Patent Description:
In EUV lithography the position of the EUV producing plasma has to be stable within roughly a few tens of µm to ensure good imaging properties of the scanner. In a EUV radiation generating device like that known from <CIT>, the position of the emission center of the plasma is determined in two directions by the pointing stability of the trigger laser and in the third direction by the position of the electrode surface from which the metal melt is being evaporated by the same laser. However, this last position is not completely fixed in space since the electrode wheel heats up during operation and thus will expand in radial direction. Due to this the EUV hot spot (emission center of plasma) is shifted towards the other electrode. This would not be a problem in case of steady-state operation, as the position would be constant after a short time that is necessary to reach the thermal steady state. However, in a scanner as known from <CIT> the light source is switched on and off on a similar time scale, so that the steady state will hardly be reached and the EUV producing plasma is moving continuously.

<CIT> discloses a method and device for generating EUV radiation with enhanced efficiency using two lasers firing with a small time delay to evaporate the metal melt. The time delay between the two constrictive pulses, which are applied within a time interval of each electrical discharge, is varied in order to achieve a maximum EUV output.

It is an object of the present invention to provide a method and device for generating EUV or soft X-ray radiation by means of electrically operated pulsed discharges, in which the position of the emission center of the plasma is stabilized.

The object is achieved with the method and device according to claims <NUM> and <NUM>. Advantageous embodiments of the method and device are subject of the dependent claims and are furthermore described in the following portions of the description.

In the proposed method the gaseous medium is produced at least partly from a liquid material, which is at least partially evaporated by for example, ion or electron beams and in a preferred embodiment laser beams.

In the proposed method and device not only one single energy beam pulse is applied for each electrode discharge, but at least two consecutive pulses are applied within the time interval of each electrical discharge or current pulse. The time interval starts with the application of the first energy beam pulse initiating the corresponding electrical discharge and ends when the capacitor bank is discharged after the corresponding current pulse. The at least two consecutive pulses can be generated by using two separate energy beam sources, in particular laser sources, which have their own trigger in order to achieve the appropriate timing. It is also possible to use only one single energy beam source, the pulsed energy beam of which is split up into two or more partial beams. The delays between the single pulses are then achieved by different delay lines for the different partial beams. Appropriate beam splitters, in particular for laser beams, for splitting up one beam into several partial beams are known in the art. Preferably the two consecutive pulses are applied with a mutual time delay of less equal <NUM> ns and with a pulse energy ranging from <NUM> mJ to ≤ <NUM> mJ.

Inventors of the present invention discovered that the position of the emission center of the plasma, in particular the distance of this center to the electrode surface, depends on the exact delay between and on the pulse energy of the two consecutive laser pulses. By variation of the time delay and pulse energy of the two laser pulses, the emission center of the plasma can be moved up to several tens of millimeters. Such a movement is enough to compensate for the thermal expansion of the electrodes, in particular of the electrode wheel in one of the embodiments of the device. In the present method and device, therefore, the time delay between the two consecutive pulses and the pulse energy of these pulses are controlled such that the emission center of the plasma is held constant during a time period which covers a multiplicity of the electrical discharges. The term constant in this context means that the position of the emission center preferably does not move over a distance of > <NUM> µm.

This control is performed based on measurements of the position of the emission center of the plasma in real time, resulting in a feedback control based on the monitoring. The control, alternatively, is based on a change in the position of an edge of at least one of the electrodes which can also be monitored. A further alternative is to monitor the electrical power applied to the electrodes for generating the plasma and to control the time delay and energy of the pulses based on the applied electrical power, which is a measure for the dissipated power. The electrical power applied to the electrodes is known from the control of the capacitor bank, i.e. the charging voltage, the capacity of the capacitor bank and the discharge frequency, and can thus be determined without measurement. The last two control mechanisms require the knowledge about the movement of the emission center of the plasma with the applied electrical power or with the movement of the electrode edge, respectively. To this end the dependency of the position of the emission center of the plasma on the time delay and/or pulse energy and on a change in position of said edge of said at least one of said electrodes is measured in advance. In the other case the dependency of the position of the emission center of the plasma on the time delay and pulse energy and on the applied electrical power is measured in advance. The measurement results are stored in order to be available for the control during operation of the device. The measurement results can also be evaluated in advance such that the required time delay and pulse energy for stabilizing the position of the emission center depending on the movement of said edge or on the applied electrical power is stored.

The proposed device thus comprises a means for monitoring a change in the position of the edge of at least one of said electrodes, wherein the control unit has access to the above stored data about the dependency of the position of the emission center on the time delay and pulse energy and on the change in position of said edge of said at least one of said electrodes and is designed to control the time delay and pulse energy based on the monitored change in position and the stored data. Alternatively, the proposed device comprises means for monitoring the electrical power applied for generating the plasma, whereby the control unit has access to the stored data about the dependency of the position of the emission center of the plasma on the time delay and pulse energy and on the applied electrical power and is designed to control the time delay and pulse energy based on the applied electrical power and the stored data.

The proposed method and device are described in the following in connection with the accompanying figures without limiting the scope of the claims. The figures show:.

<FIG> shows a schematic side view of a device for generating EUV radiation or soft x-rays to which the present method can be applied and which may be part of the device of the present invention. The device comprises two electrodes <NUM>, <NUM> arranged in a vacuum chamber. The disc shaped electrodes <NUM>, <NUM> are rotatably mounted, i.e. they are rotated during operation about rotational axis <NUM>. During rotation the electrodes <NUM>, <NUM> partially dip into corresponding containers <NUM>, <NUM>. Each of these containers <NUM>, <NUM> contains a metal melt <NUM>, in the present case liquid tin. The metal melt <NUM> is kept on a temperature of approximately <NUM>, i.e. slightly above the melting point of <NUM> of tin. The metal melt <NUM> in the containers <NUM>, <NUM> is maintained at the above operation temperature by a heating device or a cooling device (not shown in the figure) connected to the containers. During rotation the surface of the electrodes <NUM>, <NUM> is wetted by the liquid metal so that a liquid metal film forms on said electrodes. The layer thickness of the liquid metal on the electrodes <NUM>, <NUM> can be controlled by means of strippers <NUM> typically in the range between <NUM> to <NUM>. The current to the electrodes <NUM>, <NUM> is supplied via the metal melt <NUM>, which is connected to the capacitor bank <NUM> via an insulated feed through <NUM>.

The electrode wheels are advantageously arranged in a vacuum system with a basic vacuum of less than <NUM>-<NUM> hPa. A high voltage can be applied to the electrodes, for example a voltage of between <NUM> to <NUM> kV, without causing any uncontrolled electrical breakdown. This electrical breakdown is started in a controlled manner by an appropriate pulse of a pulsed energy beam, in the present example a laser pulse. The laser pulse <NUM> is focused on one of the electrodes <NUM>, <NUM> at the narrowest point between the two electrodes, as shown in the figure. As a result, part of the metal film on the electrodes <NUM>, <NUM> evaporates and bridges over the electrode gap. This leads to a disruptive discharge at this point accompanied by a very high current from the capacitor bank <NUM>. The current heats the metal vapor to such high temperatures that the latter is ionized and emits the desired EUV radiation in pinch plasma <NUM>.

In order to prevent metal vapor from escaping from the device, a debris mitigation unit <NUM> is arranged in front of the device. In order to avoid the contamination of the housing <NUM> of the device a screen <NUM> may be arranged between the electrodes <NUM>, <NUM> and the housing <NUM>. An additional metal screen <NUM> may be arranged between the electrodes <NUM>, <NUM> allowing the condensed metal to flow back into the two containers <NUM>, <NUM>.

In the proposed method and device, not only one single laser pulse per electrical discharge is used to generate the tin cloud, but at least two consecutive pulses. <FIG> shows an embodiment, in which the two consecutive laser pulses <NUM> with a mutual time delay of approximately <NUM> ns are used to evaporate the tin. In this diagram, the duration of the electrical current pulse <NUM> is also indicated as well as time of emission of the EUV radiation <NUM>. In this example, the time between the first of the two laser pulses <NUM> and the onset of the current <NUM> is around <NUM> ns.

The time delay between the two consecutive pulses <NUM> is controlled in the present method and device in order to hold the position of the emission center of plasma <NUM> constant. To this end, the position of this emission center may be monitored in real time via an appropriate camera and the time delay and pulse energy is then controlled by an active feedback control. Alternatively, the control is based on a determination or measurement of the electrical power applied for generating the plasma or on measurements of a movement of the electrode edge near the plasma. The latter measurement may also be performed with a camera. In both cases, calibration measurements suitably have been performed in advance which show the influence of the measured values on the position of the plasma pinch on the one hand and the time delay and pulse energy needed to stabilize the position of the emission center in such cases. Based on these calibration measurements and the actual monitoring of the corresponding values, the time delay between the consecutive pulses and the pulse energy of the consecutive pulses is varied in order to achieve the stable position of the plasma emission center.

<FIG> shows an example of the influence of the time delay between the two consecutive pulses on the position of the emission center of the plasma <NUM>. In the upper figure the consecutive laser pulses are applied with a time delay of <NUM> ns, wherein in the lower figure the time delay between the pulses is increased to <NUM> ns. This increase in time delay results in a movement of the position of the emission center of the plasma <NUM> about a distance of approximately <NUM>.

Claim 1:
A method of generating EUV or soft X-ray radiation by means of electrically operated pulsed discharges, in which
- a plasma (<NUM>) is ignited in a gaseous medium between at least two electrodes (<NUM>, <NUM>) in a discharge space, said plasma (<NUM>) emitting said radiation (<NUM>) that is to be generated,
- said gaseous medium is produced at least partly from a liquid material (<NUM>), which is applied to one or several surface(s) moving in said discharge space and is at least partially evaporated by one or several pulsed energy beam(s)(<NUM>),
wherein at least one of said electrodes (<NUM>, <NUM>) is set in rotation during operation, said liquid material (<NUM>) being applied to a surface of said at least one of said electrodes (<NUM>, <NUM>), and
- at least two consecutive pulses (<NUM>) of said pulsed energy beam(s)(<NUM>) are applied within a time interval of each electrical discharge onto said surface(s) to evaporate said liquid material (<NUM>),
- wherein a position of an emission center of said plasma (<NUM>) is held constant during a time period covering a multiplicity of said electrical discharges by controlling a time delay between said at least two consecutive pulses (<NUM>) and a pulse energy of said at least two consecutive pulses (<NUM>),
- wherein either the position of said emission center is monitored and said time delay and pulse energy is feedback controlled based on the monitoring, or a change in the position of an edge of at least one of said electrodes (<NUM>, <NUM>) is monitored and said time delay and pulse energy is controlled based on said change in position, or electrical power applied for generating the plasma (<NUM>) is monitored and said time delay and pulse energy is controlled based on the applied electrical power.