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JP6743752B2 - Method for manufacturing semiconductor device - Google Patents
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JP6743752B2 - Method for manufacturing semiconductor device - Google Patents

Method for manufacturing semiconductor device Download PDF

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JP6743752B2
JP6743752B2 JP2017083592A JP2017083592A JP6743752B2 JP 6743752 B2 JP6743752 B2 JP 6743752B2 JP 2017083592 A JP2017083592 A JP 2017083592A JP 2017083592 A JP2017083592 A JP 2017083592A JP 6743752 B2 JP6743752 B2 JP 6743752B2
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semiconductor substrate
semiconductor device
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JP2018182221A (en
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春彦 南竹
春彦 南竹
川瀬 祐介
祐介 川瀬
和徳 金田
和徳 金田
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Mitsubishi Electric Corp
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    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10DINORGANIC ELECTRIC SEMICONDUCTOR DEVICES
    • H10D62/00Semiconductor bodies, or regions thereof, of devices having potential barriers
    • H10D62/50Physical imperfections
    • H10D62/53Physical imperfections the imperfections being within the semiconductor body 
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10PGENERIC PROCESSES OR APPARATUS FOR THE MANUFACTURE OR TREATMENT OF DEVICES COVERED BY CLASS H10
    • H10P34/00Irradiation with electromagnetic or particle radiation of wafers, substrates or parts of devices
    • H10P34/40Irradiation with electromagnetic or particle radiation of wafers, substrates or parts of devices with high-energy radiation
    • H10P34/42Irradiation with electromagnetic or particle radiation of wafers, substrates or parts of devices with high-energy radiation with electromagnetic radiation, e.g. laser annealing
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10DINORGANIC ELECTRIC SEMICONDUCTOR DEVICES
    • H10D12/00Bipolar devices controlled by the field effect, e.g. insulated-gate bipolar transistors [IGBT]
    • H10D12/411Insulated-gate bipolar transistors [IGBT]
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10DINORGANIC ELECTRIC SEMICONDUCTOR DEVICES
    • H10D8/00Diodes

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  • Electrodes Of Semiconductors (AREA)

Description

本発明は、電磁波を照射して半導体基板を局所的に加熱する半導体装置の製造方法に関する。 The present invention relates to a method of manufacturing a semiconductor device, which locally irradiates an electromagnetic wave to heat a semiconductor substrate.

絶縁ゲート型バイポーラトランジスタ(IGBT)では、スイッチオフ時の残留少数キャリアの消滅を早くして高周波に対応させるために、キャリアのライフタイムを短くする必要がある。ライフタイムを短くする方法の一つとして、電子線、プロトン、ヘリウム等の荷電粒子の照射により半導体基板に結晶欠陥を意図的に導入する方法が広く用いられている。しかし、IGBTの全体に結晶欠陥が必要なわけではなく、例えば通電しない終端領域においては、結晶欠陥が耐圧の低下を引き起こすため、局所的に結晶欠陥を導入しない。また、IGBTとダイオードを1チップに集積化してモジュールの小型化を実現しているRC−IGBT(逆導通IGBT)においても、IGBT領域はライフタイムを短くしたいが、ダイオード領域は短くしたくない。このため、局所的に結晶欠陥を導入する技術が求められている。 In the insulated gate bipolar transistor (IGBT), it is necessary to shorten the carrier lifetime in order to expedite the disappearance of the remaining minority carriers when the switch is turned off and to cope with a high frequency. As one of the methods of shortening the lifetime, a method of intentionally introducing crystal defects into a semiconductor substrate by irradiating charged particles such as electron beams, protons and helium is widely used. However, crystal defects are not required for the entire IGBT. For example, crystal defects are not locally introduced in the termination region where no current flows because crystal defects cause a reduction in breakdown voltage. Further, also in the RC-IGBT (reverse conduction IGBT) in which the IGBT and the diode are integrated on one chip to realize the miniaturization of the module, it is desired to shorten the lifetime in the IGBT region but not to shorten the diode region. Therefore, a technique for locally introducing crystal defects is required.

局所的に結晶欠陥を導入する方法として、結晶欠陥が不要な箇所に荷電粒子が照射されないように、レジスト等の遮蔽物を半導体基板上にパターニングした上で照射する方法がある。しかし、半導体基板の表面から数十〜数百μmの深さまで結晶欠陥を導入する場合、レジスト厚みも数十〜数百μm必要となる。従って、露光時に光がレジストを透過しきれず、パターニングが困難である。また、使用するレジストの量も多く、コストが上昇してしまう。 As a method for locally introducing crystal defects, there is a method in which a shield such as a resist is patterned on a semiconductor substrate and then irradiated so that charged particles are not irradiated to an unnecessary portion. However, when crystal defects are introduced from the surface of the semiconductor substrate to a depth of several tens to several hundreds μm, the resist thickness is also required to be several tens to several hundreds μm. Therefore, light cannot pass through the resist during exposure, and patterning is difficult. In addition, the amount of resist used is large and the cost increases.

これに対して、荷電粒子を半導体基板に一様に照射しても、半導体基板を局所的に加熱して結晶欠陥を局所的に回復することができる方法が提案されている。例えば、集光したレーザを意図した場所に走査し、集光点以外の温度を上昇させることなく集光点周辺だけを加熱する方法が提案されている(例えば、特許文献1参照)。また、レーザを照射したくない領域の上に予め反射膜を形成する方法が提案されている(例えば、特許文献2参照)。これにより一様にレーザ照射しても半導体基板を局所的に加熱することができる。 On the other hand, a method has been proposed in which even if the semiconductor substrate is uniformly irradiated with charged particles, the semiconductor substrate is locally heated and crystal defects can be locally recovered. For example, a method has been proposed in which a focused laser beam is scanned at an intended location and only the periphery of the focusing point is heated without raising the temperature other than the focusing point (see, for example, Patent Document 1). Further, a method has been proposed in which a reflective film is formed in advance on a region where laser irradiation is not desired (for example, refer to Patent Document 2). As a result, the semiconductor substrate can be locally heated even if the laser is uniformly irradiated.

特開昭62−259437号公報JP 62-259437 A 特開2014−170959号公報JP, 2014-170959, A

しかし、半導体素子を形成する前に反射膜を用いて半導体基板を局所的に加熱する方法しか開示されていなかった。配線又は電極を含む半導体素子を形成した後に半導体基板を局所的に加熱するためには、従来通りレーザ等の電磁波の照射範囲を調整する必要があった。 However, only the method of locally heating the semiconductor substrate using the reflective film before forming the semiconductor element has been disclosed. In order to locally heat the semiconductor substrate after forming the semiconductor element including the wiring or the electrode, it has been necessary to adjust the irradiation range of electromagnetic waves such as laser as in the conventional case.

本発明は、上述のような課題を解決するためになされたもので、その目的は半導体素子を形成した後でも電磁波の照射範囲を調整せずに半導体基板を局所的に加熱することができる半導体装置の製造方法を得るものである。 The present invention has been made in order to solve the above-mentioned problems, and the purpose thereof is a semiconductor capable of locally heating a semiconductor substrate without adjusting the irradiation range of electromagnetic waves even after forming a semiconductor element. A method for manufacturing a device is obtained.

本発明に係る半導体装置の製造方法は、半導体基板の第1の領域に配線又は電極を含む半導体素子を形成する工程と、前記第1の領域及び前記半導体素子を覆いつつ前記半導体基板の第2の領域を覆わない反射膜を形成する工程と、前記反射膜を形成した後に前記半導体基板の前記第1及び第2の領域に電磁波を照射する工程とを備え、前記電磁波は前記反射膜により反射され、前記第2の領域に入射された前記電磁波が前記半導体基板に吸収され、前記第2の領域が局所的に加熱されることを特徴とする。
A method of manufacturing a semiconductor device according to the present invention includes a step of forming a semiconductor element including a wiring or an electrode in a first region of a semiconductor substrate, and a step of covering the first region and the semiconductor element in a second region of the semiconductor substrate. The step of forming a reflective film that does not cover the area of 1) and the step of irradiating the first and second areas of the semiconductor substrate with an electromagnetic wave after forming the reflective film, the electromagnetic wave being reflected by the reflective film. The electromagnetic wave incident on the second region is absorbed by the semiconductor substrate, and the second region is locally heated .

本発明では、第1の領域及び半導体素子を覆いつつ第2の領域を覆わない反射膜を形成した後に半導体基板の第1及び第2の領域に電磁波を照射する。これにより、半導体素子を形成した後でも電磁波の照射範囲を調整せずに半導体基板を局所的に加熱することができる。 In the present invention, the first and second regions of the semiconductor substrate are irradiated with electromagnetic waves after forming the reflective film that covers the first region and the semiconductor element and does not cover the second region. Thereby, even after the semiconductor element is formed, the semiconductor substrate can be locally heated without adjusting the irradiation range of the electromagnetic wave.

本発明の実施の形態1に係る半導体装置の製造方法を示す断面図である。FIG. 7 is a cross-sectional view showing the method of manufacturing the semiconductor device according to the first embodiment of the present invention. 本発明の実施の形態2に係る半導体装置の製造方法を示す断面図である。FIG. 7 is a cross-sectional view showing the method of manufacturing the semiconductor device according to the second embodiment of the present invention. 本発明の実施の形態3に係る半導体装置の製造方法を示す断面図である。FIG. 9 is a cross-sectional view showing the method of manufacturing a semiconductor device according to the third embodiment of the present invention. 本発明の実施の形態4に係る半導体装置の製造方法を示す断面図である。FIG. 11 is a cross-sectional view showing the method of manufacturing the semiconductor device according to the fourth embodiment of the present invention. 本発明の実施の形態5に係る半導体装置の製造方法を示す断面図である。FIG. 13 is a cross-sectional view showing the method of manufacturing the semiconductor device according to the fifth embodiment of the present invention.

本発明の実施の形態に係る半導体装置の製造方法について図面を参照して説明する。同じ又は対応する構成要素には同じ符号を付し、説明の繰り返しを省略する場合がある。 A method for manufacturing a semiconductor device according to an embodiment of the present invention will be described with reference to the drawings. The same or corresponding components are denoted by the same reference numerals, and repeated description may be omitted.

実施の形態1.
図1は、本発明の実施の形態1に係る半導体装置の製造方法を示す断面図である。まず、半導体基板1の第1及び第2の領域2,3を含む全面に電子線又はイオンビーム等の荷電粒子を照射して結晶欠陥を導入する。次に、半導体基板1の第1の領域2に配線又は電極を含む半導体素子4を形成する。例えば、半導体素子4は最表面が金で覆われた電極を含み、IGBT、PNダイオード、MOSFET、又はSBD等である。
Embodiment 1.
1A to 1D are cross-sectional views showing a method of manufacturing a semiconductor device according to a first embodiment of the present invention. First, the entire surface of the semiconductor substrate 1 including the first and second regions 2 and 3 is irradiated with charged particles such as an electron beam or an ion beam to introduce crystal defects. Next, the semiconductor element 4 including the wiring or the electrode is formed in the first region 2 of the semiconductor substrate 1. For example, the semiconductor element 4 includes an electrode whose outermost surface is covered with gold, and is an IGBT, a PN diode, a MOSFET, an SBD, or the like.

次に、半導体基板1の第1の領域2及び半導体素子4を覆いつつ半導体基板1の第2の領域3を覆わない反射膜5を形成する。反射膜5は、電磁波6の反射率が半導体基板1よりも高い材料からなり、例えばアルミニウム膜である。 Next, the reflective film 5 that covers the first region 2 and the semiconductor element 4 of the semiconductor substrate 1 but does not cover the second region 3 of the semiconductor substrate 1 is formed. The reflection film 5 is made of a material having a higher reflectance for the electromagnetic wave 6 than the semiconductor substrate 1, and is, for example, an aluminum film.

次に、半導体基板1の第1及び第2の領域2,3を含む全面に電磁波6を照射する。その後、反射膜5はエッチング等により除去する。電磁波6はランプ、レーザ、マイクロウエーブ等であり、例えば波長808nmのレーザである。電磁波6をレンズで集光して半導体基板1上を走査させてもよいし、電磁波6を半導体基板1の全体に照射してもよい。 Next, the entire surface of the semiconductor substrate 1 including the first and second regions 2 and 3 is irradiated with the electromagnetic wave 6. After that, the reflection film 5 is removed by etching or the like. The electromagnetic wave 6 is a lamp, a laser, a microwave or the like, for example, a laser having a wavelength of 808 nm. The electromagnetic wave 6 may be condensed by a lens to scan the semiconductor substrate 1, or the entire surface of the semiconductor substrate 1 may be irradiated with the electromagnetic wave 6.

反射膜5で覆われていない第2の領域3に入射した電磁波6は半導体基板1に吸収されるため、第2の領域3は局所的に加熱される。この電磁波6の照射により第2の領域3の結晶欠陥を回復させる。一方、電磁波6は反射膜5により反射されるため、電磁波6は半導体素子4及び第1の領域2まで到達しない。従って、第1の領域2は加熱されず、第1の領域2の結晶欠陥は回復しない。 The electromagnetic wave 6 incident on the second region 3 which is not covered with the reflective film 5 is absorbed by the semiconductor substrate 1, so that the second region 3 is locally heated. The irradiation of the electromagnetic wave 6 recovers the crystal defects in the second region 3. On the other hand, since the electromagnetic wave 6 is reflected by the reflective film 5, the electromagnetic wave 6 does not reach the semiconductor element 4 and the first region 2. Therefore, the first region 2 is not heated, and the crystal defects in the first region 2 are not recovered.

以上説明したように、本実施の形態では、第1の領域2及び半導体素子4を覆いつつ第2の領域3を覆わない反射膜5を形成した後に半導体基板1の第1及び第2の領域2,3を含む全面に電磁波を照射する。これにより、半導体素子4を形成した後でも電磁波の照射範囲を調整せずに半導体基板1を局所的に加熱することができる。この結果、第2の領域3の結晶欠陥のみを回復し、第1の領域2の結晶欠陥を回復せずに残すとともに、半導体素子4の配線又は電極の温度上昇を防ぐことができる。 As described above, in the present embodiment, the first and second regions of the semiconductor substrate 1 are formed after forming the reflective film 5 that covers the first region 2 and the semiconductor element 4 but does not cover the second region 3. The entire surface including 2, 3 is irradiated with electromagnetic waves. Thereby, even after the semiconductor element 4 is formed, the semiconductor substrate 1 can be locally heated without adjusting the irradiation range of the electromagnetic wave. As a result, only the crystal defects in the second region 3 can be recovered, the crystal defects in the first region 2 can be left without being recovered, and the temperature rise of the wiring or electrode of the semiconductor element 4 can be prevented.

また、RC−IGBTにおいて、IGBT領域はライフタイムを短くしたいが、ダイオード領域は短くしたくない。そこで、第1の領域2をIGBT領域とし、第2の領域3をダイオード領域とすることが好ましい。 In the RC-IGBT, the IGBT region is desired to have a short lifetime, but the diode region is not desired to be short. Therefore, it is preferable that the first region 2 is an IGBT region and the second region 3 is a diode region.

また、通電しない終端領域では、結晶欠陥が耐圧の低下を引き起こすため、局所的に結晶欠陥を導入したくない。そこで、第1の領域2を活性領域とし、第2の領域3を終端領域とすることが好ましい。 Further, in the terminal region where current does not flow, crystal defects cause a decrease in withstand voltage, so it is not desirable to introduce crystal defects locally. Therefore, it is preferable that the first region 2 is the active region and the second region 3 is the termination region.

実施の形態2.
図2は、本発明の実施の形態2に係る半導体装置の製造方法を示す断面図である。電極又は配線用の金属膜7の下部が加熱したくない領域と一致する場合、金属膜7の材料として電磁波6の反射率が半導体基板1よりも高いものを用いる。即ち、反射膜として電極又は配線用の金属膜7を用いる。これにより、別途反射膜を成膜する必要が無くなり、別途反射膜の成膜及び除去する必要が無くなり、処理工程数を減らすことが出来る。その他の構成及び効果は実施の形態1と同様である。
Embodiment 2.
FIG. 2 is a cross-sectional view showing the method of manufacturing a semiconductor device according to the second embodiment of the present invention. When the lower portion of the metal film 7 for electrodes or wirings coincides with a region which is not desired to be heated, a material having a reflectance of the electromagnetic wave 6 higher than that of the semiconductor substrate 1 is used as the material of the metal film 7. That is, the metal film 7 for electrodes or wiring is used as the reflective film. As a result, there is no need to separately form a reflective film, and there is no need to separately form and remove a reflective film, and the number of processing steps can be reduced. Other configurations and effects are similar to those of the first embodiment.

実施の形態3.
図3は、本発明の実施の形態3に係る半導体装置の製造方法を示す断面図である。反射膜5に複数の微細な穴8を形成して電磁波6の一部を透過させ、残りを反射させる。この透過した電磁波6が半導体基板1の第1の領域2に吸収され、温度が上昇する。これにより、第1の領域2の結晶欠陥の一部が回復される。穴8の密度、即ち反射膜5の面積と穴8の面積の比を変えることで電磁波6の透過量が変わるため、温度上昇量を制御することができる。その他の構成及び効果は実施の形態1又は2と同様である。
Embodiment 3.
FIG. 3 is a cross-sectional view showing the method of manufacturing a semiconductor device according to the third embodiment of the present invention. A plurality of minute holes 8 are formed in the reflective film 5 so that a part of the electromagnetic wave 6 is transmitted and the rest is reflected. This transmitted electromagnetic wave 6 is absorbed by the first region 2 of the semiconductor substrate 1, and the temperature rises. As a result, some of the crystal defects in the first region 2 are recovered. By changing the density of the holes 8, that is, the ratio of the area of the reflective film 5 to the area of the holes 8, the amount of transmission of the electromagnetic wave 6 changes, so that the amount of temperature rise can be controlled. Other configurations and effects are similar to those of the first or second embodiment.

実施の形態4.
図4は、本発明の実施の形態4に係る半導体装置の製造方法を示す断面図である。半導体基板の主面に対して斜めに電磁波を入射させる。従って、半導体基板1の主面に垂直な方向と電磁波6の入射方向の成す角度は0度より大きくなる。これにより、反射膜5の直下にも電磁波が入射するため、深さ方向の温度分布を変えることができる。その他の構成及び効果は実施の形態1〜3と同様である。
Fourth Embodiment
FIG. 4 is a cross-sectional view showing the method of manufacturing a semiconductor device according to the fourth embodiment of the present invention. Electromagnetic waves are obliquely incident on the main surface of the semiconductor substrate. Therefore, the angle formed by the direction perpendicular to the main surface of the semiconductor substrate 1 and the incident direction of the electromagnetic wave 6 is larger than 0 degree. As a result, since the electromagnetic wave is also incident directly below the reflective film 5, the temperature distribution in the depth direction can be changed. Other configurations and effects are similar to those of the first to third embodiments.

実施の形態5.
図5は、本発明の実施の形態5に係る半導体装置の製造方法を示す断面図である。電磁波6を半導体基板1の内部に集光させる。これにより、半導体基板1の表面の温度を上昇させずに半導体基板1の内部の温度を上昇させることができる。従って、半導体基板1の面内方向だけでなく深さ方向にも局所的な加熱が可能となる。また、反射膜5の表面では電磁波が集光せず、反射膜5の表面における集光する電磁波6のエネルギー密度が低下し、反射膜5の温度上昇を抑制できるため、反射膜5の熱変形と拡散を抑制することができる。その他の構成及び効果は実施の形態1〜4と同様である。
Embodiment 5.
FIG. 5 is a cross-sectional view showing the method of manufacturing a semiconductor device according to the fifth embodiment of the present invention. The electromagnetic wave 6 is focused inside the semiconductor substrate 1. Thereby, the temperature inside the semiconductor substrate 1 can be raised without raising the temperature on the surface of the semiconductor substrate 1. Therefore, local heating is possible not only in the in-plane direction of the semiconductor substrate 1 but also in the depth direction. Further, the electromagnetic waves are not condensed on the surface of the reflective film 5, the energy density of the condensed electromagnetic waves 6 on the surface of the reflective film 5 is reduced, and the temperature rise of the reflective film 5 can be suppressed, so that the thermal deformation of the reflective film 5 is suppressed. And diffusion can be suppressed. Other configurations and effects are similar to those of the first to fourth embodiments.

なお、半導体基板1は、珪素によって形成されたものに限らず、珪素に比べてバンドギャップが大きいワイドバンドギャップ半導体によって形成されたものでもよい。ワイドバンドギャップ半導体は、例えば、炭化珪素、窒化ガリウム系材料、又はダイヤモンドである。このようなワイドバンドギャップ半導体によって形成された半導体装置は、耐電圧性や許容電流密度が高いため、小型化できる。この小型化された半導体装置を用いることで、この半導体装置を組み込んだ半導体モジュールも小型化・高集積化できる。また、半導体装置の耐熱性が高いため、ヒートシンクの放熱フィンを小型化でき、水冷部を空冷化できるので、半導体モジュールを更に小型化できる。また、半導体装置の電力損失が低く高効率であるため、半導体モジュールを高効率化できる。 The semiconductor substrate 1 is not limited to the one formed of silicon, and may be formed of a wide bandgap semiconductor having a bandgap larger than that of silicon. The wide band gap semiconductor is, for example, silicon carbide, gallium nitride-based material, or diamond. A semiconductor device formed of such a wide band gap semiconductor has high withstand voltage and high permissible current density, and thus can be downsized. By using this downsized semiconductor device, a semiconductor module incorporating this semiconductor device can also be downsized and highly integrated. Further, since the semiconductor device has high heat resistance, the heat radiation fins of the heat sink can be downsized, and the water cooling unit can be air-cooled, so that the semiconductor module can be further downsized. Moreover, since the power loss of the semiconductor device is low and the efficiency is high, the efficiency of the semiconductor module can be improved.

1 半導体基板、2 第1の領域、3 第2の領域、4 半導体素子、5 反射膜、6 電磁波、7 金属膜、8 穴 1 semiconductor substrate, 2 1st area|region, 3 2nd area|region, 4 semiconductor element, 5 reflective film, 6 electromagnetic wave, 7 metal film, 8 hole

Claims (9)

半導体基板の第1の領域に配線又は電極を含む半導体素子を形成する工程と、
前記第1の領域及び前記半導体素子を覆いつつ前記半導体基板の第2の領域を覆わない反射膜を形成する工程と、
前記反射膜を形成した後に前記半導体基板の前記第1及び第2の領域に電磁波を照射する工程とを備え、
前記電磁波は前記反射膜により反射され
前記第2の領域に入射された前記電磁波が前記半導体基板に吸収され、前記第2の領域が局所的に加熱されることを特徴とする半導体装置の製造方法。
Forming a semiconductor element including wiring or electrodes in a first region of a semiconductor substrate;
Forming a reflective film that covers the first region and the semiconductor element and does not cover the second region of the semiconductor substrate;
Irradiating electromagnetic waves to the first and second regions of the semiconductor substrate after forming the reflective film,
The electromagnetic wave is reflected by the reflective film ,
The method of manufacturing a semiconductor device, wherein the electromagnetic wave incident on the second region is absorbed by the semiconductor substrate, and the second region is locally heated .
前記反射膜を形成する前に前記半導体基板の前記第1及び第2の領域に荷電粒子を照射して結晶欠陥を導入する工程を更に備え、
前記電磁波の照射により前記第2の領域の前記結晶欠陥を回復させることを特徴とする請求項1に記載の半導体装置の製造方法。
The method further comprises the step of irradiating the first and second regions of the semiconductor substrate with charged particles to introduce crystal defects before forming the reflective film,
The method of manufacturing a semiconductor device according to claim 1, wherein the crystal defects in the second region are recovered by the irradiation of the electromagnetic wave.
前記第1の領域をダイオード領域とし、前記第2の領域をIGBT領域とすることを特徴とする請求項2に記載の半導体装置の製造方法。 3. The method of manufacturing a semiconductor device according to claim 2, wherein the first region is a diode region and the second region is an IGBT region. 前記第1の領域を活性領域とし、前記第2の領域を終端領域とすることを特徴とする請求項2に記載の半導体装置の製造方法。 The method for manufacturing a semiconductor device according to claim 2, wherein the first region is an active region and the second region is a termination region. 前記反射膜として電極又は配線用の金属膜を用いることを特徴とする請求項1〜4の何れか1項に記載された半導体装置の製造方法。 The method for manufacturing a semiconductor device according to claim 1, wherein a metal film for electrodes or wiring is used as the reflective film. 前記反射膜に複数の穴を形成して前記電磁波の一部を透過させることを特徴とする請求項1〜5の何れか1項に記載された半導体装置の製造方法。 The method for manufacturing a semiconductor device according to claim 1, wherein a plurality of holes are formed in the reflective film to allow a part of the electromagnetic wave to pass therethrough. 前記半導体基板の主面に対して斜めに前記電磁波を入射させることを特徴とする請求項1〜6の何れか1項に記載された半導体装置の製造方法。 7. The method for manufacturing a semiconductor device according to claim 1, wherein the electromagnetic wave is incident on the main surface of the semiconductor substrate obliquely. 前記電磁波を前記半導体基板の内部に集光させることを特徴とする請求項1〜7の何れか1項に記載された半導体装置の製造方法。 The method of manufacturing a semiconductor device according to claim 1, wherein the electromagnetic waves are condensed inside the semiconductor substrate. 前記半導体基板はワイドバンドギャップ半導体によって形成されていることを特徴とする請求項1〜8の何れか1項に記載された半導体装置の製造方法。 9. The method for manufacturing a semiconductor device according to claim 1, wherein the semiconductor substrate is formed of a wide band gap semiconductor.
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