EP2191698B1 - Source de rayonnement - Google Patents

Source de rayonnement Download PDF

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Publication number
EP2191698B1
EP2191698B1 EP08806915A EP08806915A EP2191698B1 EP 2191698 B1 EP2191698 B1 EP 2191698B1 EP 08806915 A EP08806915 A EP 08806915A EP 08806915 A EP08806915 A EP 08806915A EP 2191698 B1 EP2191698 B1 EP 2191698B1
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EP
European Patent Office
Prior art keywords
source
radiation
conduit
buffer gas
outlet
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EP08806915A
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German (de)
English (en)
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EP2191698A2 (fr
Inventor
Vadim Yevgenyevich Banine
Vladimir Vitalevich Ivanov
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ASML Netherlands BV
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ASML Netherlands BV
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Priority claimed from US12/078,663 external-priority patent/US7763871B2/en
Application filed by ASML Netherlands BV filed Critical ASML Netherlands BV
Publication of EP2191698A2 publication Critical patent/EP2191698A2/fr
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    • 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
    • H05G2/001—X-ray radiation generated from plasma
    • H05G2/003—X-ray radiation generated from plasma being produced from a liquid or gas
    • 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
    • H05G2/001—X-ray radiation generated from plasma
    • H05G2/008—X-ray radiation generated from plasma involving a beam of energy, e.g. laser or electron beam in the process of exciting the plasma

Definitions

  • the present invention relates to a radiation source, a method of generating radiation, and to a lithographic apparatus which includes the radiation source.
  • a lithographic apparatus is a machine that applies a desired pattern onto a substrate, usually onto a target portion of the substrate.
  • a lithographic apparatus can be used, for example, in the manufacture of integrated circuits (ICs).
  • a patterning device which is alternatively referred to as a mask or a reticle, may be used to generate a circuit pattern to be formed on an individual layer of the IC.
  • This pattern can be transferred onto a target portion (e.g. comprising part of, one, or several dies) on a substrate (e.g. a silicon wafer). Transfer of the pattern is typically via imaging onto a layer of radiation-sensitive material (resist) provided on the substrate.
  • resist radiation-sensitive material
  • a single substrate will contain a network of adjacent target portions that are successively patterned.
  • lithographic apparatus include so-called steppers, in which each target portion is irradiated by exposing an entire pattern onto the target portion at one time, and so-called scanners, in which each target portion is irradiated by scanning the pattern through a radiation beam in a given direction (the "scanning"-direction) while synchronously scanning the substrate parallel or anti-parallel to this direction. It is also possible to transfer the pattern from the patterning device to the substrate by imprinting the pattern onto the substrate.
  • extreme ultraviolet radiation having a wavelength within the range of 10-20 nm, for example within the range of 13-14 nm. It has further been proposed that radiation with a wavelength of less than 10 nm could be used, for example 6.7 nm or 6.8 nm. In the context of lithography, wavelengths of less than 10 nm are sometimes referred to as 'beyond EUV'.
  • Extreme ultraviolet radiation and beyond EUV radiation may be produced using a plasma.
  • the plasma may be created for example by directing a laser at particles of a suitable material (e.g. tin), or by directing a laser at a stream of a suitable gas (e.g. Sn vapor, SnH 4 , or a mixture of Sn vapor and any gas with a small nuclear charge (for example from H2 up to Ar)).
  • a suitable material e.g. tin
  • a suitable gas e.g. Sn vapor, SnH 4 , or a mixture of Sn vapor and any gas with a small nuclear charge (for example from H2 up to Ar)
  • the plasma In addition to extreme ultraviolet radiation (or beyond EUV radiation), the plasma produces debris in the form of particles, such as thermalized atoms, ions, nanoclusters, and/or microparticles.
  • the debris may cause damage to the collector mirror (or other components).
  • a buffer gas may be provided in the vicinity of the plasma. The particles produced by the plasma collide with molecules of the buffer gas, and thereby lose energy. In this way, at least some of the particles may be slowed sufficiently that they do not reach the collector mirror. Damage caused to the collector mirror may thereby be reduced. However, even when buffer gas is used, some particles may still reach the collector mirror and cause damage to it.
  • US2006/0186356 discloses an EUV light source device for protecting a collection mirror from debris that is considered harmful to a mirror coating.
  • the EUV light source device includes: a chamber in which extreme ultra violet light is generated; a target injection unit and a target injection nozzle that supply the chamber with a material to become the target; a laser light source that applies a laser beam to the target so as to generate plasma; a collection mirror that collects the extreme ultra violet light emitted from the plasma; an X-ray source that ionizes neutral particles included in particles emitted from the plasma into charged particles; and plural magnets that generate a magnetic field within the chamber so as to trap at least the charged particles ionized by the X-ray source.
  • a radiation source as set out in claim 1.
  • a lithographic apparatus as set out in claim 16.
  • Figure 1 schematically depicts a lithographic apparatus according to one embodiment of the invention.
  • the apparatus comprises:
  • the illumination system may include various types of optical components, such as refractive, reflective, magnetic, electromagnetic, electrostatic or other types of optical components, or any combination thereof, for directing, shaping, or controlling radiation.
  • optical components such as refractive, reflective, magnetic, electromagnetic, electrostatic or other types of optical components, or any combination thereof, for directing, shaping, or controlling radiation.
  • the support structure supports, i.e. bears the weight of, the patterning device. It holds the patterning device in a manner that depends on the orientation of the patterning device, the design of the lithographic apparatus, and other conditions, such as for example whether or not the patterning device is held in a vacuum environment.
  • the support structure can use mechanical, vacuum, electrostatic or other clamping techniques to hold the patterning device.
  • the support structure may be a frame or a table, for example, which may be fixed or movable as required.
  • the support structure may ensure that the patterning device is at a desired position, for example with respect to the projection system. Any use of the terms "reticle” or “mask” herein may be considered synonymous with the more general term "patterning device.”
  • patterning device used herein should be broadly interpreted as referring to any device that can be used to impart a radiation beam with a pattern in its cross-section such as to create a pattern in a target portion of the substrate. It should be noted that the pattern imparted to the radiation beam may not exactly correspond to the desired pattern in the target portion of the substrate, for example if the pattern includes phase-shifting features or so called assist features. Generally, the pattern imparted to the radiation beam will correspond to a particular functional layer in a device being created in the target portion, such as an integrated circuit.
  • patterning devices include masks and programmable mirror arrays.
  • Masks are well known in lithography, and typically in an EUV or beyond EUV lithographic apparatus would be reflective.
  • An example of a programmable mirror array employs a matrix arrangement of small mirrors, each of which can be individually tilted so as to reflect an incoming radiation beam in different directions. The tilted mirrors impart a pattern in a radiation beam which is reflected by the mirror matrix.
  • projection system used herein should be broadly interpreted as encompassing any type of projection system. Usually, in an EUV or beyond EUV lithographic apparatus the optical elements will be reflective. However, other types of optical element may be used. The optical elements may be in a vacuum. Any use of the term “projection lens” herein may be considered as synonymous with the more general term “projection system”.
  • the apparatus is of a reflective type (e.g. employing a reflective mask).
  • the lithographic apparatus may be of a type having two (dual stage) or more substrate tables (and/or two or more mask tables). In such "multiple stage” machines the additional tables may be used in parallel, or preparatory steps may be carried out on one or more tables while one or more other tables are being used for exposure.
  • the illuminator IL receives a radiation beam from a radiation source SO.
  • the source and the lithographic apparatus may be separate entities. In such cases, the source is not considered to form part of the lithographic apparatus and the radiation beam is passed from the source SO to the illuminator IL with the aid of a beam delivery system comprising, for example, suitable directing mirrors and/or a beam expander. In other cases the source may be an integral part of the lithographic apparatus.
  • the source SO and the illuminator IL, together with the beam delivery system if required, may be referred to as a radiation system.
  • the illuminator IL may comprise an adjuster for adjusting the angular intensity distribution of the radiation beam. Generally, at least the outer and/or inner radial extent (commonly referred to as ⁇ -outer and ⁇ -inner, respectively) of the intensity distribution in a pupil plane of the illuminator can be adjusted.
  • the illuminator IL may comprise various other components, such as an integrator and a condenser. The illuminator may be used to condition the radiation beam B to have a desired uniformity and intensity distribution in its cross-section.
  • the radiation beam B is incident on the patterning device (e.g., mask MA), which is held on the support structure (e.g., mask table MT), and is patterned by the patterning device. Having been reflected by the mask MA, the radiation beam B passes through the projection system PS, which focuses the beam onto a target portion C of the substrate W.
  • the substrate table WT can be moved accurately, e.g. so as to position different target portions C in the path of the radiation beam B.
  • the first positioner PM and another position sensor IF1 can be used to accurately position the mask MA with respect to the path of the radiation beam B, e.g. after mechanical retrieval from a mask library, or during a scan.
  • movement of the mask table MT may be realized with the aid of a long-stroke module (coarse positioning) and a short-stroke module (fine positioning), which form part of the first positioner PM.
  • movement of the substrate table WT may be realized using a long-stroke module and a short-stroke module, which form part of the second positioner PW.
  • the mask table MT may be connected to a short-stroke actuator only, or may be fixed.
  • Mask MA and substrate W may be aligned using mask alignment marks M1, M2 and substrate alignment marks PI, P2.
  • the substrate alignment marks as illustrated occupy dedicated target portions, they may be located in spaces between target portions (these are known as scribe-lane alignment marks).
  • the mask alignment marks may be located between the dies.
  • the depicted apparatus could be used in at least one of the following modes:
  • Figure 2 shows schematically a source SO according to an embodiment of the invention.
  • Figure 2a shows the source SO in cross section viewed from one side
  • Figure 2b shows the source in cross section viewed from above.
  • the source SO comprises a chamber 1.
  • the chamber 1 is defined by walls 2 and a collector mirror 3.
  • the collector mirror 3 has a reflective surface which is reflective at extreme ultraviolet radiation wavelengths.
  • a supply 4 is arranged to supply droplets of material (for example tin) into the chamber 1.
  • a collector 5 is located beneath the supply 4 at the bottom of the chamber 1, and is arranged to collect material which has passed through the chamber 1.
  • the collector mirror 3 is arranged to focus radiation to a focal point FP, from where the radiation may pass into the illuminator IL of the lithographic apparatus (see figure 1 ).
  • a laser 6 is used to generate a beam of radiation 7 which is directed into the chamber 1 via an aperture 8.
  • the aperture 8 may for example comprise a window which is transmissive at the wavelength of the laser beam 7.
  • a beam dump 9 is located within the chamber 1, and is positioned such that any portion of the laser beam 7 which does not interact with material provided by the material supply 4 is incident upon (and absorbed by) the beam dump.
  • Gas coolers 10 extend into the chamber 1 from side walls of the chamber.
  • a buffer gas supply comprises a conduit 11 which extends into the chamber 1 from a side wall of the chamber, and has an outlet 12 which delivers buffer gas adjacent to an interaction point 13 at which the laser beam 7 is incident upon material supplied from the material supplied 4.
  • the chamber 1 is filled with a suitable buffer gas (for example hydrogen).
  • the laser 6 generates a laser beam 7 which passes through the aperture 8 in the collector mirror 3 and into the chamber 1.
  • the material supply 4 produces a droplet of material which falls downwards through the chamber 1 towards the collector 5.
  • the interaction of the laser beam 7 and the droplet of material causes at least some of the material to be converted into a plasma.
  • the plasma emits extreme ultraviolet radiation which is collected by the collector mirror 3 and focused to the focal point FP.
  • the extreme ultraviolet radiation passes from the focal point FP into the illuminator IL of the lithographic apparatus (see figure 1 ).
  • Parts of the droplet of material which do not interact with the laser beam 7 continue to fall through the chamber 1 and are collected by the collector 5.
  • the plasma generated by the interaction of the laser beam 7 and the droplet of material may include particles which would cause damage to the collector mirror 3.
  • the buffer gas present in the chamber 1 is intended to slow down the particles so that they do not reach the collector mirror 3.
  • the violence of the interaction between the laser beam 7 and the tin particle at the interaction point 13 is such that the buffer gas is heated and pushed away from the interaction point when the laser beam interacts with the droplet of material. This will cause the buffer gas in a region around the interaction point to have a higher temperature and a lower density.
  • the heated buffer gas may for example move towards the gas coolers 10
  • the time taken for the heated buffer gas to move away from the region around the interaction point 13 may for example be of the order of tens of milliseconds.
  • the time between delivery of successive droplets of material to the interaction point 13 may be significantly shorter than this, for example 10-20 microseconds. This means that the heated buffer gas may remain present in the region around the interaction point 13 during the generation of successive pulses of EUV radiation.
  • the region around the interaction point 13 which is occupied by the heated buffer gas may comprise a significant proportion of the volume between the interaction point 13 and the collector mirror 3.
  • the heated buffer gas in this region has a lower density than gas which has not been heated, and a result there are less interactions between the particles of the plasma and the buffer gas. Consequently, it is more likely that particles may reach the collector mirror 3. When this occurs damage may be caused to the collector mirror 3.
  • the above problem is solved or reduced in magnitude by the conduit 11 shown in Figure 2 .
  • the conduit 11 has an outlet 12 which is located adjacent to the interaction point 13, and thereby delivers unheated buffer gas adjacent to the interaction point 13.
  • the outlet 12 of the conduit 11 immediately and directly delivers unheated buffer gas into the region around the interaction point 13. Consequently, by the time the next droplet of material has reached the interaction point 13, newly delivered buffer gas will be present in the region around the interaction point 13.
  • This newly delivered buffer gas is unheated and is therefore more dense than heated buffer gas.
  • the buffer gas is therefore more effective.
  • the embodiment of the invention therefore provides improved protection of the collector mirror 3 from particles generated during plasma formation. It therefore allows the collector mirror 3 to have a longer lifetime before cleaning and/or replacement than may otherwise be the case.
  • the buffer gas may be delivered with a high velocity (for example 100-2000 m/s). This provides the advantage that it quickly pushes away heated buffer gas from the region around the interaction point 13.
  • the buffer gas may be delivered in a supersonic gas jet which is directed at or adjacent to the interaction point 13.
  • the supersonic gas jet has the advantage that the density of buffer gas within the jet may be substantially larger than mean density of buffer gas in the chamber, thereby providing an increased interaction of fast ions with the buffer gas adjacent to the interaction point 13.
  • one or more vents may be used to carry buffer gas from the chamber 1, and thereby regulate the pressure of buffer gas within the chamber.
  • the gas coolers 10 regulate the temperature of the buffer gas.
  • the conduit 11 is provided at a location which is selected such that extreme ultraviolet radiation which is obscured by the conduit 11 would have been obscured by other elements of the apparatus if the conduit 11 were not present.
  • the conduit 11 is located in front of a gas cooler 10 which would obscure the EUV radiation irrespective of whether or not the conduit 11 is present.
  • the conduit 11 is vertically displaced with respect to the laser beam 7, so that the laser beam does not pass into the conduit 11, but instead travels next to it and is incident upon the beam dump 9.
  • the outlet of the conduit 11 is adjacent to the interaction point 13.
  • the outlet of the conduit 11 may be within the outer boundary of a region within which heated buffer gas would be continually present during operation of the EUV source if buffer gas were not supplied through the conduit 11.
  • the distance between the outlet 12 of the conduit 11 and the interaction point 13 may be selected by considering the following: the closer the outlet 12 is to the interaction point 13, the more effective the delivery of unheated buffer gas to the region around the interaction point 13. However, the closer the outlet 12 is to the interaction point 13, the more the conduit 11 is likely to suffer from sputtering of ions against the conduit.
  • the outlet 12 may be 15 cm or less from the interaction point, and may be 10 cm or less from the interaction point.
  • the outlet may be 3cm or more from the interaction point.
  • the distance between the interaction point 13 and the collector mirror 3 may be 20cm.
  • the rate at which buffer gas is provided through the outlet 12 may be sufficient to substantially remove heated buffer gas from the region around the interaction point 13. The rate may be sufficient to achieve this before the next laser and material droplet interaction.
  • the rate at which buffer gas should be provided through the outlet 12 in order to achieve this may be calculated based upon the volume of buffer gas that is heated by a laser and material droplet interaction, and the frequency at which laser and material droplet interactions take place (i.e. the frequency of the EUV source).
  • FIG 3 shows a source SO viewed from one side.
  • the majority of elements of the source SO shown in figure 3 correspond with those shown in figure 2 , and are not described again here.
  • the conduit 11 of figure 2 is not present in figure 3 .
  • a conduit 21 passes through the aperture 8 in the collector mirror 3, and travels parallel to the laser beam 7.
  • the conduit 21 is provided with an outlet 22 which is adjacent to the interaction point 13.
  • the conduit 21 is used to introduce buffer gas adjacent to the interaction point 13 in an equivalent manner to that described above in relation to Figure 2 .
  • the conduit 21 is positioned such that, whilst it may obscure some EUV radiation generated by the plasma in the chamber 1, the amount of EUV radiation which is obscured is relatively small (for example, only the cross-section of the conduit obscures the EUV radiation rather than its length).
  • the distance between the outlet 22 and the interaction point 13 may be selected using the criteria that were described further above in relation to figure 2 .
  • An advantage of the embodiment shown in figure 3 is that the flow of buffer gas provided by the conduit is away from the collector mirror 3 rather than towards it (thereby helping to push heated buffer gas away from the collector mirror 3).
  • the conduit may consist of two tubes, one of which is inside the other.
  • the laser beam may be arranged to pass along the inner of the two tubes, and the buffer gas may be arranged to pass along a channel formed between the two tubes.
  • the corner shown in figure 3 may be absent from the inner of the two tubes, in order to allow the laser beam to travel unimpeded from the laser to the interaction point.
  • conduits 11, 21 having different positions and configurations have been shown in figures 2 and 3
  • other conduit positions and configurations may be used. It is preferable that the conduit position and configuration is such that it does not obscure any EUV radiation which would not otherwise be obscured by some other component of the source SO. In some instances, this may not be achievable or it may be preferred to provide the conduit in some location wherein the conduit does indeed obscure some EUV radiation. Where this is the case, it is desirable to minimise the amount of EUV radiation which is obscured by the conduits where possible. Appropriate locations and configurations for the conduit will depend upon the particular arrangement of the source within which the conduit is provided. More than one conduit may be provided (for example the conduits shown in figures 2 and 3 may both be provided in a single EUV source).
  • the invention is not limited to radiation sources which use droplets of material.
  • An embodiment of the invention and may for example generate plasma from a gas rather than from droplets of material.
  • gases include Sn vapor, SnH 4 , or a mixture of Sn vapor and any gas with a small nuclear charge (for example from H 2 up to Ar).
  • Droplets of material or gases may be considered to be examples of a plasma generating substance.
  • the wavelength of the EUV radiation referred to in the above description may for example be within the range of 10-20 nm, for example within the range of 13-14 nm.
  • the invention may also be embodied in a radiation source which generates 'beyond EUV' radiation, that is radiation with a wavelength of less than 10 nm. Beyond EUV radiation may for example have a wavelength of 6.7 nm or 6.8 nm. A radiation source which generates beyond EUV radiation may operate in the same manner as the radiation sources described above.
  • buffer gas is intended to mean buffer gas which is delivered from the outlet 12, 22 after an interaction between the laser beam and the plasma generating substance (and before the next interaction between the laser beam and the plasma generating substance).

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  • Physics & Mathematics (AREA)
  • Optics & Photonics (AREA)
  • Engineering & Computer Science (AREA)
  • Plasma & Fusion (AREA)
  • Exposure And Positioning Against Photoresist Photosensitive Materials (AREA)
  • Exposure Of Semiconductors, Excluding Electron Or Ion Beam Exposure (AREA)
  • X-Ray Techniques (AREA)
  • Plasma Technology (AREA)

Claims (16)

  1. Une source de rayonnement (SO) comprenant une chambre (1) et une amenée (4) d'une substance génératrice de plasma, la source ayant un point d'interaction (13) auquel la substance génératrice de plasma introduite dans la chambre peut interagir avec un faisceau laser (7) et produire par là même un plasma émetteur de rayonnement, la source comprenant en outre un miroir collecteur (3) configuré pour collecter le rayonnement émis par le plasma et concentrer le rayonnement sur un point focal (FP), le miroir collecteur comportant une ouverture (8) par laquelle le faisceau laser peut passer dans la chambre, et la source comprenant en outre une décharge de faisceau (9) sur laquelle le faisceau laser peut être incident, la source comprenant en outre une conduite (11) arrangée pour délivrer un gaz tampon dans la chambre, la conduite présentant une sortie (12) qui est adjacente au point d'interaction, la sortie de conduite étant située entre l'ouverture de miroir collecteur et la décharge de faisceau de telle sorte que la sortie de conduite soit cachée par rapport au système optique de la source de rayonnement et ne cause par conséquent pas d'occultation du rayonnement collecté et concentré sur le point focal par le miroir collecteur.
  2. La source de la revendication 1, dans laquelle la sortie (12) est située à l'intérieur de la limite externe d'une région au sein de laquelle du gaz tampon chauffé serait continuellement présent durant le fonctionnement de la source si le gaz tampon n'était pas amené par la conduite.
  3. La source de la revendication 1 ou de la revendication 2, dans laquelle la sortie (12) de la conduite (11) se trouve à 15 cm ou moins du point d'interaction (13).
  4. La source de la revendication 3, dans laquelle la sortie (12) de la conduite (11) se trouve à 10 cm ou moins du point d'interaction (13).
  5. La source de n'importe quelle revendication précédente, dans laquelle la sortie (12) de la conduite (11) se trouve à 3 cm ou plus du point d'interaction (13).
  6. La source de n'importe quelle revendication précédente, dans laquelle la conduite (11) est située de telle sorte qu'elle n'éclipse pas un rayonnement qu'aucun autre composant de la source n'éclipserait autrement.
  7. La source de n'importe quelle revendication précédente, dans laquelle au moins une partie de la conduite (11) longe un refroidisseur de gaz (10) de la source.
  8. La source de n'importe lesquelles des revendications 1 à 6, dans laquelle au moins une partie de la conduite (11) passe par l'ouverture (8) dans le miroir collecteur (3) de la source.
  9. La source de la revendication 8, dans laquelle au moins une partie de la conduite (11) comprend deux tubes, l'un se trouvant à l'intérieur de l'autre, le tube interne étant arrangé de telle sorte que le faisceau laser puisse passer le long de celui-ci, et un canal entre les deux tubes étant arrangé pour permettre au gaz tampon de passer le long de celui-ci.
  10. La source de n'importe quelle revendication précédente, dans laquelle la sortie (12) de la conduite (11) est plus près du point d'interaction (13) que l'amenée (4) de substance génératrice de plasma.
  11. Une méthode de génération de rayonnement comprenant le fait d'introduire une substance génératrice de plasma dans une chambre (1), de diriger un faisceau laser (7) sur celle-ci afin de produire un plasma émetteur de rayonnement, et d'utiliser un miroir collecteur (3) afin de collecter le rayonnement émis par le plasma et de concentrer le rayonnement sur un point focal (FP), dans laquelle le faisceau laser est dirigé à travers une ouverture (8) dans le miroir collecteur et est incident sur une décharge de faisceau (9), la méthode comprenant en outre le fait d'utiliser une conduite (11) ayant une sortie (12) pour introduire du gaz tampon dans la chambre à un emplacement qui est adjacent à un point auquel le faisceau laser et la substance génératrice de plasma (13) interagissent, la sortie de conduite étant située entre l'ouverture de miroir collecteur et la décharge de faisceau de telle sorte que la sortie de conduite soit cachée par rapport au système optique de la source de rayonnement et ne cause par conséquent pas d'occultation du rayonnement collecté et concentré sur le point focal par le miroir collecteur.
  12. La méthode de la revendication 11, dans laquelle l'emplacement auquel le gaz tampon est introduit se trouve à l'intérieur de la limite externe d'une région au sein de laquelle du gaz tampon chauffé serait continuellement présent durant le fonctionnement de la source si le gaz tampon n'était pas amené par la conduite (11).
  13. La méthode de la revendication 11 ou de la revendication 12, dans laquelle le gaz tampon est introduit à une vitesse de 100 m/s ou plus.
  14. La méthode de n'importe lesquelles des revendications 11 à 13, dans laquelle le gaz tampon est introduit à une vitesse de 2 000 m/s ou moins.
  15. La méthode de n'importe lesquelles des revendications 11 à 14, dans laquelle le débit auquel le gaz tampon est introduit est suffisant pour retirer substantiellement du gaz tampon chauffé d'une région autour du point d'interaction (13) préalablement à une interaction subséquente entre le faisceau laser (7) et la substance génératrice de plasma.
  16. Un appareil lithographique comprenant :
    - une source de rayonnement (SO) ;
    - un système d'illumination (IL) destiné à conditionner le rayonnement ;
    - une structure formant support (MT) destinée à supporter un dispositif pour conformer selon un motif (MA), le dispositif pour conformer selon un motif servant à conférer au faisceau de rayonnement un motif dans sa coupe transversale ;
    - une table porte-substrat (WT) destinée à porter un substrat (W) ; et
    - un système de projection (PS) destiné à projeter le faisceau de rayonnement à motif sur une portion cible du substrat ;
    dans lequel la source de rayonnement comprend une chambre (1) et une amenée (4) d'une substance génératrice de plasma, la source ayant un point d'interaction (13) auquel la substance génératrice de plasma introduite dans la chambre peut interagir avec un faisceau laser (7) et produire par là même un plasma émetteur de rayonnement, la source comprenant en outre un miroir collecteur (3) configuré pour collecter le rayonnement émis par le plasma et concentrer le rayonnement sur un point focal (FP), le miroir collecteur comportant une ouverture (8) par laquelle le faisceau laser peut passer dans la chambre, et la source comprenant en outre une décharge de faisceau (9) sur laquelle le faisceau laser peut être incident, la source comprenant en outre une conduite (11) arrangée pour délivrer un gaz tampon dans la chambre, la conduite présentant une sortie (12) qui est adjacente au point d'interaction, la sortie de conduite étant située entre l'ouverture de miroir collecteur et la décharge de faisceau de telle sorte que la sortie de conduite soit cachée par rapport au système optique de la source de rayonnement et ne cause par conséquent pas d'occultation du rayonnement collecté et concentré sur le point focal par le miroir collecteur.
EP08806915A 2007-08-23 2008-08-20 Source de rayonnement Active EP2191698B1 (fr)

Applications Claiming Priority (3)

Application Number Priority Date Filing Date Title
US93564307P 2007-08-23 2007-08-23
US12/078,663 US7763871B2 (en) 2008-04-02 2008-04-02 Radiation source
PCT/IB2008/002201 WO2009024860A2 (fr) 2007-08-23 2008-08-20 Source de rayonnement

Publications (2)

Publication Number Publication Date
EP2191698A2 EP2191698A2 (fr) 2010-06-02
EP2191698B1 true EP2191698B1 (fr) 2012-10-03

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KR (1) KR101528581B1 (fr)
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TW (1) TWI448828B (fr)
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KR20100049607A (ko) 2010-05-12
EP2191698A2 (fr) 2010-06-02
CN101785368B (zh) 2013-01-02
WO2009024860A3 (fr) 2009-04-16
NL1035863A1 (nl) 2009-02-24
CN101785368A (zh) 2010-07-21
KR101528581B1 (ko) 2015-06-12
JP5659015B2 (ja) 2015-01-28
JP2010537377A (ja) 2010-12-02
NL1035846A1 (nl) 2009-02-24
WO2009024860A2 (fr) 2009-02-26
TW200919112A (en) 2009-05-01
TWI448828B (zh) 2014-08-11

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