Loading…

Spherical Fused Silica Cells Filled with Pure Helium for NMR-Magnetometry

High magnetic fields (> 1 T) are measured by NMR magnetometers with un-rivaled precision if the precessing spin sample provides long coherence times. The longest coherence times are found in diluted \({}^{3}\)He samples, which can be hyperpolarized for sufficient signal strength. In order to have...

Full description

Saved in:
Bibliographic Details
Published in:arXiv.org 2015-09
Main Authors: Maul, Andreas, Blümler, Peter, Heil, Werner, Nikiel, Anna, Otten, Ernst, Petrich, Andreas, Schmidt, Thomas
Format: Article
Language:English
Subjects:
Online Access:Get full text
Tags: Add Tag
No Tags, Be the first to tag this record!
cited_by
cites
container_end_page
container_issue
container_start_page
container_title arXiv.org
container_volume
creator Maul, Andreas
Blümler, Peter
Heil, Werner
Nikiel, Anna
Otten, Ernst
Petrich, Andreas
Schmidt, Thomas
description High magnetic fields (> 1 T) are measured by NMR magnetometers with un-rivaled precision if the precessing spin sample provides long coherence times. The longest coherence times are found in diluted \({}^{3}\)He samples, which can be hyperpolarized for sufficient signal strength. In order to have minimal influence on the homogeneity and value of the measured magnetic field the optimal container for the \({}^{3}\)He should be a perfect sphere. A fused silica sphere with an inner diameter of 8 mm and an outer diameter of 12 mm was made from two hemispheres by diffusion bonding leaving only a small hole for cleaning and evacuation. This hole was closed in vacuum by a CO\({}_{2}\) laser and the inner volume was filled with a few mbars of \({}^3\)He via wall permeation. NMR-measurements on such a sample had coherence times of 5 min. While the hemispheres were produced with < 1 \(\mu\)m deviation from sphericity, the bonding left a step of ca. 50 \(\mu\)m at maximum. The influence of such a mismatch, its orientation and materials in the direct vicinity of the sample are analyzed by FEM-simulations and discussed in view of coherence times and absolute fields.
doi_str_mv 10.48550/arxiv.1508.00838
format article
fullrecord <record><control><sourceid>proquest</sourceid><recordid>TN_cdi_proquest_journals_2077999582</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>2077999582</sourcerecordid><originalsourceid>FETCH-LOGICAL-a522-6bf946b82e679808de48ff7bdb76bd00326806a5b3663c3cb393c100fa7dce373</originalsourceid><addsrcrecordid>eNotjV1LwzAYRoMgOOZ-gHcBr1vf5m0-einFusGm4nY_kjZxGdk6k9aPf7-BXj2cc3EeQu4KyEvFOTzo-OO_8oKDygEUqisyYYhFpkrGbsgspT0AMCEZ5zghi_VpZ6NvdaDNmGxH1z5ciNY2hEQbH8LFffthR9_GaOncBj8eqOsjfVm9Zyv9cbRDf7BD_L0l106HZGf_OyWb5mlTz7Pl6_OiflxmmjOWCeOqUhjFrJCVAtXZUjknTWekMB0AMqFAaG5QCGyxNVhhWwA4LbvWosQpuf_LnmL_Odo0bPf9GI-Xxy0DKauq4orhGeKnTSA</addsrcrecordid><sourcetype>Aggregation Database</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype><pqid>2077999582</pqid></control><display><type>article</type><title>Spherical Fused Silica Cells Filled with Pure Helium for NMR-Magnetometry</title><source>Publicly Available Content Database (Proquest) (PQ_SDU_P3)</source><creator>Maul, Andreas ; Blümler, Peter ; Heil, Werner ; Nikiel, Anna ; Otten, Ernst ; Petrich, Andreas ; Schmidt, Thomas</creator><creatorcontrib>Maul, Andreas ; Blümler, Peter ; Heil, Werner ; Nikiel, Anna ; Otten, Ernst ; Petrich, Andreas ; Schmidt, Thomas</creatorcontrib><description>High magnetic fields (&gt; 1 T) are measured by NMR magnetometers with un-rivaled precision if the precessing spin sample provides long coherence times. The longest coherence times are found in diluted \({}^{3}\)He samples, which can be hyperpolarized for sufficient signal strength. In order to have minimal influence on the homogeneity and value of the measured magnetic field the optimal container for the \({}^{3}\)He should be a perfect sphere. A fused silica sphere with an inner diameter of 8 mm and an outer diameter of 12 mm was made from two hemispheres by diffusion bonding leaving only a small hole for cleaning and evacuation. This hole was closed in vacuum by a CO\({}_{2}\) laser and the inner volume was filled with a few mbars of \({}^3\)He via wall permeation. NMR-measurements on such a sample had coherence times of 5 min. While the hemispheres were produced with &lt; 1 \(\mu\)m deviation from sphericity, the bonding left a step of ca. 50 \(\mu\)m at maximum. The influence of such a mismatch, its orientation and materials in the direct vicinity of the sample are analyzed by FEM-simulations and discussed in view of coherence times and absolute fields.</description><identifier>EISSN: 2331-8422</identifier><identifier>DOI: 10.48550/arxiv.1508.00838</identifier><language>eng</language><publisher>Ithaca: Cornell University Library, arXiv.org</publisher><subject>Bonding ; Computer simulation ; Finite element method ; Fused silica ; Helium ; Hemispheres ; Magnetic fields ; Magnetic measurement ; Magnetometers ; NMR ; Nuclear magnetic resonance ; Signal strength ; Silicon dioxide</subject><ispartof>arXiv.org, 2015-09</ispartof><rights>2015. This work is published under http://arxiv.org/licenses/nonexclusive-distrib/1.0/ (the “License”). Notwithstanding the ProQuest Terms and Conditions, you may use this content in accordance with the terms of the License.</rights><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://www.proquest.com/docview/2077999582?pq-origsite=primo$$EHTML$$P50$$Gproquest$$Hfree_for_read</linktohtml><link.rule.ids>780,784,25753,27925,37012,44590</link.rule.ids></links><search><creatorcontrib>Maul, Andreas</creatorcontrib><creatorcontrib>Blümler, Peter</creatorcontrib><creatorcontrib>Heil, Werner</creatorcontrib><creatorcontrib>Nikiel, Anna</creatorcontrib><creatorcontrib>Otten, Ernst</creatorcontrib><creatorcontrib>Petrich, Andreas</creatorcontrib><creatorcontrib>Schmidt, Thomas</creatorcontrib><title>Spherical Fused Silica Cells Filled with Pure Helium for NMR-Magnetometry</title><title>arXiv.org</title><description>High magnetic fields (&gt; 1 T) are measured by NMR magnetometers with un-rivaled precision if the precessing spin sample provides long coherence times. The longest coherence times are found in diluted \({}^{3}\)He samples, which can be hyperpolarized for sufficient signal strength. In order to have minimal influence on the homogeneity and value of the measured magnetic field the optimal container for the \({}^{3}\)He should be a perfect sphere. A fused silica sphere with an inner diameter of 8 mm and an outer diameter of 12 mm was made from two hemispheres by diffusion bonding leaving only a small hole for cleaning and evacuation. This hole was closed in vacuum by a CO\({}_{2}\) laser and the inner volume was filled with a few mbars of \({}^3\)He via wall permeation. NMR-measurements on such a sample had coherence times of 5 min. While the hemispheres were produced with &lt; 1 \(\mu\)m deviation from sphericity, the bonding left a step of ca. 50 \(\mu\)m at maximum. The influence of such a mismatch, its orientation and materials in the direct vicinity of the sample are analyzed by FEM-simulations and discussed in view of coherence times and absolute fields.</description><subject>Bonding</subject><subject>Computer simulation</subject><subject>Finite element method</subject><subject>Fused silica</subject><subject>Helium</subject><subject>Hemispheres</subject><subject>Magnetic fields</subject><subject>Magnetic measurement</subject><subject>Magnetometers</subject><subject>NMR</subject><subject>Nuclear magnetic resonance</subject><subject>Signal strength</subject><subject>Silicon dioxide</subject><issn>2331-8422</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2015</creationdate><recordtype>article</recordtype><sourceid>PIMPY</sourceid><recordid>eNotjV1LwzAYRoMgOOZ-gHcBr1vf5m0-einFusGm4nY_kjZxGdk6k9aPf7-BXj2cc3EeQu4KyEvFOTzo-OO_8oKDygEUqisyYYhFpkrGbsgspT0AMCEZ5zghi_VpZ6NvdaDNmGxH1z5ciNY2hEQbH8LFffthR9_GaOncBj8eqOsjfVm9Zyv9cbRDf7BD_L0l106HZGf_OyWb5mlTz7Pl6_OiflxmmjOWCeOqUhjFrJCVAtXZUjknTWekMB0AMqFAaG5QCGyxNVhhWwA4LbvWosQpuf_LnmL_Odo0bPf9GI-Xxy0DKauq4orhGeKnTSA</recordid><startdate>20150909</startdate><enddate>20150909</enddate><creator>Maul, Andreas</creator><creator>Blümler, Peter</creator><creator>Heil, Werner</creator><creator>Nikiel, Anna</creator><creator>Otten, Ernst</creator><creator>Petrich, Andreas</creator><creator>Schmidt, Thomas</creator><general>Cornell University Library, arXiv.org</general><scope>8FE</scope><scope>8FG</scope><scope>ABJCF</scope><scope>ABUWG</scope><scope>AFKRA</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>CCPQU</scope><scope>DWQXO</scope><scope>HCIFZ</scope><scope>L6V</scope><scope>M7S</scope><scope>PIMPY</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PTHSS</scope></search><sort><creationdate>20150909</creationdate><title>Spherical Fused Silica Cells Filled with Pure Helium for NMR-Magnetometry</title><author>Maul, Andreas ; Blümler, Peter ; Heil, Werner ; Nikiel, Anna ; Otten, Ernst ; Petrich, Andreas ; Schmidt, Thomas</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a522-6bf946b82e679808de48ff7bdb76bd00326806a5b3663c3cb393c100fa7dce373</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2015</creationdate><topic>Bonding</topic><topic>Computer simulation</topic><topic>Finite element method</topic><topic>Fused silica</topic><topic>Helium</topic><topic>Hemispheres</topic><topic>Magnetic fields</topic><topic>Magnetic measurement</topic><topic>Magnetometers</topic><topic>NMR</topic><topic>Nuclear magnetic resonance</topic><topic>Signal strength</topic><topic>Silicon dioxide</topic><toplevel>online_resources</toplevel><creatorcontrib>Maul, Andreas</creatorcontrib><creatorcontrib>Blümler, Peter</creatorcontrib><creatorcontrib>Heil, Werner</creatorcontrib><creatorcontrib>Nikiel, Anna</creatorcontrib><creatorcontrib>Otten, Ernst</creatorcontrib><creatorcontrib>Petrich, Andreas</creatorcontrib><creatorcontrib>Schmidt, Thomas</creatorcontrib><collection>ProQuest SciTech Collection</collection><collection>ProQuest Technology Collection</collection><collection>Materials Science &amp; Engineering Collection</collection><collection>ProQuest Central (Alumni)</collection><collection>ProQuest Central</collection><collection>ProQuest Central Essentials</collection><collection>AUTh Library subscriptions: ProQuest Central</collection><collection>Technology Collection</collection><collection>ProQuest One Community College</collection><collection>ProQuest Central Korea</collection><collection>SciTech Premium Collection (Proquest) (PQ_SDU_P3)</collection><collection>ProQuest Engineering Collection</collection><collection>Engineering Database</collection><collection>Publicly Available Content Database (Proquest) (PQ_SDU_P3)</collection><collection>ProQuest One Academic Eastern Edition (DO NOT USE)</collection><collection>ProQuest One Academic</collection><collection>ProQuest One Academic UKI Edition</collection><collection>Engineering collection</collection><jtitle>arXiv.org</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Maul, Andreas</au><au>Blümler, Peter</au><au>Heil, Werner</au><au>Nikiel, Anna</au><au>Otten, Ernst</au><au>Petrich, Andreas</au><au>Schmidt, Thomas</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Spherical Fused Silica Cells Filled with Pure Helium for NMR-Magnetometry</atitle><jtitle>arXiv.org</jtitle><date>2015-09-09</date><risdate>2015</risdate><eissn>2331-8422</eissn><abstract>High magnetic fields (&gt; 1 T) are measured by NMR magnetometers with un-rivaled precision if the precessing spin sample provides long coherence times. The longest coherence times are found in diluted \({}^{3}\)He samples, which can be hyperpolarized for sufficient signal strength. In order to have minimal influence on the homogeneity and value of the measured magnetic field the optimal container for the \({}^{3}\)He should be a perfect sphere. A fused silica sphere with an inner diameter of 8 mm and an outer diameter of 12 mm was made from two hemispheres by diffusion bonding leaving only a small hole for cleaning and evacuation. This hole was closed in vacuum by a CO\({}_{2}\) laser and the inner volume was filled with a few mbars of \({}^3\)He via wall permeation. NMR-measurements on such a sample had coherence times of 5 min. While the hemispheres were produced with &lt; 1 \(\mu\)m deviation from sphericity, the bonding left a step of ca. 50 \(\mu\)m at maximum. The influence of such a mismatch, its orientation and materials in the direct vicinity of the sample are analyzed by FEM-simulations and discussed in view of coherence times and absolute fields.</abstract><cop>Ithaca</cop><pub>Cornell University Library, arXiv.org</pub><doi>10.48550/arxiv.1508.00838</doi><oa>free_for_read</oa></addata></record>
fulltext fulltext
identifier EISSN: 2331-8422
ispartof arXiv.org, 2015-09
issn 2331-8422
language eng
recordid cdi_proquest_journals_2077999582
source Publicly Available Content Database (Proquest) (PQ_SDU_P3)
subjects Bonding
Computer simulation
Finite element method
Fused silica
Helium
Hemispheres
Magnetic fields
Magnetic measurement
Magnetometers
NMR
Nuclear magnetic resonance
Signal strength
Silicon dioxide
title Spherical Fused Silica Cells Filled with Pure Helium for NMR-Magnetometry
url http://sfxeu10.hosted.exlibrisgroup.com/loughborough?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2024-12-26T14%3A05%3A46IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-proquest&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=Spherical%20Fused%20Silica%20Cells%20Filled%20with%20Pure%20Helium%20for%20NMR-Magnetometry&rft.jtitle=arXiv.org&rft.au=Maul,%20Andreas&rft.date=2015-09-09&rft.eissn=2331-8422&rft_id=info:doi/10.48550/arxiv.1508.00838&rft_dat=%3Cproquest%3E2077999582%3C/proquest%3E%3Cgrp_id%3Ecdi_FETCH-LOGICAL-a522-6bf946b82e679808de48ff7bdb76bd00326806a5b3663c3cb393c100fa7dce373%3C/grp_id%3E%3Coa%3E%3C/oa%3E%3Curl%3E%3C/url%3E&rft_id=info:oai/&rft_pqid=2077999582&rft_id=info:pmid/&rfr_iscdi=true