Low spatial coherence electrically pumped semiconductor laser for speckle-free full-field imaging
The spatial coherence of laser sources has limited their application to parallel imaging and projection due to coherent artifacts, such as speckle. In contrast, traditional incoherent light sources, such as thermal sources or light emitting diodes (LEDs), provide relatively low power per independent...
Gespeichert in:
Veröffentlicht in: | Proceedings of the National Academy of Sciences - PNAS 2015-02, Vol.112 (5), p.1304-1309 |
---|---|
Hauptverfasser: | , , , , , , |
Format: | Artikel |
Sprache: | eng |
Schlagworte: | |
Online-Zugang: | Volltext |
Tags: |
Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
|
container_end_page | 1309 |
---|---|
container_issue | 5 |
container_start_page | 1304 |
container_title | Proceedings of the National Academy of Sciences - PNAS |
container_volume | 112 |
creator | Redding, Brandon Cerjan, Alexander Huang, Xue Lee, Minjoo Larry Stone, A. Douglas Choma, Michael A. Cao, Hui |
description | The spatial coherence of laser sources has limited their application to parallel imaging and projection due to coherent artifacts, such as speckle. In contrast, traditional incoherent light sources, such as thermal sources or light emitting diodes (LEDs), provide relatively low power per independent spatial mode. Here, we present a chip-scale, electrically pumped semiconductor laser based on a novel design, demonstrating high power per mode with much lower spatial coherence than conventional laser sources. The laser resonator was fabricated with a chaotic, D-shaped cavity optimized to achieve highly multimode lasing. Lasing occurs simultaneously and independently in ∼1,000 modes, and hence the total emission exhibits very low spatial coherence. Speckle-free full-field imaging is demonstrated using the chaotic cavity laser as the illumination source. The power per mode of the sample illumination is several orders of magnitude higher than that of a LED or thermal light source. Such a compact, low-cost source, which combines the low spatial coherence of a LED with the high spectral radiance of a laser, could enable a wide range of high-speed, full-field imaging and projection applications.
Significance There has been an intense search for the ideal light sources for high-speed, full-field imaging applications ranging from next-generation microscopes and laser projectors to digital holography and photolithography. Traditional lasers, although providing the required brightness (i.e., power per mode), exhibit high spatial coherence, which introduces coherent artifacts such as speckle, corrupting image formation. At the other extreme, low spatial coherence sources such as thermal sources and light emitting diodes (LEDs) avoid speckle but lack sufficient power per mode for high-speed imaging. In this work, we demonstrate a new type of semiconductor laser based on a chaotic cavity, which combines low spatial coherence with high power per mode. Such a laser could enable a wide range of full-field imaging applications. |
doi_str_mv | 10.1073/pnas.1419672112 |
format | Article |
fullrecord | <record><control><sourceid>jstor_pubme</sourceid><recordid>TN_cdi_pubmedcentral_primary_oai_pubmedcentral_nih_gov_4321308</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><jstor_id>26461402</jstor_id><sourcerecordid>26461402</sourcerecordid><originalsourceid>FETCH-LOGICAL-c556t-b131288d48e2bd0faf6d3490bfb8c10eff56b96bf9736e0f4bd39ead04c56f653</originalsourceid><addsrcrecordid>eNpdkc1v1DAQxSMEokvhzAmIxIVL2vFnnAsSqmhBWokD9Gw5znjrxRsHOwH1v8fLlm3h5JHmN8_v6VXVSwJnBFp2Po0mnxFOOtlSQuijakWgI43kHTyuVgC0bRSn_KR6lvMWADqh4Gl1QoUE0XG5qsw6_qrzZGZvQm3jDSYcLdYY0M7JWxPCbT0tuwmHOuPO2zgOi51jqoPJmGpXpjyh_R6wcQmxdksIjfMYhtrvzMaPm-fVE2dCxhd372l1ffnx28WnZv3l6vPFh3VjhZBz0xNGqFIDV0j7AZxxcmAlRu96ZQmgc0L2nexd1zKJ4Hg_sA7NANwK6aRgp9X7g-609DscLI5zMkFPqfhItzoar__djP5Gb-JPzRklDFQReHcnkOKPBfOsdz5bDMGMGJesiRSUc2CqLejb_9BtXNJY4v2h2rYrhgp1fqBsijkndEczBPS-Pr2vT9_XVy5eP8xw5P_29QDYXx7lCNVClxC8AK8OwDaXlu4FJJeEw_6HN4e9M1GbTfJZX3-lQCQA4Uopwn4DdMC1dg</addsrcrecordid><sourcetype>Open Access Repository</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype><pqid>1652779653</pqid></control><display><type>article</type><title>Low spatial coherence electrically pumped semiconductor laser for speckle-free full-field imaging</title><source>MEDLINE</source><source>PubMed Central</source><source>Alma/SFX Local Collection</source><source>Free Full-Text Journals in Chemistry</source><source>JSTOR</source><creator>Redding, Brandon ; Cerjan, Alexander ; Huang, Xue ; Lee, Minjoo Larry ; Stone, A. Douglas ; Choma, Michael A. ; Cao, Hui</creator><creatorcontrib>Redding, Brandon ; Cerjan, Alexander ; Huang, Xue ; Lee, Minjoo Larry ; Stone, A. Douglas ; Choma, Michael A. ; Cao, Hui</creatorcontrib><description>The spatial coherence of laser sources has limited their application to parallel imaging and projection due to coherent artifacts, such as speckle. In contrast, traditional incoherent light sources, such as thermal sources or light emitting diodes (LEDs), provide relatively low power per independent spatial mode. Here, we present a chip-scale, electrically pumped semiconductor laser based on a novel design, demonstrating high power per mode with much lower spatial coherence than conventional laser sources. The laser resonator was fabricated with a chaotic, D-shaped cavity optimized to achieve highly multimode lasing. Lasing occurs simultaneously and independently in ∼1,000 modes, and hence the total emission exhibits very low spatial coherence. Speckle-free full-field imaging is demonstrated using the chaotic cavity laser as the illumination source. The power per mode of the sample illumination is several orders of magnitude higher than that of a LED or thermal light source. Such a compact, low-cost source, which combines the low spatial coherence of a LED with the high spectral radiance of a laser, could enable a wide range of high-speed, full-field imaging and projection applications.
Significance There has been an intense search for the ideal light sources for high-speed, full-field imaging applications ranging from next-generation microscopes and laser projectors to digital holography and photolithography. Traditional lasers, although providing the required brightness (i.e., power per mode), exhibit high spatial coherence, which introduces coherent artifacts such as speckle, corrupting image formation. At the other extreme, low spatial coherence sources such as thermal sources and light emitting diodes (LEDs) avoid speckle but lack sufficient power per mode for high-speed imaging. In this work, we demonstrate a new type of semiconductor laser based on a chaotic cavity, which combines low spatial coherence with high power per mode. Such a laser could enable a wide range of full-field imaging applications.</description><identifier>ISSN: 0027-8424</identifier><identifier>EISSN: 1091-6490</identifier><identifier>DOI: 10.1073/pnas.1419672112</identifier><identifier>PMID: 25605946</identifier><language>eng</language><publisher>United States: National Academy of Sciences</publisher><subject>Emissions ; Lasers ; Light emitting diodes ; Light sources ; Physical Sciences ; Semiconductors</subject><ispartof>Proceedings of the National Academy of Sciences - PNAS, 2015-02, Vol.112 (5), p.1304-1309</ispartof><rights>Volumes 1–89 and 106–112, copyright as a collective work only; author(s) retains copyright to individual articles</rights><rights>Copyright National Academy of Sciences Feb 3, 2015</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c556t-b131288d48e2bd0faf6d3490bfb8c10eff56b96bf9736e0f4bd39ead04c56f653</citedby><cites>FETCH-LOGICAL-c556t-b131288d48e2bd0faf6d3490bfb8c10eff56b96bf9736e0f4bd39ead04c56f653</cites><orcidid>0000-0002-8477-7874</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Uhttp://www.pnas.org/content/112/5.cover.gif</thumbnail><linktopdf>$$Uhttps://www.jstor.org/stable/pdf/26461402$$EPDF$$P50$$Gjstor$$H</linktopdf><linktohtml>$$Uhttps://www.jstor.org/stable/26461402$$EHTML$$P50$$Gjstor$$H</linktohtml><link.rule.ids>230,314,727,780,784,803,885,27924,27925,53791,53793,58017,58250</link.rule.ids><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/25605946$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink></links><search><creatorcontrib>Redding, Brandon</creatorcontrib><creatorcontrib>Cerjan, Alexander</creatorcontrib><creatorcontrib>Huang, Xue</creatorcontrib><creatorcontrib>Lee, Minjoo Larry</creatorcontrib><creatorcontrib>Stone, A. Douglas</creatorcontrib><creatorcontrib>Choma, Michael A.</creatorcontrib><creatorcontrib>Cao, Hui</creatorcontrib><title>Low spatial coherence electrically pumped semiconductor laser for speckle-free full-field imaging</title><title>Proceedings of the National Academy of Sciences - PNAS</title><addtitle>Proc Natl Acad Sci U S A</addtitle><description>The spatial coherence of laser sources has limited their application to parallel imaging and projection due to coherent artifacts, such as speckle. In contrast, traditional incoherent light sources, such as thermal sources or light emitting diodes (LEDs), provide relatively low power per independent spatial mode. Here, we present a chip-scale, electrically pumped semiconductor laser based on a novel design, demonstrating high power per mode with much lower spatial coherence than conventional laser sources. The laser resonator was fabricated with a chaotic, D-shaped cavity optimized to achieve highly multimode lasing. Lasing occurs simultaneously and independently in ∼1,000 modes, and hence the total emission exhibits very low spatial coherence. Speckle-free full-field imaging is demonstrated using the chaotic cavity laser as the illumination source. The power per mode of the sample illumination is several orders of magnitude higher than that of a LED or thermal light source. Such a compact, low-cost source, which combines the low spatial coherence of a LED with the high spectral radiance of a laser, could enable a wide range of high-speed, full-field imaging and projection applications.
Significance There has been an intense search for the ideal light sources for high-speed, full-field imaging applications ranging from next-generation microscopes and laser projectors to digital holography and photolithography. Traditional lasers, although providing the required brightness (i.e., power per mode), exhibit high spatial coherence, which introduces coherent artifacts such as speckle, corrupting image formation. At the other extreme, low spatial coherence sources such as thermal sources and light emitting diodes (LEDs) avoid speckle but lack sufficient power per mode for high-speed imaging. In this work, we demonstrate a new type of semiconductor laser based on a chaotic cavity, which combines low spatial coherence with high power per mode. Such a laser could enable a wide range of full-field imaging applications.</description><subject>Emissions</subject><subject>Lasers</subject><subject>Light emitting diodes</subject><subject>Light sources</subject><subject>Physical Sciences</subject><subject>Semiconductors</subject><issn>0027-8424</issn><issn>1091-6490</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2015</creationdate><recordtype>article</recordtype><sourceid>EIF</sourceid><recordid>eNpdkc1v1DAQxSMEokvhzAmIxIVL2vFnnAsSqmhBWokD9Gw5znjrxRsHOwH1v8fLlm3h5JHmN8_v6VXVSwJnBFp2Po0mnxFOOtlSQuijakWgI43kHTyuVgC0bRSn_KR6lvMWADqh4Gl1QoUE0XG5qsw6_qrzZGZvQm3jDSYcLdYY0M7JWxPCbT0tuwmHOuPO2zgOi51jqoPJmGpXpjyh_R6wcQmxdksIjfMYhtrvzMaPm-fVE2dCxhd372l1ffnx28WnZv3l6vPFh3VjhZBz0xNGqFIDV0j7AZxxcmAlRu96ZQmgc0L2nexd1zKJ4Hg_sA7NANwK6aRgp9X7g-609DscLI5zMkFPqfhItzoar__djP5Gb-JPzRklDFQReHcnkOKPBfOsdz5bDMGMGJesiRSUc2CqLejb_9BtXNJY4v2h2rYrhgp1fqBsijkndEczBPS-Pr2vT9_XVy5eP8xw5P_29QDYXx7lCNVClxC8AK8OwDaXlu4FJJeEw_6HN4e9M1GbTfJZX3-lQCQA4Uopwn4DdMC1dg</recordid><startdate>20150203</startdate><enddate>20150203</enddate><creator>Redding, Brandon</creator><creator>Cerjan, Alexander</creator><creator>Huang, Xue</creator><creator>Lee, Minjoo Larry</creator><creator>Stone, A. Douglas</creator><creator>Choma, Michael A.</creator><creator>Cao, Hui</creator><general>National Academy of Sciences</general><general>National Acad Sciences</general><scope>FBQ</scope><scope>CGR</scope><scope>CUY</scope><scope>CVF</scope><scope>ECM</scope><scope>EIF</scope><scope>NPM</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7QG</scope><scope>7QL</scope><scope>7QP</scope><scope>7QR</scope><scope>7SN</scope><scope>7SS</scope><scope>7T5</scope><scope>7TK</scope><scope>7TM</scope><scope>7TO</scope><scope>7U9</scope><scope>8FD</scope><scope>C1K</scope><scope>FR3</scope><scope>H94</scope><scope>M7N</scope><scope>P64</scope><scope>RC3</scope><scope>7X8</scope><scope>5PM</scope><orcidid>https://orcid.org/0000-0002-8477-7874</orcidid></search><sort><creationdate>20150203</creationdate><title>Low spatial coherence electrically pumped semiconductor laser for speckle-free full-field imaging</title><author>Redding, Brandon ; Cerjan, Alexander ; Huang, Xue ; Lee, Minjoo Larry ; Stone, A. Douglas ; Choma, Michael A. ; Cao, Hui</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c556t-b131288d48e2bd0faf6d3490bfb8c10eff56b96bf9736e0f4bd39ead04c56f653</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2015</creationdate><topic>Emissions</topic><topic>Lasers</topic><topic>Light emitting diodes</topic><topic>Light sources</topic><topic>Physical Sciences</topic><topic>Semiconductors</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Redding, Brandon</creatorcontrib><creatorcontrib>Cerjan, Alexander</creatorcontrib><creatorcontrib>Huang, Xue</creatorcontrib><creatorcontrib>Lee, Minjoo Larry</creatorcontrib><creatorcontrib>Stone, A. Douglas</creatorcontrib><creatorcontrib>Choma, Michael A.</creatorcontrib><creatorcontrib>Cao, Hui</creatorcontrib><collection>AGRIS</collection><collection>Medline</collection><collection>MEDLINE</collection><collection>MEDLINE (Ovid)</collection><collection>MEDLINE</collection><collection>MEDLINE</collection><collection>PubMed</collection><collection>CrossRef</collection><collection>Animal Behavior Abstracts</collection><collection>Bacteriology Abstracts (Microbiology B)</collection><collection>Calcium & Calcified Tissue Abstracts</collection><collection>Chemoreception Abstracts</collection><collection>Ecology Abstracts</collection><collection>Entomology Abstracts (Full archive)</collection><collection>Immunology Abstracts</collection><collection>Neurosciences Abstracts</collection><collection>Nucleic Acids Abstracts</collection><collection>Oncogenes and Growth Factors Abstracts</collection><collection>Virology and AIDS Abstracts</collection><collection>Technology Research Database</collection><collection>Environmental Sciences and Pollution Management</collection><collection>Engineering Research Database</collection><collection>AIDS and Cancer Research Abstracts</collection><collection>Algology Mycology and Protozoology Abstracts (Microbiology C)</collection><collection>Biotechnology and BioEngineering Abstracts</collection><collection>Genetics Abstracts</collection><collection>MEDLINE - Academic</collection><collection>PubMed Central (Full Participant titles)</collection><jtitle>Proceedings of the National Academy of Sciences - PNAS</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Redding, Brandon</au><au>Cerjan, Alexander</au><au>Huang, Xue</au><au>Lee, Minjoo Larry</au><au>Stone, A. Douglas</au><au>Choma, Michael A.</au><au>Cao, Hui</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Low spatial coherence electrically pumped semiconductor laser for speckle-free full-field imaging</atitle><jtitle>Proceedings of the National Academy of Sciences - PNAS</jtitle><addtitle>Proc Natl Acad Sci U S A</addtitle><date>2015-02-03</date><risdate>2015</risdate><volume>112</volume><issue>5</issue><spage>1304</spage><epage>1309</epage><pages>1304-1309</pages><issn>0027-8424</issn><eissn>1091-6490</eissn><abstract>The spatial coherence of laser sources has limited their application to parallel imaging and projection due to coherent artifacts, such as speckle. In contrast, traditional incoherent light sources, such as thermal sources or light emitting diodes (LEDs), provide relatively low power per independent spatial mode. Here, we present a chip-scale, electrically pumped semiconductor laser based on a novel design, demonstrating high power per mode with much lower spatial coherence than conventional laser sources. The laser resonator was fabricated with a chaotic, D-shaped cavity optimized to achieve highly multimode lasing. Lasing occurs simultaneously and independently in ∼1,000 modes, and hence the total emission exhibits very low spatial coherence. Speckle-free full-field imaging is demonstrated using the chaotic cavity laser as the illumination source. The power per mode of the sample illumination is several orders of magnitude higher than that of a LED or thermal light source. Such a compact, low-cost source, which combines the low spatial coherence of a LED with the high spectral radiance of a laser, could enable a wide range of high-speed, full-field imaging and projection applications.
Significance There has been an intense search for the ideal light sources for high-speed, full-field imaging applications ranging from next-generation microscopes and laser projectors to digital holography and photolithography. Traditional lasers, although providing the required brightness (i.e., power per mode), exhibit high spatial coherence, which introduces coherent artifacts such as speckle, corrupting image formation. At the other extreme, low spatial coherence sources such as thermal sources and light emitting diodes (LEDs) avoid speckle but lack sufficient power per mode for high-speed imaging. In this work, we demonstrate a new type of semiconductor laser based on a chaotic cavity, which combines low spatial coherence with high power per mode. Such a laser could enable a wide range of full-field imaging applications.</abstract><cop>United States</cop><pub>National Academy of Sciences</pub><pmid>25605946</pmid><doi>10.1073/pnas.1419672112</doi><tpages>6</tpages><orcidid>https://orcid.org/0000-0002-8477-7874</orcidid><oa>free_for_read</oa></addata></record> |
fulltext | fulltext |
identifier | ISSN: 0027-8424 |
ispartof | Proceedings of the National Academy of Sciences - PNAS, 2015-02, Vol.112 (5), p.1304-1309 |
issn | 0027-8424 1091-6490 |
language | eng |
recordid | cdi_pubmedcentral_primary_oai_pubmedcentral_nih_gov_4321308 |
source | MEDLINE; PubMed Central; Alma/SFX Local Collection; Free Full-Text Journals in Chemistry; JSTOR |
subjects | Emissions Lasers Light emitting diodes Light sources Physical Sciences Semiconductors |
title | Low spatial coherence electrically pumped semiconductor laser for speckle-free full-field imaging |
url | https://sfx.bib-bvb.de/sfx_tum?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2024-12-25T10%3A25%3A00IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-jstor_pubme&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=Low%20spatial%20coherence%20electrically%20pumped%20semiconductor%20laser%20for%20speckle-free%20full-field%20imaging&rft.jtitle=Proceedings%20of%20the%20National%20Academy%20of%20Sciences%20-%20PNAS&rft.au=Redding,%20Brandon&rft.date=2015-02-03&rft.volume=112&rft.issue=5&rft.spage=1304&rft.epage=1309&rft.pages=1304-1309&rft.issn=0027-8424&rft.eissn=1091-6490&rft_id=info:doi/10.1073/pnas.1419672112&rft_dat=%3Cjstor_pubme%3E26461402%3C/jstor_pubme%3E%3Curl%3E%3C/url%3E&disable_directlink=true&sfx.directlink=off&sfx.report_link=0&rft_id=info:oai/&rft_pqid=1652779653&rft_id=info:pmid/25605946&rft_jstor_id=26461402&rfr_iscdi=true |