1. Introduction

1. Introduction

People have always needed to communicate. Since the times when the only way to send a message with important information was to send a runner with it, mankind has made spectacular progress with data transfer. Within just a few centuries we got to the Information Age ^[1][2][1,2], in which globalization has become a reality. Nowadays, we cannot imagine living in a world without the Internet, which is the most popular source for acquiring knowledge and a medium of information exchange. Thanks to that we can send cross-continental messages within just a few seconds, navigate without physical on-paper maps, participate in distance learning, or do shopping via a smartphone, but that is not the end. In this amazing, electronic era we may explore the universe without any telescope or even consult with a medical doctor without leaving the house. The latter has become extremely important in light of the COVID-19 pandemic, especially during the lockdowns.

Despite the spectacular progress in data transfer, people expect communication to be even faster. The more data we send or receive, the more efficient data transfer needs to be. Broadband Internet, i.e., high-speed public connectivity with a data transfer rate of at least 256 Kbit/s or more in one or both directions, is unavailable in many places and is becoming one of the most impactful problems in the modern world [3]. In some conditions like dense urban development, where the installation of optical fiber lines generates significant costs ^[4][5][6][4–6], access to wireless Internet is very popular. Wireless communication became a solution in places where the installation of fiber optic cables may be difficult or even impossible, like in areas across a road or behind water tanks, or in places of special architectural importance (e.g., historic city districts), or in national parks ^[7][8][9][7–9]. This type of data transfer has advantages such as a lower development cost, affordability of the network topology design and implementation, and flexible maintenance of operating networks, a list of benefits not found in wired communications. It has not been a long time since the inception of the first generation of wireless networks, but today’s solutions have evolved a lot.

In the last century, a deep need for fast data transfer brought about microwave links, which were a mode of data transmission via electromagnetic radiation with wavelengths between 1 mm and 1 m [10]. The basics of that technology were quite simple. When the microwave radiation reaches the conducting material, like a copper wire, electron movement occurs, leading to the flow of electric current. This technology was very popular for data transfer like radio, TV, cell phone communication, or even radars [11]. Regarding data transfer technologies, microwaves have a huge advantage, which is the fact that they go directly through space, reaching their destination without bending their signal. They also do not reflect from the ionosphere, instead of passing through it, so they can be sent from satellites or local transmitters to any point on Earth. However, maintaining such links is becoming more and more difficult due to the saturation of radio frequencies in large cities, their sensitivity to interference, and the high risk of “leakage” of confidential data. Moreover, concerns about high license fees for frequency bands and negative health effects started limiting their wide application. The last is due to the physical effects of standing behind microwave radiation. These types of electromagnetic waves cause the vibration of different molecules like water, leading to their rotation, resulting in friction between them, which is followed by a temperature rise. Of course, that behavior of matter depends on the frequency of the generated electromagnetic wave. For example, the microwave that heats food operates at frequencies of a few GHz, while it has completely different frequencies when data are transmitted. On the other hand, microwave data links use different frequencies, and their influence on humans is far smaller. An example of this can be an insufficient bandwidth, affecting the transmission of large packets of data such as high-resolution videos from teleconferences or the monitoring of closed-circuit television cameras.

The deep need for faster and more efficient data transfer gave us newer technologies without the above-mentioned disadvantages. Optical Wireless Links, also called Free-Space Optics (FSO), are devoid of many of the limitations possessed by microwave links ^[12][13][12,13]. FSO is a wireless optical communication technology that uses the emission of optical radiation in an open space to transmit data between two points without obstructing the line of sight between them [14]. Its basic ingredients are transmitters, such as lasers or light-emitting diodes, and signal receivers, like photodetectors. Figure 1 presents the schematic image of such communication between two points placed on two skyscrapers, while Figure 2 presents a connection between other places. FSO is a relatively new technology, but it shows a lot of promise, as modern-day systems enable short-range data transmission up to 8 km with a high capacity reaching up to 100 Gb/s [15]. Such systems are bidirectional due to the optical transceivers at both ends of the link. Both transceivers are connected to a data source, such as a computer with a modem.

Communication systems in open space like air or the vacuum of outer space require the use of appropriate sources of optical radiation. When selecting them, the following parameters should be considered: wavelength range, power of the emitted radiation, and compatibility of cooperation with electronic modulating systems [16]. The wavelength range of the radiation in the FSO communication system is primarily determined by the transmission properties of the medium in which the signal is transferred, like the atmosphere. This technology is very sensitive to the type of climate and the weather, including physical phenomena [17]. Another related issue is ensuring safety for both users of the FSO network and outsiders ^[18][19][18,19], as this limits both the power and frequency of light emitters in the FSO.

Figure 1. Schematic image of a Free-space Optical Communication link between two nearby skyscrapers, serving e.g., to create a LAN-to-LAN connection between A and B points.

Figure 2. Schematic image of Optical Communication links between different objects. Data transmitted on a narrow beam of laser light is marked in red.

2. Historical Background

2. Historical Background

The first long-distance messages were sent via a runner to warn of an invasion of some other danger, but that was too often too slow. To increase the speed of physical data transfer, people started to send messages by air, via pigeons and other birds. In some tribes in Africa, messages were sent by special instruments, called talking drums, while in North America some Indian tribes sent messages using smoke signals. This allowed for nearly real-time communication over medium distances. Even in the late 16th century ships used that way of signaling by employing coded flags. These systems were used in limited geographic areas, but they evolved over the centuries and developed into the technology that we know today.

The beginning of optical communication dates back to antiquity ^[20][21][20,21]. The past civilizations used mirrors, fire beacons, or smoke signals for data transfer, in very low volumes [22]. In Ancient Greece, torch-based signaling systems were made by Cleoxenus, Democleitus, and Polybius [23]. In 1672, the first acoustic telephone transferring a signal over a wire was demonstrated by Robert Hooke. The real breakthrough in the transmission of information took place in 1792 when Claude Chappe presented the idea of transmitting mechanically coded messages over long distances [24]. For this purpose, a network of special semaphores was developed. The first practical electric telegraph was invented by the Russian Baron Schilling in 1823 [25]. That invention was in use during the French Revolution, connecting the French Army and Lille headquarters in Paris. In this way, the first wireless solar telegraph (heliograph) was invented. Figure 3 shows a scheme of the heliograph. The first application of Chappe’s optical telegraph took place between Paris and Lille in July 1794, with the cities being located about 200 km apart. The following century changed telecommunication, bringing about the discovery of electromagnetism by Hans Christian Oersted in 1819 [26].

Some years later, the optical telegraph network expanded throughout Europe [27]. The light served as a medium by which it was possible to make encoded signals visible so that they could be intercepted by relay stations. In 1835, the single-wire telegraph system was developed, and electrical communications throughout the world started. Within just two years, Samuel Morse demonstrated a device sending short and long electric pulses as dots and dashes. The transmission of Morse-coded signals was fast and reliable, and, in fact, variances of this system are still in use [28].

During the Second World War, the Germans used the optical Morse code transmitter Blinkgerät, which allowed for communication over distances of about 4 km during the day and 8 km at night [29]. This was possible thanks to the use of red optical filters, which made communications nearly undetectable. The modern-day Air Traffic Control towers have special devices intended to emit multicolor light in case of radio system failures, and all the pilots know the special procedures to navigate using those lights. The next step on the path to modern communication systems was Alexander Graham Bell’s invention [30], which allowed for voice transmission over long distances. In 1880, he constructed a system for light communication called a photophone. To transfer the conversations at a distance, he used sunlight reflected from a tiny mirror, vibrating under the influence of the voice. The speech was passed through the atmosphere to the receiver using light. There, the modulated solar radiation was converted into an electrical signal in a selenium photocell that was connected to the headphones. Even though this system was never widely used, it was a good proof of concept for the FSO communication systems.

Figure 3.

A scheme of a heliograph.

The invention of artificial electric light sources made it possible to build simple optical telecommunication systems, such as: flashing signal lamps for ship-to-ship communication, ship-to-shore communication, car direction indicators, etc. [31]. These systems had a low efficiency of information transmission. In 1954, in fact, masers, microwave amplification by stimulated emission of radiation, was developed [32]. Four years later, the same team behind masers introduced lasers (Light Amplification by Stimulated Emission of Radiation) as an efficient source of light [33], a these inventions radically increased the efficiency of data transmission [34].

In the mid-1960s, NASA began experimenting with the use of a laser as a communication tool between Earth and space [35]. The first articles on FSO were published in Berlin in 1968 by Ph. D. Erhard Kube, considered to be the father of FSO [36]. The first commercial systems with a capacity of 100 kb/s to 34 Mb/s were published in 1985. In 1999, lines with a capacity of 100–155 Mb/s were developed, and a little later 622 Mb/s data rates were obtained. Currently, capacities of up to 100 Gb/s are achieved ^[37][38][37,38]. In the ‘90s, the wireless revolution began [39].

3. FSO Communication System Constructions

3. FSO Communication System Constructions

The general idea of Free-Space Optics relies on the transmission of invisible, eye-safe light beams. They are transmitted by a laser with light focused onto a highly sensitive photon detector, which serves as a receiver, equipped with a telescopic lens. In fact, the FSO operation is somewhat similar to an infrared TV remote controller. Free-Space Optical links have quite a simple construction, typically consisting of two identical heads enabling duplex data transmission, as shown in Figure 4. These heads are connected via interfaces directly to computers or with a telecommunications network. Physically, these connections are made by fiber optic cables (single and multimode) or Bayonet Neill–Concelman British Naval Connector/Spanning-Tree Protocol (BNC/STP) coaxial cables. BNC connects the computer with the coaxial cable. Generally, BNC is a commonly used plug and socket for audio, video, and networking applications that provides a tight connection.

Figure 4. The scheme of the data transmission via Free Space Optics () technology between two heads.

The block diagram of the transceiver head of a typical FSO link is presented in Figure 5. It includes two main blocks: a transmitter and a receiver of the optical radiation. The source of the optical radiation may be a light-emitting diode, a semiconductor laser, or several lasers [40]. LEDs and semiconductor lasers are used in wireless optical links for short distances (e.g., inside buildings) [41]. On the other hand, FSO links for longer distances mainly use vertical-cavity surface-emitting lasers [42].

Figure 5.

Block diagram of the FSO system.

Lasers provide more power and faster transmission speeds than LEDs [43]. The advantage of surface radiating lasers, compared to classic edge lasers, is the symmetrical spatial characteristic of the radiation.

The data transmission speed on the FSO link is strictly defined by the manufacturer of a given device. The telecommunications protocol is selected depending on the data stream transmission rate; for example, Non-Return-to-Zero (NRZ) and Return-to-Zero (RZ) modulations are used in FSO links ^[44][45][46][44–46].

The optical signal generated by the radiation source is spatially formed by a transmitting lens that creates a beam of radiation with a defined diameter. In commercial systems, the beam divergence angle is between 2 and 10 mrad. Beams with a small divergence angle can only be used in FSO systems equipped with beam targeting and stabilization systems. In simpler solutions, beams with a greater divergence angle are used. This type of solution facilitates the adjustment of the system and enables operation during vibrations of the supporting structure and when the refraction of the atmosphere is changing (e.g., due to a variable temperature or air density). A large advantage of this simplicity is also the reduction of costs of the FSO setup and maintenance. However, the divergence of the beam means that the beam spreads out quicker and hence loses power at a distance, meaning that FSO communication using such a beam is limited in range.

The existence of beam divergence causes the diameter of the optical radiation beam to increase with an increasing distance from the source. The power density distribution, in the plane that is perpendicular to the radiation propagation direction, is usually described by the Gaussian distribution. This beam creates an illuminated area in the receiver plane, with an area generally much larger than the effective receiving area. This results in a radiation power loss resulting from the ratio of these surfaces. The atmosphere causes an additional power loss because it absorbs and scatters the transmitted radiation.

The power of radiation reaching the receiver can be determined from the following formula [47]:

(1)

where P_trans is the radiation power emitted by the transmitter, D_rec is the diameter of the receiver optics, R is the distance between the transmitter and receiver, Θ is the beam divergence angle, and τ is the atmospheric transmission coefficient.

For the FSO link to operate with an acceptable bit error rate, the P_rec power must be higher than the noise. Having the defined minimum received power P_recmin, the link range can be determined from the Formula (1):

(2)

Thus, a formed and modulated optical signal reaches the opposite optical radiation receiver, which consists of a receiving lens, an optical filter, a photodiode with a power supply and cooling system, a low-noise preamplifier, and a signal processing system.

The optical system is used to focus the radiation onto the surface of the detector (avalanche or pin photodiode). For larger surfaces of the optical system, an optical signal with a higher intensity is obtained. The use of optical systems with larger surfaces is advantageous due to the possibility of using photodiodes with smaller active surfaces and due to the mitigation of the effect of photon flux fluctuation (scintillation). With a larger aperture of the receiving system, “aperture averaging” of the photon flux fluctuation also takes place. With a sufficiently large aperture, the fluctuating beam is within the lens surface, so the fluctuations will be averaged according to:

(3)

Formula (3) shows that the diameter of the lens should match the planned range of the link on a given wavelength. Thus, for a link with a range of 1 km, λ = 10 µm, the diameter of the receiving lens should be less than 10 cm. The use of a receiving lens with a larger diameter will increase the weight of the FSO head and its cost, while not bringing any large benefits to the data transmission rate.

In addition to the useful signal, the background radiation reaches the receiver of the FSO system, causing an increase in noise. As a consequence, the ratio of the signal power to noise power decreases [48]. The power of the background radiation reaching the optical system of the receiver depends on the field of view of the lens and its active surface (aperture). To improve the ratio of the signal power to the noise power, the receiver is equipped with optical filters, which narrow its spectral range down to the ∆λ band covering the transmitted signal band. Another technique used for the reduction of noise is the direct isolation of noise sources. For example, the FSO receiver set up in the shade will be protected from noise-inducing sunlight, which is especially prominent in the near-infrared band.

In the signal processing circuit, the received signal is amplified, demodulated, and then forwarded to the interface.

FSO transceivers are placed on masts, buildings, and other structural elements, so they are susceptible to strong gusts of wind. To avoid a break in communication, multibeam systems, or systems for directing and stabilizing the position of the laser beam (so-called Automatic Tracking (AT) systems) are used [49]. Using an AT system, the FSO head changes its position to search for the strongest possible signal from the transmitter. For this purpose, photoreceivers with position-sensing diode detectors and other special articulations are used to enable the positioning of the head in three planes. This is of particular importance in portable FSO systems [50].

In FSO links, systems for heating the transmitter/receiver optics can be used [51]. The use of these solutions allows the devices to operate in a wider temperature range, e.g., from −40 °C to 70 °C, and prevents the frosting of the optical systems or the dewing of the lenses.

In Table 1, the parameters of the FSO systems that are commercially available are presented.

Table 1.

Summary of the basic commercial FSO system parameters.

In the receiving circuits for some of the FSO links, special solutions may be used to regenerate the shape of the impulse waveforms. This regeneration restores the signal to its original power (Reamplifing), and restores the shape of the impulse (Reshaping) and the time relations (Retiming) by resynchronizing the local clock (resynchronization) ^[52][56].

4. Laser Wavelengths Versus FSO Links

4. Laser Wavelengths Versus FSO Links

A huge effort has been made to understand the physical phenomena related to the propagation of optical radiation in the Earth’s atmosphere ^{[53][54][55][56][57][58][59][60][61][62][63][64][65][66][67][68][69][70][71]}[57–75]. Most of the conducted research focuses on the phenomena related to the absorption and scattering of radiation by atoms and molecules that make up the atmosphere, as well as by natural and artificial pollutants: fog, rain, smoke, pollen, and dust. Indeed, the presence of rain and snow can influence the FSO links ^[72][76], while fog and water vapor droplets significantly lower data transmission efficiency, especially in the tropics ^[73][77]. The presence of water vapor molecules in the air contributes to the absorption of some light particles (photons) within the light beam due to absorption, refraction, and scattering. This causes an overall loss in power density in the received signals. This is similar to the impact that rain-fading has on Radio Frequency (RF) wireless systems, which contributes to signal attenuation. FSO may also be temporarily blocked by moving objects such as flying birds, Unmanned Aerial Vehicles (UAVs), or aircraft. Permanent blocking may also be caused by stationary objects such as trees or tall buildings ^[74][78].

Since the physics of the atmosphere cannot be changed, the wavelengths of the lasers used in FSO are selected to operate in so-called “atmospheric transmission windows”. In Figure 6, an example of the characteristics of the atmosphere transmission coefficient for a distance of 1 km is presented. The spectral ranges in which the atmosphere has relatively low absorption of radiation are noticeable. Commercial systems mainly use spectral ranges corresponding to transmission windows of around 0.8 µm and 1.5 µm.

The wavelength of the laser radiation used in FSO links depends on the transmission properties of the atmosphere, particularly fog, as well as the availability and parameters of the lasers ^[75][79]. The attenuation is classified into three groups: Rayleigh scattering (molecule scattering, when the molecule is smaller than the light wavelength), Mie scattering (aerosol scattering, when the size of the molecule is comparable to the wavelength), and nonselective scattering (geometric scattering, when the size of the molecule is larger than wavelength size) ^[76][80]. Since some attenuation processes strongly depend on the wavelength (Rayleigh scattering from air molecules), the proposed choice of wavelength is highly important. It is known that the attenuation is much greater for shorter wavelengths in the case of scattering. In fact, it varies inversely to the fourth power of the wavelength ^[77][81]. Fog causes the Mie scattering, larger particles of snow cause the geometric scattering (having similar effects to the Rayleigh scattering), while rainfall contributes to nonselective scattering ^[78][82]. Other phenomena that may affect transmission efficiency are smoke ^[79][83], sandstorms ^[80][84], and clouds ^[81][85].

Figure 6. Atmospheric transmission spectrum up to 14 μm showing the wavelength regions where particular molecules absorb the electromagnetic wave.

In addition to physical assessments, other media should also be considered when selecting the type of laser ^[82][86]. For a wavelength range of 780–880 nm, cost-effective and reliable lasers with very good parameters as well as detectors, which are used in consumer devices, are easily available. Silicon pin and avalanche photodiodes, LEDs, semiconductor laser diodes, and Vertical-Cavity Surface-Emitting Lasers (VCSEL) are used to work at these wavelengths ^[83][87]. Within a wavelength range of 1520–1600 nm, both sources and detectors of optical radiation are also readily available. In this band, semiconductor lasers made of Indium Gallium Arsenide (InGaAs) are used. Although 1550-nm lasers were developed for fiber optic connectivity, they have also found application in FSO links. For the detection of optical radiation in this wavelength range, PIN (P-type, Intrinsic, N-type semiconductor) and Avalanche Photodiode (APD) photodiodes are made of InGaAs are mainly used ^[84][88]. Currently, research is being conducted on the use of Quantum Cascade Lasers (QCLs) [89,90] in optical communication systems in the range of 10–12 μm ^[85][91]. Currently, there are no commercially available links operating at this wavelength range.

5. FSO and Safety Concerns for Humans

5. FSO and Safety Concerns for Humans

One of the most important issues relating to the use of FSO links is ensuring an appropriate level of eye safety. This is especially important not only during the link alignment, when technicians use telescopes or binoculars to look at the incoming beam but also during the ordinary operation of the FSO when unauthorized people could cross the laser path by accident. The definition of radiation that is safe for humans is included in the international standard IEC 60825 ^[86][92]. Accordingly, the intensity of laser radiation to which people may be exposed without suffering any harmful effects determines the time of the maximum permissible exposure. It depends on the wavelength of the radiation, the pulse duration, the type of tissue exposed to laser radiation, and the dimensions of the image on the retina (for wavelengths from 400 nm to 1400 nm). The main eye hazard from laser radiation is damage to the eye’s retina ^[87][93]. Burns or damages caused by the laser may lead to permanent or temporary loss of vision, depending on the exposure time. Radiation in the wavelength range above 1400 nm, as well as below 400 nm, is strongly absorbed by tissues, and therefore it does not penetrate the eye and does not damage the retina. The introduced regulations concerning the classification of devices equipped with a laser are based on criteria of the wavelength and power density of the incident laser radiation. FSO links should meet the requirements of class 1, and with optical devices, they should meet those of class 1M.

Conducted research shows that, for FSO systems operating with wavelengths of 1550 nm and 800 nm, the permissible power densities are 100 mW/cm² and 2.0 mW/cm², respectively [94]. Thus, for a transmitting lens with a diameter of 100 mm, the laser power can be increased to 160 mW for λ = 800 nm and up to 8 W for λ = 1550 nm. Thus, at a wavelength of 1550 nm, radiation can be emitted with 50 times more power than in the case of radiation with a wavelength of 800 nm. Due to eye safety, it is reasonable to use radiation sources in the far-infrared range in FSO systems. Naturally, visible light or ultraviolet links are not employed, as they carry a higher energy per photon, making them more dangerous. An additional issue to consider with visible-light-based systems is the fact that, due to the scattering of light from laser beams, beams could be visible to naked eyes during nighttime.

6. FSO Advantages and Disadvantages

6. FSO Advantages and Disadvantages

Free-Space Optical Communication is the answer to the worldwide demand for broadband communications offering flexible network connections ^[88][95]. FSO systems are more secure than RF or other wireless-based transmission systems since it is impossible to detect laser beams with spectrum analyzers or RF meters. It is difficult or even impossible to intercept the data transmission, as laser beams are narrow and invisible to the naked eye. Moreover, the information can be transmitted over an encrypted connection, which contributes significantly to increasing the security level ^[89][96]. FSO bridges the gaps in existing high-data-rate communication networks. Its ease of installation and high throughput with relatively low investment outlays make it a rapidly deployable mobile wireless communication infrastructure ^[90][97]. Freedom of licensing (no licenses are required) means that there are no administrative difficulties related to their installation ^[91][98]. Another FSO advantage includes a very low bit error rate, while extremely narrow laser beams ensure that there is almost no practical limit to the number of separate FSO links that can be installed in a given location, which is in direct contrast to omnidirectional RF links. Moreover, due to the narrow beam and easy supervision of interference in the beam, FSO links ensure high resistance to eavesdropping. The transmitted data are inaccessible to unauthorized system recipients, and the active methods of notification about any attempt to join the link, supported by appropriate transmission protocols, ensure a relatively high degree of transmitted data confidentiality ^[92][99]. FSO is also, by definition, a low-latency technology ^[93][100]. In comparison to fiber optics, there is about a 40 percent reduction in latency, as the speed of light in air is about 40 percent higher than in a fiber cable. Moreover, the direct Line of Sight path between two endpoints is shorter than any curved path taken by a fiber-optic cable.

FSO links are comparable to radio ones in terms of the transmission medium; however, they exceed them in terms of bandwidth, operating costs, and installation speed. They provide ranges of up to several kilometers ^[94][101]. Hence, they can be used in crises and military communication systems. It should also be emphasized that the return on investment costs is very fast in comparison to the cost of building a fiber-optic line connecting buildings that are separated by, e.g., 1000 m.

As was mentioned in the “Laser wavelengths used in the FSO links” section, the main phenomena that disrupt FSO communication are rain, which absorbs radiation, and smoke/haze/fog-induced Mie scattering. Disruptions are also caused by Rayleigh scattering and photon absorption, snow, scintillations (fluctuations in the refractive index), and industrial pollution (smog and particulate matter in 2.5- and 10-micrometer dimensions (PM2.5/PM10)) [20]. High concentrations of carbon dioxide in the air can also cause the absorption of transmitted signals, which is particularly significant for near-infrared links and less so for SWIR band links ^[95][102]. Additionally, even heavy rain and snow enable data transmission, even though they weaken the signal reaching the receiver and lead to an increase in the bit error rate. However, the most dangerous weather phenomenon that can break the connection is fog ^[78][82].

One of the factors that may make the employment of the FSO system impractical occurs when the transceiver heads are oriented east-west, due to the possibility of transmission interference caused by direct solar radiation, especially during sunset/sunrise ^[96][97][103,104]. This applies in particular to 850-nm systems. With a different link setting and the use of nontransparent covers, sunlight does not have a significant effect on the operation of the system.

FSO links have a wide range of applications in different fields, such as connections between Base Transceiver Stations (BTS) of mobile telephony, Local Area Network (LAN-LAN) connections between office buildings with Fast Ethernet or Gigabit Ethernet speeds ^[98][105], confidential communication networks (i.e., financial, medical, and military networks ^[99][106]), temporary connections (e.g., HD image transmission from cameras, large screen connection, Internet access, e.g., during the Olympic Games). Due to its stability and flexibility, FSO is a good solution for building-to-building connectivity. Its use can help solve the last mile problem for connections at fiber speeds ^[100][101][107,108]. FSO enables the quick rebuilding of connections after damage and disasters. Moreover, it can serve as an additional backup for fiber-optic networks, and it can complement other wireless technologies.

FSO systems also have their drawbacks and limitations. As was already mentioned, the spreading loss is high, and there is atmospheric loss resulting from water and carbon dioxide molecules. The power consumption is higher than for typical RF links. The transmitter and receiver should be in the line of sight, so there may be significant restrictions on the location of their installation because the transmitter could get blocked due to trees, buildings, etc. Furthermore, birds and scintillation cause beam interruptions. High-powered lasers may not be safe for bystanders, and the installation must be performed by qualified personnel. The costs of the system and its installation are also a big limitation, as the cost of equipment could be between $3000 and $10,000. It is also worth mentioning that the laser diodes used in FSO transceivers have a limited life before they fail, typically about 7–8 years, in comparison to radio links, which can last much longer.

7. The Communication Networks in the Future

7. The Communication Networks in the Future

The crucial issue in Free-Space Communication is to expand the maximum usable distance between transceivers ^[102]. In Figure 7, FSO types are presented according to their maximum operational range. In the nearest future, the communication network infrastructure must adjust to the fifth-generation (5G) ^[103][104] and the sixth-generation (6G) standards ^[105][106]. This is connected with the designing and implementation of high-speed detectors. The main difficulty is the effective collection of the data-carrying optical beam. Some advances were made by the Facebook Team, including the use of fluorescent materials to collect and focus the light into a ti

The crucial issue in Free-Space Communication is to expand the maximum usable distance between transceivers [109]. In Figure 7, FSO types are presented according to their maximum operational range. In the nearest future, the communication network infrastructure must adjust to the fifth-generation (5G) [1110,111] and the sixth-generation (6G) standards [112,113]. This is connected with the designing and implementation of high-speed detectors. The main difficulty is the effective collection of the data-carrying optical beam. Some advances were made by the Facebook Team, including the use of fluorescent materials to collect and focus the light into a ti

ny optical detector ^[107][114].

Figure 7.

Classification of FSO systems based on their coverage.

In long-range FSO, Deep-Space Optical Communications (DSOC) will take high bandwidth communications to the next level ^[108][115,116]. They aim to provide high bandwidth optical downlinks from outside cis-lunar space. NASA also funded a Deep-Space Optical Terminals (DOT) project to develop a tool that allows live High Definition (HD) video, telepresence, and human exploration beyond cis-lunar space. The implementation of this system is expected to enable a ten-fold or even 100-fold increase in data returns compared to present Radio Frequency (RF) space communications.

8. Conclusions

8. Conclusions

The need to improve data transfer drives the research and application of new technologies. Because approaches based on electric cables and optical fibers have many limitations, cable-free technology was developed. One of the representatives of wireless connections is Free Space Optics, which is based on the application of a laser for communication. Currently, FSO links operate using lasers with wavelengths of 800–900 nm and 1.5 µm. Already with these parameters, they revolutionized data transfer. The selection of radiation sources should be done according to two main factors, i.e., the transmission properties of the atmosphere and eye safety. The maximum ranges of these links are determined by the properties of the transmitting and receiving systems, as well as by weather conditions. To increase the FSO’s reliability, several solutions are employed, and among them are such systems as the automatic resumption of packet transmission, appropriate data stream transmission protocols, systems for targeting and stabilizing the position of the laser beam, or automatic gain control systems. Others include using systems to regenerate the shape of impulse waveforms, elements for optical systems heating, adaptive optics systems, and multibeam systems ^[108][117]. Still, the optimal structure of an FSO link depends on a compromise between the price, range, and data transfer rate concerning the intended applications. A practical hint to FSO link designers is that they must specify the requirements for the components of the individual link. This is extremely important to ensure the required transmission speed and the appropriate power of the optical signal. Other essential factors include the selection of an appropriate data stream transmission protocol in the optical channel, and the application of an automatic tracking procedure of the relative positions of the transmitting and receiving systems. A significant drawback of the available systems is the fact that they are sensitive to harsh weather conditions, and in particular to fog.

Author Contributions: Conceptualization, M. Garlinska, and A.Pregowska.; writing—original draft preparation, M.Garlinska, A.Pregowska, M.Osial, K.Masztalerz; writing—review and editing A.Pregowska and M.Garlinska; visualization, M.Osial. All authors have read and agreed to the published version of the manuscript.

Funding: This research received no external funding.

Conflicts of Interest: The authors declare no conflict of interest.

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