Abstract:
There is disclosed a manufacturing method of a phase shift mask blank in which dispersions of phase angle and transmittance among blanks can be reduced as much as possible and yield is satisfactory. In the manufacturing method of the phase shift mask blank, a process of using a sputtering method to continuously form a thin film on a transparent substrate comprises: successively subjecting a plurality of substrates to a series of process of supplying the transparent substrate into a sputtering chamber, forming the thin film for forming a pattern in the sputtering chamber, and discharging the transparent substrate with the film formed thereon from the sputtering chamber; supplying and discharging the transparent substrate substantially at a constant interval; and setting a film formation time to be constant among a plurality of blanks.

Description:
This application is a continuation of copending U.S. application Ser. No. 10/821,508 filed Apr. 9, 2004 now U.S. Pat. No. 7,282,121 which is a divisional of U.S. application Ser. No. 09/952,445 filed Sep. 12, 2001 (now U.S. Pat. No. 6,783,634 issued Aug. 31, 2004). 
    
    
     BACKGROUND OF THE INVENTION 
     i) Field of the Invention 
     The present invention relates to a manufacturing method and apparatus of a phase shift mask blank which is suitable particularly for ArF or F 2  excimer laser. 
     ii) Description of the Related Art 
     In recent years, it has been clarified that high resolution and focus depth are two important properties required for photolithography but are in a contradictory relation with each other, and that a practical resolution cannot be enhanced only by high NA and short wavelength of a lens of an exposure apparatus (Monthly Semiconductor World 1990.12, Applied Physics Vol. 60, November, 1991, and the like). 
     Under such situation, phase shift lithography has been noted as the next-generation photolithography technique, and partially brought to practical use. The phase shift lithography is a method for enhancing the resolution of photolithography by change only of a mask without changing an optical system. When a phase difference is applied between exposure lights transmitted through the photo mask, mutual interference of the transmitted lights can be utilized to rapidly enhance the resolution. 
     The phase shift mask is a mask for using light strength information together with phase information. Various types of the masks are known such as Levenson type, auxiliary pattern type, and self-matching type (edge emphasizing type). These phase shift masks have a complicated constitution and requires a high degree of manufacturing technique as compared with the conventional photo mask which has only the light strength information. 
     In recent years, a so-called halftone type phase shift mask has been developed as one of the phase shift masks. 
     In the halftone phase shift mask, a light semi-transmission section has two functions: a shield function of substantially shielding the exposure light; and a phase shift function of shifting (usually reversing) a light phase. Therefore, it is unnecessary to separately form a shield film pattern and phase shift film pattern. This type of phase shift mask is simple in constitution and easy in manufacturing. 
     In the halftone phase shift mask, a mask pattern is processed by a dry etching process. However, in a method of realizing the shield function and phase shift function by separate layers, a high degree of control is necessary for both the layer having the shield function and the layer having the phase shift function in order to obtain a satisfactory pattern shape. On the other hand, when a single-layer light semi-transmission portion having both the shield function and the phase shift function is constituted, a single etching process can be used. Therefore, a manufacturing process of the mask can be simplified, and a satisfactory pattern shape can easily be obtained. 
     For the halftone phase shift mask, as shown in  FIG. 10 , a mask pattern formed on a transparent substrate  100  is constituted of a light transmission portion (transparent substrate exposed portion)  200  for transmitting a light which is strong enough to substantially contribute to exposure, and a light semi-transmission portion (shield and phase shifter portion)  300  for transmitting a light which is not strong enough to substantially contribute to the exposure ( FIG. 10A ). Additionally, the phase of the light transmitted to the light semi-transmission portion is shifted, and the light semi-transmission portion is brought to a substantially reversed relation with respect to the phase of the light transmitted through the light transmission portion ( FIG. 10B ). The lights transmitted in the vicinity of a boundary between the light semi-transmission portion and the light transmission portion and turned to the opposite portions by diffraction phenomenon cancel each other. Thereby, light strength in the boundary is substantially set to zero, and contrast, that is, resolution of the boundary is enhanced ( FIG. 10C ). 
     Additionally, the light semi-transmission portion or film (phase shift layer) in the halftone phase shift mask or blank needs to indicate a required optimum value with respect to both transmittance and phase shift amount. Concretely, (1) the transmittance in exposure wavelength of i-ray, KrF excimer laser, ArF excimer laser, or the like can be adjusted in a range of 3 to 20%, (2) a phase angle can be adjusted usually to a value in the vicinity of 180° in the exposure wavelength, and (3) the transmittance needs to be usually testable in a range of 65% or less in test wavelengths such as 257 nm, 266 nm, 364 nm, and 488 nm. 
     However, with shortening of the wavelength of laser for use in exposure to ArF excimer laser (193 nm) from i-ray (365 nm) and KrF excimer laser (248 nm), the following problem is generated in the conventional halftone phase shift mask and the manufacturing method of the mask. 
     That is, in mass production of the phase shift mask blanks, when there are dispersions of the phase angle and transmittance among the blanks or in the plane, yield is bad. Particularly in the mask blanks for the short wavelength of ArF or F 2  excimer laser, the dispersions of the phase angle and transmittance among the blanks and in the plane in the conventional mask blanks for i-ray and KrF excimer laser are large, and the yield is bad. Therefore, the mask blanks cannot be applied as they are. 
     SUMMARY OF THE INVENTION 
     The present invention has been developed under the aforementioned background, and a first object thereof is to provide a manufacturing method of a phase shift mask blank in which dispersions of a phase angle and transmittance among blanks can be reduced as much as possible and a yield is satisfactory. 
     Moreover, a second object is to provide a manufacturing method of the phase shift mask blank in which the dispersions of the phase angle and transmittance in a plane of the blanks can be reduced as much as possible and the yield is satisfactory. 
     Furthermore, a third object is to provide a manufacturing apparatus of the phase shift mask blank in which the dispersions of the phase angle and transmittance among the blanks can be reduced as much as possible and which can be manufactured with a satisfactory yield. 
     Additionally, a fourth object is to provide a manufacturing apparatus of the phase shift mask blank in which the dispersions of the phase angle and transmittance in the plane of the blanks can be reduced as much as possible and which can be manufactured with the satisfactory yield. 
     To achieve the aforementioned objects, the present invention has the following constitutions. (Constitution 1) A method of continuously manufacturing a plurality of phase shift mask blanks each having at least a phase shift film on a transparent substrate, the method comprising a step of: 
     using a sputtering method to continuously form the phase shift film on the transparent substrate, 
     wherein a dispersion of a phase angle of the phase shift film among the plurality of blanks is within ±2°.
     (Constitution 2) A method of continuously manufacturing a plurality of halftone phase shift mask blanks each having at least a light semi-transmission film on a transparent substrate, the method comprising a step of:   

     using a sputtering method to continuously form the light semi-transmission film on the transparent substrate, 
     wherein dispersions of a phase angle and a transmittance of the light semi-transmission film among the plurality of halftone phase shift mask blanks are within ±2° and within ±4%, respectively.
     (Constitution 3) A method of continuously manufacturing a plurality of photo mask blanks each having at least a thin film for forming a pattern on a transparent substrate, the method comprising a step of:   

     using a sputtering method to continuously form the thin film on the transparent substrate, 
     wherein the step of using the sputtering method to continuously form the thin film on the transparent substrate comprises steps of: successively subjecting a plurality of substrates to a series of processes of supplying the transparent substrate into a sputtering chamber, forming the thin film for forming the pattern in the sputtering chamber, and discharging the transparent substrate with the film formed thereon from the sputtering chamber; and supplying and discharging the transparent substrate substantially at a constant interval in order to set a film formation time to be constant among the plurality of blanks, and 
     at least first to fifth photo mask blanks after start of film formation are excluded from the photo mask blanks obtained in the step.
     (Constitution 4) The manufacturing method according to constitution 3 wherein the thin film for forming the pattern is a phase shift film, and the photo mask blank is a phase shift mask blank.   (Constitution 5) The manufacturing method according to constitution 3 wherein the thin film for forming the pattern is a light semi-transmission phase shift film, and the photo mask blank is a halftone phase shift mask blank.   (Constitution 6) A manufacturing method of a photo mask blank having a thin film for forming at least a pattern on a transparent substrate, the method comprising steps of:   

     rotating the substrate; sputtering a target disposed opposite to a position whose center axis deviates from a center axis of the substrate; and forming the thin film.
     (Constitution 7) The manufacturing method according to constitution 6 wherein the target and the substrate are disposed so that opposite surfaces of the substrate and target form a predetermined angle therebetween.   (Constitution 8) The manufacturing method according to constitution 6 or 7 wherein the step of forming the film comprises a step of rotating the transparent substrate integer times between start of film formation and end of the film formation.   (Constitution 9) The manufacturing method according to any one of constitutions 6 to 8 wherein the thin film for forming the pattern is a phase shift film, and the photo mask blank is a phase shift mask blank.   (Constitution 10) The manufacturing method according to constitution 9 wherein a dispersion of a phase angle of the phase shift film in a plane is within ±2°.   (Constitution 11) The manufacturing method according to any one of constitutions 6 to 10 wherein the thin film for forming the pattern is a light semi-transmission phase shift film, and the photo mask blank is a halftone phase shift mask blank.   (Constitution 12) The manufacturing method according to constitution 11 wherein a dispersion of a phase angle of the light semi-transmission phase shift film in a plane is within ±2° and a dispersion of a transmittance in the plane is within ±4%.   (Constitution 13) The manufacturing method according to constitution 11 or 12 wherein the light semi-transmission phase shift film is formed by sputtering the target formed of a metal and silicon in an atmosphere containing nitrogen, contains the metal, silicon and nitrogen as main constituting components, and is formed so that a content of nitrogen in the light semi-transmission phase shift film is larger than a content of silicon.   (Constitution 14) A photo mask manufactured by patterning the thin film in the photo mask blank according to any one of constitutions 1 to 13.   (Constitution 15) A pattern transfer method of using the photo mask according to constitution 14 to transfer a pattern.   (Constitution 16) A manufacturing apparatus of a photo mask blank, comprising at least: a load lock mechanism for introducing substrates one by one; a substrate conveying mechanism for introducing the substrates one by one to a sputtering chamber from a load lock chamber at a constant interval; the sputtering chamber for forming a film on the substrate; and an unload lock mechanism for discharging the substrates one by one from the sputtering chamber.   (Constitution 17) A manufacturing apparatus of a photo mask blank, comprising: a substrate laying base having a rotation mechanism; and a target disposed opposite to a position whose center axis deviates from a center axis of a substrate.   (Constitution 18) The manufacturing apparatus according to constitution 17 wherein the target and the substrate are disposed so that opposite surfaces of the substrate and target form a predetermined angle therebetween.   (Constitution 19) The manufacturing apparatus of the halftone phase shift mask blank according to any one of constitutions 16 to 18, comprising: means for detecting a rotation position of the substrate; and means for turning OFF electric discharge (ending film formation) when the substrate rotated integer times after turning ON the electric discharge (starting the film formation) is allowed to reach the same rotation angle position as a rotation angle position for turning ON the electric discharge.   

     According to the constitutions 1 and 2, the dispersion of the phase angle of the phase shift film among the phase shift mask blanks is within ±2°, or the dispersions of the phase angle and transmittance of the light semi-transmission film among the halftone phase shift mask blanks are within ±2° and within ±4%, respectively. Therefore, the phase shift mask for a short wavelength of ArF or F 2  excimer laser can be manufactured in a mass and can practically be used. When this range is exceeded, it is difficult to mass-manufacture and practically use the phase shift mask for the short wavelength of ArF or F 2  excimer laser. 
     Additionally, even in the present situation, the masks for KrF excimer laser can practically be used. However, smaller dispersions of the phase angle and transmittance of the light semi-transmission film among the mask blanks are preferable. Therefore, the invention according to the constitutions 1 and 2 can also be applied to the phase shift mask blank for the KrF excimer laser. 
     According to the constitutions 3 to 5, the dispersions of film properties (transmittance (OD), film thickness, and the like) in the photo mask blank among the blanks can be suppressed. It is particularly possible to realize the manufacturing of the phase shift mask in which the dispersion of the phase angle of the phase shift film among the phase shift mask blanks is within ±2°, or the dispersions of the phase angle and transmittance of the light semi-transmission film among the halftone phase shift mask blanks are within ±2° and within ±4%, respectively. 
     According to the constitutions 6 to 12, the dispersions of the film properties (transmittance (OD), film thickness, and the like) in the plane in the photo mask blank can be suppressed. It is particularly possible to realize the phase shift mask blank in which the dispersion of the phase angle of the phase shift film in the plane of the phase shift mask blank is within ±2°, or the dispersions of the phase angle and transmittance of the light semi-transmission film in the plane of the halftone phase shift mask blank are within ±2° and within ±4%, respectively. Therefore, the phase shift mask for the short wavelength of the ArF or F 2  excimer laser can be brought to practical use. When this range is exceeded, it is difficult to practically use the phase shift mask for the short wavelength of the ArF or F 2  excimer laser. 
     Additionally, even in the present situation, the mask for the KrF excimer laser can practically be used. However, smaller dispersions of the phase angle and transmittance of the light semi-transmission film in the plane of the mask blank are preferable. Therefore, the invention according to the constitutions 6 and 12 can also be applied to the phase shift mask blank for the KrF excimer laser. 
     According to the constitution 13, the dispersion of the phase angle can further be suppressed. 
     According to the constitution 14, it is possible to obtain the photo mask in which the dispersion among the masks or in the mask plane is suppressed. 
     According to the constitution 15, a superior fine pattern processing can be realized. 
     According to the apparatus of the constitutions 16 to 19, the dispersions of the film properties (transmittance (OD), film thickness, and the like) in the photo mask blank among the blanks or in the plane can be suppressed. It is particularly possible to realize the manufacturing of the phase shift mask blank in which the dispersion of the phase angle of the phase shift film among the phase shift mask blanks or in the plane is within ±2°, or the dispersions of the phase angle and transmittance of the light semi-transmission film among the halftone phase shift mask blanks or in the plane are within ±2° and within ±4%, respectively. 
     The present invention will be described hereinafter in more detail. 
     As a result of pursuing of researches in order to achieve the aforementioned objects, the following has been obtained. 
     In the halftone phase shift mask, it is functionally important to adjust the phase angle and transmittance of the light semi-transmission portion and obtain desired values. For an error range of the phase angle and transmittance, fluctuation among blanks (dispersion among blanks), and in-blank distribution (in-plane dispersion) require to be about ±2°, and ±4°, respectively. Examples of a factor which changes the phase angle and transmittance include: (1) film formation procedure of the light semi-transmission film; (2) property of a sputtering apparatus for forming the light semi-transmission film, and (3) material of the light semi-transmission film. 
     (1) The film formation procedure for forming the light semi-transmission film will be described in detail. 
     To determine a film formation time of the light semi-transmission film at the start and end of sputtering, when an interval between the sputtering end and the next sputtering start is set to be constant, the fluctuations of the phase angle and transmittance among blanks (dispersion among blanks) are effectively within ±2°, and within ±4° (reproducibility is effectively enhanced). In sputtering phenomenon, temperature and surface state of a target or a shield are changed, and a degree of vacuum in a vacuum tank is also changed. In a conventional intermittent sputtering in which the interval between the sputtering end and the next sputtering start is not constant, the state of the target or the shield changes every moment. However, in the present invention, when the interval between the sputtering end and the next sputtering start, and sputtering time and condition are always set to be constant, the fluctuations of the phase angle and transmittance are reduced on and after forming five to ten blanks. That is, when the light semi-transmission film is continuously formed at a constant interval, and fifth to tenth blanks formed after the start are excluded, it is possible to steadily manufacture the halftone phase shift mask blanks having less fluctuations of the phase angle and transmittance. Concretely, it is possible to steadily manufacture the halftone phase shift mask blanks in which the dispersions of the phase angle and transmittance among the blanks are within ±2°, and within ±4°, respectively. 
     In order to realize this process, as shown in  FIG. 1 , a load lock mechanism needs to be disposed which can constantly hold a sputtering vacuum tank (sputtering chamber) in a high vacuum state. In this apparatus constitution, introduction of the substrate to the sputtering chamber from a load lock chamber is continuously performed at a constant interval. For this, the load lock mechanism for introducing the substrates one by one needs to be disposed. Additionally, a capacity of the load lock chamber needs to be designed such that the substrate is continuously introduced to the sputtering chamber from the load lock chamber at the constant interval. 
     In the conventional manufacturing apparatus of the halftone phase shift mask blanks, about ten substrates are set in the load lock chamber from a viewpoint of throughput. In this system (or an in-line system), since the capacity of the load lock chamber is large, much time is required for setting the inside of the load lock chamber at a predetermined degree of vacuum, and film formation is not performed in the sputtering chamber during this time. Therefore, when the film formation all ends and the next cassette is set in the load lock chamber in order to perform the film formation, the substrate is not continuously supplied to the sputtering chamber at the constant interval. In this case, when the substrate is not continuously introduced to the sputtering chamber at the constant interval, the film formation in the sputtering chamber is not stabilized, the dispersions of the phase angle and transmittance among the blanks are large in the first five to ten blanks, and yield is disadvantageously bad. 
     In  FIG. 1 , a valve  12  for separating a load lock chamber  11  from the atmosphere, and a valve  14  for separating the load lock chamber  11  from a sputtering chamber  13  are attached to the load lock chamber  11 . The load lock chamber  11  has a sheets system in which the substrate can continuously be introduced to the sputtering chamber at the constant interval as described above. The load lock chamber is also designed to have a predetermined capacity. The sputtering chamber  13  has a function equivalent to a function of the vacuum tank in which sputtering is performed as described later and shown in  FIG. 2 . When the substrate is introduced to the sputtering chamber  13  by a robot arm, a conveying chamber  15  may be disposed between the sputtering chamber  13  and the load lock chamber  11 . For a robot arm  19 , when an arm  19   a  opens/closes in a direction A, a hand  19   b  can move in a direction B. Moreover, the robot arm  19  can rotate in a direction C. The robot arm  19  is also constituted to be movable in a vertical direction with respect to a sheet surface. Furthermore, in order to enhance throughput of film formation, an unload lock chamber  16  having a constitution similar to that of the load lock chamber  11  may be added. An example of the process for forming the light semi-transmission film on the transparent substrate will be described with reference to  FIG. 1 . 
     1) After the valve  14  is closed, the inside of the load lock chamber  11  is set to be in an atmospheric pressure through venting. 
     2) The valve  12  is opened and one transparent substrate is introduced into the load lock chamber  11 . 
     3) The valve  12  is closed and the load lock chamber  11  is evacuated. 
     4) After the load lock chamber  11  reaches a predetermined degree of vacuum, the valve  14  is opened and the transparent substrate is moved to the sputtering chamber  13 . 
     5) A constitution described later and shown in FIG.  2  is used to form the light semi-transmission film in the sputtering chamber  13 . 
     6) After the end of formation of the light semi-transmission film, a valve  17  is opened and the substrate is moved to the unload lock chamber  16 . In this case, it is necessary to evacuate the unload lock chamber  16  to the predetermined degree of vacuum. 
     7) After the valve  17  is closed, the unload lock chamber is brought to the atmospheric pressure through venting. 
     8) A valve  18  is opened and the substrate is removed. 
     From when the light semi-transmission film is formed in the sputtering chamber  13 , until the substrate is moved to the unload lock chamber  16  from the sputtering chamber  13 , steps 1) to 4) are ended, and the next substrate is allowed to be on standby in the load lock chamber  11 . When the previous film formation ends, and the substrate is moved to the unload lock chamber  16  from the sputtering chamber  13 , the transparent substrate having been on standby is moved to the sputtering chamber  13 , and the light semi-transmission film is successively formed. By this process, it is possible to successively (continuously) form the light semi-transmission film at the constant interval excluding a time of maintenance of the apparatus. 
     (2) The property of the sputtering apparatus for forming the light semi-transmission film will next be described in detail. Since a gas pressure during the sputtering for forming the light semi-transmission film, output of a sputtering DC power supply, and a sputtering time directly influence the transmittance and phase angle, precision of a gas flow rate controller, DC power supply or another apparatus needs to be enhanced. It is also necessary to enhance the precision of a set signal emitted from the controller. Since the gas pressure during the sputtering is also influenced by exhaust conductance of the apparatus, a mechanism able to accurately determine an open degree of an exhaust port valve and a position of the shield is also necessary. A concrete control precision will be described later. 
     Moreover, for a film containing silicon nitride, moisture generated from an inner wall of the vacuum tank, or another gas largely influences an optical property of the film. It is therefore necessary to dispose a pump which can sufficiently evacuate the vacuum tank, and a mechanism which can bake the inner wall of the vacuum tank. The degree of vacuum in the vacuum tank needs to be about 2×10 −5  pa or less at a film formation speed of 10 nm/min, and 1×10 −5  pa or less at a film formation speed of 5 nm/min. 
     Furthermore, in order to suppress the distributions of the phase angle and transmittance in the blanks (dispersions in the plane) within ±2° and ±4°, the transparent substrate needs to be rotated during the film formation. It is further necessary to rotate the transparent substrate integer times between the start and the end of the film formation while the film formation is performed. To this end, for example, the rotation angle position of the substrate of a time at which electric discharge is turned ON (start of film formation) is detected by a sensor for detecting the rotation angle position of the substrate. Furthermore, by this sensor, when the substrate rotates integer times and reaches the same rotation angle position as that of the ON time of the electric discharge, the electric discharge is turned OFF (film formation is ended). This mechanism needs to be disposed. 
     The distributions of the phase angle and transmittance in the plane also change with a positional relation between the substrate and the target. The positional relation between the target and the substrate will be described with reference to  FIG. 8 . 
     An offset distance (distance between a center axis of the substrate and a straight line passed through a center of the target and extended in parallel to the center axis of the substrate) is adjusted by an area in which the distributions of the phase angle and transmittance are to be secured. Generally in a large area in which the distributions are to be secured, a necessary offset distance is large. In order to realize the phase angle distribution within ±2° and transmittance distribution within ±4° in a 152 mm square substrate as in the present embodiment, the offset distance needs to be in a range of about 200 mm to 350 mm, and a preferable offset distance is in a range of 240 mm to 280 mm. 
     An optimum range of a vertical distance between the target and the substrate (T/S) changes with the offset distance. However, in order to realize the phase angle distribution within ± 2 ° and transmittance distribution within ±4° in the 152 mm square substrate, the vertical distance between the target and the substrate (T/S) needs to be about 200 mm to 380 mm, and preferable T/S is in a range of 210 mm to 300 mm. 
     A target inclination angle influences the film formation speed. In order to obtain a high film formation speed, the target inclination angle is appropriate in a range of 0° to 45°, and a preferable target inclination angle is in a range of 10° to 30°. 
       FIG. 9  shows upper and lower limits of T/S with which the phase angle distribution within ±2° and transmittance distribution within ±4° can be realized in the 152 mm square substrate with the change of the offset distance. 
     (3) The influence of the material of the light semi-transmission film on the phase angle and transmittance will next be described in detail. The phase angle and transmittance of the light semi-transmission film change with the film formation speed and degree of nitriding. The film formation speed and degree of nitriding are influenced by a nitrogen partial pressure during sputtering. However, when the light semi-transmission film is completely nitrided, the influence of the nitrogen partial pressure during sputtering is reduced. In a nitrided metal silicide film, a flow rate of nitrogen introduced during sputtering is adjusted so that a content of nitrogen measured by ESCA is larger than that of silicon. This can reduce the influence of a fluctuation of nitrogen partial pressure on the optical property. With this method, the distributions of the phase angle and transmittance in the plane can also be reduced. Additionally, when oxygen is added together with nitrogen during sputtering, the phase angle and transmittance are largely influenced by a fluctuation of a flow rate of oxygen. However, at least the influence of flow rate fluctuation of nitrogen can be reduced in the aforementioned method. 
     Additionally, examples of the photo mask blank in the constitution of the present invention include a shield film (chromium, a chromium compound containing oxygen, nitrogen, carbon, and the like in chromium, another chromium compound, and the like) in the photo mask, the phase shift film in the phase shift mask blank, and the like. 
     Moreover, the phase shift mask blank in the constitution of the present invention is not limited to the halftone phase shift mask blank. For a purpose of setting the dispersion of the phase angle within ±2°, the present invention can also be applied to the blank for manufacturing various types of the phase shift masks such as Levenson type, auxiliary pattern type, and self-matching type (edge emphasizing type). 
    
    
     
       BRIEF DESCRIPTION OF THE DRAWINGS 
         FIG. 1  is an explanatory view of transfer principle of a halftone phase shift mask. 
         FIG. 2  is a schematic view of a sputtering chamber in a DC magnetron sputtering apparatus used in an embodiment. 
         FIG. 3  is a graph showing dispersions of a phase angle and transmittance among blanks in the embodiment. 
         FIG. 4  is a graph showing dispersions of the phase angle and transmittance among the blanks in another embodiment. 
         FIG. 5  is a graph showing a relation between DC power and phase angle. 
         FIG. 6  is a graph showing a relation of a film formation time with the phase angle and transmittance. 
         FIG. 7  is a graph showing a relation between a nitrogen flow rate and phase angle. 
         FIG. 8  is a schematic diagram showing a positional relation between a target and a substrate. 
         FIG. 9  is a graph showing upper and lower limits of T/S with which a phase angle distribution within ±2° and a transmittance distribution within ±4° can be realized with a change of an offset distance. 
         FIG. 10  is a schematic diagram showing a sputtering apparatus of the present invention. 
     
    
    
     DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS 
     Examples of the present invention will be described hereinafter in further detail. 
     A DC magnetron sputtering apparatus described above with reference to  FIG. 1  was used to continuously form films of 200 halftone phase shift mask blanks for ArF excimer laser (193 nm) one by one at constant intervals. 
     Concretely, a mixed target (Mo:Si=8:92 mol %) of molybdenum (Mo) and silicon (Si) was used to form a nitrided thin film (film thickness of about 670 angstroms) of molybdenum and silicon (MoSiN) on a transparent substrate by reactive sputtering (DC sputtering) in a mixed gas atmosphere (Ar:N 2 =10%:90%, pressure: 0.1 Pa) of argon (Ar) and nitrogen (N 2 ). In this manner, the phase shift mask blank (film composition: Mo:Si:N=7:45:48) for ArF excimer laser (wavelength of 193 nm) was obtained. 
     Here, a sputtering chamber  13  in the DC magnetron sputtering apparatus shown in  FIG. 1  has a vacuum tank  1  as shown in  FIG. 2 . A magnetron cathode  2  and substrate holder  3  are disposed in the vacuum tank  1 . A sputtering target  5  bonded to a backing plate  4  is attached to the magnetron cathode  2 . In the example, oxygen-free steel is used in the backing plate  4 , and indium is used to bond the sputtering target  5  to the backing plate  4 . The backing plate  4  is directly or indirectly cooled by a water cooling mechanism. The magnetron cathode  2 , backing plate  4  and sputtering target  5  are electrically connected to one another. A transparent substrate  6  is attached to the substrate holder  3 . 
     Additionally, in a constitution of the apparatus used in the present example, the sputtering target  5  and substrate  6  in  FIG. 2  are arranged so that opposite surfaces of the substrate and target form a predetermined angle as shown in  FIG. 8 . In this case, an offset distance between the sputtering target and the substrate was set to 340 mm, a vertical distance between the target and the substrate (T/S) was 380 mm, and a target inclination angle was 15°. 
     The vacuum tank  1  is evacuated by a vacuum pump via an exhaust port  7 . An atmosphere in the vacuum tank reaches a degree of vacuum which does not influence a property of the formed film, a mixed gas containing nitrogen is then introduced via a gas introduction port  8 , a DC power supply  9  is used to apply a negative voltage to the magnetron cathode  2 , and sputtering is performed. The DC power supply  9  has an arc detecting function, and can monitor an electric discharge state during sputtering. A pressure inside the vacuum tank  1  is measured by a pressure gauge  10 . 
     A transmittance of a light semi-transmission film formed on the transparent substrate is adjusted by a type and mixture ratio of gases introduced via the gas introduction port  8 . When the mixed gas contains argon and nitrogen, the transmittance is increased by increasing a ratio of nitrogen. When a desired transmittance cannot be obtained by adjusting the ratio of nitrogen, oxygen is added to the mixed gas containing nitrogen, and the transmittance can further be increased. 
     A phase angle of the light semi-transmission film was adjusted by a sputtering time, and the phase angle in an exposure wavelength was adjusted to about 180°. 
     Evaluation of Dispersion Among Blanks 
     Dispersions of the phase angle and transmittance among the blanks were checked with respect to  200  phase shift mask blanks (size: 15.2 cm square) obtained as described above. Results are shown in  FIG. 3 . 
     As seen from  FIG. 3 , on and after the third blank, the halftone phase shift mask blanks whose dispersions of the phase angle and transmittance among the blanks are within ±2° and within ±4°, respectively, can steadily be manufactured. Additionally, it was confirmed also with respect to the 11-th blank to 200-th blank that the dispersions of the phase angle and transmittance among the blanks were within ±2° and within ±4°, respectively. In this case, yield is 100% with respect to the phase angle and transmittance. 
     Additionally, in Example 2, 200 blanks were prepared similarly as the aforementioned Example 1 except that the sputtering chamber was opened for maintenance midway (at 190-th blank), and the dispersions of the phase angle and transmittance among the blanks were checked. Results are shown in  FIG. 4 . 
     As seen from  FIG. 4 , with use of the apparatus of the present invention, the halftone phase shift mask blanks whose dispersions of the phase angle and transmittance among the blanks are within ±2° and within ±4°, respectively, can steadily be manufactured excluding first several blanks and five blanks immediately after opening the sputtering chamber. It is also seen that the yield is 100% with respect to the phase angle and transmittance. 
     Moreover, a conventional manufacturing apparatus in which about ten substrates were disposed in a load lock chamber, and an in-line type manufacturing apparatus were used to manufacture the halftone phase shift mask blanks. However, in either apparatus, it was difficult to suppress the dispersions of the phase angle and transmittance among the blanks within ±2° and within ±4°, respectively, and the yield was bad. 
     Moreover, in Example 1, the transparent substrate was rotated during film formation. Furthermore, the transparent substrate was rotated integer times from the start till the end of the film formation, while the film formation was performed. The dispersions of the phase angle and transmittance in a plane were checked. 
     As a result, it was confirmed that the halftone phase shift mask blanks having the dispersions of the phase angle and transmittance in the plane within ±2° and ±4°, respectively, can steadily be manufactured. 
     Furthermore, the following was seen in the aforementioned examples. 
     As shown in  FIG. 5 , in order to suppress the dispersion of the phase angle in a range of about 180° to about 172°, it is necessary to control a power of the DC power supply in a range of about 1.77 kW to about 1.825 kW (preferably in a range of about 1.82 kW to 1.81 kW in order to suppress the dispersion of the phase angle in a range of about 180° to about 178°). Therefore, it is necessary to suppress a fluctuation of the power of the DC power supply at a center value ±0.5%. 
     Similarly, as seen from  FIG. 6 , in order to suppress the dispersions of the phase angle and transmittance, it is necessary to control the film formation time in a range of about 560 seconds to about 615 seconds (preferably about 600 seconds to about 594 seconds in order to suppress the dispersion of the phase angle in a range of about 180° to about 178°). Therefore, it is necessary to suppress a fluctuation of the film formation time at a center value ±0.5%. 
     Similarly, as seen from  FIG. 7 , in order to suppress the dispersion of the phase angle, a flow rate of nitrogen introduced during sputtering is adjusted so that a content of nitrogen measured by ESCA in a nitrided metal silicide film is larger than a content of silicon, and an influence of a fluctuation of nitrogen partial pressure on an optical property is reduced. For this purpose, it is necessary to control the flow rate of nitrogen in a range of about 35 sccm or more (preferably about 35 sccm to about 35.5 sccm in order to suppress the dispersion of the phase angle in a range of about 180° to about 178°). Additionally, the nitrogen flow rate with which the influence of the fluctuation of nitrogen partial pressure on the optical property can be reduced changes with an exhaust property and DC power of the apparatus. 
     Evaluation of Dispersion in Plane 
     The dispersions of the phase angle and transmittance in a plane were checked with respect to one of the phase shift mask blanks obtained as described above. 
     As a result, the dispersion of the phase angle was within ±0.8° (average value of 179.5°, range of 178.8° to 180.3°) in a range of 132 mm square excluding a substrate peripheral portion of 10 mm. Moreover, the dispersion of the transmittance was within ±1.3% (average value of 6.16%, range of 6.08% to 6.23%). 
     Additionally, for comparison, when the film formation was performed at an offset distance of 340 mm, a vertical distance between the target and the substrate (T/S) of 400 mm, and a target inclination angle of 15°, the dispersion of the phase angle was ±3.5° (average value of 178.8°, range of 175.3° to 181.7°). Moreover, the dispersion of the transmittance was ±8% (average value of 6.07%, range of 5.83% to 6.56%). 
     Furthermore, for comparison, when the target was disposed opposite to the substrate (offset distance of 0 mm, and target inclination angle of 0°), the dispersion of the phase angle was ±2.7° (average value of 179.8°, range of 177.1° to 182.0°) in a target diameter of 16 inchesφ. Moreover, the dispersion of the transmittance was ±4.2% (average value of 6.19%, range of 6.00% to 6.45%). 
     With a larger offset distance, it is easier to reduce the dispersion in the plane. However, when the offset distance is excessively large, a capacity of the vacuum tank increases, evacuation property is therefore deteriorated, and further a film formation speed is lowered. 
     Additionally, the dispersion in the plane was evaluated by judging whether or not both a maximum point (plus value) and minimum point (minus value) with respect to the average value (center value) were within a defined range. 
     The preferred examples of the present invention have been described above, but the present invention is not limited to the aforementioned examples. 
     For example, molybdenum was used as a metal constituting the light semi-transmission film, but this is not limited, and zirconium, titanium, vanadium, niobium, tantalum, tungsten, nickel, palladium, and the like can be used. 
     Moreover, the target of molybdenum and silicon was used as the target containing metal and silicon, but this is not limited. In the target containing metal and silicon, molybdenum is particularly superior among the aforementioned metals in controllability of the transmittance and in that a target density increases and particles in the film can be reduced with use of the sputtering target containing metal and silicon. Titanium, vanadium, and niobium are superior in resistance to an alkaline solution, but slightly inferior to molybdenum in the target density. Tantalum is superior in the resistance to the alkaline solution and target density, but slightly inferior to molybdenum in the controllability of transmittance. Tungsten has properties similar to those of molybdenum, but is slightly inferior to molybdenum in an electric discharge property during sputtering. Nickel and palladium are superior in the optical property and resistance to the alkaline solution, but dry etching is slightly difficult to perform. Zirconium is superior in the resistance to the alkaline solution, but inferior to molybdenum in the target density, and the dry etching is slightly difficult to perform. Considering these, molybdenum is most preferable at present. Molybdenum is also preferable for a nitrided molybdenum and silicon (MoSiN) thin film (light semi-transmission film) in superior chemicals resistance such as acid resistance and alkali resistance. 
     Moreover, in order to obtain the thin film of a composition in which electric discharge stability is secured during film formation and various properties of the phase shift mask are satisfied, the target containing 70 to 95 mol % of silicon, and metal is preferably subjected to DC magnetron sputtering in the atmosphere containing nitrogen. Thereby, the light semi-transmission film containing nitrogen, metal and silicon is preferably formed. 
     When the content of silicon in the target is larger than 95 mol %, a voltage is not easily applied (electricity is not easily passed) to a target surface (erosion portion) in the DC sputtering, and the electric discharge becomes unstable. Moreover, when the content of silicon is less than 70 mol %, the film constituting a light semi-transmission portion with a high transmittance cannot be obtained. Furthermore, electric discharge stability is further enhanced by combination of the nitrogen gas with the DC sputtering. 
     Additionally, the electric discharge stability during film formation also influences film quality. When the electric discharge stability is superior, the light semi-transmission film with a satisfactory film quality is obtained. 
     As described above, according to the present invention, there can be provided the manufacturing method of the phase shift mask blank in which the dispersions of phase angle and transmittance among blanks can be reduced as much as possible and the yield is satisfactory. 
     Moreover, there can be provided the manufacturing method of the phase shift mask blank in which the dispersions of phase angle and transmittance in the plane of the blanks can be reduced as much as possible and the yield is satisfactory. 
     Furthermore, there can be provided the manufacturing apparatus of the phase shift mask blank in which the dispersions of phase angle and transmittance among the blanks can be reduced as much as possible and which can be manufactured with the satisfactory yield. 
     Additionally, there can be provided the manufacturing apparatus of the phase shift mask blank in which the dispersions of phase angle and transmittance in the plane of the blanks can be reduced as much as possible and which can be manufactured with the satisfactory yield.