We have developed a chip-size light source which can emit arbitrary beam patterns by controlling the spatial phase of the light. We named this device iPMSEL® (integrable Phase Modulating Surface Emitting Lasers, US trademark Reg. No. 5410112).
Recently, LiDAR technology has been attracting much attention in various fields such as collision prevention, surveying, and 3D measurement. LiDAR requires a light source that can scan beam patterns. For this purpose, a suitable light source should satisfy several conditions: small size, lack of mechanical moving structures, electrical control of beam patterns, etc. The size and weight of the light source are particularly important for drones, because the weight and available space in drones are severely limited (see Fig. 1). Small beam-scanning light sources have application possibilities in other fields such as capsule endoscopy (Fig. 2) and natural 3D displays (Fig. 3).

Figure 1 Application of iPMSEL 1 (LiDAR for drone)

Figure 1 Application of iPMSEL 1 (LiDAR for drone)

Figure 3 Application of iPMSEL 3 (3D display)


We have successfully demonstrated a Static-iPMSEL device which emits static arbitrary beam patterns. As shown in Fig. 4, it can emit designated arbitrary beam patterns from a needle-size chip. Even though the beam pattern is static, the potential applications of this technology include 3D measurement and indication such as head-up display. As an example of 3D measurement, we can measure a 3D shape by projecting beam patterns such as multi dot, fringe, and mesh patterns onto the object, then taking pictures, and calculating the position from the distortion of the projecting beam patterns (see Fig. 5, left). If the light source is miniaturized into a needle-size chip, a portable 3D measurement system can also be possible (see Fig. 5, right). We also demonstrated large-scale multi-dot beam patterns of more than 10,000 points which is useful to 3D measurement (see Fig. 6). 3D measurement systems are in high demand for facial recognition and 3D modeling in mobile phones. We therefore believe that Static-iPMSEL can be used for these purposes.
In addition to developing the Static-iPMSEL and Arrayed-iPMSEL devices, in which static beam patterns are projected or switched, we are also developing a Dynamic-iPMSEL device, in which arbitrary beam patterns are emitted and controlled dynamically from a chip.

Figure 4 Far field patterns of Static-iPMSELs

Figure 5 Principle of 3D measurement

Figure 6 Large-scale multi-dot beam patterns of Static-iPMSELs

Features of Static-iPMSELs

The schematics of static-iPMSELs compared with those of the conventional technique (a combination of DOEs and VCSELs) are shown in Flg. 7.
Because the size of the static-iPMSELs is one order of magnitude smaller, two orders of denser integration are feasible, enabling us to switch between numbers of patterns that are two orders of magnitude larger than those of the conventional technique from the same area. Note that the beam divergence increases due to the small size. Meanwhile, vertical spot noise beams are not shown in the static-iPMSELs, and we believe that they are suitable for dense integration.

Fig. 7 Schematics of 2D pattern light source

  Conv. (DOE & VCSEL) Static-iPMSEL
Size Several mm × several mm Several hundreds of µm × several hundreds of µm
Beam divergence
Spot noise beam Yes No

*DOE: Diffractive optical element, VCSEL: Vertical cavity surface emitting laser

Operation of the Arrayed-iPMSELs

Future applications

■Natural 3D display
The rays emitted from 3D objects can be reproduced by the pixel arrays which can control the beam pattern arbitrary. This type of mechanism is widely utilized in a “light-field display”. For this purpose, the Dynamic-iPMSEL can be used as the pixel of 3D display in the future. When a natural 3D display is developed and widely spread, it will offer a possibility for a vivid communication between family members and friends who live at a distance from each other, becoming a new indispensable communication tool.


Recently, LiDAR technology is applied in collision prevention of automobiles, surveying, and 3D measurement. Ordinary LiDAR systems are equipped with mechanical beam-scanning units which make the system size large. Development of a chip-size electrical beam-scanning system without mechanical moving structures will lead to a significant reduction of the system’s size and weight. A light source of this kind will be a key device in drones, for example, where the total weight and available space are limited. We believe that iPMSEL will be perfect for such applications.


■Laser scalpel in capsule endoscopy
Medical examination involving endoscopy can be particularly painful. However, a capsule endoscope can mitigate the insertion pain during diagnostic examination. In fact, simultaneous diagnosis and treatment of the affected part in vivo will be possible if the capsule endoscope will be equipped with a laser scalpel which can control beam patterns arbitrary. We think that iPMSEL can be used for this purpose in the future.


■3D measurement
3D shape can be measured by the following simple procedure. Projecting beam patterns such as multi dot, fringe, and mesh patterns onto the object and taking pictures, then calculating the 3D shape from the distortion of the beam pattern. So far, we succeeded to emit such beam patterns from Static-iPMSEL device which emits static arbitrary beam patterns.


Static-iPMSEL device emits characters or even gray scale beam patterns, as shown in Fig. 4. Moreover, the beam patterns can be switched from the chip-scale device, as shown in the video of Arrayed-iPMSEL. Therefore, we think that they can be applied in small head-up displays where the number of beam patterns is limited, or in a chip-scale indicating device which indicates a variety of marks.

Detailed description of the device

In this section, we describe the structure and the operating principle of the Static-iPMSEL. Schematics of the device is shown in Fig. 8. Similar to an ordinary semiconductor laser, the Static-iPMSEL consists of the cladding layers, which confine carriers (electrons and holes) between them, and the active layer, where light is generated by radiative recombination on substrates. In contrast to the ordinary laser diode, the novel phase-modulating layer, where sub µm-scale holes are arranged, is formed near the active layer. Then, what does this layer act as? As shown in the top-view SEM image of the phase-modulating layer in Fig. 8, there are holes which seem to be arranged periodically at first glance. However, the holes are slightly shifted from the periodic lattice point of a square lattice. In fact, the centers of gravity of the holes are rotationally shifted on the circle whose center corresponds to the lattice point O of the square lattice. According to the target beam patterns, the positional shift of each hole is determined by using computer-generated hologram technique.

Figure 8 Structure of iPMSELs

Figure 9 Principle of in-plane resonance in iPMSELs

When currents are injected into the device, the light waves are generated at the active layer due to the radiative recombination and emitted in various directions. Parts of these light waves are coupled to the phase-modulating layers near the active layer.
Then what happens in the phase-modulating layer? Here, we consider a periodic hole array (2D photonic crystal) for simplicity, because the shift of the holes is small and negligible. When the light wave from left side incident to the periodic holes as shown in fig. 9, the light wave is scattered spherically at each hole. Note that the waves scattering from each hole interfere constructively in four directions in Fig. 9 (namely, up, down, left, and right) because the period of the holes corresponds to the wavelength, which results in a 2π-phase shift of the scattering waves at each hole in four directions. This is called “diffraction” in physics. When these four diffracted light waves propagate, they are also diffracted to the same four directions, coupled with each other, and spread over the entire in-plane region. Note that coupling of counter-propagating waves creates standing waves which do not propagate in any direction and oscillate at a stationary position. Therefore, 2D standing waves are formed in the phase-modulating layers. The phase-modulating layer acts as a resonance cavity of the laser because of the standing waves. (“Formation of 2D standing wave”.)

When the period of the hole equals the light wavelength as shown in Fig. 10(a), four in-plane diffracted waves are also diffracted in vertical directions, and plane waves are emitted in vertical directions. Since the plane waves are emitted from a broad area that expands to several hundreds of micrometer, it gives rise to a narrow spot beam whose beam divergence angle is less than 1º.
Next, we explain intuitively what happens in the phase-modulating layers where holes are shifted from periodic arrangement. Since the positional shift of the holes is small, 2D standing waves are still formed while the output beam patterns are changed. Figure 10(b) shows the schematics of the output beam patterns diffracted from the phase-modulating layer. Due to the positional shift of the holes from the periodic position, the vertically diffracted waves proceed/retard locally, so that the wave front is spatially modulated (“spatial modulation of beam patterns”). Based on our matured skills in holography, we can easily design the “spatial phase modulation” for the arbitrary target beam patterns. In summary, the phase-modulating layer forms “2D standing waves” that act as a resonance cavity of the laser and a “spatial phase modulation” of the output beam patterns at the same time. Thus, the Static-iPMSEL device can emit arbitrary beam patterns from a needle-tip size chip.

Figure 10 Principle of phase modulation in iPMSELs


  1. Y. Kurosaka, et al., “Phase-modulating lasers toward on-chip integration,” Scientific Reports 6, 30138 (2016).
  2. Y. Takiguchi, et al., “Principle of beam generation in on-chip 2D beam pattern projecting lasers,” Optics Express 26, 10787-10800 (2018).
  3. K. Hirose, et al., “Removal of surface-normal spot beam from on-chip 2D beam pattern projecting lasers,” Optics Express 26, 29854-29866 (2018).
  4. Y. Kurosaka, et al., "Beam Pattern Projecting On-Chip Lasers at Visible Wavelength," CLEO 2019, SM4N.2, (2019).
  5. K. Hirose et al., “200×200 µm2 structured light source,” Optics Express 28, 37307-37321 (2020).
  6. Y. Kurosaka, et al., “Replication of band structure in an arbitrary wave vector by holographic modulation,” Physical Review B 103, 245310 (2021).

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