CA2255450C - Optical modulator using isolator and optical transmitter including the same - Google Patents
Optical modulator using isolator and optical transmitter including the same Download PDFInfo
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- CA2255450C CA2255450C CA002255450A CA2255450A CA2255450C CA 2255450 C CA2255450 C CA 2255450C CA 002255450 A CA002255450 A CA 002255450A CA 2255450 A CA2255450 A CA 2255450A CA 2255450 C CA2255450 C CA 2255450C
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- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
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- G—PHYSICS
- G02—OPTICS
- G02F—OPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
- G02F1/00—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
- G02F1/01—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour
- G02F1/09—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour based on magneto-optical elements, e.g. exhibiting Faraday effect
- G02F1/093—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour based on magneto-optical elements, e.g. exhibiting Faraday effect used as non-reciprocal devices, e.g. optical isolators, circulators
Abstract
An optical modulator using an isolator, and an optical transmitter including the same are provided. The optical modulator modulates a carrier wave generated by an optical source according to a predetermined electrical signal, and includes an isolator including a Faraday rotator in which the rotation angle of polarization is different according to the intensity of an applied magnetic field, for controlling isolation of an optical signal according to the polarization rotation angle and outputting a modulated optical signal, a magnetic field generator for producing a magnetic field whose intensity is controlled by a predetermined electrical signal, and applying the produced magnetic field to the isolator, and a signal generator for supplying the electrical signal to the magnetic field generator and controlling the intensity of the electrical signal. The magnetic field generator is mounted on the optical isolator, the electric signal applied to the magnetic field generator isadjusted to control the intensity of the magnetic field formed in the isolator.
Accordingly, isolation of an optical signal is activated or deactivated, therebymodulating a continuous wave optical signal. Therefore, a small and cheap optical modulator having an excellent temperature property can be realized and easily housed in the transmitter.
Accordingly, isolation of an optical signal is activated or deactivated, therebymodulating a continuous wave optical signal. Therefore, a small and cheap optical modulator having an excellent temperature property can be realized and easily housed in the transmitter.
Description
CA 022~4~0 l998-l2-07 OPTICAL MODULATOR USING ISOLATOR AND
OPTICAL TRANSMITTER INCLUDING THE SAME
BACKGROUND OF THE INVENTION
1. Field of the Invention The present invention relates to an optical modulator using an isolator and an optical transmitter including the same, and more particularly, to an optical modulator for modulating a continuous wave optical beam by provoking optical attenuation by varying a magnetic field applied to an isolator, and an optical transmitter including the same.
OPTICAL TRANSMITTER INCLUDING THE SAME
BACKGROUND OF THE INVENTION
1. Field of the Invention The present invention relates to an optical modulator using an isolator and an optical transmitter including the same, and more particularly, to an optical modulator for modulating a continuous wave optical beam by provoking optical attenuation by varying a magnetic field applied to an isolator, and an optical transmitter including the same.
2. Description of the Related Art An optical modulator modulates a continuous wave optical beam into an optical signal which has the same form as an electrical signal. When several wavelength optical signals are simultaneously transmitted by a wavelength division multiplexing (WDM) system, their center wavelengths are jittered by the chirpingproperty of an optical signal spectrum which is generated by applying an electrical signal, thus degrading the transmission characteristics. In order to solve this problem, a laser diode is driven to output a continuous wave, and a beam output by the laser diode is modulated. Optical modulation is accomplished by an external modulator such as an electro-optic modulator or a lithumnaobate (LiNbO3) modulator.
FIG. 1 is a block diagram illustrating the configuration of a conventional optical modulator. Referring to FIG. 1, the optical modulator is comprised of a laser diode 100, first and second optical waveguides 102 and 104, an electrode plate 106 and an electric signal source 108.
The operations of the above elements will now be described. First, a continuous optical signal applied from the laser diode 100 is coupled into the two optical waveguides 102 and 104. When an electrical signal is applied from the electrical signal source 108 to the electrode plate 106, the refractive index of the first optical waveguide 102 is changed. The changed refractive index changes thepropagation constant of the first optical waveguide 102, and the changed CA 022~4~0 l998-l2-07 propagation constant changes the phase of an optical signal passing through the first optical waveguide. Accordingly, there is a phase difference between a phase-changed optical signal of the first optical waveguide 102 and a non-phase-changed optical signal of the second optical waveguide 104.
s The output optical signal of an optical modulator is modulated according to this phase difference. That is, when the two phases are the same, the output optical signal is intensified, but when the two phases have a difference of 180~, the output optical signal is canceled out. In this way, the output optical signal is turned on/off (modulated) at an output port. The extinction ratio in an off state is about 22dB.
However, in this optical modulator, insertion loss is high (generally, about 6dB), and a change in its characteristics due to polarization is severe. Also, this modulator requires a high reference voltage and an electrical modulation signal.This modulator also requires a heat release process since internal heat becomes high when such a high voltage is applied.
In a low-cost optical modulation technique for a subscriber network, a spectrum sliced source using amplified spontaneous emission of an optical amplifier is used as a continuous wave optical source, and a method of modulating an electrical signal into an optical signal using the aforementioned external modulator is adopted. In this case, more costs are required in order to include a subscriber network, due to the high cost of an expensive optical modulator.
SUMMARY OF THE INVENTION
To solve the above problem, it is an object of the present invention to provide an optical modulator using an isolator, by which an output optical signal is modulated by changing the polarization of a Faraday rotator by generating and applying a magnetic field to the isolator, and an optical transmitter including the same.
Accordingly, to achieve the above object, there is provided an optical modulator using an isolator, for modulating a carrier wave generated by an optical source according to a predetermined electrical signal, the optical modulator comprising: an isolator including a Faraday rotator in which the rotation angle of polarization is different according to the intensity of an applied magnetic field, for CA 022~4~0 l998-l2-07 controlling isolation of an optical signal according to the polarization rotation angle and outputting a modulated optical signal; a magnetic field generator for producing a magnetic field whose intensity is controlled by a predetermined electrical signal, and applying the produced magnetic field to the isolator; and a signal generator for 5 supplying the electrical signal to the magnetic field generator and controlling the intensity of the electrical signal.
To achieve the above object, there is provided an optical transmitter comprising: an optical source for generating a carrier wave; an isolator including a Faraday rotator in which the rotation angle of polarization is different according to 10 the intensity of an applied magnetic field, for controlling isolation of the carrier wave optical signal generated by the optical source according to the polarization rotation angle and outputting a modulated optical signal; a magnetic field generator for producing a magnetic field whose intensity is controlled by a predetermined electrical signal, and applying the produced magnetic field to the15 isolator; a signal generator for supplying the electrical signal to the magnetic field generator and controlling the intensity of the electrical signal; and an opticalamplifier for amplifying an optical signal modulated in the isolator and transmitting the amplified optical signal to a transmission channel.
BRIEF DESCRIPTION OF THE DRAWINGS
The above object and advantage of the present invention will become more apparent by describing in detail a preferred embodiment thereof with reference to the attached drawing(s) in which:
FIG. 1 is a block diagram illustrating the configuration of a conventional optical modulator;
FIG. 2 is a block diagram of an optical modulator using an isolator, according to the present invention;
FIG. 3 is a block diagram of the isolator of FIG. 2; and FIG. 4 is a block diagram illustrating a transmitter including an optical modulator using an isolator according to the present invention.
DESCRIPTION OF THE PREFERRED EMBODIMENT
, CA 022~4~0 l998-l2-07 Referring to FIG. 2, an optical modulator includes an isolator 200, a magnetic field generator 204, and a signal generator 202. The magnetic field generator 204 is preferably an electromagnet in which a magnetic field can be generated by an electrical signal.
The operation of the present invention will now be described based on the above-described configuration. First, an input continuous wave optical signal enters via an optical fiber input end (not shown), and is blocked by an isolator 200.
An electrical signal generated by a signal generator 202 activates/deactivates the electromagnetic field of the magnetic field generator 204 to enable/disable isolation of the isolator 200. The on/off of the isolation can be considered as the on/off of attenuation with respect to an input optical signal. That is, when an electric signal generated by the signal generator 202 is applied to the magneticfield generator 204, a magnetic field is formed, for example, when the magnetic field generator 204 is an electromagnet and when the electric signal is "1" (high).
Then, the input continuous wave optical signal incident upon the isolator 200 passes through the isolator 200 and is output to an output end. When the electric signal is "0" (low), a magnetic field is not formed in the isolator 200. Thus, the input continuous wave optical signal does not pass through the isolator 200 and cannot be output to an output end. The continuous wave optical signal is turned on or off depending on the on/off state of the electric signal, thereby achieving optical modulation. In the optical modulator operating as described above, the extinction ratio can range between 0.5dB and 50dB.
FIG. 3 is a block diagram of the isolator of FIG. 2. The isolator allows light to be transmitted from an input projection port to an output port with low loss, and prevents reverse traveling and recombination of light with high loss, to thus stably maintain the operation of the system. For example, while light emitted by a laser diode travels in a light transmission direction, a reflected light is generated in a connecter where optical fibers are spliced to each other, or where a reflective noise is generated due to light traveling backward when connected to various other devices. The isolator prevents the above problems, and is necessary particularly in optical communications of no less than 1Gbps speed and a high sensitivity sensor where problems are generated by a reflected light.
CA 022~4~0 l998-l2-07 The isolator of FIG. 3 includes a first collimator 300, a first double refraction element 302, a Faraday rotator 304, a second double refraction element 306, and a second collimator 308. Rutile or calcite is suitable as the materials of the first and second double refraction elements. The first double refraction element 302 5 operates as a polarizer, and the second double refraction element 306 operates as an analyzer. The principle is that only polarized light of one direction passes and polarized light vertical to the above polarized light does not pass. The essential parameter between the polarizer and the analyzer is the extinction ratio of the passing polarized light to the polarized light that is vertical to the passing polarized 10 light.
The Faraday rotator 304 rotates the polarization plane of incident light by 45~. The light rotated 45~ is reflected in a reverse direction by the rear end of the Faraday rotator 304 and reenters it, and then is rotated 45~ again. Thus, the light is rotated at a total of 90~. Accordingly, the reflected wave rotated 90~ is blocked 15 by the polarizer. The Faraday rotator generates a Faraday rotation by a Faraday effect when a magnetic field is applied to the magneto-optic material in a traveling direction. The Faraday effect is that the polarization plane of light rotates while the light passes through a magneto-optic material.
The performance of the isolator is determined by forward insertion loss and 20 backward isolation. The isolator usually has insertion loss of about 1dB and isolation of about 30dB due to reflection at an element junction, and a defective polarizer and a defective rotator.
The operation of the isolator of FIG. 3 will now be described. The first collimator 300 collects and collimates light emitted by a first optical fiber or a laser 25 diode (not showri). The collimated light is divided into two beams whose polarized directions are perpendicular to each other by the first double refraction element 302, and the two beams pass through different paths, and are incident upon the Faraday rotator 304. The light entering the Faraday rotator 304 is rotated 45~ in existing polarized light directions while polarized directions are kept perpendicular 30 to each other. While the polarization direction-changed beams again pass through the second double refraction element 306, the two beams are united into one.
Then, the two beams are collimated by the second collimator 308, and the collimated beam enters a second optical fiber (not shown). Here, the Faraday CA 022~4~0 l998-l2-07 rotator 304 allows the isolator to maintain a constant magnetic field so that polarization can be changed by 45~. However, if a magnetic field is generated inthe vicinity of the isolator, the magnetic field of a magnet comprising the Faraday rotator is affected. Also, the Faraday rotator changes the rotation angle of 5 polarization according to the intensity of the magnetic field as represented by the following Equation 1:
~ =VBI . (1 ) wherein 0 is a rotation angle, V is a constant, B is the intensity of a magnetic field, and I is an interaction length.
When polarization is changed by an external magnetic field as represented in Equation 1, the paths of light beams polarized perpendicular to each other bythe second double refraction element 306 are changed, which consequently changes the amount of light incident upon the second optical fiber via the second collimator 308. That is, the intensity of the magnetic field varies with the intensity 15 of an external electric signal (current), and the loss characteristics of the isolator differs depending on the variation of the magnetic field intensity.
FIG. 4 is a block diagram of an optical transmitter including an optical modulator using an isolator according to the present invention. The optical transmitter of FIG. 4 includes an optical source 400, an optical modulator 402 20 using an isolator, and an amplifier 404.
The operations of the above-mentioned elements will now be described.
First, when a carrier wave for information transmission is generated by the optical source 400 such as a laser diode or a light emitting diode, the carrier wave emitted by the optical source 400 is switched on or off at an appropriate time by 25 the optical modulator 402 using the isolator. A modulated and produced optical signal is amplified by the amplifier 404, and transmitted to the next port via atransmission channel.
As to the transmission of a wavelength division multiplexed (WDM) optical signal, carrier wave beams from various optical sources are modulated and 30 multiplexed, and then transmitted. In an optical subscriber network, light carrying information and carrier wave light are transmitted from an optical transmission system to a subscriber port. At the subscriber port, the light carrying information is applied to a detector and converted into an electrical signal, and the carrier .
CA 022~4~0 1998-12-07 wave light carries information on a subscriber via the optical modulator using the isolator and is transmitted back to the optical transmission system.
According to the present invention, a magnetic field generator is mounted on an optical isolator, an electric signal applied to the magnetic field generator is 5 adjusted to control the intensity of a magnetic field formed in the isolator.
Accordingly, isolation of an optical signal is activated or deactivated, therebymodulating a continuous wave optical signal. Therefore, a small and cheap optical modulator having an excellent temperature property can be realized and easily mounted on a transmitter. Also, the optical modulator is fixed to a laser diode and 10 can perform optical modulation by changing only the intensity of an electrical signal. Hence, it is not sensitive to external factors such as dust, temperature, and humid, and there is little phase difference with respect to polarization.
, . . . ~
FIG. 1 is a block diagram illustrating the configuration of a conventional optical modulator. Referring to FIG. 1, the optical modulator is comprised of a laser diode 100, first and second optical waveguides 102 and 104, an electrode plate 106 and an electric signal source 108.
The operations of the above elements will now be described. First, a continuous optical signal applied from the laser diode 100 is coupled into the two optical waveguides 102 and 104. When an electrical signal is applied from the electrical signal source 108 to the electrode plate 106, the refractive index of the first optical waveguide 102 is changed. The changed refractive index changes thepropagation constant of the first optical waveguide 102, and the changed CA 022~4~0 l998-l2-07 propagation constant changes the phase of an optical signal passing through the first optical waveguide. Accordingly, there is a phase difference between a phase-changed optical signal of the first optical waveguide 102 and a non-phase-changed optical signal of the second optical waveguide 104.
s The output optical signal of an optical modulator is modulated according to this phase difference. That is, when the two phases are the same, the output optical signal is intensified, but when the two phases have a difference of 180~, the output optical signal is canceled out. In this way, the output optical signal is turned on/off (modulated) at an output port. The extinction ratio in an off state is about 22dB.
However, in this optical modulator, insertion loss is high (generally, about 6dB), and a change in its characteristics due to polarization is severe. Also, this modulator requires a high reference voltage and an electrical modulation signal.This modulator also requires a heat release process since internal heat becomes high when such a high voltage is applied.
In a low-cost optical modulation technique for a subscriber network, a spectrum sliced source using amplified spontaneous emission of an optical amplifier is used as a continuous wave optical source, and a method of modulating an electrical signal into an optical signal using the aforementioned external modulator is adopted. In this case, more costs are required in order to include a subscriber network, due to the high cost of an expensive optical modulator.
SUMMARY OF THE INVENTION
To solve the above problem, it is an object of the present invention to provide an optical modulator using an isolator, by which an output optical signal is modulated by changing the polarization of a Faraday rotator by generating and applying a magnetic field to the isolator, and an optical transmitter including the same.
Accordingly, to achieve the above object, there is provided an optical modulator using an isolator, for modulating a carrier wave generated by an optical source according to a predetermined electrical signal, the optical modulator comprising: an isolator including a Faraday rotator in which the rotation angle of polarization is different according to the intensity of an applied magnetic field, for CA 022~4~0 l998-l2-07 controlling isolation of an optical signal according to the polarization rotation angle and outputting a modulated optical signal; a magnetic field generator for producing a magnetic field whose intensity is controlled by a predetermined electrical signal, and applying the produced magnetic field to the isolator; and a signal generator for 5 supplying the electrical signal to the magnetic field generator and controlling the intensity of the electrical signal.
To achieve the above object, there is provided an optical transmitter comprising: an optical source for generating a carrier wave; an isolator including a Faraday rotator in which the rotation angle of polarization is different according to 10 the intensity of an applied magnetic field, for controlling isolation of the carrier wave optical signal generated by the optical source according to the polarization rotation angle and outputting a modulated optical signal; a magnetic field generator for producing a magnetic field whose intensity is controlled by a predetermined electrical signal, and applying the produced magnetic field to the15 isolator; a signal generator for supplying the electrical signal to the magnetic field generator and controlling the intensity of the electrical signal; and an opticalamplifier for amplifying an optical signal modulated in the isolator and transmitting the amplified optical signal to a transmission channel.
BRIEF DESCRIPTION OF THE DRAWINGS
The above object and advantage of the present invention will become more apparent by describing in detail a preferred embodiment thereof with reference to the attached drawing(s) in which:
FIG. 1 is a block diagram illustrating the configuration of a conventional optical modulator;
FIG. 2 is a block diagram of an optical modulator using an isolator, according to the present invention;
FIG. 3 is a block diagram of the isolator of FIG. 2; and FIG. 4 is a block diagram illustrating a transmitter including an optical modulator using an isolator according to the present invention.
DESCRIPTION OF THE PREFERRED EMBODIMENT
, CA 022~4~0 l998-l2-07 Referring to FIG. 2, an optical modulator includes an isolator 200, a magnetic field generator 204, and a signal generator 202. The magnetic field generator 204 is preferably an electromagnet in which a magnetic field can be generated by an electrical signal.
The operation of the present invention will now be described based on the above-described configuration. First, an input continuous wave optical signal enters via an optical fiber input end (not shown), and is blocked by an isolator 200.
An electrical signal generated by a signal generator 202 activates/deactivates the electromagnetic field of the magnetic field generator 204 to enable/disable isolation of the isolator 200. The on/off of the isolation can be considered as the on/off of attenuation with respect to an input optical signal. That is, when an electric signal generated by the signal generator 202 is applied to the magneticfield generator 204, a magnetic field is formed, for example, when the magnetic field generator 204 is an electromagnet and when the electric signal is "1" (high).
Then, the input continuous wave optical signal incident upon the isolator 200 passes through the isolator 200 and is output to an output end. When the electric signal is "0" (low), a magnetic field is not formed in the isolator 200. Thus, the input continuous wave optical signal does not pass through the isolator 200 and cannot be output to an output end. The continuous wave optical signal is turned on or off depending on the on/off state of the electric signal, thereby achieving optical modulation. In the optical modulator operating as described above, the extinction ratio can range between 0.5dB and 50dB.
FIG. 3 is a block diagram of the isolator of FIG. 2. The isolator allows light to be transmitted from an input projection port to an output port with low loss, and prevents reverse traveling and recombination of light with high loss, to thus stably maintain the operation of the system. For example, while light emitted by a laser diode travels in a light transmission direction, a reflected light is generated in a connecter where optical fibers are spliced to each other, or where a reflective noise is generated due to light traveling backward when connected to various other devices. The isolator prevents the above problems, and is necessary particularly in optical communications of no less than 1Gbps speed and a high sensitivity sensor where problems are generated by a reflected light.
CA 022~4~0 l998-l2-07 The isolator of FIG. 3 includes a first collimator 300, a first double refraction element 302, a Faraday rotator 304, a second double refraction element 306, and a second collimator 308. Rutile or calcite is suitable as the materials of the first and second double refraction elements. The first double refraction element 302 5 operates as a polarizer, and the second double refraction element 306 operates as an analyzer. The principle is that only polarized light of one direction passes and polarized light vertical to the above polarized light does not pass. The essential parameter between the polarizer and the analyzer is the extinction ratio of the passing polarized light to the polarized light that is vertical to the passing polarized 10 light.
The Faraday rotator 304 rotates the polarization plane of incident light by 45~. The light rotated 45~ is reflected in a reverse direction by the rear end of the Faraday rotator 304 and reenters it, and then is rotated 45~ again. Thus, the light is rotated at a total of 90~. Accordingly, the reflected wave rotated 90~ is blocked 15 by the polarizer. The Faraday rotator generates a Faraday rotation by a Faraday effect when a magnetic field is applied to the magneto-optic material in a traveling direction. The Faraday effect is that the polarization plane of light rotates while the light passes through a magneto-optic material.
The performance of the isolator is determined by forward insertion loss and 20 backward isolation. The isolator usually has insertion loss of about 1dB and isolation of about 30dB due to reflection at an element junction, and a defective polarizer and a defective rotator.
The operation of the isolator of FIG. 3 will now be described. The first collimator 300 collects and collimates light emitted by a first optical fiber or a laser 25 diode (not showri). The collimated light is divided into two beams whose polarized directions are perpendicular to each other by the first double refraction element 302, and the two beams pass through different paths, and are incident upon the Faraday rotator 304. The light entering the Faraday rotator 304 is rotated 45~ in existing polarized light directions while polarized directions are kept perpendicular 30 to each other. While the polarization direction-changed beams again pass through the second double refraction element 306, the two beams are united into one.
Then, the two beams are collimated by the second collimator 308, and the collimated beam enters a second optical fiber (not shown). Here, the Faraday CA 022~4~0 l998-l2-07 rotator 304 allows the isolator to maintain a constant magnetic field so that polarization can be changed by 45~. However, if a magnetic field is generated inthe vicinity of the isolator, the magnetic field of a magnet comprising the Faraday rotator is affected. Also, the Faraday rotator changes the rotation angle of 5 polarization according to the intensity of the magnetic field as represented by the following Equation 1:
~ =VBI . (1 ) wherein 0 is a rotation angle, V is a constant, B is the intensity of a magnetic field, and I is an interaction length.
When polarization is changed by an external magnetic field as represented in Equation 1, the paths of light beams polarized perpendicular to each other bythe second double refraction element 306 are changed, which consequently changes the amount of light incident upon the second optical fiber via the second collimator 308. That is, the intensity of the magnetic field varies with the intensity 15 of an external electric signal (current), and the loss characteristics of the isolator differs depending on the variation of the magnetic field intensity.
FIG. 4 is a block diagram of an optical transmitter including an optical modulator using an isolator according to the present invention. The optical transmitter of FIG. 4 includes an optical source 400, an optical modulator 402 20 using an isolator, and an amplifier 404.
The operations of the above-mentioned elements will now be described.
First, when a carrier wave for information transmission is generated by the optical source 400 such as a laser diode or a light emitting diode, the carrier wave emitted by the optical source 400 is switched on or off at an appropriate time by 25 the optical modulator 402 using the isolator. A modulated and produced optical signal is amplified by the amplifier 404, and transmitted to the next port via atransmission channel.
As to the transmission of a wavelength division multiplexed (WDM) optical signal, carrier wave beams from various optical sources are modulated and 30 multiplexed, and then transmitted. In an optical subscriber network, light carrying information and carrier wave light are transmitted from an optical transmission system to a subscriber port. At the subscriber port, the light carrying information is applied to a detector and converted into an electrical signal, and the carrier .
CA 022~4~0 1998-12-07 wave light carries information on a subscriber via the optical modulator using the isolator and is transmitted back to the optical transmission system.
According to the present invention, a magnetic field generator is mounted on an optical isolator, an electric signal applied to the magnetic field generator is 5 adjusted to control the intensity of a magnetic field formed in the isolator.
Accordingly, isolation of an optical signal is activated or deactivated, therebymodulating a continuous wave optical signal. Therefore, a small and cheap optical modulator having an excellent temperature property can be realized and easily mounted on a transmitter. Also, the optical modulator is fixed to a laser diode and 10 can perform optical modulation by changing only the intensity of an electrical signal. Hence, it is not sensitive to external factors such as dust, temperature, and humid, and there is little phase difference with respect to polarization.
, . . . ~
Claims (4)
1. An optical modulator for modulating a carrier wave generated by an optical source according to a predetermined electrical signal, said optical modulator comprising:
an isolator including a Faraday rotator in which a rotation angle of polarization is different according to an intensity of an applied magnetic field, said isolator controlling isolation of an optical signal according to the rotation angle of polarization and outputting a modulated optical signal;
a magnetic field generator for producing a magnetic field having an intensity which is controlled by a predetermined electrical signal, and for applying the produced magnetic field to the isolator; and a signal generator for supplying the electrical signal to the magnetic field generator and for controlling an intensity of the electrical signal;
wherein said isolator includes double refracting means for splitting said optical signal into two optical signal outputs having different polarization, said two optical signal outputs being provided as an input to said Faraday rotator; and wherein said isolator further includes additional double refracting means connected to outputs of said Faraday rotator for forming a single optical output from said outputs of said Faraday rotator, and collimator means for receiving said single optical output and providing said modulated optical signal.
an isolator including a Faraday rotator in which a rotation angle of polarization is different according to an intensity of an applied magnetic field, said isolator controlling isolation of an optical signal according to the rotation angle of polarization and outputting a modulated optical signal;
a magnetic field generator for producing a magnetic field having an intensity which is controlled by a predetermined electrical signal, and for applying the produced magnetic field to the isolator; and a signal generator for supplying the electrical signal to the magnetic field generator and for controlling an intensity of the electrical signal;
wherein said isolator includes double refracting means for splitting said optical signal into two optical signal outputs having different polarization, said two optical signal outputs being provided as an input to said Faraday rotator; and wherein said isolator further includes additional double refracting means connected to outputs of said Faraday rotator for forming a single optical output from said outputs of said Faraday rotator, and collimator means for receiving said single optical output and providing said modulated optical signal.
2. The optical modulator of claim 1, wherein the magnetic field generator comprises an electromagnet.
3. The optical modulator of claim 2, wherein said isolator isolates the optical signal according to a level of the electrical signal, said level being one of high and low.
4. An optical transmitter, comprising:
an optical source for generating a carrier wave optical signal;
an isolator including a Faraday rotator in which a rotation angle of polarization is different according to an intensity of an applied magnetic field, said isolator controlling isolation of an optical signal according to the rotation angle of polarization and outputting a modulated optical signal;
a magnetic field generator for producing a magnetic field having an intensity which is controlled by a predetermined electrical signal, and for applying the produced magnetic field to the isolator; and a signal generator for supplying the electrical signal to the magnetic field generator and for controlling an intensity of the electrical signal;
wherein said isolator includes double refracting for splitting said optical signal into two optical signal outputs having different polarization, and two optical signal outputs being provided as an input to said Faraday rotator; and wherein said isolator further includes additional double refracting means connected to outputs of said Faraday rotator for forming a single optical output from said outputs of said Faraday rotator, and collimator means for receiving said single optical output and providing said modulated optical signal.
an optical source for generating a carrier wave optical signal;
an isolator including a Faraday rotator in which a rotation angle of polarization is different according to an intensity of an applied magnetic field, said isolator controlling isolation of an optical signal according to the rotation angle of polarization and outputting a modulated optical signal;
a magnetic field generator for producing a magnetic field having an intensity which is controlled by a predetermined electrical signal, and for applying the produced magnetic field to the isolator; and a signal generator for supplying the electrical signal to the magnetic field generator and for controlling an intensity of the electrical signal;
wherein said isolator includes double refracting for splitting said optical signal into two optical signal outputs having different polarization, and two optical signal outputs being provided as an input to said Faraday rotator; and wherein said isolator further includes additional double refracting means connected to outputs of said Faraday rotator for forming a single optical output from said outputs of said Faraday rotator, and collimator means for receiving said single optical output and providing said modulated optical signal.
Applications Claiming Priority (2)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| KR97-66750 | 1997-12-08 | ||
| KR1019970066750A KR100288443B1 (en) | 1997-12-08 | 1997-12-08 | Optical modulator using isolator and optical transmitter comprising it |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| CA2255450A1 CA2255450A1 (en) | 1999-06-08 |
| CA2255450C true CA2255450C (en) | 2002-07-02 |
Family
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Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| CA002255450A Expired - Fee Related CA2255450C (en) | 1997-12-08 | 1998-12-07 | Optical modulator using isolator and optical transmitter including the same |
Country Status (9)
| Country | Link |
|---|---|
| US (1) | US6141140A (en) |
| JP (1) | JPH11237594A (en) |
| KR (1) | KR100288443B1 (en) |
| CN (1) | CN1113264C (en) |
| BR (1) | BR9805235A (en) |
| CA (1) | CA2255450C (en) |
| DE (1) | DE19856586A1 (en) |
| FR (1) | FR2772150A1 (en) |
| GB (1) | GB2332066A (en) |
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| Publication number | Priority date | Publication date | Assignee | Title |
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| KR100274810B1 (en) * | 1997-12-09 | 2000-12-15 | 윤종용 | Optical attenuator using isolator and optical communication system comprising it |
| US6233082B1 (en) * | 1999-10-12 | 2001-05-15 | Lucent Technologies Inc. | Optical transmitter for WDM systems |
| US6490070B1 (en) * | 2000-07-28 | 2002-12-03 | Terabeam Corporation | Method and apparatus for polarization tracking in wireless optical communication systems |
| US6912080B2 (en) * | 2002-03-26 | 2005-06-28 | Matsushita Electric Industrial Co., Ltd. | Magneto-optic modulator and optical communication system using the same |
| US6927909B2 (en) * | 2002-05-09 | 2005-08-09 | Matsushita Electric Industrial Co., Ltd. | Integrated magneto-optical modulator with optical isolator, method of manufacturing the same and optical communication system using the same |
| US7361171B2 (en) | 2003-05-20 | 2008-04-22 | Raydiance, Inc. | Man-portable optical ablation system |
| US9022037B2 (en) | 2003-08-11 | 2015-05-05 | Raydiance, Inc. | Laser ablation method and apparatus having a feedback loop and control unit |
| US8921733B2 (en) | 2003-08-11 | 2014-12-30 | Raydiance, Inc. | Methods and systems for trimming circuits |
| US8173929B1 (en) | 2003-08-11 | 2012-05-08 | Raydiance, Inc. | Methods and systems for trimming circuits |
| US8135050B1 (en) | 2005-07-19 | 2012-03-13 | Raydiance, Inc. | Automated polarization correction |
| US7308171B2 (en) * | 2005-11-16 | 2007-12-11 | Raydiance, Inc. | Method and apparatus for optical isolation in high power fiber-optic systems |
| US8189971B1 (en) | 2006-01-23 | 2012-05-29 | Raydiance, Inc. | Dispersion compensation in a chirped pulse amplification system |
| US7444049B1 (en) | 2006-01-23 | 2008-10-28 | Raydiance, Inc. | Pulse stretcher and compressor including a multi-pass Bragg grating |
| US8232687B2 (en) | 2006-04-26 | 2012-07-31 | Raydiance, Inc. | Intelligent laser interlock system |
| US7822347B1 (en) | 2006-03-28 | 2010-10-26 | Raydiance, Inc. | Active tuning of temporal dispersion in an ultrashort pulse laser system |
| US8125704B2 (en) | 2008-08-18 | 2012-02-28 | Raydiance, Inc. | Systems and methods for controlling a pulsed laser by combining laser signals |
| US8554037B2 (en) | 2010-09-30 | 2013-10-08 | Raydiance, Inc. | Hybrid waveguide device in powerful laser systems |
| JP6131954B2 (en) * | 2012-07-26 | 2017-05-24 | 富士通オプティカルコンポーネンツ株式会社 | Optical modulator and optical transmitter |
| US10466515B2 (en) | 2016-03-15 | 2019-11-05 | Intel Corporation | On-chip optical isolator |
| US20180059446A1 (en) * | 2016-08-29 | 2018-03-01 | Woosung Kim | Optical iso-modulator |
| CN108169857A (en) * | 2017-12-27 | 2018-06-15 | 中国科学院半导体研究所 | A kind of bidirectional optical amplifier transmitted applied to extra long distance split-second precision |
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| Publication number | Priority date | Publication date | Assignee | Title |
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| GB1060778A (en) * | 1963-04-23 | 1967-03-08 | Western Electric Co | Optical rotation medium |
| US3811096A (en) * | 1972-09-21 | 1974-05-14 | Bell Telephone Labor Inc | Magneto-optic modulators |
| GB1442366A (en) * | 1972-12-27 | 1976-07-14 | Owens Illinois Inc | Glass articles |
| US4027948A (en) * | 1976-03-15 | 1977-06-07 | The United States Of America As Represented By The Secretary Of The Army | Low loss laser modulator |
| US4239329A (en) * | 1978-08-04 | 1980-12-16 | Nippon Telegraph And Telephone Public Corporation | Optical nonreciprocal device |
| JPS57100410A (en) * | 1980-12-15 | 1982-06-22 | Fujitsu Ltd | Optical isolator |
| JPS5849916A (en) * | 1981-09-19 | 1983-03-24 | Fujitsu Ltd | Optical switch |
| JPH03144417A (en) * | 1989-10-30 | 1991-06-19 | Nec Corp | Light modulation circuit |
| US5402509A (en) * | 1991-09-12 | 1995-03-28 | Fujitsu Limited | Optical fiber coupling device including lenses and magnetooptics |
| JP2775547B2 (en) * | 1992-02-17 | 1998-07-16 | 秩父小野田株式会社 | Optical isolator |
| IT1256222B (en) * | 1992-12-23 | 1995-11-29 | Pirelli Cavi Spa | OPTICAL GENERATOR OF HIGH POWER SIGNALS FOR TELECOMMUNICATION SYSTEMS |
| US5657151A (en) * | 1993-12-09 | 1997-08-12 | Lucent Technologies Inc. | Polarization scrambler/modulator |
| JPH07209603A (en) * | 1994-01-21 | 1995-08-11 | Fujitsu Ltd | Optical isolator |
| JPH08171075A (en) * | 1994-12-19 | 1996-07-02 | Fuji Elelctrochem Co Ltd | Optical switch |
| JP3730299B2 (en) * | 1996-02-07 | 2005-12-21 | 富士通株式会社 | Optical equalization amplifier and optical equalization amplification method |
| GB2313675B (en) * | 1996-05-27 | 1999-01-13 | Samsung Electronics Co Ltd | Optical isolator |
-
1997
- 1997-12-08 KR KR1019970066750A patent/KR100288443B1/en not_active IP Right Cessation
-
1998
- 1998-12-07 JP JP10347057A patent/JPH11237594A/en active Pending
- 1998-12-07 CA CA002255450A patent/CA2255450C/en not_active Expired - Fee Related
- 1998-12-07 FR FR9815411A patent/FR2772150A1/en active Pending
- 1998-12-07 CN CN98123166A patent/CN1113264C/en not_active Expired - Fee Related
- 1998-12-08 DE DE19856586A patent/DE19856586A1/en not_active Withdrawn
- 1998-12-08 BR BR9805235-7A patent/BR9805235A/en not_active IP Right Cessation
- 1998-12-08 US US09/207,580 patent/US6141140A/en not_active Expired - Fee Related
- 1998-12-08 GB GB9826846A patent/GB2332066A/en not_active Withdrawn
Also Published As
| Publication number | Publication date |
|---|---|
| CN1113264C (en) | 2003-07-02 |
| CN1221118A (en) | 1999-06-30 |
| GB2332066A (en) | 1999-06-09 |
| KR19990048135A (en) | 1999-07-05 |
| US6141140A (en) | 2000-10-31 |
| GB9826846D0 (en) | 1999-01-27 |
| CA2255450A1 (en) | 1999-06-08 |
| JPH11237594A (en) | 1999-08-31 |
| BR9805235A (en) | 1999-11-23 |
| DE19856586A1 (en) | 1999-07-01 |
| KR100288443B1 (en) | 2001-05-02 |
| FR2772150A1 (en) | 1999-06-04 |
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