[https://portal.mardi4nfdi.de/wiki/Person:3242071 Ferenc Berencz] table#1 { ["head"] = table#2 { ["vars"] = table#3 { "propertyLabel", "value", "valueLabel", [0] = "property", }, }, ["results"] = table#4 { ["bindings"] = table#5 { [0] = table#6 { ["property"] = table#7 { ["type"] = "uri", ["value"] = "https://portal.mardi4nfdi.de/prop/direct/P200", }, ["propertyLabel"] = table#8 { ["type"] = "literal", ["value"] = "https://portal.mardi4nfdi.de/prop/direct/P200", }, ["value"] = table#9 { ["type"] = "uri", ["value"] = "https://portal.mardi4nfdi.de/entity/Q3226563", }, ["valueLabel"] = table#10 { ["type"] = "literal", ["value"] = "Acta Physica Academiae Scientiarum Hungaricae", ["xml:lang"] = "en", }, }, }, }, } table#1 { ["head"] = table#2 { ["vars"] = table#3 { "subjectLabel", "itemType", [0] = "subject", }, }, ["results"] = table#4 { ["bindings"] = table#5 { }, }, } table#1 { ["head"] = table#2 { ["vars"] = table#3 { "propertyLabel", "value", "valueLabel", [0] = "property", }, }, ["results"] = table#4 { ["bindings"] = table#5 { }, }, } table#1 { ["head"] = table#2 { ["vars"] = table#3 { "propertyLabel", "value", "valueLabel", [0] = "property", }, }, ["results"] = table#4 { ["bindings"] = table#5 { }, }, } table#1 { ["head"] = table#2 { ["vars"] = table#3 { "propertyLabel", "value", "valueLabel", [0] = "property", }, }, ["results"] = table#4 { ["bindings"] = table#5 { [0] = table#6 { ["property"] = table#7 { ["type"] = "uri", ["value"] = "https://portal.mardi4nfdi.de/prop/direct/P223", }, ["propertyLabel"] = table#8 { ["type"] = "literal", ["value"] = "https://portal.mardi4nfdi.de/prop/direct/P223", }, ["value"] = table#9 { ["type"] = "uri", ["value"] = "https://portal.mardi4nfdi.de/entity/Q5820465", }, ["valueLabel"] = table#10 { ["type"] = "literal", ["value"] = "Eigenfunctions ofS2by a Spin Operator Method", ["xml:lang"] = "en", }, }, }, }, }

The relation between Löwdin’s spin projection operator and Pratt’s spin operator