METHOD OF LASER SEPARATION OF THE EPITAXIAL FILM OR OF THE EPITAXIAL FILM LAYER FROM THE GROWTH SUBSTRATE OF THE EPITAXIAL SEMICONDUCTOR STRUCTURE (VARIATIONS)

Technical Field

Group of the inventions relates to the laser treatment of the solid materials, in particular, to the method of separation of the semiconductors' surface layers with laser radiation, namely the laser separation of the epitaxial film or of the epitaxial film layer from the growth substrate of the epitaxial semiconductor structure.

Background Art

Laser separation of the epitaxial layers of the semiconductor crystals from the growth substrates with their transfer on to the ungrowth substrates is widely used now in manufacturing of the light diodes (patents US7241667, US7202141) and laser diodes (US6365429) according to the flip-chip technology.

In the first time, laser separation of the gallium nitride layers from the transparent growth sapphire substrates was proposed in the work Kelly et al Physica Status Solidi (a) vol. 159, pp. R3,R4, (1997). In this work the ultraviolet excimer laser with wave length λ = 355 nm satisfying the ratio 2nhc/E _g i < λ < 2nhc/E _g2 was used, for which the quantum energy is within the forbidden gap of the substrate E _g i made of sapphire, but exceeds the width of the forbidden gap of the epitaxial film E _g2 , consisting of gallium nitride. Later, the method of laser separation based on the difference between the widths of the forbidden gaps of the growth substrate and epitaxial film was improved. In particular, to improve quality of the separated epitaxial film and to suppress its cracking, it was proposed to use additional sacrifial layer with the width of the forbidden gap less than the widths of the forbidden gaps of the growth substrate and epitaxial film, as well to use scanning of the heteroepitaxial interface between the growth substrate and epitaxial film (patents US6071795, US6365429) . The general scheme of the laser separation methods based on the difference between the widths of the forbidden gaps of the growth substrate and epitaxial film is shown in Fig.l.

When exposing to ultraviolet from the side of the substrate from heteroepitaxial semiconductor gallium nitride film 102 grown on the substrate 101 of sapphire having the width of the forbidden gap more than the light quantum energy, ultraviolet laser radiation passes through sapphire and is absorbed in the thin layer of gallium nitride nearby the heteroepitaxial interface 105 gallium nitride - sapphire. On exposure to ultraviolet laser radiation, gallium nitride in the area 104 defined by crossing of the ultraviolet laser radiation 103 with heteroepitaxial interface 105 is heated up to the temperature ΤΊ, exceeding the decomposition temperature T ₀ - 900°C, and decomposes into gaseous nitrogen and liquid gallium, and as a result epitaxial film of gallium nitride separates from sapphire.

All before proposed methods of laser separation of epitaxial films from the growth substrates are based on the difference between the widths of the forbidden gaps of the epitaxial film E _g2 and substrate E _gi . These methods can be successfully used for separating the epitaxial films obtained using heteroepitaxy method, i.e., technology of growing the epitaxial film onto the growth substrate made of the material which differs from the epitaxial film material. However, to obtain high quality epitaxial films without integrated mechanical stresses, it is often happened to be necessary to use a homoepitaxy method, which provides growing of the epitaxial film on the growth substrate from the same material as the epitaxial film. In this case growth substrate and epitaxial film have an equal width of the forbidden gap, and the usual laser separation method disclosed above becomes unapplied .

The object of the present invention is an expansion of the method application field, namely providing the possibility of separating the epitaxial films from the substrates made of the same crystal material as the epitaxial film.

Disclosure of Invention

To solve this object, two variations of the method for laser separation of the epitaxial film or epitaxial film layer from the growth substrate of the epitaxial semiconductor structure were proposed.

In the first variation of the method in growing the epitaxial film or epitaxial film layer, selective doping with small donor or acceptor impurities of some areas of the epitaxial structure is used, so that the resulting concentration of the small impurities in the selectively doped areas substantially exceeds the background concentration in the undoped areas. Then, the focused laser beam is directed onto the epitaxial structure consisting of the substrate and epitaxial film so that the beam focus is placed in the selectively doped areas of the crystal structure in which absorption of the laser radiation takes place. Laser beam is moved with scanning the selectively doped areas of the epitaxial structures with beam focus with partial thermal decomposition of selectively doped areas and decreasing their mechanical strength. After laser scanning the epitaxial structure is glued on the temporary substrate and the epitaxial film or the epitaxial film layer is separated from the growth substrate or the growth substrate with a part of the epitaxial film by applying mechanical or thermomechanical stress.

The second variation of the method is characterized by : the same features, and differs from the first method in that the epitaxial structure is glued on the temporary substrate before laser scanning, then laser scanning of the epitaxial structure glued on the temporary substrate is performed, and after laser scanning the epitaxial film or the epitaxial film layer is separated from the growth substrate or the growth substrate with a part of the epitaxial film by applying mechanical or thermomechanical stress.

Preferably, the epitaxial film or the epitaxial film layer is grown by the homoepitaxy method.

Preferably, the selectively doped area is the substrate or the surface layer of the substrate.

Preferably, the selectively doped area is the epitaxial film or the lower layer of the epitaxial film.

Preferably, the material of the crystalline structure consisting of the substrate and epitaxial film, is the semiconductor from the elements of the forth group or the semiconductor compound from the elements of the forth group, or the semiconductor compound from the elements of the third and fifth group, or the semiconductor compound from the elements of the second and sixth group of the periodic system .

Preferably, the laser wave length for separating the homoepitaxial films from the growth substrate is in the following wave length range: for silicon, germanium and, gallium arsenide semiconductors in the range of 6 ym ≤ λ ≤ 48 ym, for gallium nitride in the range of 4 μιη < λ ≤ 32 ym, for silicon carbide 3 ym ≤ λ ≤ 24 ym, for alumina nitride in the range of 2,5 ym ≤ λ ≤ 20 ym, and for diamond 2 ym ≤ λ ≤ 16 ym.

Preferably, infrared gas pulse pumped silicon dioxide C0 ₂ or silicon oxide CO is used as a laser.

The proposed variations of the laser separation method allow separating the homoepitaxial films from the substrates made of the same crystalline material as the epitaxial film. This new laser separation method is based on the usage of the selective doping of the substrate and epitaxial film with the fine donor or acceptor impurities. In the selective doping, concentrations of the free carriers in the epitaxial film and substrate may significantly differ, and this can lead to a strong difference between the light absorption factors in the infrared region near the region of the residual beams, where free carriers and phonon-plasmon interaction of the optical phonons with free carriers make an essential contribution to infrared absorption of the optical phonons. With the appropriate selection of the doping levels and frequency of infrared laser radiation it is possible to achieve that laser radiation is absorbed in general in the region of strong doping near the interface substrate- homoepitaxial film. When scanning the interface substrate- homoepitaxial film with the focused laser beam of sufficient power, thermal decomposition of the semiconductor crystal takes place with subsequent separation of the homoepitaxial film. To realize the proposed method of laser separation, it is preferably to use laser radiation with wave length λ being within the infrared region of relative transparence of the undoped semiconductor, namely near the edge of the residual beams region where a strong absorption of light at the expense of one- or two-phonon processes is not possible, but a relatively weak absorption of light may present at the expense of three- or more phonon processes.

Preferably, wave length λ of the laser beam is within the range of c/4v ₀ ≤ λ ≤ 2c/v _0l where v ₀ is a frequency of LO- optical phonon for a semiconductor material of the growth substrate, c is a light velocity.

The inequality given above follows that the preferable laser wave length for separating the homoepitaxial films from the growth substrate is within the following wave length ranges: for silicon, germanium and gallium arsenide semiconductors in the range of 6 μπι ≤ λ ≤ 48 μκι, for gallium nitride in the range of 4 pm ≤ λ ≤ 32 μπι, for silicon carbide 3 μπ ≤ λ ≤ 24 μπι, for alumina nitride in the range of 2,5 μπι ≤ λ ≤ 20 μπι, and for diamond 2 μπι ≤ λ ≤ 16 μπι.

The technical result of the proposed invention consists in offering a new method of laser separation of the epitaxial films in comparison with the known ones which allows to separate homoepitaxial films from the substrates, i.e., homoepitaxial films having the same width of the forbidden gap as the initial semiconductor substrate. Also, the proposed method allows using the high-effective and inexpensive infrared gas silicon dioxide C0 ₂ or silicon oxide CO lasers for separation of- the epitaxial films.

Brief Description of the Drawings

The present invention is illustrated by the drawings in which the prior art is shown Fig.l, schemes illustrating the realization of the present invention Fig. 2-5, and calculated spectral dependences of the light absorption factor in gallium nitride at various levels of doping with fine donor impurities Fig.6.

Fig. 1 shows the scheme of the known prior art method of laser separation of the heteroepitaxial film of semiconductor crystal from a foreign growth substrate using focused laser radiation with wave length λ for which a light quantum energy is within the forbidden gap of the substrate E _g i , and exceeds the width of the forbidden gap of the epitaxial film E _g2 material .

Fig.2 shows a scheme illustrating the proposed method of laser separation of the homoepitaxial film from the semiconductor substrate consisting of the same semiconductor material as the homoepitaxial film. The scheme illustrates laser separation for the case of selective doping the substrate and homoepitaxial film with fine donor or acceptor impurities when the doping level in the homoepitaxial film exceeds the doping level in the semiconductor substrate.

Fig.3 shows a scheme illustrating the proposed method of laser separation of the homoepitaxial film from the semiconductor substrate consisting of the same semiconductor material as the homoepitaxial film. The scheme illustrates laser separation for the case of selective doping the substrate and homoepitaxial film with fine donor or acceptor impurities when the doping level in the semiconductor substrate exceeds the doping level in the homoepitaxial film.

Fig. 4 shows a scheme illustrating the proposed method of laser separation of the undoped upper layer of the homoepitaxial film from the undoped semiconductor substrate with a laser beam passing through the substrate and absorbed in the lower level of the homoepitaxial film doped with fine donor or acceptor impurities. Fig. 5 shows a scheme illustrating the proposed method of laser separation of the undoped upper layer of the homoepitaxial film from the undoped semiconductor substrate with a laser beam passing through the upper undoped layer and absorbed in the lower level of the homoepitaxial film doped with fine donor or acceptor impurities.

Fig. 6 shows the calculated spectral dependences of the light absorption factor near the residual beams region for semiconductor crystal of gallium nitride at various levels of doping with fine donor impurities. Dependences 601, 602 and 603 refer to the doping levels 10 ¹⁷ , 10 ¹⁸ and 5-10 ¹⁹ cm ^'3 respectively .

Best Mode for Carrying Out the Invention

The present invention will become readily apparent from the following detailed description of exemplary embodiments. It should be noted that the consequent description of these embodiments is only illustrative, but not exhaustive.

Example 1. Separation of homoepitaxial gallium nitride film doped with fine donor impurities from the undoped semiconductor gallium nitride substrate with laser beam passing through the substrate.

Fig. 2 shows a scheme of laser separation of homoepitaxial gallium nitride film 202, 50 m wide from the semiconductor gallium nitride substrate 101, 200 pm wide. Level of doping with fine silicon donor impurities in the homoepitaxial film 202 is of 5Ί0 ¹⁹ cm ^"3 , and exceeds the background concentration of fine oxygen and silicon donors in the semiconductor substrate 101 equalled 10 ¹⁷ cm ^-3 . For separating of the homoepitaxial gallium nitride film,

CO ₂ pulse pumped laser is used operating at the wave length λ = 10.6 μπι and generating pulses of energy 0.1 J, duration 50 ns and repetition rate 100 Hz.

Absorption factor of laser radiation with wave length λ = 10 μπι in the homoepitaxial gallium nitride film 202 doped with fine silicon donor impurities of concentration 5-10 ¹⁹ cm ^"3 , equals 4·10 ⁴ cm ^"1 , whereas the absorption factor of this radiation in the undoped semiconductor gallium nitride substrate 101 with background concentration of fine oxygen and silicon donors equalled 10 ¹⁷ cm ^"3 is 5-10 ¹ cm ^"1 .

The respective spectral dependences of the light absorption factor near the residual beams region which we calculated for the semiconductor gallium nitride crystals with different levels of doping with fine donor impurities are given in Fig.6. The curves 601, 602 and 603 refer to the doping levels lO ¹⁷ , 10 ¹⁸ and 5-10 ¹⁹ cm ^"3 respectively.

Scheme in Fig. 2 shows that infrared laser beam 203 passes through the substrate 101 and is focused into the spot 1 mm in diameter which provides the energy density of 10 J/cm ² . Under the action of infrared laser beam 203 of pulse CO ₂ laser with wave length λ = 10 m focused into the spot 1 mm in diameter weakly absorbed in the undoped semiconductor gallium nitride substrate 101 and strongly absorbed in the homoepitaxial gallium nitride film 202 doped with fine donor impurities, local heating of the homoepitaxial film 202 takes place in the region 204 defined by crossing of the infrared laser beam 203 with the homoepitaxial interface 205 between the undoped semiconductor substrate 101 and the doped homoepitaxial film 202. Local heating above temperature 900 °C leads to chemical decomposition of gallium nitride crystal into gaseous nitrogen and liquid gallium in the region 204. Movement of the laser beam 203 focus with velocity of 10 cm/s in the horizontal plane which is parallel to homoepitaxial interface 205 leads to subsequent decomposition of gallium nitride in the set of regions 204 and weakening of the homoepitaxial interface 205 between the undoped semiconductor substrate 101 and the doped homoepitaxial film 202. Then when pasting the homoepitaxial film 202 on the temporary metallic ceramic or plastic substrate and applying small mechanical or thermomechanical stress it is possible to separate the homoepitaxial film 202 from the substrate 101.

Example 2. Separation of undoped homoepitaxial gallium nitride film from semiconductor gallium nitride substrate doped with fine donor impurities, by means of laser beam passing through the homoepitaxial film.

Fig. 3 shows the scheme of laser separation of undoped homoepitaxial gallium nitride film 100 m thick from semiconductor gallium nitride substrate 1 mm thick. The background concentration of fine oxygen and silicon donors in the homoepitaxial film 202 is 10 ¹⁷ cm ^"3 and is essentially less than the concentration of fine silicon donor impurities in the doped semiconductor substrate 101 equalled 5-10 ¹⁹ cm ^"3 . For separating of the homoepitaxial gallium nitride film,

C0 ₂ pulse pumped laser is used operating at the wave length λ = 10.6 μιη and generating pulses of energy 0.1 J, duration 50 ns and repetition rate 100 Hz. Absorption factor of laser radiation with wave length λ = 10 μιη in the undoped homoepitaxial gallium nitride film 202, with background concentration of fine oxygen and silicon donors equalled 10 ¹⁷ cm ^"3 , is of 5-10 ¹ cm ^"1 , whereas the absorption factor of this radiation in the semiconductor gallium nitride substrate 101 doped with fine silicon donor impurities of concentration 5-10 ¹⁹ cm ^-3 , equals 4-10 ⁴ cm ^"1 . The respective spectral dependences of the light absorption factor near the residual beams region which we calculated for the semiconductor gallium nitride crystals with different levels of doping with fine donor impurities are given in Fig.6. The curves 601, 602 and 603 refer to the doping levels 10 ¹⁷ , 1018 and 5-10 ¹⁹ cm ^"3 respectively .

Scheme in Fig. 3 shows that the infrared laser beam 203 passes through homoepitaxial film 202 and focused into the spot 1 mm in diameter which provides the energy density of 10 J/cm ² .

Under the action of infrared laser beam 203 of pulse C0 ₂ laser with wave length λ = 10.6 μπι focused into the spot 1 mm in diameter weakly absorbed in the undoped homoepitaxial gallium nitride film 202 and strongly absorbed in the semiconductor gallium nitride substrate 101 doped with fine donor impurities, local heating of the substrate 101 takes place in the region 204 defined by crossing of the infrared laser beam 203 with the homoepitaxial interface 205 between the doped semiconductor substrate 101 and the undoped homoepitaxial film 202. Local heating above temperature 900°C leads to chemical decomposition of gallium nitride crystal into gaseous nitrogen and liquid gallium in the region.204. Movement of the laser beam 203 focus with velocity of 10 cm/s in the horizontal plane which is parallel to homoepitaxial interface 205 leads to the subsequent decomposition of gallium nitride in the set of regions 204 and to weakening of the homoepitaxial interface 205 between the doped semiconductor substrate 101 and the undoped homoepitaxial film 202. Then when pasting the homoepitaxial film 202 on the temporary metallic, ceramic or plastic substrate and applying a small mechanical or thermomechanical stress it is possible to separate the homoepitaxial film 202 from the substrate 101. Example 3. Separation of the undoped upper layer of the homoepitaxial gallium nitride film from the undoped semiconductor gallium nitride substrate with laser beam passing through the substrate and absorbed in lower layer of homoepitaxial film doped with fine donor impurities. Fig. 4 shows the scheme of laser separation of the undoped homoepitaxial gallium nitride film 202, 50 ym thick from the undoped semiconductor gallium nitride substrate 101, 200 ym thick using the doped lower layer 406 of the homoepitaxial film, 1 ym thick. Level of doping with fine silicon donor impurities in the lower layer 406 of the homoepitaxial gallium nitride film is 5·10 ¹⁹ cm ^"3 and exceeds the background concentration of fine silicon and oxygen donor impurities in the semiconductor substrate 101 and the upper layer of the homoepitaxial film 202 equaled 10 ¹⁷ cm ^-3 . For separating of the homoepitaxial gallium nitride film,

C0 ₂ pulse pumped laser is used operating at the wave length λ = 10.6 ym and generating pulses of energy 0.1 J, duration 50 ns and repetition rate 100 Hz.

Absorption factor of laser radiation with wave length λ = 10, 6 ym in the lower layer 406 of the homoepitaxial gallium nitride film doped with fine silicon donor impurities with concentration 5-10 ¹⁹ cm ^"3 equals 4-10 ⁴ cm ^"1 , whereas the absorption factor of this laser radiation in the undoped semiconductor gallium nitride substrate 101 and in the undoped upper layer 402 of the homoepitaxial gallium nitride film with background concentrations of fine oxygen and silicon donors of 10 ¹⁷ cm ^"3 equals 5-10 ¹ cm ^"1 .

The. respective spectral dependences of the light absorption factor near the residual beams region which we calculated for the semiconductor gallium nitride crystals with different levels of doping with fine donor impurities are given in Fig.6. The curves 601, 602 and 603 refer to the doping levels 10 ¹⁷ , 10 ¹⁸ and 5-10 ¹⁹ cm ^"3 respectively.

Scheme in Fig. 4 shows that the laser beam 203 passes through the substrate 101 and is focused into the spot 1 mm in diameter which provides the energy density of 10 J/cm ² . Under the action of infrared laser beam 203 of pulse C0 ₂ laser with wave length λ = 10.6 μπι focused into the spot 1 mm in diameter weakly absorbed in the undoped semiconductor gallium nitride substrate 101 and strongly absorbed in the lower layer 406 of the homoepitaxial gallium nitride film 202 doped with fine donor impurities, local heating of the lower layer 406 of the homoepitaxial film takes place in the region 404, defined by crossing of the infrared laser beam 203 with the homoepitaxial interface 405 between the undoped semiconductor substrate 101 and the doped lower layer 406 of the homoepitaxial film 202. Local heating - above temperature 900°C leads to chemical decomposition of gallium nitride crystal into gaseous nitrogen and liquid gallium in the region 404. Movement of the laser beam 203 focus with velocity of 10 cm/s in the horizontal plane which is parallel to homoepitaxial interface 405 leads to the subsequent decomposition of gallium nitride in the set of regions 404 and to weakening of the homoepitaxial interface 405 between the undoped semiconductor substrate 101 and the doped lower layer 406 of the homoepitaxial film. Then when pasting the undoped upper layer 402 of the homoepitaxial film on the temporary metallic, ceramic or plastic substrate and applying a small mechanical or thermomechanical stress it is possible to separate the undoped upper layer 402 of the homoepitaxial film with non-evaporated part of the lower doped layer 406 from the substrate 101.

Example 4. Separation of the undoped upper layer of the homoepitaxial gallium nitride film from the undoped semiconductor gallium nitride substrate with laser beam passing through the upper layer of the homoepitaxial film and absorbed in lower layer of homoepitaxial film doped with fine donor impurities.

Fig.5 shows a scheme of laser separation of the undoped layer of the homoepitaxial gallium nitride film 202, lOOpm thick from the undoped semiconductor gallium nitride substrate 101, 2 μτη thick using the doped lower layer 406 of the homoepitaxial gallium nitride film 1 μπ thick. Level of doping with fine silicon donor impurities in the lower layer 406 of the homoepitaxial gallium nitride film is 5-10 ¹⁹ cm ^-3 , and exceeds background concentration of fine oxygen and silicon donor in the semiconductor substrate 101 and in the upper layer 402 of the homoepitaxial film equaled 10 ¹⁷ cm ^"3 .

For separating of the homoepitaxial gallium nitride film, C0 ₂ pulse pumped laser is used operating at the wave length λ = 10.6 μηα and generating pulses of energy 0.1 J, duration 50 ns and repetition rate 100 Hz.

Absorption factor of laser radiation with wave length λ = 10.6 μπι in the lower layer 406 of the homoepitaxial gallium nitride film doped with fine silicon donor impurities with concentration 5·10 ¹⁹ cm ^-3 equals 4·10 ⁴ cm ^-1 , whereas the absorption factor of this laser radiation in the undoped semiconductor gallium nitride substrate 101 and in the undoped upper layer 402 of the homoepitaxial gallium nitride film with background concentrations of fine oxygen and silicon donors of 10 ¹⁷ cm ^"3 equals 5-10 ¹ cm ^"1 .

The respective spectral dependences of the light absorption factor near the residual beams region which we calculated for the semiconductor gallium nitride crystals with different levels of doping with fine donor impurities are given in Fig.6. The curves 601, 602 and 603 refer to the doping levels 10 ¹⁷ , 10 ¹⁸ and 5-10 ¹⁹ cm ^"3 respectively.

Scheme in Fig. 5 shows that the laser beam 203 passes through the upper layer 402 of the homoepitaxial film and is focused into the spot 1 mm in diameter which provides the energy density of 10 J/cm ² . Under the action of infrared laser beam 203 of pulse CO2 laser with wave length λ = 10,6 μιη focused into the spot 1 mm in diameter weakly absorbed in the undoped upper layer 402 of the homoepitaxial gallium nitride film and strongly absorbed in the lower layer 406 of the homoepitaxial gallium nitride film doped with fine donor impurities, local heating of the lower layer 406 of the homoepitaxial gallium nitride film takes place in the region 404 defined by crossing of the infrared laser beam 203 with the interface 505 between the undoped upper layer 402 and the doped lower layer 406 of the homoepitaxial gallium nitride film. Local heating above temperature 900°C leads to chemical decomposition of gallium nitride crystal into gaseous nitrogen and liquid gallium in the region 404. Movement of the laser beam 203 focus with velocity of 10 cm/s in the horizontal plane which is parallel to the interface 405 leads to the subsequent decomposition of gallium nitride in the set of regions 404 and to weakening of the interface 405 between the undoped upper layer 402 and the doped lower layer 406 of the homoepitaxial film. Then when pasting the undoped upper layer 402 of the homoepitaxial film on the temporary metallic, ceramic or plastic substrate and applying a small mechanical or thermomechanical stress it is possible to separate the undoped upper layer 402 of the homoepitaxial film from the non-evaporated part of the lower doped layer 406 and from the substrate 101.

Example 5. Separation of the undoped homoepitaxial silicon carbide 4H-SiC film from the semiconductor silicon carbide 4H-SiC substrate doped with fine donor impurities by means of the laser beam passing through the homoepitaxial film.

Fig.. 3 shows a scheme of laser separation of the undoped homoepitaxial silicon carbide 4H-SiC film 202, 100 μτα thick from the semiconductor silicon carbide 4H-SiC substrate 101, 400 μιη thick. The background concentration of the fine donors in the epitaxial film 202 is less than 10 ¹⁷ cm ^-3 , and essentially less than the concentration of the fine nitrogen donor impurities in the doped semiconductor substrate 101 equaled 5·10 ¹⁹ cm ^-3 . For separating of the homoepitaxial silicon carbide 4H-

SiC film, CO pulse pumped laser is used operating at the wave length λ = 5.2 μπι and generating pulses of energy 0.4 J, duration 50 ns and repetition rate 10 Hz. Absorption factor of laser radiation with wave length λ = 5.2 μπι in the undoped homoepitaxial silicon carbide 4H-SiC film 202, with the background concentration of the fine donors less than 10 ¹⁷ cm ^{" 3} is 10 cm ^-1 (A.M. Hofmeister, K.M. Pitman, A.F. Goncharov, and A.K. Speck The Astrophysical Journal, 696:1502-1516, 2009 May 10) , whereas the absorption factor of this radiation in the semiconductor silicon carbide 4H-SiC substrate 101 doped with the fine nitrogen donor impurities of concentration 5·10 ¹⁹ cm ^-3 exceeds 10 ⁴ cm ^"1 .

Scheme in Fig. 3 shows that the infrared laser beam 203 passes through the homoepitaxial film 202 and is focused into the spot 1 mm in diameter which provides the energy density of 50 J/cm ² .

Under the action of infrared laser beam 203 of pulse CO laser with wave length λ = 5.2 ym focused into the spot 1 mm in diameter weakly absorbed in the undoped homoepitaxial silicon carbide 4H-SiC film 202 and strongly absorbed in the semiconductor silicon carbide 4H-SiC substrate 101 doped with the fine donor impurities, local heating of the substrate 101 takes place in the region 204, defined by crossing of the infrared laser beam 203 with the interface 205 between the doped semiconductor substrate 101 and undoped homoepitaxial film 202. Local heating to temperature above 2800°C leads to chemical decomposition of silicon carbide 4H-SiC of the gallium nitride crystal into silicon and carbon in the region 204. Movement of the laser beam 203 focus with velocity of 2 cm/s in the horizontal plane which is parallel to the interface 205 leads to subsequent decomposition of silicon carbide 4H-SiC in the set of regions 204 and to weakening of the interface 205 between the doped semiconductor substrate 101 and the undoped homoepitaxial film 202. Then when pasting the epitaxial film 202 on the temporary metallic, ceramic or plastic substrate and applying a small mechanical or thermomechanical stress it is possible to separate the epitaxial film 202 from the substrate 101.

Example 6. Separation of weakly doped homoepitaxial silicon film from the semiconductor silicon substrate strongly doped with fine boron acceptor impurities using laser beam passing through the homoepitaxial film.

Fig. 3 shows the scheme of laser 'separation of weakly doped homoepitaxial silicon film 202, 50. μπι thick from the semiconductor silicon substrate 101, 700 μπι thick. Concentration of the fine boron acceptor impurities equals 10 ¹⁷ cm ^-3 , and essentially less than the concentration of the fine boron acceptor impurities in the doped semiconductor substrate 101 equaled 10 ¹⁹ cm ^"3 .

For separating of the homoepitaxial silicon film, C0 ₂ pulse pumped laser is used operating at the wave length λ = 10.6 μτη and generating pulses of energy 0.1 J, duration 50 ns and repetition rate 100 Hz. Absorption factor of laser radiation with the wave length λ = 10.6 μπι in the weakly doped homoepitaxial silicon film 202 with concentration of fine acceptors of 10 ¹⁷ cm ^-3 is 12 cm ^"1 (Hara, H. and Y. Nishi, J. Phys . Soc. Jpn 21, 6, 1222, 1966) , whereas the absorption factor of this radiation in the semiconductor silicon substrate 101 doped with the fine boron acceptor impurities of concentration 10 ¹⁹ cm ^-3 equals 3000 cm ^-1 .

Scheme in Fig. 3 shows that the infrared laser beam 203 passes through the homoepitaxial film 202 and is focused into the spot 0.5 mm in diameter which provides the energy density of 40 J/cm ² .

Under the action of infrared laser beam 203 of pulse C0 ₂ laser with wave length λ = 10.6 μιη focused into the spot 0.5 mm in diameter weakly absorbed in the undoped homoepitaxial silicon film 202 and strongly absorbed in the semiconductor silicon substrate 101 doped with fine boron acceptor impurities, local heating of the substrate 101 takes place in the region 204, defined by crossing of the infrared laser beam 203 with the interface 205 between the strongly doped semiconductor substrate 101 and weakly doped homoepitaxial film 202. Local heating to temperature above 1400°C leads to partial melting and amorphicity of the silicon crystal in the region 204. Movement of the laser beam 203 focus with velocity of 20 cm/s in the horizontal plane which is parallel to the interface 205 leads to subsequent melting and amorphycity of silicon crystal in the set of regions 204 and to weakening of the interface 205 between the strongly doped semiconductor substrate 101 and weakly doped homoepitaxial film 202. Then when pasting the epitaxial film 202 on the temporary metallic, ceramic or plastic substrate and applying a small mechanical or thermomechanical stress it is possible to separate the epitaxial film 202 from the substrate 101.

Despite the fact that the present invention was described and illustrated by the examples of the invention embodiments it should be noted that the present invention is in no case limited by the examples given.