PMID-sentid	Pub_year	Sent_text		comp_official_name	comp_offsetprotein_name	organism	prot_offset
34862380-4	2021	Using RuO2 as a representative compensated antiferromagnet exhibiting spin-independent conductance along the (001) direction but a non-spin-degenerate Fermi surface, we design a RuO2/TiO2/RuO2 (001) AFMTJ, where a globally spin-neutral charge current is controlled by the relative orientation of the Neel vectors of the two RuO2 electrodes, resulting in the TMR effect as large as ~500%.	ruthenium dioxide	6-10	spindlin 1	Homo sapiens	70-74	
34862380-4	2021	Using RuO2 as a representative compensated antiferromagnet exhibiting spin-independent conductance along the (001) direction but a non-spin-degenerate Fermi surface, we design a RuO2/TiO2/RuO2 (001) AFMTJ, where a globally spin-neutral charge current is controlled by the relative orientation of the Neel vectors of the two RuO2 electrodes, resulting in the TMR effect as large as ~500%.	ruthenium dioxide	6-10	spindlin 1	Homo sapiens	135-139	
34862380-4	2021	Using RuO2 as a representative compensated antiferromagnet exhibiting spin-independent conductance along the (001) direction but a non-spin-degenerate Fermi surface, we design a RuO2/TiO2/RuO2 (001) AFMTJ, where a globally spin-neutral charge current is controlled by the relative orientation of the Neel vectors of the two RuO2 electrodes, resulting in the TMR effect as large as ~500%.	ruthenium dioxide	6-10	spindlin 1	Homo sapiens	223-227	
34862380-4	2021	Using RuO2 as a representative compensated antiferromagnet exhibiting spin-independent conductance along the (001) direction but a non-spin-degenerate Fermi surface, we design a RuO2/TiO2/RuO2 (001) AFMTJ, where a globally spin-neutral charge current is controlled by the relative orientation of the Neel vectors of the two RuO2 electrodes, resulting in the TMR effect as large as ~500%.	ruthenium dioxide	178-182	spindlin 1	Homo sapiens	70-74	
34862380-4	2021	Using RuO2 as a representative compensated antiferromagnet exhibiting spin-independent conductance along the (001) direction but a non-spin-degenerate Fermi surface, we design a RuO2/TiO2/RuO2 (001) AFMTJ, where a globally spin-neutral charge current is controlled by the relative orientation of the Neel vectors of the two RuO2 electrodes, resulting in the TMR effect as large as ~500%.	ruthenium dioxide	178-182	spindlin 1	Homo sapiens	135-139	
34862380-4	2021	Using RuO2 as a representative compensated antiferromagnet exhibiting spin-independent conductance along the (001) direction but a non-spin-degenerate Fermi surface, we design a RuO2/TiO2/RuO2 (001) AFMTJ, where a globally spin-neutral charge current is controlled by the relative orientation of the Neel vectors of the two RuO2 electrodes, resulting in the TMR effect as large as ~500%.	ruthenium dioxide	178-182	spindlin 1	Homo sapiens	223-227	
34862380-4	2021	Using RuO2 as a representative compensated antiferromagnet exhibiting spin-independent conductance along the (001) direction but a non-spin-degenerate Fermi surface, we design a RuO2/TiO2/RuO2 (001) AFMTJ, where a globally spin-neutral charge current is controlled by the relative orientation of the Neel vectors of the two RuO2 electrodes, resulting in the TMR effect as large as ~500%.	ruthenium dioxide	188-192	spindlin 1	Homo sapiens	70-74	
34862380-4	2021	Using RuO2 as a representative compensated antiferromagnet exhibiting spin-independent conductance along the (001) direction but a non-spin-degenerate Fermi surface, we design a RuO2/TiO2/RuO2 (001) AFMTJ, where a globally spin-neutral charge current is controlled by the relative orientation of the Neel vectors of the two RuO2 electrodes, resulting in the TMR effect as large as ~500%.	ruthenium dioxide	188-192	spindlin 1	Homo sapiens	135-139	
34862380-4	2021	Using RuO2 as a representative compensated antiferromagnet exhibiting spin-independent conductance along the (001) direction but a non-spin-degenerate Fermi surface, we design a RuO2/TiO2/RuO2 (001) AFMTJ, where a globally spin-neutral charge current is controlled by the relative orientation of the Neel vectors of the two RuO2 electrodes, resulting in the TMR effect as large as ~500%.	ruthenium dioxide	188-192	spindlin 1	Homo sapiens	223-227	
34862380-4	2021	Using RuO2 as a representative compensated antiferromagnet exhibiting spin-independent conductance along the (001) direction but a non-spin-degenerate Fermi surface, we design a RuO2/TiO2/RuO2 (001) AFMTJ, where a globally spin-neutral charge current is controlled by the relative orientation of the Neel vectors of the two RuO2 electrodes, resulting in the TMR effect as large as ~500%.	ruthenium dioxide	324-328	spindlin 1	Homo sapiens	70-74	
34862380-4	2021	Using RuO2 as a representative compensated antiferromagnet exhibiting spin-independent conductance along the (001) direction but a non-spin-degenerate Fermi surface, we design a RuO2/TiO2/RuO2 (001) AFMTJ, where a globally spin-neutral charge current is controlled by the relative orientation of the Neel vectors of the two RuO2 electrodes, resulting in the TMR effect as large as ~500%.	ruthenium dioxide	324-328	spindlin 1	Homo sapiens	135-139	
34862380-4	2021	Using RuO2 as a representative compensated antiferromagnet exhibiting spin-independent conductance along the (001) direction but a non-spin-degenerate Fermi surface, we design a RuO2/TiO2/RuO2 (001) AFMTJ, where a globally spin-neutral charge current is controlled by the relative orientation of the Neel vectors of the two RuO2 electrodes, resulting in the TMR effect as large as ~500%.	ruthenium dioxide	324-328	spindlin 1	Homo sapiens	223-227