Semiconductor light receiving device
09735296 ยท 2017-08-15
Assignee
Inventors
Cpc classification
Y02E10/50
GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
G02B6/2813
PHYSICS
H10F77/413
ELECTRICITY
H10F77/14
ELECTRICITY
International classification
H01L31/028
ELECTRICITY
H01L31/0352
ELECTRICITY
G02B6/28
PHYSICS
H01L31/0232
ELECTRICITY
Abstract
A semiconductor light receiving device includes a substrate, a semiconductor fine line waveguide provided on the substrate, and a light receiving circuit that is provided on the substrate and that absorbs light propagating through the semiconductor fine line waveguide. The light receiving circuit includes a p type first semiconductor layer, a number of second semiconductor mesa structures provided on the p type first semiconductor layer in such a manner that an n type second semiconductor layer is provided on top of an i type second semiconductor layer, a p side electrode connected to the p type first semiconductor layer in a location between the second semiconductor mesa structures, and an n side electrode connected to the n type second semiconductor layer. The refractive index and the optical absorption coefficient of the second semiconductor layers are greater than the refractive index and the optical absorption coefficient of the first semiconductor layer.
Claims
1. A semiconductor light receiving device, comprising: a substrate; a semiconductor fine line waveguide provided on the substrate; and a light receiving circuit configured to be provided on the substrate and absorb light propagating through the semiconductor fine line waveguide, wherein the light receiving circuit includes: a p type first semiconductor layer; a number of second semiconductor mesa structures provided on the p type first semiconductor layer in such a manner that an n type second semiconductor layer is provided on top of an i type second semiconductor layer; a p side electrode connected to the p type first semiconductor layer in a location between the second semiconductor mesa structures; and an n side electrode connected to the n type second semiconductor layer, the refractive index and the optical absorption coefficient of the second semiconductor layers are greater than the refractive index and the optical absorption coefficient of the first semiconductor layer, a positive bias power supply is connected to the n side electrode, and a signal line is connected to the p side electrode.
2. The semiconductor light receiving device according to claim 1, wherein the first semiconductor layer is an Si layer, and the second semiconductor layers are made of either Si.sub.xGe.sub.1-x (where 0x0.5) or Ge.sub.1-xSn.sub.x (where 0x0.1).
3. The semiconductor light receiving device according to claim 1 further comprising between the semiconductor fine line waveguide and the light receiving circuit an optical branching circuit configured to branch either light that propagates through the semiconductor fine line waveguide or the intensity peak location of light into the same number as that of the second semiconductor mesa structures.
4. The semiconductor light receiving device according to claim 3, wherein the optical branching circuit is a multi-mode interferometer coupler.
5. The semiconductor light receiving device according to claim 4, wherein the p type first semiconductor layer provides a part of the multi-mode interferometer coupler.
6. The semiconductor light receiving device according to claim 3, wherein the optical branching circuit is a directional coupler.
7. The semiconductor light receiving device according to claim 3, wherein the optical branching circuit is a branching waveguide.
8. The semiconductor light receiving device according to claim 1, wherein the number of the second semiconductor mesa structures is three.
9. The semiconductor light receiving device according to claim 1, wherein the number of the second semiconductor mesa structures is two, and the semiconductor fine line waveguide includes: a first semiconductor fine line waveguide from which light enters into one of the second semiconductor mesa structures from the first direction; and a second semiconductor fine line waveguide from which light enters into the other of the second semiconductor mesa structures from a second direction opposite to the first direction.
10. The semiconductor light receiving device according to claim 1, wherein the substrate is a single crystal semiconductor substrate where a buried insulator layer is provided on a surface.
Description
BRIEF DESCRIPTION OF DRAWINGS
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DESCRIPTION OF EMBODIMENTS
(21) Here, the semiconductor light receiving device according to an embodiment of the present invention is described in reference to
(22) At this time, the refractive index and the optical absorption coefficient of the second semiconductor layer are greater than the refractive index and the optical absorption coefficient of the first semiconductor layer. Typically, an Si layer is used for the first semiconductor layer, and either Si.sub.xGe.sub.i-x (here, 0x 0.5) or Ge.sub.i-xSn.sub.x (here, 0x0.1) is used for the second semiconductor layer.
(23) In addition, an optical branching unit 5 that branches either light 16 that propagates through the semiconductor fine line waveguide 4 or the position of the light intensity peak into the same number of pieces as that of the second semiconductor mesa structures 8 may be provided between the semiconductor fine line waveguide 4 and the light receiving unit 6.
(24) A multimode interferometer coupler (MMI coupler) may be used as the optical branching unit 5. At this time, the multimode interferometer coupler is integrated in such a manner that the p type first semiconductor layer 7 becomes part of the multimode interferometer coupler, and thus, the yield in the manufacture increases. Alternatively, a directional coupler or a branching waveguide such as a Y type branching waveguide may be used as the optical branching unit 5.
(25) Though two is a typical number of the second semiconductor mesa structures 8, three structures may be provided, and in this case, it is possible to increase the amplitude by using a differential signal.
(26) In the case where two second semiconductor mesa structures 8 are provided, a semiconductor fine line waveguide through which light enters into one of the second semiconductor mesa structures 8 in the first direction and a semiconductor fine line waveguide through which light enters into the other second semiconductor mesa structure 8 in the second direction that is opposite to the first direction may be provided. By providing such a bidirectional, light entering type semiconductor light receiving device, it becomes easy to incorporate the semiconductor light receiving device into an optical multiplexor using an add-drop type ring resonator array.
(27) As for the substrate 1 on which such a semiconductor light receiving device is formed, a typical example is an SOI substrate where a single crystal semiconductor layer is provided on a single crystal semiconductor substrate 2 with a buried insulating layer 3 in between. In this case, the semiconductor fine line waveguide 4, the optical branching unit 5 and the first semiconductor layer may be formed by processing this single crystal semiconductor layer.
(28) In the semiconductor light receiving device according to the embodiment of the present invention, a signal 18 is taken out from the p side electrode 14 that is formed on the p type first semiconductor layer 7 between the second semiconductor mesa structures 8, and a positive bias power supply 15 for applying an electrical field is connected to the n side electrodes 13 provided on the n type second semiconductor layer 10. The structure has a number of paths through which a photocurrent flows, and therefore is a structure that is appropriate for high speed operation where the device resistance is suppressed.
(29) In addition, a reverse bias state can be achieved from the relationship between the bias power supply path and the signal output path without using a bias Tee or a negative voltage supply, and therefore, the semiconductor light receiving device is very advantageous regarding the cost as compared to the conventional structure. Furthermore, the bias power supply path is the n side electrodes 13 that make contact with the n type second semiconductor layer 10, and therefore, the power supply that is required at the time when a reverse bias that is necessary for a photodiode is applied may be a positive voltage supply in the same manner as for the operation of a TIA, and as a result, no more than one voltage supply is necessary in the whole receiver. Moreover, the number of signal lines 17 is at the minimum, which can prevent an excessive parasitic capacitance or an excessive parasitic inductance from being generated at the time of circuit connection.
(30) In addition, the same polarities as in the conventional structure can be maintained as the polarities of the semiconductor materials within the photodiode, and therefore, such problems that the intensity of the electrical field generated in the Ge materials on Si lowers and the sensitivity in the reception deteriorates together with this can be avoided in the case where the polarities of the semiconductor materials are altered from the conventional structure.
EXAMPLE 1
(31) Next, the semiconductor light receiving device according to Example 1 of the present invention is described in reference to
(32) A p side electrode 38 is provided so as to make contact with the p type Si layer between the two mesa structures, and at the same time, n side electrodes 37 are provided so as to make contact with the n type Ge layer 35. Though not shown, a positive bias power supply is connected to the n side electrodes 37, and a signal line is connected to the p side electrode 38.
(33) An SiO.sub.2 film 30 works as a mask for selective area growth when the mesa structures are formed, and an SiO.sub.2 film 36 becomes an insulating passivation film when the n side electrodes 37 and the p side electrode 38 are formed. In addition, the BOX layer 22 becomes a lower clad layer for the Si fine line waveguide 25, and the SiO.sub.2 films 30 and 36 become an upper clad layer, and therefore, light is effectively confined within the Si fine line waveguide 25.
(34) Light that propagates through the Si fine line waveguide 25 is converted to a guided mode having two intensity peaks by the MMI coupler 26, and after that is led to and absorbed by the i type Ge layer 32 through the evanescent optical coupling so as to generate photocarriers. A reverse bias is applied to this pin structure by the positive bias power supply, and therefore, the photocarriers are drawn out, and thus, the pin structure operates as a photodiode.
(35) Next, the manufacturing process for the semiconductor light receiving device according to Example 1 of the present invention is described in reference to
(36) Next, as illustrated in
(37) Next, as illustrated in
(38) Next, as illustrated in
(39) Next, as illustrated in
(40) Next, as illustrated in
(41) Next, as illustrated in
(42) Next, the patterned photoresist 33 is removed, and after that, an SiO.sub.2 film 36 is grown on the entire surface in accordance with a CVD method. Contact holes that reach the n type Ge layer 35 and the p type Si layer 29 are created in the SiO.sub.2 film 36 through photolithography and dry etching. Subsequently, an Al film is deposited in accordance with a sputtering method, and after that, the Al film is patterned through photolithography and dry etching so as to form n side electrodes 37 and a p side electrode 38, and thus, the basic structure of the semiconductor light receiving device according to Example 1 of the present invention is complete.
(43) In Example 1 of the present invention, the light receiving unit is provided with two mesa structures having the same arrangement as the related art in terms of the conductivity types, where a positive bias power supply is connected to the mesa structures and a signal line is connected to the p type Si layer, and therefore, the structure has two paths through which a photocurrent flows, and thus is appropriate for high speed operation with the device resistance being reduced.
(44) In addition, a reverse bias state can be achieved from the relationship between the bias power supply path and the signal output path without using a bias Tee or a negative voltage supply, and therefore, the present structure is very advantageous in terms of cost as compared to the conventional structure. In addition, the signal line is only one line, and therefore can prevent the parasitic capacitance and the parasitic inductance from being excessively generated at the time of circuit connection.
EXAMPLE 2
(45) Next, the semiconductor light receiving device according to Example 2 of the present invention is described in reference to
(46) A p side electrode 38 is provided so as to make contact with the p type Si layer between the two mesa structures, and at the same time, n side electrodes 37 are provided so as to make contact with the n type Ge layer 35. Though not shown, a positive bias power supply is connected to the n side electrodes 37, and a signal line is connected to the p side electrode 38.
(47) Light that propagates through the Si fine line waveguide 25 is split into two beams by the directional coupler 39, and after that is led to and absorbed by the i type Ge layer 32 through evanescent optical coupling so as to generate photocarriers. A reverse bias is applied to this pin structure by the positive bias power supply, and therefore, the photocarriers are drawn out, and thus, the pin structure operates as a photodiode. In the case of Example 2, the semiconductor light receiving device is different from that in Example 1 only in the optical branching structure, and thus has the same basic working effects as in Example 1.
EXAMPLE 3
(48) Next, the semiconductor light receiving device according to Example 3 of the present invention is described in reference to
(49) A p side electrode 38 is provided so as to make contact with the p type Si layer between the two mesa structures, and at the same time, n side electrodes 37 are provided so as to make contact with the n type Ge layer 35. Though not shown, a positive bias power supply is connected to the n side electrodes 37, and a signal line is connected to the p side electrode 38.
(50) Light that propagates through the Si fine line waveguide 25 is split into two directions by the Y-branch waveguide, and after that is led to and absorbed by the i type Ge layer 32 through evanescent optical coupling so as to generate photocarriers. A reverse bias is applied to this pin structure by the positive bias power supply, and therefore, the photocarriers are drawn out, and thus, the pin structure operates as a photodiode. In the case of Example 3, the semiconductor light receiving device is different from that in Example 1 only in the optical branching structure, and thus has the same basic working effects as in Example 1.
EXAMPLE 4
(51) Next, the semiconductor light receiving device according to Example 4 of the present invention is described in reference to
(52) A p side electrode 38 is provided so as to make contact with the p type Si layer between the two mesa structures, and at the same time, n side electrodes 37 are provided so as to make contact with the n type Ge layer 35. Though not shown, a positive bias power supply is connected to the n side electrodes 37, and a signal line is connected to the p side electrode 38.
(53) Light that propagates through the Si fine line waveguide 25 is led to and absorbed by the i type Ge layer 32 through the evanescent optical coupling so as to generate photocarriers while being converted to a guided mode having two intensity peaks by the MMI coupler 41. A reverse bias is applied to this pin structure by a positive bias power supply, and therefore, the photocarriers are drawn out so that the pin structure operates as a photodiode.
(54) In Example 4, the MMI coupler 41 is integrated with the p type Si layer 29, which makes it possible to miniaturize the device and makes the processing pattern simpler, and therefore, the manufacture yield increases.
EXAMPLE 5
(55) Next, the semiconductor light receiving device according to Example 5 of the present invention is described in reference to
(56) A p side electrode 38 is provided so as to make contact with the p type Si layer between the two mesa structures, and at the same time, n side electrodes 37 are provided so as to make contact with the n type SiGe layer 43. Though not shown, a positive bias power supply is connected to the n side electrodes 37, and a signal line is connected to the p side electrode 38.
(57) Light that propagates through the Si fine line waveguide 25 is converted to a guided mode having two intensity peaks by the MMI coupler 26, and after that is led to and absorbed by the i type SiGe layer 42 through the evanescent optical coupling so as to generate photocarriers. A reverse bias is applied to this pin structure by a positive bias power supply, and therefore, the photocarriers are drawn out so that the pin structure operates as a photodiode.
(58) In Example 5, the mesa structures are formed of an SiGe layer, and therefore, lattice mismatching vis--vis Si is mitigated as compared to a case where the mesa structures are formed of a Ge layer, and thus, epitaxial growth becomes easier. Though SiGe is used here, Ge.sub.1-xSn.sub.x (where 0x0.1) may be used.
EXAMPLE 6
(59) Next, the semiconductor light receiving device according to Example 6 of the present invention is described in reference to
(60) p side electrodes 38 are provided so as to make contact with the p type Si layer in two locations between the three mesa structures, and at the same time, n side electrodes 37 are provided so as to respectively make contact with three portions of the n type Ge layer 35. Though not shown, a positive bias power supply is connected to the three n side electrodes 37, and a signal line is connected to the two p side electrodes 38.
(61) In Example 6, three mesa structures and two signal lines are provided, and therefore, it is possible to increase the amplitude of a signal by carrying out a differential operation on the signal.
EXAMPLE 7
(62) Next, the semiconductor light receiving device according to Example 7 of the present invention is described in reference to
(63) In this case as well, a p side electrode 38 is provided so as to make contact with the p type Si layer between each pair of mesa structures, and at the same time, n side electrodes 37 are provided so as to make contact with the n type Ge layer 35. Though not shown, a positive bias power supply is connected to the n side electrodes 37, and a signal line is connected to the p side electrodes 38.
(64) Light that propagates through the Si fine line waveguide 44 is led to the i type Ge layer 32 in the mesa structure on the left side in the figure through the evanescent optical coupling and is absorbed so as to generate photocarriers. Meanwhile, light that propagates through the Si fine line waveguide 45 is led to the i type Ge layer 32 in the mesa structurese on the right side in the figure through the evanescent optical coupling and is absorbed so as to generate photocarriers. At this time, the photocarriers are generated at the same time in the left and right mesa structures. A reverse bias is applied to this pin structure by a positive bias power supply, and therefore, the photocarriers are drawn out so that the pin structure operates as a single bidirectional entering type photodiode 50.
(65) Next, an application of the semiconductor light receiving device according to Example 7 of the present invention is described in reference to
(66) In addition, a number of ring waveguides 55.sub.1 through 55.sub.3, each made of an Si fine line waveguide having a different optical path length, that form an add-drop type ring resonator array are optically coupled to the loop waveguide 53. Furthermore, output waveguides 56.sub.1 through 56.sub.3, each made of an Si fine line waveguide having two output ports, are optically coupled to the ring waveguides 55.sub.1 through 55.sub.3, respectively, on the drop port side.
(67) In this case, the radius of curvature R of the ring waveguides 55.sub.1 through 55.sub.3 is optimized so as to control the demultiplexed wavelength, and thus, this add-drop type ring resonator array becomes a demultiplexer. Bidirectional entering type photodiodes 50.sub.1 through 50.sub.3 are respectively connected to the output waveguides 56.sub.1 through 56.sub.3 that extend from these two output ports in such a manner that the optical distances are equal between the polarization splitter 52 and one mesa structure in the pair in each bidirectional entering type photodiodes 50.sub.1 through 50.sub.3, and between the polarization splitter 52 and the other mesa structure in the pair.
(68) A WDM light signal that has been inputted into the input waveguide 51 is divided into a TM light signal and a TE light signal depending on the polarization plane by the polarization splitter 52, and then the signals propagate through the loop waveguide 52 in the direction opposite to each other. The TM light signal is converted to a TE* light signal of which the polarization plane has been rotated by 90 by the polarization rotator 54. The TE light signal and the TE* light signal that propagate through the loop waveguide 53 are demultiplexed into the respective wavelengths (1 through 3) by the ring waveguides 55.sub.1 through 55.sub.3 that form add-drop type ring resonators.
(69) Light signals that have been demultiplexed into the respective wavelengths are inputted into bidirectional entering type photodiodes 50.sub.1 through 50.sub.3 as a TE light signal or a TE* optical signal in the same polarization state and are outputted as the sum of the currents that flow from the two mesa structures in the pair. In addition, light that has leaked out from the terminal of each bidirectional entering type photodiode 50.sub.1 through 50.sub.3 on the side opposite to the entering plane does not go through any of the output waveguides 56.sub.1 through 56.sub.3 in the opposite direction or enter into the loop waveguide 53 via a ring resonator, and therefore, excess noise generated by the leaked light can be suppressed.
(70) All examples and conditional language provided herein are intended for the pedagogical purposes of aiding the reader in understanding the invention and the concepts contributed by the inventor to further the art, and are not to be construed as limitations to such specifically recited examples and conditions, nor does the organization of such examples in the specification relate to a showing of the superiority and inferiority of the invention. Although one or more embodiments of the present invention have been described in detail, it should be understood that the various changes, substitutions, and alterations could be made hereto without departing from the spirit and scope of the invention.