High-Power 3345 nm Distributed Feedback Laser (TOP Wavelength)

References

nanoplus Nanosystems and Technologies GmbH Products DFB Laser HP 3345 nm

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Distributed Feedback Laser

High-Power 3345 nm
TOP Wavelength

High-power DFB interband cascade lasers at 3345 nm are used for ethane detection.

Please have a look at the key features, specifications and applications.

Specifications

Mountings & Accessories

Applications

Papers & Links

Specifications

parameters	symbol	unit	minimum	typical	maximum
parameters operating wavelength (at T_op, I_op)	symbol λop	unit nm	minimum	typical 3345	maximum
parameters optical output power (at λ_op)	symbol P_op	unit mW	minimum	typical 40	maximum
parameters operating current	symbol I_op	unit mA	minimum	typical	maximum 120
parameters operating voltage	symbol V_op	unit V	minimum	typical 5	maximum
parameters threshold current	symbol I_th	unit mA	minimum 15	typical 25	maximum 40
parameters side mode suppression ratio	symbol SMSR	unit dB	minimum	typical > 35	maximum
parameters current tuning coefficient	symbol C_I	unit nm / mA	minimum	typical 0.10	maximum
parameters temperature tuning coefficient	symbol C_T	unit nm / K	minimum	typical 0.35	maximum
parameters operating chip temperature	symbol T_op	unit °C	minimum +15	typical +20	maximum +40
parameters operating case temperature (non-condensing)	symbol T_C	unit °C	minimum -20	typical +25	maximum +55
parameters storage temperature (non-condensing)	symbol T_S	unit °C	minimum -30	typical +20	maximum +70

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Mountings & Accessories

SM-BTF - our fiber-coupled workhorse

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availability: 760 nm - 5500 nm
TEC: integrated TEC
NTC: integrated NTC

plug&play: fiber-coupled beam
size: large footprint
costs: higher cost than free space

TO66 - our workhorse for ICLs

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availability: 2800 nm - 6500 nm
TEC: integrated large TEC
NTC: integrated NTC
cap: AR coated cap (optional)

window: AR coated window (optional)
plug&play: collimation required
size: small footprint
costs: low cost

chip on heatspreader - high-end OEM integration

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availability: 760 nm - 6000 nm
TEC: no TEC
NTC: integrated NTC
cap: NA

window: NA
plug&play: collimation required
size: smallest footprint
costs: low cost

Heatsink for TO5 / TO66

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availability: 760 nm - 6500 nm
NTC: integrated (optional)
heat distribution: warranted
connectors: for laser diode driver & temperature controller
posts: M6 thread for optical table

cage system: standard
collimation: none

Lens on cap

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availability: 1850 nm - 6500 nm
heat distribution: none, use separate heatsink
connectors: TO66 connectors only
posts: none, use separate heatsink

cage system: none, use separate heatsink
collimation: high-end collimation, divergence < 4 mrad

Applications

C₂H₆ & C₂H₂

Monitoring of breath gas: C₂H₆ and C₂H₂

Medical breath analysis considers ethane and acetelyne as a biomarkers for asthma, schizophrenia or lung cancer. The research field of breath analysis uses methane as a biomarker for intestinal problems.

[ 187 , 10 ]

C₂H₆

Emission control by methane source identification: C₂H₆

Ethane is a by-product of methane emissions. The ethane ratio varies between methane emissions from thermogenic and biogenic sources. This allows differentiating oil and gas reserves from those of livestock, landfills, wetlands or stagnant water. Studies are executed on behalf of the US Environmental Protection Agency to quantify methane emissions caused byincreased natural gas exploration and production in the US. A newly developed ethane spectrometer delivers 1 second ethane measurements with sub-ppb precision in an ethane-methane mixture.

[ 187 , 61 ]

C₂H₆

Emission control of greenhouse gases: C₂H₆

Ethane is an important greenhouse gas that has a critical impact on climate change. Emissions are related to fossil fuel and biofuel consumption, biomass combustion and natural gas losses. Trace gas detection of ethane is an important tool to monitor greenhouse gases.

[ 187 , 146 , 145 , 128 , 119 , 10 ]

Papers & Links

# 9 DFB Lasers Between 760 nm and 16 µm for Sensing Applications

W. Zeller, L. Naehle, P. Fuchs, F. Gerschuetz, L. Hildebrandt, J. Koeth , Sensors, 10, 2010, pp. 2492-2510,

# 10 Continuous wave, distributed feedback diode laser based sensor for trace-gas detection of ethane

K. Krzempek, R. Lewicki, L. Naehle, M. Fischer, J. Koeth, S. Belahsene, Y. Rouillard, L. Worschech, F.K. Tittel , Appl. Phys. B , 106, 2, 2012, pp 251-255.,

# 53 CW DFB RT diode laser-based sensor for trace-gas detection of ethane using a novel compact multipass gas absorption cell

K. Krzempek, M. Jahjah, R. Lewicki, P. Stefanski, S. So, D. Thomazy, F.K. Tittel, Appl. Phys. B, 112, 4. September 2013, pp. 461-465.,

# 61 Demonstration of an Ethane Spectrometer for Methane Source Identification

T.I. Yacovitch, S.C. Herndon, J.R. Roscioli, C. Floerchinger, R.M. McGovern, M. Agnese, G. Petron, J. Kofler, C. Sweeney, A. Karion, S.A. Conley, E.A. Kort, L. Naehle, M. Fischer, L. Hildebrandt,.J. Koeth, J.B. McManus, D.D. Nelson, M.S. Zahniser, C.E. Kolb, Environ. Sci. Technol., 48, 2014, 8028-8034.,

# 63 Breath Analysis Using Laser Spectroscopic Techniques: Breath Biomarkers, Spectral Fingerprints, and Detection Limits

C. Wang and P. Sahay, Sensors, 9, 2009, 8230 - 8262,

# 77 Compact TDLAS based sensor design using interband cascade lasers for mid-IR trace gas sensing

L. Dong, F. K. Tittel, C. Li, N. P. Sanchez, H. Wu, C. Zheng, Y. Yu, A. Sampaolo, R. J. Griffin , Optics Express, Vol. 24, Issue 6, 2016, pp. A528-A535.,

# 82 Ppb-level mid-infrared ethane detection based on three measurement schemes using a 3.34 μm continuous-wave interband cascade laser

C. Li, C. Zheng, L. Dong, W. Ye, F. K. Tittel, Y. Wang , Appl. Phys. B, July 2016, 122:185.,

# 106 Recent progress in laser‑based trace gas instruments: performance and noise analysis

J. B. McManus, M. S. Zahniser, D. D. Nelson et. al., Appl. Phys. B, 2015, 119: 203.,

# 119 Interband cascade laser based quartz-enhanced photoacoustic sensor for multiple hydrocarbons detection

A. Sampaolo, S. Csutak, P. Patimisco, M. Giglio, G. Menduni, V. Passaro, F. K. Tittel, M. Deffenbaugh, V. Spagnolo, Proc. SPIE 10540, Quantum Sensing and Nano Electronics and Photonics XV , 26th January 2018, 105400C,

# 122 A streamlined approach to hybrid-chemistry modeling for a low cetane-number alternative jet fuel

N. H. Pinkowski, Y. Wang , S. J. Cassady , D. F. Davidson , R. K. Hanson , Combustion and Flame, Vol.208, October 2019, pp. 15-26.,

# 123 Multi-wavelength speciation of high-temperature 1-butene pyrolysis

N. H. Pinkowski, S. J. Cassady, D. F. Davidson, R. K. Hanson, Fuel, Vol. 244, 15th May 2019, pp. 269-281.,

# 124 Tomographic laser absorption imaging ofcombustion species and temperature in the mid-wave infrared

C. Wei, D. I. Pineda, C. S. Goldenstein, R. M. Spearrin, Opt. Exp., Vol. 26, Iss. 16, 2018, pp. 20944 - 20951.,

# 125 Time-resolved laser absorption imaging of ethane at 2 kHz in unsteady partially premixed flames

K. K. Schwarm, C. Wei, D. I. Pineda, R. M. Spearrin, Appl. Opt., Vol. 58, Iss. 21, Juli 2019, pp. 5656 - 5662.,

# 128 Quartz-enhanced photoacoustic spectroscopy for hydrocarbon trace gas detection and petroleum exploration

A. Sampaoloa, G. Mendunib,P. Patimiscoa, M. Giglioa, V. M.N. Passaroc, L. Donga, H. Wua, F. K. Tittel, V. Spagnoloa, , Fuel, Vol.277, 2020,

# 140 Interband cascade laser arrays for simultaneous and selective analysis of C1–C5 hydrocarbons in petrochemical industry

J. Scheuermann, P. Kluczynski, K. Siembab, M. Straszewski, J. Kaczmarek, R. Weih, M. Fischer, J. Koeth, A. Schade, S. Höfling, Appl. Spectrosc, January 2021, 2021,

# 142 Methane, ethane and propane detection using a compact quartz enhanced photoacoustic sensor and a single interband cascade laser

A. Sampaolo, S. Csutak, P. Patimisco, M. Giglio, G. Menduni, V. Passaro, F. K. Tittel, M. Deffenbaugh, V. Spagnolo, Sensors and Actuators B: Chemical, Vol. 282, 2019, pp. 952-960.,

# 145 High resolution spectra of 13C ethane and propane isotopologues photoacoustically measured using interband cascade lasers near 3.33 and 3.38 μm, respectively

A. Loh, M. Wolff, Journal of Quantitative Spectroscopy & Radiative Transfer, 227, 2019, pp. 111 – 116.,

# 146 Multivariate analysis of photoacoustic spectra for the detection of short-chained hydrocarbon isotopologues

A. Loh, M. Wolff, MDPI, 2020, 25, 2266.,

# 151 The interband cascade laser

J. R. Meyer, W. Bewley, C. L. Canedy, C. S. Kim, M. Kim, C. D. Merritt, I. Vurgaftman, Photonics, Vol. 7, No. 3 (75), 2020,

# 174 Dual-comb optical activity spectroscopy for the analysis of vibrational optical activity induced by external magnetic field

D. Peng, C. Gu, Z. Zuo, Y. Di,X. Zou, L. Tang, L. Deng1, D. Luo1, Y. Liu, W. Li, Nat. Commun., 14, 2023, 883,

# 178 Quartz-Enhanced Photoacoustic Sensors for Detection of Eight Air Pollutants

R. De Palo, A. Elefante, G. Biagi, F. Paciolla, R. Weih, V. Villada, A. Zifarelli, M. Giglio, A. Sampaolo, V. Spagnolo, P. Patimisco, Adv. Phot. Res., Vo. 4, Iss. 6, 2023,

# 185 Comparison of photoacoustic spectroscopy and cavity ring-down spectroscopy for ambient methane monitoring at Hohenpeißenberg

M. Müller, S. Weigl, J. Müller-Williams, M. Lindauer, T. Rück, S. Jobst, R. Bierl, and F.-M. Matysik, Atmos. Meas. Tech., 16, 2023, 4263–4270,

# 187 Characterizing a sensitive compact mid-infrared photoacoustic sensor for methane, ethane and acetylene detection considering changing ambient parameters and bulk composition (N₂, O₂ and H₂O)

J. Pangerl, M. Müller, T. Rück, S. Weigl, R. Bierl, Sens. Actuators B Chem., 352, 2022, 130962,

# 188 An Algorithmic Approach to Compute the Effect of Non-Radiative Relaxation Processes in Photoacoustic Spectroscopy

M. Müller, T. Rück, S. Jobst, J. Pangerl, S. Weigl, R. Bierl, F.-M. Matysik, Photoacoustics, 26, 2022, 100371,

# 189 Digital Twin of a photoacoustic trace gas sensor for monitoring methane in complex gas compositions

M. Müller, T. Rück, S. Jobst, J. Pangerl, S. Weigl, R. Bierl, F.-M. Matysik, Sens. Actuators B Chem., 378, 2023, 133119,

Optical properties

nanoplus distributed feedback lasers show outstanding spectral, tuning and electrical properties.

Spectrum 3345 nm DFB high-power

Typical spectrum of a nanoplus high-power 3345 nm distributed feedback interband cascade laser

Tuning 3345 nm DFB high-power

Typical mode hop free tuning of a nanoplus high-power 3345 nm distributed feedback interband cascade laser

PI Curve 3345 nm DFB high-power

Typical power, current and voltage characteristics of a nanoplus high-power 3345 nm distributed feedback interband cascade laser

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Product Brief

More information

nanoplus uses a unique and patented technology for DFB laser manufacturing. We apply a lateral metal grating along the ridge waveguide, which is independent of the material system. Read more about our patented distributed feedback technology.

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High-Power 3345 nmTOP Wavelength

Distributed Feedback Laser

High-Power 3345 nmTOP Wavelength

Optical properties

Product Brief

Your Requirement

High-Power 3345 nm
TOP Wavelength

High-Power 3345 nm
TOP Wavelength