WO2018040588A1 - Magnetron element and magnetron sputtering apparatus - Google Patents
Magnetron element and magnetron sputtering apparatus Download PDFInfo
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- WO2018040588A1 WO2018040588A1 PCT/CN2017/081325 CN2017081325W WO2018040588A1 WO 2018040588 A1 WO2018040588 A1 WO 2018040588A1 CN 2017081325 W CN2017081325 W CN 2017081325W WO 2018040588 A1 WO2018040588 A1 WO 2018040588A1
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- target
- magnetron
- closed
- plasma path
- magnetic pole
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- C—CHEMISTRY; METALLURGY
- C23—COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; CHEMICAL SURFACE TREATMENT; DIFFUSION TREATMENT OF METALLIC MATERIAL; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL; INHIBITING CORROSION OF METALLIC MATERIAL OR INCRUSTATION IN GENERAL
- C23C—COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; SURFACE TREATMENT OF METALLIC MATERIAL BY DIFFUSION INTO THE SURFACE, BY CHEMICAL CONVERSION OR SUBSTITUTION; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL
- C23C14/00—Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material
- C23C14/22—Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material characterised by the process of coating
- C23C14/34—Sputtering
- C23C14/35—Sputtering by application of a magnetic field, e.g. magnetron sputtering
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J25/00—Transit-time tubes, e.g. klystrons, travelling-wave tubes, magnetrons
- H01J25/50—Magnetrons, i.e. tubes with a magnet system producing an H-field crossing the E-field
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J37/00—Discharge tubes with provision for introducing objects or material to be exposed to the discharge, e.g. for the purpose of examination or processing thereof
- H01J37/32—Gas-filled discharge tubes
- H01J37/34—Gas-filled discharge tubes operating with cathodic sputtering
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J37/00—Discharge tubes with provision for introducing objects or material to be exposed to the discharge, e.g. for the purpose of examination or processing thereof
- H01J37/32—Gas-filled discharge tubes
- H01J37/34—Gas-filled discharge tubes operating with cathodic sputtering
- H01J37/3402—Gas-filled discharge tubes operating with cathodic sputtering using supplementary magnetic fields
- H01J37/3405—Magnetron sputtering
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J2225/00—Transit-time tubes, e.g. Klystrons, travelling-wave tubes, magnetrons
- H01J2225/50—Magnetrons, i.e. tubes with a magnet system producing an H-field crossing the E-field
Definitions
- the present invention relates to the field of magnetron sputtering technology, and in particular to a magnetron element and a magnetron sputtering device.
- Sputtering refers to the phenomenon in which charged particles (such as argon ions) bombard a solid surface, causing various particles on the surface, such as atoms, molecules or bunches, to escape from the surface of the object.
- a plasma is generated in a chamber, and positive ions of the plasma are attracted by a cathode negative, bombarding a target in the chamber, knocking out atoms of the target, and depositing on the substrate.
- the gas is an inert gas such as argon.
- reactive sputtering a reactive gas is used together with an inert gas.
- Magnetron sputtering equipment is widely used in integrated circuits, liquid crystal displays, thin film solar and LED fields.
- a magnet is used in the vicinity of the target, which can force the electrons in the plasma to move according to a certain orbit, increasing the movement time of the electrons, thereby increasing the chance of electrons colliding with the gas to be ionized, thereby obtaining High density plasma provides high deposition rates.
- the orbit of the electron controlled by the magnet affects the erosion rate of the target at different positions, affecting the life of the target. It also affects the uniformity of deposition of the film.
- the magnetron 6 adopts a kidney-shaped nested structure as in Figure 1a.
- the magnetron 6 is fixedly mounted on the magnetron mounting plate 9, and the magnetron mounting plate 9 is fixed on the driving plate 8.
- the driving plate 8 and the bracket 10 are movably connected by the shaft 14, and the driving plate 8 is rotatable about the shaft 14.
- a spring 5 is also coupled between the bracket 10 and the drive plate 8; the bracket 10 is movably coupled to the drive shaft 4, and the bracket 10 is rotatable about the drive shaft 4.
- the drive shaft 4 is correspondingly located at the center of the target.
- the carrier 10 drives the driving board 8 and the magnetron 6 to rotate around the driving shaft 4, such as: driving The shaft 4 rotates counterclockwise at a certain rotational speed such that the centrifugal force of the magnetron 6 exceeds the spring force of the spring 5 when the rotational speed is sufficiently high, and the drive plate 8 and its fixed magnetron mounting plate 9 are turned to the outside around the shaft 14 on the bracket 10. (Fig. 1b), so that the magnetron 6 is correspondingly located in the edge region of the target 7, at which time the edge region of the target 7 is plasma etched under the action of the magnetron 6.
- the present invention is directed to the above technical problems existing in the prior art, and provides a magnetron element and a magnetron sputtering apparatus.
- the magnetron component can achieve full target corrosion of the target, avoid particles in the central region of the target, improve the utilization of the target, and improve the ionization rate of the metal target during sputtering; and improve the through hole on the wafer.
- the fill effect can be achieved.
- the invention provides a magnetron element for a sputtering target, comprising a closed magnetron and a non-closed magnetron, wherein a closed plasma is formed between an inner magnetic pole and an outer magnetic pole of the closed magnetron a path between the first magnetic pole and the second magnetic pole of the non-closed magnetron forming a non-closed plasma path, the closed plasma path and the non-closed plasma path at least corresponding to the target a center to a radius region of the edge of the target, and the effective extension length of the closed plasma path in the radial direction of the target and the non-closed plasma path are effective in the radial direction of the target The sum of the extension lengths is greater than or equal to the radius of the target.
- the areas through which the closed plasma path and the non-closed plasma path pass do not coincide with each other, and the center of rotation of the magnetron element corresponds to In the closed plasma path or the non-closed plasma path, the center of rotation of the magnetron element coincides with the center of the target.
- an orthographic projection of the closed magnetron in a plane of the target corresponds to an edge region of the target, and an orthographic projection of the non-closed magnetron at a plane of the target is located at the edge The central area of the target.
- an orthographic projection of the closed magnetron at a plane of the target corresponds to a central region of the target, and an orthographic projection of the non-closed magnetron at a plane of the target is located at the The edge area of the target.
- the effective extension length of the non-closed plasma path in the radial direction of the target is equal to the diameter length of the target.
- the outer magnetic pole of the closed magnetron is connected to the first magnetic pole of the non-closed magnetron.
- the outer magnetic pole of the closed magnetron is used as the first magnetic pole of the non-closed magnetron, and the non-closed plasma is formed between the outer magnetic pole and the second magnetic pole path.
- the present invention also provides a magnetron sputtering apparatus comprising a target, further comprising the above-mentioned magnetron element, the magnetron element being disposed directly above the target; further comprising a DC power source and/or a RF power source, a DC power source and/or the RF power source is coupled to the target for The target provides sputtering power.
- the frequency range of the radio frequency power source is 400k-60MHz.
- the frequency of the radio frequency power source is 400 kHz, 2 MHz, 13.56 MHz, 40 MHz or 60 MHz.
- the magnetron element provided by the present invention has at least a closed plasma path and a non-closed plasma path corresponding to a radius region located at a center of the target to an edge of the target, and the closed plasma
- the sum of the effective extension length of the path in the radial direction of the target and the effective extension length of the non-closed plasma path in the radial direction of the target is greater than or equal to the radius of the target, which can not only achieve the target corrosion of the target, but also improve the utilization of the target.
- the reduction in area can increase the power density of the closed plasma path acting on the target, thereby increasing the ionization rate of the target and also improving the filling effect of the via holes on the wafer.
- the magnetron sputtering device of the present invention by using the above-described magnetron element, not only the ionization rate of the metal target but also the total target corrosion is achieved.
- 1a is a schematic view showing the movement of a magnetron relative to a target in the prior art
- Figure 1b is a schematic view showing the rotational position of the driving plate relative to the bracket when the rotation speed of the magnetron is high in Figure 1a;
- Figure 1c is a schematic view showing the rotational position of the driving plate relative to the bracket when the rotation speed of the magnetron is low in Figure 1a;
- Embodiment 2 is a plan view showing the structure of a magnetron element in Embodiment 1 of the present invention
- Figure 3 is a plan view showing another structure of the magnetron element in Embodiment 1 of the present invention.
- FIG. 4 is a top plan view showing still another structure of the magnetron element in Embodiment 1 of the present invention.
- Figure 5 is a plan view showing the structure of a magnetron element in Embodiment 2 of the present invention.
- Figure 6 is a plan view showing the structure of a magnetron element in Embodiment 3 of the present invention.
- Figure 7 is a plan view showing the structure of a magnetron element in Embodiment 4 of the present invention.
- Figure 8 is a schematic view showing the structure of a magnetron sputtering apparatus in Embodiment 5 of the present invention.
- the present embodiment provides a magnetron element for sputtering a target, as shown in FIG. 2, comprising a closed magnetron 1 and a non-closed magnetron 2, closing the inner magnetic pole 11 and the outer magnetic pole 12 of the magnetron 1.
- a closed plasma path 13 is formed between the first magnetic pole 21 and the second magnetic pole 22 of the non-closed magnetron 2 to form a non-closed plasma path 23, a closed plasma path 13 and a non-closed plasma path.
- the effective extension length of the closed plasma path 13 in the radial direction of the target and the effective extension length of the non-closed plasma path 23 in the radial direction of the target The sum is greater than or equal to the radius of the target.
- the closed plasma path 13 and the non-closed plasma path 23 Corresponding to a radius region located at the center of the target to the edge of the target, and the effective extension length of the closed plasma path 13 in the radial direction of the target and the effective extension length of the non-closed plasma path 23 in the radial direction of the target Equal to the radius of the target.
- the outer magnetic pole 12 of the closed magnetron 1 has a closed annular shape, the inner magnetic pole 11 is nested inside the outer magnetic pole 12, and a space is formed between the inner magnetic pole 11 and the outer magnetic pole 12, and the inner magnetic pole 11 and the outer magnetic pole 12 are formed.
- the space between the gaps is in a closed loop, which is the effective magnetic field region of the closed magnetron 1, which is the closed plasma path 13 of the closed magnetron 1.
- the non-closed magnetron 2 means that the first magnetic pole 21 and the second magnetic pole 22 included therein are not closed, and are spaced apart from each other to form a spacing region, and the spacing region is in a non-closed pattern, and the non-closed spacing region is
- the effective magnetic field region of the non-closed magnetron 2 formed by the first magnetic pole 21 and the second magnetic pole 22 is the non-closed plasma path 23 of the non-closed magnetron 2.
- the effective magnetic field region referred to in the present application means that the magnetic field strength of the magnetic field region is relatively strong, and the magnetic control component mainly exerts a magnetic field through the effective magnetic field region, but the magnetic control component does not only have its effective magnetic field.
- the area has a magnetic field.
- the magnetron element rotates around its center of rotation during the magnetron sputtering process to sweep its plasma path across the process surface of the target, thereby causing the target to corrode under the magnetic field of the plasma path.
- what actually acts in the radial direction of the target is the portion of the equivalent straight line segment of the plasma path in the radial direction of the target. Since each side of the closed plasma path 13 may be linear, it may also be curved, and the closed plasma path 13 of the linear side may be parallel to the radial direction of the target, or may not be radial to the target.
- the effective extension length of the closed plasma path 13 in the radial direction of the target refers to the length of the equivalent straight line segment of the closed plasma path 13 in the radial direction of the target.
- the non-closed plasma path 23 can be linear, it can also be curved, and the linear non-closed plasma path 23 can be parallel to the radial direction of the target, and can also be the diameter of the target. Non-parallel, so, non-closed, etc.
- the effective extension length of the ion path 23 in the radial direction of the target refers to the length of the equivalent straight line segment of the non-closed plasma path 23 in the radial direction of the target.
- the target is circular
- the closed plasma path 13 and the non-closed plasma path 23 of the magnetron correspond to a radius region located at the center of the target to the edge of the target, and the closed plasma path 13
- the effective extension length in the radial direction of the target and the effective extension length of the non-closed plasma path 23 in the radial direction of the target are equal to the radius of the target, such that the magnetron is rotated during the process of the plasma
- the path as a whole can correspond to sweeping the entire target, thereby achieving full target corrosion of the target and improving the utilization of the target; meanwhile, when the magnetron rotates during the process, due to the closed plasma path 13 and non-closed
- the plasma path 23 can exactly sweep across the entire target, so that the entire target can be corroded, thereby avoiding the target central region caused by etching the edge region of the target first and then corroding the central region.
- the corresponding wafer area has a problem of particles, which in turn improves the quality of the
- the areas through which the closed plasma path 13 and the non-closed plasma path 23 pass do not coincide with each other, and the center of rotation P of the magnetron element corresponds to the non-closed plasma.
- the entire plasma path can be swept across the entire target, thereby achieving full target corrosion.
- the center of rotation P of the magnetron element coincides with the center of the target, so that the entire target corrosion can be achieved without setting a plasma path with a large area, thereby saving the amount of the magnet under the premise of ensuring corrosion of the entire target.
- the magnetron element As long as the magnetron element rotates around its rotation center P, full target corrosion can be achieved, and it is not necessary to change the position of the magnetron during the rotation of the magnetron by means of a spring or the like as in the prior art.
- the magnetron element provided in this embodiment does not need to be provided with an aging component such as a spring, so that the structure is not only simple, but also does not affect the sputtering due to the change of the working state of the aging component such as a spring. Stability.
- the magnetron element is only provided with a closed plasma path in the radius region of the target.
- the corresponding radius region of the target is provided.
- the closed plasma path 13 is disposed, and the non-closed plasma path 23 is disposed, and the regions swept by the two during the rotation of the magnetron are not coincident with each other, so that the area of the closed plasma path 13 is relatively reduced.
- the reduction in area can increase the power density of the closed plasma path 13 acting on the target, thereby increasing the ionization rate of the target and improving the on-wafer pass. The filling effect of the hole.
- the orthographic projection of the closed magnetron 1 in the plane of the target corresponds to the edge region of the target
- the orthographic projection of the non-closed magnetron 2 in the plane of the target corresponds to the central region of the target.
- the closed plasma path 13 corresponds to sweeping the edge region of the target
- the non-closed plasma path 23 corresponds to sweeping the central region of the target
- the closed plasma The sum of the effective extension length of the body path 13 in the radial direction of the target and the effective extension length of the non-closed plasma path 23 in the radial direction of the target is greater than or equal to the radius of the target, such that when the magnetron 1 and the non-closed magnetic are closed After the control tube 2 rotates around the rotation center P, the area swept by the orthographic projection of the closed plasma path 13 on the target is a circle centered on P, and the non-closed plasma path 23 is on the target.
- the area swept by the orthographic projection is a circle centered on P (i.e., a circle formed by the non-closed plasma path 23), and the inner diameter of the ring is smaller than or equal to the diameter of the circle (the circle formed by the path 23).
- the outer magnetic pole 12 of the closed magnetron 1 and the first magnetic pole 21 of the non-closed magnetron 2 are connected. So set up, during the rotation of the magnetron element about its center of rotation P, It is better enough to make the closed plasma path 13 and the non-closed plasma path 23 sweep across the radius region of the target, thereby avoiding partial leakage of the radius region of the target, thereby better achieving full target corrosion.
- the closed magnetron 1 and the non-closed magnetron 2 may also be disconnected, that is, the two are disposed independently of each other, and during the rotation of the magnetron, the closed plasma path 13
- the radius region is provided with both a closed plasma path 13 and a non-closed plasma path 23, and the regions swept by the two during the rotation of the magnetron element only partially overlap, so that the closed plasma path 13
- the area is relatively reduced, and in the case where a direct current power source is applied to the target, the reduction in area can increase the power density of the closed plasma path 13 acting on the target, thereby increasing the ionization rate of the target and improving the target.
- the magnetron element further includes a backing plate 3, and the closed magnetron 1 and the non-closed magnetron 2 are disposed on the same side of the backing plate 3.
- the shape of the back plate 3 is circular, and the back plate 3 is the same size as the target, the back plate 3 completely coincides with the target, and the back plate 3 can be rotated by the motor, thereby driving the closed magnetron 1 and the non-closed magnetic field.
- Control tube 2 rotates.
- the arrangement of the backing plate 3 enables a set distance between the closed magnetron 1 and the non-closed magnetron 2 and the target to ensure the stability of the magnetron sputtering.
- the closed shapes of the inner magnetic pole 11 and the outer magnetic pole 12 of the closed magnetron 1 are both kidney-shaped.
- the closed shapes of the inner magnetic pole 11 and the outer magnetic pole 12 of the closed magnetron 1 may also be circular (as shown in FIG. 4), or the closed shape of the inner magnetic pole 11 and the outer magnetic pole 12 of the closed magnetron 1 may be closed. It can also be other closed shapes.
- the spacing between the inner magnetic pole 11 and the outer magnetic pole 12 of the magnetron 1 (i.e., the width of the closed plasma path 13) and the first magnetic pole 21 and the second of the non-closed magnetron 2 are closed.
- the spacing between the poles 22 (i.e., the width of the non-closed plasma path 23) is equal.
- the arrangement is such that the magnetic field strength within the closed plasma path 13 and the non-closed plasma path 23 is the same, thereby facilitating uniform sputtering of the target.
- the width of the closed plasma path 13 and the width of the non-closed plasma path 23 may also be unequal.
- the present embodiment provides a magnetic control element.
- the outer magnetic pole 12 of the closed magnetron 1 serves as the first magnetic pole of the non-closed magnetron 2, and the outer magnetic pole 12 A non-closed plasma path is formed between the second pole 22 and the second pole. That is, the second magnetic pole 22 of the non-closed magnetron 2 and the outer magnetic pole 12 of the closed magnetron 1 are spaced apart from each other and form a spacing region in which an effective magnetic field is formed, which is a non-closed plasma. Path 23.
- the closed plasma path 13 corresponds to sweeping a portion of the region within the radius of the target
- the non-closed plasma path 23 corresponds to sweeping the entire target.
- the closed plasma path 13 and the non-closed plasma path 23 jointly correspond to the radius region of the target, thereby achieving full target corrosion and improving target utilization.
- the problem of particles appearing in the wafer region corresponding to the central region of the target caused by etching the edge region of the target and then corroding the central region of the target is avoided, thereby improving the quality and product of the sputtering process.
- the magnetron element is only provided with a closed plasma path in the radius region of the target, and the magnetron element in FIG. 5 is provided with a closed state corresponding to the radius region of the target.
- the plasma path 13 is again provided with a non-closed plasma path 23, and the regions swept by the two during the rotation of the magnetron element only partially overlap. Therefore, the area of the closed plasma path 13 is relatively reduced, and in the case where a direct current power source is applied to the target, the reduction in area can increase the power density of the closed plasma path 13 acting on the target, thereby increasing the target.
- the ionization rate of the material and the filling effect of the through holes on the wafer are examples of the material and the filling effect of the through holes on the wafer.
- This embodiment provides a magnetic control element. Different from Embodiment 1-2, as shown in FIG. 6, the orthographic projection of the closed magnetron 1 in the plane of the target corresponds to the central region of the target, and the non-closed magnetic The orthographic projection of the control tube 2 in the plane of the target corresponds to the edge region of the target.
- the closed plasma path 13 corresponds to sweeping the central region of the target, and the non-closed plasma path 23 corresponds to the edge region of the target, closed plasma path 13
- the non-closed plasma path 23 corresponds to the radius region of the target, thereby achieving full target corrosion and improving the utilization of the target; and avoiding the prior art by etching the edge region of the target.
- Corrosion of the central region causes a problem of particles in the wafer region corresponding to the central region of the target, thereby improving the quality of the sputtering process and the yield of the product; meanwhile, the magnetic control component corresponding to the target in the prior art
- the radius region is only provided with a closed plasma path.
- a closed plasma path 13 is provided corresponding to the radius region of the target, a non-closed plasma path 23 is provided, and both are magnetic.
- the areas swept during the rotation of the control element do not coincide with each other, so the area of the closed plasma path 13 is relatively reduced, and a DC power source is applied to the target.
- reducing the area of the plasma can be improved closed path 13 is applied to the power density on the target, thereby increasing the ionization rate of the target, and to improve the through-holes on the wafer filling effect.
- the center of rotation P of the magnetron element in this embodiment corresponds to the plasma located in the closed state.
- the plasma path can be swept across the entire target, so that full target corrosion can be achieved.
- the present embodiment provides a magnetron element.
- the effective extension length of the closed plasma path 13 in the radial direction of the target and the non-closed plasma path 23 are The sum of the effective extension lengths in the radial direction of the target is greater than the radius of the target.
- the effective extension length of the non-closed plasma path 23 in the radial direction of the target is equal to the diameter length of the target. That is, the length of the equivalent straight line segment of the non-closed plasma path 23 in the radial direction of the target is equal to the diameter length of the target.
- the arrangement of the closed magnetron 1 in this embodiment is the same as that of any of Embodiments 1-3.
- the closed plasma path 13 corresponds to a portion of the radius of the target
- the non-closed plasma path 23 corresponds to sweeping the entire diameter of the target
- the plasma path 13 and the non-closed plasma path 23 jointly correspond to sweeping the entire diameter region of the target, thereby achieving full target corrosion and improving the utilization of the target; and avoiding prior corrosion in the prior art.
- the edge region of the target re-corrodes the central region to cause the problem of particles in the wafer region corresponding to the central region of the target, thereby improving the quality of the sputtering process and the yield of the product; meanwhile, compared with the prior art, the magnetic control
- the component corresponds to the case where only the closed plasma path is provided in the radius region of the target, and the magnetron element in FIG. 3 is provided with a closed plasma path 13 and a non-closed plasma due to the corresponding radius region of the target.
- the body path 23, and the areas swept by the two during the rotation of the magnetron element only partially overlap, so the area of the closed plasma path 13 is made Relatively reduced, in the case where a DC power source is applied to the target, the reduction in area can increase the power density of the closed plasma path 13 acting on the target, thereby increasing The ionization rate of the target and the filling effect of the through holes on the wafer.
- Embodiments 1-4 are configured such that the closed plasma path and the non-closed plasma path correspond at least to a radius from the center of the target to the edge of the target The region, and the effective extension length of the closed plasma path in the radial direction of the target and the effective extension length of the non-closed plasma path in the radial direction of the target are greater than or equal to the radius of the target, and not only the full target of the target can be achieved Corrosion, improve the utilization of the target; and avoid particles in the wafer area corresponding to the central area of the target, improve the quality of the magnetron sputtering process and product yield; and, at the same time, apply DC power to the target Due to the reduced area of the closed plasma path, the power density of the closed plasma path acting on the target can be increased, thereby increasing the ionization rate of the target and improving the filling effect of the via holes on the wafer.
- the present embodiment provides a magnetron sputtering apparatus, as shown in FIG. 8, comprising a target 7, and further comprising a magnetron element 15 in any of Embodiments 1-4, the magnetron element 15 being disposed on the target 7 Above; the magnetron sputtering device further comprises a radio frequency power source 16 and/or a DC power source 17, and its control element 18, the RF power source 16 and/or the DC power source 17 is connected to the target 7, and the control element 18 is connected to the RF power source 16 and/or The DC power source 17, control element 18 is used to control the RF power source 16 and/or the DC power source 17 to provide sputtering power to the target 7.
- the control element 18 controls the RF power source 16 and the DC power source 17 to be alternately applied to the target 7 to provide sputtering power to the target 7.
- the closed plasma path and the non-closed plasma path correspond at least to a radius region located at the center of the target 7 to the edge of the target 7, and the closed plasma path is at the target 7 diameter
- Effective extension of the upward effective length and non-closed plasma path in the radial direction of the target 7 The sum of the elongations is greater than or equal to the radius of the target 7, which can make the surface corrosion of the target 7 more uniform, achieve full target corrosion, and the target utilization rate is high, and at the same time, can improve the ionization rate of the target 7;
- the closed plasma path area of the closed magnetron since the closed plasma path area of the closed magnetron is relatively reduced, the power density of the closed plasma path acting on the target 7 is increased, thereby increasing the ionization rate of the target 7, and
- the frequency range of the radio frequency power source is 400k-60MHz.
- the frequency of the radio frequency power source is 400 kHz, 2 MHz, 13.56 MHz, 40 MHz or 60 MHz.
- Embodiment 5 the magnetron sputtering apparatus provided in Embodiment 5, by using the magnetron element of any of Embodiments 1-4, not only improves the ionization rate of the metal target but also realizes the total target corrosion.
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Abstract
Description
本发明涉及磁控溅射技术领域,具体地,涉及一种磁控元件和磁控溅射装置。The present invention relates to the field of magnetron sputtering technology, and in particular to a magnetron element and a magnetron sputtering device.
溅射是指荷能粒子(例如氩离子)轰击固体表面,引起表面各种粒子,如原子、分子或团束从该物体表面逸出的现象。在磁控溅射装置中,等离子体产生于腔室中,等离子体的正离子被阴极负电所吸引,轰击腔室中的靶材,撞出靶材的原子,并沉积到衬底上。在非反应溅射的情况下,气体是惰性气体,例如氩气。在反应溅射中,则采用反应气体和惰性气体一起使用。磁控溅射设备广泛的应用于集成电路、液晶显示器、薄膜太阳能及LED领域等。Sputtering refers to the phenomenon in which charged particles (such as argon ions) bombard a solid surface, causing various particles on the surface, such as atoms, molecules or bunches, to escape from the surface of the object. In a magnetron sputtering apparatus, a plasma is generated in a chamber, and positive ions of the plasma are attracted by a cathode negative, bombarding a target in the chamber, knocking out atoms of the target, and depositing on the substrate. In the case of non-reactive sputtering, the gas is an inert gas such as argon. In reactive sputtering, a reactive gas is used together with an inert gas. Magnetron sputtering equipment is widely used in integrated circuits, liquid crystal displays, thin film solar and LED fields.
为了改善溅射的效果,在靶材附近使用了磁铁,它可以迫使等离子中的电子按照一定的轨道运动,增加了电子的运动时间,从而增加了电子和要电离的气体碰撞的机会,从而得到高密度的等离子体,提供高的沉积速率。同时磁铁所控的电子的轨道会影响不同位置的靶材的侵蚀速率,影响靶材的寿命。同时还会影响薄膜的沉积的均匀性。In order to improve the effect of sputtering, a magnet is used in the vicinity of the target, which can force the electrons in the plasma to move according to a certain orbit, increasing the movement time of the electrons, thereby increasing the chance of electrons colliding with the gas to be ionized, thereby obtaining High density plasma provides high deposition rates. At the same time, the orbit of the electron controlled by the magnet affects the erosion rate of the target at different positions, affecting the life of the target. It also affects the uniformity of deposition of the film.
为了实现溅射过程中靶材的全靶腐蚀,如图1a至1c所示,在现有技术一中,磁控管6采用如图1a中的肾形嵌套式结构。磁控管6固定安装在磁控管安装板9上,磁控管安装板9固定在驱动板8上,驱动板8与托架10通过轴14活动连接,驱动板8能绕轴14转动,托架10与驱动板8之间还连接有弹簧5;托架10与驱动轴4活动连接,且托架10能绕驱动轴4转动。驱动轴4对应位于靶材的中心。磁控溅射工艺开始时,托架10带动驱动板8和磁控管6绕驱动轴4旋转,如:驱动
轴4以一定转速逆时针旋转,转速足够高时使得磁控管6的离心力超过弹簧5的弹力,驱动板8和其固定的磁控管安装板9绕着托架10上的轴14转向外侧(如图1b),从而使磁控管6对应位于靶材7的边缘区域,此时,在磁控管6的作用下,等离子体刻蚀靶材7的边缘区域。相反,转速很低时,驱动轴4仍然逆时针转动,但很低的转速使得磁控管6的离心力小于弹簧5的弹力,弹簧5将驱动板8和其固定的磁控管安装板9绕着托架10上的轴14拉向内侧(如图1c),从而使磁控管6被拉回到对应靶材7的中心区域的位置,此时,在磁控管6的作用下,等离子体刻蚀靶材7的中心区域。在整个工艺过程中,通过改变托架10的转速控制磁控管6在对应靶材7的边缘区域和中心区域之间进行位置转换,从而实现对靶材7的边缘区域和中心区域的腐蚀,最终实现全靶腐蚀。In order to achieve full target corrosion of the target during sputtering, as shown in Figures 1a to 1c, in the
但是,现有技术一中只能通过控制托架10的转速使靶材7的边缘区域和中心区域先后完成腐蚀,即,先腐蚀靶材7的边缘区域再腐蚀其中心区域,然而这样会导致靶材7的中心区域所对应的晶片区域出现颗粒,从而导致溅射工艺质量和产品良率都比较低。However, in the
另外,现有技术一中,由于弹簧存在弹性性能损耗问题,所以很难通过不同转速准确控制磁控管的位置而实现全靶腐蚀。In addition, in the
发明内容Summary of the invention
本发明针对现有技术中存在的上述技术问题,提供一种磁控元件和磁控溅射装置。该磁控元件能够实现靶材的全靶腐蚀,避免靶材的中心区域出现颗粒,提高靶材的利用率;还能提高溅射过程中金属靶材的离化率;同时提高晶片上通孔的填充效果。The present invention is directed to the above technical problems existing in the prior art, and provides a magnetron element and a magnetron sputtering apparatus. The magnetron component can achieve full target corrosion of the target, avoid particles in the central region of the target, improve the utilization of the target, and improve the ionization rate of the metal target during sputtering; and improve the through hole on the wafer. The fill effect.
本发明提供一种磁控元件,用于溅射靶材,包括闭合磁控管和非闭合磁控管,所述闭合磁控管的内磁极和外磁极之间组成闭合的等离子体 路径,所述非闭合磁控管的第一磁极和第二磁极之间组成非闭合的等离子体路径,所述闭合的等离子体路径和所述非闭合的等离子体路径至少对应位于所述靶材的中心到所述靶材的边缘的半径区域,且所述闭合的等离子体路径在所述靶材径向上的有效延伸长度和所述非闭合的等离子体路径在所述靶材径向上的有效延伸长度之和大于等于所述靶材的半径。The invention provides a magnetron element for a sputtering target, comprising a closed magnetron and a non-closed magnetron, wherein a closed plasma is formed between an inner magnetic pole and an outer magnetic pole of the closed magnetron a path between the first magnetic pole and the second magnetic pole of the non-closed magnetron forming a non-closed plasma path, the closed plasma path and the non-closed plasma path at least corresponding to the target a center to a radius region of the edge of the target, and the effective extension length of the closed plasma path in the radial direction of the target and the non-closed plasma path are effective in the radial direction of the target The sum of the extension lengths is greater than or equal to the radius of the target.
优选地,在所述磁控元件的旋转过程中,所述闭合的等离子体路径和所述非闭合的等离子体路径所经过的区域互不重合,所述磁控元件的旋转中心对应位于所述闭合的等离子体路径或者所述非闭合的等离子体路径中,所述磁控元件的旋转中心与所述靶材的中心重合。Preferably, during the rotation of the magnetron element, the areas through which the closed plasma path and the non-closed plasma path pass do not coincide with each other, and the center of rotation of the magnetron element corresponds to In the closed plasma path or the non-closed plasma path, the center of rotation of the magnetron element coincides with the center of the target.
优选地,所述闭合磁控管在所述靶材所在平面的正投影对应位于所述靶材的边缘区域,所述非闭合磁控管在所述靶材所在平面的正投影对应位于所述靶材的中心区域。Preferably, an orthographic projection of the closed magnetron in a plane of the target corresponds to an edge region of the target, and an orthographic projection of the non-closed magnetron at a plane of the target is located at the edge The central area of the target.
优选地,所述闭合磁控管在所述靶材所在平面的正投影对应位于所述靶材的中心区域,所述非闭合磁控管在所述靶材所在平面的正投影对应位于所述靶材的边缘区域。Preferably, an orthographic projection of the closed magnetron at a plane of the target corresponds to a central region of the target, and an orthographic projection of the non-closed magnetron at a plane of the target is located at the The edge area of the target.
优选地,所述非闭合的等离子体路径在所述靶材径向上的有效延伸长度等于所述靶材的直径长度。Preferably, the effective extension length of the non-closed plasma path in the radial direction of the target is equal to the diameter length of the target.
优选地,所述闭合磁控管的外磁极和所述非闭合磁控管的第一磁极连接。Preferably, the outer magnetic pole of the closed magnetron is connected to the first magnetic pole of the non-closed magnetron.
优选地,所述闭合磁控管的所述外磁极用作所述非闭合磁控管的所述第一磁极,所述外磁极和所述第二磁极之间组成所述非闭合的等离子体路径。Preferably, the outer magnetic pole of the closed magnetron is used as the first magnetic pole of the non-closed magnetron, and the non-closed plasma is formed between the outer magnetic pole and the second magnetic pole path.
本发明还提供一种磁控溅射装置,包括靶材,还包括上述的磁控元件,所述磁控元件设置在所述靶材的正上方;还包括直流电源和/或射频电源,所述直流电源和/或所述射频电源连接所述靶材,用于为所述 靶材提供溅射功率。The present invention also provides a magnetron sputtering apparatus comprising a target, further comprising the above-mentioned magnetron element, the magnetron element being disposed directly above the target; further comprising a DC power source and/or a RF power source, a DC power source and/or the RF power source is coupled to the target for The target provides sputtering power.
优选地,所述射频电源的频率范围为400k-60MHz。Preferably, the frequency range of the radio frequency power source is 400k-60MHz.
优选地,所述射频电源的频率为400kHz、2MHz、13.56MHz、40MHz或60MHz。Preferably, the frequency of the radio frequency power source is 400 kHz, 2 MHz, 13.56 MHz, 40 MHz or 60 MHz.
本发明的有益效果:本发明所提供的磁控元件,通过使闭合的等离子体路径和非闭合的等离子体路径至少对应位于靶材的中心到靶材的边缘的半径区域,且闭合的等离子体路径在靶材径向上的有效延伸长度和非闭合的等离子体路径在靶材径向上的有效延伸长度之和大于等于靶材的半径,不仅能够实现靶材的全靶腐蚀,提高靶材的利用率;而且能够避免靶材的中心区域所对应的晶片区域出现颗粒,提高磁控溅射工艺的质量和产品良率;同时,在靶材上施加直流电源的情况下,由于闭合的等离子体路径面积的减小,能提高闭合的等离子体路径作用到靶材上的功率密度,从而提高了靶材的离化率,而且还提高了晶片上通孔的填充效果。Advantageous Effects of Invention: The magnetron element provided by the present invention has at least a closed plasma path and a non-closed plasma path corresponding to a radius region located at a center of the target to an edge of the target, and the closed plasma The sum of the effective extension length of the path in the radial direction of the target and the effective extension length of the non-closed plasma path in the radial direction of the target is greater than or equal to the radius of the target, which can not only achieve the target corrosion of the target, but also improve the utilization of the target. Rate; and can avoid particles in the wafer area corresponding to the central region of the target, improve the quality of the magnetron sputtering process and product yield; and, at the same time, apply a DC power supply to the target due to the closed plasma path The reduction in area can increase the power density of the closed plasma path acting on the target, thereby increasing the ionization rate of the target and also improving the filling effect of the via holes on the wafer.
本发明所提供的磁控溅射装置,通过采用上述磁控元件,不仅提高了金属靶材的离化率,而且实现了全靶腐蚀。According to the magnetron sputtering device of the present invention, by using the above-described magnetron element, not only the ionization rate of the metal target but also the total target corrosion is achieved.
图1a为现有技术一中磁控管相对靶材的运动示意图;1a is a schematic view showing the movement of a magnetron relative to a target in the prior art;
图1b为图1a中磁控管的转速较高时驱动板相对托架的转动位置示意图;Figure 1b is a schematic view showing the rotational position of the driving plate relative to the bracket when the rotation speed of the magnetron is high in Figure 1a;
图1c为图1a中磁控管的转速较低时驱动板相对托架的转动位置示意图;Figure 1c is a schematic view showing the rotational position of the driving plate relative to the bracket when the rotation speed of the magnetron is low in Figure 1a;
图2为本发明实施例1中磁控元件的结构俯视图;2 is a plan view showing the structure of a magnetron element in
图3为本发明实施例1中磁控元件的另一种结构俯视图;Figure 3 is a plan view showing another structure of the magnetron element in
图4为本发明实施例1中磁控元件的又一种结构俯视图;
4 is a top plan view showing still another structure of the magnetron element in
图5为本发明实施例2中磁控元件的结构俯视图;Figure 5 is a plan view showing the structure of a magnetron element in Embodiment 2 of the present invention;
图6为本发明实施例3中磁控元件的结构俯视图;Figure 6 is a plan view showing the structure of a magnetron element in
图7为本发明实施例4中磁控元件的结构俯视图;Figure 7 is a plan view showing the structure of a magnetron element in
图8为本发明实施例5中磁控溅射装置的结构示意图。Figure 8 is a schematic view showing the structure of a magnetron sputtering apparatus in Embodiment 5 of the present invention.
其中的附图标记说明:The reference numerals are as follows:
1.闭合磁控管;11.内磁极;12.外磁极;13.闭合的等离子体路径;2.非闭合磁控管;21.第一磁极;22.第二磁极;23.非闭合的等离子体路径;P.磁控元件的旋转中心;3.背板;4.驱动轴;5.弹簧;6.磁控管;7.靶材;8.驱动板;9.磁控管安装板;10.托架;14.轴;15.磁控元件;16.射频电源;17.直流电源;18.控制元件;19.晶片。1. Close the magnetron; 11. Inner magnetic pole; 12. External magnetic pole; 13. Closed plasma path; 2. Non-closed magnetron; 21. First magnetic pole; 22. Second magnetic pole; 23. Non-closed Plasma path; P. rotation center of magnetron element; 3. back plate; 4. drive shaft; 5. spring; 6. magnetron; 7. target; 8. drive plate; 9.
为使本领域的技术人员更好地理解本发明的技术方案,下面结合附图和具体实施方式对本发明所提供的一种磁控元件和磁控溅射装置作进一步详细描述。In order to enable those skilled in the art to better understand the technical solutions of the present invention, a magnetic control element and a magnetron sputtering apparatus provided by the present invention will be further described in detail below with reference to the accompanying drawings and specific embodiments.
实施例1:Example 1:
本实施例提供一种磁控元件,用于溅射靶材,如图2所示,包括闭合磁控管1和非闭合磁控管2,闭合磁控管1的内磁极11和外磁极12之间组成闭合的等离子体路径13,非闭合磁控管2的第一磁极21和第二磁极22之间组成非闭合的等离子体路径23,闭合的等离子体路径13和非闭合的等离子体路径23至少对应位于靶材的中心到靶材的边缘的半径区域,且闭合的等离子体路径13在靶材径向上的有效延伸长度和非闭合的等离子体路径23在靶材径向上的有效延伸长度之和大于等于靶材的半径。The present embodiment provides a magnetron element for sputtering a target, as shown in FIG. 2, comprising a
如图2中,闭合的等离子体路径13和非闭合的等离子体路径23
对应位于靶材的中心到靶材的边缘的半径区域,且闭合的等离子体路径13在靶材径向上的有效延伸长度和非闭合的等离子体路径23在靶材径向上的有效延伸长度之和等于靶材的半径。As in Figure 2, the
其中,闭合磁控管1的外磁极12呈闭合的环状,内磁极11嵌套于外磁极12的内部,且内磁极11与外磁极12之间形成间隔区域,内磁极11和外磁极12之间的间隔区域呈闭合的环状,该闭合的环状的间隔区域为闭合磁控管1的有效磁场区域,该有效磁场区域即为闭合磁控管1的闭合的等离子体路径13。非闭合磁控管2指其所包含的第一磁极21和第二磁极22各自均不闭合且二者之间相互间隔形成间隔区域,该间隔区域呈非闭合图形,该非闭合的间隔区域为第一磁极21和第二磁极22所形成的非闭合磁控管2的有效磁场区域,该有效磁场区域即为非闭合磁控管2的非闭合的等离子体路径23。需要说明的是,本申请中所说的有效磁场区域是指该磁场区域的磁场强度相对较强,且磁控元件主要通过其有效磁场区域发挥磁场作用,但磁控元件并不是只有其有效磁场区域才具有磁场。The outer
需要说明的是,磁控元件在磁控溅射工艺过程中绕其旋转中心旋转,以使其等离子体路径扫过靶材的工艺面,从而使靶材在等离子体路径的磁场作用下进行腐蚀,无论等离子体路径是什么形状,实际在靶材径向上发生作用的是等离子体路径在靶材径向上的等效直线段所对应的部分。由于闭合的等离子体路径13的每一边可以呈直线状,也可以呈曲线状,且直线状边的闭合的等离子体路径13可以与靶材的径向平行,也可以与靶材的径向不平行,所以,闭合的等离子体路径13在靶材径向上的有效延伸长度指的是:闭合的等离子体路径13在靶材的径向上的等效直线段长度。同理,由于非闭合的等离子体路径23的可以呈直线状,也可以呈曲线状,且直线状的非闭合的等离子体路径23可以与靶材的径向平行,也可以与靶材的径向不平行,所以,非闭合的等
离子体路径23在靶材径向上的有效延伸长度指的是:非闭合的等离子体路径23在靶材的径向上的等效直线段长度。It should be noted that the magnetron element rotates around its center of rotation during the magnetron sputtering process to sweep its plasma path across the process surface of the target, thereby causing the target to corrode under the magnetic field of the plasma path. Regardless of the shape of the plasma path, what actually acts in the radial direction of the target is the portion of the equivalent straight line segment of the plasma path in the radial direction of the target. Since each side of the
本实施例中,靶材为圆形,磁控元件的闭合的等离子体路径13和非闭合的等离子体路径23对应位于靶材的中心到靶材的边缘的半径区域,且闭合的等离子体路径13在靶材径向上的有效延伸长度和非闭合的等离子体路径23在靶材径向上的有效延伸长度之和等于靶材的半径,这样,磁控元件在工艺过程中旋转时,其等离子体路径整体能够恰好对应扫过整个靶材,从而实现靶材的全靶腐蚀,提高了靶材的利用率;同时,磁控元件在工艺过程中旋转时,由于闭合的等离子体路径13和非闭合的等离子体路径23能够恰好对应扫过整个靶材,所以能使整个靶材都遭受腐蚀,从而避免现有技术中因先腐蚀靶材的边缘区域再腐蚀其中心区域所导致的靶材中心区域所对应的晶片区域出现颗粒的问题,进而提高了溅射工艺的质量和产品良率。In this embodiment, the target is circular, and the
本实施例中,在磁控元件的旋转过程中,闭合的等离子体路径13和非闭合的等离子体路径23所经过的区域互不重合,磁控元件的旋转中心P对应位于非闭合的等离子体路径23中,这样,通过旋转磁控元件可以使等离子体路径整体扫过全靶,从而能够实现全靶腐蚀。优选的,磁控元件的旋转中心P与靶材中心重合,如此设置,无需设置面积很大的等离子体路径,即可实现全靶腐蚀,从而在保证全靶腐蚀的前提下节约了磁体的用量;而且本实施例中只要该磁控元件绕其旋转中心P自转即可实现全靶腐蚀,无需像现有技术那样,需要借助弹簧等部件在磁控管旋转过程中改变磁控管的位置,以便覆盖更多的靶材区域;因此,本实施例提供的磁控元件无需设置弹簧等易老化部件,这样不仅结构简单,而且也不会因弹簧等易老化部件的工作状态变化而影响溅射的稳定性。同时,相对于现有技术中磁控元件对应在靶材的半径区域只设置有闭合等离子体路径的情况,本实施例中由于对应在靶材的半径区域既设
置有闭合的等离子体路径13,又设置有非闭合的等离子体路径23,且二者在磁控元件旋转过程中扫过的区域互不重合,所以使闭合的等离子体路径13的面积相对减小,在靶材上施加直流电源的情况下,面积的减小能提高闭合的等离子体路径13作用到靶材上的功率密度,从而提高了靶材的离化率,以及提高了晶片上通孔的填充效果。In this embodiment, during the rotation of the magnetron element, the areas through which the
本实施例中,闭合磁控管1在靶材所在平面的正投影对应位于靶材的边缘区域,非闭合磁控管2在靶材所在平面的正投影对应位于靶材的中心区域。如此,磁控元件在工艺过程中旋转时,闭合的等离子体路径13便对应扫过靶材的边缘区域,非闭合的等离子体路径23便对应扫过靶材的中心区域,并且,闭合的等离子体路径13在靶材径向上的有效延伸长度和非闭合的等离子体路径23在靶材径向上的有效延伸长度之和大于等于靶材的半径,这样,当闭合磁控管1和非闭合磁控管2绕旋转中心P旋转一周后,闭合的等离子体路径13在靶材上的正投影所扫过的区域为以P为圆心的圆环,非闭合的等离子体路径23在靶材上的正投影所扫过的区域为以P为圆心的圆(即非闭合的等离子体路径23所构成的圆),且圆环的内径小于等于圆(路径23所构成的圆)的直径。如此设置,通过旋转磁控元件可以使磁控元件的等离子体路径整体扫过全靶,实现全靶腐蚀,从而提高了靶材的利用率。磁控元件绕旋转中心P旋转过程中,由于闭合的等离子体路径13对应扫过靶材的边缘区域,同时非闭合的等离子体路径23对应扫过靶材的中心区域,在工艺过程中,靶材的中心区域和靶材的边缘区域同时遭受腐蚀,因此能够避免现有技术中因先腐蚀靶材的边缘区域再腐蚀中心区域导致的靶材中心区域所对应晶片区域出现颗粒的问题,从而提高了溅射工艺的质量和产品良率。In this embodiment, the orthographic projection of the
本实施例中,闭合磁控管1的外磁极12和非闭合磁控管2的第一磁极21连接。如此设置,在磁控元件绕其旋转中心P旋转过程中,能
够更好地使闭合的等离子体路径13和非闭合的等离子体路径23共同扫过靶材的半径区域,从而避免靶材的半径区域局部被遗漏,进而更好地实现全靶腐蚀。In the present embodiment, the outer
需要说明的是,如图3所示,闭合磁控管1与非闭合磁控管2也可以不连接,即二者相互独立设置,且在磁控元件旋转过程中,闭合的等离子体路径13和非闭合的等离子体路径23所经过的区域部分重合,闭合磁控管1形成的闭合的等离子体路径13和由非闭合磁控管2形成的非闭合的等离子体路径23共同扫过靶材的半径区域。如此设置,同样能够实现全靶腐蚀;同时,相对于现有技术中磁控元件对应在靶材的半径区域只设置有闭合等离子体路径的情况,图3中的磁控元件由于对应在靶材的半径区域既设置有闭合的等离子体路径13,又设置有非闭合的等离子体路径23,且二者在磁控元件旋转过程中扫过的区域只有部分重合,所以使闭合的等离子体路径13的面积相对减小,在靶材上施加直流电源的情况下,面积的减小能提高闭合的等离子体路径13作用到靶材上的功率密度,从而提高了靶材的离化率,以及提高了晶片上通孔的填充效果。It should be noted that, as shown in FIG. 3, the
本实施例中,磁控元件还包括背板3,闭合磁控管1和非闭合磁控管2设置在背板3的同一面上。背板3的形状为圆形,且背板3与靶材大小相同,背板3与靶材完全重合,背板3能在电机的带动下旋转,从而带动闭合磁控管1和非闭合磁控管2旋转。背板3的设置能使闭合磁控管1和非闭合磁控管2与靶材之间保持设定距离,确保磁控溅射的稳定性。In this embodiment, the magnetron element further includes a
本实施例中,如图2所示,闭合磁控管1的内磁极11和外磁极12的闭合形状均为肾形。当然,闭合磁控管1的内磁极11和外磁极12的闭合形状也可以均为圆形(如图4所示),或者,闭合磁控管1的内磁极11和外磁极12的闭合形状也可以为其他的闭合形状。
In the present embodiment, as shown in FIG. 2, the closed shapes of the inner
另外,本实施例中,闭合磁控管1的内磁极11和外磁极12之间的间距(即闭合的等离子体路径13的宽度)与非闭合磁控管2的第一磁极21和第二磁极22之间的间距(即非闭合的等离子体路径23的宽度)相等。如此设置,能使闭合的等离子体路径13与非闭合的等离子体路径23内的磁场强度相同,从而有利于实现靶材的均匀溅射。当然,闭合的等离子体路径13的宽度与非闭合的等离子体路径23的宽度也可以不相等。In addition, in the present embodiment, the spacing between the inner
实施例2:Example 2:
本实施例提供一种磁控元件,与实施例1中不同的是,如图5所示,闭合磁控管1的外磁极12用作非闭合磁控管2的第一磁极,外磁极12和第二磁极22之间组成非闭合的等离子体路径。即非闭合磁控管2的第二磁极22与闭合磁控管1的外磁极12之间相互间隔并形成间隔区域,该间隔区域内形成有效磁场,该有效磁场区域即为非闭合的等离子体路径23。The present embodiment provides a magnetic control element. Unlike the first embodiment, as shown in FIG. 5, the outer
本实施例中,在磁控元件绕其旋转中心P旋转过程中,闭合的等离子体路径13对应扫过靶材半径区域内的部分区域,非闭合的等离子体路径23对应扫过靶材的整个半径区域,在靶材溅射过程中,通过闭合的等离子体路径13和非闭合的等离子体路径23共同对应扫过靶材的半径区域,从而实现了全靶腐蚀,提高了靶材的利用率;同时还避免了现有技术中因先腐蚀靶材的边缘区域再腐蚀其中心区域所导致的靶材中心区域所对应的晶片区域出现颗粒的问题,从而提高了溅射工艺的质量和产品良率;另外,相对于现有技术中磁控元件对应在靶材的半径区域只设置有闭合等离子体路径的情况,图5中的磁控元件由于对应在靶材的半径区域既设置有闭合的等离子体路径13,又设置有非闭合的等离子体路径23,且二者在磁控元件旋转过程中扫过的区域只有部分重合,
所以使闭合的等离子体路径13的面积相对减小,在靶材上施加直流电源的情况下,面积的减小能提高闭合的等离子体路径13作用到靶材上的功率密度,从而提高了靶材的离化率,以及提高了晶片上通孔的填充效果。In this embodiment, during the rotation of the magnetron about its center of rotation P, the
本实施例中磁控元件的其他结构与实施例1中相同,此处不再赘述。Other structures of the magnetron component in this embodiment are the same as those in
实施例3:Example 3:
本实施例提供一种磁控元件,与实施例1-2不同的是,如图6所示,闭合磁控管1在靶材所在平面的正投影对应位于靶材的中心区域,非闭合磁控管2在靶材所在平面的正投影对应位于靶材的边缘区域。This embodiment provides a magnetic control element. Different from Embodiment 1-2, as shown in FIG. 6, the orthographic projection of the
在磁控元件绕其旋转中心P旋转过程中,闭合的等离子体路径13对应扫过靶材的中心区域,非闭合的等离子体路径23对应扫过靶材的边缘区域,闭合的等离子体路径13和非闭合的等离子体路径23共同对应扫过靶材的半径区域,从而实现了全靶腐蚀,提高了靶材的利用率;同时还避免了现有技术中因先腐蚀靶材的边缘区域再腐蚀其中心区域所导致的靶材中心区域所对应的晶片区域出现颗粒的问题,从而提高了溅射工艺的质量和产品良率;同时,相对于现有技术中磁控元件对应在靶材的半径区域只设置有闭合等离子体路径的情况,本实施例中由于对应在靶材的半径区域既设置有闭合的等离子体路径13,又设置有非闭合的等离子体路径23,且二者在磁控元件旋转过程中扫过的区域互不重合,所以使闭合的等离子体路径13的面积相对减小,在靶材上施加直流电源的情况下,面积的减小能提高闭合的等离子体路径13作用到靶材上的功率密度,从而提高了靶材的离化率,以及提高了晶片上通孔的填充效果。During rotation of the magnetron about its center of rotation P, the
相应地,本实施例中磁控元件的旋转中心P对应位于闭合的等离子
体路径13中。如此设置,通过旋转磁控元件可以使等离子体路径整体扫过全靶,如此可以实现全靶腐蚀。Correspondingly, the center of rotation P of the magnetron element in this embodiment corresponds to the plasma located in the closed state.
In the
本实施例中磁控元件的其他结构与实施例1或2中相同,此处不再赘述。Other structures of the magnetron element in this embodiment are the same as those in
实施例4:Example 4:
本实施例提供一种磁控元件,与实施例1-3不同的是,如图7所示,闭合的等离子体路径13在靶材径向上的有效延伸长度和非闭合的等离子体路径23在靶材径向上的有效延伸长度之和大于靶材的半径。优选地,非闭合的等离子体路径23在靶材径向上的有效延伸长度等于靶材的直径长度。即非闭合的等离子体路径23在靶材的径向上的等效直线段长度等于靶材的直径长度。本实施例中闭合磁控管1的设置方式与实施例1-3中的任意一个相同。The present embodiment provides a magnetron element. Unlike Embodiment 1-3, as shown in FIG. 7, the effective extension length of the
如此设置,在磁控元件绕其旋转中心P旋转过程中,闭合的等离子体路径13对应扫过靶材的部分半径区域,非闭合的等离子体路径23对应扫过靶材的整个直径区域,闭合的等离子体路径13和非闭合的等离子体路径23共同对应扫过靶材的整个直径区域,从而实现了全靶腐蚀,提高了靶材的利用率;同时还避免了现有技术中因先腐蚀靶材的边缘区域再腐蚀其中心区域所导致的靶材中心区域所对应的晶片区域出现颗粒的问题,从而提高了溅射工艺的质量和产品良率;同时,相对于现有技术中磁控元件对应在靶材的半径区域只设置有闭合等离子体路径的情况,图3中的磁控元件由于对应在靶材的半径区域既设置有闭合的等离子体路径13,又设置有非闭合的等离子体路径23,且二者在磁控元件旋转过程中扫过的区域只有部分重合,所以使闭合的等离子体路径13的面积相对减小,在靶材上施加直流电源的情况下,面积的减小能提高闭合的等离子体路径13作用到靶材上的功率密度,从而提高了
靶材的离化率,以及提高了晶片上通孔的填充效果。So, during the rotation of the magnetron about its center of rotation P, the
本实施例中磁控元件的其他结构与实施例1-3中的任意一个相同,此处不再赘述。Other structures of the magnetron component in this embodiment are the same as those in any of Embodiments 1-3, and are not described herein again.
实施例1-4的有益效果:实施例1-4中所提供的磁控元件,通过使闭合的等离子体路径和非闭合的等离子体路径至少对应位于靶材的中心到靶材的边缘的半径区域,且闭合的等离子体路径在靶材径向上的有效延伸长度和非闭合的等离子体路径在靶材径向上的有效延伸长度之和大于等于靶材的半径,不仅能够实现靶材的全靶腐蚀,提高靶材的利用率;而且能够避免靶材的中心区域所对应的晶片区域出现颗粒,提高磁控溅射工艺的质量和产品良率;同时,在靶材上施加直流电源的情况下,由于闭合的等离子体路径面积的减小,能提高闭合的等离子体路径作用到靶材上的功率密度,从而提高了靶材的离化率,以及提高了晶片上通孔的填充效果。Advantages of Embodiments 1-4: The magnetron elements provided in Embodiments 1-4 are configured such that the closed plasma path and the non-closed plasma path correspond at least to a radius from the center of the target to the edge of the target The region, and the effective extension length of the closed plasma path in the radial direction of the target and the effective extension length of the non-closed plasma path in the radial direction of the target are greater than or equal to the radius of the target, and not only the full target of the target can be achieved Corrosion, improve the utilization of the target; and avoid particles in the wafer area corresponding to the central area of the target, improve the quality of the magnetron sputtering process and product yield; and, at the same time, apply DC power to the target Due to the reduced area of the closed plasma path, the power density of the closed plasma path acting on the target can be increased, thereby increasing the ionization rate of the target and improving the filling effect of the via holes on the wafer.
实施例5:Example 5:
本实施例提供一种磁控溅射装置,如图8所示,包括靶材7,还包括实施例1-4任意一个中的磁控元件15,磁控元件15设置在靶材7的正上方;磁控溅射装置还包括射频电源16和/或直流电源17,及其控制元件18,射频电源16和/或直流电源17连接至靶材7,控制元件18连接射频电源16和/或直流电源17,控制元件18用于控制射频电源16和/或直流电源17为靶材7提供溅射功率。The present embodiment provides a magnetron sputtering apparatus, as shown in FIG. 8, comprising a target 7, and further comprising a
其中,控制元件18控制射频电源16和直流电源17交替施加到靶材7上,以便为靶材7提供溅射功率。在射频电源16的作用下,因为闭合的等离子体路径和非闭合的等离子体路径至少对应位于靶材7的中心到靶材7的边缘的半径区域,且闭合的等离子体路径在靶材7径向上的有效延伸长度和非闭合的等离子体路径在靶材7径向上的有效延
伸长度之和大于等于靶材7的半径,能使靶材7的表面腐蚀更加均匀,实现全靶腐蚀,且靶材利用率较高,同时还能提高靶材7的离化率;在直流电源17的作用下,因为闭合磁控管的闭合等离子体路径面积相对减小,提高了闭合的等离子体路径作用到靶材7上的功率密度,从而提高了靶材7的离化率,而且还提高了晶片19表面的通孔填充效果。射频电源16和直流电源17交替作用于靶材7,即可在实现全靶腐蚀,并提高靶材利用率;同时还能提高靶材7的离化率,获得较好的通孔填充效果。Therein, the
本实施例中,射频电源的频率范围为400k-60MHz。优选射频电源的频率为400kHz、2MHz、13.56MHz、40MHz或60MHz。In this embodiment, the frequency range of the radio frequency power source is 400k-60MHz. Preferably, the frequency of the radio frequency power source is 400 kHz, 2 MHz, 13.56 MHz, 40 MHz or 60 MHz.
实施例5的有益效果,实施例5所提供的磁控溅射装置,通过采用实施例1-4任意一个中的磁控元件,不仅提高了金属靶材的离化率,而且实现了全靶腐蚀。Advantageous Effects of Embodiment 5, the magnetron sputtering apparatus provided in Embodiment 5, by using the magnetron element of any of Embodiments 1-4, not only improves the ionization rate of the metal target but also realizes the total target corrosion.
可以理解的是,以上实施方式仅仅是为了说明本发明的原理而采用的示例性实施方式,然而本发明并不局限于此。对于本领域内的普通技术人员而言,在不脱离本发明的精神和实质的情况下,可以做出各种变型和改进,这些变型和改进也视为本发明的保护范围。 It is to be understood that the above embodiments are merely exemplary embodiments employed to explain the principles of the invention, but the invention is not limited thereto. Various modifications and improvements can be made by those skilled in the art without departing from the spirit and scope of the invention. These modifications and improvements are also considered to be within the scope of the invention.
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| CN201610779067.9A CN107799375B (en) | 2016-08-30 | 2016-08-30 | A kind of magnetic control element and magnetic control sputtering device |
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| CN111809157B (en) * | 2020-07-17 | 2022-11-25 | 北京北方华创微电子装备有限公司 | Semiconductor process equipment and magnetron mechanism thereof |
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