Directly modulated laser for PON applications
View Patent ↗In an embodiment, a distributed Bragg reflector (DBR) laser includes a gain section and a passive section. The gain section includes an active region, an upper separate confinement heterostructure (SCH), and a lower SCH. The upper SCH is above the active region and has a thickness of at least 60 nanometers (nm). The lower SCH is below the active region and has a thickness of at least 60 nm. The passive section is coupled to the gain section, the passive section having a DBR in optical communication with the active region.
1. A distributed Bragg reflector (DBR) laser comprising:
a gain section comprising:
an active region;
an upper separate confinement heterostructure (SCH) above the active region having a thickness of at least 60 nanometers (nm); and
a lower SCH below the active region having a thickness of at least 60 nm; and
a passive section coupled to the gain section, the passive section comprising a Bragg filter in optical communication with the active region.
2. The DBR laser of claim 1 , further comprising a gain electrode coupled to the gain section, the gain electrode configured to be coupled to a direct modulation source providing a modulation signal having a data rate of about 10 gigabits per second or higher.
3. The DBR laser of claim 2 , wherein in response to application of the modulation signal to the gain electrode, the DBR laser is configured to generate an optical signal having a frequency modulation profile exhibiting both transient chirp and adiabatic chirp, a ratio of transient chirp to adiabatic chirp being in a range from 1:3 to 1:4.
4. The DBR laser of claim 1 , wherein a modulation signal applied to the gain section has a modulation swing of at least 40 milli amps peak-to-peak (mApp).
5. The DBR laser of claim 4 , wherein the gain section has a length of 300 micrometers (um) or less.
6. The DBR laser of claim 5 , wherein the modulation signal applied to the gain section has a modulation swing of about 60 mApp and the gain section has a length of about 200 um.
7. The DBR laser of claim 1 , wherein the DBR laser has a reach of 21 kilometers or more with a bit error rate of about 1×10-3.
8. The DBR laser of claim 1 , wherein the thickness of the upper SCH is less than 125 nm and the thickness of the lower SCH is less than 125 nm.
9. The DBR laser of claim 1 , wherein the DBR laser is tuned toward a long wavelength side of a Bragg peak associated with the DBR laser.
10. The DBR laser of claim 1 , wherein the DBR laser comprises a front DBR laser in which the passive section is positioned between the gain section and a front side of the front DBR laser having an antireflection (AR) coating.
11. The DBR laser of claim 1 , wherein the DBR laser comprises a rear DBR laser in which the gain section is positioned between the passive section and a front side of the rear DBR laser having an antireflection (AR) coating.
12. The DBR laser of claim 1 , wherein:
the passive section comprises a first passive section;
the Bragg filter comprises a first Bragg filter;
the DBR laser further comprises a second passive section including a second Bragg filter in optical communication with the active region; and
the gain section is positioned between the first passive section and the second passive section such that the DBR laser comprises a front/rear DBR laser.
13. The DBR laser of claim 1 , wherein a relaxation oscillation frequency of the DBR laser is at least 12 gigahertz (GHz) and a damping caused by carrier transport effect in the gain section is at least 12 GHz.
14. The DBR laser of claim 13 , wherein the relaxation oscillation frequency of the DBR laser is at least 16 GHz.
15. The DBR laser of claim 1 , wherein:
the thickness of the upper SCH is about 100 nanometers (nm);
the thickness of the lower SCH is about 100 nm; and
a K factor of the DBR laser is 0.32 nanoseconds (ns).
16. An optical transmitter comprising:
a direct modulation source;
a high-pass electrical filter coupled to the direct modulation source, the high-pass electrical filter having a time constant on the order of 1 nanosecond (ns); and
a distributed Bragg reflector (DBR) laser coupled to the high-pass electrical filter, the DBR laser comprising:
a gain section including:
an active region;
an upper separate confinement heterostructure (SCH) above the active region having a thickness of at least 60 nanometers (nm); and
a lower SCH below the active region having a thickness of at least 60 nm; and
a passive section coupled to the gain section, the passive section including a Bragg filter in optical communication with the active region.
17. The optical transmitter of claim 16 , wherein the high-pass electrical filter comprises a capacitor coupled in parallel with a first resistor, the parallel-coupled capacitor and first resistor being coupled in series with a second resistor.
18. The optical transmitter of claim 17 , wherein the capacitor has a capacitance of about 50 picofarads (pF), the first resistor has a resistance of about 15 Ohms (Ω), and the second resistor has a resistance of about 45Ω.
19. The optical transmitter of claim 16 , wherein:
the thickness of the upper SCH is about 125 nanometers (nm);
the thickness of the lower SCH is about 125 nm; and
a K factor of the DBR laser is 0.34 nanoseconds (ns).
20. A distributed feedback laser comprising:
a gain section, the gain section including:
an active region;
an upper separate confinement heterostructure (SCH) above the active region having a thickness of at least 60 nanometers (nm); and
a lower SCH below the active region having a thickness of at least 60 nm;
wherein the gain section is biased with a relatively high bias current density of at least 0.2 milli amps (mA) per micrometer (um).