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Pulsed electron paramagnetic resonance spectroscopy powered by a free-electron laser
A free-electron laser is used to power a pulsed electron paramagnetic resonance spectrometer at 240 GHz, demonstrating a range of experimental possibilities such as the manipulation of spin-1/2 systems with 6-ns pulses and the measurement of ultrashort decoherence times. Pulsed EPR spectroscopy The...
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Published in: | Nature (London) 2012-09, Vol.489 (7416), p.409-413 |
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description | A free-electron laser is used to power a pulsed electron paramagnetic resonance spectrometer at 240 GHz, demonstrating a range of experimental possibilities such as the manipulation of spin-1/2 systems with 6-ns pulses and the measurement of ultrashort decoherence times.
Pulsed EPR spectroscopy
The technique of electron paramagnetic resonance (EPR) spectroscopy probes unpaired electrons and can provide valuable information on dynamic local structure in biological systems, optoelectronic devices and fundamental quantum systems. Like nuclear magnetic resonance, EPR spectroscopy becomes more powerful at high magnetic fields and frequencies, and using uses pulses rather than continuous waves. Overcoming a major bottleneck in producing powerful pulses at frequencies above 100 gigahertz, the authors use a free-electron laser to power a pulsed spectrometer at 240 gigahertz. This enables them to demonstrate a range of new experimental possibilities, such as the manipulation of spin-1/2 systems with 6 nanosecond pulses and ultrashort decoherence times.
Electron paramagnetic resonance (EPR) spectroscopy interrogates unpaired electron spins in solids and liquids to reveal local structure and dynamics; for example, EPR has elucidated parts of the structure of protein complexes that other techniques in structural biology have not been able to reveal
1
,
2
,
3
,
4
. EPR can also probe the interplay of light and electricity in organic solar cells
5
,
6
,
7
and light-emitting diodes
8
, and the origin of decoherence in condensed matter, which is of fundamental importance to the development of quantum information processors
9
,
10
,
11
,
12
,
13
. Like nuclear magnetic resonance, EPR spectroscopy becomes more powerful at high magnetic fields and frequencies, and with excitation by coherent pulses rather than continuous waves. However, the difficulty of generating sequences of powerful pulses at frequencies above 100 gigahertz has, until now, confined high-power pulsed EPR to magnetic fields of 3.5 teslas and below. Here we demonstrate that one-kilowatt pulses from a free-electron laser can power a pulsed EPR spectrometer at 240 gigahertz (8.5 teslas), providing transformative enhancements over the alternative, a state-of-the-art ∼30-milliwatt solid-state source. Our spectrometer can rotate spin-1/2 electrons through π/2 in only 6 nanoseconds (compared to 300 nanoseconds with the solid-state source). Fourier-transform EPR on nitrogen impurities in diamond demonstrates excit |
doi_str_mv | 10.1038/nature11437 |
format | article |
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Pulsed EPR spectroscopy
The technique of electron paramagnetic resonance (EPR) spectroscopy probes unpaired electrons and can provide valuable information on dynamic local structure in biological systems, optoelectronic devices and fundamental quantum systems. Like nuclear magnetic resonance, EPR spectroscopy becomes more powerful at high magnetic fields and frequencies, and using uses pulses rather than continuous waves. Overcoming a major bottleneck in producing powerful pulses at frequencies above 100 gigahertz, the authors use a free-electron laser to power a pulsed spectrometer at 240 gigahertz. This enables them to demonstrate a range of new experimental possibilities, such as the manipulation of spin-1/2 systems with 6 nanosecond pulses and ultrashort decoherence times.
Electron paramagnetic resonance (EPR) spectroscopy interrogates unpaired electron spins in solids and liquids to reveal local structure and dynamics; for example, EPR has elucidated parts of the structure of protein complexes that other techniques in structural biology have not been able to reveal
1
,
2
,
3
,
4
. EPR can also probe the interplay of light and electricity in organic solar cells
5
,
6
,
7
and light-emitting diodes
8
, and the origin of decoherence in condensed matter, which is of fundamental importance to the development of quantum information processors
9
,
10
,
11
,
12
,
13
. Like nuclear magnetic resonance, EPR spectroscopy becomes more powerful at high magnetic fields and frequencies, and with excitation by coherent pulses rather than continuous waves. However, the difficulty of generating sequences of powerful pulses at frequencies above 100 gigahertz has, until now, confined high-power pulsed EPR to magnetic fields of 3.5 teslas and below. Here we demonstrate that one-kilowatt pulses from a free-electron laser can power a pulsed EPR spectrometer at 240 gigahertz (8.5 teslas), providing transformative enhancements over the alternative, a state-of-the-art ∼30-milliwatt solid-state source. Our spectrometer can rotate spin-1/2 electrons through π/2 in only 6 nanoseconds (compared to 300 nanoseconds with the solid-state source). Fourier-transform EPR on nitrogen impurities in diamond demonstrates excitation and detection of EPR lines separated by about 200 megahertz. We measured decoherence times as short as 63 nanoseconds, in a frozen solution of nitroxide free-radicals at temperatures as high as 190 kelvin. Both free-electron lasers and the quasi-optical technology developed for the spectrometer are scalable to frequencies well in excess of one terahertz, opening the way to high-power pulsed EPR spectroscopy up to the highest static magnetic fields currently available.</description><identifier>ISSN: 0028-0836</identifier><identifier>EISSN: 1476-4687</identifier><identifier>DOI: 10.1038/nature11437</identifier><identifier>PMID: 22996555</identifier><identifier>CODEN: NATUAS</identifier><language>eng</language><publisher>London: Nature Publishing Group UK</publisher><subject>639/301/1019/1020/1087 ; 639/766/930/527 ; Advantages ; Allyl Compounds - chemistry ; Benzene - chemistry ; Cyclic N-Oxides - chemistry ; Diamond - chemistry ; Electromagnetism; electron and ion optics ; Electron paramagnetic resonance ; Electron Spin Resonance Spectroscopy - instrumentation ; Electron Spin Resonance Spectroscopy - methods ; Electrons ; Exact sciences and technology ; Fourier Analysis ; Free electron lasers ; Free Radicals - chemistry ; Fundamental areas of phenomenology (including applications) ; Humanities and Social Sciences ; Infrared, submillimeter wave, microwave and radiowave instruments, equipment and techniques ; Instruments, apparatus, components and techniques common to several branches of physics and astronomy ; Laser beams ; Lasers ; letter ; Magnetic fields ; multidisciplinary ; Nanocomposites ; Nanomaterials ; Nanostructure ; Nitrogen Oxides - chemistry ; NMR ; Nuclear magnetic resonance ; Observations ; Physics ; Radiation by moving charges ; Science ; Science (multidisciplinary) ; Semiconductors ; Solar cells ; Spectrometers ; Spectroscopy ; Spectrum analysis ; Submillimeter wave, microwave and radiowave spectrometers; magnetic resonance spectrometers, auxiliary equipments and techniques ; Temperature ; Time Factors</subject><ispartof>Nature (London), 2012-09, Vol.489 (7416), p.409-413</ispartof><rights>Springer Nature Limited 2012</rights><rights>2014 INIST-CNRS</rights><rights>COPYRIGHT 2012 Nature Publishing Group</rights><rights>Copyright Nature Publishing Group Sep 20, 2012</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c652t-758446dfb70b7a4f6a01e6bc6a39933ddabc9a68d6c056c8f1e4374264c1625a3</citedby><cites>FETCH-LOGICAL-c652t-758446dfb70b7a4f6a01e6bc6a39933ddabc9a68d6c056c8f1e4374264c1625a3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,27924,27925</link.rule.ids><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&idt=26350599$$DView record in Pascal Francis$$Hfree_for_read</backlink><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/22996555$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink></links><search><creatorcontrib>Takahashi, S.</creatorcontrib><creatorcontrib>Brunel, L.-C.</creatorcontrib><creatorcontrib>Edwards, D. T.</creatorcontrib><creatorcontrib>van Tol, J.</creatorcontrib><creatorcontrib>Ramian, G.</creatorcontrib><creatorcontrib>Han, S.</creatorcontrib><creatorcontrib>Sherwin, M. S.</creatorcontrib><title>Pulsed electron paramagnetic resonance spectroscopy powered by a free-electron laser</title><title>Nature (London)</title><addtitle>Nature</addtitle><addtitle>Nature</addtitle><description>A free-electron laser is used to power a pulsed electron paramagnetic resonance spectrometer at 240 GHz, demonstrating a range of experimental possibilities such as the manipulation of spin-1/2 systems with 6-ns pulses and the measurement of ultrashort decoherence times.
Pulsed EPR spectroscopy
The technique of electron paramagnetic resonance (EPR) spectroscopy probes unpaired electrons and can provide valuable information on dynamic local structure in biological systems, optoelectronic devices and fundamental quantum systems. Like nuclear magnetic resonance, EPR spectroscopy becomes more powerful at high magnetic fields and frequencies, and using uses pulses rather than continuous waves. Overcoming a major bottleneck in producing powerful pulses at frequencies above 100 gigahertz, the authors use a free-electron laser to power a pulsed spectrometer at 240 gigahertz. This enables them to demonstrate a range of new experimental possibilities, such as the manipulation of spin-1/2 systems with 6 nanosecond pulses and ultrashort decoherence times.
Electron paramagnetic resonance (EPR) spectroscopy interrogates unpaired electron spins in solids and liquids to reveal local structure and dynamics; for example, EPR has elucidated parts of the structure of protein complexes that other techniques in structural biology have not been able to reveal
1
,
2
,
3
,
4
. EPR can also probe the interplay of light and electricity in organic solar cells
5
,
6
,
7
and light-emitting diodes
8
, and the origin of decoherence in condensed matter, which is of fundamental importance to the development of quantum information processors
9
,
10
,
11
,
12
,
13
. Like nuclear magnetic resonance, EPR spectroscopy becomes more powerful at high magnetic fields and frequencies, and with excitation by coherent pulses rather than continuous waves. However, the difficulty of generating sequences of powerful pulses at frequencies above 100 gigahertz has, until now, confined high-power pulsed EPR to magnetic fields of 3.5 teslas and below. Here we demonstrate that one-kilowatt pulses from a free-electron laser can power a pulsed EPR spectrometer at 240 gigahertz (8.5 teslas), providing transformative enhancements over the alternative, a state-of-the-art ∼30-milliwatt solid-state source. Our spectrometer can rotate spin-1/2 electrons through π/2 in only 6 nanoseconds (compared to 300 nanoseconds with the solid-state source). Fourier-transform EPR on nitrogen impurities in diamond demonstrates excitation and detection of EPR lines separated by about 200 megahertz. We measured decoherence times as short as 63 nanoseconds, in a frozen solution of nitroxide free-radicals at temperatures as high as 190 kelvin. Both free-electron lasers and the quasi-optical technology developed for the spectrometer are scalable to frequencies well in excess of one terahertz, opening the way to high-power pulsed EPR spectroscopy up to the highest static magnetic fields currently available.</description><subject>639/301/1019/1020/1087</subject><subject>639/766/930/527</subject><subject>Advantages</subject><subject>Allyl Compounds - chemistry</subject><subject>Benzene - chemistry</subject><subject>Cyclic N-Oxides - chemistry</subject><subject>Diamond - chemistry</subject><subject>Electromagnetism; electron and ion optics</subject><subject>Electron paramagnetic resonance</subject><subject>Electron Spin Resonance Spectroscopy - instrumentation</subject><subject>Electron Spin Resonance Spectroscopy - methods</subject><subject>Electrons</subject><subject>Exact sciences and technology</subject><subject>Fourier Analysis</subject><subject>Free electron lasers</subject><subject>Free Radicals - chemistry</subject><subject>Fundamental areas of phenomenology (including applications)</subject><subject>Humanities and Social Sciences</subject><subject>Infrared, submillimeter wave, microwave and radiowave instruments, equipment and techniques</subject><subject>Instruments, apparatus, components and techniques common to several branches of physics and astronomy</subject><subject>Laser beams</subject><subject>Lasers</subject><subject>letter</subject><subject>Magnetic fields</subject><subject>multidisciplinary</subject><subject>Nanocomposites</subject><subject>Nanomaterials</subject><subject>Nanostructure</subject><subject>Nitrogen Oxides - chemistry</subject><subject>NMR</subject><subject>Nuclear magnetic resonance</subject><subject>Observations</subject><subject>Physics</subject><subject>Radiation by moving charges</subject><subject>Science</subject><subject>Science (multidisciplinary)</subject><subject>Semiconductors</subject><subject>Solar cells</subject><subject>Spectrometers</subject><subject>Spectroscopy</subject><subject>Spectrum analysis</subject><subject>Submillimeter wave, microwave and radiowave spectrometers; magnetic resonance spectrometers, auxiliary equipments and techniques</subject><subject>Temperature</subject><subject>Time Factors</subject><issn>0028-0836</issn><issn>1476-4687</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2012</creationdate><recordtype>article</recordtype><recordid>eNqF0l2L1DAUBuAiiju7euW9FBdB0a75bnI5DH4sLCo64mU5TU-HLp20m7S48-_NuOPujFSWXASS55yQ5E2SZ5ScUcL1OwfD6JFSwfMHyYyKXGVC6fxhMiOE6Yxoro6S4xAuCSGS5uJxcsSYMUpKOUuWX8c2YJVii3bwnUt78LCGlcOhsanH0DlwFtPQ_9kPtus3ad_9Qh-Lyk0Kae0Rs9vyFgL6J8mjGmLbp7v5JPnx4f1y8Sm7-PLxfDG_yKySbMhyqYVQVV3mpMxB1AoIRVVaBdwYzqsKSmtA6UpZIpXVNcV4R8GUsFQxCfwkeXXTt_fd1YhhKNZNsNi24LAbQ0FzySXXiqn7qeAm19zQ_H5KlGFEK64jPf2HXnajd_HOBaWUMUaNZHdqBS0Wjau7wYPdNi3mnHAhiZEmqmxCrdChh7ZzWDdx-cC_mPC2b66KfXQ2geKocN3Yya6vDwqiGfB6WMEYQnH-_duhffN_O1_-XHye1DbGKHisi943a_Cb-KDFNsjFXpCjfr572bFcY3Vr_yY3gpc7AMFCW_sY0ybcOcUlkWZ77NsbF-KWW6Hf-6KJc38DkzkEzw</recordid><startdate>20120920</startdate><enddate>20120920</enddate><creator>Takahashi, S.</creator><creator>Brunel, L.-C.</creator><creator>Edwards, D. 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Academic</collection><collection>Computer and Information Systems Abstracts</collection><collection>Electronics & Communications Abstracts</collection><collection>Engineered Materials Abstracts</collection><collection>Mechanical & Transportation Engineering Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>METADEX</collection><collection>ANTE: Abstracts in New Technology & Engineering</collection><collection>Materials Research Database</collection><collection>ProQuest Computer Science Collection</collection><collection>Civil Engineering Abstracts</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>Computer and Information Systems Abstracts Academic</collection><collection>Computer and Information Systems Abstracts Professional</collection><jtitle>Nature (London)</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Takahashi, S.</au><au>Brunel, L.-C.</au><au>Edwards, D. T.</au><au>van Tol, J.</au><au>Ramian, G.</au><au>Han, S.</au><au>Sherwin, M. S.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Pulsed electron paramagnetic resonance spectroscopy powered by a free-electron laser</atitle><jtitle>Nature (London)</jtitle><stitle>Nature</stitle><addtitle>Nature</addtitle><date>2012-09-20</date><risdate>2012</risdate><volume>489</volume><issue>7416</issue><spage>409</spage><epage>413</epage><pages>409-413</pages><issn>0028-0836</issn><eissn>1476-4687</eissn><coden>NATUAS</coden><abstract>A free-electron laser is used to power a pulsed electron paramagnetic resonance spectrometer at 240 GHz, demonstrating a range of experimental possibilities such as the manipulation of spin-1/2 systems with 6-ns pulses and the measurement of ultrashort decoherence times.
Pulsed EPR spectroscopy
The technique of electron paramagnetic resonance (EPR) spectroscopy probes unpaired electrons and can provide valuable information on dynamic local structure in biological systems, optoelectronic devices and fundamental quantum systems. Like nuclear magnetic resonance, EPR spectroscopy becomes more powerful at high magnetic fields and frequencies, and using uses pulses rather than continuous waves. Overcoming a major bottleneck in producing powerful pulses at frequencies above 100 gigahertz, the authors use a free-electron laser to power a pulsed spectrometer at 240 gigahertz. This enables them to demonstrate a range of new experimental possibilities, such as the manipulation of spin-1/2 systems with 6 nanosecond pulses and ultrashort decoherence times.
Electron paramagnetic resonance (EPR) spectroscopy interrogates unpaired electron spins in solids and liquids to reveal local structure and dynamics; for example, EPR has elucidated parts of the structure of protein complexes that other techniques in structural biology have not been able to reveal
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,
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,
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. EPR can also probe the interplay of light and electricity in organic solar cells
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and light-emitting diodes
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, and the origin of decoherence in condensed matter, which is of fundamental importance to the development of quantum information processors
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,
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,
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,
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. Like nuclear magnetic resonance, EPR spectroscopy becomes more powerful at high magnetic fields and frequencies, and with excitation by coherent pulses rather than continuous waves. However, the difficulty of generating sequences of powerful pulses at frequencies above 100 gigahertz has, until now, confined high-power pulsed EPR to magnetic fields of 3.5 teslas and below. Here we demonstrate that one-kilowatt pulses from a free-electron laser can power a pulsed EPR spectrometer at 240 gigahertz (8.5 teslas), providing transformative enhancements over the alternative, a state-of-the-art ∼30-milliwatt solid-state source. Our spectrometer can rotate spin-1/2 electrons through π/2 in only 6 nanoseconds (compared to 300 nanoseconds with the solid-state source). Fourier-transform EPR on nitrogen impurities in diamond demonstrates excitation and detection of EPR lines separated by about 200 megahertz. We measured decoherence times as short as 63 nanoseconds, in a frozen solution of nitroxide free-radicals at temperatures as high as 190 kelvin. Both free-electron lasers and the quasi-optical technology developed for the spectrometer are scalable to frequencies well in excess of one terahertz, opening the way to high-power pulsed EPR spectroscopy up to the highest static magnetic fields currently available.</abstract><cop>London</cop><pub>Nature Publishing Group UK</pub><pmid>22996555</pmid><doi>10.1038/nature11437</doi><tpages>5</tpages></addata></record> |
fulltext | fulltext |
identifier | ISSN: 0028-0836 |
ispartof | Nature (London), 2012-09, Vol.489 (7416), p.409-413 |
issn | 0028-0836 1476-4687 |
language | eng |
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source | Nature |
subjects | 639/301/1019/1020/1087 639/766/930/527 Advantages Allyl Compounds - chemistry Benzene - chemistry Cyclic N-Oxides - chemistry Diamond - chemistry Electromagnetism electron and ion optics Electron paramagnetic resonance Electron Spin Resonance Spectroscopy - instrumentation Electron Spin Resonance Spectroscopy - methods Electrons Exact sciences and technology Fourier Analysis Free electron lasers Free Radicals - chemistry Fundamental areas of phenomenology (including applications) Humanities and Social Sciences Infrared, submillimeter wave, microwave and radiowave instruments, equipment and techniques Instruments, apparatus, components and techniques common to several branches of physics and astronomy Laser beams Lasers letter Magnetic fields multidisciplinary Nanocomposites Nanomaterials Nanostructure Nitrogen Oxides - chemistry NMR Nuclear magnetic resonance Observations Physics Radiation by moving charges Science Science (multidisciplinary) Semiconductors Solar cells Spectrometers Spectroscopy Spectrum analysis Submillimeter wave, microwave and radiowave spectrometers magnetic resonance spectrometers, auxiliary equipments and techniques Temperature Time Factors |
title | Pulsed electron paramagnetic resonance spectroscopy powered by a free-electron laser |
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