The present application claims priority from Japanese application JP 2017-139805, filed on Jul. 19, 2017, the content of which is hereby incorporated by reference into this application.
The present invention relates to an optical transmission module.
Recently, multi-level modulation such as PAM4 (Four Level Pulse Amplitude Modulation) have been intensively investigated for larger size transmission and higher transmission rate of data in an optical communication system. PAM4 utilizes light intensity of transmission signals with four intensity levels to realize 2 bit/baud of the transmission signals.
An Electro-Absorption Optical Modulator (EA modulator) or a laser diode integrated with the EA modulator monolithically (EA modulator laser diode) is used to generate PAM4 optical modulation signals. The EA modulator comprises a semiconductor quantum well structure sandwiched between a p-type conductor and an n-type conductor. The EA modulator controls output intensity of incident light by utilizing a shift of an optical absorption edge of the semiconductor quantum well structure to longer wavelength in response to application of a voltage to the semiconductor quantum well structure to change an amount of absorption of the incident light in the semiconductor quantum well structure. An optical signal generator comprising the EA modulator is proposed in JP2017-003729A, for example.
As mentioned in the previous paragraph, JP2017-003729A discloses the optical signal generator comprising the EA modulator. The optical signal generator comprises a plurality of modulation parts connected in series in a path of an optical signal, and adapted to generate a multilevel-coded modulated optical signal by modulating an intensity of an input optical signal from a light source based on a modulation signal using the modulation parts, and including an electro-absorption optical modulator provided to each of the modulation parts, and switched between an ON state of optical absorption and an OFF state of the optical absorption in accordance with the modulation signal, wherein regarding an extinction ratio of the ON state to the OFF state in each of the modulation parts, at least two of the modulation parts have respective values different from each other, and the modulation parts having the respective extinction ratios different from each other are located so that the lower the extinction ratio is, the closer to the light source the modulation part is located.
The plurality of modulation parts disclosed in JP2017-003729A generates a modulation signal by converting a plurality of binary electric signals to a multi-level electric signal. However, such conversion of the plurality of binary electric signals to the multi-level electric signal needs a dedicated IC, and thus makes the optical transmission module larger in size, and increase its power consumption.
Therefore, it is an object of the invention to provide an optical transmission module which can generate PAM4 optical modulation signals without converting a plurality of binary electric signals to a multi-level electric signal.
(1) An optical transmission module according to the invention comprises a light source for emitting continuous waveform (CW) light, optical modulators arranged in series with a path of the CW light configured to modulate the CW light by switching relatively large absorption and relatively small absorption of the optical modulators in response to a modulation signal applied to the respective optical modulators, and an arithmetic logic circuit configured to receive a plurality of binary electrical signals, and then to perform logic operation on the plurality of binary electrical signals for generating a new plurality of binary electrical signals, wherein each of the new plurality of binary electrical signals is applied to the respective optical modulators as the modulation signal.
(2) An optical transmission module according to (1) wherein each of the new plurality of binary electrical signals is applied to the respective optical modulators as the modulation signal by the arithmetic logic circuit.
(3) An optical transmission module according to (1) further comprises a driver for driving the optical modulators, wherein each of the new plurality of binary electrical signals is applied to the respective optical modulators as the modulation signal by the driver.
(4) An optical transmission module according to any one of (1)-(3) wherein the arithmetic logic circuit performs logic operation on the plurality of binary electrical signals based on a Gray code.
(5) An optical transmission module according to any one of (1)-(3) wherein the arithmetic logic circuit performs logic operation on the plurality of binary electrical signals based on a NRZ encoding.
(6) An optical transmission module according to any one of (1)-(5) wherein the light source and the optical modulators are integrated on one device.
The invention will be described in detail with reference to the following drawings in which:
Like reference numerals designate the same or similar elements throughout all views so as to avoid any redundant description of the same or similar elements. It should be noted that the drawings are not to precise scale and may be exaggerated in thickness of lines or sizes of components for descriptive convenience and clarity only.
The first optical modulator 51, the second optical modulator 52, the third optical modulator 53, the light source 60, via holes 70, and a chip capacitor 80 are disposed on a GND pattern 90. The via holes 70 are disposed so as to connect to a grounded back plane of the optical transmission module 200. Thus, the GND pattern 90 is grounded.
The light source 60 is preferably a Distributed Feedback Laser Diode (DFB-LD). However, the light source 60 is not limited to the DFB-LD. The light source 60 is a CW light source. The light source 60 can be operated by a driver 300. The chip capacitor 80 can be disposed between a current path connecting the light source 60 with the driver 300 and the GND pattern 90. The chip capacitor 80 prevents RF components in the new plurality of binary electrical signals applied to the respective optical modulators from flowing into the light source 60, and prevents the light source 60 from breaking by electrostatic discharge.
The first optical modulator 51, the second optical modulator 52, and the third optical modulator 53 are EA modulators. An EA modulator utilizes a change of optical absorption of a quantum well structure of the EA modulator with a modulation signal (electric field) applied to the quantum well structure to switch ON and OFF states of the EA modulator. Specifically, when a voltage is applied to the quantum well structure, potential energy of the quantum well structure changes. As a result, the quantum level of the conduction band of the quantum well structure shifts to lower and the quantum level of the valence band of the quantum well structure shifts to higher. In other words, the applied voltage narrows the effective energy gap of the quantum well structure to change optical absorption of the quantum well structure. The larger the applied voltage is, the more the optical absorption is. This change in the optical absorption of the quantum well structure with the applied voltage is known as Quantum Confined Stark Effect (QCSE).
The first optical modulator 51, the second optical modulator 52 and the third optical modulator 53 are arranged in series with the path of the CW light emitted from the light source 60. The first optical modulator 51 is located closest to the light source 60. The second optical modulator 52 is located on the side opposite to the light source 60 and adjacent to the first optical modulator 51. The third optical modulator 53 is located closest to the output end of the optical transmission module 200. To suppress divergence of output light from the light source 60, the first optical modulator 51 and the second optical modulator 52, a first lens 41 can be disposed between the light source 60 and the first optical modulator 51, a second lens 42 can be disposed between the first optical modulator 51 and the second optical modulator 52, and a third lens 43 can be disposed between the second optical modulator 52 and the third optical modulator 53. Although not shown in
The arithmetic logic circuit 100 comprises a higher bit 1 and a lower bit 2 as inputs. The higher bit 1 and the lower bit 2 are binary electrical signals. The arithmetic logic circuit 100 is connected to the first optical modulator 51 and the second optical modulator 52 and the third optical modulator 53 via RF lines 11, 1213 and Au wires 21, 22, 23, respectively. The first optical modulator 51, the second optical modulator 52 and the third optical modulator 53 are connected to thin-film resistors 31, 32, 33 as terminal resistors, respectively.
The arithmetic logic circuit 100 performs logic operation on binary electrical signals from the higher and lower bits 1, 2 to generate new binary electrical signals. Then, the new binary electrical signals are applied to the first optical modulator 51, the second optical modulator 52 and the third optical modulator 53 as modulation signals, respectively. The first optical modulator 51, the second optical modulator 52 and the third optical modulator 53 change the respective optical absorption in response to the applied modulation signals.
The optical transmission module 200 can further comprise a driver (not shown) for driving the first optical modulator 51, the second optical modulator 52 and the third optical modulator 53. The driver can amplify the modulation amplitude of the new binary electrical signals, or alter the modulation amplitude to a predetermined voltage, and then apply the modulation amplitude to the first optical modulator 51, the second optical modulator 52 and the third optical modulator 53. However, the optical transmission module 200 can operate without the driver because the modulation amplitude of the new binary electrical signals is small. Individual optical modulators having small extinction ratio can work.
The first optical modulator 51, the second optical modulator 52 and the third optical modulator 53 modulate the CW light from the light source 60 by changing the optical absorption of the first optical modulator 51, the second optical modulator 52 and the third optical modulator 53 in response to the new binary electrical signals applied to the first optical modulator 51, the second optical modulator 52 and the third optical modulator 53, respectively. In multi-level light intensity modulation, intensity difference between any two adjacent levels of the light intensity is preferably kept constant. Thus, extinction ratio of the first optical modulator 51, the second optical modulator 52 and the third optical modulator 53 is configured such that difference of the light intensity between the two adjacent levels of the light intensity is kept constant.
Table 1 shows a relationship between PAM4 light intensity (relative value) and extinction ratio. In order to assign four levels of the PAM4 light intensity (relative value) to, for example, 10, 7, 4 and 1, respectively, extinction ratio (unit:dB) at each level should be configured with respect to the maximum light intensity and the next level as shown in Table 1. Throughout the description, unless explicitly noted, PAM4 relates to four-valued light intensity modulation signals.
Table 2 shows a relationship between PAM4 signal levels and ON/OFF states of each EA modulator. As shown in Table 2, when a PAM4 signal level is zero (where the extinction ratio is the highest), all the EA modulators are set to the ON state (where the light is most absorbed); when the PAM4 signal level is one, the first optical modulator 51 and the second optical modulator 52 are set to the ON state while the third optical modulator 53 remains the OFF state (where the light is transmitted through the third optical modulator 53); when the PAM4 signal level is two, the first optical modulator 51 is set to the ON state while the second optical modulator 52 and the third optical modulator 53 remain the OFF state; and when the PAM4 signal level is three (where the extinction ratio is the lowest), all the EA modulators remain the OFF state (where the light is least absorbed).
All the EA modulators are set to the ON state when the PAM4 signal level is zero. Thus, the EA modulators attenuate (the light intensity of) the CW light from the light source 60. Only the first optical modulator 51 and the second optical modulator 52 are set to the ON state when the PAM4 signal level is one. Thus, only the first optical modulator 51 and the second optical modulator 52 attenuate the CW light from the light source 60. Only the first optical modulator 51 is set to the ON state when the PAM4 signal level is two. Thus, only the first optical modulator 51 attenuates the CW light from the light source 60. All the EA modulators remain the OFF state when the PAM4 signal level is three. Thus, no EA modulators attenuate the CW light from the light source 60. However, strictly speaking, the light intensity when the light is emitted from the light source 60 is different from the light intensity when the light is transmitted through the third optical modulator 53 because of coupling loss in the optical system of the optical transmission module 200 and slight optical absorption of each EA modulator. An amount of light extinction at each EA modulator is configured such that intensity ratio between any two adjacent PAM4 signal levels is constant by considering other extinction factors than the voltage applied to each EA modulator. Combination of the ON/OFF states of the EA modulators in this manner makes it possible to generate a multi-level modulations signal comprising a plurality of levels of the light intensity, such as a PAM4 signal. Therefore, in order to generate PAM4 light modulation signals, it is important to select the EA modulator(s) to be driven in response to binary electrical signals (a higher bit and a lower bit) input to the optical transmission module 200.
Table 3 shows a relationship among higher and lower bits of two-bit signals, PAM4 signal levels (0,1,2,3), and states of the first optical modulator 51 (EA1), the second optical modulator 52 (EA2) and the third optical modulator 53 (EA3). Table 4 shows correspondence between new binary electrical signals generated in response to the higher and lower bits of the two-bit signals in Table 3 and then input to the EA1, and the operating (ON/OFF) states of the EA1. Likewise, Table 5 shows correspondence between new binary electrical signals generated in response to the higher and lower bits of the two-bit signals in Table 3 and then input to the EA2, and the operating (ON/OFF) states of the EA2. Table 6 shows similar correspondence for the EA3. As mentioned above, the arithmetic logic circuit 100 according to some embodiments is characterized by receiving the plurality of binary electrical signals (higher and lower bits), and then generating a new plurality of binary electrical signals (which is input to each EA).
As shown in Table 4, the arithmetic logic circuit 100 outputs zero only if one is input to both the higher and lower bits of the arithmetic logic circuit 100, then the EA1 does not absorb the CW light from the light source 60, and the CW light is transmitted through the EA1 and reaches the EA2. Otherwise, the arithmetic logic circuit 100 outputs one. Then, the EA1 receives the output from the arithmetic logic circuit 100 and operates in the ON state. In other words, the EA1 absorbs the CW light. As shown in Table 5, the arithmetic logic circuit 100 outputs one to the EA2 if zero is input to the higher bit, and outputs zero to the EA2 if one is input to the higher bit. As shown in Table 6, the arithmetic logic circuit 100 outputs one to the EA3 only if zero is input to both the higher and lower bits, and otherwise outputs zero to the EA3. In this manner, the arithmetic logic circuit 100 generates the new plurality of binary electrical signals depending on the values of the higher and lower bits, switches the ON/OFF states of the first optical modulator 51, the second optical modulator 52 and the third optical modulator 53 to generate a PAM4 light signal.
Table 7 shows correspondence among higher and lower bits of two-bit signals, PAM4 signal levels (0,1,2,3), and states of the first optical modulator 51 (EA1), the second optical modulator 52 (EA2) and the third optical modulator 53 (EA3). Table 8 shows correspondence between new binary electrical signals generated in response to the higher and lower bits of the two-bit signals in Table 7 and then input to the EA1, and the operating (ON/OFF) states of the EA1. Likewise, Table 9 shows correspondence between new binary electrical signals generated in response to the higher and lower bits of the two-bit signals in Table 3 and then input to the EA2, and the operating (ON/OFF) states of the EA2. Table 10 shows similar correspondence for the EA3. As mentioned above, the arithmetic logic circuit 100 according to some embodiments is characterized by receiving the plurality of binary electrical signals (higher and lower bits), and then generating a new plurality of binary electrical signals (which is input to each EA).
As shown in Table 8, the arithmetic logic circuit 100 outputs zero only if one and zero are input to the higher and lower bits of the arithmetic logic circuit 100, respectively, then the EA1 does not absorb the CW light from the light source 60, and the CW light is transmitted through the EA1 and reaches the EA2. Otherwise, the arithmetic logic circuit 100 outputs one. Then, the EA1 receives the output from the arithmetic logic circuit 100 and operates in the ON state. In other words, the EA1 absorbs the CW light. As shown in Table 9, the arithmetic logic circuit 100 outputs one to the EA2 if zero is input to the higher bit, and outputs zero to the EA2 if one is input to the higher bit. As shown in Table 10, the arithmetic logic circuit 100 outputs one to the EA3 only if zero is input to both the higher and lower bits, and otherwise outputs zero to the EA3. In this manner, the arithmetic logic circuit 100 generates the new plurality of binary electrical signals depending on the values of the higher and lower bits, switches the ON/OFF states of the first optical modulator 51, the second optical modulator 52 and the third optical modulator 53 to generate a PAM4 light signal.
The optical transmission module according to some embodiments controls the ON/OFF states of the plurality of the optical modulators based on binary electrical signals input to the plurality of the optical modulators to generate PAM4 light modulation signals. Unlike the prior optical transmission module, the optical transmission module according to some embodiments can directly obtain multi-level light intensity modulation from binary electrical signals without converting binary electrical signals into multi-level electrical signals. In other words, the optical transmission module according to some embodiments eliminates any circuits to convert binary electrical signals into multi-level electrical signals, and thus comprises simple circuitry. As a result, increase in size and power consumption of the optical transmission module is suppressed. Furthermore, the optical transmission module according to some embodiments eliminates a step of converting binary electrical signals into multi-level electrical signals, and thus provides shorter latency.
The optical transmission module according to some embodiments eliminates conversion of binary electrical signals into multi-level electrical signals, and thus suppresses degradation of light signals to be transmitted. As a result, the optical transmission module according to some embodiments realizes more reliable signal transmission.
While there have been described what are at present considered to be certain embodiments of the invention, it will be understood that various modifications may be made thereto, and it is intended that the appended claims cover all such modifications as fall within the true spirit and scope of the invention.
Number | Date | Country | Kind |
---|---|---|---|
2017-139805 | Jul 2017 | JP | national |
Number | Name | Date | Kind |
---|---|---|---|
5359679 | Tanaka et al. | Oct 1994 | A |
5434693 | Tanaka | Jul 1995 | A |
5510919 | Wedding | Apr 1996 | A |
5706116 | Sugata | Jan 1998 | A |
5706117 | Imai | Jan 1998 | A |
5751455 | Shibutani | May 1998 | A |
6271950 | Hansen | Aug 2001 | B1 |
6381056 | Ellis | Apr 2002 | B1 |
6490069 | Kahn | Dec 2002 | B1 |
6678479 | Naoe et al. | Jan 2004 | B1 |
7149256 | Vrazel | Dec 2006 | B2 |
7734189 | Ranganath | Jun 2010 | B2 |
9172472 | Daunt | Oct 2015 | B2 |
9733542 | Bai | Aug 2017 | B2 |
9746698 | Goodwill | Aug 2017 | B2 |
9787423 | Nagarajan | Oct 2017 | B2 |
9806821 | Nakamura | Oct 2017 | B2 |
9900021 | Elliott | Feb 2018 | B1 |
9933639 | Lin | Apr 2018 | B1 |
20010053165 | Wang | Dec 2001 | A1 |
20020171899 | Gurusami | Nov 2002 | A1 |
20020195622 | Ishimura | Dec 2002 | A1 |
20030011854 | Kahn et al. | Jan 2003 | A1 |
20030057456 | Wada | Mar 2003 | A1 |
20040032646 | Koren | Feb 2004 | A1 |
20040197106 | Noda | Oct 2004 | A1 |
20050018732 | Bond | Jan 2005 | A1 |
20050025500 | Hallemeier | Feb 2005 | A1 |
20050036791 | Gunn, III | Feb 2005 | A1 |
20050275920 | Sumi et al. | Dec 2005 | A1 |
20050276615 | Ranganath | Dec 2005 | A1 |
20060120729 | Bai | Jun 2006 | A1 |
20070212076 | Roberts | Sep 2007 | A1 |
20070230854 | Felix Keil | Oct 2007 | A1 |
20070230969 | Yutani | Oct 2007 | A1 |
20070237444 | Keil | Oct 2007 | A1 |
20080089634 | Mosinskis | Apr 2008 | A1 |
20080095486 | Shastri et al. | Apr 2008 | A1 |
20100156679 | Ehrlichman | Jun 2010 | A1 |
20110044573 | Webster | Feb 2011 | A1 |
20110091221 | De Gabory | Apr 2011 | A1 |
20120045163 | Wu | Feb 2012 | A1 |
20120087653 | Sawada | Apr 2012 | A1 |
20120230626 | Metz | Sep 2012 | A1 |
20120237160 | Shastri | Sep 2012 | A1 |
20130010343 | Hirayama | Jan 2013 | A1 |
20130176609 | Noguchi | Jul 2013 | A1 |
20130272700 | Satoh | Oct 2013 | A1 |
20140169723 | Kato | Jun 2014 | A1 |
20140233962 | Kato | Aug 2014 | A1 |
20140321864 | Bliss | Oct 2014 | A1 |
20140369638 | Doerr | Dec 2014 | A1 |
20150063822 | Noguchi | Mar 2015 | A1 |
20150110500 | Noguchi | Apr 2015 | A1 |
20150249501 | Nagarajan | Sep 2015 | A1 |
20150295650 | Lee | Oct 2015 | A1 |
20160103340 | Ding | Apr 2016 | A1 |
20160164613 | Menezo | Jun 2016 | A1 |
20160365929 | Nakamura et al. | Dec 2016 | A1 |
20170090268 | O'Sullivan | Mar 2017 | A1 |
20170093513 | Nagarajan | Mar 2017 | A1 |
20170310400 | Nagarajan | Oct 2017 | A1 |
20190018262 | Nejadmalayeri | Jan 2019 | A1 |
Number | Date | Country |
---|---|---|
5-341242 | Dec 1993 | JP |
2001-221985 | Aug 2001 | JP |
2003-5141 | Jan 2003 | JP |
2003-98492 | Apr 2003 | JP |
2005-352219 | Dec 2005 | JP |
2010-507131 | Mar 2010 | JP |
2012-49801 | Mar 2012 | JP |
2017-003729 | Jan 2017 | JP |
2000-75254 | Sep 2018 | JP |
Entry |
---|
Quadir et al, A 56Gbs PAM4 VCSEL driver circuit, Jun. 2012, ISSC, Pages All Document. |
Japanese Office Action received in corresponding Japanese Application No. 2015-116486 dated Sep. 25, 2018. |
Number | Date | Country | |
---|---|---|---|
20190028204 A1 | Jan 2019 | US |