PMC:7594251 / 35423-35790 JSONTXT

{"project":"LitCovid-PD-MONDO","denotations":[{"id":"T21","span":{"begin":72,"end":74},"obj":"Disease"}],"attributes":[{"id":"A21","pred":"mondo_id","subj":"T21","obj":"http://purl.obolibrary.org/obo/MONDO_0019903"}],"text":"In a typical CPMG experiment, the effective transverse relaxation rate, R2,eff, is typically measured by fitting the signal decay as a function of a variable number of CPMG blocks [174]. The experimental half-height linewidth (d) of a given resonance signal is directly related to T2* (also called as ‘effective’ or “observed’’) by the following equation:(1) d=1π T2*"}

{"project":"LitCovid-PD-CLO","denotations":[{"id":"T37945","span":{"begin":3,"end":4},"obj":"http://purl.obolibrary.org/obo/CLO_0001020"},{"id":"T67693","span":{"begin":117,"end":123},"obj":"http://purl.obolibrary.org/obo/SO_0000418"},{"id":"T74144","span":{"begin":133,"end":134},"obj":"http://purl.obolibrary.org/obo/CLO_0001020"},{"id":"T61672","span":{"begin":147,"end":148},"obj":"http://purl.obolibrary.org/obo/CLO_0001020"},{"id":"T776","span":{"begin":233,"end":234},"obj":"http://purl.obolibrary.org/obo/CLO_0001020"},{"id":"T90184","span":{"begin":251,"end":257},"obj":"http://purl.obolibrary.org/obo/SO_0000418"},{"id":"T29187","span":{"begin":281,"end":283},"obj":"http://purl.obolibrary.org/obo/CLO_0050160"},{"id":"T80855","span":{"begin":364,"end":366},"obj":"http://purl.obolibrary.org/obo/CLO_0050160"}],"text":"In a typical CPMG experiment, the effective transverse relaxation rate, R2,eff, is typically measured by fitting the signal decay as a function of a variable number of CPMG blocks [174]. The experimental half-height linewidth (d) of a given resonance signal is directly related to T2* (also called as ‘effective’ or “observed’’) by the following equation:(1) d=1π T2*"}

{"project":"LitCovid-PD-CHEBI","denotations":[{"id":"T345","span":{"begin":281,"end":283},"obj":"Chemical"},{"id":"T347","span":{"begin":364,"end":366},"obj":"Chemical"}],"attributes":[{"id":"A345","pred":"chebi_id","subj":"T345","obj":"http://purl.obolibrary.org/obo/CHEBI_29298"},{"id":"A346","pred":"chebi_id","subj":"T345","obj":"http://purl.obolibrary.org/obo/CHEBI_75710"},{"id":"A347","pred":"chebi_id","subj":"T347","obj":"http://purl.obolibrary.org/obo/CHEBI_29298"},{"id":"A348","pred":"chebi_id","subj":"T347","obj":"http://purl.obolibrary.org/obo/CHEBI_75710"}],"text":"In a typical CPMG experiment, the effective transverse relaxation rate, R2,eff, is typically measured by fitting the signal decay as a function of a variable number of CPMG blocks [174]. The experimental half-height linewidth (d) of a given resonance signal is directly related to T2* (also called as ‘effective’ or “observed’’) by the following equation:(1) d=1π T2*"}

{"project":"LitCovid-sentences","denotations":[{"id":"T247","span":{"begin":0,"end":186},"obj":"Sentence"},{"id":"T248","span":{"begin":187,"end":367},"obj":"Sentence"}],"namespaces":[{"prefix":"_base","uri":"http://pubannotation.org/ontology/tao.owl#"}],"text":"In a typical CPMG experiment, the effective transverse relaxation rate, R2,eff, is typically measured by fitting the signal decay as a function of a variable number of CPMG blocks [174]. The experimental half-height linewidth (d) of a given resonance signal is directly related to T2* (also called as ‘effective’ or “observed’’) by the following equation:(1) d=1π T2*"}