Off-resonance effects and selectivity profiles in pulsed nitrogen-14 nuclear quadrupole resonance
In order to alleviate base-line distortions in nitrogen-14 NQR spectra originating from pulse breakthrough, low power radio-frequency (rf) pulses were applied. It is recalled that the required power is four times lower than that for an equivalent NMR experiment. This is easily explained by the fact...
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description | In order to alleviate base-line distortions in nitrogen-14 NQR spectra originating from pulse breakthrough, low power radio-frequency (rf) pulses were applied. It is recalled that the required power is four times lower than that for an equivalent NMR experiment. This is easily explained by the fact that, in NMR, half the amplitude of the rf field is active. Moreover, the selectivity profile (i.e. the peak amplitude as a function of the difference between the carrier frequency and the resonance frequency) exhibits a shape which is, in most cases, more favorable in NQR than in NMR. An appropriate theory has been developed for explaining these experimental observations. It is concluded that low power NQR is perfectly feasible and should even be recommended for most applications, provided that the line-width of the NQR signal is not too large.
[Display omitted]
► Nuclear quadrupole resonance can accomodate low-amplitude radio-frequency fields. ► One of the advantages is to avoid spurious signals in case of very low sensitivity. ► Selectivity profiles (available frequency range) remain quite acceptable. ► Experimental and theoretical selectivity profiles agree perfectly (NQR and NMR). |
doi_str_mv | 10.1016/j.ssnmr.2012.08.004 |
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[Display omitted]
► Nuclear quadrupole resonance can accomodate low-amplitude radio-frequency fields. ► One of the advantages is to avoid spurious signals in case of very low sensitivity. ► Selectivity profiles (available frequency range) remain quite acceptable. ► Experimental and theoretical selectivity profiles agree perfectly (NQR and NMR).</description><identifier>ISSN: 0926-2040</identifier><identifier>EISSN: 1527-3326</identifier><identifier>DOI: 10.1016/j.ssnmr.2012.08.004</identifier><identifier>PMID: 23063174</identifier><language>eng</language><publisher>Netherlands: Elsevier Inc</publisher><subject>Amplitudes ; Carrier frequencies ; Chemical Sciences ; Distortion ; Engineering Sciences ; Equivalence ; Fluids mechanics ; Low power radiofrequency field ; Mechanics ; Nitrogen-14 ; NQR ; Nuclear magnetic resonance ; Nuclear power generation ; Nutation curves ; Offset effect ; or physical chemistry ; Selectivity ; Selectivity profile ; Spectra ; Theoretical and</subject><ispartof>Solid state nuclear magnetic resonance, 2012-10, Vol.47-48, p.39-46</ispartof><rights>2012 Elsevier Inc.</rights><rights>Copyright © 2012 Elsevier Inc. All rights reserved.</rights><rights>Distributed under a Creative Commons Attribution 4.0 International License</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c426t-b498a570aff8e7b0d6bd4e58028088aeee82a00740236f6e75910e0d14073a073</citedby><cites>FETCH-LOGICAL-c426t-b498a570aff8e7b0d6bd4e58028088aeee82a00740236f6e75910e0d14073a073</cites><orcidid>0000-0003-0196-2271</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://dx.doi.org/10.1016/j.ssnmr.2012.08.004$$EHTML$$P50$$Gelsevier$$H</linktohtml><link.rule.ids>230,315,781,785,886,3551,27926,27927,45997</link.rule.ids><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/23063174$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink><backlink>$$Uhttps://hal.univ-lorraine.fr/hal-01477862$$DView record in HAL$$Hfree_for_read</backlink></links><search><creatorcontrib>Guendouz, L.</creatorcontrib><creatorcontrib>Robert, A.</creatorcontrib><creatorcontrib>Retournard, A.</creatorcontrib><creatorcontrib>Leclerc, S.</creatorcontrib><creatorcontrib>Aissani, S.</creatorcontrib><creatorcontrib>Canet, D.</creatorcontrib><title>Off-resonance effects and selectivity profiles in pulsed nitrogen-14 nuclear quadrupole resonance</title><title>Solid state nuclear magnetic resonance</title><addtitle>Solid State Nucl Magn Reson</addtitle><description>In order to alleviate base-line distortions in nitrogen-14 NQR spectra originating from pulse breakthrough, low power radio-frequency (rf) pulses were applied. It is recalled that the required power is four times lower than that for an equivalent NMR experiment. This is easily explained by the fact that, in NMR, half the amplitude of the rf field is active. Moreover, the selectivity profile (i.e. the peak amplitude as a function of the difference between the carrier frequency and the resonance frequency) exhibits a shape which is, in most cases, more favorable in NQR than in NMR. An appropriate theory has been developed for explaining these experimental observations. It is concluded that low power NQR is perfectly feasible and should even be recommended for most applications, provided that the line-width of the NQR signal is not too large.
[Display omitted]
► Nuclear quadrupole resonance can accomodate low-amplitude radio-frequency fields. ► One of the advantages is to avoid spurious signals in case of very low sensitivity. ► Selectivity profiles (available frequency range) remain quite acceptable. ► Experimental and theoretical selectivity profiles agree perfectly (NQR and NMR).</description><subject>Amplitudes</subject><subject>Carrier frequencies</subject><subject>Chemical Sciences</subject><subject>Distortion</subject><subject>Engineering Sciences</subject><subject>Equivalence</subject><subject>Fluids mechanics</subject><subject>Low power radiofrequency field</subject><subject>Mechanics</subject><subject>Nitrogen-14</subject><subject>NQR</subject><subject>Nuclear magnetic resonance</subject><subject>Nuclear power generation</subject><subject>Nutation curves</subject><subject>Offset effect</subject><subject>or physical chemistry</subject><subject>Selectivity</subject><subject>Selectivity profile</subject><subject>Spectra</subject><subject>Theoretical and</subject><issn>0926-2040</issn><issn>1527-3326</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2012</creationdate><recordtype>article</recordtype><recordid>eNqFkUtvGyEUhVHUqnHT_oJKFctmMdPLYwAvuoiipolkKZt0jfBwSbHGjAMzlvLvi-PUy2aBQOg793EOIV8YtAyY-r5pS0nb3HJgvAXTAsgzsmAd140QXL0jC1hy1XCQcE4-lrIBAM2E-kDOuQAlmJYL4u5DaDKWMbnUI8UQsJ8KdcnTgkN9x32cnukujyEOWGhMdDcPBT1NccrjI6aGSZrmfkCX6dPsfJ5344D0VPMTeR9cVXx-vS_I75ufD9e3zer-19311arpJVdTs5ZL4zoNLgSDeg1erb3EzgA3YIxDRMNdXUACFyoo1N2SAYJnErRw9VyQy2PdP26wuxy3Lj_b0UV7e7Wyhz9gUmuj-J5V9tuRrXs9zVgmu42lx2FwCce5WKZ0rVt91W-jTArDO1BdRcUR7fNYSsZwGoOBPURmN_YlMnuIzIKxNbKq-vraYF5v0Z80_zKqwI8jgNW9fcRsSx-xOutjrgFZP8b_NvgLevunpw</recordid><startdate>20121001</startdate><enddate>20121001</enddate><creator>Guendouz, L.</creator><creator>Robert, A.</creator><creator>Retournard, A.</creator><creator>Leclerc, S.</creator><creator>Aissani, S.</creator><creator>Canet, D.</creator><general>Elsevier Inc</general><general>Elsevier</general><scope>NPM</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7X8</scope><scope>7U5</scope><scope>8FD</scope><scope>L7M</scope><scope>1XC</scope><orcidid>https://orcid.org/0000-0003-0196-2271</orcidid></search><sort><creationdate>20121001</creationdate><title>Off-resonance effects and selectivity profiles in pulsed nitrogen-14 nuclear quadrupole resonance</title><author>Guendouz, L. ; Robert, A. ; Retournard, A. ; Leclerc, S. ; Aissani, S. ; Canet, D.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c426t-b498a570aff8e7b0d6bd4e58028088aeee82a00740236f6e75910e0d14073a073</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2012</creationdate><topic>Amplitudes</topic><topic>Carrier frequencies</topic><topic>Chemical Sciences</topic><topic>Distortion</topic><topic>Engineering Sciences</topic><topic>Equivalence</topic><topic>Fluids mechanics</topic><topic>Low power radiofrequency field</topic><topic>Mechanics</topic><topic>Nitrogen-14</topic><topic>NQR</topic><topic>Nuclear magnetic resonance</topic><topic>Nuclear power generation</topic><topic>Nutation curves</topic><topic>Offset effect</topic><topic>or physical chemistry</topic><topic>Selectivity</topic><topic>Selectivity profile</topic><topic>Spectra</topic><topic>Theoretical and</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Guendouz, L.</creatorcontrib><creatorcontrib>Robert, A.</creatorcontrib><creatorcontrib>Retournard, A.</creatorcontrib><creatorcontrib>Leclerc, S.</creatorcontrib><creatorcontrib>Aissani, S.</creatorcontrib><creatorcontrib>Canet, D.</creatorcontrib><collection>PubMed</collection><collection>CrossRef</collection><collection>MEDLINE - Academic</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>Hyper Article en Ligne (HAL)</collection><jtitle>Solid state nuclear magnetic resonance</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Guendouz, L.</au><au>Robert, A.</au><au>Retournard, A.</au><au>Leclerc, S.</au><au>Aissani, S.</au><au>Canet, D.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Off-resonance effects and selectivity profiles in pulsed nitrogen-14 nuclear quadrupole resonance</atitle><jtitle>Solid state nuclear magnetic resonance</jtitle><addtitle>Solid State Nucl Magn Reson</addtitle><date>2012-10-01</date><risdate>2012</risdate><volume>47-48</volume><spage>39</spage><epage>46</epage><pages>39-46</pages><issn>0926-2040</issn><eissn>1527-3326</eissn><abstract>In order to alleviate base-line distortions in nitrogen-14 NQR spectra originating from pulse breakthrough, low power radio-frequency (rf) pulses were applied. It is recalled that the required power is four times lower than that for an equivalent NMR experiment. This is easily explained by the fact that, in NMR, half the amplitude of the rf field is active. Moreover, the selectivity profile (i.e. the peak amplitude as a function of the difference between the carrier frequency and the resonance frequency) exhibits a shape which is, in most cases, more favorable in NQR than in NMR. An appropriate theory has been developed for explaining these experimental observations. It is concluded that low power NQR is perfectly feasible and should even be recommended for most applications, provided that the line-width of the NQR signal is not too large.
[Display omitted]
► Nuclear quadrupole resonance can accomodate low-amplitude radio-frequency fields. ► One of the advantages is to avoid spurious signals in case of very low sensitivity. ► Selectivity profiles (available frequency range) remain quite acceptable. ► Experimental and theoretical selectivity profiles agree perfectly (NQR and NMR).</abstract><cop>Netherlands</cop><pub>Elsevier Inc</pub><pmid>23063174</pmid><doi>10.1016/j.ssnmr.2012.08.004</doi><tpages>8</tpages><orcidid>https://orcid.org/0000-0003-0196-2271</orcidid></addata></record> |
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subjects | Amplitudes Carrier frequencies Chemical Sciences Distortion Engineering Sciences Equivalence Fluids mechanics Low power radiofrequency field Mechanics Nitrogen-14 NQR Nuclear magnetic resonance Nuclear power generation Nutation curves Offset effect or physical chemistry Selectivity Selectivity profile Spectra Theoretical and |
title | Off-resonance effects and selectivity profiles in pulsed nitrogen-14 nuclear quadrupole resonance |
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