JPH025202A - Digital magnetic recording device - Google Patents
Digital magnetic recording deviceInfo
- Publication number
- JPH025202A JPH025202A JP15588788A JP15588788A JPH025202A JP H025202 A JPH025202 A JP H025202A JP 15588788 A JP15588788 A JP 15588788A JP 15588788 A JP15588788 A JP 15588788A JP H025202 A JPH025202 A JP H025202A
- Authority
- JP
- Japan
- Prior art keywords
- circuit
- recording device
- magnetic recording
- digital magnetic
- pass
- 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.)
- Pending
Links
- 238000010586 diagram Methods 0.000 description 9
- 238000007493 shaping process Methods 0.000 description 3
- 230000007423 decrease Effects 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 239000000696 magnetic material Substances 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
- 238000000034 method Methods 0.000 description 1
Landscapes
- Digital Magnetic Recording (AREA)
- Signal Processing For Digital Recording And Reproducing (AREA)
Abstract
(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.
Description
【発明の詳細な説明】 [産業上の利用分野] 本発明は、ディジタル磁気記録装置に関する。[Detailed description of the invention] [Industrial application field] The present invention relates to a digital magnetic recording device.
[従来の技術]
従来、ディジタル磁気記録装置では、第6図に示すよう
に、記録媒体1より磁気ヘッド2により再生された信号
をアンプ3により増幅して、低域通過回路4により高域
の雑音を除去し微分器6により微分し、波形整形回路7
により零クロス点を検出しディジタルデータ8としてい
た。[Prior Art] Conventionally, in a digital magnetic recording device, as shown in FIG. After removing noise and differentiating it with a differentiator 6, the waveform shaping circuit 7
The zero cross point was detected as digital data 8.
[発明の解決しようとする課題及び目的]しかし、かか
る再生回路では、装置の記録容量を上げるため、線記録
密度を上げようとすると、磁気ヘッドのギャップ長の狭
小化や記録媒体の磁性体の膜厚の薄膜化などの製造技術
上の困難を伴う方法しかないという問題があった。[Problems and objects to be solved by the invention] However, in such a reproducing circuit, when trying to increase the linear recording density in order to increase the recording capacity of the device, it is necessary to narrow the gap length of the magnetic head and to increase the magnetic material of the recording medium. There has been a problem in that the only methods that involve difficulties in manufacturing technology such as thinning the film are available.
そこで、本発明はこのような問題を解決するもので、そ
の目的とするところは、線記録密度の向上により、装置
の記録容量を増大する手段を提供するところにある。The present invention is intended to solve these problems, and its purpose is to provide a means for increasing the recording capacity of an apparatus by improving the linear recording density.
[課題を解決するための手段]
本発明のディジタル磁気記#装置は、再生信号帯域の高
周波部分を強調する回路と位相特性のみに影響を与える
いわゆる全域通過回路を組合せた再生回路を持つ事を特
徴とする。[Means for Solving the Problems] The digital magnetic recording device of the present invention has a reproducing circuit that combines a circuit that emphasizes the high frequency portion of the reproduced signal band and a so-called all-pass circuit that affects only the phase characteristics. Features.
[作用]
本発明の上記の構成によれば、再生信号の高域部分の*
gにより、再生信号の帯域が広がるため、線記録密度を
上げる事ができる。又、通常の高域強調回路では、位相
特性に企みが生じろため再生波形に歪みが生じるが、全
域通常回路・に、1り補正することにより歪みの彫響を
消す事が・Cきる。[Operation] According to the above configuration of the present invention, *
Since the band of the reproduced signal is widened by g, the linear recording density can be increased. In addition, in a normal high frequency emphasizing circuit, distortion occurs in the reproduced waveform due to a change in the phase characteristics, but by making one correction in the full range normal circuit, it is possible to eliminate the distortion.
[実施例]
第1図は、本発明の実施例の再生回路のゾl−Jツク図
である。記録媒体lと磁劇、、〜・ラド2 +: J、
り再生される信号はア〕/プ3により増幅され、高域強
調された低域通過回路!〕を通り、位相特性ヌζ犬、−
1と等価な遅延特性を補正“する全域通過11□11路
2豊:: J:り波形歪みを除去されで、微分器6と波
形整形回路7によりディジタルデータ8となる。低域通
過回路9と全域通過回路5のJi(波数特性Lt第2図
(a)、第2図(b)のようになり・Cいる。実線は、
両回路の合計の特性であり、破線は、低域通過回路のみ
の特性であンi
第3図は、実施例の各部の信号波影図“eある、アンプ
出力信号13では、高域流、分が少ないため、波形器干
渉が大きな波形であるが、高域強調された低域通過回路
9を通る事により、信号の高域りは強調され低域通過凹
陥出力信号14では1、波形量子)jl;が少なくなり
、線記録密度をトげる事がCきろ波形となる遅延特性の
歪みにユリ波形は歪んで・いる。ごこれを全域通過回路
5を通ず事にJ、す、その出力1;5では、波形歪みを
とることができる。[Embodiment] FIG. 1 is a block diagram of a reproducing circuit according to an embodiment of the present invention. Recording medium l and magnetic drama, ... Rad 2 +: J,
The signal that is played back is amplified by A/P 3 and a low-pass circuit that emphasizes the high frequencies! ], the phase characteristic nuζdog, −
All-pass 11 □ 11-way 2 Toyo:: J: Corrects the delay characteristics equivalent to 1. The waveform distortion is removed, and the digital data 8 is obtained by the differentiator 6 and the waveform shaping circuit 7. The low-pass circuit 9 and Ji of the all-pass circuit 5 (wave number characteristics Lt are as shown in FIGS. 2(a) and 2(b).The solid line is
The broken line is the characteristic of only the low-pass circuit. Figure 3 is a signal wave shadow diagram of each part of the embodiment. , the waveform has a large interference with the waveformer due to the small number of minutes, but by passing through the high-frequency emphasized low-pass circuit 9, the high frequency of the signal is emphasized, and the low-pass concave output signal 14 has a waveform of 1. The Yuri waveform is distorted due to the distortion of the delay characteristic, which becomes the C waveform as the linear recording density decreases and the linear recording density increases.By passing this through the all-pass circuit 5, , its output 1;5 can take waveform distortion.
この、J:うな、全・域通過回路(“シは、第4図又は
第5)図のJ:う(、”′構成することがでさる。This can be constructed by constructing an all-pass circuit (Fig. 4 or 5).
上の実施例では、低域通過回路9に16号の高域強調の
役目を負わゼたが、通常の微53器では、その特性は完
全な微分ど、低域通過特性の和となつ凌゛いるため、微
分器に);り信号のρ1域強調をする事もできる。In the above embodiment, the low-pass circuit 9 has the role of emphasizing the high frequency range of No. 16, but in a normal differential amplifier, its characteristics are completely differentiated, and are superior to the sum of the low-pass characteristics. Since there is a ρ1 region in the differentiator, it is also possible to emphasize the ρ1 region of the signal.
又、微分器+3を゛ア゛ン/3に扮え配置する構成も可
能”11ある、
[発明の効果]
以上述べたように本発明によれば、磁気ヘッドの再生信
号の高j壱を強、:li、l [、、ごれに全域通過回
路に、I:9波形歪みの11ト正を行う事により、線記
録密度の向」二を行)事が′C−きる。It is also possible to have a configuration in which the differentiator +3 is arranged as an /3. Strong, :li,l [,,By correcting the I:9 waveform distortion in the all-pass circuit, the direction of the linear recording density can be increased.
第1図は、本発明の実施例の再生回路のグロック図。
第2図(a)は、本発明の再生回y);・の利得の周り
、ケ数特性図。第2図(b)は、本発明の再生回路の遅
延時間の周波数特性図。
第3図は、本発明の実施例の各部の信号波形図6第4図
は、本発明で使用する全域通過回路を示す構成図。
第5図は、本発明で使用する他の仝城通過l−11路を
示す構成図。
第6図は、従来の再生回路のブロック図“Pある。
:1・・・高域強調さi′シた低域通過回路量 上
出1!11人 士イ:J−エプソン株式会社代理人 1
1理士 鉛本喜二部 他1名磁苑、媒体
磁気ヘッド
アンプ
1氏域通過回路
全域通過回路
11分器
波形整形回路
デイジタルデーク
第
図
第
図
(α)
第
図(b)
第
図FIG. 1 is a block diagram of a reproducing circuit according to an embodiment of the present invention. FIG. 2(a) is a characteristic diagram of the number of reproduction times around the gain of the present invention. FIG. 2(b) is a frequency characteristic diagram of delay time of the reproducing circuit of the present invention. FIG. 3 is a diagram of signal waveforms at various parts in an embodiment of the present invention. FIG. 4 is a configuration diagram showing an all-pass circuit used in the present invention. FIG. 5 is a configuration diagram showing another I-11 road passing through the city used in the present invention. Figure 6 is a block diagram of a conventional reproduction circuit. 1
1 Physician Kijibu Hinamoto 1 other person Soen, media Magnetic head amplifier 1 Range pass circuit Full range pass circuit 11 Divider waveform shaping circuit Digital data Fig. (α) Fig. (b) Fig.
Claims (1)
みに影響を与えるいわゆる全域通過回路を組合せた再生
回路を持つ事を特徴とするディジタル磁気記録装置。A digital magnetic recording device characterized by having a reproducing circuit that combines a circuit that emphasizes the high frequency portion of the reproduced signal band and a so-called all-pass circuit that affects only the phase characteristics.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP15588788A JPH025202A (en) | 1988-06-23 | 1988-06-23 | Digital magnetic recording device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP15588788A JPH025202A (en) | 1988-06-23 | 1988-06-23 | Digital magnetic recording device |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH025202A true JPH025202A (en) | 1990-01-10 |
Family
ID=15615676
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP15588788A Pending JPH025202A (en) | 1988-06-23 | 1988-06-23 | Digital magnetic recording device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH025202A (en) |
-
1988
- 1988-06-23 JP JP15588788A patent/JPH025202A/en active Pending
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