JP3395949B2 - Metal phthalocyanine crystal and method for producing the same - Google Patents
Metal phthalocyanine crystal and method for producing the sameInfo
- Publication number
- JP3395949B2 JP3395949B2 JP19157997A JP19157997A JP3395949B2 JP 3395949 B2 JP3395949 B2 JP 3395949B2 JP 19157997 A JP19157997 A JP 19157997A JP 19157997 A JP19157997 A JP 19157997A JP 3395949 B2 JP3395949 B2 JP 3395949B2
- Authority
- JP
- Japan
- Prior art keywords
- crystal
- phthalocyanine
- phthalocyanine crystal
- metal phthalocyanine
- filamentous
- 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 - Fee Related
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- Photoreceptors In Electrophotography (AREA)
- Nitrogen Condensed Heterocyclic Rings (AREA)
Description
【0001】[0001]
【発明の属する技術分野】本発明は、太陽電池、電子写
真感光体などの電荷発生物質、ガスセンサーのガス分子
吸着物質などとして使用される金属フタロシアニン結晶
に関するものであり、詳細には簡便に成膜可能な金属フ
タロシアニン結晶の提供を目的とするものである。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a metal phthalocyanine crystal used as a charge generating substance for a solar cell, an electrophotographic photoreceptor, a gas molecule adsorbing substance for a gas sensor, and the like. The object is to provide a film-capable metal phthalocyanine crystal.
【0002】[0002]
【従来の技術】固体の金属フタロシアニン結晶の形態と
しては、針状結晶、或いは、不定形結晶が知られてい
る。例えば銅フタロシアニン結晶の場合、昇華法により
図6に示すような針状結晶90が生成でき、また、濃硫
酸を用いるアシッドペースティング法により図7に示す
ような不定形結晶91を生成できる。2. Description of the Related Art Needle crystals or amorphous crystals are known as solid metal phthalocyanine crystals. For example, in the case of a copper phthalocyanine crystal, a needle crystal 90 as shown in FIG. 6 can be produced by the sublimation method, and an amorphous crystal 91 as shown in FIG. 7 can be produced by the acid pasting method using concentrated sulfuric acid.
【0003】結晶の大きさについては、結晶の生成条件
を変えるか、或いは、生成した後に粉砕などの処理を行
うことによりある程度は制御することができる。また、
上記の形態の結晶あるいは粉末を膜状とする用途に用い
る場合には、バインダー樹脂中に有機溶剤と共にそれら
結晶、粉末を分散させた液を調整し、その液を用いて塗
布法、ディップ法、スピンコート法などにより成膜す
る。The size of the crystals can be controlled to some extent by changing the conditions for producing the crystals or by performing a process such as crushing after the production. Also,
When the crystals or powders of the above forms are used in the form of a film, prepare a liquid in which the crystals and powders are dispersed in a binder resin together with an organic solvent, and apply the liquid.
A film is formed by a cloth method , a dip method, a spin coating method, or the like.
【0004】[0004]
【発明が解決しようとする課題】しかしながら、金属フ
タロシアニン結晶の用途としては、例えば太陽電池の電
荷発生物質、電子写真感光体の電荷発生物質、あるい
は、ガスセンサのガス分子吸着物質など、バインダー樹
脂を用いない状態で成膜した膜が要求される場合が多々
ある。ところが、上記の針状結晶、粉末状とした金属フ
タロシアニンでは、金属フタロシアニンがどのような有
機溶剤にも実質的には溶けないために、溶液として調製
することができない。However, as the use of the metal phthalocyanine crystal, a binder resin such as a charge generating substance for a solar cell, a charge generating substance for an electrophotographic photoreceptor, or a gas molecule adsorbing substance for a gas sensor is used. In many cases, a film formed without the film is required. However, the above-mentioned needle-like crystals and powdery metal phthalocyanine cannot be prepared as a solution because the metal phthalocyanine is substantially insoluble in any organic solvent.
【0005】従って、上記のような用途に対しては、真
空槽、排気装置など比較的に大規模な装置を必要とする
真空蒸着法などにより成膜を行わなくては成らないもの
となり、塗布法、ディップ法、スピンコート法など簡便
な成膜法が採用できず、結果として太陽電池あるいは電
子写真感光体など製品全体をコストアップさせる問題点
を生じるものとなり、この点の解決が課題とされるもの
となっている。Accordingly, for applications as described above, the vacuum chamber, without the need for film deposition by vacuum evaporation method which requires a large apparatus relatively such exhaust system becomes that does not become the coating The simple film-forming method such as the coating method , the dipping method, and the spin coating method cannot be adopted, and as a result, there arises a problem that the cost of the entire product such as the solar cell or the electrophotographic photosensitive member is increased. It has become one.
【0006】[0006]
【課題を解決するための手段】本発明は上記した従来の
課題を解決するための具体的な手段として、軸配位子を
持たない亜鉛フタロシアニンまたはコバルトフタロシア
ニンを、不活性ガスにより一定の圧力に調整された容器
内で加熱するガス中蒸発法により微粒子化した後に、ベ
ンゼンに浸し結晶転移処理を行うことで準安定型の糸状
の亜鉛フタロシアニン結晶またはコバルトフタロシアニ
ン結晶を得ることを特徴とする亜鉛フタロシアニン結晶
またはコバルトフタロシアニン結晶の製造方法、およ
び、前記製造方法により得られる糸状結晶構造の亜鉛フ
タロシアニンまたはコバルトフタロシアニンを提供する
ことで、バインダー樹脂を用いない状態でも塗布など簡
易な手段での成膜を可能として課題を解決するものであ
る。As a concrete means for solving the above-mentioned conventional problems, the present invention makes zinc phthalocyanine or cobalt phthalocyanine having no axial ligand a constant pressure by an inert gas. Zinc phthalocyanine characterized by obtaining a metastable thread-like zinc phthalocyanine crystal or cobalt phthalocyanine crystal by immersing in benzene and subjecting it to crystal transition treatment after atomizing by a gas evaporation method heating in a prepared container By providing a method for producing a crystal or cobalt phthalocyanine crystal, and zinc phthalocyanine or cobalt phthalocyanine having a thread-like crystal structure obtained by the above-mentioned production method, it is possible to form a film by a simple means such as coating without using a binder resin. Is to solve the problem.
【0007】[0007]
【発明の実施の形態】つぎに、本発明に係る金属フタロ
シアニン結晶の製造方法について詳細に説明する。本発
明は、軸配位子を持たない金属フタロシアニンを対象と
した糸状結晶の製造方法であり、先ず最初に、排気装置
で減圧された容器に不活性ガスを導入し、所定の圧力範
囲に調整する。BEST MODE FOR CARRYING OUT THE INVENTION Next, a method for producing a metal phthalocyanine crystal according to the present invention will be described in detail. The present invention is a method for producing a filamentous crystal targeting a metal phthalocyanine having no axial ligand. First, an inert gas is introduced into a container whose pressure is reduced by an exhaust device to adjust the pressure within a predetermined pressure range. To do.
【0008】この容器内で固体の金属フタロシアニン、
例えば銅フタロシアニンを加熱し蒸発させることによ
り、金属フタロシアニンの微粒子を生成する。一般に、
このような手段による微粒子の生成方法はガス中蒸発法
と称される代表的な方法の1つである。Solid metal phthalocyanine in this container,
For example, by heating and evaporating copper phthalocyanine, fine particles of metal phthalocyanine are generated. In general,
The method of producing fine particles by such means is one of the typical methods called the in-gas evaporation method.
【0009】このときに、前記した微粒子の生成条件で
ある不活性ガスの種類、流量、雰囲気の圧力、および、
加熱方法などの条件は、100nm以下の大きさの微粒子
が得られるものであれば、本発明においては特に制約を
設けるものではなく、如何なる条件で行うことも自在で
ある。At this time, the type of the inert gas, the flow rate, the pressure of the atmosphere, and the conditions for producing the above-mentioned fine particles, and
Conditions such as a heating method are not particularly limited in the present invention as long as fine particles having a size of 100 nm or less can be obtained, and any conditions can be freely used.
【0010】ここで、本発明の発明者は、上記のガス中
蒸発法により微粒子化された金属フタロシアニンをベン
ゼンで処理、すなわち、処理原料を一定温度のベンゼン
に一定時間以上浸す結晶転移処理を行うことにより、糸
状で準安定型の金属フタロシアニン結晶が得られること
を見いだした。尚、ここでは、加熱処理で結晶転移を生
じない結晶を安定型と称し、加熱処理により結晶転移を
生じる結晶を準安定型と称する。Here, the inventor of the present invention treats the metal phthalocyanine atomized by the above-mentioned gas evaporation method with benzene, that is, performs a crystal transition treatment in which the raw material for treatment is immersed in benzene at a constant temperature for a certain time or more. As a result, it was found that thread-like metastable metal phthalocyanine crystals were obtained. It should be noted that, here, a crystal that does not cause crystal transition by heat treatment is called a stable type, and a crystal that causes crystal transition by heat treatment is called a metastable type.
【0011】一般に、金属フタロシアニンを結晶転移さ
せる方法の1つとして溶媒処理が知られているが、通
常、適当な有機溶媒で処理を行った場合、準安定型の金
属フタロシアニン結晶は、短冊状で安定型の結晶へと変
化するとされているので、金属フタロシアニンをベンゼ
ン処理を行うことにより、糸状で準安定型の金属フタロ
シアニン結晶が得られる本発明の製造方法は、これまで
にない新規の結果が得られるものであり、このような結
果が得られる要因は、ガス中蒸発法により生成した微粒
子をベンゼン処理すると言う本発明特有の製造方法とし
たからである。Generally, solvent treatment is known as one of the methods for crystal transition of metal phthalocyanine. However, when treated with an appropriate organic solvent, metastable metal phthalocyanine crystals are generally strip-shaped. Since it is said that the crystals are changed to stable crystals, the production method of the present invention in which a thread-like metastable metal phthalocyanine crystal is obtained by subjecting the metal phthalocyanine to benzene treatment has a novel result that has never been obtained. The reason why such a result is obtained is that the production method peculiar to the present invention is that the fine particles generated by the gas evaporation method are treated with benzene.
【0012】[0012]
実施例1:市販の銅フタロシアニン(東京化成工業株式
会社製、P1005)を原料とし、He(ヘリウム)ガ
ス、圧力1Torrの雰囲気の下、抵抗加熱で上記の原料を
加熱することにより微粒子を生成し、この生成された微
粒子を走査型電子顕微鏡で観察したところ、50nm程度
の大きさの不定形粒子であった。Example 1: A commercially available copper phthalocyanine (manufactured by Tokyo Chemical Industry Co., Ltd., P1005) was used as a raw material, and the above raw material was heated by resistance heating under an atmosphere of He (helium) gas and a pressure of 1 Torr to produce fine particles. When the produced fine particles were observed with a scanning electron microscope, they were amorphous particles having a size of about 50 nm.
【0013】生成した銅フタロシアニン微粒子を室温に
てベンゼン(濃度1g/リットル)中に分散させ、12
時間放置することにより図1、図2に示すような幅50
nmから100nmの糸状結晶1が得られた。前記糸状結晶
1の可視から近赤外域の吸収スペクトルは、波長614nm
と774nm とに特徴的な吸収極大をもつスペクトルであっ
た。但し、分散媒は、濃度0.1%のPolyoxyethylene(10)
Octylphenyl Ether (略称 Triton X-100)の水溶液で
ある。The copper phthalocyanine fine particles thus produced were dispersed in benzene (concentration 1 g / liter) at room temperature to obtain 12
The width 50 as shown in FIG. 1 and FIG.
Filamentous crystal 1 having a size of 100 nm was obtained. The absorption spectrum of the filamentous crystal 1 in the visible to near infrared region has a wavelength of 614 nm.
The spectra have absorption maximums at and 774 nm. However, the dispersion medium is polyoxyethylene (10) with a concentration of 0.1%.
It is an aqueous solution of Octylphenyl Ether (abbreviation: Triton X-100).
【0014】上記糸状結晶1のベンゼン分散液をガラス
基板上に塗布することにより、銅フタロシアニンの糸状
結晶からなる膜が生成できた。X線粉末法により測定し
た糸状結晶膜のX線回折スペクトルBSは図3に示すよ
うに、主要ピークの回折角2θは、5.8 、7.8 、10.0、
17.5 degree であり、準安定型の結晶であった。尚、こ
のときにX線としては、CuKα線、波長1.542 Åを用
いた。By coating the glass substrate with the benzene dispersion of the filamentous crystals 1, a film made of filamentous crystals of copper phthalocyanine could be produced. As shown in FIG. 3, the X-ray diffraction spectrum BS of the filamentous crystal film measured by the X-ray powder method shows that the diffraction angles 2θ of the main peaks are 5.8, 7.8, 10.0,
It was 17.5 degree and was a metastable crystal. At this time, CuKα rays and a wavelength of 1.542 Å were used as X-rays.
【0015】実施例2:市販の亜鉛フタロシアニン(東
京化成工業株式会社製、P0767)を原料とし、Heガ
ス、圧力1Torrの雰囲気の下、抵抗加熱で上記の原料を
加熱することにより微粒子を生成し、この生成された微
粒子を走査型電子顕微鏡で観察したところ、50nm程度
の大きさの不定形粒子であった。Example 2: Using commercially available zinc phthalocyanine (P0767 manufactured by Tokyo Chemical Industry Co., Ltd.) as a raw material, the above raw material was heated by resistance heating under an atmosphere of He gas and a pressure of 1 Torr to produce fine particles. When the produced fine particles were observed with a scanning electron microscope, they were amorphous particles having a size of about 50 nm.
【0016】生成した亜鉛フタロシアニン微粒子をベン
ゼン(濃度1g/リットル)中に分散させた後、40℃
の恒温槽中にて4時間放置することにより、図4に示す
ように上記の銅フタロシアニンの場合と同様な幅50nm
から100nmの糸状結晶2が得られた。The zinc phthalocyanine fine particles thus produced were dispersed in benzene (concentration: 1 g / liter), and then 40 ° C.
As shown in Fig. 4, by leaving it in the constant temperature bath for 4 hours, the same width of 50 nm as in the case of the above copper phthalocyanine is obtained.
From which a filamentous crystal 2 of 100 nm was obtained.
【0017】前記糸状結晶2の可視から近赤外域の吸収
スペクトルは、波長619nm と786nmとに特徴的な吸収極
大をもつスペクトルであり、この糸状結晶2のベンゼン
分散液をガラス基板上に塗布することにより、亜鉛フタ
ロシアニンの糸状結晶2からなる膜が生成できた。粉末
法により糸状結晶2のX線回折スペクトルを測定したと
ころ、図3とほヾ同じスペクトルであり、準安定型の結
晶であった。The visible to near-infrared absorption spectrum of the filamentous crystal 2 is a spectrum having a characteristic absorption maximum at wavelengths of 619 nm and 786 nm, and the benzene dispersion of the filamentous crystal 2 is coated on a glass substrate. As a result, a film composed of the zinc phthalocyanine filamentous crystals 2 could be produced. When the X-ray diffraction spectrum of the filamentous crystal 2 was measured by the powder method, the spectrum was almost the same as in FIG. 3, and it was a metastable crystal.
【0018】実施例3:市販のコバルトフタロシアニン
(東京化成工業株式会社製、P0887)を原料とし、
Heガス、圧力1Torrの雰囲気の下、抵抗加熱で上記の原
料を加熱することにより微粒子を生成し、この生成され
た微粒子を走査型電子顕微鏡で観察したところ、50nm
程度の大きさの不定形粒子であった。Example 3 Using commercially available cobalt phthalocyanine (P0887 manufactured by Tokyo Chemical Industry Co., Ltd.) as a raw material,
Fine particles were generated by heating the above raw materials by resistance heating under an atmosphere of He gas and a pressure of 1 Torr, and the generated fine particles were observed with a scanning electron microscope.
The particles were irregularly sized particles.
【0019】生成したコバルトフタロシアニン微粒子を
ベンゼン(濃度1g/リットル)中に分散させた後、4
0℃の恒温槽中にて5時間放置することにより、図5に
示すように幅50nmから100nmの糸状結晶3が得ら
れ、この糸状結晶3の可視から近赤外域の吸収スペクト
ルは、波長620nm と750nm とに特徴的な吸収極大をもつ
スペクトルであった。The cobalt phthalocyanine fine particles thus produced were dispersed in benzene (concentration: 1 g / liter), and then 4
By leaving it in a constant temperature bath at 0 ° C. for 5 hours, a filamentous crystal 3 with a width of 50 nm to 100 nm is obtained as shown in FIG. 5, and the absorption spectrum of this filamentous crystal 3 in the visible to near infrared region has a wavelength of 620 nm. The spectrum has absorption maximums at and 750 nm.
【0020】この糸状結晶2のベンゼン分散液をガラス
基板上に塗布することにより、コバルトフタロシアニン
の糸状結晶3からなる膜が生成できた。粉末法により糸
状結晶3のX線回折スペクトルを測定したところ、図3
とほヾ同じスペクトルであり、準安定型の結晶であっ
た。By coating the glass substrate with this benzene dispersion of filamentous crystals 2, a film composed of filamentous crystals 3 of cobalt phthalocyanine could be produced. The X-ray diffraction spectrum of the filamentous crystal 3 was measured by the powder method.
The spectrum was almost the same, and it was a metastable crystal.
【0021】以上に説明したように本発明により、軸配
位子を持たない亜鉛フタロシアニンまたはコバルトフタ
ロシアニンを、不活性ガスにより一定の圧力に調整され
た容器内で加熱するガス中蒸発法により微粒子化した後
に、ベンゼンに浸し結晶転移処理を行うことで準安定型
の糸状の亜鉛フタロシアニン結晶またはコバルトフタロ
シアニン結晶を得ることを特徴とする亜鉛フタロシアニ
ン結晶またはコバルトフタロシアニン結晶の製造方法と
したことで、従来はバインダーを使用しないこれらフタ
ロシアニンの膜が要求されるときには、例えば比較的に
大規模な装置を必要とする真空蒸着法などにより成膜を
行なわなくては成らないものとなり、この膜を使用する
太陽電池、電子写真感光体、あるいは、ガスセンサーな
ど製品全体がコストアップするものとなっていたのを、
糸状結晶として形成可能としたことで塗布など極めて簡
便な手段での成膜を可能とし、これにより太陽電池、電
子写真感光体あるいは、ガスセンサーなど製品全体のコ
ストダウンに極めて優れた効果を奏するものである。As described above, according to the present invention, zinc phthalocyanine or cobalt phthalocyanine having no axial ligand is atomized by the vaporization method in a gas, which is heated in a container adjusted to a constant pressure by an inert gas. After that, it was immersed in benzene and subjected to a crystal transition treatment to obtain a metastable thread-like zinc phthalocyanine crystal or cobalt phthalocyanine crystal. When a film of these phthalocyanines that does not use a binder is required, the film must be formed by, for example, a vacuum evaporation method that requires a relatively large-scale device, and a solar cell that uses this film. , The entire product such as the electrophotographic photoreceptor or the gas sensor The had become shall be up,
Since it can be formed as a filamentous crystal, it is possible to form a film by an extremely simple means such as coating, which is extremely effective in reducing the cost of the entire product such as a solar cell, an electrophotographic photoreceptor or a gas sensor. Is.
【図1】 本発明に係る金属フタロシアニン結晶の第一
実施例である銅フタロシアニン結晶の形状を拡大した状
態で示す説明図である。FIG. 1 is an explanatory view showing an enlarged shape of a copper phthalocyanine crystal which is a first example of a metal phthalocyanine crystal according to the present invention.
【図2】 同じく第一実施例である銅フタロシアニン結
晶の形状を更に拡大して示す説明図である。FIG. 2 is an explanatory view showing the shape of the copper phthalocyanine crystal of the first embodiment in a further enlarged manner.
【図3】 本発明に係る金属フタロシアニン結晶の第一
実施例である銅フタロシアニン結晶のX線回折スペクト
ルを示すグラフである。FIG. 3 is a graph showing an X-ray diffraction spectrum of a copper phthalocyanine crystal that is a first example of the metal phthalocyanine crystal according to the present invention.
【図4】 同じく本発明に係る金属フタロシアニン結晶
の第二実施例である亜鉛フタロシアニン結晶の形状を拡
大した状態で示す説明図である。FIG. 4 is an explanatory diagram showing an enlarged shape of a zinc phthalocyanine crystal which is a second example of the metal phthalocyanine crystal according to the present invention.
【図5】 同じく本発明に係る金属フタロシアニン結晶
の第三実施例であるコバルトフタロシアニン結晶の形状
を拡大した状態で示す説明図である。FIG. 5 is an explanatory view showing an enlarged shape of a cobalt phthalocyanine crystal which is a third example of the metal phthalocyanine crystal according to the present invention.
【図6】 従来例の金属フタロシアニン結晶の形状であ
る針状結晶の形状を拡大した状態で示す説明図である。FIG. 6 is an explanatory view showing an enlarged shape of a needle-like crystal which is a shape of a metal phthalocyanine crystal of a conventional example.
【図7】 従来例の金属フタロシアニン結晶の形状であ
る不定形結晶の形状を拡大した状態で示す説明図であ
る。FIG. 7 is an explanatory diagram showing an enlarged shape of an amorphous crystal which is a shape of a conventional metal phthalocyanine crystal.
1……銅フタロシアニンの糸状結晶 2……亜鉛フタロシアニンの糸状結晶 3……コバルトフタロシアニンの糸状結晶 BS……X線回析スペクトル 1 ... Filamentous crystal of copper phthalocyanine 2 ... Filamentous crystal of zinc phthalocyanine 3 ... Filamentous crystal of cobalt phthalocyanine BS: X-ray diffraction spectrum
フロントページの続き (58)調査した分野(Int.Cl.7,DB名) C07D 487/22 C09B 47/04 C09B 67/50 CA(STN) REGISTRY(STN)Front page continuation (58) Fields surveyed (Int.Cl. 7 , DB name) C07D 487/22 C09B 47/04 C09B 67/50 CA (STN) REGISTRY (STN)
Claims (2)
またはコバルトフタロシアニンを、不活性ガスにより一
定の圧力に調整された容器内で加熱するガス中蒸発法に
より微粒子化した後に、ベンゼンに浸し結晶転移処理を
行うことで準安定型の糸状の亜鉛フタロシアニン結晶ま
たはコバルトフタロシアニン結晶を得ることを特徴とす
る亜鉛フタロシアニン結晶またはコバルトフタロシアニ
ン結晶の製造方法。1. Zinc phthalocyanine or cobalt phthalocyanine having no axial ligand is atomized by a gas evaporation method in which it is heated in a vessel adjusted to a constant pressure by an inert gas, and then crystallized by immersing in benzene. A method for producing a zinc phthalocyanine crystal or a cobalt phthalocyanine crystal, which comprises obtaining a metastable thread-like zinc phthalocyanine crystal or a cobalt phthalocyanine crystal by performing a treatment.
またはコバルトフタロシアニンを、不活性ガスにより一
定の圧力に調整された容器内で加熱するガス中蒸発法に
より微粒子化した後に、ベンゼンに浸し結晶転移処理を
行うことで準安定型の糸状とされていることを特徴とす
る亜鉛フタロシアニン結晶またはコバルトフタロシアニ
ン結晶。2. Zinc phthalocyanine or cobalt phthalocyanine having no axial ligand is atomized by a gas evaporation method in which it is heated in a container adjusted to a constant pressure by an inert gas, and then crystallized by immersion in benzene. A zinc phthalocyanine crystal or a cobalt phthalocyanine crystal, which is formed into a metastable thread-like shape by treatment.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP19157997A JP3395949B2 (en) | 1997-07-16 | 1997-07-16 | Metal phthalocyanine crystal and method for producing the same |
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| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP19157997A JP3395949B2 (en) | 1997-07-16 | 1997-07-16 | Metal phthalocyanine crystal and method for producing the same |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH1135582A JPH1135582A (en) | 1999-02-09 |
| JP3395949B2 true JP3395949B2 (en) | 2003-04-14 |
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| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP19157997A Expired - Fee Related JP3395949B2 (en) | 1997-07-16 | 1997-07-16 | Metal phthalocyanine crystal and method for producing the same |
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| Country | Link |
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| CN1328415C (en) * | 2005-11-11 | 2007-07-25 | 吉林大学 | Equipment and method of lifting phthalocganine compound mono crystal growth by evaporation process |
Citations (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2871577B2 (en) | 1996-01-17 | 1999-03-17 | スタンレー電気株式会社 | Copper phthalocyanine crystal and method for producing the same |
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Patent Citations (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2871577B2 (en) | 1996-01-17 | 1999-03-17 | スタンレー電気株式会社 | Copper phthalocyanine crystal and method for producing the same |
Also Published As
| Publication number | Publication date |
|---|---|
| JPH1135582A (en) | 1999-02-09 |
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