Solutions Category: Free Space Solutions

Offset-free mid-infrared frequency comb based on a mode-locked semiconductor laser

Robert Rockmore, Alexandre Laurain, Jerome V. Moloney, and R. Jason Jones

Abstract

We demonstrate a carrier-envelope offset-free frequency comb in the mid-wavelength infrared (MWIR) based on a passively mode-locked vertical external cavity surface emitting laser (VECSEL) operating at a 1.6 GHz repetition rate. The 290 mW output spanning 3.0–3.5 μm is generated through difference frequency generation (DFG) in periodically poled lithium niobate. The VECSEL pulse train is centered at 1030 nm and amplified up to 11 W in a Yb fiber amplifier system. The output is split to generate a second pulse train at 1560 nm through nonlinear broadening in a Si3N4Si3N4 waveguide followed by amplification in an Er gain fiber. DFG between the 1030 and 1560 nm pulse trains results in a coherent and offset-free MWIR frequency comb, verified with optical heterodyne beat note measurements. Active stabilization of the VECSEL repetition rate provides a fully stabilized high repetition rate frequency comb in the MWIR, uniquely suited for applications in molecular spectroscopy.

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Picosecond Pulsed Squeezing in Thin-Film Lithium Niobate Strip-Loaded Waveguides at Telecommunication Wavelengths

Daniel Peace, Alexander Zappacosta, Robert Cernansky, Ben Haylock, Andreas Boes, Arnan Mitchell, Mirko Lobino

Abstract

Achieving high level of pulsed squeezing, in a platform which offers integration and stability, is a key requirement for continuous-variable quantum information processing. Typically highly squeezed states are achieved with narrow band optical cavities and bulk crystals, limiting scalability. Using single-pass parametric down conversion in an integrated optical device, we demonstrate quadrature squeezing of picosecond pulses in a thin-film lithium niobate strip-loaded waveguide. For on-chip peak powers of less than 0.3 W, we measure up to -0.33±0.07 dB of squeezing with an inferred on-chip value of -1.7±0.4 dB. This work highlights the potential of the strip-loaded waveguide platform for broadband squeezing applications and the development of photonic quantum technologies.

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WHITE PAPER: Wavelength Engineering Using Non-Linear Optical Crystals

Non-linear optical crystals

Non-linear optical (NLO) crystals provide an enormously flexible solution for generating new wavelengths from existing, off-the-shelf laser sources. The optical wavelength spectrum is utilized by a large and continually expanding variety of applications, from UV sterilization, quantum networking & computing, visible imaging, telecommunications, environmental sensing, through to terahertz spectroscopy as well as many others. For all of these applications, the light source is a critical component providing the required illumination wavelength, power, linewidth and other key spectral properties.

Although there are a wide variety of commercially available laser sources covering the extended optical spectrum it is still not always possible to find a direct or cost-effective light source for all
applications. It is in the cases where a practical, direct source is not available that wavelength conversion using highly efficient, non-linear optical crystals provides a powerful solution.

WHICH APPLICATIONS?

“PPLN crystals are used in a diverse range of applications from space and defence technologies through to quantum computing. Through our research and the work conducted by our customers we are constantly discovering new applications for our solutions.”
Prof. Corin Gawith, CTO, Covesion

Principle of wavelength conversion

The principle of wavelength conversion using non-linear optical effects has existed for decades and with the developments in laser technology, combined with the discovery of high-quality crystals with large optical non-linearities, the corresponding gains in conversion efficiency have enabled the practical use of NLO crystals in both research and commercial environments. 1,2 One of the most important developments has been the adoption of materials which can be domain engineered enabling quasi-phase matching (QPM) to be used as the method by which the relative phase between the interacting waves is maintained.3

In comparison to more conventional birefringent phase matching (BPM) used in homogeneous materials, micro-structured QPM materials offer the benefits of simple co-linear optical alignment, non critical angular walk-off, access to the largest non-linear coefficients, and a highly flexible design space.

NLO crystals provide a practical solution for the generation of wavelengths that are not readily accessible via direct laser sources.

Domain engineering to support quasi-phase matching (QPM)

Choice of NLO crystal

The choice of NLO crystal for a particular application is driven by the required wavelength, available pump sources and NLO conversion efficiency. Secondary considerations include the required output power, linewidth, operating temperature etc. When considering different crystal materials, lithium niobate (LiNbO3) is a particularly attractive option since it has a very high non-linear coefficient.4

Comparison of effective non-linear coefficients

Lithium niobate is a ferroelectric material in which the domain structure can be inverted by application of an electric field. By applying a spatially patterned electric field, so called periodic poling, a periodic reversal in the in-built polarization can be produced within the crystal. This then enables QPM to be used to access the highest (d33) non-linear coefficient. Doping with 5% MgO significantly increases the optical and photorefractive resistance of the crystal while preserving its high non-linear coefficient. With a higher damage threshold MgO:PPLN becomes suitable for higher power applications.

With its high non-linear coefficient, ability to be periodically poled and broad optical transmission, MgO:PPLN becomes a highly flexible solution for the generation wavelengths from the blue (<400nm) through the mid-IR and beyond (THz). The required wavelength is obtained by tailoring the PPLN crystal design to access the most appropriate non-linear process; SHG, SFG, DFG, etc.

Second order non-linear processes

Non-linear optical processes

Second harmonic generation (SHG), or frequency doubling, is the most commonly used second order non-linear process. In SHG, two input pump photons with the same wavelength λP are combined through a nonlinear process to generate a third photon at λSHG, where, λSHG = λP/2 (or in terms of frequency fSHG = 2fP).

MgO:PPLN SHG crystals can be fabricated with QPM grating periods suitable for a wide range of commercially available pump laser wavelengths from 976 nm to 2100 nm, allowing generation of frequency doubled light between 488nm and 1050nm.

Sum frequency generation (SFG) combines two input photons at λP and λS to generate an output photon at λSFG , where λSFG = (1/ λP + 1/ λS)-1 (or in terms of frequency fSHG = f+ fS).

By combining readily available fixed (e.g. 1550nm) and tunable (e.g. 780/810nm) pump laser sources MgO:PPLN SFG crystals can provide tunable output light between 500-700nm.

Difference frequency generation (DFG) occurs when two input photons at λP and λS are incident on the crystal, the presence of the lower frequency signal photon, λS, stimulates the pump photon, λP, to emit a signal photon λS and idler photon at λi , where λi = (1/ λP – 1/ λS)-1 (or in terms of frequency fi = fP – fS). In this process, two signal photons and one idler photon exit the crystal resulting in an amplified signal field. This is known as optical parametric amplification (OPA). Furthermore, by placing the nonlinear crystal within an optical resonator, also known as an optical parametric oscillator (OPO), the efficiency can be significantly enhanced.

MgO:PPLN DFG crystals can be designed to work with common fixed and tunable pump wavelengths (e.g 1064/1550/775nm) to cover a broad, continuous output tuning range from the near-IR to beyond 4.5μm in the mid-IR.

MgO:PPLN QPM grating design can be further extended to access third-order processes such as third harmonic generation (THG). Although 3rd order efficiency is significantly lower than 2nd order the generation of useful levels of UV light has been demonstrated by 3rd order SFG (1064nm + 532nm ->355nm) in MgO:PPLN. 5

Example non-linear optical (NLO) processes

Real world applications

MgO;PPLN can be readily manufactured into a variety of forms from bulk crystal to waveguide providing both wide application range as well as enhanced conversion efficiency. Wavelength conversion chips, either using bulk crystal or waveguide forms, can then easily be packaged with fiber-coupled input and output – for enhanced ease of use. The combination of a fiber-coupled package together with a high precision temperature controller provides a plug and play wavelength conversion solution.

Waveguide module wavelength conversion solution

Real-world examples showing the benefit of wavelength engineering using PPLN crystals include;

780nm generation from 1560nm source (SHG).

Magneto optical trapping (MOT) of Rb atoms in applications utilizing cold atom interferometry such as gravimetric sensing and atomic clocks.6 In this application COTS telecoms lasers at 1560nm can be efficiently frequency doubled to 780nm, with conversion efficiencies of up to 70% demonstrated for waveguide solutions.7 The combination of off-the-shelf pump laser components together with a frequency doubling crystal provides cost effective generation of both the 780nm power and narrow linewidth required for supporting Rb atom trapping.

Bi-directional conversion of 422nm <-> 1550nm (SFG/DFG).

Quantum networking to facilitate quantum key distribution (QKD). This application requires efficient conversion between the short wavelength, atomic transitions used for trapped-ion qubits and the telecom C-band for low loss fiber transmission. The use of specially designed PPLN crystals has demonstrated both up- and down- conversion at the single photon level between 422nm (Sr+ emission) and 1550nm. This thereby providing a crucial component for the construction of large-scale quantum networks.8

To conclude

In conclusion NLO crystals provide a practical solution for the generation of a wide range of wavelengths that are not readily accessible via direct laser sources. The use of highly efficient materials that can be micro-structured to enable QPM, such as MgO:PPLN, provide a highly flexible product eco-system. As a leading supplier of PPLN-based wavelength conversion products Covesion is able to offer advice on customer specific solutions, as well as technical support in their set-up, use and optimization. With an extensive portfolio of COTS products, as well as custom design capabilities, Covesion is well placed to support the widest range of wavelength conversion applications.

References

  1. Maker et al, Phys. Rev. Lett., 8(1):21–23, 1962
  2. Hum et al, C. R. Physique 8 (2007) 180–198
  3. Armstrong et al, Phys. Rev., 127(6):1918–1939, 1962
  4. M. Houe et al, J. Phys. D Appl. Phys., 28:1747–1763, 1995
  5. Hsu et al, Proc. SPIE 1126412 (2 March 2020)
  6. Devani et al, CEAS Space Journal volume 12, 539–549 (2020)
  7. Berry et al, OSA Continuum, Vol. 2, No. 12, 15 December 2019, 3456
  8. Wright et al, Phys Rev Appl 10, 044012 (2018)

WHITE PAPER: Wavelength Conversion in Harsh Environments

Quantum Timing and Sensing

There is a near term, high priority need for next generation timing and sensing solutions for important applications including:

  • Autonomonous navigation and inertial sensing (for use in GPS denied environments)
  • Gravimetric and magnetic sensing (including earth orbit environmental monitoring and land-based site surveying)

The next generation technology providing these solutions utilizes quantum effects, with a key enabler being the magneto-optical trap based upon the Rubidium atom (Rb-MOT). The Rb-MOT enables “Cold atoms” to be used as ultra-precise atomic clocks and ultra-sensitive sensors for measuring acceleration.1

It is predicted that demand across these and other applications will drive a large increase in the quantum sensing and timing markets. Quantum sensors have a current market size of $260M and are expected to grow to $565M by 2027 (CAGR 16.8%).2

These sensing and timing applications require the quantum technology to be transferred ‘out of the lab’ and to be in a robust form capable of being deployed and operated in remote and harsh environments (land, sea, air or space based).

IUK CASPA project – satellite based environmental sensing

Wavelength Conversion

Periodically poled lithium niobate (PPLN) is a non-linear optical crystal that can be used to change the wavelength of lasers. For quantum applications, PPLN enables off-the-shelf lasers to be converted to atom- or ion-specific wavelengths that are otherwise difficult to obtain. For Rb atom traps, PPLN enables industry-standard 1560nm telecoms lasers to be converted to the 780nm wavelength needed for Rb cooling. This approach is particularly appealing for operation in harsh environments, such as space, as telecoms lasers are reliable, robust, and rated for thousands of hours of operation.

PPLN waveguides offer the further benefit of very high conversion efficiencies of up to 70%3 and can operate up to the Watt level, enabling rapid cycling of Rb sensing measurements.

PPLN waveguide under test

UK Investment

Current global investment in quantum technologies is estimated at more than $20bn per year. Within this the UK has committed to investing £1bn over 10 years. This includes Innovate UK (IUK) funded R&D programs investigating the potential for ruggedization of quantum technologies including the enabling systems and components. Covesion has been an active participant in a number of these projects;

  • QT Assemble – an underpinning program to develop the UK supply chain for quantum-enabling optical products and systems.
  • CASPA – Cold Atom Space Payload. The aim of CASPA was to build a system capable of cold atom trapping Rb atoms autonomously in the space environment. CASPA was the first step to verify the basic concept and gain heritage on the subsystems and overall design of a basic cold atom demonstrator. Covesion supplied the PPLN waveguide chip for integration into the optical subsystem.
  • SNORQL – Space-certified Nonlinear Optics for Rugged Quantum Lasers. The aim of SNORQL was to demonstrate Covesion fiber-coupled, PPLN waveguides in a Rb-MOT and perform trials to assess package performance in simulated environmental conditions (thermal, vibration, shock, radiation) for pre-space qualification.
STFC RAL Space Rb-MOT

“Current global investment in quantum technologies is estimated at more than $20bn per year. Within this the UK has committed to investing £1bn over 10 years.”

PPLN waveguide performance

Three key criteria need to be met in order to demonstrate that PPLN waveguides are a viable solution for wavelength conversion in harsh environments;

  • The waveguide must deliver the required power and conversion efficiency needed by the quantum technology (Rb-MOT)
  • Fiber coupled packaging must be available in order to move the technology out of the lab and provide plug and play system integration
  • The waveguide package must demonstrate long term reliable operation and be able to withstand the environmental conditions it will be exposed to (thermal, vibration, shock, radiation).
PPLN waveguide prior to packaging

Covesion has taken our standard, off-the-shelf, component waveguide package and tested it against these criteria. It should be highlighted that this fibercoupled module was NOT designed to withstand harsh environments and that this work was therefore undertaken to assess its performance and inform the development needed for ruggedization.

Covesion component waveguide module

“By exploiting the quantum properties of cooled and trapped Rubidium atoms, ultra-precise gravity measurements can be taken, which have many potential practical applications.” Tristan Valenzuela, Head of Quantum Sensors, STFC RAL Space.

Lifetime and efficiency testing

The Covesion waveguide module has demonstrated high efficiency wavelength conversion for more than 1000 hours of operation. With an overall second harmonic generation (SHG) conversion efficiency of up to 50% the module delivers the Watt level output at 780nm needed in order to enable rapid cycling of Rb-MOT sensing measurements.

Lifetime testing (>1000 hours operation) – SHG output power variation entirely due to amplifier drift

A key target of the SNORQL project was to deliver 1W SHG output for minimal pump power as a primary requirement for space-based gravimetric sensing.

High conversion efficiency (up to 50% at 2W pump power)

Environmental testing

Environmental testing (thermal, vibration, shock, radiation) has been performed to MIL standards (MIL-STD-883K) to assess the robustness of the waveguide module and the need for further ruggedization.

Overall the module performs well despite not being specifically designed for rugged operation. A summary of the results of the testing are shown in the table, the results are split into 4 package properties; mechanical – refers to the module casing; electrical – refers to the internal electrical connections; optical path – refers to the optical beam path from fiber input to fiber output; waveguide chip – refers to the PPLN waveguide chip. For each property a tick signifies that the package has passed the specific environmental test and a ‘D’ signifies that further work is needed and a development path has been identified.

It should be noted that for all tests the PPLN waveguide chip itself passed with no evidence of damage (breakage, cracking etc) and performed SHG with the same efficiency pre- and post-test. This demonstrates that the underpinning PPLN material technology provides a robust solution to operation in harsh environments.

Vibration test result, SHG output power pre and post exposure to vibration, power variation solely due to optical coupling variation of the test measurement

Both the mechanical and electrical properties of the package also survived all tests, showing that the weak point of the package (unsurprisingly) is the optical path. The optical path was degraded in a number of different ways depending on the test exposure. The fiber-pigtails suffered both thermal and radiation damage however this is easily solvable through the use high temperature and radiation hard optical fiber. Optical coupling of the fiber pigtails on the input and output suffered damage during vibration and shock testing. Improvements to the waveguide and fiber support structure are therefore required. A low risk path to achieving these has been identified via engineering re-design and the use of optimized bonding materials.

D – development path identified

Summary

Covesion’s approach has been to leverage its internal investment through participation in IUK funded collaborations with UK and European partners in the quantum technology community. This has enabled us to develop a route to market for rugged wavelength conversion modules meeting the demands of applications within harsh and hostile environments. These modules are needed to enable the exploitation of key quantum applications including; next generation atomic clocks, ultra-sensitive accelerometers and gravitometers.

An extensive test and development program has been undertaken to extend the use of PPLN, fiber-coupled waveguide modules to harsh environments including space. Environmental testing has shown that with modest further development our existing waveguide package is suitable for ruggedization and a low risk path has been identified to develop rugged modules suitable for operation in harsh environments including space certification.

Acknowledgements

Covesion acknowledge the support of Innovate UK, the UK’s national innovation agency.

References

  1. M. Odstrcil, et al., “Nonlinear ptychographic coherent diffractive imaging,” Optics Express, pp. 20245-20252, 2016.
  2. Hsiang-Yu Lo, et. al, “All-solid-state continuous-wave laser systems for ionization, cooling and quantum state manipulation of beryllium ions, “Applied Physics B, vol 114, pp. 17-25, 2014.
  3. Diviya Devani, et al., “Gravity sensing: cold atom trap onboard a 6U CubeSat,” CEAS Space Journal, vol. 12, p. 539–549, 2020.
  4. Sam A. Berry, et al, “Zn-indiffused diced ridge waveguides in MgO:PPLN generating 1 watt 780 nm SHG at 70% efficiency,” OSA Continuum, vol. 2, no. 12, pp. 3456-3464, 2019.
  5. Thomas A. Wright, et al, “Two-Way Photonic Interface for Linking the Sr+ Transition at 422 nm to the Telecommunication,” Phys. Rev. Applied, vol. 10, p. 044012, 2018.

WHITE PAPER: Non-linear Optical Crystals Used for Quantum Technology

Quantum Technology

Quantum Technology (QT) is an exciting area of science which is already making a difference to our lives. The impact of QT will increase in the coming years and non-linear optical (NLO) crystals will have a key role to play in the commercialisation of the technology. QT is expected to have utility across multiple applications in three primary categories:

  • Sensing and Timing: The extreme sensitivity of quantum systems to environmental influences can be exploited to measure physical properties with more precision.
  • Communications: Attempts to observe a quantum communication channel will irreversibly alter the state of the system in a way that is detectable by the parties exchanging information. A quantum network can distribute entangled photons as ‘keys’ between distant users to ensure that the data is not being intercepted.
  • Computing: Using the principles of superposition and entanglement, significant speedup over classical computers is theoretically possible for some problem types. Quantum Computing promises to revolutionise computing especially where large data sets and complex calculations are involved.

Early products are being commercialised today, but the QT industry is still in its infancy and will require new components and systems from a range of providers creating a stable supply chain currently emerging in the field. Photonics will be at the heart of the supply chain and whether its generating entangled Photon pairs, cooling atoms or generating stable quantum states NLO crystals and components will be key enablers.

In comparison to more conventional birefringent phase matching (BPM) used in homogeneous materials, micro-structured QPM materials offer the benefits of simple co-linear optical alignment, non critical angular walk-off, access to the largest non-linear coefficients, and a highly flexible design space.

Types of Non-linear crystals

MgO doped lithium niobate (MgO:LN)has a well-established wafer supply chain due to the widespread use of the material in other components and it can be periodically poled to increase frequency conversion efficiency. It has the highest nonlinear effective nonlinear coefficient among commercial nonlinear materials and a wide transmission range of 380nm to 5um making it extremely well-suited to high-efficiency frequency conversion of CW and pulse sources.

Potassium Titanyl Phosphate (KTP) has a lower nonlinearity than MgO:LN and is used when higher resistance to photorefractive damage is required. KTP can also be periodically poled to allow improved SHG efficiency at shorter wavelengths but has limited use in the Mid-IR due to a narrower transmission window of 350nm to 4um. KTP also suffers from a supply chain that is not as well established as MgO:LN and thus the material quality has greater variability and is more expensive.

Beta Barium Borate (BBO) and Lithium Borate (LBO) crystals have become popular for generation of wavelengths in the near-UV to blue portions of the spectrum, because their transparency at these short wavelengths is better than KTP and MgO:LN. BBO is transparent down to 190nm and LBO is transparent to 155nm. Both crystals are used in a bulk unpoled configuration, and while BBO has a larger nonlinearity and temperature tuning bandwidth than LBO, LBO has a smaller walk off angle, higher damage threshold, and broader angle and wavelength tuning capabilities. Both crystal types are hampered by a much lower nonlinearity than lithium niobate, but the ability to use large crystals with very high input powers allows both crystal types to be used effectively in larger frequency conversion systems.

The choice of NLO crystal for a particular application is driven by the required wavelength, available pump sources and NLO conversion efficiency and if the application requires significant volumes the cost of material and stability of the supply chain. Other considerations include the required output power, linewidth, operating temperature etc.

When considering different crystal materials, lithium niobate (LiNbO3) is a particularly attractive option since it has a very high non-linear coefficient.1 MgO:LN and KTP are a ferroelectric materials in which the domain structure can be inverted by application of an electric field. By applying a spatially patterned electric field, so called periodic poling, a periodic reversal in the in-built polarization can be produced within the crystal. This then enables Quasi Phase Matching to be used to access the highest (d33) non-linear coefficient. This Technique is not suitable for use with LBO and BBO.

Comparison of effective non-linear coefficients

Non-linear frequency conversion processes

NLO crystals can deliver frequency conversion using a number of different mechanisms which make them a very flexible solution for producing narrow linewidth, high beam quality, stable sources of light across their transmission window. This flexibility combined with readily available commercial sources driven by the telecoms industry make them ideal for wavelengths of interest in QT. The diagram below highlights some target wavelengths that can be obtained for atomic transitions of interest.

The processes include:

Second harmonic generation (SHG), or frequency doubling, is the most commonly used second order non-linear process. In SHG, two input pump photons with the same wavelength λP are combined through a nonlinear process to generate a third photon at λSHG, where, λSHG = λP/2 (or in terms of frequency fSHG = 2fP). NLO SHG crystals can be fabricated with QPM grating periods suitable for a wide range of commercially available pump laser wavelengths from 976nm to 3300nm, allowing generation of frequency doubled light between 488nm and 1550nm.

Sum frequency generation (SFG) combines two input photons at λP and λS to generate an output photon at λSFG , where λSFG = (1/ λP + 1/ λS)-1 (or in terms of frequency fSHG = fP + fS). By combining readily available fixed (e.g. 1550nm) and tunable (e.g. 780/810nm) pump laser sources NLO SFG crystals can provide tunable output light between 500-700nm.

Difference frequency generation (DFG)occurs when two input photons at λand λS are incident on the crystal, the presence of the lower frequency signal photon, λS, stimulates the pump photon, λP, to emit a signal photon λS and idler photon at λi , where λi = (1/ λP – 1/ λS)-1 (or in terms of frequency fi = fP – fS). In this process, two signal photons and one idler photon exit the crystal resulting in an amplified signal field. This is known as optical parametric amplification (OPA). Furthermore, by placing the nonlinear crystal within an optical resonator, also known as an optical parametric oscillator (OPO), the efficiency can be significantly enhanced. NLO DFG crystals can be designed to work with common fixed and tunable pump wavelengths (e.g. 1064/1550/775nm) to cover a broad, continuous output tuning range from the near-IR to beyond 4.5μm in the mid-IR.

Second order non-linear processes

Wavelengths of Interest to Quantum Applications

The special structure of alkali metal atoms is the foundation of precision spectra, laser cooling and trapping of atoms, atom interferometers, atomic frequency standards. Amongst these atoms, Rubidium (Rb), Caesium (Cs), Beryllium (Be), Barium (Ba), Strontium (Sr) have been studied in detail. NLO crystals are most commonly used in quantum optics systems where narrow linewidth lasers are needed to access specific atomic transitions to manipulate and cool atoms and ions where diode lasers do not produce the power, linewidth, beam quality or wavelength required or are not readily available.

NLO crystals are a very attractive option in these systems as they can be precisely designed to give the required output power and wavelength. They also are attractive as they build upon an existing supply chain where pump sources are low cost due to commercially available Telecoms lasers, thus watt level power output at precise wavelengths is readily achievable via NLO crystal wavelength conversion.

The wavelengths generated can either be the target wavelength for the desired atomic transition or an intermediate state which then is further converted by another crystal e.g. the combination of 1051nm and 1550nm in MgO:PPLN gives an output of 626nm which is then doubled to 313nmby BBO.2

Examples of NLO Crystal use in Quantum Applications

Atom Cooling and trapping. Laser cooling and trapping is the technology to get atoms down to near absolute zero, and to confine and support these atoms in the traps. The atoms in their ground state can store the quantum information and long-range interactions between highly excited Rydberg atoms are essential for successful operation of many quantum information protocols in quantum computing.

The high precision and scalable technology offered by atom interferometry enables more sensitive detection of features e.g. smaller size or greater depth. Many atom optics applications favour a high laser power whilst maintaining a narrow linewidth and high spatial beam quality. For example 780nm generation from a 1560nm source (SHG) is required for Magneto optical trapping (MOT) of Rb atoms in applications utilizing cold atom interferometry such as gravimetric sensing and atomic clocks.3

In these application commercial off-the-shelf (COTS) telecoms lasers at 1560nm can be efficiently frequency doubled to 780nm, with conversion efficiencies of up to 70% demonstrated for waveguide solutions4. The combination of COTS pump laser components together with a frequency doubling crystal provides cost effective generation of both the 780nm power and narrow linewidth required for supporting Rb atom trapping.

Quantum Key distribution (QKD). Quantum keys are used in secure transmission of data. It enables two parties to produce a shared random secret key known only to them, which can then be used to encrypt and decrypt messages. Bi-directional conversion of 422nm <-> 1550nm (SFG/DFG) facilitates QKD. This application requires efficient conversion between the short wavelength, atomic transitions used for trapped-ion qubits and the telecom C-band for low loss fiber transmission. The use of specially designed PPLN crystals has demonstrated both up- and down conversion at the single photon level between 422nm (Sr+ emission) and 1550nm. This thereby providing a crucial component for the construction of large-scale quantum networks.5

Quantum networking to facilitate quantum key distribution (QKD). This application requires efficient conversion between the short wavelength, atomic transitions used for trapped-ion qubits and the
telecom C-band for low loss fiber transmission. The use of specially designed PPLN crystals has demonstrated both up- and down- conversion at the single photon level between 422nm (Sr+ emission) and 1550nm. This thereby providing a crucial component for the construction of large-scale quantum networks.

Accessible wavelength range for PPLN based NLO crystals

Conclusion

NLO crystal-based laser systems have been used in many quantum applications. MgO:PPLN crystal has the highest effective non-linear coefficient among commercial NLO crystals and is the crystal of choice for applications in the 380nm to 5μm range, however where very high power (e.g. >3W CW at 532nm) or wavelengths outside the optical range are required KTP, BBO and LBO crystals can be used.

Non-linear frequency generation is an efficient way to get desired output wavelengths with low phase noise, high beam quality and narrow linewidth for QT. As a leading supplier of PPLN-based wavelength conversion products Covesion is able to offer advice on customer specific solutions, as well as technical support in their set-up, use and optimization. With an extensive portfolio of COTS products as shown on the diagram below, as well as having custom design and manufacturing capabilities for nonstock items, Covesion is your ideal partner to support the widest range of wavelength conversion applications.

References

  1. M. Odstrcil, et al., “Nonlinear ptychographic coherent diffractive imaging,” Optics Express, pp. 20245-20252, 2016.
  2. Hsiang-Yu Lo, et. al, “All-solid-state continuous-wave laser systems for ionization, cooling and quantum state manipulation of beryllium ions, “Applied Physics B, vol 114, pp. 17-25, 2014.
  3. Diviya Devani, et al., “Gravity sensing: cold atom trap onboard a 6U CubeSat,” CEAS Space Journal, vol. 12, p. 539–549, 2020.
  4. Sam A. Berry, et al, “Zn-indiffused diced ridge waveguides in MgO:PPLN generating 1 watt 780 nm SHG at 70% efficiency,” OSA Continuum, vol. 2, no. 12, pp. 3456-3464, 2019.
  5. Thomas A. Wright, et al, “Two-Way Photonic Interface for Linking the Sr+ Transition at 422 nm to the Telecommunication,” Phys. Rev. Applied, vol. 10, p. 044012, 2018.

WHITE PAPER: MgO:PPLN Applications

Introduction

Nowadays, scientists are focusing on the development of narrow linewidth, powerful and stable lasers based on compact experimental setups and small footprint components. These lasers are popular for applications such as high resolution spectroscopy, environmental science, optical clocks, fundamental research and quantum technology. Because of its high non-linear coefficient, lithium niobate (LN) is one of the most important crystals, delivering frequency conversion from IR to visible in a basic single-pass and compact configuration. Several different mechanisms, e.g. second harmonic generation, sum frequency generation, spontaneous parametric down conversion, difference frequency generation or optical parametric oscillation, can be used to produce narrow linewidth, high beam quality, stable sources of light across its wide transmission window.

MgO doped periodically poled lithium niobate (MgO:PPLN) is a non-linear optical crystal for high efficiency wavelength conversion in the 400nm-5100nm range. Adding 5% MgO to lithium niobate significantly increases the optical and photorefractive resistance of the crystal while preserving its high nonlinear coefficient. This allows more stable operation at visible wavelengths and lower temperature operation than a similar undoped crystal. MgO:PPLN can be operated at ambient  temperatures and in some cases, without temperature stabilization. With temperatures from ambient up to 200°C, MgO:PPLN offers significantly wider wavelengths operation than undoped PPLN.

MgO doped periodically poled lithium niobate (MgO:PPLN) is a non-linear optical crystal

Applications

Covesion offers PPLN solutions for efficient frequency conversion of lasers allowing users to reach wavelengths that cannot be achieved with conventional solid-state or diode lasers.. MgO:PPLN can be used to:

  • Frequency double a 1064nm laser to 532nm, for use in iodine clocks or seabed surveying equipment1.
  • Convert 1064nm to 3um, used for gas detection or microscopy imaging techniques.
  • Generate a narrow linewidth laser source for targeting specific atomic transitions for atom cooling and trapping applications.

Alternatively, PPLN has often been used to frequency double a high power tuneable 1550nm fiber source as a low cost and compact alternative to the Ti:Sapphire laser. Such a source can be used in microscopy systems for live-cell imaging, or terahertz time-domain spectroscopy where chemical fingerprints can be identified for homeland security applications.

PPLN devices are commonly used for high power mid-IR generation in an optical parametric oscillator. Tuneable mid-IR systems are used in a wide range of microscopy imaging techniques as well as spectroscopic applications for environmental imaging. With pulse energies in excess of 1mJ, these mid-IR sources are also used in the defence industry for laser countermeasures and LIDAR systems.

Nanosecond optical parametric oscillator for mid-IR generation, image courtesy of Elforlight

Terahertz generation

Terahertz (1-10THz) radiation has important applications in our daily life, such as security checks, biomedicine and quality inspection. Due to its strong nonlinearities, high photorefractive damage threshold, and small absorption coefficient in the infrared spectral region, LN is one of the best-suited materials for THz generation, which can be pumped with ultrashort femtosecond pulsed laser or CW sources. Such crystals have been used to generate THz radiation in different ways, for example, optical rectification in periodically poled crystals, as well as phase-matched operation in a terahertz parametric oscillator or in an injection seeded terahertz parametric generator.  MgO:PPLN is a promising candidate because its phase matching condition can be optimised through application specific design of the periodically poled structure. In this case, multi-cycle THz pulses are obtained from MgO:PPLN via the optical rectification effect2. MgO: LN waveguides can also be used for CW THz-DFG, by realizing the phase matching in a non-collinear emission scheme within a LN surface waveguide. Waveguides have the advantage of a reduction in of the area of interacting wave fronts which minimize THz absorption losses3.

Femtosecond lasers

An Optical Frequency Comb is a broad spectrum source composed of equidistant narrow lines. Initially developed for frequency metrology, scientists also use it for spectroscopy over broad spectral bandwidths, of particular relevance to molecules. The spectrum in the visible and near infrared has good overlap with the electronic transitions of optical clocks and alkali atoms, while frequency combs in the mid-IR enable vibrational spectroscopy for molecular detection3. Mid-IR frequency combs are typically generated by nonlinear optics, e.g. difference frequency generation (DFG) and optical parametric oscillation (OPO), providing high average power, high power per comb line and narrow comb linewidth. An efficient version of DFG is to divide the spectrum of an amplified and spectrally broadened femtosecond NIR laser into two portions, which are used as pump and signal for DFG. Researchers have demonstrated a simple and powerful method for generating broadband frequency combs across the 3-5um mid-IR atmospheric window using intrapulse DFG driven by few-cycle pulses with a MgO:PPLN crystal4. Synchronously- pumped OPOs using MgO:PPLN provide another efficient way to transfer fs NIR frequency combs to the mid-IR region5.

Bio-Photonics

Laser-based spectroscopy and microscopy is becoming an essential tool in  biochemical and medical applications. Coherent anti-Stokes Raman Spectroscopy (CARS) is a nonlinear process, not only sensitive to the same vibrational signatures of molecules as seen in Raman spectroscopy, but also employs multiple photons to address the molecular vibrations, and produces a coherent signal, by using a pump and  a probe, causing Stokes waves interact with a sample, generating an anti-Stokes wave that contains information about molecular vibrations6. CARS can also be combined with other nonlinear imaging techniques e.g. two-photon excitation fluorescence microscopy (TPEF) and second harmonic generation (SHG) on a single microscope system using a multi-channel output scheme. Combining these imaging methods has been done via a technique called multimodal-CARS, which can be used in a variety of applications that require structure- and chemical-specific image contrast. Researchers have used MgO:PPLN crystal to build a compact and reliable, tuneable, CW seeded synchronization-free OPA with a robust, commercial pico-second pump laser. Another MgO:PPLN frequency doubling crystal is used to generate visible spectra to excite the CARS anti-Stokes signals. This laser and OPA combination have been shown to be well suited for label-free CARS and concurrent SHG and TPEF microscopy in an epi-detection geometry7.

Multimodal CARS/SHG/TPEF bioimaging with OPA/SHG source

Fluorescence lifetime imaging microscopy (FLIM)is a powerful imaging technique based on the differences in the exponential decay rate of the photon emission of a fluorophore from a sample. FLIM is a useful tool for observing the localization and migration of specific molecules and proteins in cells and tissue. The fluorescence lifetime is determined by the types of fluorescent molecules and the environment surrounding the molecules, it shows little dependence on the concentration of fluorescent molecules, photobleaching, and excitation/ detection efficiency. It’s more quantitative than fluorescence intensity. Researchers have presented scan-less full-field FLIM based on one-to-one correspondence between 2D image pixels and frequency-multiplexed radio frequency signals. Dual-comb optical beats are obtained by using femtosecond laser, PPLN crystal and beam splitter. It will be very useful for rapid quantitative fluorescence image in life science8.

Quantum Optics

“Quantum technology (QT) is an exciting area of science which is already making a difference to our lives.”

The impact of QT will increase in the coming years and Nonlinear Optical (NLO) Crystals will have a key role to play in the commercialization of the Technology. QT is expected to have utility across multiple applications in three primary categories:

MgO:PPLN crystals can deliver frequency conversion using a number of different mechanisms (e.g. second harmonic generation, sum frequency generation, spontaneous parametric down conversion, difference frequency generation, optical parametric amplification, etc.) which makes them a very flexible solution for producing narrow linewidth, high beam quality, stable sources of light across their transmission window.

Laser cooling and trapping is the technique to cool atoms down to near absolute zero, and to confine and support these atoms in the traps. The atoms in their ground state can store quantum information and long-range interactions between highly excited Rydberg atoms are essential for successful operation of many quantum information protocols in quantum computing. The high precision and scalable technology offered by atom interferometry enables more sensitive detection of gravity features e.g. smaller size or greater depth . Many atom optics applications favour high laser power whilst maintaining a narrow linewidth and high spatial beam quality. As an example, 780nm generation from a 1560nm source (SHG) is required for Magneto optical trapping (MOT) of Rb atoms in applications utilizing cold atom interferometry such as gravimetric sensing and atomic clocks9. In these applications commercial off-the-shelf (COTS) telecoms lasers at 1560nm can be efficiently frequency doubled to 780nm, with conversion efficiencies of up to 70% demonstrated for waveguide solutions10. The combination of COTS pump laser components together with a frequency doubling crystal provides cost effective generation of both the 780nm power and narrow linewidth required for supporting Rb atom trapping.

Quantum technology is already delivering on its potential

“By exploiting the quantum properties of cooled and trapped Rubidium atoms, ultra-precise gravity measurements can be taken, which have many potential practical applications.” Tristan Valenzuela, Head of Quantum Sensors, STFC RAL Space.

Quantum keys are used in secure transmission of data. It enables two parties to share a random secret key known only to them, which can then be used to encrypt and decrypt messages. Bi-directional conversion of 422nm ↔ 1550nm (SFG/DFG) facilitates quantum key distribution (QKD). This application requires efficient conversion between the short wavelength, atomic transitions used for trapped-ion qubits and the telecom C-band for low loss fiber transmission. The use of specially designed PPLN crystals has demonstrated both up- and down- conversion at the single photon level between 422nm (Sr+ emission) and 1550nm, thereby providing a crucial component for the construction of large-scale quantum networks11.

Environment Sensing

Environmental monitoring is of great interest because of increased awareness of environmental harm caused by air pollution, caused by human activities in industrial processes. Various international agreements call for limiting and reducing CO2 and other gaseous emissions, Mid-IR contains fundamental vibrational-rotational absorption bands of various gases, which allows remote or local gas analysis of the atmosphere using lasers with suitable wavelengths. These laser sources are widely used in atmospheric pollution monitoring and remote detection using techniques such as differential absorption lidar. Optical parametric oscillators (OPO) via MgO:PPLN crystal are used in the range of 3-5um because of its wide tunability range and narrow linewidth12.

CH4, CO2, CO, NO and H2O can be detected using the 3-5um spectrum

Laser remote sensing is a technique which is widely used in environmental analysis. High-power single frequency laser systems have become attractive because of their high spatial and temporal coherence. Researchers have used MgO:PPLN crystal to produce a high power laser system for use with Rubidium Atom Traps to generate very sensitive gravity measurements. This technology has practical applications in areas such as identifying what infrastructures are hidden under a road before starting civil engineering projects. Rubidium Atoms Traps can also be used for a number of climate monitoring activities such as measuring water tables, remote surveying and ice mass monitoring.

Conclusion

MgO:PPLN is nonlinear optical crystal for high efficiency wavelength conversion in the range of 400nm-5100nm, which allows users to produce narrow linewidth wavelengths difficult and expensive to achieve using conventional sources. Covesion Ltd. has more than 20 years of manufacturing experience delivering PPLN bulk crystals and waveguides to optical research labs and OEMs worldwide. Covesion has patented, innovative approaches to bulk crystal poling and waveguide fabrication which can meet our customers’ needs.

We work with partners worldwide to integrate our crystals and waveguides into a range of scientific instrumentation including optical sources & detectors, frequency combs, frequency convertors, gravitometers, and many more. We design and manufacture PPLN products that can be used in many spectroscopic or environmental science applications. These include narrow-linewidth laser sources for gas spectroscopy applications or picosecond and femtosecond ultrafast laser sources for specific wavelengths in fluorescence spectroscopy. Our products are already successfully integrated into a number of existing systems enabling future research and development into novel applications. Our wide range of bulk crystals and waveguides are commonly used in quantum systems where narrow linewidth lasers are needed to access specific atomic transitions. Covesion PPLN crystals can be used in a range of cold atom applications utilizing Rb, Sr, Be and Ca, as well as: entangled photon generation, sensing & detection, quantum computing and cold atom applications. We also enable users to develop innovative experimental and practical applications. Our team can discuss your requirements and advise on the right solution utilising their unrivalled capabilities for engineering PPLN. This means we can assist with many wavelengths that are applicable to a wide range of pump powers, whether your source is pulsed or CW. If we don’t have a stock item to fit your arrangement, we can custom design crystals and waveguides to meet your specific need.

References

  1. Y. Liao, et al , “Reduction of Scattering Clutters in an Underwater Lidar System by Using an Optical Vortex,” IEEE Photonics Technology Letters , vol. 34, no. 17, pp. 927-930, 2022.
  2. J. Hamazaki, et al., “THz Pulse Generation Emitted From Slant-Stripe-Type PPLN Via Optical Rectification Effect,” OSA Technical Digest, p. cc_6_2, 2019.
  3. A. Schliesser, et al. , “Mid-infrared frequency combs,” Nature Photonics, vol. 6, pp. 440-449, 2012.
  4. A. J. Lind, et al. , “Mid-Infrared Frequency Comb Generation and Spectroscopy with Few-Cycle pulses and x(2) nonlinear optics,” Physical Review Letters , vol. 124, p. 133904, 2020.
  5. M. Vainio, et al., “Fully stabilized mid-infrared frequency comb for high-precision molecular spectroscopy,” Optics Express, vol. 25, p. 4190, 2017.
  6. C. Evans et al. , “Coherent anti-stokes raman scattering microscopy: chemical imaging for biology and medicine,” The Annual Review of Analytical Chemistry , vol. 1, pp. 883-909, 2008.
  7. D. Xu et al. , “Widely-tunable synchronisation-free picosecond laser source for multimodal CARS, SHG, and two-photon microscopy,” Biomedical Optics Express, vol. 12, p. 1010, 2021.
  8. T. Mizuno et al. , “Full-field fluorescence lifetime dual-comb microscopy using spectral mapping and frequency multiplexing of dual-comb optics beats,” Science Advances , vol. 7, 2021.
  9. Diviya Devani, et al., “Gravity sensing: cold atom trap onboard a 6U CubeSat,” CEAS Space Journal, vol. 12, p. 539–549, 202
  10. Sam A. Berry, et al, “Zn-indiffused diced ridge waveguides in MgO:PPLN generating 1 watt 780 nm SHG at 70% efficiency,” OSA Continuum, vol. 2, no. 12, pp. 3456-3464, 2019.
  11. Thomas A. Wright, et al, “Two-Way Photonic Interface for Linking the Sr+ Transition at 422 nm to the Telecommunication,” Phys. Rev. Applied, vol. 10, p. 044012, 2018.
  12. D B Kolker, et. al, “Tunable mid-infrared laser sources for trace-gas analysis,” J. Phys.: Conf. Ser., vol. 2067, 2021.
  13. D. Popa et al. , “Towards Integrated Mid-Infrared Gas Sensors,” Sensors, vol. 19, p. 2076, 2019.

High-power, fiber–laser-based source for magic-wavelength trapping in neutral-atom optical clocks

William J. Ecknera, Aaron W. Young, Nathan Schine, and Adam M. Kaufman

Abstract

We present a continuous-wave, 810 nm laser with watt-level powers. Our system is based on difference-frequency generation of 532 and 1550 nm fiber lasers in a single pass through periodically poled lithium niobate. We measure the broadband spectral noise and relative intensity noise to be compatible with off-resonant dipole trapping of ultracold atoms. Given the large bandwidth of the fiber amplifiers, the output can be optimized for a range of wavelengths, including the strontium clock-magic-wavelength of 813 nm. Furthermore, with the exploration of more appropriate nonlinear crystals, we believe that there is a path toward scaling this proof-of-principle design to many watts of power and that this approach could provide a robust, rack-mountable trapping laser for future use in strontium-based optical clocks.

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A two-way photonic interface for linking Sr+ transition at 422 nm to the telecommunications C-band

Thomas A. Wright, Robert J.A. Francis-Jones, Corin B.E. Gawith, Jonas N. Becker, Patrick M. Ledingham, Peter G.R. Smith, Joshua Nunn, Peter J. Mosley, Benjamin Brecht, Ian A. Walmsley

Abstract

We report a single-stage bi-directional interface capable of linking Sr+ trapped ion qubits in a long-distance quantum network. Our interface converts photons between the Sr+ emission wavelength at 422 nm and the telecoms C-band to enable low-loss transmission over optical fiber. We have achieved both up- and down-conversion at the single photon level with efficiencies of 9.4% and 1.1% respectively. Furthermore we demonstrate noise levels that are low enough to allow for genuine quantum operation in the future.

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Widely-tunable synchronisation-free picosecond laser source for multimodal CARS, SHG, and two-photon microscopy

Duanyang Xu, Sijing Liang, Lin Xu, Konstantinos N. Bourdakos, Peter Johnson, James Read, Jonathan H. V. Price, Sumeet Mahajan, and David J. Richardson

Abstract

We demonstrate a continuous wave (CW) seeded synchronization-free optical parametric amplifier (OPA) pumped by a picosecond, 1 µm laser and show its performance when used as a simple yet powerful source for label-free coherent anti-Stokes Raman scattering (CARS), concurrent second harmonic generation (SHG), and two-photon fluorescence microscopy in an epi-detection geometry. The average power level of above 175 mW, spectral resolution of 8 cm−1, and 2 ps pulse duration are well optimized for CARS microscopy in bio-science and bio-medical imaging systems. Our OPA is a much simpler setup than either the “gold-standard” laser and optical parametric oscillator (OPO) combination traditionally used for CARS imaging, or the more recently developed OPA systems pumped with femtosecond pulses [1]. Rapid and accurate tuning between resonances was achieved by changing the poled channels and temperature of the periodically-poled lithium niobate (PPLN) OPA crystal together with the OPA seed wavelength. The Pump-Stokes frequency detuning range fully covered the C-H stretching band used for the imaging of lipids. By enabling three multiphoton techniques using a compact, synchronization free laser source, our work paves the way for the translation of label-free multi-photon microscopy imaging from biomedical research to an imaging based diagnostic tool for use in the healthcare arena.

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High power, tunable, ultrafast yellow laser using cascaded second harmonic generation of mid-IR Cr2+:ZnS laser in MgO:PPLN crystals

Anirban Ghosh, Deepika Yadav, Ravi Kiran Saripalli, Goutam K. Samanta

Abstract

We report on efficient, two stage single-pass second harmonic generation of ultrafast Cr2+:ZnS laser with spectral bandwidth of 138 nm centered at ~2360 nm and pulse width of ~43 fs at a repetition rate of 80 MHz into tunable yellow radiation across 577 – 589 nm in multi-grating MgO:PPLN crystals. A maximum average output power ~940 mW at 589 nm wavelength with a single-pass conversion efficiency as high as 41% was achieved. The yellow radiation has a spectral bandwidth of 2 nm and pulse-width of ~913 fs in absence of any pulse compression with a time-bandwidth product of 1.58.

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