Note 1 to entry: The proper distance DAB is the largest of the Euclidean distances d′AB in all other frames S′ where t′A≠t′B. For inertial frame S′, DAB= γ′ D′AB where γ′ is the Lorentz factor corresponding to the speed between frames S and S′.
Note 2 to entry: For events A and B separated by an infinitesimally small squared space-time interval, the proper distance DAB is the largest of the Euclidean distances d′AB in all frames S′ and DAB= γ′ d′AB.
Note 3 to entry: The proper distance is a Lorentz scalar.
Note 4 to entry: The coherent SI unit of proper distance is metre, m.
Note 1 to entry: The proper distance D AB MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbbjxAHX garuavP1wzZbItLDhis9wBH5garuGqV92AGeKB0LwC1fgarmWu51My VXgarqqtubsr4rNCHbGeaGqipG0dh9qqqrpepC0xbbL8F4rqqrFfpe ea0xe9Lq=Jc9vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0Firpe peKkFr0xfr=xfr=xb9adbaGaamGaciqaaqaaceGaaiGacmqbaaGcba GaamiramaaBaaaleaacaqGbbGaaeOqaaqabaaaaa@3A21@ is the largest of the Euclidean distances d ′ AB MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbbjxAHX garuavP1wzZbItLDhis9wBH5garuGqV92AGeKB0LwC1fgarmWu51My VXgarqqtubsr4rNCHbGeaGqipG0dh9qqqrpepC0xbbL8F4rqqrFfpe ea0xe9Lq=Jc9vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0Firpe peKkFr0xfr=xfr=xb9adbaGaamGaciqaaqaaceGaaiGacmqbaaGcba GabmizayaafaWaaSbaaSqaaiaabgeacaqGcbaabeaaaaa@3A4C@ in all other frames S′ where t ′ A ≠ t ′ B MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbbjxAHX garuavP1wzZbItLDhis9wBH5garuGqV92AGeKB0LwC1fgarmWu51My VXgarqqtubsr4rNCHbGeaGqipG0dh9qqqrpepC0xbbL8F4rqqrFfpe ea0xe9Lq=Jc9vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0Firpe peKkFr0xfr=xfr=xb9adbaGaamGaciqaaqaaceGaaiGacmqbaaGcba GabmiDayaafaWaaSbaaSqaaiaabgeaaeqaaOGaeyiyIKRabmiDayaa faWaaSbaaSqaaiaabkeaaeqaaaaa@3D5F@ . For inertial frame S′, D AB = γ ′ D ′ AB MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbbjxAHX garuavP1wzZbItLDhis9wBH5garuGqV92AGeKB0LwC1fgarmWu51My VXgarqqtubsr4rNCHbGeaGqipG0dh9qqqrpepC0xbbL8F4rqqrFfpe ea0xe9Lq=Jc9vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0Firpe peKkFr0xfr=xfr=xb9adbaGaamGaciqaaqaaceGaaiGacmqbaaGcba GaamiramaaBaaaleaacaqGbbGaaeOqaaqabaGccqGH9aqpcaaMi8Ua aGPaVlqaeo7agaqbaiaaykW7ceWGebGbauaadaWgaaWcbaGaaeyqai aabkeaaeqaaaaa@43AA@ where γ ′ MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbbjxAHX garuavP1wzZbItLDhis9wBH5garuGqV92AGeKB0LwC1fgarmWu51My VXgarqqtubsr4rNCHbGeaGqipG0dh9qqqrpepC0xbbL8F4rqqrFfpe ea0xe9Lq=Jc9vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0Firpe peKkFr0xfr=xfr=xb9adbaGaamGaciqaaqaaceGaaiGacmqbaaGcba Gabq4SdyaafaGaaGPaVdaa@3A76@ is the Lorentz factor corresponding to the speed between frames S and S′.
Note 2 to entry: For events A and B separated by an infinitesimally small squared space-time interval, the proper distance D AB MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbbjxAHX garuavP1wzZbItLDhis9wBH5garuGqV92AGeKB0LwC1fgarmWu51My VXgarqqtubsr4rNCHbGeaGqipG0dh9qqqrpepC0xbbL8F4rqqrFfpe ea0xe9Lq=Jc9vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0Firpe peKkFr0xfr=xfr=xb9adbaGaamGaciqaaqaaceGaaiGacmqbaaGcba GaamiramaaBaaaleaacaqGbbGaaeOqaaqabaaaaa@3A21@ is the largest of the Euclidean distances d ′ AB MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbbjxAHX garuavP1wzZbItLDhis9wBH5garuGqV92AGeKB0LwC1fgarmWu51My VXgarqqtubsr4rNCHbGeaGqipG0dh9qqqrpepC0xbbL8F4rqqrFfpe ea0xe9Lq=Jc9vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0Firpe peKkFr0xfr=xfr=xb9adbaGaamGaciqaaqaaceGaaiGacmqbaaGcba GabmizayaafaWaaSbaaSqaaiaabgeacaqGcbaabeaaaaa@3A4C@ in all frames S′ and D AB = γ ′ d ′ AB .