Pub Date : 2025-11-10eCollection Date: 2025-01-01DOI: 10.5194/mr-6-243-2025
Lucky N Kapoor, Natália Ružičková, Predrag Živadinović, Valentin Leitner, Maria Anna Sisak, Cecelia Mweka, Jeroen Dobbelaere, Georgios Katsaros, Paul Schanda
Conference travel contributes to the climate footprint of academic research. Here, we provide a quantitative estimate of the carbon emissions associated with conference attendance by analyzing travel data from participants of 10 international conferences in the field of magnetic resonance, namely EUROMAR, ENC and ICMRBS. We find that attending a EUROMAR conference produces, on average, more than 1 t . For the analyzed conferences outside Europe, the corresponding value is about 2-3 times higher, on average, with intercontinental trips amounting to up to 5 t. We compare these conference-related emissions to other activities associated with research and show that conference travel is a substantial portion of the total climate footprint of a researcher in magnetic resonance. We explore several strategies to reduce these emissions, including the impact of selecting conference venues more strategically and the possibility of decentralized conferences. Through a detailed comparison of train versus air travel - accounting for both direct and infrastructure-related emissions - we demonstrate that train travel offers considerable carbon savings. These data may provide a basis for strategic choices of future conferences in the field and for individuals deciding on their conference attendance.
{"title":"Quantifying the carbon footprint of conference travel: the case of NMR meetings.","authors":"Lucky N Kapoor, Natália Ružičková, Predrag Živadinović, Valentin Leitner, Maria Anna Sisak, Cecelia Mweka, Jeroen Dobbelaere, Georgios Katsaros, Paul Schanda","doi":"10.5194/mr-6-243-2025","DOIUrl":"10.5194/mr-6-243-2025","url":null,"abstract":"<p><p>Conference travel contributes to the climate footprint of academic research. Here, we provide a quantitative estimate of the carbon emissions associated with conference attendance by analyzing travel data from participants of 10 international conferences in the field of magnetic resonance, namely EUROMAR, ENC and ICMRBS. We find that attending a EUROMAR conference produces, on average, more than 1 t <math> <mrow><msub><mi>CO</mi> <mrow><mn>2</mn> <mspace></mspace> <mi>eq</mi> <mo>.</mo></mrow> </msub> </mrow> </math> . For the analyzed conferences outside Europe, the corresponding value is about 2-3 times higher, on average, with intercontinental trips amounting to up to 5 t. We compare these conference-related emissions to other activities associated with research and show that conference travel is a substantial portion of the total climate footprint of a researcher in magnetic resonance. We explore several strategies to reduce these emissions, including the impact of selecting conference venues more strategically and the possibility of decentralized conferences. Through a detailed comparison of train versus air travel - accounting for both direct and infrastructure-related emissions - we demonstrate that train travel offers considerable carbon savings. These data may provide a basis for strategic choices of future conferences in the field and for individuals deciding on their conference attendance.</p>","PeriodicalId":93333,"journal":{"name":"Magnetic resonance (Gottingen, Germany)","volume":"6 2","pages":"243-256"},"PeriodicalIF":0.0,"publicationDate":"2025-11-10","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.ncbi.nlm.nih.gov/pmc/articles/PMC12658769/pdf/","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145650229","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-09-03eCollection Date: 2025-01-01DOI: 10.5194/mr-6-229-2025
Jorge A Villanueva-Garibay, Andreas Tilch, Ana Paula Aguilar Alva, Guillaume Bouvignies, Frank Engelke, Fabien Ferrage, Agnes Glémot, Ulric B le Paige, Giulia Licciardi, Claudio Luchinat, Giacomo Parigi, Philippe Pelupessy, Enrico Ravera, Alessandro Ruda, Lucas Siemons, Olof Stenström, Jean-Max Tyburn
Combining high-resolution high-field nuclear magnetic resonance (NMR) with an evolution of spin systems at a low magnetic field offers many opportunities for the investigation of molecular motions and hyperpolarization and the exploration of field-dependent spin dynamics. Fast and reproducible transfer between high and low fields is required to minimize polarization losses due to longitudinal relaxation. Here, we introduce a new design of a sample shuttle that achieves remarkably high speeds ( 27 m s-1). This hybrid pneumatic-mechanical apparatus is compatible with conventional probes at the high-field center. We show applications in water relaxometry in solutions of paramagnetic ions, high-resolution proton relaxometry of a small molecule, and sample shuttling of a solution of a 42 kDa protein. Importantly, this fast sample shuttle (FSS) system is narrow, with a diameter of 6 mm for the sample shuttle container based on a standard 5 mm outer diameter glass tube, which should allow near access to the sample for magnetic manipulation at a low field.
高分辨率高场核磁共振(NMR)与低磁场下自旋系统的演化相结合,为分子运动和超极化的研究以及场相关自旋动力学的探索提供了许多机会。为了最大限度地减少由于纵向弛豫造成的极化损失,需要在高场和低场之间进行快速和可重复的转移。在这里,我们介绍了一种新设计的样品穿梭,可以达到非常高的速度(v max ~ 27 m s-1)。这种气动机械混合装置与传统的高场中心探头兼容。我们展示了在顺磁离子溶液中的水弛豫测量,小分子的高分辨率质子弛豫测量以及42 kDa蛋白质溶液的样品穿梭中的应用。重要的是,这种快速样品穿梭(FSS)系统很窄,基于标准外径5mm的玻璃管的样品穿梭容器直径为d = 6 mm,这应该允许在低场下接近样品进行磁操作。
{"title":"A fast sample shuttle to couple high and low magnetic fields and applications in high-resolution relaxometry.","authors":"Jorge A Villanueva-Garibay, Andreas Tilch, Ana Paula Aguilar Alva, Guillaume Bouvignies, Frank Engelke, Fabien Ferrage, Agnes Glémot, Ulric B le Paige, Giulia Licciardi, Claudio Luchinat, Giacomo Parigi, Philippe Pelupessy, Enrico Ravera, Alessandro Ruda, Lucas Siemons, Olof Stenström, Jean-Max Tyburn","doi":"10.5194/mr-6-229-2025","DOIUrl":"10.5194/mr-6-229-2025","url":null,"abstract":"<p><p>Combining high-resolution high-field nuclear magnetic resonance (NMR) with an evolution of spin systems at a low magnetic field offers many opportunities for the investigation of molecular motions and hyperpolarization and the exploration of field-dependent spin dynamics. Fast and reproducible transfer between high and low fields is required to minimize polarization losses due to longitudinal relaxation. Here, we introduce a new design of a sample shuttle that achieves remarkably high speeds ( <math> <mrow><msub><mi>v</mi> <mi>max</mi></msub> </mrow> </math> <math><mo>∼</mo></math> 27 m s<sup>-1</sup>). This hybrid pneumatic-mechanical apparatus is compatible with conventional probes at the high-field center. We show applications in water relaxometry in solutions of paramagnetic ions, high-resolution proton relaxometry of a small molecule, and sample shuttling of a solution of a 42 kDa protein. Importantly, this fast sample shuttle (FSS) system is narrow, with a diameter of <math><mi>d</mi></math> <math><mo>=</mo></math> 6 mm for the sample shuttle container based on a standard 5 mm outer diameter glass tube, which should allow near access to the sample for magnetic manipulation at a low field.</p>","PeriodicalId":93333,"journal":{"name":"Magnetic resonance (Gottingen, Germany)","volume":"6 2","pages":"229-241"},"PeriodicalIF":0.0,"publicationDate":"2025-09-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.ncbi.nlm.nih.gov/pmc/articles/PMC12614101/pdf/","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145544112","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-07-29eCollection Date: 2025-01-01DOI: 10.5194/mr-6-199-2025
Sagar Wadhwa, Nan Wang, Klaus-Martin Reichert, Manuel Butzer, Omar Nassar, Mazin Jouda, Jan G Korvink, Ulrich Gengenbach, Dario Mager, Martin Ungerer
Additive manufacturing has enabled rapid prototyping of components with minimum investment in specific fabrication infrastructure. These tools allow for a fast iteration from design to functional prototypes within days or even hours. Such prototyping technologies exist in many fields, including three-dimensional mechanical components and printed electric circuit boards (PCBs) for electrical connectivity, to mention two. In the case of nuclear magnetic resonance (NMR) spectroscopy, one needs the combination of both fields; we need to fabricate three-dimensional electrically conductive tracks as coils that are wrapped around a sample container. Fabricating such structures is difficult (e.g., six-axis micro-milling) or simply not possible with conventional methods. In this paper, we modified an additive manufacturing method that is based on the extrusion of conductive ink to fast-prototype solenoidal coil designs for NMR. These NMR coils need to be as close to the sample as possible and, by their shape, have specific inductive values. The performance of the designs was first investigated using electromagnetic field simulations and circuit simulations. The coil found to have optimal parameters for NMR was fabricated by extrusion printing, and its performance was tested in a 1.05 imaging magnet. The objective is to demonstrate reproducible rapid prototyping of complicated designs with high precision that, as a side effect, hardly produces material waste during production.
{"title":"Automated manufacturing process for sustainable prototyping of nuclear magnetic resonance transceivers.","authors":"Sagar Wadhwa, Nan Wang, Klaus-Martin Reichert, Manuel Butzer, Omar Nassar, Mazin Jouda, Jan G Korvink, Ulrich Gengenbach, Dario Mager, Martin Ungerer","doi":"10.5194/mr-6-199-2025","DOIUrl":"10.5194/mr-6-199-2025","url":null,"abstract":"<p><p>Additive manufacturing has enabled rapid prototyping of components with minimum investment in specific fabrication infrastructure. These tools allow for a fast iteration from design to functional prototypes within days or even hours. Such prototyping technologies exist in many fields, including three-dimensional mechanical components and printed electric circuit boards (PCBs) for electrical connectivity, to mention two. In the case of nuclear magnetic resonance (NMR) spectroscopy, one needs the combination of both fields; we need to fabricate three-dimensional electrically conductive tracks as coils that are wrapped around a sample container. Fabricating such structures is difficult (e.g., six-axis micro-milling) or simply not possible with conventional methods. In this paper, we modified an additive manufacturing method that is based on the extrusion of conductive ink to fast-prototype solenoidal coil designs for NMR. These NMR coils need to be as close to the sample as possible and, by their shape, have specific inductive values. The performance of the designs was first investigated using electromagnetic field simulations and circuit simulations. The coil found to have optimal parameters for NMR was fabricated by extrusion printing, and its performance was tested in a 1.05 <math><mrow><mi>T</mi></mrow> </math> imaging magnet. The objective is to demonstrate reproducible rapid prototyping of complicated designs with high precision that, as a side effect, hardly produces material waste during production.</p>","PeriodicalId":93333,"journal":{"name":"Magnetic resonance (Gottingen, Germany)","volume":"6 2","pages":"199-210"},"PeriodicalIF":0.0,"publicationDate":"2025-07-29","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.ncbi.nlm.nih.gov/pmc/articles/PMC12332885/pdf/","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"144818591","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-07-17eCollection Date: 2025-01-01DOI: 10.5194/mr-6-183-2025
Jesús I Martínez, Susana Frago, Milagros Medina, Inés García-Rubio
<p><p>Flavoproteins are a versatile class of proteins involved in numerous biological processes, including redox reactions, electron transfer, and signal transduction, often relying on their ability to stabilize different oxidation states of their flavin cofactor. A critical feature of flavin cofactors is their capacity to achieve, within particular protein environments, a semiquinone state that plays a pivotal role in mediating single-electron transfer events and that is key to understanding flavoprotein reactivity. Hyperfine interactions between the unpaired electron and magnetic nuclei in the isoalloxazine ring provide valuable insights into the semiquinone state and its mechanistic roles. This study investigates the hyperfine interactions of isotopically labeled flavodoxin (Fld) with <math> <mrow><msup><mi></mi> <mn>13</mn></msup> <mi>C</mi></mrow> </math> and <math> <mrow><msup><mi></mi> <mn>15</mn></msup> <mi>N</mi></mrow> </math> in specific positions of the flavin mononucleotide (FMN) ring using advanced electron paramagnetic resonance (EPR) techniques. The combination of continuous-wave (CW) EPR at the X-band and ELDOR-detected NMR and HYSCORE at the Q-band revealed a strong and anisotropic hyperfine interaction with the nucleus of <math> <mrow><msup><mi></mi> <mn>13</mn></msup> <mi>C</mi></mrow> </math> at 4a and yielded principal tensor values of 40, <math><mrow><mo>-</mo> <mn>13.5</mn></mrow> </math> , and <math><mrow><mo>-</mo> <mn>9</mn></mrow> </math> MHz, the first of which is associated with the axis perpendicular to the flavin plane. On the other hand, as predicted, the hyperfine interaction with the <math> <mrow><msup><mi></mi> <mn>13</mn></msup> <mi>C</mi></mrow> </math> nucleus in position 2 was minimal. Additionally, HYSCORE experiments on <math> <mrow><msup><mi></mi> <mn>15</mn></msup> <mi>N</mi></mrow> </math> -FMN-labeled Fld provided precise axial hyperfine parameters, i.e., (74, 5.6, 5.6) <math><mrow><mi>MHz</mi></mrow> </math> for <math> <mrow><msup><mi></mi> <mn>15</mn></msup> <mi>N</mi></mrow> </math> (5) and (38, 3.2, 3.2) <math><mrow><mi>MHz</mi></mrow> </math> for <math> <mrow><msup><mi></mi> <mn>15</mn></msup> <mi>N</mi></mrow> </math> (10). These were used to refine quadrupole tensor values for <math> <mrow><msup><mi></mi> <mn>14</mn></msup> <mi>N</mi></mrow> </math> nuclei through isotope-dependent scaling. These results showcase the potential of combining CW EPR, ELDOR-detected NMR, and HYSCORE with isotopic labeling to probe electronic and nuclear interactions in flavoproteins. The new data complete and refine the existing experimental map for the electronic structure of the flavin cofactor and expose systematic divergences between the calculated and experimental values of hyperfine couplings of the atoms that contribute most to the semi-occupied orbital (SOMO). This could indicate a slight but significant shift in the unpaired electron density from position 4a towards the central nitrogens of the pyrazine ri
{"title":"Determining large hyperfine interactions of a model flavoprotein in the semiquinone state using pulse EPR (electron paramagnetic resonance) techniques.","authors":"Jesús I Martínez, Susana Frago, Milagros Medina, Inés García-Rubio","doi":"10.5194/mr-6-183-2025","DOIUrl":"10.5194/mr-6-183-2025","url":null,"abstract":"<p><p>Flavoproteins are a versatile class of proteins involved in numerous biological processes, including redox reactions, electron transfer, and signal transduction, often relying on their ability to stabilize different oxidation states of their flavin cofactor. A critical feature of flavin cofactors is their capacity to achieve, within particular protein environments, a semiquinone state that plays a pivotal role in mediating single-electron transfer events and that is key to understanding flavoprotein reactivity. Hyperfine interactions between the unpaired electron and magnetic nuclei in the isoalloxazine ring provide valuable insights into the semiquinone state and its mechanistic roles. This study investigates the hyperfine interactions of isotopically labeled flavodoxin (Fld) with <math> <mrow><msup><mi></mi> <mn>13</mn></msup> <mi>C</mi></mrow> </math> and <math> <mrow><msup><mi></mi> <mn>15</mn></msup> <mi>N</mi></mrow> </math> in specific positions of the flavin mononucleotide (FMN) ring using advanced electron paramagnetic resonance (EPR) techniques. The combination of continuous-wave (CW) EPR at the X-band and ELDOR-detected NMR and HYSCORE at the Q-band revealed a strong and anisotropic hyperfine interaction with the nucleus of <math> <mrow><msup><mi></mi> <mn>13</mn></msup> <mi>C</mi></mrow> </math> at 4a and yielded principal tensor values of 40, <math><mrow><mo>-</mo> <mn>13.5</mn></mrow> </math> , and <math><mrow><mo>-</mo> <mn>9</mn></mrow> </math> MHz, the first of which is associated with the axis perpendicular to the flavin plane. On the other hand, as predicted, the hyperfine interaction with the <math> <mrow><msup><mi></mi> <mn>13</mn></msup> <mi>C</mi></mrow> </math> nucleus in position 2 was minimal. Additionally, HYSCORE experiments on <math> <mrow><msup><mi></mi> <mn>15</mn></msup> <mi>N</mi></mrow> </math> -FMN-labeled Fld provided precise axial hyperfine parameters, i.e., (74, 5.6, 5.6) <math><mrow><mi>MHz</mi></mrow> </math> for <math> <mrow><msup><mi></mi> <mn>15</mn></msup> <mi>N</mi></mrow> </math> (5) and (38, 3.2, 3.2) <math><mrow><mi>MHz</mi></mrow> </math> for <math> <mrow><msup><mi></mi> <mn>15</mn></msup> <mi>N</mi></mrow> </math> (10). These were used to refine quadrupole tensor values for <math> <mrow><msup><mi></mi> <mn>14</mn></msup> <mi>N</mi></mrow> </math> nuclei through isotope-dependent scaling. These results showcase the potential of combining CW EPR, ELDOR-detected NMR, and HYSCORE with isotopic labeling to probe electronic and nuclear interactions in flavoproteins. The new data complete and refine the existing experimental map for the electronic structure of the flavin cofactor and expose systematic divergences between the calculated and experimental values of hyperfine couplings of the atoms that contribute most to the semi-occupied orbital (SOMO). This could indicate a slight but significant shift in the unpaired electron density from position 4a towards the central nitrogens of the pyrazine ri","PeriodicalId":93333,"journal":{"name":"Magnetic resonance (Gottingen, Germany)","volume":"6 2","pages":"183-197"},"PeriodicalIF":0.0,"publicationDate":"2025-07-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.ncbi.nlm.nih.gov/pmc/articles/PMC12326372/pdf/","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"144796350","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-07-17eCollection Date: 2025-01-01DOI: 10.5194/mr-6-173-2025
Mengjia He, Neil MacKinnon, Dominique Buyens, Burkhard Luy, Jan G Korvink
The implementation of parallel nuclear magnetic resonance detection aims to enhance measurement throughput in support of high-throughput-screening applications, including, for example, drug discovery. In support of modern pulse sequences and solvent suppression methods, each detection site must have independent pulsed field gradient capabilities. Hereby, a challenge is introduced in which the local gradients applied in parallel detectors introduce field spillover into adjacent channels, leading to spin dephasing and, hence, to signal suppression. This study proposes a compensation scheme employing optimized pulses to achieve coherence locking during gradient pulse periods. The design of coherence-locking pulses utilizes optimal control to address gradient-induced field inhomogeneity. These pulses are applied in a pulsed-gradient spin echo (PGSE) experiment and a parallel heteronuclear single quantum coherence (HSQC) experiment, demonstrating their effectiveness in protecting the desired coherences from gradient field spillover. This compensation scheme presents a valuable solution for magnetic resonance probes equipped with parallel and independently switchable gradient coils.
{"title":"Coherence locking in a parallel nuclear magnetic resonance probe defends against gradient field spillover.","authors":"Mengjia He, Neil MacKinnon, Dominique Buyens, Burkhard Luy, Jan G Korvink","doi":"10.5194/mr-6-173-2025","DOIUrl":"10.5194/mr-6-173-2025","url":null,"abstract":"<p><p>The implementation of parallel nuclear magnetic resonance detection aims to enhance measurement throughput in support of high-throughput-screening applications, including, for example, drug discovery. In support of modern pulse sequences and solvent suppression methods, each detection site must have independent pulsed field gradient capabilities. Hereby, a challenge is introduced in which the local gradients applied in parallel detectors introduce field spillover into adjacent channels, leading to spin dephasing and, hence, to signal suppression. This study proposes a compensation scheme employing optimized pulses to achieve coherence locking during gradient pulse periods. The design of coherence-locking pulses utilizes optimal control to address gradient-induced field inhomogeneity. These pulses are applied in a pulsed-gradient spin echo (PGSE) experiment and a parallel heteronuclear single quantum coherence (HSQC) experiment, demonstrating their effectiveness in protecting the desired coherences from gradient field spillover. This compensation scheme presents a valuable solution for magnetic resonance probes equipped with parallel and independently switchable gradient coils.</p>","PeriodicalId":93333,"journal":{"name":"Magnetic resonance (Gottingen, Germany)","volume":"6 2","pages":"173-181"},"PeriodicalIF":0.0,"publicationDate":"2025-07-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.ncbi.nlm.nih.gov/pmc/articles/PMC12302023/pdf/","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"144736011","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-07-16eCollection Date: 2025-01-01DOI: 10.5194/mr-6-143-2025
Jop W Wolffs, Jennifer S Gómez, Gerrit E Janssen, Gilles A de Wijs, Arno P M Kentgens
Nuclear quadrupole resonance (NQR), a technique related to nuclear magnetic resonance, is extremely sensitive to local crystal composition and structure. Unfortunately, in disordered materials, this sensitivity also leads to very large linewidths, presenting a technical challenge and requiring a serious time investment to get a full spectrum. Here, we describe our newly developed, automated NQR set-up to acquire high-quality wide-line spectra. Using this set-up, we carried out 127I NQR on three mixed-cation lead-halide perovskites (LHPs) of the form MA x FA1-x PbI3 (where MA denotes methylammonium; FA denotes formamidinium; and 0.25, 0.50 and 0.75) at various temperatures. We achieve a signal-to-noise ratio of up to for lineshapes with a full width at half maximum of acquired with a spectral width of 20 MHz in the course of 2-3 d. The spectra, which at least partially exhibit features encoding structural information, are interpreted using a statistical model. This model finds a degree of MA-MA and FA-FA clustering ( ). This proof-of-principle for both the wide-line NQR set-up and the statistical model widens the applicability of an underutilised avenue of non-invasive structural research.
{"title":"Automated wide-line nuclear quadrupole resonance of mixed-cation lead-halide perovskites.","authors":"Jop W Wolffs, Jennifer S Gómez, Gerrit E Janssen, Gilles A de Wijs, Arno P M Kentgens","doi":"10.5194/mr-6-143-2025","DOIUrl":"10.5194/mr-6-143-2025","url":null,"abstract":"<p><p>Nuclear quadrupole resonance (NQR), a technique related to nuclear magnetic resonance, is extremely sensitive to local crystal composition and structure. Unfortunately, in disordered materials, this sensitivity also leads to very large linewidths, presenting a technical challenge and requiring a serious time investment to get a full spectrum. Here, we describe our newly developed, automated NQR set-up to acquire high-quality wide-line spectra. Using this set-up, we carried out <sup>127</sup>I NQR on three mixed-cation lead-halide perovskites (LHPs) of the form MA <sub><i>x</i></sub> FA<sub>1-<i>x</i></sub> PbI<sub>3</sub> (where MA denotes methylammonium; FA denotes formamidinium; and <math><mrow><mi>x</mi> <mspace></mspace> <mo>=</mo></mrow> </math> 0.25, 0.50 and 0.75) at various temperatures. We achieve a signal-to-noise ratio of up to <math><mrow><mo>∼</mo> <mspace></mspace> <mn>400</mn></mrow> </math> for lineshapes with a full width at half maximum of <math><mrow><mo>∼</mo> <mspace></mspace> <mn>2.5</mn> <mspace></mspace> <mi>MHz</mi></mrow> </math> acquired with a spectral width of 20 MHz in the course of 2-3 d. The spectra, which at least partially exhibit features encoding structural information, are interpreted using a statistical model. This model finds a degree of MA-MA and FA-FA clustering ( <math><mrow><mn>0.2</mn> <mspace></mspace> <mo>≤</mo> <mspace></mspace> <mi>S</mi> <mspace></mspace> <mo>≤</mo> <mspace></mspace> <mn>0.35</mn></mrow> </math> ). This proof-of-principle for both the wide-line NQR set-up and the statistical model widens the applicability of an underutilised avenue of non-invasive structural research.</p>","PeriodicalId":93333,"journal":{"name":"Magnetic resonance (Gottingen, Germany)","volume":"6 2","pages":"143-155"},"PeriodicalIF":0.0,"publicationDate":"2025-07-16","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.ncbi.nlm.nih.gov/pmc/articles/PMC12285786/pdf/","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"144700596","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-07-16eCollection Date: 2025-01-01DOI: 10.5194/mr-6-157-2025
Tayeb Kakeshpour, Martin D Gelenter, Jinfa Ying, Ad Bax
Standard solution NMR measurements use 5 mm outer diameter (OD) sample tubes that require ca. 0.5 mL of solvent to minimize "end effects" on magnetic field homogeneity in the active volume of the sample. Shigemi cells reduce the solvent requirement to ca. 0.29 mL. At high ionic strength or at ultrahigh magnetic fields, smaller OD samples are needed to study samples in conductive, radiofrequency-absorbing solvents such as water. We demonstrate an effective and inexpensive alternative for reducing the active sample volume to 0.13 mL by 3D printing ellipsoidal shaped cells that are inserted into 5 mm OD NMR tubes. Static magnetic susceptibility, , of printer resin was measured using a simple slice-selection pulse sequence. We found that the of water increases linearly with NaCl concentration from to ppm for 0 to 2 M NaCl. The of D2O was measured to be ppm. The susceptibility difference between the resin ( ppm) and water can be minimized by paramagnetic doping of the resin. Such doping was found to be unnecessary for obtaining high-quality protein NMR spectra when using ellipsoidal-shaped cells that are insensitive to susceptibility mismatching. The microcells offer outstanding radiofrequency (RF) and good homogeneities. Integrated 600 MHz heteronuclear single quantum coherence (HSQC) signal intensities for the microcell sample in phosphate-buffered saline (PBS) buffer were % lower than for 0.5 mL of the same protein solution in a regular 5 mm sample tube. The cell is demonstrated for N-acetylated -synuclein in PBS buffer and for observing tetramerization of melittin at 2 M NaCl.
{"title":"3D-printed microcell for protein NMR at high ionic strengths and small sample volumes.","authors":"Tayeb Kakeshpour, Martin D Gelenter, Jinfa Ying, Ad Bax","doi":"10.5194/mr-6-157-2025","DOIUrl":"10.5194/mr-6-157-2025","url":null,"abstract":"<p><p>Standard solution NMR measurements use 5 mm outer diameter (OD) sample tubes that require ca. 0.5 mL of solvent to minimize \"end effects\" on magnetic field homogeneity in the active volume of the sample. Shigemi cells reduce the solvent requirement to ca. 0.29 mL. At high ionic strength or at ultrahigh magnetic fields, smaller OD samples are needed to study samples in conductive, radiofrequency-absorbing solvents such as water. We demonstrate an effective and inexpensive alternative for reducing the active sample volume to 0.13 mL by 3D printing ellipsoidal shaped cells that are inserted into 5 mm OD NMR tubes. Static magnetic susceptibility, <math><mi>χ</mi></math> , of printer resin was measured using a simple slice-selection pulse sequence. We found that the <math><mi>χ</mi></math> of water increases linearly with NaCl concentration from <math><mrow><mo>-</mo> <mn>9.05</mn></mrow> </math> to <math><mrow><mo>-</mo> <mn>8.65</mn></mrow> </math> ppm for 0 to 2 M NaCl. The <math><mi>χ</mi></math> of D<sub>2</sub>O was measured to be <math><mrow><mo>-</mo> <mn>9.01</mn></mrow> </math> ppm. The susceptibility difference between the resin ( <math><mrow><mi>χ</mi> <mo>=</mo> <mo>-</mo> <mn>9.40</mn></mrow> </math> ppm) and water can be minimized by paramagnetic doping of the resin. Such doping was found to be unnecessary for obtaining high-quality protein NMR spectra when using ellipsoidal-shaped cells that are insensitive to susceptibility mismatching. The microcells offer outstanding radiofrequency (RF) and good <math> <mrow><msub><mi>B</mi> <mi>o</mi></msub> </mrow> </math> homogeneities. Integrated 600 MHz heteronuclear single quantum coherence (HSQC) signal intensities for the microcell sample in phosphate-buffered saline (PBS) buffer were <math><mrow><mn>6.5</mn> <mo>±</mo> <mn>4</mn></mrow> </math> % lower than for 0.5 mL of the same protein solution in a regular 5 mm sample tube. The cell is demonstrated for N-acetylated <math><mi>α</mi></math> -synuclein in PBS buffer and for observing tetramerization of melittin at 2 M NaCl.</p>","PeriodicalId":93333,"journal":{"name":"Magnetic resonance (Gottingen, Germany)","volume":"6 2","pages":"157-172"},"PeriodicalIF":0.0,"publicationDate":"2025-07-16","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.ncbi.nlm.nih.gov/pmc/articles/PMC12296210/pdf/","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"144736010","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-07-14eCollection Date: 2025-01-01DOI: 10.5194/mr-6-131-2025
Yi Jiun Tan, Elwy H Abdelkader, Iresha D Herath, Ansis Maleckis, Gottfried Otting
<p><p>Using cell-free protein synthesis, the protein G B1 domain (GB1) was prepared with uniform high-level substitution of leucine by (2 <math><mi>S</mi></math> ,4 <math><mi>S</mi></math> )-5-fluoroleucine (FLeu1), (2 <math><mi>S</mi></math> ,4 <math><mi>R</mi></math> )-5-fluoroleucine (FLeu2), or 5,5<sup>'</sup>-difluoroleucine (diFLeu). <math> <mrow><msup><mi></mi> <mn>19</mn></msup> <mi>F</mi></mrow> </math> nuclear magnetic resonance (NMR) spectra showed chemical shift ranges spanning more than 9 <math><mrow><mi>ppm</mi></mrow> </math> . Through-space scalar <math> <mrow><msup><mi></mi> <mn>19</mn></msup> <mi>F</mi> <msup><mtext>-</mtext> <mn>19</mn></msup> <mi>F</mi></mrow> </math> couplings between <math> <mrow><msub><mi>CH</mi> <mn>2</mn></msub> <mi>F</mi></mrow> </math> groups arising from transient fluorine-fluorine contacts are readily manifested in [ <math> <mrow><msup><mi></mi> <mn>19</mn></msup> <mi>F</mi></mrow> </math> , <math> <mrow><msup><mi></mi> <mn>19</mn></msup> <mi>F</mi></mrow> </math> ]-TOCSY spectra. The <math> <mrow><msup><mi></mi> <mn>19</mn></msup> <mi>F</mi></mrow> </math> chemical shifts correlate with the three-bond <math> <mrow><msup><mi></mi> <mn>1</mn></msup> <mi>H</mi></mrow> </math> - <math> <mrow><msup><mi></mi> <mn>19</mn></msup> <mi>F</mi></mrow> </math> couplings ( <math> <mrow><msup><mi></mi> <mn>3</mn></msup> <msub><mi>J</mi> <mi>HF</mi></msub> </mrow> </math> ), confirming the <math><mi>γ</mi></math> -gauche effect as the predominant determinant of the <math> <mrow><msup><mi></mi> <mn>19</mn></msup> <mi>F</mi></mrow> </math> chemical shifts of the <math> <mrow><msub><mi>CH</mi> <mn>2</mn></msub> <mi>F</mi></mrow> </math> groups. Different <math> <mrow><msup><mi></mi> <mn>3</mn></msup> <msub><mi>J</mi> <mi>HF</mi></msub> </mrow> </math> couplings of different <math> <mrow><msub><mi>CH</mi> <mn>2</mn></msub> <mi>F</mi></mrow> </math> groups indicate that the rotation of the <math> <mrow><msub><mi>CH</mi> <mn>2</mn></msub> <mi>F</mi></mrow> </math> groups can be sufficiently restricted in different protein environments to result in the preferential population of a single rotamer. The <math> <mrow><msup><mi></mi> <mn>3</mn></msup> <msub><mi>J</mi> <mi>HF</mi></msub> </mrow> </math> couplings also show that <math> <mrow><msub><mi>CH</mi> <mn>2</mn></msub> <mi>F</mi></mrow> </math> groups populate the different rotameric states differently in the 5,5<sup>'</sup>-difluoroleucine residues than in the monofluoroleucine analogues, showing that two <math> <mrow><msub><mi>CH</mi> <mn>2</mn></msub> <mi>F</mi></mrow> </math> groups in close proximity influence each other's conformation. Nonetheless, the <math> <mrow><msup><mi></mi> <mn>19</mn></msup> <mi>F</mi></mrow> </math> resonances of the <math> <mrow><msup><mi>C</mi> <mrow><mi>δ</mi> <mn>1</mn></mrow> </msup> <msub><mi>H</mi> <mn>2</mn></msub> <mi>F</mi></mrow> </math> and <math> <mrow><msup><mi>C</mi> <mrow><mi>δ</mi> <mn>2</mn></mrow> </msup> <msub><mi>H</mi>
{"title":"Inter-residue through-space scalar <sup>19</sup>F-<sup>19</sup>F couplings between CH<sub>2</sub>F groups in a protein.","authors":"Yi Jiun Tan, Elwy H Abdelkader, Iresha D Herath, Ansis Maleckis, Gottfried Otting","doi":"10.5194/mr-6-131-2025","DOIUrl":"10.5194/mr-6-131-2025","url":null,"abstract":"<p><p>Using cell-free protein synthesis, the protein G B1 domain (GB1) was prepared with uniform high-level substitution of leucine by (2 <math><mi>S</mi></math> ,4 <math><mi>S</mi></math> )-5-fluoroleucine (FLeu1), (2 <math><mi>S</mi></math> ,4 <math><mi>R</mi></math> )-5-fluoroleucine (FLeu2), or 5,5<sup>'</sup>-difluoroleucine (diFLeu). <math> <mrow><msup><mi></mi> <mn>19</mn></msup> <mi>F</mi></mrow> </math> nuclear magnetic resonance (NMR) spectra showed chemical shift ranges spanning more than 9 <math><mrow><mi>ppm</mi></mrow> </math> . Through-space scalar <math> <mrow><msup><mi></mi> <mn>19</mn></msup> <mi>F</mi> <msup><mtext>-</mtext> <mn>19</mn></msup> <mi>F</mi></mrow> </math> couplings between <math> <mrow><msub><mi>CH</mi> <mn>2</mn></msub> <mi>F</mi></mrow> </math> groups arising from transient fluorine-fluorine contacts are readily manifested in [ <math> <mrow><msup><mi></mi> <mn>19</mn></msup> <mi>F</mi></mrow> </math> , <math> <mrow><msup><mi></mi> <mn>19</mn></msup> <mi>F</mi></mrow> </math> ]-TOCSY spectra. The <math> <mrow><msup><mi></mi> <mn>19</mn></msup> <mi>F</mi></mrow> </math> chemical shifts correlate with the three-bond <math> <mrow><msup><mi></mi> <mn>1</mn></msup> <mi>H</mi></mrow> </math> - <math> <mrow><msup><mi></mi> <mn>19</mn></msup> <mi>F</mi></mrow> </math> couplings ( <math> <mrow><msup><mi></mi> <mn>3</mn></msup> <msub><mi>J</mi> <mi>HF</mi></msub> </mrow> </math> ), confirming the <math><mi>γ</mi></math> -gauche effect as the predominant determinant of the <math> <mrow><msup><mi></mi> <mn>19</mn></msup> <mi>F</mi></mrow> </math> chemical shifts of the <math> <mrow><msub><mi>CH</mi> <mn>2</mn></msub> <mi>F</mi></mrow> </math> groups. Different <math> <mrow><msup><mi></mi> <mn>3</mn></msup> <msub><mi>J</mi> <mi>HF</mi></msub> </mrow> </math> couplings of different <math> <mrow><msub><mi>CH</mi> <mn>2</mn></msub> <mi>F</mi></mrow> </math> groups indicate that the rotation of the <math> <mrow><msub><mi>CH</mi> <mn>2</mn></msub> <mi>F</mi></mrow> </math> groups can be sufficiently restricted in different protein environments to result in the preferential population of a single rotamer. The <math> <mrow><msup><mi></mi> <mn>3</mn></msup> <msub><mi>J</mi> <mi>HF</mi></msub> </mrow> </math> couplings also show that <math> <mrow><msub><mi>CH</mi> <mn>2</mn></msub> <mi>F</mi></mrow> </math> groups populate the different rotameric states differently in the 5,5<sup>'</sup>-difluoroleucine residues than in the monofluoroleucine analogues, showing that two <math> <mrow><msub><mi>CH</mi> <mn>2</mn></msub> <mi>F</mi></mrow> </math> groups in close proximity influence each other's conformation. Nonetheless, the <math> <mrow><msup><mi></mi> <mn>19</mn></msup> <mi>F</mi></mrow> </math> resonances of the <math> <mrow><msup><mi>C</mi> <mrow><mi>δ</mi> <mn>1</mn></mrow> </msup> <msub><mi>H</mi> <mn>2</mn></msub> <mi>F</mi></mrow> </math> and <math> <mrow><msup><mi>C</mi> <mrow><mi>δ</mi> <mn>2</mn></mrow> </msup> <msub><mi>H</mi>","PeriodicalId":93333,"journal":{"name":"Magnetic resonance (Gottingen, Germany)","volume":"6 2","pages":"131-142"},"PeriodicalIF":0.0,"publicationDate":"2025-07-14","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.ncbi.nlm.nih.gov/pmc/articles/PMC12281167/pdf/","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"144700597","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-06-03eCollection Date: 2025-01-01DOI: 10.5194/mr-6-119-2025
Evgeny Nimerovsky, Jonas Mehrens, Loren B Andreas
Enhanced transverse relaxation near rotary resonance conditions is a well-documented effect for anisotropic solid samples undergoing magic-angle spinning (MAS). We report transverse signal decay associated with rotary resonance conditions for rotating liquids, a surprising observation, since first-order anisotropic interactions are averaged at a much faster timescale compared with the spinning frequency. We report measurements of and signal intensities under spin lock for spinning samples of polybutadiene rubber, polyethylene glycol solution, and 99.96 % . A drastic reduction in spin-lock signal intensities is observed when the spin-lock frequency matches 1 or 2 times the MAS rate. In addition, oscillations of the signal are observed, consistent with a coherent origin of the effect, a pseudo rotary resonance relaxation dispersion (pseudo-RRD). Through simulations, we qualitatively describe the appearance of pseudo-RRD, which can be explained by time dependence caused by sample rotation and an inhomogeneous field, the origin of which is an instrumental imperfection. Consideration of this effect is important for MAS experiments based on rotary resonance conditions and motivates the design of new MAS coils with improved radio frequency (RF)-field homogeneity.
{"title":"Pseudo rotary resonance relaxation dispersion effects in isotropic samples.","authors":"Evgeny Nimerovsky, Jonas Mehrens, Loren B Andreas","doi":"10.5194/mr-6-119-2025","DOIUrl":"10.5194/mr-6-119-2025","url":null,"abstract":"<p><p>Enhanced transverse relaxation near rotary resonance conditions is a well-documented effect for anisotropic solid samples undergoing magic-angle spinning (MAS). We report transverse signal decay associated with rotary resonance conditions for rotating liquids, a surprising observation, since first-order anisotropic interactions are averaged at a much faster timescale compared with the spinning frequency. We report measurements of <math> <mrow><msup><mi></mi> <mn>13</mn></msup> <mi>C</mi></mrow> </math> and <math> <mrow><msup><mi></mi> <mn>1</mn></msup> <mi>H</mi></mrow> </math> signal intensities under spin lock for spinning samples of polybutadiene rubber, polyethylene glycol solution, and 99.96 % <math> <mrow><msub><mi>D</mi> <mn>2</mn></msub> <mi>O</mi></mrow> </math> . A drastic reduction in spin-lock signal intensities is observed when the spin-lock frequency matches 1 or 2 times the MAS rate. In addition, oscillations of the signal are observed, consistent with a coherent origin of the effect, a pseudo rotary resonance relaxation dispersion (pseudo-RRD). Through simulations, we qualitatively describe the appearance of pseudo-RRD, which can be explained by time dependence caused by sample rotation and an inhomogeneous field, the origin of which is an instrumental imperfection. Consideration of this effect is important for MAS experiments based on rotary resonance conditions and motivates the design of new MAS coils with improved radio frequency (RF)-field homogeneity.</p>","PeriodicalId":93333,"journal":{"name":"Magnetic resonance (Gottingen, Germany)","volume":"6 1","pages":"119-129"},"PeriodicalIF":0.0,"publicationDate":"2025-06-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.ncbi.nlm.nih.gov/pmc/articles/PMC12247080/pdf/","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"144628062","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-04-17eCollection Date: 2025-01-01DOI: 10.5194/mr-6-113-2025
Charles-Emmanuel Dutoit, Raffaella Soleti, Jean-Marie Doux, Vincent Pelé, Véronique Boireau, Christian Jordy, Simon Pondaven, Hervé Vezin
Usually, conventional electron paramagnetic resonance (EPR) spectroscopy and imaging employ a microwave cavity operating at X-band, i.e., with an excitation frequency of around 9.6 GHz, and this remains the most popular mode for the magnetic characterization of lithium batteries to date. Here, we provide the first low-frequency EPR investigations with respect to monitoring the metallic lithium structures in solid-state pouch cell batteries. We show that L-band, i.e., a microwave frequency of around 1.01 GHz, is an invaluable method to probe the electrode components directly through a standard pouch cell using aluminum-laminated film for packaging without opening the battery. These results offer a new approach for monitoring the nucleation of micrometric and submicrometric lithium particles, such as dendritic lithium structures, and is an important step in the development of reliable solid-state batteries.
{"title":"Innovative L-band electron paramagnetic resonance investigation of solid-state pouch cell batteries.","authors":"Charles-Emmanuel Dutoit, Raffaella Soleti, Jean-Marie Doux, Vincent Pelé, Véronique Boireau, Christian Jordy, Simon Pondaven, Hervé Vezin","doi":"10.5194/mr-6-113-2025","DOIUrl":"10.5194/mr-6-113-2025","url":null,"abstract":"<p><p>Usually, conventional electron paramagnetic resonance (EPR) spectroscopy and imaging employ a microwave cavity operating at X-band, i.e., with an excitation frequency of around 9.6 GHz, and this remains the most popular mode for the magnetic characterization of lithium batteries to date. Here, we provide the first low-frequency EPR investigations with respect to monitoring the metallic lithium structures in solid-state pouch cell batteries. We show that L-band, i.e., a microwave frequency of around 1.01 GHz, is an invaluable method to probe the electrode components directly through a standard pouch cell using aluminum-laminated film for packaging without opening the battery. These results offer a new approach for monitoring the nucleation of micrometric and submicrometric lithium particles, such as dendritic lithium structures, and is an important step in the development of reliable solid-state batteries.</p>","PeriodicalId":93333,"journal":{"name":"Magnetic resonance (Gottingen, Germany)","volume":"6 1","pages":"113-118"},"PeriodicalIF":0.0,"publicationDate":"2025-04-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.ncbi.nlm.nih.gov/pmc/articles/PMC12557915/pdf/","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145395931","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}