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JP4338542B2 - Light receiving element - Google Patents
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JP4338542B2 - Light receiving element - Google Patents

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JP4338542B2
JP4338542B2 JP2004030008A JP2004030008A JP4338542B2 JP 4338542 B2 JP4338542 B2 JP 4338542B2 JP 2004030008 A JP2004030008 A JP 2004030008A JP 2004030008 A JP2004030008 A JP 2004030008A JP 4338542 B2 JP4338542 B2 JP 4338542B2
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concentration
light receiving
electrode
light
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JP2005223160A (en
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稲葉  昌治
晋 西村
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Sanyo Electric Co Ltd
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Tottori Sanyo Electric Co Ltd
Sanyo Electric Co Ltd
Sanyo Consumer Electronics Co Ltd
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Description

本発明は、赤外から可視光の光を受光することができる受光素子にかかわり、特に、短波長の光をモニターする用途に好適な受光素子に関する。   The present invention relates to a light receiving element that can receive visible light from infrared, and more particularly to a light receiving element suitable for use in monitoring light having a short wavelength.

赤外から赤色の波長を持つレーザ光の出力をモニターする受光素子は、シリコンからなる半導体基板に、P,N型の不純物を拡散させてPIN構造の受光素子として利用している(例えば特許文献1参照)。このような受光素子は、図10に示すように、低濃度のN型不純物を含んだシリコン製の半導体基板100の表面に、B(ボロン)等のP型不純物を高濃度に拡散させてP型高濃度不純物層101とそれらを覆う絶縁膜102を形成し、絶縁膜102の一部にコンタクトホール103を形成し、これを介してP型電極104を接続することによって一定面積の受光領域を形成する。半導体基板100の裏側にP(燐)等のN型不純物を高濃度に拡散させてN型高濃度不純物層105を形成し、これにN型電極106を接続して受光素子を構成している。   A light receiving element that monitors the output of a laser beam having a wavelength from infrared to red is used as a light receiving element having a PIN structure by diffusing P and N type impurities into a semiconductor substrate made of silicon (for example, Patent Document 1). 1). As shown in FIG. 10, such a light receiving element has a P-type impurity such as B (boron) diffused at a high concentration on the surface of a semiconductor substrate 100 made of silicon containing a low-concentration N-type impurity. A high-concentration impurity layer 101 and an insulating film 102 covering them are formed, a contact hole 103 is formed in a part of the insulating film 102, and a P-type electrode 104 is connected through the contact hole 103 to form a light-receiving region having a constant area. Form. An N-type impurity layer 105 is formed by diffusing N-type impurities such as P (phosphorus) at a high concentration on the back side of the semiconductor substrate 100, and an N-type electrode 106 is connected to the N-type impurity layer 105 to constitute a light receiving element. .

このような受光素子を波長が短い青、青紫のLEDやレーザダイオードのモニター用に用いると、受光素子表面、特に高濃度不純物層101での光吸収が大きいため、赤や赤外の波長における感度に比べて1/5程度の感度しか得られない。
特開平4−76964号公報
When such a light receiving element is used for monitoring a blue or blue-violet LED or laser diode having a short wavelength, the light absorption at the surface of the light receiving element, particularly the high-concentration impurity layer 101, is large. In comparison with this, only a sensitivity of about 1/5 can be obtained.
Japanese Patent Laid-Open No. 4-76964

そこで本発明は、受光素子の感度を高め、青や青紫の短波長の光を効率的に受光して感度を高めること、並びにそれに適した構造を提供することを課題とする。   Therefore, an object of the present invention is to increase the sensitivity of a light receiving element, efficiently receive light of blue or blue-violet short wavelength light, increase the sensitivity, and provide a structure suitable for it.

本発明の受光素子は請求項1に記載の様に、低不純物濃度の半導体基板に高濃度の一導電型不純物層と逆導電型不純物層を形成し、電極に接続した一導電型の高濃度不純物層を基板表面に配置して一定面積の受光領域を形成したPN型あるいはPIN型の受光素子において、前記受光領域の中に前記半導体基板の低濃度不純物層が基板表面に露出する低濃度層露出領域を複数形成し、これらの低濃度層露出領域を前記受光領域に分散して配置するとともに、前記電極に接続した高濃度不純物層を前記電極を中心として前記受光領域の全体に亘って放射状に延びるように配置し、前記電極を前記受光領域の中央に配置し、この電極を囲むように前記低濃度層露出領域を分散して配置したことを特徴とする。 As described in claim 1, the light receiving element of the present invention has a high concentration of one conductivity type formed by forming a high concentration one conductivity type impurity layer and a reverse conductivity type impurity layer on a semiconductor substrate having a low impurity concentration and connecting to the electrode. In a PN-type or PIN-type light-receiving element in which a light-receiving region having a certain area is formed by arranging an impurity layer on the substrate surface, a low-concentration layer in which the low-concentration impurity layer of the semiconductor substrate is exposed on the substrate surface in the light-receiving region A plurality of exposed regions are formed, and these low-concentration layer exposed regions are arranged in a dispersed manner in the light-receiving region, and a high-concentration impurity layer connected to the electrode is radiated over the light-receiving region around the electrode. The electrode is arranged in the center of the light receiving region, and the low concentration layer exposed regions are distributed and arranged so as to surround the electrode .

本発明によれば、短波長の光であっても受光素子表面での光吸収が抑制されるので、感度を高めることができる。電極を受光領域の中央に配置し、この電極を囲むように前記低濃度層露出領域を分散して配置し、露出領域と高濃度層の配置を適正化することによって、感度を高めるに適した構造を提供することができる。特に、高濃度不純物層を電極を中心として受光領域の全体に亘って放射状に延びるように配置したので、光電流を高濃度不純物層によって効率よく電極に集めることができる。 According to the present invention, since light absorption on the surface of the light receiving element is suppressed even for light with a short wavelength, sensitivity can be increased. An electrode is arranged in the center of the light receiving region, the low-concentration layer exposed region is dispersed and arranged so as to surround the electrode, and the arrangement of the exposed region and the high-concentration layer is optimized, so that it is suitable for increasing sensitivity. Structure can be provided. In particular, since the high-concentration impurity layer is disposed so as to extend radially over the entire light receiving region with the electrode as the center, the photocurrent can be efficiently collected on the electrode by the high-concentration impurity layer.

以下本発明の実施形態を図面を参照して説明する。図1は本発明の一実施形態を示す平面図、図2は図1のA−Aに沿った断面図、図3は図1のB−Bに沿った断面図である。これらの図において、受光素子1は、低濃度の不純物を含んだシリコン製の半導体基板2にP型とN型の不純物を拡散させてPN型あるいはPIN型の受光素子としている。   Embodiments of the present invention will be described below with reference to the drawings. 1 is a plan view showing an embodiment of the present invention, FIG. 2 is a cross-sectional view taken along line AA in FIG. 1, and FIG. 3 is a cross-sectional view taken along line BB in FIG. In these figures, the light receiving element 1 is a PN type or PIN type light receiving element by diffusing P-type and N-type impurities into a silicon semiconductor substrate 2 containing low-concentration impurities.

半導体基板2は、I層として機能するに必要な低濃度の不純物を含む単結晶シリコンによって構成している。半導体基板2はN型とされ、その不純物濃度は例えば4×1012cm-3以下としている。 The semiconductor substrate 2 is made of single crystal silicon containing low-concentration impurities necessary to function as an I layer. The semiconductor substrate 2 is N-type, and its impurity concentration is, for example, 4 × 10 12 cm −3 or less.

半導体基板2の表面の大部分に、所定形状の拡散マスクを用いてB(ボロン)等のP型不純物を高濃度に拡散させることによってP型高濃度不純物層3を形成している。P型高濃度不純物層3の厚さは1〜2μmとされ、不純物濃度は例えば約1×1020cm-3としている。このP型高濃度不純物層3が半導体基板2の表面に一定面積の受光領域4を形成する。P型高濃度不純物層3が形成された半導体基板2の表面を覆うように、窒化シリコンや酸化シリコン等からなる絶縁膜5を形成している。受光領域4上の絶縁膜5の一部にコンタクトホール6を形成し、これを介してP型電極7をP型高濃度不純物層3にオーミック接続している。半導体基板2の裏側にP(リン)等のN型不純物を高濃度に拡散させてN型高濃度不純物層8を形成し、これにN型電極9をオーミック接続している。N型高濃度不純物層8の厚さは20〜50μmとされ、不純物濃度は例えば約1×1020cm-3としている。 A P-type high-concentration impurity layer 3 is formed on most of the surface of the semiconductor substrate 2 by diffusing P-type impurities such as B (boron) at a high concentration using a diffusion mask having a predetermined shape. The thickness of the P-type high concentration impurity layer 3 is 1 to 2 μm, and the impurity concentration is, for example, about 1 × 10 20 cm −3 . The P-type high concentration impurity layer 3 forms a light receiving region 4 having a certain area on the surface of the semiconductor substrate 2. An insulating film 5 made of silicon nitride, silicon oxide or the like is formed so as to cover the surface of the semiconductor substrate 2 on which the P-type high concentration impurity layer 3 is formed. A contact hole 6 is formed in a part of the insulating film 5 on the light receiving region 4, and the P-type electrode 7 is ohmically connected to the P-type high concentration impurity layer 3 through the contact hole 6. N-type impurities such as P (phosphorus) are diffused at a high concentration on the back side of the semiconductor substrate 2 to form an N-type high-concentration impurity layer 8, and an N-type electrode 9 is ohmically connected thereto. The thickness of the N-type high concentration impurity layer 8 is 20 to 50 μm, and the impurity concentration is, for example, about 1 × 10 20 cm −3 .

通常の場合、受光領域4は一導電型(この例ではP型)の不純物層で埋め尽くされるが、この不純物層が光(特に青色〜青紫の波長付近の短波長)の吸収層として作用するので、本発明ではその光吸収を抑制するための低濃度層露出領域10を受光領域4に複数形成している。この低濃度層露出領域10は、前記半導体基板2を構成する低濃度不純物層が基板表面に露出することによって構成される。低濃度層露出領域10は、高濃度不純物層3を選択拡散によって形成する際のマスクパターンの形状を変更することによって形成される。この実施形態は、低濃度層露出領域10を微小な正方形状あるいは長方形状とし、それらを受光領域4の略全体にわたって2次元のマトリックス状に分散して配列している。よって、受光領域に入射する光の一部は、この低濃度層露出領域10を通って入射するので、高濃度不純物層3における光吸収が抑制される。   In a normal case, the light receiving region 4 is filled with an impurity layer of one conductivity type (P type in this example), but this impurity layer acts as an absorption layer for light (especially near a wavelength of blue to blue-violet). Therefore, in the present invention, a plurality of low concentration layer exposed regions 10 for suppressing the light absorption are formed in the light receiving region 4. The low concentration layer exposed region 10 is formed by exposing a low concentration impurity layer constituting the semiconductor substrate 2 to the substrate surface. The low-concentration layer exposed region 10 is formed by changing the shape of the mask pattern when the high-concentration impurity layer 3 is formed by selective diffusion. In this embodiment, the low-concentration layer exposed region 10 is formed into a minute square shape or rectangular shape, and these are dispersed and arranged in a two-dimensional matrix shape over substantially the entire light receiving region 4. Therefore, part of the light incident on the light receiving region is incident through the low concentration layer exposed region 10, so that light absorption in the high concentration impurity layer 3 is suppressed.

前記電極間に一定の逆バイアスを印加させると、半導体基板のI層として機能する低濃層部分において、入射した光のエネルギーによって正負のキャリアが発生し、前記逆バイアスによって正負キャリアが各々P、N高濃度不純物層の一方に移動することによって光電流が発生する。このような光電変換によって入射した光が電気に変換される。   When a constant reverse bias is applied between the electrodes, positive and negative carriers are generated by the energy of incident light in the low-concentration layer portion functioning as the I layer of the semiconductor substrate. A photocurrent is generated by moving to one of the N high-concentration impurity layers. Incident light is converted into electricity by such photoelectric conversion.

図4、5は、低濃度層露出領域10の形状を変更した別の実施形態を示す。他の構成は先の実施形態と同じであるので、相違点を中心に説明する。図4に示す実施形態は、低濃度層露出領域10の形状を帯状として前記受光領域4に一定の方向に分散して配置したことを特徴とする。低濃度層露出領域10を受光領域4に分散して配置することによって、受光領域の全体に亘って光の変換効率を高めることができる。   4 and 5 show another embodiment in which the shape of the low-concentration layer exposed region 10 is changed. Since other configurations are the same as those of the previous embodiment, the differences will be mainly described. The embodiment shown in FIG. 4 is characterized in that the low-concentration layer exposed region 10 has a strip shape and is distributed in the light receiving region 4 in a certain direction. By disposing the low-concentration layer exposed region 10 in the light receiving region 4, the light conversion efficiency can be enhanced over the entire light receiving region.

図5に示す実施形態は、低濃度層露出領域10を帯状として前記受光領域に複数の方向に分散して配置したことを特徴とする。すなわち、縦長と横長の低濃度層露出領域10を受光領域4の対角線の一方を境界に区分けして配置したことを特徴とする。低濃度層露出領域10を受光領域4に分散して配置することによって、受光領域4の全体に亘って光の変換効率を高めることができる。   The embodiment shown in FIG. 5 is characterized in that the low-concentration layer exposed region 10 is arranged in a strip shape and dispersed in a plurality of directions in the light receiving region. That is, it is characterized in that the vertically and horizontally long low-concentration layer exposed regions 10 are arranged by dividing one of the diagonal lines of the light receiving region 4 as a boundary. By disposing the low-concentration layer exposed region 10 in the light receiving region 4, the light conversion efficiency can be improved over the entire light receiving region 4.

図1、図5に示す実施形態は、電極7を中心として高濃度不純物層3(低濃度層露出領域10と10の間に位置する)が放射状に延びている点で共通している。このように高濃度不純物層3が電極7を中心として受光領域4の全体に亘って放射状に延びているので、光電流を高濃度不純物層3によって効率よく電極7に集めることができる。   The embodiment shown in FIGS. 1 and 5 is common in that the high-concentration impurity layer 3 (located between the low-concentration layer exposed regions 10 and 10) extends radially around the electrode 7. Thus, since the high concentration impurity layer 3 extends radially over the entire light receiving region 4 with the electrode 7 as the center, the photocurrent can be efficiently collected on the electrode 7 by the high concentration impurity layer 3.

図6、7は、低濃度層露出領域10の形状と電極7の配置を変更したさらに別の実施形態を示す。ここで、図7は、図6のC−Cに沿った断面図である。他の構成は先の実施形態と同じであるので、相違点を中心に説明する。図6、7に示す実施形態は、電極7を受光領域4の中央部に配置し、この電極7を囲むように低濃度層露出領域10を環状に分散配置したことを特徴とする。低濃度層露出領域10を受光領域4に分散して配置することによって、受光領域の全体に亘って光の変換効率を高めることができる。電極7を囲むように配置した低濃度層露出領域10を完全な環ではなく、その一部が高濃度不純物層3によって分断された形状とすることによって、図1,5に示す形態と同様に、高濃度不純物層3が電極7を中心として受光領域4の全体に亘って放射状に延びた形態とすることができるので、光電流を高濃度不純物層3によって効率よく電極7に集めることができる。   6 and 7 show still another embodiment in which the shape of the low-concentration layer exposed region 10 and the arrangement of the electrodes 7 are changed. Here, FIG. 7 is a cross-sectional view taken along the line CC of FIG. Since other configurations are the same as those of the previous embodiment, the differences will be mainly described. The embodiment shown in FIGS. 6 and 7 is characterized in that the electrode 7 is disposed at the center of the light receiving region 4 and the low-concentration layer exposed regions 10 are annularly distributed so as to surround the electrode 7. By disposing the low-concentration layer exposed region 10 in the light receiving region 4, the light conversion efficiency can be enhanced over the entire light receiving region. The low-concentration layer exposed region 10 arranged so as to surround the electrode 7 is not a complete ring, but a part thereof is divided by the high-concentration impurity layer 3, so that the configuration shown in FIGS. Since the high-concentration impurity layer 3 can be configured to extend radially over the entire light receiving region 4 around the electrode 7, the photocurrent can be efficiently collected on the electrode 7 by the high-concentration impurity layer 3. .

図8、9は高濃度不純物層8と電極9の形状と配置を変更したさらに別の実施形態を示す。ここで、図9は、図8のD−Dに沿った断面図である。他の構成は先の実施形態と同じであるので、相違点を中心に説明する。図8,9に示す実施形態は、半導体基板2の裏側に配置していた高濃度不純物層8と電極9を電極7とともに半導体基板2の表側に配置したことを特徴とする。高濃度不純物層8は、受光領域4の外側に一定の間隔を持って環状に配置している。電極9は、絶縁膜に形成したコンタクトホールを介して高濃度不純物層8にオーミック接続している。電極7,9を同一面に配置することによって、電極配置の自由度を高めることができる。また、PN層の配置が、図1から7に示す実施形態では基板の厚さ方向であるのに対して、図8,9に示す実施形態では基板の表面と同方向であるので、PN接合の配置自由度を高めることができる。   8 and 9 show still another embodiment in which the shape and arrangement of the high concentration impurity layer 8 and the electrode 9 are changed. Here, FIG. 9 is a cross-sectional view taken along the line DD of FIG. Since other configurations are the same as those of the previous embodiment, the differences will be mainly described. The embodiment shown in FIGS. 8 and 9 is characterized in that the high concentration impurity layer 8 and the electrode 9 arranged on the back side of the semiconductor substrate 2 are arranged on the front side of the semiconductor substrate 2 together with the electrode 7. The high-concentration impurity layer 8 is annularly arranged outside the light receiving region 4 with a certain interval. The electrode 9 is ohmically connected to the high concentration impurity layer 8 through a contact hole formed in the insulating film. By arranging the electrodes 7 and 9 on the same plane, the degree of freedom of electrode arrangement can be increased. In addition, since the arrangement of the PN layer is in the thickness direction of the substrate in the embodiments shown in FIGS. 1 to 7, the PN junction is in the same direction as the surface of the substrate in the embodiments shown in FIGS. The degree of freedom of arrangement can be increased.

上記実施形態においては、低濃度層露出領域10を拡散マスクの変更によって選択的に形成したので、半導体基板2の表面が平坦となる。
低濃度層露出領域10は、受光領域4の前面に高濃度不純物層を形成後に、この層を選択的に除去して基板表面に凹凸を形成することによって形成することも可能である。上記実施形態はシリコン半導体を用いる場合を例示したが、それ以外の半導体を用いて受光素子を形成する場合にも本発明を適用することができる。また、上記の不純物のP、Nの極性を反対の極性に変更することもできる。
In the above embodiment, since the low-concentration layer exposed region 10 is selectively formed by changing the diffusion mask, the surface of the semiconductor substrate 2 becomes flat.
The low-concentration layer exposed region 10 can also be formed by forming a high-concentration impurity layer on the front surface of the light-receiving region 4 and then selectively removing this layer to form irregularities on the substrate surface. In the above embodiment, the case where a silicon semiconductor is used has been exemplified. However, the present invention can also be applied to the case where a light receiving element is formed using another semiconductor. Further, the polarities of P and N of the impurities can be changed to opposite polarities.

赤外から可視光に受光感度を持つ受光素子に利用することができる。青色から青紫に波長を有するLEDやレーザダイオードのモニター用の受光素子として利用することができる。   It can be used for a light receiving element having light receiving sensitivity from infrared to visible light. It can be used as a light-receiving element for monitoring LEDs or laser diodes having a wavelength from blue to blue-violet.

本発明の一実施形態を示す平面図である。It is a top view which shows one Embodiment of this invention. 図1のA−Aに沿った断面図である。FIG. 2 is a cross-sectional view taken along AA in FIG. 1. 図1のB−Bに沿った断面図である。It is sectional drawing along BB of FIG. 本発明の別の実施形態を示す平面図である。It is a top view which shows another embodiment of this invention. 本発明の別の実施形態を示す平面図である。It is a top view which shows another embodiment of this invention. 本発明の別の実施形態を示す平面図である。It is a top view which shows another embodiment of this invention. 図6のC−Cに沿った断面図である。It is sectional drawing along CC of FIG. 本発明の別の実施形態を示す平面図である。It is a top view which shows another embodiment of this invention. 図8のD−Dに沿った断面図である。It is sectional drawing along DD of FIG. 従来例を示す断面図である。It is sectional drawing which shows a prior art example.

符号の説明Explanation of symbols

1 受光素子
2 半導体基板
3 一導電型高濃度不純物層
4 受光領域
5 絶縁膜
6 コンタクトホール
7 電極
8 逆導電型高濃度不純物層
9 電極
10 低濃度層露出領域
DESCRIPTION OF SYMBOLS 1 Light receiving element 2 Semiconductor substrate 3 One conductivity type high concentration impurity layer 4 Light receiving region 5 Insulating film 6 Contact hole 7 Electrode 8 Reverse conductivity type high concentration impurity layer 9 Electrode 10 Low concentration layer exposure region

Claims (1)

低不純物濃度の半導体基板に高濃度の一導電型不純物層と逆導電型不純物層を形成し、電極に接続した一導電型の高濃度不純物層を基板表面に配置して一定面積の受光領域を形成したPN型あるいはPIN型の受光素子において、前記受光領域の中に前記半導体基板の低濃度不純物層が基板表面に露出する低濃度層露出領域を複数形成し、これらの低濃度層露出領域を前記受光領域に分散して配置するとともに、前記電極に接続した高濃度不純物層を前記電極を中心として前記受光領域の全体に亘って放射状に延びるように配置し、前記電極を前記受光領域の中央に配置し、この電極を囲むように前記低濃度層露出領域を分散して配置したことを特徴とする受光素子。 A high-concentration one-conductivity-type impurity layer and a reverse-conductivity-type impurity layer are formed on a low-impurity concentration semiconductor substrate, and the one-conductivity-type high-concentration impurity layer connected to the electrode is disposed on the substrate surface to form a light-receiving region having a certain area. In the formed PN-type or PIN-type light-receiving element, a plurality of low-concentration layer exposed regions in which the low-concentration impurity layer of the semiconductor substrate is exposed on the substrate surface are formed in the light-receiving region. Dispersed and arranged in the light receiving region, a high-concentration impurity layer connected to the electrode is arranged so as to extend radially over the entire light receiving region around the electrode, and the electrode is arranged in the center of the light receiving region The light-receiving element is characterized in that the low-concentration layer exposed region is dispersed and arranged so as to surround the electrode .
JP2004030008A 2004-02-06 2004-02-06 Light receiving element Expired - Fee Related JP4338542B2 (en)

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JP4338542B2 true JP4338542B2 (en) 2009-10-07

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