LUMINESCENT SEMICONDUCTOR ELEMENT

Abstract: A luminescent semiconductor element in which a thin film of a semiconductor or an insulating material is sand­ wiched with first and second semiconductor layers having a small forbidden band energy gap to form a heterostruc­ ture, which is further sandwiched with semiconductor layers having a forbidden band energy gap greater than those of the first and second semiconductor layers, in a manner that the electron-hole pairs formed via the thin film recombine together owing to the tunnel effect to produce laser oscilla­ tion. Means is further provided to control the probability of recombination by applying an electric field from the external side. Being constructed as described above, the semicon­ ductor element produces the laser oscillation with a low threshold current maintaining a uniform wavelength and a uniform phase.

Description: The present invention relates to a semiconductor optical device capable of emitting an optical beam which is coherent in its wavelength and phase. Fig. 1 shows an energy band diagram in case a bias is applied forward to a double heterostructure (constructed of a laser active layer 10, an n-type cladding layer 4 and a p-type cladding layer 5), which is used in a semiconductor laser of the prior art. Electrons 6 injected from the cladding layer 4 and positive holes 7 injected from the cladding layer 5 recombine in the active region 10 to emit an optical beam 11. In this scheme, the electrons and the positive holes are Fermi particles, and the carrier distribution in the band is determined in dependence upon the density of states and the Fermi distribution. In the band structure diagram, incidentally, reference numeral 8 denotes the bottom of the conduction band, and numeral 9 denotes the upper end of the valence electron band. If this distribution extends, the laser threshold current increases. If the active layer of the laser is assumed to have a quantum well structure, the density of state is changed from a parabolic function to a step function to establish a quantum level. As a result, the quantum size effect reduces the width of emission spectra to about 1/2 to 1/3. In this case, however the carriers are the Fermi particles. Therefore the individual electrons and positive holes are absolutely independent, phases of each wave function are different, and they do not make coherent movement. In case a signal is to be transmitted through a laser beam, therefore, the overall average value of many carriers has to be changed. US-A-3353114 discloses a semiconductor optical device having a heterostructure which has first and second semiconductor layers with an intermediate insulating barrier layer of thickness less than or equal to 10nm, so that carriers produced in the first semiconductor layer are acted upon by an electric field applied across the heterostructure to tunnel through the barrier layer, then recombine in the second semiconductor layer to give rise to laser emisssion. This document corresponds to the precharacterised part of claim 1. The present invention seeks to provide a semiconductor optical device capable of emitting an optical beam which is coherent in its phase and wavelength. Thus, according to the present invention a semiconductor optical device having a hetero-structure with first and second semiconductor layers opposed to each other via a thin film of a semiconductor or insulator having a thickness not greater than 15 nm (150Å); wherein the semiconductor layers having a smaller forbidden band energy gap than that of said thin film; said hetero-structure being such that emissions by recombination are based mainly on the recombinations by tunnelling between electrons and positive holes contained in said semiconductor layers; and the device having means for controlling the number of electrons and positive holes related to the recombinations by tunnelling by applying an electric field from the outside. In the present invention, a spatially separated electron-hole pair being a Bose particle, Bose condensation is effected by increasing the density of the electrons and the positive holes while being cooled, thus establishing a scheme which is completely coherent in its phase. The emission from this scheme is remarkably coherent in both its phase and wavelength. Fig. 2 is an energy band diagram of a semiconductor laser which is necessary for effecting the Bose condensation. The changes of a conduction band 8 and a valence electron band 9 in the direction of thickness are shown in the state wherein the bias voltage is applied in the forward direction. Semiconductor layers 2 and 3 appearing in Fig. 2 are laser active layers which have smaller band gaps than semiconductor layers 4 and 5. The type of conductivity can be exemplified by the following cases: (1) both the semiconductor layers 2 and 3 are undoped; (2) only one of the semiconductor layers 2 and 3 is undoped whereas the other has the same type of conductivity as that of the cladding layer 4 or 5 contacting therewith; and (3) the semiconductor layers 2 and 4 and the semiconductor layers 3 and 5 are respectively of the same type of conductivity. In Fig. 2, incidentally, reference numeral 4 denotes an n-type cladding layer, and numeral 5 denotes a p-type cladding layer. The difference from the semiconductor layer by the prior art resides in that there is formed in the laser active layer a barrier layer 1 for spatially separating the electrons 6 and the positive holes 7. The process of effecting the Bose condensation in that scheme will be described in the following. The theoretical investigations of the conditions for the electrons and the positive holes opposed through the barrier layer to effect the Bose condensation have been made in 1975 by Yu. E. Lozovik et al. (as is disclosed in Soviet Physics (JETP. Lett.), vol. 22, pp. 274, 1975). The electrons and the positive holes (which are present in layers 13 and 14 of superconductive thin films) opposed through a barrier layer 12, as shown in Fig. 3, are turned into a kind of excitons 15 and 16 migrating in the plane of the layer 12 while attracting each other by the Coulomb force, in case the thickness d of the layer 12 is small. Those excitons are subjected to the Bose condensaiton because they are the Bose particles if they are kept at a low temperature to have their density increased. According to the estimations by Lozovik et al., if the distance between the excitons is designated as ℓ, the probability of recombination of the carriers due to the tunnel effect is about 1 x 10⁻²⁶ and can be neglected in fact, if the thickness d of the barrier and the distance ℓ are about 10nm (100 Å), and the temperature for the condensation is about 100°K. Incidentally, since what has been intended by them is to realize the superconduction in the scheme of the Bose condensation, the thickness of the barrier layer is so chosen that the electrons and the positive holes may not recombine by the tunnel effect. This point is essentially different from that of the present invention. More specifically, the present invention is similar in the fundamental process of the Bose condensation to the aforementioned theory of Lozovik et al., but is different from the scheme of Lozovik et al. in that the thickness d of the barrier layer is made small to promote the radiative recombination process between the electrons and the positive holes by choosing an optimum tunneling probability. Since only the superconduction is the target of the Lozovik's scheme, the electron-hole recombination process by the tunnel effect is an unnecessary process which reduces the number of electron-hole pairs, and therefore the recombination must be prevented by using a 10nm (100Å) thick barrier layer in the case of Lozovik. If the barrier layer has its potential barrier height made excessively small or its thickness made excessively small, on the other hand, the electrons and the positive holes are caused to recombine one after another by the tunnel effect so that the concentration of the electron-hole pairs cannot be sufficient for establishing the Bose condensation. The main target of the present invention is to sequentially establish the Bose condensation and the recombination-emission process of the excitons by optimizing the thickness of that barrier layer. In Fig. 2, those of the electrons 6 injected into the active layer 2 and the positive holes 7 injected into the active layer 3, which are present near the barrier layer 1, are caused to attract each other to become excitons by the Coulomb force. If the Bose condensation is effected by the cooling treatment at a low temperature, the electrons and the positive holes near the barrier successively make pairs so that the emissions obtained from the excitons have a high density and a coherent phase. The gist of the present invention will be summarized in the following. 1. A semiconductor optical device characterized: by having a hetero-structure which is constructed of first and second semiconductor layers opposed to each other through a thin film (which will become a barrier layer) of a semiconductor or insulator having a thickness not greater than 15 nm (150Å); and having a smaller forbidden band energy, gap than that of said thin film; by making said hetero-structure such that emissions by recombination are based mainly on the recombinations by tunnelling between electrons and positive holes contained in said semiconductor layers; and by having means for controlling the number of electron and positive holes related to the tunneling recombinations by applying an electric field from the outside. The aforementioned tunneling recombination emissions are caused by the recombinations of the excitons which are made of the electrons and the positive holes by the Coulomb force. When said semiconductor optical device is cooled at a temperature not higher than 150°K, moreover, the aforementioned recombination emissions are due to the super-radiance from the excitons having been subjected to the Bose condensation. We have also found that the super-radiance is established by making the barrier layer such that the tunneling probability T falls within a range of 0.6 to 1 x 10⁻¹⁰ in case the relationship among the tunneling probability and the thickness D (Å) and the height H (eV) of the barrier layer satisfies the following Equation: T = exp [- 0.4 D √ H ]. Moreover, we have found that, in case the excitons are dissociated by the electric field, the electrons and the positive holes are not sufficiently separated by the electric field when the thickness of the barrier is not less than 15nm (150Å) or sufficiently 10nm (100Å), so that they combine without the tunneling recombination to provide none of the effects of the present invention. Still moreover, we have found it preferable to make the overlap of the wave functions of the electrons and the positive holes through said thin layer larger than the overlap of the wave functions of the electrons and the positive holes in the same one of said semiconductor layers by making the thicknesses of said first and second semiconductor layers not smaller than 20nm (200Å) (or preferably 40nm (400Å) thereby to push said electrons and said positive holes to the opposite sides of their respective ones of said semiconductor layers by the composition of cystals or a doped impurity in the crystal or a pseudo-potential established by the two and/or an external field. Furthermore, the following modes of embodiment of the invention are also preferable: A semiconductor optical device characterized by having means for applying an electric field in a direction normal to said thin film to said semiconductor layers opposed to each other through said thin film to collect said electrons at one of the interfaces between said thin film and said semiconductor layers and said positive holes at the other interface; A semiconductor optical device characterized in that the composition and/or impurity density of one or both of said first and second semiconductor layers are made uneven in the direction of the thickness of said thin film to collect said electrons and said positive holes in the vicinity of said thin film; A semiconductor optical device characterized in that a layered structure constructed of at least said thin film and said first and second semiconductor layers is sandwiched between third and fourth semiconductor layers which have larger forbidden band energy gaps than said first and second semiconductor layers and which have different types of conductivity; A semiconductor optical device characterized in that said thin film is made of Ga 1-x Aℓ x As, said first semiconductor layer is made of Ga 1-y Aℓ y As, and said second semiconductor layer is made of Ga 1-z Aℓ z As, wherein: x > y and z; 1 ≧ x > 0.1; and 0.4 > y and z ≧ 0; and A semiconductor optical device characterized in that said thin film is made of Ga x In 1-x P y As 1-y (which holds even for x = 0 and y = 0), and said first and second semiconductor layers are made of Ga m In 1-m P x As 1-x . BRIEF DESCRIPTION OF DRAWINGS Fig. 1 is an energy band diagram showing the semiconductor laser by the prior art; Fig. 2 is an energy band diagram showing a spatially separated electron-hole pair type semiconductor laser according to the present invention; Fig. 3 is a diagram for explaining that the Bose condensation is caused in case the electrons and the positive holes are excited through a barrier; Figs. 4 and 5 are diagrams explaining the principle of operation of a semiconductor optical device according to an embodiment of the present invention; Fig. 6 is a graph depicting the temperature characteristics of the laser oscillations described with reference to Fig. 4; Figs. 7, 9 and 10 are sections showing individual semiconductor optical devices of the present invention; and Fig. 8 is an energy band diagram of a semiconductor optical device in which the electrons and the positive holes are pushed toward the barrier. Example 1 Fig. 4 schematically shows the changes in the direction of thickness of the band gaps of the bottom 17 of the conduction band and the upper end 18 of the valance electron band of the device according to the embodiment of the present invention. Fig. 9 is a section taken normal to the optical beam which is emitted from the semiconductor optical device of the present example. This state is realized by the following method. On an n-type GaAs substrate 40, there were caused to grow sequentially by the use of the molecular beam epitaxial method 0.5 microns or an n-type GaAs buffer layer 41, followed by an undoped Ga 0.7 Aℓ 0.3 As cladding layer 22 (2 microns), an undoped GaAs layer 20 (0.1 micron), an undoped Ga 0.5 Aℓ 0.5 As barrier layer 19 (which has a thickness of 2nm (20Å), an undoped GaAs layer 21 (0.1 micron), an undoped Ga 0.7 Aℓ 0.3 As cladding layer 23 (2 microns), and a p-type GaAs layer 42 (0.2 microns) as a cap layer. An n-side electrode 43 was formed after the back of the n-type substrate had been polished and chemically etched. The gap layer was further coated with a p-side electrode 44 in the form of a stripe having a width of 10 microns, and the aforementioned epitaxy layer was etched from the layer 23 to the layer 22 by using the electrode as the mask. Moreover, cleavage was conducted so that the laser resonator might have a length of 300 microns. The type was identical to that of the mesa-stripe type semiconductor laser. The chip thus obtained was bonded to a submount and fixed in a cryostat which can cool from room temperature to 10°K. The mesa-stripe was irradiated transversely with the laser beam of a Kr ion laser having a band of 647 to 676 nanometers. The beam having that wavelength was absorbed by the semiconductor layers 20 and 21 to generate electrons 24 and positive holes 25 respectively in those layers. This behavior was shown in Fig. 4. With this state being left as it is, the electrons and the positive holes will not be separated but recombined in the GaAs layers 20 and 21 to emit light. By increasing this excited light, the ordinary laser oscillations will occur. Now, the changes of the band gap in case an electric field is applied in the backward direction to the p- and n-side electrodes in the optically excited state are shown in Fig. 5. The electrons and the positive holes are pushed onto the respective ends of the GaAs layers 20 and 21. Since these layers have a thickness of 0.1 microns, the electrons and positive holes (26 and 29, and 27 and 28) present in the same layer cannot be recombined. However, the electrons 26 and the positive holes 28 are caused to make the electron-hole pairs by the Coulomb force because only the barrier layer having a thickness of 2nm (20Å) is interposed inbetween. The measurements of the changes of the output beam from the laser by using the temperature of the device as a parameter are depicted against the intensity of the pumping light in the state having the electric field applied in Fig. 6. As the device is cooled down to lower temperatures, the threshold current of the laser oscillations decreased, and drastically drops in case the temperature becomes lower than 100°K, to raise the efficiency of light emission. At this temperature, the Base condensation occurred so that the laser oscillatons were observed from the state in which the phases of the excitons became coherent. The spectrum width of this light beam was one-tenth of that of the semiconductor laser beam of the prior art. Fig. 10 shows the state in which both the sides of the semiconductor layered body for the light emission are buried in a semiconductor layer 45. This is an example in which a concept similar to the case of the ordinary BH (i.e., Buried Hetero-structure) type laser was adopted. The reference numerals appearing in Fig. 10 denotes the same parts as those of Fig. 9. Example 2 The semiconductor laser having the structure shown in Fig. 7 was fabricated by the MO-CVD (i.e., Metal-Organic Chemical-Vapor Deposition) method. After an n-type GaAs/Ga 0.7 Aℓ 0.3 As super-lattice buffer layer 33 had been grown to have a thickness of 1 micron on an n-type GaAs substrate 32, were subsequently grown an n-type Ga 0.7 Aℓ 0.3 As cladding layer 4 of 2 microns, an undoped GaAs active layer 2 (which had a thickness of 0.1 microns), an undoped Aℓ As barrier layer 1 (which had a thickness of 3nm (30Å)), an undoped GaAs active layer 3 (which had a thickness of 0.1 microns), a p-type Ga 0.7 Aℓ 0.3 As cladding layer 5 (which had a thickness of 1.5 microns), and a p-type GaAs cap layer 34 (which had a thickness of 0.2 microns). The aforementioned super-lattice buffer layer 33 was sufficiently exemplified by the ordinary super-lattice layer. By using a process similar to that of the ordinary semiconductor laser, p- and n-side electrodes 35 and 36 were formed, and the opposite face of the resonator was cleaved and bonded to the electrodes. The energy band diagram in case a bias was applied in the forward direction and carriers were injected to the p-n junction of the semiconductor laser element thus obtained in shown in Fig. 2. The characteristics were examined by changing the injection current while the device was being cooled at a low temperature. The semiconductor laser obtained had an oscillatory threshold current of 1 microampere at 92°K. Example 3 In the semiconductor laser having been described in connection with the Example 2, the band gap of the laser active layers 2 and 3 present at both the sides of the insulating film 1 can be reduced at the barrier, as shown in Fig. 8, by changing the Aℓ compositional ratio of the Ga 1-x Aℓ x As and the concentration of the impurity in the direction of the thickness of crystal. The carriers in both the conduction and valence bands are pushed to the barrier by the electric bias to increase the probability of generating the excitons. In Fig. 8, the bias is applied in the forward direction to the p-n junction. Example 4 In the semiconductor laser having been described in connection with the Example 2, the insulating film 1 was made of Ga x In 1-x P y As 1-y (inclusive of x=0, y=0), and the laser active layers 2 and 3 at both the sides of the insulating film 1 were made of Ga m In 1-m P x As 1-x , thus fabricating the semiconductor optical device. This device had a threshold current of 1.5 microamperes. In the optical device according to the present invention, the generation of a signal is conducted by the scheme having been subjected to the Bose condensation so that the information can be transmitted with a remarkably small number of photons. The superradiance of the excitons having conducted the Bose condensation has a spectrum width of one tenth as wide as that of the semiconductor laser of the prior art, and the threshold current of the laser oscillations is one-ten thousandth Thus, the performance of the semiconductor laser is drastically improved. Because of the Bose condensation of the excitons through the thin film barrier, moreover, it is practically advantageous that the condensation takes place at a high temperature of 100°K (although the temperature for establishing the ordinary super-conductive state is lower by about one order). The condensation of the excitons in the case without any barrier is not caused by a high-density excitation no matter how the temperature might be reduced. This is because the excitons become the electron-hole drops or molecules. These exciton molecules themselves experience the Bose condensation at a low temperature of several °K. Since the exciton molecules will dissociate into excitons in the course of their emissions and since the emissions of the two are different in wavelength, however, there has never been any report of the laser oscillations. In summary, the present invention can provide a semiconductor optical element which is enabled to emit an optical beam having a narrow spectrum band by causing the electrons and the positive holes to recombine, in a condition which cause Bose degeneration of the excitons by controlling the thickness and the aplied electric field of the barrier layer, artificially. It is also possible to drop the threshold current of the device. In short, the effect of the invention to provide a semiconductor device for emitting an optical beam coherent in wavelength and phase on the basis of the novel concept highly contributes to the industry.

Claims: A semiconductor optical device having a hetero-structure with first and second semiconductor layers (20,21;2,3) opposed to each other via a thin film (19;1) of a semiconductor or insulator having a thickness not greater than 15 nm (150Å); characterised in that: the semiconductor layers having a smaller forbidden band energy gap than that of said thin film; said hetero-structure being such that emissions by recombination are based mainly on the recombinations by tunnelling between electrons (26) and positive holes (28) contained in said semiconductor layers (20,21;2,3); and the device having means (43,44;35,36) for controlling the number of electrons and positive holes related to the recombinations by tunnelling by applying an electric field from the outside. A semiconductor optical device according to claim 1, wherein the probability T of the tunnelling recombination of the electrons and positive holes, in which the thickness D (Å) and the height H (eV) of the barrier constructing said thin film are expressed by T = exp [- 0.4 D√ H ] , falls within a range of 0.6 to 1 x 10⁻¹⁰ in the state having no voltage applied. A semiconductor optical device according to claim 1 or claim 2 wherein the overlap of the wave functions of the electrons and the positive holes through said thin layer is made larger than the overlap of the wave functions of the electrons and the positive holes in said semiconductor layers by making the thickness of said first and second semiconductor layers not smaller than 20 nm (200Å)(or preferably 40nm (400Å)) thereby to push said electrons and said positive holes to the opposite sides of their respective ones of said semiconductor layers by the composition of crystal, of a doped impurity in the crystal, or a pseudo-potential established by the two and/or an external field. A semiconductor optical device according to any one of the preceding claims wherein said thin film is made of a semiconductor of direct transition type. A semiconductor optical device according to any one of the preceding claims, wherein said thin film has a thickness ranging from that of a monoatomic layer to 10 nm (100Å). A semiconductor optical device according to any one of the preceding claims having means (43,44;35,36) for applying an electric field in a direction normal to said thin film to said semiconductor layers opposed to each other through said thin film to collect said electrons at one of the interfaces between said thin film and said semiconductor layers and said positive holes at the other interface. A semiconductor optical device according to any one of the preceding claims wherein the composition and/or impurity density of one or both of said first and second semiconductor layers are made uneven in the direction of the thickness of said thin film to collect said electrons and said positive holes in the vicinity of said thin film. A semiconductor optical device according to any one of the preceding claims wherein a layered structure constructed of at least said thin film and said first and second semiconductor layers is sandwiched between third and fourth semiconductor layers (22,23;4,5) which have a larger forbidden band energy gap than said first and second semiconductor layers and which have different types of conductivity. A semiconductor optical device according to any one of the preceding claims wherein said thin film is made of Ga 1-x Aℓ x As, said first semiconductor layer is made of Ga 1-y Aℓ y As, and said second semiconductor layer is made of Ga 1-z Aℓ z As, and wherein: x > y and z; 1 ≧ x > 0.1; and 0.4 > y and z ≧ 0. A semiconductor optical device according to any one of the preceding claims wherein said thin film is made of Ga x In 1-x P y As 1-y (which holds even for x = 0 and y = 0), and said first and second semiconductor layers are made of Ga m In 1-m P x AS 1-x .

Inventors: FUKUZAWA, TADASHI, HIRUMA, KENJI, MATSUMURA, HIROYOSHI, YAMADA, EIZABURO
Applicants: HITACHI, LTD.
Application year: 1986
Main classification: H01S3
IPC codes: H01S5