JPS608956B2 - Diode array for thermal head - Google Patents
Diode array for thermal headInfo
- Publication number
- JPS608956B2 JPS608956B2 JP54119682A JP11968279A JPS608956B2 JP S608956 B2 JPS608956 B2 JP S608956B2 JP 54119682 A JP54119682 A JP 54119682A JP 11968279 A JP11968279 A JP 11968279A JP S608956 B2 JPS608956 B2 JP S608956B2
- Authority
- JP
- Japan
- Prior art keywords
- type
- parasitic
- current
- diode
- region
- 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
Links
- 239000000758 substrate Substances 0.000 claims description 24
- 238000010438 heat treatment Methods 0.000 claims description 17
- 239000004065 semiconductor Substances 0.000 claims description 7
- 230000003071 parasitic effect Effects 0.000 description 33
- 238000009792 diffusion process Methods 0.000 description 8
- 238000000034 method Methods 0.000 description 7
- 238000010586 diagram Methods 0.000 description 6
- XUIMIQQOPSSXEZ-UHFFFAOYSA-N Silicon Chemical compound [Si] XUIMIQQOPSSXEZ-UHFFFAOYSA-N 0.000 description 3
- 238000003491 array Methods 0.000 description 3
- 230000000694 effects Effects 0.000 description 3
- 229910052710 silicon Inorganic materials 0.000 description 3
- 239000010703 silicon Substances 0.000 description 3
- 238000004519 manufacturing process Methods 0.000 description 2
- 238000000926 separation method Methods 0.000 description 2
- ZOXJGFHDIHLPTG-UHFFFAOYSA-N Boron Chemical compound [B] ZOXJGFHDIHLPTG-UHFFFAOYSA-N 0.000 description 1
- 241000282373 Panthera pardus Species 0.000 description 1
- 241000270666 Testudines Species 0.000 description 1
- 229910052796 boron Inorganic materials 0.000 description 1
- 239000000969 carrier Substances 0.000 description 1
- 230000015556 catabolic process Effects 0.000 description 1
- 238000007796 conventional method Methods 0.000 description 1
- 239000013078 crystal Substances 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 239000012535 impurity Substances 0.000 description 1
- 238000002347 injection Methods 0.000 description 1
- 239000007924 injection Substances 0.000 description 1
- 239000011159 matrix material Substances 0.000 description 1
- 239000002184 metal Substances 0.000 description 1
Classifications
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10D—INORGANIC ELECTRIC SEMICONDUCTOR DEVICES
- H10D89/00—Aspects of integrated devices not covered by groups H10D84/00 - H10D88/00
- H10D89/10—Integrated device layouts
- H10D89/105—Integrated device layouts adapted for thermal considerations
Landscapes
- Electronic Switches (AREA)
- Semiconductor Memories (AREA)
Description
【発明の詳細な説明】
本発明はサーマルヘッド‘こ実装されるィンラィンに配
列された集積化されたダイオードアレイに関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an in-line integrated diode array implemented in a thermal head.
近年、ハードコピィの一手段として感熱記録方式が多用
されるようになり、感熱記録における解像度の向上のた
めに、サーマルヘッドのドット密度の向上が努力されて
いる。In recent years, thermal recording methods have come into widespread use as a means of hard copying, and efforts are being made to improve the dot density of thermal heads in order to improve resolution in thermal recording.
通常、サーマルヘッドの発熱体は、これと直列にダイオ
ードが挿入され、マトリックス構成での個々の発熱ドッ
トの相互の電気的分離がおこなわれている。Usually, a diode is inserted in series with the heating element of a thermal head, and the individual heating dots in a matrix configuration are electrically isolated from each other.
か)るサーマルヘッドの電気的接続方法を第1図に示す
が、図においてR,,R2………R64が発熱体であり
、ドット数がたとえば768ドットであれば768個の
抵抗体であらわされる。この発熱体を発熱させるために
は、Q,,Q2…・・・Q32のトランジスタスイッチ
群とQ,’,Q2′……Q%′のトランジスタスィツチ
群に信号を加えて導適状態とすることによって選択され
た抵抗体に通電発熱させるわけであるが、たとえばQ,
とQ,′のみがオン状態となった場合、Q,→R33→
R34→R2→Q,′と経由して流れないためにそれぞ
れの発熱体に直列にD,,D2・・・・・・D64で示
されるダイオード群が挿入されなければならない。この
ダイオード群は通常サーマルヘッド基板上に発熱体と一
体になって実装されるが、このためにはサーマルヘッド
密度とほぼ同じ配列密度が要求されるためたとえば図の
例ではD,〜D32,D33〜D64と云うように集積
化された32個のィンラィン配列されたダイオードアレ
イの半導体チップが24個配列されて、合計768個の
ダイオードを構成する。Fig. 1 shows the electrical connection method of the thermal head. It will be done. In order to generate heat from this heating element, a signal is applied to the transistor switch group Q,, Q2...Q32 and the transistor switch group Q,', Q2'...Q%' to make them conductive. For example, Q,
When only Q,′ and Q,′ are turned on, Q,→R33→
In order to prevent the flow from passing through R34→R2→Q,', a group of diodes shown as D, , D2, . . ., D64 must be inserted in series with each heating element. This group of diodes is usually mounted on the thermal head board integrally with the heating element, but for this purpose, an arrangement density that is almost the same as the thermal head density is required, so for example, in the example shown in the figure, D, ~ D32, D33 24 semiconductor chips of 32 in-line diode arrays integrated as D64 are arranged to form a total of 768 diodes.
従来か)るダイオードアレイの構成は、第2図に示す如
き通常の集積回路技術によってなされていた。Conventional diode arrays have been constructed using conventional integrated circuit technology as shown in FIG.
すなわち、第2図について説明するとP型のシリコン結
晶基板にN型のェピタキシャル層2を形成し、P型分離
層3によって島4及び5を形成し、その中に更にP型拡
散層6,7を形成してP型電極8とN型電極9によって
ダイオードD,を、またP型電極10とN型電極11と
によってダイオードD2を構成させていた。第2図は従
来のダイオードアレイ基体構成を説明するための概念図
であるため、実際の表面酸化膜や金属配線等については
省略してある。また、実際にはN型電極のとり出しには
N+拡散層やコレターウオールを形成したり「寄生効果
を防ぐ意味もあって埋込層を形成するがこれも図では省
略してある。さて、従来はか)る構成のダイオードアレ
イを用いていたが、実装するサーマルヘッドの4・型化
や印字ドットの高密度化にともなって、か)るダイオー
ドアレイの配列密度を高くしなければならず、高密度化
に伴って寄生効果が無視できなくなって来た。すなわち
、第1図のP,のみに発熱させるため約40mAの電流
をD,?R,に通電した場合、それ以外の発熱体が発熱
しては困るが、第2図のD,に40mAを流した場合、
P型拡散層6とN型の島領域4とP型基板1によって構
成される寄生PNPトランジスタのhFEが0.02あ
ると基板には0.8mAが流れ込み、これが基板−とN
型の島5によって構成されるPNダイオードを経てダイ
オードD2のN型電極1 1に流れ出してしまう。これ
が寄生の洩れ電流となってR2を発熱させてしまう不都
合が生じる。またD,のみでなく、D3〜D32までも
同時に通電し、D2のみがオフ状態のときには、ほぼ0
.8mA×31=24.8のAの洩れ電流が○2のN型
電極11もこ流れ出し、これがR2を流れるため、発熱
体R2が発熱し、本来現われてはならない感熱紙の所定
部が発色する。通常か)る集積化した半導体装置の寄生
トランジスタ効果を防止するために、N型ェピタキシャ
ル層の不純物濃度を増したり「厚みを増加させたり、埋
込層やコレクタウオールを入れたり、基板にAu拡散を
したりと云うことが試みられるが「これらの方策は他の
設計的条件「すなわち順方向オン電圧や耐圧との関係か
らも制約を受け、これらのダィオ−ドの配列密度が10
0ミクロンピッチともなって来ると寄生hFEを0.0
2以下に抑えることは不可能となって来る。That is, to explain FIG. 2, an N-type epitaxial layer 2 is formed on a P-type silicon crystal substrate, islands 4 and 5 are formed by a P-type separation layer 3, and a P-type diffusion layer 6, 7, a P-type electrode 8 and an N-type electrode 9 constitute a diode D, and a P-type electrode 10 and an N-type electrode 11 constitute a diode D2. Since FIG. 2 is a conceptual diagram for explaining the structure of a conventional diode array substrate, actual surface oxide films, metal wiring, etc. are omitted. Also, in reality, an N+ diffusion layer or colleter wall is formed to take out the N-type electrode, and a buried layer is formed to prevent parasitic effects, but these are also omitted in the diagram. Conventionally, a diode array with the above configuration was used, but as the thermal head to be mounted becomes 4-inch and the density of printed dots becomes higher, the arrangement density of the diode array has to be increased. First, as density increases, parasitic effects have become impossible to ignore.In other words, if a current of about 40 mA is applied to D, ?R, in order to generate heat only in P, in Figure 1, the heat generated in other areas will increase. It is a problem if the body generates heat, but if 40mA is applied to D in Figure 2,
If hFE of the parasitic PNP transistor constituted by the P-type diffusion layer 6, the N-type island region 4, and the P-type substrate 1 is 0.02, 0.8 mA flows into the substrate, and this
It flows out to the N-type electrode 11 of the diode D2 through the PN diode formed by the mold island 5. This causes a problem in that it becomes a parasitic leakage current and causes R2 to generate heat. Also, not only D, but also D3 to D32 are energized at the same time, and when only D2 is in the off state, almost 0
.. A leakage current of 8 mA x 31 = 24.8 A flows out of the N-type electrode 11 of ○2 and flows through R2, so that the heating element R2 generates heat, and a predetermined portion of the thermal paper that should not appear in the first place develops color. In order to prevent parasitic transistor effects in integrated semiconductor devices, it is necessary to increase the impurity concentration of the N-type epitaxial layer, increase the thickness, add a buried layer or collector wall, or add Au to the substrate. Attempts have been made to do things such as diffusion, but these measures are constrained by other design conditions, such as forward on-voltage and breakdown voltage, and the arrangement density of these diodes is limited to 10
When the pitch becomes 0 micron, the parasitic hFE becomes 0.0.
It becomes impossible to keep it below 2.
本発明はか)る従来の欠点にかんがみ「ダイオードアレ
イの高密度化によって問題となる寄生洩れ電流を防止し
たダイオードアレイの構造およびその後続方法を提供す
ることを目的とするものである。SUMMARY OF THE INVENTION In view of these conventional drawbacks, it is an object of the present invention to provide a diode array structure and its subsequent method that prevents the parasitic leakage current that becomes a problem due to increased density of diode arrays.
本発明は印字させるべき発熱体に直列に接続されたダイ
オードと半導体基板を経由して本来は発熱させない他の
抵抗体にいたる寄生回路とを完全に分離することによっ
て、印字電流が寄生電流を駆動することを完全に防止せ
んとしたものである。The present invention completely separates the diode connected in series to the heating element to be printed from the parasitic circuit that runs through the semiconductor substrate to other resistors that do not normally generate heat, so that the printing current drives the parasitic current. The aim is to completely prevent this from happening.
通常、半導体集積回路ではか)る寄生回路の発生を防止
するために、PN接合を用いて基板内に電気的に分離さ
れた島領域を形成し、基板を最低電位「出来れば接地電
位、島領域を最高電位に固定する。Normally, in order to prevent the generation of parasitic circuits that occur in semiconductor integrated circuits, electrically isolated island regions are formed in the substrate using PN junctions, and the substrate is placed at the lowest potential (preferably ground potential). Fix the area to the highest potential.
しかし、サーマルヘッド用ダイオードア0レィはそのサ
ーマルヘッド上に配列設置される構造上の制約から基板
を固定電位とすることが困難で「基板がフローティング
電位となっている特殊性がある。従って第1図及び第2
図の寄生回路を含めた等価回路は第3図のごとくになる
。図中の5番号は第1図、第2図に対応している。今、
Q2が開放していると、7と5で構成されているダイオ
ードD2は電流が流れず、また島領域4と基板亀と島領
域5とで構成されるNPNトランジスタはト通常極めて
hFEが小さいから、この第3図の0等価回路は更に簡
単化して第4図の如くに表現することが出来る。すなわ
ち、Q,及びQ,′が導適状態になるとP型拡散層6と
N型島領域4によって構成されるPN接合を流れる主電
流がR,を流れて発熱抵抗体R,夕を発熱させるが、P
N接合からN型島領域4に注入されたホールは一部が基
板1にも到達する。However, due to the structural limitations of the diode array for thermal heads, which are arranged and installed on the thermal head, it is difficult to set the substrate at a fixed potential. Figure 1 and 2
The equivalent circuit including the parasitic circuit shown in the figure is as shown in FIG. 3. The number 5 in the figure corresponds to FIGS. 1 and 2. now,
If Q2 is open, no current will flow through the diode D2, which is made up of 7 and 5, and the NPN transistor, which is made up of the island region 4, the substrate turtle, and the island region 5, usually has an extremely small hFE. , this 0 equivalent circuit of FIG. 3 can be further simplified and expressed as shown in FIG. 4. That is, when Q and Q,' become conductive, the main current flowing through the PN junction formed by the P-type diffusion layer 6 and the N-type island region 4 flows through R, causing the heating resistor R to generate heat. But, P
Some of the holes injected into the N-type island region 4 from the N junction also reach the substrate 1.
つまりP型拡散層6とN型島領域4とP型基板1が寄生
PNPトランジスタを構成しており、この寄生トランジ
スタの電流増中率hFEによって注入ホ−0ルの一部が
コレク夕となる基板1に流れこむ。基板1と隣りの島5
はPNダイオードとなっており、順方向にバイアスされ
ているので、基板1に流れこんだキャリアはそのまま隣
りの島5に流れこんでR2を発熱させる。夕 云いかえ
ると、発熱体R,に主電流を流すと寄生トランジスタの
hFEに応じて発熱体R2にも寄生効果洩れ電流が流れ
てしまうと云うことである。In other words, the P-type diffusion layer 6, the N-type island region 4, and the P-type substrate 1 constitute a parasitic PNP transistor, and a part of the injection hole 0 becomes a collector due to the current increase rate hFE of this parasitic transistor. It flows into the substrate 1. Board 1 and neighboring island 5
is a PN diode and is biased in the forward direction, so carriers flowing into the substrate 1 directly flow into the adjacent island 5, causing R2 to generate heat. In other words, when the main current flows through the heating element R, a parasitic effect leakage current also flows through the heating element R2 according to the hFE of the parasitic transistor.
これは正規の印字電流が寄生PNPトランジスタ0のベ
ース電流となり、このME倍の電流が隣りの発熱体にも
流れこむことを物語っている。This shows that the normal printing current becomes the base current of the parasitic PNP transistor 0, and this ME times the current also flows into the adjacent heating element.
このことは寄生電流が正規の電流で駆動されているに等
しく「その原因は正規のダイオードPN接合が寄生トラ
ンジスタのェミッタ・ベース接合を構成している点にあ
る。本発明はこの点にかんがみ、正規の電流路と寄生回
路を全く分離した点にその特長がある。This means that the parasitic current is driven by a normal current.The reason for this is that the normal diode PN junction constitutes the emitter-base junction of the parasitic transistor. Its feature is that the normal current path and the parasitic circuit are completely separated.
本発明は一般の半導体装置製造技術として周知の手段を
用い、かつ従来の寄生洩れ電流を完全に抑えた構成を提
供するものである。以下、本発明の具体的な実施例につ
き図面によって詳細に説明する。第5図は本発明の一実
施例を示すダイオードアレイの模式断面図とそのダイオ
ードアレイと発熱体抵抗との接続方法を示したものであ
る。N型のシリコン基板30の一方の面に互いに分離さ
れた複数個のP型島領域31,32,33が形成され、
そのP型島領域内にそれぞれN+型領域34,35,3
6が形成されてなるダイオードアレイD,.,D22,
D33があって、それぞれのP型島領域31,32,3
3には画信号スイッチを構成するトランジスタQ,,Q
2,Qが接続され、それぞれのN+型領域34,35,
36には発熱体抵抗R,.,R22,R33が接続され
ている。The present invention uses well-known means as a general semiconductor device manufacturing technique and provides a configuration in which conventional parasitic leakage current is completely suppressed. Hereinafter, specific embodiments of the present invention will be described in detail with reference to the drawings. FIG. 5 is a schematic cross-sectional view of a diode array showing an embodiment of the present invention and a method of connecting the diode array to a heating element resistor. A plurality of P-type island regions 31, 32, 33 are formed on one surface of an N-type silicon substrate 30, and are separated from each other.
N+ type regions 34, 35, 3 within the P type island region, respectively.
A diode array D, . ,D22,
D33, each P-type island region 31, 32, 3
3 includes transistors Q, , Q that constitute the image signal switch.
2, Q are connected, and the respective N+ type regions 34, 35,
36 is a heating element resistor R, . , R22, and R33 are connected.
Q,とQ,′が導適状態になると電源VccによってQ
,一P領域31−N十領域34−抵抗R,.−Q,′と
云う回路に電流が流れる。このためR,.が発熱して感
熱記録紙に発色を与えるわけで、Q2,Qがオフ状態な
らば、R22,R33は発色せず発色はR,.の部分だ
けとなる。この場合、ダイオードD,.には寄生回路が
並列に接続されているが、ダイオードD,.の接合はP
領域31とN+領域34の界面となるため、寄生回路の
PNPNすなわちP領域31、N型基板30、P領域3
2、N+領域35とは完全に分離されており、従来で説
明した場合のように正規の電流が寄生PNPN回路を駆
動することはない。ここで、本発明はダイオードのN側
をN+にしているのでダイオードの直列抵抗が低く、サ
ーマルヘッド用のダイオードとしての特性が向上する。
N側をN+にするためにはN型基板を用いなければ、な
らない。又、第2図の如くするとボロン表面濃度が低く
N側は島領域なのでPもNも高濃度に出来ない欠点を有
する。第6図は本実施例の等価回路である。When Q, and Q,′ become conductive, the power supply Vcc reduces Q.
, one P region 31-N ten regions 34-resistance R, . A current flows through the circuit called -Q,'. For this reason, R, . generates heat and gives color to the thermal recording paper, so if Q2 and Q are off, R22 and R33 will not develop color and R, . Only that part will be included. In this case, diodes D, . A parasitic circuit is connected in parallel to the diodes D, . The junction of is P
Since this is the interface between the region 31 and the N+ region 34, the PNPN of the parasitic circuit, that is, the P region 31, the N type substrate 30, and the P region 3
2. It is completely separated from the N+ region 35, and the normal current does not drive the parasitic PNPN circuit as in the conventional case. Here, in the present invention, since the N side of the diode is set to N+, the series resistance of the diode is low, and the characteristics as a diode for a thermal head are improved.
In order to make the N side N+, an N type substrate must be used. Further, if the structure is as shown in FIG. 2, the surface concentration of boron is low and the N side is an island region, so it has the disadvantage that it is not possible to increase the concentration of both P and N. FIG. 6 shows an equivalent circuit of this embodiment.
第4図と比較すると本発明の主旨がはっきりする。すな
わち、第4図の従釆の例ではダイオードD,が寄生PN
Pトランジスタのヱミツタ・ベースを構成し、寄生トラ
ンジスタのコレクタにR,を通電する雷流の船E倍の電
流が流れ、これがR2に流れこむ。それに対して第6図
の場合はダイオードD,.を流れる電流と寄生回路の電
流は分離されているため、R,.を流れる電流がR22
を流れる奇生PNPN電流を駆動することはなく、寄生
PNPNのターンオン電圧がVccよりも高ければQ,
のスイッチオンに対してR22に電流が流れこむことは
ない。寄生PNPNはP型島領域31、N型基板30、
隣りのP型領域32,N十領域35で構成されるがこの
Q,十Q2 を1以下にすることは容易であるからター
ンオンは容易に防げる。たとえば今第5図のダイオード
アレイのN型シリコン基板30の比抵抗をIQ−抑,P
型島領域31,32,33の比抵抗を0.50一肌,厚
みを6ミクロン、N+型領域34,35,36の拡散深
さを2ミクロン、各々の島を分離する分離拡散層(図で
は島と島の間のN型領域)の幅をマスク上で10ミクロ
ン、ダイオードアレイの燥返し配列ピッチを100ミク
ロンとし、通常の周知の集積回路技術でか)る構造を形
成したのちに全面に拡散を1000qoで20分おこな
ってキラーを導入する。A comparison with FIG. 4 will make the gist of the present invention clear. That is, in the example of the slave shown in FIG. 4, the diode D is parasitic PN.
A current E times the electric current flowing through R, which forms the emitter base of the P transistor, flows into the collector of the parasitic transistor, and this current flows into R2. On the other hand, in the case of FIG. 6, the diodes D, . Since the current flowing through R and the parasitic circuit current are separated, R, . The current flowing through R22
Q, if the parasitic PNPN turn-on voltage is higher than Vcc.
No current flows into R22 when the switch is turned on. The parasitic PNPN includes a P-type island region 31, an N-type substrate 30,
It is composed of an adjacent P-type region 32 and an N+ region 35, but since it is easy to reduce Q and N+Q2 to 1 or less, turn-on can be easily prevented. For example, the specific resistance of the N-type silicon substrate 30 of the diode array shown in FIG.
The specific resistance of the type island regions 31, 32, and 33 is 0.50 mm, the thickness is 6 microns, the diffusion depth of the N+ type regions 34, 35, and 36 is 2 microns, and a separation diffusion layer separating each island (Fig. In this case, the width of the N-type region between the islands was set to 10 microns on the mask, and the pitch of the diode array was set to 100 microns. Introduce the killer by diffusing at 1000 qo for 20 minutes.
か)るダイオードアレイを用い、発熱抵抗体の抵抗値を
3000、電源電圧Vccを16.5Vとすると、Q,
,Q,′の飽和電圧が両方で0.5Vとしてダイオード
D,.の順方向電圧降下0.9Vのとき、D,.の順方
向特性に対しR,.の負荷線を引いた特性、すなわち5
0のAの電流がR,.に流れる。従来で説明したように
、第2図の場合にはこれだけ流れると隣りのオフした状
態の抵抗にもhFE倍の電流が流れこみ、価Eが0.0
2ならば1のAが洩れ電流として隣りに流れこむ。しか
るに、本実施例では第6図でも明確なように、寄生回路
はD,.に流れる電流とは関係なく、単にVccに対し
て寄生PNPNとR22が負荷として接続された形のた
め、PNPNがターンオンしない限り単純な接合リーク
電流のみである。) using a diode array, the resistance value of the heating resistor is 3000, and the power supply voltage Vcc is 16.5V, then Q,
, Q,' are both 0.5V and the diodes D, . When the forward voltage drop of D, . For the forward characteristic of R, . Characteristics with the load line drawn, that is, 5
The current at A of 0 is R, . flows to As previously explained, in the case of Fig. 2, when this much current flows, a current times hFE flows into the adjacent resistor which is in the OFF state, and the value E becomes 0.0.
If it is 2, 1 A will flow into the neighboring area as a leakage current. However, in this embodiment, as is clear from FIG. 6, the parasitic circuits are D, . Since the parasitic PNPN and R22 are simply connected as a load to Vcc, there is only a simple junction leakage current unless the PNPN is turned on.
本実施例ではP型島領域31−N型基板30−隣りのP
型領域32で構成される寄生PNPトランジスタの電流
増中率Q,が0.001,N型基板30−隣りのP型島
領域32−その中のN十領域35で構成される寄生NP
Nトランジスタの電流増中率Q2が0.02であり、Q
,十Q2《1であるためR22に流れる電流はR,.に
流れる電流が50のAであってもわづかに0.001肌
A以下であった。従って第2図の場合と第5図の場合の
製造工程の難易度は殆んど変わらず、洩れ電流に関して
は実に千分の1に減少しその効果は著るしいものがある
。しかも更に高密度化して寄生NPNトランジスタのQ
2 が相当高くなっても、たとえば0.親華度になって
も洩れ電流には殆んど変化はなく〜従来の方式ではQが
0.8(hFEではご4)になれば洩れ電流は実に本釆
の印字電流の4倍(実際には電源の関係で電流帰還がか
かる)が流れることになり「本発明の効果は高密度化す
る程その効果は顕著になる。In this embodiment, the P-type island region 31-N-type substrate 30-adjacent P-type island region 31-N-type substrate 30-
The current increase rate Q of the parasitic PNP transistor composed of the type region 32 is 0.001, and the parasitic NP transistor composed of the N type substrate 30 - the adjacent P type island region 32 - the N0 region 35 therein
The current increase rate Q2 of the N transistor is 0.02, and Q
, 10Q2《1, so the current flowing through R22 is R, . Even if the current flowing through the tube was 50 A, it was slightly less than 0.001 A. Therefore, the difficulty of the manufacturing process in the case of FIG. 2 and the case of FIG. 5 is almost the same, and the leakage current is reduced to one thousandth, which is a remarkable effect. Moreover, with even higher density, the Q of the parasitic NPN transistor
Even if 2 becomes considerably high, for example, 0. There is almost no change in the leakage current even when the temperature becomes fertile.In the conventional method, if Q becomes 0.8 (4 for hFE), the leakage current is actually 4 times the printing current of the main button (actually Current feedback is applied due to the power source), and the effect of the present invention becomes more pronounced as the density increases.
第1図はサーマルヘッドの電気的接続方法を示す図、第
2図はサーマルヘッド用ダイオードアレイの従釆例を説
明するダイオード断面図、第3図,第4図はその等価回
路図、第6図は本発明のダイオード及び発熱体の接続方
法を示す一実施例の回路図、第6図はその等価回路を示
す図である。
30州..。
N型半導体基板、31,32,33……P型島領域、3
4, 35,36……N+型領域「R,.亨R22,R
33・…・・発熱ドット用抵抗。節1隣豹2図
繁3図
第4図
第5図
第6図Fig. 1 is a diagram showing the electrical connection method of the thermal head, Fig. 2 is a cross-sectional view of a diode explaining an example of a diode array for the thermal head, Figs. 3 and 4 are equivalent circuit diagrams, and Fig. 6 The figure is a circuit diagram of an embodiment showing a method of connecting a diode and a heating element according to the present invention, and FIG. 6 is a diagram showing an equivalent circuit thereof. 30 states. .. . N-type semiconductor substrate, 31, 32, 33...P-type island region, 3
4, 35, 36...N+ type region "R,.HoriR22,R
33... Resistor for heating dots. Section 1 Neighboring Leopard 2 Figure 3 Figure 4 Figure 5 Figure 6
Claims (1)
P型島領域と、該P型島領域内に形成されたN^+型領
域とにより形成される複数のダイオードを備え、上記ダ
イオードのそれぞれのN^+領域側に発熱ドツト用抵抗
群が接続されていることを特徴とするサーマルヘツド用
ダイオードアレイ。1 A plurality of diodes formed by a plurality of P-type island regions formed separately from each other in an N-type semiconductor substrate and an N^+-type region formed within the P-type island region, A diode array for a thermal head, characterized in that a resistance group for heating dots is connected to each N^+ region side.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP54119682A JPS608956B2 (en) | 1979-09-17 | 1979-09-17 | Diode array for thermal head |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP54119682A JPS608956B2 (en) | 1979-09-17 | 1979-09-17 | Diode array for thermal head |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5643759A JPS5643759A (en) | 1981-04-22 |
| JPS608956B2 true JPS608956B2 (en) | 1985-03-06 |
Family
ID=14767431
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP54119682A Expired JPS608956B2 (en) | 1979-09-17 | 1979-09-17 | Diode array for thermal head |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS608956B2 (en) |
Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS61135349U (en) * | 1985-02-12 | 1986-08-23 | ||
| JPS61148070U (en) * | 1985-03-06 | 1986-09-12 | ||
| JPH0236847U (en) * | 1988-09-01 | 1990-03-09 |
-
1979
- 1979-09-17 JP JP54119682A patent/JPS608956B2/en not_active Expired
Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS61135349U (en) * | 1985-02-12 | 1986-08-23 | ||
| JPS61148070U (en) * | 1985-03-06 | 1986-09-12 | ||
| JPH0236847U (en) * | 1988-09-01 | 1990-03-09 |
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5643759A (en) | 1981-04-22 |
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