Surface-emitting laser element and laser module using the same

Abstract

A cavity is formed by a lower multilayer mirror and an upper multilayer mirror and an active layer is arranged between the lower multilayer mirror and the upper multilayer mirror in a surface-emitting laser element. A relaxation oscillation frequency at a bias point in the cavity is set to exceed an optical communication frequency for modulating a laser light output from the surface-emitting laser element.

Description

BACKGROUND OF THE INVENTION

1. Field of the Invention

The present invention relates to a vertical cavity surface-emitting laser (VCSEL) (hereinafter, “surface-emitting laser element”), and more particularly, to a surface-emitting laser element that can improve critical back-reflection tolerance and a laser module using the surface-emitting laser element.

2. Description of the Related Art

In recent years, a surface-emitting laser element has been used in a high-speed communication system with communication speed of 2.5 Gbps to 10 Gbps. In this surface-emitting laser element, a pair of semiconductor multilayer mirrors that use GaAs/AlGaAs or the like are formed on a semiconductor substrate of GaAs, InP, or the like. An active layer serving as a light-emitting region is provided between the pair of semiconductor multilayer mirrors. The surface-emitting laser element emits a laser light in a direction perpendicular to the semiconductor substrate (see, for example, Japanese Patent Application Laid-Open No. 2004-15027).

However, a back-reflection to a light source is caused by reflection in a coupling portion of a light source such as a surface-emitting laser element and an optical fiber or reflection from an optical transmission line such as an optical fiber. The back-reflection causes noise in the light source. Thus, an isolator or the like is inserted in the coupling portion or the like to prevent the back-reflection from being made incident on the light source.

On the other hand, the surface-emitting laser element has been considered to be resistible against back-reflection because reflectance thereof is as high as 99.5%. However, it has been found that the surface-emitting laser element is not always resistible against back-reflection because a cavity length thereof is short. In this case, although it is possible to control the back-reflection by inserting an isolator, cost of a laser module, which uses the surface-emitting laser element, is increased by the insertion of the isolator.

SUMMARY OF THE INVENTION

It is an object of the present invention to at least partially solve the problems in the conventional technology.

A surface-emitting laser element according to one aspect of the present invention includes a cavity that is formed by a lower multilayer mirror and an upper multilayer mirror and an active layer that is arranged between the lower multilayer mirror and the upper multilayer mirror. A relaxation oscillation frequency at a bias point in the cavity is set to exceed an optical communication frequency for modulating a laser light output from the surface-emitting laser element.

A laser module according to another aspect of the present invention includes a surface-emitting laser element in which a cavity is formed by a lower multilayer mirror and an upper multilayer mirror and an active layer is arranged between the lower multilayer mirror and the upper multilayer mirror. A relaxation oscillation frequency of the surface-emitting laser element at a bias point in the cavity is set to exceed an optical communication frequency for modulating a laser light output from the surface-emitting laser element. The laser light emitted from the surface-emitting laser element is output to outside via an optical fiber.

A surface-emitting laser element array according to still another aspect of the present invention includes a plurality of surface-emitting laser elements arranged in either one of a one-dimensional array and a two-dimensional array. Each of the surface-emitting laser elements includes a cavity formed by a lower multilayer mirror and an upper multilayer mirror; and an active layer arranged between the lower multilayer mirror and the upper multilayer mirror. A relaxation oscillation frequency at a bias point in the cavity is set to exceed an optical communication frequency for modulating a laser light output from the surface-emitting laser element.

A laser module according to still another aspect of the present invention includes a surface-emitting laser element array in which a plurality of surface-emitting laser elements are one-dimensionally or two-dimensionally arranged. Each of the surface-emitting laser elements includes a cavity formed by a lower multilayer mirror and an upper multilayer mirror; and an active layer arranged between the lower multilayer mirror and the upper multilayer mirror. A relaxation oscillation frequency at a bias point in the cavity is set to exceed an optical communication frequency for modulating a laser light output from the surface-emitting laser element. The laser light emitted from the surface-emitting laser element is output to outside via an optical fiber.

The above and other objects, features, advantages and technical and industrial significance of this invention will be better understood by reading the following detailed description of presently preferred embodiments of the invention, when considered in connection with the accompanying drawings.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 is a cross section of a surface-emitting laser element according to a first embodiment of the present invention, viewed from an oblique direction;

FIG. 2 is a cross section of a detailed structure near an active layer;

FIG. 3 is a graph of relaxation-oscillation-frequency dependency of critical back-reflection;

FIG. 4 is a graph of modulation-doping-amount dependency of critical back-reflection;

FIG. 5 is a graph of a change in RIN with respect to the back-reflection;

FIG. 6 is a graph of a frequency characteristic of RIN;

FIG. 7 is a graph of reflectance dependency of critical back-reflection with a relaxation oscillation frequency set as a parameter;

FIG. 8 is a graph of a gain spectrum for explaining detuning in a direction for increasing a differential gain according to a second embodiment of the present invention;

FIG. 9 is a graph of detuning-amount dependency of critical back-reflection;

FIG. 10 is a graph of a relation between detuning that occurs in a surface-emitting laser element formed on a wafer and an oscillation wavelength; and

FIG. 11 is a schematic of a surface-emitting laser element array according to a third embodiment of the present invention.

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS

Exemplary embodiments of the present invention are explained in detail below with reference to the accompanying drawings.

FIG. 1 is a cross section of a surface-emitting laser element 10 according to a first embodiment of the present invention, viewed from an oblique direction. The surface-emitting laser element 10 has a structure in which an n-GaAs buffer layer (n=1×10¹⁸ cm⁻³) 21, a lower multilayer mirror 12, an active region 13, an upper multilayer mirror 16 including a current confinement layer 15, and a contact layer 17 are stacked on an n-GaAs substrate 11 of a surface one after another, an n-side electrode 23 is provided below the n-GaAs substrate 11, and a ring-shaped p-side electrode 18 and an electrode pad 20 for leading the p-side electrode 18 are provided above the contact layer 17. The active region 13, and the upper multilayer mirror 16 form a cylindrical mesa post with the periphery thereof removed. A sidewall of the mesa post and an upper portion of the lower multilayer mirror 12 are covered with a silicon nitride film 19. The periphery of the mesa post is filled with a polyimide 22 via the silicon nitride film 19.

The lower multilayer mirror 12 has a structure in which 25.5 pairs of multilayer films with AlAs and GaAs set as a pair are stacked from the n-GaAs substrate 11 side and ten pairs of multilayer films with Al0.9Ga_0.1As and GaAs set as a pair are stacked above the 25.5 pairs of multilayer films. The active region 13 has an active layer 32 sandwiched by Cladding layers 31 and 33. The active layer 32 forms a multiple quantum well structure of Ga_0.63In_0.37N_0.01As_0.974Sb_0.016 (a quantum well layer)/GaAs_0.93P_0.07 (a barrier layer) and has three quantum well layers. Carbon with p=5×10¹⁸ cm⁻³ is doped in the barrier layer. The upper multilayer mirror 16 has a structure in which twenty-three or twenty-six multilayer films with Al_0.9Ga_0.1As and GaAs set as a pair is stacked. An oscillation wavelength of the surface-emitting laser element 10 is about 1300 nm.

A method of manufacturing the surface-emitting laser element 10 is explained. First, the n-GaAs buffer layer (n=1×10¹⁸ cm⁻³) 21, the lower multilayer mirror 12, the active region 13, the upper multilayer mirror 16, and the contact layer 17 formed of GaAs are stacked on the n-GaAs substrate 11 one after another according to the metal organic chemical vapor deposition (MOCVD) and molecular beam epitaxy (MBE) method. The current confinement layer 15 formed of AlAs with thickness of 20 nm is stacked as a lowermost layer of the upper multilayer mirror 16.

Thereafter, a silicon nitride film is formed on a growing surface of the contact layer 17 according to the plasma CVD method. A circular pattern with a diameter of about 40 μm to 45 μm is transferred onto the silicon nitride film using the photolithography by a photoresist. The silicon nitride film is etched using the circular resist mask transferred according to the reactive ion etching (RIE) method that uses a CF₄ gas. The etching is further performed according to the reactive ion beam etching (RIBE) method that uses a chloride gas until the etching reaches the lower multilayer mirror 12 to form a mesa post of a columnar structure. Depth of the etching by the RIBE method is set to stop the etching in the lower multilayer mirror 12.

In this state, the stacked layers are heated to 400° C. in a water vapor atmosphere and left as they are to selectively oxidize the current confinement layer 15 in the lowermost layer of the upper multilayer mirror 16. Consequently, a selective oxidation layer 14 is formed. A current injection path of the current confinement layer 15 in which the selective oxidation layer 14 is not formed is 3 μm to 10 μm in diameter.

After completely removing the silicon nitride film according to the RIE method, a silicon nitride film is formed over the entire surface again according to the plasma CVD method, the periphery of the mesa post is filled with the polyimide 22.

Thereafter, the silicon nitride film in the upper portion of the mesa post is removed in a circular shape. The p-side electrode 18, which is a ring-shaped AuZn/Au electrode, is formed in the portion where the silicon nitride film is removed. The electrode pad 20 of Ti/Pt/Au is formed for electrode leading. An area of the electrode pad 20 is 3000 μm2. Thereafter, after grinding the n-GaAs substrate 11 to about 200 μm, the AuGeNi/Au electrode is deposited on the surface of the n-GaAs substrate 11. Finally, the stacked layers are annealed at about 400° C. in a nitrogen atmosphere.

FIG. 2 is a diagram of a sectional structure near the active region 13. As shown in FIG. 2, the active layer 32 has a triple quantum well structure in which three quantum well layers 42a to 42c made of Ga_0.63IN_0.37N_0.01As_0.974Sb_0.016 with thickness of 7.3 nm are sandwiched among four barrier layers 41a to 41d made of GaAs_0.93P_0.07 with thickness of 15 nm. As described above, carbon with p=5×10¹⁸ cm⁻³ is doped in the respective barrier layers 41a to 41d. The Cladding layers 31 and 33 with thickness of 128 nm are provided above and below the active layer 32. Thickness of each of the upper multilayer mirror 16 and the lower multilayer mirror 12 is λ/4.

In the surface-emitting laser element 10, it is possible to increase back-reflection tolerance by doping the p-type impurity in the barrier layers 41a to 41d. When there is back-reflection to a semiconductor laser element, a noise level at which noise suddenly increases depends on a characteristic of the semiconductor laser element. In general, a critical back-reflection fextc in an edge emitting laser element is represented by fextc=(t_L²/16|C_e|²)·(K·fr²+1/t_e)²·((1+a²)/a⁴)   (1) where ι_L is a light confinement time of a cavity, C_e is efficiency of coupling with back-reflection at a laser emission end, K is a K factor, fr is a relaxation oscillation frequency, ι_e is an electron life, and α is a spectral-linewidth enhancement factor.

Increasing the critical back-reflection fextc means increasing back-reflection tolerance. It has been found that, in the case of the surface-emitting laser element, to increase the critical back-reflection fextc without spoiling an optical output, an increase in the relaxation oscillation frequency fr contributes most. FIG. 3 is a diagram of relaxation-oscillation-frequency fr dependency of the critical back-reflection fextc. As shown in FIG. 3, the critical back-reflection fextc increases according to an increase in the relaxation oscillation frequency fr. For example, when the relaxation frequency fr is 5 GHz, the critical back-reflection fextc is about −30 dB. When the relaxation frequency fr is increased to 20 GHz, the critical back-reflection fextc increases to about −10 dB. In other words, even if there is back-reflection as large as −10 dB, it is possible to control noise that occurs in the surface-emitting laser element.

The relaxation oscillation frequency fr has a relation expressed by fr∝(a(dg/dn)·(I−Ith))^1/2   (2) Therefore, to increase the relaxation oscillation frequency fr, a differential gain (dg/dn) and a current injection amount (I-Ith) only have to be increased. The current injection amount (I-Ith) is a dynamic amount of an electric current injected into the surface-emitting laser element. Thus, it is seen that the differential gain (dg/dn) only has to be increased.

It is possible to realize the increase of the differential gain (dg/dn) by doing an impurity in the barrier layers 41a to 41d of the active layer 32. FIG. 4 is a graph of modulation-doping-amount dependency of the critical back-reflection fextc. As shown in FIG. 4, when a doping amount in the barrier layers 41a to 41d is increased, the critical back-reflection fextc increases. For example, when the modulation doping amount is changed from p=1×10¹⁷ cm⁻³ to p=1×10¹⁹ cm⁻³, it is possible to increase the critical back-reflection fextc by about 10 dB. According to the first embodiment, carbon with p=5×10¹⁸ cm⁻³ is doped.

In the surface-emitting laser element 10 according to the first embodiment, an opening area formed by the selective oxidation layer 14 is 30 μm². Continuous wave at a threshold current of 1 mA, slope efficiency of 0.3 W/A, and 100° C. was obtained. The relaxation oscillation frequency fr in this case was 6 GHz at a bias current of 5 mA when modulation doping for the barrier layers was not performed. The relaxation oscillation frequency fr was successfully increased to 9 GHz by performing the modulation doping. In other words, as shown in FIG. 3, a critical back-reflection was successfully increased from −28 dB to −22 dB.

Back-reflection dependency of relative intensity noise that occurs in the surface-emitting laser element 10 is considered. As shown in FIG. 5, the RIN increases according to an increase in back-reflection. There are two critical points of the RIN. One critical point is a critical point Γc where mode competition between a cavity mode of the surface-emitting laser element itself and an external cavity mode. The other critical point is a critical point (critical back-reflection) fextc due to coherent collapse. When a distance between the surface-emitting laser element and a reflection point of the back-reflection decreases, the critical point Γc and fextc are closer to each other. The RIN slightly increases when the RIN passes the critical point Γc according to the increase in the back-reflection. The RIN suddenly increases when the RIN passes the critical point fextc. Therefore, it is possible to control occurrence of large RIN by increasing a value of the critical point fextc. In other words, as shown in FIG. 5, when the critical point fextc is changed to a critical point fextc′, a characteristic curve of the RIN and the back-reflection is deformed to an increasing side of the back-reflection. Thus, it is possible to expand back-reflection regions E1 and E2 where the value of the RIN is small and increase large back-reflection tolerance. This critical point fextc is the critical back-reflection fextc described above.

An optical communication performed using the surface-emitting laser element 10 is considered. FIG. 6 is a graph of a frequency characteristic of the RIN. As shown in FIG. 6, the RIN takes a large value near the relaxation oscillation frequency fr. In FIG. 6, since the relaxation oscillation frequency fr is 5 GHz, a value of the RIN near the relaxation oscillation frequency fr is large. When transmission speed of the optical communication is about 2 GHz, it is possible to perform communication without being affected by the relaxation oscillation frequency fr. However, when the transmission speed of the optical communication is increased to about 8 GHz, the relaxation oscillation frequency of 5 GHz affects communication as noise. In this case, if the relaxation oscillation frequency is shifted to a relaxation oscillation frequency fr′ that exceeds a communication frequency band E_H of 0 to 8 GHz and at which noise due to a relaxation oscillation frequency does not affect the communication frequency band E_H, a value of the RIN decreases and it is possible to perform satisfactory communication. According to the first embodiment, since the relaxation oscillation frequency is successfully shifted from 6 GHz to 9 GHz, it is possible to hold down a value of the RIN at the time of communication with transmission speed of, for example, about 8 GHz.

A differential gain is increased by the modulation doping, a relaxation oscillation frequency is increased by the increase in the differential gain, and a value of the RIN is reduced by the increase in the relaxation oscillation frequency. This makes it possible to increase critical back-reflection tolerance.

A critical back-reflection increases according to the increase in the relaxation oscillation frequency and also increases according to an increase in reflectance of the upper multilayer mirror 16. FIG. 7 is a graph of dependency on reflectance of a critical back-reflection at the time when a relaxation oscillation frequency is set as a parameter. As shown in FIG. 7, the critical back-reflection not only increases according to the increase in the relaxation oscillation frequency but also increases according to the increase in the reflectance of the upper multilayer mirror 16. The increase in the reflectance means reduction of an output of the surface-emitting laser element. On the other hand, it is not easy to increase an output of the surface-emitting laser element. Therefore, the increase in the relaxation oscillation frequency by the modulation doping makes it possible to increase back-reflection tolerance without decreasing an optical output of the surface-emitting laser element and also makes it possible to perform satisfactory high-speed communication. For example, in FIG. 7, the relaxation oscillation frequency is set to 10 GHz, −24 dB of a critical back-reflection standard for a DFB laser element in the present situation is cleared by setting the reflectance to 0.995 and setting the relaxation oscillation frequency to 10 GHz.

Examples of the surface-emitting laser element subjected to the modulation doping include the following. A surface-emitting laser element in a long wavelength band that has the critical back-reflection fextc, with which a value of the RIN at 0 GHz to 2 GHz becomes −115 dB/Hz, equal to or larger than −30 dB and the relaxation oscillation frequency fr at a bias point equal to or higher than 5 GHz is realized. This makes it possible to satisfactorily perform communication at transmission speed of 2.6 Gbps. A surface-emitting leaser element in a 1.3-μm band that has the critical back-reflection fextc, with which a value of the RIN at 0 GHz to 8 GHz becomes −115 dB/Hz, equal to or larger than −20 dB and the relaxation oscillation frequency fr at a bias point equal to or higher than 10 GHz is realized. This makes it possible to satisfactorily perform communication at transmission speed of 10 Gbps. Moreover, a surface-emitting laser element in a 1.55-μm band that has the critical back-reflection fextc, with which a value of the RIN at 0 GHz to 8 GHz becomes −115 dB/Hz, equal to or larger than −30 dB and the relaxation oscillation frequency fr at a bias point equal to or higher than 10 GHz is realized. This makes it possible to satisfactorily perform communication at transmission speed of 10 Gbps.

According to the first embodiment, modulation doping density is p=5×10¹⁸ cm⁻³. However, the modulation doping density is preferably set to p=1×10¹⁸ cm⁻³ to p=2×10¹⁹ cm⁻³. According to the first embodiment, carbon is used as the p-type impurity for performing p-type doping. However, the p-type impurity is not limited to carbon. Be, Zn, Mg, or the like may be used as the p-type impurity. These kinds of materials may be simultaneously used.

Furthermore, according to the first embodiment, the semiconductor film is used for both the upper multilayer mirror 16 and the lower multilayer mirror 12. However, the multilayer mirrors are not limited to the semiconductor film. For example, a dielectric film may be used. According to the first embodiment, the lower multilayer mirror is formed by the multilayer films with AlAs/GaAs set as a pair and the upper multilayer mirror is formed by the multilayer films with Al_0.9Ga_0.1As/GaAs set as a pair. However, it is also possible to form both the multilayer mirrors with multilayer films with AlGaAs/AlGaAs having different Al compositions set as a pair. Moreover, it is also possible to provide gradient composition layers in which compositions are gradually changed may be provided among these respective layers.

Moreover, according to the first embodiment, GaInNAsSb is used as the quantum well layers 42a to 42c. However, a material of the quantum well layers 42a to 42c is not limited to this material. For example, a GaInNAssemiconductor material, an AlGaInAs semiconductor material, a GaInAsP semiconductor material, an InGaAsSb semiconductor material, a TlGaInAsP semiconductor material, or the like may be used. According to the first embodiment, the active layer 32 has the quantum well structure. However, the active layer 32 is not limited to this structure. The active layer 32 may have a quantum wire structure or a quantum dot structure.

Furthermore, according to the first embodiment, the surface-emitting laser element is the surface-emitting laser element having an oscillation wavelength of about 1310 nm. However, it is also possible to form a surface-emitting laser element having other oscillation wavelengths, for example, an oscillation wavelength in a 300-nm to 1600-nm band. For example, it is also possible to form a surface-emitting laser element having an oscillation wavelength in an 850-nm band. However, in this case, a quantum well layer is formed of GaAs or AlGaInAs.

Moreover, according to the first embodiment, back-reflection tolerance of the surface-emitting laser element itself is described. However, the present invention is not limited to this back-reflection tolerance. It is also possible to apply the present invention to back-reflection tolerance with a laser module including this surface-emitting laser element set as a unit. In the laser module, the surface-emitting laser element is bonded to a CAN package, other plastic packages, or the like. An optical fiber receptacle or a pigtail is attached to the laser module. In this case, since the back-reflection tolerance is high, an optical element such as an isolator does not have to be mounted. Thus, it is possible to realize reduction in cost of the laser module itself.

When this laser module is set as a unit, since a loss due to coupling of the surface-emitting laser element and an optical fiber is intrinsic, a critical back-reflection decreases in appearance. When the loss due to coupling is about 3 dB, the critical back-reflection increases by a loss of 6 dB from the surface-emitting laser element to the optical fiber and vice versa. As a result, a laser module having a surface-emitting laser element in the long wavelength band that has the critical back-reflection fextc, with which a value of the RIN at 0 GHz to 2 GHz becomes −115 dB/Hz, equal to or larger than −24 dB and the relaxation oscillation frequency fr at a bias point equal to or higher than 5 GHz is realized. This makes it possible to satisfactorily perform communication at transmission speed of 2.5 Gbps. A laser module having a surface-emitting laser element in the 1.3-μm band that has the critical back-reflection fextc, with which a value of the RIN at 0 GHz to 8 GHz becomes −115 dB/Hz, equal to or larger than −14 dB and the relaxation oscillation frequency fr at a bias point equal to or higher than 10 GHz is realized. This makes it possible to satisfactorily perform communication at transmission speed of 10 Gbps. Moreover, a laser module having a surface-emitting laser element in the 1.55-μm band that has the critical back-reflection, with which a value of the RIN at 0 GHz to 8 GHz becomes −115 dB/Hz, equal to or larger than −24 dB and the relaxation oscillation frequency fr at a bias point equal to or higher than 10 GHz is realized. This makes it possible satisfactorily perform communication at transmission speed of 10 Gbps.

According to the first embodiment, the modulation doping is applied to the barrier layers 41a to 41d as means for increasing the relaxation oscillation frequency fr. However, according to the second embodiment, detuning is performed to increase a differential gain, whereby the relaxation oscillation frequency fr is increased.

It is possible to increase the differential gain (dg/dn) of the relaxation oscillation frequency fr shown in Equation (2) not only with the demodulation doping but also with the detuning. FIG. 8 is a graph for explaining an increase in a differential gain by the detuning according to a second embodiment of the present invention. In FIG. 8, a gain of a laser light has wavelength dependency and temperature dependency. On a gain curve L11 at the time of a room temperature operation, a gain decreases to a short wavelength side and a long wavelength side with a gain peak wavelength λg1 as a peak. Similarly, on a gain curve L12 at the time of a low temperature operation, a gain decreases to a short wavelength side and a long wavelength side with a gain peak wavelength λg2 as a peak. On the gain curve L12 at the time of the low temperature operation, a high gain is generally obtained compared with the gain curve L11 at the time of the room temperature operation. An oscillation wavelength λ1 is an oscillation wavelength at the time of the room temperature operation and coincides with the gain peak wavelength λg1. An oscillation wavelength λ2 is an oscillation wavelength of oscillation shifted to the short wavelength side by the detuning at the time of the low temperature operation. The oscillation wavelength λ2 may coincide with the gain peak wavelength λg2.

The detuning according to the second embodiment is different from usual detuning. In the usual detuning, a gain curve is shifted to the long wavelength side at the time of a high temperature operation and an oscillation wavelength is shifted to a high temperature side. However, since respective shift amounts are different, this deviation is corrected to adjust the oscillation wavelength to a high gain state at the time of the high temperature operation. On the other hand, in the detuning according to the second embodiment, unlike the usual detuning, an oscillation wavelength is shifted to the short wavelength side.

The detuning is defined as a difference Dc between a gain peak wavelength λg and an oscillation wavelength λlasing at the room temperature (Dc=λg−λlasing). In FIG. 8, a gain spectrum L11 at the time of low current inject at the time of the room temperature, a gain spectrum L12 at the time of high current injection, and set oscillation wavelength λlasing1 and λlasing2 at the room temperature are shown. The differential gain (dg/dn) is Δg/Δn at the oscillation wavelength λlasing. As shown in FIG. 8, the differential gain (dg/dn) is larger when the gain peak wavelength λg is set larger than the oscillation wavelength λlasing.

FIG. 9 is a graph of detuning-amount dependency of the critical back-reflection. As shown in FIG. 9, according to an increase in a detuning amount shifted to the short wavelength side, the critical back-reflection increases. It is possible to obtain critical back-reflection equal to or higher than −30 dB. In particular, when the detuning amount is set as large as 50 nm, it is possible to increase the critical back-reflection to near −20 dB.

A surface-emitting laser element, which was the surface-emitting laser element described according to the first embodiment and was not subjected to the modulation doping, was manufactured. In the surface-emitting laser element, barrier layers corresponding to the barrier layers 41a to 41d were formed of GaAs, thickness of the barrier layers was set to 20 nm, a cavity length was adjusted, the oscillation wavelength λlasing at the time of the room temperature operation was set to 1300 nm, and the gain peak wavelength λg was set to 1325 nm. Thickness of the respective multilayer films of the upper multilayer mirror 16 and the lower multilayer mirror 12 is also adjusted to be λ/4. This surface-emitting laser element has an opening area of 30 μm and continuously oscillates at a threshold current of 1.5 mA and slope efficiency of 0.25 W/A. When the detuning to the short wavelength side of +25 nm was performed, the relaxation oscillation frequency fr increased from 6 GHz to 10 GHz. When optical communication of 10 Gbps was actually performed, satisfactory communication was successfully performed without any jitter or the like in an eye pattern.

A result obtained by applying the detuning to a plurality of surface-emitting laser element formed on a wafer using an error in manufacturing is explained. FIG. 10 is a graph for explaining a range of a detuning amount on the wafer. In FIG. 10, a characteristic curve R1 indicates reflectance of the upper multilayer mirror 16, a characteristic curve R2 indicates reflectance of the lower multilayer mirror 12, and a characteristic curve R1 indicates a geometric mean of the upper multilayer mirror 16 and the lower multilayer mirror 12. A black circle mark indicates a gain peak wavelength at the time of the room temperature operation and an X mark indicates an oscillation wavelength at the time of the room temperature operation. As shown in FIG. 10, the gain peak wavelength is shifted to the short wavelength side as a radius (a distance) from the center of the wafer increases. The oscillation wavelength is shifted to the long wavelength side as the distance from the center of the wafer increases. When the distance from the center of the wafer reaches near 20 mm, reflectance suddenly decreases and, according to the decrease, the surface-emitting laser elements stop oscillating. As described above, a value calculated by subtracting an oscillation wavelength at the time of the room temperature operation from a gain peak wavelength at the time of the room temperature operation is a detuning amount. Thus, in FIG. 10, a largest detuning amount Dcmax is obtained in a surface-emitting laser element placed at a distance from the center of about 3 mm. Therefore, in the surface-emitting laser element in the 1.3-μm band, it is possible to perform the detuning to about 0 nm to 25 nm, or about 0 meV to 20 meV.

The respective surface-emitting laser elements on the wafer are elements in the 1.3-μm band. However, it is possible to apply the detuning to about 0 nm to 35 nm (about 0 meV to 20 meV) to a surface-emitting laser element in the 1.55-μm band. This indicates that a detuning amount (a wavelength) in the 1.3-μm band only has to be converted into energy and set as an energy shift amount. This means that it is possible to apply detuning for causing energy shift of 20 meV to the respective surface-emitting laser element in the 1.3-μm band and the 1.55-μm band.

The surface-emitting leaser element described above is a surface-emitting laser element in the 1.3-μm band. However, it goes without saying that it is also possible to increase a differential gain by applying the detuning to the short wavelength side to the surface-emitting laser element in the 1.55-μm band and increase a relaxation oscillation frequency to thereby increase back-reflection tolerance.

For example, a surface-emitting laser element, which was the surface-emitting laser element described according to the first embodiment and was not subjected to the modulation doping, was manufactured. In the surface-emitting laser element, the quantum well layers 42a to 42c were formed of Ga_0.55In_0.45N_0.025As_0.945Sb_0.03, barrier layers corresponding to the barrier layers 41a to 41d were formed of GaN_0.02As_0.9Sb_0.08, thickness of the quantum well layers and the barrier layers was set to 20 nm, a cavity length was adjusted, and the gain peak wavelength λg at the time of the room temperature operation was set to 1580 nm and the oscillation wavelength λlasing at the time of the room temperature operation was set to 1550 nm. Thickness of the respective multilayer films of the upper multilayer mirror 16 and the lower multilayer mirror 12 is also adjusted to be λ/4. This surface-emitting laser element has an opening area of 30 μm² and continuously oscillates at a threshold current of 1.5 mA and slope efficiency of 0.25 W/A. When the detuning to the short wavelength side of +30 nm was performed, the relaxation oscillation frequency fr increased from 6 GHz to 10 GHz. When optical communication of 10 Gbps was actually performed, satisfactory communication was successfully performed without any jitter or the like in an eye pattern.

According to the second embodiment, a differential gain is increased by performing the detuning to the short wavelength side and the relaxation oscillation frequency fr is increased by the increase in the differential gain, whereby a surface-emitting laser element with large back-reflection tolerance is realized without decreasing an output.

Furthermore, according to the second embodiment, the modulation doping described according to the first embodiment is not applied. However, the modulation doping may be applied according to the second embodiment. This makes it possible to further improve a differential gain and, as a result, realize a surface-emitting laser element with larger back-reflection tolerance without decreasing an output;

When the detuning according to the second embodiment is applied, for-example, a surface-emitting laser element in the long wavelength band that has the critical back-reflection fextc, with which a value of the RIN at 0 GHz to 2 GHz becomes −115 dB/Hz, equal to or larger than −30 dB and the relaxation oscillation frequency fr at a bias point equal to or higher than 5 GHz is realized. This makes it possible to satisfactorily perform communication at transmission speed of 2.5 Gbps. A surface-emitting laser element in the 1.3-μm band that has the critical back-reflection fextc, with which a value of the RIN at 0 GHz to 8 GHz becomes −115 dB/Hz, equal to or larger than −20 dB and the relaxation oscillation frequency fr at a bias point equal to or higher than 10 GHz is realized. This makes it possible to satisfactorily perform communication at transmission speed of 10 Gbps. Moreover, a surface-emitting laser element in the 1.55-μm band that has the critical back-reflection fextc, with-which a value of the RIN at 0 GHz to 8 GHz becomes −115 dB/Hz, equal to or larger than −30 dB and the relaxation oscillation frequency fr at a bias point equal to or higher than 10 GHz is realized. This makes it possible to satisfactorily perform communication at transmission speed of 10 Gbps.

Moreover, according to the second embodiment, the semiconductor film is used for both the upper multilayer mirror 16 and the lower multilayer mirror 12. However, the multilayer mirrors are not limited to the semiconductor film. For example, a dielectric film may be used. According to the second embodiment, the lower multilayer mirror is formed by the multilayer films with AlAs/GaAs set as a pair and the upper multilayer mirror is formed by the multilayer films with Al_0.9Ga_0.1As/GaAs set as a pair. However, it is also possible to form both the multilayer mirrors with multilayer films with AlGaAs/AlGaAs having different Al compositions set as a pair. Moreover, it is also possible to provide gradient composition layers in which compositions are gradually changed may be provided among these respective layers.

Furthermore, according to the first embodiment, GaInNAsSb is used as the quantum well layers 42a to 42c. However, a material of the quantum well layers 42a to 42c is not limited to this material. For example, an AlGaInAs semiconductor material, a GaInAsP semiconductor material, an InGaAsSb semiconductor material, a TlGaInAsP semiconductor material, or the like may be used. According to the first embodiment, the active layer 32 has the quantum well structure. However, the active layer 32 is not limited to this structure. The active layer 32 may have a quantum wire structure or a quantum dot structure.

Moreover, according to the second embodiment, the surface-emitting laser element is the surface-emitting laser element having an oscillation wavelength in the 1310-nm band and the 1550-nm band. However, it is also possible to form a surface-emitting laser element having other oscillation wavelengths, for example, an oscillation wavelength in a 300-nm to 1600-nm band. For example, it is also possible to form a surface-emitting laser element having an oscillation wavelength in an 850-nm band. However, in this case, a quantum well layer is formed of GaAs.

Furthermore, according to the second embodiment, back-reflection tolerance of the surface-emitting laser element itself is described. However, the present invention is not limited to this back-reflection tolerance. It is also possible to apply the present invention to back-reflection tolerance with a laser module including this surface-emitting laser element set as a unit. In the laser module, the surface-emitting laser element is bonded to a CAN package, other plastic packages, or the like. An optical fiber receptacle or a pigtail is attached to the laser module. In this case, since the back-reflection tolerance is high, an optical element such as an isolator does not have to be mounted. Thus, it is possible to realize reduction in cost of the laser module itself.

When this laser module is set as a unit, since a loss due to coupling of the surface-emitting laser element and an optical fiber is intrinsic, a critical back-reflection decreases in appearance. When the loss due to coupling is about 3 dB, in the laser module, the critical back-reflection increases by a loss of 6 dB from the surface-emitting laser element to the optical fiber and vice versa. As a result, a laser module having a surface-emitting laser element in the long wavelength band that has the critical back-reflection fextc, with which a value of the RIN at 0 GHz to 2 GHz becomes −115 dB/Hz, equal to or larger than −24 dB and the relaxation oscillation frequency fr at a bias point equal to or higher than 5 GHz is realized. This makes it possible to satisfactorily perform communication at transmission speed of 2.5 Gbps. A laser module having a surface-emitting laser element in the 1.3-μm band that has the critical back-reflection fextc, with which a value of the RIN at 0 GHz to 8 GHz becomes −115 dB/Hz, equal to or larger than −14 dB and the relaxation oscillation frequency fr at a bias point equal to or higher than 10 GHz is realized. This makes it possible to satisfactorily perform communication at transmission speed of 10 Gbps. Moreover, a laser module having a surface-emitting laser element in the 1.55-μm band that has the critical back-reflection, with which a value of the RIN at 0 GHz to 8 GHz becomes −115 dB/Hz, equal to or larger than −24 dB and the relaxation oscillation frequency fr at a bias point equal to or higher than 10 GHz is realized. This makes it possible satisfactorily perform communication at transmission speed of 10 Gbps.

According to the first and the second embodiments, the surface-emitting laser element is the surface-emitting laser element formed on the n-type substrate. However, the surface-emitting laser element is not limited to this surface-emitting laser element. The surface laser element may be a surface-emitting laser element formed on a p-type substrate. In this case, the selective oxidation layer 14 is provided on a p-side, that is, the lower multilayer mirror side and performs current confinement.

FIG. 11 is a schematic of a surface-emitting laser element array 50 according to a third embodiment of the present invention. In the surface-emitting laser element array 50, a plurality of surface-emitting laser elements 10 described in the first embodiment are arranged on a substrate, as shown in FIG. 11. For the purpose of heat radiation, a two-dimensional surface-emitting laser element array 50 is set on a heat sink 60 made of AlN, CuW, or the like. In the two-dimensional surface-emitting laser element array 50, five surface-emitting laser elements 10 shown in FIG. 1 are two-dimensionally arranged in five rows such that twenty-five surface-emitting laser elements 10 are arranged in total. In the two-dimensional surface-emitting laser element array 50, upper and lower multilayer mirrors and a semiconductor layer serving as the active layer 32 or the like are uniformly stacked on an n-GaAs substrate 11 and, then, a large number of surface-emitting laser elements are simultaneously formed by treatment such as etching. A space among the respective surface-emitting laser elements is about 150 micrometers. Grooves reaching the depth of the lower multilayer mirror 12 are formed to prevent electrical interference.

In providing a laser array module using such a surface-emitting laser element array in which a plurality of surface-emitting laser elements are integrated, if isolators are inserted in the respective surface-emitting laser elements to control external feedback, a size of the module is increased and cost of manufacturing the module is also increased. According to the third embodiment, the respective surface-emitting laser elements constituting the surface-emitting laser element array 50 are formed as elements excellent in external feedback tolerance, which makes it unnecessary to insert isolators and makes it possible to provide a small laser array module.

A surface-emitting laser element array in which surface-emitting laser elements are two-dimensionally arranged on a substrate is described above. However, the same holds true for a surface-emitting laser element array in which surface-emitting laser elements are one-dimensionally arranged.

According to an embodiment of the present invention, a relaxation oscillation frequency at the bias point in the cavity is set to exceed an optical communication frequency for modulating a laser light output from the surface-emitting leaser element. Specifically, a p-type impurity is doped in the barrier layer forming the active layer or detuning to an oscillation wavelength at the time of an operation from a gain peak wavelength at the time of the room temperature is performed toward a short wavelength side. Consequently, a differential gain is increased, the relaxation oscillation frequency is increased to be set to exceed the optical communication frequency, and back-reflection tolerance is improved. Thus, there is an effect that it is possible to improve back-reflection tolerance without reducing an optical output by increasing reflectance and realize reduction in cost of the laser module.

Although the invention has been described with respect to a specific embodiment for a complete and clear disclosure, the appended claims are not to be thus limited but are to be construed as embodying all modifications and alternative constructions that may occur to one skilled in the art that fairly fall within the basic teaching herein set forth.

Claims

1. A surface-emitting laser element in which a cavity is formed by a lower multilayer mirror and an upper multilayer mirror and an active layer is arranged between the lower multilayer mirror and the upper multilayer mirror, wherein a relaxation oscillation frequency at a bias point in the cavity is set to exceed an optical communication frequency for modulating a laser light output from the surface-emitting laser element.

2. The surface-emitting laser element according to claim 1, wherein the relaxation oscillation frequency is set by increasing a differential gain.

3. The surface-emitting laser element according to claim 1, wherein a p-type impurity is doped in a barrier layer forming the active layer.

4. The surface-emitting laser element according to claim 3, wherein a doping concentration of the p-type impurity is in a range between 1×1018 cm−3 and 2×1019 cm−3.

5. The surface-emitting laser element according to claim 3, wherein the p-type impurity includes at least one of carbon, beryllium, zinc, and magnesium.

6. The surface-emitting laser element according to claim 1, wherein the relaxation oscillation frequency is set by performing a detuning from a gain peak wavelength at a room temperature to an oscillation wavelength at an operation toward a short wavelength side.

7. The surface-emitting laser element according to claim 6, wherein a value of the detuning is a value with which at least a differential gain is increased after the detuning.

8. The surface-emitting laser element according to claim 6, wherein a value of the detuning is an energy shift value obtained by converting a wavelength into an energy and is equal to or less than 20 milli-electron volts.

9. The surface-emitting laser element according to claim 1, wherein an oscillation frequency is in a range between 300 nanometers and 1600 nanometers.

10. The surface-emitting laser element according to claim 1, wherein a selective oxidation layer obtained by oxidizing a part of a current confinement layer containing at least aluminum and arsenide is provided to confine an injection current.

11. The surface-emitting laser element according to claim 1, wherein a quantum well layer or a barrier layer forming the active layer uses any one of Gax1In1-xNy1Asy2Sb1-y1-y2 (0≦x1, y1, y2≦1) , Alx2Gax3In1-x2-x3As (0≦x2, x3≦1), and Tlx4Gax5In1-x4-x5Asy3P1-y3 (0≦x4, x5, y4≦1).

12. The surface-emitting laser element according to claim 1, wherein the active layer includes any one of a quantum well structure, a quantum wire structure, and a quantum dot structure.

13. The surface-emitting laser element according to claim 1, wherein both the upper multilayer mirror and the lower multilayer mirror are semiconductor multilayer films or dielectric multilayer films, or one of the upper multilayer mirror and the lower multilayer mirror is a semiconductor multilayer film and other of the upper multilayer mirror and the lower multilayer mirror is a dielectric multilayer film.

14. The surface-emitting laser element according to claim 1, wherein the upper multilayer mirror, the active layer, and the lower multilayer mirror are formed on a gallium arsenide substrate, and the upper multilayer mirror and the lower multilayer mirror includes a plurality of pairs of multilayer films of Alx6Ga1-x6As (0≦x6<1) and Alx7Ga1-7xAs (0≦x7≦1, x6<x7) set as a pair.

15. The surface-emitting laser element according to claim 1, wherein a critical back-reflection, with which a value of relative intensity noise becomes −115 decibels per hertz in a region of the optical communication frequency of 0 gigahertz to 2 gigahertz, is equal to or larger than −30 decibels in magnitude, and the relaxation oscillation frequency at the bias point is equal to or higher than 5 gigahertz.

16. The surface-emitting laser element according to claim 1, wherein a critical back-reflection, with which a value of relative intensity noise becomes −115 decibels per hertz in a region of the optical communication frequency of 0 gigahertz to 8 gigahertz, is equal to or larger than −20 decibels in magnitude, the relaxation oscillation frequency at the bias point is equal to or higher than 10 gigahertz, and an oscillation wavelength is in a 1300-nanometer band.

17. The surface-emitting laser element according to claim 1, wherein a critical back-reflection, with which a value of relative intensity noise becomes −115 decibels per hertz in a region of the optical communication frequency of 0 gigahertz to 8 gigahertz, is equal to or larger than −30 decibels in magnitude, the relaxation oscillation frequency at the bias point is equal to or higher than 10 gigahertz, and an oscillation wavelength is in a 1550-nanometer band.

18. A laser module comprising: a surface-emitting laser element in which a cavity is formed by a lower multilayer mirror and an upper multilayer mirror and an active layer is arranged between the lower multilayer mirror and the upper multilayer mirror, wherein a relaxation oscillation frequency of the surface-emitting laser element at a bias point in the cavity is set to exceed an optical communication frequency for modulating a laser light output from the surface-emitting laser element, and the laser light emitted from the surface-emitting laser element is output to outside via an optical fiber.

19. The laser module according to claim 18, wherein the relaxation oscillation frequency is set by doping a p-type impurity in a barrier layer forming the active layer to increase a differential gain.

20. The laser module according to claim 18, wherein the relaxation oscillation frequency is set by performing a detuning from a gain peak wavelength at a room temperature to an oscillation wavelength at an operation toward a short wavelength side, and a value of the detuning is a value with which at least a differential gain is increased after the detuning.

21. The laser module according to claim 18, further comprising: a CAN-type package to which the surface-emitting laser element is bonded.

22. The laser module according to claim 18, further comprising: an optical fiber receptacle for interfacing the laser module with an external device.

23. The laser module according to claim 18, further comprising: an optical fiber pigtail for interfacing the laser module with an external device.

24. The laser module according to claim 18, wherein a critical back-reflection, with which a value of relative intensity noise becomes −115 decibels per hertz in a region of the optical communication frequency of 0 gigahertz to 2 gigahertz, is equal to or larger than −30 decibels in magnitude, and the relaxation oscillation frequency at the bias point is equal to or higher than 5 gigahertz.

25. The laser module according to claim 18, wherein a critical back-reflection, with which a value of relative intensity noise becomes −115 decibels per hertz in a region of the optical communication frequency of 0 gigahertz to 8 gigahertz, is equal to or larger than −20 decibels in magnitude, the relaxation oscillation frequency at the bias point is equal to or higher than 10 gigahertz, and an oscillation wavelength is in a 1300-nanometer band.

26. The laser module according to claim 18, wherein a critical back-reflection, with which a value of relative intensity noise becomes −115 decibels per hertz in a region of the optical communication frequency of 0 gigahertz to 8 gigahertz, is equal to or larger than −30 decibels in magnitude, the relaxation oscillation frequency at the bias point is equal to or higher than 10 gigahertz, and an oscillation wavelength is in a 1550-nanometer band.

27. A surface-emitting laser element array comprising: a plurality of surface-emitting laser elements arranged in either one of a one-dimensional array and a two-dimensional array, wherein each of the surface-emitting laser elements includes a cavity formed by a lower multilayer mirror and an upper multilayer mirror; and an active layer arranged between the lower multilayer mirror and the upper multilayer mirror, and a relaxation oscillation frequency at a bias point in the cavity is set to exceed an optical communication frequency for modulating a laser light output from the surface-emitting laser element.

28. The surface-emitting laser element array according to claim 27, wherein the relaxation oscillation frequency of the surface-emitting laser element is set by doping a p-type impurity in a barrier layer forming the active layer, to increase a differential gain.

29. The surface-emitting laser element array according to claim 27, wherein the relaxation oscillation frequency of the surface-emitting laser element is set by performing a detuning from a gain peak wavelength at a room temperature to an oscillation wavelength at an operation toward a short wavelength side and setting a value of the detuning to a value with which at least a differential gain is increased after the detuning.

30. The surface-emitting laser element array according to claim 27, wherein a critical back-reflection, with which a value of relative intensity noise of the surface-emitting laser element becomes −115 decibels per hertz in a region of the optical communication frequency of 0 gigahertz to 2 gigahertz, is equal to or larger than −24 decibels in magnitude, and the relaxation oscillation frequency at the bias point is equal to or higher than 5 gigahertz.

31. The surface-emitting laser element array according to claim 27, wherein a critical back-reflection, with which a value of relative intensity noise of the surface-emitting laser element becomes −115 decibels per hertz in a region of the optical communication frequency of 0 gigahertz to 2 gigahertz, is equal to or larger than −20 decibels in magnitude, the relaxation oscillation frequency at the bias point is equal to or higher than 10 gigahertz, and an oscillation wavelength of the surface-emitting laser element is in a 1300-nanometer band.

32. The surface-emitting laser element array according to claim 27, wherein a critical back-reflection, with which a value of relative intensity noise of the surface-emitting laser element becomes −115 decibels per hertz in a region of the optical communication frequency of 0 gigahertz to 2 gigahertz, is equal to or larger than −30 decibels in magnitude, the relaxation oscillation frequency at the bias point is equal to or higher than 10 gigahertz, and an oscillation wavelength of the surface-emitting laser element is in a 1550-nanometer band.

33. A laser module comprising: a surface-emitting laser element array in which a plurality of surface-emitting laser elements are one-dimensionally or two-dimensionally arranged, wherein each of the surface-emitting laser elements includes a cavity formed by a lower multilayer mirror and an upper multilayer mirror; and an active layer arranged between the lower multilayer mirror and the upper multilayer mirror, a relaxation oscillation frequency at a bias point in the cavity is set to exceed an optical communication frequency for modulating a laser light output from the surface-emitting laser element, and the laser light emitted from the surface-emitting laser element is output to outside via an optical fiber.