Photon etc.
{{Short description|Canadian manufacturer of scientific instruments}}
{{COI|date=August 2021}}
{{Infobox company
| name = Photon etc.
| type = Corporation
| location_city = Montreal, Québec
| location_country = Canada
| founded = 2002
| key_people = CEO: Sébastien Blais-Ouellette, Ph. D.
CTO : Marc Verhaegen, Ph.D.
Director of Electronic & Software Engineering : Simon Lessard
| industry = {{hlist|Biomedical imaging|nanotechnology|industrial quality control/sorting}}
| area_served = International
| num_employees = 25-30
| homepage = {{URL|photonetc.com}}
}}
Photon etc. is a Canadian manufacturer of infrared cameras, widely tunable optical filters, hyperspectral imaging and spectroscopic scientific instruments for academic and industrial applications. Its main technology is based on volume Bragg gratings, which are used as filters either for swept lasers or for global imaging.
History
As a spin-off of the California Institute of Technology,http://innovation.caltech.edu/startups {{Webarchive|url=https://web.archive.org/web/20150106103032/http://innovation.caltech.edu/startups |date=2015-01-06 }}, CALTECH Office of Technology Transfer, "Past/Current Startups", retrieved January 2015 the company was founded in 2003 by Sébastien Blais-Ouellette {{cite web|last1=Champagne|first1=Stéphane|title=Des étoiles à l'entrepreneuriat|url=http://affaires.lapresse.ca/pme/201301/07/01-4608904-des-etoiles-a-lentrepreneuriat.php|website=lapresse.ca|access-date=21 December 2014}}{{cite web|last1=Turcotte|first1=Claude|title=Portrait d'entreprise - Voir grand dans l'outil optique|url=https://www.ledevoir.com/economie/actualites-economiques/380975/voir-grand-dans-l-outil-optique|website=ledevoir.com|date=17 June 2013 |access-date=31 January 2015}} who was working on narrow band imaging tunable filters for the detection of hydroxyl groups in the Earth atmosphere. This is how he developed the main technology of the company, a patented S. Blais-Ouellette; "Method and apparatus for a Bragg grating tunable filter", US patent 7557990 (B2), issued Jul 7, 2009, https://patents.google.com/patent/US7557990S. Blais-Ouellette; E. Wishnow; "Spectrographic multi-band camera", US patent 8237844 (B2), issued Apr 25, 2006, https://patents.google.com/patent/US8237844S. Blais-Ouellette; K. Matthews; C. Moser; "Efficient multi-line narrow-band large format holographic filter", US patent US7221491 (B2), issued Apr 18, 2006, https://patents.google.com/patent/US7221491 volume Bragg grating for filtering purposes.
The company was first established in the J.-Armand Bombardier Incubator at Université de Montréal where it benefited from a complete infrastructure and proximity to researchers. After 5 years, Photon etc. moved to its actual location at the "Campus des technologies de la santé″ in the Rosemont district of Montréal. Photon etc. has 25 employees in Canada and has received several awards and recognition (Québec Entrepreneur of the Year (finalist),{{cite web|title=EY announces 2014 Québec Entrepreneur of the YearTM finalists today | url= http://www.newswire.ca/en/story/1383477/ey-announces-2014-quebec-entrepreneur-of-the-yeartm-finalists-today | website= www.newswire.ca |access-date=29 January 2015}} CCFC (winner),{{cite web|title=Grand Prix d'excellence en affaires France-Québec 2009 | url=http://blog.akova.ca/2009/10/inca-et-gid-design-gagnent-le-grand-prix-dexcellence-en-affaires-france-quebec-2009/ | website=akova.ca|access-date=29 January 2015}} Fondation Armand-Frappier (winner - prix émergence),{{cite news|last1=Tanguay|first1=Claude|title=Pour l'avancement de la recherche en santé - rapport annuel|url=http://www.fondation-afrappier-inrs.ca/documents/pdf/Francais/RapportsAnnuels/rapport_annuel_2007_08.pdf|access-date=29 January 2015}} Prism Award (finalist) {{cite web|title=Prism Awards Finalists | url=http://www.photonics.com/Article.aspx?AID=35970 | website=www.photonics.com|access-date=29 January 2015}}). In the last ten years, the company has developed numerous collaborations,{{cite news|last1=Malorie|first1=Bertrand|title=Research-business partnership creates unique image system|url=http://www.innovation.ca/en/ResearchInAction/OutcomeStory/Researchbusinesspartnershipcreatesuniqueimagesystem|access-date=19 March 2015|agency=INNOVATION|date=February 24, 2015}}{{cite news|title=IRDEP to Showcase Photon etc's Hyperspectral Analyzer for Photovoltaics Industry|url=http://www.azocleantech.com/news.aspx?newsID=12366|access-date=19 March 2015|agency=AZO Cleantech|date=October 6, 2010}}{{cite web|last1=Pouliot|first1=François|title=Une alliance internationale qui donne plus de crédibilité à Photon etc.|url=http://www.lesaffaires.com/archives/generale/une-alliance-internationale-qui-donne-plus-de-credibilite-a-photon-etc/555819|access-date=2 September 2014}} filed several patents and created spin-off companies in various domains: [http://www.photonicknowledge.com/index-en.asp Photonic Knowledge] (mining exploration), [http://www.nuvucameras.com/ Nüvü Cameras] (EMCCD cameras) {{cite web|last1=Ouatik|first1=Bouchra|title=Nüvü Caméras: voir ce que les autres ne voient pas|url=http://affaires.lapresse.ca/pme/201101/21/01-4362603-nuvu-cameras-voir-ce-que-les-autres-ne-voient-pas.php|website=lapresse.ca|access-date=31 January 2015}} and [http://www.optinadx.com/index.html Optina Diagnostics] (retinal imaging).{{cite web|last1=Dubuc|first1=André|title=Maladies de la rétine: une caméra qui détecte de façon précoce|url=http://affaires.lapresse.ca/pme/201402/24/01-4741872-maladies-de-la-retine-une-camera-qui-detecte-de-facon-precoce.php|website=lapresse.ca|access-date=31 January 2015}} More recently, in June 2015, Photon etc. expanded its expertise in nanotechnology and launched a new division, [http://www.photonnano.com/ Photon Nano]. Photon Nano provides Raman, fluorescence and plasmonic labels synthesized by top research laboratories. Those labels are mainly employed in multiplexing applications for cellular imaging.
Technology
Photon etc.'s core technology is a continuously tunable filter based on volume Bragg gratings. It consists of a photo-thermo-refractive glass with a periodically varying index of refraction in which the modulation structure can be orientated to transmit or reflect incident light.{{cite book |author=A. L. Glebov |title=Micro-Optics 2012 |chapter=Volume Bragg gratings as ultra-narrow and multiband optical filters |series=Proceedings of the SPIE |volume=8428 |pages=84280C |date=2012 |doi= 10.1117/12.923575|display-authors=etal|bibcode=2012SPIE.8428E..0CG |s2cid=20980117 |editor1-link=Hugo Thienpont |editor1-last=Thienpont |editor1-first=Hugo |editor2-last=Mohr |editor2-first=Jürgen |editor3-last=Zappe |editor3-first=Hans |editor4-last=Nakajima |editor4-first=Hirochika }} In order to select a particular wavelength that will be filtered (diffracted), the angle of the filter is adjusted to meet Bragg condition:{{cite book|last1=C. Kress|first1=Bernard|title=Applied Digital Optics : From Micro-optics to Nanophotonics|date=2009|isbn=978-0-470-02263-4}}{{cite book|last1=Ciapurin|first1=Igor V|last2=Glebov|first2=Leonid B.|last3=Smirnov|first3=Vadim I. |title=Practical Holography XIX: Materials and Applications |chapter=Modeling of Gaussian beam diffraction on volume Bragg gratings in PTR glass |date=2005 |series=Proceedings of the SPIE |volume=5742|pages=183|doi=10.1117/12.591215 |bibcode=2005SPIE.5742..183C|s2cid=43830811|editor1-last=Jeong|editor1-first=Tung H|editor2-last=Bjelkhagen|editor2-first=Hans I}}
:
where {{math|n}} is an integer, {{math|λ}}B is the wavelength that will be diffracted, {{math|Λ}} is the step of the grating, {{math|θ}} is the angle between the incident beam and the normal of the entrance surface and {{math|φ}} is the angle between the normal and the grating vector. For transmission gratings, Bragg planes are perpendicular to the entrance surface ({{math|φ}}={{math|π}}/2) while for reflection gratings, Bragg plans are parallel to the entrance surface ({{math|φ}}=0). If the beam does not meet the Bragg condition, it passes through the filter, undiffracted.
In a Bragg filter, the incoming collimated light is first diffracted by a volume filter and only a small fraction of the spectrum is affected. Then, by using a second parallel filter with the same modulation period, light can be recombined and an image can be reconstructed.{{cite book |author=S. Blais-Ouellette |title=Ground-based and Airborne Instrumentation for Astronomy |chapter=The imaging Bragg tunable filter: A new path to integral field spectroscopy and narrow band imaging |series=SPIE Conference Series |volume=6269 |pages=62695H |date=2006 |doi= 10.1117/12.672614|display-authors=etal |bibcode=2006SPIE.6269E..5HB |s2cid=53076655 |editor1-last=McLean |editor1-first=Ian S |editor2-last=Iye |editor2-first=Masanori }}
=Hyperspectral imaging=
The company commercializes hyperspectral imaging systems based on volume Bragg gratings. This technique combines spectroscopy and imaging: each image is acquired on a narrow band of wavelengths (as small as 0.3 nm). The monochromatic images acquired from a hyperspectral data cube, which contains both the spatial (x- and y-axes) and spectral (z-axis) information of a sample.
In this technique, global imaging is used in order to acquire a large area of a sample without damaging it.{{cite journal |author=W. Havener|title=High-throughput Graphene Imaging on Arbitrary Substrates with Wide-field Raman Spectroscopy |journal=ACS Nano |date=2012 | doi= 10.1021/nn2037169 |volume=6 |issue=1 |pages=373–380|display-authors=etal |pmid=22206260|s2cid=20056064 }} In global imaging, the whole field of view of the microscope objective is acquired at the same time compared to point-by-point techniques where either the sample or the excitation laser needs to be moved in order to reconstruct a map. When combined to microscopy, darkfield or brightfield illumination can be employed and various experiments can be carried out such as:
{{columns-list|colwidth=30em|style=width: 600px|
- Photoluminescence
- Fluorescence
- Electroluminescence
- Raman imaging
- Wide-field imaging
}}
=Tunable filters=
The volume Bragg grating technology is also used to design tunable bandpass filters for various light sources. This technology combines an out-of-band rejection of <-60 dB and an optical density higher than OD 6{{cite book|last1=Daniel|first1=Gagnon|last2=Laura-Isabelle|first2=Dion-Bertrand|title=Widely tunable filter: technology and measurement of critical specifications|date=September 9, 2015|url=http://photonetc.ekomobi.com/api/files/55f0527b9f27ea695f000478-WIDELY-TUNABLE-FILTER-2015R10.pdf}} with a tunability over the visible and near infrared regions of the electromagnetic spectrum.
=Tunable lasers=
The Bragg grating filtering technology can be coupled to a supercontinuum laser in order to generate a tunable laser source. Supercontinuum sources are usually a high-power fibre laser which delivers ultra-broadband radiation and can be used for steady-state or lifetime experiments. This ultra broad radiation is obtained when a laser is directed through a nonlinear medium. From there, a collection of highly nonlinear optical processes (e.g.: four-wave mixing, Raman shifting of the solitons) add up together which create the supercontinuum emission. Coupled with the proper filter it can deliver a quasi-monochromatic output over a spectral range going from 400 nm to {{formatnum:2300}} nm. This tool can be used in several experiments and fields of research which includes:
{{columns-list|colwidth=30em|style=width: 600px|
- Photoluminescence excitation (PLE)
- Photoluminescence
- Reflection/Absorption Spectroscopy
- Steady state pump-probe experiment
- Hyperspectral imaging
- Detector calibration
}}
= Infrared cameras=
Photon etc. designs and manufactures low noise infrared cameras sensitive from 850 nm to {{formatnum:2500}} nm. Their HgCdTe (MCT) focal plane array (FPA) were first developed for faint flux measurements and are now used for astronomy, spectroscopy, quality control and sorting.
Applications
= Photovoltaics =
Photovoltaic devices can be characterized by global hyperspectral imaging by electroluminescence (EL) and photoluminescence (PL) mapping. This technique allows the characterization of different aspects of photovoltaic cells : open circuit voltage, transport mechanisms,{{cite book |author=A. Delamarre |title=Physics, Simulation, and Photonic Engineering of Photovoltaic Devices |chapter=Characterization of solar cells using electroluminescence and photoluminescence hyperspectral images |volume=8256 |pages=825614 |date=2012 |doi=10.1117/12.906859|display-authors=etal |bibcode=2012SPIE.8256E..14D |s2cid=121877474 |editor1-last=Freundlich |editor1-first=Alexandre |editor2-last=Guillemoles |editor2-first=Jean-Francois F }} external quantum efficiency,{{cite book |author=A. Delamarre |title=Physics, Simulation, and Photonic Engineering of Photovoltaic Devices II |chapter=Evaluation of micrometer scale lateral fluctuations of transport properties in CIGS solar cells |volume=100 |pages=862009 |date=2013 | doi=10.1117/12.2004323|display-authors=etal |bibcode=2013SPIE.8620E..09D |s2cid=120825849 |editor1-last=Freundlich |editor1-first=Alexandre |editor2-last=Guillemoles |editor2-first=Jean-Francois }} saturation currents,{{cite journal |author=A. Delamarre|title=Contactless mapping of saturation currents of solar cells by photoluminescence |journal=Appl. Phys. Lett. |date=2012 |doi=10.1063/1.3697704 |volume=100 |issue=13 |pages=131108|display-authors=etal|bibcode=2012ApPhL.100m1108D|url=https://hal.archives-ouvertes.fr/hal-03795259 }} composition map, uniformity components, crystallographic domains, stress shifts and lifetime measurement for material quality. It has in fact already been employed for the characterization of Cu(In,Ga)Se2 (CIGS) {{cite journal |author=A. Delamarre|title=Quantitative luminescence mapping of Cu(In,Ga)Se2 thin-film solar cells |journal=Progress in Photovoltaics |volume=23 |issue=10 |pages=1305–1312 |date=2014 | doi=10.1002/pip.2555|s2cid=98472503 |display-authors=etal}} and GaAs solar cells. In their study, researchers from [http://www.irdep.cnrs-bellevue.fr/ IRDEP] (Institute of Research and Development on Photovoltaic Energy) were able to extract maps of the quasi-fermi level splitting and of the external quantum efficiency with the help of photoluminescence and electroluminescence hyperspectral measurements combined with a spectral and photometric absolute calibration method.
= Health and Life Science =
Since global hyperspectral imaging is a non-invasive technique, it gained popularity in the last few years in the health domain.{{cite book|last1=Grahn|first1=F. Hans|last2=Geladi|first2=Paul|title=Techniques and applications of hyperspectral image analysis|url=https://archive.org/details/techniquesapplic00grah_005|url-access=registration|date=October 2007|publisher=Wiley|isbn=978-0-470-01086-0|pages=[https://archive.org/details/techniquesapplic00grah_005/page/n333 313]–332}}{{cite journal|last1=Lu|first1=Guolan|last2=Fei|first2=Baowei|title=Medical hyperspectral imaging: a review|journal=Journal of Biomedical Optics|date=January 20, 2014|volume=19|issue=1|doi=10.1117/1.JBO.19.1.010901|pages=010901|pmid=24441941|pmc=3895860|bibcode=2014JBO....19a0901L}} For example, it has been used for the early diagnosis of retina anomalies (e.g.: age-related macular degeneration (AMD), retinal vessel oxygen saturation {{cite journal |author=A.M. Shahidi| title=Regional variation in human retinal vessel oxygen saturation |journal=Experimental Eye Research|volume=113|date=2013 |doi=10.1016/j.exer.2013.06.001 |pages=143–147|display-authors=etal |pmid=23791637}}), in the biomedical field in addition to neurology and dermatology for the identification and location of certain proteins (e.g.: hemoglobin) or pigments (e.g.: melanin).
In life science, this technique is used for darkfield and epifluorescence microscopy. Several studies showed hyperspectral imaging results of gold nanoparticles (AuNPs) targeting CD44+ cancer cells {{cite journal |author=S. Patskovsky|title= Wide-field hyperspectral 3D imaging of functionalized gold nanoparticles targeting cancer cells by reflected light microscopy|journal=Journal of Biophotonics |pages=401–407 |date=2014 | doi= 10.1002/jbio.201400025 |pmid= 24961507|volume=9999|issue= 5|s2cid= 6797985|display-authors=etal}} and quantum dots (QDs) for the investigation of molecular dynamics in the central nervous system (CNS).
Moreover, hyperspectral imaging optimized in the near-infrared is a well-suited tool to study single carbon nanotube photoluminescence in living cells and tissues. In a Scientific Reports paper, Roxbury et al.{{cite journal|last1=Roxbury|first1=Daniel|last2=Prakrit V|first2=Jena|last3=M. Williams|first3=Ryan|last4=Enyedi|first4=Balázs|last5=Niethammer|first5=Philipp|last6=Stéphane|first6=Marcet|last7=Verhaegen|first7=Marc|last8=Blais-Ouelette|first8=Sébastien|last9=Daniel|first9=Heller|title=Hyperspectral Microscopy of Near-Infrared Fluorescence Enables 17-Chirality Carbon Nanotube Imaging|journal=Scientific Reports|date=18 August 2015|volume=5|doi=10.1038/srep14167|pages=14167|pmid=26387482|pmc=4585673|bibcode=2015NatSR...514167R}} presents simultaneous imaging of 17 nanotube chiralities, including 12 distinct fluorescent species within living cells. The measurements were performed ex vivo and in vivo.
= Semiconductors =
After the invention of the transistor in 1947, the research on semiconductor materials took a big step forward. One technique that emerged from this consists of combining Raman spectroscopy with hyperspectral imaging which permits characterization of samples due to Raman diffusion specificity. For example, it is possible to detect stress, strain and impurities in silicon (Si) samples based on frequency, intensity, shape and width variation in the Si phonon band (~520 cm−1).{{cite book | chapter = Chapter 15: Spectroscopic Imaging with Nanometer Resolution Using Near-Field Methods | last1 = Yeo | first1 = Boon-Siang | last2 = Schmid | first2 = Thomas | last3 = Zhang | first3 = Weihua | last4 = Zenobi | first4 = Renato | publisher = Wiley-VCH Verlag GmbH & Co. KGaA | isbn = 9783527628230 | doi = 10.1002/9783527628230.ch15 | page = [https://archive.org/details/infraredramanspe00salz/page/n493 473] | editor1-last = Salzer | editor1-first = Reiner | editor2-last = W. Siesler | editor2-first = Heinz | title = Infrared and Raman Spectroscopic Imaging | url = https://archive.org/details/infraredramanspe00salz | url-access = registration | year = 2009}}J.D. Caldwell, L. Lombez, A. Delamarre, J.F. Guillemoles, B. Bourgoin, B. Hull, M. Verhaegen, Luminescence Imaging of Extended Defects in SiC via Hyperspectral Imaging. Silicon carbide and related materials 2011, PTS2, Materials Science Forum, 717-720, 403-406, [http://www.scientific.net/MSF.717-720.403 10.4028/www.scientific.net/MSF.717-720.403] Generally, it is possible to assess material's crystalline quality, local stress/strain, dopant and impurity levels and surface temperature.{{cite book |author=S. Marcet |title=Photonics North 2012|chapter=Raman spectroscopy hyperspectral imager based on Bragg tunable filters|volume=8412| pages=84121J |date=2012 |doi=10.1117/12.2000479|display-authors=etal | bibcode=2012SPIE.8412E..1JM | s2cid=119859405 | editor1-last=Kieffer | editor1-first=Jean-Claude }}
= Nanomaterials =
Nanomaterials have recently raised a huge interest in the field of material science because of their colossal collection of industrial, biomedical and electronic applications. Global hyperspectral imaging combined with photoluminescence, electroluminescence or Raman spectroscopy offers a way to analyze those emerging materials. It can provide mapping of samples containing quantum dots,Fogel P. et al., "Evaluation of unmixing methods for the separation of Quantum Dot sources," Hyperspectral Image and Signal Processing: Evolution in Remote Sensing, 2009. WHISPERS '09. First Workshop on, 2009 doi: 10.1109/WHISPERS.2009.5289020, https://ieeexplore.ieee.org/stamp/stamp.jsp?tp=&arnumber=5289020&isnumber=5288971 nanowires, nanoparticles, nanotracers,Univalor Infoletter, May 2013, Univalor, "Photon etc. starts the commercialization of Raman nanotracers invented by Professor Richard Martel of the Université de Montréal", Montreal, http://www.univalor.ca/en/node/359Robic VOL.17 N°1, 2013, "Fighting Counterfeiting: Photon Etc. and the University of Montreal Develop Technology for Molecular Signature", Montreal, http://newsletter.robic.ca/nouvelle.aspx?lg=EN&id=256 etc. Global hyperspectral imaging can also be used to study the diameter and chirality distribution {{cite journal | last1 = Nesbitt | first1 = J. | last2 = Smith | first2 = D. | year = 2013 | title = Measurements of the Population Lifetime of D Band and G′ Band Phonons in Single-Walled Carbon Nanotubes | journal = Nano Letters | volume = 13 | issue = 2| pages = 416–422 | doi = 10.1021/nl303569n | pmid=23297761| bibcode = 2013NanoL..13..416N }} and radial breathing modes (RBM) M. Verhaegen; S. Blais-Ouellette; Carbon Nanotube Characterization by Resonance Raman Spectroscopy, Spectroscopy Application Notebook, September 2010, http://www.spectroscopyonline.com/spectroscopy/article/articleDetail.jsp?id=688629 of carbon nanotubes. It can deliver maps of the uniformity, defects and disorder while providing information on the number and relative orientation of layers, strain, and electronic excitations. It can hence be employed for the characterization of 2D materials such as graphene and molybdenum disulfide (MoS2).{{cite journal | last1 = Ferrari | first1 = A.C. | display-authors = etal | year = 2013| title = Raman spectroscopy as a versatile tool for studying the properties of graphene | journal = Nature Nanotechnology | volume = 8 | issue = 4| pages = 235–246 | doi = 10.1038/nnano.2013.46 | pmid = 23552117 | arxiv = 1306.5856| bibcode = 2013NatNa...8..235F| s2cid = 205450422 }}
= Industrial =
Hyperspectral imaging allows extracting information on the composition and the distribution of specific compounds. Those properties make hyperspectral imaging a well-suited technique for the mining industry. Taking advantage of the specific spectral signature of minerals Photonic Knowledge's Core Mapper™ offers instant mineral identification. This technology delivers monochromatic images and fast mineralogy mapping. The wide-field modality renders possible the identification of mineral signatures but also the classification of plants (e.g.: weeds, precision agriculture) and food (e.g.: meat freshness, fruit defects) and can be used for various outdoor applications.{{cite journal|last1=Eckhard|first1=Jia|last2=Eckhard|first2=Timo|last3=Valero|first3=Eva M.|last4=Nieves|first4=Juan Luis|last5=Contreras|first5=Estibaliz Garrote|title=Outdoor scene re ectance measurements using a Bragg-grating based hyperspectral imager|journal=Applied Optics|date=February 13, 2015|doi=10.1364/ao.54.000d15|volume=54|issue=13|pages=D15|bibcode=2015ApOpt..54D..15E|s2cid=121105708}}
Being able to quickly and efficiently detect explosive liquid precursors represents an important asset to identify potential threats. An hyperspectral camera in the SWIR region allows such detection by acquiring rapidly spectrally resolved images. The monochromatic full-frame images obtained permit fast identification of chemical compounds. Detection of sulfur by laser-induced breakdown spectroscopy (LIBS) can also be easily achieved with holographic Bragg grating used as filtering elements.{{cite journal |author=D. Gagnon|title=Multiband Sensor Using Thick Holographic Gratings for Sulphur Detection by Laser-Induced Breakdown Spectroscopy |journal=Applied Optics|date=2012 |doi= 10.1364/AO.51.0000B7 |pmid=22410928 |volume=51 |issue=7 |pages=B7-12|display-authors=etal|bibcode=2012ApOpt..51B...7G}}
=Instrument Calibration and Characterization=
The calibration of measuring instruments (e.g. : photodetector, spectrometer) is essential if researchers want to be able to compare their results with those of different research groups and if we want to maintain high standards. Spectral calibration is often needed and requires a well-known source that can cover a wide part of the electromagnetic spectrum. Tunable laser sources possess all of the above requirements and are hence particularly appropriate for this type of calibration.
Before the Gemini Planet Imager (GPI) was sent to Gemini South, it was necessary to calibrate its coronagraph. For this matter, a nearly achromatic and collimated source that could cover 0.95-2.4 μm was needed. Photon etc.’s efficient tunable laser source was chosen to test the coronagraph. The tunable source was able to provide an output across the whole GPI wavelength domain.{{cite book |author=S. R. Soummer |title= Techniques and Instrumentation for Detection of Exoplanets IV|chapter= The Gemini Planet Imager coronagraph testbed|volume= 7440|pages= 74400R|date=2009 | doi= 10.1117/12.826700|display-authors=etal |bibcode= 2009SPIE.7440E..0RS|s2cid= 122904075|editor1-last= Shaklan|editor1-first= Stuart B}}Testing the Gemini Planet Imager coronograph: http://www.photonetc.com/space-astronomy
Thin-film filters are necessary elements in optical instrumentation. Band-pass, notch and edge filters now possess challenging specifications that are sometimes strenuous to characterize. Indeed, an optical density (OD) higher than 6 is difficult to identify. This is why a group of researchers from Aix Marseille Université developed a spectrally resolved characterization technique based on a supercontinuum source and a laser line tunable filter. The method is described in detail in the Liukaityte et al. paper from Optics Letter {{cite journal|last1=Liukaityte|first1=Simona|last2=Lequime|first2=Michel|last3=Zerrad|first3=Myriam|last4=Begou|first4=Thomas|last5=Amra|first5=Claude|title=Broadband spectral transmittance measurements of complex thin-film filters with optical densities of up to 12|journal=Optics Letters|volume=40|issue=14|pages=3225–3228|doi=10.1364/OL.40.003225|pmid=26176435|bibcode=2015OptL...40.3225L|year=2015}} and allowed to study thin-film filters with optical densities from 0 to 12 in a wavelength range between 400 nm and 1000 nm.
References
{{Reflist|2}}
External links
- [http://www.photonetc.com Company website]
- [http://www.ctssante.com/ Campus des technologies de la santé website]
Category:Manufacturing companies based in Montreal
Category:Companies established in 2002