JP4779694B2 - Hologram recording medium evaluation apparatus and hologram recording medium evaluation method - Google Patents

Hologram recording medium evaluation apparatus and hologram recording medium evaluation method Download PDF

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JP4779694B2
JP4779694B2 JP2006043502A JP2006043502A JP4779694B2 JP 4779694 B2 JP4779694 B2 JP 4779694B2 JP 2006043502 A JP2006043502 A JP 2006043502A JP 2006043502 A JP2006043502 A JP 2006043502A JP 4779694 B2 JP4779694 B2 JP 4779694B2
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洋一 丸山
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Pulstec Industrial Co Ltd
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Description

本発明は、ホログラム記録媒体の特性を評価するためのホログラム記録媒体の評価装置及びホログラム記録媒体の評価方法に関する。   The present invention relates to a hologram recording medium evaluation apparatus and a hologram recording medium evaluation method for evaluating the characteristics of a hologram recording medium.

従来より、ホログラム記録媒体の評価用特性の1つとして、Mナンバー(M/#)が用いられている。このMナンバー(M/#)は、例えば特許文献1に記載されているように、ホログラム記録媒体の記録層内の同一領域に記録が出来なくなるまでnページのホログラムを多重記録し、再生した際のホログラムからの回折効率により求められる特性である。   Conventionally, the M number (M / #) is used as one of the evaluation characteristics of a hologram recording medium. This M number (M / #) is, for example, as described in Patent Document 1, when n-page holograms are multiplexed and reproduced until recording is not possible in the same area in the recording layer of the hologram recording medium. It is a characteristic calculated | required by the diffraction efficiency from this hologram.

このMナンバー(M/#)は、nページのホログラムを多重記録した後、参照レーザ光をホログラム記録媒体に照射し、各々の記録における回折効率を測定すれば求めることができる。回折効率は、参照レーザ光において透過した光の強度と回折した光の強度を測定することで検出することができる。
特開2005−208426号公報
The M number (M / #) can be obtained by multiplex-recording n-page holograms, irradiating the hologram recording medium with a reference laser beam, and measuring the diffraction efficiency in each recording. The diffraction efficiency can be detected by measuring the intensity of light transmitted through the reference laser light and the intensity of diffracted light.
JP-A-2005-208426

しかしながら、ホログラム記録媒体には、多重記録数が大きくても各々の記録の回折効率が小さいものがある。このようなホログラム記録媒体は、Mナンバー(M/#)は大きくなるが、ホログラム記録媒体に記録した情報を精度よく再生するには、参照レーザ光の回折効率が少なくとも1%程度あることが必要であり、もし各々の記録の回折効率がこれより小さかったとすると、データの再生においてフォトセンサの受光光量が小さく、精度のよいデータの再生を行うことができない。すなわち、従来のホログラム記録媒体の評価用特性であるMナンバー(M/#)は、その値が大きくても、各々の記録の回折効率が小さければ精度のよい再生ができない記録が多数されているということであり、必ずしも多重記録性能を表しているとはいえない場合がある。   However, some hologram recording media have a low diffraction efficiency for each recording even if the number of multiple recordings is large. Such a hologram recording medium has a large M number (M / #), but in order to accurately reproduce information recorded on the hologram recording medium, it is necessary that the diffraction efficiency of the reference laser beam is at least about 1%. If the diffraction efficiency of each recording is smaller than this, the amount of light received by the photosensor is small in data reproduction, and accurate data reproduction cannot be performed. That is, the M number (M / #), which is a characteristic for evaluation of a conventional hologram recording medium, has a large number of recordings that cannot be reproduced accurately even if the diffraction efficiency of each recording is small. In other words, it may not necessarily represent the multiple recording performance.

本発明は、このような事情に鑑みてなされたもので、ホログラム記録媒体の多重記録性能を正しく把握することが可能なホログラム記録媒体の評価装置及びホログラム記録媒体の評価方法を提供することにある。   The present invention has been made in view of such circumstances, and provides a hologram recording medium evaluation apparatus and a hologram recording medium evaluation method capable of correctly grasping the multiplex recording performance of the hologram recording medium. .

請求項1記載のホログラム記録媒体の評価装置は、ホログラム記録媒体を保持するテーブルと、ホログラム記録媒体にデータを記録する際、ホログラム記録媒体に記録データに相当する信号を含んだ情報レーザ光を照射する情報レーザ光照射手段と、ホログラム記録媒体にデータを記録する際、ホログラム記録媒体に情報レーザ光とは異なった角度で記録用参照レーザ光を照射する記録用参照レーザ光照射手段と、ホログラム記録媒体にデータを記録する際、ホログラム記録媒体の記録領域の回折効率を測定する回折効率測定手段と、ホログラム記録媒体に所定の該回折効率になるまで多重記録を行い、多重記録を行える限界回数を評価用特性として計測する多重記録限界計測手段とを備えることを特徴とする。   The apparatus for evaluating a hologram recording medium according to claim 1, when recording data on the hologram recording medium, a table for holding the hologram recording medium, and irradiating the hologram recording medium with information laser light including a signal corresponding to the recording data Information laser light irradiating means, recording reference laser light irradiating means for irradiating the hologram recording medium with a recording reference laser light at an angle different from the information laser light when recording data on the hologram recording medium, and hologram recording When recording data on the medium, diffraction efficiency measuring means for measuring the diffraction efficiency of the recording area of the hologram recording medium, and the maximum number of times that multiple recording can be performed on the hologram recording medium until the predetermined diffraction efficiency is achieved. Multiple recording limit measurement means for measuring as an evaluation characteristic is provided.

請求項2記載のホログラム記録媒体の評価装置は、回折効率測定手段が、情報レーザ光及び記録用参照レーザ光とは異なる波長の回折効率測定用レーザ光をホログラム記録媒体の記録領域へ照射する回折効率測定用レーザ光照射手段と、回折効率測定用レーザ光がホログラム記録媒体の記録領域において回折したレーザ光の強度及び透過したレーザ光の強度をそれぞれ測定するレーザ光強度測定手段と、レーザ光強度測定手段により測定した回折したレーザ光の強度及び透過したレーザ光の強度により、ホログラム記録媒体の記録領域における回折効率を計算する回折効率計算手段とを備えることを特徴とする。   3. The hologram recording medium evaluation apparatus according to claim 2, wherein the diffraction efficiency measuring means irradiates the recording region of the hologram recording medium with a diffraction efficiency measuring laser beam having a wavelength different from that of the information laser beam and the recording reference laser beam. Laser beam irradiation means for measuring efficiency, laser beam intensity measuring means for measuring the intensity of the laser beam diffracted by the laser beam for measuring the diffraction efficiency in the recording area of the hologram recording medium and the intensity of the transmitted laser beam, and the laser beam intensity And a diffraction efficiency calculating means for calculating the diffraction efficiency in the recording area of the hologram recording medium based on the intensity of the diffracted laser light measured by the measuring means and the intensity of the transmitted laser light.

請求項3記載のホログラム記録媒体の評価方法は、ホログラム記録媒体にデータを記録する際、ホログラム記録媒体の記録領域の回折効率を測定し、ホログラム記録媒体に所定の回折効率になるまで多重記録を行い、多重記録を行える限界回数を評価用特性として計測することを特徴とする。   The method for evaluating a hologram recording medium according to claim 3 is characterized in that when data is recorded on the hologram recording medium, the diffraction efficiency of the recording area of the hologram recording medium is measured, and multiple recording is performed on the hologram recording medium until a predetermined diffraction efficiency is achieved. And the limit number of times that multiple recording can be performed is measured as an evaluation characteristic.

請求項4記載のホログラム記録媒体の評価方法は、記録データに相当する信号を含んだ情報レーザ光及び情報レーザ光とは異なった角度で照射する記録用参照レーザ光の2つのレーザ光とは異なる波長の回折効率測定用レーザ光をホログラム記録媒体の記録領域へ照射し、回折効率測定用レーザ光がホログラム記録媒体の記録領域において回折したレーザ光の強度及び透過したレーザ光の強度をそれぞれ測定し、測定した回折したレーザ光の強度及び透過したレーザ光の強度により、ホログラム記録媒体の記録領域における回折効率を計算することを特徴とする。   The method for evaluating a hologram recording medium according to claim 4 is different from the two laser beams of the information laser beam including a signal corresponding to the recording data and the recording reference laser beam irradiated at a different angle from the information laser beam. The laser beam for measuring the diffraction efficiency of the wavelength is irradiated to the recording area of the hologram recording medium, and the intensity of the laser beam diffracted by the laser beam for measuring the diffraction efficiency in the recording area of the hologram recording medium and the intensity of the transmitted laser beam are measured. The diffraction efficiency in the recording area of the hologram recording medium is calculated from the measured intensity of the diffracted laser beam and the intensity of the transmitted laser beam.

請求項1及び請求項3の発明によれば、ホログラム記録媒体に所定の回折効率になるまで多重記録を行い、多重記録を行える限界回数を評価用特性として計測することから、ホログラム記録媒体に精度のよい再生を行える記録を何回行うことができるかを表す数値を求めることができ、ホログラム記録媒体の実質上の多重記録性能を正しく把握することが可能である。   According to the first and third aspects of the present invention, multiple recording is performed on the hologram recording medium until a predetermined diffraction efficiency is obtained, and the limit number of times that multiple recording can be performed is measured as an evaluation characteristic. Therefore, it is possible to obtain a numerical value indicating how many times recording can be performed with good reproduction, and to correctly grasp the substantial multiplex recording performance of the hologram recording medium.

請求項2及び請求項4の発明によれば、回折効率測定用レーザ光がホログラム記録媒体の記録領域において回折したレーザ光の強度及び透過したレーザ光の強度をそれぞれ測定し、測定した回折したレーザ光の強度及び透過したレーザ光の強度により、ホログラム記録媒体の記録領域における回折効率を計算することから、各々の記録において所定の回折効率になるまで記録を行うことができ、多重記録を行える限界回数によりホログラム記録媒体の実質上の多重記録性能を正しく把握することが可能である。   According to the second and fourth aspects of the invention, the diffraction efficiency measurement laser beam measures the intensity of the laser beam diffracted in the recording area of the hologram recording medium and the intensity of the transmitted laser beam, respectively, and measures the diffracted laser. Since the diffraction efficiency in the recording area of the hologram recording medium is calculated based on the intensity of the light and the intensity of the transmitted laser beam, it is possible to perform recording until a predetermined diffraction efficiency is achieved in each recording, and the limit for performing multiple recording It is possible to correctly grasp the actual multiplex recording performance of the hologram recording medium based on the number of times.

以下、本発明の形態について図面を参照しながら具体的に説明する。図1は、本発明に係るホログラム記録媒体評価装置の一例を示す構成図である。図2は、レーザ光の照射時間に対するホログラム記録媒体の回折効率ηの変化を示した図である。図3は、η%多重数測定用プログラムにおけるホログラム記録媒体評価装置の動作を示すフローチャートである。   Hereinafter, embodiments of the present invention will be specifically described with reference to the drawings. FIG. 1 is a configuration diagram showing an example of a hologram recording medium evaluation apparatus according to the present invention. FIG. 2 is a graph showing a change in the diffraction efficiency η of the hologram recording medium with respect to the irradiation time of the laser beam. FIG. 3 is a flowchart showing the operation of the hologram recording medium evaluation apparatus in the η% multiplex number measurement program.

図において、ホログラム記録媒体5の特性を評価するホログラム記録媒体評価装置1は、レーザ光源100,110、各種光学系素子102〜112、フォトセンサ114,116、レーザ駆動回路52,54、角度制御回路62、位置制御回路64、コントローラ20、入力装置22、表示装置24等から構成されている。   In the figure, a hologram recording medium evaluation apparatus 1 for evaluating characteristics of a hologram recording medium 5 includes laser light sources 100 and 110, various optical system elements 102 to 112, photosensors 114 and 116, laser drive circuits 52 and 54, and an angle control circuit. 62, a position control circuit 64, a controller 20, an input device 22, a display device 24, and the like.

コントローラ20は、ホログラム記録媒体評価装置1の全体の制御を行うもので、データを入力するための入力装置22及び、データや各種設定を表示する表示装置24が接続されている。そして、後述するレーザ駆動回路52,54、角度制御回路62、位置制御回路64等が接続され、それらの制御を行うことで全体の制御が行われる。   The controller 20 controls the entire hologram recording medium evaluation apparatus 1, and is connected to an input device 22 for inputting data and a display device 24 for displaying data and various settings. Laser drive circuits 52 and 54, an angle control circuit 62, a position control circuit 64, and the like, which will be described later, are connected, and overall control is performed by performing these controls.

尚、以降の説明で、ホログラム記録媒体5への多重記録における各々の記録において、所定の回折効率になるまで記録を行った際の多重記録を行える限界回数を、「η%多重数」という。各々の記録におけるレーザ照射時間と回折効率の変化を図で示すと図2のようになる。多重記録を行っていくにしたがい、回折効率の上昇速度が落ちていき、ある回数までいくといくらレーザ光を照射しても所定の回折効率にまで達しない(飽和した回折効率が設定した回折効率より低い)状態になる。この状態になるまでに行った多重記録の回数が「η%多重数」である。   In the following description, the limit number of times that multiple recording can be performed when recording is performed until a predetermined diffraction efficiency is achieved in each recording in the multiplex recording on the hologram recording medium 5 is referred to as “η% multiplex number”. Changes in laser irradiation time and diffraction efficiency in each recording are shown in FIG. As multiple recording is performed, the rate of increase in diffraction efficiency decreases, and no matter how many times the laser beam is irradiated, it does not reach the specified diffraction efficiency (the diffraction efficiency set by the saturated diffraction efficiency). Lower). The number of times of multiplex recording performed until this state is reached is “η% multiplex number”.

次に、本実施例のホログラム記録媒体評価装置1の詳細な構成及び動作を説明する。まず、記録用のレーザ光源100から出射したレーザ光は、コリメートレンズ102で平行光になった後、ビームスプリッタ104で情報レーザ光と記録用参照用レーザ光に分割される。この場合の情報レーザ光は、SLM(空間光変調素子)を通していないので、実質的には情報レーザ光と記録用参照用レーザ光とは同一である。2つに分割されたレーザ光はミラー106、108で反射されて異なる角度でホログラム記録媒体5に照射され記録が行われる(この場合は情報を持たない記録)。   Next, the detailed configuration and operation of the hologram recording medium evaluation apparatus 1 of the present embodiment will be described. First, the laser light emitted from the recording laser light source 100 is collimated by the collimator lens 102 and then split by the beam splitter 104 into information laser light and recording reference laser light. Since the information laser beam in this case does not pass through the SLM (spatial light modulation element), the information laser beam and the recording reference laser beam are substantially the same. The laser beam divided into two is reflected by the mirrors 106 and 108 and irradiated onto the hologram recording medium 5 at different angles for recording (in this case, recording without information).

記録用のレーザ光とは別に、回折効率測定用レーザ光がある。回折効率測定用レーザ光のレーザ光源110から照射されたレーザ光は、コリメー卜レンズ112で平行光になった後、情報レーザ光と記録用参照用レーザ光とは異なった角度でホログラム記録媒体5に照射される。ホログラム記録媒体5で回折したレーザ光は、フォトセンサ114で受光され、透過したレーザ光はフォトセンサ116で受光されて、受光光量に相当する信号が出力される。このように構成されたホログラム記録媒体評価装置1において、作業者はホログラム記録媒体5をステージにセットした後、入力装置22からコントローラ20に、図3に示された流れのプログラムの実行を指示することにより、自動でη%多重数が測定され、表示装置24に表示されることになる。   Apart from the recording laser beam, there is a diffraction efficiency measuring laser beam. The laser light emitted from the laser light source 110 of the diffraction efficiency measurement laser light is converted into parallel light by the collimator lens 112, and then the information laser light and the recording reference laser light are at different angles at the hologram recording medium 5. Is irradiated. The laser beam diffracted by the hologram recording medium 5 is received by the photosensor 114, and the transmitted laser beam is received by the photosensor 116, and a signal corresponding to the received light amount is output. In the hologram recording medium evaluation apparatus 1 configured as described above, after the operator sets the hologram recording medium 5 on the stage, the operator instructs the controller 20 to execute the program of the flow shown in FIG. As a result, the η% multiplexing number is automatically measured and displayed on the display device 24.

以下、図3に示すフローチャートに従って説明する。尚、以後の説明において、括弧内の符号は図3のフローチャートの符号に対応している。まず、個々の記録における回折効率として設定する値X%を、適切な値(例えば1.5%)を入力装置22で入力する(S102)。次に、回折効率測定用レーザ光が照射され(S106)、記録用参照用レーザ光の照射角度(ミラーの位置と角度)が設定される(S108)。   Hereinafter, description will be given according to the flowchart shown in FIG. In the following description, the reference numerals in parentheses correspond to the reference numerals in the flowchart of FIG. First, an appropriate value (for example, 1.5%) is input from the input device 22 as a value X% set as the diffraction efficiency in each recording (S102). Next, the laser beam for measuring the diffraction efficiency is irradiated (S106), and the irradiation angle (mirror position and angle) of the recording reference laser beam is set (S108).

次に、情報レーザ光と記録用参照レーザ光の2つが照射され記録が開始される(S110)。既に回折効率測定用レーザ光は照射され、フォトセンサ114,116が検出した光量はコントローラ20に入力しているので、回折効率ηが計算される(S116)。回折効率ηがX%以上になったか確認し(S118)、なってなければ回折効率が飽和していないか確認した後(S128〜S136)、飽和していなければ計算値をクリアして(S130)、回折効率の計算(S116)に戻る。   Next, the information laser beam and the recording reference laser beam are irradiated to start recording (S110). Since the laser beam for measuring the diffraction efficiency has already been irradiated and the amount of light detected by the photosensors 114 and 116 has been input to the controller 20, the diffraction efficiency η is calculated (S116). It is confirmed whether the diffraction efficiency η is equal to or greater than X% (S118). If not, it is confirmed whether the diffraction efficiency is not saturated (S128 to S136), and if not saturated, the calculated value is cleared (S130). ), And returns to the calculation of the diffraction efficiency (S116).

そして、回折効率ηがX%以上になったときは(S118)、レーザ光を停止し(S120)、nの数を1増やし(S122)、照射時間計測を停止し、計測値をリセットして(S124)、レーザ光の照射角度(ミラーの位置と角度)を変更し(S126)、上述のレーザ光の照射(S110)に戻る。そして次の多重記録を行う。nの数が多重記録の回数になる。   When the diffraction efficiency η becomes X% or more (S118), the laser beam is stopped (S120), the number of n is increased by 1 (S122), the irradiation time measurement is stopped, and the measurement value is reset. (S124) The laser beam irradiation angle (mirror position and angle) is changed (S126), and the process returns to the above-described laser beam irradiation (S110). Then, the next multiple recording is performed. The number n is the number of times of multiple recording.

次に、回折効率が飽和していないかの確認(S128〜S136)について以下に説明する。まず、レーザ光の照射(S110)と共に計測開始(S112)した照射時間Tが、時間m・Y(時間Yはあらかじめ設定される。mは時間Yがたつごとに1ずつ増える)になったか確認し(S128)、なってなければ計算値をクリアして(S130)、回折効率の計算(S116)に戻る。なっていれば前回の回折効率ηとの差を比較する(S132)。このとき差がZ(実質的に差がないとされる値、計測精度の範囲内で予め定める)より大きければ、回折効率ηはまだ増え続けているとして今回の回折効率ηをメモリし(S134)、計算値をクリアして(S130)、回折効率の計算(S116)に戻る。前回の回折効率ηとの差がZより小さければ(S132)、時間Yの間に回折効率ηは変化していないと判断する。すなわち回折効率は飽和したと判断して、レーザ光を停止し(S138、S140)、照射時聞Tの計測を停止して(S142)、「η%多重数」としてnの値を表示装置24に表示し(S144)、プログラムを停止する。   Next, confirmation of whether the diffraction efficiency is not saturated (S128 to S136) will be described below. First, it is confirmed whether the irradiation time T when the measurement is started (S112) together with the laser beam irradiation (S110) is time m · Y (time Y is set in advance. M is incremented by 1 for each time Y). If not (S128), the calculated value is cleared (S130), and the process returns to the calculation of diffraction efficiency (S116). If so, the difference from the previous diffraction efficiency η is compared (S132). At this time, if the difference is larger than Z (a value that is not substantially different, predetermined within the range of measurement accuracy), the current diffraction efficiency η is stored as the diffraction efficiency η is still increasing (S134). ), The calculated value is cleared (S130), and the process returns to the calculation of diffraction efficiency (S116). If the difference from the previous diffraction efficiency η is smaller than Z (S132), it is determined that the diffraction efficiency η has not changed during time Y. That is, it is determined that the diffraction efficiency is saturated, the laser beam is stopped (S138, S140), the measurement of the irradiation time T is stopped (S142), and the value of n is displayed as the “η% multiplex number” on the display device 24. (S144) and the program is stopped.

上記はレーザ光の強度を一定にして回折効率が最初に設定したX%を超えずに飽和したとき、多重記録の限界と判定する方法であるが、レーザ光の強度を変化させ、多重記録の限界を判定してもよい。例えば、記録用のレーザ光の照射開始時点の回折効率の変化のスピードが落ちてきたら、それに伴いレーザ光の強度を上げていき、最初のレーザ光の強度より所定の倍率(例えば2倍)に上がったらそれ以上レーザ光の強度を上げるのをやめ、最初に設定したX%を超えずに飽和したとき、多重記録の限界と判定するようにしてもよい。   The above is a method of determining the limit of multiplex recording when the diffraction efficiency is saturated without exceeding the initially set X% with the laser beam intensity constant, but by changing the laser beam intensity, The limit may be determined. For example, when the speed of change of the diffraction efficiency at the start of irradiation of the recording laser beam decreases, the intensity of the laser beam is increased accordingly, and is set to a predetermined magnification (for example, twice) from the intensity of the first laser beam. If the laser beam intensity increases, the intensity of the laser beam is not increased any more, and if the saturation does not exceed the initially set X%, it may be determined that the limit of multiplex recording is reached.

また、飽和した回折効率に伴い、レーザ光の強度を上げていって同じようにしてもよい。さらに、回折効率が最初に設定したX%を超えずに飽和することが予想されるまで同一のレーザ光の強度にし、予想されたとき一度にそのレーザ強度より所定の倍率(例えば2倍)に上げて記録を行い、最初に設定したX%を超えずに飽和したとき、多重記録の限界と判定するようにしてもよい。   Further, the intensity of the laser beam may be increased in accordance with the saturated diffraction efficiency. Furthermore, the same laser beam intensity is used until the diffraction efficiency is expected to saturate without exceeding the initially set X%, and when expected, the laser intensity is increased to a predetermined magnification (for example, twice) at a time. It is also possible to perform recording and raise it, and when it is saturated without exceeding the initially set X%, it may be determined that there is a limit of multiple recording.

以上のように、本実施例のホログラム記録媒体評価装置1によれば、ホログラム記録媒体5に所定の回折効率になるまで多重記録を行い、多重記録を行える限界回数であるη%多重数を評価用特性として計測することから、ホログラム記録媒体5の実質上の多重記録性能を正しく把握することが可能である。すなわち、η%多重数は精度のよい再生を行なえる記録を何回多重記録することができるかを意味する特性であり、η%多重数により評価すればMナンバー(M/#)により評価するよりもホログラム記録媒体5の多重記録性能を実際の有用性に合致する値で評価することができる。   As described above, according to the hologram recording medium evaluation apparatus 1 of the present embodiment, multiplex recording is performed on the hologram recording medium 5 until a predetermined diffraction efficiency is achieved, and the η% multiplex number that is the limit number of times that multiplex recording can be performed is evaluated. Since it is measured as a characteristic for use, it is possible to correctly grasp the substantial multiplex recording performance of the hologram recording medium 5. In other words, the η% multiplex number is a characteristic that means how many times a record that can be reproduced with high accuracy can be multiplex-recorded. If it is evaluated by the η% multiplex number, it is evaluated by the M number (M / #). Rather, the multiplex recording performance of the hologram recording medium 5 can be evaluated with a value that matches the actual utility.

また、回折効率測定用レーザ光がホログラム記録媒体5の記録領域において回折したレーザ光の強度及び透過したレーザ光の強度をそれぞれ測定し、測定した回折したレーザ光の強度及び透過したレーザ光の強度により、ホログラム記録媒体5の記録領域における回折効率を計算することで、各々の記録において所定の回折効率になるまで記録を行うことができ、η%多重数によりホログラム記録媒体5の実質上の多重記録性能を正しく把握することが可能である。   Further, the intensity of the laser beam diffracted by the diffraction efficiency measurement laser beam in the recording region of the hologram recording medium 5 and the intensity of the transmitted laser beam are measured, respectively, and the measured intensity of the diffracted laser beam and the intensity of the transmitted laser beam are measured. Thus, by calculating the diffraction efficiency in the recording region of the hologram recording medium 5, it is possible to perform recording until a predetermined diffraction efficiency is obtained in each recording, and the multiplex magnification of η% is a substantial multiplexing of the hologram recording medium 5. It is possible to correctly grasp the recording performance.

以上のように、本発明によれば、ホログラム記録媒体の多重記録性能を正しく把握することが可能なホログラム記録媒体の評価装置及びホログラム記録媒体の評価方法を提供できる。   As described above, according to the present invention, it is possible to provide a hologram recording medium evaluation apparatus and a hologram recording medium evaluation method that can correctly grasp the multiplex recording performance of the hologram recording medium.

本発明に係るホログラム記録媒体評価装置の一例を示す構成図である。It is a block diagram which shows an example of the hologram recording-medium evaluation apparatus which concerns on this invention. レーザ光の照射時間に対するホログラム記録媒体の回折効率ηの変化を示した図である。It is the figure which showed the change of the diffraction efficiency (eta) of the hologram recording medium with respect to the irradiation time of a laser beam. η%多重数測定用プログラムにおけるホログラム記録媒体評価装置の動作を示すフローチャートである。10 is a flowchart showing the operation of the hologram recording medium evaluation apparatus in the η% multiplexing number measurement program.

符号の説明Explanation of symbols

1・・・・・ホログラム記録媒体評価装置
5・・・・・ホログラム記録媒体
20・・・・コントローラ
22・・・・入力装置
24・・・・表示装置
52・・・・レーザ駆動回路
54・・・・レーザ駆動回路
62・・・・角度制御回路
64・・・・位置制御回路
100・・・レーザ光源
102・・・コリメートレンズ
104・・・ビームスプリッタ
106・・・ミラー
108・・・ミラー
110・・・レーザ光源
112・・・コリメートレンズ
114・・・フォトセンサ
116・・・フォトセンサ
DESCRIPTION OF SYMBOLS 1 ... Hologram recording medium evaluation apparatus 5 ... Hologram recording medium 20 ... Controller 22 ... Input device 24 ... Display device 52 ... Laser drive circuit 54- ... Laser drive circuit 62 ... Angle control circuit 64 ... Position control circuit 100 ... Laser light source 102 ... Collimator lens 104 ... Beam splitter 106 ... Mirror 108 ... Mirror 110 ... Laser light source 112 ... Collimating lens 114 ... Photo sensor 116 ... Photo sensor

Claims (4)

ホログラム記録媒体の評価装置において、
該ホログラム記録媒体を保持するテーブルと、
該ホログラム記録媒体にデータを記録する際、該ホログラム記録媒体に記録データに相当する信号を含んだ情報レーザ光を照射する情報レーザ光照射手段と、
該ホログラム記録媒体にデータを記録する際、該ホログラム記録媒体に該情報レーザ光とは異なった角度で記録用参照レーザ光を照射する記録用参照レーザ光照射手段と、
該ホログラム記録媒体にデータを記録する際、該ホログラム記録媒体の記録領域の回折効率を測定する回折効率測定手段と、
該ホログラム記録媒体に所定の該回折効率になるまで多重記録を行い、該多重記録を行える限界回数を評価用特性として計測する多重記録限界計測手段とを備えることを特徴とするホログラム記録媒体の評価装置。
In the hologram recording medium evaluation apparatus,
A table for holding the hologram recording medium;
An information laser beam irradiation means for irradiating the hologram recording medium with an information laser beam including a signal corresponding to the recording data when recording data on the hologram recording medium;
A recording reference laser beam irradiation means for irradiating the hologram recording medium with a recording reference laser beam at an angle different from that of the information laser beam when recording data on the hologram recording medium;
Diffraction efficiency measuring means for measuring the diffraction efficiency of the recording area of the hologram recording medium when recording data on the hologram recording medium;
An evaluation of a hologram recording medium, comprising: multiple recording limit measurement means for performing multiple recording on the hologram recording medium until a predetermined diffraction efficiency is obtained, and measuring a limit number of times the multiple recording can be performed as an evaluation characteristic apparatus.
前記回折効率測定手段が、
前記情報レーザ光及び前記記録用参照レーザ光とは異なる波長の回折効率測定用レーザ光を前記ホログラム記録媒体の記録領域へ照射する回折効率測定用レーザ光照射手段と、
該回折効率測定用レーザ光が該ホログラム記録媒体の記録領域において回折したレーザ光の強度及び透過したレーザ光の強度をそれぞれ測定するレーザ光強度測定手段と、
該レーザ光強度測定手段により測定した回折したレーザ光の強度及び透過したレーザ光の強度により、該ホログラム記録媒体の記録領域における回折効率を計算する回折効率計算手段とを備えることを特徴とする請求項1記載のホログラム記録媒体の評価装置。
The diffraction efficiency measuring means is
Diffraction efficiency measurement laser light irradiation means for irradiating a recording area of the hologram recording medium with a diffraction efficiency measurement laser light having a wavelength different from that of the information laser light and the recording reference laser light;
Laser beam intensity measuring means for measuring the intensity of the laser beam diffracted by the diffraction efficiency measuring laser beam in the recording region of the hologram recording medium and the intensity of the transmitted laser beam, respectively;
And a diffraction efficiency calculating means for calculating the diffraction efficiency in the recording area of the hologram recording medium based on the intensity of the diffracted laser light measured by the laser light intensity measuring means and the intensity of the transmitted laser light. Item 2. The apparatus for evaluating a hologram recording medium according to Item 1.
ホログラム記録媒体の評価方法において、
該ホログラム記録媒体にデータを記録する際、該ホログラム記録媒体の記録領域の回折効率を測定し、
該ホログラム記録媒体に所定の該回折効率になるまで多重記録を行い、該多重記録を行える限界回数を評価用特性として計測することを特徴とするホログラム記録媒体の評価方法。
In the evaluation method of the hologram recording medium,
When recording data on the hologram recording medium, measure the diffraction efficiency of the recording area of the hologram recording medium,
A method for evaluating a hologram recording medium, comprising: performing multiplex recording on the hologram recording medium until a predetermined diffraction efficiency is obtained, and measuring a limit number of times the multiplex recording can be performed as an evaluation characteristic.
記録データに相当する信号を含んだ情報レーザ光及び該情報レーザ光とは異なった角度で照射する記録用参照レーザ光の2つのレーザ光とは異なる波長の回折効率測定用レーザ光を前記ホログラム記録媒体の記録領域へ照射し、
該回折効率測定用レーザ光が該ホログラム記録媒体の記録領域において回折したレーザ光の強度及び透過したレーザ光の強度をそれぞれ測定し、
測定した回折したレーザ光の強度及び透過したレーザ光の強度により、該ホログラム記録媒体の記録領域における回折効率を計算することを特徴とする請求項3記載のホログラム記録媒体の評価方法。
Recording hologram light with a diffraction efficiency measurement laser beam having a wavelength different from the two laser beams of an information laser beam including a signal corresponding to recording data and a recording reference laser beam irradiated at an angle different from the information laser beam Irradiate the recording area of the medium,
The diffraction efficiency measurement laser beam measures the intensity of the laser beam diffracted in the recording area of the hologram recording medium and the intensity of the transmitted laser beam, respectively.
4. The method for evaluating a hologram recording medium according to claim 3, wherein the diffraction efficiency in the recording area of the hologram recording medium is calculated from the measured intensity of the diffracted laser beam and the intensity of the transmitted laser beam.
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