Classifications

• • 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
  • H01—ELECTRIC ELEMENTS
  • H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
  • H01J61/00—Gas-discharge or vapour-discharge lamps
  • H01J61/02—Details
  • H01J61/04—Electrodes; Screens; Shields
  • H01J61/06—Main electrodes
  • H01J61/09—Hollow cathodes

Definitions

• the invention relates to a gas discharge lamp for extreme ultraviolet radiation according to the preamble of claim 1.
• Preferred areas of application are those which require extreme ultraviolet (EUN) radiation, preferably in the wavelength range from approximately 10 to 20 nm, for example semiconductor lithography. It is generally known as a dense hot plasma
• WO 01/91532 A2 teaches the use of an EUV radiation source with a plurality of partial electrodes arranged in the form of a segment of a circle, between which ion beams are accelerated.
• the ion beams open into a plasma discharge space and form a dense, hot plasma there, which emits radiation in the EUN wavelength range.
• means are also provided for the electrical neutralization of the ions.
• X-ray radiation is disclosed in WO 01/01736 AI, in which two main electrodes are provided, between which there is a gas-filled intermediate space.
• the main electrodes have one or more openings.
• the configuration of the main electrodes means that the plasma ignites only within the cylinder determined by the diameter of the two central openings and is subsequently compressed to an even smaller cylinder due to the pinch effect. In this respect, only a single plasma channel is formed.
• the invention is based on the technical problem of providing a gas discharge lamp with a pinch plasma emitting in the EUN wavelength range, in which a spatially highly localized one
• a gas discharge lamp for extreme ultraviolet radiation with an anode and a hollow cathode, in which the hollow cathode has at least two openings and the anode has a through opening, and in which the longitudinal axes of the hollow cathode openings have a common intersection S, which lies on the axis of symmetry of the anode opening.
• the invention is based on the finding that cathode erosion can be reduced by distributing the entire electron current emanating from the cathode over several cathode openings.
• the cathode of a gas discharge source has to deliver a very high electron current of several kiloamps during a current pulse. This leads to the formation of so-called cathode spots in the inner surface of the cathode opening and in the immediately adjacent surface area of the cathode facing the anode. The electrons preferentially emerge from these cathode spots. At these locations, however, erosion of the cathode material can go far beyond the purely thermal evaporation. By selecting several hollow cathode openings, the current density occurring at a cathode spot is reduced. Overall, this leads to less erosion of the cathode, in particular in the opening area, and to an improved service life of the gas discharge lamp.
• 1 shows a gas discharge lamp according to the invention with an anode
• Anode 1, cathode 2 and cavity 8 are in a gas atmosphere at pressures of typically 1 to 100 Pa.
• a voltage is applied to the electrode system. Gas pressure and electrode spacing are selected such that the plasma is ignited on the left branch of the Paschen curve, ie the ionization processes start along the long electrical field lines, which is preferred occur in the area of the openings of the anode and cathode.
• the hollow cathode space 8 is not potential-free, rather the potential protrudes or the electrical field lines also protrude into the hollow cathode space 8.
• a hollow cathode plasma is created there with high efficiency of plasma formation due to oscillating electrons.
• FIG. 1 shows an arrangement with planar electrodes 1, 2 which is technically particularly simple to implement.
• An arrangement in the form of a segment of a circle is also possible, for example in FIG. 3 with a hollow cathode 2 in the form of a segment of a circle.
• This arrangement has the advantage that the electrode walls are further away from the plasma, the cooling of the electrodes is easier, and there are also larger angles to the axis of symmetry 6 can be realized.
• the wall 7 opposite the respective cathode opening 3, 3 ', 3 can be perpendicular to the longitudinal axis 5, 5', 5" of this opening, and can thus contribute by ionization in the electrode interspace, preferably in the area of the common Intersection S has a high electrical conductivity.
• the current pulses used advantageously have amplitudes with a two-digit kiloampere number and period durations in the two- to three-digit ⁇ anosecond range.
• the plasma is adequately compressed and heated in that it reaches the temperature required for the radiation emission.
• Xenon is mainly used as the working gas of the discharge source, in pure form or in a mixture with other gases.
• gases with other emitters such as lithium or tin, in elemental form or as a chemical compound, can also be used to ensure the highest possible radiation efficiency.
• the working pressure is in the range of 1-100 Pascal.
• the working point is chosen so that the product of the electrode distance and discharge pressure lies on the left branch of the Paschen curve. In this case, the ignition voltage rises with falling gas pressure with a fixed electrode geometry.
• a plasma 13 is generated in the hollow cathode 2 according to FIG. 2a.
• this plasma 13 passes through the cathode openings and forms conductive channels 11 between the cathode and anode, cf. see Fig. 2b.
• the beam 11 of ions and electrons emerging from the hollow cathode openings has a certain spatial extent.
• the common intersection point S should also be understood to be that spatial area 12 within which these spatially extended beams intersect or overlap.
• a rapid increase in the current occurs along the channels 11, as a result of which the plasma is magnetically compressed to a small volume 14 on the axis of symmetry 6 of the arrangement according to FIG. 2c.
• a cigar-shaped plasma can be realized on and in the direction of the main axis of symmetry 6.
• the length of this plasma region in the axial direction is approximately 2 to 5 mm, and perpendicular to this approximately 0.5 to 2 mm.
• the focus of this plasma area is approximately at the intersection S. Due to the sharp rise in temperature, the gas atoms in it are ionized several times and emit the desired EUV radiation.
• the alignment of the hollow cathode openings to a common one
• Intersection S has the effect that the electron or plasma rays generated in the initial phase of the discharge meet at one point, namely the intersection S, and thus predetermine current channels directed to a spatial point. In the later phase of high current flow, a very localized plasma is formed in this way due to the pinch effect.
• At least two cathode openings are provided; the use of an even larger number of cathode openings is advantageous.
• the use of a larger number of cathode openings increases the electrode area even more and reduces the stress that each individual cathode opening experiences. If desired, this reduces the erosion of the cathode.
• the longitudinal axis 5 of the respective hollow cathode opening 3 is substantially perpendicular to the part of the hollow cathode wall 7 opposite the hollow cathode opening 3, ie the rear wall of the hollow cathode space, see FIG. 3.
• the orientation of the hollow cathode wall 7 is in relation to the longitudinal axis of the hollow cathode opening namely, strong influence on the direction of the electron or plasma beam and on its current intensity when it emerges from the cathode opening.
• electrons are namely emitted from the rear walls 7 of the hollow cathode or the hollow cathodes, in each case perpendicular to the wall.
• a hollow cathode can also be understood to mean a cathode with at least two openings 3, 3 ′ with at least one assigned hollow cathode space 8.
• Hollow cathode 2 has no opening on the axis of symmetry 6, see FIGS. 5a and 5b. If there is an opening at this point, determine experimentally that the current flow from this opening often significantly exceeds the current flows from the other openings 3, 3 '. By not providing an opening at this point, one avoids the risk that this opening is subject to particularly severe erosion. In other words, the distribution of the total current over the individual flows is particularly uniform.
• a variant not shown in the drawing, consists in choosing a continuous hollow cathode opening on the axis of symmetry, the diameter of which is smaller than the diameter of the other hollow cathode openings.
• the central hollow cathode opening that is to say the hollow cathode opening on the (main) axis of symmetry of the electrode arrangement, plays no role in the ignition of the plasma.
• one or more hollow cathode openings 3, 3 ',... are designed as a blind hole, see FIGS. 6a and 6b. This design is particularly easy to manufacture.
• the arrangement more tolerant of erosion in the opening area. Play any rounding or existing removal of the cathode on the edge of the opening in the case of a blind hole for the transport of electricity and thus for the pinch plasma, it is not as important as in a geometry with a continuous opening. In the latter case, the geometry of the pinch plasma is essentially determined by the current approach and its development over time in the opening, experience having shown that the eroded edge has a negative effect on the pinch geometry. The pinch plasma becomes longer and means that less radiation can be coupled out. In this respect, the blind hole means that despite erosion, the plasma remains unchanged in terms of position and geometry.
• the anode 1 contains a continuous central main opening 4 on the axis of symmetry 6.
• the anode 1 can have at least two further openings 4 ', 4 ".
• the plasma volume to be compressed will turn out to be smaller overall. This compresses the plasma to an even smaller volume. This has the advantage that an even higher proportion of the EUV radiation generated can be coupled out along the axis of symmetry 6 and made usable for the application. Since lower pulse energies are required to achieve a specified EUV output power, the erosion of the cathode material can be restricted further.
• the additional anode openings can be designed differently. Viewed from S, behind the anode opening 4 ', 4 "in FIG. 7 there is an open space area, in FIG. 8a this space area is closed.
• the closed design has the consequence that the plasma cannot be disturbed by processes in said space area , and the plasma emission takes place in a particularly trouble-free manner.
• the variant according to FIG. 8b is structurally particularly simple in that the closed spatial area consists of an anode opening 4 ', 4 "designed as a blind hole.
• the main opening 4 can also be designed as a grid, the open areas of which are strip-like or checkerboard-like. In this case, the grid acts as electrical shielding during the ignition phase of the plasma.
• This configuration the central main opening of the anode is mainly at
• trigger devices are provided for the hollow cathode space or spaces. In this way, the Trigger the ignition of the discharge precisely as required, in particular the simultaneity of the ignition of the partial discharges can also be improved.
• an additional electrode 10 can be provided in the cavity 8 as a trigger device.
• This additional electrode 10 can be prevented by igniting the discharge by igniting it at a positive potential with respect to the cathode 2. If the trigger electrode is switched to cathode potential by a control pulse on the trigger electronics, the discharge is ignited in a precisely controllable manner. The same applies in the event that a dielectric trigger is used.
• a pulsed high-frequency source 10, 10 ', 10 can be used as
• Trigger device can be provided, and for example a microwave source can be used to trigger the discharge.
• the radio frequency is injected through the opening in the direction of the dash-dotted axes into the hollow cathode space or spaces 8, 8 ', 8 ", and there triggers the build-up of the hollow cathode plasma and finally the main discharge.
• Glow discharge units can also be provided for triggering according to FIG. 10b.
• a glow discharge is maintained within these units before the main discharge.
• Electrons are then extracted from the glow plasma by applying a positive voltage pulse to the grid electrode facing the hollow cathode 2, which electrons initiate the main discharge in the hollow cathode space 8, 8 ', 8 "and in the space between the anode and cathode, that is to say in the space between the electrodes.
• laser beams 15, 15 ', 15 "of a pulsed laser beam source focused on the respective hollow cathode openings can be used to trigger primary electrons from the cathode surface and to ignite the discharge.
• One or more focused laser beams can be used both from the anode side, see FIG. 10d, and through openings from the cathode side, see FIG. 10c.
• FIG. 11 shows a double plasma arrangement with an auxiliary anode 17.
• the auxiliary anode and anode 1 are electrically connected to one another via lines 19.
• a plasma builds up in the hollow cathode spaces 8, 8 ', 8 ", from which an electron beam propagates in the direction of the anode 1 and also in the direction of the auxiliary anode 17.
• space 18, 18' 18 "between the openings 16, 16 ', 16" and auxiliary anode 17 a plasma which in turn emits an ion beam in the direction of the hollow cathode 2.
• the ion beam crosses the hollow cathode space 8,8', 8 “and passes through the openings 3,3 ', 3 "into the gap between the electrodes.
• Embodiments of cathode, anode (s), respective openings and associated trigger devices can also be combined as desired.

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

Applications Claiming Priority (3)

Publications (1)

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Family Cites Families (17)

• 2002
  • 2002-12-04 DE DE10256663A patent/DE10256663B3/de not_active Expired - Lifetime
• 2003
  • 2003-11-28 JP JP2004556668A patent/JP4594101B2/ja not_active Expired - Lifetime
  • 2003-11-28 CN CNB2003801049941A patent/CN100375219C/zh not_active Expired - Lifetime
  • 2003-11-28 AU AU2003302551A patent/AU2003302551A1/en not_active Abandoned
  • 2003-11-28 US US10/536,918 patent/US7397190B2/en active Active
  • 2003-11-28 EP EP03812235A patent/EP1570507A2/de not_active Withdrawn
  • 2003-11-28 WO PCT/IB2003/005496 patent/WO2004051698A2/de active Application Filing
  • 2003-12-02 TW TW092133834A patent/TW200503045A/zh unknown

Non-Patent Citations (1)

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