://dx.doi.org/10.2172/808716.

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9

Heifets, Samuel A. Single-mode coherent synchrotron radiation instability. Office of Scientific and Technical Information (OSTI), janvier 2003. http://dx.doi.org/10.2172/812613.

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10

Brown, Dennis Eugene. Nuclear dynamical diffraction using synchrotron radiation. Office of Scientific and Technical Information (OSTI), mai 1993. http://dx.doi.org/10.2172/10162176.

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