Enlarging the Eyebox of Maxwellian Displays with a Customized Liquid Crystal Dammann Grating

: The Maxwellian view offers a promising approach to overcome the vergence-accommodation conﬂict in near-eye displays, however, its pinhole-like imaging naturally limits the eyebox size. Here, a liquid crystal polymer-based Dammann grating with evenly distributed energy among different diffraction orders is developed to enlarge the eyebox of Maxwellian view displays via pupil replication. In the experiment, a 3-by-3 Dammann grating is designed and fabricated, which exhibits good efﬁciency and high brightness uniformity. We further construct a proof-of-concept Maxwellian view display breadboard by inserting the Dammann grating into the optical system. The prototype successfully demonstrates the enlarged eyebox and full-color operation. Our work provides a promising route of eyebox expansion in Maxwellian view displays while maintaining full-color operation, simple system conﬁguration, compactness, and lightweight.


Introduction
Augmented reality (AR), virtual reality (VR), and mixed reality (MR) near-eye displays are emerging rapidly [1] because of their potential to revolutionize entertainment, education, engineering, and healthcare. A major obstacle that influences the user experience of these AR/VR displays is the vergence-accommodation conflict (VAC) [2,3]. For most existing near-eye displays, the depth cue is generated by binocular disparity, where two different images are respectively delivered to the observer's left and right eyes. On the other hand, the virtual image plane is fixed so that the accommodation distance is not image-dependent. Such a mismatch between vergence and accommodation cues results in visual discomfort and fatigue.
To tackle VAC, plethora of methods have been proposed, including but not limited to multi-focal plane displays [4][5][6], varifocal plane displays [7,8], integral imaging-based displays [9,10], holographic displays [11][12][13], and Maxwellian view displays [14][15][16][17][18]. Among them, Maxwellian view is a special display to bypass this VAC issue by providing a very large depth of focus. Moreover, the optical system of a Maxwellian view display is usually quite energy efficient, simple, and compact. However, due to its pinhole-like imaging, the eyebox is limited. Upon eye movement, the viewpoint can be easily missed out by the pupil.
In this paper, we propose and demonstrate a Maxwellian view near-eye display with an enlarged eyebox achieved by viewpoint replication. To create multiple viewpoints at the same time, we propose to insert a Dammann grating with multiple diffraction orders, good overall efficiency, and high brightness uniformity into the optical system. In the experiment, we design and fabricate a customized Dammann grating based on patterned liquid crystal (LC) polymers. A simple proof-of-concept prototype is also established. The use of a Dammann grating in a Maxwellian view near-eye display can offer full-color imaging and enlarged eyebox, while keeping a compact size and lightweight.

Maxwellian View Near-Eye Displays
Figure 1a depicts a typical configuration of Maxwellian view near-eye display. The image produced by the laser beam scanning projector (LP) is incident on an optical combiner (OC) with focusing power. The eye views the image by placing the pupil near the focal point of the OC. The image is directly formed on the retina and is always in focus, regardless of the optical power of the eye lens. Ascribed to this pinhole-like imaging, this focal point of OC can be easily missed upon eye movement. To ensure that the image can be observed by the eye (as shown in Figure 1b), two common approaches have been investigated, namely pupil steering and pupil replication.
Crystals 2021, 11, x FOR PEER REVIEW use of a Dammann grating in a Maxwellian view near-eye display can offer f aging and enlarged eyebox, while keeping a compact size and lightweight.

Maxwellian View Near-Eye Displays
Figure 1a depicts a typical configuration of Maxwellian view near-eye image produced by the laser beam scanning projector (LP) is incident on an biner (OC) with focusing power. The eye views the image by placing the pu focal point of the OC. The image is directly formed on the retina and is alwa regardless of the optical power of the eye lens. Ascribed to this pinhole-like i focal point of OC can be easily missed upon eye movement. To ensure that th be observed by the eye (as shown in Figure 1b), two common approaches h vestigated, namely pupil steering and pupil replication. Pupil steering is generally more energy efficient, as it creates one viewpo This can be realized by adjusting the eyebox in spatial frequency domain or chanically movable device [14]. However, these methods usually result in a complex, high cost or large volume display system. By contrast, generating mu ing points in space at the same time can be much easier, but some of the op will be inevitably lost. Previously, 1D and 2D pupil replication in Maxwellian eye displays with simple optical systems have been reported [15,16]. Nonet either suffer from single color operation, image artifacts, or limited eyebox ex

Improved LC Dammann Gratings
For viewpoint replication in Maxwellian view near-eye displays, mu points with uniform brightness distribution are desired. Generating multip space can be realized by diffracting beams into multiple orders in the angu Although using an arbitrary grating may create a lot of viewpoints, it can har requirement of evenly distributed optical power in those diffraction orders. Dammann gratings with optimizable diffraction orders can meet this challen binary gratings with calculated transition points within a period [19].
Here, patterned LC polymers are employed to fabricate the Dammann shown in Figure 2a, the LC polymer consists of a photoreactive mesogen and a layer. To create the patterned binary phase, the LCs are aligned in either 0° or desired alignment pattern created from a spatial light modulator (SLM), and ymer film serves as a patterned half-wave plate. For incident left-handed circu ized light, its polarization is flipped to right-handed upon transmitting thro wave plate and a geometric phase term is added [20]. Most previous Damm designs have focused on achieving perfect binary gratings. However, in a Dammann grating, line defects can appear at the LC alignment domain boun As we will compare later, if LC alignment at the domain boundary has an abr the overall alignment quality would deteriorate, causing unwanted misalig Pupil steering is generally more energy efficient, as it creates one viewpoint at a time. This can be realized by adjusting the eyebox in spatial frequency domain or using a mechanically movable device [14]. However, these methods usually result in a much more complex, high cost or large volume display system. By contrast, generating multiple viewing points in space at the same time can be much easier, but some of the optical power will be inevitably lost. Previously, 1D and 2D pupil replication in Maxwellian view near-eye displays with simple optical systems have been reported [15,16]. Nonetheless, they either suffer from single color operation, image artifacts, or limited eyebox expansion.

Improved LC Dammann Gratings
For viewpoint replication in Maxwellian view near-eye displays, multiple viewpoints with uniform brightness distribution are desired. Generating multiple views in space can be realized by diffracting beams into multiple orders in the angular domain. Although using an arbitrary grating may create a lot of viewpoints, it can hardly fulfil the requirement of evenly distributed optical power in those diffraction orders. Fortunately, Dammann gratings with optimizable diffraction orders can meet this challenge. They are binary gratings with calculated transition points within a period [19].
Here, patterned LC polymers are employed to fabricate the Dammann grating. As shown in Figure 2a, the LC polymer consists of a photoreactive mesogen and an alignment layer. To create the patterned binary phase, the LCs are aligned in either 0 • or 90 • with the desired alignment pattern created from a spatial light modulator (SLM), and the LC polymer film serves as a patterned half-wave plate. For incident left-handed circularly polarized light, its polarization is flipped to right-handed upon transmitting through such a wave plate and a geometric phase term is added [20]. Most previous Dammann grating designs have focused on achieving perfect binary gratings. However, in an LC-based Dammann grating, line defects can appear at the LC alignment domain boundaries [21]. As we will compare later, if LC alignment at the domain boundary has an abrupt change, the overall alignment quality would deteriorate, causing unwanted misalignment and light scattering. Therefore, in our design, we take this boundary continuity into account by inserting a single alignment transition pixel line with a 45 • alignment angle in between two domains. With predefined rotation direction in between two domains, the unwanted misalignment can be mostly eliminated. During the optical optimization of the Dammann grating, the diffraction effect from the transition buffer pixels is also considered. Meanwhile, since we are using an SLM for patterning, the effect of discrete pixels needs to be accounted for as well.
Crystals 2021, 11, x FOR PEER REVIEW 3 of light scattering. Therefore, in our design, we take this boundary continuity into accoun by inserting a single alignment transition pixel line with a 45° alignment angle in between two domains. With predefined rotation direction in between two domains, the unwanted misalignment can be mostly eliminated. During the optical optimization of the Dammann grating, the diffraction effect from the transition buffer pixels is also considered. Mean while, since we are using an SLM for patterning, the effect of discrete pixels needs to b accounted for as well. To prove the concept, a 3-by-3 Dammann grating is optimized with good efficiency and high uniformity. The optimization is performed by sweeping the transition points o a 2D binary grating and the efficiency of each diffraction order is numerically calculated by the Huygens-Fresnel principle with the Fraunhofer approximation. As a comparison we also adopt a design from perfect binary gratings [19]. The transition points for th control design and our design are 0.7353 and 0.2766, respectively, as depicted in Figur 2b,c. It is important to note that for LC polarization gratings with continuous LC directo rotation, the diffraction pattern is strongly circular polarization-dependent [16]. For ou customized Dammann gratings, the grating is almost binary and symmetric in 2D space and thus the far-field diffraction pattern will be nearly the same for both circular polari zations. Consequently, the Dammann grating is suitable for both unpolarized and polar ized light operations.
In experiment, both reference and customized Dammann gratings are fabricated, fol lowing the procedure shown in Figure 3a. First, a thin film of photoalignment material 0.4wt% Brilliant Yellow (BY, from Tokyo Chemistry Industry) dissolved in dimethylfor mamide (DMF) solvent, is spin-coated onto cleaned glass substrates with 500 rpm for 5 and 3000 rpm for 30 s. Then, the substrates coated with BY are mounted on the sampl holder for exposure. The photoalignment material is responsive to linearly polarized short-wavelength light (e.g., UV, blue). Upon illumination, the photoalignment material will be aligned perpendicular to the linear polarization of light, resulting in a minimum free-energy state [22,23]. The exposure setup is shown in Figure 3b, which is similar t that reported in [24], is to create the desired linear polarization field that matches the de sign. The employed SLM is a phase-only liquid-crystal-on-silicon (LCoS) device (Hima HX7322), the lens used in the setup has a focal length of ~8 cm, and the recording wave length is 488 nm. In this setup, the incident light is linearly polarized along 45°, assuming that the LC alignment direction in SLM is along 0°. The fast axis of the quarter-wave plat is also placed along 45°. In this way, by increasing the phase retardation of SLM from 0 t 2π, the output linear polarization direction will be continuously rotated by π, and thus full linear polarization control is achieved. The linear polarization patterning can be un derstood by the Jones matrix calculation [24]. After exposure, a reactive mesogen solution consisting of 97wt% reactive mesogen RM257 (from LC Matter) and 3wt% photo initiato Irgacure 651 (from BASF) dissolved in toluene with a weight ratio of 1:3, is spin-coated To prove the concept, a 3-by-3 Dammann grating is optimized with good efficiency and high uniformity. The optimization is performed by sweeping the transition points of a 2D binary grating and the efficiency of each diffraction order is numerically calculated by the Huygens-Fresnel principle with the Fraunhofer approximation. As a comparison, we also adopt a design from perfect binary gratings [19]. The transition points for the control design and our design are 0.7353 and 0.2766, respectively, as depicted in Figure 2b,c. It is important to note that for LC polarization gratings with continuous LC director rotation, the diffraction pattern is strongly circular polarization-dependent [16]. For our customized Dammann gratings, the grating is almost binary and symmetric in 2D space, and thus the far-field diffraction pattern will be nearly the same for both circular polarizations. Consequently, the Dammann grating is suitable for both unpolarized and polarized light operations.
In experiment, both reference and customized Dammann gratings are fabricated, following the procedure shown in Figure 3a. First, a thin film of photoalignment material, 0.4wt% Brilliant Yellow (BY, from Tokyo Chemistry Industry) dissolved in dimethylformamide (DMF) solvent, is spin-coated onto cleaned glass substrates with 500 rpm for 5 s and 3000 rpm for 30 s. Then, the substrates coated with BY are mounted on the sample holder for exposure. The photoalignment material is responsive to linearly polarized short-wavelength light (e.g., UV, blue). Upon illumination, the photoalignment materials will be aligned perpendicular to the linear polarization of light, resulting in a minimum free-energy state [22,23]. The exposure setup is shown in Figure 3b, which is similar to that reported in [24], is to create the desired linear polarization field that matches the design. The employed SLM is a phase-only liquid-crystal-on-silicon (LCoS) device (Himax HX7322), the lens used in the setup has a focal length of~8 cm, and the recording wavelength is 488 nm. In this setup, the incident light is linearly polarized along 45 • , assuming that the LC alignment direction in SLM is along 0 • . The fast axis of the quarter-wave plate is also placed along 45 • . In this way, by increasing the phase retardation of SLM from 0 to 2π, the output linear polarization direction will be continuously rotated by π, and thus a full linear polarization control is achieved. The linear polarization patterning can be understood by the Jones matrix calculation [24]. After exposure, a reactive mesogen solution, consisting of 97wt% reactive mesogen RM257 (from LC Matter) and 3wt% photo initiator Irgacure 651 (from BASF) dissolved in toluene with a weight ratio of 1:3, is spin-coated onto the substrates with 2000 rpm for 30 s. As the final step, the samples are cured by a UV light (365 nm) for 5 min with ∼10 mW/cm 2 irradiance.  To characterize the fabricated LC Dammann gratings, polarized optical (POM) images of reference grating and designed grating are recorded, as Figu Here, the alignment direction within a domain is parallel to the polarizer's o that sense, both 0° and 90° aligned LC domains will be dark under POM. How boundary of different alignment directions, light leakage will be observed du fects (Figure 4a) or alignment transition ( Figure 4b). As can be seen, the light le outline the alignment pattern, which agrees well with the designed phase pat in Figure 2. For the reference grating, the light leakage lines are narrower. Ho wanted misalignment and defects are quite visible. Interestingly, with a alignment transition, the alignment quality is much improved. The grating p customized grating is roughly 75 μm, which corresponds to ~0.41° first-order angle in the air for a green wavelength. The half-wave wavelength of both fabricated Dammann gratings is chara inserting them in between two circular polarizers with the same handedness. strated in Figure 5a, the central wavelength appears at   530 nm. Noticeab tomized Dammann grating can reach a reasonably good dark state, while th grating shows ~5% light leakage at   530 nm. This light leakage is mainly asc misalignment and defects, which cause light scattering. For the customized overall diffraction efficiency should follow the sin 2 (Γ/2) law upon waveleng To characterize the fabricated LC Dammann gratings, polarized optical microscope (POM) images of reference grating and designed grating are recorded, as Figure 4 shows. Here, the alignment direction within a domain is parallel to the polarizer's optic axis. In that sense, both 0 • and 90 • aligned LC domains will be dark under POM. However, at the boundary of different alignment directions, light leakage will be observed due to line defects (Figure 4a) or alignment transition ( Figure 4b). As can be seen, the light leakage lines outline the alignment pattern, which agrees well with the designed phase pattern shown in Figure 2. For the reference grating, the light leakage lines are narrower. However, unwanted misalignment and defects are quite visible. Interestingly, with a predefined alignment transition, the alignment quality is much improved. The grating period of the customized grating is roughly 75 µm, which corresponds to~0.41 • first-order diffraction angle in the air for a green wavelength.  To characterize the fabricated LC Dammann gratings, polarized optical microscope (POM) images of reference grating and designed grating are recorded, as Figure 4 shows. Here, the alignment direction within a domain is parallel to the polarizer's optic axis. In that sense, both 0° and 90° aligned LC domains will be dark under POM. However, at the boundary of different alignment directions, light leakage will be observed due to line defects (Figure 4a) or alignment transition ( Figure 4b). As can be seen, the light leakage lines outline the alignment pattern, which agrees well with the designed phase pattern shown in Figure 2. For the reference grating, the light leakage lines are narrower. However, unwanted misalignment and defects are quite visible. Interestingly, with a predefined alignment transition, the alignment quality is much improved. The grating period of the customized grating is roughly 75 μm, which corresponds to ~0.41° first-order diffraction angle in the air for a green wavelength. The half-wave wavelength of both fabricated Dammann gratings is characterized by inserting them in between two circular polarizers with the same handedness. As demonstrated in Figure 5a, the central wavelength appears at   530 nm. Noticeably, the customized Dammann grating can reach a reasonably good dark state, while the reference grating shows ~5% light leakage at   530 nm. This light leakage is mainly ascribed to the misalignment and defects, which cause light scattering. For the customized grating, its overall diffraction efficiency should follow the sin 2 (Γ/2) law upon wavelength changes, The half-wave wavelength of both fabricated Dammann gratings is characterized by inserting them in between two circular polarizers with the same handedness. As demonstrated in Figure 5a, the central wavelength appears at λ ≈ 530 nm. Noticeably, the customized Dammann grating can reach a reasonably good dark state, while the reference grating shows~5% light leakage at λ ≈ 530 nm. This light leakage is mainly ascribed to the misalignment and defects, which cause light scattering. For the customized Crystals 2021, 11, 195 5 of 8 grating, its overall diffraction efficiency should follow the sin 2 (Γ/2) law upon wavelength changes, where Γ is the phase retardation of the LC polymer [20]. In fact, to overcome this wavelength-dependent diffraction efficiency, a multi-twist structure along thickness direction can be introduced, as reported in [25,26]. To observe the diffraction pattern of fabricated Dammann gratings, we put the samples in front of a green point source and use a camera to capture the transmitted light, as shown in Figure 5b. The diffraction patterns of reference grating and designed grating are manifested in Figure 5c,d, respectively. For both gratings, multiple diffraction orders are observed. Nevertheless, for the reference grating, the central 0th order shows much higher efficiency than other orders. Moreover, the higher orders of the reference grating exhibit a greater efficiency than those of the customized grating, and the diffraction pattern of the reference grating is more blurred, which is due mainly to LC misalignment and defects. For a well-aligned LC Dammann grating, the designed diffraction orders have more evenly distributed energy. Per our measurements, the diffraction efficiency of the customized Dammann gratings for green light and central 3-by-3 diffraction orders is~45%, which is close to the simulation results (~55%). Here, the diffraction efficiency is defined as the power sum of the central 3-by-3 orders (in total 9 orders) divided by the total transmitted power. The uniformity, defined as (I max − I min )/(I max + I min ), where I max is the maximum intensity and I min is minimum intensity, is measured as~0.13, which agrees well with the simulation (~0.08).

Crystals 2021, 11, x FOR PEER REVIEW
where Γ is the phase retardation of the LC polymer [20]. In fact, to overcome this w length-dependent diffraction efficiency, a multi-twist structure along thickness direc can be introduced, as reported in [25,26]. To observe the diffraction pattern of fabric Dammann gratings, we put the samples in front of a green point source and use a cam to capture the transmitted light, as shown in Figure 5b. The diffraction patterns of r ence grating and designed grating are manifested in Figure 5c,d, respectively. For gratings, multiple diffraction orders are observed. Nevertheless, for the reference gra the central 0 th order shows much higher efficiency than other orders. Moreover, the hi orders of the reference grating exhibit a greater efficiency than those of the custom grating, and the diffraction pattern of the reference grating is more blurred, which is mainly to LC misalignment and defects. For a well-aligned LC Dammann grating, the signed diffraction orders have more evenly distributed energy. Per our measurem the diffraction efficiency of the customized Dammann gratings for green light and cen 3-by-3 diffraction orders is ~45%, which is close to the simulation results (~55%). Here diffraction efficiency is defined as the power sum of the central 3-by-3 orders (in to orders) divided by the total transmitted power. The uniformity, defined as (Imax − Imin)/ + Imin), where Imax is the maximum intensity and Imin is minimum intensity, is measure ~0.13, which agrees well with the simulation (~0.08).

Maxwellian View Displays With an Enlarged Eyebox
To show that Dammann grating can enlarge the eyebox of a Maxwellian view n eye display, a proof-of-concept breadboard demo is constructed, as schematically sh in Figure 6. A laser beam scanning projector (Sony MP-CL1) is firstly collimated by a (L1). After passing through the fabricated Dammann grating (DG), an eyepiece lens (L used to form the viewpoints. Since our Dammann grating is a 2D grating with mul diffraction orders, the eyebox is enlarged in 2D space by several times. Here we ma focus on the central 3-by-3 views, as numbered in Figure 6.

Maxwellian View Displays With an Enlarged Eyebox
To show that Dammann grating can enlarge the eyebox of a Maxwellian view near-eye display, a proof-of-concept breadboard demo is constructed, as schematically shown in Figure 6. A laser beam scanning projector (Sony MP-CL1) is firstly collimated by a lens (L 1 ). After passing through the fabricated Dammann grating (DG), an eyepiece lens (L 2 ) is used to form the viewpoints. Since our Dammann grating is a 2D grating with multiple diffraction orders, the eyebox is enlarged in 2D space by several times. Here we mainly focus on the central 3-by-3 views, as numbered in Figure 6.
To show that Dammann grating can enlarge the eyebox of a Maxwellian view neareye display, a proof-of-concept breadboard demo is constructed, as schematically shown in Figure 6. A laser beam scanning projector (Sony MP-CL1) is firstly collimated by a lens (L1). After passing through the fabricated Dammann grating (DG), an eyepiece lens (L2) is used to form the viewpoints. Since our Dammann grating is a 2D grating with multiple diffraction orders, the eyebox is enlarged in 2D space by several times. Here we mainly focus on the central 3-by-3 views, as numbered in Figure 6. In our experiment, the optical combiner is a 2-inch non-polarizing beam splitter, and a camera is placed at the focal plane of the eyepiece lens to record the projected images. As demonstrated in Figure 7a, when the camera is shifted in the horizontal direction, different views of a red letter, C, is captured. To show that the Dammann grating is broadband, we also recorded the images of a green letter, A, and a blue letter, B, at view #8, which corresponds to the first diffraction order in the vertical direction. In our experiment, the optical combiner is a 2-inch non-polarizing beam splitter, a a camera is placed at the focal plane of the eyepiece lens to record the projected imag As demonstrated in Figure 7a, when the camera is shifted in the horizontal direction, d ferent views of a red letter, C, is captured. To show that the Dammann grating is broa band, we also recorded the images of a green letter, A, and a blue letter, B, at view # which corresponds to the first diffraction order in the vertical direction. In our feasibility demonstration, the distance between different viewpoints is ~1 mm along both x and y directions in the 2D space. From the geometry of the optical sy tem, the viewpoint separation is closely related to the grating pitch (thus diffraction ang and focal length of the eyepiece. Since here the grating pitch is quite large (~75 μm), t eyepiece needs to have a long focal distance (20 cm) to ensure a reasonable separati distance. In our demo, the field of view (FOV) is defined by the illumination system. Ho ever, if we have an illumination system that provides a large enough illumination ar covering the entire eyepiece, the FOV of the Maxwellian view near-eye display will ul mately depend on the f/# of the eyepiece. In our optical setup, the eyepiece has an f/3 which corresponds to a maximum horizontal FOV of ~14.5° in theory. To enlarge the ma imum FOV, a smaller f/# eyepiece is required, and thus a smaller grating pitch is neede To fabricate a smaller pitch Dammann grating, decreasing the magnification factor of t exposure setup (Figure 3b) is an option. However, the total effective area of the grati will also be shrunk. Other options include using a predesigned photomask instead of SLM or applying a different material other than LC polymer. With an improved fabric tion technique, a Dammann grating with more uniform higher orders (e.g., 3-by-5) will an intriguing choice for further enlarging the eyebox.

Conclusions
We proposed and demonstrated a Maxwellian view near-eye display with an e In our feasibility demonstration, the distance between different viewpoints is~1.4 mm along both x and y directions in the 2D space. From the geometry of the optical system, the viewpoint separation is closely related to the grating pitch (thus diffraction angle) and focal length of the eyepiece. Since here the grating pitch is quite large (~75 µm), the eyepiece needs to have a long focal distance (20 cm) to ensure a reasonable separation distance. In our demo, the field of view (FOV) is defined by the illumination system. However, if we have an illumination system that provides a large enough illumination area covering the entire eyepiece, the FOV of the Maxwellian view near-eye display will ultimately depend on the f /# of the eyepiece. In our optical setup, the eyepiece has an f /3.9, which corresponds to a maximum horizontal FOV of~14.5 • in theory. To enlarge the maximum FOV, a smaller f /# eyepiece is required, and thus a smaller grating pitch is needed. To fabricate a smaller pitch Dammann grating, decreasing the magnification factor of the exposure setup (Figure 3b) is an option. However, the total effective area of the grating will also be shrunk. Other options include using a predesigned photomask instead of an SLM or applying a different material other than LC polymer. With an improved fabrication technique, a Dammann grating with more uniform higher orders (e.g., 3-by-5) will be an intriguing choice for further enlarging the eyebox.

Conclusions
We proposed and demonstrated a Maxwellian view near-eye display with an enlarged eyebox for AR/VR/MR displays. The eyebox expansion is achieved by pupil replication, which is physically realized by inserting a Dammann grating into the optical system. In the experiment, a customized 3-by-3 Dammann grating was fabricated using patterned LC polymers which achieved good efficiency and high brightness uniformity. Through constructing a Maxwellian view display breadboard, an enlarged eyebox and full color operation are proven. To further enlarge FOV, a smaller pitch Dammann grating is desired. Our work shows a very promising means of eyebox expansion in Maxwellian view display while maintaining full-color operation, simple system configuration, compactness, and lightweight.