Simultaneous stimulated Raman scattering second harmonic generation in periodically poled lithium niobate

 

Gail McConnell

Centre for Biophotonics, Strathclyde Institute for Biomedical Sciences, University of Strathclyde, 27 Taylor Street,

Glasgow, G4 0NR, UK.

g.mcconnell@strath.ac.uk

 

Allister I. Ferguson

Department of Physics, University of Strathclyde, 107 Rottenrow, Glasgow G4 0NG, UK.

Text Box: Abstract: Simultaneous stimulated Raman scattering (SRS) and second
harmonic generation (SHG) are demonstrated in periodically poled lithium
niobate (PPLN). Using a simple single-pass geometry, conversion
efficiencies of up to 12% and 19% were observed for the SRS and SHG
processes respectively. By changing the PPLN period interacting with the
photonic crystal fibre based pump source and varying the PPLN
temperature, the SHG signal was measured to be tunable from λ=584 nm to
λ=679 nm. The SRS output spectrum was measured at λ=1583 nm, with a
spectral full-width at half-maximum of λ=85 nm.
 

  

 

 

 

 

 

 

 

 

 

 

 

 


 

1. Introduction

Extending the spectral coverage of stable laser sources is key to improving the range and

efficiency of applications as diverse as optical microscopy, spectroscopy and remote sensing.

For this reason, nonlinear optical frequency conversion methods are often used to create

coherent sources with emission wavelengths that are difficult or impossible to access with

standard laser gain media [1-3]. Stimulated Raman scattering (SRS) is one-such powerful yet

simple example of a nonlinear method that exploits the third-order material response to evoke

an intensity-dependent Raman shift of the input wavelength. This frequency shift to a longer

wavelength increases the spectral range of the existing platform source. We report the

application of periodically poled lithium niobate (PPLN) to perform simultaneous SRS and

second harmonic generation (SHG) to extend the wavelength range of a soliton self frequency

shifted (SSFS) Nd3+:YLF laser. Use of a PPLN crystal provides access to a very high

nonlinear gain coefficient for high efficiency of the SRS and SHG processes. In the simple

single-pass configuration adopted, conversion efficiencies of 19% and 12% were measured

for the SHG and SRS outputs respectively. Changing the interaction period and the

temperature of the PPLN crystal created a SHG signal that was tunable over λ=584 nm to

λ=679 nm. The concurrently generated SRS output spanned a full-width at half-maximum

(FWHM) of λ=85 nm, centred at λ=1583 nm.

 

2. Background

Periodically poled crystals are invaluable media for performing nonlinear optical frequency

conversion as they provide access to high nonlinear coefficients, possess high damage

thresholds and have simple phase-matching requirements [4]. The quasi-phase-matching

(QPM) procedure typically involves applying a high-magnitude electric field in a predetermined

pattern to a ferroelectric material such as lithium niobate, resulting in alternating

polarity domain periods of length Λ, which is twice the coherence length for this process.

After one coherence length, the wave-vector mismatch ∆k is reset to zero by reversing the

sign of the nonlinear coefficient, leading to a constructive conversion process. For the

specific case of periodically poled lithium niobate (PPLN), use of the d33 tensor component in

this arrangement allows second-order nonlinear coefficients of up to 16 pm/V to be accessed

[5]. This is a five-fold increase over the effective nonlinear gain coefficient of bulk lithium

niobate using birefringence phase matching. Furthermore, the acceptance bandwidth for

QPM structures is typically larger than those for conventionally phase-matched devices since

QPM allows the use of the same polarization for the input and generated frequencies [6].

Solid-state nonlinear materials such as PPLN are well-suited to efficiently generating

SRS radiation as the nonlinear gain coefficient is higher than in fluid media due to an increase

in the concentration of Raman scattering centres [7]. Although there are many reports of SRS

in bulk nonlinear materials, reports on SRS in periodically poled materials are currently

limited. Pasiskevicius et al [8] described SRS in an optical parametric oscillator (OPO) based

on periodically poled KTiOPO4 (PPKTP). PPLN has a substantially higher third-order

nonlinear gain coefficient than PPKTP [5, 9] and therefore potentially enables more efficient

SRS. The use of a material with a higher nonlinear gain coefficient also means that more

efficient single-pass SRS can be performed. Application of this more straightforward

experimental strategy circumvents possible stability problems caused by OPO cavity length

tolerances.

In a study by Sidorov et al [10], substantial Raman peaks in bulk lithium niobate were

observed in the X(ZZ)Y orientation. This is the standard orientation adopted in PPLN

crystals, as it provides access to the highest nonlinear coefficient. We therefore employed a

PPLN crystal cut in the X(YY)Z plane as a basis for our observations and study of

simultaneous SRS and SHG in PPLN.

The SRS process is acknowledged to be extremely sensitive to the wavelength of the

pump source [8]. We therefore exploit the SSFS effect in photonic crystal fibre (PCF) to

create a suitable high peak power source for investigating the SRS process in PPLN. The

SSFS occurs when Raman self-pumping of a soliton transfers energy from shorter to longer

wavelengths, as described recently by Reid et al [11] in PCF. The overall effect is a

nonlinearly dependent red-shift of the pulse centre wavelength, creating a soliton-pulsed laser

source emitting at longer wavelengths than the input source.

 

3. Experiment

The experimental arrangement for instigating SRS and SHG in PPLN involved a horizontally

polarised continuous-wave mode-locked Nd3+:YLF laser (Biolight, Coherent) and PCF

serving as the platform source, as shown in Fig. 1. The Nd3+:YLF source comprised a

picosecond-pulsed laser with an externalfiber-grating pulse compressor. The average output

power from the compressor was 680 mW. The emission wavelength of the source from the

compressor was λ=1047 nm with a 6 nm spectral FWHM, measured using a fibre-coupled

spectrometer (Ocean Optics). After compresson, pulses of 400 fs duration were measured

using a second harmonic autocorrelator, corresponding to a time-bandwidth product of 0.68.

Given the source repetition rate of 120 MHz, the peak power of the source was therefore

approximately 14 kW.

 

 

Text Box: Fig. 1. Experimental set-up. The output of a continuous wave mode-locked Nd3+:YLF laser was sent through a half-wave plate into photonic crystal fiber (PCF) using an aspheric lens (A) of focal length f=+8 mm. Using a spherical lens (C) of focal length f=+40mm, the soliton selffrequency shifted output and the residual pump light The fibre output was collimated using another aspheric lens (B) of focal length f=+4.5 mm. was focused into a 6.5 mm long PPLN crystal.
 

  

 

 

 

 

 

 

 


 

 

 

This pump light was propagated through a λ/2 plate that was anti-reflection coated for the

pump wavelength. Rotating the half-wave plate in the set-up and hence changing the state of

the pump light entering the fibre was used to determine the polarization dependence on the

efficiency of the SSFS process. The transmitted light was focused into an 84 cm long section

of photonic crystal fibre (PCF) using an aspheric lens of focal length f=+8 mm with a

numerical aperture of N.A.=0.5. The average power incident on the PCF was measured to be

480 mW. The PCF used in this investigation (Crystal Fibre A/S) had a hexagonal

arrangement of air holes surrounding a 3.5 µm diameter core. The separation between

neighbouring air holes was 1.8 ± 0.2 µm, with a pitch of approximately 0.35. This resulted in

a high non-linearity fibre with a zero-dispersion wavelength of around λ0=800 nm. At the

pump wavelength, the fibre exhibited a low and anomalous dispersion. The transmitted output

from the fibre was collimated using another aspheric lens of f=+4.5 mm focal length lens and

N.A.=0.55. Neither the focusing nor collimating aspheric lenses were anti-reflection coated at

the pump or SSFS wavelengths and therefore contributed to Fresnel losses. The collimated

PCF output was focused using a spherical lens with an anti-reflection coating at λ=1064 nm

of focal length f=+40 mm into a plane-faced PPLN crystal (Crystal Technologies). The spotsize

within the PPLN was approximately 31 µm, matching the theoretically optimum beam

size for second harmonic generation of the SSFS light calculated using the Boyd and

Kleinman method [12]. The uncoated PPLN crystal was 0.5 mm-thick and 6.5 mm-long, and

was cut along the X(ZZ)Y direction to provide access to the highest nonlinear gain

coefficient. The crystal comprised five regular grating periods of Λ = 10 µm to Λ = 12 µm in

0.5 µm increments. This period length was intentionally chosen to maximise SHG of the

SSFS output. The crystal was heated in a custom-built oven with 0.2 °C accuracy to 110 °C

to minimise photorefractive damage observed at lower temperatures [13]. Fast wavelength

changes were made possible by changing the period of the PPLN interacting with the input

beam by translating the crystal relative to the source.

 

 

4. Results

The total average power measured at the PCF output (transmission) was 211 mW, with the

reduction in power attributed to non-optimal and uncoated fibre input coupling optics and

PCF loss. The SSFS average power was measured using two long-wave pass interference

filters with a total transmission of 35% at λ>1135 nm and a calorimeter.

 

 

 

Text Box: Fig. 2. By rotating the half-wave plate prior to the PCF, a weak polarization dependence of the pump polarization on the SSFS power was observed, with a measured decrease in average power of up to 24%.

  

 

 

 

 

 


 

 

 

 

At wavelengths longer than λ=1135 nm, with optimum half-wave plate orientation, up to 56

mW of average power was measured, corresponding to a generated average power of 160

mW of frequency shifted light. A relative average power decrease of up to 24% was

measured when the half-wave plate was rotated through 90ş, as shown in Fig. 2. The

maximum conversion efficiency from pump to SSFS radiation was therefore 24%.

 

 

 

Text Box: Fig. 3. The SSFS optical spectrum transmitted by the PCF (±1 nm wavelength accuracy, linear scale). The pump laser is evident as a small peak at 1047 nm. The SSFS maximum was measured at 1258 nm.

 

 

 

 

 

 

 


 

 

A maximum shift peak at λ=1258 nm with a spectral FWHM of λ=91 nm was measured using

a fibre-coupled spectrometer (Hewlett-Packard). Figure 3 shows an example of the recorded

trace for 160 mW of SSFS radiation. It was noted that when the pulse duration delivered by

the Nd3+:YLF laser was increased by varying the grating spacing in the pulse compressor, the

SSFS spectrum became increasingly narrow. This was not symmetric about the peak

wavelength. Instead, the longer wavelength components of the SSFS spectrum disappeared.

For the remainder of this report, the optimum pulse duration possible from the Nd3+:YLF for

maximum average power SSFS generation was employed.

In order to determine the pulse duration of the SSFS output from the PCF, a collinear

scanning autocorrelator based on two-photon absorption in a biased GaAsP photodiode

(Hamamatsu) was used. Pulses of 220 fs FWHM duration were measured, as shown in Fig. 4.

Assuming a sech2 pulse shape, this indicated pulses of approximately 140 fs duration. From

the spectral and power data, this measured pulse duration results in a time-bandwidth product

of 2.47 and a calculated peak power of around 9kW. The SSFS source served as the platform

for studying single-pass SRS and SHG in PPLN.

 

 

Text Box: Fig. 4. Two-photon autocorrelation of the SSFS PCF output. The FWHM of the measured pulse was 220 fs. Assuming a sech2 pulse shape, this corresponded to a pulse width of approximately 140 fs.

  

 

 

 

 


 

 

 

 

 

 

 

Collinear SHG of the SSFS source was observed in PPLN. Continuously tunable output from

λ=584 nm to λ=679 nm was measured using a fibre-coupled optical spectrometer with a

resolution of 1 nm (Ocean Optics). Temperature tuning the PPLN crystal from 80 şC to 170

şC and changing the PPLN grating period achieved this broad tuning range. Figure 5 shows a

typical tuning range measured by varying the PPLN period, at a fixed temperature of 110 şC.

 

Text Box: Fig. 5. The SHG spectra as measured at the PPLN output, where the PPLN crystal was held at a fixed temperature of 110 °C. The legend refers to the period length chosen to interact with the input SSFS radiation. The bandwidth of the SHG output varies from 2.8 nm to 4.2
nm.
 

  

 

 

 

 

 

 

 


 

 

 

 

 

By changing the PPLN period, the spectral FWHM varied from 2.8 nm to 4.2 nm. An

average power maximum at λ=628 ± 3.1 nm of 30 mW was measured using a calorimeter and

optical bandpass filter (Chroma), which is 19% efficient conversion from the SSFS source.

This correlates with the spectral range of the fundamental SSFS radiation as already described

in Fig. 3. Additionally, 39 mW of radiation at λ=1047 nm and 24 mW of radiation at

wavelengths longer than λ=1135 nm were measured in crystal transmission. For input pulses

of 140 fs duration, the effective crystal length should ideally be sub-mm for maximum second

harmonic conversion. However, the application of longer crystals is understood to reduce the

threshold and increase the efficiency of the SRS process [7]. For this reason and also for ease

of handling, the 6.5 mm long crystal was retained, although we acknowledge that this

ultimately reduced the SHG conversion efficiency.

Using the SSFS output with a spectral maximum at λ=1258 nm as previously described,

at a fixed temperature of 110 şC the SRS spectral maximum was centred at λ=1583 nm (632

cm-1) and had a FWHM of λ=85 nm. This is shown in Fig. 6. The SRS output was observed

to propagate noncollinearly with the SSFS input beam at an angle of 28° with a 4 mW

threshold, and was therefore easily distinguishable from the generated SHG. With full

incident power at the SSFS wavelengths focussed into the PPLN crystal, the power in the SRS

spectrum was measured to be 18 mW across the measurable spectral range. The conversion

efficiency from SSFS to SRS radiation was therefore calculated to be 12%. The second

harmonic of the SRS radiation was also emitted collinearly with the SRS output, at an average

power of approximately 1 mW. With the long-wave pass filters placed prior to the PPLN

crystal, the SRS signal was reduced in magnitude by almost a factor of two. This was

attributed to the 65% decrease in peak power delivered to the PPLN crystal.

 

Text Box: Fig. 6. The SRS spectrum resulting from pumping the PPLN with the SSFS source. The spectral peak was measured at λ=1583 nm, with a λ=85 nm FWHM.

  

 

 

 

 


 

 

 

 

 

5. Conclusion

In conclusion, we have demonstrated simultaneous SHG and noncollinear SRS in PPLN.

This system was based on SSFS in PCF providing the pump wavelengths necessary for the

concurrent SHG and SRS. A simple single-pass geometry provided conversion efficiencies of

the SSFS radiation to SHG and SRS of 19% and 12% respectively. The SHG process created

a tunable source from λ=584-679 nm and the SRS output was at a peak wavelength of

λ=1583, with a spectral FWHM of λ=85 nm.

With the application of a shorter crystal, the SHG average power would increase but the

SRS efficiency would be reduced. One approach to solving this problem would be to power

scale the initial laser platform, where the output powers of both the SHG and SRS processes

could feasibly reach >100 mW at the novel spectral regions described. Additionally, with

increased interest in understanding and exploiting the nonlinear processes in PCF, we

envisage the future development of a more efficient SSFS source to study simultaneous SHG

and SRS. Applying high-quality anti-reflection coatings to both the PPLN and the aspheric

lenses would also increase the efficiency of both the SRS and SHG processes. Future work

enabled by this novel wavelength source includes remote sensing of CO2 in the L-band, which

extends from 1565 nm to 1620 nm, and further spectroscopy applications.

Acknowledgments

 

This work was supported by the Royal Society of Edinburgh.

 

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