Thermal compensation for burst-mode laser wavelength drift

Patent metadata

Field	Value
Publication number	US-9537287-B2
Application number	US-201514969610-A
Country	US
Kind code	B2
Filing date	Dec 15, 2015
Priority date	Oct 8, 2014
Publication date	Jan 3, 2017
Grant date	Jan 3, 2017

Abstract

An apparatus comprising a burst-mode laser comprising an active layer and configured to emit an optical signal during a burst period, wherein a temperature change of the burst-mode laser causes the optical signal to shift in wavelength, and a heater thermally coupled to the active layer and configured to reduce a wavelength shift of the optical signal during the burst period by applying heat to the active layer based on timing of the burst period.

First claim

What is claimed is:

1. An apparatus comprising;
a burst-mode laser comprising an active layer and configured to emit an optical signal during a burst period, wherein a temperature change of the burst-mode laser causes a wavelength shift of the optical signal; and
a heater thermally coupled to the active layer and configured to:
receive an electric current for generating heat, wherein the electric current is at a first level during a first period before a start of the burst period and at a second level during a second period after the start, and wherein the first level is greater than the second level; and
apply the heat to the active layer before the start and based on timing of the burst period in order to substantially stabilize a temperature of the burst-mode laser during the burst period and to reduce the wavelength shift during the burst period.

2. The apparatus of claim 1 , wherein the electric current is dedicated to the heater.

3. The apparatus of claim 1 , wherein a duration of the burst period is about 125 microseconds (μs), wherein the temperature varies no more than about 0.2 degrees Celsius (° C.) during the burst period, and wherein the wavelength shift is no more than about 0.02 nanometers (nm) during the burst period.

4. The apparatus of claim 1 , further comprising a driving circuit coupled to the heater and comprising a constant current source configured to generate the electric current.

5. The apparatus of claim 4 , wherein the constant current source comprises:
a transistor comprising a base; and
a diode coupled to the base,
wherein the transistor and the diode have similar voltage-temperature characteristics such that the transistor and the diode are configured to create a constant voltage difference that is substantially independent of an ambient temperature of the driving circuit.

6. The apparatus of claim 1 , wherein the burst-mode laser is a distributed feedback (DFB) laser, wherein the heater comprises a silicon dioxide (SiO 2 ) layer, and wherein a thickness of the SiO 2 layer allows heat transfer from the heater to the active layer, but blocks current injection from the heater to the active layer.

7. An apparatus comprising:
a burst-mode laser comprising an active layer and configured to emit an optical signal during a burst period, wherein a temperature change of the burst-mode laser causes a wavelength shift of the optical signal; and
a heater thermally coupled to the active layer and configured to:
receive an electric current for generating heat, wherein the electric current reaches at least two levels during the burst period, reaches a first level no later than a start of the burst period, and then decreases from the first level; and
apply the heat to the active layer at the start and based on timing of the burst period in order to reduce the wavelength shift during the burst period.

8. The apparatus of claim 7 , wherein the electric current:
reaches the first level from zero in no more than about 2 nanoseconds (ns);
stays at the first level for no more than about 1 microsecond (μs);
decreases to a second level;
stays at the second level for no more than about 10 μs; and
decreases to zero for a remainder of the burst period.

9. The apparatus of claim 7 , wherein the electric current continuously decreases from the first level to zero by following an exponential curve.

10. A method for temperature compensation during operation of a burst-mode laser that is thermally coupled to a heater, the method comprising:
receiving a burst enable signal indicating a start of a burst period;
emitting an optical signal with at least one wavelength during the burst period;
supplying an electric current to the heater, wherein the electric current reaches a first level no later than the start and then decreases from the first level thereafter;
applying, using the heater, a heat to the burst-mode laser based on the burst enable signal; and
substantially maintaining, based on the applying, a temperature of the burst-mode laser throughout an emission of the optical signal in order to reduce a wavelength shift of the optical signal.

11. The method of claim 10 , further comprising:
applying, using the heater, the heat to the burst-mode laser prior to the start; and
terminating application of the heater to the burst-mode laser at least during a latter portion of the burst period.

12. The method of claim 11 , wherein the electric current:
reaches the first level at least about 4 microseconds (μs) before the start; and
decreases to a second level for a first portion of the burst period and until the terminating.

13. The method of claim 11 , wherein a duration of the burst period is about 125 microseconds (μs), wherein the temperature of the burst-mode laser varies no more than about 0.2 degrees Celsius (° C.) during the burst period, and wherein the wavelength shift is no more than about 0.02 nanometers (nm) during the burst period.

14. The method of claim 10 , further comprising simultaneously receiving the electric current and the burst enable signal at the start.

15. The method of claim 10 , wherein the electric current:
reaches the first level from zero in no more than about 2 nanoseconds (ns);
stays at the first level for no more than about 1 microsecond (μs);
decreases to a second level;
stays at the second level for no more than about 10μs; and
decreases to zero for a remainder of the burst period.

16. The method of claim 10 , further comprising supplying the electric current to the heater using a driving circuit, wherein the driving circuit comprises a constant current source, wherein the constant current source comprises a transistor and a diode coupled to the transistor, and wherein the transistor and the diode have similar voltage-temperature characteristics.

17. The method of claim 16 , further comprising creating, using the transistor and the diode, a constant voltage difference that is substantially independent of an ambient temperature of the driving circuit.

18. A laser system comprising:
a burst-mode laser comprising a metallic layer configured to serve as an electrode pad for the burst-mode laser; and
an electric heater situated atop the burst-mode laser and comprising:
a first titanium (Ti) layer atop the metallic layer;
a silicon dioxide (SiO 2 ) layer atop the first Ti layer, comprising a first thickness no more than 300 nanometers (nm), and configured to allow efficient heat transfer from the electric heater to the burst-mode laser;
a second Ti layer atop the SiO 2 layer; and
a platinum (Pt) layer atop the second Ti layer,
wherein the second Ti layer and the Pt layer are configured to serve as a heating pad for the electric heater, and
wherein the SiO 2 layer is further configured to block current injection from the heating pad to the electrode pad.

19. The laser system of claim 18 , wherein the first thickness is no less than about 100 nm, wherein the first Ti layer comprises a second thickness of about 4 nm to about 10 nm, and wherein the second Ti layer has a third thickness of about 280 nm to about 320 nm.

20. The laser system of claim 18 , wherein the burst-mode laser further comprises:
an active layer configured to generate an optical wave when a burst enable voltage is applied on the electrode pad;
a cladding layer atop the active layer and comprising p-type indium phosphide (p-InP); and
an ohmic contact layer atop the cladding layer, underneath the metallic layer, and comprising heavily-doped p-type indium gallium ars

Assignees

• Futurewei Technologies Inc

Inventors

• Yan Xuejin
• Gong Jianmin
• Lei Hongbing
• Gao Jianhe

Classifications

• H01S5/02453

  Heating, e.g. the laser is heated for stabilisation against temperature fluctuations of the environment (H01S5/0612 takes precedence, for monolithically integrated heaters see also H01S5/0261) · CPC title

• H01S5/0612 Primary

  controlled by temperature · CPC title

• H01S2301/176

  Specific passivation layers on surfaces other than the emission facet · CPC title

• H01S5/12

  the resonator having a periodic structure, e.g. in distributed feedback [DFB] lasers (comprising a photonic bandgap structure H01S5/11; surface-emitting lasers H01S5/18) · CPC title

• H01S5/06216

  Pulse modulation or generation · CPC title