Patent Publication Number: US-2023152661-A1

Title: High frequency optical modulator with laterally displaced conduction plane relative to modulating electrodes

Description:
CROSS REFERENCE TO RELATED APPLICATIONS 
     This application is a continuation of U.S. patent application Ser. No. 16/934,884 (now U.S. 2020/0348577), to Chen et al., filed Jul. 21, 2020, entitled “High Frequency Optical Modulator With Laterally Displaced Conduction Plane Relative to Modulating Electrodes,” which is a divisional of U.S. patent application Ser. No. 15/462,099, (now U.S. 2018/0252982) to Chen et al., filed on Mar. 17, 2017, entitled “High Frequency Optical Modulator With Laterally Displaced Conduction Plane Relative to Modulating Electrodes,” which claims priority to copending U.S. provisional patent application 62/466,694 to Chen et al. filed on Mar. 3, 3017, entitled “High Frequency Optical Modulator With Laterally Displaced Conduction Plane Relative to Modulated Electrodes,” incorporated herein by reference. 
    
    
     FIELD OF THE INVENTION 
     The invention relates to optical modulators that can be useful in optical communications for various information transfer. The optical modulators can be useful for high bandwidth RF modulation delivered with an RF transmission line coupled with a semiconductor optical waveguide. 
     BACKGROUND OF THE INVENTION 
     Optical modulators incorporating Mach-Zehnder interferometer structures can be used to impose RF modulation on an optical signal, such as light from a laser source. The RF modulation can encode information within the optical signal for transport to remote locations through an optical communications network. The encoded information can include, for example, data signals, voice signals, video signals and/or other communication information. 
     The Mach-Zehnder interferometer structure splits the optical signal into two arms that interfere when recombined. The RF signal is superimposed onto the optical signal using the RF transmission line through alteration of the index of refraction of the optical waveguide by an electromagnetic RF signal. High fidelity transfer of the RF signal into modulation of the optical signal becomes more challenging as the frequency of the RF signal increases to accommodate higher bandwidth in the optical signal. 
     SUMMARY OF THE INVENTION 
     In a first aspect, the invention pertains to an optical modulator comprising a submount, electrical conduction pathways designed to carry RF signals, and an optical chip comprising a substrate and two semiconductor optical waveguides with electrical conductive elements along at least a portion of the optical waveguide surface. In some embodiment, the optical chip is attached to the submount with the optical chip substrate oriented away from the submount and the two semiconductor optical waveguides oriented toward the submount. The submount can comprise a conducting plane offset from the conductive RF electrodes of the optical chip. Generally, the optical chip further comprises two conductive RF electrodes adjacent respectively to corresponding optical waveguides and additional conductive elements connecting one of the conductive RF electrodes to the corresponding conductive element along a surface of the corresponding optical waveguide, and the electrical conduction pathways electrically connect to the conductive RF electrodes of the optical chip. 
     In a further aspect, the invention pertains to an optical modulator comprising a Mach-Zehnder interferometer and a pair of RF electrodes interfaced with the Mach-Zehnder interferometer, the Mach-Zehnder interferometer comprising an optical splitter connected to an optical input waveguide, two optical waveguide arms optically connected to the optical splitter and an optical combiner optically connected to the two optical waveguides and to an output waveguide. The optical waveguides can comprise a semiconductor optical material, and an electrical contact can be located on portions of the optical waveguide arms surface. Each RF electrode of the pair can comprise transmission line electrodes connected by additional electrodes to electrical contacts on respective optical waveguides. In some embodiments, a ground plane is spaced away in a distinct plane from the transmission line electrodes. The optical modulator can be used in a method for modulating an optical telecommunication signal, in which the method comprises exposing laser light split between the two optical waveguides of the Mach-Zehnder interferometer to separate RF electric fields transmitted along RF transmission lines; and recombining the light from the two optical waveguides to form a modulated optical signal. Furthermore, the method can further comprise embodiments of optical modulators with four Mach-Zehnder interferometers, delivering separate RF electric fields to each individual Mach-Zehnder interferometer; and multiplexing the optical signal by combining the resulting optical signal in orthogonal phase states and polarization states. 
     In another aspect, the invention pertains to a method of forming an optical modulator in which the method comprises bonding an inverted optical chip to a submount. The inverted optical chip can comprise a Mach-Zehnder interferometer with optical waveguides and two RF electrodes associated with distinct arms of the Mach-Zehnder interferometer. The submount can comprise electrical contacts aligned with electrical contact points along the adjacent surface of the waveguide structure. The submount can comprise a ground plane spaced away from the mounting surface of the submount. 
    
    
     
       BRIEF DESCRIPTION OF THE DRAWINGS 
         FIG.  1    is a schematic perspective view of an optical modulator of the present application with an optical chip interfaced with a submount. 
         FIG.  2    is a schematic perspective view of optical chip and submount of  FIG.  1    in which the optical chip is disconnected from the submount and inverted to show the surface of the optical chip that interfaces with the submount. 
         FIG.  3    is a fragmentary expanded view of a portion of the optical chip of  FIG.  2   . 
         FIG.  4    is sectional side view of the modulator of  FIGS.  1  and  2    taken at line  4 . 
         FIG.  5    is sectional side view of the modulator of  FIGS.  1  and  2    taken at line  5  showing the bridge electrodes. 
         FIG.  6    is a sectional side view of a modulator along the same view as  FIG.  4    with an alternative embodiment of the submount. 
         FIG.  7    is a sectional side view of a modulator along the same view as  FIG.  5    with the alternative embodiment of the submount depicted in  FIG.  6   . 
         FIG.  8    is a sectional side view of pairs of representative semiconductor optical waveguides for a modulator of the present application on corresponding substrates with an electrical connection on the top surface of the optical waveguides. 
         FIG.  9    is a fragmentary perspective view of an optical chip with optical waveguides interfaces with transmission line RF electrodes. 
         FIG.  10    is an expanded view of a portion of the structure in  FIG.  9   . 
         FIG.  11    is a further expanded view of a portion of the structure in  FIG.  10    with a schematic view of electrical contacts interfaced with the optical waveguides. 
         FIG.  12    is a schematic top view of a modulator of this application with the substrate of the optical chip invisible to show the interface between the optical chip and the submount. 
         FIG.  13    is a fragmentary schematic view of an optical modulator having 4 Mach-Zehnder waveguides interfaced with RF microstrip transmitter. 
         FIG.  14    is a schematic view of the optical modulator of  FIG.  13    with a portion of the optical chip removed to show underlying structure. 
         FIG.  15    is a schematic view of an optical modulator of the present application interfaced with other components of an optical transmitter. 
         FIG.  16    is a schematic view of a dual polarization quadrature phase shift keying modulator. 
         FIG.  17    is a schematic view of the coupling of the X output waveguide and the Y output waveguide of  FIG.  16    passing through a polarizer and a polarization optical coupler. 
     
    
    
     DETAILED DESCRIPTION OF INVENTION 
     An optical modulator can be formed with desirable high frequency performance using a mounting structure or submount with a conduction plane and an optical chip with optical waveguides for the arms of a Mach-Zehnder interferometer that can be positioned with RF electrodes on the optical waveguides. The conduction plane provides a convenient electrical ground plane to support the RF traveling wave that modulates an adjacent optical signal transmitted through the optical waveguides, generally semiconductor waveguides, but potentially other types of electro-optic waveguides. The resulting configuration effectively confines the electric field primarily within the structure providing for low cross talk with neighboring structures. Generally, the resulting mounted structure forms a RF transmission line. The direct mounting of the optical chip onto the submount provides for a convenient RF electrode configuration that introduces manufacturing efficiencies consistent with integration with associated optical components. Specifically, a ball or bump joining process can be used to form the electrical connections between aligned conduction elements such that heating flows a deposit of conductive metal, such as gold or silver, associated with one of the conductive elements to form the conductive bond with little or no manually-produced connections. The modulators described herein are designed to provide appropriate broadband signal modulation at RF frequencies extending to greater than 40 GHz, which are desirable for state of the art optical telecommunication systems as well as future anticipated systems. At high RF frequencies, the RF electrode configurations herein can be appropriately designed to provide for appropriate alignment of RF transmission speeds with the optical transmission through the semiconductor or other electro-optic waveguides. 
     Optical modulators can be used to introduce a modulation to a continuous wave optical transmission to encode the optical transmission with a desired data signal. To provide the modulation of the optical transmission, a radio frequency (RF) transmission line is placed in close proximity to an optical waveguide. The wavelength of the optical signal can be selected for incorporation into an optical telecommunication network, such as operating with C-Band from 1530 nm to 1565 nm or S-Band from 1460 nm to 1530 nm, or L-band from 1565 nm to 1620 nm. 
     The modulators described herein have a Mach-Zehnder interferometer (MZI) that comprises two optical couplers/splitters with two optical waveguides connecting the couplers/splitters that form arms of the MZI. The MZI arms each interface with electrodes of an RF transmitter. The electrodes generally are traveling-wave electrodes that consist of at least two electrodes that form a transmission line (one for each arm), for example, oriented approximately parallel to the optical waveguides. A series of electrode extensions or conductive elements connected to the transmission line electrodes are positioned more proximal to the optical waveguide. Specifically, these conductive elements directly adjacent to the optical waveguides are connected through bridge conductors to the transmission line electrodes. Electric fields from the transmission line electrodes and connected elements, as well as the ground, interact with the properties of optical waveguide material, and therefore the optical signals in the arms of the MZI. Generally, the two respective traveling RF electrodes are driven in an anti-phase (opposite voltages relative to ground) sense relative to each other. Due to the optical modulation, the interference of the optical signals when recombined from the MZI arms constructively or destructively interfere as a function of the modulation so that the transmitted optical signal from the MZI optical circuit is modulated based on the RF signals, and deconvolution of the modulated optical signal at a receiver can extract out the encoded information from the transmitted optical signal. 
     The speed of the optical signal through the waveguides depends on the index of refraction of the optical waveguide, which is generally a semiconductor or high-index dielectric. Similarly, the speed of the RF wave is dependent on the effective RF index of refraction for the RF transmission line electrodes in combination with a ground electrode and surrounding medium. Typically, the speed of the optical signal in the optical waveguide is noticeably different than the speed of the electrical signal in a simple corresponding transmission line. If the speeds of the optical signal and the electrical signal are sufficiently different from each other to result in a walk-off on the order of the modulation wavelength, such as on the order of a centimeter, the signal encoded by the modulation can be distorted, washed out, or lost. Adjusting the speed of optical propagation in the optical waveguide by an appreciable amount is generally impractical. Therefore, efforts have been made to design the structure of the RF transmission lines to better match the RF transmission speed to the optical propagation speed. As RF frequencies increase to allow for a higher bandwidth, the RF wavelengths shrink and the matching of the RF transmission to the optical propagation is correspondingly evaluated using tighter tolerances. 
     The design of the RF electrodes as well as a ground electrode influences the RF transmission. In particular, the electrode design influences power consumption, modulation efficiency and speed of RF transmission. At the same time that the RF transmission speed should appropriately match the optical propagation, it is desirable to have a low power consumption and low cross talk between other modulators mounted nearby while maintaining a desirable degree of signal modulation. An additional constraint is that the electrical impedance of the modulator should be matched to the output impedance of the RF source, including, but not limited to, an external generator or amplifier, or a co-packaged driver. The modulator designs described herein involve the location of the modulator on a submount, i.e. a mount structure that provides matching degree of freedom to match electrical impedance, also enabling high performance while providing suitable commercial processing. With the RF electrode facing toward the ground plane associated with the submount, the RF mode is confined in the submount without significant sensitivity to the airgap between the semiconductor chip and the submount. 
     With respect to the modulator structures herein, the mount provides a lateral displacement, i.e., non-coplanar relationship, between (a) the modulating electrodes placed on or adjacent the surface of the semiconductor based optical waveguide and connected to adjacent transmission lines and (b) a ground supported in a spaced away configuration laterally displaced from the plane of the modulating electrodes. The effective RF index of refraction seen by the RF signal depends on the structure. The optical waveguide structure is mounted in an inverted configuration relative to the supporting structure in the sense that the modulating electrodes are generally placed on “top” of the semiconductor optical waveguides relative to a substrate on which the optical waveguides are formed. Generally, the semiconductor optical waveguide is formed with a p-doped semiconductor layer adjacent the modulating RF electrodes, so the structure described herein can be referred to as a ‘p-down’ structure, although any reference to top or up or the like necessarily has some reference to a supposed orientation of the composite structure since any of the composite structures can be moved around in free space to reorient the structures. While the discussion herein focuses on current commercial processing approaches that are convenient for the structures described, the structures themselves can in principle be formed using direct build up of the desired structures as commercial processing evolves and may make such approaches competitive with the separate formation and mounting processes connecting an optical chip with a mounting structure. 
     In contrast, the use of coplanar grounding electrodes suitable for high frequency modulation are described in U.S. Pat. No. 8,917,958B2 to Prosyk (hereinafter the &#39;958 patent), entitled “Electric Waveguide Transmission Device for Use With a Mach-Zehnder Optical Modulator,” incorporated herein by reference. The &#39;958 patent has a design intended to remove a ground electrode between the transmission line modulator electrodes while maintaining an effective optical modulator. Another RF optical modulator design with coplanar positioned ground conductors is presented in U.S. Pat. No. 9,069,223B2 to Prosyk (hereinafter the &#39;223 patent), entitled “Mach-Zehnder Optical Modulator Using a Balanced Coplanar Strip Line With Lateral Ground Planes,” incorporated herein by reference. The &#39;223 patent asserts to achieve lower waveguide capacitance with reduced power consumption and reduced cross talk using “a balanced coplanar stripline with lateral ground planes.” In contrast with these applications, the present modulators are augmented by coupling to a submount in an inverted configuration relative to the submount, and having a ground plane is positioned vertically displaced within the submount. In some embodiments, no lateral ground plane is present. The vertically displaced ground plane is distinct from a non-grounded, i.e., floating, semiconductor conduction plane linking the semiconductor optical waveguides, and a floating semiconductor conduction plane is generally inherent in the present system on the opposite side of the semiconductor optical waveguides away from the electrically conductive ground plane. 
     An embodiment of the RF optical modulator as described herein is shown in  FIG.  1   . Referring to  FIG.  1   , an optical modulator structure  100  is shown with an optical chip  102  mounted on a submount  104 . An exploded or separated view is shown in  FIG.  2    with optical chip  102  rotated relative to submount  104  to show the mated structures.  FIG.  3    shown an expanded view of a portion of optical chip  102 . Referring to  FIGS.  2  and  3   , optical chip  102  has substrate  108 , two optical waveguides  110 ,  112 , two transmission line RF electrodes  114 ,  116  and respective bridge electrodes  118 ,  120 . The transmission line RF electrodes can be, in some embodiments, from about 10 microns to about 30 microns wide, respective RF transmission line electrodes  114 ,  116  can be spaced apart from each other, in some embodiments, from about 50 microns to 150 microns apart. Respective transmission line RF electrodes  114 ,  116  terminate respectively with bond pads  122 ,  124  and  126 ,  128 . Submount  104  comprises substrate  130 , conduction stripes  132 ,  134 ,  136 ,  138  connected respectfully with bond pads  140 ,  142 ,  144 ,  146 , and conductive plane  148 . Substrate  130  can comprise a ceramic material, such as Aluminum Nitride, Alumina, or others; and/or a polymer material, such as polycarbonate or PET or the like. Electrically conductive elements of submount  104  can be formed with metal films, such as copper, silver, gold, alloys thereof or the like. Bond pads  140 ,  142  are configured for respective attachment to bond pads  122 ,  124 , and bond pads  144 ,  146  are configured for respective attachment to bond pads  126 ,  128 . Conductive plane  148  generally can be grounded to provide a ground for RF electrodes  114 ,  116 . Collectively, RF electrodes  114 ,  116  and conductive plane  148  (ground) form a RF transmission line in which the electric and magnetic fields extends through the optical waveguides. 
     Sectional views of optical modulator  100  are shown in  FIGS.  4  and  5   . The cross section of  FIG.  5    is positioned to show the bridge electrodes, which are not shown in  FIG.  4   . The figure shows the spatial relationship of transmission line RF electrodes  114 ,  116  with conductive plane  148  that functions as a ground plane. In general, the airgap between RF electrodes  114 ,  116  and the top of the submount can be on the order of 10 s of microns, and the thickness of the submount can be on the order of 100 microns. An alternative embodiment is shown in  FIGS.  6  and  7   . In this embodiment, substrate  150  of the submount comprises a conductive plane  152  within the substrate structure rather than on a surface, as shown in  FIGS.  4  and  5   . With such an alternative embodiment, the distance from the conductive plane to the transmission line can be designed to achieve desired RF performance without fixing the thickness of the submount. Also, the conductive plane can be on the top surface of the submount across an airgap from the RF transmission line, although it is generally desirable for the conductive plane to be a further distance from the RF line to provide for managed RF mode confinement and control of impedance in the RF line. 
     Generally, for these MZI based optical modulators, the optical waveguides can be semiconductor based materials. A basic exemplified structure of a semiconductor optical waveguide is shown in  FIG.  8   , with both arms of the MZI depicted. Referring to  FIG.  8   , optical structure  160  comprises first optical waveguide  162 , second optical waveguide  164 , semiconductor support  166  and base support layer  168 . First optical waveguide  162  and second optical waveguide  164  generally each comprise a p-i-n diode structure or more generally a c-n-c (conductive-nonconductive-conductive) structure, although additional layers and/or sublayers within the depicted layers can be included to provide desired performance. In the present context of semiconductor materials, as would be recognized by a person of ordinary skill in the art, a non-conductive material would not be absolutely non-conductive, but it would have a very significant electrical resistance, and conductive materials would not necessarily be as conductive as a metal, but in a relative sense the conductive materials would generally have a conductivity at least a factor of ten greater conductivity than the non-conductive regions and in many embodiments at least a factor of a hundred greater conductivity and in further embodiments at least a factor of 1000 greater conductivity. Specifically, in the depicted embodiments first optical waveguide  162  can comprise electrical contact  170  (connected to a bridge electrode), doped (such as p-doped) or conducting layer  172 , intrinsic or non-conducting layer  174  and doped (such as n-doped) or conducting layer  176 , and second optical waveguide  164  can comprise electrical contact  180 , doped (such as p-doped) or conducting layer  182 , intrinsic layer  184  and doped (such as n-doped) or conducting layer  186 . First optical waveguide  162  and second optical waveguide  164  can be spaced sufficiently to reduce any optical interactions to a desired level, and a person of ordinary skill in the art can evaluate appropriate distances based on the material in the optical waveguides. Semiconductor support  166  generally can comprise a doped or conducting semiconductor layer, and base support layer  168  can comprise an intrinsic or non-conducting semiconductor layer. Electrical contacts  170 ,  180  generally comprise metal layers, such as silver, gold, platinum or copper, and as indicated in  FIG.  3    and shown more explicitly in reference to  FIGS.  9 - 11    below, the electrical contacts can only be associated with portions of the optical waveguides. For the other portions of the waveguide, the structure can be the same without the electrical contact layer. Suitable semiconductors or other optical-waveguide substrates include, for example, InP, GaAs, LiNbO 3 , Si or other suitable material. Suitable dopants to generate conducting semiconductors generally include Si, S or P as an n dopant and Zn or B as a p dopant as well as other suitable dopant elements. A substrate can support the optical waveguide structure, such as a silicon support. Bulk support layer  168  can have a thickness of 10s to 100s of microns to provide a desirable level of support. The remaining layers are generally on the order of 50 nanometers (nm) to 5 microns. Also, there can be additional semiconductor layers or sublayers within a specific optical waveguide design. InP based modulators offer the possibility of a compact modulator format, but low impedance in conventional designs can limit the interaction lengths between electrical and optical waves. An approach to address these issues are described in Dummer et al., “Periodic Loading and Selective Undercut Etching for High-Impedance Traveling-Wave Electroabsorption Modulators,” incorporated herein by reference. Because the position of the submount ground plane influences the impedance of the RF transmission line mode, the modulator designs herein offer an effective solution to these concerns with a convenient processing approach suitable for commercial manufacturing. 
     Sequentially expanded views of a fragment of the optical chip  102  (sectional view in  FIG.  4   ) are shown in  FIGS.  9 - 11   . In these views, the two arms of an MZI are shown with two corresponding transmission line RF electrodes with corresponding bridges to the electrical contacts located on the optical waveguides. Referring to  FIG.  9   , optical chip  200  comprises a substrate  202 , RF electrodes  204 ,  206 , optical waveguides  208 ,  210 , and two sets of electrode bridges  212 ,  214 , which are generally formed from appropriately patterned metal films. Referring to the further expanded view in  FIG.  10   , the connection of electrical bridges  212 ,  214  to electrical contacts  216 ,  218  associated with respective optical waveguides  208 ,  210 . Electrical contacts  216 ,  218  cover selected portions of optical waveguides  208 ,  210 . Electrical contacts correspond with electrical contacts  170 ,  180  in the structure of  FIG.  8   . Referring to the further expanded view of  FIG.  11   , a doped or conducting substrate  220  and base substrate  222  can be seen in association with optical waveguides  208 ,  210 . Doped or conducting substrate  220  and base substrate  222  correspond respectively with semiconductor support  166  and bulk support layer  168  in the structure of  FIG.  8   . 
     The larger integration of the components of a modulator  250  are shown for an example embodiment in  FIG.  12    with the optical chip substrate and any overlapping elements being transparent to show the interface of the optical chip with the submount in an assembled configuration. As a result of this depiction, the optical chip and submount are not readily distinguishable in this view, although they are distinguishable in other figures. Referring to  FIG.  12   , optical waveguides  252 ,  254  connect with couplers/splitters  256 ,  258  at their ends. An input waveguide  260  of optical coupler/splitter  256  is optically connected to an optical connector  262  at the edge of modulator  250  to provide for attachment to an optical fiber or an optical waveguide of another device, such as a laser structure. In some embodiments, input waveguide  260  of coupler/splitter  256  can interface with additional integrated optical elements on the optical chip as an alternative to directly interfacing with an optical connector. Optical coupler/splitter  258  interfaces with an output waveguide  264 . 
     Transmission line RF electrodes  270 ,  272  connect respectively with optical waveguides  252 ,  254  through bridge electrodes  274 ,  276 . Transmission line RF electrode  270  connects with conductive pads  280 ,  282 , and conductive pads  280 ,  282  are in electrical contact with, respectively, conductive elements  288 ,  290  that terminate at conductive pads  280 ,  282 . Transmission line RF electrode  272  connects with conductive pads  284 ,  286 , and conductive pads  284 ,  286  are in electrical contact with, respectively, conductive elements  292 ,  294  that terminate at conductive pads  284 ,  286 . Conductive elements  288 ,  290 ,  292 ,  294  are supported by the submount. Conductive pads  280 ,  282 ,  284 ,  286  connect electrodes along the optical waveguides on the optical chip with electrodes supported on the submount. The connection pads associated with conductive elements  288 ,  290 ,  292 ,  294  can be wired or otherwise electrically connected to the RF generator associated with providing the modulation signals and a suitable impedance matched RF termination network. 
     For use in present state of the art coherent optical communication, it can be desirable to group 4 MZI based modulator elements in association with each other, although smaller numbers of MZI based modulators such as one, two or three, can be integrated in a single optical chip for transmission of coherent or non-coherent communication signals based on further integrated structures. As used in the art, coherent refers to optical communication signals that carry information in both the amplitude and phase of the optical field and its polarization. For these signals, it is typical that two orthogonal polarization states of the optical signal are independently modulated, each according to the two degrees of optical phase and amplitude, and then recombined for transmission, which together can be referred to as polarization multiplexing (PM). Applying different schemes of electrical modulation to the embedded MZIs can generate various standard forms of coherent optical constellations to encode the data transmission. For instance, if the optical output for each polarization is at a constant amplitude and modulated to one of four optical phases separated by 90-degrees, this is conventionally referred to as “quadrature phase-shift keying” (QPSK). When used this way, the four-MZI configuration described provides “PM-QPSK” coherent optical transmission. This provides four binary ‘bits’ of information in each transmitted optical symbol (two polarizations times two bits—any of four possible phases—per polarization). Alternatively, it is possible to vary both the phase and amplitude of each transmitted polarization through modulation. This is conventionally called “nQAM” (n quadrature-amplitude modulation, where ‘n’ is the number of phase-amplitude states in the allowed palette). Typically desired modulation patterns include 16QAM (4 bits per polarization) and 64QAM (6 bits per polarization). The 4-MZI configuration group described herein is generally optimal for supporting transmission of any of the existing coherent transmission formats (e.g. PM-QPSK, PM-16QAM) or emerging formats (e.g. PM-64QAM, or other). Although not a widely-adopted terminology at the time of the present application, all these and other suitable coherent formats can be gathered under the readily-recognized term ‘PM-IQ’ (polarization multiplexed; in-phase/quadrature amplitudes). The 4-MZI embodiments described as example herein may therefore be referred to as PM-IQ modulators. Of course, larger groups of MZI based modulators can be packaged together, optionally in multiples of 4, to for instance to provide PM-IQ modulation of multiple independent optical wavelengths. To support a more specific discussion of packaging, for convenience, the immediately following discussion focuses on modulator structures with 4 MZI based modulator elements. 
     For assembly, the optical chip is formed using appropriate patterning and layer build up processing, such as CVD and photolithography. For the application of metal electrodes, sputtering, other chemical or physical vapor deposition approaches, conductive paste that can be cured for metal film formation, or the like can be used. The optical components can be formed, for example, on a smooth InP or silicon wafer and then diced to form the individual components. The metal electrodes are added along with the bridge electrodes and electrical contacts on the optical waveguide through bridge electrodes supported on appropriate support structure, as part of the RF transmission line and provide connection points to the submount. The submount can be a printed circuit board, flex-circuit, ceramic, metal layer stack or other similar structure that provides a desired structure with an insulating substrate and designed electrical connections. If a commercial printed circuit board, flex-circuit, ceramic or other appropriate structure has an appropriate thickness, a conductive layer can be placed along its surface distal to the optical chip as a ground plane. Alternatively a submount can be constructed with an appropriately elsewhere positioned conductive plane as a ground, such as within the submount, as described above, or along the proximal surface across an air gap from the optical chip. The optical chip can be inverted and placed onto the submount. The submount can comprise insulating support elements to support at least portions of the optical chip in a spaced away relationship from the surface of the submount. Support elements can be, for example, glass posts, ceramic columns, or the like. The electrical connections with the optical chip electrodes can be made by wire bonding, but in some embodiments appropriate assembly can be performed using mated bonding pads on the submount so that positioning of the optical chip with the submount aligns the bonding pads on each that can then be connected, such as with reflow of solder. In some embodiments, conductive metal bonding balls or pads can have appropriate dimensions to support the optical chip on the submount, which can then replace insulating posts or the like. Since wire bonding balls would be placed at suitable locations, there is no concern that they are conductive with no corresponding insulating structures between the elements. Other suitable processing approaches can be used. 
     Referring to  FIG.  13   , a fragmentary view of a modulator  300  is shown with an optical chip  302  supported on a submount  304 . Optical chip  302  has 4 MZI structures  310 ,  312 ,  314 ,  316  mounted on the chip to modulate a coherent optical signal that results following the combining of the 4 separately modulated polarizations and amplitude-phase states from each MZI modulator component. Glass posts or wirebond balls  318  support optical chip  302  mounted on submount  304 . As shown in  FIG.  13   , pairs of optical waveguides  320 ,  322 ,  324 ,  326  associated with each MZI structure  310 ,  312 ,  314 ,  316 , respectively, pass through modulation zones between transmission line RF electrodes connected to electrical contacts on the optical waveguides and continue on both ends of the modulation zones. As suggested in  FIG.  12   , the two arms of each pair are directed on both ends to an optical combiner/splitter, and also then the four optical signals from the 4 MZI elements can be combined with an optical combiner to form a modulated output optical signal for transition. Each transmission line RF electrode is connected to a bond pad at or near each end, which electrically connects to electrodes  330  on submount  304 . In this embodiment, a conduction plane  332  is shown located on the lower surface of submount  304 , although locations within submount  304  can be equally effective. Submount  304  directly or indirectly provides electrical connection with an RF generator that provides desired modulation for data transmission. Referring to  FIG.  14   , an alternative view of modulator  300  is shown with portions of the optical chip removed. 
     A schematic layout of a modulator as described herein is shown in  FIG.  15    as a portion of an optical telecommunications transmitter. A laser  350 , such as a semiconductor diode laser or laser array, directs light output to a light channel  352 , such as a waveguide or optical fiber, which interfaces with modulator  354 . Through appropriate optical elements, modulator  354  ultimately interfaces with an optical fiber  356  that is part of an optical telecommunications network for transmission generally to a location remote from modulator  354 . Modulator  354  generally is also electrically connected to an RF generator  358  through appropriate electrical connections  360  that have an electrical termination  362 . Modulator  354  generally can have the various designs described herein to provide desirable modulator function. The connections of modulator  354  with the input and output components noted in  FIG.  15    can use planar components, free space components or combinations thereof along with appropriate connectors, such as those known in the art to connect planar lightwave circuit to each other and/or optical fibers to planar lightwave circuits. 
     Referring to  FIG.  16   , the layout is shown of a coherent optical chip  380  for a corresponding modulator. Coherent optical chip  380  comprises an input waveguide  382  connected to an optical splitter  384 , which is connected by split waveguides  386 ,  388  to a first coupled pair of modulated Mach-Zehnder interferometers (MZI)  390  and a second coupled pair of modulated MZI  392 . The coupled pairs of modulated Mach-Zehnder interferometers can be referred to as I-Q pairs based on terminology in the coherent optical telecommunications art. First coupled pair of modulated MZI  390  comprises optical splitter  400 , first MZI  402 , second MZI  404 , input split waveguides  406 ,  408  connecting optical splitter  400  with first MZI  402  and second MZI  404 , optical coupler  410 , output split waveguides  412 ,  414  connecting optical coupler  410  with first MZI  402  and second MZI  404 , and X output waveguide  416 . First MZI  402  comprises optical splitter  420 , first MZI arm  422 , second MZI arm  424  and optical coupler  426 . RF electrodes  428 ,  430  interface respectively with first MZI arm  422  and second MZI arm  424  with appropriate electrical connections as described herein. Similarly, second MZI  404  comprises optical splitter  440 , first MZI arm  442 , second MZI arm  444  and optical coupler  446 . RF electrodes  448 ,  450  interface respectively with first MZI arm  442  and second MZI arm  444  with appropriate electrical connections as described herein. Second coupled pair of modulated MZI  392  comprises optical splitter  460 , third MZI  462 , fourth MZI  464 , input split waveguides  466 ,  468  connecting optical splitter  460  with third MZI  462  and fourth MZI  464 , optical coupler  470 , output split waveguides  472 ,  474  connecting optical coupler  470  with third MZI  462  and fourth MZI  464 , and Y output waveguide  476 . Third MZI  462  and fourth MZI  464  comprise similar structure as first MZI  402  and second MZI  404  which is not labeled in the drawing to simplify the drawing. While optical chip  380  is described as a single planar optical structure, in some embodiments, the functions described for optical chip  380  can be divided in three or more planar optical structures  500 ,  502 ,  504  divided by the dashed lines in  FIG.  16    that have suitable optical coupling connecting them. Optical structure  500  can be an optical chip with semiconductor waveguides forming the MZI while optical structures  502 ,  504  can be, for example, optical chips comprising silica glass waveguides forming splitters and combiners and associated optical components. 
     To introduce the polarization dependence, a polarizer and polarization beam combiner can be used based on the X output signal and the Y output signal. Referring to  FIG.  17   , X output waveguide  416  interfaces with a 90 degree polarizer  510 , such as a waveplate, that rotates the polarization for this signal. Polarized waveguide from polarizer  510  is directed to polarization beam combiner  512  that is also connected to Y output waveguide  476 . Polarization beam combiner  512  directs output to polarization multiplexed output waveguide  514 . The structure shown in  FIG.  17    performs multiplexing of the optical signal by combining the resulting optical signal in orthogonal phase states and polarization states. Polarization beam combiners are described, for example, in U.S. Pat. No. 9,442,248 to Yamazaki, entitled “Polarization Beam Combiner/Splitter, Polarization Beam Combining/Splitting Structure, Light Mixer, Optical Modulator Module, and Method for Manufacturing Polarization Beam Combiner/Splitter,” incorporated herein by reference. 
     The embodiments above are intended to be illustrative and not limiting. Additional embodiments are within the claims. In addition, although the present invention has been described with reference to particular embodiments, those skilled in the art will recognize that changes can be made in form and detail without departing from the spirit and scope of the invention. Any incorporation by reference of documents above is limited such that no subject matter is incorporated that is contrary to the explicit disclosure herein. To the extent that specific structures, compositions and/or processes are described herein with components, elements, ingredients or other partitions, it is to be understood that the disclosure herein covers the specific embodiments, embodiments comprising the specific components, elements, ingredients, other partitions or combinations thereof as well as embodiments consisting essentially of such specific components, ingredients or other partitions or combinations thereof that can include additional features that do not change the fundamental nature of the subject matter, as suggested in the discussion, unless otherwise specifically indicated.