EP2095695A1 - Onduleur planaire hélicoïdal - Google Patents

Onduleur planaire hélicoïdal

Info

Publication number
EP2095695A1
EP2095695A1 EP07846613A EP07846613A EP2095695A1 EP 2095695 A1 EP2095695 A1 EP 2095695A1 EP 07846613 A EP07846613 A EP 07846613A EP 07846613 A EP07846613 A EP 07846613A EP 2095695 A1 EP2095695 A1 EP 2095695A1
Authority
EP
European Patent Office
Prior art keywords
undulator
section
winding
planar
coil
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Withdrawn
Application number
EP07846613A
Other languages
German (de)
English (en)
Inventor
Max Beckenbach
Theo Schneider
Bernd Lott
Marion KLÄSER
Matthias Eisele
Pauline Leys
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Karlsruher Institut fuer Technologie KIT
Original Assignee
Forschungszentrum Karlsruhe GmbH
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Forschungszentrum Karlsruhe GmbH filed Critical Forschungszentrum Karlsruhe GmbH
Publication of EP2095695A1 publication Critical patent/EP2095695A1/fr
Withdrawn legal-status Critical Current

Links

Classifications

    • H—ELECTRICITY
    • H05—ELECTRIC TECHNIQUES NOT OTHERWISE PROVIDED FOR
    • H05H—PLASMA TECHNIQUE; PRODUCTION OF ACCELERATED ELECTRICALLY-CHARGED PARTICLES OR OF NEUTRONS; PRODUCTION OR ACCELERATION OF NEUTRAL MOLECULAR OR ATOMIC BEAMS
    • H05H13/00—Magnetic resonance accelerators; Cyclotrons
    • H05H13/04—Synchrotrons
    • H—ELECTRICITY
    • H05—ELECTRIC TECHNIQUES NOT OTHERWISE PROVIDED FOR
    • H05G—X-RAY TECHNIQUE
    • H05G2/00—Apparatus or processes specially adapted for producing X-rays, not involving X-ray tubes, e.g. involving generation of a plasma
    • H—ELECTRICITY
    • H05—ELECTRIC TECHNIQUES NOT OTHERWISE PROVIDED FOR
    • H05H—PLASMA TECHNIQUE; PRODUCTION OF ACCELERATED ELECTRICALLY-CHARGED PARTICLES OR OF NEUTRONS; PRODUCTION OR ACCELERATION OF NEUTRAL MOLECULAR OR ATOMIC BEAMS
    • H05H7/00—Details of devices of the types covered by groups H05H9/00, H05H11/00, H05H13/00
    • H05H7/04—Magnet systems, e.g. undulators, wigglers; Energisation thereof

Definitions

  • the invention relates to a planar-helical undulator for electrically variable and with respect to the undulator length partially different polarization of the photon radiation emitted from it.
  • the undulator is a light source that emits polarized radiation. For this purpose, it is positioned along one or an accelerator path.
  • the undulator interacts with the near-axis region of its magnetic field to the continuous, electrically charged particle flow. Due to its velocity in the undulator region, the particle flow interacts with the undulator magnetic field according to the relationship vx * > , a deflecting field strength or a deflecting field
  • Undulators are used in particular for the generation of short-wave electromagnetic radiation, predominantly X-radiation, in synchrotrons.
  • the beam axis of the photon radiation emitted by the undulator is tangent to the particle beam axis.
  • a coil consists of two sections, a hot section and a planar section, of which the planer section m is inserted and positioned in the hot section.
  • the sections each consist of a coil body made of non-magnetic material, in which planar winding chambers are emgefrast around the coil axis.
  • the planar winding chambers are perpendicular to the coil axis, the hot winding chambers similarly penetrated at an angle 45 ° from the hot coil axis.
  • the distances of the successive winding chambers, the structural period length ⁇ b , are the same in both bobbins.
  • the Undulatorachse and the coil axes are parallel to each other and lie m a plane, the axial plane.
  • each winding chamber the winding base
  • the bottom of each winding chamber, the winding base is convex, especially circular at the inserted planar section.
  • the location in the winding ground with the largest radius of curvature or the area with the largest radius of curvature in the hot section is the Undulatorachse centered to the axis plane closest.
  • a section consists of an input and output region for the winding wire on the lateral surface in one end region and a winding wire connection on the lateral surface in the other end region, between them is the winding chamber region, wherein a section is in one piece or with small number of winding chambers from the two end regions or at a larger number of winding chambers from the two end portions and at least one chamber portion therebetween, wherein the at least two section parts are connected to each other via axial connecting elements forming a section.
  • the winding wire is a normal electrical conductor or a technical superconductor, with him a section under constant, predetermined tension in always the same winding sense wound as follows:
  • a first piece of winding wire extends from the winding wire entry form fitting incident on the lateral surface to the winding base of the first winding chamber and traverses this form-fitting Inset. It then cuts through the jacket to the next, second winding chamber to the winding base and is wound up high. From there, the winding wire cuts through the jacket to the next, third winding chamber, where it runs to the winding base and traverses it in a positively fitting manner. Further, it cuts the jacket to the winding base of the following, fourth winding chamber and is wound in the same direction as before high.
  • a second piece of winding wire runs from the winding wire output form fitting lying over the lateral surface to the winding base of the first winding chamber and is wound in the same direction as in the even-numbered winding chambers. It then cuts through the jacket to the second winding, crosses it, then cuts through the jacket to the third winding chamber on the winding base and is wound in the same direction as previously high. Then it cuts through the jacket to the fourth winding chamber, crosses it, then cuts through the jacket to the fifth winding chamber on the winding base and is wound up high. In this manner, until the last even-numbered winding chamber from which it crosses the even-numbered winding and leads to the winding wire connection.
  • the underpasses and overpasses as well as the conductor connections and conductor connections lie in the area of the coil body facing away from the undulator axis.
  • the windings are electrically connected to each other in series, but generate when energized magnetic fields whose opposite magnetic field axes are opposite, in the case of the hot section opposite in parallel.
  • the number of turns in the winding chambers of a section is constant.
  • the amounts of currents applied to the superconducting material in the individual sub-undulators can be adjusted independently of each other, whereby the resulting undulator field resulting from the superposition of the undulator field generated by the sub-undulators , determines the polarization direction of the synchrotron radiation, to which a first subundulator is arranged so that its first undulator field is substantially perpendicular to the direction of particle flow, and a second subundulator is arranged so that its second undulator field is a non-zero component both in direction of the first undulator field as well as in the direction which is substantially perpendicular to the direction of the first undulator field and in the direction Substantially perpendicular to the direction of the particle flow has.
  • the technical problem is the production of an undulator and thus the realization of the windings of such an undulator.
  • locally high magnetic field strengths and strong field gradients can be achieved with which a safe operation without degradation and spontaneous transition from the superconductivity to the normal line, the quenching effect or quenching is possible.
  • the object of the physics described in DE 103 58 225 is to provide an undulator of electromagnetic components, with which the desired polarization of the out of the. Only on the change of the current in the undulator magnetic field generating conductor sections and not on mechanically / locally moving undulator Undulator emitted light can be adjusted.
  • a technical solution of a planar-helical undulator is to be specified, with which either only the linear or only the circular or only the elliptical polarization can be set, but also the technical solution of a planar-helical undulator can be specified the emitted light beam, the synchrotron light from the undulator, partially different polarized occurs.
  • the magnetic field generating devices of the undulator in a known manner from e- lektrisch normalêt, especially superconducting solenoidalen Windings exist.
  • the boundary conditions for the production of superconducting coils are also complied with; at least: suitable superconductors, suitable bobbins, electrical insulation of the bobbin, conductor guidance in the winding chambers, conductor guidance at Spulenein- and output, conductor guidance in the crossings, Spulenein- and output, surges, Lorentz forces, quenching safety.
  • each winding chamber is, viewed from the outside, convex and the location or area in the winding base with the largest radius of curvature is closest to the undulator axis centered to the axis plane and the two sections of a coil have equal numbers or different numbers of winding chambers. In the case of the same number of winding chambers, the longitudinal areas of the two sections coincide. In the case of different numbers, the section with the smaller number of winding chambers is completely positioned in the longitudinal region of the longer section.
  • the planar section In the case of two equally long sections of a coil and annular winding chambers of the planar section and in each case a constant number of windings in both sections, the planar section is positioned around the vertical section. Also, in the case of equally long sections of a coil, the number of turns in the winding chambers is not constant in at least one section of a coil. However, it then changes symmetrically over the length of the section to its section center. In this case, the planar section may also be in the vertical section or vice versa, the planar section surrounds the hot section.
  • the number of turns in the winding chambers is constant or in at least one section of the coil, the number of turns in the winding chambers is not constant, but changes symmetrically over the length of the section to its section center.
  • Short sections can follow each other in the long section of the long section, but only if the long section is very long compared to a short section.
  • three polarization sections namely two identical ones, which are interrupted by a different polarization section, can then be generated.
  • the sequence of equal polarization is interrupted according to the number of short sections by a generally different polarization.
  • the magnetic field which can be generated by the respective planar section of the two coils of the planar helical undulator and about the undulator / beam axis, which is perpendicular to this axis, has a periodic, sinusoidal course, ie, between two successive winding chambers in the course of the undulator axis a magnetic field maximum and at the winding chamber center, the magnetic field generated therefrom is zero, or this magnetic field makes there along the Undulatorachse a reversal of direction.
  • a magnetic field perpendicular to the beam axis is generated along and around the undulator / beam axis, which has a planar portion of the magnetic field and thus, as explained above, is periodic, and one to and to the beam axis has further field share, which also along the beam axis periodically, but now cosinus-like, ie between two consecutive hot winding chambers, there is a zero crossing and thus a change in direction of the generated by the successive hot winding chambers hot field component.
  • the number of winding chambers of the planar section due to the sinusoidal magnetic field characteristic even or uneven be radiereig, because in any case, along the beam axis through the eterulator flying electrically charged particle undergoes complete compensation / neutralization of its experienced by the undulator magnet field orbit disturbances.
  • the planar-helical transder can be represented in two ways. According to claim 2, it is formed by folding the one ündulatorspule by 180 ° to the beam or undulator axis. He is thus made by two identical to ⁇ identical coils with planar and hot section. The other illustration is according to claim 3, the symmetrical to the undulator axis position of a coil to another. However, this situation can not be realized with two identical coils but only with two identical but not identical coils, because then the hot section is in a coil mirror image of the coil axis of the other of the other coil.
  • planar-helical undulator When constructing the planar-helical undulator according to claim 2 or claim 3, attention must be paid to the energization of the two hot sections so that the necessary magnetic field addition between the two coils is achieved in order to obtain a hot magnetic field component of the inductor field.
  • the mirrored hot section is for generating the magnetic field opposite the folded hot section Claim 2 opposite flows through the stream. Claim 2 describes the technically simpler solution to the planar-helical undulatory tor, since this consists of two identical coils.
  • the positioning of the two coils of the planar-helical undulator to each other can also be done in two ways, namely according to claim 4, the two coils of the undulator are mechanically not coupled together and are thus anchored individually adjusted in their environment. According to claim 5, both coils are mechanically coupled together while maintaining a passband for the passing, electrically charged particle beam or the electron beam to measure, so that the planar-helical undulator is adjusted as a whole with respect to the beam axis path.
  • the bobbin material is dielectric and / or metallic, wherein a bobbin depending on the structure consists of one or the other or a combination of bobbin parts.
  • the winding wire has round, usually circular or rectangular cross section with a predetermined aspect ratio.
  • the conductor for the winding in the winding chamber may even be markedly band-shaped.
  • the winding wire is electrically normally conductive.
  • the winding wire is electrically normally conductive.
  • only the contact at the winding input, winding output and the winding wire connection may be normally conductive.
  • Another type of conductor is characterized in claim 10. Thereafter, the winding wire is a technical superconductor.
  • the superconductor is for example of NbTi or NbXTi or MgB.
  • the winding of the winding wire in a winding chamber is at least single-layered and at least single-conducting. At least one conductor is located per layer of a winding. This is the case anyway with a purely band-shaped winding (pancake).
  • the winding input, output, winding wire connection, undercrossing at the bottom of the winding chamber, and traversing the winding in a winding chamber are in the region away from the undulator axis, i. the formation of the magnetic field influenced there by the under- and overpass of the winding wire / -band has no influence on the undulator magnetic field.
  • the two planar sections are in operation flowed through by the same current I 2 and the current direction in the relative to the undulator axis opposite planar windings when penetrating the axial plane is the same. This is best achieved by an electrically corresponding series connection of the two planar sections.
  • the two hot sections in operation flowed through by the same current Ii and the current direction in the respect to the Undulatorachse opposite to each other hot windings when penetrating the axial plane is the same.
  • a modified variant is described in claim 17. There, the two hot sections are in operation flowed through by the same current Ii and the current direction in the respect to the Undulatorachse opposite each other, hot windings is opposite to the penetration of the axial plane.
  • the setting of the two section currents Ii and I2 results in a generally elliptical polarization depending on the respective section length emitted by the undulator reaches the photon radiation, wherein the elliptical polarization by current setting circular, or can be degenerate to a linear polarization.
  • the planar-helical undulator has a region or regions with only planar sections, ie there is a purely planar undulator, a photon beam with only linear polarization is generated there. Conversely, an area or areas with only a hot section will generate or produce a photon beam of generally elliptical polarization.
  • one of the two coils emerges by mirroring the other at the plane through the undulator / beam axis, which is perpendicular to the axial plane, and thus at least partially a planar-helical undulator, depending on the current direction through the respective hot section either a linear Polarization of the photon radiation emitted by the undulator or generates a generally elliptical polarization of the photon radiation emitted by the undulator.
  • section-dependent polarization is described in detail in the above-cited scientific report FZKA 6997 for the situation of equal section length, inner planar section with circular winding chambers and constant number of turns in the winding chambers of the two sections and thus directly on the sections of the planar-helical undulator with both sections transferable. Portions of the planar-helical undulator with only the two planar sections generate light with only linear polarization. Conversely, portions of the planar-helical undulator with only the two hot sections produce light of generally elliptical polarization.
  • Figure 1 planar helical coil with partially surrounding hot section
  • FIG. 2 shows a planar-helical undulator formed by folding
  • FIG. 3 shows a planar-helical undulator resulting from reflection
  • Figure 4 planar helical coil with partially surrounding planar section;
  • FIG. 5 planar helical undulator resulting from folding
  • FIG. 6 shows a planar-helical coil with an overlapping surrounding planar section
  • FIG. 7 shows a planar-helical undulator formed by folding
  • Figure 8 planar-helical undulator coil with overlapping surrounding hot section
  • FIG. 9 shows a planar-helical undulator formed by folding
  • the two planar sections in the planar-helical undulator are in the two identical planar-helical coils and in relation to the Undulatorachse mirror-symmetrical planar helical coils electrically also in series with each other and are connected to a controllable and controllable power supply, as the two hot sections such that the two magnetic field components which can be generated are adjustable independently of one another along and around the undulator / beam axis.
  • magnetic field addition and subtraction and reversal of the magnetic field direction for the undulator magnetic field with stationary undulator coils can be set as desired only via the current setting.
  • the two coils mechanically adjusted to the planar-helical undulator remain in this adjusted position.
  • Figure 1 illustrates the planar helical coil in which the hot section surrounds the planar one.
  • the planar section consists of 11, ie odd, axially juxtaposed nikrmgformigen windings, which is not axially within its long range of the clairvoyance section of 4 axially juxtaposed, elliptical annular windings surrounded.
  • the planar section is longer than the surrounding hot, both are not long identical.
  • the windings of both sections have the same winding spacing and the hot winding area or the two hot winding areas with the largest radius of curvature come closest to the winding area of the associated planar winding. It is here are only 4 planar-helical Wicklungsproving- or winding pairs in the coil.
  • FIG. 2 shows the planar helical undulator composed of two identical coils according to FIG. 1, that is to say folding of one coil 180 ° about the undulator axis produces the other coil. Both coils with their respective non-identical planar and hot sections are identical.
  • FIG. 3 shows the planar helical undulator composed of two coils which are relative to one another with respect to the undulator axis. Both coils with their respective non-identical planar and hot sections are no longer identical.
  • the electrically charged particles flying along the undulator axis usually electrons, emit light in the magnetic field around and along the undulator axis, monochromatic or narrow-band X-ray light, the undulator light, in the particle path direction with sections of different polarization, namely, the electrons from At the left side of the undulator, first a purely linear polarization in the first flying through, free-standing planar section, then a generally elliptical polarization in the coincident planar-helical section and finally again pure linear polarization in the planar section on the right.
  • undulator light is generated with sections of different polarization.
  • the polarization sections are determined by the velocity / energy (see, for example, equations 2.11 to 2.13 in the FZK 6997 scientific report) of the passing electrons and the length of the exposed planar sections and the length of the actually planar-helical section, ie the formation of the to the undulator axis and in the same vertical magnetic field, determined / fixed.
  • Figure 2 in DE 103 58 225 shows the planar-helical undulator with two identical coils, in which the planar and the hot section have the same number of winding chambers and also windings and the planar section is surrounded by the hot congruent ones Section 3 there are long identical.
  • Figure 3 represents the planar helical coil in which the hot section also surrounds the planar one.
  • the planar section consists of 7 axially juxtaposed Vietnameseringformigen windings, which is not axially within their Langs Kunststoffs surrounded by the hot section of 10 axially juxtaposed, elliptical annular windings.
  • the planar section is shorter here than the surrounding one, so both are not long identical either.
  • the windings of both sections also have the same winding spacing and the hot winding area or the two hot winding areas with the greatest radius of curvature come closest to the winding area of the associated planar winding.
  • there are 7 planar-helical Wicklungssch- or winding pairs in the coil here.
  • the hot section of the coil overhangs the planar bilateral.
  • the planar-helical undulator comes in the manner described by folding by 180 ° about the ündulatorachse and thus consists of two identical coils ( Figure 5), or by mirroring a coil on the Ündulatorachse and thus consists of two identical but not identical coils. The latter is no longer shown, but can be seen from Figure 3 accordingly.
  • a light beam is generated tangentially to the electron beam axis by the flying electrical charge carriers / electrons, which occurs in sequence sections with elliptical, then elliptical or linear and then elliptical polarization.
  • the elliptical polarization may also be circular in particular.
  • Figure 6 illustrates the planar helical coil in which the hot section is surrounded by the planar one.
  • the planar section here consists of 7 axially lined elliptical annular windings or winding chambers with elliptical winding ground, which is not axially centered within the Langs Symposiums the hot section of here 10 axially juxtaposed, also elliptical annular windings.
  • the planar section is shorter than the inside lying hot.
  • both sections of the coil are not identical in length. Axial the windings of both sections have the same winding distance, and the hot winding area or the two hot winding areas with the largest radius of curvature comes, or come to the winding area of the associated planar Winding with the largest radius of curvature also next.
  • planar-winding winding chamber or winding pairs there are 7 planar-winding winding chamber or winding pairs in the coil.
  • the planar-undulating undulator according to FIG. 7 formed therefrom also comes about here in the two manners described above by two identically constructed coils (folding by 180 °). (The likewise possible generation of the undulator by reflection is no longer represented in this case.)
  • this undulator a light beam is generated tangentially to the electron beam axis by the electric charge carriers / electrons passing through, which in turn result in sections with elliptical, then elliptical or linear and then elliptical Polarization occurs.
  • the elliptical polarization can again be especially circular.
  • FIG. 8 illustrates the planar helical coil in which the hot section is surrounded by the planar one.
  • the planar section now consists of 9 elliptical or annular windings arranged axially adjacent to each other or of winding hammers with an elliptical winding base which do not axially axially overlap the longitudinal region of the vertical section of 4 axially aligned, likewise elliptically annular windings on both sides.
  • the planar section is longer than the internal one. Both sections of the coil are not long identical.
  • the windings of both sections have the same winding spacing, and the hot winding area or the two hot winding areas with the largest radius of curvature come closest to the winding area of the associated planar winding with the largest radius of curvature.
  • there are 4 planar-helical Wicklungs hunt- or winding pairs in the coil.
  • the planar-helical undulator also comes here in the two ways described above by two identical or two bauver Kunststoffene different coils. Shown in Figure 9 is only the generation of the undulator by 180 ° - folding.
  • a light beam is generated tangentially to the electron beam axis by the electric charge carriers / electrons passing through, which consequently results in sections with linear, then adjustable elliptical or linear and then planar polarization. occurs.
  • the adjustable elliptical polarization can also be circular in particular.
  • a planar-helical undulator can be built to produce a light beam with more than 2 sections of pure linear or pure elliptical polarization, depending on the coil design. See above for a comment on several axially successive small sections in the long range of a very long section. In the long range of the very long planar section, for example, there were then more than two hot sections or vice versa, actually an axial sequence of more than two planar-helical undulators - a technically complex device.
  • a natural limitation of the entire undulator length lies in the divergence of the light beam generated in it, in particular in the initial region.

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  • Physics & Mathematics (AREA)
  • Engineering & Computer Science (AREA)
  • Plasma & Fusion (AREA)
  • Spectroscopy & Molecular Physics (AREA)
  • Optics & Photonics (AREA)
  • Particle Accelerators (AREA)

Abstract

L'onduleur planaire hélicoïdal selon l'invention est composé, pour la polarisation électrique entièrement variable de 360° des rayons X qu'il émet, de deux bobines identiques ou de construction identique, qui ont respectivement une section planaire et une section hélicoïdale. Le fond de chaque chambre d'enroulement dans une section est convexe, vu de l'extérieur, et le point ou la zone au fond de l'enroulement qui présente le plus grand rayon de courbure se situe au plus près du centre de l'axe de l'onduleur, de manière centrée par rapport au plan de l'axe. Les deux sections d'une bobine ont un nombre égal ou différent de chambres d'enroulement. Les zones longitudinales des deux sections se recouvrent ou la plus petite se situe entièrement dans la grande. Dans le cas de sections de même longueur d'une bobine et de chambres d'enroulement circulaires de la section planaire, ainsi que d'un nombre constant d'enroulements dans les deux sections, la section planaire est placée autour de la section hélicoïdale. Dans le cas de deux sections de même longueur d'une bobine dans au moins une section d'une bobine, le nombre d'enroulements dans les chambres d'enroulement n'est pas constant et varie sur la longueur de la section symétriquement par rapport au milieu de ladite section. Dans le cas de sections de longueur différente, le nombre d'enroulements dans les chambres d'enroulement est constant ou le nombre d'enroulements dans les chambres d'enroulement n'est pas constant ou varie sur la longueur de la section symétriquement par rapport au milieu de ladite section, au moins dans une section de la bobine. Le nombre de chambres d'enroulement de la section planaire est >= 2 et le nombre de chambres d'enroulement de la section hélicoïdale d'une bobine est >= 2 et pair.
EP07846613A 2006-11-28 2007-11-16 Onduleur planaire hélicoïdal Withdrawn EP2095695A1 (fr)

Applications Claiming Priority (2)

Application Number Priority Date Filing Date Title
DE102006056052A DE102006056052B4 (de) 2006-11-28 2006-11-28 Planar-helischer Undulator
PCT/EP2007/009900 WO2008064779A1 (fr) 2006-11-28 2007-11-16 Onduleur planaire hélicoïdal

Publications (1)

Publication Number Publication Date
EP2095695A1 true EP2095695A1 (fr) 2009-09-02

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US (1) US8134440B2 (fr)
EP (1) EP2095695A1 (fr)
JP (1) JP2010511273A (fr)
DE (1) DE102006056052B4 (fr)
WO (1) WO2008064779A1 (fr)

Families Citing this family (13)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP2342953A4 (fr) * 2008-09-15 2014-09-17 Univ Singapore Mini-onduleur supraconducteur à bobine simple
DE102008053162B3 (de) * 2008-10-24 2010-07-29 Karlsruher Institut für Technologie Undulator zur Erzeugung von Synchrotronstrahlung
DE102009048400A1 (de) * 2009-10-06 2011-04-14 Siemens Aktiengesellschaft HF-Resonatorkavität und Beschleuniger
CN102638113B (zh) * 2012-04-11 2014-08-27 华中科技大学 一种磁耦合谐振装置
DE102012214063A1 (de) 2012-08-08 2014-02-13 Carl Zeiss Smt Gmbh Beleuchtungssystem für eine Projektionsbelichtungsanlage für die EUV-Projektionslithographie
DE102012219936A1 (de) * 2012-10-31 2014-04-30 Carl Zeiss Smt Gmbh EUV-Lichtquelle zur Erzeugung eines Nutz-Ausgabestrahls für eine Projektionsbelichtungsanlage
CN102945722B (zh) * 2012-11-27 2015-04-15 中国科学院上海应用物理研究所 一种二硼化镁超导波荡器
EP3514630B1 (fr) 2013-06-18 2022-06-22 ASML Netherlands B.V. Laser à électrons libres et procédé de génération d'un faisceau de rayonnement à uv extrême utilisant le même
WO2015044182A2 (fr) * 2013-09-25 2015-04-02 Asml Netherlands B.V. Appareil d'acheminement de faisceau et procédé associé
DE102014205579A1 (de) 2014-03-26 2015-10-01 Carl Zeiss Smt Gmbh EUV-Lichtquelle für eine Beleuchtungseinrichtung einer mikrolithographischen Projektionsbelichtungsanlage
US9355767B2 (en) 2014-09-03 2016-05-31 Uchicago Argonne, Llc Undulator with dynamic compensation of magnetic forces
US10249420B2 (en) * 2015-12-08 2019-04-02 Uchicago Argonne, Llc Continuous winding magnets using thin film conductors without resistive joints
CN118679528A (zh) * 2022-03-14 2024-09-20 普林斯顿大学受托公司 平面线圈仿星器

Family Cites Families (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4523168A (en) * 1982-09-27 1985-06-11 Scanditronix Inc. Electromagnet
EP0305685B1 (fr) * 1987-09-03 1990-11-28 Peter Schuster Entraînement linéaire sans contact
US4764743A (en) * 1987-10-26 1988-08-16 The United States Of America As Represented By The Secretary Of The Army Permanent magnet structures for the production of transverse helical fields
EP0577874A1 (fr) * 1992-07-08 1994-01-12 Siemens Aktiengesellschaft Ondulateur comportant des agencements de bobines concentriques
JPH0660998A (ja) * 1992-08-04 1994-03-04 Sumitomo Electric Ind Ltd 収束型多極アンジュレータ
US5675304A (en) * 1995-07-26 1997-10-07 Raytheon Engineers & Constructors Magnet structure and method of operation
US6876288B2 (en) * 2002-03-29 2005-04-05 Andrey V. Gavrilin Transverse field bitter-type magnet
US6858998B1 (en) * 2002-09-04 2005-02-22 The United States Of America As Represented By The United States Department Of Energy Variable-period undulators for synchrotron radiation
DE10358225B3 (de) * 2003-12-12 2005-06-30 Forschungszentrum Karlsruhe Gmbh Undulator und Verfahren zu dessen Betrieb

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
See references of WO2008064779A1 *

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US20100045410A1 (en) 2010-02-25
DE102006056052A1 (de) 2008-05-29
US8134440B2 (en) 2012-03-13
WO2008064779A1 (fr) 2008-06-05
JP2010511273A (ja) 2010-04-08
DE102006056052B4 (de) 2009-04-16

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