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JPH031379B2 - - Google Patents
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JPH031379B2 - - Google Patents

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Publication number
JPH031379B2
JPH031379B2 JP9256886A JP9256886A JPH031379B2 JP H031379 B2 JPH031379 B2 JP H031379B2 JP 9256886 A JP9256886 A JP 9256886A JP 9256886 A JP9256886 A JP 9256886A JP H031379 B2 JPH031379 B2 JP H031379B2
Authority
JP
Japan
Prior art keywords
pulsed
evaporation
molecular beam
vapor deposition
gas
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired
Application number
JP9256886A
Other languages
Japanese (ja)
Other versions
JPS62250167A (en
Inventor
Shoichi Nozoe
Nobuyuki Nishinomya
Kimyuki Jinno
Hitoshi Sato
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
National Institute of Advanced Industrial Science and Technology AIST
Original Assignee
Agency of Industrial Science and Technology
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Agency of Industrial Science and Technology filed Critical Agency of Industrial Science and Technology
Priority to JP9256886A priority Critical patent/JPS62250167A/en
Publication of JPS62250167A publication Critical patent/JPS62250167A/en
Publication of JPH031379B2 publication Critical patent/JPH031379B2/ja
Granted legal-status Critical Current

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Description

【発明の詳細な説明】[Detailed description of the invention]

〔発明の技術分野〕 本発明は改良された真空蒸着方法およびその装
置に関し、より詳細には蒸着材の気体をパルス状
に真空蒸着装置に供給する真空蒸着方法とその装
置に関する。 〔従来技術〕 従来、化成蒸着法と呼ばれる蒸着方法では、
10-3〜10T-4orr程度の比較的圧力の高い蒸着材
の気体を蒸着装置中の蒸着容器中に導入して、ま
たは導入しながら減圧下で被蒸着材に蒸着材を蒸
着していた。 ところが、かかる化成蒸着方法では、蒸着材の
気体の蒸着容器への導入および停止に時間がかか
り、蒸着条件の精密な制御が難であつた。 しかも蒸着材気体の導入によつて蒸着容器の平
均的真空度が低下するので、蒸着膜をその都度分
析することが不可能であつた。 〔発明の目的〕 本発明は上記従来の欠点を解消し、蒸着材の気
体流の真空蒸着装置への供給を高速で遮断するこ
とができ、蒸着条件の精密な制御が可能であり、
しかも蒸着中の蒸着膜を基の場で分析することが
できる蒸着方法とその装置を提供することを目的
とするものである。 〔発明の構成〕 上記目的を達成する本発明のパルス分子線蒸着
方法は、真空蒸着装置内の被蒸着材上に蒸着材の
気体流をパルス状で噴射させて該被蒸着材に前記
蒸着材を蒸着させることを特徴とするものであ
る。 また本発明のパルス分子線蒸着装置は、パルス
分子線発生装置と真空蒸着装置との組合せからな
り、該パルス分子線発生装置が蒸着材の気体を収
容する容器と、該容器の噴出口の内側に設けた噴
出気体流の高速遮断手段、および該手段と連結し
たパルス電圧発生源とからなることを特徴とする
ものである。 まず、本発明のパルス分子線蒸着装置を図面に
もとづき説明する。 第1図は本発明において真空蒸着装置と組合さ
れるパルス分子線発生装置の態様を示す。 パルス分子線発生装置1は蒸着材の気体を収容
するる容器2と、この容器2に形成された気体流
噴出口3の内側に設けた噴出気体流の高速遮断手
段4およびこの高速遮断手段4と連結したパルス
電圧発生源5とから構成され、容器2内には通常
では10気圧以下の蒸着材気体が収容され、この気
体2は弁8および管路9を経て導入される。 ここで本発明における気体流とは、通常の気体
の流れの他に、気相の中を移動することが可能な
あらゆる形態のもの、例えば金属蒸気、金属クラ
スター、超微粒子、イオンのようなものの流れを
も含むものである。 従つて、この意味において本発明は分子線に限
定されるものではなく、広い範囲の気相中のビー
ムを対象とするものである。 噴出気体流の高速遮断手段4は、例えば圧電体
素子6、または電磁ソレノイド素子、或いはこれ
らと同様の作用を有する素子と、この素子6の先
端に接着された気体流噴出口閉鎖部材7とから形
成されている。 気体噴出口閉鎖部材7は、高硬度材料、例えば
タングステンカーバイドあるいは樹脂、例えばバ
イトンからなり、気体噴出口3に接する側は表面
が平滑に研摩されているる。 この閉鎖部材7は、通常は容器2内に収容され
た蒸着材の気体によつて噴出口3に押し付けられ
ていて、噴出口3からの蒸着材気体の漏洩を防い
でいる。 パルス電圧発生源からは、圧電子素子6に80〜
140Vのパルス電圧が印加され、圧電体素子6は
収縮して、容器2に収容されていた蒸着材気体が
噴出口3から噴出する。 パルス電圧の印加が中止すると、圧電体素子6
の形状が元に復し、閉鎖部材7が再び噴出口3に
接して噴出口3が閉鎖される。 このように圧電体素子6へのパルス電圧の印
加、中止が繰り返されることによつて蒸着材気体
が噴出口3からパルス状に噴出される。 容器5の外壁には、蒸着材からの輻射熱による
圧電素体子6の性能低下を防止するために冷却機
構、たとえば冷却剤の循環管が取り付けられてい
る。 噴出口3からパルス状に噴出した蒸着材気体
は、パルス分子線発生装置が組合された真空蒸着
装置(図示せず)に導かれ、被蒸着材に照射さ
れ、以後は通常の蒸着装置のおけると同様の過程
に従つて被蒸着材に蒸着される。 ここで本発明において、パルス分子線発生装置
と組み合される真空蒸着装置は特に限定されるも
のではなく、例えば通常の真空蒸着装置の外に、
クラスターイオンビーム装置、クヌーセンセルを
用いた蒸着装置、イオン化蒸着装置、イオンスパ
ツタリグ装置、マグネトロンスパツタリワング装
置等を挙げることができる。 一回のパルスによつて被蒸着材に照射される蒸
着材気体の量は、圧電素子体に印加されるパルス
電圧の持続時間Δt、容器2内に導入される蒸着
材気体の圧力およびパルスの回数によつて変える
ことができる。 また本発明においては、上述したパルス分子線
発生装置のみでも被蒸着材に蒸着材の薄膜を形成
することができるが、パルス分子線発生装置で形
成された蒸着材気体流を、他の如何なる蒸着材気
体発生装置で形成された気体流と組み合せて使用
することもできる。 この場合には、パルス分子線発生装置で発生し
た気体流を、他の蒸着材気体流発生装置からの気
体流と合併して、または交互に被蒸着材に供給す
ることにより蒸着が行われる。 更に、前記パルス分子線発生装置は、2台以上
を同時に同一の蒸着装置に組み込むことも可能で
ある。 この場合には、2台以上のパルス分子線発生装
置を同時に、または交互に作動させて蒸着が行な
われる。 更にまた、前記パルス分子線発生装置からのパ
ルス状気体流を電子、イオンまたは光によつて活
性化して被蒸着材への蒸着を促進することもでき
る。 次に本発明のパルス分子線蒸着装置の機能をパ
ルス分子線発生装置が電子線加熱蒸着源を有する
真空蒸着装置と組合された場合について説明す
る。 第2図においては、パルス分子線発生装置1が
2基の電子線加熱蒸着源11および12と組合わ
されて真空蒸着装置13が形成されている。 電子線加熱蒸着源11,12は、それぞれ水晶
式膜厚計14,15によりり蒸着速度をコントロ
ールすることが可能であり、所定の膜厚に達した
ときにシヤツター機構16,17によりそれぞれ
独立に蒸着源からのビームを遮断することが可能
である。 このようにして、電子線加熱蒸着源11,12
により生成したビームを、加熱装置18により所
定の温度に保持された被蒸着材19、たとえば蒸
着基板に照射して蒸着を行う。 一方、パルス分子線発生装置1で発生したパル
ス状の蒸着材気体を蒸着源11,12からのビー
ムと同時に、または蒸着源11,12からのビー
ムで蒸着を行わせた後にパルス分子線発生装置1
からのパルス状気体流を所定回数噴射させる操作
を蒸着基板19上の全膜厚が所定の値に達するま
で交互に繰り返す。 なお、蒸着基板19上の膜厚、組成および構造
は高速電子線回折装置20および21によつて、
蒸着膜表面からの解析パターンを時々刻々解析す
ることにより知ることができる。 〔発明の効果〕 以上述べたように本発明によれば、気体噴出流
の高速遮断手段によつパルス状の蒸着材気体流が
形成され、この気体流が真空蒸着装置に供給され
るので、真空蒸着装置全体の真空雰囲気を大きく
変化させることがなく、被蒸着材近傍のガス圧の
みを高速制御できる。 また、真空度は、高速電子線回折装置や質量分
析計を作動させるのに十分な真空度に保つことが
可能であり、薄膜作製中に蒸着膜をその場で分析
することができる。 従つて、組成および構造がよく制御された薄膜
を被蒸着材上に形成することができる。 以下、本発明の実施例を述べる。 〔実施例〕 第2図に示したパルス分子線蒸着装置を用いて
酸化チタンの薄膜を基板上に形成した。 電子線加熱蒸着源11,12で発生したチタニ
ウム蒸気を、蒸着速度0.5Å/secで、700℃に保
持した石英基板19上に2.25Å蒸着し、しかる後
にパルス分子線発生装置1の背圧に酸素ガスを
0.34気圧導入してパルス状気体流をパルス印加電
圧120V、パルス巾3msecの条件でN回、基板1
9上に噴射させた。 このサイクルを600回繰り返して下記第1表に
示した酸化チタンの薄膜を得た。
[Technical Field of the Invention] The present invention relates to an improved vacuum evaporation method and apparatus, and more particularly to a vacuum evaporation method and apparatus for supplying a vapor of evaporation material in a pulsed manner to a vacuum evaporation apparatus. [Prior art] Conventionally, in a vapor deposition method called chemical vapor deposition method,
The evaporation material was deposited on the material to be evaporated under reduced pressure by introducing, or while introducing, the vapor of the evaporation material under a relatively high pressure of about 10 -3 to 10T -4 orr into the evaporation container of the evaporation equipment. . However, in such a chemical vapor deposition method, it takes time to introduce and stop the vapor of the vapor deposition material into the vapor deposition container, and it is difficult to precisely control the vapor deposition conditions. Moreover, since the average degree of vacuum in the vapor deposition container is lowered by introducing the vapor deposition material gas, it has been impossible to analyze the vapor deposited film each time. [Object of the Invention] The present invention solves the above-mentioned conventional drawbacks, can quickly cut off the supply of a vapor deposition material gas flow to a vacuum evaporation apparatus, and allows precise control of evaporation conditions.
Moreover, it is an object of the present invention to provide a vapor deposition method and an apparatus for the same, which can analyze a vapor-deposited film in situ. [Structure of the Invention] The pulsed molecular beam evaporation method of the present invention achieves the above object by injecting a gas flow of the evaporation material in a pulsed manner onto the material to be evaporated in a vacuum evaporation apparatus. It is characterized by vapor-depositing. Further, the pulsed molecular beam evaporation apparatus of the present invention is composed of a combination of a pulsed molecular beam generation apparatus and a vacuum evaporation apparatus, and the pulsed molecular beam generation apparatus includes a container containing a vapor of a vapor deposition material, and an inner side of the ejection port of the container. The device is characterized in that it comprises a high-speed cutoff means for the ejected gas flow, and a pulse voltage generation source connected to the means. First, the pulsed molecular beam evaporation apparatus of the present invention will be explained based on the drawings. FIG. 1 shows an embodiment of a pulsed molecular beam generator that is combined with a vacuum evaporation apparatus in the present invention. The pulsed molecular beam generator 1 includes a container 2 containing the gas of the evaporation material, a high-speed blocking means 4 for the ejected gas flow provided inside a gas flow jetting port 3 formed in the container 2, and this high-speed blocking means 4. The container 2 normally contains a vapor deposition material gas of 10 atmospheres or less, and this gas 2 is introduced through a valve 8 and a pipe 9. Here, the gas flow in the present invention refers to not only normal gas flow but also all forms of things that can move in the gas phase, such as metal vapor, metal clusters, ultrafine particles, and ions. It also includes flow. Therefore, in this sense, the present invention is not limited to molecular beams, but is directed to beams in a wide range of gas phases. The high-speed cutoff means 4 for the ejected gas flow includes, for example, a piezoelectric element 6, an electromagnetic solenoid element, or an element having a similar function, and a gas flow outlet closing member 7 bonded to the tip of the element 6. It is formed. The gas outlet closing member 7 is made of a highly hard material, such as tungsten carbide, or a resin, such as Viton, and the surface thereof in contact with the gas outlet 3 is polished smooth. This closing member 7 is normally pressed against the spout 3 by the vapor deposition material gas contained in the container 2, and prevents the vapor deposition material gas from leaking from the spout 3. From the pulse voltage source, the piezoelectric element 6 receives 80~
A pulse voltage of 140 V is applied, the piezoelectric element 6 contracts, and the vapor deposition material gas contained in the container 2 is ejected from the ejection port 3. When the application of the pulse voltage is stopped, the piezoelectric element 6
The shape of is restored to its original state, and the closing member 7 comes into contact with the spout 3 again to close the spout 3. By repeating application and termination of the pulse voltage to the piezoelectric element 6 in this manner, the vapor deposition material gas is ejected from the ejection port 3 in a pulsed manner. A cooling mechanism, such as a coolant circulation pipe, is attached to the outer wall of the container 5 in order to prevent performance deterioration of the piezoelectric element 6 due to radiant heat from the vapor deposition material. The vapor deposition material gas ejected in a pulsed manner from the ejection port 3 is guided to a vacuum evaporation device (not shown) combined with a pulsed molecular beam generator and irradiated onto the material to be evaporated. It is vapor-deposited on the material to be vapor-deposited according to the same process as above. Here, in the present invention, the vacuum evaporation device combined with the pulsed molecular beam generator is not particularly limited, and for example, in addition to a normal vacuum evaporation device,
Examples include a cluster ion beam device, a vapor deposition device using a Knudsen cell, an ionization vapor deposition device, an ion sputtering device, a magnetron sputtering device, and the like. The amount of vapor deposition material gas irradiated onto the material to be vaporized by one pulse is determined by the duration Δt of the pulse voltage applied to the piezoelectric element body, the pressure of the vapor deposition material gas introduced into the container 2, and the pulse voltage. It can be changed depending on the number of times. Furthermore, in the present invention, although it is possible to form a thin film of the evaporation material on the material to be evaporated using only the above-mentioned pulsed molecular beam generation device, the evaporation material gas flow formed by the pulsed molecular beam generation device can be used in any other evaporation method. It can also be used in combination with a gas stream generated by a gas generator. In this case, evaporation is performed by supplying the gas flow generated by the pulsed molecular beam generator to the material to be evaporated, either in combination with the gas flow from other evaporation material gas flow generators, or alternately. Furthermore, two or more of the pulsed molecular beam generators can be incorporated into the same vapor deposition apparatus at the same time. In this case, vapor deposition is performed by operating two or more pulsed molecular beam generators simultaneously or alternately. Furthermore, the pulsed gas flow from the pulsed molecular beam generator can be activated by electrons, ions, or light to promote deposition on the material to be deposited. Next, the functions of the pulsed molecular beam evaporation apparatus of the present invention will be described in the case where the pulsed molecular beam generation apparatus is combined with a vacuum evaporation apparatus having an electron beam heating evaporation source. In FIG. 2, the pulsed molecular beam generator 1 is combined with two electron beam heating evaporation sources 11 and 12 to form a vacuum evaporation apparatus 13. The electron beam heating evaporation sources 11 and 12 can control the evaporation speed using crystal film thickness gauges 14 and 15, respectively, and when a predetermined film thickness is reached, they are independently controlled by shutter mechanisms 16 and 17, respectively. It is possible to block the beam from the deposition source. In this way, the electron beam heating evaporation sources 11, 12
Vapor deposition is performed by irradiating the beam generated by the heating device 18 onto a material 19 to be vapor-deposited, such as a vapor deposition substrate, which is maintained at a predetermined temperature. On the other hand, the pulsed evaporation material gas generated by the pulsed molecular beam generator 1 is evaporated simultaneously with the beams from the evaporation sources 11 and 12, or after the evaporation is performed with the beams from the evaporation sources 11 and 12, the pulsed molecular beam generator 1
The operation of injecting a pulsed gas flow from 2 to 3 is alternately repeated a predetermined number of times until the total film thickness on the deposition substrate 19 reaches a predetermined value. The film thickness, composition, and structure on the vapor deposition substrate 19 were determined by high-speed electron diffraction devices 20 and 21.
This can be determined by analyzing the analysis pattern from the surface of the deposited film from time to time. [Effects of the Invention] As described above, according to the present invention, a pulsed vapor deposition material gas flow is formed by the high-speed gas jet flow blocking means, and this gas flow is supplied to the vacuum vapor deposition apparatus. Only the gas pressure near the material to be evaporated can be controlled at high speed without significantly changing the vacuum atmosphere of the entire vacuum evaporation apparatus. Further, the degree of vacuum can be maintained at a degree sufficient to operate a high-speed electron beam diffraction device or a mass spectrometer, and a deposited film can be analyzed on the spot during thin film production. Therefore, a thin film whose composition and structure are well controlled can be formed on the material to be deposited. Examples of the present invention will be described below. [Example] A thin film of titanium oxide was formed on a substrate using the pulsed molecular beam evaporation apparatus shown in FIG. Titanium vapor generated by the electron beam heating evaporation sources 11 and 12 is deposited at a deposition rate of 0.5 Å/sec to 2.25 Å on a quartz substrate 19 maintained at 700°C, and then applied to the back pressure of the pulsed molecular beam generator 1. oxygen gas
0.34 atm was introduced and a pulsed gas flow was applied to the substrate 1 N times under the conditions of a pulse applied voltage of 120 V and a pulse width of 3 msec.
9 was sprayed on top. This cycle was repeated 600 times to obtain the titanium oxide thin films shown in Table 1 below.

【表】 酸化チタンの組成は、X線回折法によつてそれ
ぞれ単一相であることを確認した。 パルス分子線発生装置1からのパルス状気体流
は、半値巾3msecで真空蒸着装置13内に噴出さ
れ、噴出終了後、10msec以内に真空蒸着装置の
容器内真空度はベースの真空度に戻つた。 しかも、パルス分子線発生装置からのパルス状
酸素流は、方向性を有する分子線ビームとして基
板19上に噴射されるので、真空蒸着装置の容器
内の平均的真空度を低く抑えたまま、基板上での
実効的気体分圧を上げることが可能である。 また、第2図では、2基の電子線加熱蒸着源1
1,12と、シヤツター機構16,17との併用
によつて、多層薄膜の作製が可能であるが、2台
以上のパルス分子線発生装置を用いることにより
TiO/TiNのような多層薄膜を作製することがで
きる。 この場合、窒素源としては、N2ガスを用いる
ことができるが、場合によつては、N2ビームを
イオン化することによつて反応を促進させること
もできる。 従来の、気体をガス導入バルブによつて蒸着装
置の容器内に導入する方法では、高速で雰囲気ガ
スを交換または排気することが困難であつたの
で、繰り返し周期の多い多層構造膜を作製するこ
とは、ほとんど不可能であつた。
[Table] The composition of each titanium oxide was confirmed to be a single phase by X-ray diffraction method. The pulsed gas flow from the pulsed molecular beam generator 1 is ejected into the vacuum evaporator 13 with a half width of 3 msec, and after the ejection ends, the degree of vacuum in the container of the vacuum evaporator returns to the base vacuum level within 10 msec. . Moreover, since the pulsed oxygen flow from the pulsed molecular beam generator is injected onto the substrate 19 as a directional molecular beam beam, it is possible to maintain the average degree of vacuum inside the vacuum evaporation device container at a low level. It is possible to increase the effective gas partial pressure above. In addition, in FIG. 2, two electron beam heating evaporation sources 1
1 and 12 and the shutter mechanisms 16 and 17, it is possible to fabricate a multilayer thin film, but by using two or more pulsed molecular beam generators,
Multilayer thin films such as TiO/TiN can be created. In this case, N 2 gas can be used as the nitrogen source, but in some cases, the reaction can also be promoted by ionizing the N 2 beam. With the conventional method of introducing gas into the container of a vapor deposition apparatus using a gas introduction valve, it was difficult to exchange or exhaust the atmospheric gas at high speed, so it was necessary to create a multilayer structure film with a large number of repetition cycles. was almost impossible.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は本発明のパルス分子製蒸着装置に使用
されるパルス分子線発生装置の態様を示す概要説
明図、第2図は本発明のパルス分子線蒸着装置の
説明図である。 1…パルス分子線発生装置、2…蒸着材気体収
容装置、3…噴出口、4…噴出気体流高速遮断手
段、6…パルス電圧発生源。
FIG. 1 is a schematic explanatory view showing an aspect of a pulsed molecular beam generator used in the pulsed molecular beam vapor deposition apparatus of the present invention, and FIG. 2 is an explanatory view of the pulsed molecular beam vapor deposition apparatus of the present invention. DESCRIPTION OF SYMBOLS 1...Pulse molecular beam generator, 2...Deposited material gas storage device, 3...Ejection port, 4...Ejected gas flow high-speed cutoff means, 6...Pulse voltage generation source.

Claims (1)

【特許請求の範囲】 1 真空蒸着装置内の被蒸着材上に蒸着材の気体
流をパルス状で噴射させて該被蒸着材に前記蒸着
材を蒸着させることを特徴とするパルス分子線蒸
着方法。 2 パルス分子線発生装置と真空蒸着装置との組
合せからなり、該パルス分子線発生装置が蒸着材
の気体を収容する容器と、該容器の噴出口の内側
に設けた噴出気体流の高速遮断手段、および該手
段と連結したパルス電圧発生源とからなることを
特徴とするパルス分子線蒸着装置。
[Scope of Claims] 1. A pulsed molecular beam evaporation method characterized by injecting a gas flow of the evaporation material in a pulsed manner onto a material to be deposited in a vacuum evaporation apparatus to deposit the evaporation material onto the material to be deposited. . 2 Consisting of a combination of a pulsed molecular beam generator and a vacuum evaporation device, the pulsed molecular beam generator includes a container containing the vapor of the evaporation material, and a high-speed blocking means for the ejected gas flow provided inside the ejection port of the container. , and a pulsed voltage generation source connected to the means.
JP9256886A 1986-04-22 1986-04-22 Method and apparatus for pulse molecular ray vapor deposition Granted JPS62250167A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP9256886A JPS62250167A (en) 1986-04-22 1986-04-22 Method and apparatus for pulse molecular ray vapor deposition

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP9256886A JPS62250167A (en) 1986-04-22 1986-04-22 Method and apparatus for pulse molecular ray vapor deposition

Publications (2)

Publication Number Publication Date
JPS62250167A JPS62250167A (en) 1987-10-31
JPH031379B2 true JPH031379B2 (en) 1991-01-10

Family

ID=14058028

Family Applications (1)

Application Number Title Priority Date Filing Date
JP9256886A Granted JPS62250167A (en) 1986-04-22 1986-04-22 Method and apparatus for pulse molecular ray vapor deposition

Country Status (1)

Country Link
JP (1) JPS62250167A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
FR2771810B1 (en) * 1997-11-28 2000-02-11 Sgs Thomson Microelectronics IMPROVING THE REAL-TIME THICKNESS MEASUREMENT OF A MATERIAL DEPOSITED IN AN EVAPORATION DEPOSIT INSTALLATION

Also Published As

Publication number Publication date
JPS62250167A (en) 1987-10-31

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