Source: https://patents.google.com/patent/TW579536B/en
Timestamp: 2020-07-11 08:15:48
Document Index: 397540777

Matched Legal Cases: ['Application No. 196', 'Application No. 199', 'Application No. 100', 'Application No. 09', 'Application No. 20001', 'Application No. 90122060', 'Application No. 10', 'Application No. 0218', 'Application No. 196', 'application No. 6', 'application No. 9', 'application No. 15', 'application No. 17', 'application No. 23']

TW579536B - Examining system for the particle-optical imaging of an object, deflector for charged particles as well as method for the operation of the same - Google Patents
TW579536B
TW579536B TW91113922A TW91113922A TW579536B TW 579536 B TW579536 B TW 579536B TW 91113922 A TW91113922 A TW 91113922A TW 91113922 A TW91113922 A TW 91113922A TW 579536 B TW579536 B TW 579536B
TW91113922A
Zeiss Carl Semiconductor Mfg
2001-07-02 Priority to DE2001131931 priority Critical patent/DE10131931A1/en
2001-12-14 Priority to DE10161526 priority
2002-06-25 Application filed by Zeiss Carl Semiconductor Mfg filed Critical Zeiss Carl Semiconductor Mfg
2004-03-11 Publication of TW579536B publication Critical patent/TW579536B/en
239000002245 particles Substances 0.000 title claims abstract description 50
238000007689 inspection Methods 0.000 claims description 71
An examining system for imaging an object is proposed which is positionable in an object plane, comprising an illumination device (31) for supplying energy to a delimited field of the object (3) such that charged particles emerge from locations of the field, the field being displaceable in the plane of the object (3), a first deflector (23, 24) for providing a variable deflection field for guiding charged particles emerging from locations of a selectable region (7) of the object (3) through a fixed, predetermined beam cross-section (27), and a position-sensitive detector (5) disposed in the beam path such that the charged particles, after having passed through the first deflector (23, 24), impinge on the same, wherein particles emerging from different locations of the region (7) are imaged on different locations of the position-sensitive detector (5) which are allocated to the locations of emergence.
2. Description of the invention (1 Definition of invention. Scope The present invention relates to an inspection system capable of two-dimensionally imaging the structure of an object by using some charged particles like electrons and the like on a receiver such as a camera. There is a special inspection system. In other words, these structures to be inspected may be structures which are usually inspected by electron microscopy, in which the backscattered electrons, secondary electrons, transmitted electrons, or photoelectrons emitted from the object are observed. The invention is not intended to be limited to these types of electrons. In particular, the observation of ions emitted from an object will also be expected. In addition, the invention relates to a required steering state of a beam of charged particles. In other words, this type of steering gear is suitable for the above-mentioned inspection system for inspecting the object. However, the purpose of this steering gear is not intended to be limited to this application example. In addition, the present invention relates to such a steering gear. Methods required for operation. The possible application range of this inspection system is in some methods for manufacturing miniaturized devices, here, especially in identifying such devices during their manufacture and for that. A method for blemishes such as lithography masks used for one purpose. BACKGROUND OF THE INVENTION US Patent No. 5,578,821 discloses an inspection system related to this purpose, in which an electron beam is focused on it. Above a point (pixel) of the object under inspection. Their backscattered electrons, secondary electrons, and transmitted electrons emitted from this object will be recorded by several suitable detectors. In this system, a The deflector is used to displace its focused beam and hit the location on the object. These individual detectors can be 4 (Please read the precautions on the back before filling this page) This paper size applies China National Standard (CNS) A4 specification (210X297 mm) 579536 V. Description of the invention (2: standing at ::: of; position 'and integratedly receive all backscattered electrons and electrons, and transmitted electrons. Such detection The detector is not position sensitive, but if the intensity recorded by the detector is such that the beam allocated to its deflector hits the point on the object, it will be a bit of the structure of the secret piece. Analyze the image. By the operation of its redirector, the beam is continuously turned to different parts of the object (illusion, the measured intensity assigned to these different parts will be recorded, and its Two-dimensional images can be composed of such continuously recorded intensities. This method is extremely time-consuming. US Patent No. 6,097,659 discloses _ a kind of inspection system for this purpose, in which one of the objects is two-dimensional The extended field is irradiated with some primary electrons, and the secondary electrons emitted from the object are imaged on the position-sensitive detector. Different from the system disclosed in US Patent No. 5,578,821 This system will make the pixel sequence made by a redirector unnecessary. More precisely, multiple pixels can be detected at the same time. However, if you want a high-magnification image, its imaging will be detected. The field above the device will be too small to image a larger two-dimensionally extended object at the same time. Therefore, there is a mechanical shift table that is set to shift the object 旎 relative to its irradiation field so that its detector can continuously capture most of the image of the object in time. The latter is gradually shifted to The image of the entire object can finally be obtained by combining most of these images. Once again, this system is extremely time consuming, and even requires a shift meter, the mechanical precision of which is roughly equivalent to the desired resolution of its image. Summary of the present invention The paper size conversion _ home standard (_ A4 size (2 offers 297 public love) (Please read the precautions on the back before filling out this page) Order 579536 A7 B7 "V. Description of the invention (3) Therefore It is an object of the present invention to provide an inspection system that can be used to make an object f. Please read the precautions on the back, and then the imaging of the can and nest pages. It can make some two-dimensionally extended objects comparable. It is quickly imaged. In addition, it is an object of the present invention to provide an inspection system in which the requirements that a mechanical displacement of an object with respect to the inspection system should satisfy can be reduced. Provided is an inspection system that can be used to image an object that can be displaced in the object plane. The inspection system 'includes a position-sensitive detector on which the object can be imaged into the two-dimensionally extended field. The charged particles that are emitted ..., a bite, and in addition, there is a -the first redirector, which is set to generate a variable turning magnetic field, so that it can image the area above the valence detector by these charged particles, which can in The object is shifted in the plane of the object. Fee This first deflector is used to guide the charged particles that enter the first deflection set from different directions according to the displacement of the area in the object plane. Through a substantially fixed predetermined beam cross-section. Here, its particle beam is detected independently of the position of its imaging area in the plane of the object, without ever pointing to the same section of its detector. Area. The projection position of the imaging area above this detection area will not be shifted when the area imaged above its detector is shifted. In particular, its particle beam can be independent of the area. Position, and can always be roughly in the same two directions, for example, parallel to an optical axis, passing through the fixed cross-section described above. The effect of passing through this is independent of the displacement of the imaging area in the plane of the object. The size of this paper is turned over (CNS) A Na (210X297 mm) 579536 A7 -------- B7____ 5. Description of the invention (4) After the beam cross section, these charged particles may pass through an optical system, To increase its image magnification, and After hitting its position-sensing detector. Due to the displaceability of the imaging of the area in the plane of the above object on its detector, it will be possible to image the structure of some fairly large objects in two dimensions, and It is not necessary to move the object mechanically relative to the inspection system. The inspection system further includes an irradiation system that can supply energy to the object so that charged particles can be ejected from some parts of the object, such ejection The particles are then supplied to their detector to obtain an image of the object. The above energy can be supplied to the object in the form of charged particles, especially electrons, or in the form of electromagnetic radiation (light waves). Therefore, This illumination system therefore includes a light source like laser, or a particle source, especially a plutonium electron source. The particles' emitted from the object as a result of this energy supply are preferably photoelectrons or backscattered electrons , Secondary electrons, or transmitted electrons. The inspection system further includes a controller that can control its first deflector 'so that the area where the object is imaged on the detector is changed. The controller is set to further control its irradiation system so that The limited field of energy in the object is shifted along with the area 'imaged above the detector in the plane of the object. The irradiated area should preferably be substantially coincident with the area it is imaging on the detector. So 'it's not the whole thing that is energized. More specifically, only one of its areas is energized so that the thermal stress to which the object is subjected can be kept to a minimum. As a result, the reduction in particle flow rate will increase the size of this paper) &quot;-: (Please read the notes on the back before filling out this page). Order | V. Invention Description (5) was achieved. So that, for example, their space charge effects can be reduced. The right 4th irradiated field coincides with its imaging area, and the thermal stress of the object will not be higher than what it absolutely needs to produce an image of the object. * Between the object and its beam path, where the charged particles extending towards the detector pass through the fixed beam cross section, it is best to set a first lens that has a focusing lens effect on the particles emitted by the object Focusing lens device. In order to obtain a sufficient magnification of its image, the focusing lens device must be positioned relatively close to the object. In addition, if the system used, 'first suspected rotation symmetrical magnetic lens', its boring diameter must be selected to be quite small, to avoid aberrations, so that when a circle with a small boring diameter is known, it is placed close When the object is, the area imaged on the detector and the flat towel of the object cannot be shifted. Because the imaging of their large-area objects is intended not to be mechanically moved relative to the inspection system, their lens devices are preferably used as the first focusing lens here. Magnetic lenses because they can be used in other components of this inspection system, such as another optical magnification system in front of its detector. A preferred possible embodiment of such a first focusing lens device which can provide its focusing and steering magnetic field over a considerable area covering its beam direction is disclosed in German Patent Application No. 196 34 456 A1, The entire disclosure of this document is incorporated into this specification by reference. This condensing ... transparency display system includes a cylindrical lens and a quadrupole lens positioned relative to the cylindrical lens. The axis of its cylindrical lens extends across its beam direction, and its beam is focused in a direction transverse to its circle 579536 A7-B7 V. Description of the invention (6) In the direction of the axis of the cylindrical lens . The main axis of its quadrupole lens is roughly coincident with the axis of its cylindrical lens, and the magnetic% of its cylindrical lens, and the magnetic field of its quadrupole lens will cooperate to generate charged particles that pass through this lens. Focus effect. Yet another preferred embodiment of the above-mentioned first focusing lens device is described in German Patent Application No. 199 44 857 A1. The entire disclosure of this document is the inner valley, which is incorporated into this specification by reference. The focusing lens device disclosed therein also includes a cylindrical lens whose axis extends across its beam direction. The steering magnetic field provided by this cylindrical lens also overlaps the magnetic field of a quadrupole lens, however, the latter is not static but can be shifted in the direction of its cylindrical lens. To this end, the lens arrangement includes a plurality of electrodes that are paired in pairs along the axis of the cylinder. Their voltages allow selective application of these electrodes so that they can provide an electric field with quadrupole symmetry at a selectable location along the axis of their cylinder. When using this first focusing lens device, its controller can be arranged to further arrange the part of the quadrupole electric field currently generated so as to be positioned above the detector corresponding to which it is turned in the plane of the object. Around the center of the charged particle beam emitted from the imaged area. Further, the first focusing lens means is preferably a lens provided as a variable axis. Such lenses are described on pages 255 to following of the paper "MOL" ("Mobile Objectives") by E. Got et al. Optic 48 (1977), or in US Patent No. No. 4,376,249. This is a preferred embodiment of the first focusing lens device which is a magnetically variable axis lens. It explains that in our applicant's related application, the paper size applies to the Chinese National Standard (CNS) A4 specification (210X297 mm). ) 9 (Please read the notes on the back before constructing this page j.WI., ^ 579536. V. Description of the invention (Subscription of German Patent Application No. 100 44 199.8, and the corresponding US Patent Application No. 09/949 No. 193, Japanese Patent Application No. 20001-272363, Taiwan Patent Application No. 90122060, and Korean Patent Application No. 10-2001-0054790, these documents are also referred to by reference. Incorporated into this description. The focusing lens device includes a magnetic lens that generates a rotationally symmetric steering magnetic field, and additionally includes a magnetic lens that is arranged in its rotationally symmetric steering magnetic field to produce an adjustable size there. The coil configuration of the dipole magnetic field. The rotationally symmetrical steering magnetic field and the direction of the above magnetic field are oriented in a direction that crosses the axis of the symmetrical magnetic field and the dipole magnetic field of its beam direction. The rotating symmetrical magnetic field, however, its axis of symmetry is shifted relative to the axis of symmetry of its static lens according to the intensity of this dipole magnetic field. The intensity of this dipole magnetic field, and therefore the focus lens device described above, The displacement of the effective optical axis is also subject to the above-mentioned controller: the whole circle, so that the displacement of its axis is the displacement of the object area in the plane of the object and the object imaged on the detector. The position is controlled by b. 70 It is best to control the optical axis of the focusing lens magnetic field provided by the first focusing lens device so that it intersects the area imaged on the sensor, especially in the center. The configuration of this inspection system 'is preferably such that the backscattered electrons, or secondary electrons, or transmitted electrons, or electrons emitted by the object are imaged on the corresponding so-called detector. The photoelectron can be imaged on its detector, and its illumination system, therefore, includes a photon source that can illuminate the field in the plane of the object. The photon paper size is applicable to Chinese national standards (CNS> A4) Specifications (210X297 public love) 10 579536 A7 ___B7__ I. 5. Description of the invention (8) &quot; ~ The source and the emitted photons are best guided to a -removable redirector, which causes these photons to be reflected to the Above the object. The movement of this steering device H 爿 the control of the above-mentioned controller, so as to change the orientation of this steering device to obtain the turning of the irradiation field in the object plane. / Check their transmission electron imaging in its detection Above the device, the inspection system includes-an electron source and-a small hole, so that the electrons emitted by this electron source can form a beam that illuminates the field of the object plane. In addition, a second turn H It can be arranged so that its electron beam is turned transversely to its beam direction, and thus the displacement of the irradiation field in the plane of the object is achieved. The # 第 -Director and Detector ’In this case, it is arranged on the side of the object opposite to the plane of the object—above the side, to measure the transmitted electrons across the object. In order to detect the backscattering and secondary electrons respectively, the electron sources and detectors are arranged on the same side of the object relative to the plane of the object ©. Preferably, the first deflector is not only used to displace the area of the object + plane that is imaged on the money detector by emitting electrons, but also to displace the electron source in the plane of the object The field irradiated by the emitted electrons ° its first deflector 'is thus crossed by its electron beam extending from the electron source to the object in one direction and by its extending from the object to the detection in the other direction The electron beam of the detector passes through. Generally, the kinetic energy of the electrons that it transports from the source to the object is higher than the kinetic energy of the electrons that it runs from the object to the detector. The steering device is set up so that it provides roughly the same steering angle to the electrons running in both directions. Such a steering gear constitutes a second feature of the present invention. __________ This paper is suitable for financial standards (_ A4 size ⑽ X297n ——-(Please read the notes on the back before filling out this page) • Order 丨; Threat 丨 579536 5. Description of the invention (9 Based on this project, the present invention A steering device is provided, which can generate a -steering electric field and a -steering magnetic field in the body needle. The direction of these electrons and the direction of the electric and magnetic fields are paired with respect to each other. Orthogonal and oriented. For example, its turning electric field can be provided by 'and its turning magnetic field' can be provided by the current conductor winding configuration f. In this case, according to the present invention, a -controller is provided therein They can adjust the current flowing through their current conductor winding configuration and the voltage they apply to their electrode configuration so that they run from the electron source to the object's electrons, and from the object to the tester's electrons, generally Move on the same or similar trajectory. According to another feature of the present invention, in order to make these electrons moving in the opposite direction passing through its steering gear to obtain accurate steering, its steering gear is set on the system It consists of sleeve-to-phase interphase rings made of most materials with high magnetic permeability, and each of the current conductor windings is wound around at least one ring. The above materials with high magnetic permeability, System_A kind of material whose permeability coefficient is much higher than vacuum. To avoid eddy current, this material is preferably non-conductive or an electrical insulator. An example of such a material is a ceramic ferromagnet. Η its electrode configuration The electrodes are preferably arranged radially inside the ring bodies and the current conductor windings surrounding them. According to a preferred embodiment, when the charged particles are guided in a vacuum, the current conductor windings are The configuration is set to correspond to the outside of the vacuum case, and the electrode configuration is arranged radially inside the vacuum case. In order to change the steering angle supplied to these electrodes by its deflector, this paper size applies to China National Standard (CNS) A4 specification (210X297 mm) (Please read the notes on the back before filling out this page) • Order · 12 579536 A7 _______B7 _ _ V. Description of the invention (11) Figure 12 is based on the invention Of A schematic diagram of an embodiment of the inspection system, where backscattered electrons are observed; FIG. 13 is a schematic diagram of a variation of the embodiment shown in FIG. 12; FIG. 14 is another inspection according to the present invention A schematic diagram of an embodiment of the system, in which transmission electrons are observed; FIG. 15 is a schematic diagram of a variation of the inspection system shown in FIG. 14; and FIG. 16 is another inspection system according to the present invention The schematic diagram of the embodiment, in which the photoelectron is observed. Detailed description of the preferred embodiment FIG. 1 is a schematic diagram of the first embodiment of the inspection system 1 according to the present invention. The inspection system 1, for example, It is used to image a structure similar to objects such as semiconductor wafers 3, or other miniaturized structures such as lithographic photomasks, or a biological sample. The structure of the object 3 is inspected so that the secondary electrons emitted by the object 3 are imaged on a position-sensitive detector 5. The position-sensitive detector 5 has two-dimensional position sensitivity, including a plurality of image points or pixels arranged in a two-dimensional matrix. Each pixel collects information that can be read, and indicates the intensity of an electron impinging on the pixel during the exposure period. The detector is preferably a kind of intensity distribution of charged particles that can be integrally impacted over time in a two-dimensional analysis mode in the measurement area. The f-signal detected in this way can be supplied for further processing to—external paper size suitable for financial countries_standards (CNS) (please read the precautions on the back before filling this page) -Order 丨 14 579536 V. Description of the invention (12 ^ Li's as an example and Lu, it can also form _ part of the holding unit that controls the entire system. In particular, this detector can include-or more CCD chips. Work (please (Read the precautions on the back before filling this page.) Between these objects 3 and controller 5, there are some electro-optical components, which can make a two-dimensional finite rectangular field 7 in the plane of the above object 3 ,,, Imaging on its valence detector 5. This imaging is completed by causing the secondary electrons emitted from different parts of the above-mentioned field 7 to hit different pixels on its detector 5. Therefore, the above object 3 Structures that differ from each other in terms of the intensity of the emitted secondary electrons will be represented graphically. In the first figure, two secondary electrons are emitted at different angles from a certain part of the above-mentioned field 7. The holding lines 9, 10 are represented by symbols. The secondary electrons emitted from kinetic energy around eV to 5 eV will first be accelerated to a kinetic energy of about 20 keV. This acceleration acts on the completion by means of a supply provided to the above-mentioned object 3 and a device arranged in front of this object. The electric field between the electrodes 13. After being accelerated, these electrons will pass through a focusing lens pair consisting of a focusing lens 5 and a focusing lens 17 located farther away from the object. Its electrode 13 can be matched with the above-mentioned focusing lens 15 next to the object, and the first focusing unit 'and its second focusing unit which can define its counterpart together are defined by the above-mentioned distant focusing lens! 7 These first and second focusing units together can produce an effect on the secondary electrons relative to the telescope doublet lens. After the electrons have passed through the pair, the electrons hit their detection Before the detector 5, the other optical magnification system 19, which is composed of one or more particle optical lenses and other components, may perform its image magnification function.
L 15 This paper size applies the Chinese national standard (O ^ g) A4 specification (21 × 297 mm) 5. Description of the invention (l3) These focusing lenses 15, 17 and 5 are used for checking 19 and the detection electron optical imaging are performed on the detection main axis 21, and in the field 7 which traverses this h 7 can be shifted relative to the X · direction that it crosses over the main axis 21. For this purpose, the focusing lenses 15 and 23, 24 are used. ^ The picture shows :: a situation in which there are two steering, Schotting fields in which the image on the detector 5 is shifted from the main axis 21 to the distance M. In the above-mentioned focusing lens 布置 arranged immediately adjacent to the object 3, the lines of these electrons extend parallel to the z axis or the main axis 21. It is arranged closer to the deflector 24 of the object, which can turn these trajectories to a corner ", so that the electrons' will extend towards its main axis 21. Then, it is arranged farther away from the deflection of the object 3 Device 23, these steering lines can be turned at an angle of 10 ', so that these electrons will extend towards their z axis again. The above-mentioned field or 7 deflection ratio μ from its main axis 21, so the upper two steering devices 23 , 24, the distance between each other, and the steering angle / 5 provided by these steering gears 23, 24, respectively. In addition, it is provided with a controller 25, which can control the steering gears 23 and 24 to make the above operation The turning angle of the field 7 from the main axis 21 is cold, and thus the deflection rate M can be adjusted. The turning angles of / 5 are adjusted so that the existing ones have passed through and are far away from the object 3 The secondary electrons behind the deflector 23 can pass through a beam cross-section that is positioned relative to the inspection system independently of its deflection rate M. This beam cross-section that is independent of its deflection rate M is in section 1 The figure is indicated with reference number 27 and its main axis 2 1 as the center. It has been adopted by the reference number 27 and is independent of its 16 paper standards. The Chinese paper standard (〇 丨 5) A4 specification (210X297 mm) 579536 A7 B7 5. Description of the invention (M Deflection rate M After the beam money ©, these reciprocations will continue to travel along the beam path, which is also independent of its deflection rate M. In the embodiment shown in the figure, this additionally-extends to its detection The beam of the device is also centered on its main axis 21. However, it is also possible to set up some beam redirectors and other components 'such as energy filters' in the cross section independent of their steering rate. " With its device 5, the above beam is guided away from its main: line 21. In order to extract the secondary electrons from the field 7 of the object 3 imaged on its controller 5, the field 7 is subject to The first electron irradiation._ The original electron beam 29 is formed by-electron grab 31-magnetic lens 33, and-beam forming hole 35. The kinetic energy of the original electrons of this beam 29 is approximately. Ebara electron beam 29 ', extended by a beam combiner 37, as described above The secondary electrons facing the detector 5 overlap. The beam combiner "is arranged in the beam path between the above-mentioned secondary electrons between the focusing lens 17 and another" learning system 19 ", and It is for these secondary electrons to pass straight back and forth. The primary electrons that enter the beam combiner blade at an angle with respect to the main axis 21 will be turned by this beam combiner 37 so that the primary electrons will pass through After passing through the beam coupler 37, it can be directed toward the object 3 along its main axis 2. After having passed through its beam coupler 37, the primary electrons will pass the focusing lenses Π and the above independent The beam cross-section 27 'due to its deflection rate "and then passes through its deflector 23, which can steer them at an angle away from their main axis 21 ^. Then 'these primary electrons will be turned by their steering gear% towards an angle towards their main axis 21, so that they will turn to this ^ national standard (⑽A4 specification-(2i〇x; ^ y ---- V ----- ,, ............ Order ...... Aw ; (Please read the notes on the back before filling this page) 17 579536 A7 B7 V. Description of the invention (IS) (Please read the notes on the back before filling this page) State 23, 24, and finally can be extended parallel to it again The main axis, but it has also been moved a distance M from its main axis 21. The primary electrons will then pass through the focusing lenses 15 and above them in the field? Before the secondary electron, it will be decelerated to a kinetic energy of about 2 keV by the electric field generated by its electrode 13. The above-mentioned kinetic energy used to generate about 2 keV of the secondary electron, as shown here, is an exemplary value The primary electrons can also be decelerated to other energies, for example, 'to an energy in the range of 100ev to 5 keV. And secondary electrons Provide the same displacement M described above across the z-axis or main axis 21. For this purpose, the structure and function of these two diverters 23, 24 are symmetrical with respect to each other, and are exemplified in sections 2 to 4 In the diagram shown in Figure 2, the primary electrons 29 will enter their diverter 23 from the left, and their secondary electrons 9 and 0 will enter their diverter 23 from the right. In the -volume 36, its deflector 23 will generate an electric field through the electrode 38, plus a magnetic field indicated by the reference symbol 40. The directions of these electric and magnetic fields are directional, relative to each other and relative z_ direction After passing through its redirector 23, the direction of the electron movement has an angle point relative to the direction of their movement before entering the redirector. This angle / 3 is used in non-relativity calculations. , Derived from the equation: mV'2 where the paper size is in accordance with China National Fresh (CNS) A4 specification (2 297 mm) 18 579536 A7 —----—____ B7_____ 5. Description of the invention (1) e means basic The amount of charge shows the mass of electrons and the volume of its magnetic field. Εχ line length in the z-direction represents the field strength of
By means its magnetic field strength, and
Vz is the velocity of these electrons in the Z direction. The steering angles 々 and-/ 5 of these primary and secondary electrons are equal to each other when the electric and magnetic field strengths satisfy the following relationship: Β (Εχ) = ψ [ζ2 · Ε (ΕΧ) among them,
Vzl indicates the velocity of the primary electron, and Vz2 indicates the velocity of the secondary electron. The above-mentioned relationships between the electric and magnetic field strengths are approximate in application. If the theory of relativity and the higher order terms are taken into account, the above formula may be biased when the fringe and stray fields of the electric and magnetic fields are taken into account. The relationship selected between the electric and magnetic field strengths in this way enables the primary and secondary electrons to be steered by their redirectors 23 at equal but opposite sign angles, and thus their trajectory phases coincide. »Hai et al. Turned to 023 and 24. Each department includes ceramic ferromagnetic ring body 43 and ceramic ferromagnetic ring body 45 with equal diameters. They are alternately superimposed on each other with their main drawing line 21 as the center. 'This stack is at the end in the z_ direction.
This paper size applies to China National Standard (CNS) A4 specification (210X297 male D (please read the precautions on the back before filling out this page) • 、 may | 19 579536 A7 ___B7_ 5. Description of the invention (17) A ceramic ring body is formed Each ceramic ring body arranged at the end of the stack includes a plurality of through holes distributed in a circle for the current conductor winding 47 to pass through. Each current conductor winding 47 is parallel to its main axis 21 and extend 'and tie around most ceramic ferromagnetic ring bodies 43. The distribution of these current conductor windings 47 in the circumferential direction of the ring body 43 is clearly shown in Figure 4. This situation results from The angle center to 07 has the following values: 01 = 216., 02 = 41 · 6 °, 03 = 47 · 6., 04 = 62.4., 05 = 68.4., 06 = 78.5., And 07 = 84_5 ° These angles are selected in such a way that the magnetic% generated by their current conductor windings 0 is a uniform magnetic field oriented substantially in the y · direction. There are eight partially cylindrical electrodes 38, Isocyclic bodies 43 and 45 are radially distributed in a uniform circle, and some electrode voltages can be applied to them So that they provide a substantially uniform electric field oriented in the 乂 direction in their volume. The beam will be described below, but it can also be turned in the y-direction to illuminate the object. The field steering also makes a slight turn in the y_ direction. Its controller 25 can adjust the voltages applied to the electrodes 38 and the currents flowing through the windings 47 so that the currents generated in its volume 36 The electric field and the magnetic field generated within it can satisfy the above-defined relationship. The focusing lenses 15, which are arranged next to the object, are shown in perspective to show that the surface is not in Figure 5. It includes two planar holes The electrodes 5 丨, are orthogonal to the z-direction in orientation, and are arranged alternately with each other in the z-direction. Each-hole electrode 51, 53 is formed with a slit 55 'extending in the χ-direction. For the passage of these primary and secondary electrons. If there is an electric dust application, the paper size applies the Chinese National Standard (CNS) A4 specification (21〇 &gt; &lt; 297). This page) Order · 20 V. Description of the invention (〗 8) = Such Correction, 53, an electric field will be generated for each of these electrodes: Yizhi Electrical Reading, which is schematically shown in Figure 6a. This electric field can act like the same cylindrical lens, and act on these through electrodes 51 Electrons of 53 and 53. In the z_ direction between the upper electrodes 51 and 53, two rows of finger electrodes 57 extending in the X · direction and parallel to each other are arranged. The primary and secondary electrons will pass through this Two columns. These refer to the entirety of the electrode 57 and define an electrode configuration 'which is hereinafter referred to as the comb electrode 58.-Voltages that can be independently adjusted' can be applied to each of them under control 25 One finger electrode 57 °-its voltage pattern is then applied to these finger electrodes 57 so that the electric field generated by these finger electrodes 57 is approximately quadrupole symmetrical as shown in Figure 6b. By properly controlling the finger electrodes 57, the main axis 59 of the quadrupole magnetic field can be shifted in the χ_ direction by its controller 25. As a result, the overlapping field of the cylindrical lens according to Fig. 6a and the quadrupole magnetic field according to Fig. 2 will act on the electrons passing through its focusing lens 15. The overlapping fields of these electric fields, as shown in the schematic diagram in Fig. 6c, are relative to a circular lens magnetic field with an axis of symmetry 59. This means that its lens 15 acts like the same focusing circular lens on the electrons passing through it. However, the axis of symmetry 59 of its circular lens magnetic field can be shifted in the X-direction by its controller 25. In operation, the “voltage pattern applied by the controller 2 5 to the finger electrodes 5 7” is to shift the symmetrical axis 59 of the above-mentioned circular lens magnetic field away from its main axis 21 so as to detect the imaging with the above-mentioned object 3 The amount M of the center of the field 7 above the measuring device 5. As a result, the effect of the focusing electrons 15 on the secondary electrons emitted from the field 7 is substantially independent of the turning rate M of the field 7 to be illuminated. 579536 V. Description of the invention (19, σ, σ, etc. The aberrations produced by the traditional circular lens magnetic field far away from the circular lens magnetic field symmetry and the beam path extending by the line can be largely eliminated. The lens 15 described in Figs. 5 and 6 can also be used in its 2 different application examples from electron microscopy. They may include any application example, in which a focusing or / and turning effect is generated, which is directed to a In particular, the beam of V electron particles of erbium ions, and the center of the axis of this focusing effect can be shifted beyond its beam direction. This application example also includes the application of lithography procedures, in which the light The structure of the cover is transferred to a light-emitting sensing layer by their charged particles. In addition, some application examples are expected, in which a few sufficient distances from each other in the direction of the slit: locations, which The comb-shaped hole will generate some quadrupole magnetic fields to generate a focusing effect at these four 4-bit positions. This allows these lenses to focus the beams of these charged particles at the same time. In particular, here —In case On the hole electrodes 51 and 53, an equal potential can be applied to make the charged particles have the same kinetic energy in the z-direction before and after passing through the lens. However, it may also make the upper two Electron and 53 are at a different potential so that the charged particles' can be accelerated or decelerated by the lens. In the case of both, these four electrodes' may have -average potential ', that is, except The quadrupole potential provided by them is equal to the potential of the hole electrode 51 or / and the hole electrode 53, or the part refers to the electrode 57, which can provide an average potential, which is different from that of the hole electrodes 51 and 53. The electric potential 'and, in particular, the highest one that is higher than the upper two-hole electrodes 51 and 53' and the lower one that is lower than the upper two-hole electrodes 51. Electricity 53 This paper is in accordance with the Chinese National Standard (CNS) A4 size (21〇 × 297 male sauce ^
........— (Please read the notes on the back before filling out this page) Order · .f 579536 A7 ------------- B7 _ —____ 5. Description of the invention ( 20) In the application example described above with reference to FIG. 1, the lens 15 with the arrangement of the hole electrode and the finger electrode is arranged directly in front of the object 3. Here, in addition to its focusing function, its lens 15 is also expected to be able to perform the acceleration function of the secondary electrons emitted from the object 3 and the deceleration function corresponding to its primary electron. In this case, its lens 15 functions as an immersion lens, and its aperture electrodes 51 and 53 must be at a different potential. In addition, at this point, it is hoped that there is a certain potential difference between the above-mentioned object 3 and the above-mentioned hole electrode 53 facing the object, so that the ejection part of the above-mentioned object 3 has secondary electrons with extremely low kinetic energy. The lens 15 has already been accelerated on its way (drawing out these secondary electrons). However, here, the electric field that accelerates the second electrons that are slowly moving at first is provided by the hole electrode 53 which faces the object and focuses in the y-direction, the cylindrical lens of this hole electrode 53 The effect of the field on the above-mentioned slow-moving electrons is stronger than the effect of the quadrupole field of its finger electrode 57 on the already fast electrons. Therefore, in the operation of the lens 15 shown in the same figure as the same immersion lens, it is perceived by the particle beams passing through this lens as the combined effect of a cylindrical lens field and a quadrupole field of a circular lens, that is, These two games as a whole will be disturbed. Figures 7 and 8 are cross-sectional views schematically showing a variation of the focusing device shown in Figure 5 in consideration of this problem, that is, a more precise circular lens effect can be achieved. The function and structure of the focusing device corresponding to the components of FIG. 5 are designated by the same reference numerals of FIG. 5, however, an additional letter is attached for the difference. The focusing lens 15f shown in FIG. 7 includes two hole electrodes 51f and 53f that are spaced apart from each other along the center direction. In addition, a majority of the electrodes are not shown in FIG. 7. The paper size applies the Chinese National Standard (CNS) A4 specification. (21GX297 public love) * ---- (Please read the notes on the back before filling this page) •, ^ τ— Φ, 579536 V. Description of the invention (21 (Please read the notes on the back before filling this page) The middle finger is composed of a comb lens 58f. Between the hole electrode 53f which is arranged close to the object 靠近 and the object, there is another hole electrode 101. All the electrodes 51f, 58f, 53f, and 101, Each is formed by a centrally arranged elongated opening or slit 55f, and these primary and secondary electrons are respectively passed through it. In the y-direction, that is, across the extending direction of the slits 55f They have a width yi taking 4 mm as an example. In the x direction, that is, in the extending direction of the slits 55f, they have a length taking 50 as an example. In In one embodiment of this dimension, the hole electrode 10 is arranged close to the object 3 € and the object 3f is close to the object 3f. The area of its opening is separated by a distance Zl of 2mm, and it is at a potential of i kv relative to the object 玎. It is close to the hole electrode 53f of the hole electrode 101, and it is separated from the area near the opening by 4 The distance a of mm is at a potential of 15 kv. The comb lens 58f is always separated by a distance of 3 mm Z3 from its hole electrode 53f and at a potential of 20 kV. It refers to the electrode system along The length a extends 3 mm in the direction of the center of the heart. The hole electrode 5 1 f 'arranged away from the object is always separated from its comb electrode 5 8f by a distance of 4 mm z5 and at a potential of 15 kV. The aperture electrodes 51f, 53f, and 101 are each formed of a metal sheet having a thickness of 0.5 mm. In FIG. 9, the curve 103 is in arbitrary coordinates, and the lens 15f is shown The progress of the potential from the object 3f along the z-axis. In addition, FIG. 9 shows the first derivative of the position with respect to its position of the potential curve 103 by the curve 105 and the curve 107 The second derivative relative to its potential curve 103. First, at In a region 109, the potential increases linearly, so that the emitted secondary electrons are uniformly accelerated. The size of the paper is applicable to the Chinese national standard (CNS> A4 specification (210X297 mm) 24 579536 A7 _ B7_ 5. Description of the invention (22) The focal cylindrical lens field is effective in the area lu within the center of its lens 15f, which can be seen in the upward projection of the first derivative of its potential curve 105. However, Between the regions 109 and 1U, the electrode systems provide a region 113 in which the potential curve 103 does not increase violently, and forms a platform. In this region 113, the first derivative of the potential curve 105 shows an upward projection, so that there will be a defocused cylindrical field for the electrons there. This defocused cylindrical lens field is used to reduce the above-mentioned total cylindrical lens effect provided by the comb hole 58f, so that the weight between the total cylindrical lens effect and the quadrupole lens effect can approach a circle. Lens effect. Even in the case where its lens 15f operates as the same immersion lens. In the lens 15f shown in the z-direction in FIG. 7, this favorable field curve is attributed to the interphase electrodes 53 'and 丨. The structure of the focusing lens 15g shown in FIG. 8 is similar to that of the lens shown in FIG. However, in contrast to this, no additional hole electrode is provided near the object. In contrast, a hole electrode 53g that is close to 58g of the comb lens and faces the object 3g in the Z-direction is not formed of a thin metal sheet, but as shown in the wearing view in FIG. 8, it is a 55g opening. A trapezoid with increasing thickness on both sides. In one of the possible configurations of the lens 15g, the sizes' Z, Z2, Z3, Z4, Z5, and yi are the same as the corresponding sizes in FIG. Here, the hole electrode 53g near the object 3g is at a potential of 1 kV ', its comb lens 58g is at an intermediate potential of 20 kV, and the hole electrode 5g away from the object 3g is at At a potential of 15 kV. The hole electrode 53g with the above-mentioned increased thickness and arranged next to the object will provide the two electrodes 101 and 53f of the embodiment shown in Fig. 7. This paper is suitable for financial standards._Home standard (⑽Μ⑽⑽X297 公 爱) 25 (Please read the notes on the back before filling out this page) Order. T 579536 V. Description of the invention (23) Director: For similar defocused cylindrical lens fields. Fig. 10 is a detailed view of the comb hole 58f used in the embodiment of Fig. 7. The finger electrodes 57f are arranged as a plurality of plates side by side in the X-direction, and the adjacent finger electrodes 57f are separated by a plate 105 of some ceramic insulating material 1 and their electrode plates 57f are separated by 1 mm. The thickness is X1, and each of the insulating plates 105 has a thickness of -0.5 mm &amp;. It means that the electrode plate and the insulating plate 105 extend over the height z4 of 4 mm in the 2 • direction. In a direction towel extending toward the opening 55f, the electrode plate 57f thereof is projected into the opening 55f relative to the insulating plate 105 by a distance of 25 mm. Fig. 11 illustrates how different potentials can be applied to the finger electrodes of the embodiment shown in Figs. 7 and 8 for the quadrupole field of their comb holes. In the embodiment of Fig. 11, each finger electrode 57f is assigned a separate driver 109 'to apply a desired voltage to its corresponding finger electrode 57f. These drives 10 and 9 are controlled by a higher-level focusing lens controller 25f, so that in the operation of their lenses 5f, when their circular Cui effect is to be shifted, they are driven 1 0. The voltage pattern generated in 9 is shifted in the X-direction. In particular, by constantly changing the voltage applied to the finger electrode, this shift of the quadrupole field in the X-direction is also often possible. In addition, the displacement can also be completed step by step. Among them, for example, a constant voltage pattern applied to a finger electrode can be switched from one finger electrode group to another finger electrode group. As for the alternative body of the embodiment of the focusing lens 15 described with reference to Figs. 5 to 11, e 'may be a variable axis line lens derived from e. Goto which has been described above. This paper size applies the Chinese National Standard (CNS) A4 specification (210X297 mm). 5. Description of the invention (24) Due to the different kinetic energy and speed of the primary and secondary electrons, as far as the two types of electrons are concerned, It is possible to provide some equivalent steering angle points or steering angles away from the main axis by these steering gears 23, 24. However, due to the different kinetic energy of these electrons, the focusing lens 5 and the focusing lens 17 'will each exhibit different focusing effects and different focal lengths for the two types of electrons'. Here, the focusing lenses 15 and 17 are thus optimized so that they can be related to the focusing effect related to the secondary electrons, so as to obtain the maximum resolution of the optical image whose field 7 is above the device 5 degree. These focusing lenses 15 and 17 are adaptive, so that only the primary electrons irradiating their fields are optimized. However, this system is permissible because it only irradiates its field 7, for example, it does not need to have its holes 35 precisely imaged in the plane of the object 3. The two-dimensional image of the structure of the above-mentioned object 3 by this inspection system can be obtained as follows. The maximum turning rate M of its field miscellaneous axis 21 is limited by the length of the slit 55 in the x_ direction 'and the maximum beam shift that can be obtained by these deflectors: First of all, the deflectors 23, 24 The focus lens 15 is adjusted by its control state so that the field with the largest turning in the direction can be imaged on its detector 5. The detector 5 is twice The electrons will be known to shoot until there is a sufficient contrast image, which can be read out and stored. Then, its turning rate M is reduced to a value corresponding to the extension length of its field 7 in the direction, and its detection The device will get a new image 'It is also stored. This process will be repeated step by step until «Domain 7 is arranged to its maximum turning point in the (+ χ) direction. The receiver' is on the top. Object 3 is by means of a drive not shown in these figures, phase 579536. V. INTRODUCTION (μ here the inspection system 'mechanically moves in the y_ direction corresponding to its field 7 in the y- direction. Extending the distance. The captured Γ image will once again have its corresponding different turn rate Machine 5 plus 1 capture. If the entire seal of the object has been scanned in this way, it will be combined to obtain a two-dimensional image of the structure of the object. X These steering devices 23 , 24 can also be-in addition, can also be a turn = the maximum turn rate in the direction 'is less than the maximum turn rate in its x_ direction', that is, the turn is relatively small in the y direction At the detection rate, a sufficient quality image of the irradiation field 7 can be paid on its detector surface. It is therefore possible to mechanically shift the object 3 in the direction relative to the inspection system and correspond to The object 3 is mechanically shifted relative to the inspection system in the direction of the factory, and along with this moving object "quotes together" its irradiation field. F A plane with a primary flow of 3.2 // A and the plane of the object Under a field of 7 at a mesoscale of 100 / zm X 10 "m, a secondary electron with a flow rate of about ^ // A will be generated. If its camera has a resolution of 1,000 pixels and 1,000 pixels This inspection system will get a resolution of 10011111. If there are about 2000 electrons to strike Above each pixel of its camera, this inspection system will be able to scan the surface of objects of 0.2 cm2 / sec or 720 cm2 / h. In the following, some variations of the invention will be described. They are functionally and structurally equivalent to the first The components of the embodiment illustrated in Figs. 11 to 11 are designated by the same reference numerals as in Figs. 1 to 11, however, for the difference, an additional letter is attached. Fig. 12 is shown in a schematic diagram. The inspection system la is used to image the paper. The paper size is in accordance with the Chinese National Standard (CNS) A4 specification (210X297 mm). 28. Description of the invention (26) Scattered electrons, which are from the field of an object 3a to be inspected Within the range 7a, it is emitted onto the position-sensitive debt detector 5a. As in the above embodiment, the field 7a imaged on the detector 5 can also be turned from a main axis 21a (turning rate M). Because backscattered electrons have a much higher kinetic energy than secondary electrons, a separate electrode to accelerate these backscattered electrons (see electrode 13 in the figure) is not necessarily required. However, if necessary, a corresponding electrode can be set to increase the kinetic energy of the backscattered electrons. After emitting from the surface of the object 3a, first, the backscattered electrons will pass through a focusing lens 15a arranged next to the object, and then pass through two deflectors 24a, 23a. The steering angle is set on the system. The backscattered electrons emitted from the field 7a will pass through a fixed beam cross-section 27a without reducing the deflection rate M of the field 7a. After having passed this fixed beam cross section 27a, the backscattered electrons will pass through another focusing lens 17a and a beam splitter or beam combiner 37a, which is used to reverse these The beams of the scattered electrons overlap with the beams of the original electrons 29a. The latter is shaped by an electronic grab 31a, a focusing lens 33a, and a hole 35a. The flow of its primary electrons is, for example, 10 "A, and its kinetic energy is, for example, 10 keV. After having passed through its beam combiner 37a, these primary electrons will pass through its focusing lens one after another. 17a, two diverters 23a, 24 &amp;, and focus through I ^ 15a. Here, these diverters 23a and 24 &amp; are set again, so that they also provide this to these primary electrons-turn ratio M, so that the area irradiated by the original electrons on the above object 3 can be roughly detected by its detector 579536 A7 -------------- B7 _ V. Field of imaging (27) Phase 7 coincides. (Please read the notes on the back before filling out this page.) Because these backscattered electrons have a relatively wide energy distribution, they are between the beam combiners 37a and another optical amplification system 19a. Therefore, an image maintaining energy filter 67 is provided to select some electrons with a smaller energy spectrum from the backscattered electrons, and they are then amplified by the optical system 19a and imaged on the detector 5a. The energy filter 67 is a magnet 69 including a plurality of segments. And the configuration is such that the geometric imaging of its field 7a on detection 5 will not be disturbed by this filter 67. An example of this kind of energy filter 67 is described in the applicant's European patent Application No. 0218 920 B1. The entire disclosure of this document is incorporated into this description by reference. The structure of the focusing lens 15a arranged next to the object 3a can be the same as the reference 5 to 5 above. The embodiment described in FIG. 11 is the same. However, it is also possible to use the above-mentioned variable axis lens from E. Goto for this purpose. The inspection system 113 depicted in a schematic diagram in FIG. 13 is structurally Is similar to the inspection system shown in Figure 12. It is also used to image the backscattered electrons on a detector 5b. These backscattered electrons are obtained from an object 3b The field 7b shifted in the plane is emitted. However, in contrast to the embodiment shown in FIG. 12, here, the variable turning rate μ of the field 7b to be imaged is not caused by two separate Steering gear to provide. Instead, only one steering Provided by 23b, the function of the second redirector is assumed by a focusing lens 15b arranged next to the object 3b. The structure of the focusing lens 15b suitable for this purpose is disclosed in German Patent Application No. 196 34 456 The size of A1, and it includes an electrical or magnetic cylinder. The paper size applies the Chinese National Standard (CNS) A4 specification (210X297 mm) 30 579536, the invention description (28-shaped lens field, and superimposed with static electrical or magnetic Quadrupole field. The inspection system 丄 c M shown in Figure 14 is used to make their transmission electrons pass through the detector 5c. These transmission electrons are emitted from the field in the plane of the object 3c. The object aperture is a mask used to image a structure 75 on a lithographic wafer in a lithographic process. The field above the detector by transmission electron imaging can be shifted in the plane of the object (turning rate M). In order to shape the beams of the primary electrons 29c used to illuminate the field in the plane of the object to be imaged on its detector 5c, it is provided with an electron pick-up 31c hole 3 5c and a focusing lens 33c. After having passed its focusing lens 33C, its original electron beam will successively pass through these deflectors 23c and 24c, they are in phase with each other, and they can turn the beam equal to the opposite angle of inversion, To cause its turn rate M. The primary electron beams 29c are thus focused by the focusing lens 15c on the object 3C so as to be illuminated. The field to be imaged. The focusing lens 15c is a lens derived from E. and / or having a foul optical axis. For this purpose, it includes a circular lens 77 'which provides a focusing magnetic field that is rotationally symmetrical with respect to a main axis 21c, and some coils 78, 79 which can generate a magnetic dipole field. The current flowing through these dipole pole field coils 78, 79 can be adjusted by its controller 25c so that the overlap of the stationary circular lens magnetic field and the magnetic dipole field can produce a circular lens magnetic field. The effect, its axis of symmetry 59c, is also shifted by an amount M from its main axis 21c. In Figure 14, reference numeral 81 indicates a dynamic focusing coil, which is also controlled by its controller 25e, thereby optimizing the effectiveness of its focusing lens 15c at different steering rates μ
. Sentences 丨 (Please read the notes on the back before filling out this page) 5. Description of the invention (29)
When the field is turned, in order to return the transmitted electrons passing through the object 3c to its main axis 21c or a fixed beam cross section indicated by 27c in FIG. 14, and this beam cross section, Independent of its turn rate M, a beam guide is provided for the transmitted electrons, which includes components that are structurally symmetrical to this beam guide assembly and can turn the original electrons. These components for guiding the beam of transmitted electrons are designated by the same reference numerals as those corresponding components for guiding the beam of primary electrons, but are appended with an additional '. The beam guide therefore includes a variable axis focusing lens 15c, and two deflectors 24c, and 23c, which are arranged immediately adjacent to the object. It turns downstream of the independent beam cross-section 27c, and in its beam path 'before the transmitted electrons impinge on its detector 5C, there is another optical magnification system with two circular lenses 83, 84. 19c. From the transmission electron beam path shown in Figure 14, it can be seen how an object size 85 can be imaged as an image 88 above its detector 5c via the intermediate images 86, 97. For other types of focusing lenses 15c and 15c 'which are arranged next to the object 3a and have variable axes, one or both of these lenses may be substituted as described above with reference to 5 to The lens depicted in Figure 13. Fig. 15 is a schematic diagram showing an inspection system Id similar in structure to that shown in Fig. 14. It is used to image a% field arranged in the object plane 3d above a detector 5 d, and the field field can be shifted relative to a main axis 21 d. In contrast to the above-mentioned 579536 A7 B7 set in the embodiment according to FIG. 14 V. Description of the invention (30 two separate deflectors so that an original beam 29d is off the turning rate of its main axis 2ld, here It is only provided with a separate redirector 23d, and its second redirector function is provided by a focusing lens 15d arranged next to the object 3d. As for its component, it is a transmission electron that returns to its main axis 2 丨 d Or make the beam path set towards its beam cross-section 27d independent of its turn rate μ, symmetrical to the beam navigation associated with the original electrons, and the components set for this purpose corresponding to The reference number is used to indicate it, but an additional 'is attached. The inspection system shown in the diagram in Figure 16e is used to image the photoelectrons on a detector 5e. These photoelectrons are to be The two-dimensional finite field on the surface of the inspection object 3e is projected. The field 7e 'to be imaged can be turned relative to a main axis 21e and a fixed beam cross-section 27e, respectively. This is used to Guide the photoelectron emitted by its object 3e The electron optical system toward its detector 5e is structurally similar to the system related to backscattered electrons used to guide to its detector as described above with reference to the embodiment shown in Figure 7. However, It is provided with an electrode [3e] to accelerate the photoelectrons emitted from its object 3e. Its turn rate M is caused by two deflectors 23e and 24e, which are in the direction of the main axis 21a of each other Arranged alternately, and a focusing lens 15e arranged next to the object, is a lens with a variable axis, and includes dipole coils 78e and 79e, plus some dynamics that are controlled based on its turn rate μ Focusing coil 77e. In addition, it is provided with an image maintaining energy filter 67e, so as to limit the energy spectrum of the photoelectrons supplied to another optical magnification system 19e. This energy applies to the Chinese National Standard (OK) A4 specification on this paper scale 210 father 297 male Chu) (please read the notes on the back before filling this page) -Order — _ 费 _ 33 V. Description of the invention (3 丨) The filter 67e is a magnet including several sections, such photoelectrons The energy filter and wave filter 67e are turned by the segment magnets 69e that they entered first, and leave their main axis 21e. They need to generate photoelectrons by photons to illuminate the imaging field 7e. The light source 91 is used to complete, and it can generate a beam 93 directed to a turning mirror 95 arranged on its main axis 21e. The turning mirror% is a beam of their optoelectronics arranged on its main axis 21e. It has been steered away from its average axis 21e by its first segment magnet 69e. The steering mirror 95 is pivoted by a driver 97 controlled by its controller 25e. Its controller 25e The movement of the steering mirror% can be controlled based on the turning rate M of its field imaged on its detector 5e, so that its imaged field 7e can always be illuminated by the photons of its light source 91. The area from the 3e plane of the object to the area where the photon is irradiated, as far as its geometric structure is concerned, corresponds generally to the field 7e which is imaged electro-optically on its detector 5e. As for the other body that is a variable axis lens relative to the configuration of the focusing lens 15e disposed next to the object 3e, it is also possible to use the lens of the focusing lens 15e described above with reference to FIGS. 5 to 11. In addition, in order to cause steering, it may not be provided with two separate steering gears 23e and 24e, but only a single steering gear, and, as reflected in the embodiment described above with reference to FIG. 8 By its focusing lens 15d, it provides the function of its second redirector. In the above-described embodiments, the secondary electrons and the reverse electrons are used to image the detector on its detector. The original steering gear is the original: and its secondary or backscattered electrons. Through. This requires extremely strict requirements on its steering system, because it is necessary to impose substantially the same steering rate-its primary electrons and its secondary or backscattered electrons. However, in the embodiment where the transmission electrons and photoelectrons are imaged on the picker, the requirements on the steering device are not high, because only the electrons that run from the object to the detector must be Turned in a defined way. In this case, it is also possible that some can only provide a variable electric field or a variable magnetic field director. In the above-mentioned embodiment operating by optoelectronics, an actuating mirror is used to shift the field to which the photon is illuminated in its object plane. For other types of bodies, other measures can also be used to variably shift these photons. -An example related to this is-acousto-optic modulator. With reference to Figs. 5 to 11, an embodiment of the first focusing lens has been described, which is a particle optical focusing device having a -comb hole operation. Regardless of whether the inspection system described above uses this focusing device or not, its modifications can be expected. For example, the hole described above as a simple slit hole in the arrangement of the focusing lens closest to the object is set as a comb hole so that the potential curve of the focusing device can be additionally subjected to this comb shape. The effect of holes, and in addition this effect can be done in a way that can be displaced in the direction of its slit. It is also possible to arrange one or even both of the holes 51 and 53 adjacent to the comb-shaped hole 58 in FIG. 2 as comb-shaped holes. 579536 A7 B7 V. Description of the invention (33) Component number comparison 1 ... inspection system 7b ... field la ... inspection system 7 e ... field 1 b ... inspection system 9, 10 ... wire lc ... inspection system 13 ... electrode Id ... Inspection system 13e ... electrode le ... inspection system 15 ... focus lens 3 ... object 15a ... focus lens 3 a ... object 15b ... focus lens 3 b ... object 15c ... focus lens 3c ... object 15c '... variable axis focus lens 3 d ... object plane 15d ... focusing lens 3 e ... object 15e ... focusing lens 3 f ... object 15f ... focusing lens 3g ... object 15g ... focusing lens 5 ... position sensing detector 17 ... focusing lens 5a ... position sensing detection Detector 17a ... Focus lens 5b ... Detector 19 ... Optical magnification system 5c ... Detector 19a ... Optical magnification system 5cl ... Detector 19c ... Optical magnification system 5e ... Detector 19e ... Optical magnification System 7… Two-dimensional finite rectangular field 2 · Main axis 7a… Field 21a… Main axis (please read the precautions on the back before filling this page) This paper size is applicable to China National Standard (CNS) A4 specification (210X297 (Centimeters) 36 579536 A7 B7 V. Description of the invention (34) 21 c ... main axis 21 d ... main axis 21 e ... main axis 23, 24 ... steering 23a, 24a ... steering 23b ... steering 23c, 24c ... steering 23cl ... Steering gears 23e, 24e ... Steering gears 24c ', 23c' ... Steering gear 25 ... Controller 25c ... Controller 25e ... Controller 27 ... Beam cross section 27a ... Beam cross section 27c ... Fixed beam cross Cross section 27d ... beam cross section 27e ... fixed beam cross section 29 ... original electron beam 29a ... original electron 29c ... original electron 29d ... original beam 3 1 ... electron gun 31a ... electron grab 3 lc ... electron grab 33 ... Magnetic lens 33a ... Focusing lens 3 3 c ... Focusing lens 35 ... Beam shaping hole 3 5 a ... Hole
3 5 c · · · 37 L 37 ... beam combiner 37a ... beam splitter or beam combiner 38 ... electrode 4 3 ... ceramic ferromagnetic ring body 45 ... ceramic ferromagnetic ring body 47 ... current conductor winding 51,53 ·· hole electrode 51f, 53f ... hole electrode 5 1 g ... hole electrode 53g ·· hole electrode 55 ... slot 55f ... open 55f ... slot 55g ... open 57 ... refer to electrode 57f ... refer to electrode (please (Please read the notes on the back before filling this page) 37 This paper size applies the Chinese National Standard (CNS) A4 specification (210X297 mm) 579536 A7 B7 V. Description of the invention (35) 58 ... comb electrode 58f ... comb lens 58g … Comb lens 5 9… principal axis 59 c… its axis of symmetry 67… energy filter 67 e… image maintenance energy filter 6 9… magnet 6 9 e… segment magnet 75… structure 77… round lens 77 e… dynamic focus coil 78 , 79 ... Coil 78e, 79e ... Dipole coil 81 ... Dynamic focus coil 8 3, 8 4 ... Round lens 8 5 ... Object size 86, 97 ... Intermediate image 88 ... Image 91 ... Light source 93 ... Beam 9 5… Steering mirror 97… Driver 101 ·· Hole electrode 105 ··· Ceramic insulation board (please read the back first Note to fill out this page) This paper scale applicable Chinese National Standard (CNS) A4 size (210X297 mm) 38
6. Application for Patent Scope No. 091113922 Patent Application for Patent Scope Amendment Date of this amendment: October 1992 1. An inspection system that can be shifted in a plane and can be used to image an object (3), which includes : An irradiation device (31; 91), which can supply energy to a limited field of the object (3), so that charged particles can be emitted from some parts of the field, and this field can be in the object (3) Shift in the plane; a first deflector (23,24), which can provide a variable turning field to guide the charged particles emitted from some parts of a selectable area (7) of the object (3) To pass a fixed predetermined beam cross section (27); a position inductive detector (5) arranged in the beam path, which enables such charged particles to pass through the first deflector After (23,24), it can hit it, where the particles emitted from different parts of the area (?) Are imaged on different parts of the position-sensitive detector (5) assigned to the emitted parts Above, and a controller (25), which can control the photo Shooting device (3 丨; 91) to change the displacement of the illuminated field, and to control the diverter (23, 24), so that the area (7) of the object being imaged on the detector is in place The illuminated fields in the object plane are shifted together. 2 · If the scope of patent application is the first! The inspection system of item, wherein the illuminated field is substantially coincident with the area (7) imaged above the detector. 3. The inspection system according to item 1 of the patent application scope, further comprising: a patent-defining scope focusing lens device (15) arranged between the object (3) and the fixed beam cross-section (27), using In order to provide a steering field, the steering field acts like a focusing lens on particles emitted from a portion of the area imaged above the detector (5). For example, the inspection system of claim 3, wherein the turning field is variable, and the controller is further configured to control the first focusing lens device (15) so that an optical axis of the focusing lens (59) Displaceable in a direction transverse to its axis. For example, the inspection system according to item 4 of the patent application, wherein the controller (25) is further configured to control the first focusing lens device (15), so that the optical axis (59) of the focusing lens device, regardless of The displacement of the imaged area (7) intersects the imaged area (7) at substantially the center. For example, the inspection system of claim 3, wherein the first focusing lens device (15) is a particle optical focusing device for providing a turning field with a focusing effect to a charged particle beam, and includes: at least two Each hole is electrically insulated and spaced apart from one another in the direction of a beam (z), each of these holes including an area having a continuous opening through which a free beam can pass; each such opening Extends over a length in a first direction (X) transverse to the beam direction, the length being greater than the openings in a second direction positioned transverse to the first direction and transverse to the beam direction (Y) the width; and at least one of which is arranged between two holes adjacent to each other in the beam direction in position, and is arranged like a comb-shaped, patent-applied hole 'Dang along the first Looking at the direction, the comb-shaped hole includes a plurality of electrodes that are electrically insulated and arranged on each other on each side of the opening. For example, the inspection system of the sixth scope of the patent application, in which a -hole system different from the shaped hole includes ... at least-an electrode region, which in the area of the opening extends over a- Distance, which is 25 times larger than the width of the opening in this area, preferably 0.5 times larger, more preferably 0.75 times larger, and particularly preferably 0.9 or 1.3 times larger. . For example, the inspection system of the patent application No. 6 includes a first hole and a second hole, each of which is different from the comb hole, and the other of them is arranged alternately with each other along the beam direction and is Directly next to each other, each of these second and third holes includes at least one electrode region in the-region of the opening, the electrode regions being arranged at a distance from each other in the beam direction, The distance is 0.5 times larger than the width of the opening located in this area, preferably 0 times larger, and particularly preferably 0.9 times or 1.3 times larger. For example, the inspection system of claim 6 of the patent scope, wherein the particle optical focusing device further includes a steering field controller, Xiao Xiao adds some potential to the electrodes of the comb hole, so that the electrodes produce a A roughly quadrupole magnetic field, the axis of symmetry of the magnetic field extending substantially in the beam direction within the opening. For example, the inspection system of the scope of patent application No. 9, wherein the steering field controller is set to supply the potentials so that the axis of symmetry can be determined. 6. The scope of the patent application is located at several selectable locations. The parts are offset from each other in the first direction. The inspection system of the patent claim No. 10, wherein the axis of symmetry is substantially continuously shiftable along the first direction (x). 12. The inspection system according to item 9 of the patent application scope, wherein the steering field controller is set to adjust the average potential of at least two holes relative to each other. 13. The inspection system according to item 6 of the scope of patent application, wherein the electrode of the comb-shaped hole has a size in the beam direction of about 0.5 to 1.5 times the width of the opening located in the area of the electrodes . 14. The inspection system according to item 6 of the scope of patent application, wherein the -or / and the second or / and the third hole are arranged like comb holes, so that the selective potentials can be determined by The steering field controller supplies the electrodes to the (or) holes. 15. The inspection system according to claim 1, wherein the irradiation device includes a photon source ㈤ that can illuminate the field, and the charged particles emitted from some parts of the imaged area ⑺ include the photon source ( 9 Photoelectron produced by photon of osmium. 16. If the inspection system of patent application No. 15 further includes a redirector (95) with a movable mirror, so that the illuminated field can be moved by the movement of 2 mirrors. 17. The inspection system according to item 3 of the patent application scope, wherein the irradiation device includes an electron source which can irradiate the field, and charged particles emitted from some parts of the imaged area, including charged particles. Secondary electricity VI. Patent application scope or / and backscattered electrons or / and transmitted electrons generated by the electrons of the electron source (31). 18. Such as the inspection system in the scope of patent application No. 17 where the irradiation The device includes at least one hole (35) for shaping an irradiation beam (29) for irradiating the field or / and a numerical hole for adjusting the irradiation. 19. Inspection as described in item π of the scope of patent application system The irradiation device (31c) and the first focusing lens device (15c,) are arranged on the opposite sides of the object plane, and the irradiation device (31c) includes a second deflector (15c) for field displacement. The second redirector is controlled by the controller (25c). 20_ The inspection system according to item 17 of the patent application scope, wherein the irradiation device (31; 31a; 31b) and the first focusing lens device ( 15; ⑸;] is arranged on the same side relative to the plane of the object. 21. The inspection system of item 20 of the patent application, wherein a beam guiding device is provided to guide the radiation source (31 3U; 31b) The electrons emitted pass through the fixed predetermined beam cross-section (27; 27a; 27b) and are directed toward the object ⑺ 'these electrons running toward the object (3) also pass through the first steering device ( 23,24) and the first focusing lens device (M). A The inspection system according to item 21 of the patent application scope, wherein, when passing through the first deflector (23,24), these orientated objects (3) run The electron system has a kinetic energy higher than that of the self-propelled object (3). The sub-owner and the first diverter (23, 24) are set up so that the turning field generated by the subordinates is used for the electrons running toward the object and the objects (3) from this object to Electronic tester (5) 6. Apply for a patent scope for a substantially equal turn rate (M). 23. ^ The inspection system for the scope of patent application item 22, ten of which the first turn benefit includes at least-area (37 ) Has a steering electric field that can be changed by the controller (M) and a steering magnetic field (40) that can be changed by the controller, and the steering electric field and the field of the steering magnetic field in this region (37) The direction and the direction of the electron movement are positioned in pairs so as to be substantially orthogonal to each other. It is considered that the inspection system of the scope of patent application No. 23, wherein the controller ⑽ can control the first steering gear (23, 24), so that in at least one area (37), the following relationship B = k · E is roughly This is consistent, where B is the field strength of the magnetic field in the region (37), E is the field strength of the electric field in the region (37), and K is a constant. 25. According to the inspection system in the scope of patent application, an imaging energy filter (67) for the π electric particles is set between the fixed beam cross section (27) and the detector ( 5) in the beam path. 26 · A redirector capable of redirecting a first beam (29) of charged particles passing through a redirector (23, 24) in a first direction, which has a first The volume (36) of the beam, such a redirector system includes: a current conductor winding arrangement including a plurality of circumferentially distributed along an axis (2) to generate a turning magnetic field within the volume (36) 579536
6. Patented current conductor winding (47); an electrode configuration including a number of electric currents that are circumferentially distributed along the axis (z) to generate a turning electric field (4) in the volume (36) An electrode (38); a control line (25) for adjusting the current to be supplied to the conductor winding (47), and for adjusting the voltage to be supplied to the electrode (38);
Wherein: the redirector (23, 24) is further arranged to turn a second beam (9, 10) of the charged particles passing through the redirector in a second direction, the second direction is opposite to The first direction; and the controller can adjust the current and voltage so that the first beam (29) is steered via an angle (/ 5), the angle (/ 9) is substantially opposite to make the The second beam (9,10) is turned to the angle of passing (_cold). 27. A first beam of charged particles that can pass through the diverter (23,24)
(29) A diverter turned in a first direction, having a volume (36) capable of providing a turning magnetic field to the first beam, this diverter comprises: a current conductor winding arrangement including A number of current conductor windings (47) which are distributed circumferentially along the -axis (z) to generate a -turning magnetic field (40) within the volume (36); an electrode arrangement including a plurality of Electric electrodes (38) that can be distributed within the "xuan volume (36) _ turning electric field (40); 45 579536 6. Patent application scope (25), used to adjust to be supplied to the conductor A motor of the winding () and a voltage for adjusting the voltage to be supplied to the electrode (38); wherein the current conductor winding configuration includes one or more ring bodies (43), which are spaced apart from each other in the axial direction, and Made of a material with 冋 permeability, each current conductor winding ⑷) is coupled around at least one ring body (43).
It is considered that the redirector of the 27th scope of the patent application further includes a mounting system such as a true Erlu family and is arranged radially outward of the vacuum tube, and the electrodes are arranged radially toward the inside of the vacuum tube.
29 ·-A method of operation-a deflector (23, 24), which is crossed by a first charged particle beam (29) and provides an electric field in the volume (36), the direction of this electric field is Positioned generally orthogonal to the direction of the beam, and a magnetic field is provided in the volume (36), the direction of this magnetic field is positioned to be generally orthogonal to the direction of the beam and generally orthogonal to the direction of the electric field This method includes: adjusting the electric and magnetic fields so that one direction of the first beam (29) can have a direction relative to the first beam (29) after it has passed through the redirector (23, 24). A first angle (/ 5) passing in a direction before the deflector (23, 24), and guiding a pair of second charged particle beams (9, 10) standing on the first beam to pass through the The diverter (23, 24), so that the direction of the second beam (9, 10), after having passed the diverter (23, 24), can have the second beam pass through the The first one of the steering gear (23,24) 46 579536 6. The second angle (-/ 3) of the direction of the patent application range, where the electric field and the magnetic field are advanced Adjusted so that the first angle (/ 5) is substantially equal to a line opposite the second angle (- cold). 30. The method of claim 29, wherein the first and second angles are changed by changing the electric and magnetic fields, and the following relationship B (a) = k · Ε (α) is substantially Yes, where: B is the field strength of the magnetic field, E is the field strength of the electric field, α is the first angle, and k is a constant. 31. If the method of applying for item 30 of the patent scope, wherein the following relationship 5⑷ =
Έ {α) is roughly matched, where: Vzl represents the velocity of the electrons of the first beam, and vz2 represents the velocity of the electrons of the second beam.
47 579536
TW91113922A 2001-07-02 2002-06-25 Examining system for the particle-optical imaging of an object, deflector for charged particles as well as method for the operation of the same TW579536B (en)
TW579536B true TW579536B (en) 2004-03-11
TW91113922A TW579536B (en) 2001-07-02 2002-06-25 Examining system for the particle-optical imaging of an object, deflector for charged particles as well as method for the operation of the same
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2002-07-01 JP JP2002192581A patent/JP4476538B2/en active Active
2002-07-02 KR KR1020020037942A patent/KR100920189B1/en active IP Right Grant
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2010-12-21 MM4A Annulment or lapse of patent due to non-payment of fees